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Low Energy Galactic Center Gamma Rays from Low Mass X-Ray Binaries

Published online by Cambridge University Press:  23 September 2016

W. Kluźniak
Affiliation:
Department of Physics and Astrophysics Laboratory Columbia University, New York, N.Y. 10027
M. Ruderman
Affiliation:
Department of Physics and Astrophysics Laboratory Columbia University, New York, N.Y. 10027
J. Shaham
Affiliation:
Department of Physics and Astrophysics Laboratory Columbia University, New York, N.Y. 10027
M. Tavani
Affiliation:
Department of Physics and Astrophysics Laboratory Columbia University, New York, N.Y. 10027

Abstract

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The hard X-ray and low energy γ-ray emission from the galactic center region (GCR) has four components: a power-law continuum between 20/50 keV and 200/300 keV with a power-law photon index β in the range ~ 2.5 to ~ 3.1; a harder spectrum with β ~ 1.–1.5 between 200/300 keV and ~ 511 keV; a narrow electron-positron annihilation line at 511 keV, reported to disappear in less than < 1/2 yr, although the temporal variation is controversial; and an equally variable continuum emission between 511 keV and several MeV (“MeV bump”). All four have luminosities 1037–1038 erg s−1, if they are located 10 kpc away. We propose non-thermal processes in low mass X-ray binaries (LMXB's) concentrated in the galactic bulge as the direct source of the three continuum components of the emission, as well as of an escaping electron-positron e± wind whose positron annihilation relatively far from the star could be the source of the 511 keV line. We consider a model for energetic emission from LMXB's that reproduces the softer power-law component of the GCR continuum through synchrotron emission of relativistic electrons in the strongly non-uniform (dipolar) magnetic field of the neutron star. We also explain, with less confidence, the variable MeV bump as the result of interaction of harder γ-rays with the power-law photons. The harder power law might be due to Compton scattering of relativistic electrons or photons.

Type
The High - Energy View
Copyright
Copyright © Kluwer 1989 

References

[1] Riegler, G.R., Ling, J.C., Mahoney, W.A., Wheaton, W.A., and Jacobson, A.S. in Positron-Electron Pairs in Astrophysics , eds. Burns, M. L., Harding, A. K. and Ramaty, R., AIP Conference Proceedings No. 101 (New York: AIP), pp. 230236 (1983).Google Scholar
[2] Riegler, G.R., Ling, J.C., Mahoney, W.A., Wheaton, W.A., and Jacobson, A.S., Ap. J. (Letters) , 294, L13L15 (1985).CrossRefGoogle Scholar
[3] Riegler, G.R. et al., Ap. J. (Letters) , 248, L13L16 (1981).Google Scholar
[4] Leventhal, M., MacCallum, C.J., Huters, A.F., and Stang, P.D., Ap. J. (Letters) , 260, L1L5 (1982).Google Scholar
[5] Share, G.H., Kinzer, R.L., Kurfess, J.D., Messina, D.C., Purcell, W.R., Chupp, E.L., Forrest, D.J., and Reppin, C., Ap. J. , 326, 717732 (1988).Google Scholar
[6] Skinner, G. K. et al., Nature , 330, 544547 (1987) and this Symposium. Google Scholar
[7] Cook, W. R. et al., this Symposium. Google Scholar
[8] Lingenfelter, R. E. and Ramaty, R. in The Galactic Center , ed. Riegler, G. R. and Blandford, R. D., AIP Conference Proceedings No. 83 (New York: AIP), pp. 148159 (1982).Google Scholar
[9] Ruderman, M., Shaham, J., Tavani, M., and Eichler, D., 1987, “Late Evolution of Very Low Mass X-ray Binaries Sustained by Gamma-Rays from their Primaries”, Ap. J. , in press.Google Scholar
[10] Ruderman, M., in Proc. NATO ASI High Energy Phenomena around Collapsed Stars , ed. Pacini, F. (Norwell, Mass.: Reidel), p. 145– (1986).Google Scholar
[11] Gorham, P.W. et al., Ap. J. , 309, 114121 (1986).Google Scholar
[12] Lamb, R.C. in 13th Texas Symposium of Relativistic Astrophysics , ed. Ulmer, M. P. (Singapore: World Scientific), pp. 589594 (1987).Google Scholar
[13] Leventhal, M., MacCallum, C.J., and Stang, P.D., Ap. J. (Letters) , 225, L11L14 (1982).Google Scholar
[14] Maurer, G.S., Johnson, W.N., Kurfess, J.D., and Strickman, M.S., Ap. J. , 254, 271278 (1982).Google Scholar
[15] White, N.E. and Holt, S.S., Ap. J. , 257, 318337 (1982).CrossRefGoogle Scholar
[16] Levine, A.M. et al., Ap. J. Supp. , 54, 581– (1984).Google Scholar
[17] Knight, F.K., Johnson, W.N., Kurfess, J.D., and Strickman, M.S., Ap. J. , 290, 557567 (1985).Google Scholar
[18] White, N.E. and Mason, K.O., Sp. Sci. Rev. , 40, 167– (1985).CrossRefGoogle Scholar
[19] White, N.E., Stella, L. and Parmar, A.N., Ap. J. , 324, 363– (1987).Google Scholar