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NSR database version of April 26, 2024.

Search: Author = M.Weiss

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2024AP01      Eur.Phys.J. C 84, 138 (2024)

E.Aprile, K.Abe, S.Ahmed Maouloud, L.Althueser, B.Andrieu, E.Angelino, J.R.Angevaare, V.C.Antochi, D.Anton Martin, F.Arneodo, L.Baudis, A.L.Baxter, M.Bazyk, L.Bellagamba, R.Biondi, A.Bismark, E.J.Brookes, A.Brown, S.Bruenner, G.Bruno, R.Budnik, T.K.Bui, C.Cai, J.M.R.Cardoso, D.Cichon, A.P.Cimental Chavez, A.P.Colijn, J.Conrad, J.J.Cuenca-Garcia, J.P.Cussonneau, V.D'Andrea, M.P.Decowski, P.Di Gangi, S.Diglio, K.Eitel, A.Elykov, S.Farrell, A.D.Ferella, C.Ferrari, H.Fischer, M.Flierman, W.Fulgione, C.Fuselli, P.Gaemers, R.Gaior, A.Gallo Rosso, M.Galloway, F.Gao, R.Glade-Beucke, L.Grandi, J.Grigat, H.Guan, M.Guida, R.Hammann, A.Higuera, C.Hils, L.Hoetzsch, N.F.Hood, J.Howlett, M.Iacovacci, Y.Itow, J.Jakob, F.Joerg, A.Joy, M.Kara, P.Kavrigin, S.Kazama, M.Kobayashi, G.Koltman, A.Kopec, F.Kuger, H.Landsman, R.F.Lang, L.Levinson, I.Li, S.Li, S.Liang, S.Lindemann, M.Lindner, K.Liu, J.Loizeau, F.Lombardi, J.Long, J.A.M.Lopes, Y.Ma, C.Macolino, J.Mahlstedt, A.Mancuso, L.Manenti, F.Marignetti, T.Marrodan Undagoitia, K.Martens, J.Masbou, D.Masson, E.Masson, S.Mastroianni, M.Messina, K.Miuchi, A.Molinario, S.Moriyama, K.Mora, Y.Mosbacher, M.Murra, J.Muller, K.Ni, U.Oberlack, B.Paetsch, J.Palacio, Q.Pellegrini, R.Peres, C.Peters, J.Pienaar, M.Pierre, G.Plante, T.R.Pollmann, J.Qi, J.Qin, D.Ramirez Garcia, N.Sarcevic, J.Shi, R.Singh, L.Sanchez, J.M.F.dos Santos, I.Sarnoff, G.Sartorelli, J.Schreiner, D.Schulte, P.Schulte, H.Schulze Eissing, M.Schumann, L.Scotto Lavina, M.Selvi, F.Semeria, P.Shagin, S.Shi, E.Shockley, M.Silva, H.Simgen, A.Takeda, P.-L.Tan, A.Terliuk, D.Thers, F.Toschi, G.Trinchero, C.Tunnell, F.Tonnies, K.Valerius, G.Volta, C.Weinheimer, M.Weiss, D.Wenz, C.Wittweg, T.Wolf, V.H.S.Wu, Y.Xing, D.Xu, Z.Xu, M.Yamashita, L.Yang, J.Ye, L.Yuan, G.Zavattini, M.Zhong, T.Zhu, XENON collaboration

Design and performance of the field cage for the XENONnT experiment

doi: 10.1140/epjc/s10052-023-12296-y
Citations: PlumX Metrics

2023AP04      Phys.Rev. D 108, 072015 (2023)

