This option works similarly to the previous one, V2, although the initial part is very different. At the beginning, all the necessary files (including forces) are read in. The data must be available for all representation, otherwise, you cannot proceed. Once everything is read in, the following V3-menu appears:
>>>>>>>>>>>>>>>>>>>>>>>>><<<<<<<<<<<<<<<<<<<<<<<<<<<
MOLECULE: lattice translations IGNORED
========= CHOOSE an OPTION:
Am. Change atomic masses for a range of atoms
--- A c t i o n s w i t h v i b r a t i o n s -----
Ei. Solve the eigenvalue problem
------------ p h o n o n D O S ---------
pD. Choose atoms for projected phonon DOS
------- G e n e r a l I n f o r m a t i o n ------
Co. Show information about atoms
Sy. Show the point symmetry group info
-------- G e n e r a l S e t t i n g s --------
XY. Format of <movie.xyz> file is for Xmol
Hs. H atoms to be added to <movie.xyz> file: NO
Da. Distortion amplitude for movies: 0.05000
Nd. Number of dispersions: 1
Sg. Dispersion for DOS (cm-1): 10.00000
St. Step for DOS (cm-1): 0.10000
Up. Upper limit for DOS: not set
W. Write <geom.xyz> file to preview current geometry
Q. Proceed/Quit
-----> Choose an appropriate option:
At this point the FCM in the Cartesian representation, is available via Eq. (2.10). Change masses2.3 in Am (symmetry is not used, therefore, division of atoms into orbits is irrelevant here), and then solve the eigenproblem in Ei. After you are done, the natural logarithm of the product of all real nonzero frequencies will be shown just under Ei. This is useful for the calculation of the transition rates prefactors. Also, three new options appear just under ``Actions with vibrations'':
Am. Change atomic masses for a range of atoms
--- A c t i o n s w i t h v i b r a t i o n s -----
Ei. Solve the eigenvalue problem <= Done!
Nat. logarithm of product of frequencies = 170.087612
Sv. Show eigenvalues/vectors
Sa. Show frequencies and normal modes
Vs. Write xyz movie file for a mode
These are similar to those of the V2-menu:
If a set of atoms is chosen via pD, the phonon DOS projected on these atoms can be previewed using D2. In this case only a single dispersion (the first one if there are many) will be used.
Some other miscellaneous options controlling DOS: