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

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

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

Harmonic fermionic oscillator (2).<br />

Operators f † , f act on a state |nF >, <strong>and</strong> the energy spectrum of<br />

the fermionic oscillator can be calculated using of the<br />

anticommutation relations:<br />

EF = ωF (nF − 1<br />

2 )<br />

where nF = 0, 1 (Pauli principle, due to {f † , f † } = 0 there exist<br />

only vacuum state |0 > <strong>and</strong> |1 >= f † |0 >, because (f † ) 2 = 0 ),<br />

<strong>and</strong> nF are the eigenvalues of the fermionic number operator<br />

NF = f † f .<br />

And fermionic harmonic oscillator is built only from two states |0 ><br />

<strong>and</strong> |1 > with energy E0 = − 1<br />

2 �ωF <strong>and</strong> E1 = 1<br />

2 �ωF<br />

Anna Pachol GV,SUSY ans SHO

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