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), 2015. Published by Science Publishing Group |
Cooling Time, Inverse-Compton Scattering, Neutron Star, Pulsar, Pulsar Wind Nebula
[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]. |
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
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
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
@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} }
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 -