Very-high-energy gamma ray


Very-high-energy gamma ray denotes gamma radiation with photon energies of 100 GeV to 100 TeV, i.e., 1011 to 1014 electronvolts. This is approximately equal to
wavelengths between 10−17 and 10−20 meters, or frequencies of 2 × 1025 to 2 × 1028 Hz. Such energy levels have been detected from emissions from astronomical sources such as some binary star systems containing a compact object. For example, radiation emitted from Cygnus X-3 has been measured at ranges from GeV to exaelectronvolt-levels. Other astronomical sources include BL Lacertae, 3C 66A Markarian 421 and Markarian 501. Various other sources exist that are not associated with known bodies. For example, the H.E.S.S. catalog contained 64 sources in November 2011.

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. 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. Instruments include the planned Cherenkov Telescope Array, GT-48 in Crimea, MAGIC on La Palma, High Energy Stereoscopic System in Namibia VERITAS 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. 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.
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.
Very-high-energy gamma rays are too low energy to show the Landau–Pomeranchuk–Migdal effect. Only magnetic fields perpendicular to the path of the photon causes pair production, so that photons coming in parallel to the geomagnetic field lines can survive intact until they meet the atmosphere. These photons that come through the magnetic window can make a Landau–Pomeranchuk–Migdal shower.

energyenergyenergyfrequencywavelengthcomparisonproperties
eVeVJoulesHertzmetersin real world
110.1602 aJ241.8 THz1.2398 μmnear infrared photonfor comparison
Very-high-energy gamma rays100 GeV1 × 10110.01602 μJ2.42 × 1025 Hz1.2 × 10−17 mZ boson
Very-high-energy gamma rays1 TeV1 × 10120.1602 μJ2.42 × 1026 Hz1.2 × 10−18 mflying mosquitoproduces Cherenkov light
Very-high-energy gamma rays10 TeV1 × 10131.602 μJ2.42 × 1027 Hz1.2 × 10−19 mair shower reaches ground
Very-high-energy gamma rays100 TeV1 × 10140.01602 mJ2.42 × 1028 Hz1.2 × 10−20 mping pong ball falling off a batcauses nitrogen to fluoresce
Ultra-high-energy gamma rays1 PeV1 × 10150.1602 mJ2.42 × 1029 Hz1.2 × 10−21 m
Ultra-high-energy gamma rays10 PeV1 × 10161.602 mJ2.42 × 1030 Hz1.2 × 10−22 mpotential energy of golf ball on a tee
Ultra-high-energy gamma rays100 PeV1 × 10170.01602 J2.42 × 1031 Hz1.2 × 10−23 mpenetrate geomagnetic field
Ultra-high-energy gamma rays1 EeV1 × 10180.1602 J2.42 × 1032 Hz1.2 × 10−24 m
Ultra-high-energy gamma rays10 EeV1 × 10191.602 J2.42 × 1033 Hz1.2 × 10−25 mair 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.
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 interactions with the cosmic microwave background by way of the Greisen–Zatsepin–Kuzmin limit cutoff above 50 EeV.