NSR Query Results
Output year order : Descending NSR database version of May 8, 2024. Search: Author = F.Smend Found 56 matches. 2004KO11 Eur.Phys.J. A 19, 391 (2004) K.Kossert, M.Camen, F.Wissmann, J.Ahrens, J.R.M.Annand, H.-J.Arends, R.Beck, G.Caselotti, P.Grabmayr, O.Jahn, P.Jennewein, M.I.Levchuk, A.I.L'vov, J.C.McGeorge, A.Natter, V.Olmos de Leon, V.A.Petrunkin, G.Rosner, M.Schumacher, B.Seitz, F.Smend, A.Thomas, W.Weihofen, F.Zapadtka Quasi-free π0 photoproduction from the bound nucleon NUCLEAR REACTIONS 2H(γ, π0n), (γ, π0p), E=200-400 MeV; 1H(γ, π0), E=200-400 MeV; measured σ(E, θ). 1n(γ, π0), E=300 MeV; deduced quasifree σ(θ).
doi: 10.1140/epja/i2003-10130-3
2003KO08 Eur.Phys.J. A 16, 259 (2003) K.Kossert, M.Camen, F.Wissmann, J.Ahrens, J.R.M.Annand, H.-J.Arends, R.Beck, G.Caselotti, P.Grabmayr, O.Jahn, P.Jennewein, M.I.Levchuk, A.I.L'vov, J.C.McGeorge, A.Natter, V.Olmos de Leon, V.A.Petrun'kin, G.Rosner, M.Schumacher, B.Seitz, F.Smend, A.Thomas, W.Weihofen, F.Zapadtka Quasi-free Compton scattering and the polarizabilities of the neutron NUCLEAR REACTIONS 1H(γ, γ'), E=200-400 MeV; 2H(γ, γ'n), (γ, γ'p), E=200-400 MeV; measured Eγ, Ep, En, σ(E, θ). 1n(γ, γ'), E=200-400 MeV; deduced σ(E, θ). 1n deduced polarizabilities. Tagged photons.
doi: 10.1140/epja/i2002-10093-9
2002CA13 Phys.Rev. C65, 032202 (2002) M.Camen, K.Kossert, F.Wissmann, J.Ahrens, H.-J.Arends, R.Beck, G.Caselotti, P.Grabmayr, P.D.Harty, O.Jahn, P.Jennewein, R.Kondratiev, M.I.Levchuk, V.Lisin, A.I.Lvov, J.C.McGeorge, A.Natter, V.Olmos de Leon, M.Schumacher, B.Seitz, F.Smend, A.Thomas, W.Weihofen, F.Zapadtka Backward Spin Polarizability γπ of the Proton NUCLEAR REACTIONS 1H(γ, γ), E=200-470 MeV; measured Compton scattering σ(θ=136°), pγ-coin. 1H deduced backward spin polarizability. Comparisons with model predictions, previous results.
doi: 10.1103/PhysRevC.65.032202
2002KO21 Phys.Rev.Lett. 88, 162301 (2002) K.Kossert, M.Camen, F.Wissmann, J.Ahrens, J.R.M.Annand, H.-J.Arends, R.Beck, G.Caselotti, P.Grabmayr, O.Jahn, P.Jennewein, M.I.Levchuk, A.I.Lvov, J.C.McGeorge, A.Natter, V.Olmos de Leon, V.A.Petrunkin, G.Rosner, M.Schumacher, B.Seitz, F.Smend, A.Thomas, W.Weihofen, F.Zapadtka Neutron Polarizabilities Investigated by Quasifree Compton Scattering from the Deuteron NUCLEAR REACTIONS 2H(γ, n), E=200-400 MeV; measured Eγ, nγ-coin. 1n deduced polarizabilities.
