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NSR database version of April 11, 2024.

Search: Author = P.Rymuza

Found 17 matches.

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2006GO30      Eur.Phys.J. A 27, Supplement 1, 181 (2006)

A.Gojska, D.Chmielewska, P.Rymuza, J.Rzadkiewicz, Z.Sujkowski, T.Adachi, H.Fujita, Y.Fujita, Y.Shimbara, K.Hara, Y.Shimizu, H.P.Yoshida, Y.Haruyama, J.Kamiya, H.Ogawa, M.Saito, M.Tanaka

Radiative and non-radiative electron capture from carbon atoms by relativistic helium ions

ATOMIC PHYSICS C(3He, 3He), E=150 MeV/nucleon; measured ionization yields following radiative and non-radiative electron capture.

doi: 10.1140/epja/i2006-08-027-4
Citations: PlumX Metrics


1996LU13      Phys.Rev. A54, 232 (1996)

T.Ludziejewski, P.Rymuza, Z.Sujkowski, G.Borchert, J.-Cl.Dousse, C.Rheme, M.Polasik

Electron-Impact-Induced K Plus M Shell Ionization in Solid Targets of Medium-Z Elements Studied by Means of High-Resolution X-Ray Spectroscopy

ATOMIC PHYSICS Zr, 93Nb, Mo, Pd(e, X), E=150, 300 keV; measured X-ray spectra; deduced total K-, M-shell ionization probabilities vs target Z. Multi-configuration Dirac-Fock calculations.

doi: 10.1103/PhysRevA.54.232
Citations: PlumX Metrics


1996RY02      Acta Phys.Pol. B27, 573 (1996)

P.Rymuza, Th.Stohlker, H.Geissel, C.Kozhuharov, P.H.Mokler, R.Moshammer, F.Nickel, C.Scheidenberger, Z.Stachura, A.Warczak

State Selective Capture Measured for Fast H-Like Bi Projectiles in Collisions with Ni Target Atoms

NUCLEAR REACTIONS Ni(209Bi, X), E ≈ 82-200 MeV/nucleon; measured Doppler corrected (X-ray)(e)-coin, I(K X-ray) ratio; deduced electron capture σ(E).


1995BO36      Phys.Rev. A51, 3650 (1995)

B.Boschung, J.-Cl.Dousse, B.Galley, Ch.Herren, J.Hoszowska, J.Kern, Ch.Rheme, Z.Halabuka, T.Ludziejewski, P.Rymuza, Z.Sujkowski, M.Polasik

Kα Hypersatellite Lines of Medium-Mass Atoms Induced by 100-MeV 4He2+ Ions

NUCLEAR REACTIONS Zr, Mo, Pd(α, X), E=100 MeV; measured X-ray spectra; deduced double K-shell ionization σ. Model comparison.

ATOMIC PHYSICS Zr, Mo, Pd(α, X), E=100 MeV; measured X-ray spectra; deduced double K-shell ionization σ. Model comparison.

doi: 10.1103/PhysRevA.51.3650
Citations: PlumX Metrics


1995BO44      Phys.Rev. A52, 3889 (1995)

B.Boschung, M.W.Carlen, J.-Cl.Dousse, B.Galley, Ch.Herren, J.Hoszowska, J.Kern, Ch.Rheme, T.Ludziejewski, P.Rymuza, Z.Sujkowski, Z.Halabuka

Probabilities for L-Shell Ionization in Intermediate-Velocity Collisions of Medium-Mass Elements with 4He2+ Ions

NUCLEAR REACTIONS Zr, Mo, Pd, Pr(α, X), E=28-100 MeV; measured X-ray spectra; deduced L-shell ionization probabilities. High resolution transmission curved crystal spectrometer.

ATOMIC PHYSICS Zr, Ho, Pd, Pr(α, X), E=28-100 MeV; measured X-ray spectra; deduced L-shell ionization probabilities. High resolution transmission curved crystal spectrometer.

doi: 10.1103/PhysRevA.52.3889
Citations: PlumX Metrics


1995KA61      Z.Phys. D35, 15 (1995)

T.Kandler, Th.Stohlker, P.H.Mokler, C.Kozhuharov, H.Geissel, C.Scheidenberger, P.Rymuza, Z.Stachura, A.Warczak, R.W.Dunford, J.Eichler, A.Ichihara, T.Shirai

Photon Angular Distribution of Radiative Electron Capture into the M Shell of He-Like Uranium Ions at 110-140 MeV/u

NUCLEAR REACTIONS C(U, X), E at 110-140 MeV/nucleon; measured radiative electron capture (into M-shell) associated γ(θ).

doi: 10.1007/BF01439978
Citations: PlumX Metrics


1995LU24      Phys.Rev. A52, 2791 (1995)

T.Ludziejewski, P.Rymuza, Z.Sujkowski, B.Boschung, J.-Cl.Dousse, B.Galley, Z.Halabuka, Ch.Herren, J.Hoszowska, J.Kern, Ch.Rheme, M.Polasik

High-Resolution Study of the Kβ2 X-Ray Spectra Induced by Proton and Photon Impact on Zr, Mo, and Pd Targets

NUCLEAR REACTIONS Zr, Mo, Pd(γ, X), E ≤ 25 keV; Zr, Mo, Pd(p, X), E=16, 25, 45 MeV; measured X-ray spectra; deduced sub-shell ionization probabilities. Transmission bent crystal spectrometer.

