ENTRY 11139 20210317 148311139 0 1 SUBENT 11139001 20210317 148311139 1 1 BIB 8 29 11139 1 2 TITLE The Slow Neutron Cross Sections of Indium, Gold, 11139 1 3 Silver, Antimony, Lithium, and Mercury as Measured 11139 1 4 with a Neutron Beam Spectrometer 11139 1 5 AUTHOR (W.W.Havens Jr,J.Rainwater) 11139 1 6 REFERENCE (J,PR,70,154,1946) 11139 1 7 #doi:10.1103/PhysRev.70.154 11139 1 8 INSTITUTE (1USACOL) 11139 1 9 FACILITY (CYCLO,1USACOL) 11139 1 10 METHOD (TRN,TOF) The variations of the slow neutron 11139 1 11 transmissions of In, Au, Ag, Sb, Li, and Hg have been 11139 1 12 investigated as a function of the time-of-flight of 11139 1 13 the incident neutrons for a 5.4-meter path by use of 11139 1 14 a neutron beam spectrometer. 11139 1 15 COMMENT Compiler's comment: Plots were digitized vs. neutron 11139 1 16 time of flight in microsec/meter and converted to 11139 1 17 energy by compiler using the relation 11139 1 18 E = (72.3/t)**2 eV which gives the neutron 11139 1 19 energy for a timing t, microsec/meter from. Formula 11139 1 20 was taken from Phys. Rev. 71, 165 (1947) and verified 11139 1 21 using the method of visual inspection. Transmission 11139 1 22 data are more reliable, while cross section scale is 11139 1 23 less obvious. 11139 1 24 HISTORY (19760628T) Translated from SCISRS. 11139 1 25 (19800814A) Converted to reaction formalism. 11139 1 26 (20210317A) BP: Updated to new date formats, lower 11139 1 27 case. Corrections according last EXFOR rules and 11139 1 28 Dict. Added thermal cross section data based on cross 11139 1 29 section curve approximations, sample, method and doi. 11139 1 30 Digitized the data. Subentries 10-33 were added. 11139 1 31 ENDBIB 29 0 11139 1 32 NOCOMMON 0 0 11139 1 33 ENDSUBENT 32 0 11139 199999 SUBENT 11139002 20210317 148311139 2 1 BIB 7 31 11139 2 2 REACTION (3-LI-0(N,ABS),,SIG) 11139 2 3 REL-REF (R,,H.H.Goldsmith+,J,PR,50,328,1936) 11139 2 4 (R,,G.A.Fink,J,PR,50,738,1936) Fluorine cross sections.11139 2 5 SAMPLE This salt was tightly packed in an aluminum container 11139 2 6 such that there were 4.85 g/cm2 of LiF and 0.418 11139 2 7 g/cm2 of aluminum in the beam for the thicker sample 11139 2 8 and 0.862 g/cm2 of LiF and 0.418 g/cm2 of aluminum in 11139 2 9 the beam for the thinner sample. The lithium fluoride 11139 2 10 was obtained from the City Chemical Corporation and 11139 2 11 was of analytical reagent grade. The salt was dried 11139 2 12 at 120 degrees C for 48 hours before being packed in 11139 2 13 the container. 11139 2 14 ANALYSIS If the cross section of aluminum is assumed to be 11139 2 15 1.5x10**(-24) cm2/atom, and that of fluorine 11139 2 16 2.5x10**(-24) cm2/atom and these cross sections are 11139 2 17 assumed constant over the energy interval studied, 11139 2 18 then the absorption due to the aluminum and the 11139 2 19 fluorine will be equivalent to a reduction in the 11139 2 20 transmission to T=0.938 for the 0.862 g/cm2 sample 11139 2 21 and to T=0.826 for the 4.85 g/cm2 sample. The 11139 2 22 experimental results then indicate that the slow 11139 2 23 neutron cross section of lithium follows a 1/v law 11139 2 24 and may be expressed as the sum of a constant term 11139 2 25 and a 1/v term: sigma = [(11.5+- 0.2) *E**-1/2 + 11139 2 26 (1.7+- 0.2) ]*10**-24 cm2/atom if the cross section 11139 2 27 of fluorine is assumed to be constant at 2.5x10**24 11139 2 28 cm2/atom. E is the neutron energy in eV. 11139 2 29 ERR-ANALYS (DATA-ERR) Cross section curve calculations. 11139 2 30 HISTORY (20210317A) BP: Added sample and analysis, corrected 11139 2 31 cross section values using formula. 11139 2 32 STATUS (TABLE) Page 169. 11139 2 33 ENDBIB 31 0 11139 2 34 NOCOMMON 0 0 11139 2 35 DATA 3 1 11139 2 36 EN DATA DATA-ERR 11139 2 37 EV B B 11139 2 38 2.53E-02 7.40E+01 1.45 11139 2 39 ENDDATA 3 0 11139 2 40 ENDSUBENT 39 0 11139 299999 SUBENT 11139003 20210317 148311139 3 1 BIB 6 17 11139 3 2 REACTION (3-LI-0(N,TOT),,SIG) 11139 3 3 SAMPLE This salt was tightly packed in an aluminum container 11139 3 4 such that there were 4.85 g/cm2 of LiF and 0.418 11139 3 5 g/cm2. The lithium fluoride was obtained from the 11139 3 6 City Chemical Corporation and was of analytical 11139 3 7 reagent grade. The salt was dried at 120 degrees C 11139 3 8 for 48 hours before being packed in the container. 11139 3 9 METHOD Resolution width was approximately 20 microsec/meter. 11139 3 10 ANALYSIS Outside resonances, the cross section from the 11139 3 11 experimental transmission T by using the formula 11139 3 12 T=exp(-n sigma), where n is the number of atoms per 11139 3 13 cm2 in the sample. 11139 3 14 STATUS (DEP,11139013) 11139 3 15 (CURVE) Fig. 14, page 168; values converted by 11139 3 16 compiler as described under the compiler's comment. 11139 3 17 HISTORY (20210317A) BP: Replaced SCISRS data with plot 11139 3 18 digitization. 11139 3 19 ENDBIB 17 0 11139 3 20 NOCOMMON 0 0 11139 3 21 DATA 2 11 11139 3 22 EN DATA 11139 3 23 EV B 11139 3 24 31.696 1.563 11139 3 25 12.474 2.393 11139 3 26 6.767 4.220 11139 3 27 3.420 5.568 11139 3 28 2.715 6.844 11139 3 29 1.950 8.465 11139 3 30 1.525 9.810 11139 3 31 1.145 11.364 11139 3 32 0.784 14.089 11139 3 33 0.647 15.607 11139 3 34 0.553 16.919 11139 3 35 ENDDATA 13 0 11139 3 36 ENDSUBENT 35 0 11139 399999 SUBENT 11139004 20210317 148311139 4 1 BIB 6 22 11139 4 2 REACTION (47-AG-0(N,TOT),,SIG) 11139 4 3 SAMPLE A 19.8 g/cm2 disk of metallic silver was used. A 11139 4 4 preliminary run on the thin sample in the thermal 11139 4 5 region gave sufficient data to indicate the thickness 11139 4 6 of the sample which would give best results in this 11139 4 7 region. Therefore, the thick sample was cut 11139 4 8 approximately in half and a sample containing 7.84 11139 4 9 g/cm2 was used for the rest of the measurements an 11139 4 10 silver. 