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NSR database version of April 11, 2024.

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2024PA12      Phys.Rev. C 109, 025807 (2024)

P.T.H.Pang, L.Sivertsen, R.Somasundaram, T.Dietrich, S.Sen, I.Tews, M.W.Coughlin, Ch.Van Den Broeck

Probing quarkyonic matter in neutron stars with the Bayesian nuclear-physics multimessenger astrophysics framework

doi: 10.1103/PhysRevC.109.025807
Citations: PlumX Metrics


2021SE01      Nucl.Phys. A1006, 122059 (2021)

S.Sen, N.C.Warrington

Finite-temperature quarkyonic matter with an excluded volume model

doi: 10.1016/j.nuclphysa.2020.122059
Citations: PlumX Metrics


2020JE02      Phys.Rev. C 101, 035201 (2020)

K.S.Jeong, L.McLerran, S.Sen

Dynamically generated momentum space shell structure of quarkyonic matter via an excluded volume model

doi: 10.1103/PhysRevC.101.035201
Citations: PlumX Metrics


2018BE15      Phys.Rev. C 98, 015802 (2018)

P.F.Bedaque, S.Reddy, S.Sen, N.C.Warrington

Neutrino-nucleon scattering in the neutrino-sphere

doi: 10.1103/PhysRevC.98.015802
Citations: PlumX Metrics


2015BE30      Phys.Rev. C 92, 035809 (2015)

P.F.Bedaque, A.N.Nicholson, S.Sen

Massive and massless modes of the triplet phase of neutron matter

doi: 10.1103/PhysRevC.92.035809
Citations: PlumX Metrics


2015CO15      Nucl.Phys. A942, 39 (2015)

T.D.Cohen, S.Sen

Deconfinement transition at high isospin chemical potential and low temperature

doi: 10.1016/j.nuclphysa.2015.07.018
Citations: PlumX Metrics


2014BE07      Phys.Rev. C 89, 035808 (2014)

P.Bedaque, S.Sen

Neutrino emissivity from Goldstone boson decay in magnetized neutron matter

doi: 10.1103/PhysRevC.89.035808
Citations: PlumX Metrics


2013BE40      Phys.Rev. C 88, 055801 (2013)

P.F.Bedaque, S.Mahmoodifar, S.Sen

Friedel crystals and the outer crust of magnetars

doi: 10.1103/PhysRevC.88.055801
Citations: PlumX Metrics


2012GO05      Phys.Scr. 85, 035201 (2012)

R.Goswami, S.Sen

Fingerprint states in 115, 117, 119I in the framework of the particle-rotor model

NUCLEAR STRUCTURE 115,117,119I; calculated energy levels, J, π, B(M1)/B(E2) ratios, B(M1), B(E2), transition probabilities. Particle-rotor model, comparison with available data.

doi: 10.1088/0031-8949/85/03/035201
Citations: PlumX Metrics


2004DA14      Phys.Rev. C 69, 044317 (2004)

P.Datta, S.Chattopadhyay, P.Banerjee, S.Bhattacharya, B.Dasmahapatra, T.K.Ghosh, A.Goswami, S.Pal, M.S.Sarkar, S.Sen, H.C.Jain, P.K.Joshi, Amita

Observation of magnetic rotation in odd-odd 104Ag

NUCLEAR REACTIONS 76Ge(35Cl, 3nα), E=132 MeV; measured Eγ, Iγ, γγ-coin, DSA. 104Ag deduced high-spin levels, J, π, configurations, T1/2, B(M1), B(E2), magnetic rotation.

doi: 10.1103/PhysRevC.69.044317
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Data from this article have been entered in the XUNDL database. For more information, click here.


2003DA07      Phys.Rev. C 67, 014325 (2003)

P.Datta, S.Chattopadhyay, P.Banerjee, S.Bhattacharya, J.Chatterjee, B.Dasmahapatra, C.C.Dey, T.K.Ghosh, A.Goswami, S.Pal, I.Ray, M.S.Sarkar, S.Sen, H.C.Jain, P.K.Joshi, Amita

Possible coexistence of principal and tilted axis rotation in 103Ag

NUCLEAR REACTIONS 76Ge(35Cl, 4nα), E=135 MeV; measured Eγ, Iγ, γγ-coin. 103Ag deduced high-spin levels, J, π, configurations, B(M1)/B(E2), tilted axis rotation. Comparison with model predictions, neighboring isotopes.

doi: 10.1103/PhysRevC.67.014325
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Data from this article have been entered in the XUNDL database. For more information, click here.


2001ZH01      Appl.Radiat.Isot. 54, 89 (2001)

X.Zhang, Q.Li, W.Li, R.Sheng, S.Sen

Production of No-Carrier-Added 186Re via Deuteron Induced Reactions on Isotopically Enriched 186W

NUCLEAR REACTIONS 186W(d, 2n), (d, p), (d, nα), E=16 MeV; measured thick-target yields.

doi: 10.1016/S0969-8043(00)00268-2
Citations: PlumX Metrics


2000SI38      Eur.Phys.J. A 9, 197 (2000)

A.K.Singh, G.Gangopadhyay, D.Banerjee, R.Bhattacharya, R.K.Bhowmik, S.Muralithar, R.P.Singh, A.Goswami, S.Bhattacharya, B.Dasmahapatra, S.Sen

Level Structure of Odd-Odd 68Ga

NUCLEAR REACTIONS 55Mn(16O, n2p), E=55 MeV; measured Eγ, Iγ, γγ-coin. 68Ga deduced high-spin levels, J, π, configurations.

doi: 10.1007/s100500070037
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1999SI03      Phys.Rev. C59, 2440 (1999)

A.K.Singh, G.Gangopadhyay, D.Banerjee, R.Bhattacharya, R.K.Bhowmik, S.Muralithar, R.P.Singh, A.Mukherjee, U.D.Pramanik, A.Goswami, S.Chattopadhyay, S.Bhattacharya, B.Dasmahapatra, S.Sen

Level Structure of the Odd-Odd 62Cu Isotope

NUCLEAR REACTIONS 50Cr(16O, n3p), E=75 MeV; measured Eγ, Iγ, γγ-coin. 62Cu deduced high-spin levels, J, π, configurations. IBFFM calculations.

doi: 10.1103/PhysRevC.59.2440
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1998CH04      Phys.Rev. C57, R471 (1998)

S.Chattopadhyay, A.Mukherjee, U.D.Pramanik, A.Goswami, S.Bhattacharya, B.Dasmahapatra, S.Sen, H.C.Jain, P.K.Joshi

