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Highlights from
slatec

from slatec by Ben Barrowes
The slatec library converted into matlab functions.

[z,fnu,kode,n,cy,nz,ierr]=cbesj(z,fnu,kode,n,cy,nz,ierr);
function [z,fnu,kode,n,cy,nz,ierr]=cbesj(z,fnu,kode,n,cy,nz,ierr);
%***BEGIN PROLOGUE  CBESJ
%***PURPOSE  Compute a sequence of the Bessel functions J(a,z) for
%            complex argument z and real nonnegative orders a=b,b+1,
%            b+2,... where b>0.  A scaling option is available to
%            help avoid overflow.
%***LIBRARY   SLATEC
%***CATEGORY  C10A4
%***TYPE      COMPLEX (CBESJ-C, ZBESJ-C)
%***KEYWORDS  BESSEL FUNCTIONS OF COMPLEX ARGUMENT,
%             BESSEL FUNCTIONS OF THE FIRST KIND, J BESSEL FUNCTIONS
%***AUTHOR  Amos, D. E., (SNL)
%***DESCRIPTION
%
%         On KODE=1, CBESJ computes an N member sequence of complex
%         Bessel functions CY(L)=J(FNU+L-1,Z) for real nonnegative
%         orders FNU+L-1, L=1,...,N and complex Z in the cut plane
%         -pi<arg(Z)<=pi.  On KODE=2, CBESJ returns the scaled functions
%
%            CY(L) = exp(-abs(Y))*J(FNU+L-1,Z),  L=1,...,N and Y=Im(Z)
%
%         which remove the exponential growth in both the upper and
%         lower half planes as Z goes to infinity.  Definitions and
%         notation are found in the NBS Handbook of Mathematical
%         Functions (Ref. 1).
%
%         Input
%           Z      - Argument of type COMPLEX
%           FNU    - Initial order of type REAL, FNU>=0
%           KODE   - A parameter to indicate the scaling option
%                    KODE=1  returns
%                            CY(L)=J(FNU+L-1,Z), L=1,...,N
%                        =2  returns
%                            CY(L)=J(FNU+L-1,Z)*exp(-abs(Y)), L=1,...,N
%                            where Y=Im(Z)
%           N      - Number of terms in the sequence, N>=1
%
%         Output
%           CY     - Result vector of type COMPLEX
%           NZ     - Number of underflows set to zero
%                    NZ=0    Normal return
%                    NZ>0    CY(L)=0, L=N-NZ+1,...,N
%           IERR   - Error flag
%                    IERR=0  Normal return     - COMPUTATION COMPLETED
%                    IERR=1  Input error       - NO COMPUTATION
%                    IERR=2  Overflow          - NO COMPUTATION
%                            (Im(Z) too large on KODE=1)
%                    IERR=3  Precision warning - COMPUTATION COMPLETED
%                            (Result has half precision or less
%                            because abs(Z) or FNU+N-1 is large)
%                    IERR=4  Precision error   - NO COMPUTATION
%                            (Result has no precision because
%                            abs(Z) or FNU+N-1 is too large)
%                    IERR=5  Algorithmic error - NO COMPUTATION
%                            (Termination condition not met)
%
% *Long Description:
%
%         The computation is carried out by the formulae
%
%            J(a,z) = exp( a*pi*i/2)*I(a,-i*z),  Im(z)>=0
%
%            J(a,z) = exp(-a*pi*i/2)*I(a, i*z),  Im(z)<0
%
%         where the I Bessel function is computed as described in the
%         prologue to CBESI.
%
%         For negative orders, the formula
%
%            J(-a,z) = J(a,z)*cos(a*pi) - Y(a,z)*sin(a*pi)
%
%         can be used.  However, for large orders close to integers, the
%         the function changes radically.  When a is a large positive
%         integer, the magnitude of J(-a,z)=J(a,z)*cos(a*pi) is a
%         large negative power of ten.  But when a is not an integer,
%         Y(a,z) dominates in magnitude with a large positive power of
%         ten and the most that the second term can be reduced is by
%         unit roundoff from the coefficient.  Thus, wide changes can
%         occur within unit roundoff of a large integer for a.  Here,
%         large means a>abs(z).
%
%         In most complex variable computation, one must evaluate ele-
%         mentary functions.  When the magnitude of Z or FNU+N-1 is
%         large, losses of significance by argument reduction occur.
