ENTRY O2356 20180211 O064O235600000001 SUBENT O2356001 20180211 O064O235600100001 BIB 11 42 O235600100002 TITLE Spectroscopy of 46Ar by the (t,p) two-neutron O235600100003 transfer reaction O235600100004 AUTHOR (K.Nowak,K.Wimmer,S.Hellgartner,D.Mucher,V.Bildstein, O235600100005 J.Diriken,J.Elseviers,L.P.Gaffney,R.Gernhauser, O235600100006 J.Iwanicki,J.G.Johansen,M.Huyse,J.Konki,T.Kroll, O235600100007 R.Krucken,R.Lutter,R.Orlandi,J.Pakarinen,R.Raabe, O235600100008 P.Reiter,T.Roger,G.Schrieder,M.Seidlitz,O.Sorlin, O235600100009 P.Van Duppen,N.Warr,H.De Witte,M.Zielinska) O235600100010 INSTITUTE (2GERMUN,2JPNTOK,1CANGUE,2BLGLEU,2UK LVP,2DENAAU, O235600100011 2ZZZCER,2SF HLS,2SF JYV,2GERTHD,1CANUBC,2GERMUU, O235600100012 2GERKLN,2FR GAN,3POLWWA,2SPNIEM) O235600100013 REFERENCE (J,PR/C,93,044335,2016) O235600100014 #doi:10.1103/PhysRevC.93.044335 O235600100015 FACILITY (SYNCH,2ZZZCER) O235600100016 SAMPLE Tritium-loaded titanium foil, with width of 4.5 mm O235600100017 and thickness of 0.5 mg/cm**2. The tritium / O235600100018 titanium ratio was 1.3:1, corresponding to an O235600100019 effective tritium thickness of 36 ug/cm**2. O235600100020 INC-SOURCE The radioactive 44Ar beam was produced by 1.4-GeV O235600100021 protons on an uranium carbide target. The target was O235600100022 heated to reduce contamination via CO2. The 44Ar ions O235600100023 then were transferred into the FEBIAD ion source to O235600100024 achieve high ionization efficiency for 1+ state. O235600100025 Afterwards, the ions were accelerated to 30 keV and O235600100026 led through the HRS separator. The ions were then O235600100027 accumulated in the REX trap for 60 ms, before O235600100028 injection into the REX EBIS ion source. Before O235600100029 acceleration the ions were separated by their mass to O235600100030 charge ratio. O235600100031 DETECTOR (SISD) T-REX silicon detector array O235600100032 (HPGE) MINIBALL germanium detector array O235600100033 METHOD (EDE,EXTB,GSPEC,SITA)The 44Ar(t,p) transfer reaction O235600100034 was studied by radioactive beams at REX ISOLDE, The O235600100035 44Ar ions were accelerated by the REX LINAC to 2.16 O235600100036 MeV, and directed to the tritiated titanium target. O235600100037 The average beam intensity was 2*10**5 ions/sec. The O235600100038 angular distribution of protons from the reaction was O235600100039 measured. Doppler corrected gamma spectra were also O235600100040 acquired. O235600100041 ADD-RES (COMP) The experimental results were compared with O235600100042 theoretical calculations using the DWBA reaction model.O235600100043 HISTORY (20180201C) MPT O235600100044 ENDBIB 42 0 O235600100045 COMMON 1 3 O235600100046 EN O235600100047 MEV/A O235600100048 2.16 O235600100049 ENDCOMMON 3 0 O235600100050 ENDSUBENT 49 0 O235600199999 SUBENT O2356002 20180211 O064O235600200001 BIB 3 4 O235600200002 REACTION ((1-H-3(18-AR-44,P)18-AR-46,PAR,DA,RSD)= O235600200003 (18-AR-44(T,P)18-AR-46,PAR,DA)) O235600200004 STATUS (TABLE) Data were obtained from Dr. Wimmer. O235600200005 ERR-ANALYS (DATA-ERR) No detailed error analysis was provided. O235600200006 ENDBIB 4 0 O235600200007 NOCOMMON 0 0 O235600200008 DATA 5 87 O235600200009 E-LVL ANG ANG-ERR DATA DATA-ERR O235600200010 KEV ADEG ADEG MB/SR MB/SR O235600200011 0. 134.27 2.42 2.05E-02 1.18E-02 O235600200012 0. 126.79 2.85 4.29E-03 4.29E-03 O235600200013 0. 123.82 3.10 8.46E-03 5.98E-03 O235600200014 0. 120.59 3.39 7.30E-03 5.16E-03 O235600200015 0. 117.03 3.71 9.50E-03 5.49E-03 O235600200016 0. 113.16 3.99 2.62E-02 8.73E-03 O235600200017 0. 109.05 4.33 1.12E-02 4.19E-03 O235600200018 0. 104.50 4.73 5.23E-03 3.02E-03 O235600200019 0. 99.60 5.02 1.47E-02 4.91E-03 O235600200020 0. 94.45 5.27 5.09E-03 2.94E-03 O235600200021 0. 89.06 5.49 7.05E-03 3.52E-03 O235600200022 0. 