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arXiv 0909.4118gr-qc
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高频引力波电磁耦合探测系统中的信号光通量和背景噪声

Signal Photon Flux and Background Noise in a Coupling Electromagnetic Detecting System for High Frequency Gravitational Waves

F. Y. Li, N. Yang, Z. Y. Fang, R. M. L. Baker, G. V. Stephenson, H. Wen

摘要:

利用高斯型微波光子通量、静磁场和分形膜(或其它等效微波透镜)之间的耦合系统可以探测微波波段的高频引力波(HFGW)。研究了耦合系统中的信号光通量、背景光通量和信号光所需的最小积累时间。与GHz频段高频地波引起的纯粹的逆Gertsenshtein效应(G效应)不同,中美高频地波研究小组提出的电磁探测方案(EDS)是基于同步谐振效应和逆G效应的复合效应。方案中的关键参数包括一阶微扰光子通量(PPF)而不是二阶PPF,可分辨的信号是横向的一阶PPF而不是纵向的PPF;由分形膜或其它等效微波透镜聚焦的光子通量不仅是横向一阶PPF而且是总横向光子通量,并且这些光子通量在不同的接收表面处具有不同的信噪比。理论分析和数值估算表明,对于典型的实验室条件和$h_{r.m.s.}\sim10^{-26}-10^{-30}$的参数,在5GHz,带宽$\sim$ 1Hz时,信号在特定接收面和背景噪声起伏中所需的最小积累时间为$\sim10^3-10^5$秒。此外,我们回顾了HFGW的电磁检测中的逆G效应,它表明,在实验室条件下,仅基于纯逆G效应的电磁检测方案将是没有用的HFGW在微波波段的检测。

英文摘要:

A coupling system between Gaussian type-microwave photon flux, static magnetic field and fractal membranes (or other equivalent microwave lenses) can be used to detect high-frequency gravitational waves (HFGWs) in the microwave band. We study the signal photon flux, background photon flux and the requisite minimal accumulation time of the signal in the coupling system. Unlike pure inverse Gertsenshtein effect (G-effect) caused by the HFGWs in the GHz band, the the electromagnetic (EM) detecting scheme (EDS) proposed by China and the US HFGW groups is based on the composite effect of the synchro-resonance effect and the inverse G-effect. Key parameters in the scheme include first-order perturbative photon flux (PPF) and not the second-order PPF; the distinguishable signal is the transverse first-order PPF and not the longitudinal PPF; the photon flux focused by the fractal membranes or other equivalent microwave lenses is not only the transverse first-order PPF but the total transverse photon flux, and these photon fluxes have different signal-to-noise ratios at the different receiving surfaces. Theoretical analysis and numerical estimation show that the requisite minimal accumulation time of the signal at the special receiving surfaces and in the background noise fluctuation would be $\sim10^3-10^5$ seconds for the typical laboratory condition and parameters of $h_{r.m.s.}\sim10^{-26}-10^{-30}$ at 5GHz with bandwidth $\sim$1Hz. In addition, we review the inverse G-effect in the EM detection of the HFGWs, and it is shown that the EM detecting scheme based only on the pure inverse G-effect in the laboratory condition would not be useful to detect HFGWs in the microwave band.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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