doi: 10.1103/PhysRevLett.88.162301
2000WI05 Nucl.Phys. A663-664, 397c (2000) F.Wissmann, P.Achenbach, J.Ahrens, H.-J.Arends, R.Beck, R.Bilger, M.Camen, G.P.Capitani, G.Caselotti, G.Galler, P.Grabmayr, F.Harter, T.Hehl, E.Heid, V.Hejny, O.Jahn, P.Jennewein, R.Kondratev, K.Kossert, M.Kotulla, B.Krusche, V.Kuhr, M.Lang, R.Leukel, M.I.Levchuk, V.Lisin, A.I.Lvov, A.M.Massone, V.Metag, A.Natter, R.Novotny, V.Olmos de Leon, P.Ottonello, J.Peise, A.Polonsky, I.Preobrashenskij, S.Proff, F.Rambo, A.Robbiano, D.Rosenkranz, M.Sanzone, E.Schilling, A.Schmidt, M.Schumacher, B.Seitz, U.Siodlaczek, F.Smend, H.Stroher, H.Vorwerk, Th.Walcher, J.Weiss, M.Wolf, S.Wolf, F.Zapadtka Compton Scattering from the Free and Bound Proton Above π-Threshold NUCLEAR REACTIONS 1,2H(γ, γ'X), E=200-800 MeV; measured σ(θ).
doi: 10.1016/S0375-9474(99)00626-0
1999PR01 Nucl.Phys. A646, 67 (1999) S.Proff, C.Poch, T.Glebe, J.-O.Adler, K.Fissum, K.Hansen, M.-Th.Hutt, O.Kaltschmidt, M.Lundin, B.Nilsson, B.Schroder, M.Schumacher, D.Sims, F.Smend, F.Wissmann Electromagnetic Polarizabilities of Nucleons Bound in 40Ca, 16O and 4He NUCLEAR REACTIONS 40Ca(γ, γ), E=58, 74 MeV; 4He, 16O(γ, γ), E=61 MeV; measured σ(θ); deduced nucleons in-medium electromagnetic polarizabilities.
doi: 10.1016/S0375-9474(98)00636-8
1999RA29 Nucl.Phys. A660, 69 (1999) F.Rambo, P.Achenbach, J.Ahrens, H.-J.Arends, R.Beck, S.J.Hall, V.Hejny, P.Jennewein, S.S.Kamalov, M.Kotulla, B.Krusche, V.Kuhr, R.Leukel, V.Metag, R.Novotny, V.Olmos de Leon, A.Schmidt, M.Schumacher, U.Siodlaczek, F.Smend, H.Stroher, J.Weiss, F.Wissmann, M.Wolf Coherent π0 Photoproduction from 4He NUCLEAR REACTIONS 4He(γ, π0), E=200-400 MeV; measured σ, σ(θ); deduced in-medium modification of Δ resonance parameters. Tagged coherent bremsstrahlung beam, DWIA analysis.
doi: 10.1016/S0375-9474(99)00383-8
1998BE59 Nucl.Phys. A639, 209c (1998) C.Bennhold, S.Goers, J.Barth, W.Braun, R.Burgwinkel, J.Ernst, K.H.Glander, J.Hannappel, N.Jopen, H.Kalinowsky, U.Kirch, F.Klein, F.J.Klein, E.Klempt, A.Kozela, R.Lawall, Z.Li, J.Link, T.Mart, D.Menze, W.Neuerburg, M.Paganetti, E.Paul, H.van Pee, R.Plotzke, M.Schumacher, W.J.Schwille, F.Smend, J.Smyrski, H.-N.Tran, M.Q.Tran, F.Wehnes, B.Wiegers, F.W.Wieland, J.Wisskirchen K0-Σ+ Photoproduction with SAPHIR NUCLEAR REACTIONS 1H(γ, K0), E=1.0-1.6 GeV; measured hyperon production σ(θ), σ. Model comparisons.
doi: 10.1016/S0375-9474(98)00275-9
1998ER03 Nucl.Phys. A639, 213c (1998) J.Ernst, H.Jungst, H.Kalinowsky, E.Klempt, J.Link, H.van Pee, R.Plotzke, J.Barth, W.Braun, R.Burgwinkel, K.H.Glander, S.Goers, J.Hannappel, N.Jopen, U.Kirch, F.Klein, F.-J.Klein, R.Lawall, D.Menze, W.Neuerburg, M.Paganetti, E.Paul, W.-J.Schwille, M.Q.Tran, F.Wehnes, B.Wiegers, F.W.Wieland, J.Wisskirchen, M.Schumacher, F.Smend, H.-N.Tran, A.Kozela, J.Smyrski, C.Bennhold First Results of η' Photoproduction with SAPHIR NUCLEAR REACTIONS 1H(γ, X), E=1.5-2.5 GeV; measured preliminary η' production σ.
