"Electroweak theory"의 두 판 사이의 차이
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introduction==
recipe==
weak interactions==
consequences==
W-boson==
Z-boson==
weak force==
three classes of weak interactions==
Higgs mechanism==
encyclopedia==
articles==
imported>Pythagoras0 잔글 (찾아 바꾸기 – “</h5>” 문자열을 “==” 문자열로) |
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| 1번째 줄: | 1번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">introduction | + | <h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">introduction== |
* Glashow-Weinberg-Salam model<br> | * Glashow-Weinberg-Salam model<br> | ||
| 12번째 줄: | 12번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 2em;">recipe | + | <h5 style="margin: 0px; line-height: 2em;">recipe== |
* start with the local gauge symmetric SU(2) Lagrangian with massless gauge fields<br> | * start with the local gauge symmetric SU(2) Lagrangian with massless gauge fields<br> | ||
| 22번째 줄: | 22번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 2em;">adjoining U(1) symmetry | + | <h5 style="margin: 0px; line-height: 2em;">adjoining U(1) symmetry== |
<math>\begin{pmatrix}\gamma \\Z^0 \end{pmatrix} = \begin{pmatrix}\cos \theta_W & \sin \theta_W \\-\sin \theta_W & \cos \theta_W \end{pmatrix} \begin{pmatrix}B^0 \\W^0 \end{pmatrix} </math> | <math>\begin{pmatrix}\gamma \\Z^0 \end{pmatrix} = \begin{pmatrix}\cos \theta_W & \sin \theta_W \\-\sin \theta_W & \cos \theta_W \end{pmatrix} \begin{pmatrix}B^0 \\W^0 \end{pmatrix} </math> | ||
| 32번째 줄: | 32번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 2em;">weak interactions | + | <h5 style="margin: 0px; line-height: 2em;">weak interactions== |
* massive gauge bosons <br> | * massive gauge bosons <br> | ||
| 41번째 줄: | 41번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 2em;">consequences | + | <h5 style="margin: 0px; line-height: 2em;">consequences== |
* neutral currents<br> | * neutral currents<br> | ||
| 52번째 줄: | 52번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 2em;">W-boson | + | <h5 style="margin: 0px; line-height: 2em;">W-boson== |
* massive charged spin 1 boson<br> | * massive charged spin 1 boson<br> | ||
| 60번째 줄: | 60번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 2em;">Z-boson | + | <h5 style="margin: 0px; line-height: 2em;">Z-boson== |
* massive neutral spin 1 boson<br> | * massive neutral spin 1 boson<br> | ||
| 68번째 줄: | 68번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 2em;">weak force | + | <h5 style="margin: 0px; line-height: 2em;">weak force== |
* neutron beta decay<br> | * neutron beta decay<br> | ||
| 78번째 줄: | 78번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 2em;">three classes of weak interactions | + | <h5 style="margin: 0px; line-height: 2em;">three classes of weak interactions== |
* leptonic reactions<br> | * leptonic reactions<br> | ||
| 88번째 줄: | 88번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 2em;">Higgs mechanism | + | <h5 style="margin: 0px; line-height: 2em;">Higgs mechanism== |
* Higges field<br> | * Higges field<br> | ||
| 108번째 줄: | 108번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">related items | + | <h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">related items== |
| 114번째 줄: | 114번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">books | + | <h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">books== |
* [[2009년 books and articles|찾아볼 수학책]] | * [[2009년 books and articles|찾아볼 수학책]] | ||
| 127번째 줄: | 127번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">encyclopedia | + | <h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">encyclopedia== |
* http://en.wikipedia.org/wiki/Electroweak_interaction | * http://en.wikipedia.org/wiki/Electroweak_interaction | ||
| 141번째 줄: | 141번째 줄: | ||
| − | <h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">articles | + | <h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">articles== |
* [http://arxiv.org/abs/hep-ex/9606001 Why do we want a linear collider]<br> | * [http://arxiv.org/abs/hep-ex/9606001 Why do we want a linear collider]<br> | ||
** Hitoshi Murayama, 1996 | ** Hitoshi Murayama, 1996 | ||
2012년 10월 28일 (일) 15:26 판
introduction==
- Glashow-Weinberg-Salam model
- doublets of leptons and quarks => SU(2) symmetry
- W-boson mass causes some trouble
- Goldston boson
- Higgs mechanism
recipe==
- start with the local gauge symmetric SU(2) Lagrangian with massless gauge fields
- introduce the Higgs field
- break the local gauge symmetry in such a way by a new interaction between the Higgs field and gauge fields so as to generate terms in the Lagrangian that look like mass terms for gauge fields
adjoining U(1) symmetry== \(\begin{pmatrix}\gamma \\Z^0 \end{pmatrix} = \begin{pmatrix}\cos \theta_W & \sin \theta_W \\-\sin \theta_W & \cos \theta_W \end{pmatrix} \begin{pmatrix}B^0 \\W^0 \end{pmatrix} \)
weak interactions==
- massive gauge bosons
- W and Z bosons
- W and Z bosons
consequences==
- neutral currents
- new mesons
- parity violating effects
- W and Z bosons
W-boson==
- massive charged spin 1 boson
Z-boson==
- massive neutral spin 1 boson
weak force==
- neutron beta decay
- muon decay
- high-energy neutrino collisions with matter
three classes of weak interactions==
- leptonic reactions
- semi-leptonic reactions
- hadronic weak reactions
Higgs mechanism==
- Higges field
- pervasive universal background field that modifies the simple electroweak gauge theory as the gravitational field caused by mass
- two initial charged massless weak field W, W^{+}
- mix with Higgs fields H^{+}, H^{-}
- W fields get mass
- two electrically neutral massless fields W^0, G^0
- mix with neutral Higgs field H^0
- Z-field massive neutral weak field
- resulting bosons
- W - massive charged spin 1
- Z- massive neutral spin 1 boson
- photon - massless spin 1
- Higgs - massive neutral scalar spin 0
- pervasive universal background field that modifies the simple electroweak gauge theory as the gravitational field caused by mass
- mix with Higgs fields H^{+}, H^{-}
- W fields get mass
- mix with neutral Higgs field H^0
- Z-field massive neutral weak field
- W - massive charged spin 1
- Z- massive neutral spin 1 boson
- photon - massless spin 1
- Higgs - massive neutral scalar spin 0
related items==
books==
encyclopedia==
- http://en.wikipedia.org/wiki/Electroweak_interaction
- http://en.wikipedia.org/wiki/Quantum_electrodynamics
- http://en.wikipedia.org/wiki/Beta_decay
- http://en.wikipedia.org/wiki/weak_force
- http://en.wikipedia.org/wiki/
- http://en.wikipedia.org/wiki/
- Princeton companion to mathematics(Companion_to_Mathematics.pdf)
articles==
- Why do we want a linear collider
- Hitoshi Murayama, 1996
- Hitoshi Murayama, 1996