{"id":26453,"date":"2020-02-15T17:13:34","date_gmt":"2020-02-15T17:13:34","guid":{"rendered":"http:\/\/sitepourvtc.com\/?page_id=26453"},"modified":"2023-06-28T17:57:20","modified_gmt":"2023-06-28T17:57:20","slug":"what-are-semiconductors-properties-of-semiconductors","status":"publish","type":"page","link":"https:\/\/sitepourvtc.com\/nuclear-engineering\/radiation-detection\/semiconductor-detectors\/what-are-semiconductors-properties-of-semiconductors\/","title":{"rendered":"What are Semiconductors &#8211; Properties of Semiconductors"},"content":{"rendered":"<div   id="8n9s8rpp6h"     class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights \"><div   id="8n9s8rpp6h"     class=\"inside-grid-column\">\n<figure id=\"attachment_26115\" aria-describedby=\"caption-attachment-26115\" style=\"width: 290px\" class=\"wp-caption alignright\"><a href=\"http:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/silicon-strip-detector-semiconductors.png\"><img loading=\"lazy\" class=\"size-medium wp-image-26115\" src=\"http:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/silicon-strip-detector-semiconductors-300x197.png\" alt=\"silicon strip detector - semiconductors\" width=\"300\" height=\"197\" srcset=\"https:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/silicon-strip-detector-semiconductors-300x197.png 300w, https:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/silicon-strip-detector-semiconductors.png 736w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/><\/a><figcaption id=\"caption-attachment-26115\" class=\"wp-caption-text\">Silicin Strip Detector Source: micronsemiconductor.co.uk<\/figcaption><\/figure>\n<p>In general, <strong>semiconductors<\/strong> are materials, inorganic or organic, which can control their conduction depending on chemical structure, temperature, illumination, and presence of dopants. The name <strong>semiconductor<\/strong> comes from the fact that these materials have <strong>electrical conductivity<\/strong> between a metal, like copper, gold, etc., and an insulator, like glass. They have an <strong>energy gap<\/strong> of less than 4eV (about 1eV). In solid-state physics, this energy gap or band gap is an energy range between the valence band and conduction band where electron states are forbidden. In contrast to conductors, electrons in a semiconductor must obtain energy (e.g., from ionizing radiation) to cross the band gap and reach the conduction band. <strong>Properties of semiconductors<\/strong> are determined by the energy gap between valence and conduction bands. To understand a semiconductor, we have to define these terms.<\/p>\n<h2>Properties of Semiconductors<\/h2>\n<p>To understand the difference between <strong>metals<\/strong>, <strong>semiconductors,<\/strong> and <strong>electrical insulators<\/strong>, we have to define the following terms from solid-state physics:<\/p>\n<ul>\n<li><strong><a href=\"http:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/Valence-Band-Conduction-Band-Band-Gap.png\"><img loading=\"lazy\" class=\"alignright wp-image-26111\" src=\"http:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/Valence-Band-Conduction-Band-Band-Gap.png\" alt=\"Valence Band - Conduction Band - Band Gap\" width=\"469\" height=\"324\" srcset=\"https:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/Valence-Band-Conduction-Band-Band-Gap.png 917w, https:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/Valence-Band-Conduction-Band-Band-Gap-300x207.png 300w, https:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/Valence-Band-Conduction-Band-Band-Gap-768x530.png 768w\" sizes=\"(max-width: 469px) 100vw, 469px\" \/><\/a>Valence Band<\/strong>. In solid-state physics, the <strong>valence band<\/strong> and <strong>conduction band<\/strong> are the bands closest to the <strong>Fermi level<\/strong> and thus determine the electrical conductivity of the solid. In electrical insulators and semiconductors, the valence band is the highest range of electron energies in which electrons are normally present at absolute zero temperature. For example, a <strong>silicon<\/strong> atom has fourteen electrons. In the ground state, they are arranged in the electron configuration <strong>[Ne]3s<sup>2<\/sup>3p<sup>2<\/sup><\/strong>. Of these, <strong>four are valence electrons<\/strong>, occupying the 3s orbital and two of the 3p orbitals. The distinction between the valence and conduction bands is meaningless in metals because conduction occurs in one or more partially filled bands that take on the properties of both the valence and conduction bands.