Topological Aspects of Classical and Quantum(2+1)-dimensional Gravity
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ID | 31751 |
本文ファイル | |
別タイトル | 古典及び量子(2+1)次元重力の位相的側面
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著者 |
早田 次郎
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NDC |
物理学
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抄録(英) | In order to understand (3+1)-dimensional gravity, (2+1)-dimensional gravity is studied as a toy model. Our emphasis is on its topological aspects, because (2+1)-dimensional gravity without matter fields has no local dynamical degrees of freedom. Starting from a review of the canonical ADM formalism and York's formalism for the initial value problem, we will solve the evolution equations of (2+1)-dimensional gravity with a cosmological constant in the case of g = 0 and g = 1, where g is the genus of Riemann surface. The dynamics of it is understood as the geodesic motion in the moduli space. This remarkable fact is the same with the case of (2+1)-dimensional pure gravity and seen more apparently from the action level. Indeed we will show the phase space reduction of (2+1)-dimensional gravity in the case of g = 1. For g ≥ 2, unfortunately we are not able to explicitly perform the phase space reduction of (2+1)-dimensional gravity due to the complexity of the Hamiltonian constraint equation. Based on this result, we will attempt to incorporate matter fields into (2+1)-dimensional pure gravity. The linearization and mini-superspace methods are used for this purpose. By using the linearization method, we conclude that the transverse-traceless part of the energy-momentum tensor affects the geodesic motion. In the case of the Einstein-Maxwell theory, we observe that the Wilson lines interact with the geometry to bend the geodesic motion. We analyze the mini-superspace naoclel of (2+1)-dimensional gravity with the matter fields in the case of g = 0 and y = 1. For g = 0, a wormhole solution is found but for g = 1 we can not find an analogous solution. Quantum gravity is also considered and we succeed to perform the phase space reduction of (2+1)-dimensional gravity in the case of g = 1 at the quantum level. From this analysis we argue that the conformal rotation is not necessary in the sense that the Euclidean quantum gravity is inappropriate for the full gravity.
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目次 | ABSTRACT / p3
CONTENTS / p4 1 Introduction / p5 2 ADM Canonical Formalism / p9 3 York's Formalism / p13 4 Evolution of the Geometry / p17 5 Phase Space Reduction / p23 6 Linearized Gravity / p27 7 Mini-superspace / p31 8 Quantum Gravity / p35 9 Conclusion / p44 Appendix A / p46 Appendix B / p48 Appendix C / p54 |
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言語 |
英語
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NII資源タイプ |
学位論文
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広大資料タイプ |
学位論文
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DCMIタイプ | text
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フォーマット | application/pdf
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著者版フラグ | ETD
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権利情報 | Copyright(c) by Author
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関連情報(references) | ・A. Hosoya and J. Soda, Mod. Phys. Lett. A4 (1989) 2539,
・J. Soda, to be published in Prog. Theor. Phys. Vol.83 No.4 (April),
・Y. Fujiwara and J. Soda, to be published in Frog. Theor. Phys. Vol.83 No.4 (April).
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関連情報URL(references) | http://dx.doi.org/10.1142/S0217732389002847
http://dx.doi.org/10.1143/PTP.83.805
http://dx.doi.org/10.1143/PTP.83.733
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学位記番号 | 甲第831号
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授与大学 | 広島大学(Hiroshima University)
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学位名 | 博士(理学)
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学位名の英名 | Physical Science
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学位の種類の英名 | doctoral
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学位授与年月日 | 1990-03-26
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部局名 |
理学研究科
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