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000050276 0247_ $$2DOI$$a10.1016/j.nuclphysa.2005.08.024
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000050276 0247_ $$2arXiv$$aarXiv:nucl-th/0504043$$cnucl-th
000050276 0247_ $$2arXiv$$aarXiv:oai:arXiv.org:nucl-th/0504043
000050276 0247_ $$2Handle$$a2128/10631
000050276 035__ $$9arXiv$$anucl-th/0504043$$cnucl-th
000050276 035__ $$9arXiv$$aoai:arXiv.org:nucl-th/0504043$$zoai:arXiv.org:nucl-th/0504043
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000050276 084__ $$2WoS$$aPhysics, Nuclear
000050276 1001_ $$0P:(DE-HGF)0$$aBogner, S. K.$$b0
000050276 245__ $$aIs nuclear matter perturbative with low-momentum interactions?
000050276 260__ $$aAmsterdam$$bNorth-Holland Publ. Co.$$c2005
000050276 300__ $$a59
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000050276 440_0 $$04646$$aNuclear Physics A$$v763$$x0375-9474
000050276 500__ $$aRecord converted from VDB: 12.11.2012
000050276 500__ $$9arXiv$$a24 pages, 7 figures, references and attractive c4 contribution added, figures updated, conclusions unchanged: minor additions, to appear in Nucl. Phys. A Subj-class: Nuclear Theory: Other
000050276 520__ $$aThe nonperturbative nature of inter-nucleon interactions is explored by varying the momentum cutoff of a two-nucleon potential. Conventional force models, which have large cutoffs, are nonperturbative because of strong short-range repulsion, the iterated tensor interaction, and the presence of bound or nearly-bound states. But for low-momentum interactions with cutoffs around 2 fm(-1), the softened potential combined with Pauli blocking leads to corrections in nuclear matter in the particle-particle channel that are well converged at second order in the potential, suggesting that perturbation theory can be used in place of Brueckner resummations. Calculations of nuclear matter using the low-momentum two-nucleon force V-lowk with a corresponding leading-order three-nucleon (3N) force from chiral effective field theory (EFT) exhibit nuclear binding in the Hartree-Fock approximation, and become less cutoff dependent with the inclusion of the dominant second-order contributions. The role of the 3N force is essential to obtain saturation, and the contribution to the total potential energy is compatible with EFF power-counting estimates. (c) 2005 Elsevier B.V. All rights reserved.
000050276 536__ $$0G:(DE-Juel1)FUEK241$$2G:(DE-HGF)$$aPhysik der Hadronen$$cM01$$x0
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000050276 7001_ $$0P:(DE-HGF)0$$aSchwenk, A.$$b1
000050276 7001_ $$0P:(DE-HGF)0$$aFurnstahl, R. J.$$b2
000050276 7001_ $$0P:(DE-Juel1)131273$$aNogga, A.$$b3$$uFZJ
000050276 773__ $$0PERI:(DE-600)1466542-6$$a10.1016/j.nuclphysa.2005.08.024$$gVol. 763, p. 59$$p59$$q763<59$$tNuclear physics <Amsterdam> / A$$v763$$x0375-9474$$y2005
000050276 8567_ $$uhttp://dx.doi.org/10.1016/j.nuclphysa.2005.08.024
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