Observation of a Deformed Band in 98Rh

NUCLEAR REACTIONS 70Ge(32S, n3p), E=128 MeV; measured Eγ, Iγ, γγ-coin, DCO. 98Rh deduced levels, J, π, band structure, signature inversion. Particle-rotor model calculations.

doi: 10.1103/PhysRevC.57.R471
Citations: PlumX Metrics


1998PR04      Nucl.Phys. A632, 307 (1998)

U.D.Pramanik, A.Mukherjee, A.K.Singh, S.Chattopadhyay, G.Gangopadhyay, A.Goswami, M.S.Sarkar, R.K.Bhowmik, R.P.Singh, S.Muralithar, B.Dasmahapatra, S.Sen, S.Bhattacharya

Rotational Bands in the Doubly Odd 138Pm

NUCLEAR REACTIONS 115In(28Si, 3n2p), E=145 MeV; measured Eγ, Iγ, γγ-coin, DCO ratios. 138Pm deduced high-spin levels, J, π, B(M1)/B(E2).

doi: 10.1016/S0375-9474(97)00816-6
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1998PR05      Nucl.Phys. A637, 327 (1998)

U.D.Pramanik, A.Mukherjee, P.Basu, S.Chattopadhyay, A.Goswami, M.S.Sarkar, B.Dasmahapatra, M.L.Chatterjee, S.Sen, S.Bhattacharya

Oblate Bands in Doubly Odd 134La

NUCLEAR REACTIONS 133Cs(α, 3n), E=40 MeV; measured Eγ, Iγ(θ), γγ-coin, DCO ratios. 134La deduced high-spin levels, J, π, B(M1)/B(E2), δ.

doi: 10.1016/S0375-9474(98)00224-3
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1998SA25      J.Phys.(London) G24, 1277 (1998)

M.S.Sarkar, A.Goswami, S.Bhattacharya, B.Dasmahapatra, P.Bhattacharya, P.Basu, M.L.Chatterjee, S.Sen

Nuclear Structure of 124Xe

NUCLEAR REACTIONS 123Te(α, 3n), E=40 MeV; measured Eγ, Iγ(θ), γγ-coin. 124Xe deduced high-spin levels, J, π, δ.

NUCLEAR STRUCTURE 124Xe; calculated quasiparticle levels, splitting vs triaxial deformation. Cranked shell model.

doi: 10.1088/0954-3899/24/7/009
Citations: PlumX Metrics


1998SI04      Phys.Rev. C57, 1617 (1998)

A.K.Singh, G.Gangopadhyay, D.Banerjee, R.Bhattacharya, R.K.Bhowmik, S.Muralithar, R.P.Singh, A.Mukherjee, U.D.Pramanik, A.Goswami, S.Chattopadhyay, S.Bhattacharya, B.Dasmahapatra, S.Sen

High Spin States in 63Zn

NUCLEAR REACTIONS 50Cr(16O, n2p), E=75 MeV; measured Eγ, Iγ(θ), γγ-coin. 63Zn deduced high-spin levels, J, π, configurations. Interacting boson-fermion model calculations.

doi: 10.1103/PhysRevC.57.1617
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Data from this article have been entered in the XUNDL database. For more information, click here.


1997SA09      J.Phys.(London) G23, 169 (1997)

M.S.Sarkar, A.Goswami, S.Bhattacharya, B.Dasmahapatra, P.Bhattacharya, P.Basu, M.L.Chatterjee, S.Sen

Shape of the 123Xe Nucleus

NUCLEAR REACTIONS 122Te(α, 3n), E=40 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 123Xe deduced high-spin levels, γ-multipolarity, δ, branching ratio, B(λ). Symmetric rotor-particle model.

doi: 10.1088/0954-3899/23/2/005
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Data from this article have been entered in the XUNDL database. For more information, click here.


1997SA61      Phys.Rev. C56, 3140 (1997)

M.S.Sarkar, S.Sen

Cranked Hartree-Fock-Bogoliubov Calculations in the Xe-Ba Region

NUCLEAR STRUCTURE 120,122Te, 122,124,126,128,130,132Xe, 130,132,134,142,144,146Ba, 132,134,146,148Ce; calculated low-lying states deformation, pairing gap. Cranked Hartree-Fock-Bogoliubov calculations, several parameter sets compared.

doi: 10.1103/PhysRevC.56.3140
Citations: PlumX Metrics


1997SE10      Phys.Rev. B55, 3512 (1997)

S.Sen, J.F.Stebbins

Na-Ion Transport in Borate and Germanate Glasses and Liquids: A 23Na and 11B NMR spin-lattice-relaxation study

NUCLEAR MOMENTS 23Na, 11B; measured NMR spectra; deduced spin-lattice relaxation times in borate glasses.

doi: 10.1103/PhysRevB.55.3512
Citations: PlumX Metrics


1996MU01      Nucl.Phys. A596, 299 (1996)

A.Mukherjee, U.D.Pramanik, M.S.Sarkar, A.Goswami, P.Basu, S.Bhattacharya, S.Sen, M.L.Chatterjee, B.Dasmahapatra

7Li + 12C and 7Li + 13C Fusion Reactions at Subbarrier Energies

NUCLEAR REACTIONS 12C(7Li, X), E(cm)=2.14-6.32 MeV; 13C(7Li, X), E(cm)=1.47-7.77 MeV; measured σ(E, Eγ) for transitions in 11,12B, 14,15N, 16,17,18O, 18,19F; deduced partial, total fusion σ. Statistical model analysis. High purity Ge-detector, heavy-ion surface barrier detector, enriched targets.

doi: 10.1016/0375-9474(95)00392-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0946.


1996SI15      Nucl.Phys. A607, 350 (1996)

A.K.Singh, G.Gangopadhyay, D.Banerjee, R.Bhattacharya, R.K.Bhowmik, S.Muralithar, G.Rodrigues, R.P.Singh, A.Goswami, S.Chattopadhyay, S.Bhattacharya, B.Dasmahapatra, S.Sen

High-Spin Structure in 112Sb

NUCLEAR REACTIONS 103Rh(12C, 3n), E=75 MeV; measured Eγ, γγ-coin, DCO ratios. 112Sb deduced high-spin levels, J, π, B(M1)/B(E2) ratios.

doi: 10.1016/S0375-9474(96)00255-2
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Data from this article have been entered in the XUNDL database. For more information, click here.


