S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound...

98
95Na01 Orthogonality Nodes and the Three-Body Bound State Collapse S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995).

Transcript of S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound...

Page 1: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na01 Orthogonality Nodes and the Three-Body Bound State Collapse

S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995).

Page 2: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na02 Study of Pre-Scission Evaporation for 84Kr + 27Al at 10.6 MeV/u using 3π-Phoswich Detector System

T. Nakagawa, K. Yuasa-Nakagawa, K. Furutaka, K. Matsuda, K. Yoshida, Y. Futami, T. Mizota, Y. Honjo, N. Tomita, S. M.Lee, J. Kasagi, W. Q. Shen, Nucl. Phys. A583, 149c (1995).

Nuclear Reactions: 27Al(84Kr,F), E=10.6 MeV/nucleon; measured charged particle spectra, multiplicity, fission(fragment)(fragment)-coin; deduced pre-scission particles emission related features.

Page 3: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na03 Octupole Correlations in Excited Bands of Superdeformed 152Dy

T. Nakatsukasa, K. Matsuyanagi, S. Mizutori, W. Nazarewicz, Phys. Lett. 343B, 19 (1995).

Nuclear Structure: 152Dy; calculated superdeformed band dynamical moments of inertia; deduced rotation, octupole vibrationinterplay features. Cranked shell model, RPA.

Page 4: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na04 Study of Double Strangeness Nuclei by an Emulsion-Scintillating Fiber Hybrid Method

K. Nakazawa, Nucl. Phys. A585, 75c (1995).

Page 5: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na05 Application of Microscopic Dynamical Theory to Examination of Fragmentation of Highly Excited Hypernuclei

Y. Nara, A. Ohnishi, T. Harada, Nucl. Phys. A585, 325c (1995).

Nuclear Reactions: 12C(π+,K+), E at 1050 MeV/c; calculated hyperfragments formation probabilities. Microscopic dynamicaltheory.

Page 6: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na06 Study of Hyperfragments Production in Stopped K- Reaction within the Antisymmetrized Molecular Dynamics

Y. Nara, A. Ohnishi, T. Harada, Nucl. Phys. A585, 329c (1995).

Nuclear Reactions: 12C(K-,π-), E at rest; calculated hyperfragment production, formation probability vs mass number. Antisym-metrized molecular dynamics model.

Page 7: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na07 Systematics of Fragment Angular Momentum in Low-Energy Fission of Actinides

H. Naik, S. P. Dange, R. J. Singh, T. Datta, Nucl. Phys. A587, 273 (1995).

Nuclear Reactions: 229Th, 235, 233U, 239, 241Pu, 245Cm(n,F), E=thermal; measured fission fragment independent isomeric yieldratio for Sb, Te, I, Xe, Cs isotopes. Radiochemical, γ-spectroscopic techniques.

Radioactivity: 252Cf(SF); measured fission fragment independent isomeric yield ratio for Sb, Te, I, Xe, Cs isotopes. Radiochemi-cal, γ-spectroscopic techniques.

Page 8: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na08 Target Mass Dependence of 4H(Lambda) Formation Mechanism from K- Absorption at Rest

Y. Nara, A. Ohnishi, T. Harada, Phys. Lett. 346B, 217 (1995).

Nuclear Reactions: 16O, 12C, 9Be, 7Li(K-, X), E=8-20 MeV; calculated 4H(lambda) hypernucleus formation probability.

Page 9: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na09 Lifetimes in the Decay of 40Ca and 47V Studied by Crystal Blocking

V. Nanal, M. B. Kurup, K. G. Prasad, Phys. Rev. C51, 2439 (1995).

Nuclear Reactions: 28Si(12C,X), E=45-84 MeV; 28Si(19F, X), E=60, 88 MeV; measured evaporation residues blocking patterns.40Ca, 47V deduced evaporation decay T1/2. Single Si < 100 > crystal.

Page 10: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na10 Algebraic Realization of the Quantum Rotor-Odd-A Nuclei

H. A. Naqvi, C. Bahri, D. Troltenier, J. P. Draayer, A. Faessler, Z. Phys. A351, 259 (1995).

Nuclear Structure: 25Mg; calculated normal SU(3) symmetry eigenvalues. 159Dy, 165Er; calculated pseudo-SU(3) symmetryeigenvalues. Quantum rotor algebraic realizations. 23Na; calculated eigenstates. Algebraic realization of the many-particle Nils-son model.

Page 11: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na11 Coulomb Dissociation of a Halo Nucleus 11Be and Direct Breakup Mechanism

T. Nakamura, S. Shimoura, T. Kobayashi, T. Teranishi, K. Abe, N. Aoi, Y. Doki, M. Fujimaki, N. Inabe, N. Iwasa, K. Katori, T.Kubo, H. Okuno, T. Suzuki, I. Tanihata, Y. Watanabe, A. Yoshida, M. Ishihara, Nucl. Phys. A588, 81c (1995).

Nuclear Reactions: Pb(11Be,10Be), E=72 MeV/nucleon; measured σ(φ) in 11Be rest frame; deduced reaction mechanism. 11Bededuced dipole strength distribution. Kinematically complete experiment, Coulomb dissociation.

Page 12: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na12 Saturation Properties and Incompressibility of Nuclear Matter: A consistent determination from nuclear masses

R. Nayak, V. S. Uma Maheswari, L. Satpathy, Phys. Rev. C52, 711 (1995).

Page 13: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na13 Multiclustering and Physics of Exotic Nuclear Shapes

W. Nazarewicz, S. Cwiok, J. Dobaczewski, J. X. Saladin, Acta Phys. Pol. B26, 189 (1995).

Nuclear Structure: 220, 224Rn, 222, 226, 230Ra, 224, 228, 232Th, 226, 230, 234U; compiled, reviewed, analyzed potential energy surfacepredictions; deduced hyperdeformed minimum resemblance to di-nucleus. Multi-cluster model.

Page 14: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na14 Boson-Fermion Mapping of Collective Fermion-Pair Alegebras

P. Navratil, H. B. Geyer, J. Dobaczewski, Phys. Rev. C52, 1394 (1995).

Page 15: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na15 Refinement of the Gross Theory of β-Decay for Odd-Odd Nuclei

H. Nakata, T. Tachibana, M. Yamada, Nucl. Phys. A594, 27 (1995).

Nuclear Structure: A ≤ 250; calculated β--decay, (β++EC)-decay T1/2, log ft, other aspects for odd-odd nuclei. Refined β-decaygross theory.