ATOMIC PHYSICS Zr, Mo, Pd(γ, X), E ≤ 25 keV; Zr, Mo, Pd(p, X), E=16, 25, 45 MeV; measured X-ray spectra; deduced sub-shell ionization probabilities. Transmission bent crystal spectrometer.

doi: 10.1103/PhysRevA.52.2791
Citations: PlumX Metrics


1994CA20      Phys.Rev. A49, 2524 (1994)

M.W.Carlen, B.Boschung, J.-Cl.Dousse, Z.Halabuka, J.Hoszowska, J.Kern, Ch.Rheme, M.Polasik, P.Rymuza, Z.Sujkowski

M-Shell Ionization Resulting from Near-Central Collisions of Mid-Z Atoms with 5.5-MeV/amu Oxygen Ions

NUCLEAR REACTIONS Pd, La(16O, X), E=5.5 MeV/nucleon; measured K X-ray spectra; deduced average M-shell, M-subshell ionization probabilities. Multiconfiguration Dirac-Fock calculations.

ATOMIC PHYSICS Pd, La(16O, X), E=5.5 MeV/nucleon; measured K X-ray spectra; deduced average M-shell, M-subshell ionization probabilities. Multiconfiguration Dirac-Fock calculations.

doi: 10.1103/PhysRevA.49.2524
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1994LU09      Acta Phys.Pol. B25, 699 (1994)

T.Ludziejewski, P.Rymuza, Z.Sujkowski, D.Anagnostopoulos, G.Borchert, M.Carlen, J.-Cl.Dousse, J.Hoszowska, J.Kern, Ch.Rheme

L-Shell Ionization Probabilities in Near Central Heavy Ion-Atom Collisions

NUCLEAR REACTIONS U(Ne, X), E=500 MeV; Pd(O, X), E=86.4 MeV; Tb(Ne, X), E=300 MeV; Tb(N, X), E=210 MeV; Mo(O, X), E=88 MeV; Nd(N, X), E=210 MeV; Ta(N, X), E=350 MeV; La(N, X), E=403 MeV; measured X-ray yield distributions; deduced L-shell ionization probabilities.

ATOMIC PHYSICS U(Ne, X), E=500 MeV; Pd(O, X), E=86.4 MeV; Tb(Ne, X), E=300 MeV; Tb(N, X), E=210 MeV; Mo(O, X), E=88 MeV; Nd(N, X), E=210 MeV; Ta(N, X), E=350 MeV; La(N, X), E=403 MeV; measured X-ray yield distributions; deduced L-shell ionization probabilities.


1994SC42      Nucl.Instrum.Methods Phys.Res. B90, 36 (1994)

C.Scheidenberger, H.Geissel, Th.Stohlker, H.Folger, H.Irnich, C.Kozhuharov, A.Magel, P.H.Mokler, R.Moshammer, G.Munzenberg, F.Nickel, M.Pfutzner, P.Rymuza, W.Schwab, J.Ullrich, B.Voss

Charge States and Energy Loss of Relativistic Heavy Ions in Matter

NUCLEAR REACTIONS C, 27Al, Ni(209Bi, X), E=82 MeV/nucleon; measured X-ray spectra. C, Ni(209Bi, X), (197Au, X), E=80-1000 MeV/nucleon; measured total EC-capture σ vs E, ionization σ. Solid, gaseous media.

doi: 10.1016/0168-583X(94)95506-9
Citations: PlumX Metrics


1992LU02      Nucl.Instrum.Methods Phys.Res. B63, 494 (1992)

J.Ludziejewski, J.Hoszowska, P.Rymuza, Z.Sujkowski, D.Anagnostopoulos, G.Borchert, M.Carlen, J.-Cl.Dousse, Ch.Rheme, A.G.Drentje

In-Beam Bent-Crystal Spectrometer for Studies of Multiple Inner Shell Ionization

RADIOACTIVITY 170Tm(β-); measured γ-line profile, X-ray spectra; deduced 170Yb γ-line calibration. Bent quartz crystal spectrometer.

