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. convex_hull
  20. 16. volume
  21. 17. integral
  22. 18. divergence
  23. 19. limit_net
  24. 20. topology
  25. 21. compact
  26. 22. connected
  27. 23. topology_struct_operation
  28. 24. exponential
  29. 25. angle
  30. geometry
  31. 26. manifold
  32. 27. metric
  33. 28. metric_connection
  34. 29. geodesic_derivative
  35. 30. curvature_of_metric
  36. 31. Einstein_metric
  37. 32. constant_sectional_curvature
  38. 33. simple_symmetric_space
  39. 34. principal_bundle
  40. 35. group
  41. 36. stereographic_projection
  42. 37. Hopf_bundle
  43. field_theory
  44. 38. point_particle_non_relativity
  45. 39. point_particle_relativity
  46. 40. scalar_field
  47. 41. scalar_field_current
  48. 42. scalar_field_non_relativity
  49. 43. projective_lightcone
  50. 44. spacetime_momentum_spinor_representation
  51. 45. Lorentz_group
  52. 46. spinor_field
  53. 47. spinor_field_current
  54. 48. electromagnetic_field
  55. 49. Laplacian_of_tensor_field
  56. 50. Einstein_metric
  57. 51. interaction
  58. 52. harmonic_oscillator_quantization
  59. 53. spinor_field_misc
  60. 54. reference
  61. ไธญๆ–‡
  62. 55. notice
  63. ้€ป่พ‘
  64. 56. ้€ป่พ‘
  65. 57. ๅŸบ็ก€
  66. 58. ๆ˜ ๅฐ„
  67. 59. ๅบ
  68. 60. ็ป„ๅˆ
  69. ๅพฎ็งฏๅˆ†
  70. 61. ๅฎžๆ•ฐ
  71. 62. ๆ•ฐๅˆ—ๆž้™
  72. 63. ๅฏ้™คไปฃๆ•ฐ
  73. 64. Euclidean ็ฉบ้—ด
  74. 65. Minkowski ็ฉบ้—ด
  75. 66. ๅคš้กนๅผ
  76. 67. ่งฃๆž (Euclidean)
  77. 68. ่งฃๆž struct ็š„ๆ“ไฝœ
  78. 69. ๅธธๅพฎๅˆ†ๆ–น็จ‹
  79. 70. convex_hull
  80. 71. ไฝ“็งฏ
  81. 72. ็งฏๅˆ†
  82. 73. ๆ•ฃๅบฆ
  83. 74. ็ฝ‘ๆž้™
  84. 75. ๆ‹“ๆ‰‘
  85. 76. ็ดง่‡ด
  86. 77. ่ฟž้€š
  87. 78. ๆ‹“ๆ‰‘ struct ็š„ๆ“ไฝœ
  88. 79. ๆŒ‡ๆ•ฐๅ‡ฝๆ•ฐ
  89. 80. ่ง’ๅบฆ
  90. ๅ‡ ไฝ•
  91. 81. ๆตๅฝข
  92. 82. ๅบฆ่ง„
  93. 83. ๅบฆ่ง„็š„่”็ปœ
  94. 84. Levi_Civita ๅฏผๆ•ฐ
  95. 85. ๅบฆ่ง„็š„ๆ›ฒ็އ
  96. 86. Einstein ๅบฆ่ง„
  97. 87. ๅธธๆˆช้ขๆ›ฒ็އ
  98. 88. simple_symmetric_space
  99. 89. ไธปไธ›
  100. 90. ็พค
  101. 91. ็ƒๆžๆŠ•ๅฝฑ
  102. 92. Hopf ไธ›
  103. ๅœบ่ฎบ
  104. 93. ้ž็›ธๅฏน่ฎบ็‚น็ฒ’ๅญ
  105. 94. ็›ธๅฏน่ฎบ็‚น็ฒ’ๅญ
  106. 95. ็บฏ้‡ๅœบ
  107. 96. ็บฏ้‡ๅœบ็š„ๅฎˆๆ’ๆต
  108. 97. ้ž็›ธๅฏน่ฎบ็บฏ้‡ๅœบ
  109. 98. ๅ…‰้”ฅๅฐ„ๅฝฑ
  110. 99. ๆ—ถ็ฉบๅŠจ้‡็š„่‡ชๆ—‹่กจ็คบ
  111. 100. Lorentz ็พค
  112. 101. ๆ—‹้‡ๅœบ
  113. 102. ๆ—‹้‡ๅœบ็š„ๅฎˆๆ’ๆต
  114. 103. ็”ต็ฃๅœบ
  115. 104. ๅผ ้‡ๅœบ็š„ Laplacian
  116. 105. Einstein ๅบฆ่ง„
  117. 106. ็›ธไบ’ไฝœ็”จ
  118. 107. ่ฐๆŒฏๅญ้‡ๅญๅŒ–
  119. 108. ๆ—‹้‡ๅœบๆ‚้กน
  120. 109. ๅ‚่€ƒ