Page 16: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na16 Unique Potentials for the Elastic Scattering of 350 MeV 7Li from 12C and 28Si

A. Nadasen, J. Brusoe, J. Farhat, T. Stevens, J. Williams, L. Nieman, J. S. Winfield, R. E. Warner, F. D. Becchetti, J. W.Janecke, T. Annakkage, J. Bajema, D. Roberts, H. S. Govinden, Phys. Rev. C52, 1894 (1995).

Nuclear Reactions: 12C, 28Si(7Li,7Li), E=350 MeV; measured σ(θ); deduced optical model parameters. Double-folding calcula-tions.

Page 17: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na17 Even-Odd Staggering of Pairing-Force Strength

R. C. Nayak, J. M. Pearson, Phys. Rev. C52, 2254 (1995).

Nuclear Structure: Z=30-100; N=30-144; analyzed mass data; deduced fourth-order even-odd mass difference rms errors.A=80-235; analyzed Q(β) data; deduced rms errors. High speed Hartree-Fock approximation, Skyrme force.

Page 18: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na18 Limiting Temperatures of Neutron Rich Nuclei: A possible interpretation of data from isotope yield ratios

J. B. Natowitz, K. Hagel, R. Wada, Z. Majka, P. Gonthier, J. Li, N. Mdeiwayeh, B. Xiao, Y. Zhao, Phys. Rev. C52, R2322(1995).

Nuclear Reactions: 197Au(197Au,X), E=600 MeV/nucleon; analyzed He, Li isotopes yield ratios data; deduced neutron rich nucleilimiting temperature related features.

Page 19: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na19 Temperature Dependence of Heavy Meson Masses

F. S. Navarra, C. A. A. Nunes, Phys. Lett. 356B, 439 (1995).

Page 20: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na20 Physics of Exotic Nuclear States

W. Nazarewicz, J. Dobaczewski, T. R. Werner, Phys. Scr. T56, 9 (1995).

Nuclear Structure: Z=18-28; compiled, reviewed two-proton separation energies. Z=8-28; compiled, reviewed charge radii.N=88-120; A=138-170; compiled, reviewed two neutron separation energies. Exotic nuclear states, other aspects discussed.

Page 21: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na21 Fusion l Distribution in 16O, 28Si + 115In Reactions at Near- and Sub-Barrier Energies

B. K. Nayak, R. K. Choudhury, L. M. Pant, D. M. Nadkarni, S. S. Kapoor, Phys. Rev. C52, 3081 (1995).

Nuclear Reactions: 115In(16O,X), E=55-80 MeV; 115In(28Si, X), E=105-115 MeV; measured Eα, γ-multiplicity distributions;deduced l-distribution moments. One-dimensional barrier penetration model.

Page 22: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na22 Spallation Neutron Measurement by the Time-of-Flight Method with a Short Flight Path

T. Nakamoto, K. Ishibashi, N. Matsufuji, N. Shigyo, K. Maehata, S. -I. Meigo, H. Takada, S. Chiba, M. Numajiri, T. Nakamura,Y. Watanabe, J. Nucl. Sci. Technol. (Tokyo) 32, 827 (1995).

Nuclear Reactions: C, Pb(p,xn), E=0.8, 1.5 GeV; measured σ(θ,En). Tof, liquid scintillators. HETC calculations.

Page 23: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na23 Compton Scattering of 20- to 40-keV Photons

Y. Namito, S. Ban, H. Hirayama, N. Nariyama, H. Nakashima, Y. Nakane, Y. Sakamoto, N. Sasamoto, Y. Asano, S. Tanaka,Phys. Rev. A51, 3036 (1995).

Nuclear Reactions: 27Al, C, Fe, Cu, 197Au, Pb(γ,γ), E=20-40 keV; measured Compton scattering spectra; deduced incoherentscattering function. High purity Ge detectors.

Atomic Physics: +27}Al, C, Fe, Cu, 197Au, Pb(γ,γ), E=20-40 keV; measured Compton scattering spectra; deduced incoherentscattering function. High purity Ge detectors.

Page 24: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na24 Phase Shift Analyses of pp Elastic Scattering between 500 and 800 MeV

J. Nagata, H. Yoshino, M. Matsuda, Prog. Theor. Phys. (Kyoto) 93, 559 (1995).

Nuclear Reactions: 1H(polarized p,p), E=447-735 MeV; analyzed polarization observables data; deduced scattering amplitudes.Phase shift analysis.

Page 25: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na25 Effect of Nuclear Recoil Energy on Backward Bremsstrahlung of Polarized Electrons

I. M. Nadzhafov, G. R. Rustamova, A. M. Aliev, N. I. Nadzhafov, Bull. Rus. Acad. Sci. Phys. 59, 1919 (1995).

Page 26: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na26 Beam of Linearly Polarized Shower γ-Quanta in Crystals with Regard to Fermion Helicity

I. M. Nadzhafov, M. R. Radzhabov, N. I. Nadzhafov, Bull. Rus. Acad. Sci. Phys. 59, 1924 (1995).

Page 27: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na27 Development of a Thin Drift Chamber for the Double Beta Decay Experiment

K. Nagata, H. Ejiri, K. Hayashi, T. Shima, J. Tanaka, Nucl. Instrum. Methods Phys. Res. A362, 261 (1995)

Radioactivity: 214Bi(α), (β-); 214Po(α) [from 214Bi(β-decay)]; measured γ spectra, delayed α-spectra; deduced 214Bi contaminationin Mo source to be used for 2β-decay studies.

Page 28: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na28 Measurements of Response Function of Organic Liquid Scintillator for Neutron Energy Range up to 135 MeV

N. Nakao, T. Nakamura, M. Baba, Y. Uwamino, N. Nakanishi, H. Nakashima, S. -I. Tanaka, Nucl. Instrum. Methods Phys. Res.A362, 454 (1995)

Page 29: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na29 Light Output Measurements of C6H6 and C6H12 Scintillators for Protons

A. A. Naqvi, M. M. Nagadi, S. Shaheen, A. Bari, Nucl. Instrum. Methods Phys. Res. A356, 330 (1995)

Page 30: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na30 Central Force of the Hyperon-Nucleon Interaction in the SU6 Quark Model

C. Nakamoto, Y. Suzuki, Y. Fujiwara, Prog. Theor. Phys. (Kyoto) 94, 65 (1995).

Page 31: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na31 Instrumental Neutron Activation Analysis of Al, V and Ti Employing 252Cf as a Thermal Neutron Source

S. S. Narkhede, Z. R. Turel, J. Radioanal. Nucl. Chem. 200, 435 (1995).

Nuclear Reactions: 27Al, 51V, 50Ti(n,γ), E=thermal; measured Eγ, Iγ; deduced rapid element determination possibility in ores,alloys. Neutron from 252Cf isotopic source.

