"Characters of superconformal algebra and mock theta functions"의 두 판 사이의 차이

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* Yutaka Matsuo [http://ptp.ipap.jp/link?PTP/77/793/ Character Formula of C<1 Unitary representation of N=2 Superconformal Algebra] , Prog. Theor. Phys. Vol. 77 No. 4 (1987) pp. 793-797
 
* Yutaka Matsuo [http://ptp.ipap.jp/link?PTP/77/793/ Character Formula of C<1 Unitary representation of N=2 Superconformal Algebra] , Prog. Theor. Phys. Vol. 77 No. 4 (1987) pp. 793-797
 
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2020년 12월 28일 (월) 06:42 판

introduction

\(\mathcal{N}=4\) superconformal algebra

generators and relations

\[[L_m,L_n]=(m-n)L_{m+n}+\frac{c}{12}(m^3-m)\delta_{m+n}\]

\[[J_m^i,J_n^j]=\epsilon_{ijk}J_{m+n}^k+\delta_{m+n}\delta^{i,j}\frac{c}{3},\quad i,j,k\in \{1,2,3\},\quad m,n\in \mathbb{Z}\] \[[L_m,J_n^i]=-nJ_{m+n}^i,\quad m,n\in \mathbb{Z}\]

  • fermionic operators

\[ G_r^a,\overline{G}_s^b,\quad a,b\in \{1,2\} \]

\(c=6k\) with \(k=1\) case

  • non-BPS characters \[h>k/4,\ell=1/2\]

\[ \operatorname{ch}^{\tilde R}_{h=1/4+n,\ell=0}=q^{h-3/8}\frac{[\theta_{11}(z;\tau)]^2}{\eta^3}=q^{n-1/8}\frac{[\theta_{11}(z;\tau)]^2}{\eta^3} \]

  • BPS characters \[h=1/4,\ell=0,1/2\]

\[ \operatorname{ch}^{\tilde R}_{h=1/4,\ell=0}=\frac{[\theta_{11}(z;\tau)]^2}{\eta^3}\mu(z;\tau)\\ \operatorname{ch}^{\tilde R}_{h=1/4,\ell=1/2}+2\operatorname{ch}^{\tilde R}_{h=1/4,\ell=0}=q^{-1/8}\frac{[\theta_{11}(z;\tau)]^2}{\eta^3} \] where \(\mu(z;\tau)\) is the Appell-Lerch sums which is a holomorphic part of a mock modular form


\(k\geq 2\) case

  • this is related to Umbral moonshine and elliptic genus of hyperKahler manifolds of complex dimension \(2k\)




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