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Spherical amoebae and a spherical logarithm map

Victor Batyrev Megumi Harada Johannes Hofscheier  and  Kiumars Kaveh
Abstract.

Let GG be a connected reductive algebraic group over \mathbb{C} with a maximal compact subgroup KK. Let G/HG/H be a (quasi-affine) spherical homogeneous space. In the first part of the paper, following Akhiezer’s definition of spherical functions, we introduce a KK-invariant map sLogΓ,t:G/Hs\operatorname{sLog}_{\Gamma,t}:G/H\to\mathbb{R}^{s} which depends on a choice of a finite set Γ\Gamma of dominant weights and s=|Γ|s=|\Gamma|. We call sLogΓ,t\operatorname{sLog}_{\Gamma,t} a spherical logarithm map. We show that when Γ\Gamma generates the highest weight monoid of G/HG/H, the image of the spherical logarithm map parametrizes KK-orbits in G/HG/H. This idea of using the spherical functions to understand the geometry of the space K\G/HK\backslash G/H of KK-orbits in G/HG/H can be viewed as a generalization of the classical Cartan decomposition. In the second part of the paper, we define the spherical amoeba (depending on Γ\Gamma and tt) of a subvariety YY of G/HG/H as sLogΓ,t(Y)\operatorname{sLog}_{\Gamma,t}(Y), and we ask for conditions under which the image of a subvariety YG/HY\subset G/H under sLogΓ,t\operatorname{sLog}_{\Gamma,t} converges, as t0t\to 0, in the sense of Kuratowski to its spherical tropicalization as defined by Tevelev and Vogiannou. We prove a partial result toward answering this question, which shows in particular that the valuation cone is always contained in the Kuratowski limit of the spherical amoebae of G/HG/H. We also show that the limit of the spherical amoebae of G/HG/H is equal to its valuation cone in a number of interesting examples, including when G/HG/H is horospherical, and in the case when G/HG/H is the space of hyperbolic triangles.


Comments are welcomed.

Introduction

Let Y()nY\subset(\mathbb{C}^{*})^{n} be an algebraic subvariety of the nn-dimensional complex algebraic torus. The (classical) amoebae 𝒜t(Y)\mathcal{A}_{t}(Y) of YY, for a varying real parameter tt, have been much studied in the past few decades in several contexts, including in tropical and non-Archimedean geometry. The amoeba 𝒜t(Y)\mathcal{A}_{t}(Y) is defined to be the image of YY under the logarithm map Logt:()nn\operatorname{Log}_{t}:(\mathbb{C}^{*})^{n}\to\mathbb{R}^{n} defined for fixed t>0t>0 by

Logt(x1,,xn):=(logt|x1|,,logt|xn|).\operatorname{Log}_{t}(x_{1},\ldots,x_{n}):=(\log_{t}|x_{1}|,\ldots,\log_{t}|x_{n}|).

Note that the map Logt\operatorname{Log}_{t} is invariant under the action of the compact torus (S1)n()n(S^{1})^{n}\subset(\mathbb{C}^{*})^{n}. In fact, with respect to the isomorphism (x1,,xn)((θ1,,θn),(r1,,rn))(x_{1},\ldots,x_{n})\mapsto((\theta_{1},\ldots,\theta_{n}),(r_{1},\ldots,r_{n})) where xi=rieiθix_{i}=r_{i}e^{i\theta_{i}} between ()n(\mathbb{C}^{*})^{n} and (S1)n×>0n(S^{1})^{n}\times\mathbb{R}_{>0}^{n}, the logarithm map Logt\operatorname{Log}_{t} can be seen to be the projection onto the second component(s), followed by the usual logarithm function rilogtrir_{i}\mapsto\log_{t}r_{i}.

For an algebraic subvariety YY in ()n(\mathbb{C}^{*})^{n}, it is well-known that the amoeba 𝒜t(Y)\mathcal{A}_{t}(Y) stretches to infinity in several directions, also known as its tentacles. These tentacles indicate the directions in which YY approaches infinity, or in other words, they parametrize the orbits at infinity in its tropical compactification. The precise statement is as follows (cf. [Jonsson]): as t0t\to 0, 𝒜t(Y)\mathcal{A}_{t}(Y) converges to the tropical variety trop(Y)\operatorname{trop}(Y) as subsets in n\mathbb{R}^{n}, where convergence is defined here in the sense of Kuratowksi (see Definition 3.3). The theory of amoebae and tropicalization connects classical complex geometry with tropical geometry, which studies piecewise-linear objects in Euclidean space, and the study of these interactions is an active research area.

In this paper, we take initial steps toward generalizing the above to the non-abelian setting. More precisely, we choose to view the complex torus ()n(\mathbb{C}^{*})^{n} as a special case of a spherical homogeneous space in which the group is abelian. We then see whether, or how, the abelian story (as briefly outlined above) might be generalized for non-abelian spherical homogeneous spaces. Before further details, we first briefly recall the setting. Let GG be a complex connected reductive algebraic group. A homogeneous space G/HG/H of GG is called spherical if a Borel subgroup BB of GG has a dense orbit, with respect to the usual action by left multiplication. (See Section 1 for details.) Thus, the complex torus ()n(\mathbb{C}^{*})^{n} is the special case in which G=()nG=(\mathbb{C}^{*})^{n} is the torus itself, H={1}H=\{1\} is the trivial subgroup, and the Borel subgroup BB is again the torus ()n(\mathbb{C}^{*})^{n} itself.

One of our fundamental motivations for this paper is the desire to better understand the KK-orbit space of a spherical homogeneous space G/HG/H as above, where KK is a maximal compact subgroup of GG. Indeed, in the abelian case, the logarithm map Logt\operatorname{Log}_{t} can be viewed as the quotient map of ()n(\mathbb{C}^{*})^{n} by its maximal compact subgroup (S1)n(S^{1})^{n}, and we can view n>0\mathbb{R}^{n}_{>0} as the parameter space of the (S1)n(S^{1})^{n}-orbits in ()n(\mathbb{C}^{*})^{n}. Similarly we may ask whether there exists a non-abelian, or spherical, analogue of the classical logarithm map on G/HG/H which allows us to naturally parametrize the KK-orbit space K\G/HK\backslash G/H of G/HG/H. This problem can be viewed as a generalization of the classical Cartan and polar decompositions in Lie theory. However, as far as we know, there is no general and concrete description of the KK-orbit space K\G/HK\backslash G/H known. (For some important results in this direction see [Knopetal].) A main motivation for the present paper is the belief that there should be a natural isomorphism between K\G/HK\backslash G/H and the real closure of the valuation cone 𝒱G/H\mathcal{V}_{G/H} (see Section 1.1 for the definition) of an arbitrary spherical variety G/HG/H (over \mathbb{C}). In the abelian case, the valuation cone is precisely n\mathbb{R}^{n}, so the logarithm Logt\operatorname{Log}_{t} provides this natural isomorphism. We think of this paper as taking some steps forward in the search of such a natural isomorphism (see also Conjecture 6). (We also note that related ideas have appeared in [Feu].) However, it should be noted that the results we obtain are of a different nature than a direct generalization of the torus case. In contrast to the abelian situation in which Logt\operatorname{Log}_{t} is an isomorphism K\G/H𝒱¯G/HK\backslash G/H\cong\overline{\mathcal{V}}_{G/H}, what we see in our results is that, in the limit as t0t\to 0, the image of our spherical logarithm map sLogt\operatorname{sLog}_{t} (to be defined precisely below) converges in an appropriate sense to the valuation cone. In particular, for fixed tt, our sLogt\operatorname{sLog}_{t} does not provide the desired canonical isomorphism.

In addition to the above, we were motivated by the notion of a spherical tropicalization map associated to a spherical homogeneous space G/HG/H. Spherical tropical geometry was introduced and developed by Tevelev and Vogiannou [Vogiannou] and by the fourth author and Manon [Kaveh-Manon]. We believe that there should be a theory of spherical amoebae for G/HG/H which correspond to the classical amoebae in the abelian case, such that the “spherical amoebae converge to the spherical tropicalization” in an appropriate sense (see also Remark 3.2).

With these motivations in mind, we now describe more precisely the contributions of this article. Let G/HG/H be a spherical homogeneous space as above. For technical reasons we additionally assume that G/HG/H is quasi-affine. (This is not terribly restrictive, as we explain in Remark 1.6.) Let Λ+G/H\Lambda^{+}_{G/H} denote the semigroup of BB-highest-weights of irreducible GG-representations appearing in the coordinate ring [G/H]\mathbb{C}[G/H], considered as a GG-module in the natural way. Following some rather little-known work of Akhiezer [Akhiezer-rk], we define a KK-invariant spherical function ϕλ\phi_{\lambda} on G/HG/H associated to a BB-weight λ\lambda for λΛ+G/H\lambda\in\Lambda^{+}_{G/H}. We normalize these spherical functions by setting ϕλ(eH)=1\phi_{\lambda}(eH)=1. Our first observations concerning Akhiezer’s spherical functions is the following; see Propositions 2.6 and 2.11 for precise statements.

Theorem 1.

Suppose λ1,,λsΛG/H+\lambda_{1},\ldots,\lambda_{s}\in\Lambda_{G/H}^{+} generate Λ+G/H\Lambda^{+}_{G/H} as a semigroup. Then the corresponding spherical functions ϕλ1,,ϕλs\phi_{\lambda_{1}},\ldots,\phi_{\lambda_{s}} generate the algebra of KK-invariant functions on G/HG/H. It follows that the image of the spherical logarithm map corresponding the choice of {λ1,,λs}\{\lambda_{1},\ldots,\lambda_{s}\}, parametrizes the KK-orbit space K\G/HK\backslash G/H. Moreover, the spherical functions separate KK-orbits. More precisely, for any two distinct (hence disjoint) orbits KK-orbits O1O_{1} and O2O_{2} in G/HG/H, there exists some λΛ+G/H\lambda\in\Lambda^{+}_{G/H} such that ϕλ(O1)ϕλ(O2)\phi_{\lambda}(O_{1})\neq\phi_{\lambda}(O_{2}).

Motivated by the above, let Γ={λ1,,λs}Λ+G/H\Gamma=\{\lambda_{1},\ldots,\lambda_{s}\}\subset\Lambda^{+}_{G/H}. We define ΦΓ:G/H0s\Phi_{\Gamma}:G/H\to\mathbb{R}_{\geq 0}^{s} by:

ΦΓ(x)=(ϕλ1(x),,ϕλs(x))\Phi_{\Gamma}(x)=(\phi_{\lambda_{1}}(x),\ldots,\phi_{\lambda_{s}}(x))

(details are in Section 2). For a fixed t>0t>0, we then define the spherical logarithm map (depending on Γ\Gamma and with base tt) to be the map sLogΓ,t:=logt(ΦΓ):G/Hs\operatorname{sLog}_{\Gamma,t}:=\log_{t}(\Phi_{\Gamma}):G/H\to\mathbb{R}^{s} (see Definition 2.12). 111Note that the spherical tropicalization map defined by the fourth author and Manon in [Kaveh-Manon] naturally takes values in a \mathbb{Q}-vector space. However, since our spherical logarithm map uses a logarithm, we need to work with \mathbb{R} coefficients. If we assume that the above subset Γ\Gamma generates Λ+G/H\Lambda^{+}_{G/H} as a semigroup, then from Theorem 1 it follows that we obtain a parametrization of K\G/HK\backslash G/H, i.e., the points in the image sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) parameterize KK-orbits in G/HG/H. This is a positive step in the broader program of understanding K\G/HK\backslash G/H. We will have more to say about the relation between the image of sLogΓ,t\operatorname{sLog}_{\Gamma,t} and the valuation cone 𝒱G/H\mathcal{V}_{G/H} below.

The spherical functions used to define sLogΓ,t\operatorname{sLog}_{\Gamma,t} have somewhat subtle properties. The next result, below, gives an inequality involving a product of two spherical functions. The essential point here is that spherical functions are not necessarily multiplicative: given two BB-weights λ\lambda and μ\mu, in general we can have ϕλϕμϕλ+μ\phi_{\lambda}\phi_{\mu}\neq\phi_{\lambda+\mu} (see Example 2.10). However, it is worth emphasizing that when G/HG/H is horospherical the multiplicativity indeed holds (Lemma 2.5). When G/HG/H is not horospherical, our next result gives some information about the relation between the product ϕλϕμ\phi_{\lambda}\phi_{\mu} and the other spherical functions. To state it, we need the following notation. For a BB-weight λ\lambda, let VλV_{\lambda} denote the irreducible GG-representation with highest weight λ\lambda. Given a GG-module WW we say VλV_{\lambda} appears in WW if the decomposition of WW into irreducible GG-representations contains a copy of VλV_{\lambda}. Here we view [G/H]\mathbb{C}[G/H] as a GG-module. Given VλV_{\lambda} and VμV_{\mu} both appearing in [G/H]\mathbb{C}[G/H], we let VλVμ\langle V_{\lambda}\cdot V_{\mu}\rangle denote the \mathbb{C}-span of the set of products fg[G/H]f\cdot g\in\mathbb{C}[G/H] where fVλf\in V_{\lambda} and gVμg\in V_{\mu}. We have the following; for a precise statement see Proposition 2.9.

Theorem 2.

Suppose VλV_{\lambda} and VμV_{\mu} appear in [G/H]\mathbb{C}[G/H] and suppose VγV_{\gamma} appears in VλVμ[G/H]\langle V_{\lambda}\cdot V_{\mu}\rangle\subseteq\mathbb{C}[G/H]. Then there exists a constant c>0c>0 such that for all xG/Hx\in G/H we have

ϕλ(x)ϕμ(x)cϕγ(x).\phi_{\lambda}(x)\phi_{\mu}(x)\geq c\phi_{\gamma}(x).

In particular, since Vλ+μV_{\lambda+\mu} always appears in VλVμ\langle V_{\lambda}\cdot V_{\mu}\rangle, we see that there is a constant c>0c>0 such that ϕλ(x)ϕμ(x)cϕλ+μ(x)\phi_{\lambda}(x)\phi_{\mu}(x)\geq c\phi_{\lambda+\mu}(x) for all xG/Hx\in G/H.

As we have observed, our definition of sLogΓ,t\operatorname{sLog}_{\Gamma,t} depends on the choice of Γ\Gamma. In the special case when G/HG/H is horospherical and thus the spherical functions are multiplicative, we can define the spherical logarithm map sLogt\operatorname{sLog}_{t} canonically (i.e. independently of the choice of ΓΛ+G/H\Gamma\subset\Lambda^{+}_{G/H}) by

sLogΓ,t(x):=logt(Φ(x)) for xG/H\operatorname{sLog}_{\Gamma,t}(x):=\log_{t}(\Phi(x))\,\,\textup{ for }x\in G/H

where Φ(x)\Phi(x) is defined by Φ(x),λ=ϕλ(x)\langle\Phi(x),\lambda\rangle=\phi_{\lambda}(x), λΛ+G/H\forall\lambda\in\Lambda^{+}_{G/H}. In this case, the image of the map sLogt\operatorname{sLog}_{t} lands naturally in the rr-dimensional vector space 𝒬G/H:=Hom(Λ+G/H,)\mathcal{Q}_{G/H}\otimes\mathbb{R}:=\operatorname{Hom}(\Lambda^{+}_{G/H},\mathbb{R}), where rr is the rank of the spherical variety G/HG/H. This is also the vector space in which the valuation cone 𝒱G/H\mathcal{V}_{G/H} naturally lies (see Section 1, as well as Remark 2.13). As we mentioned above, this paper was partly motivated by the search for a natural isomorphism between K\G/HK\backslash G/H and the valuation cone. Since sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) parametrizes K\G/HK\backslash G/H, it is natural to ask for a relationship between it and 𝒱G/H\mathcal{V}_{G/H}. A choice of generating set ΓΛ+G/H\Gamma\subset\Lambda^{+}_{G/H} gives a linear embedding of the valuation cone 𝒱G/H\mathcal{V}_{G/H} into s\mathbb{R}^{s}, the codomain of sLogΓ,t\operatorname{sLog}_{\Gamma,t} in the general case, given by:

v(v,λ1,,v,λs),v𝒱G/H.v\mapsto(\langle v,\lambda_{1}\rangle,\ldots,\langle v,\lambda_{s}\rangle),\quad v\in\mathcal{V}_{G/H}.

When comparing 𝒱G/H\mathcal{V}_{G/H} with sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) in what follows, we identify 𝒱G/H\mathcal{V}_{G/H} with its image in s\mathbb{R}^{s} under the above embedding.

We now turn to the related question of spherical amoebae. Let YG/HY\subset G/H be a subvariety of G/HG/H. We define the spherical amoeba of YY to be the image sLogΓ,t(Y)\operatorname{sLog}_{\Gamma,t}(Y) of YY under the spherical logarithm. One of our motivations for this manuscript was to ask: do the spherical amoebae approach (in a suitable sense) the spherical tropicalization of YY as t0t\to 0? Of course, as in the classical (abelian) case, one needs to be precise about what the word “approach” means. Following [Jonsson], here we take it to mean the convergence of subsets in the sense of Kuratowski (Definition 3.3). Moreover, in the non-abelian case, the image of the spherical homogeneous space G/HG/H under the spherical tropicalization map is not necessarily the entire codomain; instead, the image is the valuation cone 𝒱G/H\mathcal{V}_{G/H}. This is in contrast to the classical case G=()nG=(\mathbb{C}^{*})^{n}, in which the image is the entire vector space n\mathbb{R}^{n}. We ask the following (cf. Question 3.4):

(1) Under what conditions do the images sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) approach the valuation cone 𝒱G/H\mathcal{V}_{G/H} as t0t\to 0 in the sense of Kuratowski convergence of subsets? (2) For YG/HY\subseteq G/H a subvariety, under what conditions do the spherical amoebae sLogΓ,t(Y)\operatorname{sLog}_{\Gamma,t}(Y) approach strop(Y)\operatorname{strop}(Y) as t0t\to 0 in the sense of Kuratowski convergence of subsets?

In Remark 3.6 we sketch a proof strategy to give a positive answer to Part (1) of the above question; moreover, as we discuss further below, in Section 4 we show that in many examples, the Kuratowski limit of sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) is indeed the valuation cone 𝒱G/H\mathcal{V}_{G/H}. We expect that a proof of Part (2) to be more difficult, and (as in the torus case [Jonsson]), an answer might require tools from non-Archimedean geometry. Nevertheless we conjecture the following.

Conjecture 3.

If G/HG/H is horospherical, and YG/HY\subseteq G/H is a subvariety, then the statement in the Question (2) (as stated above) holds, i.e., the spherical amoebae sLogΓ,t(Y)\operatorname{sLog}_{\Gamma,t}(Y) approaches strop(Y)\operatorname{strop}(Y) in the sense of Kuratowski as t0t\to 0.

We also note that progress on (1) above would partially answer the broad motivating question of finding a relation between K\G/HK\backslash G/H and 𝒱G/H\mathcal{V}_{G/H}. In this paper, we prove some preliminary results which address the question (1) above. Firstly, we answer the “curve case”, as follows. The precise statement is Theorem 3.1.

Theorem 4.

Let vγ𝒱G/Hv_{\gamma}\in\mathcal{V}_{G/H} be the GG-invariant valuation associated to a formal Laurent curve γ\gamma in G/HG/H, convergent for small enough tt. Let λΛ+G/H\lambda\in\Lambda^{+}_{G/H} and let ϕλ:G/H>0\phi_{\lambda}:G/H\to\mathbb{R}_{>0} be the corresponding spherical function. Then for any highest weight vector fλVλ[G/H]f_{\lambda}\in V_{\lambda}\subset\mathbb{C}[G/H] we have

limt0logt(ϕλ(γ(t)))=2vγ(fλ).\lim_{t\to 0}\log_{t}(\phi_{\lambda}(\gamma(t)))=2v_{\gamma}(f_{\lambda}).

Theorem 4 yields the following corollary (see Corollary 3.5).

Corollary 5.

(1) The Kuratowski limit, as t0t\to 0, of the image sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) contains the valuation cone 𝒱G/H\mathcal{V}_{G/H}. (2) When G/HG/H is horospherical, this limit is the entire vector space, which in this case coincides with the valuation cone.

Statement (1) in Corollary 5 shows that 𝒱G/H\mathcal{V}_{G/H} is contained in the Kuratowski limit of the images sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H). When is the limit exactly 𝒱G/H\mathcal{V}_{G/H}? In Section 4, we give some examples for which, with appropriate choices of Γ\Gamma, the images sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) limits to 𝒱G/H\mathcal{V}_{G/H} as t0t\to 0: (i) the basic (quasi) affine space SLn()/U\operatorname{SL}_{n}(\mathbb{C})/U (cf. Example 1.1(4)), (ii) the “group case” with SLn()×SLn()\operatorname{SL}_{n}(\mathbb{C})\times\operatorname{SL}_{n}(\mathbb{C}) acting on SLn()\operatorname{SL}_{n}(\mathbb{C}) (cf. Example 1.1(5)), (iii) SLn()/SLn1()\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}), and (iv) the space of hyperbolic triangles. These examples give some evidence that the answer to the question (1) above may be positive, and hence the KK-orbits K\G/HK\backslash G/H is related, in an appropriate limit, to 𝒱G/H\mathcal{V}_{G/H}. In fact, the first author previously conjectured a tight relation between K\G/HK\backslash G/H and 𝒱G/H\mathcal{V}_{G/H}. Since the conjecture is not recorded elsewhere, we put it here.

Conjecture 6 (Batyrev).

The KK-orbit space K\G/HK\backslash G/H is a stratified manifold with corners where the boundary faces XσX_{\sigma} are in natural bijection with the faces σ\sigma of the valuation cone 𝒱G/H\mathcal{V}_{G/H}, and the stabilizers of the points in the relative interior of XσX_{\sigma} are maximal compact subgroups in the corresponding satellite subgroup of HH (as defined in [Batyrev-Moreau]). Moreover, K\G/HK\backslash G/H is homeomorphic to the valuation cone as a stratified space, i.e., there is a homeomorphism Φ:𝒱G/HK\G/H\Phi:\mathcal{V}_{G/H}\to K\backslash G/H that, for every face σ𝒱G/H\sigma\subset\mathcal{V}_{G/H}, restricts to a homeomorphism between the relative interior of σ\sigma and that of XσX_{\sigma}.

As a special case we also state the following conjecture.

Conjecture 7.

A spherical homogeneous space G/HG/H is horospherical if and only if the KK-orbits space K\G/HK\backslash G/H is homeomorphic to a Euclidean space.

We believe that the spherical logarithm maps sLogΓ,t\operatorname{sLog}_{\Gamma,t} may provide a tool to attack Conjecture 7.