1995GA02      Z.Phys. A351, 1 (1995)

G.Gangopadhyay, A.K.Singh, D.Banerjee, R.Bhattacharya, R.K.Bhowmik, S.Muralithar, G.Rodrigues, R.P.Singh, A.Goswami, S.Bhattacharya, B.Dasmahapatra, S.Sen

Rotational Band in 111Sn

NUCLEAR REACTIONS 103Rh(12C, 3np), E=75 MeV; measured γγ-coin. 111Sn deduced levels, J, π, high-spin band structure.

doi: 10.1007/BF01292775
Citations: PlumX Metrics


1995GH07      Phys.Rev. C51, 3507 (1995)

D.Ghosh, S.Sarkar, S.Sen, J.Roy

Modified Two-Sources Quantum Statistical Model and Multiplicity Fluctuation in the Finite Rapidity Region

NUCLEAR REACTIONS Ag, Br(16O, X), E=2.1 GeV/nucleon; Ag, Br(24Mg, X), E at 4.5 GeV/c; analyzed data. Modified two-source model.

doi: 10.1103/PhysRevC.51.3507
Citations: PlumX Metrics


1995GO28      Z.Phys. A352, 391 (1995)

R.Goswami, B.Sethi, M.S.Sarkar, S.Sen

Band Structures of 121,123I

NUCLEAR STRUCTURE 121,123I; calculated levels. Particle-rotor model.

doi: 10.1007/BF01299756
Citations: PlumX Metrics


1995GO29      Z.Phys. A353, 231 (1995)

A.Goswami, M.S.Sarkar, U.D.Pramanik, P.Banerjee, P.Basu, P.Bhattacharya, S.Bhattacharya, M.L.Chatterjee, S.Sen, B.Dasmahapatra

Band Structure in 104Ag

NUCLEAR REACTIONS 103Rh(α, 3n), E=40, 45 MeV; measured γγ-coin. 104Ag deduced high-spin levels, J, π, band structure. Two quasiparticle-plus-rotor model.

doi: 10.1007/BF01292323
Citations: PlumX Metrics


1994MU09      Phys.Rev. C50, 1868 (1994)

A.Mukherjee, U.D.Pramanik, M.Sarkar, S.Sen

Particle-Rotor Model Analysis of Low-Spin Identical Bands in Neighboring Odd-A and Even-Even Nuclei

NUCLEAR STRUCTURE 159Ho, 161,169,159Tm, 171,173,175,177Lu, 171,173,175,177,179,181Ta, 181,185Re, 163,165Dy, 163,165Er, 171,173Yb; calculated Coriolis attenuation factor, average transition energies in some cases. Particle-rotor model.

doi: 10.1103/PhysRevC.50.1868
Citations: PlumX Metrics


1994MU13      Nucl.Phys. A579, 125 (1994)

G.Murillo, S.Sen, S.E.Darden

A Study of the Reactions 14C(d(pol), d')14C and 14C(d(pol), p)15C at 16.0 MeV

NUCLEAR REACTIONS 14C(polarized d, d'), (polarized d, p), E=16 MeV; measured iT11(θ), σ(θ); deduced model parameters. 14,15C levels deduced β(L), spectroscopic factors. Enriched target.

doi: 10.1016/0375-9474(94)90797-8
Citations: PlumX Metrics


1994SA13      Phys.Rev. C49, 2460 (1994)

M.Saha, S.Sen

Energy Systematics of Even-Even Nuclei in the N(p)N(n) Scheme

NUCLEAR STRUCTURE 158Dy, 160Er, 170,166Yb, 172Hf, 176,182W, 80Kr, 104Ru, 128Ba, 134Ce, 232Th, 236U, 242Pu, 248Cm; calculated levels; deduced even-even nuclei energy systematics. Other nuclei discussed, N(p)N(n) scheme.

doi: 10.1103/PhysRevC.49.2460
Citations: PlumX Metrics


1994SA40      Phys.Rev. C50, 2794 (1994)

M.S.Sarkar, S.Sen

Simple Phenomenology for the Ground-State Bands of Even-Even Nuclei

NUCLEAR STRUCTURE A=70-224; analyzed level energy, energy ratio data; deduced pairing, np-interaction energy dependences role in correlation systematics. Phenomenological approach.

doi: 10.1103/PhysRevC.50.2794
Citations: PlumX Metrics


1993AY01      Nucl.Phys. A562, 1 (1993)

Z.Ayer, S.E.Darden, S.Sen, R.E.Warner

Spin Polarization Effects in the 3He(d, 3Hep)n and the 3He(d, tp)p Reactions at E(d) = 17 MeV

NUCLEAR REACTIONS 3He(polarized d, p3He), (polarized d, pt), E=17 MeV; measured σ(θp, θ(3He)), σ(θp, θt) vs E(particle), vector, tensor analyzing power vs θ. Plane wave, distorted wave impulse approximation calculations.

doi: 10.1016/0375-9474(93)90029-W
Citations: PlumX Metrics


1993SA05      Phys.Rev. C47, 884 (1993)

M.Saha, S.Sen

N(p)N(n) Scheme and the Saturation of Collectivity in the A ≈ 170 and 230 Regions

NUCLEAR STRUCTURE 156,158,160,162,164,166Dy, 160,162,164,166,168Er, 162,164,166,168,170,172,174,176Yb, 164,166,168,170,172,174,176,178Hf, 166,168,170,172,174,176,178,180W, 228,230,232Th, 230,232,234,236,238,240U, 236,238,240,242,244,246Pu, 242,244,246,248,250Cm, 244,248,250,252Cf; calculated levels, B(λ); deduced saturation effects. Other isotopes studied, NpNn scheme.

doi: 10.1103/PhysRevC.47.884
Citations: PlumX Metrics


1993SA08      Nucl.Phys. A552, 37 (1993)

M.Saha, S.Sen

Magnetic Moments of Even Rare-Earth Nuclei in the Cranked HFB Approach

NUCLEAR STRUCTURE 152,154,156Sm, 156,158,160Gd, 158,160,162,164Dy, 162,164,166,168,170Er, 168,170,172,174Yb, 184W, 188Os; calculated yrast levels, g-factors. Cranked HFB model.

doi: 10.1016/0375-9474(93)90329-V
Citations: PlumX Metrics


1992GU01      Phys.Rev. C45, 22 (1992)

E.Gulmez, D.L.Adams, S.Beedoe, M.Bleszynski, J.Bystricky, V.Ghazikhanian, G.Igo, T.Jaroszewicz, A.G.Ling, M.Nasser, M.W.McNaughton, S.Penttila, G.Glass, G.Kahrimanis, W.F.Kielhorn, K.H.McNaughton, P.J.Riley, S.Sen, D.Wolfe

Elastic Scattering of N-, L-, and S-Type Polarized 794 MeV Protons from an ND3 Target Polarized in the S-L Plane

NUCLEAR REACTIONS 2H(polarized p, p), E=794 MeV; measured spin observables. S, L-type target polarization, used all three beam polarizations. Model comparison.