<\/li>\n<li><strong>Conduction Band<\/strong>. In solid-state physics, the valence band and conduction band are the bands closest to the Fermi level and thus determine the electrical conductivity of the solid. The <strong>conduction band<\/strong> is the lowest range of <strong>vacant electronic states <\/strong>in electrical insulators and semiconductors. On a graph of the electronic band structure of a material, the valence band is located below the Fermi level, while the <strong>conduction band<\/strong> is above it. In semiconductors, <a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/atomic-nuclear-physics\/fundamental-particles\/what-is-electron-properties-of-electron\/\">electrons<\/a> may reach the conduction band when they are <strong>excited<\/strong>, for example, by <a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/atomic-nuclear-physics\/radiation\/ionizing-radiation\/\">ionizing radiation<\/a> (i.e., they must obtain energy higher than <strong>E<sub>gap<\/sub><\/strong>). For example, diamond is a wide-bandgap semiconductor (E<sub>gap\u00a0<\/sub>= 5.47 eV) with high potential as an electronic device material in many devices. On the other side, germanium has a small band gap energy (E<sub>gap<\/sub> = 0.67 eV), which requires operating the detector at cryogenic temperatures. The distinction between the valence and conduction bands is meaningless in metals because conduction occurs in one or more partially filled bands that take on the properties of both the valence and conduction bands.<\/li>\n<li><strong>Band Gap<\/strong>. In solid-state physics, the <strong>energy gap<\/strong> or the <strong>band gap<\/strong> is an energy range between the valence band and conduction band where electron states are forbidden. In contrast to conductors, electrons in a semiconductor must obtain energy (e.g., from ionizing radiation) to cross the band gap and reach the conduction band. <strong>Band gaps<\/strong> are naturally different for different materials. For example, diamond is a wide-bandgap semiconductor (E<sub>gap\u00a0<\/sub>= 5.47 eV) with high potential as an electronic device material in many devices. On the other side, germanium has a small band gap energy (E<sub>gap<\/sub> = 0.67 eV), which requires operating the detector at cryogenic temperatures.<\/li>\n<li><strong>Fermi Level<\/strong>. The term \u201cFermi level\u201d comes from <strong>Fermi-Dirac statistics<\/strong>, which describes a distribution of particles over energy states in systems consisting of fermions (electrons) that obey the <a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/atomic-nuclear-physics\/atomic-theory\/pauli-exclusion-principle\/\">Pauli exclusion principle<\/a>. Since they cannot exist in identical energy states, Fermi level is the term used to describe the top of the collection of <strong>electron energy levels<\/strong> at <a href=\"http:\/\/sitepourvtc.com\/nuclear-engineering\/thermodynamics\/thermodynamic-properties\/what-is-temperature-physics\/absolute-zero-temperature\/\">absolute zero temperature<\/a>. The <strong>Fermi level<\/strong> is the surface of the <strong>Fermi sea<\/strong> at absolute zero, where no electrons will have enough energy to rise above the surface. In metals, the Fermi level lies in the hypothetical conduction band giving rise to free conduction electrons. In semiconductors, the position of the Fermi level is within the band gap, approximately in the middle of the band gap.<\/li>\n<li><strong><a href=\"http:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/extrinsic-doped-semiconductor-p-type-acceptor.png\"><img loading=\"lazy\" class=\"alignright wp-image-26108\" src=\"http:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/extrinsic-doped-semiconductor-p-type-acceptor.png\" alt=\"extrinsic - doped semiconductor - p-type - acceptor\" width=\"569\" height=\"392\" srcset=\"https:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/extrinsic-doped-semiconductor-p-type-acceptor.png 808w, https:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/extrinsic-doped-semiconductor-p-type-acceptor-300x206.png 300w, https:\/\/sitepourvtc.com\/wp-content\/uploads\/2019\/02\/extrinsic-doped-semiconductor-p-type-acceptor-768x528.png 