For historical context, we should note here that it has been known for some time that the theory of moment maps from symplectic geometry can be used to parametrize KK-orbits for multiplicity-free spaces. The theory of multiplicity-free Hamiltonian spaces are related to this question of KK-orbits on spherical G/HG/H for the following reason: if XX is smooth spherical variety embedded in a projective space which is equipped with a linear KK-action and a KK-invariant Hermitian structure (and hence has a KK-invariant Kähler structure), then XX is a multiplicity-free Hamiltonian KK-space. Thus, a KK-equivariant embedding of G/HG/H into a projective space gives G/HG/H such a structure. Moreover, for a multiplicity-free Hamiltonian KK-space MM, it is known that the Kirwan map222 The Kirwan map is the composition of the KK-moment map Φ:M𝔨\Phi:M\to\mathfrak{k}^{*} with the quotient map 𝔨/K𝔱+\mathfrak{k}^{*}/K\cong\mathfrak{t}^{*}_{+} where 𝔱\mathfrak{t} denotes the Lie algebra of the (compact) maximal torus TT of KK. provides a parametrization of the KK-orbits in MM (see [Brion-moment, Proposition 5.1]). Thus, this Kirwan map provides another potential approach to Conjectures 6 and 7.

We now outline the contents of the paper. In Section 1 we briefly recall necessary background, including the definition of the spherical tropicalization map as in [Vogiannou, Kaveh-Manon]. Then in Section 2 we define the spherical functions, following Akhiezer, and prove several properties about them. We also define the notion of a spherical logarithm map. In Section 3 we give precise statements of the Kuratowski convergence of subsets, and formulate our questions concerning the convergence of spherical amoebae. We also prove the “curve case” recounted above, as well as the horospherical case. Finally, in Section 4 we compute spherical functions in several important examples, and in some examples, we also give some natural parametrizations of the KK-orbit space K\G/HK\backslash G/H.

Acknowledgements. We would like to thank Dmitri Timashev for invaluably helpful personal discussions and correspondences clarifying several details. In particular, Example 2.10(1) is due to him. We also thank Stéphanie Cupit-Foutou for helpful correspondence (and in particular for Remark 2.8). Some of this work was conducted at the Fields Institute for Research in the Mathematical Sciences during the fourth author’s stay there as a Fields Research Fellow, and we thank the Fields for its support and hospitality. The second author was supported in part by a Natural Science and Engineering Research Council of Canada Discovery Grant and a Canada Research Chair (Tier 2) from the Government of Canada. The fourth author was partially supported by a National Science Foundation Grant (DMS-1601303) and a Simons Collaboration Grant for Mathematicians.

1. Preliminaries on spherical varieties and tropicalization

In this section, we set some notation and briefly review some facts regarding spherical varieties.

1.1. Background on spherical geometry

Let GG be a connected reductive algebraic group over \mathbb{C}. Let BB denote a choice of Borel subgroup BB of GG and let TT be a maximal torus with TBT\subseteq B. The weight lattice of TT is denoted by Λ\Lambda, and the semigroup of dominant weights corresponding to the choice of BB is correspondingly denoted by Λ+\Lambda^{+}. The cone generated by Λ+\Lambda^{+} is the positive Weyl chamber Λ+\Lambda^{+}_{\mathbb{R}}. For a dominant weight λΛ+\lambda\in\Lambda^{+} we denote the irreducible GG-module with highest weight λ\lambda by VλV_{\lambda}. We usually denote a highest weight vector in VλV_{\lambda} by vλv_{\lambda}.

Recall that a normal GG-variety XX is called spherical, or a spherical (GG-)variety, if there exists a dense BB-orbit in XX. (Since all the Borel subgroups are conjugate, this condition is independent of the choice of Borel subgroup BB). A homogeneous space G/H{G/H} is called spherical if it is spherical with respect to the left action of GG on itself by multiplication.

Let XX be a spherical GG-variety and let (X)\mathbb{C}(X) be the field of rational functions on XX. Since GG acts on XX, there is also a natural GG-action on (X)\mathbb{C}(X). We say that f(X)f\in\mathbb{C}(X) is a BB-eigenfunction (sometimes also called BB-semi-invariants) if it has the property that bf=eλ(b)fb\cdot f=e^{\lambda}(b)f for some BB-weight λ\lambda where eλe^{\lambda} denotes the character associated to λ\lambda, i.e., for all xXx\in X we have (bf)(x)=f(b1x)=eλ(b)f(x)(b\cdot f)(x)=f(b^{-1}x)=e^{\lambda}(b)f(x). Let (X)(B)\mathbb{C}(X)^{(B)} denote the set of BB-eigenfunctions in (X)\mathbb{C}(X), and let ΛX\Lambda_{X} denote the subset of Λ\Lambda consisting of all weights arising from BB-eigenfunctions, namely,

ΛX:={λ B-eigenfunction f(X) with bf=eλ(b)f}.\Lambda_{X}:=\{\lambda\,\mid\,\exists\textup{ $B$-eigenfunction }f\in\mathbb{C}(X)\textup{ with }b\cdot f=e^{\lambda}(b)f\}\text{.}

Consider the map (X)(B)Λ\mathbb{C}(X)^{(B)}\to\Lambda associating to a BB-eigenfunction its corresponding weight (in the notation above, the map sends ff to λ\lambda). It is clear that this is a group homomorphism with respect to multiplication in (X)(B)\mathbb{C}(X)^{(B)} and addition in Λ\Lambda and that its image is ΛX\Lambda_{X} by definition. Hence ΛX\Lambda_{X} is a sublattice of Λ\Lambda. Moreover, since XX is spherical and thus there exists an open dense BB-orbit, it follows that this map has kernel precisely the (non-zero) constant functions \cong\mathbb{C}^{*}, thus inducing an isomorphism between (X)(B)/\mathbb{C}(X)^{(B)}/\mathbb{C}^{*} and ΛX\Lambda_{X}.

We briefly recall some standard examples of spherical varieties.

Example 1.1.
  • (1)

    Let G=T=()nG=T=(\mathbb{C}^{*})^{n} be an algebraic torus. In this case, G=B=T=()nG=B=T=(\mathbb{C}^{*})^{n}, and therefore a spherical TT-variety is the same as a toric TT-variety.

  • (2)

    Let X=G/PX=G/P be a partial flag variety, equipped with the usual left action of GG by multiplication. By the Bruhat decomposition, XX is then a spherical GG-variety. This is an example of a projective spherical GG-variety for a non-abelian GG.

  • (3)

    Let G=SL(2,)G=\operatorname{SL}(2,\mathbb{C}) and cnsider the natural action of G=SL(2,)G=\operatorname{SL}(2,\mathbb{C}) on 𝔸2\mathbb{A}^{2} by the usual (left) matrix multiplication. It is straightforward to see that GG acts transitively on 𝔸2{(0,0)}\mathbb{A}^{2}\setminus\{(0,0)\}. Moreover, the stabilizer of the point (1,0)(1,0) is the maximal unipotent subgroup UU of upper triangular matrices in SL(2,)\operatorname{SL}(2,\mathbb{C}) with 11’s on the diagonal. Thus 𝔸2{(0,0)}\mathbb{A}^{2}\setminus\{(0,0)\} can be identified with the homogeneous space G/UG/U. Let BB be the subgroup of upper triangular matrices in SL(2,)\operatorname{SL}(2,\mathbb{C}). Then it is not hard to see that the BB-orbit of the point (0,1)(0,1) is the dense open subset {(x,y)y0}\{(x,y)\mid y\neq 0\} of 𝔸2\mathbb{A}^{2}. Thus, 𝔸2{(0,0)}G/U\mathbb{A}^{2}\setminus\{(0,0)\}\cong G/U is a spherical variety. This is an example of a quasi-affine (but not affine) spherical variety. Similarly, it can be verified that 𝔸n{0}\mathbb{A}^{n}\setminus\{0\} is a spherical variety for the natural action of G=SLn()G=\operatorname{SL}_{n}(\mathbb{C}). (However, for n>2n>2, the SLn()\operatorname{SL}_{n}(\mathbb{C})-stabilizer of a point in 𝔸n{0}\mathbb{A}^{n}\setminus\{0\} is larger than a maximal unipotent subgroup).

  • (4)

    More generally, consider X=G/UX=G/U where UU is a maximal unipotent subgroup of GG, equipped with the left action of GG. Again by the Bruhat decomposition, XX is a spherical GG-variety, and it is well-known that XX is quasi-affine. It is useful to note that there is a natural fiber bundle G/UG/BG/U\to G/B, where BB is the Borel subgroup containing UU, with fiber isomorphic to the torus B/UTB/U\cong T.

  • (5)

    Let X=GX=G and consider the “left-right” action of G×GG\times G on X=GX=G given by (g,h)k=gkh1(g,h)\cdot k=gkh^{-1}. Clearly this action is transitive, and the stabilizer of the identity ee is the diagonal subgroup Gdiag={(g,g)gG}G×GG_{\operatorname{diag}}=\{(g,g)\mid g\in G\}\subseteq G\times G. Thus X=GX=G can be identified with the homogeneous space (G×G)/Gdiag(G\times G)/G_{\operatorname{diag}}. Again from the Bruhat decomposition it follows that X=GX=G is a (G×G)(G\times G)-spherical variety. Here the Borel subgroup of G×GG\times G is chosen to be B×BB\times B^{-}, where BB is a Borel subgroup of GG and BB^{-} is its opposite. The (G×G)(G\times G)-equivariant completions of GG are usually called group compactifications.

For the rest of the paper we restrict attention to the setting of spherical homogeneous spaces, i.e., X=G/HX=G/H. In the setting of spherical homogeneous spaces X=G/HX=G/H, it turns out there is a convenient way to view the sublattice ΛX=ΛG/H\Lambda_{X}=\Lambda_{G/H}, as follows. Choose BB a Borel subgroup so that the BB-orbit of eHG/HeH\in G/H is dense in G/HG/H; such a BB exists since G/HG/H is spherical. Now let SS be a maximal torus in the intersection BHB\cap H and choose TT to be a maximal torus in BB containing SS. Define TG/H:=T/ST_{G/H}:=T/S. It is known that the character lattice of TG/HT_{G/H} can be identified with ΛG/H\Lambda_{G/H}.

We next briefly review the theory of valuations on (G/H)\mathbb{C}(G/H). In this manuscript, by a valuation ν\nu on (G/H)\mathbb{C}(G/H) we will mean a discrete \mathbb{Q}-valued valuation on (G/H)/\mathbb{C}(G/H)/\mathbb{C}, i.e., we assume

  1. (1)

    ν:(G/H)\nu:\mathbb{C}(G/H)^{*}\to\mathbb{Q} and ν(0)=\nu(0)=\infty,

  2. (2)

    ν((G/H))\nu(\mathbb{C}(G/H)^{*})\cong\mathbb{Z} or {0}\{0\},

  3. (3)

    ν()=0\nu(\mathbb{C}^{*})=0,

  4. (4)

    ν(fg)=ν(f)+ν(g)\nu(fg)=\nu(f)+\nu(g),

  5. (5)

    ν(f+g)min{ν(f),ν(g)}\nu(f+g)\geq\min\{\nu(f),\nu(g)\}.

A valuation v:(G/H){0}v:\mathbb{C}(G/H)\setminus\{0\}\to\mathbb{Q} is GG-invariant if for any gGg\in G and f(G/H)f\in\mathbb{C}(G/H) we have v(f)=v(gf)v(f)=v(g\cdot f). We define

(1) 𝒱G/H:={ G-invariant valuations on (G/H)}.\mathcal{V}_{G/H}:=\{\textup{ $G$-invariant valuations on }\mathbb{C}(G/H)\}.

From the Luna-Vust theory, it is known that any GG-invariant valuation in the sense explained above is a geometric valuation, or more precisely, is induced by (up to multiplying by a constant in \mathbb{Q}) a divisor (i.e. is the order of vanishing along a divisor).

Example 1.2.

Let G=T=()nG=T=(\mathbb{C}^{*})^{n} and H={1}H=\{1\}. Then G/H=()nG/H=(\mathbb{C}^{*})^{n}. For any vector wnw\in\mathbb{Q}^{n} we can construct a G=TG=T-invariant valuation vwv_{w} as follows. For f=αcαxα[G/H][T][x1±,,xn±]f=\sum_{\alpha}c_{\alpha}x^{\alpha}\in\mathbb{C}[G/H]\cong\mathbb{C}[T]\cong\mathbb{C}[x_{1}^{\pm},\ldots,x_{n}^{\pm}] we define

vw(f):=min{wαcα0}.v_{w}(f):=\min\{w\cdot\alpha\,\mid\,c_{\alpha}\neq 0\}.

Then vwv_{w} extends to the field of rational functions (G/H)\mathbb{C}(G/H) and this is easily checked to be TT-invariant.

Let vv be a GG-invariant valuation. By the definition of valuations, ν\nu gives rise to a homomorphism ν:(G/H)(B)\nu:\mathbb{C}(G/H)^{(B)}\to\mathbb{Q}, where the group operation on (G/H)(B)\mathbb{C}(G/H)^{(B)} is multiplication of functions. Moreover, by assumption, the valuation evaluates trivially on constant functions, so in fact we obtain a group homomorphism (G/H)(B)/\mathbb{C}(G/H)^{(B)}/\mathbb{C}^{*}\to\mathbb{Q}. The identification (G/H)(B)/ΛG/H\mathbb{C}(G/H)^{(B)}/\mathbb{C}^{*}\cong\Lambda_{G/H} above then allows us to view this as a linear map ΛG/H\Lambda_{G/H}\to\mathbb{Q}. We denote this linear map by ρ(v)Hom(ΛG/H,)\rho(v)\in\operatorname{Hom}(\Lambda_{G/H},\mathbb{Q}). We introduce the notation 𝒬G/H:=Hom(ΛG/H,)\mathcal{Q}_{G/H}:=\operatorname{Hom}(\Lambda_{G/H},\mathbb{Q}) for this \mathbb{Q}-vector space. With this notation, the correspondence vρ(v)Hom(ΛG/H,)v\mapsto\rho(v)\in\operatorname{Hom}(\Lambda_{G/H},\mathbb{Q}) is a mapping

(2) ρ:𝒱G/H𝒬G/H:=Hom(ΛG/H,).\rho:\mathcal{V}_{G/H}\to\mathcal{Q}_{G/H}:=\operatorname{Hom}(\Lambda_{G/H},\mathbb{Q}).

The following is well-known [Luna-Vust, 7.4 Prop].

Theorem 1.3.

With the assumptions as above, the map ρ:𝒱G/H𝒬G/H\rho:\mathcal{V}_{G/H}\to\mathcal{Q}_{G/H} is injective, i.e., a GG-invariant valuation is uniquely determined by its restriction to the BB-eigenfunctions.

Due to the above theorem, we may henceforth identify 𝒱G/H\mathcal{V}_{G/H} with its image ρ(𝒱G/H)𝒬G/H\rho(\mathcal{V}_{G/H})\subseteq\mathcal{Q}_{G/H}.

Note there is a natural pairing between GG-invariant valuations and the lattice ΛG/H\Lambda_{G/H} given by v,λ:=ρ(v)(λ)\langle v,\lambda\rangle:=\rho(v)(\lambda).

Example 1.4.

Continuing Example 1.2, the lattice ΛG/H\Lambda_{G/H} in the case G/H=T=()nG/H=T=(\mathbb{C}^{*})^{n} is isomorphic to n\mathbb{Z}^{n}. The BB-semi-invariant functions (G/H)(B)=(T)(T)\mathbb{C}(G/H)^{(B)}=\mathbb{C}(T)^{(T)} are the monomials xα=x1α1x2α2xnαnx^{\alpha}=x_{1}^{\alpha_{1}}x_{2}^{\alpha_{2}}\cdots x_{n}^{\alpha_{n}}, and the monomial xαx^{\alpha} corresponds to the B=TB=T-weight α=(α1,,αn)nΛG/H\alpha=(\alpha_{1},\ldots,\alpha_{n})\in\mathbb{Z}^{n}\cong\Lambda_{G/H}. In this special case, it is straightforward to explicitly compute the natural pairing described above. For a G(=T)G(=T)-invariant valuation vwv_{w} as constructed in Example 1.2, the element ρ(vw)Hom(ΛG/H,)\rho(v_{w})\in\operatorname{Hom}(\Lambda_{G/H},\mathbb{Q}) sends α\alpha to νw(xα)=wα\nu_{w}(x^{\alpha})=w\cdot\alpha (by definition of vwv_{w}), i.e., the usual dot product of wnw\in\mathbb{Q}^{n} with αn\alpha\in\mathbb{Z}^{n}.

The following result is due to Brion [VUGen] and Knop [WeylMom].

Theorem 1.5.

The set 𝒱G/H\mathcal{V}_{G/H} is a co-simplicial cone in the vector space 𝒬G/H\mathcal{Q}_{G/H}. Moreover, it is the fundamental domain for the action of a Weyl group of a root system. More precisely, there exists a set of simple roots β1,,β\beta_{1},\ldots,\beta_{\ell} in this root system such that the cone 𝒱G/H\mathcal{V}_{G/H} is defined by:

𝒱G/H={v𝒬G/Hv,βi0,i=1,,}\mathcal{V}_{G/H}=\{v\in\mathcal{Q}_{G/H}\mid\langle v,\beta_{i}\rangle\leq 0,~{}\forall i=1,\ldots,\ell\}

where the pairing ,\langle\cdot,\cdot\rangle is the one described above, and the βi\beta_{i} lie in ΛG/H\Lambda_{G/H}.

The set of simple roots {β1,,β}\{\beta_{1},\ldots,\beta_{\ell}\} is called the system of spherical roots of G/HG/H. This Weyl group of the spherical root system is also called the little Weyl group of G/HG/H.

Henceforth, we additionally assume that the spherical variety G/HG/H is quasi-affine.

Remark 1.6.

This assumption is not severe. Following [Akhiezer-rk] one can show that, by adding an extra \mathbb{C}^{*} component if necessary, we can assume that G/HG/H is quasi-affine. More precisely, let G~=G×\tilde{G}=G\times\mathbb{C}^{*}. Take a character χ:H\chi:H\to\mathbb{C}^{*} and define H~={(h,χ(h))hH}G~\tilde{H}=\{(h,\chi(h))\mid h\in H\}\subset\tilde{G}. The homogeneous space G~/H~\tilde{G}/\tilde{H} is spherical for the action of G~\tilde{G}. In fact, if BB is a Borel such that BHBH is open in GG then B~H~\tilde{B}\tilde{H} is open in G~\tilde{G} where B~=B×\tilde{B}=B\times\mathbb{C}^{*}. Also, one can show that for a suitable choice of a character χ\chi, the homogeneous space G~/H~\tilde{G}/\tilde{H} can be equivariantly embedded in some finite dimensional G~\tilde{G}-module [Humphreys, Section 11.2] and is thus quasi-affine. The projection G~G\tilde{G}\to G, (g,z)g(g,z)\mapsto g, induces a GG-equivariant morphism G~/H~G/H\tilde{G}/\tilde{H}\to G/H which is a fiber bundle with fibers isomorphic to \mathbb{C}^{*}.

Assuming that G/HG/H is quasi-affine, let [G/H]\mathbb{C}[G/H] denote the ring of regular functions on G/HG/H. When [G/H]\mathbb{C}[G/H] is considered as a GG-representation in the natural manner, it is known that [G/H]\mathbb{C}[G/H] can be decomposed into finite-dimensional irreducible GG-representations (see e.g. [Timashev, Appendix p.250]) so we have

(3) [G/H]λWλ\mathbb{C}[G/H]\cong\bigoplus_{\lambda}W_{\lambda}

where WλW_{\lambda} denotes the λ\lambda-isotypic component of [G/H]\mathbb{C}[G/H]. When G/HG/H is quasi-affine, sphericity of G/HG/H is equivalent to the ring of regular functions 𝒪(G/H)\mathcal{O}(G/H) being a multiplicity-free GG-module [Timashev, Theorem 25.1(MF5)]. The decomposition above motivates the following definition.

Definition 1.7.

Assuming that G/HG/H is quasi-affine, we define Λ+G/H\Lambda^{+}_{G/H} to be the set of highest weights in Λ+\Lambda^{+} which appear in the decomposition (3), i.e., the set of λ\lambda for which Wλ0W_{\lambda}\neq 0 in the RHS of (3). Thus, by definition we have [G/H]λΛ+G/HWλ\mathbb{C}[G/H]\cong\oplus_{\lambda\in\Lambda^{+}_{G/H}}W_{\lambda}. Moreover, since G/HG/H is spherical, each WλW_{\lambda} for λΛ+G/H\lambda\in\Lambda^{+}_{G/H} is an irreducible GG-module.

We denote by ΛG/H\Lambda_{G/H} the sublattice of Λ\Lambda generated by Λ+G/H\Lambda^{+}_{G/H}. There is an analogue of the usual dominant order for the sublattice ΛG/H\Lambda_{G/H}, defined as follows. Let λ,μΛG/H\lambda,\mu\in\Lambda_{G/H}. We say that λG/Hμ\lambda\geq_{G/H}\mu if μλ\mu-\lambda is a linear combination of the spherical roots with nonnegative coefficients. We call >G/H>_{G/H} the spherical dominant order. One has the following [Knop-LV, Section 5].

Theorem 1.8.

Let G/HG/H be a quasi-affine spherical homogeneous space. Let [G/H]λΛG/H+Wλ\mathbb{C}[G/H]\cong\bigoplus_{\lambda\in\Lambda_{G/H}^{+}}W_{\lambda} be the ring of regular functions on G/HG/H. Let fWλf\in W_{\lambda}, gWμg\in W_{\mu}. Then the product fgfg lies in

γG/Hλ+μWγ.\bigoplus_{\gamma\geq_{G/H}\lambda+\mu}W_{\gamma}.

Let λ,μΛG/H+\lambda,\mu\in\Lambda_{G/H}^{+} and let WνW_{\nu} appear in the product WλWμW_{\lambda}W_{\mu}, where here WλWμW_{\lambda}W_{\mu} denotes the span of all products of the form fgfg for fWλ,gWμf\in W_{\lambda},g\in W_{\mu}. For such a triple λ,μ,νΛG/H+\lambda,\mu,\nu\subset\Lambda_{G/H}^{+}, we call the weight λ+μν\lambda+\mu-\nu a tail. The tail cone 𝒯G/H\mathcal{T}_{G/H} of G/HG/H is defined to be the closure of the cone in ΛG/H\Lambda_{G/H}\otimes\mathbb{Q} generated by all the tails. We have the following (see e.g. [Knop-LV, Lemma 5.1]).

Proposition 1.9.

Let G/HG/H be a quasi-affine spherical homogeneous space. Then the tail cone 𝒯G/H\mathcal{T}_{G/H} is the dual cone to the (negative of the) valuation cone, 𝒱G/H-\mathcal{V}_{G/H}.

Remark 1.10.

From Theorem 1.5 and Theorem 1.8, we see that the set of spherical roots generates the tail cone 𝒯G/H\mathcal{T}_{G/H} of G/HG/H.

1.2. Spherical tropicalization

We start by recalling the notions of a germ of a curve and a formal curve (see for example [Timashev, Section 24]). We let 𝒪=[[t]]\mathcal{O}=\mathbb{C}[[t]] denote the algebra of formal power series with coefficients in \mathbb{C} and 𝒦=((t))\mathcal{K}=\mathbb{C}((t)) its field of fractions, i.e. the field of formal Laurent series with finitely many negative exponents. If f𝒦f\in\mathcal{K} we denote by ordt(f)\operatorname{ord}_{t}(f) the order of tt in the Laurent series ff. Clearly ordt\operatorname{ord}_{t} is a \mathbb{Z}-valued valuation on the field 𝒦\mathcal{K}.

