chapter 6 gamma function and related functions
DESCRIPTION
Detailed explanation of GammaTRANSCRIPT
6. Gamma Function and Related Functions
PHILIP J. DAVIS
Con tents
Mathematical Properties. . . . . . . . . . . . . . . . . . . .
6.1. Gamma Function. . . . . . . . . . . . . . . . . . . .
6.2. Beta Function . . . . . . . . . . . . . . . . . . . . .
6.3. Psi (Digamma) Function. . . . . . . . . . . . . . . . . 6.4. Polygamma Functions. . . . . . . . . . . . . . . . . . 6.5. Incomplete Gamma Function. . . . . . . . . . . . . . . 6.6. Incomplete Beta Function. . . . . . . . . . . . . . . .
Numerical Methods . . . . . . . . . . . . . . . . . . . . . .
6.7. Use and Extension of the Tables. . . . . . . . . . . . . 6.8. Summation of Rational Series by Means of Polygamma Func-
tions. . . . . . . . . . . . . . . . . . . . . . . . .
References. . . . . . , . . . . . . . , . . . . . . . . . . . .
Table 6.1. Gamma, Digamma and Trigamma Functions (1 5 s l 2 ) . .
r(x), ~n r(x), +(z), +'(z), ~=i(.oo5)2, IOD
Table 6.2. Tetragamma and Pentagamma Functions (1 5 x 5 2 ) . . .
+"(x), $J3'(2), ~=1(.01)2, 1OD
Table 6.3. Gamma and Digamma Functions for Integer and Half- Integer Values ( l l n 5 1 0 1 ) . . . . . . . . . . . . . . . . . .
r(n), 11s +(n), IOD
l/r(n), 9s n!/[(2?r)h"+3]~", 8D
r(n+$), 8s Inn-+@), 8D
n=1(1.)101
Table 6.4. Logarithms of the Gamma Function (1 I n 5 101). . . . . .
loglo r(n>, 8s log10 r(n+$), 8s
log10 r(n+#), 8 s In r(n)-(n-$) lnn+n, 8D
log10 r(n+$), 8s
n= l(1) 101
Page
255
255 258 258 260 260 263
263
263
2 64
265
267
27 1
272
274
National Bureau of Standards.
253
254 GAMMA FUNCTION AND RELATED FUNCTIONS
Page Table 6.5. Auxiliary Functions for Gamma and Digamma Func-
Table 6.6. Factorials for Large Arguments (1005nS 1000) . . .
n!, n= 100(100) 1000, 20s
Table 6.7. Gamma Function for Complex Arguments. . . . . .
In r(z+iy), 2=1(.1)2, y=0(.1)10, 12D
Table 6.8. Digamma Function for Complex Arguments . . . . .
+(z+iy), 2=1(.1)2, y=0(.1)10, 5D
%‘+U+iy), 10D B’+(l+iy)-ln y, y l= . l l (-.Ol)O, 8D
. . 276
. . 276
. . 277
. . 288
The author acknowledges the assistance of Mary Orr in the preparation and checking of the tables; and the assistance of Patricia Farrant in checking the formulas.
=.57721 56649. . . Y is known as Euler's constant and is given to 25 decimal places in chapter 1. r(z) is single valued
for the points z=-n(n=O, 1, 2, . . . ) where it possesses simple poles with residue (- 1) "/n!. Its reciprocal i/r (z) is an entire function possessing simple zeros at the points z= -n(n=O, 1, 2, . . .).
Hankel's Contour Integral
and analytic over the entire complex plane, save
(kl< =) 6.1.4 -=-s 1 i (-t)-'e-'dt
r(z) 2, c
The path of integration C starts at + QD on the real axis, circles the origin in the counterclockwise direction and returns to the starting point.
Factorial and II Notations
6.1.5 n(z)=z!=r(z+i)
Integer Values
6.1.6
6.1.7
r(n+1)=1.2.3 . . . (n-l)n=n!
lim -=o= 1 1 (n=O, 1, 2, . . .) z+,, r(-z) (-n-l)!
