/* 2005-02-24 FILE IS GENERATED BY HENDEL */ \\BIB,1[60; D#=D1809; TITLE=/Spectral measurements of neutrons, protons, deuterons and tritons produced by 100 MeV/nucleon He bombardment/; PURPOSE=/To present the angular-energy distributions of neutrons, protons, deuterons and tritons produced from thick carbon, aluminum, copper and lead targets bombarded by 100 MeV/nucleon helium ion. /; ATH=(T.KUROSAWA'1', T.NAKAMURA'1', N.NAKAO'2', T.SHIBATA'3', Y.UWAMINO'4', A.FUKUMURA'5'); INST-ATH=(2JPNTOH'1', 2JPNKEK'2', 2JPNKEK'3', 2JPNIPC'4', 2JPNIRS'5'); /* '1' Cyclotron and Radioisotope Center */ /* '2' Tanashi Branch */ REF=NIM/A; VLP=430(1999)400; RCTS=(12C(ALPHA,P)X, 27AL(ALPHA,P)X, CU(ALPHA,P)X, PB(ALPHA,P)X, 12C(ALPHA,D)X, 27AL(ALPHA,D)X, CU(ALPHA,D)X, PB(ALPHA,D)X, 12C(ALPHA,T)X, 27AL(ALPHA,T)X, CU(ALPHA,T)X, PB(ALPHA,T)X); PHQS=ENGY-SPEC'6'; /* '6' Double differential thick target yield */ \\EXP,1[60; /* 2003-09-13 : Compiled */ PHQ=ENGY-SPEC'7'; /* '7' Double differential thick target yield */ ENR=X%; CHM=ELM; PHYS-FORM=SLD; POL-TGT=0%; ALGN-TGT=0%; ACC=SYN'8'; /* '8' Heavy Ion Medical Accelerator in Chiba (HIMAC) */ INST-ACC=2JPNIRS; INC-ENGY-LAB=100MEV/A; POL-PRJ=0%; COINC=NO; ANT-COINC=NO; DET-SYS=(SCT'9',SCT'10',TOF'11',EDE'12'); /* '9' Plastic scintillator (NE102A) was used as the delta-E counter, ToF start signal detector, and incident projectile counter */ /* '10' Liquid scintillator (NE213) was used as the E counter */ /* '11' To measure the energy of outgoing neutrons, protons, deuterons and tritons */ /* '12' To eliminate charged particles */ ANL=MONTE-MTHD'13'; /* '13' LAHET Monte Carlo Code System, LCS [R.E. Prael, H. Lichtenstein, LA-UR-89-3014, Los Alamos National Laboratory, 1989.] */ /* Experimental Method: - Time-of-flight (To measure the energy of outgoing neutrons, protons, deuterons and tritons) - Particle identification by 'E/Delta E' measurement (To eliminate charged particles) */ \\EXP,1; RCT=12C(ALPHA,P)X; THK-TGT=8850MG/CM**2; DET-PARTCL=P; \\DATA,1; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'14',<1%'15',<1%'16'); /* '14' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '15' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '16' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'17'; /* '17' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'18'; /* '18' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'19' (MEV) (MEV) (1/SR/MEV/PARTCL) 28.636 31.739 0.00098559 31.739 35.386 0.0021321 35.386 39.194 0.0028856 39.194 43.668 0.0031680 43.668 48.975 0.0029538 48.975 54.480 0.0033945 54.480 61.001 0.0030331 61.001 67.605 0.0035588 67.605 75.390 0.0033417 75.390 84.667 0.0025631 84.667 93.841 0.0025051 93.841 104.68 0.0018373 104.68 117.64 0.00094644 117.64 133.34 0.00049025 133.34 148.47 0.00038412 148.47 166.57 0.00027273 166.57 188.54 0.00013048 188.54 215.70 4.1913e-05 215.70 240.61 2.1961e-05 240.61 270.72 8.2100e-06 270.72 307.81 2.0550e-06 307.81 354.53 1.4500e-07 \END; /* Data (Fig.10, p411 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '19' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,2; RCT=12C(ALPHA,P)X; THK-TGT=8850MG/CM**2; DET-PARTCL=P; \\DATA,2; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'20',<1%'21',<1%'22'); /* '20' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '21' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '22' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'23'; /* '23' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'24'; /* '24' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN'25' ENGY-EMT-LAB-MAX DN/DOMEGA/DE'26' (MEV) (MEV) (1/SR/MEV/PARTCL) X 28.320 0.00027559 28.320 31.370 0.0013878 31.370 34.950 0.0016169 34.950 38.685 0.0020089 38.685 43.067 0.0020770 43.067 48.259 0.0019929 48.259 53.637 0.0022584 53.637 59.998 0.0018814 59.998 66.430 0.0020083 66.430 73.999 0.0017817 73.999 83.001 0.0011937 83.001 91.885 0.0010873 91.885 102.36 0.00074722 102.36 114.85 0.00052710 114.85 129.94 0.00024569 129.94 144.44 0.00018307 144.44 161.72 0.00011393 161.72 182.63 5.4059e-05 182.63 208.33 1.5875e-05 208.33 231.79 7.9058e-06 231.79 260.01 2.7938e-06 260.01 294.53 8.0600e-07 \END; /* Data (Fig.10, p411 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '25' Lower limit energy of lowest bin is missed by authors. */ /* '26' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,3; RCT=12C(ALPHA,P)X; THK-TGT=8850MG/CM**2; DET-PARTCL=P; \\DATA,3; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'27',<1%'28',<1%'29'); /* '27' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '28' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '29' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'30'; /* '30' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'31'; /* '31' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN'32' ENGY-EMT-LAB-MAX DN/DOMEGA/DE'33' (MEV) (MEV) (1/SR/MEV/PARTCL) X 29.234 6.9946e-05 29.234 32.528 0.00041749 32.528 36.424 0.00081258 36.424 41.082 0.00077065 41.082 45.700 0.00095522 45.700 51.165 0.00090319 51.165 57.706 0.00067750 57.706 63.919 0.00079038 63.919 71.233 0.00070920 71.233 79.937 0.00060440 79.937 90.424 0.00047682 90.424 103.24 0.00025576 103.24 114.85 0.00023528 114.85 128.67 0.00015950 128.67 145.35 0.00010087 145.35 165.81 5.9213e-05 165.81 191.38 2.7876e-05 191.38 212.25 2.6309e-05 212.25 237.15 1.3655e-05 237.15 267.35 4.9379e-06 267.35 304.65 2.2650e-06 304.65 351.84 5.7186e-07 351.84 413.35 1.2698e-07 \END; /* Data (Fig.10, p411 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '32' Lower limit energy of lowest bin is missed by authors. */ /* '33' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,4; RCT=12C(ALPHA,P)X; THK-TGT=8850MG/CM**2; DET-PARTCL=P; \\DATA,4; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'34',<1%'35',<1%'36'); /* '34' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '35' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '36' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'37'; /* '37' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'38'; /* '38' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'39' (MEV) (MEV) (1/SR/MEV/PARTCL) 29.533 32.860 7.2453e-05 32.860 36.408 0.00011489 36.408 40.577 0.00010777 40.577 44.989 0.00011138 44.989 50.183 8.6598e-05 50.183 55.618 8.5280e-05 55.618 62.019 6.1780e-05 62.019 68.606 6.2406e-05 68.606 76.347 4.8354e-05 76.347 85.541 3.3254e-05 85.541 94.882 2.5701e-05 94.882 105.93 1.9640e-05 105.93 119.17 1.0331e-05 119.17 132.32 8.4530e-06 132.32 147.97 4.4786e-06 147.97 166.82 1.7673e-06 166.82 184.88 9.2214e-07 184.88 206.38 6.1535e-07 206.38 232.34 2.8316e-07 232.34 264.22 1.5366e-08 \END; /* Data (Fig.10, p411 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '39' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,5; RCT=12C(ALPHA,P)X; THK-TGT=8850MG/CM**2; DET-PARTCL=P; \\DATA,5; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'40',<1%'41',<1%'42'); /* '40' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '41' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '42' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'43'; /* '43' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=60DEG; DELTA-DN/DOMEGA/DE=<4%'44'; /* '44' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN'45' ENGY-EMT-LAB-MAX DN/DOMEGA/DE'46' (MEV) (MEV) (1/SR/MEV/PARTCL) X 27.550 2.7664e-06 27.550 30.829 6.5582e-06 30.829 34.213 5.4472e-06 34.213 38.199 4.8999e-06 38.199 42.942 3.0074e-06 42.942 47.767 3.2746e-06 47.767 53.479 2.5741e-06 53.479 60.316 1.5085e-06 60.316 67.106 1.2927e-06 67.106 75.160 7.9011e-07 75.160 84.828 3.1777e-07 84.828 94.044 1.6669e-07 94.044 104.94 1.6116e-07 104.94 117.96 3.3687e-08 \END; /* Data (Fig.10, p411 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '45' Lower limit energy of lowest bin is missed by authors. */ /* '46' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,6; RCT=12C(ALPHA,P)X; THK-TGT=8850MG/CM**2; DET-PARTCL=P; \\DATA,6; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'47',<1%'48',<1%'49'); /* '47' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '48' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '49' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'50'; /* '50' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=90DEG; DELTA-DN/DOMEGA/DE=<4%'51'; /* '51' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN'52' ENGY-EMT-LAB-MAX DN/DOMEGA/DE'53' (MEV) (MEV) (1/SR/MEV/PARTCL) X 29.533 8.9460e-07 29.533 32.696 1.4502e-06 32.696 36.408 1.1743e-06 36.408 40.805 7.3050e-07 40.805 45.256 4.6383e-07 45.256 50.499 4.8130e-07 50.499 56.738 2.5735e-07 56.738 62.898 2.9794e-07 62.898 70.159 1.5797e-07 70.159 78.810 1.0606e-07 78.810 89.250 2.1974e-08 \END; /* Data (Fig.10, p411 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '52' Lower limit energy of lowest bin is missed by authors. */ /* '53' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,7; RCT=27AL(ALPHA,P)X; THK-TGT=10800MG/CM**2; DET-PARTCL=P; \\DATA,7; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'54',<1%'55',<1%'56'); /* '54' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '55' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '56' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'57'; /* '57' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'58'; /* '58' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'59' (MEV) (MEV) (1/SR/MEV/PARTCL) 23.198 25.700 7.6787e-06 25.700 28.636 8.0960e-05 28.636 31.739 0.00071886 31.739 35.386 0.0013996 35.386 39.194 0.0019124 39.194 43.668 0.0021566 43.668 48.975 0.0019876 48.975 54.480 0.0022692 54.480 61.001 0.0020077 61.001 67.605 0.0023416 67.605 75.390 0.0022249 75.390 84.667 0.0016464 84.667 93.841 0.0016735 93.841 104.68 0.0012217 104.68 117.64 0.00064244 117.64 133.34 0.00034948 133.34 148.47 0.00027534 148.47 166.57 0.00019846 166.57 188.54 9.2888e-05 188.54 215.70 3.0599e-05 215.70 240.61 1.6581e-05 240.61 270.72 6.6976e-06 270.72 307.81 1.5540e-06 307.81 354.53 1.5420e-07 \END; /* Data (Fig.11, p412 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '59' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,8; RCT=27AL(ALPHA,P)X; THK-TGT=10800MG/CM**2; DET-PARTCL=P; \\DATA,8; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'60',<1%'61',<1%'62'); /* '60' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '61' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '62' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'63'; /* '63' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'64'; /* '64' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'65' (MEV) (MEV) (1/SR/MEV/PARTCL) 21.660 24.152 1.3577e-05 24.152 26.817 9.6266e-05 26.817 29.955 0.00057933 29.955 33.286 0.0011986 33.286 37.216 0.0012291 37.216 41.338 0.0014450 41.338 46.205 0.0013552 46.205 51.224 0.0015920 51.224 57.136 0.0016075 57.136 64.172 0.0013283 64.172 71.333 0.0013738 71.333 79.818 0.0011447 79.818 89.992 0.00074613 89.992 100.12 0.00063800 100.12 112.16 0.00041971 112.16 126.68 0.00022618 126.68 140.58 0.00015884 140.58 157.10 0.00010398 157.10 177.00 4.9957e-05 177.00 201.37 1.7559e-05 201.37 223.51 8.7770e-06 223.51 249.99 3.1316e-06 249.99 282.20 9.1495e-07 \END; /* Data (Fig.11, p412 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '65' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,9; RCT=27AL(ALPHA,P)X; THK-TGT=10800MG/CM**2; DET-PARTCL=P; \\DATA,9; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'66',<1%'67',<1%'68'); /* '66' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '67' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '68' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'69'; /* '69' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'70'; /* '70' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'71' (MEV) (MEV) (1/SR/MEV/PARTCL) 24.770 27.774 2.4945e-05 27.774 30.814 0.00014305 30.814 34.392 0.00051671 34.392 38.646 0.00055070 38.646 42.839 0.00068204 42.839 47.773 0.00067915 47.773 53.637 0.00064947 53.637 60.689 0.00050210 60.689 67.422 0.00057103 67.422 75.390 0.00049367 75.390 84.928 0.00041266 84.928 96.499 0.00024132 96.499 106.90 0.00022969 106.90 119.18 0.00015998 119.18 133.88 0.00010820 133.88 151.70 6.5406e-05 151.70 173.68 4.1636e-05 173.68 201.37 1.7672e-05 201.37 224.13 1.4464e-05 224.13 251.49 6.8545e-06 251.49 284.97 2.9993e-06 284.97 326.79 9.0188e-07 326.79 380.42 3.8350e-07 \END; /* Data (Fig.11, p412 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '71' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,10; RCT=27AL(ALPHA,P)X; THK-TGT=10800MG/CM**2; DET-PARTCL=P; \\DATA,10; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'72',<1%'73',<1%'74'); /* '72' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '73' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '74' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'75'; /* '75' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'76'; /* '76' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'77' (MEV) (MEV) (1/SR/MEV/PARTCL) 24.249 26.934 4.3204e-07 26.934 29.814 3.9473e-05 29.814 33.190 0.00015676 33.190 36.795 0.00017894 36.795 41.034 0.00016592 41.034 45.525 0.00017470 45.525 50.817 0.00013531 50.817 56.361 0.00013321 56.361 62.898 0.00010547 62.898 69.635 9.4704e-05 69.635 77.563 7.5253e-05 77.563 86.995 4.9935e-05 86.995 96.594 3.9194e-05 96.594 107.97 2.7969e-05 107.97 121.63 1.3651e-05 121.63 135.23 1.0798e-05 135.23 151.45 7.1993e-06 151.45 171.06 2.5247e-06 171.06 189.90 1.4773e-06 189.90 212.41 5.1552e-07 212.41 239.68 1.5593e-07 239.68 273.36 3.4446e-08 \END; /* Data (Fig.11, p412 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '77' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,11; RCT=27AL(ALPHA,P)X; THK-TGT=10800MG/CM**2; DET-PARTCL=P; \\DATA,11; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'78',<1%'79',<1%'80'); /* '78' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '79' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '80' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'81'; /* '81' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=60DEG; DELTA-DN/DOMEGA/DE=<4%'82'; /* '82' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'83' (MEV) (MEV) (1/SR/MEV/PARTCL) 21.862 24.456 5.9994e-07 24.456 27.177 1.0489e-05 27.177 30.388 1.3364e-05 30.388 33.696 1.4483e-05 33.696 37.587 1.1734e-05 37.587 42.211 8.6048e-06 42.211 46.907 7.1828e-06 46.907 52.456 5.2055e-06 52.456 59.085 2.4265e-06 59.085 65.656 1.8165e-06 65.656 73.433 9.5636e-07 73.433 82.745 3.9009e-07 82.745 91.598 3.3215e-07 91.598 102.03 9.9445e-08 102.03 114.48 4.1703e-08 \END; /* Data (Fig.11, p412 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '83' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,12; RCT=27AL(ALPHA,P)X; THK-TGT=10800MG/CM**2; DET-PARTCL=P; \\DATA,12; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'84',<1%'85',<1%'86'); /* '84' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '85' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '86' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'87'; /* '87' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=90DEG; DELTA-DN/DOMEGA/DE=<4%'88'; /* '88' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'89' (MEV) (MEV) (1/SR/MEV/PARTCL) 17.590 19.663 1.8170e-07 19.663 21.862 1.1986e-06 21.862 24.456 9.4316e-07 24.456 27.177 9.6859e-07 27.177 30.388 1.7594e-06 30.388 33.696 1.3657e-06 33.696 37.587 1.4997e-06 37.587 42.211 9.3652e-07 42.211 46.907 6.0135e-07 46.907 52.456 4.4102e-07 52.456 59.085 2.8397e-07 59.085 65.656 1.4326e-07 65.656 73.433 1.6945e-07 73.433 82.745 6.0652e-08 82.745 91.598 4.2529e-08 91.598 102.03 1.8039e-08 \END; /* Data (Fig.11, p412 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '89' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,13; RCT=CU(ALPHA,P)X; THK-TGT=13395MG/CM**2; DET-PARTCL=P; \\DATA,13; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'90',<1%'91',<1%'92'); /* '90' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '91' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '92' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'93'; /* '93' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'94'; /* '94' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'95' (MEV) (MEV) (1/SR/MEV/PARTCL) 24.152 26.817 2.0427e-05 26.817 29.955 0.00010004 29.955 33.286 0.00074989 33.286 37.216 0.00091929 37.216 41.338 0.0011455 41.338 46.205 0.0011044 46.205 51.224 0.0012969 51.224 57.136 0.0013615 57.136 64.172 0.0011584 64.172 71.333 0.0013106 71.333 79.818 0.0011947 79.818 89.992 0.00086322 89.992 100.12 0.00081252 100.12 112.16 0.00047858 112.16 126.68 0.00025107 126.68 140.58 0.00020322 140.58 157.10 0.00013987 157.10 177.00 8.3874e-05 177.00 201.37 3.0582e-05 201.37 223.51 1.8535e-05 223.51 249.99 8.3768e-06 249.99 282.20 2.6646e-06 282.20 322.14 6.2893e-07 \END; /* Data (Fig.12, p413 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '95' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,14; RCT=CU(ALPHA,P)X; THK-TGT=13395MG/CM**2; DET-PARTCL=P; \\DATA,14; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'96',<1%'97',<1%'98'); /* '96' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '97' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '98' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'99'; /* '99' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'100'; /* '100' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'101' (MEV) (MEV) (1/SR/MEV/PARTCL) 