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

[integral-piecewise-constant-function]

constant function support on simplex + countable infinite combination + absolutely convergent

[integral-simplicial-function]

Or use continuous piecewise affine linear or simplicial function e.g. for simplex with vertices , . The integral is defined as the average of the values according to the vertices i.e. the result of the affine center mapping

According to the decomposition of simplex intersection and subtraction, the finite addition and subtraction of piecewise constant functions is still a piecewise constant function

Define the integral distance . Or use norm

[Lebesgue-integrable]

:= there exist piecewise constant functions such that and

Similarly for

In the piecewise constant space, similar to the definition of measurable sets, for integral distance, triangle inequality, the limit is unique

[Lebesgue-integral]

So that we can define and

Example But it should be noted that, although the integral distance Cauchy net is always integrally convergent, there exists an integral distance Cauchy net that does not converge pointwise to the limit function

The bisection walk sequence is Cauchy in integral distance, and the measure tends to

It does not follow the definition of pointwise convergence

Although conceptually it converges to the empty set

[integrable-exist-subnet-almost-everywhere-pointwise-convergence] (ref-5, p.129โ€“130)

But for all integral distances, there exists a subnet in the Cauchy net that converges almost everywhere pointwise to the target integrable function. This comes from the fact that there exists a set with arbitrarily small measure such that it converges absolutely and uniformly on

The measurable set defined by L^1,L^2 is a Lebesgue measurable set, which may be disconnected

What we define is absolutely integrable. Other integral operations, such as , are special limit operations based on absolute integrability, and are related to the environment of the problem

The linear change of coordinates gives the integral change of variable formula formula

[integral-on-form] For the integral over an -region, integrating a function over a volume is equivalent to integrating an -form. If considered as an integral of an -form, then the integral is invariant.

[integral-change-of-variable-formula]

let almost everywhere analytic

The change of variable formula formula for diffeomorphisms of integrals is or

The differential of the coordinate transformation map at each simplex center as an affine map acting on the domain simplex is used to obtain the range space simplex for approximation, then use (high order) mean-value-theorem-analytic, then take partition limit (ref-12, p.92โ€“99)

It is necessary to first perform compact uniform control on the bounded region for the approximation of the differential mean value theorem

Then the unbounded region is a countable approximation from the bounded region, using the technique

If it is considered as integrating an form, (cf. integral-on-form) then the integral change of variable formula is equivalent to form integration is diffeomorphism invariant

[integral-on-manfold] Question

According to the change of variable formula, the integral of form in the coordinates on the manifold is invariant (cf. integral-on-form)

But what if we want to integrate the form defined on the entire orientable manifold?

One way is, similar to the proof of integral-change-of-variable-formula, in coordinate, linear approximation + compact uniformly control + partition limit, then use countable cover to approximate entire manifold

In order to define the integral, some kind of countability assumption is needed. The simplest assumption is that the manifold can be covered by countable coordinate cards. Let's use this assumption

Now the problem is that the integral at the intersection of the coordinate cards is repeated and needs to be removed

I will not use measurable sets being closed under intersection and set-minus, nor use curved simplex (box) type region partition alias triangulation, which is even more difficult to proof

Instead, I will use the linear approximation version of triangulation. Under linear approximation, simplex is closed under intersection and set-minus (polyhedra decompose to to simplex)

e.g. the differential of the transition map at each simplex (box) center as an affine-map-point-ver (linear-map) to transform the simplex (box) to the simplex of the coordinate region . Then the intersection and reduction of the simplex (box) can be decomposed into the simplex (box) again.

Taking the limit of this approximation, require style absolute convergence, gives the integral on the manifold

Prove that the result does not depend on the choice of coordinate system and linear approximation method

The measures and integrals defined by rectangles and simplexes (without fixed coordinate axes) are equivalent, because rectangles and simplexes can be countably approximated to each other

[Fubini-theorem]

Because the piecewise constant value of the rectangular region is product decomposable, and then use the absolutely convergent upper bound to control it

Fubini theorem 2 โ€ฆ (ref-5)

Fubini's theorem can be used to prove that the volume calculation below the graph of a function is the integral of the height function with respect to the volume of the base

Example polar coordinate, 2d, 3d, hyperbolic โ€ฆ

area coarea formula โ€ฆ

[low-dim-integral]

The integral of a form over a -simplex is also invariant, and there's no need to define volume for lower-dimensional simplices.

constant-type form

simplicial map type form := Let be the vertices of the simplex, then

Similar to the -order case, the integral of a simplicial map form on a -chain is defined as

Even if two -simplices are adjacent, their orientations might be discontinuous. This is different from the -order case, where the codimension is zero, so all -simplices have the same orientation.

Two adjacent -simplices share common vertices, and the form acting on these points might have different values. The integral of a simplicial type form is also equivalent to taking the average of the directions at the vertices.

A good approximation would require the -directions to have good regularity, but without additional structure, it seems difficult to define such a concept (even for a Grassmann manifold?).

submanifold structure can simply eliminate this -direction discontinuity.

[integral-on-submanfold]

let be dimension manifold, form restrict to orientable submanifold tangent space

form in is equivalent to scalar function, but how to control form by integral? try ?

if unnecessary, do not introduce metric to define or now