Nuclear Science References (NSR)

NUCLEAR REACTIONS ¹H(p-bar, X), E(cm)=2222-2239 MeV; measured π⁰π⁰, π⁰η, ηη production σ, angular distrubutions; deduced tensor glueball production upper limit.

doi: 10.1016/S0375-9474(99)00664-8
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2000SE11 Nucl.Phys. A675, 25c (2000)

K.K.Seth

Present Status of Glueball Searches

doi: 10.1016/S0375-9474(00)00211-6
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1999AM07 Phys.Rev. D60, 032002 (1999)

M.Ambrogiani, S.Bagnasco, W.Baldini, D.Bettoni, G.Borreani, A.Buzzo, R.Calabrese, R.Cester, P.Dalpiaz, X.Fan, G.Garzoglio, K.E.Gollwitzer, A.Hahn, S.Jin, J.Kasper, G.Lasio, M.Lo Vetere, E.Luppi, P.Maas, M.Macri, M.Mandelkern, F.Marchetto, M.Marinelli, W.Marsh, M.Martini, E.Menichetti, R.Mussa, M.M.Obertino, M.Pallavicini, N.Pastrone, C.Patrignani, T.K.Pedlar, J.Peoples, Jr., S.Pordes, E.Robutti, J.Rosen, P.Rumerio, A.Santroni, M.Savrie, J.Schultz, K.K.Seth, G.Stancari, M.Stancari, J.Streets, A.Tomaradze, S.Werkema, G.Zioulas

Measurements of the Magnetic Form of the Proton in the Timelike Region at Large Momentum Transfer

NUCLEAR REACTIONS ¹H(p-bar, ee⁺), E(cm)=2.9-4.3 GeV; measured σ, invariant mass spectra. ¹H deduced magnetic form factor. Non-magnetic spectrometer.

doi: 10.1103/PhysRevD.60.032002
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1999SE13 Nucl.Phys. A655, 390c (1999)

K.K.Seth

Prospects for Antiproton Physics in the USA

doi: 10.1016/S0375-9474(99)00229-8
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1998GO24 Phys.Rev.Lett. 81, 4325 (1998)

M.G.Gornov, Yu.Gurov, S.Lapushkin, P.Morokhov, V.Pechkurov, T.K.Pedlar, K.K.Seth, J.Wise, D.Zhao

Excited States of ¹¹Li

NUCLEAR REACTIONS ¹⁴C(π^-, pd), E at rest; measured proton, deuteron spectra, coincidences; deduced missing mass spectra. ¹¹Li deduced excited states, continuum components.

doi: 10.1103/PhysRevLett.81.4325
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1998SE03 Nucl.Phys. A629, 358c (1998)

K.K.Seth

Charmonium - In and Out of the Nucleus

doi: 10.1016/S0375-9474(97)00711-2
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1997WI23 Phys.Rev. C56, 3152 (1997)

C.F.Williamson, T.C.Yates, W.M.Schmitt, M.Osborn, M.Deady, P.D.Zimmerman, C.C.Blatchley, K.K.Seth, M.Sarmiento, B.Parker, Y.Jin, L.E.Wright, D.S.Onley

Quasielastic Electron Scattering from ⁴⁰Ca

NUCLEAR REACTIONS ⁴⁰Ca(e, e'), E=130-841 MeV; measured σ(θ, E); deduced transverse, longitudinal response functions, agreement with Fermi gas predictions.

doi: 10.1103/PhysRevC.56.3152
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1996AD10 Nucl.Instrum.Methods Phys.Res. A368, 617 (1996)

T.Adams, J.M.Bishop, R.Cady, N.M.Cason, J.Gress, C.Kopp, J.M.LoSecco, J.J.Manak, A.H.Sanjari, W.D.Shepard, D.L.Stienike, S.A.Taegar, D.R.Thompson, S.U.Chung, R.W.Hackenburg, C.Olchanski, D.P.Weygand, H.J.Willutzki, S.Denisov, A.Dushkin, V.Kochetkov, I.Shein, A.Soldatov, B.B.Brabson, R.R.Crittenden, A.R.Dzierba, J.Gunter, R.Lindenbusch, D.R.Rust, E.Scott, P.T.Smith, T.Sulanke, S.Teige, Z.Bar-Yam, J.P.Dowd, P.Eugenio, M.Hayek, W.Kern, E.King, N.Shenhav, V.A.Bodyagin, A.M.Gribushin, M.A.Kostin, V.L.Korotkikh, A.I.Ostrovidov, A.S.Proskuryakov, L.I.Sarycheva, N.B.Sinev, I.N.Vardanyan, A.A.Yershov, D.S.Brown, T.K.Pedlar, K.K.Seth, J.Wise, D.Zhao, G.S.Adams, J.Napolitano, M.Nozar, J.A.Smith, M.Witkowski