22.968 25.432 2.5209e-05 25.432 28.320 0.00014722 28.320 31.370 0.00059726 31.370 34.950 0.00069086 34.950 38.685 0.00086177 38.685 43.067 0.00089102 43.067 48.259 0.00082429 48.259 53.637 0.00096695 53.637 59.998 0.00082151 59.998 66.430 0.00086985 66.430 73.999 0.00077914 73.999 83.001 0.00053635 83.001 91.885 0.00049794 91.885 102.36 0.00034880 102.36 114.85 0.00024512 114.85 129.94 0.00011831 129.94 144.44 8.9557e-05 144.44 161.72 5.7804e-05 161.72 182.63 2.6557e-05 182.63 208.33 8.2350e-06 208.33 231.79 4.4911e-06 231.79 260.01 1.6004e-06 260.01 294.53 3.8156e-07 \END; /* Data (Fig.12, p413 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '101' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,15; RCT=CU(ALPHA,P)X; THK-TGT=13395MG/CM**2; DET-PARTCL=P; \\DATA,15; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'102',<1%'103',<1%'104'); /* '102' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '103' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '104' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'105'; /* '105' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'106'; /* '106' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'107' (MEV) (MEV) (1/SR/MEV/PARTCL) 24.770 27.774 1.3911e-05 27.774 30.814 0.00010547 30.814 34.392 0.00032409 34.392 38.646 0.00033713 38.646 42.839 0.00039674 42.839 47.773 0.00041147 47.773 53.637 0.00039202 53.637 60.689 0.00029832 60.689 67.422 0.00033940 67.422 75.390 0.00030929 75.390 84.928 0.00025476 84.928 96.499 0.00014665 96.499 106.90 0.00014520 106.90 119.18 0.00010197 119.18 133.88 6.6234e-05 133.88 151.70 4.1891e-05 151.70 173.68 2.5569e-05 173.68 201.37 1.1465e-05 201.37 224.13 1.0772e-05 224.13 251.49 4.3021e-06 251.49 284.97 2.2326e-06 284.97 326.79 7.3030e-07 326.79 380.42 1.4982e-07 \END; /* Data (Fig.12, p413 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '107' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,16; RCT=CU(ALPHA,P)X; THK-TGT=13395MG/CM**2; DET-PARTCL=P; \\DATA,16; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'108',<1%'109',<1%'110'); /* '108' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '109' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '110' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'111'; /* '111' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'112'; /* '112' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'113' (MEV) (MEV) (1/SR/MEV/PARTCL) 26.693 29.533 1.3876e-05 29.533 32.860 4.6117e-05 32.860 36.408 7.2783e-05 36.408 40.577 6.1641e-05 40.577 44.989 6.6890e-05 44.989 50.183 5.3352e-05 50.183 55.618 5.4842e-05 55.618 62.019 4.2053e-05 62.019 68.606 4.1686e-05 68.606 76.347 3.2655e-05 76.347 85.541 2.1294e-05 85.541 94.882 1.9298e-05 94.882 105.93 1.4415e-05 105.93 119.17 7.1918e-06 119.17 132.32 6.4043e-06 132.32 147.97 3.8320e-06 147.97 166.82 1.6901e-06 166.82 184.88 9.2825e-07 184.88 206.38 3.7051e-07 206.38 232.34 9.6913e-08 232.34 264.22 1.3148e-08 \END; /* Data (Fig.12, p413 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '113' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,17; RCT=CU(ALPHA,P)X; THK-TGT=13395MG/CM**2; DET-PARTCL=P; \\DATA,17; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'114',<1%'115',<1%'116'); /* '114' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '115' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '116' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'117'; /* '117' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=60DEG; DELTA-DN/DOMEGA/DE=<4%'118'; /* '118' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'119' (MEV) (MEV) (1/SR/MEV/PARTCL) 23.542 26.105 1.9690e-06 26.105 29.119 4.9631e-06 29.119 32.214 6.0416e-06 32.214 35.840 5.7752e-06 35.840 40.128 4.5775e-06 40.128 44.464 4.9593e-06 44.464 49.562 3.4105e-06 49.562 55.618 2.1609e-06 55.618 61.586 1.5665e-06 61.586 68.606 1.1985e-06 68.606 76.951 4.2564e-07 76.951 86.995 2.6061e-07 86.995 96.594 1.9477e-07 96.594 107.97 1.1502e-07 \END; /* Data (Fig.12, p413 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '119' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,18; RCT=CU(ALPHA,P)X; THK-TGT=13395MG/CM**2; DET-PARTCL=P; \\DATA,18; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'120',<1%'121',<1%'122'); /* '120' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '121' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '122' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'123'; /* '123' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=90DEG; DELTA-DN/DOMEGA/DE=<4%'124'; /* '124' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'125' (MEV) (MEV) (1/SR/MEV/PARTCL) 16.330 18.176 1.1792e-07 18.176 20.122 1.7899e-06 20.122 22.401 2.2917e-06 22.401 24.773 3.2108e-06 24.773 27.550 1.0034e-05 27.550 30.829 7.1018e-06 30.829 34.213 8.8112e-06 34.213 38.199 7.4806e-06 38.199 42.942 5.0478e-06 42.942 47.767 4.5559e-06 47.767 53.479 2.9722e-06 53.479 60.316 1.5280e-06 60.316 67.106 8.0133e-07 67.106 75.160 7.0257e-07 75.160 84.828 3.8270e-07 84.828 94.044 2.3617e-07 94.044 104.94 3.9961e-08 104.94 117.96 3.3411e-08 117.96 133.77 1.3775e-08 \END; /* Data (Fig.12, p413 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '125' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,19; RCT=PB(ALPHA,P)X; THK-TGT=17010MG/CM**2; DET-PARTCL=P; \\DATA,19; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'126',<1%'127',<1%'128'); /* '126' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '127' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '128' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'129'; /* '129' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'130'; /* '130' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'131' (MEV) (MEV) (1/SR/MEV/PARTCL) 23.198 25.700 1.4252e-06 25.700 28.636 2.8535e-05 28.636 31.739 0.00020911 31.739 35.386 0.00039305 35.386 39.194 0.00053085 39.194 43.668 0.00060994 43.668 48.975 0.00054853 48.975 54.480 0.00067215 54.480 61.001 0.00061814 61.001 67.605 0.00067361 67.605 75.390 0.00067225 75.390 84.667 0.00051829 84.667 93.841 0.00051314 93.841 104.68 0.00039607 104.68 117.64 0.00020584 117.64 133.34 0.00011375 133.34 148.47 9.4846e-05 148.47 166.57 6.6334e-05 166.57 188.54 3.4562e-05 188.54 215.70 1.1556e-05 215.70 240.61 6.1193e-06 240.61 270.72 2.6638e-06 270.72 307.81 5.2880e-07 307.81 354.53 3.8161e-08 \END; /* Data (Fig.13, p414 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '131' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,20; RCT=PB(ALPHA,P)X; THK-TGT=17010MG/CM**2; DET-PARTCL=P; \\DATA,20; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'132',<1%'133',<1%'134'); /* '132' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '133' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '134' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'135'; /* '135' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'136'; /* '136' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'137' (MEV) (MEV) (1/SR/MEV/PARTCL) 21.660 24.152 5.8088e-06 24.152 26.817 2.6864e-05 26.817 29.955 0.00018961 29.955 33.286 0.00036877 33.286 37.216 0.00038941 37.216 41.338 0.00047697 41.338 46.205 0.00043416 46.205 51.224 0.00052678 51.224 57.136 0.00053451 57.136 64.172 0.00045701 64.172 71.333 0.00048605 71.333 79.818 0.00041483 79.818 89.992 0.00028379 89.992 100.12 0.00024645 100.12 112.16 0.00016451 112.16 126.68 8.5049e-05 126.68 140.58 6.0980e-05 140.58 157.10 4.5173e-05 157.10 177.00 2.1335e-05 177.00 201.37 7.3271e-06 201.37 223.51 4.3963e-06 223.51 249.99 1.2145e-06 249.99 282.20 3.9951e-07 \END; /* Data (Fig.13, p414 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '137' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,21; RCT=PB(ALPHA,P)X; THK-TGT=17010MG/CM**2; DET-PARTCL=P; \\DATA,21; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'138',<1%'139',<1%'140'); /* '138' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '139' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '140' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'141'; /* '141' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'142'; /* '142' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'143' (MEV) (MEV) (1/SR/MEV/PARTCL) 23.631 26.422 3.7545e-06 26.422 29.234 1.8872e-05 29.234 32.528 0.00012753 32.528 36.424 0.00021851 36.424 41.082 0.00020189 41.082 45.700 0.00025070 45.700 51.165 0.00025721 51.165 57.706 0.00019600 57.706 63.919 0.00023686 63.919 71.233 0.00021588 71.233 79.937 0.00019435 79.937 90.424 0.00015932 90.424 103.24 8.9101e-05 103.24 114.85 8.0926e-05 114.85 128.67 5.9492e-05 128.67 145.35 3.7866e-05 145.35 165.81 2.1412e-05 165.81 191.38 1.0217e-05 191.38 212.25 9.5427e-06 212.25 