Paired states of fermions in two dimensions with breaking of parity
... In this paper we will make extensive use of the methods for BCS paired states, and consider the transitions between the weak and strong coupling regimes in two dimensions. In the weak-coupling regime, exotic phenomena are possible when parity and time reversal are broken. The results are applied to ...
... In this paper we will make extensive use of the methods for BCS paired states, and consider the transitions between the weak and strong coupling regimes in two dimensions. In the weak-coupling regime, exotic phenomena are possible when parity and time reversal are broken. The results are applied to ...
Gas Ejection from Spiral Galaxy Disks Jeremy Durelle
... We present the results of three proposed mechanisms for ejection of gas from a spiral arm into the halo. The mechanisms were modelled using magnetohydrodynamics (MHD) as a theoretical template. Each mechanism was run through simulations using a Fortran code: ZEUS-3D, an MHD equation solver. The firs ...
... We present the results of three proposed mechanisms for ejection of gas from a spiral arm into the halo. The mechanisms were modelled using magnetohydrodynamics (MHD) as a theoretical template. Each mechanism was run through simulations using a Fortran code: ZEUS-3D, an MHD equation solver. The firs ...
Lecture Notes in Statistical Mechanics and Mesoscopics Doron Cohen
... Later we shall define some other ”spectral” functions that are related to H. Those can be written as an expectation value of functions of H. ...
... Later we shall define some other ”spectral” functions that are related to H. Those can be written as an expectation value of functions of H. ...
Chapter 2 Coulomb’s Law
... r− 2 ⎠ 4πε 0 ⎜ ⎡ x 2 + ( y − a ) 2 ⎤ 3/ 2 ⎡ x 2 + ( y + a) 2 ⎤ 3/ 2 ⎟ 4πε 0 ⎝ r+ 2 ...
... r− 2 ⎠ 4πε 0 ⎜ ⎡ x 2 + ( y − a ) 2 ⎤ 3/ 2 ⎡ x 2 + ( y + a) 2 ⎤ 3/ 2 ⎟ 4πε 0 ⎝ r+ 2 ...
Physical mechanism of spontaneous fast reconnection evolution M. Ugai
... for the case of VC0 = 12(α = 0.5) during the nonlinear saturation phase of the fast reconnection evolution (Fig. 2), where a pair of thin current layers indicate slow (switch-off) shocks (here, the computational region is restricted to the first quadrant only because of the conventional symmetry bou ...
... for the case of VC0 = 12(α = 0.5) during the nonlinear saturation phase of the fast reconnection evolution (Fig. 2), where a pair of thin current layers indicate slow (switch-off) shocks (here, the computational region is restricted to the first quadrant only because of the conventional symmetry bou ...
Physics Formulary
... possible corrections to the physics formulary. This document is Copyright 1995, 1998 by J.C.A. Wevers. All rights are reserved. Permission to use, copy and distribute this unmodified document by any means and for any purpose except profit purposes is hereby granted. Reproducing this document by any ...
... possible corrections to the physics formulary. This document is Copyright 1995, 1998 by J.C.A. Wevers. All rights are reserved. Permission to use, copy and distribute this unmodified document by any means and for any purpose except profit purposes is hereby granted. Reproducing this document by any ...