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The | In mathematical physics, the '''ADHM construction''' or '''monad construction''' is the construction of all [[instanton]]s using methods of linear algebra by [[Michael Atiyah]], [[Vladimir Drinfeld]], [[Nigel Hitchin]], [[Yuri I. Manin]] in their paper ''Construction of Instantons''. | ||
== ADHM data == | |||
The ADHM construction uses the following data: | |||
* complex [[vector space]]s ''V'' and ''W'' of dimension ''k'' and ''N'', | |||
* ''k'' × ''k'' complex matrices ''B''<sub>1</sub>, ''B''<sub>2</sub>, a ''k'' × ''N'' complex matrix ''I'' and a ''N'' × ''k'' complex matrix ''J'', | |||
* a [[real number|real]] [[moment map]] <math>\mu_r = [B_1,B_1^\dagger]+[B_2,B_2^\dagger]+II^\dagger-J^\dagger J,</math> | |||
* a [[complex number|complex]] moment map <math>\displaystyle\mu_c = [B_1,B_2]+IJ.</math> | |||
Then the ADHM construction claims that, given certain regularity conditions, | |||
* Given ''B''<sub>1</sub>, ''B''<sub>2</sub>, ''I'', ''J'' such that <math>\mu_r=\mu_c=0</math>, an anti-self-dual [[instanton]] in a [[special unitary group|SU(''N'')]] [[gauge theory]] with [[instanton]] number ''k'' can be constructed, | |||
* All anti-self-dual [[instantons]] can be obtained in this way and are in one-to-one correspondence with solutions up to a U(''k'') rotation which acts on each ''B'' in the [[adjoint representation]] and on ''I'' and ''J'' via the [[fundamental representation|fundamental]] and antifundamental representations | |||
* The [[metric (mathematics)|metric]] on the [[moduli space]] of instantons is that inherited from the flat metric on ''B'', ''I'' and ''J''. | |||
==Generalizations== | |||
===Noncommutative instantons=== | |||
In a [[noncommutative geometry|noncommutative]] gauge theory, the ADHM construction is identical but the moment map <math>\vec\mu </math> is set equal to the self-dual projection of the noncommutativity matrix of the spacetime times the [[identity matrix]]. In this case instantons exist even when the gauge group is U(1). The noncommutative instantons were discovered by [[Nikita Nekrasov]] and [[Albert Schwarz]] in 1998. | |||
===Vortices=== | |||
Setting ''B''<sub>2</sub> and ''J'' to zero, one obtains the classical moduli space of nonabelian [[Abrikosov vortex|vortices]] in a [[supersymmetry|supersymmetric]] gauge theory with an equal number of colors and flavors, as was demonstrated in [http://www.slac.stanford.edu/spires/find/hep/www?eprint=hep-th/0306150 Vortices, instantons and branes]. The generalization to greater numbers of flavors appeared in [http://www.slac.stanford.edu/spires/find/hep/www?eprint=hep-th/0602170 Solitons in the Higgs phase: The Moduli matrix approach]. In both cases the [[Fayet-Iliopoulos term]], which determines a [[squark]] [[top quark condensate|condensate]], plays the role of the noncommutativity parameter in the real moment map. | |||
== The construction formula == | |||
Let ''x'' be the 4-dimensional [[Euclidean space|Euclidean]] [[spacetime]] coordinates written in [[quaternion]]ic notation | |||
<math>x_{ij}=\begin{pmatrix}z_2&z_1\\-\bar{z_1}&\bar{z_2}\end{pmatrix}.</math> | |||
Consider the 2''k'' × (''N'' + 2''k'') matrix | |||
:<math>\Delta= \begin{pmatrix}I&B_2+z_2&B_1+z_1\\J^\dagger&-B_1^\dagger-\bar{z_1}&B_2^\dagger+\bar{z_2}\end{pmatrix}.</math> | |||
Then the conditions <math>\displaystyle\mu_r=\mu_c=0</math> are equivalent to the factorization condition | |||
:<math>\Delta\Delta^\dagger=\begin{pmatrix}f^{-1}&0\\0&f^{-1}\end{pmatrix}</math> where ''f''(''x'') is a ''k'' × ''k'' [[Hermitian matrix]]. | |||
Then a hermitian [[projection (linear algebra)|projection]] operator ''P'' can be constructed as | |||
:<math>P=\Delta^\dagger\begin{pmatrix}f&0\\0&f\end{pmatrix}\Delta.</math> | |||
The [[nullspace]] of Δ(''x'') is of ''N'' dimension for generic ''x''. The basis vector for this null-space can be assembled into an (''N'' + 2''k'') × ''N'' matrix ''U''(''x'') with orthonormalization condition ''U''<sup>†</sup>''U'' = 1. | |||
A regularity condition on the rank of Δ guaranteed the completeness condition | |||
:<math>P+UU^\dagger=1. \, </math> | |||
The anti-selfdual [[connection (mathematics)|connection]] is then constructed from ''U'' by the formula | |||
:<math>A_m=U^\dagger \partial_m U.</math> | |||
==See also== | |||
*[[Monad (linear algebra)]] | |||
==References== | |||
*{{Citation | last1=Atiyah | first1=Michael Francis | author1-link=Michael Atiyah | title=Geometry of Yang-Mills fields | publisher=Scuola Normale Superiore Pisa, Pisa | id={{MathSciNet | id = 554924}} | year=1979}} | |||
*{{Citation | last1=Atiyah | first1=Michael Francis | author1-link=Michael Atiyah | last3=Hitchin | first3=N. J. | last2=Drinfeld | first2=V. G. | last4=Manin | first4=Yuri Ivanovich | author4-link=Yuri Ivanovich Manin | title=Construction of instantons | url=http://dx.doi.org/10.1016/0375-9601(78)90141-X | doi=10.1016/0375-9601(78)90141-X | id={{MR|598562}} | year=1978 | journal=Physics Letters A | issn=0375-9601 | volume=65 | issue=3 | pages=185–187|bibcode = 1978PhLA...65..185A }} | |||
*[http://projecteuclid.org/DPubS/Repository/1.0/Disseminate?view=body&id=pdf_1&handle=euclid.cmp/1103922679 On the Construction of Monopoles] | |||
[[Category:Quantum field theory]] | |||
[[Category:Differential geometry]] | |||
[[Category:Quantum chromodynamics]] | |||
Revision as of 08:12, 21 October 2013
In mathematical physics, the ADHM construction or monad construction is the construction of all instantons using methods of linear algebra by Michael Atiyah, Vladimir Drinfeld, Nigel Hitchin, Yuri I. Manin in their paper Construction of Instantons.