%         Consequently, if either one exceeds U1=SQRT(0.5/UR), then
%         losses exceeding half precision are likely and an error flag
%         IERR=3 is triggered where UR=R1MACH(4)=UNIT ROUNDOFF.  Also,
%         if either is larger than U2=0.5/UR, then all significance is
%         lost and IERR=4.  In order to use the INT function, arguments
%         must be further restricted not to exceed the largest machine
%         integer, U3=I1MACH(9).  Thus, the magnitude of Z and FNU+N-1
%         is restricted by MIN(U2,U3).  In IEEE arithmetic, U1,U2, and
%         U3 approximate 2.0E+3, 4.2E+6, 2.1E+9 in single precision
%         and 4.7E+7, 2.3E+15 and 2.1E+9 in doubleprecision.  This
%         makes U2 limiting in single precision and U3 limiting in
%         doubleprecision.  This means that one can expect to retain,
%         in the worst cases on IEEE machines, no digits in single pre-
%         cision and only 6 digits in doubleprecision.  Similar con-
%         siderations hold for other machines.
%
%         The approximate relative error in the magnitude of a complex
%         Bessel function can be expressed as P*10**S where P=MAX(UNIT
%         ROUNDOFF,1.0E-18) is the nominal precision and 10**S repre-
%         sents the increase in error due to argument reduction in the
%         elementary functions.  Here, S=MAX(1,ABS(LOG10(ABS(Z))),
%         ABS(LOG10(FNU))) approximately (i.e., S=MAX(1,ABS(EXPONENT OF
%         ABS(Z),ABS(EXPONENT OF FNU)) ).  However, the phase angle may
%         have only absolute accuracy.  This is most likely to occur
%         when one component (in magnitude) is larger than the other by
%         several orders of magnitude.  If one component is 10**K larger
%         than the other, then one can expect only MAX(ABS(LOG10(P))-K,
%         0) significant digits; or, stated another way, when K exceeds
%         the exponent of P, no significant digits remain in the smaller
%         component.  However, the phase angle retains absolute accuracy
%         because, in complex arithmetic with precision P, the smaller
%         component will not (as a rule) decrease below P times the
%         magnitude of the larger component.  In these extreme cases,
%         the principal phase angle is on the order of +P, -P, PI/2-P,
%         or -PI/2+P.
%
%***REFERENCES  1. M. Abramowitz and I. A. Stegun, Handbook of Mathe-
%                 matical Functions, National Bureau of Standards
%                 Applied Mathematics Series 55, U. S. Department
%                 of Commerce, Tenth Printing (1972) or later.
%               2. D. E. Amos, Computation of Bessel Functions of
%                 Complex Argument, Report SAND83-0086, Sandia National
%                 Laboratories, Albuquerque, NM, May 1983.
%               3. D. E. Amos, Computation of Bessel Functions of
%                 Complex Argument and Large Order, Report SAND83-0643,
%                 Sandia National Laboratories, Albuquerque, NM, May
%                 1983.
%               4. D. E. Amos, A Subroutine Package for Bessel Functions
%                 of a Complex Argument and Nonnegative Order, Report
%                 SAND85-1018, Sandia National Laboratory, Albuquerque,
%                 NM, May 1985.
%               5. D. E. Amos, A portable package for Bessel functions
%                 of a complex argument and nonnegative order, ACM
%                 Transactions on Mathematical Software, 12 (September
%                 1986), pp. 265-273.
%
%***ROUTINES CALLED  CBINU, I1MACH, R1MACH
%***REVISION HISTORY  (YYMMDD)
%   830501  DATE WRITTEN
%   890801  REVISION DATE from Version 3.2
%   910415  Prologue converted to Version 4.0 format.  (BAB)
%   920128  Category corrected.  (WRB)
%   920811  Prologue revised.  (DWL)
%***end PROLOGUE  CBESJ
%
persistent aa alim arg ascle atol az bb ci csgn dig elim firstCall fn fnul hpi i inu inuh ir k k1 k2 nl r1 r1m5 r2 rl rtol tol yy zn ; if isempty(firstCall),firstCall=1;end; 

if isempty(ci), ci=0; end;
if isempty(csgn), csgn=0; end;
if isempty(zn), zn=0; end;
if isempty(aa), aa=0; end;
if isempty(alim), alim=0; end;
if isempty(arg), arg=0; end;
if isempty(dig), dig=0; end;
if isempty(elim), elim=0; end;
if isempty(fnul), fnul=0; end;
if isempty(hpi), hpi=0; end;
if isempty(rl), rl=0; end;
if isempty(r1), r1=0; end;
if isempty(r1m5), r1m5=0; end;
if isempty(r2), r2=0; end;
if isempty(tol), tol=0; end;
if isempty(yy), yy=0; end;
if isempty(az), az=0; end;
if isempty(fn), fn=0; end;
if isempty(bb), bb=0; end;
if isempty(ascle), ascle=0; end;
if isempty(rtol), rtol=0; end;
if isempty(atol), atol=0; end;
if isempty(i), i=0; end;
if isempty(inu), inu=0; end;
if isempty(inuh), inuh=0; end;
if isempty(ir), ir=0; end;
if isempty(k1), k1=0; end;
if isempty(k2), k2=0; end;
if isempty(nl), nl=0; end;
if isempty(k), k=0; end;
if firstCall,   hpi=[1.57079632679489662e0];  end;
firstCall=0;
%
%***FIRST EXECUTABLE STATEMENT  CBESJ
ierr = 0;
nz = 0;
if( fnu<0.0e0 )
ierr = 1;
end;
if( kode<1 || kode>2 )
ierr = 1;
end;
if( n<1 )
ierr = 1;
end;
if( ierr~=0 )
return;
end;
%-----------------------------------------------------------------------
%     SET PARAMETERS RELATED TO MACHINE CONSTANTS.