doi: 10.1016/S0375-9474(98)00276-0
1998KR13 Phys.Lett. 432B, 45 (1998) A.Kraus, O.Selke, F.Wissmann, J.Ahrens, H.-J.Arends, R.Beck, G.Galler, M.-Th.Hutt, B.Korfgen, J.Peise, M.Schumacher, F.Smend, R.Wichmann Angular and Polarization Dependence of Compton Scattering from 4He in the Δ-Resonance Region NUCLEAR REACTIONS 4He(polarized γ, γ'), E=150-500 MeV; measured σ(Eγ, θ), asymmetry; deduced Δ-hole model failure at large scattering angles. Polarized tagged photons.
doi: 10.1016/S0370-2693(98)00635-2
1998RA12 Phys.Rev. C58, 489 (1998) F.Rambo, J.Ahrens, H.-J.Arends, R.Beck, G.Galler, J.D.Kellie, H.-P.Krahn, A.Kraus, U.Ludwig, J.Peise, A.Schmidt, M.Schumacher, F.Smend, F.Wissmann, S.Wolf Enhancement of the Linear Polarization of Coherent Bremsstrahlung by Collimation of the Photon Beam NUCLEAR REACTIONS 4He(polarized γ, π0), E=200-400 MeV bremsstrahlung; analyzed asymmetry; deduced beam polarization, collimation effect. Coherent bremsstrahlung from diamond crystals.
doi: 10.1103/PhysRevC.58.489
1998TR06 Phys.Lett. 445B, 20 (1998) M.Q.Tran, J.Barth, C.Bennhold, M.Bockhorst, W.Braun, A.Budzanowski, G.Burbach, R.Burgwinkel, J.Ernst, K.H.Glander, S.Goers, B.Guse, K.-M.Haas, J.Hannappel, K.Heinloth, K.Honscheid, T.Jahnen, N.Jopen, H.Jungst, H.Kalinowsky, U.Kirch, F.J.Klein, F.Klein, E.Klempt, D.Kostrewa, A.Kozela, R.Lawall, L.Lindemann, J.Link, J.Manns, T.Mart, D.Menze, H.Merkel, R.Merkel, W.Neuerburg, M.Paganetti, E.Paul, R.Plotzke, U.Schenk, J.Scholmann, I.Schulday, M.Schumacher, P.Schutz, W.J.Schwille, F.Smend, J.Smyrski, W.Speth, H.N.Tran, H.van Pee, W.Vogel, R.Wedemeyer, F.Wehnes, B.Wiegers, F.W.Wieland, J.Wisskirchen, A.Wolf, and the SAPHIR Collaboration Measurement of γp → K+ Λ and γp → K+Σ0 at Photon Energies up to 2 GeV NUCLEAR REACTIONS 1H(γ, K+X), E=0.8-2 GeV; measured Λ, Σ0 hyperon production σ(θ), σ, polarizations. Tagged photons.
doi: 10.1016/S0370-2693(98)01393-8
1997HO07 Phys.Rev.Lett. 78, 4697 (1997) P.Hoffmann-Rothe, M.Krebeck, J.Hey, M.Breuer, G.von Edel, E.Hourany, M.Rigney, J.Ajaka, G.Anton, J.Arends, G.Berrier-Ronsin, W.Beulertz, G.Blanpied, A.Bock, J.-P.Didelez, K.Helbing, R.Maass, G.Noldeke, B.Preedom, B.Richie, L.Rosier, B.Saghai, M.Schumacher, F.Smend Break-Up and Coherent Photoproduction of η Mesons on the Deuteron NUCLEAR REACTIONS 2H(γ, X), E ≈ 0.710-0.8 GeV bremsstrahlung; measured σ(θ(η)), coherent production; deduced neutron to proton differential σ, isoscalar, isovector amplitude ratio.
