ENTRY D0390 20071125 D057D039000000001 SUBENT D0390001 20071125 D057D039000100001 BIB 10 43 D039000100002 TITLE 16O + d Reactions at Ed < 2 MeV D039000100003 AUTHOR (S.Cavallaro,A.Cunsolo,R.Potenza,A.Rubbino) D039000100004 INSTITUTE (2ITYCAT,2ITYSIC,2ITYLNS) D039000100005 REFERENCE (J,NC/A,14,692,1973) D039000100006 FACILITY (VDG,2ITYCAT) D039000100007 METHOD (BCINT) The intensity of the beam was measured by a D039000100008 Faraday cup, 25 cm long, kept under vacuum and D039000100009 separated from the gas chamber by a thin nickel foil. D039000100010 SAMPLE A gas target was used to make absolute measurements of D039000100011 the cross-section at various angles and energies of theD039000100012 incident particles. The pressure of the gas in the D039000100013 scattering chamber was regulated by a differential D039000100014 pumping system. D039000100015 The 160 gas used as a target was approx. 99% pure. D039000100016 DETECTOR (SOLST)Four solid-state movable detectors were placed D039000100017 inside the scattering chamber at intervals of 10 degr. D039000100018 from one another D039000100019 ERR-ANALYS (ERR-DIG) Digitizing error D039000100020 (ERR-T) Total error on the absolute values of the D039000100021 cross-sections. In the cross-section evaluation, D039000100022 corrections were made to take into account the 14N D039000100023 contamination. These corrections, in the case of the D039000100024 elastic scattering were always less than 1 %. D039000100025 * The Faraday-cup efficiency was estimated to be D039000100026 better than 99.0 %. D039000100027 * The accuracy of the charge integrator introduces aD039000100028 0.8 % uncertainty in the charge absolute value. D039000100029 * The error in the geometrical factor was estimated D039000100030 to introduce a 3.5 % error in the absolute value D039000100031 of the cross-section. D039000100032 * The errors in the temperature, pressure and chargeD039000100033 were taken into account. D039000100034 * very small uncertainty in the measurement D039000100035 of the angle of the detectors. D039000100036 The statistical error is negligible for the elastic D039000100037 scattering, while for (d, p) and (d, ao) reactions it D039000100038 is of the order of a few per cent D039000100039 (EN-ERR) Energy spread. Since the target length, as D039000100040 seen by the detectors through their collimators, was D039000100041 always smaller than 3 cm, an energy spread smaller D039000100042 than 15 keV at Ed. = 1.5 MeV D039000100043 HISTORY (20060307C) SD D039000100044 (20071124A) Entry deleted. Duplication with D0152 D039000100045 ENDBIB 43 0 D039000100046 COMMON 2 3 D039000100047 EN-ERR ERR-T D039000100048 MEV PER-CENT D039000100049 0.015 6. D039000100050 ENDCOMMON 3 0 D039000100051 ENDSUBENT 50 0 D039000199999 NOSUBENT D0390002 20071125 D057D039000200001 NOSUBENT D0390003 20071125 D057D039000300001 NOSUBENT D0390004 20071125 D057D039000400001 NOSUBENT D0390005 20071125 D057D039000500001 NOSUBENT D0390006 20071125 D057D039000600001 NOSUBENT D0390007 20071125 D057D039000700001 ENDENTRY 7 0 D039099999999