ENTRY O2441 20200116 O075O244100000001 SUBENT O2441001 20200116 O075O244100100001 BIB 9 25 O244100100002 TITLE Measurement of 4He charge- and mass-changing cross O244100100003 sections on H, C, O, and Si targets in the energy O244100100004 range 70-220 MeV/u for radiation transport O244100100005 calculations in ion-beam therapy O244100100006 AUTHOR (F.Horst,G.Arico,K.-T.Brinkmann,S.Brons,A.Ferrari, O244100100007 T.Haberer,A.Mairani,K.Parodi,C.-A.Reidel,U.Weber, O244100100008 K.Zink,C.Schuy) O244100100009 INSTITUTE (2GERGSI,2ZZZCER,2GERJLU,2GERLMU,2FR ULP) O244100100010 (2GERGER) Institute of Medical Physics and Radiation O244100100011 Protection, THM University of Applied Sciences, GiessenO244100100012 (2GERGER)Heidelberg Ion-Beam Therapy Center, HeidelbergO244100100013 (2ITYITY) National Centre for Oncological HadrontherapyO244100100014 Pavia O244100100015 REFERENCE (J,PR/C,99,014603,2019) O244100100016 #doi:10.1103/PhysRevC.99.014603 O244100100017 FACILITY (SYNCH,2GERHEI) O244100100018 DETECTOR (TELES,SCIN,BAF2) a 5-mm-thick plastic scintillator O244100100019 BC-400-like and a 14-cm-thick BaF2 scintillator. O244100100020 METHOD (EDE) O244100100021 (TRN) O244100100022 ERR-ANALYS (EN-ERR) The measured cross sections are given for O244100100023 the energy at the center of the thickest target used O244100100024 with an uncertainty interval covering the energy loss O244100100025 before and after the target center. O244100100026 HISTORY (20200116C) VS O244100100027 ENDBIB 25 0 O244100100028 NOCOMMON 0 0 O244100100029 ENDSUBENT 28 0 O244100199999 SUBENT O2441002 20200116 O075O244100200001 BIB 3 8 O244100200002 REACTION (6-C-12(A,TCC),,SIG) O244100200003 ERR-ANALYS (DATA-ERR) The uncertainty estimation considers the O244100200004 statistical component originating from the finite O244100200005 amount of measured events as well as systematic O244100200006 components introduced by the application of fit O244100200007 methods and extrapolations into overlap regions in O244100200008 the measured spectra. O244100200009 STATUS (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244100200010 ENDBIB 8 0 O244100200011 NOCOMMON 0 0 O244100200012 DATA 4 1 O244100200013 EN EN-ERR DATA DATA-ERR O244100200014 MEV/A MEV/A MB MB O244100200015 74. 4. 277. 33. O244100200016 ENDDATA 3 0 O244100200017 ENDSUBENT 16 0 O244100299999 SUBENT O2441003 20200119 O075O244100300001 BIB 3 8 O244100300002 REACTION (6-C-12(A,NON),,SIG) O244100300003 ERR-ANALYS (DATA-ERR) The uncertainty estimation considers the O244100300004 statistical component originating from the finite O244100300005 amount of measured events as well as systematic O244100300006 components introduced by the application of fit O244100300007 methods and extrapolations into overlap regions in O244100300008 the measured spectra. O244100300009 STATUS (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244100300010 ENDBIB 8 0 O244100300011 NOCOMMON 0 0 O244100300012 DATA 4 1 O244100300013 EN EN-ERR DATA DATA-ERR O244100300014 MEV/A MEV/A MB MB O244100300015 74. 4. 602. 66. O244100300016 ENDDATA 3 0 O244100300017 ENDSUBENT 16 0 O244100399999 SUBENT O2441004 20200119 O075O244100400001 BIB 4 14 O244100400002 REACTION (6-C-CMP(A,TCC),,SIG) O244100400003 SAMPLE CH2 samples with density of 0.947 g/cm3 and thicknessesO244100400004 of 0.5, 1.0, 2.0 cm. O244100400005 At least two targets with different thicknesses were O244100400006 irradiated to have redundant information and to be O244100400007 able to check for robustness of the data analysis O244100400008 method. O244100400009 ERR-ANALYS (DATA-ERR) The uncertainty estimation considers the O244100400010 statistical component originating from the finite O244100400011 amount of measured events as well as systematic O244100400012 components introduced by the application of fit O244100400013 methods and extrapolations into overlap regions in O244100400014 the measured spectra. O244100400015 STATUS (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244100400016 ENDBIB 14 0 O244100400017 NOCOMMON 0 0 O244100400018 DATA 4 3 O244100400019 EN EN-ERR DATA DATA-ERR O244100400020 MEV/A MEV/A MB MB O244100400021 71. 