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| quickstart [2025/10/13 16:25] – [Simple input] werner | quickstart [2025/10/14 08:54] (current) – [Simple input] werner | ||
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| - | where avtz is a short name for the aug-cc-pVTZ basis. The prefix DF- turns on density fitting approximations for the integrals, which is strongly recommended for efficiency, in particular for larger molecules. | + | where avtz is a short name for the aug-cc-pVTZ basis, and |
| + | the geometry is provided in an external file holding the x,y,z coordinates in Angstrom. Alternatively, | ||
| + | |||
| + | The prefix DF- turns on density fitting approximations for the integrals, which is strongly recommended for efficiency, in particular for larger molecules. | ||
| A most simple example for a CCSD(T) input is: | A most simple example for a CCSD(T) input is: | ||
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| '' | '' | ||
| - | where the geometry is provided in an external file holding the x,y,z coordinates in Angstrom. Alternatively, | ||
| The entries can come in any order, for example | The entries can come in any order, for example | ||
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| PNO methods are density fitted in any case. | PNO methods are density fitted in any case. | ||
| - | For most listed correlation methods, explicitly correlated versions are available by appending -F12 to the command [e.g. ccsd(t)-f12, | + | For most listed correlation methods, explicitly correlated versions are available by appending -F12 to the command [e.g. ccsd(t)-f12, |
| Method, geometry, and basis set are compulsory for running a calculation. By default, only a single energy calculation is done. However, other calculation types can be requested by specifying one of the following directives (the parts in brackets can be omitted or are optional): | Method, geometry, and basis set are compulsory for running a calculation. By default, only a single energy calculation is done. However, other calculation types can be requested by specifying one of the following directives (the parts in brackets can be omitted or are optional): | ||
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| This computes the ground state and 4 excited states for each of the four IRREPS of C2v. | This computes the ground state and 4 excited states for each of the four IRREPS of C2v. | ||
| + | 8.)CASSCF calculation using state-averaging over three state symmetries: | ||
| + | '' | ||
| + | |||
| + | This carries out a state-averaged CASSCF calculation for symmetries 2,3,1 ($^2\Pi_x$, | ||
| + | |||
| + | 9. )MRCI calculation using state-averaged CASSCF reference functions: | ||
| + | |||
| + | '' | ||
| + | |||
| + | In this case first a state-averaged CASSCF calculation for symmetries 2,3,1 ($^2\Pi_x$, | ||
| + | |||
| + | |||
| + | 10.) Several run command lines can follow each other. For example, compute the lowest ionisation potential of H2O using MRCI: | ||
| + | |||
| + | < | ||
| + | run mrci basis=vtz geometry=h2o.xyz | ||
| + | eci=energy | ||
| + | eda=energd | ||
| + | run mrci charge=1 wfsym=3 spin=1 | ||
| + | ipci=(energy-eci)*toev | ||
| + | ipda=(energd-eda)*toev | ||
| + | </ | ||
| + | |||
| + | 11.) It is also possible to combine the run command with other standard molpro input, for example: | ||
| + | |||
| + | < | ||
| + | geometry={O; | ||
| + | H1,O,R; | ||
| + | H2, | ||
| + | basis=vtz | ||
| + | R=0.96 Ang | ||
| + | Theta=104 | ||
| + | |||
| + | run mp2 optg | ||
| + | mp4 !do single-point MP4 at MP2 geometry | ||
| + | ccsd(t) | ||
| + | </ | ||
| The following sections give more basic information about carrying electronic structure calculations with Molpro. | The following sections give more basic information about carrying electronic structure calculations with Molpro. | ||