E.Aprile, K.Abe, S.Ahmed Maouloud, L.Althueser, B.Andrieu, E.Angelino, J.R.Angevaare, V.C.Antochi, D.Anton Martin, F.Arneodo, L.Baudis, A.L.Baxter, M.Bazyk, L.Bellagamba, R.Biondi, A.Bismark, E.J.Brookes, A.Brown, S.Bruenner, G.Bruno, R.Budnik, T.K.Bui, C.Cai, J.M.R.Cardoso, A.P.Cimental Chavez, A.P.Colijn, J.Conrad, J.J.Cuenca-Garcia, V.D'Andrea, M.P.Decowski, P.Di Gangi, S.Diglio, K.Eitel, A.Elykov, S.Farrell, A.D.Ferella, C.Ferrari, H.Fischer, M.Flierman, W.Fulgione, C.Fuselli, P.Gaemers, R.Gaior, A.Gallo Rosso, M.Galloway, F.Gao, R.Glade-Beucke, L.Grandi, J.Grigat, H.Guan, M.Guida, R.Hammann, A.Higuera, C.Hils, L.Hoetzsch, N.F.Hood, J.Howlett, M.Iacovacci, Y.Itow, J.Jakob, F.Joerg, A.Joy, M.Kara, P.Kavrigin, S.Kazama, M.Kobayashi, G.Koltman, A.Kopec, F.Kuger, H.Landsman, R.F.Lang, D.G.Layos Carlos, L.Levinson, I.Li, S.Li, S.Liang, S.Lindemann, M.Lindner, K.Liu, J.Loizeau, F.Lombardi, J.Long, J.A.M.Lopes, Y.Ma, C.Macolino, J.Mahlstedt, A.Mancuso, L.Manenti, F.Marignetti, T.Marrodan Undagoitia, K.Martens, J.Masbou, D.Masson, E.Masson, S.Mastroianni, M.Messina, K.Miuchi, A.Molinario, S.Moriyama, K.Moraa, Y.Mosbacher, M.Murra, J.Muller, K.Ni, U.Oberlack, B.Paetsch, J.Palacio, Q.Pellegrini, R.Peres, C.Peters, J.Pienaar, M.Pierre, G.Plante, T.R.Pollmann, J.Qi, J.Qin, D.Ramirez Garcia, J.Shi, R.Singh, L.Sanchez, J.M.F.dos Santos, I.Sarnoff, G.Sartorelli, J.Schreiner, D.Schulte, P.Schulte, H.Schulze Eissing, M.Schumann, L.Scotto Lavina, M.Selvi, F.Semeria, P.Shagin, S.Shi, E.Shockley, M.Silva, H.Simgen, A.Takeda, P.-L.Tan, A.Terliuk, D.Thers, F.Toschi, G.Trinchero, C.Tunnell, F.Tonnies, K.Valerius, G.Volta, C.Weinheimer, M.Weiss, D.Wenz, C.Wittweg, T.Wolf, V.H.S.Wu, Y.Xing, D.Xu, Z.Xu, M.Yamashita, L.Yang, J.Ye, L.Yuan, G.Zavattini, M.Zhong, T.Zhu

Search for events in XENON1T associated with gravitational waves

doi: 10.1103/PhysRevD.108.072015
Citations: PlumX Metrics

2022AP04      Phys.Rev.Lett. 129, 161805 (2022)

E.Aprile, K.Abe, F.Agostini, S.Ahmed Maouloud, L.Althueser, B.Andrieu, E.Angelino, J.R.Angevaare, V.C.Antochi, D.Anton Martin, F.Arneodo, L.Baudis, A.L.Baxter, L.Bellagamba, R.Biondi, A.Bismark, A.Brown, S.Bruenner, G.Bruno, R.Budnik, T.K.Bui, C.Cai, C.Capelli, J.M.R.Cardoso, D.Cichon, M.Clark, A.P.Colijn, J.Conrad, J.J.Cuenca-Garcia, J.P.Cussonneau, V.D'Andrea, M.P.Decowski, P.Di Gangi, S.Di Pede, A.Di Giovanni, R.Di Stefano, S.Diglio, K.Eitel, A.Elykov, S.Farrell, A.D.Ferella, C.Ferrari, H.Fischer, W.Fulgione, P.Gaemers, R.Gaior, A.Gallo Rosso, M.Galloway, F.Gao, R.Gardner, R.Glade-Beucke, L.Grandi, J.Grigat, M.Guida, R.Hammann, A.Higuera, C.Hils, L.Hoetzsch, J.Howlett, M.Iacovacci, Y.Itow, J.Jakob, F.Joerg, A.Joy, N.Kato, M.Kara, P.Kavrigin, S.Kazama, M.Kobayashi, G.Koltman, A.Kopec, F.Kuger, H.Landsman, R.F.Lang, L.Levinson, I.Li, S.Li, S.Liang, S.Lindemann, M.Lindner, K.Liu, J.Loizeau, F.Lombardi, J.Long, J.A.M.Lopes, Y.Ma, C.Macolino, J.Mahlstedt, A.Mancuso, L.Manenti, F.Marignetti, T.Marrodan Undagoitia, K.Martens, J.Masbou, D.Masson, E.Masson, S.Mastroianni, M.Messina, K.Miuchi, K.Mizukoshi, A.Molinario, S.Moriyama, K.Mora, Y.Mosbacher, M.Murra, J.Muller, K.Ni, U.Oberlack, B.Paetsch, J.Palacio, P.Paschos, R.Peres, C.Peters, J.Pienaar, M.Pierre, V.Pizzella, G.Plante, J.Qi, J.Qin, D.Ramirez Garcia, S.Reichard, A.Rocchetti, N.Rupp, L.Sanchez, J.M.F.dos Santos, I.Sarnoff, G.Sartorelli, J.Schreiner, D.Schulte, P.Schulte, H.Schulze Eissing, M.Schumann, L.Scotto Lavina, M.Selvi, F.Semeria, P.Shagin, S.Shi, E.Shockley, M.Silva, H.Simgen, J.Stephen, A.Takeda, P.-L.Tan, A.Terliuk, D.Thers, F.Toschi, G.Trinchero, C.Tunnell, F.Tonnies, K.Valerius, G.Volta, Y.Wei, C.Weinheimer, M.Weiss, D.Wenz, C.Wittweg, T.Wolf, D.Xu, Z.Xu, M.Yamashita, L.Yang, J.Ye, L.Yuan, G.Zavattini, M.Zhong, T.Zhu

