<?xml version="1.0" encoding="utf-8"?><feed xmlns="http://www.w3.org/2005/Atom" ><generator uri="https://jekyllrb.com/" version="4.2.2">Jekyll</generator><link href="blog.randombeats.dev/feed.xml" rel="self" type="application/atom+xml" /><link href="blog.randombeats.dev/" rel="alternate" type="text/html" /><updated>2022-11-18T15:37:58+00:00</updated><id>blog.randombeats.dev/feed.xml</id><title type="html">random bits</title><entry><title type="html">sheaves of categories on manifolds are hypercomplete</title><link href="blog.randombeats.dev/2022/11/18/sheaves-on-manifolds-are-hypercomplete.html" rel="alternate" type="text/html" title="sheaves of categories on manifolds are hypercomplete" /><published>2022-11-18T00:00:00+00:00</published><updated>2022-11-18T00:00:00+00:00</updated><id>blog.randombeats.dev/2022/11/18/sheaves-on-manifolds-are-hypercomplete</id><content type="html" xml:base="blog.randombeats.dev/2022/11/18/sheaves-on-manifolds-are-hypercomplete.html"><![CDATA[<p>Consider $F\in\operatorname{Shv}(X, Pr^L)$, we show that $F$ is hypercomplete, i.e.,
it satisfies hyperdescent.</p>

<p>For any $Z \in Pr^L$, the assignment</p>

\[h_X(Z): U \mapsto \operatorname{map}(Z, F(U))\]

<p>is a sheaf of spaces because taking limit commutes with taking mapping spaces (in the second variable).</p>

<p>Note that sheaves of spaces on a manifold are hypercomplete, because it has finite homotopy dimension,
which in turn comes from the fact that it has finite covering dimension, see HTT 7.2.</p>

<p>Therefore, $h_X(Z)$ satifisfies hyperdescent. By Yoneda lemma, so does $F$.</p>

<p>Note that this argument carries actually to sheaves with coefficients in any $\infty$-category.
Thus the topos of sheaves of spaces is universal in this sense.</p>]]></content><author><name></name></author><summary type="html"><![CDATA[Consider $F\in\operatorname{Shv}(X, Pr^L)$, we show that $F$ is hypercomplete, i.e., it satisfies hyperdescent.]]></summary></entry><entry><title type="html">Abelian coulomb branches</title><link href="blog.randombeats.dev/2022/10/28/abelian-coulomb-branches.html" rel="alternate" type="text/html" title="Abelian coulomb branches" /><published>2022-10-28T00:00:00+00:00</published><updated>2022-10-28T00:00:00+00:00</updated><id>blog.randombeats.dev/2022/10/28/abelian-coulomb-branches</id><content type="html" xml:base="blog.randombeats.dev/2022/10/28/abelian-coulomb-branches.html"><![CDATA[\[\newcommand{\C}{\mathbb{C}}
\newcommand{\Gr}{\operatorname{Gr}}
\newcommand{\Kc}{\mathcal{K}}
\newcommand{\Oc}{\mathcal{O}}
\newcommand{\Rc}{\mathcal{R}}
\newcommand{\Tc}{\mathcal{T}}
\renewcommand{\Kc}{\mathcal{K}}
\newcommand{\sym}{\operatorname{Sym}}
\newcommand{\tf}{\mathfrak{t}}
\newcommand{\coker}{\operatorname{coker}}\]

<p>In <a href="https://arxiv.org/abs/1601.03586">arXiv:1601.03586</a>, coulomb branches are defined
when the matter representation $M=N\oplus N^*$ is of cotangent type.
Also computed is the coulomb branch when the gauge group is abelian.</p>

<p>The computation there is however extremely confusing to me,
largely due to the rather involved definition of convolution product
and their approach of exposition (and my incompetence of course!)</p>

<p>I will try to dot the i's and cross the t's.</p>

<p>For simplicity, assume our group is $G=T=\C^\times$, and the representation
$N = \C_\xi$ is given by a single character $\xi$.</p>

<p>A quick recap on the definition of $\Rc$.
Define $\Tc = G_\Kc\times_{G_\Oc}N_\Oc$
and consider the embedding $\Tc \hookrightarrow \Gr_G \times N_\Kc$
given by quotient on the first factor and multiplying on the second.
The variety of triples are then given by $\Rc := \Tc \cap \Gr_G \times N_\Oc$.</p>

