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| {{about|the nuclear process|the chemical process|Internal conversion (chemistry)}}
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| {{Complex|date=June 2013}}
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| '''Internal conversion''' is a [[radioactive decay]] process where an excited [[atomic nucleus|nucleus]] interacts [[electromagnetism|electromagnetically]] with an [[electron]] in one of the lower [[atomic orbital]]s, causing the electron to be emitted (ejected) from the atom.<ref name=Loveland>{{cite book|last=Loveland|first=Walter D.|title=Modern Nuclear Chemistry|year=2005|publisher=Wiley|isbn=0471115320|pages=232|url=http://books.google.co.uk/books?id=ZAHJkrJlwbYC&pg=PA233&dq=internal+conversion&hl=en&sa=X&ei=anDHUJ_bGu7s0gXS3YGQDA&redir_esc=y#v=onepage&q=internal%20conversion&f=false}}</ref> Thus, in an internal conversion process, a high-energy electron is emitted from the radioactive atom, but not from a nucleon in the nucleus. Instead, the electron is ejected as a result of an interaction between the entire nucleus and an outside electron that interacts with it. For this reason, the high-speed electrons from internal conversion are not [[beta particle]]s, since the latter come from [[beta decay]], where they are newly created in the process. Since no beta decay takes place during internal conversion, the element atomic number does not change, and thus (as is the case with [[gamma decay]]) no transmutation of one element to another is seen. However, since an electron is lost, an otherwise neutral atom becomes [[ionization|ionized]]. Also, no neutrino is emitted during internal conversion.
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| Internally converted electrons do not have the characteristic energetically spread spectrum of beta particles, which results from varying amounts of decay energy being carried off by the neutrino (or antineutrino) in beta decay. Internally converted electrons, which carry a fixed fraction of the characteristic decay energy, have a well-specified discrete energy. The energy spectrum of a beta particle is thus a broad hump, extending to a maximum decay energy value, while the spectrum of internally converted electrons has a sharp peak.
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| ==Mechanism==
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| In the internal conversion process, the [[wavefunction]] of an inner shell electron penetrates the nucleus (i.e., there is a finite probability of the electron in an '''s''' [[atomic orbital]] being found in the nucleus) and when this occurs, the electron may couple to the excited state of the nucleus and take the energy of the nuclear transition directly, without an intermediate gamma ray being first produced.
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| The process of imparting energy from the nucleus to an orbital electron is a quantum process and may be seen as taking place by means of a [[virtual photon]]. In that sense the photon involved can be considered as a "virtual gamma ray", which appears as a feature in an equation that describes the process, rather than as a directly measurable emission. The kinetic energy of the emitted electron is equal to the transition energy in the nucleus, minus the binding energy of the electron.
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| Most internal conversion (IC) electrons come from the K [[electron shell|shell]] (the 1s state), as these two electrons have the highest probability of being found inside the nucleus. However, the s state in the L, M, and N shells (i.e., the 2s, 3s, and 4s states) are also able to couple to nuclear fields and cause IC electron ejections from these shells (called LMN internal conversion). Ratios of K-shell to other L, M, or N shell internal conversion probabilities for various nuclides have been prepared.<ref>[http://www.nucleide.org/DDEP_WG/introduction.pdf] Internal conversion branch tables]</ref>
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| Since the atomic [[binding energy]] of the s electron must be supplied in order to eject it from the atom in the internal conversion process, K shell internal conversion cannot happen if the decay energy of the atom is insufficient to overcome K-shell binding energy. There are a few radionuclides in which the decay energy is not sufficient to convert (eject) a 1s (K) electron, and these nuclides, when they decay by internal conversion, must decay exclusively from the L, M, or N shells (i.e., by ejecting 2s, 3s, or 4s electrons).
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| After the IC electron has been emitted, the atom is left with a vacancy in one of its electron shells, usually an inner one. This hole will be filled with an electron from one of the higher shells, and consequently one or more [[characteristic X-ray]]s or [[Auger electron]]s will be emitted as the remaining electrons in the atom cascade down to fill the vacancy.
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| ==When the process is expected==
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| Internal conversion is favoured when the energy gap between nuclear levels is small, and is also the primary mode of de-excitation for 0<sup>+</sup>→0<sup>+</sup> (i.e. E0) transitions. These occur where an excited nucleus has zero spin. Thus, it is unable to rid itself of energy by gamma emission, but it also has insufficient decay energy to decay by [[internal pair creation]].<ref>[http://www.wiley-vch.de/books/info/0-471-35633-6/toi99/www/struct/e0.pdf] E0 rules</ref> Internal conversion is also the predominant mode of de-excitation whenever the initial and final [[Spin (physics)|spin]] states are the same (but with other different quantum numbers); however the [[multi-polarity rules]] for non-zero initial and final spin states do not necessarily forbid the competing de-excitation by emission of a gamma ray in such cases.
