Upper limit map of a background of gravitational waves. Abbott, B., Drever, R. W. P., Savov, P., Siemens, X., Thorne, K. S., Vallisneri, M., Abbott, R., Adhikari, R. X., Agresti, J., Anderson, S. B., Araya, M., Armandula, H., Ballmer, S., Barish, B. C., Bhawal, B., Billingsley, G., Black, E., Blackburn, K., Bork, R., Boschi, V., Busby, D., Cardenas, L., Cepeda, C., Chatterji, S., Coyne, D., Creighton, T. D., D'Ambrosio, E., DeSalvo, R., Dupuis, R. J., Ehrens, P., Espinoza, E., Etzel, T., Evans, M., Fairhurst, S., Fazi, D., Goggin, L. M., Heefner, J., Ivanov, A., Kells, W., Keppel, D. G., King, P., Kondrashov, V., Kozak, D., Lazzarini, A., Lei, M., Libbrecht, K., Lindquist, P., Mageswaran, M., Mailand, K., Mandic, V., Maros, E., Marx, J. N., Meshkov, S., Messaritaki, E., Meyers, D., Miyakawa, O., Patel, P., Pedraza, M., Robertson, N. A., Russell, P., Samidi, M., Sannibale, V., Sears, B., Smith, M. R., Sutton, P. J., Tarallo, M., Taylor, R., Tyler, W., Varvella, M., Vass, S., Villar, A., Waldman, S. J., Wallace, L., Ward, R., Webber, D., Weinstein, A. J., Whitcomb, S. E., Willems, P. A., Yamamoto, H., Zhang, L., & Zweizig, J. Physical Review D, 76(8):art. No. 082003, American Physical Society, October, 2007. o̧pyright 2007 American Physical Society. Received 31 January 2007. Published 29 October 2007. Publisher error corrected 28 February 2008. The work described in this paper was part of the doctoral thesis of S.W. Ballmer at the Massachusetts Institute of Technology [10]. Furthermore the authors gratefully acknowledge the support of the U.S. National Science Foundation for the construction and operation of the LIGO Laboratory and the Particle Physics and Astronomy Research Council of the United Kingdom, the Max-Planck-Society, and the State of Niedersachsen, Germany, for support of the construction and operation of the GEO600 detector. The authors also gratefully acknowledge the support of the research by these agencies and by the Australian Research Council, the Natural Sciences and Engineering Research Council of Canada, the Council of Scientific and Industrial Research of India, the Department of Science and Technology of India, the Spanish Ministerio de Educacion y Ciencia, The National Aeronautics and Space Administration, the John Simon Guggenheim Foundation, the Alexander von Humboldt Foundation, the Leverhulme Trust, the David and Lucile Packard Foundation, the Research Corporation, and the Alfred P. Sloan Foundation. This paper has been assigned the LIGO document number LIGO-P060029-00-Z.Paper abstract bibtex We searched for an anisotropic background of gravitational waves using data from the LIGO S4 science run and a method that is optimized for point sources. This is appropriate if, for example, the gravitational wave background is dominated by a small number of distinct astrophysical sources. No signal was seen. Upper limit maps were produced assuming two different power laws for the source strain power spectrum. For an f\^ (?3) power law and using the50 Hz to 1.8 kHz band the upper limits on the source strain power spectrum vary between 1.2$\times$10\^ (?48) Hz\^ (?1) (100 Hz/f)\^ 3 and 1.2$\times$10\^ (?47) Hz\^ (?1) (100 Hz/f)\^ 3, depending on the position in the sky. Similarly, in the case of constant strain power spectrum, the upper limits vary between 8.5$\times$10?49 Hz?1 and 6.1$\times$10\^ (?48) Hz\^ (?1). As a side product a limit on an isotropic background of gravitational waves was also obtained. All limits are at the 90% confidence level. Finally, as an application, we focused on the direction of Sco-X1, the brightest low-mass x-ray binary. We compare the upper limit on strain amplitude obtained by this method to expectations based on the x-ray flux from Sco-X1.