%     TOL IS THE APPROXIMATE UNIT ROUNDOFF LIMITED TO 1.0E-18.
%     ELIM IS THE APPROXIMATE EXPONENTIAL OVER- AND UNDERFLOW LIMIT.
%     EXP(-ELIM).LT.EXP(-ALIM)=EXP(-ELIM)/TOL    AND
%     EXP(ELIM).GT.EXP(ALIM)=EXP(ELIM)*TOL       ARE INTERVALS NEAR
%     UNDERFLOW AND OVERFLOW LIMITS WHERE SCALED ARITHMETIC IS DONE.
%     RL IS THE LOWER BOUNDARY OF THE ASYMPTOTIC EXPANSION FOR LARGE Z.
%     DIG = NUMBER OF BASE 10 DIGITS IN TOL = 10**(-DIG).
%     FNUL IS THE LOWER BOUNDARY OF THE ASYMPTOTIC SERIES FOR LARGE FNU.
%-----------------------------------------------------------------------
tol = max(r1mach(4),1.0e-18);
[k1 ]=i1mach(12);
[k2 ]=i1mach(13);
[r1m5 ]=r1mach(5);
k = fix(min(abs(k1),abs(k2)));
elim = 2.303e0.*(k.*r1m5-3.0e0);
k1 = fix(i1mach(11) - 1);
aa = r1m5.*k1;
dig = min(aa,18.0e0);
aa = aa.*2.303e0;
alim = elim + max(-aa,-41.45e0);
rl = 1.2e0.*dig + 3.0e0;
fnul = 10.0e0 + 6.0e0.*(dig-3.0e0);
ci = complex(0.0e0,1.0e0);
yy = imag(z);
az = abs(z);
%-----------------------------------------------------------------------
%     TEST FOR RANGE
%-----------------------------------------------------------------------
aa = 0.5e0./tol;
bb = i1mach(9).*0.5e0;
aa = min(aa,bb);
fn = fnu +(n-1);
if( az<=aa )
if( fn<=aa )
aa = sqrt(aa);
if( az>aa )
ierr = 3;
end;
if( fn>aa )
ierr = 3;
end;
%-----------------------------------------------------------------------
%     CALCULATE CSGN=EXP(FNU*HPI*I) TO MINIMIZE LOSSES OF SIGNIFICANCE
%     WHEN FNU IS LARGE
%-----------------------------------------------------------------------
inu = fix(fnu);
inuh = fix(fix(inu./2));
ir = fix(inu - 2.*inuh);
arg =(fnu-(inu-ir)).*hpi;
r1 = cos(arg);
r2 = sin(arg);
csgn = complex(r1,r2);
if( rem(inuh,2)==1 )
csgn = -csgn;
end;
%-----------------------------------------------------------------------
%     ZN IS IN THE RIGHT HALF PLANE
%-----------------------------------------------------------------------
zn = -z.*ci;
if( yy<0.0e0 )
zn = -zn;
csgn = conj(csgn);
ci = conj(ci);
end;
[zn,fnu,kode,n,cy,nz,rl,fnul,tol,elim,alim]=cbinu(zn,fnu,kode,n,cy,nz,rl,fnul,tol,elim,alim);
if( nz>=0 )
nl = fix(n - nz);
if( nl==0 )
return;
end;
rtol = 1.0e0./tol;
ascle = r1mach(1).*rtol.*1.0e+3;
for i = 1 : nl;
%       CY(I)=CY(I)*CSGN
zn = cy(i);
aa = real(zn);
bb = imag(zn);
atol = 1.0e0;
if( max(abs(aa),abs(bb))<=ascle )
zn = zn.*complex(rtol,0.0e0);
atol = tol;
end;
zn = zn.*csgn;
cy(i) = zn.*complex(atol,0.0e0);
csgn = csgn.*ci;
end; i = fix(nl+1);
return;
elseif( nz==(-2) ) ;
nz = 0;
ierr = 5;
return;
else;
nz = 0;
ierr = 2;
return;
end;
end;
end;
nz = 0;
ierr = 4;
end
%DECK CBESK

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