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| In [[nuclear engineering]], a '''delayed neutron''' is a [[neutron]] emitted after a [[nuclear fission]] event, by one of the [[fission product]]s (or actually, a fission product daughter after beta decay), any time from a few milliseconds to a few minutes after the fission event. Neutrons born within <math>10^{-14}</math> seconds of the fission are termed "prompt neutrons".
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| In a [[nuclear reactor]] large nuclides fission in two neutron-rich fission products (i.e. unstable [[nuclides]]). Many of these fission products then undergo [[radioactive decay]] (usually [[beta decay]]) and the resulting nuclides are left in an excited state. These usually immediately undergo [[gamma decay]] but a small fraction of them are excited enough to be able to decay by emitting a neutron in addition. The moment of [[beta decay]] of the precursor nuclides - which are the precursors of the delayed neutrons - happens orders of magnitude later compared to the emission of the [[prompt neutron]]s. Hence the neutron that originates from the [[neutron emission|precursor's decay]] is termed a delayed neutron. However, the "delay" in the neutron emission is due to the delay in beta decay, since neutron emission, like gamma emission, happens almost immediately after the beta decay. The various half lives of these decays that finally result in neutron emission, are thus the beta decay half lives of the precursor radionuclides.
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| Delayed neutrons play an important role in [[nuclear reactor control]] and safety analysis.
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| ==Principle==
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| Delayed neutrons are associated with the [[beta decay]] of the fission products. After prompt fission neutron emission the residual fragments are still neutron rich and undergo a beta decay chain. The more neutron rich the fragment, the more energetic and faster the beta decay. In some cases the available energy in the beta decay is high enough to leave the residual nucleus in such a highly excited state that neutron emission instead of [[gamma ray|gamma emission]] occurs.
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| Using [[Uranium-235|U-235]] as an example, this nucleus absorbs [[thermal neutron]]s, and the immediate mass products of a fission event are two large fission fragments, which are remnants of the formed U-236 nucleus. These fragments emit, on average, two or three free neutrons (in average 2.47), called [[prompt neutron|"prompt" neutrons]]. A subsequent fission fragment occasionally undergoes a stage of radioactive decay (which is a [[beta decay|beta minus decay]]) that yields a new nucleus (the precursor nucleus) in an excited state that emits an additional neutron, called a "delayed" neutron, to get to ground state. These neutron-emitting fission fragments are called delayed neutron precursor atoms.
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| '''Delayed Neutron Data for Thermal Fission in U-235'''<ref>Lamarsh, Introduction to Nuclear Engineering</ref>
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| {| class="wikitable"
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| |-
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| ! Group
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| ! Half-Life (s)
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| ! Decay Constant (s<sup>−1</sup>)
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| ! Energy (keV)
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| ! Yield, Neutrons per Fission
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| ! Fraction
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| |-
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| | 1
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| | 55.72
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| | 0.0124
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| | 250
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| | 0.00052
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| | 0.000215
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| |-
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| | 2
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| | 22.72
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| | 0.0305
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| | 560
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| | 0.00546
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| | 0.001424
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| |-
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| | 3
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| | 6.22
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| | 0.111
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| | 405
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| | 0.00310
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| | 0.001274
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| |-
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| | 4
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| | 2.30
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| | 0.301
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| | 450
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| | 0.00624
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| | 0.002568
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| |-
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| | 5
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| | 0.614
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| | 1.14
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| | -
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| | 0.00182
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| | 0.000748
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| |-
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| | 6
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| | 0.230
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| | 3.01
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| | -
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| | 0.00066
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| | 0.000273
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| |}
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| ==Importance in nuclear fission basic research==
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| The standard deviation of the final kinetic energy distribution as a function of mass of final fragments from low energy fission of uranium 234 and uranium 236, presents a peak around light fragment masses region and another on heavy fragment masses region. Simulation by Monte Carlo method of these experiments suggests that that those peaks are produced by prompt neutron emission.<ref>R. Brissot, J.P. Boucquet, J. Crançon,C.R. Guet, H.A. Nifenecker. and Montoya, M., "Kinetic-Energy Distribution for Symmetric Fission of 235U", Proc. of a Symp. On Phys. And Chem. Of Fission, IAEA. Vienna, 1980 (1979)</ref><ref>
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| [http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=APCPCS000947000001000326000001&idtype=cvips&gifs=yes | M. Montoya, E. Saettone, J. Rojas, "Effects of Neutron Emission on Fragment Mass and Kinetic Energy Distribution from Thermal Neutron-Induced Fission of 235U", "AIP Conference Proceedings", American Institute of Physics, Volume 947/October, 2007, {{doi|10.1063/1.2813826}}, pp. 326-329]</ref><ref>[http://www.ejournal.unam.mx/rmf/no535/RMF005300506.pdf M. Montoya, E. Saettone, J. Rojas, "Monte Carlo Simulation for fragment mass and kinetic energy distribution from neutron-induced fission of U 235" , Revista Mexicana de Física 53 (5) 366-370, oct 2007]</ref><ref>[http://rmf.fciencias.unam.mx/pdf/rmf/54/6/54_6_440.pdf M. Montoya, J. Rojas, I. Lobato, "Neutron emission effects on final fragments mass and kinetic energy distribution from low energy fission of U 234", Revista Mexicana de Física, 54(6) dic 2008]</ref> This effect of prompt neutron emission does not permit to obtain primary primary mass and kinetic distribution which is important to study fission dynamics from saddle to scission point.