@article{caltechauthors44548,
volume = {76},
number = {8},
month = {October},
author = {B. Abbott and R. W. P. Drever and P. Savov and X. Siemens and K. S. Thorne and M. Vallisneri and R. Abbott and Rana X. Adhikari and J. Agresti and S. B. Anderson and M. Araya and H. Armandula and S. Ballmer and B. C. Barish and B. Bhawal and G. Billingsley and E. Black and K. Blackburn and R. Bork and V. Boschi and D. Busby and L. Cardenas and C. Cepeda and S. Chatterji and D. Coyne and T. D. Creighton and E. D'Ambrosio and R. DeSalvo and R. J. Dupuis and P. Ehrens and E. Espinoza and T. Etzel and M. Evans and S. Fairhurst and D. Fazi and L. M. Goggin and J. Heefner and A. Ivanov and W. Kells and D. G. Keppel and P. King and V. Kondrashov and D. Kozak and A. Lazzarini and M. Lei and K. Libbrecht and P. Lindquist and M. Mageswaran and K. Mailand and V. Mandic and E. Maros and J. N. Marx and S. Meshkov and E. Messaritaki and D. Meyers and O. Miyakawa and P. Patel and M. Pedraza and N. A. Robertson and P. Russell and M. Samidi and V. Sannibale and B. Sears and M. R. Smith and P. J. Sutton and M. Tarallo and R. Taylor and W. Tyler and M. Varvella and S. Vass and A. Villar and S. J. Waldman and L. Wallace and R. Ward and D. Webber and A. J. Weinstein and S. E. Whitcomb and P. A. Willems and H. Yamamoto and L. Zhang and J. Zweizig},
note = {{\copyright} 2007 American Physical Society. Received 31 January 2007.
Published 29 October 2007. Publisher error corrected 28 February 2008. The work described in this paper was part of the doctoral
thesis of S.W. Ballmer at the Massachusetts Institute of
Technology [10]. Furthermore the authors gratefully acknowledge
the support of the U.S. National Science
Foundation for the construction and operation of the
LIGO Laboratory and the Particle Physics and
Astronomy Research Council of the United Kingdom, the
Max-Planck-Society, and the State of Niedersachsen,
Germany, for support of the construction and operation
of the GEO600 detector. The authors also gratefully acknowledge
the support of the research by these agencies
and by the Australian Research Council, the Natural
Sciences and Engineering Research Council of Canada,
the Council of Scientific and Industrial Research of India,
the Department of Science and Technology of India, the
Spanish Ministerio de Educacion y Ciencia, The National
Aeronautics and Space Administration, the John Simon
Guggenheim Foundation, the Alexander von Humboldt
Foundation, the Leverhulme Trust, the David and Lucile
Packard Foundation, the Research Corporation, and the
Alfred P. Sloan Foundation. This paper has been assigned
the LIGO document number LIGO-P060029-00-Z.},
title = {Upper limit map of a background of gravitational waves},
publisher = {American Physical Society},
year = {2007},
journal = {Physical Review D},
pages = {art. No. 082003},
url = {http://resolver.caltech.edu/CaltechAUTHORS:20140328-113831012},
abstract = {We searched for an anisotropic background of gravitational waves using data from the LIGO S4 science run and a method that is optimized for point sources. This is appropriate if, for example, the gravitational wave background is dominated by a small number of distinct astrophysical sources. No signal was seen. Upper limit maps were produced assuming two different power laws for the source strain power spectrum. For an f{\^{ }}(?3) power law and using the50 Hz to 1.8 kHz band the upper limits on the source strain power spectrum vary between 1.2{$\times$}10{\^{ }}(?48) Hz{\^{ }}(?1) (100 Hz/f){\^{ }}3 and 1.2{$\times$}10{\^{ }}(?47) Hz{\^{ }}(?1) (100 Hz/f){\^{ }}3, depending on the position in the sky. Similarly, in the case of constant strain power spectrum, the upper limits vary between 8.5{$\times$}10?49 Hz?1 and 6.1{$\times$}10{\^{ }}(?48) Hz{\^{ }}(?1). As a side product a limit on an isotropic background of gravitational waves was also obtained. All limits are at the 90\% confidence level. Finally, as an application, we focused on the direction of Sco-X1, the brightest low-mass x-ray binary. We compare the upper limit on strain amplitude obtained by this method to expectations based on the x-ray flux from Sco-X1.}