768w\" sizes=\"(max-width: 569px) 100vw, 569px\" \/><\/a>Electron-hole Pair<\/strong>. In semiconductors, <strong>free charge carriers<\/strong> are <strong>electrons<\/strong> and <strong>electron holes<\/strong> (electron-hole pairs). Electrons and holes are created by <strong>exciting\u00a0electrons<\/strong> from the valence band to the conduction band. An electron-hole (often called a hole) is the lack of an electron at a position where one could exist in an <a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/atomic-nuclear-physics\/atom-properties-of-atoms\/\">atom<\/a> or atomic lattice. It is one of the two types of charge carriers that are responsible for creating an electric current in semiconducting materials. Since, in a normal atom or crystal lattice, the negative charge of the electrons is balanced by the positive charge of the atomic nuclei, the absence of an electron leaves a net positive charge at the hole\u2019s location. As electrons leave their positions, positively charged holes can move from atom to atom in semiconducting materials. When an electron meets with a hole, they recombine, and these free carriers effectively vanish. The recombination means an electron that has been excited from the valence band to the conduction band falls back to the empty state in the valence band, known as the holes.<\/li>\n<\/ul>\n<p>The conductivity of a semiconductor can be modeled in terms of the <strong>band theory of solids<\/strong>. The band model of a semiconductor suggests that at ordinary temperatures, there is a finite possibility that electrons can reach the conduction band and contribute to electrical conduction. In the semiconductor, free charge carriers (electron-hole pairs) are created by the excitation of electrons from the valence band to the conduction band. This excitation left a hole in the valence band, which behaves as a positive charge, and an electron-hole pair is created. Holes can sometimes be confusing as they are not physical particles in the way that electrons are. Rather they are the absence of an electron in an atom. <strong>Holes can move from atom to atom<\/strong> in semiconducting materials as electrons leave their positions.<\/p>\n<h2>Electron Excitation in Semiconductors<\/h2>\n<p><strong>Energy for the excitation<\/strong> can be obtained in different ways.<\/p>\n<h3>Thermal Excitation<\/h3>\n<p>Electron-hole pairs are also constantly generated from thermal energy without any external energy source. Thermal excitation does not require any other form of starting impulse. This phenomenon also occurs at room temperature. It is caused by impurities, structure lattice irregularities, or dopants. It strongly depends on the E<sub>gap<\/sub> (a distance between valence and conduction band), so that for lower E<sub>gap<\/sub>, the number of thermally excited charge carriers increases. Since thermal excitation results in the detector noise, active cooling is required for some types of semiconductors (e.g., germanium). Detectors based on silicon have sufficiently low noise even at room temperature. This is caused by the large band gap of silicon (Egap= 1.12 eV), which allows us to operate the detector at room temperature, but cooling is preferred to reduce noise.<\/p>\n<h3>Optical Excitation<\/h3>\n<p>Note that the energy of a single photon of the visible light spectrum is comparable with these band gaps. Photons of wavelengths 700 nm &#8211; 400 nm have energies of \u00a01.77 eV to 3.10 eV. As a result, visible light can also excite electrons to the conduction band, which is the principle of photovoltaic panels that generate electric currents.<\/p>\n<h3>Excitation by Ionizing Radiation<\/h3>\n<p>Electrons may reach the conduction band when they are <strong>excited by ionizing radiation<\/strong> (i.e., they must obtain energy higher than Egap). In general, <a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/interaction-radiation-matter\/interaction-heavy-charged-particles\/\">heavy charged particles<\/a> transfer energy mostly by:<\/p>\n<ul>\n<li><strong>Excitation.<\/strong> The charged particle can transfer energy to the atom, raising electrons to higher energy levels.<\/li>\n<li><strong>Ionization.<\/strong> Ionization can occur when the charged particle has enough energy to remove an electron, resulting in the creation of ion pairs in surrounding matter.