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Phys. Rev. A 80, 022507 (2009) [11 pages]

Direct calculation of excited-state electronic energies and two-electron reduced density matrices from the anti-Hermitian contracted Schrödinger equation

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Gergely Gidofalvi1,2 and David A. Mazziotti1,*
1Department of Chemistry and The James Franck Institute, The University of Chicago, Chicago, Illinois 60637, USA
2Chemical Sciences and Engineering Division, Argonne National Laboratory, Argonne, Illinois 60439, USA

Received 27 May 2009; published 14 August 2009

Direct calculation of the ground-state two-electron reduced density matrix (2-RDM) and its energy has recently been achieved for many-electron atoms and molecules by solving the anti-Hermitian part of the contracted Schrödinger equation (ACSE) [ D. A. Mazziotti Phys. Rev. Lett. 97 143002 (2006)]. In this paper the ACSE method is extended to computing the 2-RDMs and energies of excited states without the many-electron wave function. The contracted Schrödinger equation (CSE) is an important ingredient for excited-state 2-RDM methods because it is a stationary-state condition for both ground and excited states. We develop the theoretical framework for the ACSE as a stationary-state condition through its connections to the CSE and the Schrödinger equation. As in previous ground-state calculations, the indeterminacy of the ACSE is removed by reconstructing its 3-RDM as a functional of its 2-RDM through a cumulant theory for RDMs [ D. A. Mazziotti Chem. Phys. Lett. 289 419 (1998)]. We calculate the initial 2-RDM from a multiconfiguration self-consistent-field calculation that includes multireference electron correlation, which can be especially important for excited states. The excited-state ACSE method is applied to computing absolute excited-state energies and vertical excitation energies of the molecules HF, H2O, and N2 as well as ground and excited potential-energy curves of HF. Comparisons are made to traditional multireference methods as well as full configuration interaction. Computed excited-state 2-RDMs nearly satisfy necessary N-representability conditions.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevA.80.022507
DOI:
10.1103/PhysRevA.80.022507
PACS:
31.10.+z

*damazz@uchicago.edu