}
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2007 American Physical Society. Received 31 January 2007. Published 29 October 2007. Publisher error corrected 28 February 2008. The work described in this paper was part of the doctoral thesis of S.W. Ballmer at the Massachusetts Institute of Technology [10]. Furthermore the authors gratefully acknowledge the support of the U.S. National Science Foundation for the construction and operation of the LIGO Laboratory and the Particle Physics and Astronomy Research Council of the United Kingdom, the Max-Planck-Society, and the State of Niedersachsen, Germany, for support of the construction and operation of the GEO600 detector. The authors also gratefully acknowledge the support of the research by these agencies and by the Australian Research Council, the Natural Sciences and Engineering Research Council of Canada, the Council of Scientific and Industrial Research of India, the Department of Science and Technology of India, the Spanish Ministerio de Educacion y Ciencia, The National Aeronautics and Space Administration, the John Simon Guggenheim Foundation, the Alexander von Humboldt Foundation, the Leverhulme Trust, the David and Lucile Packard Foundation, the Research Corporation, and the Alfred P. Sloan Foundation. This paper has been assigned the LIGO document number LIGO-P060029-00-Z.","title":"Upper limit map of a background of gravitational waves","publisher":"American Physical Society","year":"2007","journal":"Physical Review D","pages":"art. No. 082003","url":"http://resolver.caltech.edu/CaltechAUTHORS:20140328-113831012","abstract":"We searched for an anisotropic background of gravitational waves using data from the LIGO S4 science run and a method that is optimized for point sources. This is appropriate if, for example, the gravitational wave background is dominated by a small number of distinct astrophysical sources. No signal was seen. Upper limit maps were produced assuming two different power laws for the source strain power spectrum. For an f\\^ (?3) power law and using the50 Hz to 1.8 kHz band the upper limits on the source strain power spectrum vary between 1.2$\\times$10\\^ (?48) Hz\\^ (?1) (100 Hz/f)\\^ 3 and 1.2$\\times$10\\^ (?47) Hz\\^ (?1) (100 Hz/f)\\^ 3, depending on the position in the sky. Similarly, in the case of constant strain power spectrum, the upper limits vary between 8.5$\\times$10?49 Hz?1 and 6.1$\\times$10\\^ (?48) Hz\\^ (?1). As a side product a limit on an isotropic background of gravitational waves was also obtained. All limits are at the 90% confidence level. Finally, as an application, we focused on the direction of Sco-X1, the brightest low-mass x-ray binary. We compare the upper limit on strain amplitude obtained by this method to expectations based on the x-ray flux from Sco-X1.","bibtex":"@article{caltechauthors44548,\n volume = {76},\n number = {8},\n month = {October},\n author = {B. Abbott and R. W. P. Drever and P. Savov and X. Siemens and K. S. Thorne and M. Vallisneri and R. Abbott and Rana X. Adhikari and J. Agresti and S. B. Anderson and M. Araya and H. Armandula and S. Ballmer and B. C. Barish and B. Bhawal and G. Billingsley and E. Black and K. Blackburn and R. Bork and V. Boschi and D. Busby and L. Cardenas and C. Cepeda and S. Chatterji and D. Coyne and T. D. Creighton and E. D'Ambrosio and R. DeSalvo and R. J. Dupuis and P. Ehrens and E. Espinoza and T. Etzel and M. Evans and S. Fairhurst and D. Fazi and L. M. Goggin and J. Heefner and A. Ivanov and W. Kells and D. G. Keppel and P. King and V. Kondrashov and D. Kozak and A. Lazzarini and M. Lei and K. Libbrecht and P. Lindquist and M. Mageswaran and K. Mailand and V. Mandic and E. Maros and J. N. Marx and S. Meshkov and E. Messaritaki and D. Meyers and