LOSALAMOS.readme


                    Optical model parameters  
            (Provided by P. Young, 2 December 1997)
            *****************************************
Reproduced below is a full readme file prepared by P. Young:
 
***********************************************************************
     LOS ALAMOS FILES PROVIDED FOR THE IAEA/NDS/RIPL DATA BASE
***********************************************************************
 
  Three files are provided from LOS ALAMOS for the optical model segment 
of the RIPL data base, as follows:
 
LOSALAMOS.README = 
         the present README file which contains (1) a brief description
         of the three LOS ALAMOS computer files supplied to the
         IAEA/NDS for the RIPL library; and, (2) three appendices that
         describe information in the OMLIB.DAT optical model potential
         library:
 
         App. 1 - describes the format (DESC6) used for the present
                  version of the RIPL optical potential library;
         App. 2 - describes the reference numbering system (Ref.System)
                  used for the OMLIB.DAT library;
         App. 3 - provides a short list of the entries in the library
                  (REFTAB1: 1-line per entry) plus a list of references
                  for the entries (REFTAB2).  Both the REFTAB1 and REFTAB2
                  files were made by the OMTABLE code, given in the
                  OMCODE.FOR file.
 
OMLIB.DAT  = 
         (see file LOSALAMOS_OMLIB.DAT in the present directory)
         present version of the optical model potential library for the
         main RIPL optical potential library, as described by the DESC6
         format description given below and utilizing the Ref.System
         numbering criteria given below.  A short summary with
         references is also given below (REFTAB1 and REFTAB2).
 
OMCODE.FOR = 
         (see file LOSALAMOS_OMCODE.FOR in directory OPTICAL.OTHER_FILES)
         a set of two utility codes and two utility subroutines for use
         in handling the OMLIB.DAT optical potential library, as
         follows:
 
         OMIN = subroutine for retrieving data from the optical model
                library OMLIB.DAT.
         OMOUT = subroutine for writing potential data into the format
                 of the RIPL optical model library, e.g., OMLIB.DAT.
         OMSUMRY = fortran code for retrieving and writing a summary of
                   the content of the RIPL optical model library
                   OMLIB.DAT.  All information in the file on authors,
                   reference, and descriptive information are
                   retrieved.
         OMTABLE = fortran code for making an abbreviated or short
                   summary of the content of the OMLIB.DAT potential
                   library, that is, one summary line per entry plus a
                   list of references.  The REFTAB1 and REFTAB2 files
                   below were made with OMTABLE using the current
                   OMLIB.DAT library.
 
 
***********************************************************************
APPENDIX 1.  DESC6:  DESCRIPTION OF THE FORMAT USED FOR THE OMLIB.DAT
***********************************************************************
 
                         LIBRARY PARAMETERS
               (revised by Garg, received 2/20/95)
                    (revised by Young, 3/28/95)
                 (revised by Garg/Young, 4/6/95)
                    (revised by Young, 5/14/96)
          (revised by Young, 11/13/96, 12/22/96, 4/25/97)
iref
author
reference
summary
emin,emax
izmin,izmax
iamin,iamax
imodel,izproj,iaproj
 
       *****LOOP: i=1,5
jrange(i)
       *****LOOP j=1,jrange
epot(i,j)
(rco(i,j,k), k=1,11)
(aco(i,j,k), k=1,11)
(pot(i,j,k), k=1,20)
       *****END i AND j LOOPS
 
jcoul
       *****LOOP j=1,jcoul
ecoul(j),rcoul(j),rcoul0(j),beta(j)
       *****END j LOOP
 
    (1)*****SKIP TO (2)***** IF IMODEL NOT EQUAL TO 1
 
nisotopes
       *****LOOP n=1,nisotopes
iz(n),ia(n),ncoll(n),lmax(n),idef(n),bandk(n),[def(j,n),
                                           j=2,idef(n),2]
       *****LOOP k=1,ncoll(n)
ex(k,n),spin(k,n),ipar(k,n)
       *****END k AND n LOOPS
 
    (2)*****SKIP TO (3)***** IF IMODEL NOT EQUAL TO 2
 
nisotopes
       *****LOOP n=1,nisotopes
iz(n),ia(n),nvib(n)
       *****LOOP k=1,nvib(n)
exv(k,n),spinv(k,n),iparv(k,n),nph(k,n),defv(k,n),thetm(k,n)
       *****END k LOOP
       *****END n LOOP
 
    (3)*****SKIP REMAINING LINES IF IMODEL NOT EQUAL TO 3
 
nisotopes
       *****LOOP n=1,nisotopes
iz(n),ia(n),beta0(n),gamma0(n),xmubeta(n)
       *****END n LOOP
 
