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NSR database version of May 6, 2024.

Search: Author = Z.Smit

Found 12 matches.

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2000KI32      Nucl.Instrum.Methods Phys.Res. B172, 182 (2000)

M.Kiisk, P.Persson, R.Hellborg, Z.Smit, B.Erlandsson, M.Faarinen, G.Skog, K.Stenstrom

Characteristic X-Ray Production in Heavy Ion Collisions

NUCLEAR REACTIONS Cr(58Ni, X), E=15-25 MeV; measured thick target X-ray production σ. Other targets with Z=22-32 also investigated.

doi: 10.1016/S0168-583X(00)00352-9
Citations: PlumX Metrics

1995JA23      Nucl.Instrum.Methods Phys.Res. B100, 10 (1995)

H.Janzekovic, Z.Smit, M.Budnar, A.Muhleisen, M.Ravnikar, V.Ramsak, P.Pelicon

K Shell Ionization Cross Sections of Au, Pb and Bi Induced by Low Energy Proton Impact

NUCLEAR REACTIONS 197Au, Pb, 209Bi(p, X), E=0.5-1.7 MeV; measured X-ray yields, K-shell ionization σ; deduced ionization mechanism.

ATOMIC PHYSICS 197Au, Pb, 209Bi(p, X), E=0.5-1.7 MeV; measured X-ray yields, K-shell ionization σ; deduced ionization mechanism.

doi: 10.1016/0168-583X(95)00351-7
Citations: PlumX Metrics

1994SM13      Phys.Rev. A50, 1301 (1994)

Z.Smit, I.Orlic

First-Order Theories for Adiabatic L-Shell Ionization by Protons

NUCLEAR REACTIONS Sn, Dy, Pb(p, X), E not given; analyzed L shell ionization σ vs reduced velocity parameter. Adiabatic ionization, PWBA, semi-classical methods.

ATOMIC PHYSICS Sn, Dy, Pb(p, X), E not given; analyzed L shell ionization σ vs reduced velocity parameter. Adiabatic ionization, PWBA, semi-classical methods.

doi: 10.1103/PhysRevA.50.1301
Citations: PlumX Metrics

1992BU09      Nucl.Instrum.Methods Phys.Res. B63, 377 (1992)

M.Budnar, A.Muhleisen, M.Hribar, H.Janzekovic, M.Ravnikar, Z.Smit, M.Zitnik

K-MM Radiative Auger Effect in Solid Ca, Ti and Cr Targets After Ionization with 0.7-1.5 MeV Protons

NUCLEAR REACTIONS Ca, Ti, Cr(p, X), E=0.7-1.5 MeV; measured radiative Auger X-ray spectra; deduced relative yields.

doi: 10.1016/0168-583X(92)95208-9
Citations: PlumX Metrics

1992GE02      Phys.Rev. A45, 2842 (1992)

M.Geretschlager, Z.Smit, E.Steinbauer

K-Shell Ionization Cross Sections of Al, Si, S, Ca, and Zn for Oxygen Ions in the Energy Range 1.1-8 MeV

NUCLEAR REACTIONS 27Al, Si, S, Ca, Zn(16O, X), E=1.1-8 MeV; measured ionization σ. Different target thicknesses. Model comparison.

ATOMIC PHYSICS 27Al, Si, S, Ca, Zn(16O, X), E=1.1-8 MeV; measured K-shell ionization σ. Different target thicknesses. Model comparison.

doi: 10.1103/PhysRevA.45.2842
Citations: PlumX Metrics

1992SM07      Phys.Rev. A46, 1367 (1992)

Z.Smit

Light-Ion-Induced K-Shell Ionization in the Adiabatic Region

NUCLEAR REACTIONS Mg, 31P, Ti, Mo(p, X), E not given; calculated K-shell ionization σ.

ATOMIC PHYSICS Mg, 31P, Ti, Mo(p, X), E not given; calculated K-shell ionization σ.

doi: 10.1103/PhysRevA.46.1367
Citations: PlumX Metrics

1991SM05      Z.Phys. D22, 411 (1991)

Z.Smit

Semiclassical Approach to K Shell Ionization: Hydrogenic wave functions

NUCLEAR REACTIONS Ni, Ag, Ho, Pb(p, X), E ≤ 23 MeV; calculated K-shell ionization σ. Semi-classical approach.

