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If physics beyond the Standard Model enters well above the electroweak scale, its low-energy effects are described by Standard Model Effective Field Theory. Already at dimension six many operators involve the antisymmetric quark tensor…

High Energy Physics - Phenomenology · Physics 2020-05-11 Martin Hoferichter , Bastian Kubis , Jacobo Ruiz de Elvira , Peter Stoffer

An electron density functional approach for the calculation of the nuclear multipole moments is presented. The electronic matrix elements entering the experimentally observed hyperfine electron-nucleus interaction constants in atoms are…

Nuclear Theory · Physics 2007-05-23 R. L. Pavlov , P. P. Raychev , V. P. Garistov , M. Dimitrova-Ivanovich , J. Maruani

General formulas are derived for the quasiparticle effective mass and the equation of state of the Fermi system with account of the interparticle attraction at long distances and repulsion at short distances. Calculations are carried out of…

Statistical Mechanics · Physics 2015-11-25 Yu. M. Poluektov , A. A. Soroka

Weak values are traditionally obtained using a weak interaction between the measured system and a pointer state. It has, however, been pointed out that weak coupling can be replaced by a carefully tailored strong interaction. This paper…

Quantum Physics · Physics 2020-06-24 Jan Roik , Karel Lemr , Antonín Černoch , Karol Bartkiewicz

The quality of HFB wave functions are tested by comparing the theoretically calculated results with the available experimental data for a number of spectroscopic properties like yrast spectra, reduced B(E2) transition probabilities,…

Nuclear Theory · Physics 2009-11-10 P. K. Raina , A. Shukla , P. K. Rath , B. M. Dixit , K. Chaturvedi , R. Chandra , S. K. Dhiman , A. J. Singh

Coherent and incoherent neutron-matter interaction is studied inside a recently introduced approach to subdynamics of a macrosystem. The equation describing the interaction is of the Lindblad type and using the Fermi pseudopotential we show…

Quantum Physics · Physics 2008-12-18 L. Lanz , B. Vacchini

In neutrino physics, while massive states define neutrino masses, the flavor states participating in weak interactions are governed by an off-diagonal mass matrix. This work examines the complete form of this mass matrix, both for a…

High Energy Physics - Phenomenology · Physics 2025-11-13 Danil D. Shelkovkin , Oleg V. Teryaev

Experimental results for sub-barrier nuclear fusion reactions show cross section enhancements with respect to bare nuclei which are generally larger than those expected according to electron screening calculations. We point out that energy…

Astrophysics · Physics 2009-11-07 G. Fiorentini , C. Rolfs , F. L. Villante , B. Ricci

Light nuclei production as a result of nuclear coalescence effect can give some signals on final state of Quark Gluon Plasma formation. We are studying the behavior of nuclear modification factor as a function of different variables using…

Nuclear Experiment · Physics 2009-04-15 K. H. Khan , M. K. Suleymanov , Z. Wazir , E. U. Khan , Mahnaz Q. Haseeb , M. Ajaz

Including nucleon-nucleon correlations due to both Fermi statistics and nuclear forces, we have developed a general formalism for calculating the neutral-current neutrino-nucleon opacities in nuclear matter. We derive corrections to the…

Astrophysics · Physics 2008-11-26 Adam Burrows , R. F. Sawyer

Allowed weak interaction rates for sd-shell nuclei in stellar environment are calculated using a generalized form of proton-neutron quasiparticle RPA model with separable Gamow-Teller forces. Twelve different weak rates are calculated for…

Nuclear Theory · Physics 2009-10-31 J. -U. Nabi , H. V. Klapdor-Kleingrothaus

The atomic nucleus is composed of two different kinds of fermions, protons and neutrons. If the protons and neutrons did not interact, the Pauli exclusion principle would force the majority fermions (usually neutrons) to have a higher…