                        DEFINITIONS
 
      iref  = unique fixed point reference number for this
              potential
    author  = authors for this potential (up to 80 characters,
              1 line))
 reference  = reference for this potential (up to 80 characters,
              1 line)
    summary = short description of the potential (320 characters,
              4 lines)
 emin,emax  = minimum and maximum energies for validity of this
              potential
izmin,izmax = minimum and maximum Z values for this potential
iamin,iamax = minimum and maximum A values for this potential
    imodel  = 0 for spherical potential
            = 1 for coupled-channel, rotational model
            = 2 for vibrational model
            = 3 for non-axial deformed model
    izproj  = Z for incident projectile
    iaproj  = A for incident projectile
    index i = 1 real potential (Woods-Saxon)
            = 2 surface imaginary potential
            = 3 volume imaginary potential (Woods-Saxon)
            = 4 real spin-orbit potential
            = 5 imaginary spin-orbit potential
    jrange  = number of energy ranges over which the potential is
              specified
            = positive for potential strengths
            = negative for volume integrals
            = 0 if potential of type i not used
  epot(i,j) = upper energy limit for jth energy range for
              potential i
  rco(i,j,k)= coefficients for multiplying A**(1/3) for
              specification of radius R in fm where:
     R(i,j) = {abs[rco(i,j,1)] + rco(i,j,2)*E + rco(i,j,3)*eta
             + rco(i,j,4)/A + rco(i,j,5)/sqrt(A)
             + rco(i,j,6)*A**(2/3) + rco(i,j,7)*A
             + rco(i,j,8)*A**2  + rco(i,j,9)*A**3
             + rco(i,j,10)*A**(1/3)
             + rco(i,j,11)*A**(-1/3)} * [A**(1/3)]
 
and
 
if rco(2,j,1) >0.0: Woods-Saxon derivative surface potential
if rco(2,j,1) <0.0: Gaussian surface potential.
 
[Note that the A dependence of rco(i,j,11) cancels out so that rco(i,j,11)
is equivalent to adding a constant of that magnitude to the radius R(i,j)].
 
 
 aco(i,j,k) = coefficients for specification of diffuseness a in
              fm where:
 
     a(i,j) = abs(aco(i,j,1)) + aco(i,j,2)*E + aco(i,j,3)*eta
                + aco(i,j,4)/A + aco(i,j,5)/sqrt(A)
                + aco(i,j,6)*A**(2/3) + aco(i,j,7)*A
                + aco(i,j,8)*A**2 + aco(i,j,9)*A**3
                + aco(i,j,10)*A**(1/3) + aco(i,j,11)*A**(-1/3)
 
 pot(i,j,k) = strength parameters, as follows:
 
if pot(i,j,k>17) .eq. 0, then
 
V(i,j) = pot(i,j,1) + pot(i,j,7)*eta + pot(i,j,8)*Ecoul
       + pot(i,j,9)*A + pot(i,j,10)*A**(1/3)
       + pot(i,j,11)*A**(-2/3) + pot(i,j,12)*Ecoul2
       + [pot(i,j,2) + pot(i,j,13)*eta + pot(i,j,14)*A]*E
       + pot(i,j,3)*E*E + pot(i,j,4)*E*E*E + pot(i,j,6)*sqrt(E)
       + [pot(i,j,5) + pot(i,j,15)*eta + pot(i,j,16)*E]*ln(E)
       + pot(i,j,17)*Ecoul/E**2
 
if pot(i,j,18) .ne. 0, then
 
V(i,j) = pot(i,j,1) + pot(i,j,2)*eta
       + pot(i,j,3)*cos[2*pi*(A - pot(i,j,4))/pot(i,j,5)]
       + pot(i,j,6)*exp[pot(i,j,7)*E + pot(i,j,8)*E*E]
       + pot(i,j,9)*E*exp[pot(i,j,10)*E**pot(i,j,11)]
 
if pot(i,j,19) .ne. 0, then
 
V(i,j) = [pot(i,j,1) + pot(i,j,2)*eta]/
       {1 + exp[(pot(i,j,3) - E + pot(i,j,4)*Ecoul2)/pot(i,j,5)]}
       + pot(i,j,6)*exp[(pot(i,j,7)*E - pot(i,j,8))/pot(i,j,6)]
 
if pot(i,j,20) .ne. 0, then
 
V(i,j) = pot(i,j,1) + pot(i,j,2)*E
       + pot(i,j,3)*exp[-pot(i,j,4)*(E - pot(i,j,5)*EF)]
       + pot(i,j,6)*[(E-EF)**pot(i,j,8)]/[(E-EF)**pot(i,j,8)
       + pot(i,j,7)**pot(i,j,8)]
       + pot(i,j,9)*exp[-pot(i,j,10)*(E-EF)]*[(E-EF)**pot(i,j,12)]
       /[(E-EF)**pot(i,j,12) + pot(i,j,11)**pot(i,j,12)]
 
where
     E      = projectile laboratory energy in MeV
     eta    = (N-Z)/A
     Ecoul  = 0.4Z/A**(1/3)
     Ecoul2 = 1.73*Z/RC
     EF     = Fermi energy in MeV
            = -0.5*[SN(Z,A) + SN(Z,A+1)]   (for incident neutrons)
            = -0.5*[SP(Z,A) + SP(Z+1,A+1)] (for incident protons)
    SN(Z,A) = the neutron separation energy for nucleus (Z,A)
    SP(Z,A) = the proton separation energy for nucleus (Z,A).
 