237.15 4.7632e-06 237.15 267.35 2.0595e-06 267.35 304.65 6.3421e-07 304.65 351.84 2.5789e-07 351.84 413.35 5.4949e-08 \END; /* Data (Fig.13, p414 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '143' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,22; RCT=PB(ALPHA,P)X; THK-TGT=17010MG/CM**2; DET-PARTCL=P; \\DATA,22; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'144',<1%'145',<1%'146'); /* '144' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '145' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '146' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'147'; /* '147' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'148'; /* '148' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'149' (MEV) (MEV) (1/SR/MEV/PARTCL) 26.693 29.533 1.1157e-05 29.533 32.860 4.0505e-05 32.860 36.408 6.2964e-05 36.408 40.577 5.9262e-05 40.577 44.989 5.8723e-05 44.989 50.183 4.8032e-05 50.183 55.618 4.9886e-05 55.618 62.019 3.8604e-05 62.019 68.606 3.7447e-05 68.606 76.347 2.8288e-05 76.347 85.541 2.0765e-05 85.541 94.882 1.8077e-05 94.882 105.93 1.1831e-05 105.93 119.17 5.6076e-06 119.17 132.32 5.5175e-06 132.32 147.97 3.0253e-06 147.97 166.82 1.6808e-06 166.82 184.88 7.9928e-07 184.88 206.38 3.9179e-07 206.38 232.34 1.0817e-07 \END; /* Data (Fig.13, p414 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '149' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,23; RCT=PB(ALPHA,P)X; THK-TGT=17010MG/CM**2; DET-PARTCL=P; \\DATA,23; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'150',<1%'151',<1%'152'); /* '150' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '151' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '152' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'153'; /* '153' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=60DEG; DELTA-DN/DOMEGA/DE=<4%'154'; /* '154' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'155' (MEV) (MEV) (1/SR/MEV/PARTCL) 21.862 24.456 4.1458e-07 24.456 27.177 4.4148e-06 27.177 30.388 6.9820e-06 30.388 33.696 6.0699e-06 33.696 37.587 5.0681e-06 37.587 42.211 3.6841e-06 42.211 46.907 3.9327e-06 46.907 52.456 2.9079e-06 52.456 59.085 1.5686e-06 59.085 65.656 1.3644e-06 65.656 73.433 1.0374e-06 73.433 82.745 5.0063e-07 82.745 91.598 3.2404e-07 91.598 102.03 5.1541e-08 \END; /* Data (Fig.13, p414 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '155' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,24; RCT=PB(ALPHA,P)X; THK-TGT=17010MG/CM**2; DET-PARTCL=P; \\DATA,24; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'156',<1%'157',<1%'158'); /* '156' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '157' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '158' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'159'; /* '159' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=P; THTL=90DEG; DELTA-DN/DOMEGA/DE=<4%'160'; /* '160' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'161' (MEV) (MEV) (1/SR/MEV/PARTCL) 18.176 20.122 2.9588e-06 20.122 22.401 2.8864e-06 22.401 24.773 3.8128e-06 24.773 27.550 1.0515e-05 27.550 30.829 9.2162e-06 30.829 34.213 9.7205e-06 34.213 38.199 7.9431e-06 38.199 42.942 4.5948e-06 42.942 47.767 4.0479e-06 47.767 53.479 3.0235e-06 53.479 60.316 1.2629e-06 60.316 67.106 1.1808e-06 67.106 75.160 6.1260e-07 75.160 84.828 2.5518e-07 84.828 94.044 2.6771e-07 94.044 104.94 1.8874e-08 104.94 117.96 3.1560e-08 \END; /* Data (Fig.13, p414 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '161' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,25; RCT=12C(ALPHA,D)X; THK-TGT=8850MG/CM**2; DET-PARTCL=D; \\DATA,25; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'162',<1%'163',<1%'164'); /* '162' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '163' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '164' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'165'; /* '165' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'166'; /* '166' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN'167' ENGY-EMT-LAB-MAX DN/DOMEGA/DE'168' (MEV) (MEV) (1/SR/MEV/PARTCL) X 41.309 0.00027313 41.309 45.937 0.0011440 45.937 50.863 0.0017429 50.863 56.640 0.0016290 56.640 62.740 0.0019186 62.740 69.900 0.0018138 69.900 77.370 0.0022534 77.370 86.134 0.0024470 86.134 96.518 0.0023403 96.518 107.27 0.0028124 107.27 120.00 0.0027012 120.00 132.86 0.0031176 132.86 148.00 0.0028337 148.00 166.00 0.0019157 166.00 183.77 0.0017775 183.77 204.72 0.0012266 204.72 229.70 0.00064719 229.70 259.88 0.00021633 259.88 288.88 6.9622e-05 288.88 323.45 1.5725e-05 \END; /* Data (Fig.14, p415 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '167' Lower limit energy of lowest bin is missed by authors. */ /* '168' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,26; RCT=12C(ALPHA,D)X; THK-TGT=8850MG/CM**2; DET-PARTCL=D; \\DATA,26; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'169',<1%'170',<1%'171'); /* '169' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '170' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '171' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'172'; /* '172' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'173'; /* '173' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'174' (MEV) (MEV) (1/SR/MEV/PARTCL) 38.723 42.907 0.00082980 42.907 47.816 0.00094038 47.816 53.061 0.0010592 53.061 59.234 0.0010337 59.234 65.777 0.0011976 65.777 73.490 0.0011000 73.490 81.572 0.0012828 81.572 91.099 0.0011633 91.099 100.91 0.0013567 100.91 112.46 0.0012878 112.46 126.17 0.00099072 126.17 140.11 0.00094848 140.11 156.60 0.00069687 156.60 176.32 0.00038753 176.32 195.91 0.00031479 195.91 219.15 0.00020480 219.15 247.09 3.3809e-05 247.09 273.77 2.3584e-05 273.77 305.38 6.7973e-06 \END; /* Data (Fig.14, p415 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '174' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,27; RCT=12C(ALPHA,D)X; THK-TGT=8850MG/CM**2; DET-PARTCL=D; \\DATA,27; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'175',<1%'176',<1%'177'); /* '175' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '176' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '177' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'178'; /* '178' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'179'; /* '179' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'180' (MEV) (MEV) (1/SR/MEV/PARTCL) 37.950 42.529 0.00014481 42.529 47.262 0.00049687 47.262 52.844 0.00044029 52.844 58.468 0.00054088 58.468 65.056 0.00049886 65.056 72.849 0.00048793 72.849 82.164 0.00044090 82.164 91.399 0.00051406 91.399 102.33 0.00046283 102.33 115.41 0.00032008 115.41 127.84 0.00033913 127.84 142.47 0.00026457 142.47 159.88 0.00019044 159.88 180.85 0.00010076 180.85 206.48 4.4538e-05 206.48 229.70 5.3620e-05 229.70 257.34 3.0487e-05 257.34 290.71 1.0960e-05 290.71 331.62 2.6726e-06 \END; /* Data (Fig.14, p415 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '180' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,28; RCT=12C(ALPHA,D)X; THK-TGT=8850MG/CM**2; DET-PARTCL=D; \\DATA,28; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'181',<1%'182',<1%'183'); /* '181' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '182' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '183' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'184'; /* '184' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'185'; /* '185' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'186' (MEV) (MEV) (1/SR/MEV/PARTCL) 39.027 43.199 2.6892e-05 43.199 48.087 4.5007e-05 48.087 53.386 4.6324e-05 53.386 59.066 4.6324e-05 59.066 65.720 3.8435e-05 65.720 72.816 3.4315e-05 72.816 81.154 2.8852e-05 81.154 89.979 2.3209e-05 89.979 100.37 1.7074e-05 100.37 111.24 1.3477e-05 111.24 124.04 8.8804e-06 124.04 137.21 7.1034e-06 137.21 152.69 4.9683e-06 152.69 171.08 2.3981e-06 171.08 189.76 1.2588e-06 189.76 211.87 8.6453e-07 \END; /* Data (Fig.14, p415 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '186' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,29; RCT=12C(ALPHA,D)X; THK-TGT=8850MG/CM**2; DET-PARTCL=D; \\DATA,29; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'187',<1%'188',<1%'189'); /* '187' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '188' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '189' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'190'; /* '190' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=60DEG; DELTA-DN/DOMEGA/DE=<4%'191'; /* '191' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN'192' ENGY-EMT-LAB-MAX DN/DOMEGA/DE'193' (MEV) (MEV) (1/SR/MEV/PARTCL) X 38.879 1.1847e-06 38.879 43.199 1.1175e-06 43.199 48.291 5.1711e-07 48.291 53.626 7.4048e-07 53.626 59.911 5.5862e-07 59.911 66.381 3.7310e-07 66.381 73.981 3.7537e-07 