Fractional Values 6.1.8 I-()) = 2 s m e-12dt=&=1.77245 38509 . . . =(-3)!
0
FIGURE 6.1. Gumma function. *
, y-r(z), - - - - , Y=l/r(4
6.1.9 r(3/2)=$,*=.8~622 692%. . . =(3)!
6.1.10 r (n+ 3) = r(t> 1.5.9.13. . . (4n-3) 4"
r(+)=3.62560 99082. . .
r (4) 1.4-7.10. . . (3n-2) 3" 6.1.11 r(n+#)=
r($)=2.67893 85347 . . .
r (3)
r(3)
1-3-5-7.. . (2n-1) 2"
2.5.8-11.. . (3n-1) 3"
6.1.12 r(n+$) =
6.1.13 l"(n+#)=
r(#)=i.3aii 79394. . .
Ut) 3.7.11.15. . . (4n-1) 4" 6.1.14 r(n+i)=
r($)=i.22541 67024 . . .
*See page 11. 255
256 GAMMA FUNCTION AND RELATED FUNCTIONS
Recurrence Formulas
6.1.15 r(z+i)=Zr(Z)=Z!=Z(Z-i)!
r(n+~)=(n-il+z)(n-2+~) . . . (i+z)r(i+z)
= (n- 1+ z)! =(n-l+z)(n-2+2). . . (l+z)z!
6.1.16
Reflection Formula
6.1.17 r(z>r(i-z)=-zr(-z)r(z)=t a c 7rz - tz-1 0 l+ t
=J=, - dt (O< 9 2 < 1)
Duplication Formula
6.1.18 r(2~)=(2~):+ 222-3 r(z) r(z++)
6.1.19 r(3z)= ( 2 ~ ) -1 35’4 r (2) r (z+# r(z++) Triplication Formula
Gauss’ Multiplication Formula
Binomial Coefficient
Pochhammer’s Symbol 6.1.22
@lo= 1, (2),=2(2+1)(2+2) . . . (z+n-l)=- r(z+n)
r (2) Gamma Function in the Complex Plane
6.1.23 r@)=r); In r(Z)=In r(z)
6.1.24 arg r(z+l)=arg r(z)+arctan X
6.1.29 r(i~)r(-iy)=ir(i~)iz= 9r y sinh 7ry
6.1.31 r (1 + iy) r (1 - iy) = I r (1 + iY) (L “?/ sinh ry
Power Series 6.1.33
In r (1 + z) = -In (1 + z) + z (1 -7)
+5 ( - ~ ) ~ ~ ~ ( ~ ~ - ~ l ~ ” / ~ (14<2> n-2
{(n) is the Riemann Zeta Function (see chapter 23).
6.1.34
k 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26
Series Expansion * for 1 /r (2)
ck
1.00000 00000 000000 0.57721 56649 015329
-0.65587 80715 202538 -0.04200 26350 340952 0. 16653 86113 822915
-0.04219 77345 555443 -0.00962 19715 278770 0.00721 89432 466630
-0.00116 51675 918591 -0.00021 52416 741149 0.00012 80502 823882
-0.00002 01348 547807 -0.00000 12504 934821 0.00000 11330 272320
-0.00000 02056 338417 0.00000 00061 160950 0.00000 00050 020075
-0.00000 00011 812746 0.00000 00001 043427 0.00000 00000 077823
-0.00000 00000 036968 0.00000 00000 005100
-0.00000 00000 000206 -0.00000 00000 000054 0.00000 00000 000014 0.00000 00000 000001
2 The coefficients ck are from H. T. Davis, Tables of higher mathematical functions, 2 vols., Principia Press, Bloomington, Ind., 1933, 1935 (with permission) ; with corrections due to H. E. Salzer.
