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A Method to Estimate the Cooling Time of Ultra-Relativistic Electrons in Pulsar Wind Nebulae

Received: 24 February 2015    Accepted: 1 May 2015    Published: 27 May 2015
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Abstract

Pulsar is a highly magnetized rotating neutron star. It continuously emits a wind of relativistic electrons and positrons. This wind creates an electron-positron-cloud around the pulsar. This cloud, which is full of relativistic electrons and positrons, is called a Pulsar Wind Nebula (PWN). As of 2014, 33 Pulsar Wind Nebulae (PWNe) have been detected in the TeV energy band. Current understanding is, these TeV photons are produced from up-scattering low-energy photons to high-energies by ultra-relativistic electrons and positrons in PWNe, which is a non-thermal process. This process is known as inverse-Compton scattering. During inverse-Compton scattering, ultra-relativistic electrons lose their energy and cool-down to low-energies. The average time that an ultra-relativistic electron takes to cool-down by inverse-Compton scattering is called the cooling time. Estimation of cooling time is important to understand how the luminosity of a PWN changes with time. This paper describes a statistical method developed for estimating the cooling time of ultra-relativistic electrons in a given PWN. This new method is a model independent technique. Cooling time was estimated as a function of two parameters: k and γ. Here k is the high-energy electron fraction in PWN at a given time and γ is the Average Bulk Lorentz Factor of electrons in the PWN. The estimated cooling time is proportional to k and inversely proportional to γ. The developed method was applied to four PWNe: MSH 15-52, HESS J1420-607, HESS J1825-137 and HESS J1837-069. The estimated cooling times vary between 1.56 kyr to 1000 kyr for MSH 15-52, 13 kyr to 8000 kyr for HESS J1420-607, 21.4 kyr to 10000 kyr for HESS J1825-137 and 22.7 kyr to 15000 kyr for HESS J1837-069.

Published in American Journal of Astronomy and Astrophysics (Volume 3, Issue 3)
DOI 10.11648/j.ajaa.20150303.16
Page(s) 63-69
Creative Commons

This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2024. Published by Science Publishing Group

Keywords

Cooling Time, Inverse-Compton Scattering, Neutron Star, Pulsar, Pulsar Wind Nebula

