ENTRY D6261 20170322 D110D626100000001 SUBENT D6261001 20170322 D110D626100100001 BIB 9 50 D626100100002 TITLE Fusion measurements for the 18O+194Pt reaction and D626100100003 search for neutron shell closure effects D626100100004 AUTHOR (P.V.Laveen, E.Prasad, N.Madhavan, S.Pal, J.Sadhukhan, D626100100005 S.Nath, J.Gehlot, A.Jhingan, K.M.Varier, R.G.Thomas, D626100100006 A.M.Vinodkumar, A.Shamlath, T.Varughese, P.Sugathan, D626100100007 B.R.S.Babu, S.Appannababu, K.S.Golda, B.R.Behera, D626100100008 V.Singh, R.Sandal, A.Saxena, B.V.John, S.Kailas) D626100100009 INSTITUTE (3INDNSD,3INDVEC,3INDTRM,3INDCCT,3INDPUC,3AULCBR, D626100100010 1USAINU) D626100100011 (3INDIND) Central University of Kerala, Kasaragod D626100100012 (3INDIND) CS-6/1, Golf Green, Kolkata D626100100013 (3INDIND) University College Trivandrum, Kerala D626100100014 (3OMNOMN) Sultan Qaboos University, Muscat D626100100015 (3INDIND) University of Mumbai, Mumbai D626100100016 (3INDIND) S V Govt. College Ghumarwin, Bilaspur D626100100017 REFERENCE (J,JP/G,42,095105,2015) D626100100018 FACILITY (VDGT,3INDNSD) 15 UD Pelletron D626100100019 (VDGT,3INDTRM) 14 UD Pelletron D626100100020 SAMPLE 194Pt target of thickness 265 ug/cm2 on 10 ug/cm2 D626100100021 thick carbon backing D626100100022 DETECTOR (SI) Two silicon detectors were used inside the D626100100023 target chamber, placed at an angle +- 22.7 degrees, D626100100024 to detect the elastically scattered particles and D626100100025 flux normalization. D626100100026 (MWPC) The evaporation redidues reaching the focal D626100100027 plane were detected using a position sensitive D626100100028 multiwire proportional counter (MWPC) of active area D626100100029 15 x 5 cm2. This detector was operated with isobutane D626100100030 gas at 2 mbar pressure and it provided two- D626100100031 dimensional position (X, Y) signals, energy loss D626100100032 signal (cathode) and timing signal (anode). D626100100033 (TELES,SI,SI) The fission measurements were performed D626100100034 in a separate experiment using the scattering chamber D626100100035 of BARC-TIFR 14UD Pelletron accelerator facility. The D626100100036 fission fragments were collected using three dE-E D626100100037 silicon detector telescopes consisting of 15.20 um D626100100038 thick dE detectors and 300.500 um thick E detectors. D626100100039 An aluminium collimator of diameter 5 mm was used in D626100100040 front of each telescope assembly. These telescopes D626100100041 were placed at 13.6 cm from the target, on the same D626100100042 movable arm of the scattering chamber. D626100100043 (SIBAR) Two silicon surface barrier detectors were D626100100044 mounted at angle +- 20 degrees with respect to the D626100100045 beam direction, at a distance of 42 cm from the D626100100046 target center. The elastic events recorded in these D626100100047 detectors were used for the normalization of the D626100100048 fission yields and estimation of the absolute D626100100049 differential cross sections. D626100100050 METHOD (TOF,EDE) D626100100051 HISTORY (20170301C) Jagjit+BL D626100100052 ENDBIB 50 0 D626100100053 NOCOMMON 0 0 D626100100054 ENDSUBENT 53 0 D626100199999 SUBENT D6261002 20170322 D110D626100200001 BIB 3 4 D626100200002 REACTION (78-PT-194(8-O-18,FUS),,SIG,ER) D626100200003 ERR-ANALYS (DATA-ERR) The over all uncertainty is < 20% D626100200004 STATUS (TABLE) Table 1 of Journal of Phys.G:Nucl.Part.Phys., D626100200005 42(2015)095105 D626100200006 ENDBIB 4 0 D626100200007 NOCOMMON 0 0 D626100200008 DATA 3 7 D626100200009 EN-CM DATA DATA-ERR D626100200010 MEV MB MB D626100200011 71.1 50. 10. D626100200012 75.8 214. 