73.981 82.997 2.4339e-07 82.997 92.140 9.6010e-08 92.140 102.93 2.0345e-08 \END; /* Data (Fig.14, p415 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '192' Lower limit energy of lowest bin is missed by authors. */ /* '193' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,30; RCT=27AL(ALPHA,D)X; THK-TGT=10800MG/CM**2; DET-PARTCL=D; \\DATA,30; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'194',<1%'195',<1%'196'); /* '194' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '195' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '196' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'197'; /* '197' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'198'; /* '198' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'199' (MEV) (MEV) (1/SR/MEV/PARTCL) 35.127 39.077 3.4046e-05 39.077 43.320 0.00053897 43.320 48.305 0.00088719 48.305 53.633 0.0011689 53.633 59.911 0.0010977 59.911 66.571 0.0012862 66.571 74.432 0.0012450 74.432 82.677 0.0015141 82.677 92.409 0.0014289 92.409 102.45 0.0016959 102.45 114.27 0.0019215 114.27 128.34 0.0016892 128.34 142.67 0.0018187 142.67 159.64 0.0015182 159.64 179.99 0.00097372 179.99 200.24 0.00081488 200.24 224.33 0.00047012 224.33 253.36 0.00019405 253.36 281.16 6.3873e-05 281.16 314.20 1.7877e-05 314.20 354.01 2.1113e-07 \END; /* Data (Fig.15, p416 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '199' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,31; RCT=27AL(ALPHA,D)X; THK-TGT=10800MG/CM**2; DET-PARTCL=D; \\DATA,31; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'200',<1%'201',<1%'202'); /* '200' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '201' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '202' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'203'; /* '203' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'204'; /* '204' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'205' (MEV) (MEV) (1/SR/MEV/PARTCL) 34.826 38.723 0.00012155 38.723 42.907 0.00056818 42.907 47.816 0.00062332 47.816 53.061 0.00073373 53.061 59.234 0.00067861 59.234 65.777 0.00077804 65.777 73.490 0.00073823 73.490 81.572 0.00087757 81.572 91.099 0.00077808 91.099 100.91 0.00090516 100.91 112.46 0.00088274 112.46 126.17 0.00070368 126.17 140.11 0.00069235 140.11 156.60 0.00051317 156.60 176.32 0.00029572 176.32 195.91 0.00025292 195.91 219.15 0.00015996 219.15 247.09 2.7545e-05 247.09 273.77 2.1153e-05 273.77 305.38 5.8354e-06 \END; /* Data (Fig.15, p416 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '205' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,32; RCT=27AL(ALPHA,D)X; THK-TGT=10800MG/CM**2; DET-PARTCL=D; \\DATA,32; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'206',<1%'207',<1%'208'); /* '206' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '207' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '208' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'209'; /* '209' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'210'; /* '210' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'211' (MEV) (MEV) (1/SR/MEV/PARTCL) 37.950 42.529 0.00011037 42.529 47.262 0.00033881 47.262 52.844 0.00032213 52.844 58.468 0.00037249 58.468 65.056 0.00036462 65.056 72.849 0.00036039 72.849 82.164 0.00031959 82.164 91.399 0.00036483 91.399 102.33 0.00034099 102.33 115.41 0.00024437 115.41 127.84 0.00025253 127.84 142.47 0.00019713 142.47 159.88 0.00014208 159.88 180.85 7.4497e-05 180.85 206.48 3.1295e-05 206.48 229.70 3.8864e-05 229.70 257.34 2.2553e-05 257.34 290.71 7.9268e-06 290.71 331.62 2.1308e-06 \END; /* Data (Fig.15, p416 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '211' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,33; RCT=27AL(ALPHA,D)X; THK-TGT=10800MG/CM**2; DET-PARTCL=D; \\DATA,33; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'212',<1%'213',<1%'214'); /* '212' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '213' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '214' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'215'; /* '215' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'216'; /* '216' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'217' (MEV) (MEV) (1/SR/MEV/PARTCL) 39.027 43.199 4.7080e-05 43.199 48.087 8.9708e-05 48.087 53.386 8.7054e-05 53.386 59.066 8.9932e-05 59.066 65.720 7.6355e-05 65.720 72.816 7.1273e-05 72.816 81.154 5.8246e-05 81.154 89.979 5.0391e-05 89.979 100.37 3.8638e-05 100.37 111.24 3.1268e-05 111.24 124.04 1.7309e-05 124.04 137.21 1.5292e-05 137.21 152.69 8.0917e-06 152.69 171.08 3.4066e-06 171.08 189.76 2.7527e-06 189.76 211.87 1.0672e-06 \END; /* Data (Fig.15, p416 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '217' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,34; RCT=27AL(ALPHA,D)X; THK-TGT=10800MG/CM**2; DET-PARTCL=D; \\DATA,34; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'218',<1%'219',<1%'220'); /* '218' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '219' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '220' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'221'; /* '221' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=60DEG; DELTA-DN/DOMEGA/DE=<4%'222'; /* '222' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'223' (MEV) (MEV) (1/SR/MEV/PARTCL) 29.508 32.661 9.8769e-07 32.661 36.352 3.4208e-06 36.352 40.243 5.4233e-06 40.243 44.802 4.7050e-06 44.802 49.547 3.5360e-06 49.547 55.099 2.5855e-06 55.099 61.658 1.1605e-06 61.658 68.426 7.6671e-07 68.426 76.398 4.3395e-07 76.398 85.884 2.7352e-07 85.884 95.534 1.0755e-07 95.534 106.96 6.0567e-08 106.96 120.63 1.2650e-08 \END; /* Data (Fig.15, p416 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '223' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,35; RCT=CU(ALPHA,D)X; THK-TGT=13395MG/CM**2; DET-PARTCL=D; \\DATA,35; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'224',<1%'225',<1%'226'); /* '224' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '225' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '226' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'227'; /* '227' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'228'; /* '228' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'229' (MEV) (MEV) (1/SR/MEV/PARTCL) 35.127 39.077 2.3319e-05 39.077 43.320 0.00035910 43.320 48.305 0.00055436 48.305 53.633 0.00070000 53.633 59.911 0.00064207 59.911 66.571 0.00077393 66.571 74.432 0.00074432 74.432 82.677 0.00086800 82.677 92.409 0.00081505 92.409 102.45 0.00098308 102.45 114.27 0.0010936 114.27 128.34 0.00096331 128.34 142.67 0.00098090 142.67 159.64 0.00083656 159.64 179.99 0.00051509 179.99 200.24 0.00042270 200.24 224.33 0.00024659 224.33 253.36 9.6298e-05 253.36 281.16 3.5614e-05 281.16 314.20 8.9639e-06 314.20 354.01 2.8922e-07 \END; /* Data (Fig.16, p417 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '229' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,36; RCT=CU(ALPHA,D)X; THK-TGT=13395MG/CM**2; DET-PARTCL=D; \\DATA,36; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'230',<1%'231',<1%'232'); /* '230' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '231' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '232' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'233'; /* '233' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'234'; /* '234' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'235' (MEV) (MEV) (1/SR/MEV/PARTCL) 31.493 34.826 5.6466e-07 34.826 38.723 9.1738e-05 38.723 42.907 0.00033169 42.907 47.816 0.00038056 47.816 53.061 0.00041633 53.061 59.234 0.00041289 59.234 65.777 0.00048920 65.777 73.490 0.00042533 73.490 81.572 0.00050454 81.572 91.099 0.00046482 91.099 100.91 0.00053410 100.91 112.46 0.00052961 112.46 126.17 0.00042000 126.17 140.11 0.00040671 140.11 156.60 0.00031731 156.60 176.32 0.00017911 176.32 195.91 0.00015087 195.91 219.15 9.8388e-05 219.15 247.09 1.6940e-05 247.09 273.77 1.2697e-05 273.77 305.38 3.4526e-06 \END; /* Data (Fig.16, p417 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '235' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,37; RCT=CU(ALPHA,D)X; THK-TGT=13395MG/CM**2; DET-PARTCL=D; \\DATA,37; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'236',<1%'237',<1%'238'); /* '236' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '237' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '238' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'239'; /* '239' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'240'; /* '240' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'241' (MEV) (MEV) (1/SR/MEV/PARTCL) 34.077 37.950 3.2168e-06 37.950 42.529 4.8081e-05 42.529 47.262 0.00012251 47.262 52.844 0.00012246 52.844 58.468 0.00013861 58.468 65.056 0.00013033 65.056 72.849 