Page 32: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na32 Instrumental Neutron Activation Analysis of Lanthanides and Other Elements Employing Cirus Reactor as a Thermal NeutronSource

S. S. Narkhede, Z. R. Turel, J. Radioanal. Nucl. Chem. 201, 355 (1995).

Page 33: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na33 SDG Fermion-Pair Algebraic SO(12) and Sp(10) Models and Their Boson Realizations

P. Navratil, H. B. Geyer, J. Dobes, J. Dobaczewski, Ann. Phys. (New York) 243, 218 (1995).

Page 34: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na34 Effects of Linear Polarization and Doppler Broadening on the Exposure Buildup Factors of Low-Energy Gamma Rays

Y. Namito, S. Ban, H. Hirayama, Nucl. Sci. Eng. 120, 199 (1995).

Nuclear Reactions: Cu(γ,γ), E=30-40 keV; calculated scattered photon spectra; deduced linear polarization, Doppler broadeningrole in exposure buildup factors.

Atomic Physics: u(γ,γ), E=30-40 keV; calculated scattered photon spectra; deduced linear polarization, Doppler broadening rolein exposure buildup factors.

Page 35: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Na35 Intermediate Energy Nuclear Reaction Code Intercomparison: Applications to Transmutation of Long-Lived Reactor Wastes

P. Nagel, J. Rodens, M. Blann, H. Gruppelaar, Nucl. Sci. Eng. 119, 97 (1995).

Nuclear Reactions: 208Pb, 90Zr(p,xn), E=25-800 MeV; 90Zr(p, xp), E=80, 160 MeV; analyzed σ(θ,θ(nucleon)). Zr, Pb(p,xn),(p,xp), E < 1 GeV; analyzed nucleon multiplicities. Intercomparison of codes.

Page 36: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NaZT Charge Distribution of Kr Ion Passing through Thin Carbon Foil at 36 MeV/nucleon

Y. Nakai, T. Kambara, Y. Kanai, T. M. Kojima, Y. Awaya, RIKEN-94, p. 74 (1995).

Atomic Physics: (Kr,X), E=36 MeV/nucleon; measured Kr charge state distribution.

Page 37: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NaZU Development of Quasi-Monoenergetic Neutron Field with the use of 80 to 135 MeV Protons Injected on Lithium

T. Nakamura, N. Nakao, M. Takada, E. Kim, M. Imamura, T. Shibata, Y. Uwamino, N. Nakanishi, S. Fujita, S. Nakajima, T.Ichihara, T. T. Inamura, RIKEN-94, p. 58 (1995).

Nuclear Reactions: 12C(n,2nα), 27Al(n,X), 209Bi(n, xn), E=86.3, 96. 5, 106.6, 116.7 MeV; measured spallation σ.

Page 38: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NaZV An 56Fe(d,p)57Fe Mossbauer Measurement

S. Nasu, R. Hanada, Cyclotron Rad. Center, Tohoku Univ., Ann. Rept., 1994, p. 30 (1995).

Nuclear Reactions: 56Fe(d,p), E=6 MeV; measured I(ce), Mossbauer emission spectrum. In-beam Mossbauer spectroscopy.

Page 39: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NaZW (p,xn) Cross Sections for Incident Protons of 0.8, 1.5 and 3.0 GeV

T. Nakamoto, N. Matsufuji, N. Shigyo, K. Maehata, K. Ishibashi, Kyushu Univ. Tandem Acc. Lab. Rept., 1993-1994, p. 19(1995).

Nuclear Reactions: C, 27Al, Fe, In, Pb(p,xn), E=0.8, 1.5, 3 GeV; measured σ(θ,E) for neutron production.

Page 40: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NaZX Observation of D-D Fusion Reactions in Materials

K. Nakashima, R. Koyasako, K. Maeda, T. Bussaki, K. Sagara, Kyushu Univ. Tandem Acc. Lab. Rept., 1993-1994, p. 14(1995).

Nuclear Reactions: 2H(d,p), (d,n), E=20 keV; measured yield for proton, spectra; deduced d-d fusion mechanism in Si, Ni and Timetals.

Page 41: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NaZY Bimodal Nature in Low-Energy Fission of Actinides

Y. Nagame, I. Nishinaka, K. Tsukada, Y. Oura, S. Ichikawa, H. Ikezoe, Y. L. Zhao, K. Sueki, H. Nakahara, T. Ohtsuki, M.Tanikawa, H. Kudo, Y. Hamajima, Y. H. Chung, Japan Atomic Energy Res. Inst. Tandem VDG Ann. Rept., 1994, p. 43 (1995).

Nuclear Reactions: 232Th(p,F), E=15.7 MeV; measured fission σ vs fragment mass; deduced fission mechanism.

Page 42: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NaZZ Study of the 9Be(Σ) Hypernucleus in 9Be(K-, π(±)) Reactions at 600 MeV/c

T. Nagae, T. Fukuda, K. Omata, Y. Shimizu, R. S. Hayano, R. Sawafta, R. E. Chrien, S. Bart, K. Hicks, R. Michael, E. V.Hungerford, B. Mayes, J. Zhu, K. Gross, M. Barakat, K. Baker, L. G. Tang, W. Naing, S. Winnslik, B. Frankrin, Inst. Nucl.Study, Univ. Tokyo, Ann. Rept., 1994, p. 43 (1995).

Nuclear Reactions: 9Be(K-,π+), (K-,π-), E at 600 MeV/c; measured σ(θ,E).

Page 43: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne01 Symmetrical Sum-Rule Analysis of Spectroscopic Factors for One-Nucleon Transfer

R. T. Newman, S. M. Perez, Phys. Rev. C51, 1414 (1995).

Nuclear Structure: 51V, 59Co; calculated f7/2 nucleon transfer spectroscopic factors. Symmetric sum rule analysis.