doi: 10.1103/PhysRevLett.78.4697
1997KR13 Phys.Rev.Lett. 79, 3834 (1997) A.Kraus, O.Selke, F.Rambo, G.Galler, M.Schumacher, F.Smend, R.Wichmann, S.Wolf, J.Ahrens, H.-J.Arends, R.Beck, J.Peise Beam Asymmetry of Coherent π0 Photoproduction on 4He in the Δ(1232) Range Measured using Coherent Bremsstrahlung NUCLEAR REACTIONS 4He(polarized γ, π0), E=200-500 MeV bremsstrahlung; measured π0 photoproduction σ(θ) beam asymmetry; deduced beam polarization, collimation effect.
doi: 10.1103/PhysRevLett.79.3834
1992WI08 Z.Phys. A341, 453 (1992) G.-D.Wicke, G.Mondry, F.Smend, G.Fink, P.Doll, S.Hauber, M.Haupenthal, H.Schieler, H.O.Klages Radiative Capture of Polarized Neutrons by 12C in the Energy Range E(n) = 20-35 MeV NUCLEAR REACTIONS 12C(polarized n, γ), E=20-35 MeV; measured γ(θ), asymmetry vs E, γ(recoil)-coin; deduced E2, E1 capture interference. Direct semidirect model.
doi: 10.1007/BF01301389
1991FI07 Nucl.Phys. A530, 331 (1991) G.Fink, P.Doll, S.Hauber, M.Haupenthal, H.O.Klages, H.Schieler, F.Smend, G.D.Wicke Neutron-Proton Capture Using Polarized Neutrons from 19 to 50 MeV NUCLEAR REACTIONS 1H(polarized n, γ), E=19-50 MeV; measured σ(θ), analyzing power vs θ. NE213 target.
doi: 10.1016/0375-9474(91)90806-H
1991MO17 Nucl.Phys. A531, 237 (1991) G.Mondry, F.Wissmann, G.Muller, F.Schroder, P.Rullhusen, F.Smend, M.Schumacher, P.Fettweis, R.Carchon Rotational Raman Scattering in 127I NUCLEAR REACTIONS 181Ta, 127I(γ, γ), (γ, γ'), E=11.4 MeV; measured elastic, Raman scattering σ(θ). Natural targets.
doi: 10.1016/0375-9474(91)90611-9
1986KA13 Phys.Rev. C33, 1606 (1986) B.Kasten, D.Schaupp, P.Rullhusen, F.Smend, M.Schumacher, L.Kissel Coulomb Correction Effect in Delbruck Scattering and Atomic Rayleigh Scattering of 1-4 MeV Photons NUCLEAR REACTIONS Sn, Ce, Ta, Pb, U(γ, γ), E=0.8-4 MeV; measured Delbruck scattering σ(θ); deduced Coulomb correction effect.
doi: 10.1103/PhysRevC.33.1606
1985SC10 Nucl.Phys. A438, 493 (1985) M.Schumacher, U.Zurmuhl, F.Smend, R.Nolte Low-Energy Electric-Dipole Transition Widths Predicted by the Giant Dipole Resonance and Statistical Models NUCLEAR STRUCTURE A=6-20; A=21-44; calculated electric transition hindrance factors. GDR, statistical models.
doi: 10.1016/0375-9474(85)90388-4
1985WE01 Z.Phys. A320, 179 (1985) R.Wenskus, A.Baumann, P.Rullhusen, D.Schaupp, F.Smend, M.Schumacher Relativistic Double Differential Cross Sections for Compton Scattering by Bound Electrons: Test at low photon energies and predictions at intermediate photon energies ATOMIC PHYSICS Cu, Pb(γ, γ'), E=0.662, 50 MeV; C(γ, γ'), E=50 MeV; calculated Compton σ(θ, Eγ'). Relativistic impulse approximation.
