"Spin system and Pauli exclusion principle"의 두 판 사이의 차이
둘러보기로 가기
검색하러 가기
Pythagoras0 (토론 | 기여) |
|||
(사용자 3명의 중간 판 29개는 보이지 않습니다) | |||
1번째 줄: | 1번째 줄: | ||
− | < | + | ==introduction== |
+ | * {{수학노트|url=스핀과_파울리의_배타원리}} | ||
+ | * the simplest example of quantum mechanical system | ||
+ | * quantization of the angular momentum | ||
+ | * measures as being some multiple of Planck's constant divided by <math>2\pi</math> | ||
− | |||
− | |||
− | |||
− | + | ==evolution of Pauli exclusion principle== | |
+ | * originated from atomic spectroscopy | ||
+ | * Dirac-antisymmetrizing the wave function for an assembly of indistinguishable particles | ||
+ | * Pauli's spin matrices | ||
+ | * anti-commutation relations for particle creation and annihilation operators in quantum field theory | ||
− | |||
− | |||
− | + | ==representation theory== | |
+ | * concept from the representation of <math>SU(2)</math> | ||
+ | * half of highest weight is called the spin of the module | ||
+ | ** Casimir operator can also detect this number. | ||
+ | * spin <math>1/2</math> 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. | ||
− | + | ||
− | + | ||
− | + | ==spin particle statstics== | |
− | + | * Bosons | |
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | * | ||
** photon | ** photon | ||
** vector boson | ** vector boson | ||
53번째 줄: | 32번째 줄: | ||
** follows Bose-Einstein statistics | ** follows Bose-Einstein statistics | ||
** force-transmitting particles | ** force-transmitting particles | ||
− | * | + | * Fermions = spin- <math>1/2</math> particles |
− | ** | + | ** quarks and leptons |
− | ** | + | ** follows Fermi-Dirac statistics |
− | ** | + | ** matter particles |
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | + | ==Dirac wave equation== | |
− | + | * [[Dirac equation]] | |
− | |||
− | * | + | ==related items== |
+ | * [[The Story of Spin by Tomonaga]] | ||
+ | |||
− | + | [[분류:개인노트]] | |
+ | [[분류:physics]] | ||
+ | [[분류:math and physics]] | ||
− | + | == articles == | |
− | + | * Enrico Santamato, Francesco De Martini, Weyl-gauge invariant proof of the Spin-Statistics Theorem, arXiv:1604.06253 [quant-ph], April 21 2016, http://arxiv.org/abs/1604.06253 | |
+ | [[분류:migrate]] | ||
− | * [ | + | ==메타데이터== |
− | * [ | + | ===위키데이터=== |
− | * [ | + | * ID : [https://www.wikidata.org/wiki/Q131594 Q131594] |
− | * | + | ===Spacy 패턴 목록=== |
+ | * [{'LOWER': 'pauli'}, {'LOWER': 'exclusion'}, {'LEMMA': 'principle'}] | ||
+ | * [{'LOWER': 'exclusion'}, {'LOWER': 'principle'}, {'OP': '*'}, {'LOWER': 'physics'}, {'LEMMA': ')'}] | ||
+ | * [{'LOWER': 'principle'}, {'LOWER': 'of'}, {'LOWER': 'exclusion'}, {'OP': '*'}, {'LOWER': 'quantum'}, {'LOWER': 'mechanics'}, {'LEMMA': ')'}] | ||
+ | * [{'LOWER': 'exclusion'}, {'LOWER': 'principle'}, {'OP': '*'}, {'LOWER': 'fermi'}, {'OP': '*'}, {'LOWER': 'dirac'}, {'LOWER': 'statistics'}, {'LEMMA': ')'}] |
2021년 2월 17일 (수) 01:24 기준 최신판
introduction
- 틀:수학노트
- the simplest example of quantum mechanical system
- quantization of the angular momentum
- measures as being some multiple of Planck's constant divided by \(2\pi\)
evolution of Pauli exclusion principle
- originated from atomic spectroscopy
- Dirac-antisymmetrizing the wave function for an assembly of indistinguishable particles
- Pauli's spin matrices
- anti-commutation relations for particle creation and annihilation operators in quantum field theory
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.
- 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.
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
Dirac wave equation
articles
- Enrico Santamato, Francesco De Martini, Weyl-gauge invariant proof of the Spin-Statistics Theorem, arXiv:1604.06253 [quant-ph], April 21 2016, http://arxiv.org/abs/1604.06253
메타데이터
위키데이터
- ID : Q131594
Spacy 패턴 목록
- [{'LOWER': 'pauli'}, {'LOWER': 'exclusion'}, {'LEMMA': 'principle'}]
- [{'LOWER': 'exclusion'}, {'LOWER': 'principle'}, {'OP': '*'}, {'LOWER': 'physics'}, {'LEMMA': ')'}]
- [{'LOWER': 'principle'}, {'LOWER': 'of'}, {'LOWER': 'exclusion'}, {'OP': '*'}, {'LOWER': 'quantum'}, {'LOWER': 'mechanics'}, {'LEMMA': ')'}]
- [{'LOWER': 'exclusion'}, {'LOWER': 'principle'}, {'OP': '*'}, {'LOWER': 'fermi'}, {'OP': '*'}, {'LOWER': 'dirac'}, {'LOWER': 'statistics'}, {'LEMMA': ')'}]