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| ==Importance in nuclear reactors==
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| If a [[nuclear reactor]] happened to be [[prompt critical]] - even very slightly - the number of neutrons would increase exponentially at a high rate, and very quickly the reactor would become uncontrollable by means of cybernetics. The control of the power rise would then be left to its intrinsic physical stability factors, like the thermal dilatation of the core, or the increased [[resonance absorption]]s of neutrons, that usually tend to decrease the reactor's reactivity when temperature rises; but the reactor would run the risk of being damaged or destroyed by heat.
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| However, thanks to the delayed neutrons, it is possible to leave the reactor in a [[subcritical]] state as far as only prompt neutrons are concerned: the delayed neutrons come a moment later, just in time to sustain the chain reaction when it is going to die out. In that regime, neutron production overall still grows exponentially, but on a time scale that is governed by the delayed neutron production, which is slow enough to be controlled (just as an otherwise unstable bicycle can be balanced because human reflexes are quick enough on the time scale of its instability). Thus, by widening the margins of non-operation and supercriticality and allowing more time to regulate the reactor, the delayed neutrons are essential to [[Passive nuclear safety|inherent reactor safety]] and even in reactors requiring active control.
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| ==Fraction definitions==
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| The factor β is defined as:
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| :<math>
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| \beta = \frac{\mbox{precursor atoms}}
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| {\mbox{prompt neutrons}+\mbox{precursor atoms}}.
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| </math>
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| and it is equal to 0.0064 for U-235.
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| The delayed neutron fraction (DNF) is defined as:
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| :<math>
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| DNF = \frac{\mbox{delayed neutrons}}
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| {\mbox{prompt neutrons}+\mbox{delayed neutrons}}.
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| </math>
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| These two factors, β and ''DNF'', are not the same thing in case of a rapid change in the number of neutrons in the reactor.
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| Another concept, is the ''effective fraction of delayed neutrons'', which is the fraction of delayed neutrons weighted (over space, energy, and angle) on the adjoint neutron flux. This concept arises because delayed neutrons are emitted with an energy spectrum more thermalized relative to prompt neutrons. For low enriched uranium fuel working on a thermal neutron spectrum, the difference between the average and effective delayed neutron fractions can reach 50 pcm.<ref>[http://www.osti.gov/bridge/product.biblio.jsp?query_id=1&page=0&osti_id=991100 Analyses on the Average and Effective Delayed Neutron Fractions of YALINA-Thermal Subcritical Assembly]</ref>
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| ==See also==
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| *[[prompt critical]]
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| *[[Critical mass (nuclear)|critical mass]]
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| *[[nuclear chain reaction]]
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| ==References==
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| {{Reflist}}
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| ==External links==
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| *[http://lpsc.in2p3.fr/gpr/PPNPport/node47.html Hybrid nuclear reactors:delayed neutrons]
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| *[http://www.pipeline.com/~rstater/nuke1a.html Beta is not the delayed neutron (population) fraction]
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| [[Category:Nuclear technology]]
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| [[Category:Neutron|Prompt]]
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| [[de:Kritikalität#Verzögerte Neutronen]]
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| [[pl:Neutron opóźniony]]
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The writer is known by the title of Figures Wunder. One of the things he loves most is ice skating but he is struggling to find time for it. North Dakota is her beginning place but she will have to transfer 1 day or an additional. For years he's been operating as a receptionist.
Also visit my web site - http://needtoclick.me