# Gamma ray

Gamma ray

Gamma rays (denoted as &gamma;) are a form of electromagnetic radiation or light emission of frequencies produced by sub-atomic particle interactions, such as electron-positron annihilation or radioactive decay. Gamma rays are generally characterized as electromagnetic radiation having the highest frequency and energy, and also the shortest wavelength (below about 10 picometers), within the electromagnetic spectrum. Gamma rays consist of high energy photons with energies above about 100 keV. Gamma rays were discovered by Paul Villard, a French chemist and physicist, in 1900, while studying uranium.

Hard X-rays overlap the range of "long"-wavelength (lower energy) gamma rays. The distinction between the two terms, however, depends on the source of the radiation, not its wavelength; X-ray photons are generated by energetic electron processes, gamma rays by transitions within atomic nuclei.

Due to their high energy content, gamma rays can cause serious damage when absorbed by living cells.

Properties

hielding

Shielding gamma rays requires large amounts of mass. They are better absorbed by materials with high atomic numbers and high density. The higher the energy of the gamma rays, the thicker the shielding required. Materials for shielding gamma rays are typically measured by the thickness required to reduce the intensity of the gamma rays by one half (the half value layer or HVL). For example, gamma rays that require 1 cm (0.4 inches) of lead to reduce their intensity by 50% will also have their intensity reduced in half by 6 cm (2½ inches) of concrete or 9 cm (3½ inches) of packed soil.

Matter interaction

When a gamma ray passes through matter, the probability for absorption in a thin layer is proportional to the thickness of that layer. This leads to an exponential decrease of intensity with thickness. The exponential absorption holds only for a narrow beam of gamma rays. If a wide beam of gamma rays passes through a thick slab of concrete, the scattering from the sides reduces the absorption.

:$I\left(d\right) = I_0 cdot e ^\left\{-mu d\right\}.$

Here, μ = "n"σ is the absorption coefficient, measured in cm−1, "n" the number of atoms per cm3 in the material, σ the absorption cross section in cm2 and "d" the thickness of material in cm.

In passing through matter, gamma radiation ionizes via three main processes: the photoelectric effect, Compton scattering, and pair production.

* Photoelectric Effect: This describes the case in which a gamma photon interacts with and transfers its energy to an atomic electron, ejecting that electron from the atom. The kinetic energy of the resulting photoelectron is equal to the energy of the incident gamma photon minus the binding energy of the electron. The photoelectric effect is the dominant energy transfer mechanism for x-ray and gamma ray photons with energies below 50 keV (thousand electron volts), but it is much less important at higher energies.

* Compton Scattering: This is an interaction in which an incident gamma photon loses enough energy to an atomic electron to cause its ejection, with the remainder of the original photon's energy being emitted as a new, lower energy gamma photon with an emission direction different from that of the incident gamma photon. The probability of Compton scatter decreases with increasing photon energy. Compton scattering is thought to be the principal absorption mechanism for gamma rays in the intermediate energy range 100 keV to 10 MeV. Compton scattering is relatively independent of the atomic number of the absorbing material.

* Pair Production: By interaction with the electric field of a nucleus, the energy of the incident photon is converted into the mass of an electron-positron pair. Energy in excess of the equivalent rest mass of the two particles (1.02 MeV) appears as the kinetic energy of the pair and the recoil nucleus. At the end of the positron's range, it combines with a free electron. The entire mass of these two particles is then converted into two gamma photons of at least 0.51 MeV energy each (or higher according to the kinetic energy of the annihilated particles)

The secondary electrons (and/or positrons) produced in any of these three processes frequently have enough energy to produce much ionization themselves.

