Signal photon flux and background noise in a coupling electromagnetic detecting system for high-frequency gravitational waves
Signal photon flux and background noise in a coupling electromagnetic detecting system for high-frequency gravitational waves
A coupling system among Gaussian-type microwave photon flux, a 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 the pure inverse Gertsenshtein effect (G effect) caused by the HFGWs in the gigahertz band, the electromagnetic (EM) detecting scheme proposed by China and the U.S. HFGW groups is based on the composite effect of the synchroresonance effect and the inverse G effect. The key parameter in the scheme is the 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 ~103-105 seconds for the typical laboratory condition and parameters of hrms ~ 10-26-10-30/?Hz at 5 GHz with bandwidth ~1 Hz. 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
14-[pp]
Li, Fangyu
df332691-d849-4347-8b88-845e85314359
Yang, Nan
237454dd-1905-4dd0-b5bd-ef75c2c4035a
Fang, Zhenyun
180b85d7-1f10-48a9-b51a-560759578143
Baker, Robert M.L.
9bd95aaf-13f2-485e-b414-f38077fd4cc2
Stephenson, Gary V.
27877f10-af6a-4836-ab4d-782465bb53ba
Wen, Hao
2a04e120-d889-487f-96c6-25b4d9f44afc
9 September 2009
Li, Fangyu
df332691-d849-4347-8b88-845e85314359
Yang, Nan
237454dd-1905-4dd0-b5bd-ef75c2c4035a
Fang, Zhenyun
180b85d7-1f10-48a9-b51a-560759578143
Baker, Robert M.L.
9bd95aaf-13f2-485e-b414-f38077fd4cc2
Stephenson, Gary V.
27877f10-af6a-4836-ab4d-782465bb53ba
Wen, Hao
2a04e120-d889-487f-96c6-25b4d9f44afc
Li, Fangyu, Yang, Nan, Fang, Zhenyun, Baker, Robert M.L., Stephenson, Gary V. and Wen, Hao
(2009)
Signal photon flux and background noise in a coupling electromagnetic detecting system for high-frequency gravitational waves.
Physical Review D, 80 (6), .
(doi:10.1103/PhysRevD.80.064013).
Abstract
A coupling system among Gaussian-type microwave photon flux, a 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 the pure inverse Gertsenshtein effect (G effect) caused by the HFGWs in the gigahertz band, the electromagnetic (EM) detecting scheme proposed by China and the U.S. HFGW groups is based on the composite effect of the synchroresonance effect and the inverse G effect. The key parameter in the scheme is the 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 ~103-105 seconds for the typical laboratory condition and parameters of hrms ~ 10-26-10-30/?Hz at 5 GHz with bandwidth ~1 Hz. 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
This record has no associated files available for download.
More information
Published date: 9 September 2009
Organisations:
Human Sciences Group
Identifiers
Local EPrints ID: 79194
URI: http://eprints.soton.ac.uk/id/eprint/79194
ISSN: 1550-7998
PURE UUID: 7b8919b0-0424-4631-8217-fb3e0b8c273b
Catalogue record
Date deposited: 15 Mar 2010
Last modified: 14 Mar 2024 00:28
Export record
Altmetrics
Contributors
Author:
Fangyu Li
Author:
Nan Yang
Author:
Zhenyun Fang
Author:
Robert M.L. Baker
Author:
Gary V. Stephenson
Author:
Hao Wen
Download statistics
Downloads from ePrints over the past year. Other digital versions may also be available to download e.g. from the publisher's website.
View more statistics