0.00014211 72.849 82.164 0.00011751 82.164 91.399 0.00014180 91.399 102.33 0.00013719 102.33 115.41 0.00010394 115.41 127.84 0.00011593 127.84 142.47 9.2398e-05 142.47 159.88 7.2826e-05 159.88 180.85 4.6270e-05 180.85 206.48 1.8809e-05 206.48 229.70 2.1412e-05 229.70 257.34 1.2340e-05 257.34 290.71 3.0830e-06 290.71 331.62 1.0705e-06 \END; /* Data (Fig.16, p417 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '241' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,38; RCT=CU(ALPHA,D)X; THK-TGT=13395MG/CM**2; DET-PARTCL=D; \\DATA,38; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'242',<1%'243',<1%'244'); /* '242' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '243' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '244' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'245'; /* '245' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'246'; /* '246' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'247' (MEV) (MEV) (1/SR/MEV/PARTCL) 37.865 42.178 1.1860e-05 42.178 46.887 3.3296e-05 46.887 51.981 3.3577e-05 51.981 57.967 2.8505e-05 57.967 64.427 2.7382e-05 64.427 71.306 2.3221e-05 71.306 79.373 2.0215e-05 79.373 87.895 1.9384e-05 87.895 97.904 1.3444e-05 97.904 108.36 1.2636e-05 108.36 120.63 9.8008e-06 120.63 135.20 5.2084e-06 135.20 150.32 4.6857e-06 150.32 168.25 2.1980e-06 168.25 186.43 1.5446e-06 186.43 207.91 8.0037e-07 \END; /* Data (Fig.16, p417 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '247' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,39; RCT=CU(ALPHA,D)X; THK-TGT=13395MG/CM**2; DET-PARTCL=D; \\DATA,39; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'248',<1%'249',<1%'250'); /* '248' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '249' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '250' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'251'; /* '251' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=60DEG; DELTA-DN/DOMEGA/DE=<4%'252'; /* '252' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'253' (MEV) (MEV) (1/SR/MEV/PARTCL) 29.508 32.661 8.3034e-07 32.661 36.352 9.1170e-07 36.352 40.243 2.1142e-06 40.243 44.802 1.5175e-06 44.802 49.547 1.1033e-06 49.547 55.099 8.0808e-07 55.099 61.658 7.1269e-07 61.658 68.426 4.9724e-07 68.426 76.398 2.3453e-07 76.398 85.884 1.1826e-07 85.884 95.534 7.7498e-08 95.534 106.96 6.5466e-08 106.96 120.63 1.3673e-08 \END; /* Data (Fig.16, p417 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '253' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,40; RCT=PB(ALPHA,D)X; THK-TGT=17010MG/CM**2; DET-PARTCL=D; \\DATA,40; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'254',<1%'255',<1%'256'); /* '254' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '255' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '256' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'257'; /* '257' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'258'; /* '258' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'259' (MEV) (MEV) (1/SR/MEV/PARTCL) 35.127 39.077 8.8015e-06 39.077 43.320 0.00015250 43.320 48.305 0.00024948 48.305 53.633 0.00032033 53.633 59.911 0.00030217 59.911 66.571 0.00034757 66.571 74.432 0.00035404 74.432 82.677 0.00041827 82.677 92.409 0.00038696 92.409 102.45 0.00046107 102.45 114.27 0.00053739 114.27 128.34 0.00046890 128.34 142.67 0.00048955 142.67 159.64 0.00042029 159.64 179.99 0.00026149 179.99 200.24 0.00021915 200.24 224.33 0.00012913 224.33 253.36 5.2506e-05 253.36 281.16 1.9334e-05 281.16 314.20 5.6650e-06 314.20 354.01 2.6871e-07 \END; /* Data (Fig.17, p418 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '259' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,41; RCT=PB(ALPHA,D)X; THK-TGT=17010MG/CM**2; DET-PARTCL=D; \\DATA,41; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'260',<1%'261',<1%'262'); /* '260' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '261' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '262' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'263'; /* '263' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'264'; /* '264' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'265' (MEV) (MEV) (1/SR/MEV/PARTCL) 34.826 38.723 3.9829e-05 38.723 42.907 0.00017377 42.907 47.816 0.00017772 47.816 53.061 0.00020746 53.061 59.234 0.00020559 59.234 65.777 0.00022372 65.777 73.490 0.00022084 73.490 81.572 0.00024411 81.572 91.099 0.00023644 91.099 100.91 0.00028129 100.91 112.46 0.00028056 112.46 126.17 0.00023290 126.17 140.11 0.00023941 140.11 156.60 0.00018846 156.60 176.32 0.00010952 176.32 195.91 9.4885e-05 195.91 219.15 6.4452e-05 219.15 247.09 1.2350e-05 247.09 273.77 8.2002e-06 273.77 305.38 2.1626e-06 \END; /* Data (Fig.17, p418 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '265' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,42; RCT=PB(ALPHA,D)X; THK-TGT=17010MG/CM**2; DET-PARTCL=D; \\DATA,42; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'266',<1%'267',<1%'268'); /* '266' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '267' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '268' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'269'; /* '269' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'270'; /* '270' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'271' (MEV) (MEV) (1/SR/MEV/PARTCL) 34.077 37.950 2.7058e-06 37.950 42.529 4.0444e-05 42.529 47.262 0.00010305 47.262 52.844 0.00010301 52.844 58.468 0.00011660 58.468 65.056 0.00010963 65.056 72.849 0.00011954 72.849 82.164 9.8841e-05 82.164 91.399 0.00011927 91.399 102.33 0.00011540 102.33 115.41 8.7433e-05 115.41 127.84 9.7512e-05 127.84 142.47 7.7721e-05 142.47 159.88 6.1258e-05 159.88 180.85 3.8920e-05 180.85 206.48 1.5821e-05 206.48 229.70 1.8011e-05 229.70 257.34 1.0380e-05 257.34 290.71 2.5933e-06 290.71 331.62 9.0045e-07 \END; /* Data (Fig.17, p418 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '271' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,43; RCT=PB(ALPHA,D)X; THK-TGT=17010MG/CM**2; DET-PARTCL=D; \\DATA,43; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'272',<1%'273',<1%'274'); /* '272' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '273' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '274' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'275'; /* '275' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'276'; /* '276' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'277' (MEV) (MEV) (1/SR/MEV/PARTCL) 35.436 39.326 9.2813e-07 39.326 43.547 1.8051e-05 43.547 48.497 2.7063e-05 48.497 53.867 2.8233e-05 53.867 59.627 2.5207e-05 59.627 66.381 2.2508e-05 66.381 73.590 2.1699e-05 73.590 82.068 1.7220e-05 82.068 91.049 1.7595e-05 91.049 101.63 1.3983e-05 101.63 112.72 1.0092e-05 112.72 125.80 6.8108e-06 125.80 139.27 5.5963e-06 139.27 155.13 3.5412e-06 155.13 173.99 2.0412e-06 173.99 193.19 1.3370e-06 193.19 215.95 4.5826e-07 215.95 243.25 1.4688e-08 \END; /* Data (Fig.17, p418 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '277' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,44; RCT=PB(ALPHA,D)X; THK-TGT=17010MG/CM**2; DET-PARTCL=D; \\DATA,44; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'278',<1%'279',<1%'280'); /* '278' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '279' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '280' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'281'; /* '281' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=D; THTL=60DEG; DELTA-DN/DOMEGA/DE=<4%'282'; /* '282' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'283' (MEV) (MEV) (1/SR/MEV/PARTCL) 27.567 30.712 2.2810e-07 30.712 34.066 9.0868e-07 34.066 38.008 2.0925e-06 38.008 42.178 2.2357e-06 42.178 47.084 1.9005e-06 47.084 52.211 9.7911e-07 52.211 58.238 8.3293e-07 58.238 64.427 6.9526e-07 64.427 71.679 4.6977e-07 71.679 80.256 2.5085e-07 80.256 88.927 2.2746e-07 88.927 99.124 5.2752e-08 99.124 111.24 4.4406e-08 111.24 123.17 1.5023e-08 \END; /* Data (Fig.17, p418 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '283' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,45; RCT=12C(ALPHA,T)X; THK-TGT=8850MG/CM**2; DET-PARTCL=T; \\DATA,45; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'284',<1%'285',<1%'286'); /* '284' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '285' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '286' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'287'; /* '287' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'288'; /* '288' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'289' (MEV) (MEV) (1/SR/MEV/PARTCL) 45.733 50.916 0.00054138 50.916 56.533 0.00099419 56.533 62.550 0.0012364 62.550 69.594 0.0011934 69.594 77.099 0.0013868 77.099 85.908 0.0014323 85.908 95.218 