And, continuing the definitions:
 
    jcoul    = number of energy ranges for specifying coulomb
               radius and nonlocality range
   ecoul(j)  = maximum energy of coulomb energy range j
   rcoul(j), = coefficients to determine the coulomb radius,
   rcoul0(j)   RC, from the expression
                         RC = rcoul*A**(1/3) + rcoul0
    beta(j)  = nonlocality range.  Note that when beta(j).ne.0.,
               then the imaginary potential is pure derivative
               Woods-Saxon for energy range j.
  nisotopes  = number of isotopes for which deformation parameters
               and discrete levels are given
     iz,ia   = Z and A for the deformation parameters and discrete
               levels that follow
     ncoll   = number of collective states in the coupled-channel
               rotational model for this iz, ia
       lmax  = maximum l value for multipole expansion
       idef  = largest order of deformation
      bandk  = k for the rotational band
        def  = deformation parameters, l=2,4,6,...through lmax
         ex  = rotational level excitation energy (MeV)
       spin  = rotational level spin
       ipar  = rotational level parity
       nvib  = number of vibrational states in the model for this
               iz, ia
        exv  = vibrational level excitation energy (MeV)
      spinv  = vibrational level spin
      iparv  = vibrational level parity
        nph  = 1 for pure 1-photon state
             = 2 for pure 2-photon state
             = 3 for mixture of 1- and 2-photon states
       defv  = vibrational model deformation parameter
      thetm  = mixing parameter (degrees) for nph=3
      beta0  = beta deformability parameter
     gamma0  = gamma deformability parameter
    xmubeta  = non-axiality parameter
 
 
***************************************************************************
APPENDIX 2.  Ref.System:  NUMBERING SYSTEM USED FOR OMLIB.DAT LIBRARY
***************************************************************************
 
   REFERENCE NUMBERING SYSTEM FOR RIPL OPTICAL MODEL POTENTIALS
 
                P. G. Young (24 April 1997)
 
 
DEFINITION  ===>  IREF = 1000*I + JREF
 
 
Incident Particles (leading digit, I)
 
     IREF          I        Particle
 
    1 - 3999     0 - 3      Neutrons
 4000 - 5999     4 - 5      Protons
 6000 - 6999       6        Deuterons
 7000 - 7999       7        Tritons
 8000 - 8999       8        He-3
 9000 - 9999       9        He-4
 
 
Geographic Indicators (trailing 3 digits, JREF)
 
      JREF               Region
 
    1 -  99     Los Alamos National Laboratory (LANL)
  100 - 199     Other U.S. laboratories, universities
  200 - 299     Japan, JAERI
  300 - 399     Russia
  400 - 499     Western Europe, JEF community
  500 - 599     China
  600 - 649     Former Soviet Union
  650 - 699     India, Pakistan
  700 - 799     Others
  800 - 999     Reserved
 
 
***************************************************************************
APPENDIX 3A.  REFTAB1:  SHORT SUMMARY OF ENTRIES IN OMLIB.DAT LIBRARY
***************************************************************************
 
Lib.  Inc.  Model   Z-Range  A-Range    E-Range    Ref.   First
 No. Part.   Type                        (MeV)      No.   Author
 