doi: 10.1007/BF01881265
1984SC32 Z.Phys. A319, 1 (1984) D.Schaupp, H.Czerwinski, F.Smend, R.Wenskus, M.Schumacher, A.H.Millhouse, H.Schenk-Strauss Resonant Raman Scattering of Synchrotron X-Rays by Neodymium: Observation of fine structure in K-L-RRS and of K-N-RRS ATOMIC PHYSICS Nd(γ, γ), E=43.01-43.35 keV; measured resonant Raman scattering σ(θ, Eγ').
doi: 10.1007/BF01429760
1983KE02 Z.Phys. A311, 253 (1983) G.Kehlenbeck, J.Ahlert, F.Wolf, L.Ziegeler, F.Smend, M.Schumacher Electronic Rearrangement on Molecules accompanying β-Decay Investigated by Nuclear Resonance Fluorescence RADIOACTIVITY 60Co(β-); measured electron-neutrino pair recoil momentum distribution transferred to 60Ni; deduced molecular electronic rearrangement effects. Nuclear resonance fluoresence coincidence method, gaseous 60CoI2 sources.
doi: 10.1007/BF01415678
1983RU03 Phys.Rev. C27, 559 (1983) P.Rullhusen, U.Zurmuhl, F.Smend, M.Schumacher, H.G.Borner, S.A.Kerr Giant Dipole Resonances and Coulomb Correction Effect in Delbruck Scattering Studied by Elastic and Raman Scattering of 8.5 to 11.4 MeV Photons NUCLEAR REACTIONS 238U, 232Th, 209Bi(γ, γ), (γ, γ'), E=8.5-11.4 MeV; measured σ(θ) for elastic, Raman scattering; deduced Delbruck scattering Coulomb correction. 238U, 232Th, 209Bi deduced GDR parameters.
doi: 10.1103/PhysRevC.27.559
1983ZU04 Z.Phys. A314, 171 (1983) U.Zurmuhl, P.Rullhusen, F.Smend, M.Schumacher, H.G.Borner, S.A.Kerr Nuclear Resonance Scattering Studies on 238U using a Dense Series of γ-Ray Photons NUCLEAR REACTIONS 238U(γ, γ), (γ, γ'), E=4-7 MeV; measured Eγ, Iγ, σ(θγ). 238U deduced GDR, nonstatistical resonance strengths, Γ. Photon beam from 181Ta, 141Pr(n, γ), nuclear resonance fluorescence.
1982RU03 Nucl.Phys. A382, 79 (1982) P.Rullhusen, U.Zurmuhl, W.Muckenheim, F.Smend, M.Schumacher, H.G.Borner Coulomb Correction Effect in Delbruck Scattering and Nuclear Resonance Fluorescence of 2 to 10 MeV Photons on 238U NUCLEAR REACTIONS 238U(γ, γ), (γ, γ'), E=2.75-9.72 MeV; measured Eγ, Iγ, σ(θ), elastic scattering, nuclear resonance fluorescence. 238U deduced levels, γ-branching.
doi: 10.1016/0375-9474(82)90442-0
1982ZU01 Phys.Lett. 114B, 99 (1982) U.Zurmuhl, P.Rullhusen, F.Smend, M.Schumacher, H.G.Borner The Distribution of E1 Strength below Particle Threshold Studied by Resonant Scattering of Gamma Rays NUCLEAR REACTIONS 238U(γ, γ), E=2.75-6.5 MeV; measured σ(θ), total σ(absorption) vs E; 181Ta(γ, γ), E=3-6.75 MeV; 165Ho(γ, γ), E=3.5-6.75 MeV; measured total σ(absorption) vs E. 238U, 181Ta, 165Ho deduced average γ-branching ratio, E1 transition strength distribution, nonstatistical deviations from GDR Lorentzian. Nuclear resonance fluorescence.
doi: 10.1016/0370-2693(82)90123-X
1981EN03 Z.Phys. A302, 61 (1981) G.Endres, H.Langhoff, W.Muckenheim, F.Wolf, P.Rullhusen, F.Smend, M.Schumacher Resonance Fluorescence in 121Sb NUCLEAR REACTIONS 121Sb(γ, γ), E=3.452 MeV; measured σ vs source velocity. 121Sb level deduced T1/2, J, π, γ-branching. 56Fe level deduced T1/2. Nuclear resonance fluorescence technique, Doppler shift analysis, 56Co source, high speed centrifuge.
