NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = M.Kaczmarski Found 12 matches. 2024CZ01 Phys.Rev. C 109, L021601 (2024) K.Czerski, R.Dubey, M.Kaczmarski, A.Kowalska, N.Targosz-Sleczka, G.Das Haridas, M.Valat Indications of electron emission from the deuteron-deuteron threshold resonance
doi: 10.1103/PhysRevC.109.L021601
2020CZ02 Acta Phys.Pol. B51, 649 (2020) K.Czerski, N.Targosz-Sleczka, M.Kaczmarski Deuteron-Deuteron Reaction Cross Sections at Very Low Energies
doi: 10.5506/APhysPolB.51.649
2018TA21 Acta Phys.Pol. B49, 675 (2018) N.Targosz-Sleczka, K.Czerski, M.Kaczmarski, D.Weissbach, A.I.Kilic, G.Ruprecht, A.Huke, S.Policastro Electron Screening Effect in Nuclear Reactions in Metallic and Gaseous Targets NUCLEAR REACTIONS 2H(d, p)3H, E=6-25 keV; measured reaction σ enhancement in Zr under ultra-high-vacuum conditions; deduced enhancement factor; calculated, fitted enhancement factors to metalic target; deduced 0+ resonance reduces the screening energy to 105 eV in Zr and allows for much better description of deuteron energy dependence of the enhancement factor.
doi: 10.5506/aphyspolb.49.675
2017KA15 Acta Phys.Pol. B48, 489 (2017) M.Kaczmarski, K.Czerski, D.Weissbach, A.I.Kilic, G.Ruprecht, A.Huke Threshold Resonance Contribution to the Thick Target 2H(d, p)3H Reaction Yield NUCLEAR REACTIONS 2H(d, p), E=5-26 keV; calculated thick target electron screening and assumed narrow threshold rersonance influence on resonant S-factor and on σ. Compared to published thick target data of the same group.
doi: 10.5506/APhysPolB.48.489
2016CZ02 Europhys.Lett. 113, 22001 (2016) K.Czerski, D.Weissbach, A.I.Kilic, G.Ruprecht, A.Huke, M.Kaczmarski, N.Targosz-Sleczka, K.Maass Screening and resonance enhancements of the 2H(d, p)3H reaction yield in metallic environments NUCLEAR REACTIONS 2H(d, p), E<25 keV; measured reaction products. 4He; deduced σ, 0+ threshold resonance in 4He. Comparison with theoretical calculations performed within the T-matrix approximation.
doi: 10.1209/0295-5075/113/22001
2014KA19 Acta Phys.Pol. B45, 509 (2014) M.Kaczmarski, A.I.Kilic, K.Czerski, A.Kowalska, D.Weissbach, N.Targosz-Sleczka, A.Huke, G.Ruprecht New Accelerator Facility for Measurements of Nuclear Reactions at Energies Below 1 keV
doi: 10.5506/APhysPolB.45.509
2006KA09 J.Phys.(London) G32, 417 (2006) The choice of the optimum terms for semi-empirical description of s-wave neutron resonance level densities
doi: 10.1088/0954-3899/32/4/002
2005KA17 J.Phys.(London) G31, 669 (2005) The shell effects in s-wave neutron resonance level densities ρ according to combinatorial calculations and on the basis of the semi-classical approach
doi: 10.1088/0954-3899/31/7/012
2003KA23 Yad.Fiz. 66, 837 (2003); Phys.Atomic Nuclei 66, 804 (2003) The Analysis of the Densities of s-Wave Neutron Resonances Separated with Respect to Spin NUCLEAR STRUCTURE 45Sc, 51V, 55Mn, 59Co, 63,65Cu, 67Zn, 89Y, 147,149Sm, 155,157Gd, 159Tb, 163Dy, 165Ho, 167Er, 177,179Hf, 197Au, 235U, 237Np, 239Pu; analyzed neutron resonance level densities vs spin. Gilbert-Cameron formula.
doi: 10.1134/1.1576453
2000KA06 J.Phys.(London) G26, 253 (2000) The Empirical Description of the Level Density Parameter a in the Semi-Classical Model NUCLEAR STRUCTURE A=40-252; analyzed level density parameters.
doi: 10.1088/0954-3899/26/3/304
2000KA27 Yad.Fiz. 63, No 5, 828 (2000); Phys.Atomic Nuclei 63, 758 (2000) Semiempirical Formula for Describing Neutron Shell Effects in the Resonance-Level Density for s-Wave Resonances
doi: 10.1134/1.855703
1986KA09 Z.Phys. A323, 465 (1986) Calculation of Resonance Reduced Neutron Widths by Semiclassical Description NUCLEAR STRUCTURE N ≈ 10-150; calculated resonance reduced neutron widths. Semi-classical description.
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