   1   n    CC rot.  93-93   237-237   0.0- 30.0     1  P.G.Young
   2   n    vibra.   82-82   208-208   0.0-200.0     2  H.Vonach
   3   n    CC rot.  92-92   235-235   0.0- 30.0     1  P.G.Young
   4   n    CC rot.  92-92   237-237   0.0- 30.0     3  P.G.Young
   5   n    CC rot.  92-92   238-238   0.0- 30.0     3  P.G.Young
   6   n    CC rot.  94-94   242-242   0.0- 20.0     4  D.G.Madland
   7   n    CC rot.  94-94   239-239   0.0- 30.0     3  P.G.Young
   8   n    CC rot.  95-95   241-243   0.0- 30.0     5  P.G.Young
   9   n    spher.   90-95   230-250   0.0- 10.0     6  D.G.Madland
  10   n    spher.   26-26    54- 56   0.0- 52.0     7  E.D.Arthur
  11   n    spher.   27-27    59- 59   0.0- 27.5     8  E.D.Arthur
  12   n    spher.   30-30    57- 81   0.0- 20.0     9  P.G.Young
  13   n    spher.   39-39    89- 89   0.0- 21.0    10  E.D.Arthur
  14   n    spher.   40-40    90- 90   0.0- 20.0    10  E.D.Arthur
  15   n    spher.    6- 6    12- 12   0.0- 65.0    11  M.B.Chadwick
  16   n    spher.    7- 7    14- 14   0.0- 60.0    11  M.B.Chadwick
  17   n    spher.    8- 8    16- 16   0.0- 50.0    11  M.B.Chadwick
 100   n    spher.   20-92    40-238  10.0- 50.0    12  F.D.Becchetti
 101   n    spher.   12-83    24-209  11.0- 11.0    13  J.C.Ferrer
 102   n    spher.   82-82   206-208   5.0- 50.0    14  R.W.Finlay
 103   n    spher.   26-26    56- 56   0.0-100.0    15  A.Prince
 104   n    spher.   26-26    54- 54   0.0-100.0    15  A.Prince
 105   n    spher.   26-26    57- 57   0.0-100.0    15  A.Prince
 106   n    spher.   26-26    58- 58   0.0-100.0    15  A.Prince
 107   n    spher.   28-28    58- 58   0.0-100.0    15  A.Prince
 108   n    spher.   28-28    60- 60   0.0-100.0    15  A.Prince
 109   n    spher.   28-28    61- 61   0.0-100.0    15  A.Prince
 110   n    spher.   28-28    62- 62   0.0-100.0    15  A.Prince
 111   n    spher.   28-28    64- 64   0.0-100.0    15  A.Prince
 112   n    spher.   24-24    50- 50   0.0-100.0    15  A.Prince
 113   n    spher.   24-24    53- 53   0.0-100.0    15  A.Prince
 114   n    spher.   24-24    52- 52   0.0-100.0    15  A.Prince
 115   n    spher.   24-24    54- 54   0.0-100.0    15  A.Prince
 116   n    spher.   20-83    40-209   0.0-  5.0    16  P.A.Moldauer
 117   n    spher.   13-13    27- 27   0.0- 60.0    17  J.Petler
 118   n    spher.   39-51    85-125   0.0-  5.0    18  A.B.Smith
 200   n    spher.    0-69     0-146   0.0- 20.0    19  S.Igarasi
 201   n    spher.   69-95   147-999   0.0- 20.0    19  S.Igarasi
 202   n    spher.   33-37    61-107   0.0- 20.0    20  JAERI NDC
 203   n    spher.   38-42    69-116   0.0- 20.0    20  JAERI NDC
 204   n    spher.   43-45    80-125   0.0- 20.0    20  JAERI NDC
 205   n    spher.   46-48    89-134   0.0- 20.0    20  JAERI NDC
 206   n    spher.   49-51    97-141   0.0- 20.0    20  JAERI NDC
 207   n    spher.   52-54   103-150   0.0- 20.0    20  JAERI NDC
 208   n    spher.   55-55   111-153   0.0- 20.0    20  JAERI NDC
 209   n    spher.   56-56   112-154   0.0- 20.0    20  JAERI NDC
 210   n    spher.   57-58   117-156   0.0- 20.0    20  JAERI NDC
 211   n    spher.   59-59   119-160   0.0- 20.0    20  JAERI NDC
 212   n    spher.   60-60   141-143   0.0- 20.0    20  JAERI NDC
 213   n    spher.   60-60   144-148   0.0- 20.0    20  JAERI NDC
 214   n    spher.   60-60   150-999   0.0- 20.0    20  JAERI NDC
 215   n    spher.   61-61   147-999   0.0- 20.0    20  JAERI NDC
 216   n    spher.   62-62   144-144   0.0- 20.0    20  JAERI NDC
 217   n    spher.   62-62   147-147   0.0- 20.0    20  JAERI NDC
 218   n    spher.   62-62   148-148   0.0- 20.0    20  JAERI NDC
 219   n    spher.   62-62   149-149   0.0- 20.0    20  JAERI NDC
 220   n    spher.   62-62   150-150   0.0- 20.0    20  JAERI NDC
 221   n    spher.   63-63   151-999   0.0- 20.0    20  JAERI NDC
 222   n    spher.   64-64   133-171   0.0- 20.0    20  JAERI NDC
 223   n    spher.   65-65   138-175   0.0- 20.0    20  JAERI NDC