Search for New Physics in Electronic Recoil Data from XENONnT

RADIOACTIVITY ¹²⁴Xe(2EC); measured decay products, X-rays; deduced T_1/2. Comparison with available data. The XENONnT experiment, located at the INFN Laboratori Nazionali del Gran Sasso (LNGS) in Italy, was designed as a fast upgrade of XENON1T and inherits many of its systems such as cooling, gas storage, purification, and Kr removal.

doi: 10.1103/PhysRevLett.129.161805
Citations: PlumX Metrics

2009MI18      Phys.Rev.Lett. 103, 152501 (2009)

D.G.Middleton, J.R.M.Annand, M.A.Antelo, C.Ayerbe, P.Barneo, D.Baumann, J.Bermuth, J.Bernauer, H.P.Blok, R.Bohm, D.Bosnar, M.Ding, M.O.Distler, J.Friedrich, J.Garcia Llongo, D.I.Glazier, J.Golak, W.Glockle, P.Grabmayr, T.Hehl, J.Heim, W.H.A.Hesselink, E.Jans, H.Kamada, G.J.Manas, M.Kohl, L.Lapikas, I.J.D.MacGregor, I.Martin, J.C.McGeorge, H.Merkel, P.Merle, K.Monstad, F.Moschini, U.Muller, A.Nogga, R.Perez-Benito, Th.Pospischil, M.Potokar, G.Rosner, M.Seimetz, R.Skibinski, H.de Vries, Th.Walcher, D.P.Watts, M.Weinriefer, M.Weiss, H.Witala, B.Zihlmann

Investigation of the Exclusive ³He(e, e'pn)¹H Reaction

NUCLEAR REACTIONS ³He(e, e'np), E=220-270 MeV; measured Ee, Ie, Ep, Ip and En, In; deduced σ. Continuum Fadeev calculations.

doi: 10.1103/PhysRevLett.103.152501
Citations: PlumX Metrics

2008MI26      Few-Body Systems 44, 171 (2008)

D.G.Middleton, J.R.M.Annand, M.A.Antelo, C.Ayerbe, P.Barneo, D.Baumann, J.Bermuth, J.Bernauer, H.P.Blok, R.Bohm, D.Bosnar, M.Ding, M.O.Distler, J.Friedrich, J.Garcia Llongo, D.I.Glazier, P.Grabmayr, T.Hehl, J.Heim, W.H.A.Hesselink, E.Jans, G.J.Manas, M.Kohl, L.Lapikas, I.J.D.MacGregor, I.Martin, J.C.McGeorge, H.Merkel, P.Merle, K.Monstad, F.Moschini, U.Muller, R.Perez Benito, Th.Pospischil, M.Potokar, G.Rosner, M.Seimitz, H.de Vries, Th.Walcher, D.P.Watts, M.Weinriefer, M.Weiss, B.Zihlmann

³He(e, e'pp) and ³He(e, e'pn) reactions at AmPS and MAMI

NUCLEAR REACTIONS ³He(e, e'2p), (e, e'np), E not given; measured cross sections.

doi: 10.1007/s00601-008-0283-x
Citations: PlumX Metrics

2000RO21      Phys.Rev.Lett. 85, 708 (2000)