Design and Performance of a Cesium Iodide Detector

doi: 10.1016/0168-9002(95)00668-0
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1995SE03 Phys.Rev.Lett. 74, 642 (1995); Erratum Phys.Rev.Lett. 74, 3306 (1995)

K.K.Seth, R.Soundranayagam, A.Saha, C.W.de Jager, H.de Vries, B.A.Brown, B.H.Wildenthal

Absence of M3 Quenching in ²⁶Mg

NUCLEAR REACTIONS ²⁶Mg(e, e'), E not given; measured σ(θ). ²⁶Mg level deduced B(λ).

doi: 10.1103/PhysRevLett.74.642
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1994BU09 Phys.Rev. C49, 2226 (1994)

G.Burleson, G.Blanpied, W.Cottingame, G.Daw, B.Park, K.K.Seth, D.Barlow, S.Iversen, M.Kaletka, H.Nann, A.Saha, D.Smith, R.P.Redwine, W.Burger, M.Farkhondeh, B.Saghai, R.Anderson

Negative Pion-Nucleus Elastic Scattering at 20 and 40 MeV

NUCLEAR REACTIONS ¹²C, ¹⁶O, ⁴⁸Ca, ⁹⁰Zr, ²⁰⁸Pb(π^-, π^-), E=20 MeV; ¹²C, ^16,18O, ⁴⁰Ca, ⁵⁸Ni, ²⁰⁸Pb(π^-, π^-), E=40 MeV; measured σ(θ); deduced optical model parameters. Range telescope.

doi: 10.1103/PhysRevC.49.2226
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1993YA09 Phys.Lett. 312B, 382 (1993)

T.C.Yates, C.F.Williamson, W.M.Schmitt, M.Osborn, M.Deady, P.D.Zimmerman, C.C.Blatchley, K.K.Seth, M.Sarmiento, B.Parker, Y.Jin, L.E.Wright, D.S.Onley

Longitudinal Response Functions for ⁴⁰Ca from Quasi-Elastic Electron Scattering

NUCLEAR REACTIONS ⁴⁰Ca(e, e'X), E=130-480 MeV; measured σ(θ) vs energy transfer; deduced longitudinal response functions.

doi: 10.1016/0370-2693(93)90971-J
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1991SE06 Phys.Rev.Lett. 66, 2448 (1991)

K.K.Seth, B.Parker

Evidence for Dineutrons in Extremely Neutron-Rich Nuclei

NUCLEAR REACTIONS ⁶Li(π^-, π⁺), E=220 MeV; ⁶Li, ⁹Be(π^-, p), E=125 MeV; analyzed data; deduced dineutron evidence.

doi: 10.1103/PhysRevLett.66.2448
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1990PA25 Phys.Lett. 251B, 483 (1990)

B.Parker, K.K.Seth, R.Soundranayagam

Search for Superheavy Hydrogen-6

NUCLEAR REACTIONS ⁶Li(π^-, π⁺X), E=220 MeV; measured missing mass spectra; deduced no evidence for ⁶H.

doi: 10.1016/0370-2693(90)90783-3
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1990SE04 Phys.Rev. C41, 2800 (1990)

K.K.Seth, D.Barlow, S.Iversen, M.Kaletka, H.Nann, D.Smith, M.Artuso, G.Burleson, G.Blanpied, G.Daw, W.J.Burger, R.P.Redwine, B.Saghai, R.Anderson

Negative Pion-Nucleus Elastic Scattering at 30 and 50 MeV

NUCLEAR REACTIONS ^12,13C, ¹⁶O, ^40,48Ca, ⁹⁰Zr, ²⁰⁸Pb(π^-, π^-), E=30, 50 MeV; ¹²C, ⁴⁸Ca, ²⁰⁸Pb(π⁺, π⁺), E=50 MeV; measured σ(θ); deduced optical model fits. ¹³C, ⁴⁸Ca, ⁹⁰Zr, ²⁰⁸Pb enriched targets, range spectrometer. DWBA analysis.

doi: 10.1103/PhysRevC.41.2800
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1989PA20 Phys.Rev.Lett. 63, 1570 (1989)

B.Parker, K.K.Seth, C.M.Ginsburg, B.O'Reilly, M.Sarmiento, R.Soundranayagam, S.Trokenheim

Search for a T = 2 Dibaryon

NUCLEAR REACTIONS ²H(π^-, π⁺), E=291.2 MeV; measured missing mass spectra following breakup; deduced no T=2 dibaryon resonance.

doi: 10.1103/PhysRevLett.63.1570
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1988BA14 Phys.Rev. C37, 1977 (1988)

