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21: 5.6 Inequalities
22: 9.17 Methods of Computation
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►Although the Maclaurin-series expansions of §§9.4 and 9.12(vi) converge for all finite values of , they are cumbersome to use when is large owing to slowness of convergence and cancellation.
For large the asymptotic expansions of §§9.7 and 9.12(viii) should be used instead.
Since these expansions diverge, the accuracy they yield is limited by the magnitude of .
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►In the case of , for example, this means that in the sectors we may integrate along outward rays from the origin with initial values obtained from §9.2(ii).
But when the integration has to be towards the origin, with starting values of and computed from their asymptotic expansions.
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23: 36.5 Stokes Sets
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►For , there are two solutions , provided that .
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►The second sheet corresponds to and it intersects the bifurcation set (§36.4) smoothly along the line generated by , .
For the second sheet is generated by a second solution of (36.5.6)–(36.5.9), and for it is generated by the roots of the polynomial equation
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►the intersection lines with the bifurcation set are generated by , .
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►Alternatively, when
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24: 10.40 Asymptotic Expansions for Large Argument
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►as in .
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►as in .
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►Then the remainder term does not exceed the first neglected term in absolute value and has the same sign provided that .
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►where denotes the variational operator (§2.3(i)), and the paths of variation are subject to the condition that changes monotonically.
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►If with bounded and
fixed, then
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25: 6.3 Graphics
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26: 25.14 Lerch’s Transcendent
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►
25.14.1
; .
►If is not an integer then ; if is a positive integer then ; if is a non-positive integer then can be any complex number.
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25.14.3
, .
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25.14.6
if ;
, if .
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