ENTRY 23194 20130511 22352319400000001 SUBENT 23194001 20130511 22352319400100001 BIB 16 135 2319400100002 TITLE The Zr-93(n,gamma) reaction up to 8 keV neutron energy2319400100003 REFERENCE (J,PR/C,87,014622,2013) 2319400100004 #doi:10.1103/PhysRevC.87.014622 2319400100005 Main reference. 2319400100006 AUTHOR (G.Tagliente,P.M.Milazzo, K.Fujii,U.Abbondanno,G.Aerts,2319400100007 H.Alvarez, F.Alvarez-Velarde, S.Andriamonje, 2319400100008 J.Andrzejewski,L.Audouin,G.Badurek, P.Baumann,F.Becvar,2319400100009 F.Belloni, E.Berthoumieux, F.Calvino, M.Calviani, 2319400100010 D.Cano-Ott,R.Capote, C.Carrappico, P.Cennini, V.Chepel,2319400100011 E.Chiaveri, N.Colonna, G.Cortes, A.Couture, M.Dahlfors,2319400100012 S.David, I.Dillmann, C.Domingo-Pardo, W.Dridi, I.Duran,2319400100013 C.Eleftheriadis, M.Embid-Segura, A.Ferrari, 2319400100014 R.Ferreira-Marques, W.Furman, I.Goncalves, 2319400100015 E.Gonzalez-Romero, F.Gramegna, C.Guerrero, F.Gunsing, 2319400100016 B.Haas, R.Haight, M.Heil,A.Herrera-Martinez, E.Jericha,2319400100017 F.Kaeppeler, Y.Kadi,D.Karadimos,D.Karamanis, M.Kerveno,2319400100018 E.Kossionides, M.Krticka,C.Lamboudis, H.Leeb,A.Lindote,2319400100019 I.Lopes, S.Lukic, J.Marganiec, S.Marrone, T.Martinez, 2319400100020 C.Massimi, P.Mastinu, A.Mengoni, C.Moreau, M.Mosconi, 2319400100021 F.Neves, H.Oberhummer, S.O'Brien, C.Papachristodoulou, 2319400100022 C.Papadopoulos, C.Paradela, N.Patronis, A.Pavlik, 2319400100023 P.Pavlopoulos, L.Perrot, M.T.Pigni, R.Plag, A.Plompen, 2319400100024 A.Plukis,A.Poch,J.Praena,C.Pretel,J.Quesada,R.Reifarth,2319400100025 M.Rosetti, C.Rubbia, G.Rudolf, P.Rullhusen, J.Salgado, 2319400100026 C.Santos,L.Sarchiapone,I.Savvidis, C.Stephan, J.L.Tain,2319400100027 L.Tassan-Got, L.Tavora, R.Terlizzi, G.Vannini, P.Vaz, 2319400100028 A.Ventura, D.Villamarin, M.C.Vincente, V.Vlachoudis, 2319400100029 R.Vlastou, F.Voss, S.Walter, M.Wiescher, K.Wisshak) 2319400100030 INSTITUTE (2ZZZNTF) n TOF collaboration. 2319400100031 (2ZZZCER) P.Cennini,E.Chiaveri,M.Dahlfors,A.Ferrari, 2319400100032 A.Herrera-Martinez,Y.Kadi,L.Sarchiapone,V.Vlachoudis. 2319400100033 (2ZZZGEL) A.Plompen,P.Rullhusen. 2319400100034 (2ITYBAU) G.Tagliente,N.Colonna,S.Marrone,R.Terlizzi. 2319400100035 (2ITYTRI) P.M.Milazzo,K.Fujii,U.Abbondanno,F.Belloni, 2319400100036 C.Moreau. 2319400100037 (2FR SAC) G.Aerts,S.Andriamonje,E.Berthoumieux,W.Dridi,2319400100038 F.Gunsing,L.Perrot, A.Plukis. 2319400100039 (2SPNSAU) H.Alvarez,I.Duran,C.Paradela, 2319400100040 (2SPNPCM) F.Alvarez-Velarde,D.Cano-Ott,M.Embid-Segura, 2319400100041 E.Gonzalez-Romero,C.Guerrero,T.Martinez,D.Villamarin, 2319400100042 M.C.Vincente. 2319400100043 (3POLLOU) J.Andrzejewski,J.Marganiec, 2319400100044 (2GERKFK) L.Audouin,I.Dillmann,M.Heil,F.Kaeppeler, 2319400100045 M.Mosconi,R.Plag,F.Voss,S.Walter,K.Wisshak. 