D.B.Barlow, A.Saha, K.K.Seth, T.S.Bhatia, G.Glass, J.C.Hiebert, R.A.Kenefick, S.Nath, L.C.Northcliffe, W.B.Tippens, J.J.Jarmer, J.E.Simmons, R.H.Jeppesen, G.E.Tripard

Measurement of the Spin Correlation Parameters A(ll) and A(sl) for the Reaction pp → dπ⁺ in the Energy Region 500-800 MeV

NUCLEAR REACTIONS ¹H(polarized p, π⁺), E=500-800 MeV; measured spin correlation parameters; deduced no dibaryon resonances. Coupled-channels, partial wave analyses. Polarized target.

doi: 10.1103/PhysRevC.37.1977
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1988SE13 Nucl.Phys. A478, 591 (1988)

K.K.Seth

Anomalous behavior of low-energy analog double charge exchange

NUCLEAR REACTIONS ¹⁸O(π⁺, π^-), E=164 MeV; ¹⁴C, ¹⁸O, ²⁶Mg, ⁴²Ca(π⁺, π^-), E=50 MeV; ¹⁴C, ¹⁸O, ²⁶Mg, ⁴²Ca(π⁺, π^-), E<320 MeV; analyzed available data; deduced σ(θ), A-dependence at resonance energies.

doi: 10.1016/0375-9474(88)90898-6
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1988SO09 Phys.Lett. 212B, 13 (1988)

R.Soundranayagam, A.Saha, K.K.Seth, C.W.de Jager, H.de Vries, H.Blok, G.van der Steenhoven

Ground State Charge Distribution of ²⁶Mg

NUCLEAR REACTIONS ²⁶Mg(e, e), E=85-360 MeV; measured σ(θ); deduced form factors. ²⁶Mg deduced charge density, rms charge radius.

doi: 10.1016/0370-2693(88)91227-0
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1987KA45 Phys.Lett. 199B, 336 (1987)

M.Kaletka, K.K.Seth, A.Saha, D.Barlow, D.Kielczewska

Correlation Effects in Pion Double Charge Exchange in the f_7/2 Shell

NUCLEAR REACTIONS ⁴⁸Ca, ⁴⁸Ti(π⁺, π^-), E=130, 180, 235, 292 MeV; measured σ(E(π)). ⁴⁸Ti, ⁴⁸Cr deduced analog, nonanalog transition σ ratios.

doi: 10.1016/0370-2693(87)90929-4
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1987SE05 Phys.Rev.Lett. 58, 1930 (1987)

K.K.Seth, M.Artuso, D.Barlow, S.Iversen, M.Kaletka, H.Nann, B.Parker, R.Soundranayagam

Exotic Nucleus Helium-9 and Its Excited States

NUCLEAR REACTIONS ⁹Be(π^-, π⁺), E at 180 MeV/c; measured missing-mass spectrum. ⁹He deduced mass excess, neutron binding energy, levels. Magnetic spectrometer, tof.

doi: 10.1103/PhysRevLett.58.1930
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1986SE04 Phys.Lett. 173B, 397 (1986)

K.K.Seth, S.Iversen, M.Kaletka, D.Barlow, A.Saha, R.Soundranayagam

Mass of Proton-Rich ⁵⁸Zn by Pion Double Charge Exchange

NUCLEAR REACTIONS ⁵⁸Ni(π⁺, π^-), E=292 MeV; measured missing mass spectra. ⁵⁸Zn deduced mass excess.

doi: 10.1016/0370-2693(86)90402-8
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1985GL02 Phys.Rev. C31, 288 (1985)

G.Glass, T.S.Bhatia, J.C.Hiebert, R.A.Kenefick, S.Nath, L.C.Northcliffe, W.B.Tippens, D.B.Barlow, A.Saha, K.K.Seth, J.G.J.Boissevain, J.J.Jarmer, J.E.Simmons, R.H.Jeppesen, G.E.Tripard

Measurements of Spin-Correlation Parameters A(LL) and A(SL) for p(pol)p(pol) → πd between 500 and 800 MeV

NUCLEAR REACTIONS ¹H(polarized p, π), E=500, 650, 800 MeV; measured spin correlation parameters vs θ.

doi: 10.1103/PhysRevC.31.288
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1985SE10 Phys.Lett. 155B, 339 (1985)

K.K.Seth, M.Kaletka, D.Barlow, D.Kielczewska, A.Saha, L.Casey, D.Godman, R.Seth, J.Stuart

Observation of Double Analog States in ⁸⁸Zr and ⁹⁰Mo and the Neutron Excess and Mass Systematics of Pion Double Charge Exchange