Page 44: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne02 Thermal Photon Production in High-Energy Nuclear Collisions

J. J. Neumann, D. Seibert, G. Fai, Phys. Rev. C51, 1460 (1995).

Nuclear Reactions: 197Au(S,X), Pb(Pb,X), E at super proton synchrotron; calculated photon spectra. Boost-invariant, one-dimensional fluid dynamics model.

Page 45: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne03 Time Scale of Quasifission from Giant Dipole Resonance γ-Ray Yield

J. Nestler, B. B. Back, K. S. Drese, D. J. Hofman, S. Schadmand, R. Varma, P. Paul, Phys. Rev. C51, 2218 (1995).

Nuclear Reactions: 165Ho(58Ni,X), E=368 MeV; measured γ(fragment)-coin; deduced weak GDR γ-decay evidence, quasifissiontime scale.

Page 46: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne04 Study of the Nucleon Density Distribution of 6He and 8He by Proton Elastic Scattering in Inverse Kinematics

S. Neumaier, G. D. Alkhazov, M. N. Andronenko, T. Beha, K. -H. Behr, A. Brunle, K. Burkard, A. V. Dobrovolsky, P. Egelhof,C. Fischer, G. E. Gavrilov, H. Geissel, V. I. Iatsoura, H. Irnich, A. V. Khanzadeev, G. A. Korolev, A. A. Lobodenko, P. Loren-zen, G. Munzenberg, M. Mutterer, F. Nickel, W. Schwab, D. M. Seliverstov, P. Singer, T. Suzuki, J. P. Theobald, N. A.Timofeev, A. A. Vorobyov, Nucl. Phys. A583, 799c (1995).

Nuclear Reactions: 1H(α,α), E=699 MeV/nucleon; 1H(6He, 6He), E=717 MeV/nucleon; 1H(8He, 8He), E=674 MeV/nucleon; meas-ured differential σ vs four momentum transfer. 8He deduced neutron skin evidence.

Page 47: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne05 Dirac Phenomenology and Nuclear Single-Particle States

Y. Nedjadi, J. R. Rook, Nucl. Phys. A585, 641 (1995).

Nuclear Structure: 40, 48Ca, 58Ni, 90Zr, 116Sn, 208Pb; calculated single particle states, rms charge radii. Relativistic shell model.

Page 48: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne06 Static Quadrupole Moment of High-Spin Isomers in the Doubly-Odd 214Fr Nucleus

G. Neyens, I. Van Asbroeck, R. Coussement, Phys. Rev. C51, 3483 (1995).

Nuclear Structure: 214Fr; analyzed data; deduced high-spin isomers static quadrupole moment.

Page 49: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne07 Dynamic Hyperfine Interaction in Cr2O3 Observed via PAC

M. Neubauer, A. Bartos, K. P. Lieb, D. Lupascu, M. Uhrmacher, Th. Wenzel, Europhys. Lett. 29, 175 (1995).

Radioactivity: 111In(EC); measured γγ(θ,H) vs temperature; deduced electric field gradients, dynamic hyperfine interaction inCr2O3 implanted with 111In(EC)111Cd probes related features.

Page 50: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne08 Remarks on the Collective Coordinates Quantization of the SU(2) Skyrme Model

J. A. Neto, J. Phys. (London) G21, 695 (1995).

Page 51: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne09 Lifetimes of Shears Bands in 199Pb

M. Neffgen, G. Baldsiefen, S. Frauendorf, H. Grawe, J. Heese, H. Hubel, H. Kluge, A. Korichi, W. Korten, K. H. Maier, D.Mehta, J. Meng, N. Nenoff, M. Piiparinen, M. Schonhofer, R. Schubart, U. J. van Severen, N. Singh, G. Sletten, B. V. T. Rao,P. Willsau, Nucl. Phys. A595, 499 (1995).

Nuclear Reactions: 186W(18O,5n), E=92, 94 MeV; measured γγ-coin, DSA, Doppler shifts. 199Pb levels deduced T1/ 2, B(λ).Compton-suppressed Ge detectors. Tilted-axis cranking calculations.

Page 52: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne10 Generalized Vibrating Potential Model for Collective Excitations in Spherical, Deformed and Superdeformed Systems: (1)Atomic nuclei, (2) Metal clusters

V. O. Nesterenko, W. Kleinig, Phys. Scr. T56, 284 (1995).

Nuclear Structure: 158Gd; calculated E2, E3 giant resonance strength functions. Self-consistent vibrating potential model alsoapplied to atomic nuclei, metal clusters.

Page 53: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne11 Deexcitation of a Virtual Cluster in a Nucleus as a Source of Information about Unexplored Properties of the QuasielasticKnockout of Clusters by Protons

V. G. Neudatchin, A. A. Sakharuk, W. W. Kurowsky, Yu. M. Tchuvilsky, Yad. Fiz. 58, No 7, 1234 (1995); Phys. Atomic Nuclei58, 1155 (1995).

Nuclear Reactions: 12C(p,pα), E not given; calculated form factor vs anisotropy θ(q) to different final states. Clusters quasielasticknockout, Glauber-Sitenko theory.

Page 54: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne12 Nuclear Charge Radii and Electric Quadrupole Moments of Even-Even Isotopes

B. Nerlo-Pomorska, B. Mach, At. Data Nucl. Data Tables 60, 287 (1995).

Nuclear Structure: Z=20-98; calculated isotope shifts, charge mean-square radii, electric quadrupole moments. Dynamicalmicroscopic model, even-even nuclei.

Page 55: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ne13 Hyperfine Measurements in Storage Ring

R. Neumann, S. Borneis, T. Engel, B. Fricke, G. Huber, I. Klaft, T. Kuhl, D. Marx, P. Seelig, Phys. Scr. T59, 211 (1995).

Nuclear Moments: +209}Bi; measured hfs in heavy-ion storage ring.

