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

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, e.g. the manifold can be covered by countable coordinate cards

The integral at the intersection of the coordinate cards is repeated and needs to be removed

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)

Fubiniโ€™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 thereโ€™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