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NSR database version of May 24, 2024.

Search: Author = F.Schneider

Found 14 matches.

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2024TI04      Phys.Rev.Lett. 132, 182501 (2024)

J.Tiedau, M.V.Okhapkin, K.Zhang, J.Thielking, G.Zitzer, E.Peik, F.Schaden, T.Pronebner, I.Morawetz, L.T.De Col, F.Schneider, A.Leitner, M.Pressler, G.A.Kazakov, K.Beeks, T.Sikorsky, T.Schumm

Laser Excitation of the Th-229 Nucleus

RADIOACTIVITY 229Th(IT); measured resonance fluorescence signal frequency; deduced the wavelength, the fluorescence lifetime in the crystal of Th-doped CaF2, isomer T1/2 for a nucleus isolated in vacuum. Nuclear laser spectroscopy and realizing optical nuclear clocks applications.

doi: 10.1103/PhysRevLett.132.182501
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2022KA45      Phys.Rev. C 106, 054325 (2022)

O.Kaleja, B.Andjelic, O.Bezrodnova, K.Blaum, M.Block, S.Chenmarev, P.Chhetri, C.Droese, Ch.E.Dullmann, M.Eibach, S.Eliseev, J.Even, P.Filianin, F.Giacoppo, S.Gotz, Yu.Gusev, M.J.Gutierrez, F.P.Hessberger, N.Kalantar-Nayestanaki, J.J.W.van de Laar, M.Laatiaoui, S.Lohse, N.Martynova, E.Minaya Ramirez, A.K.Mistry, T.Murbock, Yu.Novikov, S.Raeder, D.Rodriguez, F.Schneider, L.Schweikhard, P.G.Thirolf, A.Yakushev

Direct high-precision mass spectrometry of superheavy elements with SHIPTRAP

ATOMIC MASSES 251,254No, 254,255,256Lr, 257Rf; measured cyclotron frequency; deduced mass excesses, two-neutron shell gap. Comparison to AME2020. Phase-imaging ion-cyclotron resonance mass spectrometry (PI-ICR MS) at SHIPTRAP setup. Isotopes produced in following reactions 206Pb(48Ca, 3n)251No, E=4.8 MeV/nucleon, 208Pb(48Ca, 2n)254No, E=4.56 MeV/nucleon, 209Bi(48Ca, 3n)254Lr, E=4.81 MeV/nucleon, 209Bi(48Ca, 2n)255Lr, E=4.56 MeV/nucleon, 209Bi(48Ca, n)256Lr, E=4.5 MeV/nucleon, 208Pb(50Ti, n)257Rf, E=4.65 MeV/nucleon at GSI Darmstadt.

RADIOACTIVITY 258Db, 254Lr(α); deduced Q values. Comparison to other experimental data.

doi: 10.1103/PhysRevC.106.054325
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2022NO01      Phys.Rev. C 105, L021302 (2022)

S.Nothhelfer, Th.E.Albrecht-Schonzart, M.Block, P.Chhetri, Ch.E.Dullmann, J.G.Ezold, V.Gadelshin, A.Gaiser, F.Giacoppo, R.Heinke, T.Kieck, N.Kneip, M.Laatiaoui, Ch.Mokry, S.Raeder, J.Runke, F.Schneider, J.M.Sperling, D.Studer, P.Thorle-Pospiech, N.Trautmann, F.Weber, K.Wendt

Nuclear structure investigations of 253-255Es by laser spectroscopy

NUCLEAR MOMENTS 253,254,255Es; measured hyperfine spectra; deduced J, isotope shifts, hyperfine constants, nuclear spins, magnetic dipole moments, electric quadrupole moments. Comparison with previous experimental data. Laser resonance ionization spectroscopy. RISIKO mass separator at Johannes Gutenberg University Mainz.

doi: 10.1103/PhysRevC.105.L021302
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2017GA14      Eur.Phys.J. Special Topics 226, 1623 (2017)

L.Gastaldo, K.Blaum, K.Chrysalidis, T.Day Goodacre, A.Domula, M.Door, H.Dorrer, Ch.E.Dullmann, K.Eberhardt, S.Eliseev, C.Enss, A.Faessler, P.Filianin, A.Fleischmann, D.Fonnesu, L.Gamer, R.Haas, C.Hassel, D.Hengstler, J.Jochum, K.Johnston, U.Kebschull, S.Kempf, T.Kieck, U.Koster, S.Lahiri, M.Maiti, F.Mantegazzini, B.Marsh, P.Neroutsos, Yu.N.Novikov, P.C.O.Ranitzsch, S.Rothe, A.Rischka, A.Saenz, O.Sander, F.Schneider, S.Scholl, R.X.Schussler, Ch.Schweiger, F.Simkovic, T.Stora, Z.Szucs, A.Turler, M.Veinhard, M.Weber, M.Wegner, K.Wendt and K.Zuber

The electron capture in 163Ho experiment - ECHo

RADIOACTIVITY 163Ho(EC); measured decay products, X-rays; calculated electron capture spectrum; deduced sensitivity towards neutrino mass measurements.

doi: 10.1140/epjst/e2017-70071-y
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2015SC13      Eur.Phys.J. A 51, 89 (2015)

