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		<id>https://wiki.tachyony.co.uk/w/index.php?title=Auger_effect&amp;diff=13494</id>
		<title>Auger effect</title>
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		<summary type="html">&lt;p&gt;35.2.65.22: &lt;/p&gt;
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&lt;div&gt;{{short description|Physical phenomenon}}&lt;br /&gt;
[[File:Auger Process.svg|thumb|340px|Two views of the Auger process. (a) illustrates sequentially the steps involved in Auger deexcitation. An incident electron (or photon) creates a core hole in the 1s level. An electron from the 2s level fills in the 1s hole, and the transition energy is imparted to a 2p electron, which is emitted. The final atomic state thus has two holes, one in the 2s orbital and the other in the 2p orbital. (b) illustrates the same process using [[X-ray notation]], KL&amp;lt;sub alt=&amp;quot;KL_1L_{2,3}&amp;quot;&amp;gt;1&amp;lt;/sub&amp;gt;L&amp;lt;sub&amp;gt;2,3&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
The &#039;&#039;&#039;Auger effect&#039;&#039;&#039; ({{IPAc-en|oʊ|ˈ|ʒ|eɪ}}; {{IPA|fr|ˈ/o.ʒe/}}) or &#039;&#039;&#039;Meitner-Auger effect&#039;&#039;&#039; is a physical phenomenon in which [[atom]]s eject [[electrons]]. It occurs when an [[inner-shell electrons|inner-shell]] vacancy in an [[atom]] is filled by an electron, releasing energy that causes the emission of another electron from a different shell of the same atom.&amp;lt;ref&amp;gt;{{GoldBookRef|title=Auger effect|file=A00520}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
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When a [[core electron]] is removed, leaving a vacancy, an electron from a higher energy level may fall into the vacancy, resulting in a release of [[energy]]. For light atoms (Z&amp;lt;12), this energy is most often transferred to a valence electron which is subsequently ejected from the atom.&amp;lt;ref name=&amp;quot;Photoabsorption&amp;quot;&amp;gt;{{cite book |last1=Berkowitz |title=Photoabsorption, Photoionization, and Photoelectron Spectroscopy |publisher=Academic Press |isbn=978-0-12-091650-4 |page=156 |doi=10.1016/B978-0-12-091650-4.50011-6 }}&amp;lt;/ref&amp;gt; This second ejected electron is called an &#039;&#039;&#039;Auger electron&#039;&#039;&#039;.&amp;lt;ref&amp;gt;{{GoldBookRef|title=Auger electron|file=A00521}}&amp;lt;/ref&amp;gt; For heavier atomic nuclei, the release of the energy in the form of an emitted [[photon]] becomes gradually more probable.&lt;br /&gt;
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==Effect==&lt;br /&gt;
Upon ejection, the [[kinetic energy]] of the Auger electron corresponds to the difference between the energy of the initial [[electronic transition]] into the vacancy and the [[ionization energy]] for the [[electron shell]] from which the Auger electron was ejected. These energy levels depend on the type of atom and the chemical environment in which the atom was located.&lt;br /&gt;
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[[Auger electron spectroscopy]] involves the emission of Auger electrons by bombarding a sample with either [[X-ray]]s or energetic electrons and measures the intensity of Auger electrons that result as a function of the Auger electron energy. The resulting spectra can be used to determine the identity of the emitting atoms and some information about their environment.&lt;br /&gt;
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[[Carrier generation and recombination#Auger recombination|Auger recombination]] is a similar Auger effect which occurs in [[semiconductor]]s. An electron and [[electron hole]] (electron-hole pair) can recombine, giving up their energy to an electron in the [[conduction band]], increasing its energy. The reverse effect is known as [[impact ionization]].&lt;br /&gt;
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The Auger effect can impact biological molecules such as DNA. Following the K-shell ionization of the component atoms of DNA, Auger electrons are ejected, leading to damage to its sugar-phosphate backbone.&amp;lt;ref&amp;gt;{{Cite journal| doi = 10.1080/09553002.2017.1312670| issn = 0955-3002| volume = 93| issue = 8| pages = 743–756| last1 = Yokoya| first1 = Akinari| last2 = Ito| first2 = Takashi| title = Photon-induced Auger effect in biological systems: a review| journal = International Journal of Radiation Biology| date = 2017-08-03| pmid = 28397587}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
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==Discovery==&lt;br /&gt;
The Auger emission process was observed and published in 1922 by [[Lise Meitner]],&amp;lt;ref&amp;gt;{{cite journal|doi=10.1007/BF01326962|author=L. Meitner|title=Über die Entstehung der β-Strahl-Spektren radioaktiver Substanzen|journal=Z. Phys. |volume=9|issue=1|year=1922|pages=131–144|bibcode= 1922ZPhy....9..131M|s2cid=121637546}}&amp;lt;/ref&amp;gt; an Austrian-Swedish physicist, as a side effect in her competitive search for the nuclear beta electrons with the British physicist [[Charles Drummond Ellis]].&lt;br /&gt;
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The French physicist [[Pierre Victor Auger]] independently discovered it in 1923&amp;lt;ref&amp;gt;P. Auger: [http://gallica.bnf.fr/ark:/12148/bpt6k3130n.image.f187.langFR Sur les rayons β secondaires produits dans un gaz par des rayons X], C.R.A.S. 177 (1923) 169–171.&amp;lt;/ref&amp;gt; upon analysis of a Wilson [[cloud chamber]] experiment and it became the central part of his PhD work.&amp;lt;ref&amp;gt;{{cite journal|doi=10.3139/146.110163|title=Pierre Auger – Lise Meitner: Comparative contributions to the Auger effect|year=2009|last1=Duparc|first1=Olivier Hardouin|journal=International Journal of Materials Research |volume=100|issue=9|pages=1162–1166|bibcode=2009IJMR..100.1162H |s2cid=229164774 }}&amp;lt;/ref&amp;gt; High-energy X-rays were applied to ionize gas particles and observe [[photoelectric]] electrons. The observation of electron tracks that were independent of the frequency of the incident photon suggested a mechanism for electron ionization that was caused by an internal conversion of energy from a radiationless transition. Further investigation and theoretical work using elementary quantum mechanics and transition rate/transition probability calculations showed that the effect was a radiationless effect more than an internal conversion effect.&amp;lt;ref&amp;gt;{{Cite book |last=Burhop |first=E. H. S |url=https://archive.org/details/augereffectother0000ehsb/mode/2up |title=The Auger effect and other radiationless transitions (Cambridge monographs on physics) |date=1952-01-01 |publisher=University Press}}&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;{{Cite book |last=Chattarji |first=Dipankar |url=https://archive.org/details/theoryofaugertra0000chat |title=The theory of auger transitions |date=1976 |publisher=London; New York: Academic Press |isbn=978-0-12-169850-8}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
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==See also==&lt;br /&gt;
*[[Auger therapy]]&lt;br /&gt;
*[[Carrier generation and recombination|Charge carrier generation and recombination]]&lt;br /&gt;
*[[Characteristic X-ray]]&lt;br /&gt;
*[[Coster–Kronig transition]]&lt;br /&gt;
*[[Electron capture]]&lt;br /&gt;
*[[Radiative Auger effect]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{Reflist|30em}}&lt;br /&gt;
&lt;br /&gt;
{{X-ray science}}{{Electron microscopy}}&lt;br /&gt;
{{Authority control}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Atomic physics]]&lt;br /&gt;
[[Category:Foundational quantum physics]]&lt;br /&gt;
[[Category:Electron spectroscopy]]&lt;/div&gt;</summary>
		<author><name>35.2.65.22</name></author>
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