ENTRY C1491 20120618 C119C149100000001 SUBENT C1491001 20120618 C119C149100100001 BIB 9 34 C149100100002 INSTITUTE (2ITYFSN,2ITYGVA,1USAANL,1USAORL) C149100100003 REFERENCE (J,PR/C,69,064614,2004) C149100100004 (J,NP/A,746,522,2004) - prelim. data C149100100005 AUTHOR (M.Romoli,E.Vardaci,M.Di Pietro,A.De Francesco, C149100100006 A.De Rosa,G.Inglima,M.La Commara,B.Martin, C149100100007 D.Pierroutsakou,M.Sandoli,M.Mazzocco,T.Glodariu, C149100100008 P.Scopel,C.Signorini,R.Bonetti,A.Guglielmetti, C149100100009 F.Soramel,L.Stroe,J.Greene,A.Heinz,D.Henderson, C149100100010 C.L.Jiang,E.F.Moore,R.C.Pardo,K.E.Rehm,A.Wuosmaa, C149100100011 J.F.Liang) C149100100012 TITLE Measurements of 17F scattering by 208Pb with a new typeC149100100013 of large solid angle detector array C149100100014 FACILITY (LINAC,1USAANL) ATLAS superconducting linear C149100100015 accelerator C149100100016 INC-SOURCE The 17F exotic beam is produced through the inverse C149100100017 reaction p(O-17,F-17)n with an intensity of about C149100100018 10**5 pps. The energy of the outcoming F-17 beam, C149100100019 measured with an Enge split pole magnetic spectrometer,C149100100020 was 90.4 MeV, with a full width at half maximum (FWHM) C149100100021 of 1.4 MeV (corresponding to a resolution of C149100100022 about 1.5%) C149100100023 SAMPLE The target was a self supporting 1-mg/cm2-thick 208Pb C149100100024 foil. C149100100025 DETECTOR (TELES,SI,SI) EXODET array consists of 16 solid state C149100100026 silicon detectors arranged in eight two-stage C149100100027 telescopes to allow the Z identification of the C149100100028 particles passing through the first layer, by means C149100100029 of the usual dE-E technique C149100100030 HISTORY (20061221C) DR C149100100031 (20120618A) SD: Ref. was added. BIB update. Data at C149100100032 E= 98 MeV were deleted from Subent 2 (data are from C149100100033 PR/C,67,044603,2003; see C1484). Subent 3 deleted C149100100034 (data from PR/C,63,064606,2001; see S0051). C149100100035 REACTION code was corrected in Subent 2. C149100100036 ENDBIB 34 0 C149100100037 NOCOMMON 0 0 C149100100038 ENDSUBENT 37 0 C149100199999 SUBENT C1491002 20120618 C119C149100200001 BIB 5 16 C149100200002 REACTION (82-PB-208(9-F-17,SCT)82-PB-208,PAR,DA,,RTH) C149100200003 Experimental energy resolution did not allow to C149100200004 separate the contributions coming from the first C149100200005 excited states both in 17F (at 0.4953 keV) and in C149100200006 208Pb (at 2.614 MeV). However, from distorted wave BornC149100200007 approximation (DWBA) calculations, these contributions C149100200008 were predicted to be very small in comparison with the C149100200009 pure elastic cross section C149100200010 EN-SEC (E-LVL1,9-F-17) C149100200011 (E-LVL2,82-PB-208) C149100200012 ERR-ANALYS (ERR-S) Statistical error C149100200013 STATUS (CURVE) Data taken from Fig. 5 of PR/C,69,064614,2004 C149100200014 HISTORY (20061221C) DR C149100200015 (20120618A) SD: Data at E= 98 MeV were deleted (data C149100200016 are from PR/C,67,044603,2003; see C1484). C149100200017 REACTION code was corrected: SF3=EL => SCT; E-LVL addedC149100200018 ENDBIB 16 0 C149100200019 COMMON 3 3 C149100200020 EN E-LVL1 E-LVL2 C149100200021 MEV KEV MEV C149100200022 90.4 0.4953 2.614 C149100200023 ENDCOMMON 3 0 C149100200024 DATA 3 41 C149100200025 ANG-CM DATA ERR-S C149100200026 ADEG NO-DIM NO-DIM C149100200027 118.423 1.007E+00 1.190E-01 C149100200028 119.204 9.974E-01 8.386E-02 C149100200029 120.181 9.671E-01 6.218E-02 C149100200030 121.452 9.927E-01 6.604E-02 C149100200031 122.235 1.012E+00 5.603E-02 C149100200032 123.114 9.975E-01 5.747E-02 C149100200033 124.092 1.012E+00 5.829E-02 C149100200034 125.071 1.026E+00 6.600E-02 C149100200035 126.049 1.041E+00 5.298E-02 C149100200036 127.025 1.012E+00 6.058E-02 C149100200037 128.001 9.836E-01 6.543E-02 C149100200038 128.786 1.036E+00 6.202E-02 C149100200039 129.859 1.002E+00 6.447E-02 C149100200040 130.931 9.204E-01 4.268E-02 C149100200041 131.811 9.248E-01 4.706E-02 C149100200042 132.691 9.315E-01 5.367E-02 C149100200043 133.765 8.904E-01 5.131E-02 C149100200044 134.548 9.249E-01 6.153E-02 C149100200045 135.626 9.722E-01 5.602E-02 C149100200046 136.503 9.250E-01 6.358E-02 C149100200047 137.384 9.495E-01 5.045E-02 C149100200048 138.459 9.406E-01 5.420E-02 C149100200049 139.436 9.339E-01 5.590E-02 C149100200050 140.218 9.317E-01 5.368E-02 C149100200051 141.293 9.121E-01 5.663E-02 C149100200052 142.075 9.143E-01 6.082E-02 C149100200053 143.053 9.252E-01 6.155E-02 C149100200054 143.936 1.005E+00 6.910E-02 C149100200055 145.010 9.912E-01 6.594E-02 C149100200056 145.886 8.993E-01 6.380E-02 C149100200057 146.962 9.122E-01 6.874E-02 C149100200058 147.744 9.080E-01 7.239E-02 C149100200059 148.718 8.297E-01 6.976E-02 C149100200060 149.598 8.436E-01 6.909E-02 C149100200061 150.667 7.094E-01 6.426E-02 C149100200062 151.354 7.654E-01 7.918E-02 C149100200063 152.236 8.161E-01 8.788E-02 C149100200064 153.310 7.820E-01 9.896E-02 C149100200065 154.283 6.945E-01 1.021E-01 C149100200066 155.256 6.227E-01 1.174E-01 C149100200067 156.036 5.924E-01 1.882E-01 C149100200068 ENDDATA 43 0 C149100200069 ENDSUBENT 68 0 C149100299999 NOSUBENT C1491003 20120618 C119C149100300001 ENDENTRY 3 0 C149199999999