J.Roche, J.M.Friedrich, D.Lhuillier, P.Bartsch, D.Baumann, J.Berthot, P.Y.Bertin, V.Breton, W.U.Boeglin, R.Bohm, N.D'Hose, S.Derber, N.Degrande, M.Ding, M.O.Distler, J.E.Ducret, I.Ewald, H.Fonvieille, J.Friedrich, P.A.M.Guichon, H.Holvoet, Ch.E.Hyde-Wright, P.Jennewein, M.Kahrau, S.Kerhoas, K.W.Krygier, B.Lannoy, A.Liesenfeld, C.Marchand, D.Marchand, J.Marroncle, J.Martino, H.Merkel, P.Merle, G.De Meyer, J.Mougey, U.Muller, R.Neuhausen, Th.Pospischil, G.Quemener, O.Ravel, Y.Roblin, D.Rohe, G.Rosner, D.Ryckbosch, H.Schmieden, G.Tamas, M.Tytgat, M.Vanderhaeghen, L.Van Hoorebeke, R.Van de Vyver, J.Van de Wiele, P.Vernin, A.Wagner, Th.Walcher, M.Weiss

First Determination of Generalized Polarizabilities of the Proton by a Virtual Compton Scattering Experiment

NUCLEAR REACTIONS ¹H(polarized e, e'γ), E=855 MeV; measured σ(E, θ(e), θ(p)). ¹H deduced dynamic structure functions, generalized polarizibilities. High-resolution spectrometers, virtual Compton scattering.

doi: 10.1103/PhysRevLett.85.708
Citations: PlumX Metrics

1999DE05      Phys.Lett. 451B, 275 (1999)

J.Decharge, J.-F.Berger, K.Dietrich, M.S.Weiss

Superheavy and Hyperheavy Nuclei in the Form of Bubbles or Semi-Bubbles

NUCLEAR STRUCTURE ²⁹²120; calculated semi-bubble nucleus single particle energies, deformation energy. ²⁹²120, ³³⁰126; calculated binding energies, densities, α-decay T_1/2. Self-consistent HFB. Heavier nuclei also considered.

doi: 10.1016/S0370-2693(99)00225-7
Citations: PlumX Metrics

1999UT01      Phys.Rev.Lett. 82, 505 (1999)

S.B.Utter, P.Beiersdorfer, A.Barnes, R.W.Lougheed, J.R.C.Lopez-Urrutia, J.A.Becker, M.S.Weiss

Reexamination of the Optical Gamma Ray Decay in ²²⁹Th

RADIOACTIVITY ²³³U(α); measured photon spectra; deduced alpha flourescence in air. ²²⁹Th deduced no observation of decay from first excited level.

doi: 10.1103/PhysRevLett.82.505
Citations: PlumX Metrics

1996KR14      Phys.Rev. C54, 2399 (1996)

S.J.Krieger, P.Bonche, H.Flocard, P.H.Heenen, R.Mehrem, M.S.Weiss

Generator Coordinate Method Calculation of the E2 Decay Lifetime of Shape Isomers in the Actinide Region

NUCLEAR STRUCTURE ^236,238,240Pu; calculated nonconstrained, constrained HF-BCS quadrupole deformation energy, quadrupole moments at different minima and barriers, proton quadrupole transition matrix elements, E2-decay T_1/2 for shape isomers. Generator coordinate method.

doi: 10.1103/PhysRevC.54.2399
Citations: PlumX Metrics

1995ME07      Nucl.Phys. A588, 597 (1995)

J.Meyer, P.Bonche, M.S.Weiss, J.Dobaczewski, H.Flocard, P.-H.Heenen

Quadrupole and Octupole Correlations in Normal, Superdeformed and Hyperdeformed States of ¹⁹⁴Pb

NUCLEAR STRUCTURE ^{192,194,196,198,200}Pb; calculated superdeformed band population evolution, spectra, energy curves vs quadrupole moment, quadrupole, octupole correlations in normal, hyperdeformed bands as well. Generator coordinate method.

doi: 10.1016/0375-9474(95)00055-6
Citations: PlumX Metrics

1994BO24      Nucl.Phys. A574, 185c (1994)

P.Bonche, E.Chabanat, B.Q.Chen, J.Dobaczewski, H.Flocard, B.Gall, P.H.Heenen, J.Meyer, N.Tajima, M.S.Weiss

Microscopic Approach to Collective Motion

NUCLEAR STRUCTURE ¹⁹²Hg, ¹⁹⁴Pb; calculated superdeformed bands, energies, quadrupole moments, dynamical, rigid body moments of inertia, Eγ. ^{194,196,198,200,202,204,206,208,210,212,214,216,218,220}Pb; calculated proton, neutron rms radii. Microscopic approach, collective motion.

doi: 10.1016/0375-9474(94)90045-0
Citations: PlumX Metrics

1994KR06      Nucl.Phys. A572, 384 (1994)