Let XX be a variety. A formal curve γ\gamma on XX is a 𝒦\mathcal{K}-point of XX. An 𝒪\mathcal{O}-point on XX is called a convergent formal curve. The limit of a convergent formal curve is the point on X()X(\mathbb{C}) obtained by setting t=0t=0 in γ\gamma. If we assume XX is embedded in an affine space 𝔸N\mathbb{A}^{N} then a formal curve γ\gamma on XX is an NN-tuple of Laurent series satisfying the defining equations of XX in 𝔸N\mathbb{A}^{N}. If γ\gamma is convergent then its coordinates are power series and their constant terms are the coordinates of the limit point γ0=limt0γ(t)\gamma_{0}=\lim_{t\to 0}\gamma(t).

Definition 1.11 (Valuation associated to a formal curve).

A formal curve γ\gamma on XX defines a valuation v^γ:(X){0}{}\hat{v}_{\gamma}:\mathbb{C}(X)\setminus\{0\}\to\mathbb{Z}\cup\{\infty\} as follows.

(4) v^γ(f)=ordt(f(γ(t))).\hat{v}_{\gamma}(f)=\operatorname{ord}_{t}(f(\gamma(t))).

We recall that the algebraic closure 𝒦¯\overline{\mathcal{K}} of the field 𝒦\mathcal{K} is the field of formal Puiseux series with coefficients in \mathbb{C}, the elements of which are formal series

γ(t)=c1ta1+c2ta2+c3ta3+\gamma(t)=c_{1}t^{a_{1}}+c_{2}t^{a_{2}}+c_{3}t^{a_{3}}+\cdots

where the cic_{i} are non-zero complex numbers for all ii, and a1<a2<a3<a_{1}<a_{2}<a_{3}<\cdots are rational numbers that have a common denominator. (Sometimes 𝒦¯\overline{\mathcal{K}} is denoted as {{t}}\mathbb{C}\{\{t\}\} in the literature.) We call a point in X(𝒦¯)X(\overline{\mathcal{K}}) a formal Puiseux curve or simply a Puiseux curve on XX. Definition 1.11 extends naturally to Puiseux curves. That is, a formal Puiseux curve γ\gamma on XX gives a valuation v^γ:(X){}\hat{v}_{\gamma}:\mathbb{C}(X)\to\mathbb{Q}\cup\{\infty\}, defined by the same equation (4).

Now we restrict attention to the case of spherical varieties and GG-invariant valuations. Following the setting in the previous section, we assume G/HG/H is a quasi-affine spherical homogeneous space. The main ingredient in the definition of spherical tropicalization, Definition 1.13 below, is the construction of a GG-invariant valuation from a given arbitrary valuation on G/H{G/H}. The following well-known result is key (see [Knop-LV, Lemma 1.4], [Sumihiro, Lemma 10 and 11], [Luna-Vust, 3.2 Lemme]).

Theorem 1.12 (Sumihiro).

Let G/HG/H be a quasi-affine spherical homogeneous space. Let v:(G/H){0}v:\mathbb{C}({G/H})\setminus\{0\}\to\mathbb{Q} be a valuation.

  • (1)

    For every 0f(G/H)0\neq f\in\mathbb{C}({G/H}), there exists a nonempty Zariski-open subset UfGU_{f}\subset G such that the value v(gf)v(g\cdot f) is the same for all gUfg\in U_{f}. We denote this value by v¯(f)\bar{v}(f), i.e.

    v¯(f):=v(gf),gUf.\bar{v}(f):=v(g\cdot f),\quad\forall g\in U_{f}.
  • (2)

    For v¯\bar{v} defined as above, we have v¯(f)=min{v(gf)gG}\bar{v}(f)=\min\{v(g\cdot f)\mid g\in G\}.

  • (3)

    v¯\bar{v} is a GG-invariant valuation on G/H{G/H}.

Recall that a formal curve γ\gamma on G/H{G/H} gives rise to a valuation v^γ\hat{v}_{\gamma}. We let vγv_{\gamma} denote the GG-invariant valuation constructed by Theorem 1.12 from v^γ\hat{v}_{\gamma}. Concretely,

vγ(f)=ordt(f(gγ(t)))v_{\gamma}(f)=\operatorname{ord}_{t}(f(g\cdot\gamma(t)))

for every f(G/H){0}f\in\mathbb{C}(G/H)\setminus\{0\} and gUfg\in U_{f} is the dense open set in GG given in Theorem 1.12(1). By Theorem 1.12 we know vγv_{\gamma} is a GG-invariant valuation, i.e., vγ𝒱G/Hv_{\gamma}\in\mathcal{V}_{G/H}.

Definition 1.13.

Let G/HG/H be a quasi-affine spherical homogeneous space. Following [Vogiannou], we call the map

strop:G/H(𝒦¯)𝒱G/H,γvγ,\operatorname{strop}:G/H(\overline{\mathcal{K}})\to\mathcal{V}_{G/H},\quad\gamma\mapsto v_{\gamma},

the spherical tropicalization map.

As in Section 1, it follows from Luna-Vust theory that the map strop\operatorname{strop} is surjective.

Example 1.14.

Let X=𝔸2{(0,0)}X=\mathbb{A}^{2}\setminus\{(0,0)\}, equipped with the natural action of G=SL(2,)G=\operatorname{SL}(2,\mathbb{C}) as in Example 1.1(3). Thus XSL2()/UX\cong\operatorname{SL}_{2}(\mathbb{C})/U and the algebra of regular functions [X]=[𝔸2{(0,0)}\mathbb{C}[X]=\mathbb{C}[\mathbb{A}^{2}\setminus\{(0,0)\} is the polynomial ring [x,y]\mathbb{C}[x,y]. It is not difficult to see that ΛG/H\Lambda_{G/H} coincides with the weight lattice Λ\Lambda\cong\mathbb{Z} of SL2()SL_{2}(\mathbb{C}). Indeed, the function f(x,y)=yf(x,y)=y on X=𝔸2{(0,0)}X=\mathbb{A}^{2}\setminus\{(0,0)\} is a BB-eigenfunction in [X]=[x,y]\mathbb{C}[X]=\mathbb{C}[x,y] whose BB-weight is 11. Let γ=(γ1,γ2)\gamma=(\gamma_{1},\gamma_{2}) be a formal curve in X=𝔸2{0}X=\mathbb{A}^{2}\setminus\{0\}, where γ1(t)=iaiti\gamma_{1}(t)=\sum_{i}a_{i}t^{i} and γ2(t)=ibiti\gamma_{2}(t)=\sum_{i}b_{i}t^{i} are elements of 𝒦=((t))\mathcal{K}=\mathbb{C}((t)). Let g=[g11g12g21g22]g=\left[\begin{matrix}g_{11}&g_{12}\\ g_{21}&g_{22}\end{matrix}\right]. We compute that f(gγ(t))=g21γ1+g22γ2f(g\cdot\gamma(t))=g_{21}\gamma_{1}+g_{22}\gamma_{2}. From the construction of the GG-invariant valuation vγv_{\gamma} above, we know vγ(y)=ordt(f(gγ(t)))v_{\gamma}(y)=\operatorname{ord}_{t}(f(g\cdot\gamma(t))) for gUfg\in U_{f} for some Zariski-open subset. It follows that

(5) vγ(y)=min(ordt(γ1(t)),ordt(γ2(t)).v_{\gamma}(y)=\min(\operatorname{ord}_{t}(\gamma_{1}(t)),\operatorname{ord}_{t}(\gamma_{2}(t)).

There is another way of understanding the GG-invariant valuation associated to a formal curve and that is through the generalized Cartan decomposition for spherical varieties. It goes back to Luna and Vust ([Luna-Vust]). A proof of it can also be found in [Gaitsgory-Nadler, Theorem 8.2.9].

Theorem 1.15 (Generalized non-Archimedean Cartan decomposition for spherical varieties over 𝒦\mathcal{K}).

The G(𝒪)G(\mathcal{O})-orbits in G/H(𝒦){G/H}(\mathcal{K}) are parameterized by ΛˇG/H𝒱G/H\check{\Lambda}_{G/H}\cap\mathcal{V}_{G/H}. Here ΛˇG/H𝒬G/H\check{\Lambda}_{G/H}\subset\mathcal{Q}_{G/H} denotes the lattice dual to the BB-weight lattice ΛG/H\Lambda_{G/H}, and a cocharacter λΛˇG/H\lambda\in\check{\Lambda}_{G/H} corresponds to the G(𝒪)G(\mathcal{O})-orbit through the formal curve λ(t)TG/H(𝒦)\lambda(t)\in T_{G/H}(\mathcal{K}).

Thus the valuation vγv_{\gamma} can be interpreted as the valuation represented by the point of intersection of the G(𝒪)G(\mathcal{O})-obit of γ\gamma in G/H(𝒦){G/H}(\mathcal{K}) and the image of valuation cone 𝒱G/H\mathcal{V}_{G/H} (under the exponential map) in G/H(𝒦){G/H}(\mathcal{K}).

Example 1.16 (non-Archimedean Cartan decomposition).

As in Example 1.1(5) consider GG with left-right action of G×GG\times G. Theorem 1.15 applied in this case recovers the a non-Archimedean version of the usual Cartan decomposition (see [Iwahori]). With notation as above, it states that:

G(𝒦)=G(𝒪)Λˇ+G(𝒪).G(\mathcal{K})=G(\mathcal{O})\cdot\check{\Lambda}^{+}\cdot G(\mathcal{O}).

Here Λˇ\check{\Lambda} is the cocharacter lattice and Λˇ+\check{\Lambda}^{+} is the intersection of Λˇ\check{\Lambda} with the dual positive Weyl chamber. We regard both as subsets of T(𝒦)T(\mathcal{K}).

When G=GL(n,)G=\operatorname{GL}(n,\mathbb{C}) the above non-Archimedean Cartan decomposition gives the well-known Smith normal form of a matrix (over the field of formal Laurent series 𝒦\mathcal{K} which is the field of fractions of the principal ideal domain 𝒪\mathcal{O}, the ring of formal power series).

Example 1.17 (Non-Archimedean Iwasawa decomposition).

As in Example 1.1(4) consider the spherical homogeneous space G/UG/U where UU is a maximal unipotent subgroup of GG. In this case Theorem 1.15 gives a non-Archimdean version of the Iwasawa decompostion (see [Iwahori]). It states that:

G(𝒦)=G(𝒪)ΛˇU(𝒦),G(\mathcal{K})=G(\mathcal{O})\cdot\check{\Lambda}\cdot U(\mathcal{K}),

where as in the previous example, Λˇ\check{\Lambda} is the dual lattice to the weight lattice Λ\Lambda and we regard it as a subset of T(𝒦)T(\mathcal{K}).

2. Spherical functions, the spherical logarithm, and separating KK-orbits

In this section, following Akhiezer [Akhiezer-rk], we define certain KK-invariant real-valued functions on a spherical homogeneous space. As in Section 1, we assume throughout that G/HG/H is a quasi-affine spherical homogeneous space. Let KK be a maximal compact subgroup of GG.

Let VλV_{\lambda} be a (non-zero) irreducible GG-representation in [G/H]\mathbb{C}[G/H]. Fix a KK-invariant Hermitian product ,\langle\cdot,\cdot\rangle on Vλ[G/H]V_{\lambda}\subset\mathbb{C}[G/H]. Let {fλ,i}Vλ\{f_{\lambda,i}\}\subset V_{\lambda} be an orthonormal basis with respect to this KK-invariant Hermitian product. Define the function ϕλ:G/H>0\phi_{\lambda}\colon G/H\to\mathbb{R}_{>0} by:

(6) ϕλ(x)=i|fλ,i(x)|2.\phi_{\lambda}(x)=\sum_{i}|f_{\lambda,i}(x)|^{2}\text{.}
Lemma 2.1.

ϕλ(eH)0\phi_{\lambda}(eH)\neq 0.

Proof.

Suppose ϕλ(eH)=0\phi_{\lambda}(eH)=0. From the definition it follows that fλ,i(eH)=0f_{\lambda,i}(eH)=0 for all ii. Since VλV_{\lambda} is a GG-representation, for any fixed jj, we know gfλ,jg\cdot f_{\lambda,j} is a linear combination of fλ,if_{\lambda,i}’s, but this implies (gfλ,j)(eH):=fλ,j(g1H)=0(g\cdot f_{\lambda,j})(eH):=f_{\lambda,j}(g^{-1}H)=0 also. Since this was true of any jj, we conclude that ϕλ(g1H)=0\phi_{\lambda}(g^{-1}H)=0 for all gGg\in G. This implies fλ,i0f_{\lambda,i}\equiv 0 as functions on G/HG/H, for all ii. This is a contradiction, since VλV_{\lambda} is a non-zero representation. ∎

By the above lemma, we may normalize our choice of ϕλ\phi_{\lambda} so that it satisfies

ϕλ(eH)=1,λΛ+G/H.\phi_{\lambda}(eH)=1,\quad\forall\lambda\in\Lambda^{+}_{G/H}\text{.}
Remark 2.2.

It is not hard to see that, with respect to any KK-invariant Hermitian product ,\langle\cdot,\cdot\rangle on VλV_{\lambda}, two TT-weight vectors corresponding to different TT-weights must be orthogonal with respect to ,\langle\cdot,\cdot\rangle. Thus we may assume without loss of generality that the orthonormal basis {fλ,i}\{f_{\lambda,i}\} consists of TT-weight vectors.

The following lemma is straightforward.

Lemma 2.3.

The function ϕλ\phi_{\lambda} is KK-invariant, and independent of the chosen orthonormal basis {fλ,i}\{f_{\lambda,i}\}.

We call the function ϕλ\phi_{\lambda} the spherical function associated to the highest weight λΛ+G/H\lambda\in\Lambda^{+}_{G/H}. Before stating the next result we need some preliminaries. First we consider the algebra of KK-invariants ([G/H][G/H]¯)K(\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]})^{K}. By multiplication of functions, we have a natural map [G/H][G/H]¯[G/H][G/H]¯\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]}\to\mathbb{C}[G/H]\cdot\overline{\mathbb{C}[G/H]} where the target denotes the \mathbb{C}-span of all \mathbb{C}-valued functions on G/HG/H of the form fg¯f\cdot\bar{g} where f,g[G/H]f,g\in\mathbb{C}[G/H]. It is possible to see, using the fact that holomorphic functions are determined by their values on any non-empty open neighborhood, and the independence of holomorphic and anti-holomorphic variables ziz_{i} and z¯i\bar{z}_{i} in some local coordinates, that this map is an isomorphism. Therefore, in what follows, we will slightly abuse notation and sometimes write [G/H][G/H]¯\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]} and sometimes write its image [G/H][G/H]¯\mathbb{C}[G/H]\cdot\overline{\mathbb{C}[G/H]}. In both cases, the GG-action is given by a diagonal GG-action on each factor, and the identification is GG-equivariant.

The following is a result of Akhiezer [Akhiezer-rk, Lemma 3].

Proposition 2.4.

[Akhiezer-rk, Lemma 3] The set of functions {ϕλλΛ+G/H}\left\{\phi_{\lambda}\mid\lambda\in\Lambda^{+}_{G/H}\right\} is a basis for ([G/H][G/H]¯)K(\mathbb{C}[G/H]\cdot\overline{\mathbb{C}[G/H]})^{K} as a vector space over \mathbb{C}. In particular,

(7) ([G/H][G/H]¯)K=λΛ+G/Hϕλ.(\mathbb{C}[G/H]\cdot\overline{\mathbb{C}[G/H]})^{K}=\bigoplus_{\lambda\in\Lambda^{+}_{G/H}}\mathbb{C}\,\phi_{\lambda}.
Proof.

The inclusion “\supset” follows by Lemma 2.3. For the reverse inclusion, first observe that

([G/H][G/H]¯)K=λ1,λ2ΛG/H+(Vλ1V¯λ2)Kλ1,λ2ΛG/H+HomK(Vλ2,Vλ1)\mathopen{}\mathclose{{}\left(\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]}}\right)^{K}=\bigoplus_{\lambda_{1},\lambda_{2}\in\Lambda_{G/H}^{+}}\mathopen{}\mathclose{{}\left(V_{\lambda_{1}}\otimes\overline{V}_{\lambda_{2}}}\right)^{K}\cong\bigoplus_{\lambda_{1},\lambda_{2}\in\Lambda_{G/H}^{+}}\operatorname{Hom}_{K}(V_{\lambda_{2}},V_{\lambda_{1}})

where HomK(Vλ2,Vλ1)\operatorname{Hom}_{K}(V_{\lambda_{2}},V_{\lambda_{1}}) denotes the set of KK-equivariant module homomorphisms and where we have used the fact that, for any rational KK-module VV, the complex conjugate KK-module V¯\overline{V} is isomorphic to the dual KK-module VV^{*} (the isomorphism depends on the choice of a KK-invariant Hermitian product on VV). By Schur’s lemma, HomK(Vλ2,Vλ1)\operatorname{Hom}_{K}(V_{\lambda_{2}},V_{\lambda_{1}})\cong\mathbb{C} if λ1=λ2\lambda_{1}=\lambda_{2} and HomK(Vλ1,Vλ2)={0}\operatorname{Hom}_{K}(V_{\lambda_{1}},V_{\lambda_{2}})=\{0\} otherwise. Thus we conclude that ([G/H][G/H]¯)KλΛ+G/HHomK(Vλ,Vλ)(\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]})^{K}\cong\bigoplus_{\lambda\in\Lambda^{+}_{G/H}}\operatorname{Hom}_{K}(V_{\lambda},V_{\lambda}). Since HomK(Vλ,Vλ)\operatorname{Hom}_{K}(V_{\lambda},V_{\lambda})\cong\mathbb{C} for each λΛ+G/H\lambda\in\Lambda^{+}_{G/H} we see that the claim will follow if we can show that ϕλ\phi_{\lambda} lies in the image VλVλ¯V_{\lambda}\otimes\overline{V_{\lambda}} of VλVλ¯V_{\lambda}\otimes\overline{V_{\lambda}} under the multiplication map and that it is non-zero. But this follows from the definition (6) of ϕλ\phi_{\lambda} and Lemma 2.1. ∎

Multiplication of spherical functions can be understood in terms of the tail cone, as follows.

Lemma 2.5.

Let λ,μΛG/H+\lambda,\mu\in\Lambda_{G/H}^{+}. Then

ϕλϕμ=λ+μγ𝒯G/HΛcγϕγ,\phi_{\lambda}\cdot\phi_{\mu}=\sum_{\lambda+\mu-\gamma\in\mathcal{T}_{G/H}\cap\Lambda}c_{\gamma}\phi_{\gamma}\text{,}

for coefficients cγc_{\gamma}\in\mathbb{R}. Moreover, we have cλ+μ0c_{\lambda+\mu}\neq 0.

Proof.

We follow the proof of Proposition 2.4. We have:

(8) ϕλϕμ(VλV¯λ)K(VμV¯μ)K(VλVμV¯λV¯μ)K,λ+μγ,λ+μγ are tails (VγV¯γ)K, by Theorem 1.8λ+μγ is a tail (VγV¯γ)K\begin{split}\phi_{\lambda}\phi_{\mu}\in(V_{\lambda}\overline{V}_{\lambda})^{K}(V_{\mu}\overline{V}_{\mu})^{K}&\subset(V_{\lambda}V_{\mu}\overline{V}_{\lambda}\overline{V}_{\mu})^{K},\\ &\subset\bigoplus_{\lambda+\mu-\gamma,\lambda+\mu-\gamma^{\prime}\textup{ are tails }}(V_{\gamma}\overline{V}_{\gamma^{\prime}})^{K},\quad\textup{ by Theorem~{}\ref{th-coor-ring-multiplication-spherical}}\\ &\subset\bigoplus_{\lambda+\mu-\gamma\textup{ is a tail }}(V_{\gamma}\overline{V}_{\gamma})^{K}\\ \end{split}

where the last inclusion is by Schur’s lemma and the fact that the multiplication map [G/H][G/H]¯[G/H][G/H]¯\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]}\to\mathbb{C}[G/H]\cdot\overline{\mathbb{C}[G/H]} is an isomorphism (so we may identify VγVγ¯V_{\gamma}\overline{V_{\gamma^{\prime}}} with VγVγ¯V_{\gamma}\otimes\overline{V_{\gamma^{\prime}}}). This proves the first claim. To prove that cλ+μ0c_{\lambda+\mu}\neq 0, we consider the space

(9) λ+μγ is a tailVγVγ¯\bigoplus_{\lambda+\mu-\gamma\textup{ is a tail}}V_{\gamma}\otimes\overline{V_{\gamma}}

(so this is the space appearing above, before taking KK-invariants) as a TK×TKT_{K}\times T_{K}-representation, for TKT_{K} a maximal torus of KK. From Theorem 1.8 and the definition of a tail, we know that γλ+μ\gamma\leq\lambda+\mu in the usual dominance order for any γ\gamma that appears in the direct sum (9). Since for γ\gamma any weight, VγV_{\gamma} denotes the irreducible GG-representation with highest weight γ\gamma, it follows that the highest TK×TKT_{K}\times T_{K}-weight that can appear in (9) is (λ+μ,(λ+μ))(\lambda+\mu,-(\lambda+\mu)) (where the partial ordering is (λ,μ)>(λ,μ)(\lambda,-\mu)>(\lambda^{\prime},-\mu^{\prime}) if λ>λ,μ>μ\lambda>\lambda^{\prime},\mu>\mu^{\prime} in the usual dominance order). Moreover, from the above it follows that the only summand in (9) which contains (λ+μ,(λ+μ))(\lambda+\mu,-(\lambda+\mu)) as a TK×TKT_{K}\times T_{K}-weight is Vλ+μVλ+μ¯V_{\lambda+\mu}\otimes\overline{V_{\lambda+\mu}}, i.e. the term corresponding to γ=λ+μ\gamma=\lambda+\mu.

