1. notice
  2. ไธญๆ–‡
  3. 1. feature
  4. ้€ป่พ‘
  5. 2. ้€ป่พ‘
  6. 3. ้›†ๅˆ่ฎบ
  7. 4. ๆ˜ ๅฐ„
  8. 5. ๅบ
  9. 6. ็ป„ๅˆ
  10. ๅพฎ็งฏๅˆ†
  11. 7. ๅฎžๆ•ฐ
  12. 8. ๆ•ฐๅˆ—ๆž้™
  13. 9. โ„^n
  14. 10. Euclidean ็ฉบ้—ด
  15. 11. Minkowski ็ฉบ้—ด
  16. 12. ๅคš้กนๅผ
  17. 13. ่งฃๆž (Euclidean)
  18. 14. ่งฃๆž (Minkowski)
  19. 15. ่งฃๆž struct ็š„ๆ“ไฝœ
  20. 16. ๅธธๅพฎๅˆ†ๆ–น็จ‹
  21. 17. ไฝ“็งฏ
  22. 18. ็งฏๅˆ†
  23. 19. ๆ•ฃๅบฆ
  24. 20. ็ฝ‘ๆž้™
  25. 21. ็ดง่‡ด
  26. 22. ่ฟž้€š
  27. 23. ๆ‹“ๆ‰‘ struct ็š„ๆ“ไฝœ
  28. 24. ๆŒ‡ๆ•ฐๅ‡ฝๆ•ฐ
  29. 25. ่ง’ๅบฆ
  30. ๅ‡ ไฝ•
  31. 26. ๆตๅฝข
  32. 27. ๅบฆ่ง„
  33. 28. ๅบฆ่ง„็š„่”็ปœ
  34. 29. Levi-Civita ๅฏผๆ•ฐ
  35. 30. ๅบฆ่ง„็š„ๆ›ฒ็އ
  36. 31. Einstein ๅบฆ่ง„
  37. 32. ๅธธๆˆช้ขๆ›ฒ็އ
  38. 33. simple-symmetric-space
  39. 34. ไธปไธ›
  40. 35. ็พคไฝœ็”จ
  41. 36. ็ƒๆžๆŠ•ๅฝฑ
  42. 37. Hopf ไธ›
  43. ๅœบ่ฎบ
  44. 38. ้ž็›ธๅฏน่ฎบ็‚น็ฒ’ๅญ
  45. 39. ็›ธๅฏน่ฎบ็‚น็ฒ’ๅญ
  46. 40. ็บฏ้‡ๅœบ
  47. 41. ็บฏ้‡ๅœบ็š„ๅฎˆๆ’ๆต
  48. 42. ้ž็›ธๅฏน่ฎบ็บฏ้‡ๅœบ
  49. 43. ๅ…‰้”ฅๅฐ„ๅฝฑ
  50. 44. ๆ—ถ็ฉบๅŠจ้‡็š„่‡ชๆ—‹่กจ็คบ
  51. 45. Lorentz ็พค
  52. 46. ๆ—‹้‡ๅœบ
  53. 47. ๆ—‹้‡ๅœบ็š„ๅฎˆๆ’ๆต
  54. 48. ็”ต็ฃๅœบ
  55. 49. ๅผ ้‡ๅœบ็š„ Laplacian
  56. 50. Einstein ๅบฆ่ง„
  57. 51. ็›ธไบ’ไฝœ็”จ
  58. 52. ่ฐๆŒฏๅญ้‡ๅญๅŒ–
  59. 53. ๆ—‹้‡ๅœบๆ‚้กน
  60. 54. ๅ‚่€ƒ
  61. English
  62. 55. notice
  63. 56. feature
  64. logic-topic
  65. 57. logic
  66. 58. set-theory
  67. 59. map
  68. 60. order
  69. 61. combinatorics
  70. calculus
  71. 62. real-numbers
  72. 63. limit-sequence
  73. 64. โ„^n
  74. 65. Euclidean-space
  75. 66. Minkowski-space
  76. 67. polynomial
  77. 68. analytic-Euclidean
  78. 69. analytic-Minkowski
  79. 70. analytic-struct-operation
  80. 71. ordinary-differential-equation
  81. 72. volume
  82. 73. integral
  83. 74. divergence
  84. 75. limit-net
  85. 76. compact
  86. 77. connected
  87. 78. topology-struct-operation
  88. 79. exponential
  89. 80. angle
  90. geometry
  91. 81. manifold
  92. 82. metric
  93. 83. metric-connection
  94. 84. geodesic-derivative
  95. 85. curvature-of-metric
  96. 86. Einstein-metric
  97. 87. constant-sectional-curvature
  98. 88. simple-symmetric-space
  99. 89. principal-bundle
  100. 90. group-action
  101. 91. stereographic-projection
  102. 92. Hopf-bundle
  103. field-theory
  104. 93. point-particle-non-relativity
  105. 94. point-particle-relativity
  106. 95. scalar-field
  107. 96. scalar-field-current
  108. 97. scalar-field-non-relativity
  109. 98. projective-lightcone
  110. 99. spacetime-momentum-spinor-representation
  111. 100. Lorentz-group
  112. 101. spinor-field
  113. 102. spinor-field-current
  114. 103. electromagnetic-field
  115. 104. Laplacian-of-tensor-field
  116. 105. Einstein-metric
  117. 106. interaction
  118. 107. harmonic-oscillator-quantization
  119. 108. spinor-field-misc
  120. 109. reference