note-math

In flat spaces, linear and affine are often mixed. Similarly, in flat spaces, polynomials are also like this. Zero-order polynomials correspond to the base point in affine.

First, handle the one-dimensional real case.

exponential power function

[polynomial_function_1d] Polynomial functions are finite linear combinations of power functions. (Affine) base point , (vector) offset

The representation of a polynomial function is not affine invariant, i.e., switching the base point yields a representation of the same degree but with different coefficients. Scaling is also like this.

[change_base_point_polynomial] Switching base point

Then

Proof Expand and compute, compare the coefficients of to get the expression for . Use the commutativity of summation to collect power function terms.

If using as the base point in coordinates and changing the symbol , then the polynomial function is expressed as

Generalizing from polynomials as finite linear combinations to countably infinite linear combinations, called exponential power series of functions.

Some functions are not defined directly from exponential power series. Example can be defined directly through division, without needing to use power series for definition.

Besides as countable infinite data, can also be used.

Changing the exponential power function to the exponential power function introduces new aspects that require attention.

  • requires a multiplicative inverse.

  • requires solving the equation and addressing the issue of whether the solution is unique.

  • is unbounded at .

  • When , repeated differentiation does not terminate .

For now, we only deal with power series, abbreviated as power series.

Now handle the higher-dimensional case i.e. .

If the codomain is , we can additionally define function multiplication and multiplicative inverse .

First, attempt to base the definitions of polynomial functions and power series on tensors i.e. multilinearity.

If not necessary, there is no need to take the linear direct sum for tensors of all orders (known as the tensor algebra) for now.

[polynomial_function] Using codomain and multilinear functions . Base point , offset , define polynomial function

Affine transformations, i.e., changing the base point i.e. translation, or linear transformations i.e. (including scaling), do not change the degree of the polynomial.

may not be collinear.

Generalization to is straightforward. For the cases of , due to non-commutativity and non-associativity, it becomes very troublesome.

There may be different tensors that give the same polynomial, but a polynomial corresponds to a unique symmetric tensor .

Change notation.

  • [power_tensor]

Using difference techniques, one can recover the -th order symmetric tensor from the -th order monomial or power tensor .

In the -th order monomial of , there is a term , but there are many other interfering terms.

The entire problem is symmetric in , so a symmetric construction should be used.

In second order

[difference_symmetric_tensor] Symmetric tensor th order difference

Question Is there an intuitive understanding of th order difference?

[successive_difference] th order difference can be written as successive first-order differences

where , ,

Due to the commutativity of summation, the order of successive differences does not affect the final result

Proof of difference_symmetric_tensor

Fully expand

A function can be viewed as a function . Thus

Define weight

Prop For any non-empty finite set ,

Proof

All can be classified according to , each corresponds to choices (combination). Thus

for

define

define

There is a bijection

Weight

Final condition

  • When , it always holds for all
  • When , it fails only when is a bijection i.e. is all th order permutations, then

    • and

Symmetric tensors make

Remaining

There are permutations of order

So the result is

The symmetry of a symmetric multilinear function allows the property of difference to be inherited

[difference_polynomial] The -th order difference of is

The -th order difference of is

From this we obtain

Prop A polynomial function determines its symmetric multilinear function representation

Proof Suppose polynomial has two symmetric multilinear function representations

First, the -th order difference gives the same . Simultaneously removing the -th order term yields a polynomial of degree and its two symmetric multilinear representations . Induction on yields the conclusion

For power series, finite-order differences can never yield zero

Formally, division and limits can be used to eliminate higher-order terms