Basic Concepts of Eletroweak Theory

碩士 === 淡江大學 === 物理學系 === 83 === Electroweak Theory involves two parts: weak interaction and electromagnetic interaction. In chapter 1, introducing the prototype quantum-field theory: QED, and some simple weak interaction processes, and the mesons W and Z0 appear. Chapter 2 discussing the s...

Full description

Bibliographic Details
Main Authors: Wu, Cheng-Ping, 吳俊平
Other Authors: Chen, Wei-Yau
Format: Others
Language:zh-TW
Published: 1995
Online Access:http://ndltd.ncl.edu.tw/handle/81060694249440970750
id ndltd-TW-083TKU03198006
record_format oai_dc
spelling ndltd-TW-083TKU031980062016-07-15T04:12:56Z http://ndltd.ncl.edu.tw/handle/81060694249440970750 Basic Concepts of Eletroweak Theory 弱電理論的基本概念 Wu, Cheng-Ping 吳俊平 碩士 淡江大學 物理學系 83 Electroweak Theory involves two parts: weak interaction and electromagnetic interaction. In chapter 1, introducing the prototype quantum-field theory: QED, and some simple weak interaction processes, and the mesons W and Z0 appear. Chapter 2 discussing the spontaneously syrnnetry breakint. There are three examples in this chapter: simplest example, Goldstone Boson and Higgs Mechanics. By these examples, we can know how symmetry is broken and what will appear. Finally, introducing the stand model of electroweak theory. By choosing apporpriate gauge groups, SU(2) and U(1), we can see how the weak and electromagnetic interactions are unified, and understand the masses about W and Z0 particles. Chen, Wei-Yau 陳惟堯 1995 學位論文 ; thesis 27 zh-TW
collection NDLTD
language zh-TW
format Others
sources NDLTD
description 碩士 === 淡江大學 === 物理學系 === 83 === Electroweak Theory involves two parts: weak interaction and electromagnetic interaction. In chapter 1, introducing the prototype quantum-field theory: QED, and some simple weak interaction processes, and the mesons W and Z0 appear. Chapter 2 discussing the spontaneously syrnnetry breakint. There are three examples in this chapter: simplest example, Goldstone Boson and Higgs Mechanics. By these examples, we can know how symmetry is broken and what will appear. Finally, introducing the stand model of electroweak theory. By choosing apporpriate gauge groups, SU(2) and U(1), we can see how the weak and electromagnetic interactions are unified, and understand the masses about W and Z0 particles.
author2 Chen, Wei-Yau
author_facet Chen, Wei-Yau
Wu, Cheng-Ping
吳俊平
author Wu, Cheng-Ping
吳俊平
spellingShingle Wu, Cheng-Ping
吳俊平
Basic Concepts of Eletroweak Theory
author_sort Wu, Cheng-Ping
title Basic Concepts of Eletroweak Theory
title_short Basic Concepts of Eletroweak Theory
title_full Basic Concepts of Eletroweak Theory
title_fullStr Basic Concepts of Eletroweak Theory
title_full_unstemmed Basic Concepts of Eletroweak Theory
title_sort basic concepts of eletroweak theory
publishDate 1995
url http://ndltd.ncl.edu.tw/handle/81060694249440970750
work_keys_str_mv AT wuchengping basicconceptsofeletroweaktheory
AT wújùnpíng basicconceptsofeletroweaktheory
AT wuchengping ruòdiànlǐlùndejīběngàiniàn
AT wújùnpíng ruòdiànlǐlùndejīběngàiniàn
_version_ 1718348985260834816