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c977aa998f
Replace amos with slatec
261 lines
11 KiB
Fortran
261 lines
11 KiB
Fortran
*DECK CBESI
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SUBROUTINE CBESI (Z, FNU, KODE, N, CY, NZ, IERR)
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C***BEGIN PROLOGUE CBESI
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C***PURPOSE Compute a sequence of the Bessel functions I(a,z) for
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C complex argument z and real nonnegative orders a=b,b+1,
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C b+2,... where b>0. A scaling option is available to
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C help avoid overflow.
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C***LIBRARY SLATEC
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C***CATEGORY C10B4
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C***TYPE COMPLEX (CBESI-C, ZBESI-C)
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C***KEYWORDS BESSEL FUNCTIONS OF COMPLEX ARGUMENT, I BESSEL FUNCTIONS,
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C MODIFIED BESSEL FUNCTIONS
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C***AUTHOR Amos, D. E., (SNL)
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C***DESCRIPTION
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C
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C On KODE=1, CBESI computes an N-member sequence of complex
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C Bessel functions CY(L)=I(FNU+L-1,Z) for real nonnegative
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C orders FNU+L-1, L=1,...,N and complex Z in the cut plane
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C -pi<arg(Z)<=pi. On KODE=2, CBESI returns the scaled functions
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C
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C CY(L) = exp(-abs(X))*I(FNU+L-1,Z), L=1,...,N and X=Re(Z)
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C
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C which removes the exponential growth in both the left and
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C right half-planes as Z goes to infinity.
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C
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C Input
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C Z - Argument of type COMPLEX
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C FNU - Initial order of type REAL, FNU>=0
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C KODE - A parameter to indicate the scaling option
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C KODE=1 returns
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C CY(L)=I(FNU+L-1,Z), L=1,...,N
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C =2 returns
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C CY(L)=exp(-abs(X))*I(FNU+L-1,Z), L=1,...,N
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C where X=Re(Z)
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C N - Number of terms in the sequence, N>=1
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C
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C Output
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C CY - Result vector of type COMPLEX
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C NZ - Number of underflows set to zero
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C NZ=0 Normal return
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C NZ>0 CY(L)=0, L=N-NZ+1,...,N
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C IERR - Error flag
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C IERR=0 Normal return - COMPUTATION COMPLETED
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C IERR=1 Input error - NO COMPUTATION
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C IERR=2 Overflow - NO COMPUTATION
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C (Re(Z) too large on KODE=1)
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C IERR=3 Precision warning - COMPUTATION COMPLETED
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C (Result has half precision or less
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C because abs(Z) or FNU+N-1 is large)
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C IERR=4 Precision error - NO COMPUTATION
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C (Result has no precision because
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C abs(Z) or FNU+N-1 is too large)
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C IERR=5 Algorithmic error - NO COMPUTATION
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C (Termination condition not met)
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C
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C *Long Description:
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C
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C The computation of I(a,z) is carried out by the power series
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C for small abs(z), the asymptotic expansion for large abs(z),
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C the Miller algorithm normalized by the Wronskian and a
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C Neumann series for intermediate magnitudes of z, and the
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C uniform asymptotic expansions for I(a,z) and J(a,z) for
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C large orders a. Backward recurrence is used to generate
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C sequences or reduce orders when necessary.
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C
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C The calculations above are done in the right half plane and
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C continued into the left half plane by the formula
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C
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C I(a,z*exp(t)) = exp(t*a)*I(a,z), Re(z)>0
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C t = i*pi or -i*pi
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C
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C For negative orders, the formula
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C
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C I(-a,z) = I(a,z) + (2/pi)*sin(pi*a)*K(a,z)
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C
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C can be used. However, for large orders close to integers the
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C the function changes radically. When a is a large positive
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C integer, the magnitude of I(-a,z)=I(a,z) is a large
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C negative power of ten. But when a is not an integer,
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C K(a,z) dominates in magnitude with a large positive power of
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C ten and the most that the second term can be reduced is by
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C unit roundoff from the coefficient. Thus, wide changes can
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C occur within unit roundoff of a large integer for a. Here,
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C large means a>abs(z).
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C
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C In most complex variable computation, one must evaluate ele-
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C mentary functions. When the magnitude of Z or FNU+N-1 is
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C large, losses of significance by argument reduction occur.
