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NSR database version of May 19, 2024.

Search: Author = H.Gauvin

Found 47 matches.

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1993BA18      Nucl.Phys. A555, 477 (1993)

Ch.O.Bacri, P.Roussel, V.Borrel, F.Clapier, R.Anne, M.Bernas, Y.Blumenfeld, H.Gauvin, J.Herault, J.C.Jacmart, F.Pougheon, J.L.Sida, C.Stephan, T.Suomijarvi, L.Tassan-Got

Measurements in the Beam Direction of the 40Ar Projectile Fragmentation at 44 MeV/A

NUCLEAR REACTIONS 58Ni, 27Al, 197Au(40Ar, X), E=44 MeV/nucleon; measured σ(fragment, θ=0°) vs exciation energy; deduced production yields for fragment mass=10-45. Study of peripheral reaction mechanism.

doi: 10.1016/0375-9474(93)90297-B
Citations: PlumX Metrics


1991JO12      Z.Phys. A340, 63 (1991)

D.Jouan, B.Borderie, M.F.Rivet, C.Cabot, H.Fuchs, H.Gauvin, C.Gregoire, F.Hanappe, D.Gardes, M.Montoya, B.Remaud, F.Sebille

Dynamics and Thermalization in Violent Collisions between 40Ar and Ag at 27 MeV/nucleon

NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured (fragment)(fragment)-coin; deduced reaction mechanism.

doi: 10.1007/BF01284482
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1988BO13      Phys.Lett. 205B, 26 (1988)

B.Borderie, M.Montoya, M.F.Rivet, D.Jouan, C.Cabot, H.Fuchs, D.Gardes, H.Gauvin, D.Jacquet, F.Monnet, F.Hanappe

Deeply Inelastic Collisions as a Source of Intermediate Mass Fragments at E/A = 27 MeV

NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured fragment σ(θ1, θ2); deduced reaction mechanism.

doi: 10.1016/0370-2693(88)90393-0
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1988RI06      Z.Phys. A330, 301 (1988)

M.F.Rivet, R.Alami, B.Borderie, H.Fuchs, D.Gardes, H.Gauvin

Fusion-Fission of Heavy Systems. Influence of the Entrance Channel Mass Asymmetry

NUCLEAR REACTIONS 209Bi(40Ar, F), E=202, 238 MeV; 187Re(56Fe, F), E=294, 307, 326 MeV; measured fission σ, fragment mass distribution widths; deduced entrance channel role in fission.


1986RI06      Phys.Rev. C34, 1282 (1986)

M.F.Rivet, B.Borderie, H.Gauvin, D.Gardes, C.Cabot, F.Hanappe, J.Peter

Deexcitation of Nuclei Formed near the Instability Temperature

NUCLEAR REACTIONS 165Ho, Ag(40Ar, X), E=1090 MeV; measured fragment σ(θ), mass distribution, velocity spectra, (fragment)(fragment)(θ); deduced reaction mechanism. Natural targets, TOF telescope, parallel plate avalanche counter.

doi: 10.1103/PhysRevC.34.1282
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1985CA35      Z.Phys. A322, 393 (1985)

C.Cabot, H.Gauvin, H.Sergolle, P.Aguer, G.Bastin, J.P.Thibaud, H.Delagrange, Y.Patin

Competition between Few Nucleon Emission and γ-Ray Deexcitation for the Reaction Systems 65Cu + 87Rb and 40Ar + 110Pd

NUCLEAR REACTIONS 87Rb(65Cu, xnyp), E=237 MeV; 110Pd(40Ar, xnyp), E=158 MeV; measured Eγ, Iγ, γγ-, γn-coin; deduced nucleon, γ emission competition. 147,146Gd, 150,151Dy deduced yrast sequence.

doi: 10.1007/BF01412074
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1984BO17      Z.Phys. A316, 243 (1984)

B.Borderie, M.F.Rivet, C.Cabot, D.Fabris, D.Gardes, H.Gauvin, F.Hanappe, J.Peter

Heavy Products from Violent Collisions in the 40Ar + (nat)Ag System at 27 MeV/u

NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured heavy evaporation residue σ(θ), velocity spectra vs mass; deduced reaction mechanism.

