Grassmann Variables, Supersymmetry and Supersymmetric ...
Grassmann Variables, Supersymmetry and Supersymmetric ...
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