83.48 5.58 2.09E-03 1.57E-03 O235600200023 0. 50.11 4.24 1.26E-01 1.70E-02 O235600200024 0. 45.88 4.01 1.62E-01 2.08E-02 O235600200025 0. 42.09 3.58 1.62E-01 2.10E-02 O235600200026 0. 38.71 3.23 1.32E-01 1.91E-02 O235600200027 0. 35.64 2.90 8.73E-02 1.65E-02 O235600200028 0. 32.92 2.55 1.23E-01 2.03E-02 O235600200029 0. 30.55 2.25 6.89E-02 1.67E-02 O235600200030 0. 28.43 2.01 1.70E-02 8.52E-03 O235600200031 0. 26.53 1.79 3.49E-02 1.32E-02 O235600200032 0. 24.84 1.60 2.34E-02 1.17E-02 O235600200033 0. 23.34 1.43 2.65E-02 1.32E-02 O235600200034 0. 21.98 1.29 3.05E-02 1.52E-02 O235600200035 0. 20.76 1.15 2.86E-02 1.65E-02 O235600200036 0. 19.68 1.14 8.29E-02 2.94E-02 O235600200037 0. 18.48 1.34 1.14E-01 3.45E-02 O235600200038 0. 17.00 1.48 5.86E-02 2.54E-02 O235600200039 1556. 134.27 2.42 5.01E-03 5.01E-03 O235600200040 1556. 129.52 2.60 3.51E-03 3.51E-03 O235600200041 1556. 126.79 2.85 5.47E-03 3.87E-03 O235600200042 1556. 123.82 3.10 2.56E-03 2.56E-03 O235600200043 1556. 117.03 3.71 5.81E-03 3.35E-03 O235600200044 1556. 113.16 3.99 5.72E-03 3.30E-03 O235600200045 1556. 109.05 4.33 9.24E-03 3.47E-03 O235600200046 1556. 104.50 4.73 7.80E-03 3.49E-03 O235600200047 1556. 99.60 5.02 1.05E-02 3.97E-03 O235600200048 1556. 94.45 5.27 4.64E-03 2.68E-03 O235600200049 1556. 89.06 5.49 1.47E-02 4.91E-03 O235600200050 1556. 83.48 5.58 1.37E-02 3.89E-03 O235600200051 1556. 50.11 4.24 3.72E-02 9.03E-03 O235600200052 1556. 45.88 4.01 3.39E-02 9.06E-03 O235600200053 1556. 42.09 3.58 4.04E-02 1.01E-02 O235600200054 1556. 38.71 3.23 3.73E-02 9.97E-03 O235600200055 1556. 35.64 2.90 5.59E-02 1.29E-02 O235600200056 1556. 32.92 2.55 5.10E-02 1.32E-02 O235600200057 1556. 30.55 2.25 4.64E-02 1.40E-02 O235600200058 1556. 28.43 2.01 5.95E-02 1.65E-02 O235600200059 1556. 26.53 1.79 5.38E-02 1.70E-02 O235600200060 1556. 24.84 1.60 4.41E-02 1.67E-02 O235600200061 1556. 23.34 1.43 6.77E-02 2.26E-02 O235600200062 1556. 21.98 1.29 3.38E-02 1.69E-02 O235600200063 1556. 20.76 1.15 4.24E-02 2.12E-02 O235600200064 1556. 19.68 1.14 2.33E-02 1.65E-02 O235600200065 1556. 18.48 1.34 4.67E-02 2.34E-02 O235600200066 3695. 140.03 3.20 8.98E-02 3.89E-02 O235600200067 3695. 136.83 2.88 3.54E-02 1.25E-02 O235600200068 3695. 134.27 2.42 7.67E-02 1.81E-02 O235600200069 3695. 132.00 2.37 6.62E-02 1.52E-02 O235600200070 3695. 129.52 2.60 7.47E-02 1.50E-02 O235600200071 3695. 126.79 2.85 4.25E-02 1.00E-02 O235600200072 3695. 123.82 3.10 4.30E-02 9.88E-03 O235600200073 3695. 120.59 3.39 4.43E-02 9.06E-03 O235600200074 3695. 117.03 3.71 3.86E-02 8.06E-03 O235600200075 3695. 113.16 3.99 6.20E-02 1.01E-02 O235600200076 3695. 109.05 4.33 6.64E-02 8.56E-03 O235600200077 3695. 104.50 4.73 5.66E-02 8.75E-03 O235600200078 3695. 99.60 5.02 7.16E-02 9.67E-03 O235600200079 3695. 94.45 5.27 8.05E-02 1.03E-02 O235600200080 3695. 89.06 5.49 8.35E-02 1.09E-02 O235600200081 3695. 83.48 5.58 4.62E-02 6.67E-03 O235600200082 3695. 50.11 4.24 2.46E-01 2.19E-02 O235600200083 3695. 45.88 4.01 2.00E-01 2.12E-02 O235600200084 3695. 42.09 3.58 1.26E-01 1.79E-02 O235600200085 3695. 38.71 3.23 1.42E-01 1.98E-02 O235600200086 3695. 35.64 2.90 8.29E-02 1.63E-02 O235600200087 3695. 32.92 2.55 7.27E-02 1.67E-02 O235600200088 3695. 30.55 2.25 5.48E-02 1.66E-02 O235600200089 3695. 28.43 2.01 1.10E-01 2.47E-02 O235600200090 3695. 26.53 1.79 1.68E-01 3.31E-02 O235600200091 3695. 24.84 1.60 4.00E-02 1.79E-02 O235600200092 3695. 23.34 1.43 6.23E-02 2.36E-02 O235600200093 3695. 21.98 1.29 1.26E-01 3.66E-02 O235600200094 3695. 20.76 1.15 1.31E-01 4.15E-02 O235600200095 3695. 19.68 1.14 1.65E-01 4.99E-02 O235600200096 3695. 18.48 1.34 2.92E-01 6.75E-02 O235600200097 3695. 17.00 1.48 3.15E-01 7.19E-02 O235600200098 ENDDATA 89 0 O235600200099 ENDSUBENT 98 0 O235600299999 ENDENTRY 2 0 O235699999999