<p>Recall that when $G$ is the torus $\C^\times$,
the affine grassmannian is just the coweight lattice $Y = \mathbb{Z}$.</p>

<p>We then have,</p>

\[\Rc = \coprod_\lambda \{\lambda\} \times (z^\lambda N_\Oc \cap N_\Oc).\]

<p>It follows that as a vector space,</p>

\[H_*^{G_\Oc}(\Rc) = \oplus_\lambda \C[\tf] r^\lambda.\]

<p>Here $r^\lambda$ is the fundamental class of the component corresponding to $\lambda$.</p>

<p>So in order to get the ring structure, it suffices to compute $r^\lambda r^\mu$.</p>

<p>Now we look at the following convolution diagram.</p>

\[\begin{CD}
\Rc \times \Rc @&lt;&lt;&lt; p^{-1}(\Rc\times\Rc) @&gt;&gt;&gt; q(p^{-1}(\Rc\times\Rc)) @&gt;&gt;&gt; \Rc \\
@VVV @VVV @VVV @VVV \\
\Tc \times \Rc @&lt;p = (p_\Tc, p_\Rc)&lt;&lt; G_\Kc \times \Rc @&gt;q&gt;&gt; G_\Kc \times_{G_\Oc} \Rc @&gt;m&gt;&gt; \Tc \\
\end{CD}\]

<p>The difficulty of analyzing this convolution product lies in the fact that
it is defined via the rather mysterious <code class="language-plaintext highlighter-rouge">restriction with support</code> morphism
giving a map $H_\bullet^{G_\Oc}(\Rc) \otimes H_\bullet^{G_\Oc}(\Rc) \rightarrow H_\bullet^{G_\Oc \times G_\Oc}(p^{-1}(\Rc\times\Rc))$
, which is the usual restriction unless everything is smooth.
Good news is everything is indeeed smooth in the abelian case.</p>

<p>Now identify $T_\Kc \times_{T_\Oc} \Rc$ with</p>

\[\coprod_{\lambda, \nu} \{\lambda\} \times \{\nu\} \times z^\lambda N_\Oc \cap z^\nu N_\Oc\]

<p>with the map given by $[g_1, [g_2, s]] \mapsto ([g_1], [g_1g_2], [g_1g_2s])$.</p>

<p>To calculate $r^\lambda r^\mu$ it is then enough to look at the component given by $(\lambda, \nu = \lambda + \mu)$.</p>

<p>Let's first have a look at the map $m$.
Under the identification
$\Tc = \coprod {\lambda} \times z^\lambda N_\Oc$,
it is simply given by the projection.</p>

\[\lambda \times \nu \times z^\lambda N_\Oc \cap z^\nu N_\Oc \rightarrow
\nu \times z^\nu N_\Oc\]

<p>The trick is to define a map
$p':T_\Kc \times_{T_\Oc} \Rc \rightarrow \Tc \times \Rc$
by sending $(\lambda,\nu,s)$ to $(\lambda, s, \nu - \lambda, z^{-\lambda}s)$.</p>

<p>It enjoys the property that $ p^\prime_{\Tc} q = p_\Tc, p^\prime_\Rc q a = p_\Rc $,</p>

<p>where $ a $ is an automorphism of $ T_\Kc\times \Rc $ inducing identity map
on the quotient $ T_\Kc\times_{T_\Oc} \Rc $.</p>

<p>Therefore, the convolution can be computed as</p>

\[r^\lambda r^\mu = m_*p'^*(r^\lambda \boxtimes r^\mu)
= m_* p'^*([z^\lambda N_\Oc \times (N_\Oc \cap z^\mu N_\Oc)]\]

<p>Recall that if $\iota: V \hookrightarrow X$ is a $T$-invariant
smooth closed subvariety, we have $\iota^\ast\iota_\ast([V]) = e(N_{V/X})[V]$
in equivariant (Borel-Moore/co-) homology.</p>

<p>Thus we have</p>

\[p'^*_\Tc([N_\Oc \cap z^\lambda N_\Oc])
= e(z^\lambda N_\Oc/N_\Oc\cap z^\lambda N_\Oc)
[z^\lambda N_\Oc \cap z^\nu N_\Oc],\]

\[p'^*_\Rc([N_\Oc \cap z^\mu N_\Oc])
= [z^\lambda N_\Oc \cap z^\nu N_\Oc]\]