 400   n    CC rot.  79-79   197-197   0.0- 57.0    21  J.P.Delaroche
 401   n    spher.   20-92    40-238   0.0- 25.0    22  D.Wilmore
 402   n    spher.   83-83   209-209   0.0- 30.0    23  O.Bersillon
 403   n    spher.   74-74   182-186   0.0- 30.0    24  J.P.Delaroche
 404   n    spher.   23-41    50- 95   0.0- 30.0    25  B.Strohmaier
 600   n    CC rot.  90-**   227-260   0.0- 20.0    26  G.Vladuca
 800   n    spher.   20-83    40-210   0.0-155.0    27  C.A.Engelbrecht
2001   n    spher.   13-82    12-208  50.0-400.0    28  D.G.Madland
2002   n    CC rot.  74-74   182-186   0.0-100.0    29  P.G.Young
2003   n    CC rot.  67-69   165-169   0.0-100.0    30  E.D.Arthur
2004   n    CC rot.  63-63   151-153   0.0- 20.0    31  R.Macklin
2005   n    CC rot.  75-75   185-187   0.0- 20.0    32  R.Macklin
2006   n    CC rot.  92-92   238-238   0.0-200.0    33  P.G.Young
2100   n    spher.   20-83    40-209  10.0- 26.0    34  R.L.Varner
2101   n    spher.   26-82    54-208  10.0- 80.0    35  R.L.Walter
2404   n    spher.   40-40    90- 90   0.0-200.0    36  A.J.Koning
4000   p    spher.   25-26    54- 56   0.0- 28.0    37  E.D.Arthur
4001   p    spher.   26-27    59- 59   0.0- 23.0    38  E.D.Arthur
4002   p    spher.   38-38    88- 89   0.0- 21.0    39  E.D.Arthur
4003   p    spher.   39-39    89- 89   0.0- 21.0    39  E.D.Arthur
4004   p    CC rot.  79-79   197-197   0.0- 57.0    40  P.G.Young
4015   p    spher.    6- 6    12- 12   0.0- 65.0    41  M.B.Chadwick
4016   p    spher.    7- 7    14- 14   0.0- 70.0    41  M.B.Chadwick
4017   p    spher.    8- 8    16- 16   0.0- 50.0    41  M.B.Chadwick
4100   p    spher.   16-49    30-100   0.0- 22.0    42  F.G.Perey
4101   p    spher.   20-83    40-209  10.0- 50.0    43  F.D.Becchetti
4102   p    spher.    6-82    12-208  30.0- 60.0    44  J.J.H.Menet
4103   p    spher.   26-26    56- 56  50.0- 50.0    45  G.S.Mani
4104   p    spher.   28-28    58- 58 100.0-100.0    46  K.Kwiatkowski
4105   p    spher.   40-40    90- 90 100.0-100.0    46  K.Kwiatkowski
4106   p    spher.   50-50   120-120 100.0-100.0    46  K.Kwiatkowski
4107   p    spher.   82-82   208-208 100.0-100.0    46  K.Kwiatkowski
4108   p    spher.   20-82    48-208  25.0- 45.0    47  D.M.Patterson
4109   p    spher.   39-39    89- 89   1.0-  7.0    48  C.H.Johnson
4110   p    spher.   41-41    93- 93   1.0-  7.0    48  C.H.Johnson
4111   p    spher.   45-45   103-103   1.0-  7.0    48  C.H.Johnson
4112   p    spher.   46-46   105-105   1.0-  7.0    48  C.H.Johnson
4113   p    spher.   47-47   107-107   1.0-  7.0    48  C.H.Johnson
4114   p    spher.   47-47   109-109   1.0-  7.0    48  C.H.Johnson
4115   p    spher.   48-48   110-110   1.0-  7.0    48  C.H.Johnson
4116   p    spher.   48-48   111-111   1.0-  7.0    48  C.H.Johnson
4117   p    spher.   48-48   113-113   1.0-  7.0    48  C.H.Johnson
4118   p    spher.   48-48   114-114   1.0-  7.0    48  C.H.Johnson
4119   p    spher.   49-49   115-115   1.0-  7.0    48  C.H.Johnson
4120   p    spher.   50-50   116-116   1.0-  7.0    48  C.H.Johnson
4121   p    spher.   50-50   122-122   1.0-  7.0    48  C.H.Johnson
4122   p    spher.   50-50   124-124   1.0-  7.0    48  C.H.Johnson
4123   p    spher.   52-52   128-128   1.0-  7.0    48  C.H.Johnson
4124   p    spher.   52-52   130-130   1.0-  7.0    48  C.H.Johnson
4125   p    spher.   40-40    92- 92   2.0-  7.0    49  D.S.Flynn
4126   p    spher.   40-40    94- 94   2.0-  7.0    49  D.S.Flynn
4127   p    spher.   40-40    96- 96   2.0-  7.0    49  D.S.Flynn
4128   p    spher.   42-42    95- 95   2.0-  7.0    49  D.S.Flynn
4129   p    spher.   42-42    98- 98   2.0-  7.0    49  D.S.Flynn
4130   p    spher.   42-42   100-100   2.0-  7.0    49  D.S.Flynn
4200   p    spher.    8- 8    16- 16  65.0- 65.0    50  H.Sagaguchi
4201   p    spher.   10-10    20- 20  65.0- 65.0    50  H.Sagaguchi
4202   p    spher.   12-12    24- 24  65.0- 65.0    50  H.Sagaguchi