doi: 10.1007/BF01425103
1981MU05 Z.Phys. A300, 43 (1981) W.Muckenheim, P.Rullhusen, F.Smend, M.Schumacher, G.Endres, H.Langhoff Nuclear Resonance Fluorescence in 238U and a New Approach to Doppler-Shift-Attenuation using High Speed Rotation NUCLEAR REACTIONS 238U(γ, γ'), E=resonance; measured Eγ, Iγ, γγ(θ), σ(θγ), resonance fluorescence yield. 238U deduced levels, J, π, γ-branching, T1/2, Γ. Cobalt-56 source. RADIOACTIVITY 56Co; measured Doppler shift attenuation of emission line. 56Fe level deduced T1/2. High speed centrifuge.
1981RU03 Phys.Rev. C23, 1375 (1981) P.Rullhusen, W.Muckenheim, F.Smend, M.Schumacher, G.P.A.Berg, K.Mork, L.Kissel Test of Vacuum Polarization by Precise Investigation of Delbruck Scattering NUCLEAR REACTIONS Zn, Mo, Sn, Ce(γ, γ), E=2.754 MeV; measured σ(θ); deduced vacuum polarization effects. Delbruck scattering, Dirac-Hartree-Fock-Slater wave functions, second-order S-matrix.
doi: 10.1103/PhysRevC.23.1375
1981SC10 Z.Phys. A300, 193 (1981) M.Schumacher, F.Smend, W.Muckenheim, P.Rullhusen, H.G.Borner Nuclear Photoexcitation and Delbruck Scattering Studied in the Energy Range 2-8 MeV NUCLEAR REACTIONS 238U, 209Bi, Pb, Tl, Hg, W, 181Ta, Nd, Ce, 127I, Sb, Sn, Cd, Nd(γ, γ), E=2.599-3.452; 238U, 209Bi, Pb, Tl, Hg, W, 181Ta, 165Ho, Ce, Sn, Mo, Zn(γ, γ), E=6.418-7.16 MeV; measured Eγ, Iγ, σ(θ). 203Tl, 100,94Mo, 186,184W, 181Ta levels deduced photoexcitation, decay mechanism. Lorentzian GDR shape, Rayleigh, Thomson, Delbruck, collective nuclear excitation effects.
doi: 10.1007/BF01412295
1980MU05 Phys.Lett. 92B, 71 (1980) W.Muckenheim, P.Rullhusen, F.Smend, M.Schumacher Evidence for Nuclear Photoexcitation Obtained in Low-Energy γ-Ray Scattering Experiments NUCLEAR REACTIONS 238U, 208Pb, Nd, 121Sb, 209Bi, 181Ta, Ce, Sn(γ, γ), E=2.5-3.5 MeV; measured σ(E, θ). 238U, 181Ta, Nd, 121Sb levels deduced Γ, spacing. Nuclear resonance fluorescence.
doi: 10.1016/0370-2693(80)90306-8
1980MU11 Nucl.Instrum.Methods 173, 403 (1980) W.Muckenheim, P.Rullhusen, F.Smend, M.Schumacher Note on the Half-Life of 24Na RADIOACTIVITY 24Na [from 27Al(d, pα)]; measured T1/2. Ge(Li) detector.
1980SC22 Nucl.Phys. A346, 418 (1980) M.Schumacher, P.Rullhusen, F.Smend, W.Muckenheim, H.G.Borner The Energy Dependence of Delbruck Scattering Investigated at Z = 73, 82 and 92 NUCLEAR REACTIONS 181Ta, 206,207,208Pb, 238U(γ, γ), E=0.279, 0.412, 0.662, 0.889, 1.121, 1.173, 1.332, 4.291, 4.767 MeV; measured σ(θ) Delbruck. Natural targets.
doi: 10.1016/0375-9474(80)90477-7
1979RU01 Nucl.Phys. A313, 307 (1979) P.Rullhusen, F.Smend, M.Schumacher Delbruck Scattering of 2.754 MeV Photons by Bi and Th NUCLEAR REACTIONS 209Bi, 232Th(γ, γ), E=2.745 MeV; measured σ(θ). Compared with Delbruck theory. Natural targets.