doi: 10.1103/PhysRevC.45.22
Citations: PlumX Metrics


1992SA16      Phys.Rev. C46, R1587 (1992)

M.Saha, S.Sen

Low-Spin Identical Bands in the N(p)N(n) Scheme

NUCLEAR STRUCTURE 156,158,160,162,164Dy, 158,160,162,164,166,168,170Er, 160,162,164,166,168,170,172,174,176Yb, 166,168,170,172,174,176,178Hf, 174,176,178,180W, 178,180,182Os; calculated 2+ level energies, transition energies, dynamical moment of inertia; deduced identical bands occurrence origin. The NpNn scheme.

doi: 10.1103/PhysRevC.46.R1587
Citations: PlumX Metrics


1992SE02      Nucl.Phys. A537, 100 (1992)

S.Sen, S.E.Darden, Z.Ayer, N.O.Gaiser

90,92,94,96Zr(d(pol), d) and (d(pol), d') Reactions at E = 16.0 MeV and the Behavior of the Elastic Vector Analyzing Power at E = 12.0 MeV

NUCLEAR REACTIONS 90,92,94,96Zr(polarized d, d), (polarized d, d'), E=12, 16 MeV; measured iT11, σ(θ). 90,92,94,96Zr levels deduced deformation parameters β(L). Enriched targets.

doi: 10.1016/0375-9474(92)90158-G
Citations: PlumX Metrics


1990DA11      J.Phys.(London) G16, 1227 (1990)

B.Dasmahapatra, S.Bhattacharya, S.Sen, M.Saha, A.Goswami

Accurate Measurement of P(K) for the 437 keV State of 133Cs in the Decay of 133Ba (10.5y)

RADIOACTIVITY 133Ba; measured γ-, X-ray spectra. 133Cs level deduced P(K).

doi: 10.1088/0954-3899/16/8/018
Citations: PlumX Metrics


1990GO15      Phys.Rev. C42, 1367 (1990)

A.Goswami, M.Saha, S.Bhattacharya, B.Dasmahapatra, P.Basu, P.Bhattacharya, M.L.Chatterjee, P.Banerjee, S.Sen

Band Structure in 95Ru

NUCLEAR REACTIONS 94Mo(α, 3n), E=40 MeV; measured Eγ, Iγ, γγ(θ). 95Ru deduced levels J, π, δ, band structure. Rotation-particle coupling model.

doi: 10.1103/PhysRevC.42.1367
Citations: PlumX Metrics


1990SA28      Phys.Rev. C42, 1386 (1990)

M.Saha, A.Goswami, S.Bhattacharya, S.Sen

Coriolis Attenuation in the A ≈ 130-150 Region

NUCLEAR STRUCTURE A=130-150; calculated band structure; deduced Coriolis attenuation pairing interaction connection. Particle-rotor model.

doi: 10.1103/PhysRevC.42.1386
Citations: PlumX Metrics


1990SA42      Phys.Lett. 252B, 181 (1990)

M.Saha, S.Sen

Magnetic Moments in the Cranked HFB Approach

NUCLEAR STRUCTURE 158,164Dy, 170,172,174Yb, 154Sm; calculated g-factor ratios. 166,168Er; calculated levels, g-factor ratios, proton, neutron pairing gaps, deformations. Cranked HFB.

doi: 10.1016/0370-2693(90)90858-4
Citations: PlumX Metrics


1989NA28      Phys.Rev. D39, 3520 (1989)

S.Nath, G.Glass, J.C.Hiebert, J.A.Holt, R.A.Kenefick, L.C.Northcliffe, D.P.Grosnick, D.Lopiano, Y.Ohashi, T.Shima, H.M.Spinka, R.Stanek, T.S.Bhatia, J.J.Jarmer, P.J.Riley, S.Sen, J.A.Faucett, G.Kyle, R.H.Jeppesen, G.E.Tripard

Spin-Correlation Parameter A(nn)(θ(*)) for n-p Elastic Scattering at 790 MeV

NUCLEAR REACTIONS 1H(polarized n, n), E=790 MeV; measured spin-correlation parameter vs θ. Phase shift analyses.

doi: 10.1103/PhysRevD.39.3520
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13540.


1989SA09      Z.Phys. A332, 383 (1989)

M.Saha, S.Bhattacharya, A.Goswami, S.Sen

Coriolis Attenuation in the Rare Earth Region

NUCLEAR STRUCTURE 163Er, 157Dy, 165Ho, 165Tm; calculated levels. 157,159,161Dy, 161,163,165Er; calculated Nilsson orbital occupation probability. 161,163Dy, 165Ho; calculated B(E2). 165Tm, 165,163,159,157Ho; calculated stripping spectroscopic factors; deduced pairing gap parameter role.


1988BH04      J.Phys.(London) G14, 717 (1988)

S.Bhattacharya, S.Sen

The Anharmonic Vibrator Model and the Electromagnetic Properties of the Ground-State Bands of Even-Even Nuclei

NUCLEAR STRUCTURE 104,106,110Pd, 126,128Xe, 128Ba, 150,152,154Sm, 152,154,156,158,160Gd, 156,158,160,162,164Dy, 156,158,160,162,164,166,168,170Er, 160,162,164,166,168,170,172,174,176Yb, 166,168,170,172,174,176,178,180Hf, 180,182,184,186W, 182,184,186,188,190,192Os, 190,192,194,196Pt, 230,232,234Th, 232,234,236,238U, 238,240,242Pu, 244,246,248Cm; calculated levels, B(E2); deduced model parameter, B(λ) correlation. Anharmonic vibrator.

doi: 10.1088/0305-4616/14/6/011
Citations: PlumX Metrics


1988CH11      Phys.Rev. C37, 1437 (1988)

D.R.Chakrabarty, M.Thoennessen, S.Sen, P.Paul, R.Butsch, M.G.Herman

Giant Dipole Resonances in Excited Er Isotopes

NUCLEAR REACTIONS 141Pr(19F, X), E=94.1, 96.5, 111.1, 129 MeV; measured γ spectra. 160Er deduced GDR energies, widths, deformation parameters, shape evolution. Statistical model analysis.

doi: 10.1103/PhysRevC.37.1437
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1988GA14      Phys.Rev. C38, 1119 (1988)

N.O.Gaiser, S.E.Darden, R.C.Luhn, H.Paetz gen.Schieck, S.Sen

Singlet Deuteron Production in the 4He(d, pα)n Reaction at 7 MeV

NUCLEAR REACTIONS 4He(polarized d, pα), E=7 MeV; measured σ(θα, θp) vs arc length, transverse tensor analyzing power; deduced deuteron substate σ(θα, θp) vs arc length. Three-body calculation comparison.

doi: 10.1103/PhysRevC.38.1119
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0896.