NUCLEAR REACTIONS ⁸⁸Sr, ⁹⁰Zr(π⁺, π^-), E=180, 292 MeV; measured σ(θ=5°), missing mass spectra; deduced neutron excess, mass systematics of reaction mechanism. ⁸⁸Zr, ⁹⁰Mo deduced double IAS excitation, energy, T.

doi: 10.1016/0370-2693(85)91583-7
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1985SE14 Phys.Lett. 158B, 23 (1985)

K.K.Seth, D.Barlow, A.Saha, R.Soundranayagam, S.Iversen, M.Kaletka, M.Bosko, D.Smith, G.W.Hoffmann, M.L.Barlett, R.Fergerson, J.McGill, E.C.Milner

Polarized Proton Inelastic Scattering from ⁴⁰Ca and ⁴⁸Ca at 500 MeV

NUCLEAR REACTIONS ^40,48Ca(polarized p, p'), E=500 MeV; measured σ(θ), analyzing power vs θ. ⁴⁰Ca(polarized p, p), E=500 MeV; analyzed spin rotation parameter vs θ; deduced optical potential parameters. ^40,48Ca deduced mass deformation parameters, lengths.

doi: 10.1016/0370-2693(85)90731-2
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1984BL19 Phys.Lett. 149B, 441 (1984)

H.Blok, H.P.Blok, J.F.A.van Hienen, G.van der Steenhoven, C.W.de Jager, H.de Vries, A.Saha, K.K.Seth

Contribution of 2(h-bar x Omega) Transition to the Excitation of 0⁺ States in ⁵⁸Ni and ²⁶Mg in Inelastic Electron Scattering

NUCLEAR REACTIONS ⁵⁸Ni, ²⁶Mg(e, e'), E not given; measured monopole form factors. ²⁶Mg, ⁵⁸Ni levels deduced monopole matrix element, EWSR, normalization factors. Shell model.

doi: 10.1016/0370-2693(84)90362-9
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1984FO18 Nucl.Phys. A426, 542 (1984)

G.Fournier, A.Gerard, J.Miller, J.Picard, B.Saghai, P.Vernin, P.Y.Bertin, B.Coupat, E.W.A.Lingeman, K.K.Seth

Differential Cross Section for Elastic π± Helium Isotopes Scattering from 25 to 65 MeV

NUCLEAR REACTIONS ³He(π⁺, π⁺), (π^-, π^-), E=30, 45, 65 MeV; ⁴He(π⁺, π⁺), (π^-, π^-), E=25, 51 MeV; measured absolute σ(θ), charge asymmetry parameter vs θ. Liquid targets, high precision.

doi: 10.1016/0375-9474(84)90163-5
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1984HA29 Phys.Rev.Lett. 53, 152 (1984)

P.Harihar, K.K.Seth, D.Barlow, S.Iversen, M.Kaletka, H.Nann, A.Saha, C.F.Williamson, J.W.Wong, M.Deady, W.J.Gerace

Direct Verification of the Coexistence Model for ⁴⁰Ca: Electroexcitation of the second monopole state

NUCLEAR REACTIONS ⁴⁰Ca(e, e'), E=81.6-380 MeV; measured σ(E(e')), form factors. ⁴⁰Ca level deduced electroexcitation transition density.

doi: 10.1103/PhysRevLett.53.152
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1984SA11 Phys.Rev.Lett. 52, 1876 (1984)

A.Saha, K.K.Seth, M.Artuso, B.Harris, R.Seth, H.Nann, W.W.Jacobs

Determination of the Relative Sign of Neutron and Proton Transition Matrix Elements for the ³⁴S(0 → 2₂⁺) Transition

NUCLEAR REACTIONS ³⁴S(α, α), (α, α'), E=120 MeV; measured σ(Eα), σ(θ). ³⁴S levels deduced neutron, proton matrix element relative sign. DWBA, CCBA analyses.

doi: 10.1103/PhysRevLett.52.1876
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1984SE04 Phys.Rev.Lett. 52, 894 (1984)

K.K.Seth, M.Kaletka, S.Iversen, A.Saha, D.Barlow, D.Smith, L.C.Liu

Core-Excitation Effects in Pion Double Charge Exchange

NUCLEAR REACTIONS ⁴²Ca(π⁺, π^-), E ≈ 125-300 MeV; measured σ(θ); deduced pion-nucleus potential characteristics. ⁴²Ca deduced ground state core excitation components. Optical model, first-, second-order one-body density terms.

doi: 10.1103/PhysRevLett.52.894
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1983BA02 Nucl.Phys. A392, 217 (1983)

B.Balestri, G.Fournier, A.Gerard, J.Miller, J.Morgenstern, J.Picard, B.Saghai, P.Vernin, P.Y.Bertin, B.Coupat, E.W.A.Lingeman, K.K.Seth