Page 56: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NeZY Nucleon Distributions of 6He and 8He from Intermediate-Energy Proton Elastic Scattering in Inverse Kinematics

S. R. Neumaier, G. D. Alkhazov, M. N. Andronenko, T. Beha, K. -H. Behr, A. Brunle, K. Burkard, A. V. Dobrovolsky, P.Egelhof, C. Fischer, G. E. Gavrilov, H. Geissel, H. M. Hofmann, H. Irnich, A. V. Khanzadeev, G. A. Korolev, A. A. Lobodenko,P. Lorenzen, G. Munzenberg, M. Mutterer, F. Nickel, W. Schwab, D. M. Seliverstov, P. Singer, T. Suzuki, J. P. Theobald, N.A. Timofeev, A. A. Vorobyov, J. Wurzer, V. I. Yatsura, Proc. Intern. Conf on Exotic Nuclei and Atomic Masses, Arles, France,June 19-23, 1995, p. 227 (1995)

Nuclear Reactions: 1H(α,α), E=699 MeV/nucleon; 1H(6He, 6He), E=717 MeV/nucleon; 1H(8He, 8He), E=674 MeV/nucleon; meas-ured differential σ vs four-momentum transfer. 4, 6, 8He deduced matter distributions, radii.

Page 57: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NeZZ Quadrupole Moment Measurements of Po-Isomers in FCC-Plantinum

G. Neyens, S. Ternier, N. Coulier, S. Michiels, R. Coussement, Proc. Intern. Conf on Exotic Nuclei and Atomic Masses, Arles,France, June 19-23, 1995, p. 149 (1995)

Nuclear Moments: +202}, 204Po; measured isomers quadrupole moments. Level-mixing-spectroscopy technique.

Page 58: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ng01 Can One See Coulomb-Nuclear Interference Effects in Nucleon-Nucleus Scattering ( Question )

Nguyen Van Giai, J. Van de Wiele, L. N. Savushkin, Phys. Rev. C52, 2266 (1995).

Nuclear Reactions: 40Ca(n,n), (p,p), (polarized p,p), (polarized n,n), E=160 MeV; calculated σ(θ), polarization vs θ, spin-rotationparameter vs θ; deduced elusive nature of Coulomb-nuclear interference term. Relativistic, nonrelativistic approach comparison.

Page 59: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni01 Spin-Isospin Response Functions and the Effects of the ∆-Hole Configurations in Finite Nuclei

K. Nishida, M. Ichimura, Phys. Rev. C51, 269 (1995).

Nuclear Reactions: 40Ca, 16O, 12C(e,e’), E not given; calculated isovector spin-longitudinal, transverse response functions;deduced ∆-isobar mixing effects.

Page 60: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni02 Multiple-Scattering Effects in the Transverse-Momentum Distributions from (e,e’p) Reactions

N. N. Nikolaev, A. Szczurek, J. Speth, J. Wambach, B. G. Zakharov, V. R. Zoller, Nucl. Phys. A582, 665 (1995).

Nuclear Reactions: 12C, 208Pb(e,e’p), E=high; calculated fast proton transverse momentum distribution. Multiple-scatteringtheory.

Page 61: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni03 Superdeformed Band in 154Dy

D. Nisius, R. V. F. Janssens, T. L. Khoo, I. Ahmad, D. Blumenthal, M. P. Carpenter, B. Crowell, D. Gassmann, T. Lauritsen,W. C. Ma, J. H. Hamilton, A. V. Ramayya, P. Bhattacharyya, C. T. Zhang, P. J. Daly, Z. W. Grabowski, R. H. Mayer, Phys.Rev. C51, R1061 (1995).

Nuclear Reactions: 122Sn(36S,4n), E=165 MeV; measured Eγ, relative Iγ, γγγ-coin. 154Dy deduced high-spin levels, J, π, super-deformation band transitions.

Page 62: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni04 Dissociation of 8He into 6He + n + X at 240 MeV/u

T. Nilsson, F. Humbert, W. Schwab, M. Zinser, Th. Blaich, M. J. G. Borge, L. V. Chulkov, H. Eickhoff, Th. W. Elze, H. Emling,B. Franzke, H. Freiesleben, H. Geissel, K. Grimm, D. Guillemaud-Mueller, P. G. Hansen, R. Holzmann, H. Irnich, L.Johannsen, B. Jonson, J. G. Keller, O. Klepper, H. Klingler, J. V. Kratz, R. Kulessa, D. Lambrecht, Y. Leifels, A. Magel, M.Mohar, E. F. Moore, A. C. Mueller, G. Munzenberg, P. Moller, F. Nickel, G. Nyman, A. Richter, K. Riisager, C. Scheiden-berger, G. Schrieder, B. M. Sherrill, H. Simon, K. Stelzer, J. Stroth, O. Tengblad, W. Trautmann, E. Wajda, E. Zude, and theS034 Collaboration, Nucl. Phys. A583, 795c (1995).

Nuclear Reactions: C, Pb(8He,X), E=240 MeV/nucleon; measured (6He+n) projectile breakup, product transverse momentumdistribution.

Page 63: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni05 Identification of the Neutron-Deficient Isotopes 213, 214Pa

V. Ninov, F. P. Hessberger, S. Hofmann, H. Folger, A. V. Yeremin, A. G. Popeko, A. N. Andreyev, S. Saro, Z. Phys. A351,125 (1995).

Nuclear Reactions: 170Er(51V,X), E=5.2-5.6 MeV/nucleon; measured Eα, Iα; deduced evidence for 213, 214Pa.

Radioactivity: 213, 214Pa(α) [from 150Er(51V, X), E=5.2-5.6 MeV/nucleon]; measured Eα, Iα, αα-correlation; deduced Q(α), T1/2.

Page 64: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni06 evidence for the pseudospin coupling scheme

D. Nisius, R. V. F. Janssens, P. Fallon, B. Crowell, I. Ahmad, C. W. Beausang, M. P. Carpenter, B. Cederwall, P. J. Daly, M.A. Deleplanque, R. M. Diamond, D. Gassmann, Z. W. Grabowski, R. G. Henry, T. L. Khoo, T. Lauritsen, I. Y. Lee, A. O. Mac-chiavelli, R. H. Mayer, F. S. Stephens, P. J. Twin, Phys. Lett. 346B, 15 (1995).

Nuclear Reactions: 122Sn(34S,5n), E=175 MeV; measured Eγ, Iγ, γγγ-coin. 151Dy deduced high-spin levels, J, π, superdeformedband.

Page 65: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni07 Quasifree Photoabsorption on Neutron-Proton Pairs in 3He

J. A. Niskanen, P. Wilhelm, H. Arenhovel, Nucl. Phys. A586, 693 (1995).

Nuclear Reactions: 3He(γ,np), (polarized γ,np), E=200-400 MeV; calculated photoabsorption σ(E), σ(θp), proton polarization,analyzing power, asymmetry vs θ. Quasifree absorption, nucleonic, meson exchange currents, ∆(1232)-isobar excitation.