2319400100046 (2AUSATI) G.Badurek,E.Jericha,H.Leeb,H.Oberhummer, 2319400100047 M.T.Pigni. 2319400100048 (2FR STR) P.Baumann,S.David,M.Kerveno,S.Lukic,G.Rudolf.2319400100049 (3CZRCHU) F.Becvar,M.Krticka. 2319400100050 (2SPNUPC) F.Calvino,G.Cortes,A.Poch,C.Pretel. 2319400100051 (2ITYPAD) M.Calviani,F.Gramegna,P.Mastinu,J.Praena. 2319400100052 (3ZZZIAE) R.Capote,A.Mengoni. 2319400100053 (2SPNSEU) R.Capote,J.Quesada. 2319400100054 (2PRTLFE) C.Carrappico,I.Goncalves,J.Salgado,C.Santos, 2319400100055 L.Tavora,P.Vaz. 2319400100056 (2PRTPRT) LIP - Coimbra and Departamento de Fisica da 2319400100057 Universidade de Coimbra, Portugal. 2319400100058 V.Chepel,R.Ferreira-Marques,A.Lindote,I.Lopes,F.Neves. 2319400100059 (1USANOT) A.Couture,S.O'Brien,M.Wiescher. 2319400100060 (2GERGSI) I.Dillmann,C.Domingo-Pardo,M.Heil, 2319400100061 J.Marganiec,R.Plag,R.Reifarth. 2319400100062 (2SPNVAL) C.Domingo-Pardo,J.L.Tain. 2319400100063 (2GRCARU) C.Eleftheriadis,C.Lamboudis,I.Savvidis. 2319400100064 (4ZZZDUB) W.Furman. 2319400100065 (2FR GRA) B.Haas. 2319400100066 (1USALAS) R.Haight,R.Reifarth. 2319400100067 (2GRCIOA) D.Karadimos,D.Karamanis,C.Papachristodoulou, 2319400100068 N.Patronis. 2319400100069 (2GRCATH) E.Kossionides. 2319400100070 (2ITYUBO) C.Massimi,G.Vannini. 2319400100071 (2GERPTB) M.Mosconi. 2319400100072 (2GRCTUA) C.Papadopoulos,R.Vlastou. 2319400100073 (2AUSVIE) A.Pavlik. 2319400100074 (2FR FR ) Pole Universitaire Leonard de Vinci, 2319400100075 Paris La Defense, Paris, France . 2319400100076 P.Pavlopoulos. 2319400100077 (2ITYBOL) M.Rosetti,A.Ventura. 2319400100078 (2ITYPAV) C.Rubbia. 2319400100079 (2FR PAR) C.Stephan,L.Tassan-Got. 2319400100080 REL-REF (I,,C.Borcea+,J,NIM/A,513,(3),524,2003) 2319400100081 Facility details . 2319400100082 (M,,U.Abbondanno+,J,NIM/A,521,454,2004) 2319400100083 PHWT - pulse height weighting technique. 2319400100084 FACILITY (SYNCY,2ZZZCER) 20-GeV/c proton synchro-cyclotron, 2319400100085 n-TOF facility, CERN. Pulsed proton beam of high 2319400100086 intensity of 7.E+12 protons per bunch. 2319400100087 INC-SOURCE (SPALL) Spallation reaction of fast protons on the 2319400100088 massive lead target moderated in a surrounding 2319400100089 5.8 cm thick water cooling layer surrounding the lead2319400100090 target.Pulse width 6 ns. 2319400100091 INC-SPECT Neutron flux 10**5 neutrons/cm2/pulse at the sample 2319400100092 position). Resolution in neutron energy is better than 2319400100093 0.1% in the range of the present measurement, i.e. 2319400100094 below 8 keV. Nearly symmetrical Gaussian-shaped beam 2319400100095 profile at the sample position. 2319400100096 The neutron flux was determined relative to the 2319400100097 235U(n,f) cross section by means of calibrated fission 2319400100098 chamber from PTB Braunschweig. During the measurement 2319400100099 the flux was checked online by a low-mass 6Li neutron 2319400100100 monitor. 