doi: 10.1007/BF01412271
Citations: PlumX Metrics


1984BO35      Z.Phys. A318, 315 (1984)

B.Borderie, M.F.Rivet, C.Cabot, D.Fabris, D.Gardes, H.Gauvin, F.Hanappe, J.Peter

Light Fragments Produced in 40Ar + (nat)Ag Reactions at 27 MeV/u

NUCLEAR REACTIONS Ag(40Ar, X), E=1.095 GeV; measured σ(fragment θ, E), fragment mass, energy distributions for Z=4-12; deduced light particle emission mechanism.

doi: 10.1007/BF01418089
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1984CA31      Nucl.Phys. A427, 173 (1984)

C.Cabot, H.Gauvin, Y.Le Beyec, H.Delagrange, J.P.Dufour, Y.Llabador, A.Fleury, J.M.Alexander

Measurements of Evaporation Residues and Fission for 40Ar + 110Pd

NUCLEAR REACTIONS 110Pd(40Ar, X), (40Ar, F), E=164-262 MeV; measured fission fragment σ(θ), evaporation residue σ(θ), fusion σ; deduced evaporation residue, fission spin zones. Different theoretical models.

doi: 10.1016/0375-9474(84)90144-1
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1984ZH04      Nucl.Phys. A422, 447 (1984)

Z.Zheng, B.Borderie, D.Gardes, H.Gauvin, F.Hanappe, J.Peter, M.F.Rivet, B.Tamain, A.Zaric

Further Experimental Evidence for Fast Fission

NUCLEAR REACTIONS 238U, 209Bi(40Ar, X), (40Ar, F), E ≈ 175-350 MeV; 197Au(40Ar, X), (40Ar, F), E=150-350 MeV; measured (fragment)(fragment)-coin, fission type fragment mass energy distributions; deduced fusion σ(E), fast fission evidence.

doi: 10.1016/0375-9474(84)90526-8
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1982DE36      Z.Phys. A307, 305 (1982)

S.Della Negra, H.Gauvin, D.Jacquet, Y.Le Beyec

Q(β) Measurements and Mass Excess Values for Neutron Deficient Isotopes near N ≈ Z ≈ 40. I. Strontium, Yttrium and Zirconium Isotopes

RADIOACTIVITY 79Sr(β+) [from 54Fe(32S, n2pα), 50Cr(32S, n2p), E=123 MeV]; measured γγ-, (X-ray)γ-coin; deduced mass excess, Q(EC), log ft. 79Rb deduced levels, J, π, ICC, T1/2, γ-multipolarity, γ-branching. 80Y(β+) [from 54Fe(32S, np), E=123 MeV]; measured T1/2, γγ-, βγ-coin; deduced log ft, Q(EC), mass excess, Q(β). 80Sr deduced levels, J, π, T1/2, ICC. 81Zr(β+) [from 54Fe(32S, nα), E=123 MeV]; 81Y(β+) [from 81Zr decay]; measured T1/2, β-endpoint energies, βγ-, γ(X-ray)-coin; deduced Q(EC), Qβ, log ft, mass excess. 81Sr deduced levels, J, π, T1/2, γ-branching. 82Zr(β+), 82Y(β+) [from 82Zr decay]; measured T1/2, βγ-coin, Eγ; deduced mass excess. 82Zr deduced Q(EC). 82Sr deduced levels, J, π, T1/2 upper limit, γ-branching. 83Zr(β+) [from 54Fe(32S, n2p)], 83Y(β+) [from 54Fe(32S, 3p)], 83mY(β+) [from 83Zr decay]; measured T1/2, Eγ, γ(X-ray), βγ-, (mass)γ-coin; deduced Q(EC), mass excess. 83Y deduced levels, J, π, ICC, γ-multipolarity, T1/2 upper limit. 83Sr deduced levels. 83Zr deduced isomer, T1/2. 84Zr(β+) [from 54Fe(32S, 2p)]; measured T1/2, γ(X-ray)-coin. 85Zr(β+) [from 58Ni(32S, n4p)]; measured T1/2, βγ-coin; deduced Q(EC), mass excess.


