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NSR database version of May 24, 2024.

Search: Author = B.Fernandez

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2021GO11      Eur.Phys.J.Plus 136, 273 (2021)

J.Gomez-Camacho, J.Garcia-Lopez, C.Guerrero, J.M.Lopez-Gutierrez, R.Garcia-Tenorio, F.J.Santos-Arevalo, E.Chamizo, F.J.Ferrer, M.C.Jimenez-Ramos, M.Balcerzyk, B.Fernandez

Research facilities and highlights at the Centro Nacional de Aceleradores (CNA)

doi: 10.1140/epjp/s13360-021-01253-x
Citations: PlumX Metrics


2019BA45      Phys.Rev. C 100, 051302 (2019)

S.Bailey, T.Kokalova, M.Freer, C.Wheldon, R.Smith, J.Walshe, N.Curtis, N.Soic, L.Prepolec, V.Tokic, F.M.Marques, L.Achouri, F.Delaunay, Q.Deshayes, M.Parlog, B.Fernandez-Dominguez, B.Jacquot, A.Soylu

Extracting the spectral signature of α clustering in 44, 48, 52Ti using a continuous wavelet transform

NUCLEAR REACTIONS 4He(40Ca, α)44Ti*, E=180 MeV; 4He(44Ca, α)48Ti*, E=207 MeV; 4He(48Ca, α)52Ti*, E=234 MeV; measured scattered α particles, Eα, Iα, differential σ using double-sided silicon strip detectors at the GANIL radioactive beam facility; deduced continuous wavelet transform (CWT) of the measured spectra, and compared with simulated spectra using the simplified R matrix for spinless particles. 44Ti; deduced high-lying α-clustered levels J, π and compared with previous measurements. Present technique combined thick target inverse kinematics (TTIK) approach and the resonant scattering measurements with the continuous wavelet transform (CWT).

doi: 10.1103/PhysRevC.100.051302
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Data from this article have been entered in the XUNDL database. For more information, click here.


2019CH20      Phys.Rev. C 99, 054628 (2019)

A.Chatillon, J.Taieb, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, J.Benlliure, G.Boutoux, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, T.Gorbinet, L.Grente, A.Heinz, H.T.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, J.-F.Martin, C.Nociforo, C.Paradela, E.Pellereau, S.Pietri, A.Prochazka, J.L.Rodriguez-Sanchez, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Experimental study of nuclear fission along the thorium isotopic chain: From asymmetric to symmetric fission

NUCLEAR REACTIONS 208Pb, 238U(219Ac, F), (220Ac, F), (223Ac, F), (227Ac, F), (221Th, F), (222Th, F), (223Th, F), (225Th, F), (226Th, F), (229Th, F), (230Th, F), (228Pa, F), (229Pa, F), (219Ac, F), (220Ac, F), (223Ac, F), (227Ac, F), (221Th, F), (222Th, F), (223Th, F), (225Th, F), (226Th, F), (229Th, F), (230Th, F), (228Pa, F), (229Pa, F), E=551.7-568.9 MeV/nucleon, [secondary Ac and Th beams from 9Be(238U, X), E=1 GeV/nucleon primary reaction, and using FRS separator at GSI facility for separation of reaction products]; measured fission fragments, (fragment)(fragment)-coin, Coulomb excitation induced fission σ, differential Coulomb excitation σ(θ), electromagnetic-induced fission yields, mass and charge distribution of fission fragments, isotonic and isobaric fission yields using the Reactions with Relativistic Radioactive Beams/Studies On FIssion with Aladin (R3B/SOFIA) apparatus at GSI accelerator facility. Comparison with local even-odd staggering, previous measurements using either the same reaction mechanism and/or thermal-neutron induced fission.

doi: 10.1103/PhysRevC.99.054628
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0074.


2019RA23      Phys.Rev.Lett. 123, 092503 (2019)

D.Ramos, M.Caamano, A.Lemasson, M.Rejmund, L.Audouin, H.Alvarez-Pol, J.D.Frankland, B.Fernandez-Dominguez, E.Galiana-Baldo, J.Piot, D.Ackermann, S.Biswas, E.Clement, D.Durand, F.Farget, M.O.Fregeau, D.Galaviz, A.Heinz, A.I.Henriques, B.Jacquot, B.Jurado, Y.H.Kim, P.Morfouace, D.Ralet, T.Roger, C.Schmitt, P.Teubig, I.Tsekhanovich

First Direct Measurement of Isotopic Fission-Fragment Yields of 239U

NUCLEAR REACTIONS 9Be(238U, 8Be)239U, E=5.88 MeV/nucleon; measured fission products, Eα, Iα; deduced isotopic fission yields of 239U.

doi: 10.1103/PhysRevLett.123.092503
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2464.


2018FE05      Phys.Lett. B 779, 124 (2018)

B.Fernandez-Dominguez, B.Pietras, W.N.Catford, N.A.Orr, M.Petri, M.Chartier, S.Paschalis, N.Patterson, J.S.Thomas, M.Caamano, T.Otsuka, A.Poves, N.Tsunoda, N.L.Achouri, J.-C.Angelique, N.I.Ashwood, A.Banu, B.Bastin, R.Borcea, J.Brown, F.Delaunay, S.Franchoo, M.Freer, L.Gaudefroy, S.Heil, M.Labiche, B.Laurent, R.C.Lemmon, A.O.Macchiavelli, F.Negoita, E.S.Paul, C.Rodriguez-Tajes, P.Roussel-Chomaz, M.Staniou, M.J.Taylor, L.Trache, G.L.Wilson

Re-examining the transition into the N = 20 island of inversion: Structure of 30Mg

NUCLEAR REACTIONS C(31Mg, n)30Mg, E=55.1 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, single-particle σ, spectroscopic factors. Comparison with shell model calculations.

doi: 10.1016/j.physletb.2018.02.002
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0931. Data from this article have been entered in the XUNDL database. For more information, click here.


2018RA07      Phys.Rev. C 97, 054612 (2018)

D.Ramos, M.Caamano, F.Farget, C.Rodriguez-Tajes, L.Audouin, J.Benlliure, E.Casarejos, E.Clement, D.Cortina, O.Delaune, X.Derkx, A.Dijon, D.Dore, B.Fernandez-Dominguez, G.de France, A.Heinz, B.Jacquot, A.Navin, C.Paradela, M.Rejmund, T.Roger, M.-D.Salsac, C.Schmitt

Isotopic fission-fragment distributions of 238U, 239Np, 240Pu, 244Cm, and 250Cf, produced through inelastic scattering, transfer, and fusion reactions in inverse kinematics

NUCLEAR REACTIONS 12C(238U, 238U), (238U, 238U'), (238U, 239Np), (238U, 240Pu), (238U, 244Cm), (238U, 250Cf), E=6.14 MeV/nucleon; measured target-like recoil nuclei from 1H to 16O, and transfer-fission channels, Eγ, fission fragment distributions of A=80-160 from fission of 238U, 239Np, 240Pu, 244Cm, and 250Cf, azimuthal angular distribution of the fragments using VAMOS spectrometer for detection of fission fragments, SPIDER telescope for detection of target-like recoils and fissioning systems, and EXOGAM array for detection of prompt γ rays at GANIL facility; deduced isotopic distribution of recoil nuclei, excitation energies of fissioning systems, mass, Z=31-66 isotopic and elemental yield distributions of fission fragments. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.97.054612
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2400.


2018TA08      Eur.Phys.J. A 54, 66 (2018)

O.B.Tarasov, O.Delaune, F.Farget, D.J.Morrissey, A.M.Amthor, B.Bastin, D.Bazin, B.Blank, L.Caceres, A.Chbihi, B.Fernandez-Dominguez, S.Grevy, O.Kamalou, S.M.Lukyanov, W.Mittig, J.Pereira, L.Perrot, M.-G.Saint-Laurent, H.Savajols, B.M.Sherrill, C.Stodel, J.C.Thomas, A.C.Villari

Fission fragment yields from heavy-ion-induced reactions measured with a fragment separator

NUCLEAR REACTIONS 9Be, 12C(238U, x), E=20, 24 MeV/nucleon; measured Eγ, Iγ, γγ-coin, (heavy fragment)γ-coin. 96Zr, 120Sn; deduced fragments charge distribution, σ vs charge and vs mass; calculated partial σ vs angular momentum for different participating processes, CN formation σ vs projectile energy for E=4-100 MeV/nucleon using LISE++ code, fusion-fission Rh fragment reduced yield vs Rh mass for different beam energies.

doi: 10.1140/epja/i2018-12500-0
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2018VA09      Phys.Rev. C 98, 011302 (2018)

J.J.Valiente-Dobon, A.Poves, A.Gadea, B.Fernandez-Dominguez

Broken mirror symmetry in 36S and 36Ca

NUCLEAR STRUCTURE 36Ca, 36S; 38Ca, 38Ar; 34Ca, 34Si; 32Ca, 32Mg; calculated low lying levels, J, π, mirror energy difference (MED) between mirror nuclei. 36Ca; predicted first excited 0+ state at 2.7 MeV, 250 keV below the first 2+ state, B(E2) for the first 2+ state, and ρ2(E0). Shell model with configuration interaction, using sdpfu-mix effective interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.98.011302
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2017GI03      Phys.Rev. C 95, 035806 (2017)

S.Giron, F.Hammache, N.de Sereville, P.Roussel, J.Burgunder, M.Moukaddam, D.Beaumel, L.Caceres, G.Duchene, E.Clement, B.Fernandez-Dominguez, F.Flavigny, G.de France, S.Franchoo, D.Galaviz-Redondo, L.Gasques, J.Gibelin, A.Gillibert, S.Grevy, J.Guillot, M.Heil, J.Kiener, V.Lapoux, F.Marechal, A.Matta, I.Matea, L.Nalpas, J.Pancin, L.Perrot, A.Obertelli, R.Raabe, J.A.Scarpaci, K.Sieja, O.Sorlin, I.Stefan, C.Stodel, M.Takechi, J.C.Thomas, Y.Togano

Spectroscopy of 61Fe via the neutron transfer reaction 2H(60Fe, p)61Fe

NUCLEAR REACTIONS 2H(60Fe, p), E=27 MeV/nucleon, [60Fe secondary beam from 9Be(64Ni, X), E=64.5 MeV/nucleon primary reaction using LISE3 at GANIL]; Measured E(p), proton σ(θ), Eγ, Iγ, pγ-coin using a DSSSD detector and four telescopes of MUST2 array and four segmented Clover detectors from EXOGAM array. 61Fe; deduced levels, l-transfers, J, π, spectroscopic factors. ADWA analysis. Comparison with shell model calculations. 60Fe(n, γ)61Fe; deduced direct component of capture cross section through the (d, p) transfer reaction in inverse kinematics.

doi: 10.1103/PhysRevC.95.035806
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2405. Data from this article have been entered in the XUNDL database. For more information, click here.


2017PA10      Phys.Rev. C 95, 044606 (2017)

C.Paradela, L.Tassan-Got, J.Benlliure, J.L.Rodriguez-Sanchez, L.Audouin, A.Boudard, E.Casarejos, T.Enqvist, J.E.Ducret, F.Farget, B.Fernandez-Dominguez, M.Fernandez-Ordonez, L.Giot, A.Heinz, V.Henzl, D.Henzlova, A.Kelic-Heil, A.Lafriaskh, S.Leray, P.Napolitani, J.Pereira, D.Perez-Loureiro, M.V.Ricciardi, C.Stephan, K.-H.Schmidt, C.Schmitt, C.Villagrasa, C.Volant, O.Yordanov

Isotopic production cross sections of residual nuclei in the spallation reaction 136Xe (200A MeV) + p

NUCLEAR REACTIONS 1H(136Xe, X)115Cd/116Cd/115In/116In/117In/118In/119In/120In/115Sn/116Sn/117Sn/118Sn/119Sn/120Sn/121Sn/122Sn/123Sn/115Sb/116Sb/117Sb/118Sb/119Sb/120Sb/121Sb/122Sb/123Sb/124Sb/125Sb/126Sb/127Sb/128Sb/117Te/118Te/119Te/120Te/121Te/122Te/123Te/124Te/125Te/126Te/127Te/128Te/129Te/130Te/131Te/132Te/119I/120I/121I/122I/123I/124I/125I/126I/127I/128I/129I/130I/131I/132I/133I/134I/135I/120Xe/121Xe/122Xe/123Xe/124Xe/125Xe/126Xe/127Xe/128Xe/129Xe/130Xe/131Xe/132Xe/133Xe/134Xe/135Xe/121Cs/122Cs/123Cs/124Cs/125Cs/126Cs/127Cs/128Cs/129Cs/130Cs/131Cs/132Cs/133Cs/134Cs/135Cs/136Cs, E=200 MeV/nucleon; measured charge distribution, energy loss and isotopic σ(A, Z) and isobaric σ(A) of the fragments using the FRS separator and multisampling ionization chambers (MUSICs) at GSI; deduced correlation plot between atomic number (Z) and mass-over-charge ratio (A/Z), identification plot, correlation between the mass identification in the two FRS sections, momentum distribution of the 125Xe. Comparison with theoretical predictions using INCL4.6 and ISABEL codes coupled to the deexcitation code ABLA07.

doi: 10.1103/PhysRevC.95.044606
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2407.