2319400100101 METHOD (TOF) Flight path 187.5 m from spallation target to 2319400100102 sample position. 2319400100103 PART-DET (G) Prompt gamma-ray cascade following neutron capture.2319400100104 DETECTOR (SCIN) Two C6-D6 liquid scintillator cells as gamma 2319400100105 detectors placed perpendicular to neutron beam at a 2319400100106 distance of about 3 cm from beam axis and 9.2 cm 2319400100107 backward from the sample position. Directly coupled 2319400100108 to EMI-9823QKB photomultiplier tubes. The light output 2319400100109 of the detectors was calibrated at 662, 1173, 1332 keV 2319400100110 by means of 137Cs and 60Co reference sources. An 2319400100111 additional calibration point at 6.13 MeV was obtained 2319400100112 by means of a composite 238Pu/13C source. 2319400100113 (FISCH,IOCH) U-235 loaded parallel-plate fission 2319400100114 chamber from PTB Braunschweig - for neutron flux 2319400100115 measurement as well as Li-6 neutron flux monitors. 2319400100116 MONITOR (92-U-235(N,F),,SIG) For the neutron flux. 2319400100117 SAMPLE Zr-O2 oxide powder pressed to pellet of 22 mm diameter,2319400100118 thickness 3.5mm, mass 4.46 g, encapsulated twice in 2319400100119 inner Al and a welded outer Ti container, both with 2319400100120 0.2 mm thick walls. 93Zr activity was 62.6 MBq. 2319400100121 Isotope composition: 2319400100122 Zr-90 - 2.29%, Zr-91 - 18.61%, Zr-92 - 18.95%, 2319400100123 Zr-93 - 19.98, Zr-94 - 20.50%, Zr-96 - 19.67%. 2319400100124 Traces of Mo and S were also present in the sample - 2319400100125 below 0.01 %, the contribution of these impurities to 2319400100126 the measured capture yield was not negligible. 2319400100127 Au and Pb samples of the same diameter were used for 2319400100128 repeated neutron flux measurements and background runs.2319400100129 ANALYSIS The intrinsic efficiency of C6D6 detectors was modified2319400100130 by the pulse height weighting technique (PHWT). 2319400100131 CORRECTION For the stable zirconium isotopes, sample impurities, 2319400100132 and the various backgrounds. 2319400100133 For the energy resolution of the neutron beam, for the 2319400100134 Doppler broadening of cross-section line shapes, for 2319400100135 self-shielding and neutron multiple scattering. 2319400100136 HISTORY (20101014C) M.M. 2319400100137 ENDBIB 135 0 2319400100138 NOCOMMON 0 0 2319400100139 ENDSUBENT 138 0 2319400199999 SUBENT 23194002 20130511 22352319400200001 BIB 6 21 2319400200002 REACTION 1(40-ZR-93(N,0),,EN) Resonance energy. 2319400200003 2(40-ZR-93(N,G),,WID/STR) Capture kernel. 2319400200004 ANALYSIS The capture yield has been investigated by means of an 2319400200005 R-matrix analysis, using SAMMY code in the Reich-Moore 2319400200006 approximation to extract individual resonance 2319400200007 parameters. 