1988GO01      Phys.Rev. C37, 370 (1988)

A.Goswami, S.Bhattacharya, M.Saha, S.Sen

Band Structure in 133,135Pr

NUCLEAR STRUCTURE 133,135Pr; calculated levels, γ-branching ratio.

doi: 10.1103/PhysRevC.37.370
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1988TH01      Phys.Rev. C37, 1762 (1988)

M.Thoennessen, D.R.Chakrabarty, R.Butsch, M.G.Herman, P.Paul, S.Sen

Onset of Deformation in Pb Isotopes at High Excitation Energies

NUCLEAR REACTIONS 181Ta(19F, X), E=93, 105 MeV; measured Eγ, Iγ. 200Pb deduced GDR, width, deformation parameter, shape transition. Statistical model.

doi: 10.1103/PhysRevC.37.1762
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1987CH03      Phys.Rev.Lett. 58, 1092 (1987)

D.R.Chakrabarty, M.Thoennessen, N.Alamanos, P.Paul, S.Sen

Evidence for Prolate Deformation in Highly Excited Neutron-Deficient Pb Isotopes

NUCLEAR REACTIONS W(16O, X), E=100, 140 MeV; 181Ta(19F, X), E=105, 126 MeV; measured γ-spectra. 198,199,200,201,202Pb deduced GDR energies, width, dipole strength distributions, deformation parameter. γ-ray multiplicity filter. Theoretical analyses.

doi: 10.1103/PhysRevLett.58.1092
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1987CH31      Phys.Rev. C36, 1886 (1987)

D.R.Chakrabarty, S.Sen, M.Thoennessen, N.Alamanos, P.Paul, R.Schicker, J.Stachel, J.J.Gaardhoje

Giant Resonances in Excited Sn Isotopes

NUCLEAR REACTIONS 93Nb(19F, X), E=80, 100, 160 MeV; 94Mo(16O, X), E=140 MeV; measured Eγ, Iγ, γ-multiplicity. 110,112Sn deduced GDR energies, width, strength distribution. Statistical model analyses, isovector GQR.

doi: 10.1103/PhysRevC.36.1886
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1987FR04      Phys.Rev. C35, 2097 (1987)

R.Freifelder, P.Braun-Munzinger, P.DeYoung, R.Schicker, S.Sen, J.Stachel

Symmetric Splitting for the System 32S + 238U at Energies near and below the Barrier

NUCLEAR REACTIONS 238U(32S, X), (32S, γ), E(cm)=150.7-175.4 MeV; measured fragment σ(θ), mass centroids vs scattering angle, capture σ(E). Theoretical analyses.

doi: 10.1103/PhysRevC.35.2097
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1987WA21      Nucl.Phys. A470, 339 (1987)

R.E.Warner, B.A.Vaughan, J.A.Ditusa, J.W.Rovine, R.S.Wakeland, C.P.Browne, S.E.Darden, S.Sen, A.Nadasen, A.Basak, T.R.Donoghue, T.Rinckel, K.Sale, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster

The Mechanism of the 7Li(d, 2α)n Reaction from E(d) = 3 to 15 MeV

NUCLEAR REACTIONS, MECPD 7Li(d, 2α), E=3-15 MeV; measured σ(θ1, θ2) vs energy difference; deduced reaction mechanism. 8Be deduced levels. Enriched 7LiF targets.

doi: 10.1016/0375-9474(87)90006-6
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1986ST03      Phys.Rev. C33, 1420 (1986)

J.Stachel, P.Braun-Munzinger, R.H.Freifelder, P.Paul, S.Sen, P.DeYoung, P.H.Zhang, T.C.Awes, F.E.Obenshain, F.Plasil, G.R.Young, R.Fox, R.Ronningen

Pion Production: A probe for coherence in medium-energy heavy-ion collisions

NUCLEAR REACTIONS Ni, 27Al(14N, π0X), E=35 MeV/nucleon; 27Al, Ni(16O, π0X), E=25 MeV/nucleon; measured inclusive pion production σ(θ(π), E(π)), invariant pion mass; deduced pion production, reabsorption mechanisms.

doi: 10.1103/PhysRevC.33.1420
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1985BH03      Phys.Rev. C32, 1026 (1985)

S.Bhattacharya, S.Sen, R.K.Guchhait

Band Structure in the N = 88 Isotones 149Pm, 151Eu, and 153Tb

NUCLEAR STRUCTURE 149Pm, 151Eu, 153Tb; calculated levels, spectroscopic factors, μ, quadrupole moment. Rotor-particle coupling.

doi: 10.1103/PhysRevC.32.1026
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1985DA23      Phys.Rev. C32, 1764 (1985)

S.E.Darden, G.Murillo, S.Sen

d3/2 1p-2h Strength in 15C

NUCLEAR REACTIONS 14C(polarized d, p), E=16 MeV; measured σ(θ), analyzing power vs θ. 15C deduced resonances, J, π, S, Γ.

doi: 10.1103/PhysRevC.32.1764
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1985LU08      Phys.Rev. C32, 11 (1985)

R.C.Luhn, S.Sen, N.O.Gaiser, S.E.Darden, Y.Koike

4He(d, p)n4He Reaction at Low Bombarding Energies

NUCLEAR REACTIONS 4He(polarized d, p), E=5.4-8.4 MeV; measured σ(θ, Ep), iT11(θ, Ep), T20(θ, Ep), T21(θ, Ep), T22(θ, Ep). Three-body calculation, varying tensor force contribution.

doi: 10.1103/PhysRevC.32.11
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1985SE05      Phys.Rev. C31, 787 (1985)

S.Sen, S.E.Darden, R.C.Luhn, N.O.Gaiser, G.Murillo, J.Ramirez

Evidence of a Shape Transition in Even-A Ge Isotopes

NUCLEAR REACTIONS 70,72,74,76Ge(polarized d, d), E=8, 16 MeV; 70,72,74,76Ge(polarized d, d'), E=16 MeV; 70,72,74,76Ge(polarized p, p), (polarized p, p'), E=11.5 MeV; measured σ(θ), vector analyzing power vs θ; deduced optical model parameters. Coupled-channels analysis, vibrational, rotational model macroscopic form factors.

doi: 10.1103/PhysRevC.31.787
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1984BH05      Phys.Rev. C30, 1014 (1984)

S.Bhattacharya, S.Sen

Phenomenological Anharmonic Vibrator Model for Ground State Bands of Even-Even Nuclei