4203   p    spher.   14-14    28- 28  65.0- 65.0    50  H.Sagaguchi
4204   p    spher.   18-18    40- 40  65.0- 65.0    50  H.Sagaguchi
4205   p    spher.   20-20    40- 40  65.0- 65.0    50  H.Sagaguchi
4206   p    spher.   20-20    44- 44  65.0- 65.0    50  H.Sagaguchi
4207   p    spher.   20-20    48- 48  65.0- 65.0    50  H.Sagaguchi
4208   p    spher.   22-22    46- 46  65.0- 65.0    50  H.Sagaguchi
4209   p    spher.   22-22    48- 48  65.0- 65.0    50  H.Sagaguchi
4210   p    spher.   22-22    50- 50  65.0- 65.0    50  H.Sagaguchi
4211   p    spher.   26-26    54- 54  65.0- 65.0    50  H.Sagaguchi
4212   p    spher.   26-26    56- 56  65.0- 65.0    50  H.Sagaguchi
4213   p    spher.   27-27    59- 59  65.0- 65.0    50  H.Sagaguchi
4214   p    spher.   28-28    58- 58  65.0- 65.0    50  H.Sagaguchi
4215   p    spher.   28-28    60- 60  65.0- 65.0    50  H.Sagaguchi
4216   p    spher.   28-28    62- 62  65.0- 65.0    50  H.Sagaguchi
4217   p    spher.   28-28    64- 64  65.0- 65.0    50  H.Sagaguchi
4218   p    spher.   39-39    89- 89  65.0- 65.0    50  H.Sagaguchi
4219   p    spher.   40-40    90- 90  65.0- 65.0    50  H.Sagaguchi
4220   p    spher.   42-42    98- 98  65.0- 65.0    50  H.Sagaguchi
4221   p    spher.   42-42   100-100  65.0- 65.0    50  H.Sagaguchi
4222   p    spher.   62-62   144-144  65.0- 65.0    50  H.Sagaguchi
4223   p    spher.   82-82   208-208  65.0- 65.0    50  H.Sagaguchi
4224   p    spher.   83-83   209-209  65.0- 65.0    50  H.Sagaguchi
4401   p    spher.   42-42    92- 92  22.3- 22.3    51  E.Cereda
4402   p    spher.   42-42    94- 94  22.3- 22.3    51  E.Cereda
4403   p    spher.   42-42    96- 96  22.3- 22.3    51  E.Cereda
4404   p    spher.   42-42    98- 98  22.3- 22.3    51  E.Cereda
4405   p    spher.   42-42   100-100  22.3- 22.3    51  E.Cereda
4406   p    spher.   44-44   102-102  22.3- 22.3    51  E.Cereda
4407   p    spher.   46-46   104-104  22.3- 22.3    51  E.Cereda
4408   p    spher.   46-46   106-106  22.3- 22.3    51  E.Cereda
4409   p    spher.   46-46   108-108  22.3- 22.3    51  E.Cereda
4410   p    spher.   46-46   110-110  22.3- 22.3    51  E.Cereda
4411   p    spher.   48-48   106-106  22.3- 22.3    51  E.Cereda
4412   p    spher.   48-48   110-110  22.3- 22.3    51  E.Cereda
4413   p    spher.   48-48   112-112  22.3- 22.3    51  E.Cereda
4414   p    spher.   48-48   116-116  22.3- 22.3    51  E.Cereda
4415   p    spher.   47-47   109-109   6.1-  6.1    52  A.Feigel
4650   p    spher.   21-21    45- 45   3.0-  5.0    53  S.Kailas
4651   p    spher.   20-20    48- 48   3.0-  5.0    53  S.Kailas
4652   p    spher.   23-23    51- 51   3.0-  5.0    53  S.Kailas
4653   p    spher.   24-24    54- 54   3.0-  5.0    53  S.Kailas
4654   p    spher.   27-27    59- 59   3.0-  5.0    53  S.Kailas
4655   p    spher.   28-28    61- 61   3.0-  5.0    53  S.Kailas
4656   p    spher.   29-29    65- 65   3.0-  5.0    53  S.Kailas
4657   p    spher.   31-31    71- 71   3.0-  5.0    53  S.Kailas
4658   p    spher.   33-33    75- 75   3.0-  5.0    53  S.Kailas
4659   p    spher.   34-34    80- 80   3.0-  5.0    53  S.Kailas
4660   p    spher.   19-19    41- 41   1.0-  7.0    54  Y.P.Viyogi
4661   p    spher.   21-21    45- 45   1.0-  7.0    54  Y.P.Viyogi
4662   p    spher.   20-20    48- 48   1.0-  7.0    54  Y.P.Viyogi
4663   p    spher.   22-22    49- 49   1.0-  7.0    54  Y.P.Viyogi
4664   p    spher.   23-23    51- 51   1.0-  7.0    54  Y.P.Viyogi
4665   p    spher.   25-25    55- 55   1.0-  7.0    54  Y.P.Viyogi
4666   p    spher.   27-27    59- 59   1.0-  7.0    54  Y.P.Viyogi
4667   p    spher.   28-28    61- 61   1.0-  7.0    54  Y.P.Viyogi
4668   p    spher.   29-29    65- 65   1.0-  7.0    54  Y.P.Viyogi
4669   p    spher.   30-30    68- 68   1.0-  7.0    54  Y.P.Viyogi
4670   p    spher.   31-31    71- 71   1.0-  7.0    54  Y.P.Viyogi
4671   p    spher.   33-33    75- 75   1.0-  7.0    54  Y.P.Viyogi
4672   p    spher.   34-34    80- 80   1.0-  7.0    54  Y.P.Viyogi