Recall that the spherical function ϕλ+μ\phi_{\lambda+\mu} is a sum fλ+μ,if¯λ+μ,i\sum f_{\lambda+\mu,i}\overline{f}_{\lambda+\mu,i} (identified with fλ+μ,if¯λ+μ,i\sum f_{\lambda+\mu,i}\otimes\overline{f}_{\lambda+\mu,i}), where {fλ+μ,i}\{f_{\lambda+\mu,i}\} is a basis of TT-weight vectors in Vλ+μV_{\lambda+\mu}. In particular, ϕλ+μ\phi_{\lambda+\mu} has a non-zero component in the one-dimensional TK×TKT_{K}\times T_{K}-weight space of weight (λ+μ,(λ+μ))(\lambda+\mu,-(\lambda+\mu)), i.e. the highest-weight space of Vλ+μVλ+μ¯V_{\lambda+\mu}\otimes\overline{V_{\lambda+\mu}}. It follows from the above discussion that in order to determine whether cλ+μ0c_{\lambda+\mu}\neq 0, it suffices to show that ϕλϕμ\phi_{\lambda}\phi_{\mu} has a non-zero component in the TK×TKT_{K}\times T_{K}-weight space in (9) of weight (λ+μ,(λ+μ))(\lambda+\mu,-(\lambda+\mu)). For the following we temporarily denote by fλf_{\lambda} (respectively fμf_{\mu}) the highest weight vector of TKT_{K}-weight λ\lambda (respectively μ\mu) in VλV_{\lambda} (respectively VμV_{\mu}). By definition, ϕλ=fλfλ¯+ terms with TK-weight <(λ,λ)\phi_{\lambda}=f_{\lambda}\overline{f_{\lambda}}+\textup{ terms with $T_{K}$-weight $<(\lambda,-\lambda)$} and similarly for ϕμ\phi_{\mu}. Hence ϕλϕμ=fλfλ¯fμfμ¯+ terms with TK×TK-weight <(λ+μ,(λ+μ))\phi_{\lambda}\phi_{\mu}=f_{\lambda}\overline{f_{\lambda}}f_{\mu}\overline{f_{\mu}}+\textup{ terms with $T_{K}\times T_{K}$-weight $<(\lambda+\mu,-(\lambda+\mu))$}. Since fλfλ¯fμfμ¯f_{\lambda}\overline{f_{\lambda}}f_{\mu}\overline{f_{\mu}} has weight (λ+μ,(λ+μ))(\lambda+\mu,-(\lambda+\mu)) and is non-zero, and all other terms are strictly smaller, there can be no cancellation and we conclude cλ+μ0c_{\lambda+\mu}\neq 0 as desired. ∎

Proposition 2.6.

If λ1,,λsΛG/H+\lambda_{1},\ldots,\lambda_{s}\in\Lambda_{G/H}^{+} generate Λ+G/H\Lambda^{+}_{G/H} as a semigroup, then ϕλ1,,ϕλs\phi_{\lambda_{1}},\ldots,\phi_{\lambda_{s}} generate ([G/H][G/H]¯)K(\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]})^{K} as an algebra.

Proof.

The proof is a standard “canceling the leading term argument”. First we consider the case where GG is semi-simple. One can construct a well-ordering >> on the semigroup Λ+G/H\Lambda^{+}_{G/H} respecting the addition, such that if λ1λ2\lambda_{1}-\lambda_{2} is a non-negative combination of spherical roots then λ1>λ2\lambda_{1}>\lambda_{2}. Take a vector ξ\xi in the interior of the dual cone to the positive Weyl chamber. Moreover, assume that ξ\xi is irrational, that is, for any nonzero weight λ\lambda, ξ,λ0\langle\xi,\lambda\rangle\neq 0. For two weights λ\lambda, μ\mu define λ>μ\lambda>\mu if and only if ξ,λ>ξ,μ\langle\xi,\lambda\rangle>\langle\xi,\mu\rangle. It is easy to see that >> has the required properties.

For f([G/H][G/H]¯)Kf\in(\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]})^{K} let f=λcλϕλf=\sum_{\lambda}c_{\lambda}\phi_{\lambda} and define

v(f)=min{λcλ0}.v(f)=\min\{\lambda\mid c_{\lambda}\neq 0\}.

For convenience we will write ϕi\phi_{i} instead of ϕλi\phi_{\lambda_{i}} for i=1,,si=1,\ldots,s. Suppose by contradiction that there exists f([G/H][G/H]¯)Kf\in(\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]})^{K} that cannot be represented as a polynomial in the ϕi\phi_{i} and v(f)v(f) is minimum among all such KK-invariant functions. Then since λ1,,λs\lambda_{1},\ldots,\lambda_{s} generate Λ+G/H\Lambda^{+}_{G/H} we can find ki0k_{i}\geq 0 such that v(f)=v(iϕiki)v(f)=v(\prod_{i}\phi_{i}^{k_{i}}). It follows that there is 0c0\neq c\in\mathbb{C} such that v(fciϕiki)<v(f)v(f-c\prod_{i}\phi_{i}^{k_{i}})<v(f). Thus fciϕikif-c\prod_{i}\phi_{i}^{k_{i}}, and hence ff, can be represented as a polynomial in the ϕi\phi_{i}. The contradiction proves the claim.

Next suppose GG is reductive. Replacing GG with a finite cover if necessary we can assume that G=G×ZG=G^{\prime}\times Z where GG^{\prime} is connected semisimple and ZZ is the connected component of the center of GG. Then as semigroups Λ+G=Λ+GΛZ\Lambda^{+}_{G}=\Lambda^{+}_{G^{\prime}}\oplus\Lambda_{Z}, where ΛZ\Lambda_{Z} is the character lattice of the torus ZZ. One shows from the definitions that if λΛ+GΛ+G/H\lambda\in\Lambda^{+}_{G^{\prime}}\cap\Lambda^{+}_{G/H} and γΛZΛ+G/H\gamma\in\Lambda_{Z}\cap\Lambda^{+}_{G/H} then

(10) ϕλ+γ=ϕλϕγ.\phi_{\lambda+\gamma}=\phi_{\lambda}\phi_{\gamma}.

The claim follows from (10) and the cancelation of the leading terms argument as in the semisimple case. ∎

Remark 2.7.

Let hλVλ[G/H]h_{\lambda}\in V_{\lambda}\subset\mathbb{C}[G/H] be a nonzero function. Consider the function h~λ\tilde{h}_{\lambda} obtained by averaging hλhλ¯h_{\lambda}\overline{h_{\lambda}} over KK, i.e.,

h~λ(x)=Khλ(kx)hλ(kx)¯dk,\tilde{h}_{\lambda}(x)=\int_{K}h_{\lambda}(k\cdot x)\overline{h_{\lambda}(k\cdot x)}\mathop{}\!\mathrm{d}k\text{,}

where dk\mathop{}\!\mathrm{d}k is the Haar measure on KK. Since (the span of) VλVλ¯V_{\lambda}\overline{V_{\lambda}} is a finite-dimensional vector space, the integral h~λ\tilde{h}_{\lambda} is still an element in VλVλ¯[G/H][G/H]¯\langle V_{\lambda}\overline{V_{\lambda}}\rangle\subseteq\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]}, and is KK-invariant by construction. From Proposition 2.4, it follows that h~λ\tilde{h}_{\lambda} is a scalar multiple of ϕλ\phi_{\lambda}.

Remark 2.8 (Highest weight monoid not necessarily free).

In general, the highest weight monoid Λ+G/H\Lambda^{+}_{G/H} may not be freely generated as a monoid. Here is an example which was communicated to us by Stéphanie Cupit-Foutou and is inspired by [Luna, §6.3]. Let G1=G2=SL2G_{1}=G_{2}=\operatorname{SL}_{2} and for i=1,2i=1,2 let TiT_{i} be a maximal tori of GiG_{i} and NiN_{i} its normalizer in GiG_{i}. Now let G=G1×G2G=G_{1}\times G_{2} and H=ker(c1c2)H=\operatorname{ker}(c_{1}c_{2}) where c1c_{1}, c2c_{2} are the non-trivial characters of N1N_{1} and N2N_{2} respectively. Then G/HG/H is spherical and affine, and its weight monoid is not free: it is generated by 2ϖ12\varpi_{1}, 2ϖ22\varpi_{2} and ϖ1+ϖ2\varpi_{1}+\varpi_{2} where ϖi\varpi_{i} denotes the fundamental weight for GiG_{i}.

Proposition 2.9.

Let λ,μ,γΛ+G/H\lambda,\mu,\gamma\in\Lambda^{+}_{G/H} and suppose λ+μγ\lambda+\mu-\gamma is a tail, i.e. VγV_{\gamma} appears in VλVμ[G/H]\mathopen{}\mathclose{{}\left\langle V_{\lambda}V_{\mu}}\right\rangle\subset\mathbb{C}[G/H], then there is constant c>0c>0 such that for all xG/Hx\in G/H we have:

ϕλ(x)ϕμ(x)cϕγ(x).\phi_{\lambda}(x)\phi_{\mu}(x)\geq c\phi_{\gamma}(x).
Proof.

By definition ϕλ=i|fλ,i|2\phi_{\lambda}=\sum_{i}|f_{\lambda,i}|^{2} and ϕμ=j|fμ,j|2\phi_{\mu}=\sum_{j}|f_{\mu,j}|^{2} where {fλ,i}\{f_{\lambda,i}\}, {fμ,j}\{f_{\mu,j}\} are orthonormal bases for VλV_{\lambda}, VμV_{\mu} respectively. Let {fγ,k}\{f_{\gamma,k}\} be an orthonormal basis for VγV_{\gamma}. As VγVλVμV_{\gamma}\subseteq\langle V_{\lambda}V_{\mu}\rangle, we can write fγ,k=i,jaijkfλ,ifμ,jf_{\gamma,k}=\sum_{i,j}a_{ijk}f_{\lambda,i}f_{\mu,j} for some aijka_{ijk}\in\mathbb{C}. For xG/Hx\in G/H, it follows that

k|fγ,k(x)|2=k|i,jaijkfλ,i(x)fμ,j(x)|2i,jk|aijkfλ,i(x)fμ,j(x)|2=i,j|fλ,i(x)fμ,j(x)|k|aijk|2ai,j|fλ,i(x)fμ,j(x)|ai,j|fλ,i(x)|2i,j|fμ,j(x)|2=adim(Vλ)dim(Vμ)i|fλ,i(x)|2j|fμ,j(x)|2\sqrt{\sum_{k}|f_{\gamma,k}(x)|^{2}}=\sqrt{\sum_{k}\Big{|}\sum_{i,j}a_{ijk}f_{\lambda,i}(x)f_{\mu,j}(x)\Big{|}^{2}}\leq\sum_{i,j}\sqrt{\sum_{k}|a_{ijk}f_{\lambda,i}(x)f_{\mu,j}(x)|^{2}}\\ =\sum_{i,j}|f_{\lambda,i}(x)f_{\mu,j}(x)|\sqrt{\sum_{k}|a_{ijk}|^{2}}\leq a\sum_{i,j}|f_{\lambda,i}(x)f_{\mu,j}(x)|\\ \leq a\sqrt{\sum_{i,j}|f_{\lambda,i}(x)|^{2}}\sqrt{\sum_{i,j}|f_{\mu,j}(x)|^{2}}=a\sqrt{\dim(V_{\lambda})\dim(V_{\mu})}\sqrt{\sum_{i}|f_{\lambda,i}(x)|^{2}}\sqrt{\sum_{j}|f_{\mu,j}(x)|^{2}}\\

where amax{k|aijk|2}a\coloneqq\max\{\sqrt{\sum_{k}|a_{ijk}|^{2}}\}, the first inequality is the triangle inequality and the third inequality is the Cauchy-Schwarz inequality. Squaring both sides we obtain ϕγ(x)(const)ϕλ(x)ϕμ(x)\phi_{\gamma}(x)\leq(const)\cdot\phi_{\lambda}(x)\phi_{\mu}(x) where the constant is >0>0, so by dividing we obtain the claim. ∎

The following examples show that spherical functions ϕλ\phi_{\lambda} need not be multiplicative. More precisely, for λ,μΛ+G/H\lambda,\mu\in\Lambda^{+}_{G/H}, ϕλ+μ\phi_{\lambda+\mu} is not necessarily a scalar multiple of ϕλϕμ\phi_{\lambda}\phi_{\mu}.

Example 2.10.

(1) This example is due to Dmitri Timashev. Let n3n\geq 3 and let G=SLn()G=\operatorname{SL}_{n}(\mathbb{C}) and H=SLn1()H=\operatorname{SL}_{n-1}(\mathbb{C}). Then it can be shown that G/HG/H is a spherical variety and can be realized as the affine variety in n×(n)\mathbb{C}^{n}\times(\mathbb{C}^{n})^{*} defined by the equation v,w=1\langle v,w\rangle=1. (All facts claimed here without proof are shown in Section 4.4.) It turns out that Λ+G/H\Lambda^{+}_{G/H} is generated by χ1=ω1,χ2=ωn1\chi_{1}=\omega_{1},\chi_{2}=\omega_{n-1}, corresponding to the standard representation n\mathbb{C}^{n} of SLn()\operatorname{SL}_{n}(\mathbb{C}) and its dual. Let ϕ1:=ϕχ1\phi_{1}:=\phi_{\chi_{1}} and ϕ2:=ϕχ2\phi_{2}:=\phi_{\chi_{2}} be the corresponding spherical functions. We wish to compare the product ϕ1ϕ2\phi_{1}\phi_{2} with the spherical function ϕχ1+χ2=ϕω1+ωn1\phi_{\chi_{1}+\chi_{2}}=\phi_{\omega_{1}+\omega_{n-1}} corresponding to Vω+ωn1V_{\omega_{+}\omega_{n-1}}.

Let {e1,,en}\{e_{1},\ldots,e_{n}\} and {e1,,en}\{e_{1}^{*},\ldots,e_{n}^{*}\} denote the standard basis of n\mathbb{C}^{n} and its dual basis of (n)(\mathbb{C}^{n})^{*} respectively. The action of SLn()SL_{n}(\mathbb{C}) on the coordinate ring

[x1,,xn,y1,,yn]/i=1nxiyi=1\mathbb{C}[x_{1},\ldots,x_{n},y_{1},\ldots,y_{n}]/\langle\sum_{i=1}^{n}x_{i}y_{i}=1\rangle

is the standard one, viewing x1,,xnx_{1},\ldots,x_{n} (respectively y1,,yny_{1},\ldots,y_{n}) as the coordinates on n\mathbb{C}^{n} (respectively (n)(\mathbb{C}^{n})^{*}) corresponding to {e1,,en}\{e_{1},\ldots,e_{n}\} (respectively {e1,,en}\{e_{1}^{*},\ldots,e_{n}^{*}\}). It is not difficult to see that the span of the {x1,,xn}\{x_{1},\ldots,x_{n}\} (respectively {y1,,yn}\{y_{1},\ldots,y_{n}\}) yields a representation of SLn()SL_{n}(\mathbb{C}) isomorphic to (n)(\mathbb{C}^{n})^{*}, the dual of the standard representation (respectively n\mathbb{C}^{n}, the standard representation). The corresponding spherical functions are therefore ϕ1(v,w)=i=1n|xi|2\phi_{1}(v,w)=\sum_{i=1}^{n}|x_{i}|^{2}, where xix_{i} are the coordinates of vv, and ϕ2(v,w)=i=1n|yi|2\phi_{2}(v,w)=\sum_{i=1}^{n}|y_{i}|^{2}, where yiy_{i} are the coordinates of ww. Hence their product is i,j|xiyj|2\sum_{i,j}|x_{i}y_{j}|^{2}.

Next we wish to compute the spherical function corresponding to χ1+χ2\chi_{1}+\chi_{2}. Since the irreducible SLn()\operatorname{SL}_{n}(\mathbb{C})-representation of highest weight ω1+ωn1\omega_{1}+\omega_{n-1} is the adjoint representation 𝔰𝔩n()\mathfrak{sl}_{n}(\mathbb{C}), we can proceed as follows. Suppose there exists a GG-equivariant embedding Ψ:G/HVω1+ωn1\Psi:G/H\to V_{\omega_{1}+\omega_{n-1}}^{*}. This induces a GG-equivariant map backwards (Vω1+ωn1)Vω1+ωn1[G/H]λΛG/H+Vλ(V_{\omega_{1}+\omega_{n-1}}^{*})^{*}\cong V_{\omega_{1}+\omega_{n-1}}\to\mathbb{C}[G/H]\cong\oplus_{\lambda\in\Lambda_{G/H}^{+}}V_{\lambda}. (Note that Vω1+ωn1=Vw0(ω1+ωn1)Vω1+ωn1V_{\omega_{1}+\omega_{n-1}}=V_{-w_{0}(\omega_{1}+\omega_{n-1})}\cong V^{*}_{\omega_{1}+\omega_{n-1}} so in our example we may identify Vω1+ωn1V_{\omega_{1}+\omega_{n-1}}^{*} with Vω1+ωn1V_{\omega_{1}+\omega_{n-1}}.) Provided that the embedding is nontrivial, by Schur’s Lemma this map must take Vω1+ωn1V_{\omega_{1}+\omega_{n-1}} to the (isomorphic copy of) Vω1+ωn1V_{\omega_{1}+\omega_{n-1}} appearing in the decomposition of [G/H]\mathbb{C}[G/H] into irreducible GG-modules. The spherical function ϕλ\phi_{\lambda} is then the pullback via the embedding Ψ\Psi of the sum of the norm-squares of the coordinates on Vω1+ωn1V_{\omega_{1}+\omega_{n-1}} (with respect to some SU(n)SU(n)-invariant inner product on 𝔰𝔩n()\mathfrak{sl}_{n}(\mathbb{C})). The Hermitian inner product X,Ytrace(XY)X,Y\mapsto\mathrm{trace}(XY^{*}) on 𝔰𝔩n()\mathfrak{sl}_{n}(\mathbb{C}) is U(n)U(n)-invariant with respect to the adjoint action of SLn()\operatorname{SL}_{n}(\mathbb{C}). Next, notice that the map Ψ:(v,w)vw1n𝐈𝐝n×n\Psi:(v,w)\mapsto v\otimes w-\frac{1}{n}\mathbf{Id}_{n\times n} gives a GG-equivariant morphism from SLn()/SLn1()\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}) to 𝔰𝔩n()\mathfrak{sl}_{n}(\mathbb{C}), where we view n(n)\mathbb{C}^{n}\otimes(\mathbb{C}^{n})^{*} as 𝔤𝔩n()\mathfrak{gl}_{n}(\mathbb{C}). Thus we obtain

(11) ϕω1+ωn(v,w)= pullback of Xtrace(XX) by Ψ=trace((vw1n𝐈𝐝n×n)(vw1n𝐈𝐝n×n))=v2w21n=(i,jxi2yj2)1n\begin{split}\phi_{\omega_{1}+\omega_{n}}(v,w)&=\textup{ pullback of $X\mapsto\mathrm{trace}(XX^{*})$ by $\Psi$}\\ &=\mathrm{trace}((v\otimes w-\frac{1}{n}\mathbf{Id}_{n\times n})^{*}(v\otimes w-\frac{1}{n}\mathbf{Id}_{n\times n}))\\ &=\|v\|^{2}\|w\|^{2}-\frac{1}{n}\\ &=(\sum_{i,j}\|x_{i}\|^{2}\|y_{j}\|^{2})-\frac{1}{n}\end{split}

which is clearly not proportional to ϕ1ϕ2\phi_{1}\phi_{2}.

(2) (Group case) Consider GG as a (G×G)(G\times G)-spherical homogeneous space. Let BB be a Borel subgroup of GG and take B×BB\times B^{-} as Borel subgroup of G×GG\times G where BB^{-} denotes the opposite Borel subgroup to BB. Then the highest weight semigroup of GG is {(λ,λ)λΛ+}Λ+×Λ\{(\lambda,-\lambda)\mid\lambda\in\Lambda^{+}\}\subset\Lambda^{+}\times\Lambda^{-}. For λΛ+\lambda\in\Lambda^{+} let us write ϕλ\phi_{\lambda} in place of the spherical function ϕ(λ,λ)\phi_{(\lambda,-\lambda)}. By reasoning similar to that in example (1) above, we have

ϕλ(g)=tr(πλ(g)πλ(g)),\phi_{\lambda}(g)=\text{tr}(\pi_{\lambda}(g)\pi_{\lambda}(g)^{*}),

where πλ:GEnd(Vλ)\pi_{\lambda}:G\to\text{End}(V_{\lambda}) is the irreducible representation of GG with highest weight λ\lambda and * stands for the Hermitian adjunction with respect to some KK-invariant Hermitian product on the representation space VλV_{\lambda}. It follows that if gg lies in the real locus of a split maximal torus TGT^{\prime}\subset G, then ϕλ(g)=tr(πλ(g)πλ(g))=tr(πλ(g2))=χλ(g2)\phi_{\lambda}(g)=\text{tr}(\pi_{\lambda}(g)\pi_{\lambda}(g))=\text{tr}(\pi_{\lambda}(g^{2}))=\chi_{\lambda}(g^{2}) where χλ\chi_{\lambda} denotes the character of the representation πλ\pi_{\lambda}. But one knows that the product of characters is the character of tensor product. This shows that the multiplicativity does not hold for the ϕλ\phi_{\lambda}.

Proposition 2.11.

Let G/HG/H be a quasi-affine spherical homogeneous space. Then the spherical functions ϕλ\phi_{\lambda}, λΛG/H+\lambda\in\Lambda_{G/H}^{+}, separate KK-orbits in G/HG/H. More precisely, for any two distinct (hence disjoint) KK-orbits O1O_{1} and O2O_{2} in G/HG/H, then there exists some λΛ+G/H\lambda\in\Lambda^{+}_{G/H} such that ϕλ(O1)ϕλ(O2)\phi_{\lambda}(O_{1})\neq\phi_{\lambda}(O_{2}).

Proof.

Since G/HG/H is quasi-affine, there exists a GG-equivariant embedding G/Hm=2mG/H\hookrightarrow\mathbb{C}^{m}=\mathbb{R}^{2m} for some mm, where m\mathbb{C}^{m} is equipped with a linear GG-action (see [Popov-Vinberg, Section 1.2]). Let O1,O2G/HO_{1},O_{2}\subset G/H be two distinct KK-orbits. Since KK is compact, both O1,O2O_{1},O_{2} are compact. As disjoint compact subsets of an affine space, by Urysohn’s lemma, there exists a continuous, real-valued function ff on 2m\mathbb{R}^{2m} such that f(O1)=0f(O_{1})=0 and f(O2)=1f(O_{2})=1. By the Stone approximation theorem (see e.g. [Cheney, Chapter 6]), there exists a real polynomial pp on 2m\mathbb{R}^{2m} that approximates ff arbitrarily well on any compact subset. Since KK acts linearly on the ambient m\mathbb{C}^{m}, we can average this polynomial by integrating over KK and obtain a KK-invariant real polynomial pp that separates O1O_{1} and O2O_{2}. The restriction of pp to G/HG/H belongs to ([G/H][G/H]¯)K=λΛ+G/Hϕλ(\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]})^{K}=\bigoplus_{\lambda\in\Lambda^{+}_{G/H}}\mathbb{C}\,\phi_{\lambda} and hence we conclude that there is some ϕλ\phi_{\lambda} that separates O1O_{1} and O2O_{2} as required. ∎

Let Γ={λ1,,λs}Λ+G/H\Gamma=\{\lambda_{1},\ldots,\lambda_{s}\}\subset\Lambda^{+}_{G/H} be a set of semigroup generators of Λ+G/H\Lambda^{+}_{G/H}. We have seen in Proposition 2.6 that the collection of associated spherical functions ϕλ1,ϕλ2,,ϕλs\phi_{\lambda_{1}},\phi_{\lambda_{2}},\cdots,\phi_{\lambda_{s}} are algebra generators of the subalgebra ([G/H][G/H]¯)K(\mathbb{C}[G/H]\otimes\overline{\mathbb{C}[G/H]})^{K}. Thus, it follows from Proposition 2.11 that they also separate KK-orbits. Thus, this set of spherical functions plays an important role in understanding the geometry of KK-orbits of G/HG/H, and motivates the following definition of the spherical logarithm map.