GAMMA FUNCTION AND RELATED F"CX'I0NS 257 Polynomial Approximations'
6.1.35 0 1 x 5 1
r (x+ 1) =z! = 1 + -alx+ -a& + 62 + ag4+ -a&+ E(Z)
55x10-6
~ l = - . 57486 46 ~ 4 = ,42455 49 Uz= .95123 63 U6=-. 10106 78 ~ 3 = - .69985 88
bl=-. 57719 1652 bs=-. 75670 4078 bs= .98820 5891 be= .48219 9394 b3= -. 89705 6937 b7= -. 19352 7818 bq= ,91820 6857 bs= .03586 8343
Stirling's Formula
6.1.37
Asymptotic Formulas
6.1.39
r(-az+b) -l/Z;;e-(U(-az)(U+b--t (la% 4<a, -a>()>
6.1.M
In r(z) -(z-+) In z-z++ I n ( 2 ~ )
(z+m in larg z~<T) B 2 m m +z 2rn(2m-1)2*-'
For B, see chapter 23 6.1.41
1 1 In r(z) -(z-& In z-z++ In (%)+--- 122 360z3
From C. Hmtings, Jr., Approximations for digital computers, Princeton Univ. Press, Princeton, N.J., 1955 (with permission).
Error Term for Asymptotic Expansion
6.1.42
If
R,(z)= In r (z)-(z-# In z+z-+ In ( 2 ~ )
B2m -5 ,,12rn(2rn--l)z an--l
then
where
K(z)=upper U l O bound(z2/(u2+z3) I
For z real and positive, R, is less in absolute value than the first term neglected and has the same i gn .
6.1.43
9th r(iy)=%?ln r(-iy)
-& In (2.) -w-+ln y, (y++
6.1.44
A n r(iy)=arg r(iy)=-arg r(-iy) = - A n r(-iy)
6.1.46
6.1.47
as z+m along any curve joining z=O and Z= m , providingz# --a, ---a-1, . . . ; zf --b, -b-1, . . . .
- (2n)! 1 2n r(n++)
1 ---
22n(n!)2-~ (n)=rtr(n+i)
- -&j [I-%+=*- * * *
1 1 1
(n+ OJ 1 Some Definite Integrals
6.1.50
e;‘~;~~’‘] T In r(z)=Jm[(z-l) e+- - ( 9 2 > 0)
=(z-+) In z-z++ In 21r
( 9 2 > 0) m arctan (t/z) dt
6.2. Beta Function
+2J, e”8-1
6.2.1
B(z,w)=J t s -1 ( 1 4 - 1 dt- -Jm&;*+. dt
= 2 r (sin t)s-1 (cos t ) tw-1 dt
( 9 2 > 0, aw > o >
r (z)r (w)=B(w,z) r(z+w)
6.3. Psi (Digamma) Function E-
#(z)=d[ln r (z)]/~z= r’(~)/r (z)
6.2.2 B(z,w)=
6.3.1
4 Some authors employ the special double factorial nota- tion as follows:
(24 ! 1 =2.4.6 . . . (24=2% i (h-1 ) ! I =1.3.5. . . ( 2 n - i ) = ~ 2” r(n++)
d 680meauthorswrite$(z)=~lnr(~+1) andeimilarlyfor
the polygamms functions.
FIGURE 6.2. Psi function.
y = $(z) = d In r kc)/&
Integer Values
n-1
k=1 6.3.2 #(l)=-’~, #(n)=-r+ Ck-’ (n22)
Fractional Values
6.3.3
#(+)=-7-2 In 2=--1.96351 00260 21423 . . .
6.3.4
#(n++)=-r-21n2+2 I+ ,+ . . - +:) 1 2n 1
(n 2 1)
( l
Recurrence Formulas
1 6.3.5
6.3.6
‘(n + ‘I= (n - 1) + z (n - 2) + z
t(Z+ l) = +(Z) + ;
l + 1 + . . .