2017PE08      Phys.Rev. C 95, 054603 (2017)

E.Pellereau, J.Taieb, A.Chatillon, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, J.Benlliure, G.Boutoux, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, T.Gorbinet, L.Grente, A.Heinz, H.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, J.-F.Martin, C.Nociforo, C.Paradela, S.Pietri, J.L.Rodriguez-Sanchez, K.-H.Schmidt, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Accurate isotopic fission yields of electromagnetically induced fission of 238U measured in inverse kinematics at relativistic energies

NUCLEAR REACTIONS 238U(238U, F), E=650 MeV/nucleon; measured mass and charge coincidences, elemental, isobaric and isotopic yields and mass distribution of fission fragments of Z=29-62, N=43-95, A=71-156 in 238U(γ, F) using the SOFIA experimental setup and around the ALADIN magnet at GSI. Comparison with the GEF model calculations, and with 238U(n, F) data in ENDF-BVII.1 and JEFF.3.1.

doi: 10.1103/PhysRevC.95.054603
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0077.


2017RO01      Nucl.Phys. A958, 246 (2017)

C.Rodriguez-Tajes, F.Farget, L.Acosta, H.Alvarez-Pol, M.Babo, F.Boulay, M.Caamano, S.Damoy, B.Fernandez-Dominguez, D.Galaviz, G.F.Grinyer, J.Grinyer, M.N.Harakeh, P.Konczykowski, I.Martel, J.Pancin, G.Randisi, F.Renzi, T.Roger, A.M.Sanchez-Benitez, P.Teubig, M.Vandebrouck

First inverse-kinematics fission measurements in a gaseous active target

NUCLEAR REACTIONS 12C(238U, F), E=6.55 MeV/nucleon; measured transfer-induced fission, neutron-rich actinides between U and Cm using active target MAYA with eight DSSSDs; deduced complete three-dimensional trajectory reconstruction, TKEL vs θ, excitation energy distribution, E* vs E(cm), σ(fusion) to σ(transfer-fusion) ratio.

doi: 10.1016/j.nuclphysa.2016.12.003
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2016WA29      Phys.Rev. C 94, 054304 (2016)

J.Walshe, M.Freer, C.Wheldon, A.Soylu, N.L.Achouri, N.I.Ashwood, W.N.Catford, I.C.Celik, N.Curtis, F.Delaunay, B.Fernandez-Dominguez, L.Grassi, Tz.Kokalova, F.M.Marques, N.A.Orr, L.Prepolec, V.Scuderi, N.Soic, V.Tokic

Experimental study of high-lying states in 28Mg using the resonant elastic scattering of α particles

NUCLEAR REACTIONS 4He(24Ne, α), E=3.8 MeV/nucleon, [24Ne secondary beam from C(26Mg, X), E=E=82 MeV/nucleon at GANIL facility]; measured Eα, Iα, σ(Eα, θ) using thick target in inverse kinematics (TTIK) technique. 28Mg; deduced levels, resonances, J, π, α and total widths, ratio of reduced width to the Wigner limit. R-Matrix analysis using AZURE2 code. Comparisons with theoretical calculations of widths using the code GAMOW.

doi: 10.1103/PhysRevC.94.054304
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2366. Data from this article have been entered in the XUNDL database. For more information, click here.


2015BA52      Phys.Lett. B 751, 371 (2015)

S.Bagchi, J.Gibelin, M.N.Harakeh, N.Kalantar-Nayestanaki, N.L.Achouri, H.Akimune, B.Bastin, K.Boretzky, H.Bouzomita, M.Caamano, L.Caceres, S.Damoy, F.Delaunay, B.Fernandez-Dominguez, M.Fujiwara, U.Garg, G.F.Grinyer, O.Kamalou, E.Khan, A.Krasznahorkay, G.Lhoutellier, J.F.Libin, S.Lukyanov, K.Mazurek, M.A.Najafi, J.Pancin, Y.Penionzhkevich, L.Perrot, R.Raabe, C.Rigollet, T.Roger, S.Sambi, H.Savajols, M.Senoville, C.Stodel, L.Suen, J.C.Thomas, M.Vandebrouck

Observation of isoscalar multipole strengths in exotic doubly-magic 56Ni in inelastic α scattering in inverse kinematics

NUCLEAR REACTIONS 4He(56Ni, α), E=50 MeV/nucleon; measured reaction products, Eα, Iα; deduced inelastic σ(θ), Isoscalar Giant Monopole Resonance (ISGMR) and the Isoscalar Giant Dipole Resonance (ISGDR) strength functions.

doi: 10.1016/j.physletb.2015.10.060
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2320. Data from this article have been entered in the XUNDL database. For more information, click here.


2015CA21      Phys.Rev. C 92, 034606 (2015)

M.Caamano, F.Farget, O.Delaune, K.-H.Schmidt, C.Schmitt, L.Audouin, C.-O.Bacri, J.Benlliure, E.Casarejos, X.Derkx, B.Fernandez-Dominguez, L.Gaudefroy, C.Golabek, B.Jurado, A.Lemasson, D.Ramos, C.Rodriguez-Tajes, T.Roger, A.Shrivastava

Characterization of the scission point from fission-fragment velocities

RADIOACTIVITY 240Pu(SF)[from 12C(238U, 10Be), E=6.1 MeV/nucleon]; 250Cf(SF)[from 12C(238U, X)250Cf*, E=6.1 MeV/nucleon]; measured fragment spectra using VAMOS spectrometer at GANIL; deduced velocity of fission fragments with Z=34-62 as a function of the neutron number of the fragment (N=45-100), average fragment velocity, average neutron excess of fragments, neutron multiplicity and total neutron evaporation multiplicity, total kinetic energy of fission fragments, total excitation energy at scission, post-neutron evaporation normalized yields, average difference between the ground states of the fissioning system and the fragments, and minimum energy released in neutron evaporation as functions of the fragment atomic number. Modeling of the fission process through correlated observables.

doi: 10.1103/PhysRevC.92.034606
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2160.


2015FA14      Eur.Phys.J. A 51, 175 (2015)

F.Farget, M.Caamano, D.Ramos, C.Rodriguez-Tajes, K.-H.Schmidt, L.Audouin, J.Benlliure, E.Casarejos, E.Clement, D.Cortina, O.Delaune, X.Derkx, A.Dijon, D.Dore, B.Fernandez-Dominguez, L.Gaudefroy, C.Golabek, A.Heinz, B.Jurado, A.Lemasson, C.Paradela, T.Roger, M.D.Salsac, C.Schmitt

Transfer-induced fission in inverse kinematics: Impact on experimental and evaluated nuclear data bases

doi: 10.1140/epja/i2015-15175-y
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2015FE02      Phys.Rev. C 91, 024307 (2015)

B.Fernandez-Dominguez, X.Pereira-Lopez, N.K.Timofeyuk, P.Descouvemont, W.N.Catford, F.Delaunay

Spectroscopic study of the exotic nucleus 25P

NUCLEAR STRUCTURE 25P, 25Ne; calculated levels, J, π, spectroscopic factors, ANCs from (d, p) transfer, partial gamma and proton widths. Proposed possible experiments to investigate levels in unbound 25P nucleus, and searches of the mirror analog of the island of inversion near N=16. Shell model, a potential model, and a microscopic-cluster model. Comparison with experimental data for 25Ne.

doi: 10.1103/PhysRevC.91.024307
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2015MA70      Eur.Phys.J. A 51, 174 (2015)

J.-F.Martin, J.Taieb, A.Chatillon, G.Belier, G.Boutoux, A.Ebran, T.Gorbinet, L.Grente, B.Laurent, E.Pellereau, H.Alvarez-Pol, L.Audouin, T.Aumann, Y.Ayyad, J.Benlliure, E.Casarejos, D.Cortina Gil, M.Caamano, F.Farget, B.Fernandez-Dominguez, A.Heinz, B.Jurado, A.Kelic-Heil, N.Kurz, C.Nociforo, C.Paradela, S.Pietri, D.Ramos, J.-L.Rodriguez-Sanchez, C.Rodriguez-Tajes, D.Rossi, K.-H.Schmidt, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Studies on fission with ALADIN - Precise and simultaneous measurement of fission yields, total kinetic energy and total prompt neutron multiplicity at GSI

doi: 10.1140/epja/i2015-15174-0
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2015MO22      Phys.Lett. B 751, 306 (2015)

P.Morfouace, S.Franchoo, K.Sieja, I.Matea, L.Nalpas, M.Niikura, A.M.Sanchez-Benitez, I.Stefan, M.Assie, F.Azaiez, D.Beaumel, S.Boissinot, C.Borcea, R.Borcea, G.Burgunder, L.Caceres, N.De Sereville, Zs.Dombradi, J.Elseviers, B.Fernandez-Dominguez, A.Gillibert, S.Giron, S.Grevy, F.Hammache, O.Kamalou, V.Lapoux, L.Lefebvre, A.Lepailleur, C.Louchart, G.Marquinez-Duran, I.Martel, A.Matta, D.Mengoni, D.R.Napoli, F.Recchia, J.-A.Scarpaci, D.Sohler, O.Sorlin, M.Stanoiu

Evolution of single-particle strength in neutron-rich 71Cu

NUCLEAR REACTIONS 2H(72Zn, 3He)71Cu, E=38 MeV/nucleon; measured reaction products; deduced strength functions, spectroscopic factors. Distorted-Wave Born Approximation (DWBA) using the DWUCK5 code calculations.

doi: 10.1016/j.physletb.2015.10.064
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Data from this article have been entered in the XUNDL database. For more information, click here.


2015RA03      Acta Phys.Pol. B46, 443 (2015)

D.Ramos, C.Rodriguez-Tajes, M.Caamano, F.Farget, L.Audouin, J.Benlliure, E.Casarejos, E.Clement, D.Cortina, O.Delaune, X.Derkx, A.Dijon, D.Dore, B.Fernandez-Dominguez, G.de France, A.Heinz, B.Jacquot, A.Navin, C.Paradela, M.Rejmund, T.Roger, M.D.Salsac, C.Schmitt

Fission Yields of Minor Actinides at Low Energy Through Multi-nucleon Transfer Reactions of 238U on 12C

NUCLEAR REACTIONS C(238U, F), E=6.1 MeV/nucleon; measured fission products; deduced yields.

doi: 10.5506/APhysPolB.46.443
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2400.


2015SA11      Eur.Phys.J. A 51, 25 (2015)

S.Sambi, R.Raabe, M.J.G.Borge, M.Caamano, S.Damoy, B.Fernandez-Dominguez, F.Flavigny, H.Fynbo, J.Gibelin, G.F.Grinyer, A.Heinz, B.Jonson, M.Khodery, T.Nilsson, R.Orlandi, J.Pancin, D.Perez-Loureiro, G.Randisi, G.Ribeiro, T.Roger, D.Suzuki, O.Tengblad, R.Thies, U.Datta

12C+p resonant elastic scattering in the Maya active target

NUCLEAR REACTIONS 1H(12C, 12C), E(cm)=0.3-3.0 MeV (above proton breakup threshold in 13N); measured recoil Ep, Ip(θ) using active target Maya; deduced proton spectra, resonances.

doi: 10.1140/epja/i2015-15025-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2273. Data from this article have been entered in the XUNDL database. For more information, click here.


