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量子場論
配分函數成為泛函積分:
Z = ∫ D ϕ exp ( i S ( ϕ ) ) {\displaystyle Z=\int D\phi \ \exp(iS(\phi ))} {\displaystyle Z=\int D\phi \ \exp(iS(\phi ))}
費米子路徑積分
費米積分、格拉斯曼數