Light interaction

High-energy (from 80 to 500 GeV) gamma rays arriving from far far-distant quasars are used to estimate the extragalactic background light in the universe: The highest-energy rays interact more readily with the background light photons and thus their density may be estimated by analyzing the incoming gamma-ray spectrum. [cite journal|last=Bock|first=R. K. |coauthors=et al|date=2008-06-27|title=Very-High-Energy Gamma Rays from a Distant Quasar: How Transparent Is the Universe?|journal=Science|volume=320|issue=5884|pages=pp 1752–1754|issn=0036-8075|doi=10.1126/science.1157087]

Gamma ray production

Gamma rays are often produced alongside other forms of radiation such as alpha or beta. When a nucleus emits an SubatomicParticle|Alpha or SubatomicParticle|Beta particle, the daughter nucleus is sometimes left in an excited state. It can then jump down to a lower level by emitting a gamma ray in much the same way that an atomic electron can jump to a lower level by emitting visible light or ultraviolet radiation.

Gamma rays, x-rays, visible light, and radio waves are all forms of electromagnetic radiation. The only difference is the frequency and hence the energy of the photons. Gamma rays are the most energetic. An example of gamma ray production follows.

First SimpleNuclide|Link|Cobalt|60 decays to excited SimpleNuclide|Link|Nickel|60 by beta decay. Then the SimpleNuclide|Nickel|60 drops down to the ground state (see nuclear shell model) by emitting two gamma rays in succession (1.17 MeV then 1.33 MeV): :

Another example is the alpha decay of SimpleNuclide|Link|americium|241 to form SimpleNuclide|Link|neptunium|237; this alpha decay is accompanied by gamma emission. In some cases, the gamma emission spectrum for a nucleus (daughter nucleus) is quite simple, (eg SimpleNuclide|Cobalt|60/SimpleNuclide|Nickel|60) while in other cases, such as with (SimpleNuclide|americium|241/SimpleNuclide|neptunium|237 and SimpleNuclide|Link|iridium|192/SimpleNuclide|platinum|192), the gamma emission spectrum is complex, revealing that a series of nuclear energy levels can exist. The fact that an alpha spectrum can have a series of different peaks with different energies reinforces the idea that several nuclear energy levels are possible.
[
CGRO spacecraft. Bright spots within the galactic plane are pulsars while those above and below the plane are thought to be quasars.]

Because a beta decay is accompanied by the emission of a neutrino which also carries energy away, the beta spectrum does not have sharp lines, but instead is a broad peak. Hence from beta decay alone it is not possible to probe the different energy levels found in the nucleus.

In optical spectroscopy, it is well known that an entity which emits light can also absorb light at the same wavelength (photon energy). For instance, a sodium flame can emit yellow light as well as absorb the yellow light from a sodium vapor lamp. In the case of gamma rays, this can be seen in Mössbauer spectroscopy. Here, a correction for the energy lost by the recoil of the nucleus is made and the exact conditions for gamma ray absorption through resonance can be attained.

This is similar to the Franck Condon effects seen in optical spectroscopy.

Uses

[
Gamma-ray Image of a truck taken with a VACIS (Vehicle and Container Imaging System)] Because the wavelength of gamma radiation is so short, a single incident photon can impart significant damage to a living cell. This property means that gamma radiation is often used to kill living organisms, in a process called irradiation. Applications of this include sterilizing medical equipment (as an alternative to autoclaves or chemical means), removing decay-causing bacteria from many foodstuffs or preventing fruit and vegetables from sprouting to maintain freshness and flavor.

Due to their tissue penetrating property, gamma rays/X-rays have a wide variety of medical uses such as in CT Scans and radiation therapy ("see X-ray"). However, as a form of ionizing radiation they have the ability to effect molecular changes, giving them the potential to cause cancer when DNA is affected. The molecular changes can also be used to alter the properties of semi-precious stones, and is often used to change white topaz into blue topaz.

Despite their cancer-causing properties, gamma rays are also used to treat some types of cancer. In the procedure called gamma-knife surgery, multiple concentrated beams of gamma rays are directed on the growth in order to kill the cancerous cells. The beams are aimed from different angles to focus the radiation on the growth while minimizing damage to the surrounding tissues.Gamma rays are also used for diagnostic purposes in nuclear medicine. Several gamma-emitting radioisotopes are used, one of which is technetium-99m. When administered to a patient, a gamma camera can be used to form an image of the radioisotope's distribution by detecting the gamma radiation emitted. Such a technique can be employed to diagnose a wide range of conditions (e.g. spread of cancer to the bones).