doi: 10.1016/0375-9474(79)90502-5
1979RU03 Phys.Lett. 84B, 166 (1979) P.Rullhusen, F.Smend, M.Schumacher Delbruck Scattering of 2754 keV Photons by Nd, Ce, I, Sn, Mo and Zn NUCLEAR REACTIONS Nd, Ce, I, Sn, Mo, Zn(γ, γ), E=2754 keV; calculated σ(θ); deduced validity of Delbruck theory.
doi: 10.1016/0370-2693(79)90274-0
1979RU08 Z.Phys. A293, 287 (1979) P.Rullhusen, F.Smend, M.Schumacher, A.Hanser, H.Rebel Coulomb Correction to Delbruck Scattering Investigated at Z = 94 NUCLEAR REACTIONS 239Pu(γ, γ), E=2.754 MeV; measured σ(θ); deduced higher-order Coulomb correction terms. Delbruck, nuclear resonance scattering analysis.
doi: 10.1007/BF01435270
1976SC10 Phys.Rev. C13, 2318 (1976) M.Schumacher, F.Smend, I.Borchert Delbruck Scattering of 2.754-MeV Photons by Pb for Angles from 15° to 150° NUCLEAR REACTIONS Pb(γ, γ), E=2.754 MeV; measured Delbruck scattering, σ(θ), θ=15°-150°.
doi: 10.1103/PhysRevC.13.2318
1975BO13 Z.Phys. A272, 197 (1975) I.Borchert, M.Schumacher, F.Smend Resonance Behaviour of a Perturbed Gamma Gamma Directional Correlation In a Magnetic Field RADIOACTIVITY 75Se; measured γγ(θ, H, t).
doi: 10.1007/BF01408147
1975CA41 Phys.Rev.Lett. 35, 1259 (1975) J.L.Campbell, B.Martin, W.D.Schmidt-Ott, F.Smend, U.Raff L3 Conversion of the 2.38-keV Isomer in 90Nb RADIOACTIVITY 90m,94mNb(IT) [from Zr(d, X)]; measured X-ray spectra, T1/2. 90,94Nb transitions deduced ICC. Implications for previously observed chemical effects discussed.
doi: 10.1103/PhysRevLett.35.1259
1975SC39 Phys.Lett. 59B, 134 (1975) M.Schumacher, I.Borchert, F.Smend, P.Rullhusen Delbruck Scattering of 2.75 MeV Photons by Lead NUCLEAR REACTIONS Pb(γ, γ), E=2.75 MeV; measured σ. Delbruck scattering.
doi: 10.1016/0370-2693(75)90685-1
1973SC11 Nucl.Phys. A206, 531 (1973) M.Schumacher, F.Smend, I.Borchert Elastic Scattering of γ-Rays from Lead for Energies from 0.145 to 1.33 MeV NUCLEAR REACTIONS Pb(γ, γ), E=889, 1120 keV; measured σ(H).
doi: 10.1016/0375-9474(73)90083-3
1973SM11 Nucl.Phys. A213, 309 (1973) F.Smend, M.Schumacher, I.Borchert The Z-Dependence of the Elastic Scattering of γ-Rays ATOMIC PHYSICS Pb, Ta, Nd, Sn, Mo, Zn(γ, γ), Eγ=662, 279 keV; measured σ(coh)(Z, θ). Deduced Z-dependence of Rayleigh scattering.
doi: 10.1016/0375-9474(73)90152-8
1972BO64 Z.Phys. 256, 441 (1972) I.Borchert, M.Schumacher, F.Smend, H.Langhoff The Perturbation of a γγ Directional Correlation of 75As in Gaseous H2 75Se Sources RADIOACTIVITY 75Se; measured γγ(θ, pressure) in H2 Se sources; deduced attenuation coefficients.
doi: 10.1007/BF01386989
1971SM07 Z.Phys. 248, 326 (1971) F.Smend, I.Borchert, H.Langhoff The Influence of the Chemical Environment on the Decay Constant of 90mNb RADIOACTIVITY 90mNb; measured T1/2 in Zr, F complex; deduced chemical environment effects.
doi: 10.1007/BF01400546
1969GF01 Z.Physik 227, 45 (1969) D.Gfoller, H.Langhoff, F.Smend, W.Weirauch, W.-D.Schmidt-Ott Der Zerfall des 122Xe(T1/2=20, 1 h) und des 122J(T1/2=3, 6 min) RADIOACTIVITY 122Xe [from 120Te(α, 2n)]; 122I [from 122Te(d, 2n)]; measured Eγ, Iγ, γγ-coin. 122I, 122Te deduced levels.