References
[1] Abeysekara, A. U. & Linnemann, J.T. (2015) Experimental Constraints on γ–ray Pulsar Gap Models and the Pulsar GeV to Pulsar Wind Nebula TeV Connection. ApJ. 804. p. 25.
[2] Aharonian, F., Akhperjanian, A. G., Aye, K.-M., et al. (2005) A&A. 435 (17).
[3] Aharonian, F., Akhperjanian, A. G., Bazer-Bachi, A. R., et al. (2006a) ApJ. 636. p. 777.
[4] Aharonian, F., Akhperjanian, A. G., Bazer-Bachi, A. R., et al. (2006b) A&A. 456. p. 245.
[5] Aharonian, F., Akhperjanian, A. G., Bazer-Bachi, A. R., et al. (2006c) A&A. 460. p. 365.
[6] Araudo, A. T., Bosch-Ramon, V. & Romero, G. E. (2009) High-energy emission from jet-clump interactions in microquasars. A&A. 503. p. 673-681.
[7] Baade, W. & Zwicky, F. (1934) On super-novae. Proc. Nat. Acad. Sci. 20. p. 254-259.
[8] Cocke, W. S., Disney, M. J. & Taylor, D. J. (1969) Nature. 221. p. 525-527.
[9] Gaensler, B. M. & Slane, P. O. (2006) ARA&A. 44. p. 17.
[10] Hester, J. Jeff (2008) The Crab Nebula: An Astrophysical Chimera. ARAA. 46 (1). p. 127–155.
[11] Hewish, A., Bell, S. J., Pilkington, J. D. H., Scott, P. F. & Collins, R. A. (1968) Observation of a rapidly pulsating radio source. Nature. 217. p. 709-713.
[12] Hobbs, M. (2014) An Introduction to Pulsars. [Online] Available from: http://www.atnf.csiro.au/outreach/education/everyone/pulsars/index.html [Accessed: 24th March 2014]
[13] Imagine (2014) IMAGINE THE UNIVERSE!. [Online] Available from: http://imagine.gsfc.nasa.gov/science/objects/pulsars2.html[Accessed: 25th March 2014]
[14] Mattana, F., Falanga, M., Gotz, D., et al. (2009) THE EVOLUTION OF THE γ - AND X-RAY LUMINOSITIES OF PULSAR WIND NEBULAE. ApJ. 694. P. 12-17.
[15] Mayer, M., Brucker, J., Holler, M., Jung, I., Valerius, K. &Stegmann, C. (2013) Predictimg the X-ray flux of evolved pulsar wind nebulae based on VHE γ ray observations. arXiv:1202.1455v3
[16] Minkowski, R. (1942) ApJ. 96. p.199-213.
[17] Oppenheimer, J. R. & Volkoff, G. (1939) On massive neutron cores. Phys. Rev. 55. p. 374-381.
[18] Pacini, F. (1967) Energy emission from a neutron star. Nature. 216. p. 567-568.
[19] Pacini, F. & Salvati, M. (1973) ApJ. 186 p. 249.
[20] Richards, D. W. & Comella, J. M. (1969) Nature. 222. p. 551-552.
[21] Rybicki, G. W. & Lightman, A.P. (1979) Radiative Processes in Astrophysics. (New York: Wiley)
[22] Staelin, D. H. & Refenstein, E. C. (1968) Science 162. p. 1481-1483.
[23] Stephenson, F. R. & Green, D. A. (2002) Historical Supernovae and Their Remnants. (Oxford: Clarendon Press)
[24] TeVCat (2014) Welcome to TeVCat!. [Online] Available from: http://tevcat.uchicago.edu/ [Accessed: 29th March 2014].
Cite This Article
  • APA Style

    K. L. I. Gunawardhana, K. P. S. C. Jayaratne, J. Adassuriya. (2015). A Method to Estimate the Cooling Time of Ultra-Relativistic Electrons in Pulsar Wind Nebulae. American Journal of Astronomy and Astrophysics, 3(3), 63-69. https://doi.org/10.11648/j.ajaa.20150303.16

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    ACS Style

    K. L. I. Gunawardhana; K. P. S. C. Jayaratne; J. Adassuriya. A Method to Estimate the Cooling Time of Ultra-Relativistic Electrons in Pulsar Wind Nebulae. Am. J. Astron. Astrophys. 2015, 3(3), 63-69. doi: 10.11648/j.ajaa.20150303.16

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    AMA Style

    K. L. I. Gunawardhana, K. P. S. C. Jayaratne, J. Adassuriya. A Method to Estimate the Cooling Time of Ultra-Relativistic Electrons in Pulsar Wind Nebulae. Am J Astron Astrophys. 2015;3(3):63-69. doi: 10.11648/j.ajaa.20150303.16