NUCLEAR STRUCTURE 96Ru, 100,102Pd, 118,124Xe, 124,126Ba, 132Ce, 150,152,154Sm, 152,154Gd, 154,164Er, 176,180,182,184Os, 182,186Pt, 238U, 248Cm; calculated levels, ground-state band energies. Anharmonic Vibrator Model.

doi: 10.1103/PhysRevC.30.1014
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1984DA18      Nucl.Phys. A429, 218 (1984)

S.E.Darden, S.Sen, G.Murillo, M.Fernandez, J.Ramirez, A.Galindo, P.L.Jolivette, B.P.Hichwa

15N(p(pol), p0)15N and the Levels of 16O for E(x) = 14.8-18.6 MeV

NUCLEAR REACTIONS 15N(polarized p, p), E=2.7-7 MeV; measured σ(θ, E(p)), A(θ, E(p)). 16O deduced resonances, parameters, J, π, L, Γ, Γ(p), mixing parameters. Enriched target.

doi: 10.1016/0375-9474(84)90206-9
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1983GU06      J.Phys.(London) G9, 631 (1983)

R.K.Guchhait, S.Bhattacharya, S.Sen

Level Structure of the N = 88 Isotones 149Pm, 151Eu and 153Tb

NUCLEAR STRUCTURE 149Pm, 151Eu, 153Tb; calculated levels, S, B(E2). Pairing, anharmonicity, unified vibrational model.

doi: 10.1088/0305-4616/9/6/008
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1983MO26      Nucl.Data Sheets 39, 741 (1983)

J.N.Mo, S.Sen

Nuclear Data Sheets for A = 67

COMPILATION 67Ni, 67Cu, 67Zn, 67Ga, 67Ge, 67As; compiled, evaluated structure data.

doi: 10.1016/S0090-3752(83)80007-6
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1983SE01      J.Phys.(London) G9, 99 (1983)

S.Sen, R.Chapman, J.L.Durell, J.N.Mo, A.Simcock, P.Woods

Neutron Orbit Sizes in the Ground States of the Molybdenum Isotopes

NUCLEAR REACTIONS 92,94,96Mo(t, d), E=3.75, 4, 4.25, 4.5 MeV; measured σ(θ). 93,95,97Mo levels deduced S, neutron orbit rms radius. DWBA analysis, sub-Coulomb stripping.

doi: 10.1088/0305-4616/9/1/015
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1982SE01      Phys.Rev. C25, 1054 (1982)

S.Sen

Spin and Parity of the 6.699 MeV Level in 17F

NUCLEAR REACTIONS 16O(polarized p, p), E=6.461-6.487 MeV; measured σ(E), σ(θ), P(θ). 17F level deduced J, π, Γ, Γp.

doi: 10.1103/PhysRevC.25.1054
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1982SE03      Phys.Rev. C26, 257 (1982)

S.Sen, L.D.Knutson

Determination of the Triton D-State Parameter D2 from Sub-Coulomb (d(pol), t) Measurements

NUCLEAR REACTIONS 91Zr(polarized d, t), E=5 MeV; 147Sm(polarized d, t), E=6.5 MeV; measured T20(θ), T21(θ), T22(θ). 3H deduced D-state parameter. Enriched targets. DWBA analysis.

doi: 10.1103/PhysRevC.26.257
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1981SE12      Phys.Rev. C24, 765 (1981)

S.Sen

2.217 MeV State in 37Ar

NUCLEAR REACTIONS 36Ar(polarized d, p), E=11 MeV; measured σ(θ), iT11(θ). 37Ar level deduced J, π, S. DWBA analysis. Enriched gas target, Si-Li detectors.

doi: 10.1103/PhysRevC.24.765
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1981WO03      Nucl.Phys. A363, 322 (1981)

P.Woods, R.Chapman, J.L.Durell, J.N.Mo, S.Sen, A.I.Warwick

The 48Ti(t, d)49Ti Reaction: A comparison with magnetic electron scattering

NUCLEAR REACTIONS 48Ti(t, d), E=2.75, 3 MeV; 48Ti(t, t), E=2-3.5 MeV; 49Ti(d, d), E=4-5 MeV; measured σ(θ); deduced optical model parameters, normalization factor. 49Ti level deduced rms radius of 2p3/2 orbit. Optical model, DWBA analyses.

doi: 10.1016/0375-9474(81)90260-8
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1980MA38      Nucl.Phys. A348, 446 (1980)

Z.Y.Ma, X.Z.Wu, G.S.Zhang, Y.C.Cho, Y.S.Wang, J.H.Chiou, S.T.Sen, F.C.Yang, J.O.Rasmussen

Calculation of Muon Final-State Probabilities after Muon-Induced Fission

NUCLEAR REACTIONS, Fission 238U(μ-, F), E at rest; calculated muon-fragment binding probability. Time dependent perturbation, different fission asymmetries, fragment dynamical conditions.

doi: 10.1016/0375-9474(80)90264-X
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1979KR02      J.Phys.(London) G5, 319 (1979)

B.Krishnarajulu, S.Sen, G.K.Mehta

Light-Charged-Particle Emission in keV Neutron-Induced Fission of 239Pu

NUCLEAR REACTIONS 239Pu(n, F), E=100-1000 keV; measured σ of light, charged fragments.

doi: 10.1088/0305-4616/5/2/019
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1979WA20      Phys.Lett. 88B, 55 (1979)

A.Warwick, R.Chapman, J.L.Durell, J.N.Mo, S.Sen

Proton Orbit Sizes and the Electric Monopole Matrix Element in 90Zr

NUCLEAR REACTIONS 90Zr(t, α), E=4.5, 4.75 MeV; measured σ(Eα, θ); deduced rms radii for 2p, 1g proton orbits, E0 matrix element, proton effective charge.

doi: 10.1016/0370-2693(79)90112-6
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1978CH18      J.Phys.(London) G4, 1339 (1978)

S.N.Chaturvedi, H.R.Prabhakara, G.K.Mehta, S.Sen

Isobaric Analogue Resonances in 56Fe Corresponding to 335.5 and 340.9 keV States in 56Mn

NUCLEAR REACTIONS 55Mn(p, γ), E=1660-1710 keV; measured σ(E, Eγ, θ). 56Fe deduced IAS, J, π, δ, γ-branching. Natural target, Ge(Li) detector.

doi: 10.1088/0305-4616/4/8/015
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1978KR10      Phys.Rev. C18, 1026 (1978)

K.Krishan, S.Sen

Quasiparticle-Phonon Coupling Model Calculations for Odd-A Nb Isotopes

NUCLEAR STRUCTURE 93,95,97Nb; calculated levels, J, π, B(E2).