Diffferential Cross Sections for Elastic π±d Scattering at 65 MeV

NUCLEAR REACTIONS ²H(π⁺, π⁺), (π^-, π^-), E=65 MeV; measured σ(θ) absolute. High precision, LD₂ target.

doi: 10.1016/0375-9474(83)90123-9
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1983SA01 Phys.Rev. C27, 405 (1983)

A.Saha, K.K.Seth, H.Nann

Systematics of Ground State (p, t) Transitions in Calcium Isotopes

NUCLEAR REACTIONS ^{48,44,43,42,40}Ca(p, t), E=40 MeV; measured absolute σ(θ), σ(Et). ^{46,42,41,40,38}Ca level deduced L=0 transition probability. DWBA analysis, pure f7/2 pickup.

doi: 10.1103/PhysRevC.27.405
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1983SA19 Phys.Rev.Lett. 51, 759 (1983)

A.Saha, K.K.Seth, D.Kielczewska, S.Iversen, M.Kaletka, D.Barlow, D.Smith

Energy Variation of the Analyzing Power in the Reaction p(pol) + p → d + π⁺

NUCLEAR REACTIONS ¹H(polarized p, π⁺), E ≈ 550, 600, 650, 700, 800 MeV; measured analyzing power vs θ; deduced isobar dominance in pion production. Phenomenological analysis, other data input, Legendre polynomial fits.

doi: 10.1103/PhysRevLett.51.759
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1983SA29 Phys.Lett. 130B, 152 (1983)

A.Saha, K.K.Seth, B.A.Brown, H.Nann

The (p, t) Reaction to ⁴⁸Ti and ⁴⁹V in the (f_7/2)(n) Model

NUCLEAR REACTIONS ⁵⁰Ti, ⁵¹V(p, t), E=40.2 MeV; measured σ(θ); deduced angle-integrated σ. ⁴⁸Ti, ⁴⁹V deduced levels, J, π, S. DWBA analysis, (f_7/2)(n) model.

doi: 10.1016/0370-2693(83)91031-6
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1983SA31 Phys.Lett. 132B, 51 (1983)

A.Saha, K.K.Seth, L.Casey, D.Godman, D.Kielczewska, R.Seth, J.Stuart, O.Scholten

Isovector Properties of Collective States and the IBA-2 Model

NUCLEAR REACTIONS ^{104,106,108,110}Pd(π⁺, π⁺'), (π^-, π^-'), E=180 MeV; measured σ(E(π)), σ(θ). ^{104,106,108,110}Pd levels deduced neutron, proton matrix elements, ratios. Interacting boson model.

doi: 10.1016/0370-2693(83)90220-4
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1983SE13 Phys.Lett. 126B, 164 (1983)

K.K.Seth, A.Saha, D.Kielczewska, S.Iversen, M.Kaletka, D.Barlow, B.Hoistad

Analyzing Power for the p(pol) + p → d + π⁺ Reaction at 0.8 GeV and Effects of Dibaryon Admixtures

NUCLEAR REACTIONS ¹H(polarized p, π⁺), E=0.8 GeV; measured σ(θ(π)), analyzing power vs θ; deduced no dibaryon admixtures. Legendre polynomial analysis.

doi: 10.1016/0370-2693(83)90583-X
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1982BA16 Czech.J.Phys. B32, 255 (1982)

B.Balestri, P.Y.Bertin, B.Coupat, G.Fournier, A.Gerard, E.W.A.Lingeman, J.Miller, J.Picard, B.Saghai, K.K.Seth, P.Vernin

Elastic π± - d and π± - ⁴He Scattering below 70 MeV

NUCLEAR REACTIONS ²H(π⁺, π⁺), (π^-, π^-), E=65 MeV; ⁴He(π⁺, π⁺), (π^-, π^-), E=51 MeV; measured σ(θ). Relativistic three-body, optical model calculations, pion absorption.

doi: 10.1007/BF01602062
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1982SA15 Phys.Lett. 114B, 419 (1982)

A.Saha, K.K.Seth, D.Barlow, H.Nann, W.W.Jacobs

Measurement of the Relative Sign of Neutron and Proton Transition Matrix Elements of the 2⁺ States in ³⁰Si

NUCLEAR REACTIONS ³⁰Si(α, α'), E=120 MeV; measured σ(θ). ³⁰Si level deduced neutron, proton matrix element relative sign. DWBA analysis.

doi: 10.1016/0370-2693(82)90083-1
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1981HO26 Phys.Rev.Lett. 47, 1436 (1981)

G.W.Hoffmann, L.Ray, M.L.Barlett, R.Fergerson, J.McGill, E.C.Milner, K.K.Seth, D.Barlow, M.Bosko, S.Iversen, M.Kaletka, A.Saha, D.Smith

