CASINO manual - Theory of Condensed Matter
CASINO manual - Theory of Condensed Matter
CASINO manual - Theory of Condensed Matter
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% SD - Single determinant inc. excitations/additions/subtractions<br />
Example:<br />
SD<br />
Single det calculation<br />
DET 1 1 PR 2 1 5 1 Promote electron in band 2 kpoint 1<br />
to band 5 kpoint 1 in determinant 1,<br />
spin 1 ("up")<br />
or<br />
DET 1 2 PL 6 1 Add electron spin 2 ("down") to det 1,<br />
band 6 kpoint 1<br />
or<br />
DET 1 2 MI 6 1<br />
Remove the added electron<br />
or<br />
% MD - Multiple determinants<br />
MD<br />
Multideterminant<br />
3 3 determinants<br />
1.d0 Determinant 1 prefactor<br />
2.d0 Determinant 2 prefactor<br />
-1.d0<br />
Determinant 3 prefactor<br />
DET 3 1 PR 2 1 5 1 Promotion as examples above<br />
ORBITAL COEFFICIENTS<br />
--------------------<br />
& CK(NUM_REAL_K*NUM_AO*NUM_AO + NUM_COMPLEX_K*NUM_AO*NUM_AO)<br />
block as follows<br />
----spin (spin-polarized calcs only)---------------------------------<br />
/ \<br />
----k (for solids)-------------------------------<br />
/ \<br />
----bands-(solids)_or MOs (molecules)------<br />
/ \<br />
-AO-basis functions grouped by shell-<br />
/ \<br />
Complex coefficients are given as 2 adjacent real numbers (real,imaginary).<br />
Ordering <strong>of</strong> d orbital coefficients;<br />
z2, xz, yz, x2-y2, xy<br />
Ordering <strong>of</strong> f,g,..: m=0,1,-1,2,-2,3,-3,4,-4.....<br />
OTHER STUFF<br />
-----------<br />
* Anything you like can be written here - intended for copy <strong>of</strong> input/output<br />
files from DFT/HF/etc. program.<br />
Note the potential issues with ‘normalizing’ contraction coefficients, e.g., with the crystal program<br />
the contraction coefficients are multiplied by that part <strong>of</strong> the normalization factor which is independent<br />
<strong>of</strong> m; the crystal output does not in fact contain the m-dependent part at all. This must be<br />
artificially multiplied into the orbital coefficients by the crystal to casino converter. Authors <strong>of</strong><br />
other interfaces must ensure this is done properly.<br />
A second issue is that for d functions only (not f or g), the scale factors <strong>of</strong> the real solid harmonics (e.g.,<br />
the 3 in 3xy) are not explicitly evaluated by the casino orbital evaluator, but must be pre-multiplied<br />
into the orbital coefficients. Again, the crystal to casino converter does this.<br />
The expressions for the real solid harmonics assumed by casino are given in the table on p. 170 <strong>of</strong><br />
Pisani, Dovesi and Roetti, Hartree-Fock ab initio treatment <strong>of</strong> crystalline systems (Springer-Verlag,<br />
78