"Spin system and Pauli exclusion principle"의 두 판 사이의 차이
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+ | <h5>angular momentum</h5> | ||
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<h5 style="line-height: 2em; margin: 0px;">sl(2)</h5> | <h5 style="line-height: 2em; margin: 0px;">sl(2)</h5> | ||
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* commutator<br><math>[E,F]=H</math><br><math>[H,E]=2E</math><br><math>[H,F]=-2F</math><br> | * commutator<br><math>[E,F]=H</math><br><math>[H,E]=2E</math><br><math>[H,F]=-2F</math><br> | ||
45번째 줄: | 48번째 줄: | ||
* Bosons<br> | * Bosons<br> | ||
− | * photon | + | ** photon |
− | * | + | ** vector boson |
− | * | + | ** Gluon |
− | * | + | ** follows Bose-Einstein statistics |
− | * | + | ** force-transmitting particles |
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* Fermions = spin- <math>1/2</math> particles<br> | * Fermions = spin- <math>1/2</math> particles<br> | ||
** quarks and leptons<br> | ** quarks and leptons<br> | ||
** follows Fermi-Dirac statistics<br> | ** follows Fermi-Dirac statistics<br> | ||
− | ** matter particles<br> | + | ** <br> matter particles<br> |
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2010년 11월 3일 (수) 17:56 판
introduction
- the simplest example of quantum mechanical system
- quantization of the angular momentum
- measures as being some multiple of Planck's constant divided by 2pi
angular momentum
representation theory
- concept from the representation of \(SU(2)\)
- half of highest weight is called the spin of the module
- Casimir operator can also detect this number.
- Casimir operator can also detect this number.
- spin \(1/2\) is the most important case since they are the matter particles
- this is why we have half-integral spin although those representation are integral highest weight representations.
operator formulation
- 파울리 행렬 (해밀턴의 사원수 참조)
\(\sigma_1 = \sigma_x = \begin{pmatrix} 0&1\\ 1&0 \end{pmatrix} \)
\(\sigma_2 = \sigma_y = \begin{pmatrix} 0&-i\\ i&0 \end{pmatrix} \)
\(\sigma_3 = \sigma_z = \begin{pmatrix} 1&0\\ 0&-1 \end{pmatrix}\) - raising and lowering 연산자
\(\sigma_{\pm}=\frac{1}{2}(\sigma_{x}\pm i\sigma_{y})\)
\(\sigma_{+}=\frac{1}{2}(\sigma_{x}+ i\sigma_{y})=\begin{pmatrix} 0&1\\ 0&0 \end{pmatrix}\)
\(\sigma_{-}=\frac{1}{2}(\sigma_{x}- i\sigma_{y})=\begin{pmatrix} 0&0\\ 1&0 \end{pmatrix}\)
\([\sigma_{z},\sigma_{\pm}]=\pm 2\sigma_{\pm}\)
sl(2)
- commutator
\([E,F]=H\)
\([H,E]=2E\)
\([H,F]=-2F\)
spin particle statstics
- Bosons
- photon
- vector boson
- Gluon
- follows Bose-Einstein statistics
- force-transmitting particles
- Fermions = spin- \(1/2\) particles
- quarks and leptons
- follows Fermi-Dirac statistics
-
matter particles
- quarks and leptons
history
encyclopedia
- http://en.wikipedia.org/wiki/
- http://www.scholarpedia.org/
- http://www.proofwiki.org/wiki/
- Princeton companion to mathematics(Companion_to_Mathematics.pdf)
books
- 2010년 books and articles
- http://gigapedia.info/1/
- http://gigapedia.info/1/
- http://www.amazon.com/s/ref=nb_ss_gw?url=search-alias%3Dstripbooks&field-keywords=
expositions
articles
- http://www.ams.org/mathscinet
- http://www.zentralblatt-math.org/zmath/en/
- http://arxiv.org/
- http://www.pdf-search.org/
- http://pythagoras0.springnote.com/
- http://math.berkeley.edu/~reb/papers/index.html
- http://dx.doi.org/
question and answers(Math Overflow)
blogs
- 구글 블로그 검색
- http://ncatlab.org/nlab/show/HomePage
experts on the field