2015VA13      Phys.Rev. C 92, 024316 (2015)

M.Vandebrouck, J.Gibelin, E.Khan, N.L.Achouri, H.Baba, D.Beaumel, Y.Blumenfeld, M.Caamano, L.Caceres, G.Colo, F.Delaunay, B.Fernandez-Dominguez, U.Garg, G.F.Grinyer, M.N.Harakeh, N.Kalantar-Nayestanaki, N.Keeley, W.Mittig, J.Pancin, R.Raabe, T.Roger, P.Roussel-Chomaz, H.Savajols, O.Sorlin, C.Stodel, D.Suzuki, J.C.Thomas

Isoscalar response of 68Ni to α-particle and deuteron probes

NUCLEAR REACTIONS 2H(68Ni, d'), 4He(68Ni, α'), E=50 MeV/nucleon, [68Ni secondary beam from 9Be(70Zn, X), E=62.3 MeV/nucleon primary reaction, and using LISE3 separator at GANIL]; measured scattered particle spectra of recoiling ions, α and deuterons using active target MAYA which is a time projection chamber (TPC). 68Ni; deduced excitation-energy spectrum, angular distributions, L transfers, centroids of isoscalar giant monopole resonances (ISGMR and soft ISGMR), isoscalar giant dipole resonances (ISGDR) and isoscalar giant quadrupole resonance (ISGQR), proton distribution coming from deuteron breakup on 68Ni. Calculated angular distributions for 68Ni(d, d') and 68Ni(α, α') by DWBA approach. Discussed systematics of isoscalar giant resonances for 56,58,60,62,64,68Ni.

doi: 10.1103/PhysRevC.92.024316
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2014BU01      Phys.Rev.Lett. 112, 042502 (2014)

G.Burgunder, O.Sorlin, F.Nowacki, S.Giron, F.Hammache, M.Moukaddam, N.de Sereville, D.Beaumel, L.Caceres, E.clement, G.Duchene, J.P.Ebran, B.Fernandez-Dominguez, F.Flavigny, S.Franchoo, J.Gibelin, A.Gillibert, S.Grevy, J.Guillot, A.Lepailleur, I.Matea, A.Matta, L.Nalpas, A.Obertelli, T.Otsuka, J.Pancin, A.Poves, R.Raabe, J.A.Scarpaci, I.Stefan, C.Stodel, T.Suzuki, J.C.Thomas

Experimental Study of the Two-Body Spin-Orbit Force in Nuclei

NUCLEAR REACTIONS 2H(34Si, p), E=20.5 MeV/nucleon; 2H(36S, p), E=19 MeV/nucleon; measured reaction products, Ep, Ip; deduced σ(θ), level energies, spectroscopic factors, reduction of spin-orbit splitting, two-body spin-orbit interaction. Comparison with strength calculations for N3LO and KLS nucleon-nucleon forces.

doi: 10.1103/PhysRevLett.112.042502
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2014RO05      Phys.Rev. C 89, 024614 (2014)

C.Rodriguez-Tajes, F.Farget, X.Derkx, M.Caamano, O.Delaune, K.-H.Schmidt, E.Clement, A.Dijon, A.Heinz, T.Roger, L.Audouin, J.Benlliure, E.Casarejos, D.Cortina, D.Dore, B.Fernandez-Dominguez, B.Jacquot, B.Jurado, A.Navin, C.Paradela, D.Ramos, P.Romain, M.D.Salsac, C.Schmitt

Transfer reactions in inverse kinematics: An experimental approach for fission investigations

NUCLEAR REACTIONS 12C(238U, 238U), (238U, 238U'), (238U, 237U)13C, (238U, 236U)14C, (238U, 239Np)11B, (238U, 240Pu)10Be, (238U, 241Pu)9Be, (238U, 242Pu)8Be, (238U, 243Am)7Li, (238U, 244Cm)6He, (238U, 246Cm)4He, E=6.14 MeV/nucleon; measured particle spectra, (particle)(fission fragment)-coin and (particle)(fission fragment)-anticoin, integral σ, σ(θ), total excitation-energy distributions, optimal Q values, Eγ, Iγ, (particle)γ-coin using VAMOS spectrometer, SPIDER array for particle detection, and EXOGAM array for γ rays at GANIL CSS1 cyclotron facility; deduced transfer induced fission probabilities for 238U, 239Np, 240,241,242Pu, 244Cm by surrogate-reaction technique. 12C, 11B, 10Be; deduced first excited level, probabilities of γ-ray emission from the first excited state. Comparison with other experimental data, and with TALYS calculations of neutron-induced fission probabilities.

doi: 10.1103/PhysRevC.89.024614
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2014VA07      Phys.Rev.Lett. 113, 032504 (2014)

M.Vandebrouck, J.Gibelin, E.Khan, N.L.Achouri, H.Baba, D.Beaumel, Y.Blumenfeld, M.Caamano, L.Caceres, G.Colo, F.Delaunay, B.Fernandez-Dominguez, U.Garg, G.F.Grinyer, M.N.Harakeh, N.Kalantar-Nayestanaki, N.Keeley, W.Mittig, J.Pancin, R.Raabe, T.Roger, P.Roussel-Chomaz, H.Savajols, O.Sorlin, C.Stodel, D.Suzuki, J.C.Thomas

Measurement of the Isoscalar Monopole Response in the Neutron-Rich Nucleus 68Ni

NUCLEAR REACTIONS 4He(68Ni, α), E=50 MeV/nucleon; measured reaction products, Eα, Iα. 68Ni; deduced σ(θ), isoscalar monopole strength. DWBA and RPA transition densities analysis.

doi: 10.1103/PhysRevLett.113.032504
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2013AL14      Phys.Rev. C 88, 034301 (2013)

T.Al Kalanee, J.Gibelin, P.Roussel-Chomaz, N.Keeley, D.Beaumel, Y.Blumenfeld, B.Fernandez-Dominguez, C.Force, L.Gaudefroy, A.Gillibert, J.Guillot, H.Iwasaki, S.Krupko, V.Lapoux, W.Mittig, X.Mougeot, L.Nalpas, E.Pollacco, K.Rusek, T.Roger, H.Savajols, N.de Sereville, S.Sidorchuk, D.Suzuki, I.Strojek, N.A.Orr

Structure of unbound neutron-rich 9He studied using single-neutron transfer

NUCLEAR REACTIONS 2H(8He, p), E=15 MeV/nucleon, [secondary 8He beam from C(13C, X), E=75 MeV/nucleon primary reaction]; 2H(16O, p), E=15 MeV/nucleon; measured proton spectra, kinetic energies and angles of recoiling protons, σ(θ) using MUST2 telescopes of Si-CsI detectors at GANIL facility. 9He, 17O; deduced levels from experimental missing mass spectra, J, π, widths, l-transfers, configurations, spectroscopic factors, parity inversion in 9He. DWBA and CCBA analyses of σ(θ) data. Reviewed previous measurements of level structure of 9He using different reactions. 16O(d, p) reaction in inverse kinematics used as a test case.

doi: 10.1103/PhysRevC.88.034301
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2013CA16      Phys.Rev. C 88, 024605 (2013); Erratum Phys.Rev. C 89, 069903 (2014)

M.Caamano, O.Delaune, F.Farget, X.Derkx, K.-H.Schmidt, L.Audouin, C.-O.Bacri, G.Barreau, J.Benlliure, E.Casarejos, A.Chbihi, B.Fernandez-Dominguez, L.Gaudefroy, C.Golabek, B.Jurado, A.Lemasson, A.Navin, M.Rejmund, T.Roger, A.Shrivastava, C.Schmitt

Isotopic yield distributions of transfer- and fusion-induced fission from 238U+12C reactions in inverse kinematics

NUCLEAR REACTIONS 12C(238U, F)240Pu/241Pu/250Cf*, E=6.1 MeV/nucleon; measured particle and γ spectra, (fragment)γ-coin, energy loss, time-of-flight, yields and angular distributions of fragments of Z=30-64, A=80-160 from fission of 250Cf, 240,241Pu using SPIDER, VAMOS, and EXOGAM detector systems at GANIL facility. Inverse kinematics and multi-nucleon transfer-induced fission. 110Ru, 144Ce; deduced levels from (fragment)γ coin spectra. Z=30, A=70-82, 85; Z=31, A=70-85; Z=32, A=71-87; Z=33, A=73-89; Z=34, A=73, 75-90; Z=35, A=79-93; Z=36, A=81-96; Z=37, A=83-99; Z=38, A=86-102; Z=39, A=88-105; Z=40, A=90-107; Z=41, A=93-110; Z=42, A=95-113; Z=43, A=97-115; Z=44, A=100-118; Z=45, A=102-120; Z=46, A=104-122; Z=47, A=107-126; Z=48, A=109-127; Z=49, A=112-131; Z=50, A=114-133; Z=51, A=116-135; Z=52, A=118-138; Z=53, A=122-141; Z=54, A=123-143; Z=55, A=126-146; Z=56, A=130-148; Z=57, A=131-150; Z=58, A=134-152; Z=59, A=137-153; Z=60, A=139-156; Z=61, A=142-158; Z=62, A=144-159; Z=63, A=149-160; Z=64, A=151-159; measured yields from fission of compound nucleus 250Cf. Z=34, A=82-88; Z=35, A=85-92; Z=36, A=85-94; Z=37, A=87-97; Z=38, A=90-101; Z=39, A=91-102; Z=40, A=94-106; Z=41, A=95-109; Z=42, A=98-111; Z=43, A=101-112; Z=44, A=104-114; Z=45, A=105-114; Z=46, A=110-116; Z=47, A=114-119; Z=48, A=115, 118-122; Z=49, A=122-130; Z=50, A=125-134, 136; Z=51, A=125-137; Z=52, A=129-139; Z=53, A=128-140; Z=54, A=130-144; Z=55, A=133-145; Z=56, A=134-145; Z=57, A=138-149; Z=58, A=142-151; Z=59, A=145-152; Z=60, A=148-154; measured yields from fission of multi-nucleon transfer induced nuclei 240,241Pu.

doi: 10.1103/PhysRevC.88.024605
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2013CR04      Phys.Rev. C 88, 044616 (2013)

E.Crema, M.A.G.Alvarez, N.H.Medina, L.R.Gasques, J.F.P.Huiza, B.Fernandez, Z.Abou-Haidar, P.N.de Faria, P.R.S.Gomes, J.Lubian, D.Verney

Quasi-elastic processes of the 48Ca+120Sn system and the 48Ca nuclear matter density

NUCLEAR REACTIONS 120Sn(48Ca, 48Ca'), E=152-175 MeV; measured particle spectra, σ(E) at Orsay tandem accelerator facility; deduced quasi-elastic barrier distributions. Large-scale coupled-channel analysis. Role of pairing correlation in 2n-neutron transfer process.

doi: 10.1103/PhysRevC.88.044616
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2013GI02      Nucl.Phys. A899, 116 (2013)

L.Giot, J.A.Alcantara-Nunez, J.Benlliure, D.Perez-Loureiro, L.Audouin, A.Boudard, E.Casarejos, T.Enqvist, J.E.Ducret, B.Fernandez-Dominguez, M.Fernandez-Ordonez, F.Farget, A.Heinz, V.Henzl, D.Henzlova, A.Kelic-Heil, A.Lafriaskh, S.Leray, P.Napolitani, C.Paradela, J.Pereira, M.V.Ricciardi, C.Stephan, K.-H.Schmidt, C.Schmitt, L.Tassan-Got, C.Villagrasa, C.Volant, O.Yordanov

Isotopic production cross sections of the residual nuclei in spallation reactions induced by 136Xe projectiles on proton at 500 A MeV

NUCLEAR REACTIONS 1H(136Xe, X), E=500 MeV/nucleon; measured spallation products mass, charge distribution using FRS magnetic spectrometer; deduced fragment isotopes yields, production σ, longitudinal momentum distributions. Compared with published data at 1000 MeV/nucleon.

doi: 10.1016/j.nuclphysa.2012.12.119
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2013HA39      Phys.Rev. C 88, 062802 (2013)

F.Hammache, A.Coc, N.de Sereville, I.Stefan, P.Roussel, S.Ancelin, M.Assie, L.Audouin, D.Beaumel, S.Franchoo, B.Fernandez-Dominguez, S.Fox, C.Hamadache, J.Kiener, A.Laird, B.Le Crom, A.Lefebvre-Schuhl, L.Lefebvre, I.Matea, A.Matta, G.Mavilla, J.Mrazek, P.Morfouace, F.de Oliveira Santos, A.Parikh, L.Perrot, A.M.Sanchez-Benitez, D.Suzuki, V.Tatischeff, P.Ujic, M.Vandebrouck

Search for new resonant states in 10C and 11C and their impact on the cosmological lithium problem

