Dynamics of Disordered Harmonic Lattices. I. Normal-Mode Frequency Spectra for Randomly Disordered Isotopic Binary Lattices

1967 ◽  
Vol 154 (3) ◽  
pp. 802-811 ◽  
Author(s):  
Daniel N. Payton ◽  
William M. Visscher

2020 ◽  
Vol 897 (1) ◽  
pp. 38 ◽  
Author(s):  
Srijan Bharati Das ◽  
Tuneer Chakraborty ◽  
Shravan M. Hanasoge ◽  
Jeroen Tromp


Author(s):  
A. V. Kalinina ◽  
V. A. Volkov ◽  
A. V. Gorbatikov ◽  
J. Arnoso ◽  
R. Vieira ◽  
...  


1976 ◽  
Vol 25 (3) ◽  
pp. 1192-1193
Author(s):  
M. S. Savogina ◽  
A. M. Aleksandrovskaya ◽  
M. V. Shchigal ◽  
M. V. Nikonov ◽  
V. V. Nikitenko


2004 ◽  
Vol 161 (7) ◽  
pp. 1597-1611 ◽  
Author(s):  
A. V. Kalinina ◽  
V. A. Volkov ◽  
A. V. Gorbatikov ◽  
J. Arnoso ◽  
R. Vieira ◽  
...  


1990 ◽  
Vol 52 (1) ◽  
pp. 50-55 ◽  
Author(s):  
M. V. Korolevich ◽  
V. A. Lastochkina ◽  
R. G. Zhbankov


2015 ◽  
Vol 81 (3) ◽  
Author(s):  
J. J. Ramos

This paper presents an explicit proof that, in the kinetic magnetohydrodynamics framework, the squared frequencies of normal-mode perturbations about a static equilibrium are real. This proof is based on a quadratic form for the square-integrable normal-mode eigenfunctions and does not rely on demonstrating operator self-adjointness. The analysis is consistent with the quasineutrality condition without involving any subsidiary constraint to enforce it, and does not require the assumption that all particle orbits be periodic. It applies to Maxwellian equilibria, spatially bounded by either a rigid conducting wall or by a plasma-vacuum interface where the density goes continuously to zero.



2012 ◽  
Vol 190 (2) ◽  
pp. 1097-1110 ◽  
Author(s):  
Toshiro Tanimoto ◽  
Chen Ji ◽  
Mitsutsugu Igarashi


Author(s):  
Guijia Chen ◽  
Rongxing Wu ◽  
Ji Wang ◽  
Jianke Du ◽  
Jiashi Yang


2012 ◽  
Vol 27 (03) ◽  
pp. 1250015
Author(s):  
HYOJOONG KIM ◽  
NAKWOO KIM ◽  
JUNG HUN LEE

We consider circular spinning string solutions in AdS5×T1, 1 and calculate the quantum corrections to the energy at one-loop on worldsheet. The fluctuations are given as a set of harmonic oscillators and we calculate their normal mode frequency in closed form. The sum of frequency is equal to the one-loop string energy, which through AdS/CFT correspondence corresponds to the leading order correction of the conformal dimension for long operators in Klebanov–Witten conifold gauge field theory.



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