1 1 +i&+,+,+9(1+4
GAMMA RTNCTION AND RELATED FUNCTIONS 259 Reflection Formula
6.3.7 +(l-z)=+(z)+* cot *z
Duplication Formula
6.3.8 +(22)=Mz)+++ (z+&) +In 2
Psi Function in the Complex Plane -
6.3.9 +GI =*(z> 6.3.10
9+(iy>=W+(-iy)=W+(l +iy)=W+(l -iy)
6-3-11 Y+(iy)=&/-'+#,~ coth xy
6.3.12 Y+(++iy) =&r tanh ?ry
1 63-13 j$(l+iy)=---+# ~ ~ 0 t h rv 2Y
= y g (n2+yS) -1 n-1
Series Expansions
6.3.14 +(l+~)=-r+C(-l)"~(n)~~-' (Iz1<1) n-2
6.3.15 +( 1 + 2) =& -1- &€ cot e- (1 -9) -'+ 1-7
- 5It(2n+ 1) - 11 ZSA (I z I <2) n-1
6.3.16
(~#-1,-2,-3, . . . )
6.3.17
9+(l+iy)=l-r-- 1 l+y2
+g (- l)"+'[r(2n+ 1) -l]y2' n=1
(IYl<2)
(- OJ <Y< -1
OD
= -r+ y2 c n-'(n*+yS) -1 a-1
Asymptotic Formulae
6.3.18
1 = Bz, -In z-s-n-l c- 2nz2"
=In z---- 1 1 1 1 + . . .
(z+- in lergzl<*)
22 1 2 9 + 1 2 0 2 4 - ~ 6
6.3.19
1 +-+. . . 1 1 =In y+-+- 12oy4 2 m Y 6
(Y+OJ)
Extremaoof r(z) - Zeros of $(z) 9 6
I
+l. 462 -0.504 -1.573 -2.611 -3.635 -4.653 -5.667 -6.678
+O. 886 -3.545 +2.302 -0.888 +O. 245 -0.053 +o. 009 -0.001
Zo=1.46163 21449 68362 r(xo)= .88560 31944 10889
6.3.20 zn=-n+(ln n)-'+o[(ln n)-*]
Definite Integrals
6.3.21
6From W. Sibagaki, Theory and applications of the gamma function, Iwanami Syoten, Tokyo, Japan, 1952 (with permission).
GAMMA FUNCTION AND RELATED FUNCTIONS 261 d
FIGURE 6.3. Incomplete gamma function. ?*(a,%)=- e-Lto-1dt
From F. G. Tricomi, Siilla funzione gamma incompleta, Annali di Matematica, IV, 33, 1950 (with permission). r(a) %-a r o
*See page n.
262 GAMMA FUNCTION AND RELATED F"CT1ONS
6.5.5 Probability Integral of the +Distribution
6.5.6
(Pearson's Form of the Incomplete Gamma Function)
m
6.5.7 C(z,a)=l tu-1 cos t dt (L@'a<l)
m
6.5.8 S(z,a)=$, ta-l sin t dt (9'a<l)
6.5.9 nm
6.5.11
Incomplete Gamma Function aa a Confluent Hypergeometric Function (eee chapter 13)
6.5.12 y(u,z)=a-lzue-tM(l, l+a,z)
=u-'zU M(a, l+a,-z)
Special Values
6.5.13
= 1 -e,,- (2) e-2
For relation to the Poisson distribution, 26.4.
6.5.14 r*(-n, z)=z"
6.5.15 I' (0, z)=le-'t-'dt=El (5)
see
6.5.16
6.5.17
6.5.18
6.5.19
6.5.20
6.5.21
6.5.22
6.5.23
6.5.24
Recurrence Formulas
9e-" P(a+l, z)=P(a, z)---- r(a+l>
y (a+ 1 ,z) = uy(a,z)
e-' V*(u-l,z) =m*(u,z) +- r (a)
Derivatives and Differential Equations
6.5.26
b" - ax" [x-T(u,s)~= (-i)nz-a-qa+n,z) (n=O, 1,2, . . .)
