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NSR database version of April 27, 2024.

Search: Author = H.Tricoire

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1988CH45      Nucl.Instrum.Methods Phys.Res. A273, 748 (1988)

Y.Charon, J.C.Cuzon, H.Tricoire, L.Valentin

A High Resolution β^- Detector

RADIOACTIVITY ³H, ³²P, ³⁵S(β^-); measured β-detector efficiency. High resolution.

doi: 10.1016/0168-9002(88)90090-3
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1986TR03      Z.Phys. A323, 163 (1986)

H.Tricoire, C.Gerschel, A.Gillibert, N.Perrin

Evidence for Large Angular Momentum Window Associated with Incomplete Fusion Reactions

NUCLEAR REACTIONS ¹¹⁶Sn(¹⁶O, xnypzα), E=125 MeV; ¹²⁴Sn(¹⁶O, xnypzα), E=90, 100 MeV; measured γ(charged particle)-coin; deduced fast α-emission probability, incomplete fusion angular momentum size.

1985GE09      Z.Phys. A322, 433 (1985)

C.Gerschel, A.Gillibert, N.Perrin, H.Tricoire

Direct Particle Emission in Incomplete Fusion Reactions of ¹⁶O ^116-124Sn Targets at 75, 90 and 125 MeV

NUCLEAR REACTIONS ¹¹⁶Sn(¹⁶O, xnypzα), E=125 MeV; meaured αα-, αp-, αn-coin; deduced particle emission threshold, reaction mechanism.

doi: 10.1007/BF01412078
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1984TR08      Z.Phys. A317, 347 (1984)

H.Tricoire

Competition between Inertial and PEP Emission in Incomplete Fusion Reactions

NUCLEAR REACTIONS ¹²⁴Sn(¹⁶O, xα), E=125 MeV; calculated σ(θα), mean polarization, initial angular momentum vs θα; deduced inertial, preequilibrium emission competition. Incomplete fusion.

doi: 10.1007/BF01438368
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1984TR11      Phys.Rev.Lett. 53, 1630 (1984)

W.Trautmann, O.Hansen, H.Tricoire, W.Hering, R.Ritzka, W.Trombik

Dynamics of Incomplete Fusion Reactions from γ-Ray Circular-Polarization Measurements

NUCLEAR REACTIONS ^144,154Sm(¹⁶O, αX), E=110, 140 MeV; ⁹³Nb(¹⁶O, αX), E=110, 120, 140 MeV; ⁹³Nb(¹⁶O, pX), E=95 MeV; measured γ CP(charged particle)-coin, inclusive σ(Eα), proton polarization.

doi: 10.1103/PhysRevLett.53.1630
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1983TR09      Z.Phys. A312, 221 (1983)

H.Tricoire

Emission of Direct Particles in Heavy Ions Collisions

NUCLEAR REACTIONS ¹²⁴Sn(¹⁶O, α), E=75, 90, 125 MeV; ¹²⁴Sn(²⁰Ne, α), E=94, 112, 156 MeV; calculated σ(θ), σ(Eα), σ(fusion), fast α-emission probability vs L, σ vs E. Prompt emission model.

doi: 10.1007/BF01412165
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1982TR02      Z.Phys. A306, 127 (1982)

H.Tricoire, C.Gerschel, N.Perin, H.Sergolle, L.Valentin, D.Bachelier, H.Doubre, J.Gizon

Direct α Particle Emission in Incomplete Fusion Reaction on a Spherical Target ¹²⁴Sn

NUCLEAR REACTIONS ¹²⁴Sn(¹⁶O, α), E=90, 105, 125 MeV; ¹²⁴Sn(¹⁹F, α), E=104 MeV; ¹²⁴Sn(²⁰Ne, α), E=112, 156 MeV; measured σ(θα), σ(Eα, θα), γ-multiplicities; deduced L(critical). Direct α-emission, incomplete fusion.

doi: 10.1007/BF01415482
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1980GE12      J.Phys.(Paris), Colloq.C-10, 239 (1980)

C.Gerschel, N.Perrin, L.Valentin, H.Tricoire, B.Ader, D.Paya

How Fast α Particles are Emitted in Massive Transfer Reactions < Question >

NUCLEAR REACTIONS ¹¹⁶Sn(¹⁶O, α), E=125 MeV; ⁹²Zr(⁴⁰Ar, α), E=193 MeV; measured σ(Eα), γα-coin, γ-multiplicity. ¹³²Ce deduced α-decay mechanisms.

1979TR10      J.Phys.(Paris), Lett. 40, L-181 (1979)

H.Tricoire, P.Colombani, C.Gerschel, D.Paya, N.Perrin, L.Valentin, N.Frascaria, J.P.Garron, C.Stephan

New Experimental Results Supporting the Hypothesis of the Excitation of Collective Modes in the ⁴⁰Ca + ⁴⁰Ca Reaction

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), E=400 MeV; measured σ(fragment E, θ), γ-multiplicity vs excitation energy for fragment Z=17, 18; deduced evidence for collective mode excitation.

doi: 10.1051/jphyslet:01979004008018100
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