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Grassmann Variables, Supersymmetry and Supersymmetric ...

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Fermionic Path Integral<br />

SUSY<br />

References<br />

The end<br />

Basic idea of <strong>Supersymmetry</strong><br />

<strong>Supersymmetry</strong><br />

<strong>Supersymmetric</strong> harmonic oscillator<br />

Hilbert space contain Fermionic <strong>and</strong> Bosonic Hilbert spaces:<br />

H = HB ⊕ HF<br />

Coordinates space : (xµ, θµ) <strong>and</strong> Momentum space : (pα, ηα)<br />

where xµ <strong>and</strong> pα are bosonic variables i.e. commuting :<br />

[xµ, xν] = 0; [pα, pβ] = 0<br />

<strong>and</strong> θµ, ηα are fermionic variables i.e. anticommuting (grassmanian<br />

numbers) : {θµ, θν} = 0; {ηµ, ην} = 0<br />

Anna Pachol GV,SUSY ans SHO

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