Measurement of $^{139}$La(n,$\gamma$) Cross Section at n_TOF
- TERLIZZI, R.
- ABBONDANNO, U.
- AERTS, G.
- ÁLVAREZ, H.
- ALVAREZ-VELARDE, F.
- ANDRIAMONJE, S.
- ANDRZEJEWSKI, J.
- ASSIMAKOPOULOS, P.
- AUDOUIN, L.
- BADUREK, G.
- BAUMANN, P.
- BEVÁ, F.
- BERTHOUMIEUX, E.
- CALVIÑO, F.
- CANO-OTT, D.
- CAPOTE, R.
- CARRILLO DE ALBORNOZ, A.
- CENNINI, P.
- CHEPEL, V.
- CHIAVERI, E.
- COLONNA, N.
- CORTES, G.
- COUTURE, A.
- COX, J.
- DAVID, S.
- DOLFINI, R.
- DOMINGO-PARDO, C.
- DALHFORS, M.
- DRIDI, W.
- DURAN, I.
- ELEFTHERIADIS, C.
- EMBID-SEGURA, M.
- FERRANT, L.
- FERRARI, Anthony
- FERREIRA-MARQUES, R.
- FITZPATRICK, L.
- FRAIS-KOELBL, H.
- FUJII, K.
- FURMAN, W.
- GUERRERO, C.
- GONCALVES, I.
- GALLINO, R.
- GONZALEZ-ROMERO, E.
- GOVERDOVSKI, A.
- GRAMEGNA, F.
- GRIESMAYER, E.
- GUNSING, F.
- HAAS, B.
- HAIGHT, R.
- HEIL, M.
- HERRERA-MARTINEZ, A.
- IGASHIRA, M.
- ISAEV, S.
- JERICHA, E.
- KADI, Y.
- KÄPPELER, F.
- KARAMANIS, D.
- KARADIMOS, D.
- KERVENO, M.
- KETLEROV, V.
- KOEHLER, P.
- KONOVALOV, V.
- KOSSIONIDES, E.
- KRTIKA, M.
- LAMBOUDIS, C.
- LEEB, H.
- LINDOTE, A.
- LOPES, I.
- LOZANO, M.
- LUKIC, S.
- MARGANIEC, J.
- MARQUES, L.
- MARRONE, S.
- MASTINU, P.
- MENGONI, A.
- MILAZZO, P.M.
- MOREAU, C.
- MOSCONI, M.
- NEVES, F.
- OBERHUMMER, H.
- O'BRIEN, S.
- OSHIMA, M.
- PANCIN, J.
- PAPACHRISTODOULOU, C.
- PAPADOPOULOS, C.T.
- PARADELA, C.
- PATRONIS, N.
- PAVLIK, A.
- PAVLOPOULOS, P.
- PERROT, L.
- PLAG, R.
- PLOMPEN, A.
- PLUKIS, A.
- POCH, A.
- PRETEL, C.
- QUESADA, J.
- RAUSCHER, T.
- REIFARTH, R.
- ROSETTI, M.
- RUBBIA, C.
- RUDOLF, G.
- RULLHUSEN, P.
- SALGADO, J.
- SARCHIAPONE, L.
- SAVVIDIS, I.
- STEPHAN, C.
- TAGLIENTE, G.
- L. TAIN, J.
- TASSAN-GOT, L.
- TAVORA, L.
- DILLMANN, I.
- VANNINI, G.
- VAZ, P.
- VENTURA, A.
- VILLAMARIN, D.
- VINCENTE, M.C.
- VLACHOUDIS, V.
- VLASTOU, R.
- VOSS, F.
- WALTER, S.
- WENDLER, H.
- WIESCHER, M.
- WISSHAK, K.
DOIAbstract
The capture cross section of the 139La has been measured relative to 197Au standard at n_TOF. We provide here a short description of the experimental apparatus and of the data analysis procedures. The extracted resonance parameters allow to calculate the fundamental nuclear quantities such as average spacing $\langleD\rangle$ 1=0 = 268 ± 22 eV, $\langleD\rangle$ 1=1 < 250 eV neutron strength functions S0 = (0.79 ± 0.03)×10-4, and S1 = (0.73 ± 0.05)×10-4 and the Maxwellian-averaged capture cross section (MACS). The MACS is particularly useful for the determination of the abundance synthesized by the main component of the s proces
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