NUCLEAR REACTIONS 10B(3He, t)10C, 11B(3He, t)11C, E=35 MeV; measured E(t), I(t), σ(θ), light fragments using split-pole magnetic spectrometer, proportional gas counter, and plastic scintillator at Orsay-ALTO tandem accelerator facility. 10,11C; deduced levels, resonances, widths. 12C, 12N, 16F; deduced levels from impurities. Discussed 7Li abundance and deficit Big-Bang nucleosynthesis (BBN).

doi: 10.1103/PhysRevC.88.062802
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2013RO33      Phys.Rev.Lett. 111, 242503 (2013)

D.M.Rossi, P.Adrich, F.Aksouh, H.Alvarez-Pol, T.Aumann, J.Benlliure, M.Bohmer, K.Boretzky, E.Casarejos, M.Chartier, A.Chatillon, D.Cortina-Gil, U.Datta Pramanik, H.Emling, O.Ershova, B.Fernandez-Dominguez, H.Geissel, M.Gorska, M.Heil, H.T.Johansson, A.Junghans, A.Kelic-Heil, O.Kiselev, A.Klimkiewicz, J.V.Kratz, R.Krucken, N.Kurz, M.Labiche, T.Le Bleis, R.Lemmon, Yu.A.Litvinov, K.Mahata, P.Maierbeck, A.Movsesyan, T.Nilsson, C.Nociforo, R.Palit, S.Paschalis, R.Plag, R.Reifarth, D.Savran, H.Scheit, H.Simon, K.Summerer, A.Wagner, W.Walus, H.Weick, M.Winkler

Measurement of the Dipole Polarizability of the Unstable Neutron-Rich Nucleus 68Ni

NUCLEAR REACTIONS Pb(68Ni, 68Ni'), (68Ni, X), E=502.7 MeV/nucleon; measured reaction products, Eγ, Iγ, En, In. 68Ni; deduced σ(E), giant and pygmy dipole resonance parameters, E1 strength, neutron skin thickness. Comparison with available data.

doi: 10.1103/PhysRevLett.111.242503
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2012BA46      J.Phys.:Conf.Ser. 337, 012059 (2012)

A.Banu, F.Carstoiu, W.N.Catford, B.Fernandez-Dominguez, M.Horoi, N.A.Orr, B.T.Roeder, P.Roussel-Chomaz, L.Trache, R.E.Tribble

Direct radiative proton capture 23Al(p, γ)24Si studied via one-proton nuclear breakup of 24Si

NUCLEAR REACTIONS 12C(24Si, p23Al), E=20-60 MeV/nucleon; measured Eγ, Iγ, (fragment)γ-coin, reaction products using SPEG energy-loss spectrometer; deduced 23Al momentum distribution; calculated 23Al momentum distribution using Glauber-type approach.

doi: 10.1088/1742-6596/337/1/012059
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2012BE38      J.Phys.:Conf.Ser. 337, 012070 (2012)

J.Benlliure, H.Alvarez-Pol, T.Kurtukian-Nieto, A.I.Morales, L.Audouin, F.Becker, B.Blank, I.Borzov, E.Casarejos, D.Cortina-Gil, B.Fernandez, J.Giovinazzo, D.Henzlova, B.Jurado, L.Langanke, G.Martinez-Pinedo, P.Napolitani, J.Pereira, F.Rejmund, K.-H.Schmidt, O.Yordanov, for the RISING Collaboration

Approaching r-process nuclei at N = 126

RADIOACTIVITY 194,195,196Re, 199,200Os, 198,201,202Ir, 203,204Pt, 204Au(β-); measured Iβ(t) using DSSSD; deduced T1/2; calculated T1/2 using Gross theory, FR droplet model and energy-density functional.

doi: 10.1088/1742-6596/337/1/012070
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2012BR01      Phys.Rev. C 85, 011302 (2012)

S.M.Brown, W.N.Catford, J.S.Thomas, B.Fernandez-Dominguez, N.A.Orr, M.Labiche, M.Rejmund, N.L.Achouri, H.Al Falou, N.I.Ashwood, D.Beaumel, Y.Blumenfeld, B.A.Brown, R.Chapman, M.Chartier, N.Curtis, G.de France, N.de Sereville, F.Delaunay, A.Drouart, C.Force, S.Franchoo, J.Guillot, P.Haigh, F.Hammache, V.Lapoux, R.C.Lemmon, A.Leprince, F.Marechal, X.Mougeot, B.Mouginot, L.Nalpas, A.Navin, N.P.Patterson, B.Pietras, E.C.Pollacco, A.Ramus, J.A.Scarpaci, I.Stefan, G.L.Wilson

Low-lying neutron fp-shell intruder states in 27Ne

NUCLEAR REACTIONS 2H(26Ne, p)27Ne, E=9.8 MeV/nucleon; measured Eγ, Iγ, γ(27Ne)-, d(26Ne)-, p(26Ne)-, p(27Ne)-coin, pγ(θ). 27Ne; deduced levels, J, π, L-transfer spectroscopic factors, negative-parity intruder states. SPIRAL facility at GANIL. Adiabatic distorted-wave approximation (ADWA) analysis of σ(θ) data. Comparison with shell-model calculations, N=20 shell gap. systematics of level energies of 25,27Ne, 29Mg.

doi: 10.1103/PhysRevC.85.011302
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2012GA45      Phys.Rev.Lett. 109, 202503 (2012)

L.Gaudefroy, W.Mittig, N.A.Orr, S.Varet, M.Chartier, P.Roussel-Chomaz, J.P.Ebran, B.Fernandez-Dominguez, G.Fremont, P.Gangnant, A.Gillibert, S.Grevy, J.F.Libin, V.A.Maslov, S.Paschalis, B.Pietras, Yu.-E.Penionzhkevich, C.Spitaels, A.C.C.Villari

Direct Mass Measurements of 19B, 22C, 29F, 31Ne, 34Na and Other Light Exotic Nuclei

ATOMIC MASSES 19B, 20,22C, 22,23N, 27,29F, 30,31Ne, 33,34Na, 43,44S, 45,46Cl, 47Ar; measured TOF for reaction products; deduced masses, two-neutron separation energies, matter radii, Borromean systems. Comparison with available data.

doi: 10.1103/PhysRevLett.109.202503
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2012TI03      Phys.Rev. C 86, 034305 (2012)

N.K.Timofeyuk, B.Fernandez-Dominguez, P.Descouvemont, W.N.Catford, F.Delaunay, J.S.Thomas

Core excitations and narrow states beyond the proton dripline: The exotic nucleus 21Al

NUCLEAR STRUCTURE 21Al; calculated levels, resonances, J, π, widths with respect to 20Mg+p channel and asymptotic normalization coefficients (ANC) for mirror states in 21O using multichannel and single-channel microscopic cluster model (MCM), and in two versions of the potential model. 21O; calculated levels, J, π, asymptotic normalization coefficients (ANC), spectroscopic factors using MCM; compared with experimental data for 20O(d, p)21O reaction.

doi: 10.1103/PhysRevC.86.034305
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2011BA27      Phys.Rev. C 84, 015803 (2011)

A.Banu, L.Trache, F.Carstoiu, N.L.Achouri, A.Bonaccorso, W.N.Catford, M.Chartier, M.Dimmock, B.Fernandez-Dominguez, M.Freer, L.Gaudefroy, M.Horoi, M.Labiche, B.Laurent, R.C.Lemmon, F.Negoita, N.A.Orr, S.Paschalis, N.Patterson, E.S.Paul, M.Petri, B.Pietras, B.T.Roeder, F.Rotaru, P.Roussel-Chomaz, E.Simmons, J.S.Thomas, R.E.Tribble

Structure of 23Al from the one-proton breakup reaction and astrophysical implications

NUCLEAR REACTIONS 12C(23Al, 22Mg), [23Al secondary beam from C(32S, X)E=95 MeV/nucleon primary reaction], E=57 MeV/nucleon; measured fragment spectra, inclusive and exclusive longitudinal momentum distributions, and widths, Eγ, (fragment)γ-coin. 22Mg; deduced levels, J, π, σ, spectroscopic factors, asymptotic normalization coefficients. 23Al; deduced g.s. Jπ, configuration mixing. Comparison with Glauber and large-scale shell model calculations. 22Mg(p, γ)23Al, E<1 MeV; deduced stellar reaction rates; discussed astrophysical significance of 22Na nucleosynthesis in ONe novae.

doi: 10.1103/PhysRevC.84.015803
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2011FE06      Phys.Rev. C 84, 011301 (2011); Pub.Note JOUR PRVCA 84 029902 (2011)

B.Fernandez-Dominguez, J.S.Thomas, W.N.Catford, F.Delaunay, S.M.Brown, N.A.Orr, M.Rejmund, M.Labiche, M.Chartier, N.L.Achouri, H.Al Falou, N.I.Ashwood, D.Beaumel, Y.Blumenfeld, B.A.Brown, R.Chapman, N.Curtis, C.Force, G.de France, S.Franchoo, J.Guillot, P.Haigh, F.Hammache, V.Lapoux, R.C.Lemmon, F.Marechal, A.M.Moro, X.Mougeot, B.Mouginot, L.Nalpas, A.Navin, N.Patterson, B.Pietras, E.C.Pollacco, A.Leprince, A.Ramus, J.A.Scarpaci, N.de Sereville, I.Stephan, O.Sorlin, G.L.Wilson

Emergence of the N = 16 shell gap in 21O

NUCLEAR REACTIONS 2H(20O, p), E=10.5 MeV/nucleon; measured E(p), I(p), Eγ, Iγ, σ(θ), p20O-, p20Oγ-coin. 21O; deduced levels, J, π, L-transfer, spectroscopic factors, configurations. Adiabatic distorted-wave approximation analysis of σ(θ) data. Comparison with shell-model calculations.

doi: 10.1103/PhysRevC.84.011301
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2011MO03      Acta Phys.Pol. B42, 541 (2011)

M.Moukaddam, G.Duchene, D.Beaumel, J.Burgunder, L.Caceres, E.Clement, D.Curien, F.Didierjean, B.Fernandez, Ch.Finck, F.Flavigny, S.Franchoo, J.Gibelin, S.Giron, A.Gillibert, A.Goasduff, S.Grevy, J.Guillot, F.Haas, F.Hammache, M.N.Harakeh, K.Kemper, V.Lapoux, Y.Matea, A.Matta, L.Nalpas, F.Nowacki, A.Obertelli, J.Pancin, L.Perrot, J.Piot, E.Pllumbi, R.Raabe, J.A.Scarpaci, N.de Sereville, K.Sieja, O.Sorlin, I.Stefan, C.Stoedel, J.C.Thomas

Search for 2d5/2 Neutron States in 69Ni

NUCLEAR REACTIONS 2H(68Ni, p), E=25.14 MeV/nucleon; measured reaction fragments, Eγ, Iγ; deduced excited states, shell gaps. Three-nucleon forces, shell model calculations.

doi: 10.5506/APhysPolB.42.541
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2010AL24      Phys.Rev. C 82, 041602 (2010)

H.Alvarez-Pol, J.Benlliure, E.Casarejos, L.Audouin, D.Cortina-Gil, T.Enqvist, B.Fernandez-Dominguez, A.R.Junghans, B.Jurado, P.Napolitani, J.Pereira, F.Rejmund, K.-H.Schmidt, O.Yordanov

Production of new neutron-rich isotopes of heavy elements in fragmentation reactions of 238U projectiles at 1A GeV

NUCLEAR REACTIONS 9Be(238U, X), E=1 GeV/nucleon; measured fragment residues using a high resolution magnetic spectrometer Fragment Separator, σ, yields. 203,204,205Pt, 207,208,209,210Au, 210,211,212,213,214,215,216Hg, 210,211,212,213,214,215,216,217Tl, 214,215,216,217,218,219,220Pb, 217,218,219,220,221,222,223,224Bi, 220,221,222,223,224,225,226,227Po, 222,223,224,225,226,227,228,229At, 225,226,227,228,229,230,231Rn, 228,229,230,232,232,233Fr; deduced yields, production σ. Comparisons of σ with the predictions obtained using the computer codes COFRA and EPAX.

doi: 10.1103/PhysRevC.82.041602
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2010CA10      Phys.Rev.Lett. 104, 192501 (2010)

W.N.Catford, C.N.Timis, R.C.Lemmon, M.Labiche, N.A.Orr, B.Fernandez-Dominguez, R.Chapman, M.Freer, M.Chartier, H.Savajols, M.Rejmund, N.L.Achouri, N.Amzal, N.I.Ashwood, T.D.Baldwin, M.Burns, L.Caballero, J.M.Casadjian, N.Curtis, G.de France, W.Gelletly, X.Liang, S.D.Pain, V.P.E.Pucknell, B.Rubio, O.Sorlin, K.Spohr, Ch.Theisen, D.D.Warner

Migration of Nuclear Shell Gaps Studied in the d(24Ne, pγ)25Ne Reaction

NUCLEAR REACTIONS 2H(24Ne, pγ)25Ne, E=10.6 MeV/nucleon; measured neutron transfer reaction products, Eγ, Iγ, p-γ-coin.; deduced σ(θ), level energies, J, π, orbital momentum, level inversion, N=16 shell gap. USD shell model.

doi: 10.1103/PhysRevLett.104.192501
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1294. Data from this article have been entered in the XUNDL database. For more information, click here.