6.5.27 b" - bX" [e"z"~* (a,x)]=e"z"-"y*(a-n, z)
(n=O, 1,2, . . .)
Series Developmente
6.5.29
GAMMA FUNCTION AND RELATED FUNCTIOXS 263
Continued Fraction
6.5.31
Asymptotic Expansions
6.5.32
Suppose Rn(a,c")=un,,(a,z)+ . . . is the re- mnintlcr nftcr n terms in this series. Then if a , ~ nrc real, w e 11avr for n>a-2
!Iin(a,z)! I lun+,(a,z)l
ni i t l sign I?, (a,z) =sign u,<+, (a,z).
0 for a>1
1 for Osa<1
6.5.35
(z+m in I nrg zl<+r) Numeric
6.7. Use and Extension of the Tables
Example 1. Compute r(6.38) to 8s. Using the r~wirr~~i icc rchtioii 6.1.16 niitl Table 6.1 wc 1 1 avc,
r (6.38) = [ (5.38) (4.38) (3.38) (2.33) ( 1.38) ] r ( 1.38) = 232.4367 1.
Example 2. Compute In r(56.38), iisiiig Table 6.4 niid liiicnr iiitrrpolation iii j... \\-e liavc
Definite Integrals
6.5.36
6.6. Incomplete Beta Function
6.6.1 Br(a,b) =J2 t~-'(l--t)b-'d2 0
6.6.2 I r (a, b) = Br (ab) /B (a,b)
For statistical applications, see 26.5.
Symmetry
6.6.3 I,(a,b)=l --I,-r(b,u)
Helation to Binomial Expansion
For binomial distribution, see 26.1.
Recurrencc Formulas
6.6.5 Ir(U,b)=XIr(U- 1,b) + (l-~)IZ(a,b- 1)
6.6.6 (a+b-a)I,(a,b) =a(l-z)12(a+ 1,b- l>+bI,(a,b+ 1)
6.6.7 (~+b)l,(a,b) =al,(a+ 1,b) +bI,(a,b+ 1)
Relation to Hypergeometric Function
6.6.8 B,(a,b)=a-'~'c"F(a,l-b; a+l; Z)
:a1 Methods
*
The crror of liiicar intrrpolation in the table of tlic function f2 is smaller than lo-' in this region. Hence, f2(56.38) = .92041 67 and In I'(56.38) = 169.85497 42.
Direct interpolation in Table 6.4 of log,, r(n) climiiiatcs tlic necessity of employing logarithms. HOWCVP~, tlic rrror of liiicar intcrpolation is .002 so tltnt log,, r(n) is obtained with a rclativc error of 10-5.
*See page 11. In r(56.38) = (56.38-3) In (56.38) - (56.38)
+ j 2 (56.38)
264 GAMMA FUNCTION AN
Example 3. Compute $(6.38) to 8s. Using the recurrence relation 6.3.6 and Table 6.1.
=1.77275 59.
Example 4. Compute (L(56.38). Using Table 6.3 we have $(56.38)=ln 56.38-j3(56.38).
The error of linear interpolation in the table of the function f3 is smaller than 8XlO-' in this region. Hence,f3(56.38)=.00889 53and$(56.38)= 4.023219.
Example 5. Compute In I'(1-i). From the reflection principle 6.1.23 and Table 6.7, In r(1-i) =In r(l+i) = -.6509+.3016i.
Example 6. Compute In F(+++i). Taking the logarithm of the recurrence relation 6.1.15 we have,
In r (&++i) =In r (#++i) -In (*+&i) - - -.23419+.03467i
-(& In *+i arctan 1) = .11239- .75073i
The logarithms of complex numbers are found from 4.1.2.