1980CA21      Phys.Lett. B96, 55 (1980)

C.Cabot, S.Della Negra, H.Gauvin, H.Delagrange, J.P.Dufour, A.Fleury

Emission of Few Nucleons, Including only One Neutron in the 63Cu + 93Nb Reaction

NUCLEAR REACTIONS 93Nb(63Cu, n), (63Cu, np), (63Cu, 2np), (63Cu, 2n2p), E=228-300 MeV; measured absolute σ(E). Statistical compound nucleus decay model.

doi: 10.1016/0370-2693(80)90211-7
Citations: PlumX Metrics


1980CA27      J.Phys.(Paris), Colloq.C-10, 234 (1980)

C.Cabot, H.Gauvin, Y.Le Beyec, H.Delagrange, J.P.Dufour, A.Fleury, Y.Llabador, J.M.Alexander

Evaporation Residue and Fission Cross-Sections for the System: 40Ar + 110Pd

NUCLEAR REACTIONS, Fission 110Pd(40Ar, xn), (40Ar, xnp), (40Ar, xnα), (40Ar, X), (40Ar, F), E=140-260 MeV; 130Te(40Ar, X), (40Ar, F), (40Ar, xn), (40Ar, xnp), E=164.5-226 MeV; measured σ(evaporation residue), σ(fission), σ(fusion) vs E. 150Gd deduced fission characteristics. Statistical model.


1980DE13      Z.Phys. A295, 103 (1980)

C.Deprun, S.Della Negra, J.P.Husson, H.Gauvin, Y.Le Beyec

Mass Excess Values of 79Sr, 82Y and 83Y Obtained from Qβ Measurements

RADIOACTIVITY 79Sr, 82,83Y; measured Eβ, Qβ, T1/2; deduced mass excess. βγ-coin technique.

NUCLEAR REACTIONS 54Fe, 58Ni(32S, X), E=100-160 MeV; measured (K X-ray)(K X-ray)-, γγ-coin; deduced yield for 79Sr, 82,83Y. Tof.

doi: 10.1007/BF01414303
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1979HA05      Phys.Rev.Lett. 42, 218 (1979)

R.L.Hahn, K.S.Toth, C.Cabot, H.Gauvin, Y.LeBeyec

Remeasurement of 40Ar and 84Kr Excitation Functions Leading to the Same Compound Nucleus, 158Er

NUCLEAR REACTIONS 118Sn(40Ar, xn), E=259 MeV; 74Ge(84Kr, xn), E=620 MeV; measured σ(E) for X=5, 6; deduced evidence for independence hypothesis of compound nucleus formation, decay.

doi: 10.1103/PhysRevLett.42.218
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1978CA11      Z.Phys. A287, 71 (1978)

C.Cabot, S.Della Negra, C.Deprun, H.Gauvin, Y.Le Beyec

Copper Ion Induced Reactions on 110-108-106Cd, 109-107Ag and 110Pd. New Rhenium, Osmium and Iridium Isotopes

RADIOACTIVITY 171,168,169,170Ir, 169,165,166,167,168Os, 168,169Re; measured Eα, T1/2.

NUCLEAR REACTIONS 110Pd, 107,109Ag, 106,108,110Cd(63Cu, X), E=260-320 MeV; measured relative yields.

doi: 10.1007/BF01408363
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0108.


1978DE34      Nucl.Instrum.Methods 156, 355 (1978)

S.Della Negra, C.Deprun, H.Jungclas, H.Gauvin, J.P.Husson, Y.Le Beyec

The Time-of-Flight Mass Identification System Connected to the Alice He-Jet. 'On-Line' Experimental Results

NUCLEAR REACTIONS 121Sb, 118Sn(40Ar, xn), E not given; measured Eα. 152,153Er levels deduced T1/2. 103Rh, Ni, 27Al(12C, xn), E=67-92 MeV; measured β-recoil; deduced masses of mother, daughter isotopes. 64Zn, 60Ni, 28Si(32S, xn)E=100-190 MeV; measured β-recoil, T1/2; deduced evidence for 82Zr, 82Nb. Tof connected to He-jet technique.