<p>So</p>

\[p'^*([(N_\Oc \cap z^\lambda N_\Oc) \times (N_\Oc \cap z^\mu N_\Oc)])
= e(z^\lambda N_\Oc/N_\Oc\cap z^\lambda N_\Oc)[z^\lambda N_\Oc \cap z^\nu N_\Oc]\]

\[m_*p'^*([(N_\Oc \cap z^\lambda N_\Oc) \times (N_\Oc \cap z^\mu N_\Oc)])
=
e(z^\nu N_\Oc/z^\lambda N_\Oc\cap z^\nu N_\Oc)
e(z^\lambda N_\Oc/N_\Oc\cap z^\lambda N_\Oc)
[z^\nu N_\Oc]\]

<p>We know $r^\lambda r^\mu$ is supported on $R_{\nu}$,
so it suffices to divide by the normal bundle of $\Rc_\nu$ in $\Tc_\nu$
to get the coefficient.</p>

<p>Therefore,</p>

\[r^\lambda r^\mu
= m_*p'^*([(N_\Oc \cap z^\lambda N_\Oc) \times (N_\Oc \cap z^\mu N_\Oc)])
=
\frac
{
  e(z^\lambda N_\Oc/N_\Oc\cap z^\lambda N_\Oc)
  e(z^{\nu}N_\Oc/z^{\lambda}N_\Oc\cap z^\nu N_\Oc)
}
{
  e(z^\nu N_\Oc/z^\nu N_\Oc \cap N_\Oc)
}
r^{\lambda + \mu}.\]

<p>Counting dimensions case-by-case shows that the above is equal to</p>

\[r^\lambda r^\mu
=
\xi^{d(\langle\lambda,\xi\rangle, \langle\mu, \xi\rangle)}
r^{\lambda + \mu}.\]

<p>Here $d(k, l):=[kl &lt; 0]\min(\lvert k \rvert,\lvert l \rvert)$.</p>

<p>This computation generalizes trivially to higher-dimensional tori
and representations, giving</p>

\[r^\lambda r^\mu
=
\prod_i
\xi_i^{d(\langle\lambda,\xi_i\rangle, \langle\mu, \xi_i\rangle)}
r^{\lambda + \mu}\]

<p>if the representation $N$ is given by characters $\xi_i$.</p>]]></content><author><name></name></author><summary type="html"><![CDATA[\[\newcommand{\C}{\mathbb{C}} \newcommand{\Gr}{\operatorname{Gr}} \newcommand{\Kc}{\mathcal{K}} \newcommand{\Oc}{\mathcal{O}} \newcommand{\Rc}{\mathcal{R}} \newcommand{\Tc}{\mathcal{T}} \renewcommand{\Kc}{\mathcal{K}} \newcommand{\sym}{\operatorname{Sym}} \newcommand{\tf}{\mathfrak{t}} \newcommand{\coker}{\operatorname{coker}}\]]]></summary></entry><entry><title type="html">Weyl character formula is torus localization</title><link href="blog.randombeats.dev/2022/03/13/weyl-character.html" rel="alternate" type="text/html" title="Weyl character formula is torus localization" /><published>2022-03-13T00:00:00+00:00</published><updated>2022-03-13T00:00:00+00:00</updated><id>blog.randombeats.dev/2022/03/13/weyl-character</id><content type="html" xml:base="blog.randombeats.dev/2022/03/13/weyl-character.html"><![CDATA[<p>There is a geometric proof from [1] of the following celebrated <a href="https://en.wikipedia.org/wiki/Weyl_character_formula">Weyl character formula</a> that I find extremely exciting.</p>

\[\operatorname{ch}(V_\lambda) =
\frac
{
    \sum_{w\in W}(-1)^{\ell(w)} e^{w(\lambda + \rho)}
}
{
    \sum_{\alpha\in R^+}(e^{\alpha/2} - e^{-\alpha/2})
}\]

<p>It is the thing that for the first time convinced me we should care about flag varieties and their K-theories and cohomologies.</p>