11139 4 11 METHOD Resolution width was approximately 50 microsec/meter. 11139 4 12 ANALYSIS Outside resonances, the cross section from the 11139 4 13 experimental transmission T by using the formula 11139 4 14 T=exp(-n sigma), where n is the number of atoms per 11139 4 15 cm2 in the sample. Silver cross sections can be 11139 4 16 expressed as sigma = [(4.2+-0.3) + (0.64+-0.02)*E**(-1/11139 4 17 2)]x10**(-24) cm2/atom. E is the neutron energy in eV. 11139 4 18 STATUS (DEP,11139016) 11139 4 19 (CURVE) Fig. 10, page 164; values converted by 11139 4 20 compiler as described under the compiler's comment. 11139 4 21 HISTORY (19820107U) BIB update. 11139 4 22 (20210317A) BP: Replaced BNL-325 data with plot 11139 4 23 digitization. 11139 4 24 ENDBIB 22 0 11139 4 25 NOCOMMON 0 0 11139 4 26 DATA 2 49 11139 4 27 EN DATA 11139 4 28 EV B 11139 4 29 432.879 7.676 11139 4 30 93.878 9.714 11139 4 31 88.902 12.710 11139 4 32 48.581 14.749 11139 4 33 11.067 12.151 11139 4 34 10.907 14.466 11139 4 35 8.703 33.797 11139 4 36 8.084 9.969 11139 4 37 6.838 60.753 11139 4 38 5.235 99.417 11139 4 39 4.342 70.005 11139 4 40 2.766 29.967 11139 4 41 2.670 22.614 11139 4 42 2.284 18.934 11139 4 43 2.064 17.706 11139 4 44 1.705 16.612 11139 4 45 1.367 17.423 11139 4 46 1.005 17.549 11139 4 47 0.771 16.995 11139 4 48 0.723 19.443 11139 4 49 0.531 20.110 11139 4 50 0.457 21.464 11139 4 51 0.436 20.236 11139 4 52 0.334 24.578 11139 4 53 0.246 25.239 11139 4 54 0.204 26.995 11139 4 55 0.165 29.837 11139 4 56 0.136 31.453 11139 4 57 0.119 34.300 11139 4 58 0.098 35.232 11139 4 59 0.084 36.576 11139 4 60 0.074 40.508 11139 4 61 0.065 42.262 11139 4 62 0.057 45.782 11139 4 63 0.051 47.535 11139 4 64 0.045 50.375 11139 4 65 0.037 53.337 11139 4 66 0.033 56.042 11139 4 67 0.032 59.162 11139 4 68 0.028 61.454 11139 4 69 0.026 64.432 11139 4 70 0.024 64.275 11139 4 71 0.022 69.159 11139 4 72 0.020 70.504 11139 4 73 0.019 70.757 11139 4 74 0.018 75.779 11139 4 75 0.017 73.993 11139 4 76 0.016 74.925 11139 4 77 0.015 81.720 11139 4 78 ENDDATA 51 0 11139 4 79 ENDSUBENT 78 0 11139 499999 SUBENT 11139005 20210317 148311139 5 1 BIB 6 17 11139 5 2 REACTION (80-HG-0(N,TOT),,SIG) 11139 5 3 SAMPLE The mercury was U.S.P. XII redistilled - purchased 11139 5 4 from the Mallinkrodt Chemical Works. For the 11139 5 5 preliminary investigation of the entire transmission 11139 5 6 curve of mercury, a sample containing 3.25 g/cm2 of 11139 5 7 the liquid was used. 11139 5 8 METHOD Resolution width was approximately 100 microsec/meter. 11139 5 9 ANALYSIS Outside resonances, the cross section from the 11139 5 10 experimental transmission T by using the formula 11139 5 11 T=exp(-n sigma), where n is the number of atoms per 11139 5 12 cm2 in the sample 11139 5 13 STATUS (DEP,11139019) 11139 5 14 (CURVE) Fig. 16, page 169; values converted by 11139 5 15 compiler as described under the compiler's comment. 11139 5 16 HISTORY (19820107U) BIB update. 11139 5 17 (20210317A) BP: Replaced BNL-325 data with plot 11139 5 18 digitization. 11139 5 19 ENDBIB 17 0 11139 5 20 NOCOMMON 0 0 11139 5 21 DATA 2 33 11139 5 22 EN DATA 11139 5 23 EV B 11139 5 24 7661.548 13.106 11139 5 25 72.078 19.348 11139 5 26 67.563 15.603 11139 5 27 16.428 21.220 11139 5 28 7.841 21.220 11139 5 29 3.194 21.220 11139 5 30 2.106 33.078 11139 5 31 1.256 44.936 11139 5 32 0.958 54.922 11139 5 33 0.755 61.787 11139 5 34 0.592 81.759 11139 5 35 0.478 77.390 11139 5 36 0.412 91.121 11139 5 37 0.351 98.610 11139 5 38 0.316 117.333 11139 5 39 0.254 127.319 11139 5 40 0.241 134.809 11139 5 41 0.206 139.177 11139 5 42 0.181 145.418 11139 5 43 0.170 154.780 11139 5 44 0.151 168.511 11139 5 45 0.118 192.851 11139 5 46 0.097 210.326 11139 5 47 0.086 225.929 11139 5 48 0.077 247.149 11139 5 49 0.065 257.759 11139 5 50 0.051 288.340 11139 5 51 0.046 306.440 11139 5 52 0.040 327.035 11139 5 53 0.037 340.142 11139 5 54 0.031 365.730 11139 5 55 0.028 386.326 11139 5 56 0.026 404.426 11139 5 57 ENDDATA 35 0 11139 5 58 ENDSUBENT 57 0 11139 599999 SUBENT 11139006 20210317 148311139 6 1 BIB 3 5 11139 6 2 REACTION 1(47-AG-0(N,0),,EN) 11139 6 3 2(47-AG-0(N,TOT),,WID,,SQ/S0) 11139 6 4 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. 11139 6 5 STATUS (DEP,11139004) 11139 6 6 (TABLE) page 166. 11139 6 7 ENDBIB 5 0 11139 6 8 NOCOMMON 0 0 11139 6 9 DATA 3 3 11139 6 10 DATA 1DATA-ERR 1DATA 2 11139 6 11 EV EV B*EV-SQ 11139 6 12 5.1 0.2 300. 11139 6 13 13.7 1. 14. 11139 6 14 43. 5. 380. 11139 6 15 ENDDATA 5 0 11139 6 16 ENDSUBENT 15 0 11139 699999 SUBENT 11139007 20210317 148311139 7 1 BIB 3 7 11139 7 2 REACTION 1(49-IN-0(N,0),,EN) 11139 7 3 2(49-IN-0(N,TOT),,WID,,SQ/S0) 11139 7 4 3(49-IN-0(N,TOT),,WID) 11139 7 5 4(49-IN-0(N,TOT),,SIG,,RES) 11139 7 6 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. 11139 7 7 STATUS (DEP,11139027) 11139 7 8 (TABLE) page 162. 11139 7 9 ENDBIB 7 0 11139 7 10 NOCOMMON 0 0 11139 7 11 DATA 6 1 11139 7 12 DATA 1DATA-ERR 1DATA 2DATA-ERR 2DATA-MAX 3DATA-MIN 411139 7 13 EV EV B*EV-SQ B*EV-SQ EV B 11139 7 14 1.44 0.04 210. 60. 0.2 5200.11139 7 15 ENDDATA 3 0 11139 7 16 ENDSUBENT 15 0 11139 799999 SUBENT 11139008 20210317 148311139 8 1 BIB 3 5 11139 8 2 REACTION 1(51-SB-0(N,0),,EN) 11139 8 3 2(51-SB-0(N,TOT),,WID,,SQ/S0) 11139 8 4 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. 11139 8 5 STATUS (DEP,11139031) 11139 8 6 (TABLE) pages 168-169. 11139 8 7 ENDBIB 5 0 11139 8 8 NOCOMMON 0 0 11139 8 9 DATA 3 2 11139 8 10 DATA 1DATA-ERR 1DATA 2 11139 8 11 EV EV B*EV-SQ 11139 8 12 6.3 0.5 20. 11139 8 13 19.2 1.0 210. 