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
***************************************************************************
APPENDIX 3B. REFTAB2: REFERENCES FOR REFTAB1 SHORT SUMMARY
***************************************************************************
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