O. Miyakawa and P. Patel and M. Pedraza and N. A. Robertson and P. Russell and M. Samidi and V. Sannibale and B. Sears and M. R. Smith and P. J. Sutton and M. Tarallo and R. Taylor and W. Tyler and M. Varvella and S. Vass and A. Villar and S. J. Waldman and L. Wallace and R. Ward and D. Webber and A. J. Weinstein and S. E. Whitcomb and P. A. Willems and H. Yamamoto and L. Zhang and J. Zweizig},\n note = {{\\copyright} 2007 American Physical Society. Received 31 January 2007. \r\nPublished 29 October 2007. Publisher error corrected 28 February 2008. The work described in this paper was part of the doctoral\r\nthesis of S.W. Ballmer at the Massachusetts Institute of\r\nTechnology [10]. Furthermore the authors gratefully acknowledge\r\nthe support of the U.S. National Science\r\nFoundation for the construction and operation of the\r\nLIGO Laboratory and the Particle Physics and\r\nAstronomy Research Council of the United Kingdom, the\r\nMax-Planck-Society, and the State of Niedersachsen,\r\nGermany, for support of the construction and operation\r\nof the GEO600 detector. The authors also gratefully acknowledge\r\nthe support of the research by these agencies\r\nand by the Australian Research Council, the Natural\r\nSciences and Engineering Research Council of Canada,\r\nthe Council of Scientific and Industrial Research of India,\r\nthe Department of Science and Technology of India, the\r\nSpanish Ministerio de Educacion y Ciencia, The National\r\nAeronautics and Space Administration, the John Simon\r\nGuggenheim Foundation, the Alexander von Humboldt\r\nFoundation, the Leverhulme Trust, the David and Lucile\r\nPackard Foundation, the Research Corporation, and the\r\nAlfred P. Sloan Foundation. This paper has been assigned\r\nthe LIGO document number LIGO-P060029-00-Z.},\n title = {Upper limit map of a background of gravitational waves},\n publisher = {American Physical Society},\n year = {2007},\n journal = {Physical Review D},\n pages = {art. No. 082003},\n url = {http://resolver.caltech.edu/CaltechAUTHORS:20140328-113831012},\n abstract = {We searched for an anisotropic background of gravitational waves using data from the LIGO S4 science run and a method that is optimized for point sources. This is appropriate if, for example, the gravitational wave background is dominated by a small number of distinct astrophysical sources. No signal was seen. Upper limit maps were produced assuming two different power laws for the source strain power spectrum. For an f{\\^{ }}(?3) power law and using the50 Hz to 1.8 kHz band the upper limits on the source strain power spectrum vary between 1.2{$\\times$}10{\\^{ }}(?48) Hz{\\^{ }}(?1) (100 Hz/f){\\^{ }}3 and 1.2{$\\times$}10{\\^{ }}(?47) Hz{\\^{ }}(?1) (100 Hz/f){\\^{ }}3, depending on the position in the sky. Similarly, in the case of constant strain power spectrum, the upper limits vary between 8.5{$\\times$}10?49 Hz?1 and 6.1{$\\times$}10{\\^{ }}(?48) Hz{\\^{ }}(?1). As a side product a limit on an isotropic background of gravitational waves was also obtained. All limits are at the 90\\% confidence level. Finally, as an application, we focused on the direction of Sco-X1, the brightest low-mass x-ray binary. We compare the upper limit on strain amplitude obtained by this method to expectations based on the x-ray flux from Sco-X1.}\n}\n\n","author_short":["Abbott, B.","Drever, R. W. P.","Savov, P.","Siemens, X.","Thorne, K. S.","Vallisneri, M.","Abbott, R.","Adhikari, R. X.","Agresti, J.","Anderson, S. B.","Araya, M.","Armandula, H.","Ballmer, S.","Barish, B. C.","Bhawal, B.","Billingsley, G.","Black, E.","Blackburn, K.","Bork, R.","Boschi, V.","Busby, D.","Cardenas, L.","Cepeda, C.","Chatterji, S.","Coyne, D.","Creighton, T. D.","D'Ambrosio, E.","DeSalvo, R.","Dupuis, R. J.","Ehrens, P.","Espinoza, E.","Etzel, T.","Evans, M.","Fairhurst, S.","Fazi, D.","Goggin, L. M.","Heefner, J.","Ivanov, A.","Kells, W.","Keppel, D. 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