<h2 id="k-theory">K-theory</h2>

<p>Let's start with some definitions. Given a rational character
$\lambda \in \hom(T,\mathbb{C}^\times)$,
we can define a line bundle $L_\lambda$ on the flag variety $\mathcal{B} = G/B$ by the formula $L_\lambda=G\times_B\mathbb{C}_\lambda$ where $B$ acts on $\mathbb{C}_\lambda$ by
$B \rightarrow B/[B,B] = T\xrightarrow{\lambda}\mathbb{C}^\times$.</p>

<p>Now assume $w_0(\lambda)$ is an anti-dominant weight, in which case $L_{w_0(\lambda)}$ is ample.
It turns out, by Borel-Weil-Bott, all higher cohomologies of $L_{w_0(\lambda)}$ vanish
and $\Gamma(\mathcal{B},{w_0(L_\lambda)})$ is the simple $G$-module with highest weight $w_0^2(\lambda)=\lambda$.</p>

<p>To make things easier, we introduce the geometric choice of positive roots
$R^+_{g} = w_0(R^+)$.
With this convention, $L_\lambda$ is ample if and only if $\lambda$ is dominant.</p>

<p>Under the above identifications, we can rewrite Weyl character formula in terms of $K$-theory as follows, where $p$ is the projection to a point.</p>

\[p_*L_{w_0(\lambda)} = \Delta^{-1}\sum_{w\in W}(-1)^{\ell(w)}e^{w(\lambda + \rho)}.\]

<p>Note that RHS is equal to
$ w_0(\Delta^{-1}) \sum_{w\in W} (-1)^{\ell(w)}e^{w(w_0\lambda + w_0\rho)}  $.
So it suffices to prove</p>

\[p_*L_\lambda = \Delta^{-1}\sum_{w\in W}(-1)^{\ell(w)}e^{w(\lambda + \rho)}\]

<p>, provided $\Delta$ and $\rho$  are defined using the geometric choice of positive roots, which we will assume from now on.</p>

<h2 id="torus-localization">Torus localization</h2>

<p>Now let's do torus localization. (finally!)</p>

<p>Let's fix a borel subalgebra $\mathfrak{b}$,
then the torus fixed $\mathcal{B}^T$ are nothing but the borel subalgebras containing $\operatorname{Lie}T$, and are given by $w(\mathfrak{b})$, indexed by the Weyl group.</p>

<p>Now by torus localization,</p>

\[[L_\lambda] = \sum_{w\in W}
\frac
{
    [L_\lambda|_{w(\mathfrak{b})}]
}
{
    \sum(-1)^i[\Lambda^iN^\vee_{w(\mathfrak{b})}\mathcal{B}]
}.\]

<p>Essentially by definition,
\(L_\lambda|_{w(\mathfrak{b})} = \mathbb{C}_{w(\lambda)}\).
On the other hand, a closer look at the of the flag variety shows that
$T_{w(\mathfrak{b})}\mathcal{B} \simeq \mathfrak{g}/w(\mathfrak{b})$.
So $N^\vee_{w(\mathfrak{b})}\mathcal{B}\simeq w(\mathfrak{n})$.
Recall that with the geometric choic of positive roots, $\mathfrak{n}$ are the negative weights.</p>

<p>Pushing-forward to a point, we have</p>

\[p_*[L_\lambda] = \sum_w
\frac
{
    [\mathbb{C}_{w(\lambda)}]
}
{
    \sum (-1)^i[\Lambda ^i w(\mathfrak n)]
}
=
\sum_w
\frac
{
    e^w(\lambda)
}
{
    \prod_{\alpha\in R^+} (1 - e^{-w(\alpha)})
}.\]

<p>Note that we have the following identity,</p>

\[\prod_{\alpha \in R^+}(1 - e^{-w(\alpha)})=e^{-w(\rho)}w(\Delta)=e^{-w(\rho)}(-1)^{\ell(w)}\Delta.\]

<p>Putting this back we get the Weyl character formula. Voila!</p>

<h2 id="references">references</h2>

<p>[1] Chriss, Neil, and Victor Ginzburg. Representation theory and complex geometry. Vol. 42. Boston: Birkhäuser, 1997.</p>]]></content><author><name></name></author><summary type="html"><![CDATA[There is a geometric proof from [1] of the following celebrated Weyl character formula that I find extremely exciting.]]></summary></entry></feed>