§5.10 Continued Fractions§5.12 Beta Function

§ 5.11. Asymptotic Expansions

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Contents

§ 5.11(i). Poincaré-Type Expansions

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Notes:
See Olver (1997b, pp. 87–88 and 293–295) for (5.11.1)–(5.11.3), (5.11.5)–(5.11.6), and (5.11.8). (5.11.7) and (5.11.9) are derived from (5.11.3).
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As z\to\infty in the sector |\mathrm{ph}z|\le\pi-\delta\;(<\pi),

5.11.1 \ln\Gamma\!\left(z\right)\sim\left(z-\tfrac{1}{2}\right)\ln z-z+\tfrac{1}{2}\ln\!\left(2\pi\right)+\sum _{{k=1}}^{\infty}\frac{B_{{2k}}}{2k(2k-1)z^{{2k-1}}}
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Symbols:
\Gamma\!\left(z\right): Gamma function, \sim: asymptotically equal, k: nonnegative integer and z: complex variable
A&S Ref:
6.1.40
Referenced by:
§5.11(i), §5.11(i), §5.11(ii), §5.11(ii)
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and

5.11.2 \psi\!\left(z\right)\sim\ln z-\frac{1}{2z}-\sum _{{k=1}}^{\infty}\frac{B_{{2k}}}{2kz^{{2k}}}.
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Symbols:
\psi\!\left(z\right): Psi or digamma function, \sim: asymptotically equal, k: nonnegative integer and z: complex variable
A&S Ref:
6.3.18
Referenced by:
§5.11(ii), §5.4(iii)
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For the Bernoulli numbers B_{{2k}}, see §Ch.24.

With the same conditions,

5.11.3 \Gamma\!\left(z\right)\sim e^{{-z}}z^{z}\left(\frac{2\pi}{z}\right)^{{1/2}}\left(\sum _{{k=0}}^{\infty}\frac{g_{k}}{z^{k}}\right),
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Defines:
g_{k}: coefficients
Symbols:
\Gamma\!\left(z\right): Gamma function, \sim: asymptotically equal, k: nonnegative integer and z: complex variable
A&S Ref:
6.1.37
Referenced by:
§5.11(i), §5.11(i), §5.11(ii), §5.11(ii), §5.21
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where

5.11.4
g_{0}=1,
g_{1}=\tfrac{1}{12},
g_{2}=\tfrac{1}{288},
g_{3}=-\tfrac{139}{51840},
g_{4}=-\tfrac{571}{24\; 88320},
g_{5}=\tfrac{1\; 63879}{2090\; 18880},
g_{6}=\tfrac{52\; 46819}{7\; 52467\; 96800}.
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Defines:
g_{k}: coefficients
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Also,

5.11.5 g_{k}=\sqrt{2}\left(\tfrac{1}{2}\right)_{{k}}a_{{2k}},
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Defines:
g_{k}: coefficients and a_{k}: coefficient
Symbols:
\left(a\right)_{{n}}: Pochhammer's symbol and k: nonnegative integer
Referenced by:
§5.11(i)
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where a_{0}=\tfrac{1}{2}\sqrt{2} and

5.11.6 a_{0}a_{k}+\frac{1}{2}a_{1}a_{{k-1}}+\frac{1}{3}a_{2}a_{{k-2}}+\dots+\frac{1}{k+1}a_{k}a_{0}=\frac{1}{k}a_{{k-1}}, k\ge 1.
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Defines:
a_{k}: coefficient
Symbols:
k: nonnegative integer
Referenced by:
§5.11(i)
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Wrench (1968) gives exact values of g_{k} up to g_{{20}}. Spira (1971) corrects errors in Wrench's results and also supplies exact and 45D values of g_{k} for k=21,22,\dots,30. For an asymptotic expansion of g_{k} as k\to\infty see Boyd (1994).

¶ Terminology

The expansion (5.11.1) is called Stirling's series (Whittaker and Watson (1927, §12.33)), whereas the expansion (5.11.3), or sometimes just its leading term, is known as Stirling's formula (Abramowitz and Stegun (1964, §6.1), Olver (1997b, p. 88)).

Next, and again with the same conditions,

5.11.7 \Gamma\!\left(az+b\right)\sim\sqrt{2\pi}e^{{-az}}(az)^{{az+b-(1/2)}},
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Symbols:
\Gamma\!\left(z\right): Gamma function, \sim: asymptotically equal, z: complex variable, b: real or complex variable and a_{k}: coefficient
A&S Ref:
6.1.39
Referenced by:
§2.10(iii), §2.10(iv), §5.11(i)
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where a\;(>0) and b\;(\in\Complex) are both fixed, and

5.11.8 \ln\Gamma\!\left(z+h\right)\sim\left(z+h-\tfrac{1}{2}\right)\ln z-z+\tfrac{1}{2}\ln\!\left(2\pi\right)+\sum _{{k=2}}^{\infty}\frac{(-1)^{k}B_{{k}}\!\left(h\right)}{k(k-1)z^{{k-1}}},
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Symbols:
\Gamma\!\left(z\right): Gamma function, \sim: asymptotically equal, k: nonnegative integer and z: complex variable
Referenced by:
§5.11(i)
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where h\;(\in[0,1]) is fixed, and B_{{k}}\!\left(h\right) is the Bernoulli polynomial defined in §Ch.24.

Lastly, as y\to\pm\infty,

5.11.9 |\Gamma\!\left(x+iy\right)|\sim\sqrt{2\pi}|y|^{{x-(1/2)}}e^{{-\pi|y|/2}},
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Symbols:
\Gamma\!\left(z\right): Gamma function, \sim: asymptotically equal, x: real variable and y: real variable
Referenced by:
§2.5(i), §5.11(i)
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uniformly for bounded real values of x.

