ENTRY C0189 20220530 C213C018900000001 SUBENT C0189001 20220530 C213C018900100001 BIB 10 18 C018900100002 INSTITUTE (1CANUWO) C018900100003 REFERENCE (J,NIM/B,45,91,1990) C018900100004 AUTHOR (S.Y.Tong,W.N.Lennard,P.F.A.Alkemade,I.V.Mitchell) C018900100005 TITLE Absolute surface carbon coverage determination via the C018900100006 12C(3He,p)14N reaction C018900100007 FACILITY (VDG,1CANUWO) C018900100008 INC-SPECT Uncertainty in beam energy does not exceed 3 keV from C018900100009 calibrated using 27Al(p,gamma)28Si reaction. C018900100010 DETECTOR (SOLST) Silicon surface-barrier detector, collimated C018900100011 using Ta aperture. Thin aluminized Mylar filter C018900100012 mounted in front of detector to attenuate elastic C018900100013 scattering yield. C018900100014 CORRECTION Corrected for deadtime losses and finite target C018900100015 thickness C018900100016 STATUS (APRVD) Approved by W. N. Lennard, 20 Nov 1998. C018900100017 HISTORY (19981026C) C018900100018 (20220410A) OS. Data correction in sub.3, updated C018900100019 ERR-ANALYS and STATUS C018900100020 ENDBIB 18 0 C018900100021 COMMON 1 3 C018900100022 ANG-ERR C018900100023 ADEG C018900100024 1.2 C018900100025 ENDCOMMON 3 0 C018900100026 ENDSUBENT 25 0 C018900199999 SUBENT C0189002 20220530 C213C018900200001 BIB 5 13 C018900200002 REACTION (6-C-12(HE3,P)7-N-14,PAR,DA) C018900200003 For 1st 3 levels in 14N. C018900200004 SAMPLE Self-supporting carbon foil, 13 microg/cm2 thick. C018900200005 MONITOR (6-C-12(A,EL)6-C-12,,DA,,RTH) 4He backscattering. C018900200006 ERR-ANALYS (ERR-T) Contributions to overall uncertainty are C018900200007 estimated to be: C018900200008 (ERR-1) uncertainty in normalization at 1 MeV (3%) C018900200009 (ERR-2) counting statistics (0.8%), C018900200010 (ERR-3) current integration (0.5%), C018900200011 (ERR-4) deadtime corrections (1%), C018900200012 (ERR-5) uncertainty in detection angle (0.3%), C018900200013 (ERR-6) uncertainty in ion beam energy (0.8%). C018900200014 STATUS (TABLE) Text on p.92, Nucl.Instr.Meth.B45,91,1990 C018900200015 ENDBIB 13 0 C018900200016 COMMON 10 6 C018900200017 EN-NRM ANG-NRM MONIT MONIT-ERR ERR-1 ERR-2 C018900200018 ERR-3 ERR-4 ERR-5 ERR-6 C018900200019 MEV ADEG MB/SR MB/SR PER-CENT PER-CENT C018900200020 PER-CENT PER-CENT PER-CENT PER-CENT C018900200021 1.000 180. 7.09 0.24 3. 0.8 C018900200022 0.5 1. 0.3 0.8 C018900200023 ENDCOMMON 6 0 C018900200024 DATA 6 1 C018900200025 EN ANG E-LVL-MIN E-LVL-MAX DATA ERR-T C018900200026 MEV ADEG MEV MEV MB/SR MB/SR C018900200027 2.389 150. 0. 