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The '''Sokolov–Ternov effect''' is the effect of self-polarization of relativistic electrons or positrons moving at high energy in a [[magnetic field]]. The self-polarization occurs through the emission of spin-flip [[synchrotron radiation]]. The effect was predicted by [[Igor Ternov]] which then were rigorously justified by [[Arsenij Sokolov]] using exact solutions to the [[Dirac equation]].<ref>{{Cite journal|first=A. A.|last=Sokolov|coauthors=I. M. Ternov|title=О поляризационных и спиновых эффектах в теории синхротронного излучения|trans_title=Polarization and spin effects in the theory of synchrotron radiation|journal=[[Doklady Akademii Nauk SSSR]]|volume=153|issue=5|pages=1052–1053|year=1963|language=Russian}}</ref><ref>{{Cite journal|author=A. A. Sokolov and I. M. Ternov|title=On Polarization and Spin Effects in Synchrotron Radiation Theory|journal=Sov. Phys. Dokl.|volume=8|pages=1203|year=1964|url=http://puhep1.princeton.edu/~mcdonald/examples/QED/sokolov_spd_8_1203_64.pdf|bibcode = 1964SPhD....8.1203S }}</ref>


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==Theory==
An [[electron]] in a magnetic field can have its [[spin (physics)|spin]] oriented in the same ("spin up") or in the opposite ("spin down") direction with respect to the direction of the magnetic field (which is assumed to be oriented "up"). The "spin down" state has a higher energy than "spin up" state. The polarization arises due to the fact that the rate of transition through emission of synchrotron radiation to the "spin down" state is slightly greater than the probability of transition to the "spin up" state. As a result, an initially unpolarized beam of high-energy electrons circulating in a [[storage ring]] after sufficiently long time will have spins oriented in the direction opposite to the magnetic field. Saturation is not complete and is explicitly described by the formula<ref name="ref1">{{Cite book|last=A. A. Sokolov and I. M. Ternov|publisher=American Institute of Physics Translation Series. Edited by C. W. Kilmister|location=New York|title=Radiation from Relativistic Electrons|year=1986|isbn=0-88318-507-5}} Section 21.3 for the theory and section 27.2 for experimental verifications of the Sokolov–Ternov effect.</ref>
:<math> \xi(t)=A\Bigl(1  -e^{-\frac{t}{\tau}}\Bigr)</math>
 
where <math>\scriptstyle A \;=\; 8\sqrt{3}/15 \;\approx\; 0.924</math> is the limiting degree of polarization (92.4%) and <math>\scriptstyle \tau</math> is the relaxation time,
:<math>\tau = A{{{\hbar}^2} \over {mc{e}^2}}\Bigl({{mc^2} \over {E}}\Bigr)^2\Bigl({H_0 \over H}\Bigr)^3</math>
 
Here <math>\scriptstyle A</math> is as before, <math>\scriptstyle m</math> and <math>\scriptstyle e</math> are the mass and charge of the electron, <math>\scriptstyle c</math> is the speed of light, <math>\scriptstyle H_0 \;\approx\; 4.41 \,\times\, 10^{13}</math> G is the [[Schwinger field]], <math>\scriptstyle H</math> is the magnetic field, and <math>\scriptstyle E</math> is the electron energy.
 
The limiting degree of polarization <math>A</math> is less than one due to the existence of spin-orbital energy exchange which allows for transitions to the "spin up" state (with probability 25.25 times less than to the "spin down" state).
 
Typical relaxation time is on the order of minutes and hours. Thus producing a highly polarized beam requires a long enough time and the use of [[storage ring]]s.
 
The self-polarization effect for [[positron]]s is similar, with the only difference that positrons will tend to have spins oriented in the direction parallel to the direction of the magnetic field.<ref>{{Cite book|last=J. Kessler|publisher=Springer|location=Berlin|title=Polarized Electrons. 2nd edition|year=1985}} Section 6.2.</ref>
 
==Experimental observation==
Sokolov–Ternov effect was experimentally observed in the [[USSR]], [[France]], [[Germany]], [[USA]], [[Japan]], and [[Switzerland]] in storage rings with electrons of energy 1-50 GeV.<ref name="ref1"/><ref>{{Cite book|last=V. A. Bordovitsyn (editor)|publisher=World Scientific|location=Singapore|title=Synchrotron Radiation Theory and Its Development: in Memory of I. M. Ternov|year=1999|isbn=981-02-3156-3|url=http://www.worldscibooks.com/physics/3492.html}}</ref>
 
*1971 — [[Budker Institute of Nuclear Physics]] (first observation), with the use of 625 MeV storage ring [[VEPP-2]].
*1971 — Orsay (France), with the use of 536 MeV АСО storage ring.
*1975 — Stanford (USA), with the use of 2.4 GeV SPEAR storage ring.
*1980 — [[DESY]], Hamburg (Germany), with the use of 15.2 GeV [[PETRA]].
 
==Applications and generalization==
The effect of radiative polarization provides a unique capability for creating polarized beams of high-energy electrons and positrons that can be used for various experiments.
 