ATOMIC PHYSICS Ni, Ag, Ho, Pb(p, X), E ≤ 23 MeV; calculated K-shell ionization σ. Semi-classical approach.

doi: 10.1007/BF01438566
Citations: PlumX Metrics

1990GE01      Phys.Rev. A41, 123 (1990)

M.Geretschlager, Z.Smit, O.Benka

K-Shell Ionization Cross Sections for Si, P, K, Ca, Zn, and Ga by Protons and Carbon Ions in the Energy Range 1-6.4 MeV

NUCLEAR REACTIONS Si, 31P, S, 39K, Ca, Zn, Ga(p, X), E=1, 2 MeV; Si, 31P, S, 39K, Ca, Zn, Ga(C, X), E=1-6.4 MeV; measured absolute K-shell ionization σ.

ATOMIC PHYSICS Si, 31P, S, 39K, Ca, Zn, Ga(p, X), E=1, 2 MeV; Si, 31P, S, 39K, Ca, Zn, Ga(C, X), E=1-6.4 MeV; measured absolute K-shell ionization σ.

doi: 10.1103/PhysRevA.41.123
Citations: PlumX Metrics

1989CI06      J.Phys.(London) B22, 2161 (1989)

V.Cindro, M.Budnar, M.Kregar, V.Ramsak, Z.Smit

Double K-Shell Vacancy Production in Ca, Ti, V and Cr Bombarded by Protons

NUCLEAR REACTIONS Ca, Ti, V, Cr(p, X), E=1.3-1.7 MeV; measured X-ray spectra; deduced double K-shell ionization σ.

ATOMIC PHYSICS Ca, Ti, V, Cr(p, X), E=1.3-1.7 MeV; measured X-ray spectra; deduced double K-shell ionization σ.

doi: 10.1088/0953-4075/22/13/020
Citations: PlumX Metrics

1989OR06      Nucl.Instrum.Methods Phys.Res. B40/41, 108 (1989)

I.Orlic, M.Budnar, V.Cindro, Z.Smit, V.Valkovic

Low-Z Inner-Shell Ionization Cross Sections for 0.5-1.5 MeV H and He Ions

NUCLEAR REACTIONS Na, Cl, Mg, 27Al, Si, O, Ga, P, Ca, F, Ti, V, Cr, Fe, 59Co, Ni, Cu, Zn, As(p, X), E=0.5-1.5 MeV; Na, Cl, Mg, 27Al, Si, O, Ga, P, Ca, F, Ti, V, Cr, Fe, 59Co, Ni, Cu, Zn, As(α, X), E=0.7-1.3 MeV; measured subshell ionization σ.

ATOMIC PHYSICS Na, Cl, Mg, 27Al, Si, O, Ga, P, Ca, F, Ti, V, Cr, Fe, 59Co, Ni, Cu, Zn, As(p, X), E=0.5-1.5 MeV; Na, Cl, Mg, 27Al, Si, O, Ga, P, Ca, F, Ti, V, Cr, Fe, 59Co, Ni, Cu, Zn, As(α, X), E=0.7-1.3 MeV; measured subshell ionization σ.

doi: 10.1016/0168-583X(89)90934-8
Citations: PlumX Metrics

1988GE07      J.Phys.(London) B21, L603 (1988)

M.Geretschlager, Z.Smit, O.Benka

Molecular Orbit Effects in K-Shell Ionisation Induced by Carbon Ions

NUCLEAR REACTIONS Si, P, S, K, Ca(12C, X), E=1-6.4 MeV; measured X-rays; deduced K-shell ionization σ.

ATOMIC PHYSICS Si, P, S, K, Ca(12C, X), E=1-6.4 MeV; measured X-rays; deduced K-shell ionization σ.

doi: 10.1088/0953-4075/21/4/014
Citations: PlumX Metrics

1984CI08      Fizika(Zagreb) 16, 225 (1984)

V.Cindro, M.Budnar, V.Ramsak, M.Ravnikar, Z.Smit, M.Kregar

Ca and Ti K(α) Hypersatellities Induced by Protons

ATOMIC PHYSICS Ca, Ti(p, X), E=1.5-1.7 MeV; measured E X-ray, I X-ray, double, single K-shell ionization σ. Thick targets.

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