S.J.Krieger, P.Bonche, H.Flocard, P.H.Heenen, M.S.Weiss

GCM Calculation of the E2 Decay Lifetimes of Shape Isomers

NUCLEAR STRUCTURE ^230,232Th, ²³⁸U; calculated deformation energy vs mass quadrupole moment, first barrier, second minimum, absolute miminum quadrupole moment, charge quadrupole transition matrix element between superdeformed, ground bands, isomer E2 decay T_1/2. Hartree-Fock BCS calculations.

doi: 10.1016/0375-9474(94)90181-3
Citations: PlumX Metrics

1993FL04      Nucl.Phys. A557, 559c (1993)

H.Flocard, B.Q.Chen, B.Gall, P.Bonche, J.Dobaczewski, P.H.Heenen, M.S.Weiss

Hartree-Fock and Hartree-Fock-Bogoliubov Calculations of Superdeformed Bands

NUCLEAR STRUCTURE ^192,194Hg, ¹⁹⁴Pb; calculated superdeformed bands quadrupole moments, dynamical, rigid body moments of inertia. Hartree-Fock, HFB calculations, limitations discussed.

doi: 10.1016/0375-9474(93)90569-J
Citations: PlumX Metrics

1993TA02      Nucl.Phys. A551, 434 (1993)

N.Tajima, P.Bonche, H.Flocard, P.-H.Heenen, M.S.Weiss

Self-Consistent Calculation of Charge Radii of Pb Isotopes

NUCLEAR STRUCTURE ^{194,202,214,220}Pb; calculated charge radii. Hartree-Fock+BCS method, Skyrme forces.

doi: 10.1016/0375-9474(93)90456-8
Citations: PlumX Metrics

1992CH08      Phys.Rev. C45, 1700 (1992)

C.R.Chinn, J.-F.Berger, D.Gogny, M.S.Weiss

Limits on the Lifetime of the Shape Isomer of ²³⁸U

RADIOACTIVITY ²³⁸U; calculated fission isomer partial T_1/2. Constrained Hartree-Fock-Bogoliubov.

doi: 10.1103/PhysRevC.45.1700
Citations: PlumX Metrics

1992CH32      Phys.Rev. C46, R1582 (1992)

B.-Q.Chen, P.-H.Heenen, P.Bonche, M.S.Weiss, H.Flocard

Observation of Identical Bands in Superdeformed Nuclei with the Cranked Hartree-Fock Method

NUCLEAR STRUCTURE ^194,192Hg, ¹⁹⁴Pb; calculated superdeformed band level energies, quadrupole moments, dynamical, rigid moments of inertia; deduced twinning characteristics. Cranked Hartree-Fock, Skyrme effective interaction.

doi: 10.1103/PhysRevC.46.R1582
Citations: PlumX Metrics

1992KR07      Nucl.Phys. A542, 43 (1992)

S.J.Krieger, P.Bonche, M.S.Weiss, J.Meyer, H.Flocard, P.-H.Heenen

Super-Deformation and Shape Isomerism: Mapping the isthmus

NUCLEAR STRUCTURE Z=108-152; calculated excitation energy, rigid moment of inertia. ^{190,192,194,196,198,200,202,204,206,210,212,214,216,218,220,222,224,226,228,230}Pb calculated rigid moment of inertia, quadrupole moment, superdeformed isomers; deduced shape isomerism isthmus superdeformation region. Microscopic Hartree-Fock-BCS formalism.

doi: 10.1016/0375-9474(92)90395-Z
Citations: PlumX Metrics

1991BO19      Phys.Rev.Lett. 66, 876 (1991)

P.Bonche, S.J.Krieger, M.S.Weiss, J.Dobaczewski, H.Flocard, P.-H.Heenen

Octupole Softness of Superdeformed ¹⁹⁴Pb

NUCLEAR STRUCTURE ¹⁹⁴Pb; analyzed data; deduced band structure, superdeformed softness features. Generator coordinate method, pairing projection.

doi: 10.1103/PhysRevLett.66.876
Citations: PlumX Metrics

1990BE17      Phys.Rev. C41, R2483 (1990)

J.F.Berger, J.D.Anderson, P.Bonche, M.S.Weiss

Microscopic Study of the ²³⁸U-²³⁸U System and Anomalous Pair Production

NUCLEAR REACTIONS ²³⁸U(²³⁸U, X), E ≈ 5.5 MeV/nucleon; calculated anomalous pair production E, Z-dependences, quasivibrational levels. Constrained HFB.

doi: 10.1103/PhysRevC.41.R2483
Citations: PlumX Metrics

1990BO40      Nucl.Phys. A519, 509 (1990)

P.Bonche, J.Dobaczewski, H.Flocard, P.H.Heenen, S.J.Krieger, J.Meyer, M.S.Weiss

Quadrupole Collective Correlations and the Depopulation of the Superdeformed Bands in Mercury