1977CA23      Z.Phys. A283, 221 (1977)

C.Cabot, S.Della Negra, C.Deprun, H.Gauvin, Y.Le Beyec

New Osmium and Iridium Isotopes Produced Through 63Cu Induced Reactions

RADIOACTIVITY 165,166,167,168Os, 170Ir; measured Eα, T1/2.

NUCLEAR REACTIONS 110Cd, 109Ag(63Cu, xnyp); measured σ(E).

doi: 10.1007/BF01418716
Citations: PlumX Metrics


1977DE18      Z.Phys. A282, 65 (1977)

S.Della Negra, H.Gauvin, H.Jungclas, Y.Le Beyec, M.Lefort

Mechanism of Formation and Decay of the Compound Nuclei 150Gd Produced By Two Entrance Channels (16O + 134Ba) and (40Ar + 110Pd)

NUCLEAR REACTIONS 134Ba(16O, X), E=60-120 MeV; 110Pd(40Ar, X), E=140-230 MeV; measured complete fusion σ(E), σ(E) for production of 145,146,147Gd, 145,146,147Eu, 141mSm, 143mSm, 140mPm, 139mNd.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0129.


1977DE19      Z.Phys. A282, 75 (1977)

S.Della Negra, H.Gauvin, H.Jungclas, Y.Le Beyec, M.Lefort

Comparison between Experimental Decay of the Compound Nuclei 150Gd and Evaporation Calculations

NUCLEAR REACTIONS 134Ba(16O, X), E=60-120 MeV; 110Pd(40Ar, X), E=140-230 MeV; analyzed data, calculated σ.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0129.


1976AG01      Z.Phys. A278, 265 (1976)

S.Agarwal, H.Gauvin, D.Guerreau, H.Jungclas, Y.Le Beyec, M.Lefort, X.Tarrago

Evaporation Residue Cross Sections in Complete Fusion Reactions between 52Cr-56Fe, 63Cu-Ni and 63Cu-Ag

NUCLEAR REACTIONS 107,109Ag, 58,60Ni(63Cu, X), E=347 MeV; 56Fe(52Cr, X), E=207, 264 MeV; measured evaporation residue σ.

doi: 10.1007/BF01409177
Citations: PlumX Metrics


1976AN02      J.Phys.(Paris), Lett. 37, 5 (1976)

C.Andre, H.Gauvin, Y.Le Beyec, N.T.Porile

(3He, xn), (3He, pxn) and (3He, fission) Reactions on 206Pb between 80 and 200 MeV

NUCLEAR REACTIONS 206Pb(3He, 3n), (3He, 4n), (3He, 5n), (3He, 6n), (3He, 7n), 206Pb(3He, 8n), (3He, 9n), (3He, 10n), (3He, 11n), (3He, 12n), (3He, 13n), (3He, 14n), (3He, 2np), (3He, 3np), (3He, 5np), (3He, F), E=80-200 MeV; measured σ(E, θ); deduced reaction mechanism.

doi: 10.1051/jphys:019760037010500
Citations: PlumX Metrics


1975CA06      Nucl.Phys. A241, 341 (1975)

C.Cabot, C.Deprun, H.Gauvin, B.Lagarde, Y.Le Beyec, M.Lefort

Ca Induced Reactions on 141Pr and 150Sm: New Gold and Lead Isotopes 176Au, 175Au, 185Pb

RADIOACTIVITY 175,176,177Au, 185,187Pb [from 141Pr, 150Sm(40Ca, xn), 155Gd(40Ar, xn)]; measured Eα, T1/2. He jet technique.

