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 />
1. Harmonic bosonic oscillator.<br />
Hamiltonian:HB = 1<br />
2p2 + 1<br />
2ω2 Bq2 where p <strong>and</strong> q are the<br />
momentum <strong>and</strong> coordinate operators respectively <strong>and</strong> [p, q] = 1<br />
Hamiltonian can be presented in terms of bosonic<br />
creation-annihilation operators: b † , b, as follows:<br />
HB = 1<br />
2 ωB{b † , b} = 1<br />
2 ωB(b † b + bb † )<br />
where � = 1; m = 1; b = 1<br />
√ 2ωB (ip + ωBq) <strong>and</strong><br />
[b, b † ] = 1; [b, b] = 0; [b † , b † ] = 0; [NB, b] = −b; [NB, b † ] = b †<br />
<strong>and</strong> NB = b † b is bosonic number operator.<br />
Anna Pachol GV,SUSY ans SHO