Type BC residue expansion identity

Fix k1k\geq 1 and c(0,)c\in(0,\infty). Let α1,,αk\alpha_1,\ldots,\alpha_k be real numbers and let F(z1,,zk)F(z_1,\ldots,z_k) satisfy αk=0\alpha_k=0, αj>αj+1+c\alpha_j>\alpha_{j+1}+c for 1jk11\leq j\leq k-1, and the stated analyticity and decay condition in each variable. For a partition λ=1m12m2k\lambda=1^{m_1}2^{m_2}\cdots\vdash k, let (λ)\ell(\lambda) denote its length, let (a)n(a)_n denote the rising factorial, and define

(u1,,u2(λ))=(w1+c2,w1c2+λ1c,,w(λ)+c2,w(λ)c2+λ(λ)c).(u_1,\ldots,u_{2\ell(\lambda)})=\big(-w_1+\tfrac{c}{2},w_1-\tfrac{c}{2}+\lambda_1c,\ldots,-w_{\ell(\lambda)}+\tfrac{c}{2},w_{\ell(\lambda)}-\tfrac{c}{2}+\lambda_{\ell(\lambda)}c\big).

Also define EcE^c by symmetrization over the hyperoctahedral group BCkBC_k as in the displayed formula below. Type BCBC residue expansion conjecture. The following identity should hold:

α1iα1+idz12πiαkiαk+idzk2πi1A<BkzAzBzAzBczA+zBzA+zBcF(z)=ckλkλ=1m12m2(1)(λ)m1!m2!αkiαk+idw12πiαkiαk+idw(λ)2πi×j=1(λ)14c(2wj+c2c)λj1(2wj2c)λjPf[uiujui+uj]i,j=12(λ)Ec(w1,w1+c,,w(λ)+c(λ(λ)1)).\begin{aligned} &\int_{\alpha_1-\mathbf{i}\infty}^{\alpha_1+\mathbf{i}\infty}\frac{dz_1}{2\pi\mathbf{i}}\cdots\int_{\alpha_k-\mathbf{i}\infty}^{\alpha_k+\mathbf{i}\infty}\frac{dz_k}{2\pi\mathbf{i}}\prod_{1\leq A<B\leq k}\frac{z_A-z_B}{z_A-z_B-c}\frac{z_A+z_B}{z_A+z_B-c}F(\vec z)\\ &=c^k\sum_{\substack{\lambda\vdash k\lambda=1^{m_1}2^{m_2}\cdots}}\frac{(-1)^{\ell(\lambda)}}{m_1!m_2!\cdots}\int_{\alpha_k-\mathbf{i}\infty}^{\alpha_k+\mathbf{i}\infty}\frac{dw_1}{2\pi\mathbf{i}}\cdots\int_{\alpha_k-\mathbf{i}\infty}^{\alpha_k+\mathbf{i}\infty}\frac{dw_{\ell(\lambda)}}{2\pi\mathbf{i}}\\ &\qquad\times\prod_{j=1}^{\ell(\lambda)}\frac{1}{4c}\frac{\left(\frac{2w_j+c}{2c}\right)_{\lambda_j-1}}{\left(\frac{2w_j}{2c}\right)_{\lambda_j}}\operatorname{Pf}\left[\frac{u_i-u_j}{u_i+u_j}\right]_{i,j=1}^{2\ell(\lambda)}E^c(w_1,w_1+c,\ldots,w_{\ell(\lambda)}+c(\lambda_{\ell(\lambda)}-1)). \end{aligned}

Here

Ec(z1,,zk)=σBCk1B<Akzσ(A)zσ(B)czσ(A)zσ(B)zσ(A)+zσ(B)czσ(A)+zσ(B)F(σ(z)).E^c(z_1,\ldots,z_k)=\sum_{\sigma\in BC_k}\prod_{1\leq B<A\leq k}\frac{z_{\sigma(A)}-z_{\sigma(B)}-c}{z_{\sigma(A)}-z_{\sigma(B)}}\frac{z_{\sigma(A)}+z_{\sigma(B)}-c}{z_{\sigma(A)}+z_{\sigma(B)}}F(\sigma(\vec z)).

The result would provide the type BCkBC_k analogue of the preceding residue expansion and is intended for the half-space polymer application. The authors state that they have a complete proof modulo a cancellation claim concerning residues generated by contour deformations; partial evidence for that claim is established in the one-string case.

Sources & referencesView supporting material

Primary source

Alexei Borodin, Alexey Bufetov and Ivan Corwin, “Directed random polymers via nested contour integrals”, arXiv:1511.07324 (2015).

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