4673   p    spher.   39-39    89- 89   1.0-  7.0    54  Y.P.Viyogi
4674   p    spher.   41-41    93- 93   1.0-  7.0    54  Y.P.Viyogi
4675   p    spher.   42-42    96- 96   1.0-  7.0    54  Y.P.Viyogi
4676   p    spher.   42-42    98- 98   1.0-  7.0    54  Y.P.Viyogi
4677   p    spher.   45-45   103-103   1.0-  7.0    54  Y.P.Viyogi
4678   p    spher.   46-46   105-105   1.0-  7.0    54  Y.P.Viyogi
4679   p    spher.   47-47   107-107   1.0-  7.0    54  Y.P.Viyogi
4680   p    spher.   47-47   109-109   1.0-  7.0    54  Y.P.Viyogi
4681   p    spher.   48-48   110-110   1.0-  7.0    54  Y.P.Viyogi
4682   p    spher.   49-49   115-115   1.0-  7.0    54  Y.P.Viyogi
4683   p    spher.   50-50   120-120   1.0-  7.0    54  Y.P.Viyogi
4684   p    spher.   50-50   124-124   1.0-  7.0    54  Y.P.Viyogi
4685   p    spher.   52-52   128-128   1.0-  7.0    54  Y.P.Viyogi
4686   p    spher.   52-52   130-130   1.0-  7.0    54  Y.P.Viyogi
5001   p    spher.   13-82    12-208  50.0-400.0    28  D.G.Madland
5002   p    CC rot.  74-74   182-186   0.0-100.0    29  P.G.Young
5003   p    CC rot.  67-69   165-169   0.0-100.0    30  E.D.Arthur
5004   p    CC rot.  63-63   151-153   0.0- 20.0    31  R.Macklin
5005   p    CC rot.  75-75   185-187   0.0- 20.0    32  R.Macklin
5006   p    CC rot.  92-92   238-238   0.0-200.0    33  P.G.Young
5100   p    spher.   20-83    40-209  16.0- 65.0    34  R.L.Varner
5101   p    spher.   26-82    54-208  10.0- 80.0    55  R.L.Walter
5404   p    spher.   40-40    90- 90   0.0-200.0    36  A.J.Koning
6001   d    spher.   20-82    40-208  11.0- 27.0    56  C.M.Perey
6100   d    spher.   20-83    40-209   8.0- 13.0    57  J.M.Lohr
6300   d    spher.   22-22    48- 48  13.6- 13.6    58  O.P.Bilanyuk
6301   d    spher.   24-24    52- 52  13.6- 13.6    58  O.P.Bilanyuk
6302   d    spher.   24-24    54- 54  13.6- 13.6    58  O.P.Bilanyuk
6400   d    spher.    6-82    12-208  20.0-100.0    59  J.Bojowald
7001   t    spher.   20-20    40- 40  17.0- 17.0    60  R.Hardekopf
7002   t    spher.   22-22    46- 46  17.0- 17.0    60  R.Hardekopf
7003   t    spher.   22-22    48- 48  17.0- 17.0    60  R.Hardekopf
7004   t    spher.   26-26    54- 54  17.0- 17.0    60  R.Hardekopf
7005   t    spher.   26-26    56- 56  17.0- 17.0    60  R.Hardekopf
7006   t    spher.   28-28    58- 58  17.0- 17.0    60  R.Hardekopf
7007   t    spher.   28-28    60- 60  17.0- 17.0    60  R.Hardekopf
7008   t    spher.   30-30    68- 68  17.0- 17.0    60  R.Hardekopf
7009   t    spher.   40-40    90- 90  17.0- 17.0    60  R.Hardekopf
7010   t    spher.   40-40    94- 94  17.0- 17.0    60  R.Hardekopf
7011   t    spher.   50-50   116-116  17.0- 17.0    60  R.Hardekopf
7012   t    spher.   58-58   140-140  17.0- 17.0    60  R.Hardekopf
7013   t    spher.   82-82   208-208  17.0- 17.0    60  R.Hardekopf
7100   t    spher.   20-82    40-208   1.0- 40.0    61  F.D.Becchetti
7101   t    spher.   20-20    40- 40  20.0- 20.0    62  P.P.Urone
7102   t    spher.   24-24    52- 52  20.0- 20.0    62  P.P.Urone
7103   t    spher.   26-26    54- 54  20.0- 20.0    62  P.P.Urone
7104   t    spher.   28-28    62- 62  20.0- 20.0    62  P.P.Urone
7105   t    spher.   28-28    64- 64  20.0- 20.0    62  P.P.Urone
7106   t    spher.   40-40    90- 90  20.0- 20.0    62  P.P.Urone
7107   t    spher.   40-40    92- 92  20.0- 20.0    62  P.P.Urone
7108   t    spher.   40-40    94- 94  20.0- 20.0    62  P.P.Urone
7109   t    spher.   50-50   118-118  20.0- 20.0    62  P.P.Urone
7110   t    spher.   12-12    26- 26  17.0- 17.0    63  P.Schwandt
7111   t    spher.   13-13    27- 27  17.0- 17.0    63  P.Schwandt
7112   t    spher.   14-14    28- 28  17.0- 17.0    63  P.Schwandt
8100  3He   spher.   20-82    40-208   1.0- 40.0    61  F.D.Becchetti
8101  3He   spher.   20-20    40- 40  21.0- 84.0    64  H.H.Chang
8102  3He   spher.   28-28    58- 58  22.0- 84.0    64  H.H.Chang
8103  3He   spher.   28-28    60- 60  29.6- 29.6    65  C.B.Fulmer
