ENTRY O0561 20101203 O043O056100000001 SUBENT O0561001 20101203 O043O056100100001 BIB 12 57 O056100100002 TITLE Proton total cross sections on 1-H, 2-H, 4-He, 9-Be, O056100100003 carbon and oxygen in the energy range 180 to 560 MeV. O056100100004 REFERENCE (J,NP/A,316,317,1979) O056100100005 AUTHOR (P.Schwaller,M.Pepin,B.Favier,C.Richard-Serre, O056100100006 D.F.Measday,P.U.Renberg) O056100100007 INSTITUTE (2SWTPSI) Swiss. Inst. For Nucl. Phys., Villigen. O056100100008 (2FR GRE) University of Grenoble. O056100100009 (2ZZZCER) O056100100010 FACILITY (SYNCY,2ZZZCER) 600 MeV Synchrocyclotron. O056100100011 METHOD (EDEG) To obtain lower energies, a degrader of boron O056100100012 carbide was used. O056100100013 (SITA) O056100100014 (COINC) See Detector O056100100015 (TRN) The Standard Transmission Technique was used. O056100100016 COMMENT All REACTION codes are given with SF8=MSC. It means O056100100017 that total cross sections were determined approximatelyO056100100018 In charged-particle induced reaction, angular O056100100019 differential cross section diverges at the most O056100100020 forwarded angle because of long-range character of O056100100021 Coulomb interaction. Therefore elastic scattering O056100100022 cross section and total cross section are infinity for O056100100023 charged-particle induced reactions. Authors used O056100100024 the extrapolation to zero solid angle and correction O056100100025 for Coulomb-Nuclear Interference (see CORRECTION) O056100100026 DETECTOR (SCIN) The detection system consisted of seven O056100100027 transmission counters, 5 mm thick. The counters O056100100028 covered solid angles in the sequence 1, 2, 3, 4, 5, 7,O056100100029 9, the smallest and largest counters being 15 and 45 cmO056100100030 in diameter, respectively. O056100100031 CORRECTION Experimental data are corrected for Coulomb-Nuclear O056100100032 Interference in elastic scattering at small angles. O056100100033 The interference correction dominates all other O056100100034 problems both in the statistical fitting of the O056100100035 various functions, but more important, in the basic O056100100036 formulation of the fitting procedure. The details of O056100100037 this interference correction are quite different for O056100100038 the three cases, hydrogen, deuterium and light complex O056100100039 nuclei. O056100100040 ADD-RES Method of Coulomb Interaction Correction. O056100100041 ERR-ANALYS (ERR-T) Total uncertainty of cross section. O056100100042 Fairly minor contributions come from - O056100100043 (ERR-1).Error in counting statistics is 0.2%, O056100100044 (ERR-2).Error in stability of the efficiency of the O056100100045 scintillation Counters is 0.05%, O056100100046 (ERR-3).Error in accidental coincidences is 0.1% O056100100047 (ERR-4).Error in the background correction is 0.15%, O056100100048 (ERR-5,0.2,0.5).Error in the Target Length is 0.2%, O056100100049 except for deuterium where one was assumed as 0.5%. O056100100050 The Energy measurement when converted to an error in O056100100051 the cross section is normally negligible less than O056100100052 0.2%, except for the energy region between 400 and O056100100053 600 MeV where it reaches 0.3% for p-d cross sections O056100100054 and 0.6% for p-p cross sections. O056100100055 HISTORY (19990825C) O056100100056 (19991117A) DATE is