Definition 2.12.

Let Γ={λ1,,λs}Λ+G/H\Gamma=\{\lambda_{1},\ldots,\lambda_{s}\}\subseteq\Lambda^{+}_{G/H} be a set of semigroup generators of Λ+G/H\Lambda^{+}_{G/H} and let ϕλ1,,ϕλ2\phi_{\lambda_{1}},\cdots,\phi_{\lambda_{2}} denote the corresponding spherical functions. We define

sLogA,t(x):=(logtϕλ1(x),,logtϕλs(x)).\operatorname{sLog}_{A,t}(x):=(\log_{t}\phi_{\lambda_{1}}(x),\ldots,\log_{t}\phi_{\lambda_{s}}(x)).

We call this the spherical logarithm map associated to Γ={λ1,,λs}\Gamma=\{\lambda_{1},\ldots,\lambda_{s}\}.

Remark 2.13.

We already noted in the introduction that when G/HG/H is horospherical, we can define a spherical logarithm map canonically, independent of a choice of Γ\Gamma. In fact, we can say more: in the horospherical case, we also do not need to assume that G/HG/H is quasi-affine. Here we briefly sketch how to define the spherical logarithm map without quasi-affineness.

First consider an rr-dimensional torus S()rS\cong(\mathbb{C}^{*})^{r} with character lattice ΛS\Lambda_{S} and maximal compact torus KS(S1)rSK_{S}\cong(S^{1})^{r}\subset S. Then there is a canonical logarithm map Log:SHom(ΛS,)r\operatorname{Log}:S\to\operatorname{Hom}(\Lambda_{S},\mathbb{R})\cong\mathbb{R}^{r} defined as follows: for xSx\in S, let Log(x)\operatorname{Log}(x) be the homomorphism of ΛS\Lambda_{S} that sends any character λΛS\lambda\in\Lambda_{S} to log(|λ(x)|)\log(|\lambda(x)|), where log\log denotes the natural logarithm. For t>0t>0, we then define Logt(x):=(1/logt)Log(x)\operatorname{Log}_{t}(x):=(1/\log t)\operatorname{Log}(x). It is clear that Logt\operatorname{Log}_{t} is KSK_{S}-invariant for any t>0t>0.

We now return to the spherical setting. Suppose G/HG/H is horospherical. In this case it is known that P=NG(H)P=N_{G}(H) is a parabolic subgroup. Moreover, for a Levi decomposition P=PuLP=P_{u}L of PP, we have H=PuL0H=P_{u}L_{0} for some subgroup L0L_{0} where LL0LL^{\prime}\subset L_{0}\subset L and LL^{\prime} denotes the commutator subgroup of LL [Timashev, Lemma 7.4]. It follows that the quotient group S:=P/HS:=P/H is abelian and hence a torus. For π:G/HG/P\pi:G/H\to G/P the natural projection, we then see that all the fibers of π\pi are tori isomorphic to SS, and in particular, π1(eP)=S\pi^{-1}(eP)=S. Now let KK be a maximal compact subgroup of GG such that KP=GKP=G. Then KK acts transitively (from the left) on G/PG/P. Since the projection π:G/HG/P\pi:G/H\to G/P is KK-equivariant and KK acts transitively on the base, it follows that every KK-orbit in G/HG/H intersects S=π1(eP)S=\pi^{-1}(eP). This yields a map φ\varphi from the space of KK-orbits K\G/HK\backslash G/H to S/KSS/K_{S} (it turns out the intersection of a KK-orbit with SS is a KSK_{S}-orbit). We can now define the spherical logarithm map sLogt:G/HHom(ΛS,)\operatorname{sLog}_{t}:G/H\to\operatorname{Hom}(\Lambda_{S},\mathbb{R}) by composing φ\varphi with the Logt\operatorname{Log}_{t} defined in the previous paragraph. It can be verified that when G/HG/H is quasi-affine this sLogt\operatorname{sLog}_{t} map coincides with the sLogt\operatorname{sLog}_{t} map defined using spherical functions (cf. the discussion after Theorem 1).

3. Spherical tropicalization, spherical amoebae and the limits of spherical logarithms

The purpose of this section is to examine relationships between the spherical tropicalization map, introduced in Section 1.2, with the spherical logarithm map of Definition 2.12. In order to do so, a slight change in perspective is useful, because the spherical logarithm is inherently a real object (it being a logarithm), i.e. defined over \mathbb{R}, whereas the valuation cone is naturally defined over \mathbb{Q}. More precisely, for the discussion that follows, we first choose an explicit identification of Hom(ΛG/H,)=𝒬G/H\operatorname{Hom}(\Lambda_{G/H},\mathbb{Q})=\mathcal{Q}_{G/H} with r\mathbb{Q}^{r} using a choice of basis. Specifically, let {λ1,,λr}Λ+G/H\{\lambda_{1},\ldots,\lambda_{r}\}\subseteq\Lambda^{+}_{G/H} be the basis of ΛG/H\Lambda_{G/H}\otimes\mathbb{R} appearing in Definition 2.12. This gives us an identification Hom(ΛG/H,)r\operatorname{Hom}(\Lambda_{G/H},\mathbb{Q})\cong\mathbb{Q}^{r}. Moreover, we additionally extend our coefficents from \mathbb{Q} to \mathbb{R} for the remainder of this manuscript, so we consider 𝒬G/HHom(ΛG/H,)\mathcal{Q}_{G/H}\otimes\mathbb{R}\cong\operatorname{Hom}(\Lambda_{G/H},\mathbb{R}) and the choice of basis above naturally also yields an identification 𝒬G/Hr\mathcal{Q}_{G/H}\otimes\mathbb{R}\cong\mathbb{R}^{r}, which we fix throughout. The embedding ρ:𝒱G/H𝒬G/H\rho:\mathcal{V}_{G/H}\hookrightarrow\mathcal{Q}_{G/H} in (2) then allows us to think of the valuation cone 𝒱G/H\mathcal{V}_{G/H} as a subset of 𝒬G/Hr\mathcal{Q}_{G/H}\otimes\mathbb{R}\cong\mathbb{R}^{r}. We let 𝒱¯G/H\overline{\mathcal{V}}_{G/H} denote the closure of 𝒱G/H\mathcal{V}_{G/H} in r\mathbb{R}^{r} with respect to the usual Euclidean topology on r\mathbb{R}^{r}. It is a co-simplicial cone in r\mathbb{R}^{r} with the same defining equations as given in Theorem 1.5. (We slightly abuse terminology and call 𝒱¯G/H\overline{\mathcal{V}}_{G/H} also the valuation cone.) The reader may note that the spherical logarithm map of Definition 2.12 uses a choice of Γ={λ1,,λs}]\Gamma=\{\lambda_{1},\ldots,\lambda_{s}\}] where it is possible that s>rs>r. In such a case, the image of sLogΓ,t\operatorname{sLog}_{\Gamma,t} lies in s\mathbb{R}^{s} and not in r\mathbb{R}^{r}, whereas the valuation cone lies in 𝒬G/Hr\mathcal{Q}_{G/H}\otimes\mathbb{R}\cong\mathbb{R}^{r}, as just described above. In this situation we will use the linear embedding of the valuation cone 𝒱G/H\mathcal{V}_{G/H} into s\mathbb{R}^{s} specified by Γ\Gamma, given by:

v(v,λ1,,v,λs)s,v𝒱G/H.v\mapsto(\langle v,\lambda_{1}\rangle,\ldots,\langle v,\lambda_{s}\rangle)\in\mathbb{R}^{s},\quad v\in\mathcal{V}_{G/H}.

In this way we can embed 𝒱G/H\mathcal{V}_{G/H} in s\mathbb{R}^{s} and identify it with its image in s\mathbb{R}^{s}, thus allowing us to compare 𝒱G/H\mathcal{V}_{G/H} with the image of the spherical logarithm.

Our first result shows that points in the valuation cone can be realized as limits of points in the image of the spherical logarithm map. As in the previous section, we assume here that G/HG/H is a quasi-affine spherical homogeneous space. Let BB be the Borel subgroup of GG such that the BB-orbit of eHeH is open in G/HG/H. Note that the multiplication map K×BGK\times B\to G (similar to the Iwasawa decomposition) is a surjection, with kernel isomorphic to KBK\cap B.

Theorem 3.1.

Let G/HG/H be a quasi-affine spherical homogeneous space. Let γG/H([[t]])\gamma\in G/H(\mathbb{C}[[t]]) be a convergent formal Laurent curve in G/HG/H which is convergent for sufficiently small t0t\neq 0. Let vγ𝒱G/Hv_{\gamma}\in\mathcal{V}_{G/H} be the GG-invariant valuation associated to the formal curve γ\gamma. Let λΛ+G/H\lambda\in\Lambda^{+}_{G/H} and let ϕλ:G/H>0\phi_{\lambda}:G/H\to\mathbb{R}_{>0} the corresponding spherical function. Then for any highest weight vector fλVλ[G/H]f_{\lambda}\in V_{\lambda}\subset\mathbb{C}[G/H] we have:

(12) limt0logt(ϕλ(γ(t)))=2vγ(fλ).\lim_{t\to 0}\log_{t}(\phi_{\lambda}(\gamma(t)))=2v_{\gamma}(f_{\lambda}).
Proof.

Let λΛ+G/H\lambda\in\Lambda^{+}_{G/H} be fixed throughout. By Theorem 1.12 there exists an open set UGU\subset G such that for gUg\in U we have vγ(fλ)=v^γ(gfλ)v_{\gamma}(f_{\lambda})=\hat{v}_{\gamma}(g\cdot f_{\lambda}) where v^γ\hat{v}_{\gamma} computes is the order in tt of gfλg\cdot f_{\lambda} after restricting to the curve γ\gamma. We claim that there is an open dense subset UKU^{\prime}\subset K such that for kUk\in U^{\prime} we have

(13) vγ(fλ)=v^γ(kfλ).v_{\gamma}(f_{\lambda})=\hat{v}_{\gamma}(k\cdot f_{\lambda}).

To see this, first note that for gUg\in U if we write g=kbg=kb with bBb\in B and kKk\in K then since fλf_{\lambda} is a BB-weight vector we have vγ(fλ)=v^γ(kfλ)v_{\gamma}(f_{\lambda})=\hat{v}_{\gamma}(k\cdot f_{\lambda}). Now let m:K×BGm:K\times B\to G be the multiplication map and pr1:B×KKpr_{1}:B\times K\to K the projection on the first factor. It suffices to take U=pr1(m1(U))U^{\prime}=pr_{1}(m^{-1}(U)). Clearly, m1(U)m^{-1}(U) is open. Note that the multiplication map m:K×BGm:K\times B\to G is a fibration with fibers isomorphic to BKB\cap K. But in a fibration the inverse image of a dense subset is dense. This shows that m1(U)m^{-1}(U) is dense in K×BK\times B as well. Since the projection map pr1pr_{1} is open, it follows that U=pr1(m1(U))U^{\prime}=pr_{1}(m^{-1}(U)) is open and dense in KK, which proves the claim.

Now let us define the KK-invariant function ψλ:G/H>0\psi_{\lambda}:G/H\to\mathbb{R}_{>0} by

(14) ψλ(x)=Kfλ(k1x)fλ(k1x)¯dk\psi_{\lambda}(x)=\int_{K}f_{\lambda}(k^{-1}\cdot x)\overline{f_{\lambda}(k^{-1}\cdot x)}dk

where dkdk is the Haar measure on KK. By Remark 2.7 we know that ψλ\psi_{\lambda} is a scalar multiple of the spherical function ϕλ\phi_{\lambda}.

Let aλ:=vγ(fλ)a_{\lambda}:=v_{\gamma}(f_{\lambda}) denote the value of the invariant valuation vγv_{\gamma} on fλf_{\lambda}. Now we claim that the limit

limt0ψλ(γ(t))t2aλ\lim_{t\to 0}\frac{\psi_{\lambda}(\gamma(t))}{t^{2a_{\lambda}}}

exists and is nonzero. We have just seen in (13) that for kUk\in U^{\prime} we have

(kfλ)(γ(t))=c(k)taλ+ higher-order terms(k\cdot f_{\lambda})(\gamma(t))=c(k)t^{a_{\lambda}}+\textup{ higher-order terms}

for some constant c(k),c(k)0c(k)\in\mathbb{C},c(k)\neq 0. Hence |(kfλ)(γ(t))|2=|c(k)|2t2aλ+ higher-order terms|(k\cdot f_{\lambda})(\gamma(t))|^{2}=|c(k)|^{2}t^{2a_{\lambda}}+\textup{ higher-order terms}, for tt\in\mathbb{R}. From the definition 14 of Ψλ\Psi_{\lambda} we have

ψλ(γ(t))\displaystyle\psi_{\lambda}(\gamma(t)) =K|(kfλ)(γ(t)|2dk,\displaystyle=\int_{K}|(k\cdot f_{\lambda})(\gamma(t)|^{2}dk,
=U|(kfλ)(γ(t))|2dk,because UK is open and dense,\displaystyle=\int_{U^{\prime}}|(k\cdot f_{\lambda})(\gamma(t))|^{2}dk,\quad\textup{because }U^{\prime}\subset K\textup{ is open and dense},
=(U|c(k)|2dk)t2aλ+ higher terms,\displaystyle=(\int_{U^{\prime}}|c(k)|^{2}dk)t^{2a_{\lambda}}+\textup{ higher terms},
=ct2aλ+ higher terms,\displaystyle=c\,t^{2a_{\lambda}}+\textup{ higher terms},

where c=U|c(k)|2dk>0c=\int_{U^{\prime}}|c(k)|^{2}dk>0, and the term-by-term integration which is implicit in the last equality is justified because, from the compactness of KK, it follows that for sufficiently small t0t\neq 0, the series c(k)taλ+c(k)t^{a_{\lambda}}+\cdots converges uniformly in kKk\in K. Finally, since ϕλ\phi_{\lambda} is a constant multiple of ψλ\psi_{\lambda}, from the above we have:

limt0logt(ϕλ(γ(t)))\displaystyle\lim_{t\to 0}\log_{t}(\phi_{\lambda}(\gamma(t))) =limt0logt(ψλ(γ(t)))\displaystyle=\lim_{t\to 0}\log_{t}(\psi_{\lambda}(\gamma(t)))
=limt0logt(t2aλ(c+(terms of positive order in t)))\displaystyle=\lim_{t\to 0}\log_{t}(t^{2a_{\lambda}}(c+\textup{(terms of positive order in $t$)}))
=2aλ+limt0ln(c+(terms of positive order in t))ln(t)\displaystyle=2a_{\lambda}+\lim_{t\to 0}\frac{\ln(c+\textup{(terms of positive order in $t$)})}{\ln(t)}
=2aλ\displaystyle=2a_{\lambda}
=2vγ(fλ)\displaystyle=2v_{\gamma}(f_{\lambda})

where the last equality is the definition of aλa_{\lambda}. This finishes the proof. ∎

Remark 3.2.

In [Kaveh-Manon, Conjecture 7.1], the fourth author and Christopher Manon conjecture an analogue of the Cartan decomposition for a spherical homogeneous space over \mathbb{C}. They also suggest a definition of a spherical logarithm map on G/HG/H whenever such a Cartan decomposition exists. In particular, in [Kaveh-Makhnatch], the singular value decomposition theorem (i.e. the Cartan decomposition for GLn()\operatorname{GL}_{n}(\mathbb{C})) is used to propose a definition of a spherical logarithm map on the group GLn()\operatorname{GL}_{n}(\mathbb{C}), and it is proven that the logarithm of singular values of a curve γ(t)\gamma(t) on GLn()\operatorname{GL}_{n}(\mathbb{C}) approach its invariant factors. This result can be regarded as a special case of Theorem 3.1. It should be noted that the definition of spherical logarithm proposed in [Kaveh-Manon] is a priori different from that given in this paper – for instance, in the “group case” GLn()\operatorname{GL}_{n}(\mathbb{C}), our definition gives (the logarithms of) symmetric functions in the singular values (cf. Section 4.2), whereas the definition in [Kaveh-Manon] gives (logarithms of) the singular values.

Theorem 3.1 holds for any weight λΛ+G/H\lambda\in\Lambda^{+}_{G/H}. By restricting attention to λΓ={λ1,,λs}\lambda\in\Gamma=\{\lambda_{1},\ldots,\lambda_{s}\} it follows that

limt0sLogΓ,t(γ(t))=2strop(γ(t))\lim_{t\to 0}\operatorname{sLog}_{\Gamma,t}(\gamma(t))=2\cdot\operatorname{strop}(\gamma(t))

where we think of the RHS as an element of 𝒱G/H𝒬G/Hr\mathcal{V}_{G/H}\subseteq\mathcal{Q}_{G/H}\otimes\mathbb{R}\cong\mathbb{R}^{r} as explained above. Thus Theorem 3.1 says that, for certain curves γG/H(𝒦¯)\gamma\in G/H(\overline{\mathcal{K}}), the image of γ\gamma under the spherical tropicalization map can also be realized as the limit of points in the image of the spherical logarithm map. This is reminiscent of the phenomenon seen in the classical case of G=TG=T, recounted in the Introduction, where the amoeba 𝒜t(Y)\mathcal{A}_{t}(Y) – the image under LogtLog_{t} map of Y()nY\subseteq(\mathbb{C}^{*})^{n} – approaches the image trop(Y)\operatorname{trop}(Y) of Y(𝒦¯)Y(\overline{\mathcal{K}}) under the valuation map. Motivated by the classical case and by Theorem 3.1, we formulate below a question relating the spherical analogues of LogtLog_{t} and trop\operatorname{trop}.

To give precise statements, we need the notion of Kuratowski convergence of subsets of a topological space, which can be thought of as a notion of continuity for the association bXbb\mapsto X_{b}.

Definition 3.3 (Kuratowski convergence (see e.g. [Kuratowski, Jonsson])).

Suppose MM and BB are topological spaces. Let XM×BX\subset M\times B and let π:XB\pi:X\to B be the restriction of the projection M×BBM\times B\to B to XX. For bBb\in B let Xb=π1(b)X_{b}=\pi^{-1}(b). Let b0Bb_{0}\in B and X0XX_{0}\subset X. We say that XbX_{b} converges to X0X_{0} in the sense of Kuratowski as bb converges to b0b_{0} if the following conditions hold:

  • (a)

    For every yMX0y\in M\setminus X_{0} there exist neighborhoods UU of yy and V0V_{0} of b0b_{0} such that XbU=X_{b}\cap U=\emptyset for all bV0b\in V_{0}.

  • (b)

    For every yX0y\in X_{0} and any neighborhood UU of yy in MM, there exists a neighborhood V0V_{0} of b0b_{0} such that XbUX_{b}\cap U\neq\emptyset for all bV0b\in V_{0}.

Suppose G/HG/H is a quasi-affine spherical variety and YG/HY\subset G/H is a subvariety. Following the terminology in the classical case, we define the spherical amoebae 𝒜t(Y):=sLogt(Y)\mathcal{A}_{t}(Y):=\operatorname{sLog}_{t}(Y) to be the images in r\mathbb{R}^{r} of YY under the spherical logarithm maps. We call strop(Y)\operatorname{strop}(Y) the spherical tropicalization of YY, considered as a subset of r\mathbb{R}^{r} via the identification ΛG/H\Lambda_{G/H}\otimes\mathbb{R} with r\mathbb{R}^{r} discussed previously. With this terminology in place, we may ask the following.

Question 3.4.

Let YG/HY\subset G/H be a subvariety as above and Γ={λ1,,λs}Λ+G/H\Gamma=\{\lambda_{1},\ldots,\lambda_{s}\}\subset\Lambda^{+}_{G/H} be a set of semigroup generators of Λ+G/H\Lambda^{+}_{G/H}. Then, as t0t\to 0, we ask:

  1. (1)

    Under what conditions do the sets sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) approach the valuation cone 𝒱¯G/H\overline{\mathcal{V}}_{G/H} in the sense of Kuratowski?

  2. (2)

    Assuming that the images sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) converge to 𝒱¯G/H\overline{\mathcal{V}}_{G/H} in the sense of Kuratowski, under what additional conditions on the subvariety YY do the spherical amoebae 𝒜t(Y)=sLogt(Y)\mathcal{A}_{t}(Y)=\operatorname{sLog}_{t}(Y) approach strop(Y)\operatorname{strop}(Y) in the sense of Kuratowski?

We note here Theorem 3.1 already gives us some information about Question 3.4. The following are straightforward corollaries of Theorem 3.1.

Corollary 3.5.

Let G/HG/H be a quasi-affine spherical homogeneous space. Let Γ={λ1,,λs}Λ+G/H\Gamma=\{\lambda_{1},\cdots,\lambda_{s}\}\subseteq\Lambda^{+}_{G/H} be a set of semigroup generators of Λ+G/H\Lambda^{+}_{G/H}. Let 𝒱G/H\mathcal{V}_{G/H} denote the valuation cone of G/HG/H.

  1. (1)

    The Kuratowski limit, as t0t\to 0, of the images sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) contains the valuation cone.

  2. (2)

    When G/HG/H is horospherical this limit is the entire vector space, which in this case coincides with the valuation cone.

Proof.

The first claim follows immediately from Theorem 3.1. The second claim uses the fact that, in the horospherical case, the valuation cone 𝒱G/H\mathcal{V}_{G/H} is the entire vector space r\mathbb{R}^{r}. Since by (1) the limit of the images must contain the valuation cone, this means the limit must be all of r\mathbb{R}^{r}. ∎

Although we do not have a complete answer to Question 3.4(1), in the remark below we give a sketch of an argument which may be useful.

Remark 3.6.

It may be possible to answer Question 3.4 (1) positively using Proposition 2.9 as follows. Suppose yy lies in the Kuratowski limit as t0t\to 0 of the sets sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H). Then by definition there exist sequences (ti)(t_{i}), tit_{i}\in\mathbb{R} with limiti=0\lim_{i\to\infty}t_{i}=0, and (xi)(x_{i}), xiG/Hx_{i}\in G/H, such that limisLogΓ,ti(xi)=y\lim_{i\to\infty}\operatorname{sLog}_{\Gamma,t_{i}}(x_{i})=y. We would like to show that yy lies in the image 𝒱¯G/H\overline{\mathcal{V}}_{G/H} of the valuation cone in s\mathbb{R}^{s}. By Proposition 2.9 we know there exists a constant c>0c>0 such that

ϕλ(xi)ϕμ(xi)cϕγ(xi).\phi_{\lambda}(x_{i})\phi_{\mu}(x_{i})\geq c\phi_{\gamma}(x_{i}).

Taking logti\log_{t_{i}} of both sides we have:

logti(ϕλ(xi))+logti(ϕμ(xi))logti(c)+logti(ϕγ(xi)).\log_{t_{i}}(\phi_{\lambda}(x_{i}))+\log_{t_{i}}(\phi_{\mu}(x_{i}))\leq\log_{t_{i}}(c)+\log_{t_{i}}(\phi_{\gamma}(x_{i})).