NUCLEAR STRUCTURE ^{190,192,194,196,198}Hg; calculated deformation energy, wave functions, proton quadrupole moments, superdeformed band decay Iγ. Self-consistent generator coordinate method, Hartree-Fock plus BCS wave functions.

doi: 10.1016/0375-9474(90)90443-P
Citations: PlumX Metrics

1990KR11      Nucl.Phys. A517, 275 (1990)

S.J.Krieger, P.Bonche, H.Flocard, P.Quentin, M.S.Weiss

An Improved Pairing Interaction for Mean Field Calculations using Skyrme Potentials

NUCLEAR STRUCTURE ¹⁹⁴Hg, ²³²Th; calculated total energy vs quadrupole moment. Mean field calculations, Skyrme potentials.

doi: 10.1016/0375-9474(90)90035-K
Citations: PlumX Metrics

1989BO24      Nucl.Phys. A500, 308 (1989)

P.Bonche, S.J.Krieger, P.Quentin, M.S.Weiss, J.Meyer, M.Meyer, N.Redon, H.Flocard, P.-H.Heenen

Superdeformation and Shape Isomerism at Zero Spin

NUCLEAR STRUCTURE ^{186,196,194,192,190,188,186,202,210}Os, ^{200,198,196,194,192,190,188,186}Pt, ^{194,202,210,218}Hg; calculated Hartree-Fock energies, energy surfaces. ^{192,194,196,198,200,202,204,206,208,210,212,214,216,218}Hg; calculated secondary minima deformations. ^194,196,198Pt; calculated axial deformation energies. ^66,68Ni, ^190,192Pt, ^206,208,210Os, ^194,196,214Hg; deduced possible superdeformation effects. Microscopic Hartree-Fock plus BCS.

doi: 10.1016/0375-9474(89)90426-0
Citations: PlumX Metrics

1986RE15      Phys.Lett. 181B, 223 (1986)

N.Redon, J.Meyer, M.Meyer, P.Quentin, M.S.Weiss, P.Bonche, H.Flocard, P.-H.Heenen

A Self-Consistent Study of Triaxial Deformations in Heavy Nuclei

NUCLEAR STRUCTURE ¹³⁸Sm, ¹⁸⁶Pt, ¹⁹²Os; calculated constant pairing matrix elements, potential energy surfaces. Lattice Hartree-Fock + BCS calculations.

doi: 10.1016/0370-2693(86)90036-5
Citations: PlumX Metrics

1985BO36      Nucl.Phys. A443, 39 (1985)

P.Bonche, H.Flocard, P.H.Heenen, S.J.Krieger, M.S.Weiss

Self-Consistent Study of Triaxial Deformations: Application to the isotopes of Kr, Sr, Zr and Mo

NUCLEAR STRUCTURE ^80,102Zr; calculated quasiparticle energies, deformation energy curves, proton, neutron rms radii, deformation, quadrupole moments, binding energies. ^{86,88,90,92,94,96,98,100,102,104}Zr, ^{90,92,96,98,104}Mo, ^{88,90,94,102,100}Sr, ^98,100Kr; calculated deformation energy surfaces. ⁹⁰Kr; calculated deformation energy surfaces, binding energy. ^{84,82,80,78,76}Zr, ^80,78,76,74Sr, ^76,74Kr; calculated deformation energy surfaces.

doi: 10.1016/0375-9474(85)90320-3
Citations: PlumX Metrics

1984FL04      Prog.Theor.Phys.(Kyoto) 72, 1000 (1984)

H.Flocard, P.H.Heenen, S.J.Krieger, M.S.Weiss

Configuration Space, Cranked Hartree-Fock Calculations for the Nuclei ¹⁶O, ²⁴Mg and ³²S

NUCLEAR STRUCTURE ¹⁶O, ³²S, ²⁴Mg; calculated levels, band structure, fission modes. Cranked Hartree-Fock method.

doi: 10.1143/PTP.72.1000
Citations: PlumX Metrics

1982FL04      Nucl.Phys. A391, 285 (1982)

H.Flocard, P.H.Heenen, S.J.Krieger, M.S.Weiss

From Ground State to Scission: The spinning life of ²⁰Ne

NUCLEAR STRUCTURE ²⁰Ne; calculated level energy, moment of inertia, quadrupole moment, asymmetry vs L. Cranked Hartree-Fock method.

doi: 10.1016/0375-9474(82)90611-X
Citations: PlumX Metrics

1981FL03      Phys.Lett. 105B, 14 (1981)

