[CPMD-list] about vibrational analysis
Yong Zhang
zhangymall11 at gmail.com
Mon Nov 13 20:41:40 CET 2006
Hi CPMDers,
I have a question about vibrational analysis in cpmd.
My system is one N-methylacetamide molecule (with N-H deuterated to N-D) in
vacuum. The situation is like this: I generated a trajectory (10ps)
following general procedure (with Nose Hoover thermostat at 300K); then 80
snapshots were taken from this traj (one every 100fs for the 8ps); for each
of these snapshots, a wavefunction ompimization was carried out, and based
on this optimized wavefunction (by "restart wavefunction..."), the freq was
calculated using FD method; Then I checked the C=O stretching frequency (so
called amide I mode). Surprisingly, the freq has a distribution over the
range as wide as 400cm-1 (1500cm-1 ~ 1900cm-1). The experimental observation
of this mode in gas phase is 1717cm-1. I did the similar calculation using
charmm force field, the freq distribution is much narrower (1685+/-15 cm-1),
which is more reasonable under harmonic approximation. So my question is,
why the freq dirtribution in CPMD calaulation is so wide?
If quench the snapshots to a minimized structure and do the freq ana, their
freq are close to each other, which might indicate a "single" local minimum.
I also tried LR for freq calculation, the resultant freq is about 10cm-1
lower than the corresponding FD one for all cases; I also tried BO dynamics,
similar results.
Any comments or suggestions are appreciated.
Best wishes
Yong
The input file for dynamics run:
==================
&CPMD
MOLECULAR DYNAMICS CP
RESTART WAVEFUNCTION COORDINATES VELOCITIES ACCUMULATORS LATEST
TEMPERATURE
300.0
NOSE IONS MASSIVE
300.0 1700.0
NOSE ELECTRONS
0.002 10000.0
TIMESTEP
4.0
MAXSTEP
10000
EMASS
500.0
TRAJECTORY XYZ SAMPLE
5
DIPOLE DYNAMICS SAMPLE WANNIER
10
WANNIER REFERENCE
0.0 0.0 0.0
&END
&SYSTEM
ANGSTROM
SYMMETRY
1
CELL
12.14 1.0 1.0 0 0 0
CUTOFF
70.0
&END
&DFT
NEWCODE
FUNCTIONAL PBE
GC-CUTOFF
5.0e-6
&END
&ATOMS
ISOTOPE
1.0
2.0
12.0
14.0
16.0
*H_MT_PBE.psp KLEINMAN-BYLANDER
LMAX=S
6
1.69080 .05583 .88430
3.28199 -.14332 .06344
2.16794 -1.45255 .00207
-1.58359 .17630 -2.35128
-.19701 .20889 -3.48962
-.49100 1.60271 -2.37391
*H_MT_PBE.psp KLEINMAN-BYLANDER
LMAX=S
1
-.22859 -.88824 -.93883
*C_MT_PBE.psp KLEINMAN-BYLANDER
LMAX=P
3
2.18368 -.34882 .01350
1.56123 .24388 -1.15711
-.53752 .48601 -2.44731
*N_MT_PBE.psp KLEINMAN-BYLANDER
LMAX=P
1
.32592 -.14815 -1.44467
*O_MT_PBE.psp KLEINMAN-BYLANDER
LMAX=P
1
2.16429 1.09559 -1.77796
&END
======================
input file for vib ana:
=====================
&CPMD
VIBRATIONAL ANALYSIS FD GAUSS SAMPLE
2
RESTART WAVEFUNCTION COORDINATES LATEST
&END
&SYSTEM
ANGSTROM
SYMMETRY
1
CELL
12.14 1.0 1.0 0 0 0
CUTOFF
70.0
&END
&DFT
NEWCODE
FUNCTIONAL PBE
GC-CUTOFF
5.0e-6
&END
&ATOMS
ISOTOPE
1.0
2.0
12.0
14.0
16.0
*H_MT_PBE.psp KLEINMAN-BYLANDER
LMAX=S
6
1.69080 .05583 .88430
3.28199 -.14332 .06344
2.16794 -1.45255 .00207
-1.58359 .17630 -2.35128
-.19701 .20889 -3.48962
-.49100 1.60271 -2.37391
*H_MT_PBE.psp KLEINMAN-BYLANDER
LMAX=S
1
-.22859 -.88824 -.93883
*C_MT_PBE.psp KLEINMAN-BYLANDER
LMAX=P
3
2.18368 -.34882 .01350
1.56123 .24388 -1.15711
-.53752 .48601 -2.44731
*N_MT_PBE.psp KLEINMAN-BYLANDER
LMAX=P
1
.32592 -.14815 -1.44467
*O_MT_PBE.psp KLEINMAN-BYLANDER
LMAX=P
1
2.16429 1.09559 -1.77796
&END
======================
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