2010LE27      J.Phys.:Conf.Ser. 202, 012035 (2010)

T.Le Bleis, D.Rossi, A.Klimkiewicz, P.Adrich, K.Boretzky, F.Aksouh, H.Alvarez-Pol, T.Aumann, J.Benlliure, M.Boehmer, E.Casarejos, M.Chartier, A.Chatillon, D.Cortina-Gil, U.D.Pramanik, H.Emling, O.Ershova, B.Fernandez-Dominguez, H.Geissel, M.Gorska, M.Heil, H.Johansson, A.R.Junghans, O.Kiselev, J.V.Kratz, N.Kurz, M.Labiche, R.Lemmon, Y.Litvinov, K.Mahata, P.Maierbeck, T.Nilsson, C.Nociforo, R.Palit, S.Paschalis, R.Plag, R.Reifarth, H.Simon, K.Smmerer, A.Wagner, W.Walus, H.Weick, M.Winkler

Target dependence in the study of collective modes in stable and exotic Ni nuclei

NUCLEAR REACTIONS C, Sn, Pb(56Ni, 55Ni), (57Ni, 56Ni), (58Ni, 57Ni), (59Ni, 58Ni), (60Ni, 59Ni), (61Ni, 60Ni), (62Ni, 61Ni), (63Ni, 62Ni), (64Ni, 63Ni), (65Ni, 64Ni), (66Ni, 65Ni), (67Ni, 66Ni), (68Ni, 67Ni), (69Ni, 68Ni), (70Ni, 69Ni), (71Ni, 70Ni), (72Ni, 71Ni), E≈500 MeV/nucleon; measured En, In, Eγ, Eγ using LAND setup (LAND neutron detector, dipole ALADIN, CSI crystals for γ); deduced Coulex σ, nuclear σ, GDR, PDR σ. Preliminary.

doi: 10.1088/1742-6596/202/1/012035
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2009AL32      Eur.Phys.J. A 42, 485 (2009)

H.Alvarez-Pol, J.Benlliure, E.Casarejos, L.Audouin, D.Cortina-Gil, T.Enqvist, B.Fernandez, A.R.Junghans, B.Jurado, P.Napolitani, J.Pereira, F.Rejmund, K.-H.Schmidt, O.Yordanov

Production cross-sections of neutron-rich Pb and Bi isotopes in the fragmentation of 238U

NUCLEAR REACTIONS 9Be(238U, X)196Pb/197Pb/198Pb/199Pb/200Pb/201Pb/202Pb/203Pb/204Pb/205Pb/206Pb/207Pb/208Pb/209Pb/210Pb/214Pb/215Pb/216Pb/217Pb/218Pb/219Pb/199Bi/200Bi/201Bi/202Bi/203Bi/204Bi/205Bi/206Bi/207Bi/208Bi/209Bi/210Bi/211Bi/212Bi/213Bi/214Bi/218Bi/219Bi/220Bi/221Bi/222Bi/223Bi, E=1 GeV/nucleon; measured production σ. Comparison with other data.

doi: 10.1140/epja/i2009-10856-8
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2009RA32      Int.J.Mod.Phys. E18, 2056 (2009)

A.Ramus, N.L.Achouri, H.Al Falou, N.I.Ashwood, D.Beaumel, Y.Blumenfeld, S.M.Brown, W.N.Catford, R.Chapman, M.Chartier, N.Curtis, F.Delaunay, B.Fernandez-Dominguez, C.Force, G.De France, S.Franchoo, J.Guillot, D.Gupta, P.Haigh, F.Hammache, M.Labiche, V.Lapoux, R.C.Lemmon, F.Marechal, B.Martin, X.Mougeot, B.Mouginot, L.Nalpas, A.Navin, N.A.Orr, N.Patterson, B.Pietras, E.C.Pollacco, A.Le Prince, M.Rejmund, J.A.Scarpaci, N.De Sereville, I.Stefan, O.Sorlin, J.S.Thomas, G.L.Wilson

Study of the 20O(d, t) reaction with the TIARA-MUST2-VAMOS-EXOGAM setup

NUCLEAR REACTIONS 2H(20O, 19O)3H, E=11 MeV/nucleon; measured reaction fragments, Eγ, Iγ; deduced J, π, σ(θ). Comparison with DWBA calculations.

doi: 10.1142/S0218301309014287
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2009SH42      Phys.Rev. C 80, 051305 (2009)

A.Shrivastava, M.Caamano, M.Rejmund, A.Navin, F.Rejmund, K.-H.Schmidt, A.Lemasson, C.Schmitt, L.Gaudefroy, K.Sieja, L.Audouin, C.O.Bacri, G.Barreau, J.Benlliure, E.Casarejos, X.Derkx, B.Fernandez-Dominguez, C.Golabek, B.Jurado, T.Roger, J.Taieb

Prompt γ-ray spectroscopy of isotopically identified fission fragments

NUCLEAR REACTIONS 12C(238U, X), E=1.45 GeV; measured Eγ, Iγ using EXOGAM array, fission fragments using VAMOS detector. 134Xe; deduced levels, J, π. 100Zr, 106,107,108,109Ru, 133Xe, 138Xe; measured Eγ. Comparison with shell model calculations for Z>49, N<83 nuclei.

doi: 10.1103/PhysRevC.80.051305
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2008CA22      Phys.Rev. C 78, 044001 (2008)

M.Caamano, D.Cortina-Gil, W.Mittig, H.Savajols, M.Chartier, C.E.Demonchy, B.Fernandez, M.B.Gomez Hornillos, A.Gillibert, B.Jurado, O.Kiselev, R.Lemmon, A.Obertelli, F.Rejmund, M.Rejmund, P.Roussel-Chomaz, R.Wolski

Experimental study of resonance states in 7H and 6H

NUCLEAR REACTIONS 12C(8He, 6H), (8He, 7H), E=15.4 MeV/nucleon; measured particle spectra. 5,6,7H; deduced excitation energies, resonances, widths. Comparison with phase space calculations.

doi: 10.1103/PhysRevC.78.044001
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2007CA28      Phys.Rev.Lett. 99, 062502 (2007)

M.Caamano, D.Cortina-Gil, W.Mittig, H.Savajols, M.Chartier, C.E.Demonchy, B.Fernandez, M.B.Gomez Hornillos, A.Gillibert, B.Jurado, O.Kiselev, R.Lemmon, A.Obertelli, F.Rejmund, M.Rejmund, P.Roussel-Chomaz, R.Wolski

Resonance State in 7H

NUCLEAR REACTIONS 12C(8He, p), E=15.4 MeV/nucleon; measured particle energies and excitation energy distributions. 7H deduced resonance energies.

doi: 10.1103/PhysRevLett.99.062502
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2007CA47      Eur.Phys.J. Special Topics 150, 9 (2007)

M.Caamano, D.Cortina-Gil, W.Mittig, H.Savajols, M.Chartier, C.E.Demonchy, B.Fernandez, A.Gillibert, M.B.Gomez Hornillos, B.Jurado, O.Kiselev, R.Lemmon, A.Obertelli, F.Rejmund, M.Rejmund, P.Roussel-Chomaz, R.Wolski

The search for 7H

NUCLEAR REACTIONS 12C(8He, 7H), E=15.4 MeV/nucleon; measured production σ(θ). 7H; deduced resonance parameters.

doi: 10.1140/epjst/e2007-00252-2
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2007FE09      Prog.Part.Nucl.Phys. 59, 389 (2007)

B.Fernandez-Dominguez, R.C.Lemmon, C.Timis, M.Labiche, W.N.Catford, M.Chartier, N.I.Ashwood, N.Amzal, T.D.Baldwin, M.Burns, L.Caballero, R.Chapman, N.Curtis, G.de France, M.Freer, W.Gelletly, X.Liang, N.A.Orr, S.D.Pain, V.P.E.Pucknell, M.Rejmund, B.Rubio, H.Savajols, O.Sorlin, K.Spohr, C.Thiesen, D.D.Warner

Single particle structure of exotic nuclei with transfer reactions

NUCLEAR REACTIONS 2H(24Ne, x), E=10 MeV/nucleon; measured Eγ, (particle)γ-coinc using EXOGAM. 25Ne; deduced level energies, J, π and spectroscopic factors.

doi: 10.1016/j.ppnp.2007.01.002
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2007NA31      Phys.Rev. C 76, 064609 (2007)

P.Napolitani, K.-H.Schmidt, L.Tassan-Got, P.Armbruster, T.Enqvist, A.Heinz, V.Henzl, D.Henzlova, A.Kelic, R.Pleskac, M.V.Ricciardi, C.Schmitt, O.Yordanov, L.Audouin, M.Bernas, A.Lafriaskh, F.Rejmund, C.Stephan, J.Benlliure, E.Casarejos, M.Fernandez-Ordonez, J.Pereira, A.Boudard, B.Fernandez, S.Leray, C.Villagrasa, C.Volant

Measurement of the complete nuclide production and kinetic energies of the system 136Xe+hydrogen at 1 GeV per nucleon

NUCLEAR REACTIONS 136Xe(p, X), E=1 GeV/nucleon; measured isotopic cross sections, kinetic energies. 6,7,8Li, 9,10,11,12Be, 10,11,12,13B, 11,12,13,14,15C, 13,14,15,16,17N, 15,16,17,18,19O, 17,18,19,20,21F, 19,20,21,22,23Ne, 22,23,24,25Na, 23,24,25,26,27Mg, 25,26,27,28,29,30Al, 28,29,30,31,32Si, 30,31,32,33,34P, 32,33,34,35,36,37,38S, 34,35,36,37,38,39,40Cl, 36,37,38,39,40,41,42,43Ar, 39,40,41,42,43,44,45K, 41,42,43,44,45,46,47Ca, 43,44,45,46,47,48,49,50Sc, 45,46,47,48,49,50,51,52Ti, 46,47,48,49,50,51,52,53,54,55V, 49,50,51,52,53,54,55,56,57Cr, 50,51,52,53,54,55,56,57,58,59,60Mn, 55,56,57,58,59,60,61,62Fe, 57,58,59,60,61,62,63,64,65Co, 59,60,61,62,63,64,65,66,67Ni, 60,61,62,63,64,65,66,67,68,69,70Cu, 62,63,64,65,66,67,68,69,70,71,72Zn, 66,67,68,69,70,71,72,73,74,75Ga, 68,69,70,71,72,73,74,75,76,77Ge, 70,71,72,73,74,75,76,77,78,79,80,81As, 72,73,74,75,76,77,78,79,80,81,82,83Se, 74,75,76,77,78,79,80,81,82,83,84,85Br, 76,77,78,79,80,81,82,83,84,85,86,87,88Kr; measured cross sections.