Page 66: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni08 Double-Dipole Excitations in 40Ca

S. Nishizaki, J. Wambach, Phys. Lett. 349B, 7 (1995).

Nuclear Structure: 40Ca; calculated dipole transition strength distribution, GDR, double GDR.

Nuclear Reactions: 40Ca(γ,X), E=15-30 MeV; calculated TRK sum rule normalized photoabsorption σ(E). Microscopic approach,1p1h-, 2p2h- model space.

Page 67: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni09 Reply to: Comment on ’ photon spectrum of the neutron-proton bremsstrahlung at 170 MeV ’: contributions of np → dγ toinclusive photon energy spectra from np and pd collisions near 200 MeV

H. Nifenecker, J. A. Pinston, Phys. Lett. 349B, 277 (1995).

Nuclear Reactions: C(n,γ), (p,γ), E ≥ 50 MeV; analyzed, reviewed data analyses; deduced energy calibration error possibilities,disagreement with capture process role, np → dγ reaction implications.

Page 68: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni10 Conversion Electron Spectroscopy at the Fragment Mass Analyzer Focal Plane: Studies of isomeric decays near the proton dripline

D. Nisius, R. V. F. Janssens, I. G. Bearden, R. H. Mayer, I. Ahmad, P. Bhattacharyya, B. Crowell, M. P. Carpenter, P. J. Daly,C. N. Davids, Z. W. Grabowski, D. J. Henderson, R. G. Henry, R. Hermann, T. L. Khoo, T. Lauritsen, H. T. Penttila, L.Ciszewski, C. T. Zhang, Phys. Rev. C52, 1355 (1995).

Radioactivity: 149, 150Er(EC) [from 94Mo(58Ni, X), E=250 MeV]; 151, 152Yb(EC) [from 96Ru(58Ni, X), E=250 MeV]; measured Eγ, Iγ,I(ce)-, γ(ce)-coin, T1/2; deduced isomer decay transitions γ-multipolarity, levels, J, π.

Page 69: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni11 Unusual Effects of Diffraction Dissociation for Multiproduction in Deep Inelastic Scattering on Nuclei

N. N. Nikolaev, B. G. Zakharov, V. R. Zoller, Z. Phys. A351, 435 (1995).

Page 70: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni12 Analysis of the (N,xN’) Reactions by Quantum Molecular Dynamics Plus Statistical Decay Model

K. Niita, S. Chiba, T. Maruyama, T. Maruyama, H. Takada, T. Fukahori, Y. Nakahara, A. Iwamoto, Phys. Rev. C52, 2620(1995).

Nuclear Reactions: 1n, 1H(p,X), E=0.5-3 GeV; calculated elastic, inelastic, total, pion production σ(E). 27Al(p, xp), (p,xπ-),E=3.17 GeV; 56Fe(p,xn), E=113, 597 MeV; 208Pb(p,xn), E=0.256-3 GeV; calculated σ(θ,E(particle)). Quantum molecular dynam-ics model.

Page 71: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni13 Pion vs. Photon Absorption on the Deuteron

J. A. Niskanen, P. Wilhelm, Phys. Lett. 359B, 295 (1995).

Nuclear Reactions: 2H(π+,p), E not given; calculated absorption σ vs pion momentum. 2H(γ,n), E=140-440 MeV; calculated pho-todisintegration σ(E).

Page 72: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni14 Fragmentation Cross Sections of Relativistic 3684Kr and 47

109Ag Nuclei in Targets from Hydrogen to Lead

B. S. Nilsen, C. J. Waddington, J. R. Cummings, T. L. Garrard, J. Klarmann, Phys. Rev. C52, 3277 (1995).

Nuclear Reactions: C, 1H, 27Al, Cu, Sn, Pb(84Kr,X), (109Ag,X), E=0.4-1 GeV/nucleon; measured charge changing σ vs targetmass.

Page 73: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni15 Measurement of Fragment Mass Dependent Kinetic Energy and Neutron Multiplicity for Thermal Neutron Induced Fission ofPlutonium-239

K. Nishio, Y. Nakagome, I. Kanno, I. Kimura, J. Nucl. Sci. Technol. (Tokyo) 32, 404 (1995).

Nuclear Reactions: 239Pu(n,F), E=thermal; measured fission fragment yield vs mass, total kinetic energy, neutron multiplicity vsfragment mass; deduced pre-neutron, post-neutron emission fragment mass. Model comparison.

Page 74: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni17 The Two Loop Long Range Effect on the Proton Decay Effective Lagrangian

T. Nihei, J. Arafune, Prog. Theor. Phys. (Kyoto) 93, 665 (1995).

Nuclear Structure: 1H; calculated effective Lagrangian for decay. Two loop long range effects.

Page 75: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni18 Separation of Actinide-Made Transurania by a Gas-Filled Magnetic Separator

V. Ninov, P. Armbruster, F. P. Hessberger, S. Hofmann, G. Munzenberg, Y. Fujita, M. Leino, A. Luttgen, Nucl. Instrum.Methods Phys. Res. A357, 486 (1995)

Nuclear Reactions: 208Pb(22Ne,X), E=5.5 MeV/nucleon; 164Dy(40Ar, X), E=5.9 MeV/nucleon; 238U(20Ne,xn), E=5.7 MeV/nucleon;238U(16O,xn), E not given; measured fragment spectra. Gas-filled magnetic separator.

Page 76: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni19 Analysis of Sensitivity of LR 115 II in Cylindrical Diffusion Chambers for Radon Concentration Determination

D. Nikezic, C. Baixeras, Nucl. Instrum. Methods Phys. Res. A364, 531 (1995)

Radioactivity: 222Rn(α); measured detector sensitivity to cylindrical diffusion chambers characteristics. Radon and its progenyinvestigated.

Page 77: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95Ni20 NMR Study on the Supertransferred Hyperfine Magnetic Field at 55Mn in Ferromagnetic Perovskites La(Co(1-x)Mg(x))(0.5)Mn(0.5)O3

N. Nishimori, K. Asai, M. Mizoguchi, J. Phys. Soc. Jpn. 64, 1326 (1995).

Nuclear Moments: +55}Mn; measured NMR; deduced hyperfine magnetic fields, magnetic properties in ferromagneticPerovskites La(Co(1-x)Mg(x))(0.5)Mn(0.5)O3.