8. 321. 47. O244100400022 119. 10. 442. 22. O244100400023 215. 5. 490. 23. O244100400024 ENDDATA 5 0 O244100400025 ENDSUBENT 24 0 O244100499999 SUBENT O2441005 20200119 O075O244100500001 BIB 4 14 O244100500002 REACTION (6-C-CMP(A,NON),,SIG) O244100500003 SAMPLE CH2 samples with density of 0.947 g/cm3 and thicknessesO244100500004 of 0.5, 1.0, 2.0 cm. O244100500005 At least two targets with different thicknesses were O244100500006 irradiated to have redundant information and to be O244100500007 able to check for robustness of the data analysis O244100500008 method. O244100500009 ERR-ANALYS (DATA-ERR) The uncertainty estimation considers the O244100500010 statistical component originating from the finite O244100500011 amount of measured events as well as systematic O244100500012 components introduced by the application of fit O244100500013 methods and extrapolations into overlap regions in O244100500014 the measured spectra. O244100500015 STATUS (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244100500016 ENDBIB 14 0 O244100500017 NOCOMMON 0 0 O244100500018 DATA 4 3 O244100500019 EN EN-ERR DATA DATA-ERR O244100500020 MEV/A MEV/A MB MB O244100500021 71. 8. 875. 103. O244100500022 119. 10. 731. 51. O244100500023 215. 5. 729. 47. O244100500024 ENDDATA 5 0 O244100500025 ENDSUBENT 24 0 O244100599999 SUBENT O2441006 20200119 O075O244100600001 BIB 4 14 O244100600002 REACTION (14-SI-28(A,TCC),,SIG) O244100600003 SAMPLE Si samples with density of 2.33 g/cm3 and thicknesses O244100600004 of 0.4, 0.8, 1.6 cm. O244100600005 At least two targets with different thicknesses were O244100600006 irradiated to have redundant information and to be O244100600007 able to check for robustness of the data analysis O244100600008 method. O244100600009 ERR-ANALYS (DATA-ERR) The uncertainty estimation considers the O244100600010 statistical component originating from the finite O244100600011 amount of measured events as well as systematic O244100600012 components introduced by the application of fit O244100600013 methods and extrapolations into overlap regions in O244100600014 the measured spectra. O244100600015 STATUS (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244100600016 ENDBIB 14 0 O244100600017 NOCOMMON 0 0 O244100600018 DATA 4 3 O244100600019 EN EN-ERR DATA DATA-ERR O244100600020 MEV/A MEV/A MB MB O244100600021 71. 8. 304. 44. O244100600022 119. 10. 487. 26. O244100600023 213. 7. 620. 26. O244100600024 ENDDATA 5 0 O244100600025 ENDSUBENT 24 0 O244100699999 SUBENT O2441007 20200119 O075O244100700001 BIB 4 14 O244100700002 REACTION (14-SI-28(A,NON),,SIG) O244100700003 SAMPLE Si samples with density of 2.33 g/cm3 and thicknesses O244100700004 of 0.4, 0.8, 1.6 cm. O244100700005 At least two targets with different thicknesses were O244100700006 irradiated to have redundant information and to be O244100700007 able to check for robustness of the data analysis O244100700008 method. O244100700009 ERR-ANALYS (DATA-ERR) The uncertainty estimation considers the O244100700010 statistical component originating from the finite O244100700011 amount of measured events as well as systematic O244100700012 components introduced by the application of fit O244100700013 methods and extrapolations into overlap regions in O244100700014 the measured spectra. O244100700015 STATUS (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244100700016 ENDBIB 14 0 O244100700017 NOCOMMON 0 0 O244100700018 DATA 4 3 O244100700019 EN EN-ERR DATA DATA-ERR O244100700020 MEV/A MEV/A MB MB O244100700021 71. 8. 961. 110. O244100700022 119. 10. 816. 59. O244100700023 213. 7. 792. 