Topological aspects of classical and quantum (2+1)-dimensional gravity 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, 1963- ソウダ, ジロウ

書誌事項

タイトル

Topological aspects of classical and quantum (2+1)-dimensional gravity

タイトル別名

古典及び量子(2+1)次元重力の位相的側面

著者名

早田, 次郎, 1963-

著者別名

ソウダ, ジロウ

学位授与大学

広島大学

取得学位

理学博士

学位授与番号

甲第831号

学位授与年月日

1990-03-26

注記・抄録

博士論文

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.

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

目次

  1. ABSTRACT / p3 (0005.jp2)
  2. CONTENTS / p4 (0006.jp2)
  3. 1 Introduction / p5 (0006.jp2)
  4. 2 ADM Canonical Formalism / p9 (0008.jp2)
  5. 3 York's Formalism / p13 (0010.jp2)
  6. 4 Evolution of the Geometry / p17 (0012.jp2)
  7. 5 Phase Space Reduction / p23 (0015.jp2)
  8. 6 Linearized Gravity / p27 (0017.jp2)
  9. 7 Mini-superspace / p31 (0019.jp2)
  10. 8 Quantum Gravity / p35 (0021.jp2)
  11. 9 Conclusion / p44 (0026.jp2)
  12. Appendix A / p46 (0027.jp2)
  13. Appendix B / p48 (0028.jp2)
  14. Appendix C / p54 (0031.jp2)
  15. COMMENT ON THE NON-RENORMALIZATION THEOREM IN THE FOUR-DIMENSIONAL SUPERSTRINGS / p73 (0036.jp2)
  16. Reducing the Huge Symmetry Occurring in the Compactification of a String / p1016 (0040.jp2)
  17. Kac Formulas for G/H Conformal Field Theories / p941 (0044.jp2)
  18. RENORMALIZATION GROUP FLOW AND OPEN STRING DYNAMICS / p1797 (0048.jp2)
  19. ABELIAN GAUGE THEORY IN TOPOLOGICALLY NON-TRIVIAL SPACE / p2539 (0054.jp2)
  20. Linearized Analysis of (2+1)-dimensional Einstein-Maxwell Theory / (0060.jp2)
  21. Teichmüller Motion of (2+1)-Dimensional Gravity with the Cosmological Constant / (0068.jp2)
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各種コード

  • NII論文ID(NAID)
    500000072700
  • NII著者ID(NRID)
    • 8000000991738
  • DOI(NDL)
  • 本文言語コード
    • eng
  • NDL書誌ID
    • 000000237014
  • データ提供元
    • 機関リポジトリ
    • NDL ONLINE
    • NDLデジタルコレクション
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