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Brodsky, Electron in a transverse harmonic cavity,’ Phys. Rev. Lett. 106, 061603 (2011). [8] J. P. Vary, Non-Perturbative Hamiltonian Light-Front Field Theory: Progress and Prospects, Proceedings of Science, PoS(LC2010)001 (available online). [9] J. P. 1071. [10] X. Zhao, H. Honkanen, P. Maris, J. P. Vary and S. J. 0553. [11] P. Navrátil, J. P. Vary and B. R. Barrett, Properties of 12-C in the ab-initio Nuclear Shell Model, Phys. Rev. Lett. 84 (2000) 5728; Large-basis ab-initio No-core Shell Model and its application to 12-C, Phys.

The cutoffs for the basis space dimensions are selected such that K increases simultaneously with the Nmax . half-integer total K, we will quote K values rounded downwards for convenience, except when the precise value is required. In our approach, the HO parameters Ω, M0 , the electron mass me , and the total longitudinal momentum K appear as prefactors for the matrix elements in the Hamiltonian. Therefore, we can rather straightforwardly vary the size of the Hamiltonian matrix by keeping Nmax fixed, and changing K alone.

Vary and A. M. Shirokov, Ab Initio no-core full configuration calculations of light nuclei, Phys. Rev. C. 3420]. [13] A. C. Hayes, P. Navrátil and J. P. Vary, Neutrino-12C Scattering in the ab initio Shell Model with a Realistic Three-Body Interaction Phys. Rev. Lett. 91, 012502 (2003); nucl-th/0305072. [14] A. M. Shirokov, J. P. Vary, A. I. Mazur and T. A. Weber, Realistic Nuclear Hamiltonian: Ab exitu approach, Phys. Letts. B 644 (2007) 33 [nucl-th/0512105]. [15] P. Navratil, V. G. Gueorguiev, J.

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