the (n,g) cross section of 135_cs

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    The (n, ) cross section of 135 Cs

    S. Dababneh, M. Heil, F. Kppeler, R. Plag Karlsruhe

    N. Patronis, P.Assimakopoulos, D.Karamanis, Ioannina

    R. Gallino , Torino

    P.E. Koehler , Oak Ridge

    A. Mengoni , CERN

    and the n_TOF Collaboration

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    Motivation

    Nuclear Astrophysics

    Branching points on the s-process path.Improve calculation for the 134 Cs(n,)cross section abundance ratio of

    s-only134

    Ba/136

    Ba Physicalconditions during s-process (neutrondensity and temperature).

    Recent models kT = 8 - 26 keV normalize the theoretical cross section.

    Nuclear Transmutation

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    Experimental MethodThe activation technique

    At 30 and 500 keV, the Karlsruhe 3.7 MVVan de Graaff was used. Neutron source: 7Li(p,n) 7Be.

    Irradiation with thermal neutrons atTRIGA, Mainz number of 135 Cs nuclei.

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    Reference: 197 Au (n,) 198 Au1/2 = 2.7 d185

    Re (n,)186

    Re 1/2 = 3.7 d187 Re (n,) 188 Re

    1/2 = 17.0 hr

    Sample: ~ 1.810 15 135 Cs atoms(~ 400 ng)

    1/2 = 2.3 106

    yno gamma rays

    Product: 136 Cs

    1/2 = 13.2 dgamma rays:818 keV, 340 keV,1048 keV, 1235 keV

    and others

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    Correction factors:decay during irradiation, waiting andmeasuring

    flux variationself absorptionsumming effectgold foil position

    C = tot N f b I f m f wk Activated nuclei

    Time (days)

    N e u t r o

    n s

    Flux history

    2 4 6 8 10

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    Neutron energy distribution inthe sample

    Measured TOFgives proton

    beam energy

    Calculateddifferential

    neutron yield

    Simulated neutron

    beam atsample

    position

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    Induced activity measurementAu samples measured with HPGe detector.

    Cs sample measured with 2 Clover detectorsn close geometry.Each Clover consists of 4 HPGe crystals.Nearly 4 geometry High efficiency.

    Event by event Flexibility.Direct vs. Addback mode.Singles vs. Coincidence mode.

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    Addback vs. Direct

    Coincidences vs. Singles

    13 days

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    Coincidence mode Correction for summing effects in the

    singles spectrum.16% in Direct ModeConfirmed by Monte-Carlo

    139 La (n,) 140 La

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    Experimental Results

    30 keV

    500 keV

    E (keV) This work ENDF /B-VI

    Ratio

    30 164

    10 204 0.804500 34.8 3.0 43.6 0.798

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    Lower rate of incineration of 135Csthan previously assumed.

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