NUCLEAR REACTIONS 159Tb(α, X), E=60 MeV; 159Tb(20Ne, X), E=300 MeV; measured K X-ray spectra; deduced L-shell ionization probabilities. Bent quartz crystal spectrometer.

doi: 10.1016/0168-583X(92)95224-F
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1990CA38      Europhys.Lett. 13, 231 (1990)

M.Carlen, J.-Cl.Dousse, M.Gasser, J.Kern, Ch.Rheme, P.Rymuza, Z.Sujkowski, D.Trautmann

X-Ray Kβ Satellites Induced in Molybdenum by 4He Ions

NUCLEAR REACTIONS Mo(α, X), E=28 MeV; measured K X-ray spectra; deduced M-shell ionization probability.

ATOMIC PHYSICS Mo(α, X), E=28 MeV; measured K X-ray spectra; deduced M-shell ionization probability.

doi: 10.1209/0295-5075/13/3/007
Citations: PlumX Metrics


1990RY05      Nucl.Phys. A517, 159 (1990)

P.Rymuza, D.Chmielewska, Z.Sujkowski, G.J.Balster, B.Kotlinski, R.H.Siemssen, H.W.Wilschut

K-Shell Ionization Induced by 4.5 MeV/u 40Ar Ions Undergoing Fusion Reactions

NUCLEAR REACTIONS 51V, 59Co, 62Ni(40Ar, xnypzα), E=180 MeV; measured E (X-ray), I(X-ray), (X-ray)γ-, (X-ray)p-, (X-ray)α-coin; deduced projectile induced K-shell ionization probability, Doppler, multiple ionization energy shifts.

ATOMIC PHYSICS 51V, 59Co, 62Ni(40Ar, xnypzα), E=180 MeV; measured E (X-ray), I (X-ray), (X-ray)γ-, (X-ray)p-, (X-ray)α-coin; deduced projectile induced K-shell ionization probability, Doppler, multiple ionization energy shifts.

doi: 10.1016/0375-9474(90)90266-O
Citations: PlumX Metrics


1989RY05      Z.Phys. D14, 37 (1989)

P.Rymuza, Z.Sujkowski, M.Carlen, J.-Cl.Dousse, M.Gasser, J.Kern, B.Perny, Ch.Rheme

Distribution of KαL(n) Satellite Yields for Medium Z Elements Bombarded with 16O Ions

NUCLEAR REACTIONS Mo, Pd(16O, X), E=5.5 MeV/nucleon; measured K-X-ray spectra; deduced satellite yield distributions, L-shell ionization probabilities. Dumond type curved crystal spectrometer.

doi: 10.1007/BF01401341
Citations: PlumX Metrics


1987PE16      Phys.Rev. A36, 2120 (1987)

B.Perny, J.-Cl.Dousse, M.Gasser, J.Kern, Ch.Rheme, P.Rymuza, Z.Sujkowski

High-resolution Study of Heavy-Ion-Induced Kα x-Ray Spectra of Molybdenum Atoms

NUCLEAR REACTIONS Mo(α, X), E=6.7 MeV/nucleon; Mo(16O, X), E=5.5 MeV/nucleon; measured K X-ray spectra.

doi: 10.1103/PhysRevA.36.2120
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1987SU14      Phys.Lett. 196B, 122 (1987)

Z.Sujkowski, D.Chmielewska, P.Rymuza, G.J.Balster, B.Kotlinski, R.H.Siemssen, H.W.Wilschut

Direct Inner Shell Ionization accompanying Nuclear Fusion Reactions with Heavy Ions

NUCLEAR REACTIONS 51V, 59Co, 62Ni(40Ar, X), E=4.5 MeV/nucleon; measured fusion evaporation residue K X-ray spectra, yields; deduced prior fusion K-shell ionization.

doi: 10.1016/0370-2693(87)90590-9
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1985KO30      Phys.Rev. C32, 1612 (1985)

R.Kossakowski, J.Jastrzebski, P.Rymuza, W.Skulski, A.Gizon, S.Andre, J.Genevey, J.Gizon, V.Barci

Heavy Residues following 5-10 MeV/Nucleon 12C- and 14N- Induced Reactions on Sm and Pr Targets

NUCLEAR REACTIONS, ICPND 147Sm, 141Pr(12C, X), E=82-110 MeV; 147Sm(12C, X), E=90-110 MeV; 154,150Sm(12C, X), E=90, 110 MeV; 152Sm(12C, X), E=71-110 MeV; 144Sm(14N, X), E=80-107 MeV; 147,150,152Sm(14N, X), E=80-120 MeV; 141Pr(14N, X), E=68-120 MeV; measured Eγ, Iγ; deduced fusion σ(E). 144,147Sm(14N, xn), E=80-120 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 153,154,155,156,157Tm deduced levels. 141Pr(14N, 3n), (14N, 4n), (14N, 5n), (14N, 6n), (14N, 7n), (14N, 2np), (14N, 3np), (14N, 4np), (14N, 5np), (14N, 6np), E=threshold-120 MeV; measured residuals production σ(E).

doi: 10.1103/PhysRevC.32.1612
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0366.


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