<\/li>\n<\/ul>\n<p>A convenient variable that describes the ionization properties of the surrounding medium is <strong>the stopping power<\/strong>, and the\u00a0classical expression describing the specific energy loss is the <a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/interaction-radiation-matter\/interaction-heavy-charged-particles\/stopping-power-bethe-formula\/\">Bethe formula<\/a>. For <a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/atomic-nuclear-physics\/fundamental-particles\/alpha-particle\/\">alpha particles<\/a> and heavier particles, <strong>the stopping power<\/strong> of most materials is very high for heavy charged particles, and these particles have very short ranges.<\/p>\n<p>In addition to these interactions, <a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/atomic-nuclear-physics\/fundamental-particles\/beta-particle\/\">beta particles<\/a> lose energy through a radiative process known as the <a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/atomic-nuclear-physics\/fundamental-particles\/beta-particle\/bremsstrahlung-2\/\"><strong>bremsstrahlung<\/strong><\/a>. From classical theory, when a charged particle is accelerated or decelerated, <strong>it must radiate energy,<\/strong> and the deceleration radiation is known as <strong>the bremsstrahlung (\u201cbraking radiation\u201d)<\/strong>.<\/p>\n<p>Photons (gamma rays and X-rays) can ionize atoms directly (despite they are electrically neutral) through the Photoelectric effect and the Compton effect, but secondary (indirect) ionization is much more significant. Although many possible interactions are known, there are three key interaction mechanisms with the matter.<\/p>\n<ul>\n<li><strong><a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/interaction-radiation-matter\/interaction-gamma-radiation-matter\/photoelectric-effect\/\">Photoelectric effect<\/a><\/strong><\/li>\n<li><strong><a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/interaction-radiation-matter\/interaction-gamma-radiation-matter\/compton-scattering\/\">Compton scattering<\/a><\/strong><\/li>\n<li><strong><a href=\"http:\/\/sitepourvtc.com\/nuclear-power\/reactor-physics\/interaction-radiation-matter\/interaction-gamma-radiation-matter\/pair-production\/\">Pair production<\/a><\/strong><\/li>\n<\/ul>\n<p>In all cases, a particle of ionizing radiation deposits a portion of its energy along its path. Particle passing through the detector ionizes the atoms of the semiconductor, producing the <strong>electron-hole pairs<\/strong>. For example, the typical thickness of a <strong>silicon detector<\/strong> is about 300 \u00b5m. Hence, the number of generated electron-hole pairs by a minimum ionizing particle (MIP) passing perpendicular through the detector is about <strong>3.2 x 10<sup>4<\/sup><\/strong>. This value is minor compared to the total number of free carriers in an intrinsic semiconductor with a surface of 1 cm<sup>2<\/sup> and the same thickness. Note that a sample of pure germanium at 20 \u00b0C contains about 1.26\u00d710<sup>21<\/sup> atoms but also contains 7.5 x 10<sup>11<\/sup> free electrons and 7.5 x 10<sup>11<\/sup> holes constantly generated from <a href=\"http:\/\/sitepourvtc.com\/nuclear-engineering\/thermodynamics\/what-is-energy-physics\/internal-energy-thermal-energy\/\">thermal energy<\/a>. As can be seen, the signal-to-noise ratio (S\/N) would be minimal. Adding 0.001% of arsenic (an impurity) donates an extra 10<sup>15<\/sup> free electrons in the same volume, and the electrical conductivity is increased by a factor of 10,000. The signal-to-noise ratio (S\/N) in doped material would be even smaller. <strong>Cooling the semiconductor<\/strong> is one way to lower this ratio.<\/p>\n<p>Improvement can be achieved by using a reverse-bias voltage to the P-N junction to deplete the detector of free carriers, which is the principle of most silicon radiation detectors. In this case, a negative voltage is applied to the p-side and positive to the second one. Holes in the p-region are attracted from the junction towards the p contact and similarly for electrons and the n contact.