Casimir Effect at Finite Temperature

Zheng Taiyu

Chinese Physics C> 1995, Vol. 19> Issue(3) : 241-244

Casimir Effect at Finite Temperature

Zheng Taiyu ^,

Department of Physics, Nor theast Normal University, Changgchun 130024

Abstract
HTML
Reference
Related

PDF

Abstract：
The contribution of the free electromagnetic field and internal fermion oneloop to Casimir force between two parallel conducting plates at finite temperature are calculated by using the Feynman path integral method.

References

[1]

I.Brevik,H.B.Nielsen,Phys.Rev.,D41（1990）1185.[2]郑泰玉，高能物理与核物理，9（1990）798.[3]D.Keppner,Phys.Today,43（1990）9.[4]郑泰玉，薛社生，科学通报，13（1992）1170.[5]V.B.Braginsky,F.Ya.Khalili,Phys.Lett,A167（1992）1.[6]A.A.Bytsenko,G.Gognola,L.Vanzo,J.Math.Phys.,33（1992）3108.[7]H.B.G.Casimir,Proc.K.Ned.Akad.Wet,51（1948）793.[8]J.Mehra,Physica,37（1967）145.

[1] A.G.Drentje . Gas-mixing: Ion Cooling or Reduced Turbulent Heating?. Chinese Physics C, 2007, 31(S1): 162-164.
Access

Get Citation

Zheng Taiyu. Casimir Effect at Finite Temperature[J]. Chinese Physics C, 1995, 19(3): 241-244.

Zheng Taiyu. Casimir Effect at Finite Temperature[J]. Chinese Physics C, 1995, 19(3): 241-244. shu

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

Received: 1900-01-01
Revised: 1900-01-01

Article Metric

Article Views(3436)
PDF Downloads(555)
Cited by(0)

Policy on re-use

To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.

通讯作者: 陈斌, bchen63@163.com

1.
沈阳化工大学材料科学与工程学院沈阳 110142

Casimir Effect at Finite Temperature

Zheng Taiyu ^,

Corresponding author: Zheng Taiyu,

Department of Physics, Nor theast Normal University, Changgchun 130024

Received Date: 1900-01-01
Accepted Date: 1900-01-01
Available Online: 1995-03-05

Abstract: The contribution of the free electromagnetic field and internal fermion oneloop to Casimir force between two parallel conducting plates at finite temperature are calculated by using the Feynman path integral method.