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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 />

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

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