NUCLEAR REACTIONS 136Xe(p, X), E=1 GeV/nucleon; measured isotopic cross sections, kinetic energies. 79,80,81,82,83,84,85,86,87,88,89,90Rb, 81,82,83,84,85,86,87,88,89,90,91,92,93Sr, 84,85,86,87,88,89,90,91,92,93,94,95,96Y, 86,87,88,89,90,91,92,93,94,95,96,97,98,99Zr, 87,88,89,90,91,92,93,94,95,96,97,98,99,100Nb, 90,91,92,93,94,95,96,97,98,99,100,101,102,103,104Mo, 92,93,94,95,96,97,98,99,100,101,102,103,104,105,106Tc, 95,96,97,98,99,100,101,102,103,104,105,106,107,108,109Ru, 97,98,99,100,101,102,103,104,105,106,107,108,109,110,111Rh, 99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115Pd, 101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122Ag, 104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125Cd, 105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127In, 108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130Sn, 110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132Sb, 111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134Te, 113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135I, 116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135Xe, 122,123,124,125,126,127,128,129,130,131,132,133,134,135,136Cs, 127,128,129,130,131,132Ba; measured cross sections.

doi: 10.1103/PhysRevC.76.064609
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2007VI06      Phys.Rev. C 75, 044603 (2007)

C.Villagrasa-Canton, A.Boudard, J.-E.Ducret, B.Fernandez, S.Leray, C.Volant, P.Armbruster, T.Enqvist, F.Hammache, K.Helariutta, B.Jurado, M.-V.Ricciardi, K.-H.Schmidt, K.Summerer, F.Vives, O.Yordanov, L.Audouin, C.-O.Bacri, L.Ferrant, P.Napolitani, F.Rejmund, C.Stephan, L.Tassan-Got, J.Benlliure, E.Casarejos, M.Fernandez-Ordonez, J.Pereira, S.Czajkowski, D.Karamanis, M.Pravikoff, J.S.George, R.A.Mewaldt, N.Yanasak, M.Wiedenbeck, J.J.Connell, T.Faestermann, A.Heinz, A.Junghans

Spallation residues in the reaction 56Fe+p at 0.3A, 0.5A, 0.75A, 1.0A, and 1.5A GeV

NUCLEAR REACTIONS 1H(56Fe, X), E=0.3, 0.5, 0.75, 1.0, 1.5 GeV/nucleon; measured spallation products isotopic yields, excitation functions.

doi: 10.1103/PhysRevC.75.044603
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1507.


2006AU01      Nucl.Phys. A768, 1 (2006)

L.Audouin, L.Tassan-Got, P.Armbruster, J.Benlliure, M.Bernas, A.Boudard, E.Casarejos, S.Czajkowski, T.Enqvist, B.Fernandez-Dominguez, B.Jurado, R.Legrain, S.Leray, B.Mustapha, J.Pereira, M.Pravikoff, F.Rejmund, M.-V.Ricciardi, K.-H.Schmidt, C.Stephan, J.Taieb, C.Volant, W.Wlazlo

Evaporation residues produced in spallation of 208Pb by protons at 500 A MeV

NUCLEAR REACTIONS 1H(208Pb, X), E=500 MeV/nucleon; measured spallation fragments isotopic production σ, momentum transfer distributions; deduced reaction mechanism features. Comparisons with model predictions and results from higher-energy reactions.

doi: 10.1016/j.nuclphysa.2006.01.006
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2005FE02      Nucl.Phys. A747, 227 (2005)

B.Fernandez-Dominguez, P.Armbruster, L.Audouin, J.Benlliure, M.Bernas, A.Boudard, E.Casarejos, S.Czajkowski, J.E.Ducret, T.Enqvist, B.Jurado, R.Legrain, S.Leray, B.Mustapha, J.Pereira, M.Pravikoff, F.Rejmund, M.V.Ricciardi, K.-H.Schmidt, C.Stephan, J.Taieb, L.Tassan-Got, C.Volant, W.Wlazlo

Nuclide cross-sections of fission fragments in the reaction 208Pb + p at 500 A MeV

NUCLEAR REACTIONS 1H(208Pb, X), E=500 MeV/nucleon; measured spallation fragments isotopic production σ, kinetic energy distributions; deduced reaction mechanism features. Comparisons with model predictions and results from higher-energy reactions.

doi: 10.1016/j.nuclphysa.2004.10.013
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2005FE07      Eur.Phys.J. A 25, 193 (2005), Erratum Eur.Phys.J. A 25, 473 (2005)

B.Fernandez-Dominguez, R.C.Lemmon, B.Blank, M.Chartier, D.Cortina-Gil, J.L.Durell, H.Geissel, J.Gerl, S.Mandal, F.Rejmund, K.Summerer

Production cross-sections from neutron-deficient 92Mo at 500A MeV

NUCLEAR REACTIONS Be(92Mo, X), E=500 MeV/nucleon; measured fragments isotopic production σ. Comparison with model predictions.

doi: 10.1140/epja/i2005-10104-5
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2005FE09      J.Phys.(London) G31, S1843 (2005)

B.Fernandez-Dominguez, R.Lemmon, B.Blank, M.Chartier, D.Cortina-Gil, H.Geissel, S.Mandal, F.Rejmund, K.Summerer

Production cross sections of N ≈ Z nuclei in the region around A ≈ 80

NUCLEAR REACTIONS Be(92Mo, X), E=500 MeV/nucleon; measured fragments isotopic production σ. Comparison with model predictions.

doi: 10.1088/0954-3899/31/10/084
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1297.


2004BE19      Nucl.Phys. A734, 609 (2004)

J.Benlliure, L.Audouin, M.Bernas, E.Casarejos, T.Enqvist, B.Fernandez, V.Henzl, A.Kelic, P.Napolitani, J.Pereira, M.V.Ricciardi, K.-H.Schmidt, J.Taieb

Momentum distributions of projectile spectators: a new tool to investigate the equation of state of nuclear matter

NUCLEAR REACTIONS Ti, Pb(208Pb, X), (238U, X), E=500-1000 MeV/nucleon; measured fragment velocity distributions; deduced post-acceleration effects.

doi: 10.1016/j.nuclphysa.2004.01.113
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2003CA29      Yad.Fiz. 66, 1459 (2003); Phys.Atomic Nuclei 66, 1413 (2003)

E.Casarejos, P.Armbruster, L.Audouin, J.Benlliure, M.Bernas, A.Boudard, R.Legrain, S.Leray, B.Mustapha, S.Czajkowski, T.Enqvist, B.Fernandez, J.Pereira, M.Pravikoff, F.Rejmund, K.-H.Schmidt, C.Stephan, J.Taieb, L.Tassan-Got, C.Villagrasa, C.Volant, W.Wlazlo

Isotopic Production Cross Sections of Residues in Reactions Induced by Relativistic Heavy Ions with Protons and Deuterons

NUCLEAR REACTIONS 1,2H(238U, X), (208Pb, X), E=1 GeV/nucleon; measured fragment isotopic yields, mass distributions.

doi: 10.1134/1.1601743
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1998CA22      Phys.Lett. 430B, 43 (1998)

J.M.Casandjian, W.Mittig, A.Pakou, N.Alamanos, G.Auger, F.Auger, M.Chartier, D.Cortina-Gil, V.Fekou-Youmbi, B.Fernandez, A.Gillibert, A.Lepine, M.MacCormick, A.Ostrowski, P.Roussel-Chomaz, J.L.Sida

Compound Nuclear Lifetimes at High Excitation Energies Via a New Statistical Fluctuation Method

NUCLEAR REACTIONS 12C(28Si, α), E=190, 277 MeV; measured α-spectra; deduced coherence width, compound nucleus lifetime. Statistical fluctuation method.

doi: 10.1016/S0370-2693(98)00342-6
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1998CO19      J.Phys.(London) G24, 1547 (1998)

M.D.Cortina-Gil, A.Pakou, N.Alamanos, W.Mittig, P.Roussel-Chomaz, F.Auger, J.Barrette, Y.Blumenfeld, J.M.Casandjian, M.Chartier, F.Dietrich, V.Fekou-Youmbi, B.Fernandez, N.Frascaria, A.Gillibert, H.Laurent, A.Lepine-Szily, N.Orr, V.Pascalon, J.A.Scarpaci, J.L.Sida, T.Suomijarvi

Charge-Exchange Reaction with Light Neutron-Rich Beams

NUCLEAR REACTIONS 1H(6He, 6Li), E=41.6 MeV/nucleon; measured σ(θ); deduced no halo effect on transition strength. Optical model analysis.

doi: 10.1088/0954-3899/24/8/032
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1998CO28      Nucl.Phys. A641, 263 (1998)

M.D.Cortina-Gil, A.Pakou, N.Alamanos, W.Mittig, P.Roussel-Chomaz, F.Auger, J.Barrette, Y.Blumenfeld, J.M.Casandjian, M.Chartier, F.Dietrich, V.Fekou-Youmbi, B.Fernandez, N.Frascaria, A.Gillibert, H.Laurent, A.Lepine-Szily, N.Orr, V.Pascalon, J.A.Scarpaci, J.L.Sida, T.Suomijarvi

Charge-Exchange Reaction Induced by 6He and Nuclear Densities

NUCLEAR REACTIONS 1H(6He, 6Li), E=41.6 MeV/nucleon; measured σ(θ) for transition to ground state, IAS; deduced dependence on interaction potential. 6He deduced density distribution.

doi: 10.1016/S0375-9474(98)00470-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0211.


1997CO04      Nucl.Phys. A616, 215c (1997)

M.D.Cortina-Gil, P.Roussel-Chomaz, N.Alamanos, J.Barrette, W.Mittig, F.Auger, Y.Blumenfeld, J.M.Casandjian, M.Chartier, V.Fekou-Youmbi, B.Fernandez, N.Frascaria, A.Gillibert, H.Laurent, A.Lepine-Szily, N.A.Orr, V.Pascalon, J.A.Scarpaci, J.L.Sida, T.Suomijarvi

Elastic Scattering and Charge Exchange Reaction with Light Neutron Rich Exotic Beams

NUCLEAR REACTIONS 1H(6He, 6He), (10Be, 10Be), (11Be, 11Be), (6He, 6Li), E=41.6-68 MeV/nucleon; measured σ(θ); deduced halo structure's presence or absence has no influence on (p, n) reaction transition strength.

doi: 10.1016/S0375-9474(97)00091-2
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1997CO11      Phys.Lett. 401B, 9 (1997)

M.D.Cortina-Gil, P.Roussel-Chomaz, N.Alamanos, J.Barrette, W.Mittig, F.S.Dietrich, F.Auger, Y.Blumenfeld, J.M.Casandjian, M.Chartier, V.Fekou-Youmbi, B.Fernandez, N.Frascaria, A.Gillibert, H.Laurent, A.Lepine-Szily, N.A.Orr, J.A.Scarpaci, J.L.Sida, T.Suomijarvi

Proton Elastic Scattering on Light Neutron-Rich Nuclei

NUCLEAR REACTIONS 1H(7Li, 7Li), E=68 MeV/nucleon; 1H(6He, 6He), E=41.6 MeV/nucleon; 1H(10Be, 10Be), E=59.3 MeV/nucleon; 1H(11Be, 11Be), E=49.3 MeV/nucleon; measured σ(θ); 1H(8He, 8He), E=72 MeV/nucleon; 1H(9Li, 9Li), E=60 MeV/nucleon; 1H(11Li, 11Li), E=62 MeV/nucleon; analyzed σ(θ); deduced break-up channels role, optical potential related features. Phenomenological, microscopic optical models.

doi: 10.1016/S0370-2693(97)00321-3
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1996AL11      Phys.Lett. 378B, 45 (1996)

J.S.Al-Khalili, M.D.Cortina-Gil, P.Roussel-Chomaz, N.Alamanos, J.Barrette, W.Mittig, F.Auger, Y.Blumenfeld, J.M.Casandjian, M.Chartier, V.Fekou-Youmbi, B.Fernandez, N.Frascaria, A.Gillibert, H.Laurent, A.Lepine-Szily, N.A.Orr, V.Pascalon, J.A.Scarpaci, J.L.Sida, T.Suomijarvi

Elastic Scattering of 6He and Its Analysis within a Four-Body Eikonal Model

NUCLEAR REACTIONS 12C(6He, 6He), E=41.6 MeV/nucleon; measured σ(θ). Four-body eikonal model analysis.

doi: 10.1016/0370-2693(96)00336-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0244.


1996CO10      Phys.Lett. 371B, 14 (1996)

M.D.Cortina-Gil, P.Roussel-Chomaz, N.Alamanos, J.Barrette, W.Mittig, F.Auger, Y.Blumenfeld, J.M.Casandjian, M.Chartier, V.Fekou-Youmbi, B.Fernandez, N.Frascaria, A.Gillibert, H.Laurent, A.Lepine-Szily, N.A.Orr, V.Pascalon, J.A.Scarpaci, J.L.Sida, T.Suomijarvi

Search for the Signature of a Halo Structure in the p(6He, 6Li)n Reaction

NUCLEAR REACTIONS 1H(6He, 6Li), (6He, 6He), E=41.6 MeV/nucleon; measured σ(θ); deduced Gamow-Teller to Fermi reduced transition strength ratio. 6He deduced ground state halo related features. Other (p, n) reaction data included.

doi: 10.1016/0370-2693(95)01582-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0245.


