scholarly journals Ground state energy of mean field model of interacting bosons in Bernoulli potential

2013 ◽  
Vol 54 (8) ◽  
pp. 081902 ◽  
Author(s):  
M. Bishop ◽  
J. Wehr
2020 ◽  
Vol 2 (1) ◽  
Author(s):  
Yibing Shen ◽  
Phillip Isaac ◽  
Jon Links

We investigate the ground-state energy of a Richardson-Gaudin integrable BCS model, generalizing the closed and open p+ip models. The Hamiltonian supports a family of mutually commuting conserved operators satisfying quadratic relations. From the eigenvalues of the conserved operators we derive, in the continuum limit, an integral equation for which a solution corresponding to the ground state is established. The energy expression from this solution agrees with the BCS mean-field result.


Author(s):  
Wei-Kuo Chen ◽  
Arnab Sen

Abstract For $p\geq 1$ and $(g_{ij})_{1\leq i,j\leq n}$ being a matrix of i.i.d. standard Gaussian entries, we study the $n$-limit of the $\ell _p$-Gaussian–Grothendieck problem defined as $$\begin{align*} & \max\Bigl\{\sum_{i,j=1}^n g_{ij}x_ix_j: x\in \mathbb{R}^n,\sum_{i=1}^n |x_i|^p=1\Bigr\}. \end{align*}$$The case $p=2$ corresponds to the top eigenvalue of the Gaussian orthogonal ensemble; when $p=\infty $, the maximum value is essentially the ground state energy of the Sherrington–Kirkpatrick mean-field spin glass model and its limit can be expressed by the famous Parisi formula. In the present work, we focus on the cases $1\leq p<2$ and $2<p<\infty .$ For the former, we compute the limit of the $\ell _p$-Gaussian–Grothendieck problem and investigate the structure of the set of all near optimizers along with stability estimates. In the latter case, we show that this problem admits a Parisi-type variational representation and the corresponding optimizer is weakly delocalized in the sense that its entries vanish uniformly in a polynomial order of $n^{-1}$.


1992 ◽  
Vol 06 (22) ◽  
pp. 3543-3553
Author(s):  
D.M. GAITONDE ◽  
SUMATHI RAO

We show that the low energy limit of relativistic fermions interacting with a statistical gauge field also includes a scalar interaction. When the Chern-Simons (CS) parameter µ=e2/2π and the scalar interaction is precisely that which is obtained through relativistic reduction, the many-body Hamiltonian can be solved exactly, directly in the fermion gauge, for the ground state energy which is zero and the ground state wavefunction which is gauge equivalent to one, characteristic of free bosons. Conversely, for N bosons interacting with a CS gauge field with µ=e2/2π, the mean-field ground state energy is πN2/m, which is characteristic of N free fermions.


1997 ◽  
Vol 12 (18) ◽  
pp. 1317-1325 ◽  
Author(s):  
Raj K. Gupta ◽  
S. K. Patra ◽  
W. Greiner

Use of the NL-SH parameter set is re-analyzed and a new parameter set TM2 is used for the first time in the axially deformed self-consistent relativistic mean-field calculations for 44 S and its neighboring nuclei 40 Mg and 42 Si . The spherical shell gap at N=28 in 44 S is found to be intact for the TM2 parameter set since it predicts the ground state of 44 S as nearly spherical, irrespective of the strength of the pairing force. The predictions of the NL-SH parameter set for 44 S are found to depend strongly on the pairing strength and, due to shape coexistence, the ground state could be strongly prolate or strongly oblate deformed. Hence, for the NL-SH parameter set, the spherical shell gap at N=28 in 44 S is broken for either of the prolate/oblate deformation. For 40 Mg and 42 Si , the spherical shell gap at N=28 is found broken under all conditions since the predicted deformations are large, independent of both the pairing strength and the choice of parameter set. This calls for immediate measurements of the deformations of these nuclei, particularly for 44 S which will decide its shell structure as well as the region of deformation in light nuclei.


2015 ◽  
Vol 93 (10) ◽  
pp. 1024-1029 ◽  
Author(s):  
Ch. Narasimha Raju ◽  
Ashok Chatterjee

A single-level Anderson–Holstein model is studied using the Lang–Firsov transformation followed by a zero-phonon averaging and a Green function method within the framework of a mean-field approximation. The ground state energy of the system, the binding energy between the impurity and conduction electrons, and the impurity–electron spectral function are calculated. The effect of the electron–phonon interaction on the local moment as well as on the specific heat of the impurity electron is explored in the anti-adiabatic regime.


2019 ◽  
Vol 31 (02) ◽  
pp. 1950005 ◽  
Author(s):  
Alessandro Michelangeli ◽  
Phan Thành Nam ◽  
Alessandro Olgiati

We consider the asymptotic behavior of a system of multi-component trapped bosons, when the total particle number [Formula: see text] becomes large. In the dilute regime, when the interaction potentials have the length scale of order [Formula: see text], we show that the leading order of the ground state energy is captured correctly by the Gross–Pitaevskii energy functional and that the many-body ground state fully condensates on the Gross–Pitaevskii minimizers. In the mean-field regime, when the interaction length scale is [Formula: see text], we are able to verify Bogoliubov’s approximation and obtain the second order expansion of the ground state energy. While such asymptotic results have several precursors in the literature on one-component condensates, the adaptation to the multi-component setting is non-trivial in various respects and the analysis will be presented in detail.


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