2319400200008 REL-REF (M,,N.M.Larson,R,ORNL-TM-9179/R7,2006) 2319400200009 Updated Users Guide for SAMMY: Multilevel R-matrix fits2319400200010 to neutron data using Bayes equations, Report 2319400200011 ORNL/TM-9179/R7. 2319400200012 FLAG (1.) Parameters for resonances with poor resolution. 2319400200013 ERR-ANALYS (ERR-S) Statistical uncertainty about 5.% . 2319400200014 (ERR-1,,2.) Systematic uncertainties introduced by PHWT2319400200015 data analysis procedure are lower than 2%. 2319400200016 (ERR-2) Uncertainty due to the energy dependence of the2319400200017 neutron flux and to the fraction of the neutron beam 2319400200018 covered by the sample; determined by applying the 2319400200019 saturated resonance technique, using 0.1 mm thick Au 2319400200020 sample, to the saturated resonance at 4.9 eV in 197Au. 2319400200021 (DATA-ERR) Not specified. 2319400200022 STATUS (TABLE) Table II of J,PR/C,87,014622,2013 . 2319400200023 ENDBIB 21 0 2319400200024 COMMON 2 3 2319400200025 ERR-2 ERR-S 2319400200026 PER-CENT PER-CENT 2319400200027 2. 5. 2319400200028 ENDCOMMON 3 0 2319400200029 DATA 5 64 2319400200030 DATA 1DATA-ERR 1DATA 2DATA-ERR 2FLAG 2319400200031 EV EV MILLI-EV MILLI-EV NO-DIM 2319400200032 110.383 0.002 37.16 0.08 2319400200033 225.035 0.004 6.64 0.05 2319400200034 669.096 0.009 25.2 0.3 2319400200035 693.27 0.01 50.0 0.4 2319400200036 882.11 0.03 3.9 0.1 2319400200037 934.34 0.01 43.7 0.5 2319400200038 1010.72 0.01 30.5 0.4 2319400200039 1237.89 0.04 7.5 0.2 2319400200040 1497.9 0.1 3.2 0.6 2319400200041 1574.72 0.04 28.9 0.7 2319400200042 1642.21 0.04 24. 1. 2319400200043 1708.5 0.1 6.4 0.7 2319400200044 1743.16 0.03 40. 1. 2319400200045 1802.42 0.03 41.4 0.8 2319400200046 2053.29 0.05 42. 1. 2319400200047 2116.32 0.08 10.9 0.5 2319400200048 2209.3 0.1 7.1 0.5 2319400200049 2320.18 0.06 44. 2. 2319400200050 2358.8 0.1 19. 1. 2319400200051 2404.0 0.1 7.0 0.5 2319400200052 2610.75 0.06 35. 2. 2319400200053 2767.4 0.4 94. 8. 2319400200054 2898.52 0.06 54. 3. 2319400200055 3008.7 0.1 69. 2. 2319400200056 3162.0 0.5 79. 9. 2319400200057 3251.43 0.07 90. 2. 2319400200058 3511.4 0.2 48. 2. 2319400200059 3690.0 0.1 43. 2. 2319400200060 3698.5 0.2 46. 2. 2319400200061 3872.3 0.2 61. 5. 2319400200062 3996.1 0.2 55. 3. 2319400200063 4093.5 0.5 11. 2. 2319400200064 4130. 1. 59. 9. 2319400200065 4156.0 0.2 44. 4. 2319400200066 4180.5 0.2 85. 4. 2319400200067 4288.2 0.4 15. 3. 2319400200068 4432.3 0.2 30. 2. 2319400200069 4483.8 0.2 64. 4. 2319400200070 4577.3 0.2 54. 3. 2319400200071 4779.7 0.2 26. 2. 2319400200072 5010.70 0.02 106. 4. 2319400200073 5027.7 0.3 48. 3. 2319400200074 5133.6 0.3 51. 3. 2319400200075 5539.2 0.3 41. 12. 2319400200076 5674.7 0.6 31. 3. 2319400200077 5738.1 0.4 37. 13. 2319400200078 5900.1 0.6 26. 10. 2319400200079 5923. 1. 25. 8. 2319400200080 6109.3 0.5 24. 