Now observe that in order to show y𝒱¯G/Hy\in\overline{\mathcal{V}}_{G/H} it would be enough to find v𝒬G/H:=Hom(ΛG/H,)v\in\mathcal{Q}_{G/H}\otimes\mathbb{R}:=\operatorname{Hom}(\Lambda_{G/H},\mathbb{R}) such that for any highest weight νΛG/H\nu\in\Lambda_{G/H} we have

limilogtiϕν(xi)=v,ν.\lim_{i\to\infty}\log_{t_{i}}\phi_{\nu}(x_{i})=\langle v,\nu\rangle.

Then by the above inequalities we have v,λ+v,μv,γ\langle v,\lambda\rangle+\langle v,\mu\rangle\leq\langle v,\gamma\rangle, for all λ\lambda, μ\mu, γ\gamma such that λ+μγ\lambda+\mu-\gamma is a tail and hence v𝒱G/Hv\in\mathcal{V}_{G/H}. We expect that the proof that such a vv exists would be a variant of the argument in the proof of Theorem 3.1. The case when s=rs=r, namely when the highest weight monoid is freely generated, might be easier to work out.

In the next section, we show that in a number of interesting cases, the sets sLogt(G/H)\operatorname{sLog}_{t}(G/H) not only contain the valuation cone, but in fact they do limit to exactly the valuation cone in the Kuratowski sense.

4. Examples

In the previous section, we asked in Question 3.4 for conditions under which, in analogy with the classical case, the spherical amoebae approach the spherical tropicalization. In this section we focus on Question 3.4(1), i.e. the case when we take Y=G/HY=G/H. We analyze the following interesting cases of spherical homogeneous spaces: (1) the “group case” of G×GG\times G acting on GG, for G=SLn()G=\operatorname{SL}_{n}(\mathbb{C}), (2) the basic affine space G/H=SLn()/UG/H=\operatorname{SL}_{n}(\mathbb{C})/U, (3) the case G/H=SLn()/SLn1()G/H=\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}), and (4) the case of the “space of hyperbolic triangles” (the precise definition is in Section LABEL:subsec:_hyperbolic_triangles). In the cases of the basic affine space SLn()/U\operatorname{SL}_{n}(\mathbb{C})/U and SLn()/SLn1()\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}), it turns out that the spherical amoebae coincide with the valuation cone for all tt, so the limit does indeed coincide with the valuation cone, with a rather trivial limiting process. However, for the “group case” and the hyperbolic triangles case, the spherical amoeba is different from the valuation cone but the limit does indeed approach the valuation cone via a non-trivial limiting process (see Figure 1).

As in Section 3, throughout this section we work over \mathbb{R}.

4.1. Two small examples with G=SL2()G=\operatorname{SL}_{2}(\mathbb{C})

4.1.1. The case of X=SL2()/T=(1×1)ΔX=\operatorname{SL}_{2}(\mathbb{C})/T=(\mathbb{P}^{1}\times\mathbb{P}^{1})\setminus\Delta

Let G=SL2()G=\operatorname{SL}_{2}(\mathbb{C}) and let H=TH=T, the maximal (diagonal) torus of GG. Consider the action of GG on 1\mathbb{P}^{1} by left multiplication, and the corresponding diagonal action of GG on 1×1\mathbb{P}^{1}\times\mathbb{P}^{1}. Then it is not hard to see that the stabilizer of the point x0=([1:0],[0:1])1×1x_{0}=([1:0],[0:1])\in\mathbb{P}^{1}\times\mathbb{P}^{1} is precisely TT, and that the orbit of x0x_{0} under the GG-action is 1×1Δ\mathbb{P}^{1}\times\mathbb{P}^{1}\setminus\Delta, where Δ\Delta denotes the diagonal copy of 1\mathbb{P}^{1} in the direct product. The compact group KK is SU(2)SU(2) in this case. The (diagonal) action of SU(2)SU(2) on 1×1\mathbb{P}^{1}\times\mathbb{P}^{1} has moment map

Φ([z],[w])=i2(zzz2+www2)(i4z2tr(zz)+i4w2tr(ww))I2×2𝔰𝔲(2)\Phi([z],[w])=\frac{i}{2}\left(\frac{zz^{*}}{\|z\|^{2}}+\frac{ww^{*}}{\|w\|^{2}}\right)-\left(\frac{i}{4\|z\|^{2}}\mathrm{tr}(zz^{*})+\frac{i}{4\|w\|^{2}}\mathrm{tr}(ww^{*})\right)\cdot I_{2\times 2}\in\mathfrak{su}(2)^{*}

where ([z],[w])([z],[w]) are homogeneous coordinates on 1×1\mathbb{P}^{1}\times\mathbb{P}^{1} (so z,wz,w are considered as elements of 2\mathbb{C}^{2}) and I2×2I_{2\times 2} denotes the 2×22\times 2 identity matrix. Composing this with the map which quotients by the coadjoint action of SU(2)SU(2) on 𝔰𝔲(2)\mathfrak{su}(2)^{*}, i.e. the so-called “sweeping map” 𝔰𝔲(2)0=𝔰𝔲(2)/SU(2)\mathfrak{su}(2)^{*}\to\mathbb{R}_{\geq 0}=\mathfrak{su}(2)/SU(2), yields that the Kirwan map 1×10\mathbb{P}^{1}\times\mathbb{P}^{1}\to\mathbb{R}_{\geq 0} is given by

([z],[w])12(|z1|2z2+|w1|2w21)2+(|z1|2|z2|2z4+2Re(z1w¯1z¯2w2)z2w2+|w1|2|w2|2w4).([z],[w])\longmapsto\frac{1}{2}\sqrt{\left(\frac{|z_{1}|^{2}}{\|z\|^{2}}+\frac{|w_{1}|^{2}}{\|w\|^{2}}-1\right)^{2}+\left(\frac{|z_{1}|^{2}|z_{2}|^{2}}{\|z\|^{4}}+\frac{2\mathrm{Re}(z_{1}\overline{w}_{1}\overline{z}_{2}w_{2})}{\|z\|^{2}\|w\|^{2}}+\frac{|w_{1}|^{2}|w_{2}|^{2}}{\|w\|^{4}}\right)}.

The Kirwan polytope (i.e. the image of 1×1\mathbb{P}^{1}\times\mathbb{P}^{1} under the above map) is the interval [0,12][0,\frac{1}{2}] and the image of the diagonal is straightforwardly computed to be 12\frac{1}{2}, so the distinguished KK-orbit (the diagonal) corresponds to the boundary value.

There is also another natural parametrization of KK-orbits which can be described in terms of the angle between two complex lines in 2\mathbb{C}^{2}. More specifically, given ([z],[w])1×1([z],[w])\in\mathbb{P}^{1}\times\mathbb{P}^{1} where z,w2{0}z,w\in\mathbb{C}^{2}\setminus\{0\}, we may define

ρ([z],[w]):=1|z,w|2z2w2,\rho([z],[w]):=1-\frac{|\langle z,w\rangle|^{2}}{\|z\|^{2}\|w\|^{2}},

where z,w\langle z,w\rangle is the standard Hermitian product on 2\mathbb{C}^{2}. Geometrically, ρ\rho is the quantity sin2(θ)\sin^{2}(\theta) where θ\theta is the angle between the two complex lines spanned by zz and ww, or equivalently, the spherical distance between two distinct points p,q1=S2p,q\in\mathbb{P}^{1}=S^{2} if we represent pp, qq by complex vectors z,w2z,w\in\mathbb{C}^{2} with z=w=1\|z\|=\|w\|=1. It turns out that ρ([z],[w])=ρ([z],[w])\rho([z],[w])=\rho([z^{\prime}],[w^{\prime}]) if and only if the two pairs ([z],[w]),([z],[w])([z],[w]),([z^{\prime}],[w^{\prime}]) are in the same K=SU(2)K=\operatorname{SU}(2)-orbit, so the function ρ\rho provides a parametrization of KK-orbits in G/TG/T. It follows from the Cauchy-Schwarz inequality that the image of ρ\rho is the interval (0,1](0,1]. Thus, composing ρ\rho with log-\log, i.e. ([z],[w])log(ρ([z],[w]))([z],[w])\longmapsto-\log(\rho([z],[w])), we obtain an identification of the KK-orbit space with the valuation cone (which in this case is 0\mathbb{R}_{\geq 0}).

Finally, there is also our spherical function ϕ2\phi_{2} corresponding to the irreducible representation of SL2()\operatorname{SL}_{2}(\mathbb{C}) of highest weight 22 in [SL2()/T]\mathbb{C}[\operatorname{SL}_{2}(\mathbb{C})/T]. This can be computed to be

ϕ2([z],[w])=1|z1w2z2w1|2(|z1w1|2+12|z1w2+w1z2|2+|z2w2|2).\phi_{2}([z],[w])=\frac{1}{\lvert z_{1}w_{2}-z_{2}w_{1}\rvert^{2}}\left(\lvert z_{1}w_{1}\rvert^{2}+\frac{1}{2}\lvert z_{1}w_{2}+w_{1}z_{2}\rvert^{2}+\lvert z_{2}w_{2}\rvert^{2}\right).

One can show that ϕ2([z],[w])1/2\phi_{2}([z],[w])\geq 1/2. On the other hand, ϕ2((1:1),(1:1))=1/2\phi_{2}((1:1),(-1:1))=1/2. This shows that the image of ϕ2\phi_{2} is [1/2,)[1/2,\infty). Hence we have a parametrization of the KK-orbits by the points in this interval. One can obtain a parametrization of the KK-orbit space by 0\mathbb{R}_{\geq 0} (the valuation cone) by taking the limit, as t0t\to 0, of the image of logt(ϕ2)-\log_{t}(\phi_{2}).

The above computations show that, in this case, we have three parametrizations of the space of KK-orbits SU(2)\SL2()/TSU(2)\backslash SL_{2}(\mathbb{C})/T by (half open) intervals in \mathbb{R}, namely: the spherical function ϕ2\phi_{2} above, the Kirwan map computed above, and the map ρ\rho as above.

4.1.2. The case of X=SL2()/N(T)X=\operatorname{SL}_{2}(\mathbb{C})/N(T)

As in the last section, we take G=SL2()G=\operatorname{SL}_{2}(\mathbb{C}) but this time we take H=N(T)H=N(T). In this situation we have N(T)/T/2N(T)/T\cong\mathbb{Z}/2\mathbb{Z} so there is a natural map SL2()/TSL2()/N(T)\operatorname{SL}_{2}(\mathbb{C})/T\to\operatorname{SL}_{2}(\mathbb{C})/N(T). The homogeneous space SL2()/N(T)\operatorname{SL}_{2}(\mathbb{C})/N(T) can be identified with 2Q\mathbb{P}^{2}\setminus Q where QQ is a smooth conic, as follows: consider the map Sym1(2)×Sym1(2)Sym2(2)\operatorname{Sym}^{1}(\mathbb{C}^{2})\times\operatorname{Sym}^{1}(\mathbb{C}^{2})\to\operatorname{Sym}^{2}(\mathbb{C}^{2}) given by multiplication. Note that Sym1(2)2\operatorname{Sym}^{1}(\mathbb{C}^{2})\cong\mathbb{C}^{2} and Sym2(2)3\operatorname{Sym}^{2}(\mathbb{C}^{2})\cong\mathbb{C}^{3}. This product map induces a morphism (1×1)Δ2Q(\mathbb{P}^{1}\times\mathbb{P}^{1})\setminus\Delta\to\mathbb{P}^{2}\setminus Q, where QQ is the smooth conic defined by the vanishing of the discriminant on Sym2(2)3\operatorname{Sym}^{2}(\mathbb{C}^{2})\cong\mathbb{C}^{3}. One sees that the natural projection SL2()/TSL2()/N(T)\operatorname{SL}_{2}(\mathbb{C})/T\to\operatorname{SL}_{2}(\mathbb{C})/N(T) is then identified with (1×1)Δ2Q(\mathbb{P}^{1}\times\mathbb{P}^{1})\setminus\Delta\to\mathbb{P}^{2}\setminus Q. The non-identity element in the quotient N(T)/T/2N(T)/T\cong\mathbb{Z}/2\mathbb{Z} corresponds to the involution on 1×1\mathbb{P}^{1}\times\mathbb{P}^{1} exchanging the two factors. This involution leaves the Kirwan map, ρ\rho and ϕ2\phi_{2} of the previous section invariant. This implies that all of these functions descend to functions on SL2()/N(T)\operatorname{SL}_{2}(\mathbb{C})/N(T) which also parametrizes the KK-orbits on SL2()/N(T)\operatorname{SL}_{2}(\mathbb{C})/N(T).

4.2. The group case

As a first example, we consider GG equipped with the action of G×GG\times G by left and right multiplication, as described in Example 1.1(5). In particular, here we identify GG with the homogeneous space G×G/GdiagG\times G/G_{\operatorname{diag}}. We choose the Borel subgroup B×BG×GB\times B^{-}\subseteq G\times G where BGB\subseteq G is a Borel subgroup of GG and BB^{-} is its opposite. By the Peter-Weyl Theorem, [G]\mathbb{C}[G] decomposes as a G×GG\times G-module as follows:

[G]λΛ+VλVλ\mathbb{C}[G]\cong\bigoplus_{\lambda\in\Lambda^{+}}V_{\lambda}\otimes V_{\lambda}^{*}

where Λ+\Lambda^{+} is the set of dominant weights of GG. It follows from Definition 1.7 that ΛG+=ΛG×G/Gdiag+Λ+\Lambda_{G}^{+}=\Lambda_{G\times G/G_{\operatorname{diag}}}^{+}\cong\Lambda^{+} and that the lattice ΛG\Lambda_{G} of GG×G/GdiagG\cong G\times G/G_{\operatorname{diag}} as a G×GG\times G-spherical variety is the sublattice {(λ,λ)λΛ}Λ×Λ\{(\lambda,-\lambda)\mid\lambda\in\Lambda\}\subset\Lambda\times\Lambda. Using Theorem 1.12, [Timashev, Theorem 24.2], [Timashev, Lemma 24.3] and the Cartan decomposition, it can then be shown that the valuation cone 𝒱G\mathcal{V}_{G} can be identified with the antidominant Weyl chamber in Λˇ\check{\Lambda}, i.e., 𝒱G={ξΛˇ:ξ,α0for all positive rootsα}\mathcal{V}_{G}=\{\xi\in\check{\Lambda}\colon\langle\xi,\alpha\rangle\leq 0\;\text{for all positive roots}\;\alpha\}.

In the case of G=SLn()G=\operatorname{SL}_{n}(\mathbb{C}), to which we now restrict, we can also give an explicit description of the spherical functions. We choose the basis {(ωi,ωi)}1in1\{(\omega_{i},-\omega_{i})\}_{1\leq i\leq n-1} for ΛSLn()\Lambda_{\operatorname{SL}_{n}(\mathbb{C})} where ωi\omega_{i} denotes the usual ii-th fundamental weight of SLn()\operatorname{SL}_{n}(\mathbb{C}). The corresponding irreducible SLn()×SLn()\operatorname{SL}_{n}(\mathbb{C})\times\operatorname{SL}_{n}(\mathbb{C})-representation is Λin(Λin)\Lambda^{i}\mathbb{C}^{n}\otimes(\Lambda^{i}\mathbb{C}^{n})^{*}. To construct the spherical function ϕ(ωi,ωi)\phi_{(\omega_{i},-\omega_{i})} corresponding to (ωi,ωi)(\omega_{i},-\omega_{i}), we need to find an isomorphic copy of Λin(Λin)\Lambda^{i}\mathbb{C}^{n}\otimes(\Lambda^{i}\mathbb{C}^{n})^{*} in [SLn()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})], considered as an SLn()×SLn()\operatorname{SL}_{n}(\mathbb{C})\times\operatorname{SL}_{n}(\mathbb{C})-representation. Let J={j1<j2<<ji},K={k1<k2<<ki}J=\{j_{1}<j_{2}<\cdots<j_{i}\},K=\{k_{1}<k_{2}<\cdots<k_{i}\} be subsets of {1,2,,n}\{1,2,\ldots,n\} of cardinality ii. Let pJ,Kp_{J,K} denote the (i×i)(i\times i) minor of an n×nn\times n matrix corresponding to the subsets JJ and KK, i.e., the determinant of the submatrix with rows in JJ and columns in KK. We view pJ,Kp_{J,K} as an element in [SLn()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})]. By explicitly analyzing the action of the Chevalley generators Eα,FαE_{\alpha},F_{\alpha} (for positive roots α\alpha) as well as by computing the TT-weights of the pJ,Kp_{J,K}, it is not difficult to see that the span of the pJ,Kp_{J,K} is a subrepresentation of [SLn()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})] isomorphic to Λin(Λin)\Lambda^{i}\mathbb{C}^{n}\otimes(\Lambda^{i}\mathbb{C}^{n})^{*}. Moreover, it is straightforward to see that each pJ,Kp_{J,K} is a TT-weight vector, and that there exists a KK-invariant inner product with respect to which the pJ,Kp_{J,K} form an orthonormal basis. Thus we have

ϕ(ωi,ωi)(x)=1(ni)J,K|pJ,K|2\phi_{(\omega_{i},-\omega_{i})}(x)=\frac{1}{\binom{n}{i}}\sum_{J,K}\lvert p_{J,K}\rvert^{2}

where the normalization factor ensures that ϕ(ωi,ωi)(x)=1\phi_{(\omega_{i},-\omega_{i})}(x)=1.

Recall the singular value decomposition theorem, which states that any ASLn()A\in\operatorname{SL}_{n}(\mathbb{C}) can be expressed as a product

A=U1DU2A=U_{1}DU_{2}

where U1,U2SUnU_{1},U_{2}\in\operatorname{SU}_{n} and DD is a diagonal matrix with positive real entries whose product is equal to 11. Let Γ={(ωi,ωi) 1in1}\Gamma=\{(\omega_{i},-\omega_{i})\,\mid\,1\leq i\leq n-1\} and consider the spherical logarithm map sLogΓ,t\operatorname{sLog}_{\Gamma,t} on SLn()\operatorname{SL}_{n}(\mathbb{C}) corresponding to Γ\Gamma. Since the spherical function ϕi\phi_{i} is (SUn×SUn)(\operatorname{SU}_{n}\times\operatorname{SU}_{n})-invariant by construction, it follows that

sLogΓ,t(SLn())={(|I|=ikIdk)n1 1in1;d1,,dn+,k=1ndk=1}.\operatorname{sLog}_{\Gamma,t}(\operatorname{SL}_{n}(\mathbb{C}))=\left\{\left(\sum_{|I|=i}\prod_{k\in I}d_{k}\right)\in\mathbb{R}^{n-1}\,\mid\,1\leq i\leq n-1;d_{1},\ldots,d_{n}\in\mathbb{R}_{+},\prod_{k=1}^{n}d_{k}=1\right\}\text{.}

(Note that the components of the function logtΦ\log_{t}\circ\Phi are exactly the symmetric functions on the eigenvalues of AA, i.e., the coefficients of the characteristic polynomial of AA.)

For the special case n=3n=3, an elementary calculus (maximization) computation shows that the resulting region is bounded by

{(logt(2x3+13x2),logt(2+x33x)):x[1,)}and{(logt(2+x33x),logt(2x3+13x2)):x[1,)}\left\{\left(\log_{t}\left(\frac{2x^{3}+1}{3x^{2}}\right),\log_{t}\left(\frac{2+x^{3}}{3x}\right)\right)\colon x\in[1,\infty)\right\}\\ \text{and}\;\left\{\left(\log_{t}\left(\frac{2+x^{3}}{3x}\right),\log_{t}\left(\frac{2x^{3}+1}{3x^{2}}\right)\right)\colon x\in[1,\infty)\right\}

from which it can be seen that as tt approaches 0, the spherical amoebae approach 𝒱¯G\overline{\mathcal{V}}_{G}. See Figure 1. Also compare with [Kaveh-Manon, Example 7.7].

Refer to caption
Figure 1. The images of the spherical logarithm im(logt(Φ))\mathrm{im}(\log_{t}(\Phi)) approach the valuation cone as t0t\to 0 for the case (SL3()×SL3())/SL3()(\operatorname{SL}_{3}(\mathbb{C})\times\operatorname{SL}_{3}(\mathbb{C}))/\operatorname{SL}_{3}(\mathbb{C}).

4.3. The basic affine space SLn()/U\operatorname{SL}_{n}(\mathbb{C})/U

Consider the spherical homogeneous space G/UG/U where UU is a maximal unipotent subgroup (see Example 1.1(4)). One knows that G/UG/U is a quasi-affine variety. The ring of regular functions [G/U]\mathbb{C}[G/U] can be identified with the ring [G]U\mathbb{C}[G]^{U} of (right) UU-invariants. Thus, as a GG-module it decomposes as:

[G]=λΛ+Vλ.\mathbb{C}[G]=\bigoplus_{\lambda\in\Lambda^{+}}V_{\lambda}^{*}\text{.}

Moreover, the multiplication in the algebra [G/U]\mathbb{C}[G/U] corresponds to Cartan multiplication between the VλV_{\lambda}^{*}. It follows that the tail cone consists of the origin only and hence the valuation cone 𝒱G/U\mathcal{V}_{G/U} is the whole vectors space 𝒬G/U=Λ\mathcal{Q}_{G/U}=\Lambda_{\mathbb{Q}}.

Let us give an explicit description of the spherical functions on G/UG/U in the case of G=SLn()G=\operatorname{SL}_{n}(\mathbb{C}). One can take UU to be the subgroup of upper triangular matrices with 11’s on the diagonal. Set V=nV=\mathbb{C}^{n} and consider the natural action of SLn()\operatorname{SL}_{n}(\mathbb{C}) on the exterior algebra ΛV\Lambda^{*}V. If e1,,ene_{1},\ldots,e_{n} are the standard basis vectors of VV, then the stabilizer of x0(e1,e1e2,,e1en)x_{0}\coloneqq(e_{1},e_{1}\wedge e_{2},\ldots,e_{1}\wedge\ldots\wedge e_{n}) is UU. As SLn()ΛV\operatorname{SL}_{n}(\mathbb{C})\to\Lambda^{*}V is a locally closed embedding with quasi-affine image, we obtain a surjective map [ΛV][SLn()/U]\mathbb{C}[\Lambda^{*}V]\to\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/U] and it straightforwardly follows that the algebra [SLn()]U\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})]^{U} is generated by the so-called flag minors: Let xSLn()x\in\operatorname{SL}_{n}(\mathbb{C}). For subsets I,J{1,,n}I,J\subset\{1,\ldots,n\} with |I|=|J|=i|I|=|J|=i, let pI,J(x)p_{I,J}(x) denote the minor of xx which is the determinant of the i×ii\times i submatrix of xx with rows corresponding to II and columns corresponding to JJ. A flag minor is a minor of the form pI,{1,,i}p_{I,\{1,\ldots,i\}}, that is when J={1,,i}J=\{1,\ldots,i\} corresponds to the first ii columns of xx.