43. D626100200013 79.5 347. 69. D626100200014 84.2 387. 77. D626100200015 87.9 401. 63. D626100200016 91.7 366. 73. D626100200017 96.4 316. 63. D626100200018 ENDDATA 9 0 D626100200019 ENDSUBENT 18 0 D626100299999 SUBENT D6261003 20170322 D110D626100300001 BIB 4 6 D626100300002 REACTION 1(78-PT-194(8-O-18,F),,DA,FF,RSD) D626100300003 2(78-PT-194(8-O-18,F),,DA,FF,RSD,DERIV) D626100300004 ANALYSIS 2 Extrapolation to 180 deg. D626100300005 ERR-ANALYS (DATA-ERR) No information on source of uncertainties D626100300006 STATUS 1(TABLE) Fig.2 of J.Phys.G 42(2015)095105 D626100300007 2(TABLE) Table 2 of J.Phys.G 42(2015)095105 D626100300008 ENDBIB 6 0 D626100300009 NOCOMMON 0 0 D626100300010 DATA 6 52 D626100300011 EN ANG-CM DATA 1DATA-ERR 1DATA 2DATA-ERR 2D626100300012 MEV ADEG NO-DIM NO-DIM NO-DIM NO-DIM D626100300013 78.2 180. 1.83 0.29D626100300014 78.2 172.08 2.03158 0.11782 D626100300015 78.2 164.12 1.81479 0.11035 D626100300016 78.2 147.74 1.47203 0.09573 D626100300017 78.2 139.28 1.33906 0.08889 D626100300018 78.2 130.52 1.31583 0.08594 D626100300019 78.2 121.34 1.22239 0.07548 D626100300020 78.2 111.90 1.15718 0.07586 D626100300021 78.2 102.11 0.99626 0.06336 D626100300022 78.2 91.95 0.96107 0.06415 D626100300023 80.2 180. 1.87 0.14D626100300024 80.2 172.11 1.99893 0.08137 D626100300025 80.2 164.18 1.90440 0.07256 D626100300026 80.2 156.12 1.88630 0.07724 D626100300027 80.2 147.85 1.60243 0.06386 D626100300028 80.2 139.40 1.60059 0.06773 D626100300029 80.2 130.67 1.30673 0.05438 D626100300030 80.2 121.49 1.20662 0.04713 D626100300031 80.2 112.06 1.06587 0.04125 D626100300032 80.2 102.26 1.03531 0.04059 D626100300033 80.2 92.10 1.01196 0.03752 D626100300034 83.2 180. 2.15 0.09D626100300035 83.2 172.16 2.23531 0.09636 D626100300036 83.2 164.27 1.94182 0.07949 D626100300037 83.2 156.24 1.85414 0.08384 D626100300038 83.2 148.01 1.53977 0.06675 D626100300039 83.2 139.59 1.36722 0.06634 D626100300040 83.2 130.87 1.22530 0.05554 D626100300041 83.2 121.71 1.12556 0.04767 D626100300042 83.2 112.28 1.06896 0.04506 D626100300043 83.2 102.49 0.99376 0.04173 D626100300044 83.2 92.32 0.98005 0.04032 D626100300045 85.3 180. 2.42 0.11D626100300046 85.3 172.19 2.43427 0.10438 D626100300047 85.3 164.33 2.07058 0.08501 D626100300048 85.3 156.33 2.01429 0.08999 D626100300049 85.3 148.11 1.66986 0.07165 D626100300050 85.3 139.72 1.40959 0.06842 D626100300051 85.3 130.91 1.08844 0.05187 D626100300052 85.3 112.44 1.03731 0.04670 D626100300053 85.3 102.64 0.94313 0.03987 D626100300054 85.3 92.47 1.01208 0.04365 D626100300055 87.3 180. 2.63 0.13D626100300056 87.3 172.22 2.71769 0.12577 D626100300057 87.3 164.34 2.27324 0.09565 D626100300058 87.3 156.35 2.10511 0.10179 D626100300059 87.3 148.22 1.58291 0.07142 D626100300060 87.3 139.84 1.36288 0.07178 D626100300061 87.3 131.05 1.10590 0.05335 D626100300062 87.3 112.59 0.92735 0.04520 D626100300063 87.3 102.79 1.04337 0.04889 D626100300064 87.3 92.61 0.93995 0.04368 D626100300065 ENDDATA 54 0 D626100300066 ENDSUBENT 65 0 D626100399999 SUBENT D6261004 20170322 D110D626100400001 BIB 3 4 D626100400002 REACTION (78-PT-194(8-O-18,F),,SIG) D626100400003 ERR-ANALYS (DATA-ERR) No information on source of uncertainties D626100400004 STATUS (TABLE) Table 2 of Journal of Phys.G:Nucl.Part.Phys., D626100400005 42(2015)095105 D626100400006 ENDBIB 4 0 D626100400007 NOCOMMON 0 0 D626100400008 DATA 3 5 D626100400009 EN-CM DATA DATA-ERR D626100400010 MEV MB MB D626100400011 71.6 12. 1. D626100400012 73.4 30. 2. D626100400013 76.1 69. 5. D626100400014 78.0 104. 7. D626100400015 79.9 153. 11. D626100400016 ENDDATA 7 0 D626100400017 ENDSUBENT 16 0 D626100499999 ENDENTRY 4 0 D626199999999