1969SM01 Z.Physik 219, 467(1969) Isomerenverhaltnis fur die Reaktion 51-V(α, 3n)52g, m-Mn NUCLEAR REACTIONS 51V(α, 3n), E=32-51 MeV; measured isomeric cross-section ratio.
doi: 10.1007/BF01400823
1968SC14 Z.Physik 217, 282 (1968) W.-D.Schmidt-Ott, W.Weirauch, F.Smend, H.Langhoff, D.Gfoller Der Zerfall des 125mXe, des 127mXe und des 127gXe NUCLEAR STRUCTURE 125Xe, 127Xe; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01394102
1968SM08 Z.Phys. 214, 437 (1968) F.Smend, W.Weirauch, W.-D.Schmidt-Ott Isomerenverhaltnisse fur die Reaktionen 107Ag(α, 2n)109g,109mIn und 109Ag(α, 2n)111g,111mIn RADIOACTIVITY 109gIn, 109mIn, 111gIn, 111mIn; measured T1/2, Eγ.
doi: 10.1007/BF01449047
1968WE03 Z.Physik 209, 289 (1968) W.Weirauch, W.-D.Schmidt-Ott, F.Smend, A.Flammersfeld Suche nach Dem Einfluss der Chemischen Bindung Auf die Halbwertszeit des 90m-Nb (T1/2=19, 2 sec) NUCLEAR STRUCTURE 90Nb; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01380076
1967SM06 Z.Physik 207, 28 (1967) F.Smend, W.Weirauch, W.-D.Schmidt-Ott, A.Flammersfeld Wirkungsquerschnitte und Isomerenverhaltnis fur die Reaktionen 89-Y(α, 3n)90g-Nb und 89-Y(α, 3n)90m-Nb NUCLEAR STRUCTURE 90Nb; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01326091
1966SC28 Nucl.Phys. 89, 565 (1966) W.-D.Schmidt-Ott, F.Smend, W.Weirauch, A.Flammersfeld Search for Nuclear Structure Effects in the K-Conversion Coefficient of the 385 keV Transition in 197Tl RADIOACTIVITY 197mTl [from 197Au(α, 4n)]; measured γγ(θ), ICC. 385 keV transition deduced mixing ratio, penetration parameter.
doi: 10.1016/0029-5582(66)90931-X
1966SM01 Z.Physik 191, 1 (1966) F.Smend, W.Weirauch, W.-D.Schmidt-Ott, A.Flammersfeld Zur Isomerie des Au197 NUCLEAR STRUCTURE 197Au; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01362464
1966WE01 Z.Phys. 192, 351 (1966) W.Weirauch, W.-D.Schmidt-Ott, F.Smend, A.Flammersfeld Der Zerfall des In109m(0, 21 sec) NUCLEAR STRUCTURE 109In; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01325673
1965SC11 Z.Physik 184, 310 (1965) W.-D.Schmidt-Ott, F.Smend, A.Flammersfeld Der Zerfall des Tb158m NUCLEAR STRUCTURE 158Tb; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01383827
1965SC18 Z.Physik 188, 282 (1965) W.-D.Schmidt-Ott, F.Smend, W.Weirauch, A.Flammersfeld Zur Isomerie des Tl197 NUCLEAR STRUCTURE 197Tl; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01325938
1965SM02 Z.Physik 185, 426 (1965) F.Smend, W.-D.Schmidt-Ott, A.Flammersfeld Die Konversion des Hg199m NUCLEAR STRUCTURE 199Hg; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01381711
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