Elastic Scattering of 500-MeV Polarized Protons from ^40,48Ca, ⁹⁰Zr, and ²⁰⁸Pb, and Breakdown of the Impulse Approximation at Small Momentum Transfer

NUCLEAR REACTIONS ^40,48Ca, ⁹⁰Zr, ²⁰⁸Pb(polarized p, p), E=500 MeV; measured σ(θ), A(θ); deduced impulse approximation breakdown. Second-order. Kerman-McManus-Thaler optical potential.

doi: 10.1103/PhysRevLett.47.1436
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1980KY01 Phys.Lett. 91B, 353 (1980)

G.S.Kyle, N.M.Hintz, M.S.Oothoudt, M.Kaletka, P.M.Lang, H.Nann, K.K.Seth, D.K.McDaniels, P.M.Varghese, T.Kozlowski, D.G.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, N.Tanaka, H.A.Thiessen, G.S.Blanpied, G.W.Hoffmann, R.P.Liljestrand, J.C.Fong, G.Igo, R.J.Ridge, C.A.Whitten, Jr.

Elastic and Inelastic Scattering of 800 MeV Protons by ⁵⁸Ni

NUCLEAR REACTIONS ⁵⁸Ni(p, p), (p, p'), E=800 MeV; measured σ(θ). ⁵⁸Ni levels deduced deformation lengths. DWBA analysis.

doi: 10.1016/0370-2693(80)90994-6
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1980NA12 Phys.Lett. B96, 261 (1980)

H.Nann, K.K.Seth, S.G.Iversen, M.O.Kaletka, D.B.Barlow, D.Smith

Identification and Measurement of the Mass of ²⁶Ne(g.s.) by the ²⁶Mg(π^-, π⁺)²⁶Ne Reaction

NUCLEAR REACTIONS ²⁶Mg(π^-, π⁺), E=162.4 MeV; measured σ(E(π⁺)), Q. ²⁶Ne deduced level, mass excess.

doi: 10.1016/0370-2693(80)90762-5
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1979IG01 Phys.Lett. 81B, 151 (1979)

G.Igo, G.S.Adams, T.S.Bauer, G.Pauletta, C.A.Whitten, Jr., A.Wriekat, G.W.Hoffmann, G.S.Blanpied, W.R.Coker, C.Harvey, R.P.Liljestrand, L.Ray, J.E.Spencer, H.A.Thiessen, C.Glashausser, N.M.Hintz, M.A.Oothoudt, H.Nann, K.K.Seth, B.E.Wood, D.K.McDaniels, M.Gazzaly

Elastic Differential Cross Sections and Analyzing Powers for Polarized p + ^40,42,44,48Ca at 0.8 GeV

NUCLEAR REACTIONS ^40,42,44,48Ca(polarized p, p), E=0.8 GeV; measured σ(θ), A(θ); deduced rms radii of neutrons. Kerman-McManus-Thaler optical potential analysis.

doi: 10.1016/0370-2693(79)90510-0
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1979IV03 Phys.Lett. 82B, 51 (1979)

S.Iversen, H.Nann, A.Obst, K.K.Seth, N.Tanaka, C.L.Morris, H.A.Thiessen, K.Boyer, W.Cottingame, C.F.Moore, R.L.Boudrie, D.Dehnhard

Neutron-Proton Radius Differences and Isovector Deformations from π⁺ and π^- Inelastic Scattering from ¹⁸O

NUCLEAR REACTIONS ¹⁸O(π⁺, π⁺), (π⁺, π⁺'), (π^-, π^-), (π^-, π^-'), E=164 MeV; measured σ(θ). ¹⁸O levels deduced isovector deformations, neutron-proton radius differences.

doi: 10.1016/0370-2693(79)90423-4
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1979NA13 Phys.Lett. 88B, 257 (1979)

H.Nann, S.Iversen, M.Kaletka, J.Hird, K.K.Seth, B.Hoistad, R.L.Burman, G.Kyle

p + p → d + π⁺ Reaction at 0.8 GeV

NUCLEAR REACTIONS ¹H(polarized p, π⁺), E=0.8 GeV; measured σ(E(π+), θ), Ay(θ). Mandl-regge formalism, coupled channels analysis.

doi: 10.1016/0370-2693(79)90461-1
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1979RA15 Phys.Lett. 83B, 275 (1979)

L.Ray, T.Kozlowski, D.G.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, N.Tanaka, H.A.Thiessen, G.S.Kyle, N.M.Hintz, M.A.Oothoudt, P.M.Lang, H.Nann, K.K.Seth, D.K.McDaniels, P.M.Varghese, G.S.Blanpied, G.W.Hoffmann, R.P.Liljestrand, J.C.Fong, G.Igo, R.J.Ridge, R.M.Rolfe, C.A.Whitten, Jr.