Nuclear Experiment · Physics 2014-12-02 O. Hen , M. Sargsian , L. B. Weinstein , E. Piasetzky , H. Hakobyan , D. W. Higinbotham , M. Braverman , W. K. Brooks , S. Gilad , K. P. Adhikari , J. Arrington , G. Asryan , H. Avakian , J. Ball , N. A. Baltzell , M. Battaglieri , A. Beck , S. May-Tal Beck , I. Bedlinskiy , W. Bertozzi , A. Biselli , V. D. Burkert , T. Cao , D. S. Carman , A. Celentano , S. Chandavar , L. Colaneri , P. L. Cole , V. Crede , A. DAngelo , R. De Vita , A. Deur , C. Djalali , D. Doughty , M. Dugger , R. Dupre , H. Egiyan , A. El Alaoui , L. El Fassi , L. Elouadrhiri , G. Fedotov , S. Fegan , T. Forest , B. Garillon , M. Garcon , N. Gevorgyan , Y. Ghandilyan , G. P. Gilfoyle , F. X. Girod , J. T. Goetz , R. W. Gothe , K. A. Griffioen , M. Guidal , L. Guo , K. Hafidi , C. Hanretty , M. Hattawy , K. Hicks , M. Holtrop , C. E. Hyde , Y. Ilieva , D. G. Ireland , B. I. Ishkanov , E. L. Isupov , H. Jiang , H. S. Jo , K. Joo , D. Keller , M. Khandaker , A. Kim , W. Kim , F. J. Klein , S. Koirala , I. Korover , S. E. Kuhn , V. Kubarovsky , P. Lenisa , W. I. Levine , K. Livingston , M. Lowry , H. Y. Lu , I. J. D. MacGregor , N. Markov , M. Mayer , B. McKinnon , T. Mineeva , V. Mokeev , A. Movsisyan , C. Munoz Camacho , B. Mustapha , P. Nadel-Turonski , S. Niccolai , G. Niculescu , I. Niculescu , M. Osipenko , L. L. Pappalardo , R. Paremuzyan , K. Park , E. Pasyuk , W. Phelps , S. Pisano , O. Pogorelko , J. W. Price , S. Procureur , Y. Prok , D. Protopopescu , A. J. R. Puckett , D. Rimal , M. Ripani , B. G. Ritchie , A. Rizzo , G. Rosner , P. Rossi , P. Roy , F. Sabatie , D. Schott , R. A. Schumacher , Y. G. Sharabian , G. D. Smith , R. Shneor , D. Sokhan , S. S. Stepanyan , S. Stepanyan , P. Stoler , S. Strauch , V. Sytnik , M. Taiuti , S. Tkachenko , M. Ungaro , A. V. Vlassov , E. Voutier , D. Watts , N. K. Walford , X. Wei , M. H. Wood , S. A. Wood , N. Zachariou , L. Zana , Z. W. Zhao , X. Zheng , I. Zonta

The model suggested by Love and Franey for description of the nucleon-nucleon interaction was used as the base. The new fitting of the model parameters was done in the energy range from 100 MeV up to 1100 MeV. It is based on the modern…

Nuclear Theory · Physics 2008-05-21 N. B. Ladygina

We investigate one-dimensional harmonically trapped two-component systems for repulsive interaction strengths ranging from the non-interacting to the strongly interacting regime for Fermi-Fermi mixtures. A new and powerful mapping between…

Quantum Gases · Physics 2017-02-17 F. F. Bellotti , A. S. Dehkharghani , N. T. Zinner

We report the results of a calculation of the response of cold neutron matter to neutral-current interactions with low energy neutrinos, carried out using an effective interaction and effective operators consistently derived within the…

Nuclear Theory · Physics 2015-06-17 Alessandro Lovato , Omar Benhar , Stefano Gandolfi , Cristina Losa

Atomic nuclei are complex, quantum many-body systems whose structure manifests itself through intrinsic quantum states associated with different excitation modes or degrees of freedom. Collective modes (vibration and/or rotation) dominate…

Nuclear Theory · Physics 2015-05-19 Alexis Diaz-Torres

A new model for calculating nuclear level densities is investigated. The single-nucleon spectra are calculated in a relativistic mean-field model with energy-dependent effective mass, which yields a realistic density of single-particle…

Nuclear Theory · Physics 2008-11-26 R. Pezer , A. Ventura , D. Vretenar

Unbiased stochastic sampling of the one- and two-body reduced density matrices is achieved in full configuration interaction quantum Monte Carlo with the introduction of a second, "replica" ensemble of walkers, whose population evolves in…

Computational Physics · Physics 2015-09-02 Robert E. Thomas , Daniel Opalka , Catherine Overy , Peter J. Knowles , Ali Alavi , George H. Booth

An exploratory study of chiral four-nucleon interactions in nuclear and neutron matter is performed. The leading-order terms arising from pion-exchange in combination with the chiral $4\pi$-vertex and the chiral NN$3\pi$-vertex are found to…

Nuclear Theory · Physics 2015-06-11 N. Kaiser

Using a fermionic renormalization group approach we analyse a model where the electrons diffusing on a quantum dot interact via Fermi-liquid interactions. Describing the single-particle states by Random Matrix Theory, we find that…

Mesoscale and Nanoscale Physics · Physics 2009-11-07 Ganpathy Murthy , Harsh Mathur