11139 8 14 ENDDATA 4 0 11139 8 15 ENDSUBENT 14 0 11139 899999 SUBENT 11139009 20210317 148311139 9 1 BIB 3 8 11139 9 2 REACTION 1(79-AU-197(N,0),,EN) 11139 9 3 2(79-AU-197(N,TOT),,WID,,SQ/S0) 11139 9 4 3(79-AU-197(N,TOT),,WID) 11139 9 5 4(79-AU-197(N,TOT),,SIG,,RES) 11139 9 6 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. 11139 9 7 STATUS (DEP,11139029) 11139 9 8 (DEP,11139030) 11139 9 9 (TABLE) page 163. 11139 9 10 ENDBIB 8 0 11139 9 11 NOCOMMON 0 0 11139 9 12 DATA 6 1 11139 9 13 DATA 1DATA-ERR 1DATA 2DATA-ERR 2DATA-MAX 3DATA-MIN 411139 9 14 EV EV B*EV-SQ B*EV-SQ EV B 11139 9 15 4.8 0.2 600. 80. 0.5 2400.11139 9 16 ENDDATA 3 0 11139 9 17 ENDSUBENT 16 0 11139 999999 SUBENT 11139010 20210410 148311139 10 1 BIB 6 13 11139 10 2 REACTION (47-AG-0(N,ABS),,SIG) 11139 10 3 SAMPLE A 19.8 g/cm2 disk of metallic silver was used. 11139 10 4 Transmission measurements were made using a thin 11139 10 5 sample containing 1.043 g/cm2, in the vicinity of 32 11139 10 6 microseconds/meter. 11139 10 7 ANALYSIS In the thermal region, the Ag 11139 10 8 cross-section curves can be resolved into the sum of 11139 10 9 a constant term and a 1/v term: sigma = [(9.05+- 11139 10 10 0.10)*E**-1/2 + (6.6+-0.5)]*10**-24 cm2/atom. 11139 10 11 E is the neutron energy in eV. 11139 10 12 ERR-ANALYS (DATA-ERR) Cross section curve calculations. 11139 10 13 STATUS (TABLE) page 165. 11139 10 14 HISTORY (20210317C) BP 11139 10 15 ENDBIB 13 0 11139 10 16 NOCOMMON 0 0 11139 10 17 DATA 3 1 11139 10 18 EN DATA DATA-ERR 11139 10 19 EV B B 11139 10 20 2.53E-02 63.5E+01 0.62 11139 10 21 ENDDATA 3 0 11139 10 22 ENDSUBENT 21 0 11139 1099999 SUBENT 11139011 20210410 148311139 11 1 BIB 6 11 11139 11 2 REACTION (51-SB-0(N,ABS),,SIG) 11139 11 3 SAMPLE The sample used contained 22.41 g/cm2 of metallic 11139 11 4 antimony. 11139 11 5 ANALYSIS In the thermal region, the Sb 11139 11 6 cross-section curves can be resolved into the sum of 11139 11 7 a constant term and a 1/v term: sigma = [(0.64+- 11139 11 8 0.02)*E**-1/2 + (4.2+-0.3)]*10**-24 cm2/atom. 11139 11 9 E is the neutron energy in eV. 11139 11 10 ERR-ANALYS (DATA-ERR) Cross section curve calculations. 11139 11 11 STATUS (TABLE) page 167. 11139 11 12 HISTORY (20210317C) BP 11139 11 13 ENDBIB 11 0 11139 11 14 NOCOMMON 0 0 11139 11 15 DATA 3 1 11139 11 16 EN DATA DATA-ERR 11139 11 17 EV B B 11139 11 18 2.53E-02 8.22E+00 0.43 11139 11 19 ENDDATA 3 0 11139 11 20 ENDSUBENT 19 0 11139 1199999 SUBENT 11139012 20210410 148311139 12 1 BIB 6 13 11139 12 2 REACTION (80-HG-0(N,ABS),,SIG) 11139 12 3 SAMPLE The mercury was U.S.P. XII redistilled - purchased 11139 12 4 from the Mallinkrodt Chemical Works. For the 11139 12 5 preliminary investigation of the entire transmission 11139 12 6 curve of mercury, a sample containing 3.25 g/cm2 of 11139 12 7 the liquid was used. 11139 12 8 ANALYSIS The Hg cross section below 5 eV was well matched 11139 12 9 by the relation sigma = [((64+-3)*E**-1/2)*((1+E)/ 11139 12 10 2.0)**-2]*10**-24 cm2/atom. 11139 12 11 E is the neutron energy in eV. 11139 12 12 ERR-ANALYS (DATA-ERR) Cross section curve calculations. 11139 12 13 STATUS (TABLE) page 171. 11139 12 14 HISTORY (20210317C) BP 11139 12 15 ENDBIB 13 0 11139 12 16 NOCOMMON 0 0 11139 12 17 DATA 3 1 11139 12 18 EN DATA DATA-ERR 11139 12 19 EV B B 11139 12 20 2.53E-02 3.81E-01 0.017 11139 12 21 ENDDATA 3 0 11139 12 22 ENDSUBENT 21 0 11139 1299999 SUBENT 11139013 20210417 148311139 13 1 BIB 5 12 11139 13 2 REACTION (3-LI-0(N,TOT),,TRN) 11139 13 3 SAMPLE This salt was tightly packed in an aluminum container 11139 13 4 such that there were 4.85 g/cm2 of LiF and 0.418 11139 13 5 g/cm2 of aluminum. The lithium fluoride was obtained 11139 13 6 from the City Chemical Corporation and was of 11139 13 7 analytical reagent grade. The salt was dried at 120 11139 13 8 degrees C for 48 hours before being packed in the 11139 13 9 container. 11139 13 10 METHOD Resolution width was approximately 20 microsec/meter. 11139 13 11 STATUS (CURVE) Fig. 14, page 168; values converted by 11139 13 12 compiler as described under the compiler's comment. 11139 13 13 HISTORY (20210317C) BP. 11139 13 14 ENDBIB 12 0 11139 13 15 COMMON 1 3 11139 13 16 THICKNESS 11139 13 17 G/CM-SQ 11139 13 18 4.85 11139 13 19 ENDCOMMON 3 0 11139 13 20 DATA 2 11 11139 13 21 EN DATA 11139 13 22 EV NO-DIM 11139 13 23 31.696 6.214E-01 11139 13 24 12.474 5.656E-01 11139 13 25 6.767 4.600E-01 11139 13 26 3.420 3.948E-01 11139 13 27 2.715 3.417E-01 11139 13 28 1.950 2.844E-01 11139 13 29 1.525 2.442E-01 11139 13 30 1.145 2.049E-01 11139 13 31 0.784 1.505E-01 11139 13 32 0.647 1.267E-01 11139 13 33 0.553 1.092E-01 11139 13 34 ENDDATA 13 0 11139 13 35 ENDSUBENT 34 0 11139 1399999 SUBENT 11139014 20210417 148311139 14 1 BIB 6 17 11139 14 2 REACTION (3-LI-0(N,TOT),,SIG) 11139 14 3 SAMPLE This salt was tightly packed in an aluminum container 11139 14 4 such that there were 0.862 g/cm2 of LiF and 0.418 11139 14 5 g/cm2 of aluminum. The lithium fluoride was obtained 11139 14 6 from the City Chemical Corporation and was of 11139 14 7 analytical reagent grade. The salt was dried at 120 11139 14 8 degrees C for 48 hours before being packed in the 11139 14 9 container. 11139 14 10 METHOD Resolution width was approximately 50 microsec/meter. 11139 14 11 ANALYSIS Outside resonances, the cross section from the 11139 14 12 experimental transmission T by using the formula 11139 14 13 T=exp(-n sigma), where n is the number of atoms per 11139 14 14 cm2 in the sample. 11139 14 15 STATUS (DEP,11139015) 11139 14 16 (CURVE) Fig. 15, page 168; values converted by 11139 14 17 compiler as described under the compiler's comment. 