Coupled-Channels Effects in 0.8 GeV Proton Inelastic Scattering from ⁵⁸Ni

NUCLEAR REACTIONS ⁵⁸Ni(p, p'), E=0.8 GeV; calculated σ(θ). Coupled channel, DWBA calculations with multistep, multiphonon mixing.

doi: 10.1016/0370-2693(79)91106-7
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1979SE08 Phys.Rev.Lett. 43, 1574 (1979); Erratum Phys.Rev.Lett. 45, 147 (1980)

K.K.Seth, S.Iversen, H.Nann, M.Kaletka, J.Hird, H.A.Thiessen

Angular Distributions for the Reaction ¹⁸O(π⁺, π^-)¹⁸Ne and Pion Double-Charge-Exchange Form Factors

NUCLEAR REACTIONS ¹⁸O(π⁺, π^-), E=164 MeV; measured reaction products, ¹⁸Ne; deduced σ(θ), reaction mechanism, analog, anti-analog states.

doi: 10.1103/PhysRevLett.43.1574
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1978BL02 Phys.Rev. C18, 1436 (1978)

G.S.Blanpied, W.R.Coker, R.P.Liljestrand, G.W.Hoffmann, L.Ray, D.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, H.A.Thiessen, T.Kozlowski, N.M.Hintz, G.S.Kyle, M.A.Oothoudt, T.S.Bauer, G.Igo, R.J.Ridge, C.A.Whitten, Jr., P.M.Lang, H.Nann, K.K.Seth

Proton Elastic and Inelastic Scattering at 0.8 GeV from ^12,13C and ²⁰⁸Pb

NUCLEAR REACTIONS ^12,13C, ²⁰⁸Pb(p, p'), E=0.8 GeV; measured σ(θ). ^12,13C, ²⁰⁸Pb deduced deformation length. Optical potential, DWBA analysis. Enriched targets.

doi: 10.1103/PhysRevC.18.1436
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1978HO05 Phys.Rev.Lett. 40, 1256 (1978)

G.W.Hoffman, G.S.Blanpied, W.R.Coker, R.P.Liljestrand, N.M.Hintz, M.A.Oothoudt, T.S.Bauer, G.Igo, G.Pauletta, J.Soukup, C.A.Whitten, Jr., D.Madland, J.C.Pratt, L.Ray, J.E.Spencer, H.A.Thiessen, H.Nann, K.K.Seth, C.Glashausser, D.K.McDaniels, J.Tinsley, P.Varghese

Analyzing Power in Proton-Nucleus Elastic Scattering at 0.8 GeV

NUCLEAR REACTIONS ¹²C, ⁵⁸Ni, ⁹⁰Zr, ²⁰⁸Pb(polarized p, p), E=0.8 GeV; measured A(θ), σ(θ).

doi: 10.1103/PhysRevLett.40.1256
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1978HO12 Phys.Lett. 76B, 383 (1978)

G.W.Hoffmann, G.S.Blanpied, W.R.Coker, R.P.Liljestrand, L.Ray, J.E.Spencer, H.A.Thiessen, N.M.Hintz, M.A.Oothoudt, T.S.Bauer, G.Igo, G.Pauletta, J.Soukup, C.A.Whitten, Jr., H.Nann, K.K.Seth, C.Glashausser, D.K.McDaniels, J.Tinsley, P.Varghese

Analysis of Elastic Scattering of 0.8 GeV Polarized Protons from ¹¹⁶Sn and ¹²⁴Sn

NUCLEAR REACTIONS ^116,124Sn(polarized p, p), E=800 MeV; analyzed A(θ), σ(θ). Spin-dependent Kerman-McManus-Thaler formalism.

doi: 10.1016/0370-2693(78)90888-2
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1978HO18 Phys.Lett. 79B, 376 (1978)

G.W.Hoffmann, G.S.Blanpied, W.R.Coker, C.Harvey, R.P.Liljestrand, G.S.Adams, T.S.Bauer, G.Igo, G.Pauletta, C.A.Whitten, Jr., A.Wriekat, L.Ray, J.E.Spencer, H.A.Thiessen, H.Nann, K.K.Seth, N.M.Hintz, G.Kyle, M.A.Oothoudt, B.E.Wood, D.K.McDaniels, C.Glashausser, M.Gazzaly

Elastic Differential Cross Sections and Analyzing Powers for p + ⁵⁴Fe, ^58,64Ni at 800 MeV

NUCLEAR REACTIONS ⁵⁴Fe, ^58,64Ni(polarized p, p), E=800 MeV; measured σ(θ); deduced neutron density distribution. Approximately model-independent analysis.