H.Flocard, M.S.Weiss

Generation of High-Frequency Components in TDHF Heavy-Ion collisions

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), E=400 MeV; calculated integrated fragment density, time evolution of fragment rms radius. TDHF.

doi: 10.1016/0370-2693(81)90029-0
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1981KR13      Phys.Rev. C24, 928 (1981)

S.J.Krieger, M.S.Weiss

Fusion Calculations with the Skyrme Interactions

NUCLEAR REACTIONS ²⁴Mg(¹⁶O, X), E(cm) ≈ 17-100 MeV; calculated σ(fusion, E); deduced nuclear interaction dependence. TDHF, Skyrme forces.

doi: 10.1103/PhysRevC.24.928
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1979BO18      Phys.Rev. C20, 641 (1979)

P.Bonche, K.T.R.Davies, B.Flanders, H.Flocard, B.Grammaticos, S.E.Koonin, S.J.Krieger, M.S.Weiss

Time-Dependent Hartee-Fock Calculations of Fusion Cross Sections for ¹⁶O + ⁴⁰Ca and ²⁸Si + ²⁸Si

NUCLEAR REACTIONS ¹⁶O(⁴⁰Ca, X), E(cm)=30-250 MeV; ²⁸Si(²⁸Si, X), E(cm)=35-250 MeV; calculated fusion σ; deduced angular momentum fusion window. Time-dependent Hartree-Fock, Skyrme interaction.

doi: 10.1103/PhysRevC.20.641
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1978DA18      Phys.Rev. C18, 2631 (1978)

K.T.R.Davies, H.T.Feldmeier, H.Flocard, M.S.Weiss

Comparison of Two- and Three-Dimensional Time-Dependent Hartree-Fock Calculations of the Reactions ¹⁶O + ¹⁶O and ⁴⁰Ca + ⁴⁰Ca

NUCLEAR REACTIONS ¹⁶O(¹⁶O, X), E=105 MeV; ⁴⁰Ca(⁴⁰Ca, X), E=192 MeV; calculated energy loss, deflection function in 2-, 3-dimensional time-dependent Hartree-Fock.

doi: 10.1103/PhysRevC.18.2631
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1978FL04      Phys.Rev. C17, 1682 (1978)

H.Flocard, S.E.Koonin, M.S.Weiss

Three-Dimensional Time-Dependent Hartree-Fock Calculations: Application to ¹⁶O + ¹⁶O Collisions

NUCLEAR REACTIONS ¹⁶O(¹⁶O, X), E=105 MeV; calculated fusion, strongly damped collisions. 3-D tdhf approximation.

doi: 10.1103/PhysRevC.17.1682
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1978FL06      Phys.Rev. C18, 573 (1978)

H.Flocard, M.S.Weiss

Comparison of Two-Dimensional and Three-Dimensional Time-Dependent Hartree-Fock for ⁴⁰Ca + ⁴⁰Ca at E(lab) = 278 MeV

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), E=2.78 MeV; calculated 2-, 3-dimensional time-dependent Hartree-Fock interactions.

doi: 10.1103/PhysRevC.18.573
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1978KO22      Phys.Lett. 77B, 13 (1978)

S.Koonin, B.Flanders, H.Flocard, M.Weiss

A Separable Approximation to Time-Dependent Hartree-Fock Calculations

NUCLEAR REACTIONS ¹⁶O(¹⁶O, ¹⁶O), ⁴⁰Ca(⁴⁰Ca, ⁴⁰Ca); calculated reaction parameters.

doi: 10.1016/0370-2693(78)90188-0
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1978SE15      Fizika, Suppl. 10, 37 (1978)

J.B.Seaborn, M.S.Weiss

Particle Transfer Width in 3D TDHF for Ca⁴⁰ + Ca⁴⁰

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), E=278 MeV; calculated particle transfer widths. Three-dimensional time-dependent Hartree-Fock.

1976CU06      Phys.Rev. C14, 1615 (1976)

R.Y.Cusson, H.P.Trivedi, H.W.Meldner, M.W.Weiss, R.E.Wright

Self-Consistent K-Matrix-Model Calculation for Finite and Superheavy Nuclei

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁹⁰Zr, ²⁰⁸Pb, ²⁹⁸Fl; calculated total binding energies, rms radii, electron scattering form factors.

doi: 10.1103/PhysRevC.14.1615
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1974SH08      Phys.Rev. C9, 1679 (1974)

C.M.Shakin, M.S.Weiss

Cluster Model and the Photodisintegration of ⁶Li

NUCLEAR REACTIONS ⁶Li(γ, p), (γ, X); calculated σ(E). Coupled channels, cluster model.

