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Related papers: J=0, J=J_{max} and quadrupole pairing

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We had previously used techniques involving isospin to count the number of states for three identical fermions in a single j shell with total angular momentum I=j. We generalize this to all I, but the main thrust of this work is to consider…

Nuclear Theory · Physics 2009-11-11 L. Zamick , A. Escuderos

For a bound state internal wave function respecting parity symmetry, it can be rigorously argued that the mean electric dipole moment must be strictly zero. Thus, both the neutron, viewed as a bound state of three quarks, and the water…

High Energy Physics - Phenomenology · Physics 2010-12-13 Y. N. Srivastava , A. Widom , J. Swain , O. Panella

We address some properties of the quadrupole-quadrupole ($Q \cdot Q$) interaction in nuclear studies. We first consider how to restore $SU(3)$ symmetry even though we use only coordinate and not momentum terms. Using the Hamiltonian…

Nuclear Theory · Physics 2007-05-23 M. S. Fayache , Y. Y. Sharon , L. Zamick

We define the ``quadrupole ratio'' $r_Q = \dfrac{Q_0(S)}{Q_0(B)}$ where $Q_0(S)$ is the intrinsic quadrupole moment obtained from the static quadrupole moment of the $2_1^+$ state of an even-even nucleus and $Q_0(B)$ the intrinsic…

Nuclear Theory · Physics 2008-08-28 Sean Yeager , Larry Zamick

We discuss the systematics of ground-state quadrupole correlations of binding energies and mean-square charge radii for all even-even nuclei, from O16 up to the superheavies, for which data are available. To that aim we calculate their…

Nuclear Theory · Physics 2009-11-11 M. Bender , G. F. Bertsch , P. -H. Heenen

The three main contributions to the nuclear Hamiltonian - monopole, quadrupole and pairing - are analyzed in a shell model context. The first has to be treated phenomenologically, while the other two can be reliably extracted from the…

Nuclear Theory · Physics 2019-05-27 A. P. Zuker

Nuclei with spin $I \ge 1$ have a weak quadrupole moment which leads to tensor contribution to the parity non-conserving interaction between nuclei and electrons. We calculate this contribution for Yb$^+$, Fr and Ra$^+$ and found it to be…

Atomic Physics · Physics 2017-09-13 V. V. Flambaum , V. A. Dzuba , C. Harabati

The pairing correlation energy for two-nucleon configurations with the spin-parity and isospin of $J^\pi=0^+$, $T$=1 and $J^\pi=1^+$, $T$=0 are calculated with $T$=1 and $T$=0 pairing interactions, respectively. To this end, we consider the…

Nuclear Theory · Physics 2015-06-12 H. Sagawa , Y. Tanimura , K. Hagino

The role of pairing correlations for nucleon pairs with isospin $T=1$ and $T=0$ is investigated for nuclei in the mass region $12 \leq A \leq 42$. For that purpose the two-nucleon densities resulting from nuclear shell-model calculations in…

Nuclear Theory · Physics 2023-06-21 H. Müther , Praveen C. Srivastava

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

Low-lying states in nuclei are investigated using an ensemble of random interactions. Both in the nuclear shell model and in the interacting boson model we find a dominance of $J^P=0^+$ ground states. It is shown that this feature is not…

Nuclear Theory · Physics 2017-11-03 R. Bijker , A. Frank , S. Pittel

Our main concern in this work is to show how higher shell admixtures affect the spectrum of a Q.Q interaction. We first review how, in the valence space, the familiar SU(3) result for the energy spectrum can be obtained using a coordinate…

Nuclear Theory · Physics 2009-10-31 M. S. Fayache , E. Moya de Guerra , P. Sarriguren , L. Zamick

In the rotational model for a K=0 band in an even-even nucleus, there is a single parameter--Q_0, the intrinsic quadrupole moment. All B(E2)'s in the band and all static quadrupole moments are expressed in terms of this one parameter. In…

Nuclear Theory · Physics 2007-06-12 A. Escuderos , L. Zamick

We show that fully aligned neutron-proton pairs play a crucial role in the low-energy spectroscopy of nuclei. with valence nucleons in a high-j orbital. Their dominance is valid in nuclei with valence neutrons and protons in different…

Nuclear Theory · Physics 2018-04-11 Y. H. Kim , M. Rejmund , P. Van Isacker , A. Lemasson

We consider systems of two and three electrons in a two-dimensional parabolic quantum dot. A magnetic field is applied perpendicularly to the electron plane of motion. We show that the energy levels corresponding to states with high angular…

Mesoscale and Nanoscale Physics · Physics 2014-10-13 Augusto Gonzalez , Ricardo Perez , Pavel Fileviez

The ground state and low-lying continuum states of 6He are found within a shell model scheme, in a basis of two-particle states built out of continuum p-states of the unbound 5He nucleus, using a simple pairing contact-delta interaction.…

Nuclear Theory · Physics 2014-12-03 L. Fortunato , R. Chatterjee , Jagjit Singh , A. Vitturi

The influence of quadrupole and hexadecapole residual interactions on rotational bands is investigated in a single-j shell model. An exact shell-model diagonalization of quadrupole-plus-hexadecapole interaction can sometimes produce a…

Nuclear Theory · Physics 2008-11-26 P. Magierski , K. Burzynski , E. Perlinska , J. Dobaczewski , W. Nazarewicz

The standard description of the nucleon in the non-relativistic quark model is an $1S,L=0$ state without orbital motion. Yet, there are several indications from phenomenology that an admixture of states with nonzero orbital motion maybe…

High Energy Physics - Phenomenology · Physics 2025-03-18 Nicholas Miesch , Edward Shuryak , Ismail Zahed

In this work we make further studies of the quadrupole quadrupole interaction used in shell model calculations.Whereas in a previous work we adjusted the single particle energies so as to obtain the rotatonal spectrum of the Elliott model,…

Nuclear Theory · Physics 2021-04-06 Mingyang Ma , Praveen C Srivastava , Larry Zamick