14.09.2014 Views

CASINO manual - Theory of Condensed Matter

CASINO manual - Theory of Condensed Matter

CASINO manual - Theory of Condensed Matter

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

% 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

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!