note-math

[symmetric-space-locally] :=

Example quadratic manifold, simple-Lie-group and related symmetric-space

constant-sectional-curvature ==> symmetric-space

simple-Lie-group := Lie-algebra & Lie-bracket cannot decompose

Killing form := for in the tangent space at

Then define the metric at to be the metric at other places generated by the action, and it is bi-invariant i.e. both forms of group action give the same metric

Such a definition makes the group action an isometry of the Killing-form

Killing-form can also be defined for non-simple-Lie-groups

Question Motivation for the definition of Killing-form?

simple-Lie-group <==> Killing-form is non-degenerate

The Killing-form of simple-Lie-group and its symmetric-space is Einstein-metric

Proof for the case of simple-Lie-group

  • for Lie algebra

Proof

Lie-algebra ==> ฮด-isometry ==> for ฮด-group-action ,

Because the Killing-form is the metric generated by the group action, the Lie-derivative is zero

For fields generated by

  • geodesic-derivative . Proof see below

  • curvature

  • . hence symmetric-space-locally

  • curvature

  • sectional-curvature for orthonormal

  • Ricci-curvature . hence Einstein-metric

  • scalar-curvature

Prop at , similarly for fields generated by (bi-invariant)

Proof

Prop

This gives

with , this gives

Proof of

need

Since group action generates , constant value ==>

need

need

by

Question any more intuitive proof?

Prop for simple-Lie-group

Integral curves of bi-invariant vector fields generated by Lie algebra are Killing-form geodesics, because

  • Geodesics can be written as
  • Assume is an integral curve of ,

Quadratic form manifold. Symmetric group of is

  • orbit type or

    • induced metric signature (normal vector )
    • isotropy-group
    • quotient
    • isometry of is (isometry assumed to preserve direction)
  • orbit type or

    • induced metric signature (normal vector )
    • isotropy-group
    • quotient
    • isometry of is

Example

  • spatial manifold has

  • spacetime quadratic manifold has and hyperboloid of one sheet

Examples of quadratic manifolds with this property

simple-Lie-group , simple-Lie-group isotropy , orbit

Lie-algebra has orthogonal decomposition , not Lie bracket decomposition

is the Lie-algebra of , is the orthogonal complement

gives the coordinates of

The Killing-form of derives the Killing-form of and the Einstein metric of