NUCLEAR REACTIONS 141Pr, 150Sm(40Ca, xn), 155Gd(40Ar, xn), 180 < E < 290 MeV; measured relative σ(E, Eα).

doi: 10.1016/0375-9474(75)90323-1
Citations: PlumX Metrics


1975CA38      J.Phys.(Paris), Lett. 36, 1-289 (1975)

C.Cabot, H.Gauvin, Y.Le Beyec, M.Lefort

Range of Orbital Angular Momenta Available for Complete Fusion between Heavy Ions

NUCLEAR REACTIONS 142Nd(16O, 5n), E=50-80 MeV; 118Sn(40Ar, 5n), E=60-110 MeV; 74Ge(84Kr, 5n), E=80-110 MeV; analyzed previous data; deduced de-excitation process.


1975CA39      C.R.Acad.Sci., Ser.B 281, 453 (1975)

C.Cabot, C.Deprun, H.Gauvin, Y.Le Beyec, M.Lefort

Mise en Evidence d'un Nouvel Isotope de Mercure de Masse 177

RADIOACTIVITY 177Hg; measured Eα.


1975GA15      Phys.Lett. 58B, 163 (1975)

H.Gauvin, D.Guerreau, Y.Le Beyec, M.Lefort, F.Plasil, X.Tarrago

Evaporation Residue Cross Sections from Reactions with Argon Ions

NUCLEAR REACTIONS Ni, Ge, Sb(40Ar, X), E=167, 197, 227 MeV; Sb, Ag(40Ar, X), E=296 MeV; measured σ.

doi: 10.1016/0370-2693(75)90628-0
Citations: PlumX Metrics


1975GA25      Ann.Phys.(Paris) 9, 241 (1975)

H.Gauvin, Y.Le Beyec, J.Livet, J.L.Reyss

Characteristics of Alpha Activities for Neutron Deficient Nuclei with 65 ≤ Z ≤ 91

COMPILATION Z=65-91; compiled α-activity data, Eα, T1/2, α-branching for neutron-deficient nuclei.


1974DE34      Rev.Phys.Appl. 9, 895 (1974)

C.Deprun, H.Gauvin, B.Lagarde, Y.Le Beyec

Application de la Technique du Jet d'Helium a l'Identification en Ligne de Nouveaux Noyaux par la Detection de Laurs Rayonnements Gamma

RADIOACTIVITY 110,111,112Sb; measured T1/2, Eγ, Iγ.

NUCLEAR REACTIONS 103Rh(12C, xn), E=50-90 MeV; measured Eγ, Iγ; deduced yields of 110,111,112,113Sb.

doi: 10.1051/rphysap:0197400905089500
Citations: PlumX Metrics


1974GA09      Nucl.Phys. A220, 84 (1974)

H.Gauvin, R.L.Hahn, B.Lagarde, Y.Le Beyec, M.Lefort

Excitation Functions and α-Decay from Compound Nuclei in Ar Induced Reactions on 144Sm and 166Er

NUCLEAR REACTIONS 144Sm(Ar, xn2p), 166Er(Ar, xn2p), E=200-300 MeV; measured σ(E). Deduced evaporation mechanism.

doi: 10.1016/0375-9474(74)90753-2
Citations: PlumX Metrics


1974GA19      Nucl.Phys. A223, 103 (1974)

H.Gauvin, Y.Le Beyec, N.T.Porile

Nuclear Reactions of 118Sn, 121Sb, and 127I with Argon Ions

NUCLEAR REACTIONS 118Sn, 121Sb, 127I(40Ar, xn), (40Ar, pxn), (40Ar, xn2p), (40Ar, xn3p), E=150-280 MeV; measured σ(E); deduced σ(CF), J(crit), p-width/n-width.

doi: 10.1016/0375-9474(74)90279-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0015.


1974GA25      Phys.Rev. C10, 722 (1974)

H.Gauvin, Y.Le Beyec, M.Lefort, R.L.Hahn

Observed Differences between Argon- and Krypton-Induced Reactions Leading to the Same Compound Nuclei, 158Er and 156Er

NUCLEAR REACTIONS 70,72,74Ge(Kr, xn), 116,118Sn(Ar, xn), E=110-300 MeV; measured σ(E), σ(fusion).

doi: 10.1103/PhysRevC.10.722
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0036.