Example 7. Compute In I'(3+7i) using the duplication formula 6.1.18. Taking the logarithm of 6.1.18, we have
-4 In 2r=- .91894 (#+7i) In 2= 1.73287+ 4.852036 In r(#+$i)=-3.31598+ 2.32553i In r(2+4$=-2.66047+ 2.938693
In r(3+7i) =-5.16252+10.11625i
Example 8. Compute In I'(3+7i) to 5D using the asymptotic formula 6.1.41. We have
In (34-79 =2.03022 15+1.16590 45i.
Then,
(2.5+7i) In (3+7i)=-3. 0857779+17.1263119i - (3+7i) = -3.0000000- 7. oooooooi 4 In (2~)= .9189385
[12(3+7i)]-'= .00431037 .01005753 -[360(3+7i)3]-i= . 0000059- . 0000022i
In r(3+7i)=-5. 16252 +io. 11625i
RELATED FUNCTIONS
6.8. Summation of Rational Series by Means of Polygamma Functions
An infinite series whose general term is a ra- tional function of the index may always be reduced to a finite series of psi and polygamma functions. The method will be illustrated by writing the ex- plicit formula when the denominator contains a triple root.
Let the general term of an infinite series have the form
where p(n) is a polynomial of degree m + 2r + 3s - 2 at most and where the constants a,, pi., and yf are distinct. Expand un in partial fractions as follows
OD
Then, we may express u, in terms of the
constants appearing in this partial fraction expan- sion as follows
n-1
Higher order repetitions in the denominator are If the denominator contains handled similarly.
GAMMA FUNCTION AND RELATED FUNCTIONS 265
only simple or double roots, omit the correapond- ing lines.
Example 9. Find - 1
Since
we have
a1=1, a2=3, as=*, al=*, &=-l, *=#.
Thus,
8= -)$(2) +$(13) -#$(It) =.047198.
Example 10.
m 1
we have,
Therefore
S= 16~(1)-16$(1~) +$'(1) +$'(li) =.013499.
Example 11.
(see also 6.3.13). 1 m
Evaluate 8 = c n-l (n2+ 1) (n*+4)
We have, 1
i -i -i i Hence, al=-, 6 e=-, 6 &=- 12 ' a 4 = 3
a1=i, az=-i, aa=2i, a,=-2i,
and therefore
s=- --z [$( 1 +i) -$(1 -ill +a i [$(1+2i) -$(1-2i)l. 6
By 6.3.9, this reduces to
1 1 3 6 8=- Y$(l+i)-- 9$(1+2{).
From Table 6.8, s=.13876.
References Texts
[6.1] E. Artin, Einfiihrung in die Theorie der Gamms- funktion (Leipzig, Germany, 1931).
[6.2] P. E. Bohmer, Differenzengleichungen und be- stimmte Integrale, chs. 3, 4, 5 (K. F. Koehler, Leipzig, Germany, 1939).
16.31 G. Doetsch, Handbuch der Laplace-Transforma- tion, vol. 11, pp. 52-61 (Birkhauser, Basel, Switzerland, 1955).
[6.4] A. Erdblyi et al., Higher transcendental functions, vol. 1, ch. 1, ch. 2, sec. 5; vol. 2, ch. 9 (McGraw- Hill Book Co., Inc., New York, N.Y., 1953).
[6.5] C. Hastings, Jr., Approximations for digital com- puters (Princeton Univ. Press, Princeton, N.J., 1955).
[6.6] F. Losch and F. Schoblik, Die Fakultiit und ver- wandte Funktionen (B. G. Teuhner, Leipzig, Germany, 1951).
[6.7] W. Sibagaki, Theory and applications of the gamma function (Iwanami Syoten, Tokyo, Japan, 1952).
[6.S] E. T. Whittaker and G. N. Watson, A course of modern analysis, ch. 12, 4th ed. (Cambridge Univ. Press, Cambridge, England, 1952).
Tables
[6.9] A. Abramov, Tables of I n r(z) for complex argu- Translated from the Russian by D. G. ment.
