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Molecular Dynamics Chapter 2. Molecular Dynamics in Various ...

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<strong>Molecular</strong> <strong>Dynamics</strong> <strong>Chapter</strong> <strong>2.</strong>1<br />

Extended Hamiltonian to Realize Grand Canonical Ensemble<br />

Adiabatic switch<strong>in</strong>g method: Extended Hamiltonian Hybrid Monte Carlo<br />

H<br />

extended<br />

1 dsr<br />

= H<br />

o<br />

( n −1)<br />

+ M<br />

r<br />

+ sr<br />

( U<br />

o<br />

− μ ) + μ<br />

2 dt<br />

2<br />

1. When Sr = 0 or 1, at a pre-set time <strong>in</strong>terval N*τ, fix<strong>in</strong>g the position<br />

of the ghost particle.<br />

<strong>2.</strong> Adiabatically switch Sr from 0 to 1 or switch Sr from 1 to 0, the<br />

energy change will be E − or E −<br />

n−1<br />

E n<br />

n+1<br />

E n<br />

ρ<br />

ρ<br />

accp<br />

accp<br />

=<br />

−<br />

m<strong>in</strong>( 1,exp( −β<br />

( En<br />

1<br />

+ u − En))<br />

=<br />

+<br />

m<strong>in</strong>( 1,exp( −β<br />

( En<br />

1<br />

− u − En))

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