"Electroweak theory"의 두 판 사이의 차이
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* Goldston boson<br> | * Goldston boson<br> | ||
* Higgs mechanism<br> | * Higgs mechanism<br> | ||
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| + | <h5 style="margin: 0px; line-height: 2em;">weak interactions</h5> | ||
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| + | * massive gauge bosons <br> | ||
| + | ** W and Z bosons<br> | ||
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* massive neutral spin 1 boson<br> | * massive neutral spin 1 boson<br> | ||
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<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> | <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> | ||
| − | * | + | * [http://arxiv.org/abs/hep-ex/9606001 Why do we want a linear collider]<br> |
| − | + | ** Hitoshi Murayama, 1996 | |
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2011년 1월 17일 (월) 08:02 판
introduction
- Glashow-Weinberg-Salam model
- W-boson mass causes some trouble
- Goldston boson
- Higgs mechanism
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
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
- 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
- mix with Higgs fields H^{+}, H^{-}
- two electrically neutral massless fields W^0, G^0
- mix with neutral Higgs field H^0
- Z-field massive neutral weak field
- mix with neutral Higgs field H^0
- resulting bosons
- W - massive charged spin 1
- Z- massive neutral spin 1 boson
- photon - massless spin 1
- Higgs - massive neutral scalar spin 0
- W - massive charged spin 1
books
- 찾아볼 수학책
- http://gigapedia.info/1/
- http://gigapedia.info/1/
- http://gigapedia.info/1/
- http://gigapedia.info/1/
- http://www.amazon.com/s/ref=nb_ss_gw?url=search-alias%3Dstripbooks&field-keywords=
encyclopedia
- 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/Electroweak_interaction
- 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