0.0017724 95.218 106.16 0.0016729 106.16 117.58 0.0020291 117.58 131.00 0.0023799 131.00 146.93 0.0020733 146.93 163.44 0.0024593 163.44 183.00 0.0022345 183.00 202.82 0.0025606 202.82 226.17 0.0023545 226.17 254.00 0.0018522 254.00 281.52 0.0015635 281.52 314.04 0.00082942 314.04 352.91 0.00025440 \END; /* Data (Fig.18, p419 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '289' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,46; RCT=12C(ALPHA,T)X; THK-TGT=8850MG/CM**2; DET-PARTCL=T; \\DATA,46; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'290',<1%'291',<1%'292'); /* '290' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '291' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '292' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'293'; /* '293' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'294'; /* '294' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'295' (MEV) (MEV) (1/SR/MEV/PARTCL) 45.368 50.487 0.00045631 50.487 56.030 0.00060009 56.030 61.964 0.00074373 61.964 68.905 0.00074621 68.905 76.295 0.00085386 76.295 84.960 0.00082714 84.960 94.109 0.00095863 94.109 104.85 0.00092580 104.85 116.06 0.0010889 116.06 129.20 0.0011047 129.20 144.78 0.00096319 144.78 160.91 0.0010127 160.91 179.99 0.00077004 179.99 199.29 0.00073335 199.29 222.00 0.00058225 222.00 249.00 0.00034456 249.00 275.65 0.00020403 275.65 307.08 6.1985e-05 \END; /* Data (Fig.18, p419 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '295' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,47; RCT=12C(ALPHA,T)X; THK-TGT=8850MG/CM**2; DET-PARTCL=T; \\DATA,47; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'296',<1%'297',<1%'298'); /* '296' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '297' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '298' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'299'; /* '299' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'300'; /* '300' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'301' (MEV) (MEV) (1/SR/MEV/PARTCL) 46.160 51.116 0.00017535 51.116 56.925 0.00032493 56.925 63.794 0.00031287 63.794 70.894 0.00037906 70.894 79.266 0.00031464 79.266 87.702 0.00036825 87.702 97.585 0.00036842 97.585 109.27 0.00036981 109.27 123.25 0.00028992 123.25 137.10 0.00031590 137.10 153.49 0.00025932 153.49 173.12 0.00016862 173.12 191.76 0.00015519 191.76 213.70 0.00011044 213.70 239.81 6.8606e-05 239.81 271.27 5.5794e-05 271.27 309.72 2.2601e-05 309.72 344.55 3.7113e-06 \END; /* Data (Fig.18, p419 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '301' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,48; RCT=12C(ALPHA,T)X; THK-TGT=8850MG/CM**2; DET-PARTCL=T; \\DATA,48; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'302',<1%'303',<1%'304'); /* '302' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '303' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '304' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'305'; /* '305' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'306'; /* '306' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'307' (MEV) (MEV) (1/SR/MEV/PARTCL) 49.162 54.729 2.3940e-05 54.729 60.834 2.6563e-05 60.834 67.478 2.6178e-05 67.478 74.641 2.1753e-05 74.641 83.027 1.9048e-05 83.027 92.042 1.6304e-05 92.042 102.64 1.0034e-05 102.64 113.98 8.6403e-06 113.98 127.36 4.5419e-06 127.36 141.57 3.6535e-06 141.57 158.38 1.8948e-06 158.38 176.05 1.3031e-06 176.05 196.97 3.9823e-07 196.97 218.61 2.4900e-07 \END; /* Data (Fig.18, p419 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '307' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,49; RCT=27AL(ALPHA,T)X; THK-TGT=10800MG/CM**2; DET-PARTCL=T; \\DATA,49; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'308',<1%'309',<1%'310'); /* '308' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '309' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '310' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'311'; /* '311' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'312'; /* '312' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'313' (MEV) (MEV) (1/SR/MEV/PARTCL) 41.308 45.733 2.7407e-05 45.733 50.916 0.00035440 50.916 56.533 0.00062702 56.533 62.550 0.00075626 62.550 69.594 0.00076461 69.594 77.099 0.00090753 77.099 85.908 0.00088579 85.908 95.218 0.0011136 95.218 106.16 0.0010467 106.16 117.58 0.0012882 117.58 131.00 0.0014756 131.00 146.93 0.0012901 146.93 163.44 0.0014597 163.44 183.00 0.0013094 183.00 202.82 0.0014487 202.82 226.17 0.0013321 226.17 254.00 0.0010531 254.00 281.52 0.00089355 281.52 314.04 0.00048445 314.04 352.91 0.00015005 \END; /* Data (Fig.19, p420 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '313' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,50; RCT=27AL(ALPHA,T)X; THK-TGT=10800MG/CM**2; DET-PARTCL=T; \\DATA,50; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'314',<1%'315',<1%'316'); /* '314' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '315' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '316' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'317'; /* '317' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'318'; /* '318' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'319' (MEV) (MEV) (1/SR/MEV/PARTCL) 40.995 45.368 5.5659e-05 45.368 50.487 0.00031878 50.487 56.030 0.00038158 56.030 61.964 0.00048450 61.964 68.905 0.00047768 68.905 76.295 0.00056037 76.295 84.960 0.00052170 84.960 94.109 0.00060256 94.109 104.85 0.00054050 104.85 116.06 0.00066337 116.06 129.20 0.00067458 129.20 144.78 0.00059924 144.78 160.91 0.00064053 160.91 179.99 0.00049567 179.99 199.29 0.00049101 199.29 222.00 0.00038983 222.00 249.00 0.00023929 249.00 275.65 0.00015050 275.65 307.08 4.6547e-05 \END; /* Data (Fig.19, p420 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '319' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,51; RCT=27AL(ALPHA,T)X; THK-TGT=10800MG/CM**2; DET-PARTCL=T; \\DATA,51; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'320',<1%'321',<1%'322'); /* '320' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '321' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '322' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'323'; /* '323' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'324'; /* '324' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN'325' ENGY-EMT-LAB-MAX DN/DOMEGA/DE'326' (MEV) (MEV) (1/SR/MEV/PARTCL) X 41.405 1.0880e-05 41.405 46.160 3.2860e-05 46.160 51.116 0.00011443 51.116 56.925 0.00021578 56.925 63.794 0.00019999 63.794 70.894 0.00023546 70.894 79.266 0.00020077 79.266 87.702 0.00023787 87.702 97.585 0.00024526 97.585 109.27 0.00023708 109.27 123.25 0.00019385 123.25 137.10 0.00021302 137.10 153.49 0.00018285 153.49 173.12 0.00011696 173.12 191.76 0.00011483 191.76 213.70 8.3208e-05 213.70 239.81 5.3701e-05 239.81 271.27 4.3593e-05 271.27 309.72 1.7832e-05 309.72 344.55 2.5741e-06 \END; /* Data (Fig.19, p420 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '325' Lower limit energy of lowest bin is missed by authors. */ /* '326' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,52; RCT=27AL(ALPHA,T)X; THK-TGT=10800MG/CM**2; DET-PARTCL=T; \\DATA,52; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'327',<1%'328',<1%'329'); /* '327' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '328' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '329' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'330'; /* '330' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'331'; /* '331' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'332' (MEV) (MEV) (1/SR/MEV/PARTCL) 44.409 49.162 1.2773e-05 49.162 54.729 4.1398e-05 54.729 60.834 4.8259e-05 60.834 67.478 4.8884e-05 67.478 74.641 4.7399e-05 74.641 83.027 3.9702e-05 83.027 92.042 3.7228e-05 92.042 102.64 2.8608e-05 102.64 113.98 2.2332e-05 113.98 127.36 1.4685e-05 127.36 141.57 1.0228e-05 141.57 158.38 4.8311e-06 158.38 176.05 3.0852e-06 176.05 196.97 1.2202e-06 196.97 218.61 8.0388e-07 \END; /* Data (Fig.19, p420 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '332' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,53; RCT=CU(ALPHA,T)X; THK-TGT=13395MG/CM**2; DET-PARTCL=T; \\DATA,53; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'333',<1%'334',<1%'335'); /* '333' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '334' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '335' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'336'; /* '336' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'337'; /* '337' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'338' (MEV) (MEV) (1/SR/MEV/PARTCL) 41.308 45.733 2.1998e-05 45.733 50.916 0.00024149 50.916 56.533 0.00039229 56.533 62.550 0.00046391 62.550 69.594 0.00045970 