11139 14 18 HISTORY (20210317C) BP 11139 14 19 ENDBIB 17 0 11139 14 20 NOCOMMON 0 0 11139 14 21 DATA 2 29 11139 14 22 EN DATA 11139 14 23 EV B 11139 14 24 985.573 1.175 11139 14 25 41.709 4.448 11139 14 26 6.648 7.336 11139 14 27 2.245 10.611 11139 14 28 0.718 16.581 11139 14 29 0.485 17.547 11139 14 30 0.340 19.667 11139 14 31 0.264 22.556 11139 14 32 0.210 27.368 11139 14 33 0.168 29.872 11139 14 34 0.133 33.339 11139 14 35 0.117 36.612 11139 14 36 0.100 38.731 11139 14 37 0.088 41.620 11139 14 38 0.076 44.893 11139 14 39 0.068 47.782 11139 14 40 0.058 50.095 11139 14 41 0.052 51.830 11139 14 42 0.047 56.834 11139 14 43 0.042 61.261 11139 14 44 0.038 63.382 11139 14 45 0.035 63.963 11139 14 46 0.032 66.852 11139 14 47 0.029 70.318 11139 14 48 0.027 73.015 11139 14 49 0.023 78.600 11139 14 50 0.021 79.952 11139 14 51 0.019 85.918 11139 14 52 0.018 86.307 11139 14 53 ENDDATA 31 0 11139 14 54 ENDSUBENT 53 0 11139 1499999 SUBENT 11139015 20210417 148311139 15 1 BIB 5 13 11139 15 2 REACTION (3-LI-0(N,TOT),,TRN) 11139 15 3 SAMPLE This salt was tightly packed in an aluminum container 11139 15 4 such that there were 0.862 g/cm2 of LiF and 0.418 11139 15 5 g/cm2 of aluminum. The lithium fluoride was obtained 11139 15 6 from the City Chemical Corporation and was of 11139 15 7 analytical reagent grade. The salt was dried at 120 11139 15 8 degrees C for 48 hours before being packed in the 11139 15 9 container. 11139 15 10 METHOD Resolution width was approximately 50 microsec/meter. 11139 15 11 STATUS (DEP,11139015) 11139 15 12 (CURVE) Fig. 15, page 168; values converted by 11139 15 13 compiler as described under the compiler's comment. 11139 15 14 HISTORY (20210317C) BP 11139 15 15 ENDBIB 13 0 11139 15 16 COMMON 1 3 11139 15 17 THICKNESS 11139 15 18 G/CM-SQ 11139 15 19 0.862 11139 15 20 ENDCOMMON 3 0 11139 15 21 DATA 2 29 11139 15 22 EN DATA 11139 15 23 EV NO-DIM 11139 15 24 985.573 9.079E-01 11139 15 25 41.709 8.502E-01 11139 15 26 6.648 8.023E-01 11139 15 27 2.245 7.513E-01 11139 15 28 0.718 6.665E-01 11139 15 29 0.485 6.538E-01 11139 15 30 0.340 6.266E-01 11139 15 31 0.264 5.913E-01 11139 15 32 0.210 5.369E-01 11139 15 33 0.168 5.106E-01 11139 15 34 0.133 4.763E-01 11139 15 35 0.117 4.460E-01 11139 15 36 0.100 4.274E-01 11139 15 37 0.088 4.034E-01 11139 15 38 0.076 3.777E-01 11139 15 39 0.068 3.565E-01 11139 15 40 0.058 3.403E-01 11139 15 41 0.052 3.287E-01 11139 15 42 0.047 2.973E-01 11139 15 43 0.042 2.720E-01 11139 15 44 0.038 2.607E-01 11139 15 45 0.035 2.577E-01 11139 15 46 0.032 2.432E-01 11139 15 47 0.029 2.268E-01 11139 15 48 0.027 2.149E-01 11139 15 49 0.023 1.921E-01 11139 15 50 0.021 1.870E-01 11139 15 51 0.019 1.659E-01 11139 15 52 0.018 1.646E-01 11139 15 53 ENDDATA 31 0 11139 15 54 ENDSUBENT 53 0 11139 1599999 SUBENT 11139016 20210417 148311139 16 1 BIB 5 13 11139 16 2 REACTION (47-AG-0(N,TOT),,TRN) 11139 16 3 SAMPLE A 19.8 g/cm2 disk of metallic silver was used. A 11139 16 4 preliminary run on the thin sample in the thermal 11139 16 5 region gave sufficient data to indicate the thickness 11139 16 6 of the sample which would give best results in this 11139 16 7 region. Therefore, the thick sample was cut 11139 16 8 approximately in half and a sample containing 7.84 11139 16 9 g/cm2 was used for the rest of the measurements an 11139 16 10 silver. 11139 16 11 METHOD Resolution width was approximately 50 microsec/meter. 11139 16 12 STATUS (CURVE) Fig. 10, page 164; values converted by 11139 16 13 compiler as described under the compiler's comment. 11139 16 14 HISTORY (20210317C) BP 11139 16 15 ENDBIB 13 0 11139 16 16 COMMON 1 3 11139 16 17 THICKNESS 11139 16 18 G/CM-SQ 11139 16 19 7.84 11139 16 20 ENDCOMMON 3 0 11139 16 21 DATA 2 49 11139 16 22 EN DATA 11139 16 23 EV NO-DIM 11139 16 24 432.879 7.302E-01 11139 16 25 93.878 6.681E-01 11139 16 26 88.902 5.863E-01 11139 16 27 48.581 5.365E-01 11139 16 28 11.067 6.007E-01 11139 16 29 10.907 5.431E-01 11139 16 30 8.703 2.338E-01 11139 16 31 8.084 6.607E-01 11139 16 32 6.838 7.222E-02 11139 16 33 5.235 1.339E-02 11139 16 34 4.342 4.825E-02 11139 16 35 2.766 2.763E-01 11139 16 36 2.670 3.807E-01 11139 16 37 2.284 4.469E-01 11139 16 38 2.064 4.715E-01 11139 16 39 1.705 4.945E-01 11139 16 40 1.367 4.773E-01 11139 16 41 1.005 4.746E-01 11139 16 42 0.771 4.862E-01 11139 16 43 0.723 4.370E-01 11139 16 44 0.531 4.244E-01 11139 16 45 0.457 4.001E-01 11139 16 46 0.436 4.221E-01 11139 16 47 0.334 3.493E-01 11139 16 48 0.246 3.393E-01 11139 16 49 0.204 3.143E-01 11139 16 50 0.165 2.776E-01 11139 16 51 0.136 2.587E-01 11139 16 52 0.119 2.285E-01 11139 16 53 0.098 2.194E-01 11139 16 54 0.084 2.069E-01 11139 16 55 0.074 1.743E-01 11139 16 56 0.065 1.614E-01 11139 16 57 0.057 1.385E-01 11139 16 58 0.051 1.283E-01 11139 16 59 0.045 1.133E-01 11139 16 60 0.037 9.957E-02 11139 16 61 0.033 8.848E-02 11139 16 62 0.032 7.723E-02 11139 16 63 0.028 6.987E-02 11139 16 64 0.026 6.136E-02 11139 16 65 0.024 6.177E-02 11139 16 66 0.022 4.992E-02 11139 16 67 0.020 4.708E-02 11139 16 68 0.019 4.655E-02 11139 16 69 0.018 3.740E-02 11139 16 70 0.017 4.042E-02 11139 16 71 0.016 3.881E-02 11139 16 72 0.015 2.886E-02 11139 16 73 ENDDATA 51 0 11139 16 74 ENDSUBENT 73 0 11139 1699999 SUBENT 11139017 20210417 148311139 17 1 BIB 5 8 11139 17 2 REACTION (47-AG-0(N,TOT),,TRN) 11139 17 3 SAMPLE Transmission measurements were made using a thin 11139 17 4 sample containing 1.043 g/cm2, in the vicinity of 32 11139 17 5 microseconds/meter. 11139 17 6 METHOD Resolution width was approximately 15 microsec/meter. 11139 17 7 STATUS (CURVE) Fig. 9, page 164; values converted by compiler 11139 17 8 as described under the compiler's comment. 