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qp2/src/non_h_ints_mu
Anthony Scemama 145e18f394
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continuous-integration/drone/push Build is failing
Fixed openmp bug
2023-09-26 18:39:13 +02:00
..
debug_fit.irp.f num integ grad & grad squared 2023-09-05 11:52:08 +02:00
debug_integ_jmu_modif.irp.f added keywords for r1 grid 2023-07-02 21:49:25 +02:00
grad_squared_manu.irp.f numerical integrals: 1 shot --> blocks over r2 2023-09-04 22:27:18 +02:00
grad_squared.irp.f numerical integrals: 1 shot --> blocks over r2 2023-09-04 22:27:18 +02:00
grad_tc_int.irp.f v0 tc integ numericall with DGEMM 2023-04-21 20:50:00 +02:00
j12_nucl_utils.irp.f DUMP for TCHint added 2023-06-28 18:57:41 +02:00
jast_deriv_utils_vect.irp.f num integ grad & grad squared 2023-09-05 11:52:08 +02:00
jast_deriv_utils.irp.f num integ grad & grad squared 2023-09-05 11:52:08 +02:00
jast_deriv.irp.f Add many call provide in TC 2023-09-22 16:26:58 +02:00
NEED Added Jastrow parameters in EZFIO 2023-09-19 15:26:50 +02:00
new_grad_tc_manu.irp.f v0 tc integ numericall with DGEMM 2023-04-21 20:50:00 +02:00
new_grad_tc.irp.f numerical integrals: 1 shot --> blocks over r2 2023-09-04 22:27:18 +02:00
numerical_integ.irp.f v0 tc integ numericall with DGEMM 2023-04-21 20:50:00 +02:00
plot_mu_of_r.irp.f added plot_mu_of_r.irp.f 2023-05-25 12:57:58 +02:00
qmckl.irp.f Fixed openmp bug 2023-09-26 18:39:13 +02:00
README.rst non_h_ints compiles 2023-02-06 19:00:35 +01:00
tc_integ_an.irp.f J_qmckl en & ee 2023-09-15 11:30:10 +02:00
tc_integ_num.irp.f normal order V2 FROZEN CORE 2023-09-06 19:52:53 +02:00
test_non_h_ints.irp.f num integ grad & grad squared 2023-09-05 11:52:08 +02:00
total_tc_int.irp.f normal order V2 FROZEN CORE 2023-09-06 19:52:53 +02:00

=============
non_h_ints_mu
=============

Computes the non hermitian potential of the mu-TC Hamiltonian on the AO and BI-ORTHO MO basis.
The operator is defined in Eq. 33 of JCP 154, 084119 (2021)

The two providers are :
+) ao_non_hermit_term_chemist which returns the non hermitian part of the two-electron TC Hamiltonian on the MO basis. 
+) mo_non_hermit_term_chemist which returns the non hermitian part of the two-electron TC Hamiltonian on the BI-ORTHO MO basis.