8. 2319400200081 6148.0 0.4 58. 4. 2319400200082 6207.4 0.5 36. 3. 2319400200083 6339.0 0.3 75. 4. 2319400200084 6376.4 0.4 39. 3. 2319400200085 6620. 1. 14. 3. 1. 2319400200086 6766.5 0.4 79. 7. 2319400200087 6822. 2.2 15. 12. 1. 2319400200088 6977.1 0.2 31. 23. 1. 2319400200089 7073.3 0.3 23. 18. 1. 2319400200090 7168.8 0.5 102. 6. 2319400200091 7407.1 0.6 45. 4. 2319400200092 7587.0 0.5 53. 17. 2319400200093 7772. 2. 41. 14. 2319400200094 7893.1 0.6 50. 5. 2319400200095 7945. 1. 141. 9. 2319400200096 ENDDATA 66 0 2319400200097 ENDSUBENT 96 0 2319400299999 SUBENT 23194003 20130511 22352319400300001 BIB 5 21 2319400300002 REACTION 1(40-ZR-90(N,0),,EN) Resonance energy. 2319400300003 2(40-ZR-90(N,G),,WID/STR) Capture kernel. 2319400300004 ANALYSIS The capture yield has been investigated by means of an 2319400300005 R-matrix analysis, using SAMMY code in the Reich-Moore 2319400300006 approximation to extract individual resonance 2319400300007 parameters. 2319400300008 REL-REF (M,,N.M.Larson,R,ORNL-TM-9179/R7,2006) 2319400300009 Updated Users Guide for SAMMY: Multilevel R-matrix fits2319400300010 to neutron data using Bayes equations, Report 2319400300011 ORNL/TM-9179/R7. 2319400300012 (A,22978010,G.Tagliente+,J,PR/C,77,035802,2008) 2319400300013 ERR-ANALYS (ERR-S) Statistical uncertainty about 5.% . 2319400300014 (ERR-1,,2.) Systematic uncertainties introduced by PHWT2319400300015 data analysis procedure are lower than 2%. 2319400300016 (ERR-2) Uncertainty due to the energy dependence of the2319400300017 neutron flux and to the fraction of the neutron beam 2319400300018 covered by the sample; determined by applying the 2319400300019 saturated resonance technique, using 0.1 mm thick Au 2319400300020 sample, to the saturated resonance at 4.9 eV in 197Au. 2319400300021 (DATA-ERR) Not specified. 2319400300022 STATUS (TABLE) Table III of J,PR/C,87,014622,2013 . 2319400300023 ENDBIB 21 0 2319400300024 COMMON 2 3 2319400300025 ERR-2 ERR-S 2319400300026 PER-CENT PER-CENT 2319400300027 2. 5. 2319400300028 ENDCOMMON 3 0 2319400300029 DATA 3 2 2319400300030 DATA 1DATA 2DATA-ERR 2 2319400300031 EV MILLI-EV MILLI-EV 2319400300032 3861. 79. 8. 2319400300033 4008. 123. 10. 2319400300034 ENDDATA 4 0 2319400300035 ENDSUBENT 34 0 2319400399999 SUBENT 23194004 20130511 22352319400400001 BIB 5 21 2319400400002 REACTION 1(40-ZR-91(N,0),,EN) Resonance energy. 2319400400003 2(40-ZR-91(N,G),,WID/STR) Capture kernel. 2319400400004 ANALYSIS The capture yield has been investigated by means of an 2319400400005 R-matrix analysis, using SAMMY code in the Reich-Moore 2319400400006 approximation to extract individual resonance 2319400400007 parameters. 2319400400008 REL-REF (M,,N.M.Larson,R,ORNL-TM-9179/R7,2006) 2319400400009 Updated Users Guide for SAMMY: Multilevel R-matrix fits2319400400010 to neutron data using Bayes equations, Report 2319400400011 ORNL/TM-9179/R7. 