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 bosonic oscillator (2).<br />
After simple calculation Hamiltonian can be presented as:<br />
HB = ωB(NB + 1<br />
2 ) = ωBNB + E0<br />
where E0 = 1<br />
2 �ωB is energy of the ground state (vacuum energy).<br />
Operators b † , b act on a state |nB >, <strong>and</strong> the energy spectrum of<br />
the hamiltonian is:<br />
EB = ωB(nB + 1<br />
2 )<br />
where nB = 0, 1, 2..., <strong>and</strong> nB are the eigenstates of the bosonic<br />
number operator.<br />
Anna Pachol GV,SUSY ans SHO
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