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