Let Γ={ω1,,ωn1}\Gamma=\{\omega_{1},\ldots,\omega_{n-1}\}. There are n1n-1 spherical functions corresponding to the fundamental weights ω1,,ωn1\omega_{1},\ldots,\omega_{n-1}. The representation VωiV_{\omega_{i}} corresponding to the ii-th fundamental weight is iV\bigwedge^{i}V and the i×ii\times i flag minors are a vector space basis consisting of weight vectors. Consider the standard Hermitian product on VV. This induces Hermitian products on iV\bigwedge^{i}V for al ii. One verifies that, for each ii, the vector {ej1eji1j1<<jii}\{e_{j_{1}}\wedge\cdots e_{j_{i}}\mid 1\leq j_{1}<\cdots<j_{i}\leq i\} is an orthonormal basis for iV\bigwedge^{i}V. It follows that the flag minors are an orthonormal basis for iV[SLn()]U\bigwedge^{i}V\subset\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})]^{U}. Thus the ii-th spherical function ϕi\phi_{i} corresponding to ωi\omega_{i} is given by:

ϕi(x)=I|pI,{1,,i}(x)|2,\phi_{i}(x)=\sum_{I}|p_{I,\{1,\ldots,i\}}(x)|^{2}\text{,}

where the sum is over all subsets I{1,,n}I\subset\{1,\ldots,n\} with |I|=i|I|=i. Note that ϕi(eU)=1\phi_{i}(eU)=1. Consider the spherical logarithm map sLogΓ,t\operatorname{sLog}_{\Gamma,t} corresponding to our choice of Γ\Gamma. We have

x=(t1t11t2tn21tn1tn11)SLn()x=\begin{pmatrix}t_{1}&&&&\\ &t_{1}^{-1}t_{2}^{\mbox{}}&&&\\ &&\ddots&&\\ &&&t_{n-2}^{-1}t_{n-1}^{\mbox{}}&\\ &&&&t_{n-1}^{-1}\end{pmatrix}\in\operatorname{SL}_{n}(\mathbb{C})

with sLogΓ,t(x)=(logt|t1|2,,logt|tn1|2)\operatorname{sLog}_{\Gamma,t}(x)=(\log_{t}|t_{1}|^{2},\ldots,\log_{t}|t_{n-1}|^{2}), and thus the image of sLogΓ,t\operatorname{sLog}_{\Gamma,t} is the whole space n1\mathbb{R}^{n-1} and agrees (for all tt) with the valuation cone.

4.4. Example of SLn()/SLn1()\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})

Throughout this section, we let G=SLn()G=\operatorname{SL}_{n}(\mathbb{C}) and H=SLn1()H=\operatorname{SL}_{n-1}(\mathbb{C}) for n3n\geq 3. The variety G/HG/H is a very well-known example of a spherical homogeneous space. Nevertheless, for the convenience of the reader we try to give details of the proofs in this section.

The maximal compact subgroup of SLn()\operatorname{SL}_{n}(\mathbb{C}) is KSUnK\coloneqq\operatorname{SU}_{n} which we realize explicitly as

SUn={An×n:A¯tA=In}\operatorname{SU}_{n}=\mathopen{}\mathclose{{}\left\{{A\in\mathbb{C}^{n\times n}\,\colon\,\overline{A}^{t}A=I_{n}}}\right\}

where A¯t\overline{A}^{t} denotes the conjugate transpose. Let SLn()\operatorname{SL}_{n}(\mathbb{C}) act on n×n\mathbb{C}^{n}\times\mathbb{C}^{n} as follows:

(15) SLn()×(n×n)n×n;(A,𝐯,𝐰)(A𝐯,tA1𝐰).\operatorname{SL}_{n}(\mathbb{C})\times\mathopen{}\mathclose{{}\left(\mathbb{C}^{n}\times\mathbb{C}^{n}}\right)\to\mathbb{C}^{n}\times\mathbb{C}^{n};(A,\mathbf{v},\mathbf{w})\mapsto(A\mathbf{v},\prescript{t}{}{A}^{-1}\mathbf{w})\text{.}

We denote the standard basis of n\mathbb{C}^{n} by 𝐞1,,𝐞n\mathbf{e}_{1},\ldots,\mathbf{e}_{n} and the coordinates on the two n\mathbb{C}^{n} factors by x1,,xnx_{1},\ldots,x_{n} and y1,,yny_{1},\ldots,y_{n} respectively. With respect to the action (15) it is straightforward to compute that the stabilizer of (e1,e1)n×n(e_{1},e_{1})\in\mathbb{C}^{n}\times\mathbb{C}^{n} is

StabSLn()(𝐞1,𝐞1)={10000()SLn1}SLn1().\operatorname{Stab}_{\operatorname{SL}_{n}(\mathbb{C})}(\mathbf{e}_{1},\mathbf{e}_{1})=\mathopen{}\mathclose{{}\left\{{\leavevmode\hbox to66.1pt{\vbox to65.64pt{\pgfpicture\makeatletter\hbox{\hskip 2.66667pt\lower-32.91942pt\hbox to0.0pt{\pgfsys@beginscope\pgfsys@invoke{ }\definecolor{pgfstrokecolor}{rgb}{0,0,0}\pgfsys@color@rgb@stroke{0}{0}{0}\pgfsys@invoke{ }\pgfsys@color@rgb@fill{0}{0}{0}\pgfsys@invoke{ }\pgfsys@setlinewidth{0.4pt}\pgfsys@invoke{ }\nullfont\hbox to0.0pt{\pgfsys@beginscope\pgfsys@invoke{ }{{}{}{}{{}}{{}}{{}}{{}}{ {}}{{}}{{}}\hbox{\hbox{\hbox{\hbox{{\pgfsys@beginscope\pgfsys@invoke{ }{\offinterlineskip{}{}{{{}}{{}}{{}}{{}}{{}}{{}}{{}}{{}}{{}}{{}}{{}}{{}}{{}}{{}}{{}}{{}}}{{{}}}{{}{}{{ {}{}}}{ {}{}} {{}{{}}}{{}{}}{}{{}{}} { }{{{{}}\pgfsys@beginscope\pgfsys@invoke{ }\pgfsys@transformcm{1.0}{0.0}{0.0}{1.0}{0.2pt}{-30.01942pt}\pgfsys@invoke{ 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{{}\pgfsys@rect{25.36723pt}{-32.71942pt}{31.9pt}{35.99442pt}\pgfsys@stroke\pgfsys@invoke{ } }{{{{}}\pgfsys@beginscope\pgfsys@invoke{ }\pgfsys@transformcm{1.0}{0.0}{0.0}{1.0}{24.36723pt}{-14.72221pt}\pgfsys@invoke{ }\hbox{{\definecolor{pgfstrokecolor}{rgb}{0,0,0}\pgfsys@color@rgb@stroke{0}{0}{0}\pgfsys@invoke{ }\pgfsys@color@rgb@fill{0}{0}{0}\pgfsys@invoke{ }\hbox{\minipage[t]{33.9pt}\endminipage} }}\pgfsys@invoke{\lxSVG@closescope }\pgfsys@endscope}}} \pgfsys@invoke{\lxSVG@closescope }\pgfsys@endscope}}}\hbox{{\pgfsys@beginscope\pgfsys@invoke{ }{{}{}{{ {}{}}}{ {}{}} {{}{{}}}{{}{}}{}{{}{}} { }{{{{}}\pgfsys@beginscope\pgfsys@invoke{ }\pgfsys@transformcm{1.0}{0.0}{0.0}{1.0}{31.40044pt}{-17.23665pt}\pgfsys@invoke{ }\hbox{{\definecolor{pgfstrokecolor}{rgb}{0,0,0}\pgfsys@color@rgb@stroke{0}{0}{0}\pgfsys@invoke{ }\pgfsys@color@rgb@fill{0}{0}{0}\pgfsys@invoke{ }\hbox{{$\operatorname{SL}_{n-1}$}} }}\pgfsys@invoke{\lxSVG@closescope }\pgfsys@endscope}}} \pgfsys@invoke{\lxSVG@closescope }\pgfsys@endscope}}} } \pgfsys@invoke{\lxSVG@closescope }\pgfsys@endscope{{ {}{}{}}}{}{}\hss}\pgfsys@discardpath\pgfsys@invoke{\lxSVG@closescope }\pgfsys@endscope\hss}}\lxSVG@closescope\endpgfpicture}}}}\right\}\cong\operatorname{SL}_{n-1}(\mathbb{C})\text{.}
Lemma 4.1.
SLn()(𝐞1,𝐞1)={(𝐱,𝐲)n×n:i=1nxiyi=𝐲t𝐱=1}n×n\operatorname{SL}_{n}(\mathbb{C})\cdot(\mathbf{e}_{1},\mathbf{e}_{1})=\mathopen{}\mathclose{{}\left\{{(\mathbf{x},\mathbf{y})\in\mathbb{C}^{n}\times\mathbb{C}^{n}\,\colon\,\sum_{i=1}^{n}x_{i}y_{i}=\mathbf{y}^{t}\mathbf{x}=1}}\right\}\subseteq\mathbb{C}^{n}\times\mathbb{C}^{n}

where we use the notation 𝐲:=(y1,,yn)\mathbf{y}:=(y_{1},\ldots,y_{n}) and 𝐱:=(x1,,xn)\mathbf{x}:=(x_{1},\ldots,x_{n}).

Proof.

The inclusion “\subseteq” is straightforward, since for any ASLn()A\in\operatorname{SL}_{n}(\mathbb{C}), it immediately follows from the definition of the action that A(e1,e1):=(𝐱=Ae1,𝐲=tA1e1)A\cdot(e_{1},e_{1}):=(\mathbf{x}=Ae_{1},\mathbf{y}=\prescript{t}{}{A}^{-1}e_{1}) would have the property 𝐲t𝐱=e1t(tA1)tAe1=e1tA1Ae1=e1te1=1\mathbf{y}^{t}\mathbf{x}=e_{1}^{t}(\prescript{t}{}{A}^{-1})^{t}Ae_{1}=e_{1}^{t}A^{-1}Ae_{1}=e_{1}^{t}e_{1}=1.

To see the inclusion “\supseteq”, suppose that (𝐱,𝐲)n×n(\mathbf{x},\mathbf{y})\in\mathbb{C}^{n}\times\mathbb{C}^{n} satisfies 𝐲t𝐱=1\mathbf{y}^{t}\mathbf{x}=1. We wish to find an element in SLn()\operatorname{SL}_{n}(\mathbb{C}) that takes (e1,e1)(e_{1},e_{1}) to (𝐱,𝐲)(\mathbf{x},\mathbf{y}). First notice that since 𝐲0\mathbf{y}\neq 0, there must exist some matrix g=(aij)SLn()g=(a_{ij})\in\operatorname{SL}_{n}(\mathbb{C}) with the property that the top row of gg is (y1,y2,,yn)(y_{1},y_{2},\ldots,y_{n}). Now define a matrix gg^{\prime} by replacing the first column of g1g^{-1} with (x1,,xn)t(x_{1},\ldots,x_{n})^{t} (a column vector). We claim that gg^{\prime} is an element in SLn()\operatorname{SL}_{n}(\mathbb{C}) and that g(e1,e1)=(𝐱,𝐲)g^{\prime}\cdot(e_{1},e_{1})=(\mathbf{x},\mathbf{y}). By construction we have ge1=𝐱ge_{1}=\mathbf{x}, so it remains to see that gSLn()g^{\prime}\in\operatorname{SL}_{n}(\mathbb{C}) and that tg1e1=𝐲\prescript{t}{}{g}^{-1}e_{1}=\mathbf{y}.

We claim gSLn()g^{\prime}\in\operatorname{SL}_{n}(\mathbb{C}). To see that det(g)=1\det(g^{\prime})=1 we make an explicit computation. Given an n×nn\times n matrix AA we denote by Ai,jA_{i,j} the (n1)×(n1)(n-1)\times(n-1) matrix obtained by deleting its ii-th row and jj-th column. Below we compute deg(g)\deg(g^{\prime}) by expansion along its left-most column, which by construction is 𝐱\mathbf{x}.

det(g)=i=1n(1)i+1xidet(gi,1)=i=1n(1)i+1xidet((g1)i,1) since g is the same as g1 except for the leftmost col=i=1nxia1,i by Cramer’s rule for matrix inverses and since (g1)1=g=i=1nxiyi since the top row of g is 𝐲 by construction=1 by assumption on 𝐱 and 𝐲.\begin{split}\det(g^{\prime})&=\sum_{i=1}^{n}(-1)^{i+1}x_{i}\cdot\det(g^{\prime}_{i,1})\\ &=\sum_{i=1}^{n}(-1)^{i+1}x_{i}\cdot\det((g^{-1})_{i,1})\textup{ since $g^{\prime}$ is the same as $g^{-1}$ except for the leftmost col}\\ &=\sum_{i=1}^{n}x_{i}a_{1,i}\textup{ by Cramer's rule for matrix inverses and since $(g^{-1})^{-1}=g$}\\ &=\sum_{i=1}^{n}x_{i}y_{i}\textup{ since the top row of $g$ is $\mathbf{y}$ by construction}\\ &=1\textup{ by assumption on $\mathbf{x}$ and $\mathbf{y}$.}\\ \end{split}

We next claim that t(g)1e1=𝐲\prescript{t}{}{(g^{\prime})}^{-1}e_{1}=\mathbf{y}, or in other words, that (g)1(g^{\prime})^{-1} has top row equal to 𝐲\mathbf{y}. By a Cramer’s rule argument similar to that above, we can see that the (1,i)(1,i)-th matrix entry of (g)1(g^{\prime})^{-1} is the (i,1)(i,1)-th cofactor of gg^{\prime}, which is equal to the (i,1)(i,1)-th cofactor of g1g^{-1}, which in turn is equal to the (1,i)(1,i)-th entry of (g1)1=g(g^{-1})^{-1}=g. But this last value is exactly yiy_{i} by construction of gg, so we are done. ∎

It follows from the above lemma that the homogeneous space SLn()/SLn1()\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}) is an affine variety and its coordinate ring may be identified as

[SLn()/SLn1()][x1,,xn,y1,,yn]/i=1nxiyi=1.\mathbb{C}\mathopen{}\mathclose{{}\left[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})}\right]\cong\mathbb{C}\mathopen{}\mathclose{{}\left[x_{1},\ldots,x_{n},y_{1},\ldots,y_{n}}\right]/\mathopen{}\mathclose{{}\left\langle\sum_{i=1}^{n}x_{i}y_{i}=1}\right\rangle\text{.}

Let BB be the Borel subgroup of upper triangular matrices in SLn()\operatorname{SL}_{n}(\mathbb{C}) and TBT\subseteq B the maximal torus consisting of all diagonal matrices in SLn()\operatorname{SL}_{n}(\mathbb{C}). Let UU be the maximal unipotent subgroup of BB consisting of upper triangular matrices with 11’s on the diagonal. We show next that the homogeneous space SLn()/SLn1()\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}) is in fact spherical, i.e., has a dense open BB-orbit. We have the following.

Lemma 4.2.

The subset

B(𝐞1+𝐞n,𝐞1)={(𝐱,𝐲)n×n:𝐲t𝐱=1 and xny10}.B\cdot(\mathbf{e}_{1}+\mathbf{e}_{n},\mathbf{e}_{1})=\mathopen{}\mathclose{{}\left\{{(\mathbf{x},\mathbf{y})\in\mathbb{C}^{n}\times\mathbb{C}^{n}\,\colon\,\mathbf{y}^{t}\mathbf{x}=1\textup{ and }x_{n}y_{1}\neq 0}}\right\}\text{.}

is a dense open BB-orbit in SLn()/SLn1()\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}). In particular, SLn()/SLn1()\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}) is a spherical homogeneous space.

Proof.

The inclusion “\subseteq” is straightforward. To show the reverse inclusion, let (𝐱,𝐲)n×n(\mathbf{x},\mathbf{y})\in\mathbb{C}^{n}\times\mathbb{C}^{n} with i=1nxiyi=1\sum_{i=1}^{n}x_{i}y_{i}=1 and xny10x_{n}y_{1}\neq 0. Consider the matrix

A(1y1y2y1yn2y1yn1xnx11y1100x210xn2y1xnxn1xn)B.A\coloneqq\begin{pmatrix}\tfrac{1}{y_{1}}&\tfrac{-y_{2}}{y_{1}}&\ldots&\tfrac{-y_{n-2}}{y_{1}}&\tfrac{-y_{n-1}}{x_{n}}&x_{1}-\tfrac{1}{y_{1}}\\ &1&0&\ldots&0&x_{2}\\ &&\ddots&\ddots&\vdots&\vdots\\ &&&1&0&x_{n-2}\\ &&&&\tfrac{y_{1}}{x_{n}}&x_{n-1}\\ &&&&&x_{n}\end{pmatrix}\in B\text{.}

We claim that AA is in the Borel subgroup BB of SLn()\operatorname{SL}_{n}(\mathbb{C}) and that A(𝐞1+𝐞n,𝐞1)=(𝐱,𝐲)A\cdot(\mathbf{e}_{1}+\mathbf{e}_{n},\mathbf{e}_{1})=(\mathbf{x},\mathbf{y}). By construction AA is upper-triangular, and from the diagonal entries it easily follows that det(A)=1\det(A)=1, so AA is in BB. It is straightforward to see from the definition of AA that A(𝐞1+𝐞n)=𝐱A(\mathbf{e}_{1}+\mathbf{e}_{n})=\mathbf{x}. To see that tA1𝐞1=𝐲\prescript{t}{}{A}^{-1}\mathbf{e}_{1}=\mathbf{y}, it suffices to see that the top row of A1A^{-1} is 𝐲\mathbf{y}. Moreover, since ixiyi=1\sum_{i}x_{i}y_{i}=1, the last entry yny_{n} is determined by 𝐱\mathbf{x} and y1,,yn1y_{1},\ldots,y_{n-1}, it in fact suffices to check the first n1n-1 entries. Fix jj with 1jn11\leq j\leq n-1. We wish to show that the (1,j)(1,j)-th entry of A1A^{-1} is equal to yjy_{j}. It is straightforward to check this explicitly using the adjoint form of AA as in the proof of the previous lemma and the explicit formula for AA given above. ∎

We now describe parts of the Luna-Vust data associated to the spherical homogeneous space G/H=SLn()/SLn1()G/H=\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}). Recall that the colors 𝒟\mathcal{D} of G/HG/H is defined to be the set of BB-invariant prime divisors of G/HG/H. From Lemma 4.2 we know the open BB-orbit is defined by the condition xny10x_{n}y_{1}\neq 0, so any BB-invariant prime divisor is contained in its complement {xn=0 or y1=0}={xn=0}{y1=0}\{x_{n}=0\textup{ or }y_{1}=0\}=\{x_{n}=0\}\cup\{y_{1}=0\}.

Lemma 4.3.

The two elements xn,y1x_{n},y_{1} are prime elements in [SLn/SLn1]\mathbb{C}[\operatorname{SL}_{n}/\operatorname{SL}_{n-1}].

Proof.

To see that xnx_{n} is a prime element, it would suffice to show that [SLn/SLn1]/xn\mathbb{C}[\operatorname{SL}_{n}/\operatorname{SL}_{n-1}]/\mathopen{}\mathclose{{}\left\langle x_{n}}\right\rangle is a domain. Note that there is an isomorphism

[SLn/SLn1]/xn=[x1,,xn1,y1,,yn]/x1y1++xn1yn11\mathbb{C}[\operatorname{SL}_{n}/\operatorname{SL}_{n-1}]/\mathopen{}\mathclose{{}\left\langle x_{n}}\right\rangle=\mathbb{C}[x_{1},\ldots,x_{n-1},y_{1},\ldots,y_{n}]/\mathopen{}\mathclose{{}\left\langle x_{1}y_{1}+\ldots+x_{n-1}y_{n-1}-1}\right\rangle

so it suffices to show that the RHS is a domain. Since the polynomial x1y1++xn1yn11x_{1}y_{1}+\ldots+x_{n-1}y_{n-1}-1 is of degree 22, if it factors non-trivially then it must be of the form x1y1++xn1yn11=ghx_{1}y_{1}+\ldots+x_{n-1}y_{n-1}-1=g\cdot h where deg(g)=deg(h)=1\deg(g)=\deg(h)=1 so both gg and hh are linear polynomials in x1,,xn1,y1,,yn1x_{1},\ldots,x_{n-1},y_{1},\ldots,y_{n-1} (with constant term). It is not hard to see by direct computation that this is impossible, so x1y1++xn1yn11x_{1}y_{1}+\ldots+x_{n-1}y_{n-1}-1 is irreducible and hence the RHS of the equality above is an integral domain. We conclude xnx_{n} is prime in [SLn/SLn1]\mathbb{C}[\operatorname{SL}_{n}/\operatorname{SL}_{n-1}], as desired. The argument for y1y_{1} is similar. ∎

From Lemma 4.3 it follows that D1={xn=0}D_{1}=\{x_{n}=0\} and D2={y1=0}D_{2}=\{y_{1}=0\} are prime divisors. Moreover, it is immediate from (15) that both are BB-invariant. It follows that D1,D2D_{1},D_{2} are the two colors in SLn(C)/SLn1()\operatorname{SL}_{n}(C)/\operatorname{SL}_{n-1}(\mathbb{C}), i.e., 𝒟={D1,D2}\mathcal{D}=\{D_{1},D_{2}\}.

Remark 4.4.

Note that (𝐞1,𝐞1)(\mathbf{e}_{1},\mathbf{e}_{1}) is not contained in the open BB-orbit and the colors consist of several BB-orbits. Indeed, we have the following “interesting” BB-orbits:

  • (𝐞1+𝐞n,𝐞1)(\mathbf{e}_{1}+\mathbf{e}_{n},\mathbf{e}_{1}) is a base point of the open BB-orbit in SLn/SLn1\operatorname{SL}_{n}/\operatorname{SL}_{n-1}.

  • B(𝐞1+𝐞n1,𝐞1)B\cdot(\mathbf{e}_{1}+\mathbf{e}_{n-1},\mathbf{e}_{1}) is the open BB-orbit of the color D1={xn=0}D_{1}=\mathopen{}\mathclose{{}\left\{{x_{n}=0}}\right\}.

  • B(𝐞1++𝐞n,𝐞2)B\cdot(\mathbf{e}_{1}+\ldots+\mathbf{e}_{n},\mathbf{e}_{2}) is the open BB-orbit of the color D2={y1=0}D_{2}=\mathopen{}\mathclose{{}\left\{{y_{1}=0}}\right\}.

Note that the colors D1,D2D_{1},D_{2} are each a union of multiple BB-orbits.

Next, we need to compute the BB-semi-invariants in the ring [SLn()/SLn1()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})]. We need some preparation.

Lemma 4.5.

The coordinate ring [SLn()/SLn1()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})] is a UFD, a unique factorization domain. Moreover, the units [SLn()/SLn1()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})]^{*} in [SLn()/SLn1()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})] consists of the non-zero constants, i.e. [SLn()/SLn1()]=\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})]^{*}=\mathbb{C}^{*}.

Proof.

