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In [[quantum mechanics]] and [[statistical mechanics]], '''parastatistics''' is one of several alternatives to the better known [[particle statistics]] models ([[Bose–Einstein statistics]], [[Fermi–Dirac statistics]] and [[Maxwell–Boltzmann statistics]]). Other alternatives include [[anyonic statistics]] and [[braid statistics]], both of these involving lower spacetime dimensions.
 
==Formalism==
Consider the [[operator algebra]] of a system of ''N'' identical particles. This is a [[star-algebra|*-algebra]]. There is an ''S<sub>N</sub>'' group ([[symmetric group]] of order ''N'')  [[group action|acting]] upon the operator algebra with the intended interpretation of [[permutation|permuting]] the ''N'' particles. Quantum mechanics requires focus on [[observable]]s having a physical meaning, and the observables would have to be [[invariant (mathematics)|invariant]] under all possible permutations of the ''N'' particles. For example in the case ''N''&nbsp;=&nbsp;2, ''R''<sub>2</sub>&nbsp;&minus;&nbsp;''R''<sub>1</sub> cannot be an observable because it changes sign if we switch the two particles, but the distance between the two particles : |''R''<sub>2</sub>&nbsp;&minus;&nbsp;''R''<sub>1</sub>| is a legitimate observable.
 
In other words, the observable algebra would have to be a *-[[subalgebra]] invariant under the action of ''S<sub>N</sub>'' (noting that this does not mean that every element of the operator algebra invariant under ''S<sub>N</sub>'' is an observable). Therefore we can have different [[superselection sector]]s, each parameterized by a [[Young diagram]] of ''S<sub>N</sub>''.
 
In particular:
 
* If we have ''N'' identical '''parabosons''' of order ''p'' (where ''p'' is a positive integer), then the permissible Young diagrams are all those with ''p'' or fewer rows.
* If we have ''N'' identical '''parafermions''' of order ''p'', then the permissible Young diagrams are all those with ''p'' or fewer columns.
* If ''p'' is 1, we just have the ordinary cases of Bose–Einstein and Fermi–Dirac statistics respectively.
* If ''p'' is infinity (not an integer, but one could also have said arbitrarily large ''p''), we have Maxwell–Boltzmann statistics.
 
==The quantum field theory of parastatistics==
A paraboson field of order ''p'', <math>\phi(x)=\sum_{i=1}^p \phi^{(i)}(x)</math> where if ''x'' and ''y'' are [[spacelike]]-separated points, <math>[\phi^{(i)}(x),\phi^{(i)}(y)]=0</math> and <math>\{\phi^{(i)}(x),\phi^{(j)}(y)\}=0</math> if <math>i\neq j</math> where [,] is the [[commutator]] and {,} is the [[anticommutator]]. Note that this disagrees with the [[spin-statistics theorem]], which is for [[boson]]s and not parabosons. There might be a group such as the [[symmetric group]] ''S<sub>p</sub>'' acting upon the ''φ''<sup>(''i'')</sup>s. [[Observable]]s would have to be operators which are [[invariant (mathematics)|invariant]] under the group in question. However, the existence of such a symmetry is not essential.
 
A parafermion field <math>\psi(x)=\sum_{i=1}^p \psi^{(i)}(x)</math> of order ''p'', where if ''x'' and ''y'' are [[spacelike]]-separated points, <math>\{\psi^{(i)}(x),\psi^{(i)}(y)\}=0</math> and <math>[\psi^{(i)}(x),\psi^{(j)}(y)]=0</math> if <math>i\neq j</math>. The same comment about [[observable]]s would apply together with the requirement that they have even [[Graded algebra|grading]] under the grading where the ''ψ''s have odd grading.
 
The ''parafermionic and parabosonic algebras'' are generated by elements that obey the commutation and anticommutation relations. They generalize the usual ''fermionic algebra'' and the ''bosonic algebra'' of quantum mechanics.<ref>K. Kanakoglou, C. Daskaloyannis: [http://books.google.com/books?id=KAZL5UBlS4cC&pg=PA207 ''Chapter 18 Bosonisation and Parastatistics'', p. 207 ff.], in: Sergei D. Silvestrov, Eugen Paal, Viktor Abramov, Alexander Stolin (eds.): ''Generalized Lie Theory in Mathematics, Physics and Beyond'', 2008, ISBN 978-3-540-85331-2</ref> The [[Dirac algebra]] and the [[Duffin–Kemmer–Petiau algebra]] appear as special cases of the parafermionic algebra for order p=1 and p=2, respectively.<ref>See citations in: Mikhail S. Plyushchay, Michel Rausch de Traubenberg: ''Cubic root of Klein-Gordon equation'', [http://arxiv.org/abs/hep-th/0001067v2 arXiv:hep-th/0001067v2] (submitted on 11 January 2000, version of 2 February 2000)</ref>
 
==Explaining parastatistics==
Note that if ''x'' and ''y'' are spacelike-separated points, ''φ''(''x'') and ''&phi;''(''y'') neither commute nor anticommute unless ''p''=1. The same comment applies to ''ψ''(''x'') and ''&psi;''(''y''). So, if we have ''n'' spacelike separated points ''x''<sub>1</sub>, ..., ''x''<sub>''n''</sub>,
 
