scholarly journals Finite-range separable pairing interaction in Cartesian coordinates

2020 ◽  
Vol 1643 ◽  
pp. 012144
Author(s):  
A. M. Romero ◽  
J. Dobaczewski ◽  
A. Pastore
2011 ◽  
Author(s):  
P. Veselý ◽  
J. Dobaczewski ◽  
N. Michel ◽  
J. Toivanen ◽  
Paraskevi Demetriou ◽  
...  

2011 ◽  
Vol 267 ◽  
pp. 012027 ◽  
Author(s):  
P Veselý ◽  
J Dobaczewski ◽  
N Michel ◽  
J Toivanen

Author(s):  
Nathalie Deruelle ◽  
Jean-Philippe Uzan

This chapter defines the mathematical spaces to which the geometrical quantities discussed in the previous chapter—scalars, vectors, and the metric—belong. Its goal is to go from the concept of a vector as an object whose components transform as Tⁱ → 𝓡ⱼ ⁱTj under a change of frame to the ‘intrinsic’ concept of a vector, T. These concepts are also generalized to ‘tensors’. The chapter also briefly remarks on how to deal with non-Cartesian coordinates. The velocity vector v is defined as a ‘free’ vector belonging to the vector space ε‎3 which subtends ε‎3. As such, it is not bound to the point P at which it is evaluated. It is, however, possible to attach it to that point and to interpret it as the tangent to the trajectory at P.


2021 ◽  
Vol 103 (6) ◽  
Author(s):  
C. Gonzalez-Boquera ◽  
M. Centelles ◽  
X. Viñas ◽  
L. M. Robledo
Keyword(s):  

2021 ◽  
Vol 3 (2) ◽  
pp. 253-261
Author(s):  
Angel Ricardo Plastino ◽  
Gustavo Luis Ferri ◽  
Angelo Plastino

We employ two different Lipkin-like, exactly solvable models so as to display features of the competition between different fermion–fermion quantum interactions (at finite temperatures). One of our two interactions mimics the pairing interaction responsible for superconductivity. The other interaction is a monopole one that resembles the so-called quadrupole one, much used in nuclear physics as a residual interaction. The pairing versus monopole effects here observed afford for some interesting insights into the intricacies of the quantum many body problem, in particular with regards to so-called quantum phase transitions (strictly, level crossings).


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