11139 17 9 HISTORY (20210317C) BP 11139 17 10 ENDBIB 8 0 11139 17 11 COMMON 1 3 11139 17 12 THICKNESS 11139 17 13 G/CM-SQ 11139 17 14 1.043 11139 17 15 ENDCOMMON 3 0 11139 17 16 DATA 2 8 11139 17 17 EN DATA 11139 17 18 EV NO-DIM 11139 17 19 7.701 0.899 11139 17 20 6.778 0.633 11139 17 21 5.965 0.566 11139 17 22 5.300 0.097 11139 17 23 4.736 0.204 11139 17 24 4.183 0.462 11139 17 25 3.838 0.625 11139 17 26 3.453 0.839 11139 17 27 ENDDATA 10 0 11139 17 28 ENDSUBENT 27 0 11139 1799999 SUBENT 11139018 20210417 148311139 18 1 BIB 5 13 11139 18 2 REACTION (47-AG-0(N,TOT),,TRN) 11139 18 3 SAMPLE A 19.8 g/cm2 disk of metallic silver was used. A 11139 18 4 preliminary run on the thin sample in the thermal 11139 18 5 region gave sufficient data to indicate the thickness 11139 18 6 of the sample which would give best results in this 11139 18 7 region. Therefore, the thick sample was cut 11139 18 8 approximately in half and a sample containing 7.84 11139 18 9 g/cm2 was used for the rest of the measurements an 11139 18 10 silver. 11139 18 11 METHOD Resolution width was approximately 5 microsec/meter. 11139 18 12 STATUS (CURVE) Fig. 11, page 165; values converted by 11139 18 13 compiler as described under the compiler's comment. 11139 18 14 HISTORY (20210317C) BP 11139 18 15 ENDBIB 13 0 11139 18 16 COMMON 1 3 11139 18 17 THICKNESS 11139 18 18 G/CM-SQ 11139 18 19 7.84 11139 18 20 ENDCOMMON 3 0 11139 18 21 DATA 2 26 11139 18 22 EN DATA 11139 18 23 EV NO-DIM 11139 18 24 1836.735 0.794 11139 18 25 459.184 0.747 11139 18 26 188.716 0.730 11139 18 27 100.277 0.730 11139 18 28 62.069 0.671 11139 18 29 43.748 0.540 11139 18 30 31.146 0.651 11139 18 31 24.607 0.648 11139 18 32 19.766 0.680 11139 18 33 15.633 0.535 11139 18 34 12.672 0.599 11139 18 35 10.803 0.707 11139 18 36 9.266 0.660 11139 18 37 7.868 0.440 11139 18 38 6.931 0.229 11139 18 39 6.039 0.065 11139 18 40 5.355 0.021 11139 18 41 4.724 0.011 11139 18 42 4.246 0.040 11139 18 43 3.823 0.078 11139 18 44 3.472 0.193 11139 18 45 3.147 0.260 11139 18 46 2.911 0.307 11139 18 47 2.644 0.358 11139 18 48 2.336 0.389 11139 18 49 2.097 0.428 11139 18 50 ENDDATA 28 0 11139 18 51 ENDSUBENT 50 0 11139 1899999 SUBENT 11139019 20210417 148311139 19 1 BIB 5 10 11139 19 2 REACTION (80-HG-0(N,TOT),,TRN) 11139 19 3 SAMPLE The mercury was U.S.P. XII redistilled - purchased 11139 19 4 from the Mallinkrodt Chemical Works. For the 11139 19 5 preliminary investigation of the entire transmission 11139 19 6 curve of mercury, a sample containing 3.25 g/cm2 of 11139 19 7 the liquid was used. 11139 19 8 METHOD Resolution width was approximately 100 microsec/meter. 11139 19 9 STATUS (CURVE) Fig. 16, page 169; values converted by 11139 19 10 compiler as described under the compiler's comment. 11139 19 11 HISTORY (20210317C) BP 11139 19 12 ENDBIB 10 0 11139 19 13 COMMON 1 3 11139 19 14 THICKNESS 11139 19 15 G/CM-SQ 11139 19 16 3.25 11139 19 17 ENDCOMMON 3 0 11139 19 18 DATA 2 33 11139 19 19 EN DATA 11139 19 20 EV NO-DIM 11139 19 21 7661.548 0.884 11139 19 22 72.078 0.831 11139 19 23 67.563 0.863 11139 19 24 16.428 0.816 11139 19 25 7.841 0.816 11139 19 26 3.194 0.816 11139 19 27 2.106 0.726 11139 19 28 1.256 0.646 11139 19 29 0.958 0.586 11139 19 30 0.755 0.547 11139 19 31 0.592 0.450 11139 19 32 0.478 0.469 11139 19 33 0.412 0.410 11139 19 34 0.351 0.381 11139 19 35 0.316 0.317 11139 19 36 0.254 0.287 11139 19 37 0.241 0.267 11139 19 38 0.206 0.256 11139 19 39 0.181 0.240 11139 19 40 0.170 0.219 11139 19 41 0.151 0.192 11139 19 42 0.118 0.151 11139 19 43 0.097 0.127 11139 19 44 0.086 0.109 11139 19 45 0.077 0.088 11139 19 46 0.065 0.080 11139 19 47 0.051 0.059 11139 19 48 0.046 0.049 11139 19 49 0.040 0.040 11139 19 50 0.037 0.035 11139 19 51 0.031 0.028 11139 19 52 0.028 0.022 11139 19 53 0.026 0.019 11139 19 54 ENDDATA 35 0 11139 19 55 ENDSUBENT 54 0 11139 1999999 SUBENT 11139020 20210417 148311139 20 1 BIB 6 15 11139 20 2 REACTION (80-HG-0(N,TOT),,SIG) 11139 20 3 SAMPLE The mercury was U.S.P. XII redistilled - purchased 11139 20 4 from the Mallinkrodt Chemical Works. A sample 11139 20 5 containing 12.9 g/cm2 of the liquid was used. 11139 20 6 METHOD Resolution width was approximately 10 microsec/meter. 11139 20 7 ANALYSIS Outside resonances, the cross section from the 11139 20 8 experimental transmission T by using the formula 11139 20 9 T=exp(-n sigma), where n is the number of atoms per 11139 20 10 cm2 in the sample. Silver cross section can be 11139 20 11 expressed as sigma = [15 + 64*E**(-1/2)]x10**(-24) 11139 20 12 cm2/atom. E is the neutron energy in eV. 11139 20 13 STATUS (DEP,11139021) 11139 20 14 (CURVE) Fig. 17, page 170; values converted by 11139 20 15 compiler as described under the compiler's comment. 11139 20 16 HISTORY (20210317C) BP 11139 20 17 ENDBIB 15 0 11139 20 18 NOCOMMON 0 0 11139 20 19 DATA 2 32 11139 20 20 EN DATA 11139 20 21 EV B 11139 20 22 3455.146 8.131 11139 20 23 795.755 8.126 11139 20 24 183.933 9.945 11139 20 25 53.954 16.012 11139 20 26 29.591 15.806 11139 20 27 17.914 15.396 11139 20 28 12.411 13.975 11139 20 29 8.358 14.375 11139 20 30 6.950 14.979 11139 20 31 6.008 15.584 11139 20 32 5.361 16.594 11139 20 33 4.814 17.199 11139 20 34 4.261 18.007 11139 20 35 3.798 19.016 11139 20 36 3.290 20.025 11139 20 37 2.877 21.236 11139 20 38 2.353 25.077 11139 20 39 2.043 26.085 11139 20 40 1.745 28.509 11139 20 41 1.525 32.756 11139 20 42 1.406 36.599 11139 20 43 1.207 37.201 11139 20 44 1.089 41.245 11139 20 45 0.960 45.289 11139 20 46 0.884 51.763 11139 20 47 0.810 48.520 11139 20 48 0.738 54.183 11139 20 49 0.680 60.454 11139 20 50 0.616 62.271 11139 20 51 0.559 70.565 11139 20 52 0.522 70.561 11139 20 53 0.494 70.760 11139 20 54 ENDDATA 34 0 11139 20 55 ENDSUBENT 54 0 11139 2099999 SUBENT 11139021 20210417 148311139 21 1 BIB 5 8 11139 21 2 REACTION (80-HG-0(N,TOT),,TRN) 11139 21 3 SAMPLE The mercury was U.S.P. XII redistilled - purchased 11139 21 4 from the Mallinkrodt Chemical Works. A sample 11139 21 5 containing 12.9 g/cm2 of the liquid was used. 11139 21 6 METHOD Resolution width was approximately 10 microsec/meter. 