|
energies_cas.irp.f
|
Good Dyall Hamiltonian
|
2016-09-07 14:49:52 +02:00 |
|
excitations_cas.irp.f
|
Phase problem fixed
|
2016-09-20 12:04:48 +02:00 |
|
fock_like_operators.irp.f
|
corrected bugs in fock for MRPT
|
2016-09-08 15:48:52 +02:00 |
|
H_apply.irp.f
|
MRPT2 new with separated classes
|
2016-08-30 18:10:44 +02:00 |
|
mrpt_dress.irp.f
|
Beginning new way for computing pt2
|
2016-09-10 12:32:33 +02:00 |
|
mrpt_utils.irp.f
|
corrected bugs in fock for MRPT
|
2016-09-08 15:48:52 +02:00 |
|
MRPT_Utils.main.irp.f
|
Good Dyall Hamiltonian
|
2016-09-07 14:49:52 +02:00 |
|
new_way.irp.f
|
new way works for the 1h2p
|
2016-09-11 13:13:46 +02:00 |
|
print_1h2p.irp.f
|
second order ok for 2h1p
|
2016-09-18 20:53:28 +02:00 |
|
psi_active_prov.irp.f
|
new way works for the 1h2p
|
2016-09-11 13:13:46 +02:00 |
|
second_order_new_2p.irp.f
|
second order works for 2p
|
2016-09-19 18:06:34 +02:00 |
|
second_order_new.irp.f
|
second order works for 2p
|
2016-09-19 18:06:34 +02:00 |