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C Consequently, if either one exceeds U1=SQRT(0.5/UR), then
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C losses exceeding half precision are likely and an error flag
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C IERR=3 is triggered where UR=R1MACH(4)=UNIT ROUNDOFF. Also,
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C if either is larger than U2=0.5/UR, then all significance is
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C lost and IERR=4. In order to use the INT function, arguments
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C must be further restricted not to exceed the largest machine
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C integer, U3=I1MACH(9). Thus, the magnitude of Z and FNU+N-1
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C is restricted by MIN(U2,U3). In IEEE arithmetic, U1,U2, and
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C U3 approximate 2.0E+3, 4.2E+6, 2.1E+9 in single precision
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C and 4.7E+7, 2.3E+15 and 2.1E+9 in double precision. This
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C makes U2 limiting in single precision and U3 limiting in
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C double precision. This means that one can expect to retain,
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C in the worst cases on IEEE machines, no digits in single pre-
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C cision and only 6 digits in double precision. Similar con-
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C siderations hold for other machines.
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C
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C The approximate relative error in the magnitude of a complex
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C Bessel function can be expressed as P*10**S where P=MAX(UNIT
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C ROUNDOFF,1.0E-18) is the nominal precision and 10**S repre-
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C sents the increase in error due to argument reduction in the
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C elementary functions. Here, S=MAX(1,ABS(LOG10(ABS(Z))),
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C ABS(LOG10(FNU))) approximately (i.e., S=MAX(1,ABS(EXPONENT OF
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C ABS(Z),ABS(EXPONENT OF FNU)) ). However, the phase angle may
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C have only absolute accuracy. This is most likely to occur
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C when one component (in magnitude) is larger than the other by
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C several orders of magnitude. If one component is 10**K larger
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C than the other, then one can expect only MAX(ABS(LOG10(P))-K,
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C 0) significant digits; or, stated another way, when K exceeds
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C the exponent of P, no significant digits remain in the smaller
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C component. However, the phase angle retains absolute accuracy
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C because, in complex arithmetic with precision P, the smaller
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C component will not (as a rule) decrease below P times the
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C magnitude of the larger component. In these extreme cases,
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C the principal phase angle is on the order of +P, -P, PI/2-P,
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C or -PI/2+P.
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C
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C***REFERENCES 1. M. Abramowitz and I. A. Stegun, Handbook of Mathe-
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C matical Functions, National Bureau of Standards
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C Applied Mathematics Series 55, U. S. Department
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C of Commerce, Tenth Printing (1972) or later.
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C 2. D. E. Amos, Computation of Bessel Functions of
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C Complex Argument, Report SAND83-0086, Sandia National
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C Laboratories, Albuquerque, NM, May 1983.
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C 3. D. E. Amos, Computation of Bessel Functions of
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C Complex Argument and Large Order, Report SAND83-0643,
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C Sandia National Laboratories, Albuquerque, NM, May
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C 1983.
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C 4. D. E. Amos, A Subroutine Package for Bessel Functions
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C of a Complex Argument and Nonnegative Order, Report
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C SAND85-1018, Sandia National Laboratory, Albuquerque,
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C NM, May 1985.
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C 5. D. E. Amos, A portable package for Bessel functions
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C of a complex argument and nonnegative order, ACM
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C Transactions on Mathematical Software, 12 (September
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C 1986), pp. 265-273.
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C
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C***ROUTINES CALLED CBINU, I1MACH, R1MACH
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C***REVISION HISTORY (YYMMDD)
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C 830501 DATE WRITTEN
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C 890801 REVISION DATE from Version 3.2
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C 910415 Prologue converted to Version 4.0 format. (BAB)
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C 920128 Category corrected. (WRB)
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C 920811 Prologue revised. (DWL)
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C***END PROLOGUE CBESI
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COMPLEX CONE, CSGN, CY, Z, ZN
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REAL AA, ALIM, ARG, DIG, ELIM, FNU, FNUL, PI, RL, R1M5, S1, S2,
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* TOL, XX, YY, R1MACH, AZ, FN, BB, ASCLE, RTOL, ATOL
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INTEGER I, IERR, INU, K, KODE, K1, K2, N, NN, NZ, I1MACH
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DIMENSION CY(N)
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DATA PI /3.14159265358979324E0/
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DATA CONE / (1.0E0,0.0E0) /
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C
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C***FIRST EXECUTABLE STATEMENT CBESI
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IERR = 0
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NZ=0
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IF (FNU.LT.0.0E0) IERR=1
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IF (KODE.LT.1 .OR. KODE.GT.2) IERR=1
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IF (N.LT.1) IERR=1
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IF (IERR.NE.0) RETURN
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XX = REAL(Z)
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YY = AIMAG(Z)
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C-----------------------------------------------------------------------
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C SET PARAMETERS RELATED TO MACHINE CONSTANTS.
