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Related papers: Partial conservation of seniority in $j=9/2$ shell…

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The shell structures for weakly interacting fermions in harmonic oscillator traps at zero temperature undergo several transitions depending on the number of particles in the trap and their interaction strength. Calculations of the one and…

Condensed Matter · Physics 2011-07-19 Henning Heiselberg , Ben Mottelson

In the present work available experimental data up to high-spin states of $^{119-126}$Sn isotopes with different seniority ($v$), including $v$ = 4, 5, 6, and 7 have been interpreted with shell model, by performing full-fledged shell model…

Nuclear Theory · Physics 2019-10-23 Praveen C. Srivastava , Bharti Bhoy , M. J. Ermamatov

As generalizations of the fermion seniority model, four multi-mode Hamiltonians are considered to investigate some of the consequences of the pairing of parafermions of order two. 2-particle and 4-particle states are explicitly constructed…

High Energy Physics - Phenomenology · Physics 2008-11-26 Charles A. Nelson

We study the nature of many-body eigenstates of a system of interacting chiral spinless fermions on a ring. We find a coexistence of fermionic and bosonic types of eigenstates in parts of the many-body spectrum. Some bosonic eigenstates,…

Strongly Correlated Electrons · Physics 2022-01-26 I. Martin , K. A. Matveev

It is noted that in a calculation with 4 nucleons with isospin 1 in a single j shell (f_{7/2}, g_{9/2}, h_{11/2}) the state with median angular momentum J = (J_{max}+1)/2 lies very low in energy becoming either an isomeric state or a ground…

Nuclear Theory · Physics 2012-06-13 Larry Zamick , Alberto Escuderos

We continue a series of numerical experiments on many-body systems with random two-body interactions, by examining correlations in ratios in excitation energies of yrast $J$ = 0, 2, 4, 6, 8 states. Previous studies, limited only to $J$ =…

Nuclear Theory · Physics 2013-05-29 Calvin W. Johnson , Hai Ah Nam

We investigate the generic pairing properties of shell-model many-body Hamiltonians drawn from ensembles of random two-body matrix elements. Many features of pairing that are commonly attributed to the interaction are in fact seen in a…

Nuclear Theory · Physics 2009-10-31 C. W. Johnson , G. F. Bertsch , D. J. Dean , I. Talmi

We study spin-1/2 fermions, interacting via a two-body contact potential, in a one-dimensional harmonic trap. Applying exact diagonalization, we investigate their behavior at finite interaction strength, and discuss the role of the…

Quantum Physics · Physics 2013-09-09 Tomasz Sowiński , Tobias Grass , Omjyoti Dutta , Maciej Lewenstein

For single-$j$ shells with $j={7/2}, {9/2}$ and 11/2, we relate the large probability of $I^+$ ground states to the largest (smallest) coefficients $\alpha^J_{I(v \beta)} = <nv \beta I |$ $A^{J \dagger} \cdot A^J | n v\beta I>$, where $n$…

Nuclear Theory · Physics 2011-05-12 Y. M. Zhao , A. Arima

We point out a simplicity that arises when we use an interaction in which only an energy with odd J is non-zero. The emphasis is on J=J_{\text{max}} and in particular J=9^{+} in the g_{9/2} shell. It is noted that high overlaps can be…

Nuclear Theory · Physics 2015-03-25 L. Zamick , A. Escuderos

In the nuclear f_7/2 shell, the nucleon-nucleon interaction can be represented by the eight values E(J)=<(f^2_{7/2})^J |V| (f^2_{7/2})^J>, J=0,1,...,7, where for even J the isospin is 1, and for odd J it is 0. If we set the T=0 (odd J)…

Nuclear Theory · Physics 2009-11-11 A. Escuderos , B. F. Bayman , L. Zamick , S. J. Q. Robinson

In this Brief Report, we propose general expressions for 6j and 9j coefficients arising in the study of the J-pairing interaction of identical fermions in a single-j shell. In the literature such coefficients are available only for a number…

Nuclear Theory · Physics 2015-05-30 Jean-Christophe Pain

In the present work we report a comprehensive analysis of shell model results for high-spin states of $^{87}$Sr and $^{87}$Zr for recently available experimental data within the full $f_{5/2}pg_{9/2}$ model space using JUN45 and jj44b…

Nuclear Theory · Physics 2016-09-20 P. C. Srivastava , Vikas Kumar , M. J. Ermamatov

We study multi-hadron systems with a single heavy quark (charm or bottom) in the limit of heavy quark mass. The spin degeneracy of the states with quantum numbers $(j+1/2)^{P}$ and $(j-1/2)^{P}$ for $j \neq 0$, known in a normal hadron, can…

High Energy Physics - Phenomenology · Physics 2019-08-07 S. Yasui , K. Sudoh , Y. Yamaguchi , S. Ohkoda , A. Hosaka , T. Hyodo

In this talk I shall discuss some regularities of many-body systems in the presence of random interactions and regularities of a single-$j$ shell for the $J$ pairing interaction which works only when two particles are coupled to spin $J$. I…

Nuclear Theory · Physics 2016-09-08 A. Arima

We discuss partial dynamical symmetries which occur in single j shell calculations mostly for high spin states for systems of three or four particles (holes). The relevant nuclei are 43Ti,43Sc, 44Ti, 52Fe,53Fe, 53Co,96Cd,97Cd, and 97In.

Nuclear Theory · Physics 2015-03-25 Larry Zamick

In an old paper [ 1] B.H. Flowers discussed calculations for odd A nuclei in the g9/2 shell. He finds when he varies the parameters of a certain interaction that the lowest energy state is always a seniority v=1 state with angular momentum…

Nuclear Theory · Physics 2022-10-05 Larry Zamick

We performed \textit{ab initio} valence-space in-medium similarity renormalization group (VS-IMSRG) calculations based on chiral two-nucleon and three-nucleon interactions to investigate the anomalous seniority breaking in the neutron…

Nuclear Theory · Physics 2024-09-17 Q. Yuan , B. S. Hu

The puzzle of finding consistent nuclear configurations for explaining both the decay probabilities and moments of the ${9/2}^-$, ${8}^+$ and ${21/2}^-$ isomers in and around $N=126$ closed shell has been approached in the generalized…

Nuclear Theory · Physics 2022-03-02 Bhoomika Maheshwari , Deepika Choudhury , Ashok Kumar Jain

We point out a simplicity that arises when we use an interaction in which only an energy with odd J is non-zero. The emphasis is on J= J_{max} and in particular J=9+ in the g_{9/2} shell. It is noted that high overlaps can be deceptive. In…

Nuclear Theory · Physics 2015-06-11 L. Zamick , A. Escuderos