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  • @article{10.11648/j.ajaa.20150303.16,
      author = {K. L. I. Gunawardhana and K. P. S. C. Jayaratne and J. Adassuriya},
      title = {A Method to Estimate the Cooling Time of Ultra-Relativistic Electrons in Pulsar Wind Nebulae},
      journal = {American Journal of Astronomy and Astrophysics},
      volume = {3},
      number = {3},
      pages = {63-69},
      doi = {10.11648/j.ajaa.20150303.16},
      url = {https://doi.org/10.11648/j.ajaa.20150303.16},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajaa.20150303.16},
      abstract = {Pulsar is a highly magnetized rotating neutron star. It continuously emits a wind of relativistic electrons and positrons. This wind creates an electron-positron-cloud around the pulsar. This cloud, which is full of relativistic electrons and positrons, is called a Pulsar Wind Nebula (PWN). As of 2014, 33 Pulsar Wind Nebulae (PWNe) have been detected in the TeV energy band. Current understanding is, these TeV photons are produced from up-scattering low-energy photons to high-energies by ultra-relativistic electrons and positrons in PWNe, which is a non-thermal process. This process is known as inverse-Compton scattering. During inverse-Compton scattering, ultra-relativistic electrons lose their energy and cool-down to low-energies. The average time that an ultra-relativistic electron takes to cool-down by inverse-Compton scattering is called the cooling time. Estimation of cooling time is important to understand how the luminosity of a PWN changes with time. This paper describes a statistical method developed for estimating the cooling time of ultra-relativistic electrons in a given PWN. This new method is a model independent technique. Cooling time was estimated as a function of two parameters: k and γ. Here k is the high-energy electron fraction in PWN at a given time and γ is the Average Bulk Lorentz Factor of electrons in the PWN. The estimated cooling time is proportional to k and inversely proportional to γ. The developed method was applied to four PWNe: MSH 15-52, HESS J1420-607, HESS J1825-137 and HESS J1837-069. The estimated cooling times vary between 1.56 kyr to 1000 kyr for MSH 15-52, 13 kyr to 8000 kyr for HESS J1420-607, 21.4 kyr to 10000 kyr for HESS J1825-137 and 22.7 kyr to 15000 kyr for HESS J1837-069.},
     year = {2015}
    }
    

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  • TY  - JOUR
    T1  - A Method to Estimate the Cooling Time of Ultra-Relativistic Electrons in Pulsar Wind Nebulae
    AU  - K. L. I. Gunawardhana
    AU  - K. P. S. C. Jayaratne
    AU  - J. Adassuriya
    Y1  - 2015/05/27
    PY  - 2015
    N1  - https://doi.org/10.11648/j.ajaa.20150303.16
    DO  - 10.11648/j.ajaa.20150303.16
    T2  - American Journal of Astronomy and Astrophysics
    JF  - American Journal of Astronomy and Astrophysics
    JO  - American Journal of Astronomy and Astrophysics
    SP  - 63
    EP  - 69
    PB  - Science Publishing Group
    SN  - 2376-4686
    UR  - https://doi.org/10.11648/j.ajaa.20150303.16
    AB  - Pulsar is a highly magnetized rotating neutron star. It continuously emits a wind of relativistic electrons and positrons. This wind creates an electron-positron-cloud around the pulsar. This cloud, which is full of relativistic electrons and positrons, is called a Pulsar Wind Nebula (PWN). As of 2014, 33 Pulsar Wind Nebulae (PWNe) have been detected in the TeV energy band. Current understanding is, these TeV photons are produced from up-scattering low-energy photons to high-energies by ultra-relativistic electrons and positrons in PWNe, which is a non-thermal process. This process is known as inverse-Compton scattering. During inverse-Compton scattering, ultra-relativistic electrons lose their energy and cool-down to low-energies. The average time that an ultra-relativistic electron takes to cool-down by inverse-Compton scattering is called the cooling time. Estimation of cooling time is important to understand how the luminosity of a PWN changes with time. This paper describes a statistical method developed for estimating the cooling time of ultra-relativistic electrons in a given PWN. This new method is a model independent technique. Cooling time was estimated as a function of two parameters: k and γ. Here k is the high-energy electron fraction in PWN at a given time and γ is the Average Bulk Lorentz Factor of electrons in the PWN. The estimated cooling time is proportional to k and inversely proportional to γ. The developed method was applied to four PWNe: MSH 15-52, HESS J1420-607, HESS J1825-137 and HESS J1837-069. The estimated cooling times vary between 1.56 kyr to 1000 kyr for MSH 15-52, 13 kyr to 8000 kyr for HESS J1420-607, 21.4 kyr to 10000 kyr for HESS J1825-137 and 22.7 kyr to 15000 kyr for HESS J1837-069.
    VL  - 3
    IS  - 3
    ER  - 

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Author Information
  • Department of Physics, University of Colombo, Colombo-03, Sri Lanka

  • Department of Physics, University of Colombo, Colombo-03, Sri Lanka

  • Astronomy & Space Science Division, Arthur C Clarke Institute for Modern Technologies, Katubedda, Moratuwa, Sri Lanka

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