2319400400012 (A,23044002,G.Tagliente+,J,PR/C,78,045804,2008) 2319400400013 ERR-ANALYS (ERR-S) Statistical uncertainty about 5.% . 2319400400014 (ERR-1,,2.) Systematic uncertainties introduced by PHWT2319400400015 data analysis procedure are lower than 2%. 2319400400016 (ERR-2) Uncertainty due to the energy dependence of the2319400400017 neutron flux and to the fraction of the neutron beam 2319400400018 covered by the sample; determined by applying the 2319400400019 saturated resonance technique, using 0.1 mm thick Au 2319400400020 sample, to the saturated resonance at 4.9 eV in 197Au. 2319400400021 (DATA-ERR) Not specified. 2319400400022 STATUS (TABLE) Table III of J,PR/C,87,014622,2013 . 2319400400023 ENDBIB 21 0 2319400400024 COMMON 2 3 2319400400025 ERR-2 ERR-S 2319400400026 PER-CENT PER-CENT 2319400400027 2. 5. 2319400400028 ENDCOMMON 3 0 2319400400029 DATA 3 5 2319400400030 DATA 1DATA 2DATA-ERR 2 2319400400031 EV MILLI-EV MILLI-EV 2319400400032 159.5 0.10 0.01 2319400400033 182.0 5.0 0.3 2319400400034 240.4 1.73 0.12 2319400400035 292.7 58. 2. 2319400400036 449.8 2.0 0.1 2319400400037 ENDDATA 7 0 2319400400038 ENDSUBENT 37 0 2319400499999 SUBENT 23194005 20130511 22352319400500001 BIB 5 21 2319400500002 REACTION 1(40-ZR-92(N,0),,EN) Resonance energy. 2319400500003 2(40-ZR-92(N,G),,WID/STR) Capture kernel. 2319400500004 ANALYSIS The capture yield has been investigated by means of an 2319400500005 R-matrix analysis, using SAMMY code in the Reich-Moore 2319400500006 approximation to extract individual resonance 2319400500007 parameters. 2319400500008 REL-REF (M,,N.M.Larson,R,ORNL-TM-9179/R7,2006) 2319400500009 Updated Users Guide for SAMMY: Multilevel R-matrix fits2319400500010 to neutron data using Bayes equations, Report 2319400500011 ORNL/TM-9179/R7. 2319400500012 (A,23117002,G.Tagliente+,J,PR/C,81,055801,2010) 2319400500013 ERR-ANALYS (ERR-S) Statistical uncertainty about 5.% . 2319400500014 (ERR-1,,2.) Systematic uncertainties introduced by PHWT2319400500015 data analysis procedure are lower than 2%. 2319400500016 (ERR-2) Uncertainty due to the energy dependence of the2319400500017 neutron flux and to the fraction of the neutron beam 2319400500018 covered by the sample; determined by applying the 2319400500019 saturated resonance technique, using 0.1 mm thick Au 2319400500020 sample, to the saturated resonance at 4.9 eV in 197Au. 2319400500021 (DATA-ERR) Not specified. 2319400500022 STATUS (TABLE) Table III of J,PR/C,87,014622,2013 . 2319400500023 ENDBIB 21 0 2319400500024 COMMON 2 3 2319400500025 ERR-2 ERR-S 2319400500026 PER-CENT PER-CENT 2319400500027 2. 5. 2319400500028 ENDCOMMON 3 0 2319400500029 DATA 3 4 2319400500030 DATA 1DATA 2DATA-ERR 2 2319400500031 EV MILLI-EV MILLI-EV 2319400500032 2013. 