corrected O056100100057 (20101002A) SD: COMMENT with description of SF8=MSC O056100100058 in all REACTION codes added in Subent 001 O056100100059 ENDBIB 57 0 O056100100060 COMMON 4 3 O056100100061 ERR-1 ERR-2 ERR-3 ERR-4 O056100100062 PER-CENT PER-CENT PER-CENT PER-CENT O056100100063 0.2 0.05 0.1 0.15 O056100100064 ENDCOMMON 3 0 O056100100065 ENDSUBENT 64 0 O056100199999 SUBENT O0561002 20101203 O043O056100200001 BIB 4 13 O056100200002 REACTION (1-H-1(P,TOT),,SIG,,MSC) O056100200003 see COMMENT in Subent 001 O056100200004 SAMPLE The cryogenic target consisted of metal cylinders, 16 mO056100200005 in diameter, with 0.25 mm thick Mylar window at both O056100200006 ends. O056100200007 Target density was determined by measuring the vapour O056100200008 pressure of hydrogen immediately above the liquid, and O056100200009 converting it into density by means of Table. O056100200010 Target length - 75 cm, thickness - 5.3 g/cm2. O056100200011 Absorption (%) at 200 MeV - 7%. O056100200012 Energy loss at 200 MeV - 52 MeV. O056100200013 ERR-ANALYS (ERR-S) Statistical error. O056100200014 STATUS (TABLE) Tbl. 3 from NP/A,316,317,1979 O056100200015 ENDBIB 13 0 O056100200016 NOCOMMON 0 0 O056100200017 DATA 4 9 O056100200018 EN DATA ERR-S ERR-T O056100200019 MEV MB MB MB O056100200020 179.0 24.2 0.12 0.24 O056100200021 267.5 23.85 0.1 0.23 O056100200022 342.5 24.55 0.1 0.23 O056100200023 388.0 25.7 0.1 0.23 O056100200024 406.5 26.5 0.1 0.23 O056100200025 439.5 27.95 0.14 0.29 O056100200026 502.5 31.25 0.15 0.34 O056100200027 513.5 31.95 0.19 0.36 O056100200028 555.0 34.8 0.24 0.39 O056100200029 ENDDATA 11 0 O056100200030 ENDSUBENT 29 0 O056100299999 SUBENT O0561003 20101203 O043O056100300001 BIB 3 12 O056100300002 REACTION (1-H-2(P,TOT),,SIG,,MSC) O056100300003 see COMMENT in Subent 001 O056100300004 SAMPLE the cryogenic target consisted of metal cylinders, 16 mO056100300005 in diameter, with 0.25 mm thick Mylar window at O056100300006 both ends. Target density was determined by measuring O056100300007 the temperature with a hydrogen gas thermometer, O056100300008 which was mounted inside the liquid, immediately O056100300009 above the target container. Target length - 35 cm, O056100300010 thickness - 5.9 g/cm2. O056100300011 Absorption (%) at 200 MeV - 10%. O056100300012 Energy loss at 200 MeV - 25 MeV. O056100300013 STATUS (TABLE) Tbl. 4 from NP/A,316,317,1979 O056100300014 ENDBIB 12 0 O056100300015 NOCOMMON 0 0 O056100300016 DATA 3 7 O056100300017 EN DATA ERR-T O056100300018 MEV MB MB O056100300019 227. 63.2 0.7 O056100300020 275. 60.8 0.7 O056100300021 348. 59.9 0.7 O056100300022 412. 61.3 0.7 O056100300023 422. 61.3 0.7 O056100300024 483. 64.6 0.7 O056100300025 560. 69.4 0.7 O056100300026 ENDDATA 9 0 O056100300027 ENDSUBENT 26 0 O056100399999 SUBENT O0561004 20101203 O043O056100400001 BIB 3 12 O056100400002 REACTION (2-HE-4(P,TOT),,SIG,,MSC) O056100400003 see COMMENT in Subent 001 O056100400004 SAMPLE the cryogenic target consisted of metal cylinders, 16 mO056100400005 in diameter, with 0.25 mm thick Mylar window at both O056100400006 ends. O056100400007 Target density was determined by measuring the vapour O056100400008 pressure of helium immediately above the liquid, and O056100400009 converting it into density by means of table. O056100400010 target length - 75 cm, thickness - 9.3 g/cm2. O056100400011 Absorption (%) at 200 MeV - 13%. O056100400012 Energy loss at 200 MeV - 37 MeV. O056100400013 STATUS (TABLE) Tbl. 5 from NP/A,316,317,1979 O056100400014 ENDBIB 12 0 O056100400015 NOCOMMON 0 0 O056100400016 DATA 3 7 O056100400017 EN DATA ERR-T O056100400018 MEV MB MB O056100400019 224. 