43. O244100700024 ENDDATA 5 0 O244100700025 ENDSUBENT 24 0 O244100799999 SUBENT O2441008 20200119 O075O244100800001 BIB 4 14 O244100800002 REACTION (14-SI-OXI(A,TCC),,SIG) O244100800003 SAMPLE Si samples with density of 2.204 g/cm3 and thicknesses O244100800004 of 0.4, 0.8, 1.6 cm. O244100800005 At least two targets with different thicknesses were O244100800006 irradiated to have redundant information and to be O244100800007 able to check for robustness of the data analysis O244100800008 method. O244100800009 ERR-ANALYS (DATA-ERR) The uncertainty estimation considers the O244100800010 statistical component originating from the finite O244100800011 amount of measured events as well as systematic O244100800012 components introduced by the application of fit O244100800013 methods and extrapolations into overlap regions in O244100800014 the measured spectra. O244100800015 STATUS (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244100800016 ENDBIB 14 0 O244100800017 NOCOMMON 0 0 O244100800018 DATA 4 3 O244100800019 EN EN-ERR DATA DATA-ERR O244100800020 MEV/A MEV/A MB MB O244100800021 71. 8. 806. 99. O244100800022 119. 10. 1240. 58. O244100800023 213. 7. 1563. 58. O244100800024 ENDDATA 5 0 O244100800025 ENDSUBENT 24 0 O244100899999 SUBENT O2441009 20200119 O075O244100900001 BIB 4 14 O244100900002 REACTION (14-SI-OXI(A,NON),,SIG) O244100900003 SAMPLE Si samples with density of 2.204 g/cm3 and thicknesses O244100900004 of 0.4, 0.8, 1.6 cm. O244100900005 At least two targets with different thicknesses were O244100900006 irradiated to have redundant information and to be O244100900007 able to check for robustness of the data analysis O244100900008 method. O244100900009 ERR-ANALYS (DATA-ERR) The uncertainty estimation considers the O244100900010 statistical component originating from the finite O244100900011 amount of measured events as well as systematic O244100900012 components introduced by the application of fit O244100900013 methods and extrapolations into overlap regions in O244100900014 the measured spectra. O244100900015 STATUS (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244100900016 ENDBIB 14 0 O244100900017 NOCOMMON 0 0 O244100900018 DATA 4 3 O244100900019 EN EN-ERR DATA DATA-ERR O244100900020 MEV/A MEV/A MB MB O244100900021 71. 8. 2317. 251. O244100900022 119. 10. 2042. 139. O244100900023 213. 7. 1959. 98. O244100900024 ENDDATA 5 0 O244100900025 ENDSUBENT 24 0 O244100999999 SUBENT O2441010 20200119 O075O244101000001 BIB 4 14 O244101000002 REACTION (1-H-WTR(A,TCC),,SIG) O244101000003 SAMPLE H2O with thicknesses 2.22 and 3.25 cm in flasks with O244101000004 2x0.18 cm polystyrene walls. O244101000005 At least two targets with different thicknesses were O244101000006 irradiated to have redundant information and to be O244101000007 able to check for robustness of the data analysis O244101000008 method. O244101000009 ERR-ANALYS (DATA-ERR) The uncertainty estimation considers the O244101000010 statistical component originating from the finite O244101000011 amount of measured events as well as systematic O244101000012 components introduced by the application of fit O244101000013 methods and extrapolations into overlap regions in O244101000014 the measured spectra. O244101000015 STATUS (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244101000016 ENDBIB 14 0 O244101000017 NOCOMMON 0 0 O244101000018 DATA 4 1 O244101000019 EN EN-ERR DATA DATA-ERR O244101000020 MEV/A MEV/A MB MB O244101000021 213. 7. 568. 35. O244101000022 ENDDATA 3 0 O244101000023 ENDSUBENT 22 0 O244101099999 SUBENT O2441011 20200119 O075O244101100001 BIB 4 14 O244101100002 REACTION (1-H-WTR(A,TCC),,SIG) O244101100003 SAMPLE H2O with thicknesses 2.22 and 3.25 cm in flasks with O244101100004 2x0.18 cm polystyrene walls. O244101100005 At least two targets with different thicknesses were O244101100006 irradiated to have redundant information and to be O244101100007 able to check for robustness of the data analysis O244101100008 method. O244101100009 ERR-ANALYS (DATA-ERR) The uncertainty estimation considers the O244101100010 statistical component originating from the finite O244101100011 amount of measured events as well as systematic O244101100012 components introduced by the application of fit O244101100013 methods and extrapolations into overlap regions in O244101100014 the measured spectra. O244101100015 STATUS (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244101100016 ENDBIB 14 0 O244101100017 NOCOMMON 0 0 O244101100018 DATA 4 1 O244101100019 EN EN-ERR DATA DATA-ERR O244101100020 MEV/A MEV/A MB MB O244101100021 213. 