44. 3. 2319400500033 2689. 121. 6. 2319400500034 4640. 106. 9. 2319400500035 5046. 145. 9. 2319400500036 ENDDATA 6 0 2319400500037 ENDSUBENT 36 0 2319400599999 SUBENT 23194006 20130511 22352319400600001 BIB 5 21 2319400600002 REACTION 1(40-ZR-94(N,0),,EN) Resonance energy. 2319400600003 2(40-ZR-94(N,G),,WID/STR) Capture kernel. 2319400600004 ANALYSIS The capture yield has been investigated by means of an 2319400600005 R-matrix analysis, using SAMMY code in the Reich-Moore 2319400600006 approximation to extract individual resonance 2319400600007 parameters. 2319400600008 REL-REF (M,,N.M.Larson,R,ORNL-TM-9179/R7,2006) 2319400600009 Updated Users Guide for SAMMY: Multilevel R-matrix fits2319400600010 to neutron data using Bayes equations, Report 2319400600011 ORNL/TM-9179/R7. 2319400600012 (A,22978014,G.Tagliente+,J,PR/C,84,015801,2011) 2319400600013 ERR-ANALYS (ERR-S) Statistical uncertainty about 5.% . 2319400600014 (ERR-1,,2.) Systematic uncertainties introduced by PHWT2319400600015 data analysis procedure are lower than 2%. 2319400600016 (ERR-2) Uncertainty due to the energy dependence of the2319400600017 neutron flux and to the fraction of the neutron beam 2319400600018 covered by the sample; determined by applying the 2319400600019 saturated resonance technique, using 0.1 mm thick Au 2319400600020 sample, to the saturated resonance at 4.9 eV in 197Au. 2319400600021 (DATA-ERR) Not specified. 2319400600022 STATUS (TABLE) Table III of J,PR/C,87,014622,2013 . 2319400600023 ENDBIB 21 0 2319400600024 COMMON 2 3 2319400600025 ERR-2 ERR-S 2319400600026 PER-CENT PER-CENT 2319400600027 2. 5. 2319400600028 ENDCOMMON 3 0 2319400600029 DATA 3 2 2319400600030 DATA 1DATA 2DATA-ERR 2 2319400600031 EV MILLI-EV MILLI-EV 2319400600032 2241. 68. 4. 2319400600033 4925. 126. 7. 2319400600034 ENDDATA 4 0 2319400600035 ENDSUBENT 34 0 2319400699999 SUBENT 23194007 20130511 22352319400700001 BIB 5 21 2319400700002 REACTION 1(40-ZR-96(N,0),,EN) Resonance energy. 2319400700003 2(40-ZR-96(N,G),,WID/STR) Capture kernel. 2319400700004 ANALYSIS The capture yield has been investigated by means of an 2319400700005 R-matrix analysis, using SAMMY code in the Reich-Moore 2319400700006 approximation to extract individual resonance 2319400700007 parameters. 2319400700008 REL-REF (M,,N.M.Larson,R,ORNL-TM-9179/R7,2006) 2319400700009 Updated Users Guide for SAMMY: Multilevel R-matrix fits2319400700010 to neutron data using Bayes equations, Report 2319400700011 ORNL/TM-9179/R7. 2319400700012 (A,22978017,G.Tagliente+,J,PR/C,84,055802,2011) 2319400700013 ERR-ANALYS (ERR-S) Statistical uncertainty about 5.% . 2319400700014 (ERR-1,,2.) Systematic uncertainties introduced by PHWT2319400700015 data analysis procedure are lower than 2%. 