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← Introduction to Vertex Operator Algebras Paper detailsSnapshot 261030.6b9c1cee3c0f
Introduction to Vertex Operator Algebras
Accepted 30 Oct 2026, 11:29 UTC
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- Snapshot 261030.6b9c1cee3c0f — Use wedge. And move properties out from definition
Section PR · Clifford modes and the vacuum space. This snapshot contains the complete paper.
Use wedge. And move properties out from definition
- Submission hash
6b9c1cee3c0f660f8d2936ab22cc0e7fa0e0084cd3ad4b322467a3a34a6a7114- Base version
261030.3c6c6609ead5
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Vertex operator superalgebras
--- Base version+++ Proposed version@@ -197,7 +197,7 @@ Let $$-F=\Lambda(\xi_0,\xi_1,\xi_2,\ldots),\qquad \mathbf1=1,+F=\bigwedge(\xi_0,\xi_1,\xi_2,\ldots),\qquad \mathbf1=1, $$ where all generators $\xi_n$ are odd and each state is a finite linear combination of exterior monomials. Define odd operators, for $n\geq0$, by@@ -208,6 +208,8 @@ \psi_{n+\frac12}=\frac{\partial}{\partial\xi_n}. $$ +:::+ The derivative is the left exterior derivative: removing the $i$th factor of a monomial contributes the sign $(-1)^{i-1}$. Thus $$@@ -221,7 +223,6 @@ $$ \psi(z)=\sum_{r\in\mathbb Z+\frac12}\psi_rz^{-r-\frac12}. $$-::: The half-integer labels are the usual Neveu–Schwarz mode convention. The field still has integer powers of $z$: in vertex-algebra notation, $\psi_{(n)}=\psi_{n+\frac12}$. Its creation part consists of $r<0$ and its annihilation part of $r>0$.
Accepted by ChenqiMeng on 30 Oct 2026, 11:29 UTC. The submitted snapshot is preserved.
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