Fry (Pergamon Press, New York, N.Y., 1960). In r(z+iy), z=O(.Ol)lO, y=0(.01)4, 6D.
[6.10] Ballistic Research Laboratory, A table of the facto- rial numbers and their reciprocals from l! through lOOO! to 20 significant digits. Technical Note NO. 381, Aberdeen Proving Ground, Md., 1951.
[6.11] British Association for the Advancement of Science, Mathematical tables, vol. 1, 3d ed., pp. 40-59 (Cambridge Univ. Press, Cambridge, England, 1951). The gamma and polygamma functions.
Also l+l ' log lD (t)!dt, z=O(.Ol)l, 10D.
[6.12] H. T. Davis, Tables of the higher mathematical functions, 2 vols. (Principia Press, Bloomington, Ind., 1933, 1935). Extensive, many place tables of the gamma and polygamma functions up to $(4)(z) and of their logarithms.
[6.13] F. J. Duarte, Nouvelles tables de log,, nl 8,33 d6ci- males depuis n= l jusqu'h n=3000 (Kundig, Geneva, Switzerland; Index Generalis, Paris, France, 1927).
266 GAMMA FUNCTION AND RELATED FUNCTIONS
[6.14] National Bureau of Standards, Tables of nl and r(n+& for the first thousand values of n, Ap- plied Math. Series 16 (U.S. Government Printing O5ce, Washington, D.C., 1951). nf, 16S;r(n+&, 8s.
[6.15] National Bureau of Standards, Table of Coulomb wave functions, vol. I, pp. 114-135, Applied Math. Series 17 (U.S. Government Printing O5ce, Washington, D.C., 1952).
9 [ryi + is)/r (1 + is] ,9 = o(.oo5) 2 (.oi) 6 (.02)1 o(. 1 20 (.2) 60( .5) 1 10,l OD ; apg r (1 + is) ,s = O(.el) 1 (.02)
3 (.05)10(.2)20(.4)30(.5)85, 8D.
[6.16] National Bureau of Standards, Table of the gamma function for complex arguments, Applied Math. Series 34 (U.S. Government Printing O5ce, Washington, D.C., 1954).
In r(z+iy), z=d(.l)lO, y=0(.1)10, 12D.
Contains an extensive bibliography. (6.171 National Physical Laboratory, Tables of Weber
parabolic cylinder functions, pp. 226-233 (Her Majesty’s Stationery Office, London, England, 1955).
Real and imaginary parts of In r(ik+$ia), k-0(1)3, a = 0 (. 1) 5(. 2) 20, 8D ; (IF (4 + +ia) /r (+ + tis) 1) -I”
~=0(.02)1(.1)5(.2)20, 8D.
[6.18] E. S. Pearson, Table of the logarithms of the com- plete r-function, arguments 2 to 1200, Tracts for Computers No. VI11 (Cambridge Univ. Press, Cambridge, England, 1922). Loglo r(p), p=2(.1) 5(.2)70(1)1200, 10D.
[6.19] J. Peters, Ten-place logarithm tables, vol. I, Ap- pendix, pp. 58-68 (Frederick Ungar Publ. Co., New York, N.Y., 1957). nl, n=1(1)60, exact;
18D. (n!)-’, n=1(1)43, 54D; Log,o(nl), n=1(1)1200,
(6.20) J. P. Stanley and M. V. Wilkes, Table of the recip- rocal of the gamma function for complex argu- ment (Univ. of Toronto Press, Toronto, Canada, 1950). Z= -.5( .01).5, y=O(.Ol)l, 6D.
I6.211 M. Zycakowski, Tablice funkcyi eulera i pokrewnych (Panstwowe Wydawnictwo Naukowe, Warsaw, Poland, 1954). Extensive tables of integrals involving gamma and beta functions.
For references to tabular material on the incomplete gamma and incomplete beta functions, see the references in chapter 26.