2319400700016 (ERR-2) Uncertainty due to the energy dependence of the2319400700017 neutron flux and to the fraction of the neutron beam 2319400700018 covered by the sample; determined by applying the 2319400700019 saturated resonance technique, using 0.1 mm thick Au 2319400700020 sample, to the saturated resonance at 4.9 eV in 197Au. 2319400700021 (DATA-ERR) Not specified. 2319400700022 STATUS (TABLE) Table III of J,PR/C,87,014622,2013 . 2319400700023 ENDBIB 21 0 2319400700024 COMMON 2 3 2319400700025 ERR-2 ERR-S 2319400700026 PER-CENT PER-CENT 2319400700027 2. 5. 2319400700028 ENDCOMMON 3 0 2319400700029 DATA 3 3 2319400700030 DATA 1DATA 2DATA-ERR 2 2319400700031 EV MILLI-EV MILLI-EV 2319400700032 301. 115. 3. 2319400700033 3821. 33. 3. 2319400700034 4135. 108. 30. 2319400700035 ENDDATA 5 0 2319400700036 ENDSUBENT 35 0 2319400799999 SUBENT 23194008 20130511 22352319400800001 BIB 4 6 2319400800002 REACTION (40-ZR-93(N,G)40-ZR-94,,SIG,,MXW/MSC) 2319400800003 MACS for energy range < 8 keV 2319400800004 ANALYSIS MACS were derived by folding capture c-s with 2319400800005 respective thermal neutron spectrum. 2319400800006 ERR-ANALYS (DATA-ERR) Not specified. 2319400800007 STATUS (TABLE) Table I of J,PR/C,87,014622,2013 . 2319400800008 ENDBIB 6 0 2319400800009 COMMON 1 3 2319400800010 EN-MAX 2319400800011 KEV 2319400800012 8. 2319400800013 ENDCOMMON 3 0 2319400800014 DATA 3 6 2319400800015 KT DATA DATA-ERR 2319400800016 KEV MB MB 2319400800017 5. 246. 12. 2319400800018 10. 95. 5. 2319400800019 15. 50. 3. 2319400800020 20. 30. 2. 2319400800021 25. 20. 1. 2319400800022 30. 15. 1. 2319400800023 ENDDATA 8 0 2319400800024 ENDSUBENT 23 0 2319400899999 SUBENT 23194009 20130511 22352319400900001 BIB 5 12 2319400900002 REACTION (40-ZR-93(N,G)40-ZR-94,,SIG,,MXW) MACS 2319400900003 ANALYSIS Results for restricted energy range were complemented2319400900004 for the neutron energy range above 8 keV with Zr-93 c-s2319400900005 from JENDL-4.0 library. 2319400900006 REL-REF (A,V0102163,Z.Y.Bao+,J,AND,76,70,2000) 2319400900007 Agree with recommended value of Z.Bao+ at 30 keV - 2319400900008 95+-10 mb . 2319400900009 ERR-ANALYS (DATA-ERR) Error includes: 2319400900010 (DATA-ERR1) Uncertainty of present data ( < 8 keV) - 5%2319400900011 (ERR-2) Uncertainty of evaluated data above 8 keV - 10%2319400900012 STATUS (TABLE) Table I of J,PR/C,87,014622,2013 . 2319400900013 (DEP,23194008) MACS for energy <8 keV. 2319400900014 ENDBIB 12 0 2319400900015 COMMON 2 3 2319400900016 DATA-ERR1 ERR-2 2319400900017 PER-CENT PER-CENT 2319400900018 5. 10. 2319400900019 ENDCOMMON 3 0 2319400900020 DATA 3 6 2319400900021 KT DATA DATA-ERR 2319400900022 KEV MB MB 2319400900023 5. 347. 19. 2319400900024 10. 215. 17. 2319400900025 15. 160. 14. 2319400900026 20. 129. 12. 2319400900027 25. 110. 10. 2319400900028 30. 96. 9. 2319400900029 ENDDATA 8 0 2319400900030 ENDSUBENT 29 0 2319400999999 ENDENTRY 9 0 2319499999999