Very-high-energy gamma ray
Very-high-energy gamma ray (VHEGR) denotes gamma radiation with photon energies of 100 GeV to 100 TeV, i.e., 1011 to 1014 electronvolts.[1] This is approximately equal to wavelengths between 1.24 × 10-17 and 1.24 × 10-20 meters, or frequencies of 2.42 × 1025 to 2.42 × 1028 Hz. Such energy levels have been detected from emissions from astronomical sources such as some binary star systems containing a compact object.[1] For example, radiation emitted from Cygnus X-3 has been measured at exaelectronvolt-levels.[1] Other astronomical sources include BL Lacertae,[2] 3C 66A[3] Markarian 421 and Markarian 501.[4] Markarian 501 has so far produced the highest measured energy for a gamma ray, of 16 TeV.[5] Various other sources exist that are not associated with known bodies. For example, the H.E.S.S. catalog contains 64 sources in November 2011.[6]
Detection
Instruments to detect this radiation commonly measure the Cherenkov radiation produced by secondary particles generated from an energetic photon entering the Earth's atmosphere.[3] This method is called imaging atmospheric Cherenkov technique or IACT. A high-energy photon produces a cone of light confined to 1° of the original photon direction. About 10,000 m2 of the earth's surface is lit by each cone of light. A flux of 10-7 photons per square meter per second can be detected with current technology, provided the energy is above 0.1 TeV.[3] Instruments include the planned Cherenkov Telescope Array, GT-48 in Crimea, MAGIC on La Palma, High Energy Stereoscopic System (HESS) in Namibia[7] VERITAS[5] and Chicago Air Shower Array which closed in 2001. Cosmic rays also produce similar flashes of light, but can be distinguished based on the shape of the light flash. Also having more than one telescope simultaneously observing the same spot can help exclude cosmic rays.[8] Extensive air showers of particles can be detected for gamma rays above 100 TeV. Water scintillation detectors or dense arrays of particle detectors can be used to detect these particle showers.[8]
Air showers of elementary particles made by gamma rays can also be distinguished from those produced by cosmic rays by the much greater depth of shower maximum, and the much lower quantity of muons.[5]
Very-high-energy gamma rays are too low energy to show the Landau–Pomeranchuk–Migdal effect. Only magnetic field perpendicular to the path of the photon causes pair production, so that photons coming in parallel to the geomagnetic field lines can survive intact till they meet the atmosphere. These photons that come through the magnetic window can make a Landau–Pomeranchuk–Migdal shower.[9]
| energy | energy | energy | frequency | wavelength | comparison | properties |
|---|---|---|---|---|---|---|
| eV | eV | Joules | Hertz | meters | in real world | |
| 1 | 1 | 0.1602 aJ | 241.8 THz | 1.2398 μm | near infrared photon | for comparison |
| 100 GeV | 1 × 1011 | 0.01602 μJ | 2.42 × 1025 Hz | 1.2 × 10-17 m | Z boson | |
| 1 TeV | 1 × 1012 | 0.1602 μJ | 2.42 × 1026 Hz | 1.2 × 10-18 m | flying mosquito | produces Cherenkov light |
| 10 TeV | 1 × 1013 | 1.602 μJ | 2.42 × 1027 Hz | 1.2 × 10-19 m | air shower reaches ground 16 TeV highest energy detected | |
| 100 TeV | 1 × 1014 | 0.01602 mJ | 2.42 × 1028 Hz | 1.2 × 10-20 m | ping pong ball falling off a bat | causes nitrogen to fluoresce |
| 1 PeV | 1 × 1015 | 0.1602 mJ | 2.42 × 1029 Hz | 1.2 × 10-21 m | ||
| 10 PeV | 1 × 1016 | 1.602 mJ | 2.42 × 1030 Hz | 1.2 × 10-22 m | potential energy of golf ball on a tee | |
| 100 PeV | 1 × 1017 | 0.01602 J | 2.42 × 1031 Hz | 1.2 × 10-23 m | penetrate geomagnetic field | |
| 1 EeV | 1 × 1018 | 0.1602 J | 2.42 × 1032 Hz | 1.2 × 10-24 m | ||
| 10 EeV | 1 × 1019 | 1.602 J | 2.42 × 1033 Hz | 1.2 × 10-25 m | air rifle shot | |
Importance
Very-high-energy gamma rays are of importance because they may reveal the source of cosmic rays. They travel in a straight line from their source to an observer. This is unlike cosmic rays which have their direction of travel scrambled by magnetic fields. Sources that produce cosmic rays will almost certainly produce gamma rays as well, as the cosmic ray particles interact with nuclei or electrons to produce photons or neutral pions which in turn decay to ultra-high-energy photons.[8]
The ratio of primary cosmic ray hadrons to gamma rays also gives a clue as to the origin of cosmic rays. Although gamma rays could be produced near the source of cosmic rays, they could also be produced by interaction with cosmic microwave background by way of the Greisen–Zatsepin–Kuzmin limit cutoff above 50 EeV.[9]
References
- 1 2 3 Ikhsanov, N. R. (October 1991), "Particle acceleration and main parameters of ultra-high energy gamma-ray binaries", Astrophysics and Space Science, 184, no. 2: 297–311., Bibcode:1991Ap&SS.184..297I, doi:10.1007/BF00642978, ISSN 0004-640X
- ↑ Neshpor, Yu I.; N. N. Chalenko; A. A. Stepanian; O. R. Kalekin; N. A. Jogolev; V. P. Fomin; V. G. Shitov. "BL Lac: A new ultrahigh-energy gamma-ray source". Astronomy Reports (Springer) 45 (4): 249–254. arXiv:astro-ph/0111448. Bibcode:2001ARep...45..249N. doi:10.1134/1.1361316.
- 1 2 3 Neshpor, Yu I.; A. A. Stepanyan; O. P. Kalekin; V. P. Fomin; N. N. Chalenko; V. G. Shitov (March 1998). "Blazar 3C 66A: Another extragalactic source of ultra-high-energy gamma-ray photons". Astronomy Letters 24 (2): 134–138. Bibcode:1998AstL...24..134N.
- ↑ "Astrophysics with H.E.S.S.". Retrieved 26 November 2011.
- 1 2 3 Dar, Arnon (4 June 2009). "High Energy Phenomena In The Universe" (PDF). 44th Rencontre De Moriond on High Energy Phenomena In The Universe. pp. 3–4. Retrieved 3 December 2011.
- ↑ "The H.E.S.S. Source Catalog". H.E.S.S. Collaboration. 2011. Retrieved 26 November 2011.
- ↑ "High Energy Stereoscopic System". Retrieved 26 November 2011.
- 1 2 3 Aharonian, Felix (24 August 2010). "The Fascinating TeV Sky" (PDF). WSPC - Proceedings. Retrieved 27 November 2011.
- 1 2 Vankov, H. P.; Inoue2, N.; Shinozaki, K. (2 February 2008). "Ultra-High Energy Gamma Rays in Geomagnetic Field and Atmosphere" (PDF). Retrieved 3 December 2011.