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Grassmann Variables, Supersymmetry and Supersymmetric ...

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Fermionic Path Integral<br />

SUSY<br />

References<br />

The end<br />

<strong>Grassmann</strong> <strong>Variables</strong><br />

Path Integral<br />

One missing step - transformation of measure<br />

when we do transformation of variables:<br />

η ′ i = Uijηj<br />

the product of new (grassmann) variables is following:<br />

n�<br />

i=1<br />

η ′ i = 1<br />

n! ɛij...lη ′ iη ′ j...η ′ l = 1<br />

n! ɛij...lUii ′ηi ′Ujj ′ηj ′...Ull ′ηl ′ =<br />

= 1<br />

n! ɛij...lUii ′Ujj ′...Ull ′ηi ′ηj ′...ηl ′<br />

Anna Pachol GV,SUSY ans SHO

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