doi: 10.1103/PhysRevC.18.1026
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1978NA08      Nucl.Phys. A305, 1 (1978)

H.Nakamura, H.Noya, S.E.Darden, S.Sen

Breakup of 15 MeV Polarized Deuterons on 4He

NUCLEAR REACTIONS 4He(polarized d, p), E=15 MeV; measured σ(Ep, θ(p)), iT11(Ep, θ(p)). Natural target.

doi: 10.1016/0375-9474(78)90161-6
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1976DA15      Nucl.Phys. A266, 29 (1976)

S.E.Darden, G.Murillo, S.Sen

The 9Be(d, d)9Be, 9Be(d, p)10Be, 9Be(d, t)8Be and 9Be(p, d)8Be Reactions at 15 MeV

NUCLEAR REACTIONS 9Be(polarized d, d), (polarized d, d'), (polarized d, p), (polarized d, t), (polarized p, d), E=15 MeV; measured σ(θ), Ay(θ). 8,10Be levels deduced S, Γ, J-admixtures. 9Be levels deduced β2. DWBA, ICC analyses. Natural target.

doi: 10.1016/0375-9474(76)90280-3
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1976HU06      Nucl.Phys. A263, 445 (1976)

G.A.Huttlin, J.A.Aymar, J.A.Bieszk, S.Sen, A.A.Rollefson

The Vector Analyzing Power for (d, t) Reactions on Even Nickel Isotopes

NUCLEAR REACTIONS 58Ni(polarized d, t), E=16.5 MeV; 60,62Ni(polarized d, t), E=15 MeV; measured analyzing power Ay(θ). 57,59,61Ni levels deduced J. Enriched targets.

doi: 10.1016/0375-9474(76)90199-8
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1976IR02      Nucl.Phys. A265, 349 (1976)

M.Irshad, J.Asai, S.Sen, R.Pigeon, R.J.Slobodrian

Polarization Effects in (3He, p) Reactions on 3He and 7Li at 14 MeV

NUCLEAR REACTIONS 3He, 7Li(3He, p), E=14 MeV; measured σ(θ), proton polarization. Enriched 3He target.

doi: 10.1016/0375-9474(76)90359-6
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1976KR06      Phys.Rev. C13, 2055 (1976)

K.Krishan, S.K.Basu, S.Sen

Level Structure of the Odd-A Rb Isotopes

NUCLEAR STRUCTURE 83,85Rb; calculated levels, J, π, B(E2), B(M1), T1/2, γ-branching. Quasiparticle-phonon coupling.

doi: 10.1103/PhysRevC.13.2055
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1976KR12      Phys.Rev. C14, 758 (1976)

K.Krishan, S.Sen

Level Structure of 85,87Y

NUCLEAR STRUCTURE 85,87Y; calculated levels, J, π, S, B(E2), B(M1). Quasiparticle-phonon coupling.

doi: 10.1103/PhysRevC.14.758
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1976SE09      Nucl.Phys. A266, 173 (1976)

S.Sen, S.E.Darden

Elastic and Inelastic Scattering of 15 MeV Vector-Polarized Deuterons by 40Ar

NUCLEAR REACTIONS 40Ar(polarized d, d), (polarized d, d'), E=14.83 MeV; measured iT11, σ(θ). 40Ar levels deduced β(L), J, π. Natural target.

doi: 10.1016/0375-9474(76)90289-X
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1976SE11      Phys.Rev. C14, 1608 (1976)

S.K.Sen, R.P.Gupta, E.Tomchuk

Anisotropic Angular Correlation between the γ Rays and the K X Rays Following Internal Conversion in 169Tm

RADIOACTIVITY 169Tm; calculated γX-ray(θ) accompanying K conversion when perturbed by the static nuclear quadrupole moment.

doi: 10.1103/PhysRevC.14.1608
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1976SI08      J.Phys.(London) G2, 159 (1976)

B.K.Sinha, S.Sen, R.Bhattacharya

Level Structure of 147Pm

RADIOACTIVITY 147Nd [from 146Nd(n, γ)]; measured βγ(t), γγ(θ, H, t). 147Pm levels deduced T1/2, δ, g. Natural targets, plastic scintillators, NaI(Tl) detectors.

doi: 10.1088/0305-4616/2/3/008
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1976YO04      Nucl.Phys. A263, 419 (1976)

W.A.Yoh, S.E.Darden, S.Sen

A Study of the 70,72,74,76Ge(d, p)71,73,75,77Ge Reactions Using Polarized Deuterons

NUCLEAR REACTIONS 70,72,74,76Ge(polarized d, p), E=12 MeV; measured polarization parameter Ay(Ed, Ep, θ), σ(Ed, Ep, θ). 71,73,75,77Ge levels deduced L, J, π, S. Enriched target.

doi: 10.1016/0375-9474(76)90198-6
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1975AL20      Nucl.Phys. A248, 214 (1975)

R.Almanza, G.Murillo, S.E.Darden, S.Sen

The Reactions 18O(p, p)18O and 18O(p, p')18O*(1.98 Mev) for E = 3.8-6.1 MeV

NUCLEAR REACTIONS 18O(p, p), (p, p'), (p, α), (polarized p, p), (polarized p, p'), (polarized p, α), E=3.8-6.1 MeV; measured σ(E, θ), σ(E, Ep', θ), σ(E, Eα, θ), P(θ). 19F deduced resonances, J, π, Γ, p-width, T.

doi: 10.1016/0375-9474(75)90163-3
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1975SE02      J.Phys.(London) G1, 286 (1975)

S.Sen

Quasiparticle-Phonon Coupling in the Odd-A Te Isotopes

NUCLEAR STRUCTURE 123,125,127Te; calculated levels, quadrupole moment, μ, B(λ).

doi: 10.1088/0305-4616/1/3/005
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1975SE13      Nucl.Phys. A250, 45 (1975)

S.Sen, S.E.Darden, W.A.Yoh, E.D.Berners

Vector Analyzing Power and Cross Section for the Reactions 40Ar(d, p)41Ar and 40Ar(d, t)39Ar

NUCLEAR REACTIONS 40Ar(polarized d, p), (polarized d, t), E=14.83 MeV; measured polarization parameters iT11(Ed, Ep, θ), iT11(Ed, Et, θ), σ(Ed, Ep, θ), σ(Ed, Et, θ). 41Ar, 39Ar levels deduced L, J, π, S. Natural target.

doi: 10.1016/0375-9474(75)90199-2
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1975SI01      J.Phys.(London) G1, 92 (1975)