doi: 10.1103/PhysRevC.9.1679
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1973AL03      Phys.Rev. C7, 1089 (1973)

J.Alster, B.F.Gibson, J.S.McCarthy, M.S.Weiss, R.M.Wright

Elastic Electron Scattering from ⁸⁸Sr

NUCLEAR REACTIONS ⁸⁸Sr(e, e), E=200, 400 MeV; measured σ(E, θ); deduced nuclear charge distributions; enriched target.

doi: 10.1103/PhysRevC.7.1089
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1973SH08      Phys.Rev. C7, 1820 (1973)

C.M.Shakin, M.S.Weiss

Threshold Photodisintegration of ⁶Li

NUCLEAR REACTIONS ⁶Li(γ, X), E=threshold-12 MeV; calculated σ(E), average neutron energy (E).

doi: 10.1103/PhysRevC.7.1820
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1973SH12      Phys.Rev. C8, 411 (1973)

C.M.Shakin, M.S.Weiss

Nuclear Polarication and the Muonic X-Ray Spectrum of Pb

NUCLEAR STRUCTURE, Mesic-Atoms ²⁰⁸Pb; calculated muonic levels.

doi: 10.1103/PhysRevC.8.411
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1972BL01      Phys.Rev. C5, 238 (1972)

S.D.Bloom, M.S.Weiss, C.M.Shakin

Nuclear γ Rays Following K^- Capture

NUCLEAR REACTIONS ¹⁶O, ²⁰⁸Pb(K^-, Xγ), E approx 0; calculated capture rates.

doi: 10.1103/PhysRevC.5.238
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1972GI11      Phys.Rev. C6, 741 (1972)

B.F.Gibson, A.Goldberg, M.S.Weiss

Effects of LAMBDA-≥ Coupling in LAMBDA⁴H, LAMBDA⁴He, and LAMBDA⁵He

doi: 10.1103/PhysRevC.6.741
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1971HA45      Phys.Rev. C4, 1189 (1971)

L.F.Hansen, J.L.Kammerdiener, M.S.Weiss

Analysis of the Scattering of 24-MeV ³He Particles from the Even Isotopes of Zinc

NUCLEAR REACTIONS ^64,66,68,70Zn(³He, ³He), (³He, ³He'), E=24 MeV; measured σ(θ); deduced optical model parameters. ^64,66,68,70Zn deduced deformation parameters.

doi: 10.1103/PhysRevC.4.1189
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1970AV03      Yad.Fiz. 11, 1133 (1970); Sov.J.Nucl.Phys. 11, 629 (1970)

M.P.Avotina, E.P.Grigorev, A.V.Zolotavin, V.O.Sergeev, M.I.Sovtsov, M.Weiss, J.Urbanec, J.Vrzal, J.Liptak

The Decays of Pm¹⁴³, Pm¹⁴⁴, and Pm¹⁴⁶

RADIOACTIVITY ^143,144,146Pm; measured Eγ, Iγ, I(ce); deduced log ft. ^143,144,146Nd, ¹⁴⁶Sm deduced levels, J, π, ICC, γ-multipolarity.

1970SH15      Phys.Rev. C2, 1809 (1970)

C.M.Shakin, M.S.Weiss

Threshold Photodisintegration of Pb²⁰⁸

NUCLEAR REACTIONS ²⁰⁸Pb(γ, n), E=9-13 MeV; ²⁰⁷Pb(n, γ), E=thermal; measured nothing; analyzed available data.

doi: 10.1103/PhysRevC.2.1809
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1965WE06      Phys.Letters 19, 393 (1965)

M.S.Weiss

Dipole Photoeffect in ¹⁶O II

NUCLEAR STRUCTURE ¹⁶O; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)90915-7
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1958FU71      Phys.Rev. 112, 560 (1958)

E.G.Fuller, M.S.Weiss

Splitting of the Giant Resonance for Deformed Nuclei

doi: 10.1103/PhysRev.112.560
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0111.

1957WE17      Bull.Am.Phys.Soc. 2, No.1, 31, JA9 (1957); Oral Report

M.M.Weiss, R.I.Walter, O.R.Gilliam, V.W.Cohen

Paramagnetic Resonance Spectrum of V⁴⁹

1950WE03      Phys.Rev. 78, 202 (1950)

M.T.Weiss, M.W.P.Strandberg, R.B.Lawrance, C.C.Loomis

On the Nuclear Spin of B¹⁰

doi: 10.1103/PhysRev.78.202
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Note: The following list of authors and aliases matches the search parameter M.Weiss: , M.M.WEISS, M.S.WEISS, M.T.WEISS, M.W.WEISS