Page 78: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NiZR Identification of the Neutron-Deficient Isotopes 213, 214Pa

V. Ninov, F. P. Hessberger, H. Folger, S. Hofmann, A. G. Popeko, A. V. Yeremin, A. N. Andreyev, S. Saro, Proc. Intern. Confon Exotic Nuclei and Atomic Masses, Arles, France, June 19-23, 1995, p. 571 (1995)

Nuclear Reactions: 170Er(51V,X), E=5.2-5.6 MeV/nucleon; measured residuals decay αα-coin; deduced evidence for 213, 214Pa.

Radioactivity: 213, 214Pa(α) [from 170Er(51V, X), E=5.2-5.6 MeV/nucleon]; measured Eα, T1/ 2.

Page 79: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NiZS New Isotopes of 213, 214Pa and Characteristics of α-Decay of Low Isotopes of Pa

V. Ninov, S. Hofmann, F. P. Hessberger, H. Folger, A. N. Andreev, A. V. Eremin, A. G. Popeko, S. Saro, Program and Thesis,Proc. 45th Ann. Conf. Nucl. Spectrosc. Struct. At. Nuclei, St. Petersburg, p. 108 (1995).

Radioactivity: 213, 214, 215, 216, 217m, 217, 218Pa(α) [from 170Er(51V, X)]; measured Eα, Iα, T1/2. Kinematical separator.

Page 80: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NiZT GT(+) Strength Distributions in N = 15 Isotones

T. Niizeki, H. Ohnuma, T. Yamamoto, K. Katoh, T. Yamashita, Y. Hara, H. Okamura, H. Sakai, S. Ishida, N. Sakamoto, H.Otsu, T. Wakasa, T. Uesaka, Y. Satou, S. Fujita, T. Ichihara, H. Orihara, H. Toyokawa, K. Hatanaka, S. Kato, S. Kubono, M.Yosoi, RIKEN-94, p. 47 (1995).

Nuclear Reactions: 26Mg, 27Al, 28Si(d,X), E=270 MeV; measured excitation energies following 2He emission. 27Mg, 26Na, 28Pdeduced Gamow-Teller strength distributions.

Page 81: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NiZU 27Al(d,2He) Reaction Studied at E(d) = 270 Mev

T. Niizeki, H. Ohnuma, T. Yamamoto, K. Katoh, T. Yamashita, Y. Hara, H. Okamura, H. Sakai, S. Ishida, N. Sakamoto, H.Otsu, T. Wakasa, T. Uesaka, Y. Satou, S. Fujita, T. Ichihara, H. Orihara, H. Toyokawa, K. Hatanaka, S. Kato, S. Kubono, M.Yosoi, RIKEN-94, p. 46 (1995).

Nuclear Reactions: 27Al(d,X), E=270 MeV; measured excitation energy following 2He emission. 27Mg deduced Gamow-Tellertransition strength distribution.

Page 82: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NiZV Effects of the Delta-Isobar on the Spin-Isospin Modes in Quasi-Elastic Scattering Region

K. Nishida, K. Kawahigashi, M. Ichimura, RCNP (Osaka), Ann. Rept., 1994, p. 128 (1995).

Nuclear Structure: 40Ca; calculated isovector spin-response functions in quasi-elastic region, σ, spins; deduced effects of delta-isobar on spin-response functions. RPA, DWIA.

Nuclear Reactions: 12C(polarized p,n), E=494 MeV; calculated σ. DWIA calculation.

Page 83: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NiZW Precise Measurement of iT11 Maximum of 3He(d(pol), p) Reaction at 6.63 15.38 MeV for d(pol) Beam Polarimeter

N. Nishimori, K. Sagara, H. Akiyoshi, R. Koyasako, K. Nakashima, T. Fujita, A. Motoshima, K. Maeda, H. Nakamura, T.Nakashima, Kyushu Univ. Tandem Acc. Lab. Rept., 1993-1994, p. 100 (1995).

Nuclear Reactions: 3He(polarized d,p), E=6.63-15.38 MeV; measured iT11, A(yy).

Page 84: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NiZX Precise Calibration of Vector and Tensor Analyzing Power of 12C(d(pol),d) and 12C(d(pol), p) between 9 and 18 MeV

N. Nishimori, H. Akiyoshi, K. Sagara, R. Koyasako, K. Nakashima, T. Fujita, A. Motoshima, K. Maeda, H. Nakamura, T.Nakashima, Kyushu Univ. Tandem Acc. Lab. Rept., 1993-1994, p. 97 (1995).

Nuclear Reactions: 12C(polarized d,d), (polarized d,p), E=9-18 MeV; measured iT11, A(yy), A(zz), A(xz).

Page 85: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NiZY n(pol)-α Experiment at E(n) = 12 MeV

N. Nishimori, T. Fujita, K. Sagara, K. Maeda, A. Motoshima, F. Wakamatsu, H. Akiyoshi, H. Nakamura, T. Nakashima, KyushuUniv. Tandem Acc. Lab. Rept., 1993-1994, p. 9 (1995).

Nuclear Reactions: 4He(polarized n,n), E=10-18 MeV; measured A(y). Polarized beams, liquid 4He target, tof.

Page 86: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NiZZ Symmetric and Asymmetric Mass Division in 16, 18O Induced Fission of 209Bi

I. Nishinaka, Y. Nagame, K. Tsukada, H. Ikezoe, S. Hamada, K. Sueki, H. Nakahara, M. Tanikawa, T. Ohtsuki, Japan AtomicEnergy Res. Inst. Tandem VDG Ann. Rept., 1994, p. 40 (1995).

Nuclear Reactions: 209Bi(16O,F), E=83, 103 MeV; 209Bi(18O, F), E=84, 111 MeV; measured fission fragment kinetic energy, σ(A),element yield; deduced fission mechanism. Tof.

Page 87: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95No01 Symmetry Analysis of Many-Body Wave Functions, with Applications to the Nuclear Shell Model

A. Novoselsky, J. Katriel, Phys. Rev. C51, 412 (1995).

Page 88: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95No02 Calculation of Fluctuation Errors in the Analysis of Data on Averaged Neutron Cross Sections

G. M. Novoselov, Yad. Fiz. 58, No 1, 23 (1995); Phys. Atomic Nuclei 58, 20 (1995).

Page 89: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95No03 High-Energy Scissors Mode

R. Nojarov, A. Faessler, M. Dingfelder, Phys. Rev. C51, 2449 (1995).

Nuclear Structure: 160Gd; calculated B(λ) distribution; deduced scissors mode related features.