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| The tendency towards internal conversion can be expressed by the [[internal conversion coefficient]], which is empirically determined by the ratio of de-excitations that go by the emission of electrons to those that go by gamma emission.
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| The internal conversion process competes with [[gamma decay]]. This competition is quantified in the form of the internal conversion coefficient which is defined as <math>\alpha = e/{\gamma}</math> where <math>e</math> is the rate of conversion electrons and <math>\gamma</math> is the rate of gamma-ray emission observed from a decaying nucleus. For example, in the decay of an excited state of the nucleus of [[Iodine-125|<sup>125</sup>I]], 7% of the decays emit energy as a gamma ray, while 93% release energy as conversion electrons. Therefore, this excited state of {{chem|125|I}} has an internal conversion coefficient of <math>\alpha = 13.3</math>. Internal conversion coefficients are observed to increase for increasing [[atomic number]] (Z) and decreasing gamma-ray energy. As one example, IC coefficients are calculated explicitly for {{chem|link=iron-55|55|Fe}}, {{chem|link=Isotopes of gallium|67|Ga}}, [[Technetium-99m|<sup>99m</sup>Tc]], {{chem|link=Isotopes of indium|111|In}}, <sup>113m</sup>In, <sup>115m</sup>In, {{chem|123|I}}, {{chem|125|I}}, [[Isotopes of platinum|<sup>193m</sup>Pt]], {{chem|link=Isotopes of thallium|201|Tl}} and {{chem|link=Isotopes of lead|203|Pb}} by Howell (1992) using [[Monte Carlo method]]s. (For {{chem|55|Fe}} the IC coefficient is zero.)
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| The energy of the emitted gamma ray is regarded as a precise measure of the difference in energy between the excited states of the decaying nucleus. However, this is not true in the case of conversion electrons. The energy of a conversion electron is given as <math>E = (E_i - E_f)-E_B</math>, where <math>E_i</math> and <math>E_f</math> are the energies of the nucleus in its initial and final states, respectively, while <math>E_B</math> is the binding energy of the electron.
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| ==Similar processes==
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| This internal conversion process is also not to be confused with the similar [[photoelectric effect]], which also may occur with electron emissions associated with [[gamma radiation]], in which an incident gamma photon emitted from a nucleus interacts with an electron, expelling the electron from the atom. Thus, gamma [[photoelectric effect|photoelectric-effect]] electron emission may ''also'' cause high-speed electrons to be emitted from radioactive atoms without [[beta decay]]. However, in internal conversion, the nucleus does not first emit an intermediate real [[gamma ray]], and therefore need not change [[angular momentum]] or electric moment.
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| Also, electrons from the gamma photoelectric effect show a spread in energy, depending on how much energy has been imparted to the ejected electron by the gamma ray that interacts with it—an amount that is variable depending on the angle of gamma photon [[Compton scattering|scattering from the electron]]. Further, a gamma ray is still emitted in photoelectric processes, but one that possesses a fraction of the energy compared to the gamma ray that left the nucleus. By contrast, in internal conversion, no gamma ray is emitted at all, and the electron energy is fixed at a single, typical value. | |
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| [[Auger electron]]s, which may also be produced after an internal conversion, arise from a mechanism that is different from that of internal conversion, but is analogous to it. Internal conversion electrons arise when an intense electric dipole field inside the nucleus accelerates an electron that has penetrated the nucleus and removes it from the atom. Auger electrons similarly arise when an electric field is produced within an atom's [[electron cloud]] due to loss of another electron, and this field again induces the acceleration and removal of yet another of the atom's [[atomic orbital]] electrons. Like IC electrons, Auger electrons also emerge in a sharp energy peak.
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| The [[electron capture]] process also involves an inner shell electron, which in this case is retained in the nucleus (changing the atomic number) and leaving the atom (not the nucleus) in an excited state. The atom can relax by [[X-ray]] emission and/or by Auger electron emission. Unstable nuclei can usually decay through both internal conversion and electron capture processes.
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| ==See also==
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| *[[Internal conversion coefficient]]
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| ==References==
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| {{cite book | last=Krane | first=Kenneth S. | title=Introductory Nuclear Physics | year=1988| publisher= J. Wiley & Sons | isbn=0-471-80553-X}}
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| {{cite book | last=L'Annunziata | first=Michael F. et al. | title=Handbook of Radioactivity Analysis | year=2003| publisher= Academic Press | isbn = 0-12-436603-1}}
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| R.W.Howell, Radiation spectra for Auger-electron emitting radionuclides: Report No. 2 of AAPM Nuclear Medicine Task Group No. 6, 1992, ''Medical Physics'' 19(6), 1371–1383
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| == External links ==
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| * [http://hyperphysics.phy-astr.gsu.edu/hbase/nuclear/radact2.html#c5 HyperPhysics]
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| {{Nuclear_processes}}
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| == References ==
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| {{reflist}}
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| [[Category:Radioactivity]]
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| [[Category:Nuclear physics]]
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