DΕΎrbasjan sum
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1: 26.10 Integer Partitions: Other Restrictions
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βΊ
denotes the number of partitions of into distinct parts.
denotes the number of partitions of into at most distinct parts.
denotes the number of partitions of into parts with difference at least .
…If more than one restriction applies, then the restrictions are separated by commas, for example, .
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βΊNote that , with strict inequality for .
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2: 28.25 Asymptotic Expansions for Large
3: 1.10 Functions of a Complex Variable
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βΊLet be a bounded domain with boundary and let .
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βΊIf is harmonic in , , and for all , then is constant in .
Moreover, if is bounded and is continuous on and harmonic in , then is maximum at some point on .
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βΊLet be a multivalued function and be a domain.
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βΊSuppose is a domain, and
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4: 19.21 Connection Formulas
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βΊThe complete case of can be expressed in terms of and :
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βΊ
is symmetric only in and , but either (nonzero) or (nonzero) can be moved to the third position by using
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βΊ
19.21.8
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βΊBecause is completely symmetric, can be permuted on the right-hand side of (19.21.10) so that if the variables are real, thereby avoiding cancellations when is calculated from and (see §19.36(i)).
βΊ
19.21.11
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5: 26.6 Other Lattice Path Numbers
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βΊ
Delannoy Number
βΊ is the number of paths from to that are composed of directed line segments of the form , , or . βΊ
26.6.1
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βΊ
26.6.5
βΊ
26.6.6
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6: 29.15 Fourier Series and Chebyshev Series
7: 1.16 Distributions
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βΊWe denote it by .
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βΊfor all .
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βΊFor any locally integrable function , its distributional derivative is .
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βΊThe distributional derivative
of is defined by
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8: 29.6 Fourier Series
9: 1.11 Zeros of Polynomials
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βΊ
βΊThe sum and product of the roots are respectively and .
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βΊLet
βΊ
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βΊThen , with , is stable iff ; , ; , .
10: 10.20 Uniform Asymptotic Expansions for Large Order
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βΊIn the following formulas for the coefficients , , , and , , are the constants defined in §9.7(i), and , are the polynomials in of degree defined in §10.41(ii).
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βΊNote: Another way of arranging the above formulas for the coefficients , and would be by analogy with (12.10.42) and (12.10.46).
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βΊEach of the coefficients , , , and , , is real and infinitely differentiable on the interval .
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βΊFor numerical tables of , and , , , and see Olver (1962, pp. 28–42).
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βΊThe equations of the curved boundaries and in the -plane are given parametrically by
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