7. 800. 58. O244101100022 ENDDATA 3 0 O244101100023 ENDSUBENT 22 0 O244101199999 SUBENT O2441012 20200119 O075O244101200001 BIB 4 9 O244101200002 REACTION (1-H-1(A,TCC),,SIG,,,DERIV) O244101200003 ANALYSIS Derived by subtraction of the elemental C cross sectionO244101200004 from those measured on CH2 compound target. O244101200005 ERR-ANALYS (DATA-ERR) Uncertainties calculated from the O244101200006 uncertainties of the CH2 and C cross sections assuming O244101200007 they are not correlated. O244101200008 STATUS (DEP,O2441004) CH2 data O244101200009 (DEP,O2435003) C data O244101200010 (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244101200011 ENDBIB 9 0 O244101200012 NOCOMMON 0 0 O244101200013 DATA 6 3 O244101200014 EN EN-ERR DATA DATA-ERR +DATA-ERR -DATA-ERR O244101200015 MEV/A MEV/A MB MB MB MB O244101200016 71. 8. 22. 57. 22.O244101200017 119. 10. 60. 31. O244101200018 213. 7. 49. 30. O244101200019 ENDDATA 5 0 O244101200020 ENDSUBENT 19 0 O244101299999 SUBENT O2441013 20200119 O075O244101300001 BIB 4 9 O244101300002 REACTION (1-H-1(A,NON),,SIG,,,DERIV) O244101300003 ANALYSIS Derived by subtraction of the elemental C cross sectionO244101300004 from those measured on CH2 compound target. O244101300005 ERR-ANALYS (DATA-ERR) Uncertainties calculated from the O244101300006 uncertainties of the CH2 and C cross sections assuming O244101300007 they are not correlated. O244101300008 STATUS (DEP,O2441005) CH2 data O244101300009 (DEP,O2435002) C data O244101300010 (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244101300011 ENDBIB 9 0 O244101300012 NOCOMMON 0 0 O244101300013 DATA 4 3 O244101300014 EN EN-ERR DATA DATA-ERR O244101300015 MEV/A MEV/A MB MB O244101300016 71. 8. 137. 69. O244101300017 119. 10. 117. 37. O244101300018 213. 7. 104. 35. O244101300019 ENDDATA 5 0 O244101300020 ENDSUBENT 19 0 O244101399999 SUBENT O2441014 20200119 O075O244101400001 BIB 4 9 O244101400002 REACTION (8-O-16(A,TCC),,SIG,,,DERIV) O244101400003 ANALYSIS Derived by subtraction of the elemental Si cross O244101400004 section from those measured on SiO2 compound target. O244101400005 ERR-ANALYS (DATA-ERR) Uncertainties calculated from the O244101400006 uncertainties of the SiO2 and Si cross sections O244101400007 assuming they are not correlated. O244101400008 STATUS (DEP,O2441006) Si data O244101400009 (DEP,O2441008) SiO2 data O244101400010 (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244101400011 ENDBIB 9 0 O244101400012 NOCOMMON 0 0 O244101400013 DATA 4 3 O244101400014 EN EN-ERR DATA DATA-ERR O244101400015 MEV/A MEV/A MB MB O244101400016 71. 8. 251. 108. O244101400017 119. 10. 377. 63. O244101400018 213. 7. 472. 64. O244101400019 ENDDATA 5 0 O244101400020 ENDSUBENT 19 0 O244101499999 SUBENT O2441015 20200119 O075O244101500001 BIB 4 9 O244101500002 REACTION (8-O-16(A,NON),,SIG,,,DERIV) O244101500003 ANALYSIS Derived by subtraction of the elemental Si cross O244101500004 section from those measured on SiO2 compound target. O244101500005 ERR-ANALYS (DATA-ERR) Uncertainties calculated from the O244101500006 uncertainties of the SiO2 and Si cross sections O244101500007 assuming they are not correlated. O244101500008 STATUS (DEP,O2441006) Si data O244101500009 (DEP,O2441008) SiO2 data O244101500010 (TABLE) Table 1 of Phys.Rev.C99(2019)014603 O244101500011 ENDBIB 9 0 O244101500012 NOCOMMON 0 0 O244101500013 DATA 4 3 O244101500014 EN EN-ERR DATA DATA-ERR O244101500015 MEV/A MEV/A MB MB O244101500016 71. 8. 678. 152. O244101500017 119. 10. 613. 88. O244101500018 213. 7. 584. 75. O244101500019 ENDDATA 5 0 O244101500020 ENDSUBENT 19 0 O244101599999 ENDENTRY 15 0 O244199999999