F.Schneider, T.Beyer, K.Blaum, M.Block, S.Chenmarev, H.Dorrer, Ch.E.Dullmann, K.Eberhardt, M.Eibach, S.Eliseev, J.Grund, U.Koster, Sz.Nagy, Yu.N.Novikov, D.Renisch, A.Turler, K.Wendt

Preparatory studies for a high-precision Penning-trap measurement of the 163Ho electron capture Q-value

doi: 10.1140/epja/i2015-15089-8
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2014EI01      Phys.Rev. C 89, 064318 (2014)

M.Eibach, T.Beyer, K.Blaum, M.Block, Ch.E.Dullmann, K.Eberhardt, J.Grund, Sz.Nagy, H.Nitsche, W.Nortershauser, D.Renisch, K.P.Rykaczewski, F.Schneider, C.Smorra, J.Vieten, M.Wang, K.Wendt

Direct high-precision mass measurements on 241, 243Am, 244Pu, and 249Cf

ATOMIC MASSES 241,243Am, 244Pu, 249Cf; measured Time-of-flight spectrum of carbon cluster ions, cyclotron frequencies by TOF-ICR technique using TRIGA-TRAP Penning-trap mass spectrometer at Mainz; deduced masses. Comparison with data in AME-2012. Analyzed AME-2012 masses of 84 nuclides in Z=82-112, N=129-166 region, and improved uncertainties with the use of new mass measurements in this work.

doi: 10.1103/PhysRevC.89.064318
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1988UN01      Hyperfine Interactions 39, 39 (1988)

S.Unterricker, F.Schneider

Quadrupole Coupling Constants of A(II)B(VI) Compounds with Wurtzite Structure

RADIOACTIVITY 111In(EC); measured γγ(θ, H, t); deduced quadrupole coupling constants in CdSe, CdTe, CdS.

doi: 10.1007/BF02394645
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1983UN01      Phys.Stat.Sol. (a) 75, 155 (1983)

S.Unterricker, F.Schneider

TDPAC Investigation of 111Cd in Silicon after Recoil Implantation of the Parent Nuclei 111In

RADIOACTIVITY 111In(EC) [from 109Ag(α, 2n)]; measured γγ(θ, H, t); deduced electric quadrupole interaction of 111Cd. Source recoil implantation in Si.

doi: 10.1002/pssa.2210750117
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1983UN02      Hyperfine Interactions 14, 119 (1983)

S.Unterricker, F.Schneider

TDPAC Measurement of the Quadrupole Interaction of 77Se in Arsenic

RADIOACTIVITY 77Br(EC), (β+) [from As(α, 2n), E=27 MeV]; measured γγ(θ, H, t); deduced electric field gradient for Se in As. 77Se level deduced quadrupole moment.

doi: 10.1007/BF02143938
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1983UN03      Hyperfine Interactions 15/16, 759 (1983)

S.Unterricker, F.Schneider, M.Zvara, P.Hlidek

111In(111Cd) Quadrupole Interaction in the Chalcogenide Spinel CdCr2Se4

RADIOACTIVITY 111In(EC); measured γγ(θ, H, t); deduced 111Cd quadrupole coupling, interaction. Chalcogenide spinel CdCr2Se4.

doi: 10.1007/BF02147360
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1981GE06      Hyperfine Interactions 9, 175 (1981)

H.Gerhardt, F.Jeschonnek, W.Makat, E.Matthias, H.Rinneberg, F.Schneider, A.Timmermann, R.Wenz, P.J.West

Nuclear Charge Radii and Nuclear Moments of Kr and Xe Isotopes by High Resolution Laser Spectroscopy

NUCLEAR MOMENTS 78,80,82,84,86Kr, 124,126,128,130,132,134,136Xe; measured optical isotope shift; deduced nuclear charge radius mass dependence. 85,83Kr, 129,131Xe; measured hfs; deduced coupling constants. 85,83Kr deduced quadrupole moment, μ ratios. High resolution laser spectroscopy, Doppler free measurement.

doi: 10.1007/BF01020915
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1980WE04      Z.Phys. A295, 303 (1980)

R.Wenz, E.Matthias, H.Rinneberg, F.Schneider

Further Evidence for a Linear Relationship between Changes in Nuclear Charge Radii and Binding Energy Per Nucleon

NUCLEAR MOMENTS 126,128,130,132,134,136,138Ba, 124,126,128,130,132,134,136Xe; analyzed isotope shift data; deduced linear variation of charge radii with binding energy per nucleon.

doi: 10.1007/BF01412212
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1979GE06      Z.Phys. A292, 7 (1979)

H.Gerhardt, E.Matthias, H.Rinneberg, F.Schneider, A.Timmermann, R.Wenz, P.J.West

Changes in Nuclear Mean Square Charge Radii of Stable Krypton Isotopes

ATOMIC PHYSICS 78,80,82,84,86Kr; measured isotope shift; deduced changes in mean-square charge radii. Optical transitions, polarization laser spectroscopy.

doi: 10.1007/BF01434624
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1978GE15      Z.Phys. A288, 327 (1978)

H.Gerhardt, E.Matthias, F.Schneider, A.Timmermann

Isotope Shifts and Hyperfine Structure of the 6s-7p Transitions in the Cesium Isotopes 133, 135, and 137

NUCLEAR STRUCTURE 133,135,137Cs; measured hfs; deduced isotope shift. Laser spectrometer.

doi: 10.1007/BF01417714
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