Nuclear Reactions: 160Gd(e,e’), E=25-125 MeV; calculated σ(θ) vs E; deduced E2, M1 excitations relative importance.

Page 90: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95No04 Probing the Limits of Complete Spectroscopy in 164Yb

A. Nordlund, R. Bengtsson, P. Ekstrom, M. Bergstrom, A. Brockstedt, H. Carlsson, H. Ryde, Y. Sun, A. Atac, G. B.Hagemann, B. Herskind, H. J. Jensen, J. Jongman, S. Leoni, A. Maj, J. Nyberg, P. O. Tjom, Nucl. Phys. A591, 117 (1995).

Nuclear Reactions: 152Sm(16O,4n), E=83.2 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 164Yb deduced levels, J, configurations, routhi-ans, alignments. Cranked shell model calculations. Array of Compton-suppressed Ge-dectors.

Page 91: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95No05 An Improved Test of the Exponential Decay Law

E. B. Norman, B. Sur, K. T. Lesko, R. -M. Larimer, D. J. DePaolo, T. L. Owens, Phys. Lett. 357B, 521 (1995).

Radioactivity: 40K(β-), (EC); measured Eγ, Iγ, decay rate; deduced exponential decay law validity. Fresh, ’old’ samples.

Page 92: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95No06 Hypernuclear Weak Decay of 12C(Λ) and 11B(Λ)

H. Noumi, S. Ajimura, H. Ejiri, A. Higashi, T. Kishimoto, D. R. Gill, L. Lee, A. Olin, T. Fukuda, O. Hashimoto, Phys. Rev. C52,2936 (1995).

Nuclear Reactions: 12C(π+,K+), E at 1.05 GeV/c; measured spectra; deduced A=11, 12 hypernuclei mesonic, nonmesonic decaybranching ratios, width ratios.

Page 93: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95No07 Competing Electric and Magnetic Excitations in Backward Electron Scattering from Heavy Deformed Nuclei

R. Nojarov, A. Faessler, M. Dingfelder, Phys. Rev. C52, 3259 (1995).

Nuclear Structure: 154Sm, 154, 156, 158Gd, 168Er; calculated B(λ), transition densities. Quasiparticle RPA.

Nuclear Reactions: 154Sm, 154, 156, 158Gd, 168Er(e, e’), E not given; calculated σ(θ). DWBA, PWBA, quasiparticle RPA.

Page 94: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95No08 Excitation Functions for the Production of Some Radioisotopes of Cs, Xe and I in Proton Bombardment of (nat)Xe up to 100MeV

F. M. Nortier, S. J. Mills, G. F. Steyn, Appl. Radiat. Isot. 46, 1377 (1995).

Nuclear Reactions: ICPND Xe(p,X)125Cs/127Cs/129Cs/130Cs/ 132Cs/136Cs/136mCs/122Xe/123Xe/ 125Xe/125mXe/127Xe/127mXe/129Xe/129mXe/124I/126I/130I/ 130mI/131I, E=threshold-100 MeV; measured residuals production σ(E). Geometry-dependent hybridmodel.

Page 95: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NoZW Heavy-Element Research at RIKEN

T. Nomura, Proc. Intern. Conf on Exotic Nuclei and Atomic Masses, Arles, France, June 19-23, 1995, p. 363 (1995)

Radioactivity: 195At, 196, 197g, 197mRn, 200Fr(α) [from 169Tm, 164, 166Er(36Ar, X), E=5, 6 MeV/nucleon]; measured Eα, T1/2.265106(α) [from 232Th(40Ar,3nα), E=7.5 MeV/nucleon]; measured Eα.

Nuclear Reactions: 232Th(40Ar,X), E=7.5 MeV/nucleon; measured Eα, Iα, αα-coin; deduced evidence for 265106.

Page 96: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NoZX Core Polarization Effects in Pion Scattering from Polarized Spin-(1/2) Nuclei

N. Nose, K. Kume, RCNP (Osaka), Ann. Rept., 1994, p. 107 (1995).

Nuclear Reactions: 13C, 15N(π+,π+), (π-, π-), E=130, 164 MeV; calculated σ(θ), A(y)(θ); deduced core polarization effects. Polar-ized nuclei, DWIA.

Page 97: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NoZY Exclusive Measurement of s1/2 Proton Knockout Reaction and Density Dependence of Effective Nucleon-Nucleon Interaction

T. Noro, M. Tanaka, M. Kawabata, K. Tamura, K. Hatanaka, N. Matsuoka, K. Takahisa, Y. Yuasa, Y. Mizuno, H. Yamazaki,K. Sagara, S. Morinobu, S. Toyama, H. Takeda, M. Nakamura, A. Okihana, RCNP (Osaka), Ann. Rept., 1994, p. 7 (1995).

Nuclear Reactions: 6Li, 12C, 40Ca, 208Pb(p,2p), E=392 MeV; measured A(y)(θ); deduced reaction mechanism. DWIA calculation.

Page 98: S. Nakaichi-Maeda, Phys. Rev. C51, 1633 (1995 ... · Orthogonality Nodes and the Three-Body Bound State Collapse ... Central Force of the Hyperon-Nucleon Interaction in the SU 6

95NoZZ Study of α Decays in the 232Th(40Ar, α3n)265Rf Reaction

T. Nomura, S. C. Jeong, Y. Tagaya, M. Wada, N. Ikeda, S. Kubono, I. Katayama, K. Morita, Y. -H. Pu, A. Yoshida, M.Kurokawa, T. Motobayashi, H. Murakami, Y. Iwata, T. Uchibori, T. Kikuchi, Y. Nagai, H. Kudo, K. Sueki, H. Nakahara, T. Shi-nozuka, M. Fujioka, H. Miyatake, Y. Fujita, T. Shimoda, M. Tanikawa, Inst. Nucl. Study, Univ. Tokyo, Ann. Rept., 1994, p. 158(1995).

Nuclear Reactions: 232Th(40Ar,3nα), E=5.2 MeV/nucleon; measured Eα, T1/2. Tof.

Radioactivity: 265106(α) [from 232Th(40Ar,3nα), E=5.2 MeV/nucleon]; measured measured Eα, T1/ 2. Tof.