| 1.15.1 | |||
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ⓘ
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| 1.15.2 | |||
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ⓘ
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if
| 1.15.3 | |||
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ⓘ
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| 1.15.4 | |||
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ⓘ
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if
| 1.15.5 | |||
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ⓘ
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For ,
| 1.15.6 | |||
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ⓘ
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if
| 1.15.7 | |||
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ⓘ
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| 1.15.8 | |||
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ⓘ
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if
| 1.15.9 | |||
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ⓘ
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Methods of summation are regular if they are consistent with conventional summation. All of the methods described in §1.15(i) are regular. For example if
| 1.15.10 | |||
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ⓘ
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then
| 1.15.11 | |||
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ⓘ
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| 1.15.12 | |||
| , | |||
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ⓘ
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| 1.15.13 | |||
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ⓘ
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As
| 1.15.14 | |||
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ⓘ
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uniformly for . (Here and elsewhere in this subsection is a constant such that .)
For ,
| 1.15.15 | |||
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ⓘ
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| 1.15.16 | |||
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ⓘ
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As
| 1.15.17 | |||
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ⓘ
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uniformly for .
| 1.15.18 | |||
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ⓘ
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where
| 1.15.19 | |||
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ⓘ
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is a harmonic function in polar coordinates (1.9.27), and
| 1.15.20 | |||
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ⓘ
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Let
| 1.15.21 | |||
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ⓘ
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, where
| 1.15.22 | |||
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ⓘ
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Then
| 1.15.23 | |||
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ⓘ
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If is periodic and integrable on , then as the Abel means and the (C,1) means converge to
| 1.15.24 | |||
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ⓘ
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at every point where both limits exist. If is also continuous, then the convergence is uniform for all .
For real-valued , if
| 1.15.25 | |||
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ⓘ
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is the Fourier series of , then the series
| 1.15.26 | |||
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ⓘ
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can be extended to the interior of the unit circle as an analytic function
| 1.15.27 | |||
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ⓘ
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Here is the Abel (or Poisson) sum of , and has the series representation
| 1.15.28 | |||
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ⓘ
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compare §1.15(v).
is Abel summable to , or
| 1.15.29 | |||
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ⓘ
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when
| 1.15.30 | |||
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ⓘ
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is (C,1) summable to , or
| 1.15.31 | |||
|
ⓘ
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when
| 1.15.32 | |||
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ⓘ
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If converges and equals , then the integral is Abel and Cesàro summable to .
| 1.15.33 | |||
| , . | |||
| 1.15.34 | |||
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ⓘ
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For each ,
| 1.15.35 | |||
| as . | |||
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ⓘ
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Let
| 1.15.36 | |||
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ⓘ
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where is the Fourier transform of (§1.14(i)). Then
| 1.15.37 | |||
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ⓘ
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is the Poisson integral of .
If is integrable on , then
| 1.15.38 | |||
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ⓘ
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Suppose now is real-valued and integrable on . Let
| 1.15.39 | |||
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ⓘ
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where and . Then is an analytic function in the upper half-plane and its real part is the Poisson integral ; compare (1.9.34). The imaginary part
| 1.15.40 | |||
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ⓘ
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is the conjugate Poisson integral of . Moreover, is the Hilbert transform of (§1.14(v)).
| 1.15.41 | |||
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ⓘ
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| 1.15.42 | |||
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ⓘ
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For each ,
| 1.15.43 | |||
| as . | |||
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ⓘ
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Let
| 1.15.44 | ||||
|
ⓘ
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| then | ||||
| 1.15.45 | ||||
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ⓘ
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If is integrable on , then
| 1.15.46 | |||
|
ⓘ
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Suggested 2017-04-22 by Tom Koornwinder
Reported 2010-10-18 by Andreas Kurt Richter
For and , the Riemann-Liouville fractional integral of order is defined by
| 1.15.47 | |||
|
ⓘ
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For see §5.2, and compare (1.4.31) in the case when is a positive integer.
| 1.15.48 | |||
| , . | |||
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ⓘ
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If
| 1.15.49 | |||
then
| 1.15.50 | |||
|
ⓘ
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Reported 2010-10-18 by Andreas Kurt Richter
For , an integer, and , the fractional derivative of order is defined by
| 1.15.51 | |||
|
ⓘ
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and satisfies the property
| 1.15.52 | |||
| . | |||
|
ⓘ
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When none of , , and is an integer
| 1.15.53 | |||
|
ⓘ
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Note that . See also Love (1972b).
If
| 1.15.54 | ||||
| , | ||||
| , , | ||||
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ⓘ
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then
| 1.15.55 | |||
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ⓘ
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If
| 1.15.56 | |||
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ⓘ
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and either or , then
| 1.15.57 | |||
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ⓘ
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