1973GA08      Nucl.Phys. A208, 360 (1973)

H.Gauvin, R.L.Hahn, Y.Le Beyec, M.Lefort, J.Livet

Reactions of 40Ar with 159Tb, 142Nd and 144Sm; New α-Activities from 189Bi, 173Pt and 177Au

RADIOACTIVITY 189Bi, 173,174,175,176Pt, 177Au [from 142Nd, 144Sm, 159Tb(40Ar, xpyn)]; measured T1/2, Eα, yield.

doi: 10.1016/0375-9474(73)90381-3
Citations: PlumX Metrics


1972BI12      Nucl.Phys. A189, 539 (1972)

R.Bimbot, H.Gauvin, Y.Le Beyec, M.Lefort, N.T.Porile, B.Tamain

Reactions de Transfert d'un Grand Nombre de Nucleons Induites par 84Kr Sur 232Th: Etude des Seuils de Reaction

NUCLEAR REACTIONS 232Th(84Kr, X), E=450-494 MeV; measured σ(E) for 226Th, 225Th, 224Ac, 223Ac formation.

doi: 10.1016/0375-9474(72)90312-0
Citations: PlumX Metrics


1972GA03      Phys.Rev.Lett. 28, 697 (1972)

H.Gauvin, Y.Le Beyec, M.Lefort, C.Deprun

Complete Fusion Nuclear Reactions Induced by Krypton Ions. Effective Threshold and Minimum Distance of Approach for the Reactions Cd116 + Kr84 and Ge72 + Kr84

NUCLEAR REACTIONS 72Ge, 116Cd(84Kr, X), E=350-494 MeV; measured σ(E); deduced threshold for complete fusion.

doi: 10.1103/PhysRevLett.28.697
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1972GA27      Phys.Rev.Lett. 29, 958 (1972)

H.Gauvin, Y.Le Beyec, M.Lefort, N.T.Porile

α Decay of Neutron-Deficient Isotopes of Bismuth and Lead Produced in (Ar, xn) and (Kr, xn) Reactions

RADIOACTIVITY 186,187,188,189,190Pb, 190,191Bi, 191mBi, 192,193Bi, 193mBi, 194,195Bi, 195mBi, 197mBi; measured Eα, T1/2; deduced α-branching ratios.

doi: 10.1103/PhysRevLett.29.958
Citations: PlumX Metrics


1971BI16      C.R.Acad.Sci., Ser.B, 273, 505 (1971)

R.Bimbot, C.Deprun, D.Gardes, H.Gauvin, Y.Le Beyec, M.Lefort, J.Peter, B.Tamain

Experiences Preliminaires sur les Reactions Nucleaires Induites par un Faisceau d'Ions Krypton de 450 a 500 MeV. Premiers Indices en Faveur de la Synthese de Noyaux Superlourds

NUCLEAR REACTIONS 74Ge, 116Cd, Th, U(Kr, X), E=450-500 MeV; measured charged particle spectra.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2216.


1971BI22      C.R.Acad.Sci., Ser.B 273, 1054 (1971)

R.Bimbot, H.Gauvin

Reactions de Spallation de Noyaux Legers Induites par des Protons de 50, 100 et 153 MeV

NUCLEAR REACTIONS N, O, 18O, F, Mg, Al, Si, Cl(p, X), E=50, 100, 153 MeV; measured σ for 7Be, 11C, 13N, 18F, 22,24Na, 34mCl formation.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2134.


1969AM01      J.Inorg.Nucl.Chem. 31, 577 (1969)

I.Amarel, H.Gauvin, A.Johnson

Delayed Neutron Emission Probabilities of Rb and Cs Precursors. The Half-Life of 97Rb

NUCLEAR REACTIONS, Fission 238U(p, F), E = 150 MeV; measured delayed neutron emission. Mass spectrometer.

RADIOACTIVITY 97Rb, 142,143,144Cs [from 238U(p, F)]; measured T1/2, delayed-n.

doi: 10.1016/0022-1902(69)80001-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23360.