1995CO05      Nucl.Phys. A583, 787c (1995)

M.D.Cortina-Gil, P.Roussel-Chomaz, N.Alamanos, F.Auger, J.Barrette, Y.Blumenfeld, J.M.Casandjian, M.Chartier, V.Fekou-Youmbi, B.Fernandez, N.Frascaria, A.Gillibert, H.Laurent, A.Lepine, W.Mittig, N.A.Orr, V.Pascalon, J.A.Scarpaci, J.L.Sida, T.Suomijarvi

Elastic Scattering, Inelastic Scattering and Charge Exchange Reaction Studies with 6He, 10,11Be Secondary Beams

NUCLEAR REACTIONS C, 1H(10Be, 10Be), E=60 MeV/nucleon; measured momentum spectra.

doi: 10.1016/0375-9474(94)00783-J
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1994CA02      Nucl.Phys. A568, 107 (1994)

C.Cabot, J.Barrette, S.K.Mark, R.Turcotte, J.Xing, N.Alamanos, F.Auger, B.Fernandez, J.Gastebois, A.Gillibert, R.Lacey, R.Liguori-Neto, P.Roussel-Chomaz, A.Miczaika, Y.Blumenfeld, N.Frascaria, J.P.Garron, J.C.Roynette, J.A.Scarpaci, A.Van der Woude, A.M.Van den Berg

Excitation and Fission Decay of 232Th by Inelastic Scattering of 17O at 84 MeV/u

NUCLEAR REACTIONS 232Th(17O, 17O'), E=1435 MeV; measured σ(fragment, θ) fission probability. 232Th deduced isoscalar giant quadrupole resonance, parameters, decay features.

doi: 10.1016/0375-9474(94)90006-X
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1993BE19      Nucl.Phys. A555, 455 (1993)

C.Berat, M.Buenerd, J.Y.Hostachy, P.Martin, J.Barrette, B.Berthier, B.Fernandez, A.Miczaika, A.Villari, H.G.Bohlen, S.Kubono, E.Stiliaris, W.von Oertzen

Electric Isovector Nuclear Response from 13C Induced Charge-Exchange Reactions

NUCLEAR REACTIONS 12C, 40Ca, 58,60Ni, 90Zr, 120Sn, 208Pb(13C, 13N), E=50 MeV/nucleon; measured σ(θ). 12B, 40K, 58,60Co, 90Y, 120In, 208Tl deduced GDR IAS. Microscopic DWBA.

doi: 10.1016/0375-9474(93)90296-A
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1993LI24      Nucl.Phys. A560, 733 (1993)

R.Liguori Neto, P.Roussel-Chomaz, L.Rochais, N.Alamanos, F.Auger, B.Fernandez, J.Gastebois, A.Gillibert, R.Lacey, A.Miczaika, D.Pierroutsakou, J.Barrette, S.K.Mark, R.Turcotte, Y.Blumenfeld, N.Frascaria, J.P.Garron, J.C.Roynette, J.A.Scarpaci, T.Suomijarvi, A.Van der Woude, A.M.Van den Berg

Excitation of Giant Resonances in 208Pb, 120Sn, 90Zr and 60Ni by 84 MeV/nucleon 17O Ions

NUCLEAR REACTIONS 60Ni, 90Zr, 120Sn, 208Pb(17O, 17O), (17O, 17O'), E=1435 MeV; measured σ(θ); deduced model parameters. 60Ni, 90Zr, 120Sn, 208Pb levels deduced B(λ), giant monopole, quadrupole reasonances.

doi: 10.1016/0375-9474(93)90043-W
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1991SC16      Phys.Lett. 258B, 279 (1991)

J.A.Scarpaci, Y.Blumenfeld, Ph.Chomaz, N.Frascaria, J.P.Garron, J.C.Roynette, T.Suomijarvi, N.Alamanos, B.Fernandez, A.Gillibert, A.Lepine, A.Van der Woude

Study of the Continuum in Heavy Ion Inelastic Spectra by Light Particle Coincidence Measurements

NUCLEAR REACTIONS 40Ca(40Ca, X), E=50 MeV/nucleon; measured (fragment)(light charged particle)-coin; deduced different mechanism components.

doi: 10.1016/0370-2693(91)91085-A
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1991TH01      Phys.Rev. C43, R12 (1991)

M.Thoennessen, J.R.Beene, F.E.Bertrand, D.J.Horen, M.L.Halbert, D.C.Hensley, J.E.Lisantti, W.Mittig, Y.Schutz, N.Alamanos, F.Auger, J.Barrette, B.Fernandez, A.Gillibert, B.Haas, J.P.Vivien, A.M.Nathan

High-Energy Target Excitations in Heavy Ion Inelastic Scattering

NUCLEAR REACTIONS 208Pb(17O, 17O'), E=84 MeV/nucleon; measured γ(17O')-coin. 208Pb deduced GDR built on highly excited states.

doi: 10.1103/PhysRevC.43.R12
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1991VI04      Phys.Lett. 268B, 345 (1991)

A.C.C.Villari, W.Mittig, E.Plagnol, Y.Schutz, M.Lewitowicz, L.Bianchi, B.Fernandez, J.Gastebois, A.Gillibert, C.Stephan, L.Tassan-Got, G.Audi, W.Zhan, A.Cunsolo, A.Foti, A.Belezyorov, S.Lukyanov, Y.Penionzhkevich

Measurements of Reaction Cross Sections for Neutron-Rich Exotic Nuclei by a New Direct Method

NUCLEAR REACTIONS Ta(48Ca, X), E=55 MeV/nucleon; measured reaction σ for fragment masses 8-40; deduced strong absorption radii for A=8-40. 4π γ-array, coincidence, anticoincidence configurations.

doi: 10.1016/0370-2693(91)91588-M
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1990BE03      Phys.Rev. C41, 920 (1990)

J.R.Beene, F.E.Bertrand, D.J.Horen, R.L.Auble, B.L.Burks, J.Gomez del Campo, M.L.Halbert, R.O.Sayer, W.Mittig, Y.Schutz, J.Barrette, N.Alamanos, F.Auger, B.Fernandez, A.Gillibert, B.Haas, J.P.Vivien

Heavy-Ion Coulomb Excitation and Photon Decay of the Giant Dipole Resonance in 208Pb

NUCLEAR REACTIONS 208Pb(17O, 17O'), E=84 MeV/nucleon; measured σ(E(17O)), γ(particle)(θ, φ) following Coulomb excitation, σ(θ). 208Pb deduced giant resonance decay features, B(λ), M(n)/M(p).

doi: 10.1103/PhysRevC.41.920
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1990BE08      Phys.Rev. C41, R1332 (1990)

J.R.Beene, F.E.Bertrand, D.J.Horen, J.L.Lisantti, M.L.Halbert, D.C.Hensley, W.Mittig, Y.Schutz, J.Barrette, N.Alamanos, F.Auger, B.Fernandez, A.Gillibert, B.Haas, J.P.Vivien, A.M.Nathan

Compound and Precompound Effects in Photon Decay of the Giant Dipole Resonance

NUCLEAR REACTIONS 208Pb, 209Bi(17O, 17O'), E=84 MeV/nucleon; measured γ-spectra, γ yield vs excitation; deduced γ production σ vs excitation. 208Pb, 209Bi deduced GDR decay features.

doi: 10.1103/PhysRevC.41.R1332
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1990BR25      Nucl.Phys. A519, 631 (1990)

M.Braeunig, W.von Oertzen, H.G.Bohlen, A.Miczaika, E.Stiliaris, M.Buenerd, C.Berat, J.Chauvin, D.Lebrun, J.Y.Hostachy, Ph.Martin, W.Mittig, J.Barrette, B.Berthier, B.Fernandez

Proton Stripping Induced by 13C at 50 MeV/Nucleon on 12C, 40Ca and 58Ni

NUCLEAR REACTIONS 12C, 40Ca, 58Ni(13C, 12B), E=50 MeV/nucleon; measured σ(θ). 13N, 41Sc, 59Cu levels deduced configurations, spectroscopic factors.

doi: 10.1016/0375-9474(90)90450-Z
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1990SU02      Nucl.Phys. A509, 369 (1990)

T.Suomijarvi, D.Beaumel, Y.Blumenfeld, Ph.Chomaz, N.Frascaria, J.P.Garron, J.C.Roynette, J.A.Scarpaci, J.Barrette, B.Fernandez, J.Gastebois, W.Mittig

Excitation of Giant Resonances in Heavy-Ion Reactions at Intermediate Energies: Results from the 40Ar + 90Zr and 208Pb experiments at 41 MeV/u

NUCLEAR REACTIONS 90Zr, 208Pb(40Ar, 40Ar), (40Ar, 40Ar'), E=41 MeV/nucleon; measured σ(θ). 90Zr, 208Pb deduced giant resonance strength distributions, multipolarity.

doi: 10.1016/0375-9474(90)90428-O
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1989BE50      Phys.Lett. 218, 299 (1989)

C.Berat, M.Buenerd, J.Chauvin, J.Y.Hostachy, D.Lebrun, P.Martin, J.Barrette, B.Berthier, B.Fernandez, A.Miczaika, W.Mittig, E.Stiliaris, W.von Oertzen, H.Lenske, H.H.Wolter

Heavy Ion Charge Exchange Reactions to Probe the Giant Electric Isovector Modes in Nuclei

NUCLEAR REACTIONS 12C, 40Ca, 58Ni(13C, 13N), E=50 MeV/nucleon; measured angle integrated spectra, σ(θ). 12B, 40K, 58Co deduced GDR analog.

doi: 10.1016/0370-2693(89)91585-2
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1989BI01      Nucl.Instrum.Methods Phys.Res. A276, 509 (1989)

L.Bianchi, B.Fernandez, J.Gastebois, A.Gillibert, W.Mittig, J.Barrette

SPEG: An energy loss spectrometer for GANIL

NUCLEAR REACTIONS 28Si(16O, 16O), E=95 MeV/nucleon; measured σ(θ). 208Pb(16O, 15N), E=793 MeV; measured σ(E(15N)), θ ≈ 0°. Energy loss spectrometer.

doi: 10.1016/0168-9002(89)90577-9
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1989SU02      Nucl.Phys. A491, 314 (1989)

T.Suomijarvi, D.Beaumel, Y.Blumenfeld, Ph.Chomaz, N.Frascaria, J.P.Garron, J.C.Jacmart, J.C.Roynette, J.Barrette, B.Berthier, B.Fernandez, J.Gastebois, P.Roussel-Chomaz, W.Mittig, L.Kraus, I.Linck

Excitation of Giant Resonances in 20Ne + 90Zr and 208Pb Inelastic Scattering at 40 MeV/u

NUCLEAR REACTIONS 90Zr, 208Pb(20Ne, 20Ne'), E=800 MeV; measured σ(E(20Ne), θ(20Ne)). 90Zr, 208Pb deduced GDR excitation strength. Macroscopic DWBA calculations, multipole analysis.

doi: 10.1016/0375-9474(89)90706-9
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1988AU03      Nucl.Phys. A481, 577 (1988)

F.Auger, B.Fernandez

Search for Low-L Fusion Window in the 16O + 16O Reaction at 4.5 MeV/Nucleon

NUCLEAR REACTIONS, ICPND 16O(16O, X), 16O(16O, 12C), (16O, 15N), E=72 MeV; measured reaction σ, σ(θ) vs Q-value, (16O)(16O)(θ), (16O)(α)(θ). 16O levels deduced J.

doi: 10.1016/0375-9474(88)90346-6
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1988BA39      Phys.Lett. 209B, 182 (1988)

J.Barrette, N.Alamanos, F.Auger, B.Fernandez, A.Gillibert, D.J.Horen, J.R.Beene, F.E.Bertrand, R.L.Auble, B.L.Burks, J.Gomez Del Campo, M.L.Halbert, R.O.Sayer, W.Mittig, Y.Schutz, B.Haas, J.P.Vivien

Coulomb Excitation of Giant Resonances in 208Pb by E = 84 MeV/Nucleon 17O Projectiles

NUCLEAR REACTIONS 208Pb(17O, 17O), (17O, 17O'), E=1428 MeV; measured σ(θ). 208Pb deduced giant resonance excitation mechanism, B(λ), EWSR.

doi: 10.1016/0370-2693(88)90929-X
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1988RO01      Nucl.Phys. A477, 345 (1988)