ADHM data
The ADHM construction uses the following data:
- complex vector spaces V and W of dimension k and N,
- k × k complex matrices B1, B2, a k × N complex matrix I and a N × k complex matrix J,
- a real moment map
- a complex moment map
Then the ADHM construction claims that, given certain regularity conditions,
- Given B1, B2, I, J such that , an anti-self-dual instanton in a SU(N) gauge theory with instanton number k can be constructed,
- All anti-self-dual instantons can be obtained in this way and are in one-to-one correspondence with solutions up to a U(k) rotation which acts on each B in the adjoint representation and on I and J via the fundamental and antifundamental representations
- The metric on the moduli space of instantons is that inherited from the flat metric on B, I and J.
Generalizations
Noncommutative instantons
In a noncommutative gauge theory, the ADHM construction is identical but the moment map is set equal to the self-dual projection of the noncommutativity matrix of the spacetime times the identity matrix. In this case instantons exist even when the gauge group is U(1). The noncommutative instantons were discovered by Nikita Nekrasov and Albert Schwarz in 1998.
Vortices
Setting B2 and J to zero, one obtains the classical moduli space of nonabelian vortices in a supersymmetric gauge theory with an equal number of colors and flavors, as was demonstrated in Vortices, instantons and branes. The generalization to greater numbers of flavors appeared in Solitons in the Higgs phase: The Moduli matrix approach. In both cases the Fayet-Iliopoulos term, which determines a squark condensate, plays the role of the noncommutativity parameter in the real moment map.
The construction formula
Let x be the 4-dimensional Euclidean spacetime coordinates written in quaternionic notation
Consider the 2k × (N + 2k) matrix
Then the conditions are equivalent to the factorization condition
- where f(x) is a k × k Hermitian matrix.
Then a hermitian projection operator P can be constructed as
The nullspace of Δ(x) is of N dimension for generic x. The basis vector for this null-space can be assembled into an (N + 2k) × N matrix U(x) with orthonormalization condition U†U = 1.
A regularity condition on the rank of Δ guaranteed the completeness condition
The anti-selfdual connection is then constructed from U by the formula
See also
References
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In case you are in search of an actual estate or Singapore property agent on-line, you simply should belief your intuition. It's because you do not know which agent is nice and which agent will not be. Carry out research on several brokers by looking out the internet. As soon as if you end up positive that a selected agent is dependable and reliable, you can choose to utilize his partnerise in finding you a home in Singapore. Most of the time, a property agent is taken into account to be good if he or she locations the contact data on his website. This may mean that the agent does not mind you calling them and asking them any questions relating to new properties in singapore in Singapore. After chatting with them you too can see them in their office after taking an appointment.
Have handed an trade examination i.e Widespread Examination for House Brokers (CEHA) or Actual Property Agency (REA) examination, or equal; Exclusive brokers are extra keen to share listing information thus making certain the widest doable coverage inside the real estate community via Multiple Listings and Networking. Accepting a severe provide is simpler since your agent is totally conscious of all advertising activity related with your property. This reduces your having to check with a number of agents for some other offers. Price control is easily achieved. Paint work in good restore-discuss with your Property Marketing consultant if main works are still to be done. Softening in residential property prices proceed, led by 2.8 per cent decline within the index for Remainder of Central Region
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15.6.1 As the agent is an intermediary, generally, as soon as the principal and third party are introduced right into a contractual relationship, the agent drops out of the image, subject to any problems with remuneration or indemnification that he could have against the principal, and extra exceptionally, against the third occasion. Generally, agents are entitled to be indemnified for all liabilities reasonably incurred within the execution of the brokers´ authority.
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