In the US, gamma ray detectors are starting to be used as part of the Container Security Initiative (CSI). These US\$5 million machines are advertised to scan 30 containers per hour. The objective of this technique is to pre-screen merchant ship containers before they enter US ports.

Health effects

Gamma rays are the most dangerous form of radiation emitted by a nuclear explosion because of the difficulty in shielding them. This is because gamma rays have the shortest wavelength of all waves in the electromagnetic spectrum, and therefore have the greatest ability to penetrate through any gap, even a subatomic one, in what might otherwise be an effective shield.

Body response

After gamma-irradiation, and the breaking of DNA double-strands, a cell can repair the damaged genetic material to the limit of its capability Fact|date=October 2007. However, a study of Rothkamm and Lobrich has shown that the repairing process works well after high-dose exposure but is much slower in the case of a low-dose exposure. This could mean that a chronic low-dose exposure cannot be fought by the body Fact|date=October 2007. The probability of detecting small alterations or of a detectable defect occurring is most likely small enough that the cell would replicate before initiating a full repair Fact|date=October 2007. Some cells can not detect their own genetic defects Fact|date=October 2007.

Risk assessment

The natural outdoor exposure in Great Britain is in the range 20-40 nSv/h. [Department for Environment, Food and Rural Affairs (Defra) UK – Keys facts about radioactivity – 2003, http://www.defra.gov.uk/environment/statistics/radioact/kf/rakf03.htm ] Natural exposure to gamma rays is about 1 to 2 millisieverts per year, and the average total amount of radiation received in one year per inhabitant in the USA is 3.6 mSv. [United Nations Scientific Committee on the Effects of Atomic Radiation Annex E: Medical radiation exposures – Sources and Effects of Ionizing – 1993, p. 249, New York, UN]

By comparison, the radiation dose from chest radiography is a fraction of the annual naturally occurring background radiation dose, [US National Council on Radiation Protection and Measurements – NCRP Report No. 93 – pp 53-55, 1987. Bethesda, Maryland, USA, NCRP] and the dose from fluoroscopy of the stomach is, at most, 0.05 Sv on the skin of the back.

For acute full-body equivalent dose, 1 Sv causes slight blood changes, 2-5 Sv causes nausea, hair loss, hemorrhaging and will cause death in many cases. More than 3 Sv will lead to death in less than two months in more than 80 percent of cases, and much over 4 Sv usually causes death (see "Sievert").Clarifyme|date=March 2008Fact|date=November 2007 For low dose exposure, for example among nuclear workers, who receive an average radiation dose of 19 mSv, the risk of dying from cancer (excluding leukemia) increases by 2 percent. For a dose of 100 mSv, that risk increase is at 10 percent. By comparison, it was 32 percent for the Atom Bomb survivors. [IARC – Cancer risk following low doses of ionizing radiation - a 15 country study – http://www.iarc.fr/ENG/Units/RCAa1.html] .

* Nuclear fission/fusion
* Gamma spectroscopy
* Gamma-ray astronomy
* Gamma ray bursts
* High energy X-rays
* α (alpha) particles
* β (beta) particles
* Types of rays:
** γ (gamma) rays
** n (neutron) rays
** δ (delta) rays
** ε (epsilon) rays
*X-rays

References

* [http://www.gcsechemistry.com/pwav46.htm GCSE information]
* [http://www.astro.caltech.edu/~ejb/faq.html Gamma ray bursts]
* [http://nucleardata.nuclear.lu.se/NuclearData/toi/ The Lund/LBNL Nuclear Data Search] - Contains information on gamma-ray energies from isotopes.
* [http://grapevine.com.au/~pbeirwirth/gamma.html Mapping soils with airborne detectors]

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