Chiral symmetry breaking in lattice gauge theory격자게이지 이론에서의 카이랄 대칭성 파탄
| DC Field | Value | Language |
|---|---|---|
| dc.contributor.advisor | Kim, Jae-Kwan | - |
| dc.contributor.advisor | 김재관 | - |
| dc.contributor.author | Jung, Dae-Yong | - |
| dc.contributor.author | 정대용 | - |
| dc.date.accessioned | 2011-12-14T07:48:24Z | - |
| dc.date.available | 2011-12-14T07:48:24Z | - |
| dc.date.issued | 1984 | - |
| dc.identifier.uri | http://library.kaist.ac.kr/search/detail/view.do?bibCtrlNo=64027&flag=dissertation | - |
| dc.identifier.uri | http://hdl.handle.net/10203/48066 | - |
| dc.description | 학위논문(석사) - 한국과학기술원 : 물리학과, 1984.2, [ [iii], 47 p. ] | - |
| dc.description.abstract | In the lattice gauge theory, chiral symmetry is naturally spontaneously broken. So we have studied it. After reviewing the lattice gauge theory in the hamiltonian one learn the lattice fermion with species doubling. The species doubling means that lattice fermion always appears a pair with zero net chirality. We have studied Susskind fermion. The chiral symmetry breaking is appeared naturally. Finally, we have studied chiral symmetry breaking in ``naive`` fermion for one color and one flavor. The result is as follow: 1. Chiral symmetry is spontaneously broken. 2. The pseudoscala, pseudoGoldstone particles correspond to antiferromagnetic spin wave excitation of the fermion vacuum. 3. m$^2$ pseudo-Goldstone $\propto$ m fermion $<\bar{4} 4>$ | eng |
| dc.language | eng | - |
| dc.publisher | 한국과학기술원 | - |
| dc.title | Chiral symmetry breaking in lattice gauge theory | - |
| dc.title.alternative | 격자게이지 이론에서의 카이랄 대칭성 파탄 | - |
| dc.type | Thesis(Master) | - |
| dc.identifier.CNRN | 64027/325007 | - |
| dc.description.department | 한국과학기술원 : 물리학과, | - |
| dc.identifier.uid | 000821283 | - |
| dc.contributor.localauthor | Jung, Dae-Yong | - |
| dc.contributor.localauthor | 정대용 | - |
- Appears in Collection
- PH-Theses_Master(석사논문)
- Files in This Item
- There are no files associated with this item.
Items in DSpace are protected by copyright, with all rights reserved, unless otherwise indicated.