§ 5.11(ii). Error Bounds and Exponential Improvement

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Referenced by:
§5.6(i)
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If the sums in the expansions (5.11.1) and (5.11.2) are terminated at k=n-1 (k\ge 0) and z is real and positive, then the remainder terms are bounded in magnitude by the first neglected terms and have the same sign. If z is complex, then the remainder terms are bounded in magnitude by {\sec^{{2n}}}\!\left(\tfrac{1}{2}\mathrm{ph}z\right) for (5.11.1), and {\sec^{{2n+1}}}\!\left(\tfrac{1}{2}\mathrm{ph}z\right) for (5.11.2), times the first neglected terms.

For the remainder term in (5.11.3) write

5.11.10 \Gamma\!\left(z\right)=e^{{-z}}z^{z}\left(\frac{2\pi}{z}\right)^{{1/2}}\left(\sum _{{k=0}}^{{K-1}}\frac{g_{k}}{z^{k}}+R_{K}(z)\right), K=1,2,3,\dots.
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Symbols:
\Gamma\!\left(z\right): Gamma function, k: nonnegative integer, z: complex variable, g_{k}: coefficients and R_{K}(z): remainder
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Then

5.11.11 \left|R_{K}(z)\right|\leq\frac{(1+\zeta\!\left(K\right))\Gamma\!\left(K\right)}{2(2\pi)^{{K+1}}\left|z\right|^{K}}\*\left(1+\min(\sec\!\left(\mathrm{ph}z\right),2K^{{\frac{1}{2}}})\right), \left|\mathrm{ph}z\right|\leq\frac{1}{2}\pi,
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Defines:
R_{K}(z): remainder
Symbols:
\Gamma\!\left(z\right): Gamma function and z: complex variable
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where \zeta\!\left(K\right) is as in Chapter 25. For this result and a similar bound for the sector \frac{1}{2}\pi\leq\mathrm{ph}z\leq\pi see Boyd (1994).

For further information see Olver (1997b, pp. 293–295), and for other error bounds see Whittaker and Watson (1927, §12.33), Spira (1971), and Schäfke and Finsterer (1990).

For re-expansions of the remainder terms in (5.11.1) and (5.11.3) in series of incomplete gamma functions with exponential improvement (§2.11(iii)) in the asymptotic expansions, see Berry (1991), Boyd (1994), and Paris and Kaminski (2001, §6.4).

§ 5.11(iii). Ratios

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Notes:
See Temme (1996, pp. 67–68), Olver (1997b, p. 119), and Paris and Kaminski (2001, pp. 50–54).
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In this subsection a, b, and c are real or complex constants.

If z\to\infty in the sector |\mathrm{ph}z|\le\pi-\delta (<\pi), then

5.11.12 \frac{\Gamma\!\left(z+a\right)}{\Gamma\!\left(z+b\right)}\sim z^{{a-b}},
5.11.13 \frac{\Gamma\!\left(z+a\right)}{\Gamma\!\left(z+b\right)}\sim z^{{a-b}}\sum _{{k=0}}^{\infty}\frac{G_{k}(a,b)}{z^{k}}.

Also, with the added condition \realpart{(b-a)}>0,

5.11.14 \frac{\Gamma\!\left(z+a\right)}{\Gamma\!\left(z+b\right)}\sim\left(z+\frac{a+b-1}{2}\right)^{{a-b}}\sum _{{k=0}}^{\infty}\frac{H_{k}(a,b)}{\left(z+\tfrac{1}{2}(a+b-1)\right)^{{2k}}}.

Here

5.11.15
G_{0}(a,b)=1,
G_{1}(a,b)=\tfrac{1}{2}(a-b)(a+b-1),
G_{2}(a,b)=\frac{1}{12}\binom{a-b}{2}(3(a+b-1)^{2}-(a-b+1)),
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Symbols:
a: real or complex variable, b: real or complex variable and G_{k}(a,b): coefficients
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5.11.16
H_{0}(a,b)=1,
H_{1}(a,b)=-\frac{1}{12}\binom{a-b}{2}(a-b+1),
H_{2}(a,b)=\frac{1}{240}\binom{a-b}{4}(2(a-b+1)+5(a-b+1)^{2}).
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Symbols:
a: real or complex variable, b: real or complex variable and H_{k}(a,b): coefficients
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In terms of generalized Bernoulli polynomials B^{{(\ell)}}_{{n}}\!\left(x\right)Ch.24), we have for k=0,1,\ldots,

5.11.17 G_{k}(a,b)=\binom{a-b}{k}B^{{(a-b+1)}}_{{k}}\!\left(a\right),
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Defines:
G_{k}(a,b): coefficients
Symbols:
k: nonnegative integer, a: real or complex variable and b: real or complex variable
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5.11.18 H_{k}(a,b)=\binom{a-b}{2k}B^{{(a-b+1)}}_{{2k}}\!\left(\frac{a-b+1}{2}\right).
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Defines:
H_{k}(a,b): coefficients
Symbols:
k: nonnegative integer, a: real or complex variable and b: real or complex variable
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Lastly, and again if z\to\infty in the sector |\mathrm{ph}z|\le\pi-\delta (<\pi), then

5.11.19 \frac{\Gamma\!\left(z+a\right)\Gamma\!\left(z+b\right)}{\Gamma\!\left(z+c\right)}\sim\sum _{{k=0}}^{\infty}(-1)^{k}\frac{\left(c-a\right)_{{k}}\left(c-b\right)_{{k}}}{k!}\Gamma\!\left(a+b-c+z-k\right).

For the error term in (5.11.19) in the case z=x\;(>0) and c=1, see Olver (1995).