11139 21 7 STATUS (CURVE) Fig. 17, page 170; values converted by 11139 21 8 compiler as described under the compiler's comment. 11139 21 9 HISTORY (20210317C) BP 11139 21 10 ENDBIB 8 0 11139 21 11 COMMON 1 3 11139 21 12 THICKNESS 11139 21 13 G/CM-SQ 11139 21 14 12.9 11139 21 15 ENDCOMMON 3 0 11139 21 16 DATA 2 32 11139 21 17 EN DATA 11139 21 18 EV NO-DIM 11139 21 19 3455.146 7.351E-01 11139 21 20 795.755 7.352E-01 11139 21 21 183.933 6.848E-01 11139 21 22 53.954 5.404E-01 11139 21 23 29.591 5.448E-01 11139 21 24 17.914 5.536E-01 11139 21 25 12.411 5.851E-01 11139 21 26 8.358 5.760E-01 11139 21 27 6.950 5.626E-01 11139 21 28 6.008 5.495E-01 11139 21 29 5.361 5.282E-01 11139 21 30 4.814 5.159E-01 11139 21 31 4.261 4.999E-01 11139 21 32 3.798 4.806E-01 11139 21 33 3.290 4.620E-01 11139 21 34 2.877 4.407E-01 11139 21 35 2.353 3.793E-01 11139 21 36 2.043 3.647E-01 11139 21 37 1.745 3.318E-01 11139 21 38 1.525 2.811E-01 11139 21 39 1.406 2.419E-01 11139 21 40 1.207 2.363E-01 11139 21 41 1.089 2.018E-01 11139 21 42 0.960 1.724E-01 11139 21 43 0.884 1.339E-01 11139 21 44 0.810 1.519E-01 11139 21 45 0.738 1.218E-01 11139 21 46 0.680 9.536E-02 11139 21 47 0.616 8.883E-02 11139 21 48 0.559 6.427E-02 11139 21 49 0.522 6.428E-02 11139 21 50 0.494 6.378E-02 11139 21 51 ENDDATA 34 0 11139 21 52 ENDSUBENT 51 0 11139 2199999 SUBENT 11139022 20210417 148311139 22 1 BIB 6 13 11139 22 2 REACTION (80-HG-0(N,TOT),,SIG) 11139 22 3 SAMPLE The mercury was U.S.P. XII redistilled - purchased 11139 22 4 from the Mallinkrodt Chemical Works. A sample 11139 22 5 containing 34.4 g/cm2 of the liquid was used. 11139 22 6 METHOD Resolution width was approximately 10 microsec/meter. 11139 22 7 ANALYSIS Outside resonances, the cross section from the 11139 22 8 experimental transmission T by using the formula 11139 22 9 T=exp(-n sigma), where n is the number of atoms per 11139 22 10 cm2 in the sample. 11139 22 11 STATUS (DEP,11139023) 11139 22 12 (CURVE) Fig. 18, page 170; values converted by 11139 22 13 compiler as described under the compiler's comment. 11139 22 14 HISTORY (20210317C) BP 11139 22 15 ENDBIB 13 0 11139 22 16 NOCOMMON 0 0 11139 22 17 DATA 2 17 11139 22 18 EN DATA 11139 22 19 EV B 11139 22 20 5431.735 6.014 11139 22 21 781.059 7.630 11139 22 22 131.203 11.614 11139 22 23 51.816 14.300 11139 22 24 26.834 15.228 11139 22 25 16.995 14.475 11139 22 26 11.728 14.791 11139 22 27 8.346 15.414 11139 22 28 6.316 16.189 11139 22 29 3.978 18.580 11139 22 30 2.734 21.582 11139 22 31 2.354 23.732 11139 22 32 2.035 26.035 11139 22 33 1.765 29.026 11139 22 34 1.555 31.023 11139 22 35 1.427 34.240 11139 22 36 1.214 37.159 11139 22 37 ENDDATA 19 0 11139 22 38 ENDSUBENT 37 0 11139 2299999 SUBENT 11139023 20210417 148311139 23 1 BIB 5 8 11139 23 2 REACTION (80-HG-0(N,TOT),,TRN) 11139 23 3 SAMPLE The mercury was U.S.P. XII redistilled - purchased 11139 23 4 from the Mallinkrodt Chemical Works. A sample 11139 23 5 containing 34.4 g/cm2 of the liquid was used. 11139 23 6 METHOD Resolution width was approximately 10 microsec/meter. 11139 23 7 STATUS (CURVE) Fig. 18, page 170; values converted by 11139 23 8 compiler as described under the compiler's comment. 11139 23 9 HISTORY (20210317C) BP 11139 23 10 ENDBIB 8 0 11139 23 11 COMMON 1 3 11139 23 12 THICKNESS 11139 23 13 G/CM-SQ 11139 23 14 34.4 11139 23 15 ENDCOMMON 3 0 11139 23 16 DATA 2 17 11139 23 17 EN DATA 11139 23 18 EV NO-DIM 11139 23 19 5431.735 5.279E-01 11139 23 20 781.059 4.480E-01 11139 23 21 131.203 2.986E-01 11139 23 22 51.816 2.272E-01 11139 23 23 26.834 2.068E-01 11139 23 24 16.995 2.234E-01 11139 23 25 11.728 2.164E-01 11139 23 26 8.346 2.032E-01 11139 23 27 6.316 1.879E-01 11139 23 28 3.978 1.474E-01 11139 23 29 2.734 1.086E-01 11139 23 30 2.354 8.730E-02 11139 23 31 2.035 6.906E-02 11139 23 32 1.765 5.093E-02 11139 23 33 1.555 4.157E-02 11139 23 34 1.427 2.996E-02 11139 23 35 1.214 2.226E-02 11139 23 36 ENDDATA 19 0 11139 23 37 ENDSUBENT 36 0 11139 2399999 SUBENT 11139024 20210417 148311139 24 1 BIB 6 13 11139 24 2 REACTION (80-HG-0(N,TOT),,SIG) 11139 24 3 SAMPLE The mercury was U.S.P. XII redistilled - purchased 11139 24 4 from the Mallinkrodt Chemical Works. A sample 11139 24 5 containing 34.4 g/cm2 of the liquid was used. 11139 24 6 METHOD Resolution width was approximately 7.5 microsec/meter. 11139 24 7 ANALYSIS Outside resonances, the cross section from the 11139 24 8 experimental transmission T by using the formula 11139 24 9 T=exp(-n sigma), where n is the number of atoms per 11139 24 10 cm2 in the sample. 11139 24 11 STATUS (DEP,11139025) 11139 24 12 (CURVE) Fig. 19, page 171; values converted by 11139 24 13 compiler as described under the compiler's comment. 11139 24 14 HISTORY (20210317C) BP 11139 24 15 ENDBIB 13 0 11139 24 16 NOCOMMON 0 0 11139 24 17 DATA 2 9 11139 24 18 EN DATA 11139 24 19 EV B 11139 24 20 4001.144 6.070E+00 11139 24 21 765.593 7.844E+00 11139 24 22 133.349 1.183E+01 11139 24 23 49.890 1.452E+01 11139 24 24 27.333 1.555E+01 11139 24 25 17.114 1.468E+01 11139 24 26 11.475 1.485E+01 11139 24 27 8.480 1.555E+01 11139 24 28 6.325 1.633E+01 11139 24 29 ENDDATA 11 0 11139 24 30 ENDSUBENT 29 0 11139 2499999 SUBENT 11139025 20210417 148311139 25 1 BIB 5 8 11139 25 2 REACTION (80-HG-0(N,TOT),,TRN) 11139 25 3 SAMPLE The mercury was U.S.P. XII redistilled - purchased 11139 25 4 from the Mallinkrodt Chemical Works. A sample 11139 25 5 containing 34.4 g/cm2 of the liquid was used. 11139 25 6 METHOD Resolution width was approximately 7.5 microsec/meter. 11139 25 7 STATUS (CURVE) Fig. 19, page 171; values converted by 11139 25 8 compiler as described under the compiler's comment. 