Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
Casimir surface force on a dilute dielectric ball. / Brevik, Iver; Marachevsky, Valery N.
в: Physical Review D – Particles and Fields, Том 60, № 8, 085006, 15.10.1999.Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
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TY - JOUR
T1 - Casimir surface force on a dilute dielectric ball
AU - Brevik, Iver
AU - Marachevsky, Valery N.
PY - 1999/10/15
Y1 - 1999/10/15
N2 - The Casimir surface force density F on a dielectric dilute spherical ball of radius a, surrounded by a vacuum, is calculated at zero temperature. We treat (n-1) (n being the refractive index) as a small parameter. The dispersive properties of the material are taken into account by adopting a simple model for the dispersion relation, involving a sharp high frequency cutoff at omega = omega(0). For a nondispersive medium there appears (after regularization) a finite, physical force F-nondisp which is repulsive. By means of a uniform asymptotic expansion of the Riccati-Bessel functions we calculate F-nondisp UP to the fourth order in 1/v. For a dispersive medium the main part of the force F-disp is also repulsive. The dominant term in F-disp is proportional to (n-1)(2)omega(0)(3)/a, and will under usual physical conditions outweigh F-nondisp by several orders of magnitude. [S0556-2821(99)05281-2].
AB - The Casimir surface force density F on a dielectric dilute spherical ball of radius a, surrounded by a vacuum, is calculated at zero temperature. We treat (n-1) (n being the refractive index) as a small parameter. The dispersive properties of the material are taken into account by adopting a simple model for the dispersion relation, involving a sharp high frequency cutoff at omega = omega(0). For a nondispersive medium there appears (after regularization) a finite, physical force F-nondisp which is repulsive. By means of a uniform asymptotic expansion of the Riccati-Bessel functions we calculate F-nondisp UP to the fourth order in 1/v. For a dispersive medium the main part of the force F-disp is also repulsive. The dominant term in F-disp is proportional to (n-1)(2)omega(0)(3)/a, and will under usual physical conditions outweigh F-nondisp by several orders of magnitude. [S0556-2821(99)05281-2].
KW - BULK ENERGY CONTRIBUTION
KW - ELECTROMAGNETIC-FIELD
KW - SOLID BALL
KW - EPSILON(OMEGA)MU(OMEGA)=1
KW - SONOLUMINESCENCE
KW - QUANTIZATION
KW - MEDIA
U2 - 10.1103/PhysRevD.60.085006
DO - 10.1103/PhysRevD.60.085006
M3 - статья
VL - 60
JO - Physical review D
JF - Physical review D
SN - 2470-0010
IS - 8
M1 - 085006
ER -
ID: 5142472