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 />
2. Harmonic fermionic oscillator.<br />
Fermionic creation-annihilation operators: f † , f obey the<br />
anticommutation relations:<br />
{f , f † } = 1; {f , f } = 0; {f † , f † } = 0<br />
Hamiltonian of the fermionic oscillator can be constructed by the<br />
analogy with the bosonic hamiltonian, as:<br />
HF = 1<br />
2 ωF [f † , f ] = 1<br />
2 ωF (f † f − ff † )<br />
Hamiltonian of the fermionic oscillator can be presented as:<br />
HF = ωF (NF − 1<br />
2 ) = ωF NF − E0<br />
where E0 = − 1<br />
2 �ωF is energy of the ground state (vacuum energy).<br />
Anna Pachol GV,SUSY ans SHO