:<math>\phi(x_1)\cdots \phi(x_n)|\Omega\rangle</math>
 
corresponds to creating ''n'' identical parabosons at ''x''<sub>1</sub>,..., ''x''<sub>''n''</sub>. Similarly,
 
:<math>\psi(x_1)\cdots \psi(x_n)|\Omega\rangle</math>
 
corresponds to creating ''n'' identical parafermions. Because these fields neither commute nor anticommute
 
:<math>\phi(x_{\pi(1)})\cdots \phi(x_{\pi(n)})|\Omega\rangle</math>
 
and
 
:<math>\psi(x_{\pi(1)})\cdots \psi(x_{\pi(n)})|\Omega\rangle</math>
 
gives distinct states for each permutation π in ''[[symmetric group|S<sub>n</sub>]]''.
 
We can define a permutation operator <math>\mathcal{E}(\pi)</math> by
 
:<math>\mathcal{E}(\pi)\left[\phi(x_1)\cdots \phi(x_n)|\Omega\rangle\right]=\phi(x_{\pi^{-1}(1)})\cdots \phi(x_{\pi^{-1}(n)})|\Omega\rangle</math>
 
and
 
:<math>\mathcal{E}(\pi)\left[\psi(x_1)\cdots \psi(x_n)|\Omega\rangle\right]=\psi(x_{\pi^{-1}(1)})\cdots \psi(x_{\pi^{-1}(n)})|\Omega\rangle</math>
 
respectively. This can be shown to be well-defined as long as <math>\mathcal{E}(\pi)</math> is only restricted to states spanned by the vectors given above (essentially the states with ''n'' identical particles). It is also [[unitary operator|unitary]]. Moreover, <math>\mathcal{E}</math> is an operator-valued [[group representation|representation]] of the symmetric group ''S<sub>n</sub>'' and as such, we can interpret it as the action of ''S<sub>n</sub>'' upon the ''n''-particle Hilbert space itself, turning it into a [[unitary representation]].
 
[[Quantum chromodynamics|QCD]] can be reformulated using parastatistics with the quarks being parafermions of order 3 and the gluons being parabosons of order 8. Note this is different from the conventional approach where quarks always obey anticommutation relations and gluons commutation relations.
 
==History of parastatistics==
H.S. (Bert) Green <ref>http://www.physics.adelaide.edu.au/mathphysics/hsg_memorial.html</ref> is credited with the invention/discovery of parastatistics in 1953 <ref>H.S. Green, A Generalized Method of Field Quantization. Phys. Rev. 90, 270–273 (1953).(c)</ref>
 
==See also==
{{Statistical mechanics|cTopic=[[Particle statistics|Particle Statistics]]}}
*[[Klein transformation]] on how to convert between parastatistics and the more conventional statistics
 
==References==
{{reflist}}
 
[[Category:Parastatistics|*]]
[[Category:Permutations]]

Latest revision as of 16:53, 21 December 2014

Whenever you compare registry products there are a amount of elements to look out for. Because of the sheer number of for registry products available found on the Internet at the moment it could be quite effortless to be scammed. Something often overlooked is that a few of these products might in actual fact end up damaging your PC. And the registry they state they have cleaned might merely cause more problems with a computer than the ones we started with.

Registry is not furthermore important to quick computer boot up, and important to the performance of a computer. If you have a registry error, you may face blue screen, freezing or even crash. It's necessary to frequently clean up the invalid, lost, junk registry keys to keep the computer healthy and running quick.

Over time a disk can equally receive fragmented. Fragmentation causes a computer to slow down considering it takes windows much longer to locate a files place. Fortunately, the PC has a built inside disk defragmenter. You are able to run this program by clicking "Start" - "All Programs" - "Accessories" - "System Tools" - "Disk Defragmenter". We might today have the way to choose which forces or partition you need to defragment. This action may take we certain time so it is advised to do this regularly so as to avoid further fragmentation and to accelerate the windows XP computer.

The problem with nearly all of the persons is the fact that they never like to spend funds. In the damaged adaptation 1 does not have to pay anything plus may download it from web easily. It is easy to install too. However, the problem comes whenever it is not able to detect all possible viruses, spyware and malware in the system. This is considering it's obsolete inside nature plus refuses to get any standard updates from the website downloaded. Thus, a program is accessible to difficulties like hacking.

The tuneup utilities 2014 must come as standard with a back up and restore center. This ought to be an convenient to apply process.That signifies which when you encounter a problem with a PC following utilizing a registry cleaning we can simply restore your settings.

Files with the DOC extension are furthermore susceptible to viruses, but this is solved by superior antivirus programs. Another problem is that .doc files may be corrupted, unreadable or damaged due to spyware, adware, plus malware. These cases might avoid consumers from correctly opening DOC files. This is whenever effective registry products become useful.

The System File Checker (SFC) could enable inside resolving error 1721 as it, by its nature, scans the system files for corruption and replaces them with their original versions. This needs you to have the Windows Installation DVD ROM for continuing.

There is a lot a advantageous registry cleaner may do for a computer. It may check for and download updates for Windows, Java and Adobe. Keeping changes present is an important piece of wise computer health. It can equally protect your individual and company confidentiality plus a online protection.