3.948 7.09 0.24 C018900200028 ENDDATA 3 0 C018900200029 ENDSUBENT 28 0 C018900299999 SUBENT C0189003 20220530 C213C018900300001 BIB 6 8 C018900300002 REACTION (6-C-12(HE3,P)7-N-14,PAR,DA) C018900300003 MONITOR (6-C-12(HE3,P)7-N-14,PAR,DA) C018900300004 For 1st 3 levels in 14N as given in this reference. C018900300005 SAMPLE Thin amorphous carbon film used, areal density about C018900300006 12 microg/cm2 mounted over a Si crystal. C018900300007 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C018900300008 STATUS (TABLE) Table 1, Nucl.Instr.Meth.B45,91,1990 C018900300009 HISTORY (20220410A) Level energy at 1 point corrected C018900300010 ENDBIB 8 0 C018900300011 COMMON 7 6 C018900300012 EN ANG-NRM E-LVL-NRM E-LVL-NRM E-LVL-NRM MONIT C018900300013 MONIT-ERR C018900300014 MEV ADEG MEV MEV MEV MB/SR C018900300015 MB/SR C018900300016 2.389 150. 0. 2.313 3.948 7.09 C018900300017 0.24 C018900300018 ENDCOMMON 6 0 C018900300019 DATA 4 37 C018900300020 E-LVL ANG DATA DATA-ERR C018900300021 MEV ADEG MB/SR PER-CENT C018900300022 0. 86. 1.85 5. C018900300023 0. 91. 1.85 5. C018900300024 0. 101. 1.85 5. C018900300025 0. 111. 1.74 5. C018900300026 0. 121. 1.63 5. C018900300027 0. 131. 1.50 5. C018900300028 0. 141. 1.30 5. C018900300029 0. 151. 1.06 5. C018900300030 2.313 86. 1.60 5. C018900300031 2.313 91. 1.81 5. C018900300032 2.313 101. 2.08 5. C018900300033 2.313 111. 2.59 5. C018900300034 2.313 121. 2.76 5. C018900300035 2.313 131. 2.83 5. C018900300036 2.313 141. 3.05 5. C018900300037 2.313 151. 3.06 5. C018900300038 3.948 86. 1.12 5. C018900300039 3.948 91. 1.30 5. C018900300040 3.948 101. 1.73 5. C018900300041 3.948 111. 2.06 5. C018900300042 3.948 121. 2.40 5. C018900300043 3.948 131. 2.57 5. C018900300044 3.948 141. 2.97 5. C018900300045 3.948 151. 2.94 5. C018900300046 4.915 91. 0.23 10. C018900300047 4.915 101. 0.24 10. C018900300048 4.915 111. 0.28 10. C018900300049 4.915 121. 0.33 10. C018900300050 4.915 131. 0.33 10. C018900300051 4.915 141. 0.38 10. C018900300052 4.915 151. 0.37 10. C018900300053 5.106 101. 1.10 8. C018900300054 5.106 111. 1.07 8. C018900300055 5.106 121. 1.18 8. C018900300056 5.106 131. 1.06 8. C018900300057 5.106 141. 0.96 8. C018900300058 5.106 151. 0.96 8. C018900300059 ENDDATA 39 0 C018900300060 ENDSUBENT 59 0 C018900399999 SUBENT C0189004 20220530 C213C018900400001 BIB 3 5 C018900400002 REACTION (6-C-12(HE3,P)7-N-14,PAR,DA) C018900400003 MONITOR (6-C-12(HE3,P)7-N-14,PAR,DA) C018900400004 For 1st 3 levels in 14N as given in this reference. C018900400005 STATUS (TABLE) Data downloaded from Sigmabase Web site; data C018900400006 taken from Table 2, Nucl.Instr.Meth.B45,91,1990 C018900400007 ENDBIB 5 0 C018900400008 COMMON 7 6 C018900400009 ANG ANG-NRM E-LVL-NRM E-LVL-NRM E-LVL-NRM MONIT C018900400010 MONIT-ERR C018900400011 ADEG ADEG MEV MEV MEV MB/SR C018900400012 MB/SR C018900400013 90. 