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NSR database version of April 11, 2024.

Search: Author = S.Saito

Found 23 matches.

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2003SE18      Mod.Phys.Lett. A 18, 327 (2003)

K.Sekiguchi, H.Sakai, H.Okamura, A.Tamii, T.Uesaka, K.Suda, N.Sakamoto, T.Wakasa, Y.Satou, T.Ohnishi, K.Yako, S.Sakoda, H.Kato, Y.Maeda, M.Hatano, J.Nishikawa, S.Saito, N.Uchigashima, N.Kalantar-Nayestanaki, K.Ermisch

Polarization transfer measurement for d-p elastic scattering: to search for three nucleon force effects

NUCLEAR REACTIONS 1H(polarized d, d), E=135 MeV/nucleon; measured polarization transfer coefficients; deduced three-nucleon force effects.

doi: 10.1142/S0217732303010442
Citations: PlumX Metrics

2001TA10      Nucl.Phys. A684, 290c (2001)

Y.Tanushi, S.Saito, M.Uehara

One-loop Calculations of Hyperon Polarizabilities Under the Large Nc Consistency Condition

doi: 10.1016/S0375-9474(01)00424-9
Citations: PlumX Metrics

2000TA10      Phys.Rev. C61, 055204 (2000)

Y.Tanushi, S.Saito, M.Uehara

One-Loop Calculations of Hyperon Polarizabilities Under the Large Nc Consistency Condition

doi: 10.1103/PhysRevC.61.055204
Citations: PlumX Metrics

1999TA31      Phys.Rev. C60, 065213 (1999)

Y.Tanushi, S.Saito, M.Uehara

Spin Polarizabilities of the Nucleon in a Large Nc Baryon Model with Dispersion Relations

NUCLEAR STRUCTURE 1n, 1H; calculated spin polarizabilities. Dispersion relations, comparison with heavy baryon chiral perturbation theory.

doi: 10.1103/PhysRevC.60.065213
Citations: PlumX Metrics

1998NI04      Phys.Lett. 422B, 26 (1998)

T.Nishikawa, S.Saito, Y.Kondo

Electric Polarizabilities of Neutral Baryons in the QCD Sum Rule

doi: 10.1016/S0370-2693(97)01567-0
Citations: PlumX Metrics

1998SA03      Nucl.Phys. A628, 112 (1998)

S.Saito, M.Uehara

Do the Seagull Terms Really Survive for the Electric Polarizability of the Nucleon ( Question )

doi: 10.1016/S0375-9474(97)00621-0
Citations: PlumX Metrics

1998TA12      Phys.Lett. 425B, 6 (1998)

Y.Tanushi, Y.Nakahara, S.Saito, M.Uehara

Spin-Dependent Polarizability of Nucleon with Dispersion Relation in the Skyrme Model

doi: 10.1016/S0370-2693(98)00184-1
Citations: PlumX Metrics

1997NI02      Nucl.Phys. A615, 417 (1997)

T.Nishikawa, S.Saito, Y.Kondo

QCD Sum Rules and Electromagnetic Polarizabilities of a Nucleon

doi: 10.1016/S0375-9474(96)00459-9
Citations: PlumX Metrics

1996KO37      Nucl.Phys. A609, 501 (1996)

Y.Kondo, S.Saito, Y.Tanushi, M.Uehara

Meson-Hyperon Couplings in the Bound-State Approach to the Skyrme Model

doi: 10.1016/S0375-9474(96)00285-0
Citations: PlumX Metrics

1996UM02      J.Phys.Soc.Jpn. 65, 3175 (1996)

K.Umemoto, S.Saito

Electronic Configurations of Superheavy Elements

NUCLEAR STRUCTURE Z=121-131; calculated superheavy elements ground state electronic configurations. Relativistic density functional theory.

ATOMIC PHYSICS Z=121-131; calculated superheavy elements ground state electronic configurations. Relativistic density functional theory.

doi: 10.1143/JPSJ.65.3175
Citations: PlumX Metrics

1994SA17      Phys.Lett. 325B, 20 (1994)

S.Saito, M.Uehara

Recalculation of Electromagnetic Polarizabilities of the Nucleon in the Skyrme Model

doi: 10.1016/0370-2693(94)90065-5
Citations: PlumX Metrics

1987SA07      Nucl.Phys. A463, 169c (1987)

S.Saito

Skyrmions and Nuclear Forces

NUCLEAR STRUCTURE 1H, 1n; calculated μ, rms radii. Skyrme model.

doi: 10.1016/0375-9474(87)90659-2
Citations: PlumX Metrics

1987SA37      Nucl.Phys. A472, 161 (1987)

S.Saito

Equivalent Local Potential of Microscopic αα Interaction

NUCLEAR REACTIONS 4He(α, α), E(cm)=5-300 MeV; calculated potential parameters. Equivalent local potential.

doi: 10.1016/0375-9474(87)90226-0
Citations: PlumX Metrics

1986OT03      Phys.Rev. C34, 1559 (1986)