The effect also has been related to the [[Unruh effect]] which, up to now, under experimentally achievable conditions is too small to be observed.
 
The equilibrium polarization given by the Sokolov and Ternov has corrections when the orbit is not perfectly planar.  The formula has been generalized by Derbenev and Kondratenko and others.<ref>http://pra.aps.org/abstract/PRA/v37/i2/p456_1 "Calculations of Bell and Leinaas and Derbenev and Kondratenko for radiative electron polarization"</ref>
 
==Patent==
* Sokolov A. A. and Ternov I. M. (1973): Award N 131 of 7 August 1973 with priority of 26 June 1963, Byull. Otkr. i Izobr., vol. '''47'''.
 
==See also==
*[[Unruh effect]]
*[[Hawking radiation]]
*[[Froissart Stora equation]]
 
==Notes==
{{Reflist|1}}
 
{{Use dmy dates|date=September 2010}}
 
{{DEFAULTSORT:Sokolov-Ternov Effect}}
[[Category:Special relativity]]
[[Category:Synchrotron radiation]]
[[Category:Particle physics]]
[[Category:Polarization (waves)]]

Revision as of 23:15, 13 October 2013

The Sokolov–Ternov effect is the effect of self-polarization of relativistic electrons or positrons moving at high energy in a magnetic field. The self-polarization occurs through the emission of spin-flip synchrotron radiation. The effect was predicted by Igor Ternov which then were rigorously justified by Arsenij Sokolov using exact solutions to the Dirac equation.[1][2]

Theory

An electron in a magnetic field can have its spin oriented in the same ("spin up") or in the opposite ("spin down") direction with respect to the direction of the magnetic field (which is assumed to be oriented "up"). The "spin down" state has a higher energy than "spin up" state. The polarization arises due to the fact that the rate of transition through emission of synchrotron radiation to the "spin down" state is slightly greater than the probability of transition to the "spin up" state. As a result, an initially unpolarized beam of high-energy electrons circulating in a storage ring after sufficiently long time will have spins oriented in the direction opposite to the magnetic field. Saturation is not complete and is explicitly described by the formula[3]

ξ(t)=A(1etτ)

where A=83/150.924 is the limiting degree of polarization (92.4%) and τ is the relaxation time,

τ=A2mce2(mc2E)2(H0H)3

Here A is as before, m and e are the mass and charge of the electron, c is the speed of light, H04.41×1013 G is the Schwinger field, H is the magnetic field, and E is the electron energy.

The limiting degree of polarization A is less than one due to the existence of spin-orbital energy exchange which allows for transitions to the "spin up" state (with probability 25.25 times less than to the "spin down" state).

Typical relaxation time is on the order of minutes and hours. Thus producing a highly polarized beam requires a long enough time and the use of storage rings.

The self-polarization effect for positrons is similar, with the only difference that positrons will tend to have spins oriented in the direction parallel to the direction of the magnetic field.[4]

Experimental observation

Sokolov–Ternov effect was experimentally observed in the USSR, France, Germany, USA, Japan, and Switzerland in storage rings with electrons of energy 1-50 GeV.[3][5]

  • 1971 — Budker Institute of Nuclear Physics (first observation), with the use of 625 MeV storage ring VEPP-2.
  • 1971 — Orsay (France), with the use of 536 MeV АСО storage ring.
  • 1975 — Stanford (USA), with the use of 2.4 GeV SPEAR storage ring.
  • 1980 — DESY, Hamburg (Germany), with the use of 15.2 GeV PETRA.

Applications and generalization

The effect of radiative polarization provides a unique capability for creating polarized beams of high-energy electrons and positrons that can be used for various experiments.

The effect also has been related to the Unruh effect which, up to now, under experimentally achievable conditions is too small to be observed.

The equilibrium polarization given by the Sokolov and Ternov has corrections when the orbit is not perfectly planar. The formula has been generalized by Derbenev and Kondratenko and others.[6]

Patent

  • Sokolov A. A. and Ternov I. M. (1973): Award N 131 of 7 August 1973 with priority of 26 June 1963, Byull. Otkr. i Izobr., vol. 47.

See also

Notes

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    In its statement, the singapore property listing - website link, government claimed that the majority citizens buying their first residence won't be hurt by the new measures. Some concessions can even be prolonged to chose teams of consumers, similar to married couples with a minimum of one Singaporean partner who are purchasing their second property so long as they intend to promote their first residential property. Lower the LTV limit on housing loans granted by monetary establishments regulated by MAS from 70% to 60% for property purchasers who are individuals with a number of outstanding housing loans on the time of the brand new housing purchase. Singapore Property Measures - 30 August 2010 The most popular seek for the number of bedrooms in Singapore is 4, followed by 2 and three. Lush Acres EC @ Sengkang

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  6. http://pra.aps.org/abstract/PRA/v37/i2/p456_1 "Calculations of Bell and Leinaas and Derbenev and Kondratenko for radiative electron polarization"