106.3 1.3 O056100400020 273. 105.7 1.3 O056100400021 345. 106.8 1.1 O056100400022 413. 110.8 1.2 O056100400023 430. 112.8 1. O056100400024 491. 117.6 1.5 O056100400025 563. 123.7 0.9 O056100400026 ENDDATA 9 0 O056100400027 ENDSUBENT 26 0 O056100499999 SUBENT O0561005 20101203 O043O056100500001 BIB 3 6 O056100500002 REACTION (4-BE-9(P,TOT),,SIG,,MSC) O056100500003 see COMMENT in Subent 001 O056100500004 SAMPLE Target length - 5 cm, thickness - 9.3 g/cm2. O056100500005 Absorption (%) at 200 MeV - 14%. O056100500006 Energy loss at 200 MeV - 34 MeV. O056100500007 STATUS (TABLE) Tbl. 6 from NP/A,316,317,1979 O056100500008 ENDBIB 6 0 O056100500009 NOCOMMON 0 0 O056100500010 DATA 3 8 O056100500011 EN DATA ERR-T O056100500012 MEV MB MB O056100500013 225. 235.7 5.2 O056100500014 279. 229.3 4.8 O056100500015 350. 231.5 3.8 O056100500016 394. 238.6 3.4 O056100500017 445. 244.4 3.4 O056100500018 466. 248. 3.1 O056100500019 518. 254. 2.6 O056100500020 557. 259.3 2.5 O056100500021 ENDDATA 10 0 O056100500022 ENDSUBENT 21 0 O056100599999 SUBENT O0561006 20101203 O043O056100600001 BIB 4 7 O056100600002 REACTION (6-C-12(P,TOT),,SIG,,MSC) O056100600003 see COMMENT in Subent 001 O056100600004 SAMPLE Target length - 5 cm, thickness - 9.2 g/cm2. O056100600005 Absorption (%) at 200 MeV - 12%. O056100600006 Energy loss at 200 MeV - 38 MeV. O056100600007 FLAG (1.) Data Measured with Ch2 target. O056100600008 STATUS (TABLE) Tbl. 7 from NP/A,316,317,1979 O056100600009 ENDBIB 7 0 O056100600010 NOCOMMON 0 0 O056100600011 DATA 4 20 O056100600012 EN DATA ERR-T FLAG O056100600013 MEV MB MB NO-DIM O056100600014 191. 282. 9. O056100600015 223. 275. 12. O056100600016 277. 283. 4. O056100600017 306. 288. 6. O056100600018 348. 286. 6. O056100600019 349. 283.5 3. O056100600020 372. 297. 4.5 O056100600021 392. 300.5 4. O056100600022 441. 298. 5. O056100600023 453. 302. 7. O056100600024 456. 301. 7. O056100600025 463. 301. 8. 1. O056100600026 467. 308. 4. O056100600027 497. 314. 8. O056100600028 502. 313. 5. 1. O056100600029 506. 313. 4. O056100600030 518. 319. 4.5 O056100600031 550. 323. 11. 1. O056100600032 553. 323. 10. O056100600033 559. 327. 6. O056100600034 ENDDATA 22 0 O056100600035 ENDSUBENT 34 0 O056100699999 SUBENT O0561007 20101203 O043O056100700001 BIB 3 7 O056100700002 REACTION (8-O-16(P,TOT),,SIG,,MSC) O056100700003 see COMMENT in Subent 001 O056100700004 SAMPLE Water was used as target. O056100700005 Target length - 8.7 cm, thickness - 8.7 g/cm2. O056100700006 Absorption (%) at 200 MeV - 12%. O056100700007 Energy loss at 200 MeV - 40 MeV. O056100700008 STATUS (TABLE) Tbl. 8 from NP/A,316,317,1979 O056100700009 ENDBIB 7 0 O056100700010 NOCOMMON 0 0 O056100700011 DATA 3 8 O056100700012 EN DATA ERR-T O056100700013 MEV MB MB O056100700014 190. 387. 30. O056100700015 222. 386. 15. O056100700016 276. 360. 7. O056100700017 348. 367. 6. O056100700018 392. 377. 6. O056100700019 442. 381. 6. O056100700020 516. 397. 4. O056100700021 558. 411. 7. O056100700022 ENDDATA 10 0 O056100700023 ENDSUBENT 22 0 O056100799999 ENDENTRY 7 0 O056199999999