11139 25 9 HISTORY (20210317C) BP 11139 25 10 ENDBIB 8 0 11139 25 11 COMMON 1 3 11139 25 12 THICKNESS 11139 25 13 G/CM-SQ 11139 25 14 34.4 11139 25 15 ENDCOMMON 3 0 11139 25 16 DATA 2 9 11139 25 17 EN DATA 11139 25 18 EV NO-DIM 11139 25 19 4001.144 5.282E-01 11139 25 20 765.593 4.401E-01 11139 25 21 133.349 2.922E-01 11139 25 22 49.890 2.215E-01 11139 25 23 27.333 1.994E-01 11139 25 24 17.114 2.181E-01 11139 25 25 11.475 2.142E-01 11139 25 26 8.480 1.992E-01 11139 25 27 6.325 1.839E-01 11139 25 28 ENDDATA 11 0 11139 25 29 ENDSUBENT 28 0 11139 2599999 SUBENT 11139026 20210417 148311139 26 1 BIB 5 9 11139 26 2 REACTION (49-IN-0(N,TOT),,TRN) 11139 26 3 SAMPLE The thin sample contained 0.193 g/cm2 of metallic 11139 26 4 indium of the metal. These samples were obtained from 11139 26 5 the Indium Company of America and were the purest 11139 26 6 indium that could be furnished by this company. 11139 26 7 METHOD Resolution width was approximately 52 microsec/meter. 11139 26 8 STATUS (CURVE) Fig. 4, page 160; values converted by compiler 11139 26 9 as described under the compiler's comment. 11139 26 10 HISTORY (20210317C) BP 11139 26 11 ENDBIB 9 0 11139 26 12 COMMON 1 3 11139 26 13 THICKNESS 11139 26 14 G/CM-SQ 11139 26 15 0.193 11139 26 16 ENDCOMMON 3 0 11139 26 17 DATA 2 15 11139 26 18 EN DATA 11139 26 19 EV NO-DIM 11139 26 20 2.084 0.845 11139 26 21 1.930 0.764 11139 26 22 1.807 0.621 11139 26 23 1.695 0.456 11139 26 24 1.574 0.194 11139 26 25 1.490 0.077 11139 26 26 1.408 0.045 11139 26 27 1.318 0.117 11139 26 28 1.236 0.254 11139 26 29 1.179 0.445 11139 26 30 1.112 0.571 11139 26 31 1.046 0.705 11139 26 32 0.998 0.691 11139 26 33 0.926 0.756 11139 26 34 0.866 0.795 11139 26 35 ENDDATA 17 0 11139 26 36 ENDSUBENT 35 0 11139 2699999 SUBENT 11139027 20210417 148311139 27 1 BIB 6 14 11139 27 2 REACTION (49-IN-0(N,TOT),,SIG) 11139 27 3 SAMPLE The thick sample contained 5.02 g/cm2 of the metal. 11139 27 4 These samples were obtained from the Indium Company 11139 27 5 of America and were the purest indium that could be 11139 27 6 furnished by this company. 11139 27 7 METHOD Resolution width was less than 50 microsec/meter. 11139 27 8 ANALYSIS Outside resonances, the cross section from the 11139 27 9 experimental transmission T by using the formula 11139 27 10 T=exp(-n sigma), where n is the number of atoms per 11139 27 11 cm2 in the sample. 11139 27 12 STATUS (DEP,11139028) 11139 27 13 (CURVE) Fig. 6, page 160; values converted by compiler 11139 27 14 as described under the compiler's comment. 11139 27 15 HISTORY (20210317C) BP 11139 27 16 ENDBIB 14 0 11139 27 17 NOCOMMON 0 0 11139 27 18 DATA 2 14 11139 27 19 EN DATA 11139 27 20 EV B 11139 27 21 0.681 117.088 11139 27 22 0.464 93.423 11139 27 23 0.335 91.848 11139 27 24 0.265 87.374 11139 27 25 0.206 92.715 11139 27 26 0.168 90.471 11139 27 27 0.141 95.146 11139 27 28 0.118 107.181 11139 27 29 0.099 108.729 11139 27 30 0.086 117.642 11139 27 31 0.076 120.085 11139 27 32 0.065 128.325 11139 27 33 0.057 136.790 11139 27 34 0.051 136.776 11139 27 35 ENDDATA 16 0 11139 27 36 ENDSUBENT 35 0 11139 2799999 SUBENT 11139028 20210417 148311139 28 1 BIB 5 9 11139 28 2 REACTION (49-IN-0(N,TOT),,TRN) 11139 28 3 SAMPLE The thick sample contained 5.02 g/cm2 of the metal. 11139 28 4 These samples were obtained from the Indium Company 11139 28 5 of America and were the purest indium that could be 11139 28 6 furnished by this company. 11139 28 7 METHOD Resolution width was less than 50 microsec/meter. 11139 28 8 STATUS (CURVE) Fig. 6, page 160; values converted by 11139 28 9 compiler as described under the compiler's comment. 11139 28 10 HISTORY (20210317C) BP 11139 28 11 ENDBIB 9 0 11139 28 12 COMMON 1 3 11139 28 13 THICKNESS 11139 28 14 G/CM-SQ 11139 28 15 5.02 11139 28 16 ENDCOMMON 3 0 11139 28 17 DATA 2 14 11139 28 18 EN DATA 11139 28 19 EV NO-DIM 11139 28 20 0.681 4.616E-02 11139 28 21 0.464 8.543E-02 11139 28 22 0.335 8.905E-02 11139 28 23 0.265 1.001E-01 11139 28 24 0.206 8.715E-02 11139 28 25 0.168 9.243E-02 11139 28 26 0.141 8.189E-02 11139 28 27 0.118 5.992E-02 11139 28 28 0.099 5.759E-02 11139 28 29 0.086 4.570E-02 11139 28 30 0.076 4.291E-02 11139 28 31 0.065 3.465E-02 11139 28 32 0.057 2.782E-02 11139 28 33 0.051 2.785E-02 11139 28 34 ENDDATA 16 0 11139 28 35 ENDSUBENT 34 0 11139 2899999 SUBENT 11139029 20210417 148311139 29 1 BIB 5 9 11139 29 2 REACTION (79-AU-197(N,TOT),,TRN) 11139 29 3 SAMPLE The first sample contained 0.2100 g/cm2. Both of 11139 29 4 these samples were fine gold obtained from Handy and 11139 29 5 Harman of New York City, who state that the purity is 11139 29 6 better than 99.999 percent. 11139 29 7 METHOD Resolution width was approximately 6 microsec/meter. 11139 29 8 STATUS (CURVE) Fig. 7, page 160; values converted by 11139 29 9 compiler as described under the compiler's comment. 11139 29 10 HISTORY (20210317C) BP 11139 29 11 ENDBIB 9 0 11139 29 12 COMMON 1 3 11139 29 13 THICKNESS 11139 29 14 G/CM-SQ 11139 29 15 0.2100 11139 29 16 ENDCOMMON 3 0 11139 29 17 DATA 2 9 11139 29 18 EN DATA 11139 29 19 EV NO-DIM 11139 29 20 7.834 0.969 11139 29 21 6.856 0.972 11139 29 22 6.037 0.755 11139 29 23 5.355 0.526 11139 29 24 4.780 0.270 11139 29 25 4.215 0.650 11139 29 26 3.911 0.884 11139 29 27 3.232 0.935 11139 29 28 2.664 0.947 11139 29 29 ENDDATA 11 0 11139 29 30 ENDSUBENT 29 0 11139 2999999 SUBENT 11139030 20210417 148311139 30 1 BIB 5 9 11139 30 2 REACTION (79-AU-197(N,TOT),,TRN) 11139 30 3 SAMPLE The second sample contained 0.856 g/cm2. Both of 11139 30 4 these samples were fine gold obtained from Handy and 11139 30 5 Harman of New York City, who state that the purity is 11139 30 6 better than 99.999 percent. 11139 30 7 METHOD Resolution width was approximately 6 microsec/meter. 