150. 0. 2.313 3.948 7.09 C018900400014 0.24 C018900400015 ENDCOMMON 6 0 C018900400016 DATA 3 72 C018900400017 E-LVL EN DATA C018900400018 MEV KEV MB/SR C018900400019 0. 2100. 6.85E-01 C018900400020 0. 2110. 7.49E-01 C018900400021 0. 2121. 6.62E-01 C018900400022 0. 2130. 6.56E-01 C018900400023 0. 2140. 6.42E-01 C018900400024 0. 2150. 7.26E-01 C018900400025 0. 2160. 6.79E-01 C018900400026 0. 2170. 6.74E-01 C018900400027 0. 2180. 6.71E-01 C018900400028 0. 2189. 7.54E-01 C018900400029 0. 2209. 7.95E-01 C018900400030 0. 2229. 7.74E-01 C018900400031 0. 2249. 8.32E-01 C018900400032 0. 2269. 9.59E-01 C018900400033 0. 2289. 9.64E-01 C018900400034 0. 2309. 1.18E+00 C018900400035 0. 2329. 1.32E+00 C018900400036 0. 2348. 1.60E+00 C018900400037 0. 2358. 1.53E+00 C018900400038 0. 2368. 1.80E+00 C018900400039 0. 2389. 1.85E+00 C018900400040 0. 2399. 1.89E+00 C018900400041 0. 2409. 2.03E+00 C018900400042 0. 2419. 2.03E+00 C018900400043 2.313 2100. 6.37E-01 C018900400044 2.313 2110. 5.23E-01 C018900400045 2.313 2121. 6.15E-01 C018900400046 2.313 2130. 6.87E-01 C018900400047 2.313 2140. 6.37E-01 C018900400048 2.313 2150. 7.51E-01 C018900400049 2.313 2160. 7.04E-01 C018900400050 2.313 2170. 7.46E-01 C018900400051 2.313 2180. 7.68E-01 C018900400052 2.313 2189. 8.54E-01 C018900400053 2.313 2209. 8.10E-01 C018900400054 2.313 2229. 9.02E-01 C018900400055 2.313 2249. 1.04E+00 C018900400056 2.313 2269. 1.13E+00 C018900400057 2.313 2289. 1.18E+00 C018900400058 2.313 2309. 1.34E+00 C018900400059 2.313 2329. 1.39E+00 C018900400060 2.313 2348. 1.51E+00 C018900400061 2.313 2358. 1.65E+00 C018900400062 2.313 2368. 1.60E+00 C018900400063 2.313 2389. 1.77E+00 C018900400064 2.313 2399. 1.85E+00 C018900400065 2.313 2409. 1.84E+00 C018900400066 2.313 2419. 1.88E+00 C018900400067 3.948 2100. 3.61E-01 C018900400068 3.948 2110. 3.56E-01 C018900400069 3.948 2121. 4.02E-01 C018900400070 3.948 2130. 4.08E-01 C018900400071 3.948 2140. 4.04E-01 C018900400072 3.948 2150. 4.73E-01 C018900400073 3.948 2160. 4.32E-01 C018900400074 3.948 2170. 4.49E-01 C018900400075 3.948 2180. 4.38E-01 C018900400076 3.948 2189. 4.62E-01 C018900400077 3.948 2209. 5.88E-01 C018900400078 3.948 2229. 6.02E-01 C018900400079 3.948 2249. 6.29E-01 C018900400080 3.948 2269. 7.41E-01 C018900400081 3.948 2289. 8.29E-01 C018900400082 3.948 2309. 9.16E-01 C018900400083 3.948 2329. 9.63E-01 C018900400084 3.948 2348. 1.10E+00 C018900400085 3.948 2358. 1.07E+00 C018900400086 3.948 2368. 1.14E+00 C018900400087 3.948 2389. 1.25E+00 C018900400088 3.948 2399. 1.20E+00 C018900400089 3.948 2409. 1.35E+00 C018900400090 3.948 2419. 1.36E+00 C018900400091 ENDDATA 74 0 C018900400092 ENDSUBENT 91 0 C018900499999 ENDENTRY 4 0 C018999999999