8104  3He   spher.   28-28    60- 60  35.1- 35.1    65  C.B.Fulmer
8105  3He   spher.   28-28    60- 60  49.7- 49.7    65  C.B.Fulmer
8106  3He   spher.   28-28    60- 60  59.8- 59.8    65  C.B.Fulmer
8107  3He   spher.   28-28    60- 60  71.1- 71.1    65  C.B.Fulmer
8108  3He   spher.   20-20    40- 40  21.0- 21.0    66  P.P.Urone
8109  3He   spher.   24-24    52- 52  21.0- 21.0    66  P.P.Urone
8110  3He   spher.   26-26    54- 54  21.0- 21.0    66  P.P.Urone
8111  3He   spher.   28-28    62- 62  21.0- 21.0    66  P.P.Urone
8112  3He   spher.   28-28    64- 64  21.0- 21.0    66  P.P.Urone
8113  3He   spher.   40-40    90- 90  21.0- 21.0    66  P.P.Urone
8114  3He   spher.   40-40    92- 92  21.0- 21.0    66  P.P.Urone
8115  3He   spher.   40-40    94- 94  21.0- 21.0    66  P.P.Urone
8116  3He   spher.   50-50   118-118  21.0- 21.0    66  P.P.Urone
8200  3He   spher.   20-20    40- 40 109.2-109.2    67  M.Hyakutake
8201  3He   spher.   28-28    58- 58 109.2-109.2    67  M.Hyakutake
8202  3He   spher.   40-40    90- 90 109.2-109.2    67  M.Hyakutake
8203  3He   spher.   50-50   116-116 109.2-109.2    67  M.Hyakutake
8204  3He   spher.   28-28    58- 58  89.3- 89.3    67  M.Hyakutake
8205  3He   spher.   28-28    58- 58 118.5-118.5    67  M.Hyakutake
8400  3He   spher.   12-12    24- 24 130.0-130.0    68  A.Djaloeis
8401  3He   spher.   40-40    90- 90 130.0-130.0    68  A.Djaloeis
8402  3He   spher.   50-50   120-120 130.0-130.0    68  A.Djaloeis
8403  3He   spher.   82-82   208-208 130.0-130.0    68  A.Djaloeis
8404  3He   spher.    3- 3     6-  6 217.0-217.0    69  N.Willis
8405  3He   spher.    4- 4     9-  9 217.0-217.0    69  N.Willis
8406  3He   spher.    6- 6    12- 12 217.0-217.0    69  N.Willis
8407  3He   spher.   14-14    28- 28 217.0-217.0    69  N.Willis
8408  3He   spher.   20-20    40- 40 217.0-217.0    69  N.Willis
8409  3He   spher.   28-28    58- 58 217.0-217.0    69  N.Willis
8410  3He   spher.   39-39    89- 89 217.0-217.0    69  N.Willis
8411  3He   spher.   40-40    90- 90 217.0-217.0    69  N.Willis
8412  3He   spher.   50-50   120-120 217.0-217.0    69  N.Willis
8413  3He   spher.   82-82   208-208 217.0-217.0    69  N.Willis
8414  3He   spher.    5- 5    10- 10  41.0- 41.0    70  H.J.Trost
8415  3He   spher.    6- 6    12- 12  41.0- 41.0    70  H.J.Trost
8416  3He   spher.    6- 6    13- 13  41.0- 41.0    70  H.J.Trost
8417  3He   spher.    8- 8    16- 16  41.0- 41.0    70  H.J.Trost
8418  3He   spher.    8- 8    18- 18  41.0- 41.0    70  H.J.Trost
8419  3He   spher.   11-11    23- 23  41.0- 41.0    70  H.J.Trost
8420  3He   spher.   12-12    24- 24  41.0- 41.0    70  H.J.Trost
8421  3He   spher.   12-12    25- 25  41.0- 41.0    70  H.J.Trost
8422  3He   spher.   12-12    26- 26  41.0- 41.0    70  H.J.Trost
8423  3He   spher.   13-13    27- 27  41.0- 41.0    70  H.J.Trost
8424  3He   spher.   20-20    40- 40  41.0- 41.0    70  H.J.Trost
8425  3He   spher.   28-28    58- 58  41.0- 41.0    70  H.J.Trost
8650  3He   spher.   28-28    58- 58 270.0-270.0    71  P.P.Singh
8651  3He   spher.   40-40    90- 90 270.0-270.0    71  P.P.Singh
8652  3He   spher.   50-50   116-116 270.0-270.0    71  P.P.Singh
8653  3He   spher.   82-82   208-208 270.0-270.0    71  P.P.Singh
9000  4He   spher.   13-26    27- 56   1.0-100.0    72  E.D.Arthur
9001  4He   spher.   27-27    59- 59   1.0-100.0    73  E.D.Arthur
9100  4He   spher.    8-82    16-208   1.0- 25.0    74  L.McFadden
9101  4He   spher.   10-92    20-235   1.0- 46.0    75  J.R.Huizenga
9400  4He   spher.   20-45    40-100   1.0- 30.0    76  B.Strohmaier
9401  4He   spher.   22-30    37- 86  20.0- 30.0    77  O.F.Lemos
9600  4He   spher.    8-96    16-250   1.0- 73.0    78  V.Avrigeanu
 
 
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APPENDIX 3B.  REFTAB2:  REFERENCES FOR REFTAB1 SHORT SUMMARY
***************************************************************************
 
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