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NSR database version of April 27, 2024.

Search: Author = C.Heitz

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2002EL14      Nucl.Instrum.Methods Phys.Res. B197, 271 (2002)

Y.El Masri, N.Moroso, V.Zaconte, C.Heitz, J.Cabrera, C.Dufauquez, V.Roberfroid, J.Van Mol, J.Lehmann, F.Vanderbist, P.Leleux, M.Couder

Analysis of ⁴He implanted in Al foils using the ⁴He(p, p)⁴He backscattering interaction

NUCLEAR REACTIONS ⁴He, Al(p, p), E ≈ 2.2 MeV; measured Ep, σ(θ); deduced helium implantation profile.

doi: 10.1016/S0168-583X(02)01467-2
Citations: PlumX Metrics

1994NE07      Nucl.Instrum.Methods Phys.Res. B85, 123 (1994)

M.Nekab, A.Pape, Ch.Heitz

A Study of the Ionization of Al, Si, S, Sc, Ti and V by Ar Ions in the Range 1-5 MeV

NUCLEAR REACTIONS ²⁷Al, Si, S, ⁴⁵Sc, Ti, V, ³¹P, Cl, K, Ca(Ar, X), E=1-5 MeV; measured X-ray yields; deduced projectile, target X-ray production σ.

ATOMIC PHYSICS ²⁷Al, Si, S, ⁴⁵Sc, Ti, V, ³¹P, Cl, K, Ca(Ar, X), E=1-5 MeV; measured X-ray yields; deduced projectile, target X-ray production σ.

doi: 10.1016/0168-583X(94)95798-3
Citations: PlumX Metrics

1990LI39      Europhys.Lett. 13, 401 (1990)

E.Liatard, J.F.Bruandet, F.Glasser, S.Kox, T.U.Chan, G.J.Costa, C.Heitz, Y.El Masri, F.Hanappe, R.Bimbot, D.Guillemaud-Mueller, A.C.Mueller

Matter Distribution in Neutron-Rich Light Nuclei and Total Reaction Cross-Section

NUCLEAR STRUCTURE ^6,7,8,9,11Li, ^{9,10,11,12,14}Be, ^{10,11,12,13,14,15,17}B; analyzed data; deduced rms radii.

doi: 10.1209/0295-5075/13/5/004
Citations: PlumX Metrics

1989SA10      Z.Phys. A332, 457 (1989)

M.G.Saint-Laurent, R.Anne, D.Bazin, D.Guillemaud-Mueller, U.Jahnke, Jin Gen-Ming, A.C.Mueller, J.F.Bruandet, F.Glasser, S.Kox, E.Liatard, Tsan Ung Chan, G.J.Costa, C.Heitz, Y.El-Masri, F.Hanappe, R.Bimbot, E.Arnold, R.Neugart

Total Cross Sections of Reactions Induced by Neutron-Rich Light Nuclei

NUCLEAR REACTIONS Cu(X, X), E not given; measured reaction σ for projectile X=^4,6He, ^6,7,8,9,11Li, ^{7,9,10,11,12,14}Be, ^{10,11,12,13,14,15,17}B, ^{11,12,13,14,15,16,17,18,19}C, ^{13,14,15,16,17,18,19}N, ^{15,16,17,18,19,20,21}O, ^18,19,20,21F, ^20,21Ne. Secondary beams, 4π γ method.

1986LI27      Z.Phys. D2, 223 (1986)

E.Liatard, J.F.Bruandet, F.Glasser, Tsan Ung Chan, G.J.Costa, C.Gerardin, C.Heitz, M.Samri, R.Seltz

K-Shell Ionization Induced by 30 MeV/u Argon and Neon Beams

NUCLEAR REACTIONS ⁵⁹Co, Cu, ⁸⁹Y, ⁹²Mo, Ag, Sm, ¹⁶⁵Ho, ¹⁸¹Ta, Pt, ¹⁹⁷Au, ²⁰⁹Bi, ²³²Th(²⁰Ne, X), (⁴⁰Ar, X), E=30 MeV/nucleon; measured X-ray spectra; deduced K-shell ionization σ ratio.

doi: 10.1007/BF01429077
Citations: PlumX Metrics

1984SZ01      ATOMKI Kozlem. 26, 67 (1984)

I.M.Szoghy, G.J.Costa, C.Gerardin, Ch.Heitz, R.Seltz

Emission of Prompt X-Rays following the Fusion of ³⁵Cl and ⁵⁹Co Nuclei

NUCLEAR REACTIONS ⁵⁹Co(³⁵Cl, X), E=100 MeV; measured E(X-ray), I(X-ray), γ(X-Ray)-coin; deduced Sr, Y, Zr, Nb, Mo relative yields. Evaporation following fusion.

1981CO23      Radiochim.Acta 28, 7 (1981)

K.E.Collins, C.H.Collins, C.Heitz

Use of Kβ/Kα Intensity Ratios for the Study of Annealing Processes in ⁵¹Cr-Doped Solids

RADIOACTIVITY ⁵¹Cr(EC); measured I(K X-ray) ratios; deduced annealing process in doped solids.