69.594 77.099 0.00055335 77.099 85.908 0.00054060 85.908 95.218 0.00064778 95.218 106.16 0.00061994 106.16 117.58 0.00073040 117.58 131.00 0.00085023 131.00 146.93 0.00074279 146.93 163.44 0.00085120 163.44 183.00 0.00076469 183.00 202.82 0.00082600 202.82 226.17 0.00073349 226.17 254.00 0.00054877 254.00 281.52 0.00045236 281.52 314.04 0.00023571 314.04 352.91 7.6012e-05 \END; /* Data (Fig.20, p421 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '338' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,54; RCT=CU(ALPHA,T)X; THK-TGT=13395MG/CM**2; DET-PARTCL=T; \\DATA,54; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'339',<1%'340',<1%'341'); /* '339' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '340' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '341' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'342'; /* '342' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'343'; /* '343' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'344' (MEV) (MEV) (1/SR/MEV/PARTCL) 40.995 45.368 4.7118e-05 45.368 50.487 0.00019796 50.487 56.030 0.00023965 56.030 61.964 0.00031394 61.964 68.905 0.00029913 68.905 76.295 0.00034808 76.295 84.960 0.00032484 84.960 94.109 0.00037164 94.109 104.85 0.00033435 104.85 116.06 0.00038567 116.06 129.20 0.00040271 129.20 144.78 0.00035153 144.78 160.91 0.00036349 160.91 179.99 0.00028710 179.99 199.29 0.00028347 199.29 222.00 0.00023382 222.00 249.00 0.00014645 249.00 275.65 8.8285e-05 275.65 307.08 2.6709e-05 \END; /* Data (Fig.20, p421 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '344' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,55; RCT=CU(ALPHA,T)X; THK-TGT=13395MG/CM**2; DET-PARTCL=T; \\DATA,55; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'345',<1%'346',<1%'347'); /* '345' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '346' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '347' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'348'; /* '348' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'349'; /* '349' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'350' (MEV) (MEV) (1/SR/MEV/PARTCL) 37.354 41.405 7.1405e-06 41.405 46.160 2.0536e-05 46.160 51.116 7.8884e-05 51.116 56.925 0.00012369 56.925 63.794 0.00011079 63.794 70.894 0.00013533 70.894 79.266 0.00011202 79.266 87.702 0.00012842 87.702 97.585 0.00013238 97.585 109.27 0.00012956 109.27 123.25 0.00010672 123.25 137.10 0.00012047 137.10 153.49 0.00010572 153.49 173.12 6.8498e-05 173.12 191.76 6.5794e-05 191.76 213.70 4.9953e-05 213.70 239.81 3.3162e-05 239.81 271.27 2.4345e-05 271.27 309.72 1.0042e-05 309.72 344.55 1.9618e-06 \END; /* Data (Fig.20, p421 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '350' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,56; RCT=CU(ALPHA,T)X; THK-TGT=13395MG/CM**2; DET-PARTCL=T; \\DATA,56; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'351',<1%'352',<1%'353'); /* '351' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '352' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '353' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'354'; /* '354' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'355'; /* '355' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'356' (MEV) (MEV) (1/SR/MEV/PARTCL) 44.409 49.162 5.2922e-06 49.162 54.729 1.7923e-05 54.729 60.834 1.9295e-05 60.834 67.478 2.0695e-05 67.478 74.641 1.9666e-05 74.641 83.027 1.4698e-05 83.027 92.042 1.3252e-05 92.042 102.64 1.1631e-05 102.64 113.98 8.6867e-06 113.98 127.36 5.8607e-06 127.36 141.57 5.0430e-06 141.57 158.38 2.6189e-06 158.38 176.05 1.4471e-06 176.05 196.97 7.0152e-07 196.97 218.61 2.1305e-07 \END; /* Data (Fig.20, p421 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '356' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,57; RCT=PB(ALPHA,T)X; THK-TGT=17010MG/CM**2; DET-PARTCL=T; \\DATA,57; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'357',<1%'358',<1%'359'); /* '357' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '358' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '359' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'360'; /* '360' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=0DEG; DELTA-DN/DOMEGA/DE=<4%'361'; /* '361' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'362' (MEV) (MEV) (1/SR/MEV/PARTCL) 41.308 45.733 9.8714e-06 45.733 50.916 0.00010559 50.916 56.533 0.00017808 56.533 62.550 0.00021318 62.550 69.594 0.00021740 69.594 77.099 0.00025012 77.099 85.908 0.00025469 85.908 95.218 0.00030563 95.218 106.16 0.00029308 106.16 117.58 0.00035265 117.58 131.00 0.00041593 131.00 146.93 0.00035953 146.93 163.44 0.00042964 163.44 183.00 0.00039300 183.00 202.82 0.00041128 202.82 226.17 0.00036721 226.17 254.00 0.00029332 254.00 281.52 0.00023142 281.52 314.04 0.00012621 314.04 352.91 4.2998e-05 \END; /* Data (Fig.21, p421 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '362' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,58; RCT=PB(ALPHA,T)X; THK-TGT=17010MG/CM**2; DET-PARTCL=T; \\DATA,58; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'363',<1%'364',<1%'365'); /* '363' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '364' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '365' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'366'; /* '366' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=7.5DEG; DELTA-DN/DOMEGA/DE=<4%'367'; /* '367' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'368' (MEV) (MEV) (1/SR/MEV/PARTCL) 40.995 45.368 2.4828e-05 45.368 50.487 0.00010653 50.487 56.030 0.00012027 56.030 61.964 0.00016454 61.964 68.905 0.00015896 68.905 76.295 0.00018806 76.295 84.960 0.00017921 84.960 94.109 0.00020024 94.109 104.85 0.00019385 104.85 116.06 0.00022854 116.06 129.20 0.00023871 129.20 144.78 0.00020369 144.78 160.91 0.00022407 160.91 179.99 0.00016917 179.99 199.29 0.00017804 199.29 222.00 0.00015329 222.00 249.00 9.6394e-05 249.00 275.65 6.3065e-05 275.65 307.08 1.9581e-05 \END; /* Data (Fig.21, p421 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '368' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,59; RCT=PB(ALPHA,T)X; THK-TGT=17010MG/CM**2; DET-PARTCL=T; \\DATA,59; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'369',<1%'370',<1%'371'); /* '369' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '370' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '371' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'372'; /* '372' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=15DEG; DELTA-DN/DOMEGA/DE=<4%'373'; /* '373' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'374' (MEV) (MEV) (1/SR/MEV/PARTCL) 37.354 41.405 4.0876e-06 41.405 46.160 1.3507e-05 46.160 51.116 4.5145e-05 51.116 56.925 7.0061e-05 56.925 63.794 6.6619e-05 63.794 70.894 7.9316e-05 70.894 79.266 6.6208e-05 79.266 87.702 7.3162e-05 87.702 97.585 7.2982e-05 97.585 109.27 7.3705e-05 109.27 123.25 6.0524e-05 123.25 137.10 6.5512e-05 137.10 153.49 5.8937e-05 153.49 173.12 4.2046e-05 173.12 191.76 4.2342e-05 191.76 213.70 3.2176e-05 213.70 239.81 2.3286e-05 239.81 271.27 1.6298e-05 271.27 309.72 6.9966e-06 309.72 344.55 1.3493e-06 \END; /* Data (Fig.21, p421 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '374' Thick Target energy spectrum [n /sr /MeV /particle] */ \\EXP,60; RCT=PB(ALPHA,T)X; THK-TGT=17010MG/CM**2; DET-PARTCL=T; \\DATA,60; INC-ENGY-LAB=100MEV/A; SYS-ERR=(<3%'375',<1%'376',<1%'377'); /* '375' Uncertainty in the number of accepted beam particles incident on the target is estimated to be less than 3%. */ /* '376' Uncertainty in the solid angle for the thickest carbon target, which has the maximum uncertainty, is less than 1%. */ /* '377' Uncertainty of charged particle detection efficiency is estimated to be 1%, considering a small fraction of the slant incidence of a particle onto the detector. */ STATIST-ERR=X%'378'; /* '378' The statistical uncertainties vary from 2-5% in the low to medium energy (5-50 MeV) region of the spectra and increase to about 30% at the highest energies. */ EMT=T; THTL=30DEG; DELTA-DN/DOMEGA/DE=<4%'379'; /* '379' Total normalization uncertainty */ \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'380' (MEV) (MEV) (1/SR/MEV/PARTCL) 44.117 48.821 3.8367e-06 48.821 54.328 1.3692e-05 54.328 60.364 1.7276e-05 60.364 66.929 1.4481e-05 66.929 74.001 1.5653e-05 74.001 82.275 1.2750e-05 82.275 91.163 1.3358e-05 91.163 101.60 9.8369e-06 101.60 112.76 8.9118e-06 112.76 125.91 6.2823e-06 125.91 139.88 4.8551e-06 139.88 156.37 2.6026e-06 156.37 173.68 1.9225e-06 173.68 194.15 8.0343e-07 \END; /* Data (Fig.21, p421 in reference) received by e-mail from T. Kurosawa by e-mail (2004.02.05) */ /* '380' Thick Target energy spectrum [n /sr /MeV /particle] */ \\END;