Emmanuel Giner c6b7acbc4e definitive version for the second order of 1h2p and 2h1p		2016-09-19 13:38:37 +02:00
..
energies_cas.irp.f	Good Dyall Hamiltonian	2016-09-07 14:49:52 +02:00
excitations_cas.irp.f	merging with new way	2016-09-10 17:00:34 +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_second_order_coef.irp.f	second order for 1h2p with mono excitations	2016-09-18 19:46:13 +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.irp.f	definitive version for the second order of 1h2p and 2h1p	2016-09-19 13:38:37 +02:00
utils_bitmask.irp.f	Formally finished to code the MRPT_Utils	2016-08-24 16:43:01 +02:00