P.Roussel-Chomaz, N.Alamanos, F.Auger, J.Barrette, B.Berthier, B.Fernandez, L.Papineau, H.Doubre, W.Mittig

16O Elastic Scattering at E(lab) = 94 MeV/Nucleon

NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(16O, 16O), E=94 MeV/nucleon; measured σ(θ); deduced model parameter energy dependence. Optical model.

doi: 10.1016/0375-9474(88)90324-7
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1988RO12      Phys.Lett. 209B, 187 (1988)

P.Roussel-Chomaz, J.Barrette, N.Alamanos, B.Berthier, B.Fernandez, J.Gastebois, W.Mittig, Y.Blumenfeld, N.Frascaria, J.P.Garron, J.C.Jacmart, J.C.Roynette, L.Kraus, I.Linck, Ph.Chomaz

Elastic and Inelastic Scattering of 86Kr on 208Pb at E(lab) = 43 MeV/Nucleon

NUCLEAR REACTIONS 208Pb(86Kr, 86Kr), (86Kr, 86Kr'), E=3.702 GeV; measured σ(θ), Coulomb excitation. 208Pb deduced giant resonance excitation mechanism.

doi: 10.1016/0370-2693(88)90930-6
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1988ZH19      Nouvelles de GANIL 25, 22 (1988)

W.Zhan, G.Audi, L.Bianchi, A.Cunsolo, H.Dumont, B.Fernandez, A.Foti, J.Gastebois, A.Gillibert, W.Mittig, M.Morjean, Y.Pranal, Y.Schutz, C.Stephan

Production et identification de nouveaux noyaux riches en neutrons dans la region Z = 21 A 28 (E69)

NUCLEAR REACTIONS Ti(86Kr, X)54Sc/55Sc/58Ti/61V/63Cr/64Cr/66Mn/69Fe/71Co/72Co/75Ni, E=44 MeV/nucleon; measured reaction products; deduced new isotopes. (SPEG + α) spectrometer.


1987GI05      Phys.Lett. 192B, 39 (1987)

A.Gillibert, W.Mittig, L.Bianchi, A.Cunsolo, B.Fernandez, A.Foti, J.Gastebois, C.Gregoire, Y.Schutz, C.Stephan

New Mass Measurements Far From Stability

NUCLEAR REACTIONS Ta(40Ar, X), E=60 MeV/nucleon; measured fragment rigidity, tof. 17B, 19,20C, 20,21,22N, 23,24O, 24,25,26F, 27,28Ne, 30,31,32Na, 31,32,33Mg, 32,33,34,35Al, 36,37Si, 37,38P deduced mass excess.

doi: 10.1016/0370-2693(87)91138-5
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1987MI27      Phys.Rev.Lett. 59, 1889 (1987)

W.Mittig, J.M.Chouvel, Zhan Wen Long, L.Bianchi, A.Cunsolo, B.Fernandez, A.Foti, J.Gastebois, A.Gillibert, C.Gregoire, Y.Schutz, C.Stephan

Measurement of Total Reaction Cross Sections of Exotic Neutron-Rich Nuclei

NUCLEAR REACTIONS Si(40Ar, X), E=60 MeV/nucleon; measured total reaction σ for fragments with Z=5-12; deduced reduced strong absorption radius vs neutron excess.

doi: 10.1103/PhysRevLett.59.1889
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1987RO04      Phys.Lett. 185B, 29 (1987)

P.Roussel, J.Barrette, F.Auger, B.Berthier, B.Fernandez, J.Gastebois, A.Gillibert, L.Papineau, W.Mittig, D.Disdier, B.Lott, V.Rauch, F.Scheibling, C.Stephan, L.Tassan-Got

16O + 28Si Elastic Scattering at E(L) = 94 MeV/Nucleon

NUCLEAR REACTIONS 28Si(16O, 16O), E=94 MeV/nucleon; measured σ(θ); deduced potential parameters. Si detectors.

doi: 10.1016/0370-2693(87)91523-1
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1987SU18      Phys.Rev. C36, 2691 (1987)

T.Suomijarvi, D.Beaumel, Y.Blumenfeld, N.Frascaria, J.P.Garron, J.C.Jacmart, J.C.Roynette, Ph.Chomaz, J.Barrette, B.Berthier, B.Fernandez, J.Gastebois, W.Mittig

Forward Angle Measurements of 60 MeV/Nucleon 40Ar Peripheral Interactions on 208Pb

NUCLEAR REACTIONS 208Pb(40Ar, X), E=2400 MeV; measured σ(fragment A, Z, θ) vs velocity inside the grazing angle; deduced reaction mechanisms, fragmentation, transfer, nuclear, Coulomb deflections.

doi: 10.1103/PhysRevC.36.2691
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1986GI10      Phys.Lett. 176B, 317 (1986)

A.Gillibert, L.Bianchi, A.Cunsolo, B.Fernandez, A.Foti, J.Gastebois, Ch.Gregoire, W.Mittig, A.Peghaire, Y.Schutz, C.Stephan

Mass Measurement of Light Neutron-Rich Fragmentation Products

NUCLEAR REACTIONS Ta(40Ar, X)20N/21N/23O/21F/22F/23F/24F/25F/26F/27F, E=44 MeV/nucleon; measured fragment yield vs mass. 20,21N, 23O, 24,25,26F deduced mass excess, two-neutron separation energy. Tof.

doi: 10.1016/0370-2693(86)90171-1
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1985RO08      Phys.Rev.Lett. 54, 1779 (1985)

P.Roussel, N.Alamanos, F.Auger, J.Barrette, B.Berthier, B.Fernandez, L.Papineau, H.Doubre, W.Mittig

Nucleus-Nucleus Potential Inside the Strong-Absorption Radius from 16O + 12C Elastic Scattering at 94 MeV/u

NUCLEAR REACTIONS 12C(16O, 16O), E=1503 MeV; measured σ(θ); deduced potential parameters.

doi: 10.1103/PhysRevLett.54.1779
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1984AL02      Phys.Lett. 137B, 37 (1984)

N.Alamanos, F.Auger, J.Barrette, B.Berthier, B.Fernandez, J.Gastebois, L.Papineau, H.Doubre, W.Mittig

Elastic Scattering of 40Ar on 60Ni, 120Sn and 208Pb at 44 MeV/u

NUCLEAR REACTIONS 60Ni, 120Sn, 208Pb(40Ar, 40Ar), E=44 MeV/nucleon; measured σ(θ); deduced potential parameters, ion-ion potential energy dependence, Coulomb rainbow effect dominance.

doi: 10.1016/0370-2693(84)91101-8
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1983ME13      Phys.Rev. C28, 1587 (1983)

M.C.Mermaz, F.Auger, B.Fernandez

Diffractional Model Fits of Alpha Transfer Reactions Induced by 16O Projectiles on 16O and 28Si Target Nuclei

NUCLEAR REACTIONS 16O, 28Si(16O, 12C), 16O(16O, 20Ne), E=50, 60, 68, 72 MeV; measured σ(θ), σ(E(12C)), σ(E(20Ne)). Diffraction model, α-particle transfer.

doi: 10.1103/PhysRevC.28.1587
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1979HI03      Nucl.Phys. A325, 216 (1979)

D.L.Hillis, J.D.Garrett, O.Christensen, B.Fernandez, G.B.Hagemann, B.Herskind, B.B.Back, F.Folkmann

Gamma-Ray Multiplicity Studies for 40Ar and 86Kr Induced Reactions Leading to Er Compound Nuclei at Limiting Angular Momenta

NUCLEAR REACTIONS 116,120,122,124Sn(40Ar, xnγ), E=161-236 MeV; 76Ge(86Kr, xnγ), E=314-376 MeV; measured γγ-coin rates, < Eγ > ; deduced moments of γ-ray multiplicity distribution as function of xn, Eγ, L(max), moments of inertia. Statistical model analysis. Enriched targets.

doi: 10.1016/0375-9474(79)90162-3
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1978BA17      Phys.Rev. C17, 978 (1978)

I.Badawy, B.Berthier, P.Charles, M.Dost, B.Fernandez, J.Gastebois, S.M.Lee

Elastic Scattering of Alpha Particles Near the Coulomb Barrier and Matter Distribution of Medium and Heavy Nuclei

NUCLEAR REACTIONS 110,112,114,116Cd, 112,114,116,118,120,122,124Sn, 122,124,128,126,130Te, 148,144,150,152Sm, 204,206,208Pb(α, α), E ≈ 8-23 MeV; measured σ(E, θ). Optical model analysis.

doi: 10.1103/PhysRevC.17.978
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1978FE04      Nucl.Phys. A306, 259 (1978)

B.Fernandez, C.Gaarde, J.S.Larsen, S.Pontoppidan, F.Videbaek

Fusion Cross Sections for the 16O + 16O Reaction

NUCLEAR REACTIONS 16O, 12C(16O, X), E=35-80 MeV; measured σ(E, θ); deduced fusion σ(E).

doi: 10.1016/0375-9474(78)90327-5
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1978HI07      Phys.Lett. 78B, 405 (1978)

D.L.Hillis, O.Christensen, B.Fernandez, A.J.Ferguson, J.D.Garrett, G.B.Hagemann, B.Herskind, B.B.Back, F.Folkmann

Anomalous Gamma-Ray Multiplicity Distributions - Evidence for Pre-Equilibrium Neutron Emission

NUCLEAR REACTIONS 124Sn(40Ar, xnγ), E=161-236 MeV; measured multiplicity distributions, < Eγ > ; deduced pre-equilibrium neutron emission at E=236 MeV.

doi: 10.1016/0370-2693(78)90471-9
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1977BR30      Phys.Rev.Lett. 39, 1458 (1977)

H.C.Britt, B.H.Erkkila, P.D.Goldstone, R.H.Stokes, B.B.Back, F.Folkmann, O.Christensen, B.Fernandez, J.D.Garrett, G.B.Hagemann, B.Herskind, D.L.Hillis, F.Plasil, R.L.Ferguson, M.Blann, H.H.Gutbrod

Angular Momentum Limits in Fusion Reactions Induced by Argon and Krypton Projectiles

NUCLEAR REACTIONS 122,124Sn(40Ar, X), 76Ge(86Kr, X); measured γ-multiplicity. 70,74Ge(86Kr, X); measured σ(A, Z).

doi: 10.1103/PhysRevLett.39.1458
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1976BA22      J.Phys.(Paris), Lett. 37, L-131 (1976)

Z.Basrak, F.Auger, B.Fernandez, J.Gastebois, N.Cindro

Resonant Behaviour in the Interaction of the 12C + 12C System at Energies Above the Coulomb Barrier

NUCLEAR REACTIONS 12C(12C, p), (12C, α), E=14-22 MeV; measured σ(E). 24Mg deduced resonances.

doi: 10.1051/jphyslet:01976003706013100
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1976BA53      Phys.Lett. 65B, 119 (1976)

Z.Basrak, F.Auger, B.Fernandez, J.Gastebois, N.Cindro

Spins of Resonances in the 12C + 12C System

NUCLEAR REACTIONS 12C(12C, α), (12C, p), E(cm)=7.5-8.85 MeV; measured σ(θ). 24Mg resonances deduced J, π.

doi: 10.1016/0370-2693(76)90008-3
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1976CH13      Phys.Lett. 62B, 289 (1976)

P.Charles, F.Auger, I.Badawy, B.Berthier, M.Dost, J.Gastebois, B.Fernandez, S.M.Lee, E.Plagnol

Resonant Behaviour of the 16O-12C Elastic Scattering Cross Section

NUCLEAR REACTIONS 12C(16O, 16O), 16O(12C, 12C), E(cm)=15-33 MeV; measured σ(E, θ). 28Si deduced resonances, J, π.

doi: 10.1016/0370-2693(76)90077-0
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1975BA74      J.Phys.(Paris), Colloq. 36, C5-117 (1975)

I.Badawy, B.Berthier, P.Charles, M.Dost, B.Fernandez, J.Gastebois, S.M.Lee

Diffusion Elastique de Particules α Autour de la Barriere Coulombienne et Densite de Matiere des Noyaux Moyens et Lourds

NUCLEAR REACTIONS 110,112,114,116Cd, 112,114,116,118,120,122,124Sn, 122,124,126,128,130Te, 144,148,150,152Sm, 204,206,208Pb(α, α), E ≈ Coulomb barrier; measured σ; deduced α-nucleus distance.


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