<\/p>\n<\/div><\/div>\n<div   id="8n9s8rpp6h"     class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights \"><div   id="8n9s8rpp6h"     class=\"inside-grid-column\"><div   id="8n9s8rpp6h"    class=\"su-spoiler su-spoiler-style-default su-spoiler-icon-plus su-spoiler-closed\" data-scroll-offset=\"0\"><div   id="8n9s8rpp6h"    class=\"su-spoiler-title\" tabindex=\"0\" role=\"button\"><span class=\"su-spoiler-icon\"><\/span>References:<\/div><div   id="8n9s8rpp6h"    class=\"su-spoiler-content su-u-clearfix su-u-trim\">\n<p><strong>Radiation Protection:<\/strong><\/p>\n<ol>\n<li>Knoll, Glenn F., Radiation Detection and Measurement 4th Edition, Wiley, 8\/2010. ISBN-13: 978-0470131480.<\/li>\n<li>Stabin, Michael G., Radiation Protection, and Dosimetry: An Introduction to Health Physics, Springer, 10\/2010. ISBN-13: 978-1441923912.<\/li>\n<li>Martin, James E., Physics for Radiation Protection 3rd Edition, Wiley-VCH, 4\/2013. ISBN-13: 978-3527411764.<\/li>\n<li>U.S.NRC, NUCLEAR REACTOR CONCEPTS<\/li>\n<li>U.S. Department of Energy, Instrumentation, and Control. DOE Fundamentals Handbook, Volume 2 of 2. June 1992.<\/li>\n<\/ol>\n<p><strong>Nuclear and Reactor Physics:<\/strong><\/p>\n<ol>\n<li>J. R. Lamarsh, Introduction to Nuclear Reactor Theory, 2nd ed., Addison-Wesley, Reading, MA (1983).<\/li>\n<li>J. R. Lamarsh, A. J. Baratta, Introduction to Nuclear Engineering, 3d ed., Prentice-Hall, 2001, ISBN: 0-201-82498-1.<\/li>\n<li>W. M. Stacey, Nuclear Reactor Physics, John Wiley &amp; Sons, 2001, ISBN: 0- 471-39127-1.<\/li>\n<li>Glasstone, Sesonske. Nuclear Reactor Engineering: Reactor Systems Engineering, Springer; 4th edition, 1994, ISBN: 978-0412985317<\/li>\n<li>W.S.C. Williams. Nuclear and Particle Physics. Clarendon Press; 1 edition, 1991, ISBN: 978-0198520467<\/li>\n<li>G.R.Keepin. Physics of Nuclear Kinetics. Addison-Wesley Pub. Co; 1st edition, 1965<\/li>\n<li>Robert Reed Burn, Introduction to Nuclear Reactor Operation, 1988.<\/li>\n<li>U.S. Department of Energy, Nuclear Physics and Reactor Theory. DOE Fundamentals Handbook, Volume 1 and 2. January 1993.<\/li>\n<li>Paul Reuss, Neutron Physics. EDP Sciences, 2008. ISBN: 978-2759800414.<\/li>\n<\/ol>\n<\/div><\/div><div   id="8n9s8rpp6h"    class=\"su-divider su-divider-style-dotted\" style=\"margin:15px 0;border-width:2px;border-color:#999999\"><\/div><\/div><\/div><div   id="8n9s8rpp6h"     class=\"lgc-column lgc-grid-parent lgc-grid-33 lgc-tablet-grid-33 lgc-mobile-grid-100 lgc-equal-heights \"><div   id="8n9s8rpp6h"     class=\"inside-grid-column\"><\/div><\/div><div   id="8n9s8rpp6h"     class=\"lgc-column lgc-grid-parent lgc-grid-33 lgc-tablet-grid-33 lgc-mobile-grid-100 lgc-equal-heights \"><div   id="8n9s8rpp6h"     class=\"inside-grid-column\">\n<h2>See above:<\/h2>\n<p>Semiconductor Detectors<a href=\"http:\/\/sitepourvtc.com\/nuclear-engineering\/radiation-detection\/semiconductor-detectors\/\" class=\"su-button su-button-style-flat\" style=\"color:#606060;background-color:#ffffff;border-color:#cccccc;border-radius:10px;-moz-border-radius:10px;-webkit-border-radius:10px\" target=\"_self\"><span style=\"color:#606060;padding:7px 20px;font-size:16px;line-height:24px;border-color:#ffffff;border-radius:10px;-moz-border-radius:10px;-webkit-border-radius:10px;text-shadow:0px 0px 0px #000000;-moz-text-shadow:0px 0px 0px #000000;-webkit-text-shadow:0px 0px 0px #000000\"><i class=\"sui sui-link\" style=\"font-size:16px;color:#5d5d5d\"><\/i> <\/span><\/a><\/p><\/div><\/div><div   id="8n9s8rpp6h"     class=\"lgc-column lgc-grid-parent lgc-grid-33 lgc-tablet-grid-33 lgc-mobile-grid-100 lgc-equal-heights \"><div   id="8n9s8rpp6h"     class=\"inside-grid-column\"><\/div><\/div>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":1,"featured_media":0,"parent":26407,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"generate_page_header":""},"_links":{"self":[{"href":"https:\/\/sitepourvtc.com\/wp-json\/wp\/v2\/pages\/26453"}],"collection":[{"href":"https:\/\/sitepourvtc.com\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/sitepourvtc.com\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/sitepourvtc.com\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/sitepourvtc.com\/wp-json\/wp\/v2\/comments?post=26453"}],"version-history":[{"count":3,"href":"https:\/\/sitepourvtc.com\/wp-json\/wp\/v2\/pages\/26453\/revisions"}],"predecessor-version":[{"id":38251,"href":"https:\/\/sitepourvtc.com\/wp-json\/wp\/v2\/pages\/26453\/revisions\/38251"}],"up":[{"embeddable":true,"href":"https:\/\/sitepourvtc.com\/wp-json\/wp\/v2\/pages\/26407"}],"wp:attachment":[{"href":"https:\/\/sitepourvtc.com\/wp-json\/wp\/v2\/media?parent=26453"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}