Consider the localization of [SLn/SLn1]\mathbb{C}[\operatorname{SL}_{n}/\operatorname{SL}_{n-1}] by the prime element xnx_{n} and observe that we have an isomorphism

[SLn/SLn1]xn[x1,,xn,y1,,yn1,xn1]\mathbb{C}[\operatorname{SL}_{n}/\operatorname{SL}_{n-1}]_{x_{n}}\cong\mathbb{C}[x_{1},\ldots,x_{n},y_{1},\ldots,y_{n-1},x_{n}^{-1}]

since yn=(1i=1n1xiyi)/xny_{n}=(1-\sum_{i=1}^{n-1}x_{i}y_{i})/x_{n}. In particular, the ring on the right hand side is a UFD. From [Eisenbud, Lemma 19.20] we know that if RR is an integral domain and pp a prime element and the localization RpR_{p} is a UFD, then RR is a UFD. Applying this to R=[SLn()/SLn1()]R=\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})] and p=xnp=x_{n}, we conclude that [SLn/SLn1]\mathbb{C}[\operatorname{SL}_{n}/\operatorname{SL}_{n-1}] is also a UFD.

Now we wish to prove the claim about the units. Embed [SLn()/SLn1()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})] into the localization [SLn()/SLn1()]xn[x1,,xn,xn1,y1,,yn1]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})]_{x_{n}}\cong\mathbb{C}[x_{1},\ldots,x_{n},x_{n}^{-1},y_{1},\ldots,y_{n-1}]. In particular, any unit in [SLn()/SLn1()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})] must also be a unit in the localization. The units of [x1,,xn,xn1,y1,,yn1]\mathbb{C}[x_{1},\ldots,x_{n},x_{n}^{-1},y_{1},\ldots,y_{n-1}] are of the form cxnkcx_{n}^{k} for cc\in\mathbb{C}^{*} and kk\in\mathbb{Z}. However, xnx_{n} is a prime element in [SLn()/SLn1()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})], so it is not a unit in [SLn()/SLn1()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})]. Thus the only units in [SLn()/SLn1()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})] are the non-zero constants. ∎

Recall that a function f[SLn()/SLn1()]f\in\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})] is called BB-semi-invariant if there exists a character χf𝒳(B)\chi_{f}\in\mathcal{X}(B) such that bf=χf(b)fb\cdot f=\chi_{f}(b)f for all bBb\in B. The set of BB-semi-invariants is denoted [SLn()/SLn1()](B)\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})]^{(B)}. From the above lemma we can deduce the following.

Corollary 4.6.

We have

[SLn()/SLn1()](B)={xnky1:k,0}.\mathbb{C}\mathopen{}\mathclose{{}\left[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})}\right]^{(B)}=\mathopen{}\mathclose{{}\left\{{x_{n}^{k}y_{1}^{\ell}\,\colon\,k,\ell\in\mathbb{Z}_{\geq 0}}}\right\}\text{.}
Proof.

Let f[SLn/SLn1](B)f\in\mathbb{C}[\operatorname{SL}_{n}/\operatorname{SL}_{n-1}]^{(B)} be non-zero and BB-semi-invariant. Then the vanishing locus of ff must be contained in {xny1=0}\{x_{n}y_{1}=0\} since ff cannot vanish on the dense open BB-orbit {xny10}\{x_{n}y_{1}\neq 0\} (see Lemma 4.2). Thus div(f)=k1D1+k2D2\operatorname{div}(f)=k_{1}D_{1}+k_{2}D_{2} for some non-negative integers k1k_{1} and k2k_{2} and f/(xnk1y1k2)f/(x_{n}^{k_{1}}y_{1}^{k_{2}}) is an invertible regular function on SLn/SLn1\operatorname{SL}_{n}/\operatorname{SL}_{n-1}. In particular, it is a unit in [SLn()/SLn1()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})]. We saw in Lemma 4.5 that the units are the non-zero constants, so we conclude that f=cxnk1y1k2f=cx_{n}^{k_{1}}y_{1}^{k_{2}} for some cc\in\mathbb{C}^{*}, as desired. ∎

We can now compute Λ+G/H\Lambda^{+}_{G/H}. Let ω1,,ωn1\omega_{1},\ldots,\omega_{n-1} be the fundamental weights associated to our choice (B,T)(B,T), i.e., for i=1,,n1i=1,\ldots,n-1 we have

ωi(b11b12b1nb22b2nbnn)=j=1ibjj=b11bii.\omega_{i}\begin{pmatrix}b_{11}&b_{12}&\ldots&b_{1n}\\ &b_{22}&\ldots&b_{2n}\\ &&\ddots&\vdots\\ &&&b_{nn}\end{pmatrix}=\prod_{j=1}^{i}b_{jj}=b_{11}\cdots b_{ii}\text{.}

It is straightforward to compute that the BB-weights of xnx_{n} and y1y_{1} are χ1ωn1\chi_{1}\coloneqq\omega_{n-1} and χ2ω1\chi_{2}\coloneqq\omega_{1} respectively. The association fχff\mapsto\chi_{f} gives a map [SLn()/SLn1()](B)𝒳(B)\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})]^{(B)}\to\mathcal{X}(B) whose image is denoted Λ+G/H=Λ+SLn/SLn1\Lambda^{+}_{G/H}=\Lambda^{+}_{\operatorname{SL}_{n}/\operatorname{SL}_{n-1}}. If f,g[SLn()/SLn1()](B)f,g\in\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})]^{(B)} then χfg=χf+χg\chi_{f\cdot g}=\chi_{f}+\chi_{g} so Λ+SLn/SLn1\Lambda^{+}_{\operatorname{SL}_{n}/\operatorname{SL}_{n-1}} is a semigroup. In our case G/H=SLn()/SLn1()G/H=\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}), the above computation shows that ΛG/H+\Lambda_{G/H}^{+} is freely generated by χ1\chi_{1} and χ2\chi_{2}, i.e. ΛG/H+0χ10χ202\Lambda_{G/H}^{+}\cong\mathbb{Z}_{\geq 0}\chi_{1}\oplus\mathbb{Z}_{\geq 0}\chi_{2}\cong\mathbb{Z}_{\geq 0}^{2}. For what follows, we choose Γ={χ1,χ2}\Gamma=\{\chi_{1},\chi_{2}\}, with associated BB-semi-invariant functions xn,y1x_{n},y_{1}. Note that Γ\Gamma is also a basis of ΛG/H\Lambda_{G/H}\otimes\mathbb{R}, and with respect to this choice of basis, the map ρ\rho of (2) becomes

ρ:𝒱SLn()/SLn1()𝒬,ν(ν(xn),ν(y1)).\rho:\mathcal{V}_{\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})}\hookrightarrow\mathcal{Q},~{}\nu\mapsto(\nu(x_{n}),\nu(y_{1})).

We have the following, where we temporarily work over \mathbb{Q}, the most natural setting for this lemma.

Lemma 4.7.

The image of 𝒱SLn()/SLn1()\mathcal{V}_{\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})} under ρ\rho is

(16) ρ(𝒱SLn()/SLn1())={(q1,q2)2:q1+q20}.\rho(\mathcal{V}_{\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})})=\mathopen{}\mathclose{{}\left\{{(q_{1},q_{2})\in\mathbb{Q}^{2}\,\colon\,q_{1}+q_{2}\leq 0}}\right\}\text{.}
Proof.

We first show that the LHS is contained in the RHS. Let ν𝒱(G/H)\nu\in\mathcal{V}(G/H). For any ii with 1in1\leq i\leq n, there is a permutation gSLn()g\in\operatorname{SL}_{n}(\mathbb{C}) of the coordinates such that gxn=xig\cdot x_{n}=x_{i}. A similar statement holds for y1y_{1} and yiy_{i}. Since ν\nu is SLn()\operatorname{SL}_{n}(\mathbb{C})-invariant, it follows that

ν(x1)==ν(xn)andν(y1)==ν(yn).\nu(x_{1})=\ldots=\nu(x_{n})\qquad\text{and}\qquad\nu(y_{1})=\ldots=\nu(y_{n})\text{.}

On the other hand, since i=1nxiyi=1\sum_{i=1}^{n}x_{i}y_{i}=1 in [SLn/SLn1]\mathbb{C}[\operatorname{SL}_{n}/\operatorname{SL}_{n-1}], we obtain from the axioms of valuations that

0=ν(1)=ν(x1y1+xnyn)min{ν(x1y1),,ν(xnyn)}=min{ν(x1)+ν(y1),,ν(xn)+ν(yn)}=ν(x1)+ν(y1)=ν(xn)+ν(y1).\begin{split}0=\nu(1)=\nu(x_{1}y_{1}+\ldots x_{n}y_{n})&\geq\mathrm{min}\{\nu(x_{1}y_{1}),\ldots,\nu(x_{n}y_{n})\}\\ &=\mathrm{min}\{\nu(x_{1})+\nu(y_{1}),\ldots,\nu(x_{n})+\nu(y_{n})\}=\nu(x_{1})+\nu(y_{1})\\ &=\nu(x_{n})+\nu(y_{1})\text{.}\\ \end{split}

Hence ρ(ν)\rho(\nu) lies in the RHS of (16), as desired.

We now claim that the RHS is contained in the LHS. By Theorem 1.5 the image ρ(𝒱SLn/SLn1)\rho(\mathcal{V}_{\operatorname{SL}_{n}/\operatorname{SL}_{n-1}}) is a (rational) polyhedral cone, in order to show that the RHS is contained in the LHS, it suffices to show that integral points in the RHS are contained in the LHS. Let (n1,n2)2(n_{1},n_{2})\in\mathbb{Z}^{2} with n1+n20n_{1}+n_{2}\leq 0. Consider the subvariety

W{u1v1++unvnwn1n2=0}n×n×W\coloneqq\mathopen{}\mathclose{{}\left\{{u_{1}v_{1}+\ldots+u_{n}v_{n}-w^{-n_{1}-n_{2}}=0}}\right\}\subseteq\mathbb{C}^{n}\times\mathbb{C}^{n}\times\mathbb{C}

and consider the SLn()\operatorname{SL}_{n}(\mathbb{C})-action on n×n×\mathbb{C}^{n}\times\mathbb{C}^{n}\times\mathbb{C} given as the product of the given SLn()\operatorname{SL}_{n}(\mathbb{C})-action on n×n\mathbb{C}^{n}\times\mathbb{C}^{n} and the trivial action on the last \mathbb{C} factor. This induces an SLn()\operatorname{SL}_{n}(\mathbb{C})-action on WW: indeed, if 𝐮tIn𝐯=wn1n2\mathbf{u}^{t}I_{n}\mathbf{v}=w^{-n_{1}-n_{2}}, then for ASLnA\in\operatorname{SL}_{n}, we have (A𝐮)tIn(At)1𝐯=wn1n2(A\mathbf{u})^{t}I_{n}(A^{t})^{-1}\mathbf{v}=w^{-n_{1}-n_{2}}. Note that D:={w=0}D:=\mathopen{}\mathclose{{}\left\{{w=0}}\right\} is SLn()\operatorname{SL}_{n}(\mathbb{C})-invariant, so W{w=0}W\setminus\mathopen{}\mathclose{{}\left\{{w=0}}\right\} is also invariant. There is an SLn\operatorname{SL}_{n}-equivariant projection

W{w=0}SLn/SLn1;(𝐮,𝐯,w)(wn1𝐮,wn2𝐯)W\setminus\mathopen{}\mathclose{{}\left\{{w=0}}\right\}\to\operatorname{SL}_{n}/\operatorname{SL}_{n-1};(\mathbf{u},\mathbf{v},w)\mapsto(w^{n_{1}}\mathbf{u},w^{n_{2}}\mathbf{v})

which induces an inclusion of the corresponding function fields (SLn/SLn1)(W)\mathbb{C}(SL_{n}/\operatorname{SL}_{n-1})\hookrightarrow\mathbb{C}(W). We claim that DD is a prime divisor in WW. Indeed, z[W]z\in\mathbb{C}[W] is a prime element, since

[u1,,un,v1,,vn,w]/i=1nuiviwn1n2,w[u1,,un,v1,,vn]/i=1nuivi\mathbb{C}[u_{1},\ldots,u_{n},v_{1},\ldots,v_{n},w]/\mathopen{}\mathclose{{}\left\langle\sum_{i=1}^{n}u_{i}v_{i}-w^{-n_{1}-n_{2}},w}\right\rangle\cong\mathbb{C}[u_{1},\ldots,u_{n},v_{1},\ldots,v_{n}]/\mathopen{}\mathclose{{}\left\langle\sum_{i=1}^{n}u_{i}v_{i}}\right\rangle

and the ring on the RHS can be seen to be an integral domain from the fact that i=1nuivi\sum_{i=1}^{n}u_{i}v_{i} is irreducible in [u1,,un,v1,,vn]\mathbb{C}[u_{1},\ldots,u_{n},v_{1},\ldots,v_{n}] by an argument similar to the proof of Lemma 4.3. Thus we may define νD\nu_{D} to be the geometric valuation on (W)\mathbb{C}(W) given by the order of vanishing of a rational function along the (prime) divisor DD. Since DD is SLn\operatorname{SL}_{n}-invariant, this is an SLn\operatorname{SL}_{n}-invariant valuation, and the restriction νD|(SLn/SLn1)\nu_{D}|_{\mathbb{C}(\operatorname{SL}_{n}/\operatorname{SL}_{n-1})} to (the image of) (SLn()/SLn1())\mathbb{C}(\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})) yields an SLn\operatorname{SL}_{n}-invariant valuation in 𝒱SLn/SLn1\mathcal{V}_{\operatorname{SL}_{n}/\operatorname{SL}_{n-1}}. We compute

νD(xn)=νD(unwn1)=n1andνD(y1)=νD(v1wn2)=n2.\nu_{D}(x_{n})=\nu_{D}(u_{n}w^{n_{1}})=n_{1}\qquad\text{and}\qquad\nu_{D}(y_{1})=\nu_{D}(v_{1}w^{n_{2}})=n_{2}\text{.}

Thus we have shown that (n1,n2)(n_{1},n_{2}) lies in the image under ρ\rho of 𝒱SLn/SLn1\mathcal{V}_{\operatorname{SL}_{n}/\operatorname{SL}_{n-1}}, as desired. ∎

As discussed above, in order to compare the valuation cone with the image of the spherical logarithm we should tensor with \mathbb{R} and consider 𝒱¯SLn/SLn1\overline{\mathcal{V}}_{\operatorname{SL}_{n}/\operatorname{SL}_{n-1}}. It is clear that the closure is {(q1,q2)2:q1+q20}\{(q_{1},q_{2})\in\mathbb{R}^{2}:q_{1}+q_{2}\leq 0\} and this is what we consider as the valuation cone in Proposition 4.9 below.

The above discussion can be summarized in the following picture. The gray half-space defined by q1+q20q_{1}+q_{2}\leq 0 is the valuation cone 𝒱¯SLn/SLn1\overline{\mathcal{V}}_{\operatorname{SL}_{n}/\operatorname{SL}_{n-1}}. We have also indicated the images under ρ\rho of the (geometric valuations corresponding to the) two colors D1D_{1} and D2D_{2}; note that these do not lie in the valuation cone since they are not GG-invariant (only BB-invariant).

𝒱\mathcal{V}ρ(vD1)\rho(v_{D_{1}})ρ(vD2)\rho(v_{D_{2}})

Next we compute the spherical functions. Consider the decomposition [SLn()/SLn1()]λΛG/H+Vλ\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})]\cong\bigoplus_{\lambda\in\Lambda_{G/H}^{+}}V_{\lambda}. Let V=nV=\mathbb{C}^{n} the natural representation of SLn()\operatorname{SL}_{n}(\mathbb{C}) and VV^{*} its dual representation. Then VV has highest weight ω1\omega_{1} while the dual representation VV^{*} has highest weight ωn1\omega_{n-1}. The standard scalar product turns the standard bases into unitary bases on VV and VV^{*} respectively. Note that VV and VV^{*} are naturally embedded in [SLn()/SLn1()]\mathbb{C}[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})] by the identifications Vy1,,ynV\cong\langle y_{1},\ldots,y_{n}\rangle and V=x1,,xnV^{*}=\langle x_{1},\ldots,x_{n}\rangle. The variables x1,,xnx_{1},\ldots,x_{n} and y1,,yny_{1},\ldots,y_{n} form weight bases (with respect to TT) of VV^{*} and VV respectively. Hence, we can define, following (6) in Section 2, the following spherical functions:

(17) ϕωn1=|x1|2++|xn|2 and ϕω1=|y1|2++|yn|2\phi_{\omega_{n-1}}=|x_{1}|^{2}+\ldots+|x_{n}|^{2}\textup{ and }\phi_{\omega_{1}}=|y_{1}|^{2}+\ldots+|y_{n}|^{2}

both of which lie in ([SLn()/SLn1()][SLn()/SLn1()]¯)SUn\mathopen{}\mathclose{{}\left(\mathbb{C}\mathopen{}\mathclose{{}\left[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})}\right]\otimes\overline{\mathbb{C}\mathopen{}\mathclose{{}\left[\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})}\right]}}\right)^{\operatorname{SU}_{n}}.

Remark 4.8.

Note that ϕωn1\phi_{\omega_{n-1}} and ϕω1\phi_{\omega_{1}} are both SUn\operatorname{SU}_{n}-invariant, because x1,,xnx_{1},\ldots,x_{n} and y1,,yny_{1},\ldots,y_{n} are orthonormal and the action of SUn\operatorname{SU}_{n} leaves lengths invariant.

Finally, we analyze the spherical amoebas, i.e. the images sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) of G/HG/H under the spherical logarithm maps, and explicitly compute their limit as t0t\to 0. In our case of G/H=SLn()/SLn1()G/H=\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}) we can prove that the limit is precisely equal to the valuation cone, see Proposition 4.9. Recall that our spherical logarithm map is given by

sLogΓ,t:SLn()/SLn1()𝒬SLn/SLn12;(x,y)(logtϕωn1,logtϕω1).\operatorname{sLog}_{\Gamma,t}\colon\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C})\to\mathcal{Q}_{\operatorname{SL}_{n}/\operatorname{SL}_{n-1}}\cong\mathbb{R}^{2};(x,y)\mapsto(\log_{t}\phi_{\omega_{n-1}},\log_{t}\phi_{\omega_{1}}).

From (17) we can also express this more explicitly as

sLogΓ,t(x,y)=(logt(|x1|2++|xn|2),logt(|y1|2++|yn|2)).\operatorname{sLog}_{\Gamma,t}(x,y)=(\log_{t}(|x_{1}|^{2}+\ldots+|x_{n}|^{2}),\log_{t}(|y_{1}|^{2}+\ldots+|y_{n}|^{2}))\text{.}

In this special case, an explicit computation yields the following.

Proposition 4.9.

Let G=SLn()G=\operatorname{SL}_{n}(\mathbb{C}) and H=SLn1()H=\operatorname{SL}_{n-1}(\mathbb{C}). Then sLogΓ,tG/H)=𝒱G/H\operatorname{sLog}_{\Gamma,t}G/H)=\mathcal{V}_{G/H} for all t<1t<1. In particular, as tt approaches 0, the sets sLogΓ,t(G/H)\operatorname{sLog}_{\Gamma,t}(G/H) converge to the valuation cone 𝒱¯G/H\overline{\mathcal{V}}_{G/H} in the sense of Kuratowski.

Proof.

Let (𝐱,𝐲)SLn()/SLn1()(\mathbf{x},\mathbf{y})\in\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}), i.e., i=1nxiyi=1\sum_{i=1}^{n}x_{i}y_{i}=1. Let tt\in\mathbb{R} with 0<t<10<t<1. Then ln(t)<0\mathrm{ln}(t)<0 which implies that logt(x)=ln(x)ln(t)\log_{t}(x)=\frac{\ln(x)}{\ln(t)} is a strictly decreasing function on >0\mathbb{R}_{>0}. Using this, we can make the following computation:

0=logt|1|=logt|i=1nxiyi|logt(i=1n|xi|2i=1n|yi|2)=logt(i=1n|xi|2)+logt(i=1n|yi|2)=12logt(ϕωn1(𝐱,𝐲))+12logt(ϕω1(𝐱,𝐲))0=\log_{t}|1|=\log_{t}|\sum_{i=1}^{n}x_{i}y_{i}|\geq\log_{t}\mathopen{}\mathclose{{}\left(\sqrt{\sum_{i=1}^{n}|x_{i}|^{2}}\cdot\sqrt{\sum_{i=1}^{n}|y_{i}|^{2}}}\right)\\ =\log_{t}\mathopen{}\mathclose{{}\left(\sqrt{\sum_{i=1}^{n}|x_{i}|^{2}}}\right)+\log_{t}\mathopen{}\mathclose{{}\left(\sqrt{\sum_{i=1}^{n}|y_{i}|^{2}}}\right)=\tfrac{1}{2}\log_{t}(\phi_{\omega_{n-1}}(\mathbf{x},\mathbf{y}))+\tfrac{1}{2}\log_{t}(\phi_{\omega_{1}}(\mathbf{x},\mathbf{y}))

where the first inequality uses the standard Cauchy-Schwartz inequality together with the fact that logt\log_{t} is a decreasing function. It follows that sLogΓ,t(SLn/SLn1)𝒱SLn/SLn1\operatorname{sLog}_{\Gamma,t}(\operatorname{SL}_{n}/\operatorname{SL}_{n-1})\subseteq\mathcal{V}_{\operatorname{SL}_{n}/\operatorname{SL}_{n-1}}. It remains to show that 𝒱SLn/SLn1sLogΓ,t(SLn()/SLn1()))\mathcal{V}_{\operatorname{SL}_{n}/\operatorname{SL}_{n-1}}\subseteq\operatorname{sLog}_{\Gamma,t}(\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}))). Let (a,b)𝒱G/H(a,b)\in\mathcal{V}_{G/H}, i.e., (a,b)2(a,b)\in\mathbb{R}^{2} with a+b0a+b\leq 0. Then bab\leq-a, and, as xtxx\mapsto t^{x} is a strictly decreasing function for 0<t<10<t<1, we get that tbtat^{b}\geq t^{-a} or equivalently tbta0t^{b}-t^{-a}\geq 0. Hence y=tbta0y=\sqrt{t^{b}-t^{-a}}\in\mathbb{R}_{\geq 0} is defined. We set 𝐱=(ta/2,0,,0)\mathbf{x}=(t^{a/2},0,\ldots,0) and 𝐲=(ta/2,y,0,,0)\mathbf{y}=(t^{-a/2},y,0,\ldots,0) and observe that (𝐱,𝐲)SLn()/SLn1()(\mathbf{x},\mathbf{y})\in\operatorname{SL}_{n}(\mathbb{C})/\operatorname{SL}_{n-1}(\mathbb{C}). Finally, we may compute that

sLogΓ,t(𝐱,𝐲)=logt(|ta/2|2,|ta/2|2+|tbta|2)=(logt(ta),logt(ta+tbta))=(a,b)\operatorname{sLog}_{\Gamma,t}(\mathbf{x},\mathbf{y})=\log_{t}(|t^{a/2}|^{2},|t^{-a/2}|^{2}+|\sqrt{t^{b}-t^{-a}}|^{2})=(\log_{t}(t^{a}),\log_{t}(t^{-a}+t^{b}-t^{-a}))=(a,b)

so (a,b)sLogΓ,t(SL