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C TOL IS THE APPROXIMATE UNIT ROUNDOFF LIMITED TO 1.0E-18.
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C ELIM IS THE APPROXIMATE EXPONENTIAL OVER- AND UNDERFLOW LIMIT.
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C EXP(-ELIM).LT.EXP(-ALIM)=EXP(-ELIM)/TOL AND
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C EXP(ELIM).GT.EXP(ALIM)=EXP(ELIM)*TOL ARE INTERVALS NEAR
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C UNDERFLOW AND OVERFLOW LIMITS WHERE SCALED ARITHMETIC IS DONE.
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C RL IS THE LOWER BOUNDARY OF THE ASYMPTOTIC EXPANSION FOR LARGE Z.
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C DIG = NUMBER OF BASE 10 DIGITS IN TOL = 10**(-DIG).
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C FNUL IS THE LOWER BOUNDARY OF THE ASYMPTOTIC SERIES FOR LARGE FNU.
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C-----------------------------------------------------------------------
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TOL = MAX(R1MACH(4),1.0E-18)
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K1 = I1MACH(12)
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K2 = I1MACH(13)
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R1M5 = R1MACH(5)
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K = MIN(ABS(K1),ABS(K2))
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ELIM = 2.303E0*(K*R1M5-3.0E0)
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K1 = I1MACH(11) - 1
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AA = R1M5*K1
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DIG = MIN(AA,18.0E0)
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AA = AA*2.303E0
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ALIM = ELIM + MAX(-AA,-41.45E0)
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RL = 1.2E0*DIG + 3.0E0
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FNUL = 10.0E0 + 6.0E0*(DIG-3.0E0)
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AZ = ABS(Z)
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C-----------------------------------------------------------------------
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C TEST FOR RANGE
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C-----------------------------------------------------------------------
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AA = 0.5E0/TOL
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BB=I1MACH(9)*0.5E0
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AA=MIN(AA,BB)
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IF(AZ.GT.AA) GO TO 140
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FN=FNU+(N-1)
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IF(FN.GT.AA) GO TO 140
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AA=SQRT(AA)
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IF(AZ.GT.AA) IERR=3
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IF(FN.GT.AA) IERR=3
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ZN = Z
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CSGN = CONE
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IF (XX.GE.0.0E0) GO TO 40
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ZN = -Z
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C-----------------------------------------------------------------------
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C CALCULATE CSGN=EXP(FNU*PI*I) TO MINIMIZE LOSSES OF SIGNIFICANCE
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C WHEN FNU IS LARGE
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C-----------------------------------------------------------------------
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INU = FNU
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ARG = (FNU-INU)*PI
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IF (YY.LT.0.0E0) ARG = -ARG
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S1 = COS(ARG)
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S2 = SIN(ARG)
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CSGN = CMPLX(S1,S2)
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IF (MOD(INU,2).EQ.1) CSGN = -CSGN
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40 CONTINUE
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CALL CBINU(ZN, FNU, KODE, N, CY, NZ, RL, FNUL, TOL, ELIM, ALIM)
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IF (NZ.LT.0) GO TO 120
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IF (XX.GE.0.0E0) RETURN
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C-----------------------------------------------------------------------
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C ANALYTIC CONTINUATION TO THE LEFT HALF PLANE
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C-----------------------------------------------------------------------
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NN = N - NZ
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IF (NN.EQ.0) RETURN
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RTOL = 1.0E0/TOL
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ASCLE = R1MACH(1)*RTOL*1.0E+3
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DO 50 I=1,NN
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C CY(I) = CY(I)*CSGN
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ZN=CY(I)
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AA=REAL(ZN)
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BB=AIMAG(ZN)
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ATOL=1.0E0
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IF (MAX(ABS(AA),ABS(BB)).GT.ASCLE) GO TO 55
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ZN = ZN*CMPLX(RTOL,0.0E0)
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ATOL = TOL
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55 CONTINUE
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ZN = ZN*CSGN
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CY(I) = ZN*CMPLX(ATOL,0.0E0)
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CSGN = -CSGN
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50 CONTINUE
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RETURN
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120 CONTINUE
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IF(NZ.EQ.(-2)) GO TO 130
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NZ = 0
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IERR=2
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RETURN
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130 CONTINUE
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NZ=0
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IERR=5
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RETURN
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140 CONTINUE
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NZ=0
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IERR=4
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RETURN
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END
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