1968DO20      Phys.Rev. 169, 836 (1968)

I.Dostrovsky, H.Gauvin, M.Lefort

(p, xp) and (p, xpyα) Reactions of 156-MeV Protons with Light Targets ( A=11 to A=27)

NUCLEAR REACTIONS B(p, x), 11B(p, 3p), C(p, x), 12C(p, 4p), 14N(p, x), 15N(p, x), 16O(p, x), 18O(p, 3p), 18O(p, x), 19F(p, 3p), 19F(p, 4p), 19F(p, x), Ne(p, x), 23Na(p, x), Mg(p, x), 27Al(p, x), Si(p, x), E=156 MeV; measured products, 9Li, 17N, 16C, Eπ, Iπ; deduced σ, σ(E). Data were imported from EXFOR entry C0237.

doi: 10.1103/PhysRev.169.836
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0237.


1967AM01      Phys.Letters 24B, 402 (1967)

I.Amarel, R.Bernas, R.Foucher, J.Jastrzebski, A.Johnson, J.Teillac, H.Gauvin

Half Life Determination of Some Short-Lived Isotopes of Rb, Sr, Cs, Ba, La and Identification of 93,94,95,96Rb as Delayed Neutron Precursors by On-Line Mass Spectrometry

NUCLEAR STRUCTURE 95Rb, 95Sr, 94Sr, 94Rb, 96Sr, 96Rb, 92Rb, 91Rb, 93Rb, 90Rb, 141Cs, 143Cs, 144Ba, 144Cs, 144La; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90305-X
Citations: PlumX Metrics


1967GA01      J.Phys. (Paris) 28, 129 (1967)

H.Gauvin, R.Chastel

Diffusion Quasi Elastique p - α dans le Carbone 12

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1051/jphys:01967002802012900
Citations: PlumX Metrics


1967GA19      J.Inorg.Nucl.Chem. 29, 2839 (1967)

H.Gauvin, L.Sauvage

Emission de Neutrons Differes dans la Fission de 238U, 232Th et 209Bi Induite par des Protons de 156 MeV

NUCLEAR REACTIONS, Fission 209Bi, 232Th, 238U(p, F), E=156 MeV; measured delayed neutron yields. 87,88Br, 137I deduced delayed neutron emission probability.

doi: 10.1016/0022-1902(67)80114-3
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0014.


1966GA15      Compt.Rend. 263B, 752 (1966)

H.Gauvin

Sections Efficaces de Production du Beryllium 7 dans Differents Isotopes d'Azote et d'Oxygene, et dans le Fluor 19. Comparaison avec la Production de Lithium 9.

NUCLEAR STRUCTURE 15N, 18O, 19F; measured not abstracted; deduced nuclear properties.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2132.


1962GA27      Nucl.Phys. 39, 447 (1962)

H.Gauvin, M.Lefort, X.Tarrago

Emission of alpha particles from the spallation reactions

NUCLEAR REACTIONS 12C(p, np), 12C(p, x), 27Al(p, x), 209Bi(p, x), 232Th(p, x), E=40-155 MeV; measured products, 227Pa, 224Ac, 225Ac, 226Ac, 228Ac, 211At, 219Ac, 210Bi, 222Ac, 208At, 209At, 210At, 22Na, 24Na, 7Be, 11C, Eπ, Iπ; deduced σ, σ(E). Data were imported from EXFOR entry C0394.

doi: 10.1016/0029-5582(62)90403-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0394.


1961GA07      Compt.Rend 253, 257 (1961)

H.Gauvin, R.Chastel, L.Vigneron

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.


1961SE13      J.Phys.Radium 22, 771 (1961)

W.Sebaoun, H.Gauvin


1960GA16      J.Phys.Radium 21, 893 (1960)

M.Garnier, H.Gauvin, W.Sebaoun

Cross Section for the Reaction C12(γ, 3α) at 14.8 and 17.6 MeV

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1051/jphysrad:019600021012089300
Citations: PlumX Metrics


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