11139 30 8 STATUS (CURVE) Fig. 7, page 160; values converted by 11139 30 9 compiler as described under the compiler's comment. 11139 30 10 HISTORY (20210317C) BP 11139 30 11 ENDBIB 9 0 11139 30 12 COMMON 1 3 11139 30 13 THICKNESS 11139 30 14 G/CM-SQ 11139 30 15 0.856 11139 30 16 ENDCOMMON 3 0 11139 30 17 DATA 2 8 11139 30 18 EN DATA 11139 30 19 EV NO-DIM 11139 30 20 7.915 0.929 11139 30 21 6.127 0.658 11139 30 22 5.344 0.200 11139 30 23 3.847 0.504 11139 30 24 3.510 0.729 11139 30 25 2.922 0.886 11139 30 26 2.476 0.864 11139 30 27 2.197 0.917 11139 30 28 ENDDATA 10 0 11139 30 29 ENDSUBENT 28 0 11139 3099999 SUBENT 11139031 20210417 148311139 31 1 BIB 6 14 11139 31 2 REACTION (51-SB-0(N,TOT),,SIG) 11139 31 3 SAMPLE The sample used contained 22.41 g/cm2 of metallic 11139 31 4 antimony. 11139 31 5 METHOD Resolution width was approximately 50 microsec/meter. 11139 31 6 ANALYSIS Outside resonances, the cross section from the 11139 31 7 experimental transmission T by using the formula 11139 31 8 T=exp(-n sigma), where n is the number of atoms per 11139 31 9 cm2 in the sample. Cross section can be expressed as 11139 31 10 sigma = [(4.2+-0.4) + (0.64+-02)*E**(-1/2)]x10**(-24) 11139 31 11 cm2/atom. E is the neutron energy in eV. 11139 31 12 STATUS (DEP,11139032) 11139 31 13 (CURVE) Fig. 12, page 166; values converted by 11139 31 14 compiler as described under the compiler's comment. 11139 31 15 HISTORY (20210317C) BP 11139 31 16 ENDBIB 14 0 11139 31 17 NOCOMMON 0 0 11139 31 18 DATA 2 40 11139 31 19 EN DATA 11139 31 20 EV B 11139 31 21 56.814 3.991 11139 31 22 31.291 5.219 11139 31 23 18.394 12.349 11139 31 24 8.053 6.210 11139 31 25 6.733 5.265 11139 31 26 6.111 15.087 11139 31 27 2.862 5.973 11139 31 28 2.706 5.264 11139 31 29 2.440 4.933 11139 31 30 1.695 4.390 11139 31 31 0.873 4.436 11139 31 32 0.614 4.577 11139 31 33 0.486 4.930 11139 31 34 0.314 5.165 11139 31 35 0.230 5.305 11139 31 36 0.188 5.824 11139 31 37 0.160 5.610 11139 31 38 0.130 5.657 11139 31 39 0.108 6.104 11139 31 40 0.091 6.292 11139 31 41 0.080 6.433 11139 31 42 0.072 6.621 11139 31 43 0.062 6.596 11139 31 44 0.055 6.760 11139 31 45 0.049 6.853 11139 31 46 0.043 7.206 11139 31 47 0.040 7.135 11139 31 48 0.036 7.417 11139 31 49 0.033 7.251 11139 31 50 0.030 7.911 11139 31 51 0.027 7.886 11139 31 52 0.026 8.334 11139 31 53 0.023 8.380 11139 31 54 0.022 8.497 11139 31 55 0.020 8.685 11139 31 56 0.019 8.991 11139 31 57 0.017 8.635 11139 31 58 0.016 9.272 11139 31 59 0.015 9.271 11139 31 60 0.014 9.600 11139 31 61 ENDDATA 42 0 11139 31 62 ENDSUBENT 61 0 11139 3199999 SUBENT 11139032 20210417 148311139 32 1 BIB 5 7 11139 32 2 REACTION (51-SB-0(N,TOT),,TRN) 11139 32 3 SAMPLE The sample used contained 22.41 g/cm2 of metallic 11139 32 4 antimony. 11139 32 5 METHOD Resolution width was approximately 50 microsec/meter. 11139 32 6 STATUS (CURVE) Fig. 12, page 166; values converted by 11139 32 7 compiler as described under the compiler's comment. 11139 32 8 HISTORY (20210317C) BP 11139 32 9 ENDBIB 7 0 11139 32 10 COMMON 1 3 11139 32 11 THICKNESS 11139 32 12 G/CM-SQ 11139 32 13 22.41 11139 32 14 ENDCOMMON 3 0 11139 32 15 DATA 2 40 11139 32 16 EN DATA 11139 32 17 EV NO-DIM 11139 32 18 56.814 6.343E-01 11139 32 19 31.291 5.532E-01 11139 32 20 18.394 2.499E-01 11139 32 21 8.053 4.954E-01 11139 32 22 6.733 5.504E-01 11139 32 23 6.111 1.842E-01 11139 32 24 2.862 5.087E-01 11139 32 25 2.706 5.505E-01 11139 32 26 2.440 5.712E-01 11139 32 27 1.695 6.069E-01 11139 32 28 0.873 6.038E-01 11139 32 29 0.614 5.944E-01 11139 32 30 0.486 5.715E-01 11139 32 31 0.314 5.568E-01 11139 32 32 0.230 5.482E-01 11139 32 33 0.188 5.175E-01 11139 32 34 0.160 5.299E-01 11139 32 35 0.130 5.273E-01 11139 32 36 0.108 5.017E-01 11139 32 37 0.091 4.913E-01 11139 32 38 0.080 4.837E-01 11139 32 39 0.072 4.737E-01 11139 32 40 0.062 4.750E-01 11139 32 41 0.055 4.664E-01 11139 32 42 0.049 4.617E-01 11139 32 43 0.043 4.439E-01 11139 32 44 0.040 4.475E-01 11139 32 45 0.036 4.337E-01 11139 32 46 0.033 4.418E-01 11139 32 47 0.030 4.105E-01 11139 32 48 0.027 4.117E-01 11139 32 49 0.026 3.916E-01 11139 32 50 0.023 3.897E-01 11139 32 51 0.022 3.846E-01 11139 32 52 0.020 3.767E-01 11139 32 53 0.019 3.641E-01 11139 32 54 0.017 3.789E-01 11139 32 55 0.016 3.529E-01 11139 32 56 0.015 3.530E-01 11139 32 57 0.014 3.403E-01 11139 32 58 ENDDATA 42 0 11139 32 59 ENDSUBENT 58 0 11139 3299999 SUBENT 11139033 20210417 148311139 33 1 BIB 5 7 11139 33 2 REACTION (51-SB-0(N,TOT),,TRN) 11139 33 3 SAMPLE The sample used contained 22.41 g/cm2 of metallic 11139 33 4 antimony. 11139 33 5 METHOD Resolution width was approximately 6 microsec/meter. 11139 33 6 STATUS (CURVE) Fig. 13, page 167; values converted by 11139 33 7 compiler as described under the compiler's comment. 11139 33 8 HISTORY (20210317C) BP 11139 33 9 ENDBIB 7 0 11139 33 10 COMMON 1 3 11139 33 11 THICKNESS 11139 33 12 G/CM-SQ 11139 33 13 22.41 11139 33 14 ENDCOMMON 3 0 11139 33 15 DATA 2 28 11139 33 16 EN DATA 11139 33 17 EV NO-DIM 11139 33 18 7201.076 0.632 11139 33 19 641.305 0.567 11139 33 20 252.496 0.548 11139 33 21 123.799 0.534 11139 33 22 74.348 0.538 11139 33 23 50.135 0.550 11139 33 24 36.138 0.499 11139 33 25 26.815 0.400 11139 33 26 21.030 0.275 11139 33 27 18.732 0.246 11139 33 28 16.759 0.329 11139 33 29 13.923 0.437 11139 33 30 11.547 0.524 11139 33 31 9.742 0.528 11139 33 32 8.293 0.480 11139 33 33 7.227 0.250 11139 33 34 6.261 0.171 11139 33 35 5.555 0.293 11139 33 36 4.983 0.402 11139 33 37 4.396 0.519 11139 33 38 3.979 0.508 11139 33 39 3.678 0.558 11139 33 40 3.315 0.538 11139 33 41 3.003 0.544 11139 33 42 2.757 0.555 11139 33 43 2.525 0.598 11139 33 44 2.340 0.590 11139 33 45 2.170 0.566 11139 33 46 ENDDATA 30 0 11139 33 47 ENDSUBENT 46 0 11139 3399999 ENDENTRY 33 0 1113999999999