B.K.Sinha, S.Sen, R.Bhattacharyya

Lifetime of the 410 keV Level of 147Pm

RADIOACTIVITY 147Nd; measured Eγ, γ(t). 147Pm level deduced T1/2.

doi: 10.1088/0305-4616/1/1/011
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1974BA17      Nucl.Phys. A220, 580 (1974)

S.K.Basu, S.Sen

Single-Hole-Core Coupling in the N = 50 Region

NUCLEAR STRUCTURE 85Kr, 85Sr, 87Sr, 89Zr; calculated levels, J, π, S, μ, quadrupole moment, T1/2, B(E2), B(M1).

doi: 10.1016/0375-9474(74)90136-5
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1974HU04      Nucl.Phys. A227, 389 (1974)

G.A.Huttlin, S.Sen, W.A.Yoh, A.A.Rollefson

Spin Assignments in 63Ni Through 62Ni(d, p)63Ni

NUCLEAR REACTIONS 62Ni(polarized d, p), E=10 MeV; measured analyzing power Aγ(θ). 63Ni levels deduced J, π. Enriched target.

doi: 10.1016/0375-9474(74)90766-0
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1974SE01      Nucl.Phys. A219, 429 (1974)

S.Sen, S.E.Darden, H.R.Hiddleston, W.A.Yoh

Study of the (d, p) Reaction to Bound and Unbound States of 19O

NUCLEAR REACTIONS 18O(polarized d, p), E=14.8 MeV; measured polarization parameters iT11(Ed, Ep, θ), σ(Ed, Ep, θ). 19O deduced J, π, S, level-width. Enriched target.

doi: 10.1016/0375-9474(74)90110-9
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1974SE07      Phys.Rev. C10, 1050 (1974)

S.Sen, W.A.Yoh, M.T.McEllistrem

Vector Analyzing Power and Cross Section for the Reaction 36Ar(d, p)37Ar

NUCLEAR REACTIONS 36Ar(polarized d, d), (polarized d, p), E=10.02 MeV; measured σ(θ), σ(Ep, θ), iT11(θ); deduced optical parameters. 37Ar deduced levels, J, π, S. DWBA analysis. Enriched target.

doi: 10.1103/PhysRevC.10.1050
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1973DA17      Nucl.Phys. A208, 77 (1973)

S.E.Darden, S.Sen, H.R.Hiddleston, J.A.Aymar, W.A.Yoh

Study of (d, p) Reactions to Unbound States of 13C and 17O

NUCLEAR REACTIONS 12C, 16O(polarized d, p), E=9.3, 13.3, 15.0 MeV; measured polarization parameters iT11(Ed, Ep, θ), cross sections σ(Ed, Ep, θ). 13C, 17O deduced S, resonance widths. Natural targets.

doi: 10.1016/0375-9474(73)90736-7
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1973SE11      J.Phys.(London) A6, L45 (1973)

S.Sen

Low-Lying Positive-Parity States of 151Eu

NUCLEAR STRUCTURE 151Eu; calculated levels, J, π, B(E2).

doi: 10.1088/0305-4470/6/4/005
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1972BR52      Phys.Rev. C6, 1837 (1972)

C.E.Brient, P.J.Riley, H.Seitz, S.Sen

107Ag(d, p)108Ag and 109Ag(d, p)110Ag Reactions

NUCLEAR REACTIONS 107,109Ag(d, p), E=10 MeV; measured σ(Ep, θ). 108,110Ag deduced levels, J, π, L, S.

doi: 10.1103/PhysRevC.6.1837
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1972HO15      Phys.Rev. C5, 1641 (1972)

C.L.Hollas, H.R.Hiddleston, V.D.Mistry, S.Sen, P.J.Riley

Study of Core Coupling in 87Rb Through Isobaric-Analog Resonances. I

NUCLEAR REACTIONS 86Kr(p, p), E=4.76-10.10 MeV; measured σ(E). 87Rb deduced isobaric analog resonances, level-width, S, L.

doi: 10.1103/PhysRevC.5.1641
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1972HO16      Phys.Rev. C5, 1646 (1972)

C.L.Hollas, H.R.Hiddleston, V.D.Mistry, S.Sen, P.J.Riley

Study of Core Coupling in 87Rb Through Isobaric-Analog Resonances. II

NUCLEAR REACTIONS 86Kr(p, p'), E=4.76-10.10 MeV; measured σ(E;Ep', θ). 87Rb deduced isobaric analog resonances, level-width. 86Kr deduced levels, isobaric analogs.

doi: 10.1103/PhysRevC.5.1646
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1972SE04      Phys.Rev. C5, 1278 (1972)

S.Sen, C.L.Hollas, C.W.Bjork, P.J.Riley

Reaction 38Ar(d, p)39Ar

NUCLEAR REACTIONS 38Ar(d, p), E=10.064 MeV; measured σ(Ep, θ). 39Ar deduced levels, L(n), J, π, S.

doi: 10.1103/PhysRevC.5.1278
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1972SE08      Phys.Rev.Lett. 28, 1295 (1972)

S.K.Sen, D.L.Salie, E.Tomchuk

Direct Detection of the K-Shell Perturbation Caused by the Static Nuclear Quadrupole Moment

RADIOACTIVITY 169Yb; measured Xce(θ), Xγ(θ); deduced K-shell perturbation by nuclear quadrupole moment.

doi: 10.1103/PhysRevLett.28.1295
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1972SE11      Nucl.Phys. A191, 29 (1972)

S.Sen

Structure of the Low-Lying States of the Odd-A In Isotopes

NUCLEAR STRUCTURE 113,115,117In; calculated levels, B(M1), B(E2), T1/2, S, μ, quadrupole moment. Semi-microscopic model.

doi: 10.1016/0375-9474(72)90592-1
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1972SE14      Can.J.Phys. 50, 2348 (1972)

S.K.Sen, D.L.Salie, E.Tomchuk

The Decay of 169Yb

RADIOACTIVITY 169Yb; measured Eγ, Iγ, E(X-ray), I(X-ray). 169Tm deduced levels, ICC, J, π.

doi: 10.1139/p72-309
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1972SE17      Phys.Rev. C6, 2201 (1972)

S.Sen, P.J.Riley, T.Udagawa

136Xe(p, p')136Xe and 136Xe(p, d)135Xe Reactions

NUCLEAR REACTIONS 136Xe(p, p'), (p, d), E=13.982 MeV; measured σ(θ); deduced optical model parameters. 136Xe deduced levels, J, π, S, β. 135Xe deduced levels, J, π.

doi: 10.1103/PhysRevC.6.2201
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Note: The following list of authors and aliases matches the search parameter S.Sen: , S.K.SEN, S.T.SEN