Sojourn-time approach to interaction time in quantum scattering: One-dimensional scattering with internal degrees of freedom

1990 ◽  
Vol 42 (9) ◽  
pp. 5253-5268 ◽  
Author(s):  
Wojciech Jaworski ◽  
David M. Wardlaw
1995 ◽  
Vol 51 (9) ◽  
pp. 5790-5799 ◽  
Author(s):  
M. Yu. Lavrentiev ◽  
H. Köppel ◽  
L. S. Cederbaum

1987 ◽  
Vol 9 (5) ◽  
pp. 571-579 ◽  
Author(s):  
F. Fischer ◽  
H. Köppel ◽  
L. S. Cederbaum

Author(s):  
H. H. Huang ◽  
C. T. Sun

Metamaterials are materials with manmade microstructures. Recently, researchers have looked at a class of metamaterials whose microstructures contain internal degrees of freedom that are different from those of the macro-medium. These metamaterials exhibit unusual dynamic behavior and if modeled as homogeneous solids then their effective mass densities would become negative in certain frequency range. Specifically, a new stop band in the vicinity of the local resonance frequency of the internal mass in the microstructure would result. In this paper, a one dimensional metamaterial is employed to investigate the meaning of the negative mass density in the material and the energy flow in and out of the microstructure. In addition, numerical solutions are used to illustrate the phenomenon.


2016 ◽  
Vol 23 (1) ◽  
pp. 85-98 ◽  
Author(s):  
Maurizio Romeo

A continuum model, based on a theory of electromagnetic media with microstructure, is exploited to deal with rigid conductors endowed with polarization and magnetization. Charge carriers are considered as a continuum superimposed to the microstructured conductor where the density of bound charges depends on the internal degrees of freedom of the continuum particle. The non-linear dynamical model is formulated, deriving the mechanical balance laws that are coupled with the electromagnetic field equations. A reduction to the micropolar linear case is performed in order to analyze admissible solutions in the form of one-dimensional plane waves. Dispersion equations are derived for modes pertaining to longitudinal and transverse fields and the effects of conductivity and polarization are evidentiated. Polariton modes, arising from the dynamics of microdeformation, are also discussed.


2019 ◽  
pp. 585-630
Author(s):  
Hans-Peter Eckle

The Bethe ansatz can be generalized to problems where particles have internal degrees of freedom. The generalized method can be viewed as two Bethe ansätze executed one after the other: nested Bethe ansatz. Electronic systems are the most relevant examples for condensed matter physics. Prominent electronic many-particle systems in one dimension solvable by a nested Bethe ansatz are the one-dimensional δ‎-Fermi gas, the one-dimensional Hubbard model, and the Kondo model. The major difference to the Bethe ansatz for one component systems is a second, spin, eigenvalue problem, which has the same form in all cases and is solvable by a second Bethe ansatz, e.g. an algebraic Bethe ansatz. A quantum dot tuned to Kondo resonance and coupled to an isolated metallic ring presents an application of the coupled sets of Bethe ansatz equations of the nested Bethe ansatz.


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