T.Otofuji, S.Saito, M.Yasuno, T.Kurihara, H.Kanada

Nucleon-Nucleon and Nucleon-Δ-Isobar Forces in a Skyrme Model with Higher Derivative Terms

NUCLEAR STRUCTURE 1H, 1n; calculated μ, g(A), charge distributions, form factors. Nucleon-nucleon, nucleon-Δ-isobar forces. Skyrme model.

doi: 10.1103/PhysRevC.34.1559
Citations: PlumX Metrics

1985KA20      Nucl.Phys. A444, 209 (1985)

H.Kanada, T.Kaneko, S.Saito, Y.C.Tang

Microscopic Study of the d + α Scattering System with the Multi-Channel Resonating-Group Method

NUCLEAR REACTIONS 4He(d, d), E ≈ 0-30 MeV; calculated phase shifts vs E. 4He(polarized d, d), E=1.957-37.33 MeV; calculated σ(θ), vector, tensor polarizations vs θ. Multi-channel resonating group method, α+d cluster, distortion effects.

doi: 10.1016/0375-9474(85)90347-1
Citations: PlumX Metrics

1983SA12      Nucl.Phys. A403, 28 (1983)

S.Saito, T.Toyama

Inclusion of the Spin-Orbit Force in an α-Cluster Model

NUCLEAR STRUCTURE 12C; calculated level energy vs cluster distance, rms charge radius vs spin-orbit potential strength. Alpha clusters, spin-orbit force.

doi: 10.1016/0375-9474(83)90185-9
Citations: PlumX Metrics

1982SC16      Z.Phys. A306, 37 (1982)

E.W.Schmid, S.Saito, H.Fiedeldey

The Concept of a Pauli Barrier in Nucleus-Nucleus Scattering

NUCLEAR REACTIONS 4He(α, α), E=2.9 MeV; 16O(α, α), E=2.44, 6, 10.61, 21 MeV; calculated equivalent local potential. Two-cluster fish bone optical model, relative motion Pauli effects.

doi: 10.1007/BF01413405
Citations: PlumX Metrics

1981NI03      Nucl.Phys. A352, 461 (1981)

T.Nishi, I.Fujiwara, N.Imanishi, H.Moriyama, K.Otozai, R.Arakawa, S.Saito, T.Tsuneyoshi, N.Takahashi, S.Iwata, S.Hayashi, S.Shibata, H.Kudo, K.Yoshida

Cross Sections of Negative-Pion-Induced Reactions in 9Be, 12C and 19F Nuclei Between 0.4 and 1.9 GeV

NUCLEAR REACTIONS 12C, 19F(π-, π-n), 12C, 9Be(π-, πn), (π-, πX), E=0.4-1.9 GeV; measured production σ(E) for 11C, 18F, 8B, 8Li, 6He; deduced reaction mechanism, T=1/2, 3/2 isobar resonances. Activation technique.

doi: 10.1016/0375-9474(81)90423-1
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetJ1880.

1980KA15      Prog.Theor.Phys.(Kyoto) 63, 842 (1980)

H.Kanada, T.Kaneko, H.Nishioka, S.Saito

Microscopic Study of d-4He Scattering by RGM with Distortion Effect, phase shifts; deduced importance of deuteron distortion. Resonating group method, realistic effective nuclear interactions.

doi: 10.1143/PTP.63.842
Citations: PlumX Metrics

1980NI07      Prog.Theor.Phys.(Kyoto) 63, 438 (1980)

H.Nishioka, S.Saito, H.Kanada, T.Kaneko

Study of Distortion Effects in the Elastic d-4He Scattering by Orthogonality Condition Model

NUCLEAR REACTIONS 4He(d, d), E(cm)=2-16 MeV; calculated phase shifts. Variational method, deuteron distortion effect, orthogonality condition.

doi: 10.1143/PTP.63.438
Citations: PlumX Metrics

1979NI06      Prog.Theor.Phys.(Kyoto) 62, 424 (1979)

H.Nishioka, S.Saito, M.Yasuno

Structure Study of 2α+t System by the Orthogonality Condition Model

NUCLEAR STRUCTURE 11B; calculated levels, wave functions, electromagnetic properties, reduced width amplitudes. Two alpha plus triton cluster model, orthogonality condition.

doi: 10.1143/PTP.62.424
Citations: PlumX Metrics

1977SA22      Progr.Theor.Phys. 58, 190 (1977)

S.Saito, H.Nishioka, M.Yasuno

A Microscopic Study of Elastic Scattering of α Particles on 7Li Nuclei

NUCLEAR REACTIONS 7Li(α, α), E=2-18 MeV; calculated σ(E, θ).

doi: 10.1143/PTP.58.190
Citations: PlumX Metrics

1972OK02      Prog.Theor.Phys. 47, 484 (1972)

S.Okai, S.Saito, R.Tamagaki

Interaction between Nucleon-Clusters with Full Exchange Effects

doi: 10.1143/PTP.47.484
Citations: PlumX Metrics

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