doi: 10.1016/0370-2693(78)90386-6
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1978IV01 Phys.Rev.Lett. 40, 17 (1978)

S.Iversen, A.Obst, K.K.Seth, H.A.Thiessen, C.L.Morris, N.Tanaka, E.Smith, J.F.Amann, R.Boudrie, G.Burleson, M.Devereux, L.W.Swenson, P.Varghese, K.Boyer, W.J.Braithwaite, W.Cottingame, C.F.Moore

Neutron Deformation Parameter from Comparative Study of π⁺ and π^- Inelastic Scattering

NUCLEAR REACTIONS ¹⁸O(π^-, π^-'), (π⁺, π⁺'), E=230 MeV; measured σ. ¹⁸O level deduced β.

doi: 10.1103/PhysRevLett.40.17
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1978MO23 Phys.Lett. 80B, 38 (1978)

C.F.Moore, W.Cottingame, K.G.Boyer, L.E.Smith, C.Harvey, W.J.Braithwaite, C.L.Morris, H.A.Thiessen, J.F.Amann, M.Devereux, G.Blanpied, G.Burleson, A.W.Obst, S.Iversen, K.K.Seth, R.L.Boudrie, R.J.Peterson

Observation of Enhanced Excitation of ¹²C by Inelastic Pion Scattering on the (3, 3) Pion-Nucleon Resonance

NUCLEAR REACTIONS ¹²C(π⁺, π⁺'), E=100-291 MeV; measured σ(θ). ¹²C deduced selective enhancement for states near 20 MeV for incident energy near pion-nucleus (3, 3) resonance.

doi: 10.1016/0370-2693(78)90300-3
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1978SE07 Phys.Rev.Lett. 41, 1589 (1978)

K.K.Seth, H.Nann, S.Iversen, M.Kaletka, J.Hird, H.A.Thiessen

Mass of ¹⁸C by Pion Double-Charge-Exchange Reaction

NUCLEAR REACTIONS ¹⁸O(π^-, π⁺), E=164 MeV; measured missing-mass spectra; deduced Q. ¹⁸C deduced mass excess.

doi: 10.1103/PhysRevLett.41.1589
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1977BE17 Phys.Lett. 67B, 16 (1977)

G.Berrier-Ronsin, G.Duhamel, E.Gerlic, J.Kalifa, H.Langevin-Joliot, G.Rotbard, M.Vergnes, J.Vernotte, K.K.Seth

Study of the Fine Structure in the 'Deeply' Bound Hole States in ¹¹⁵Sn

NUCLEAR REACTIONS ¹¹⁶Sn(d, t), E=23 MeV; measured σ(Et, θ). ¹¹⁵Sn deduced levels, L.

doi: 10.1016/0370-2693(77)90792-4
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1977BE45 Nucl.Phys. A288, 279 (1977)

G.Berrier-Ronsin, G.Duhamel, E.Gerlic, J.Kalifa, H.Langevin-Joliot, G.Rotbard, M.Vergnes, J.Vernotte, K.K.Seth, K.Heyde

The ¹¹⁶Sn(d, t)¹¹⁵Sn Reaction at 23 MeV

NUCLEAR REACTIONS ¹¹⁶Sn(d, t), E=23 MeV; measured σ(Et, θ). ¹¹⁵Sn deduced levels, J, π, S, L. Separated target.

doi: 10.1016/0375-9474(77)90135-X
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1977BL09 Phys.Rev.Lett. 39, 1447 (1977); Erratum Phys.Rev.Lett. 40, 420 (1978)

G.S.Blanpied, W.R.Coker, R.P.Liljestrand, L.Ray, G.W.Hoffman, D.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, H.A.Thiessen, N.M.Hintz, G.S.Kyle, M.A.Oothoudt, T.S.Bauer, J.C.Fong, G.Igo, R.J.Ridge, C.A.Whitten, Jr., Y.Kozlowski, D.K.McDaniels, P.Varghese, P.M.Lang, H.Nann, K.K.Seth, C.Glashausser

Elastic Scattering of 0.8-GeV Protons from ¹²C, ⁵⁸Ni, and ²⁰⁸Pb

NUCLEAR REACTIONS ¹²C, ⁵⁸Ni, ²⁰⁸Pb(p, p), E=0.8 GeV; measured σ(θ).

doi: 10.1103/PhysRevLett.39.1447
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1975NA10 Phys.Rev.Lett. 35, 609 (1975); Erratum Phys.Rev.Lett. 35, 1051 (1975)

H.Nann, B.H.Wildenthal, A.Saha, K.K.Seth

Comment on 'Prediction of Weak-Coupling Structure from a Shell-Model Basis'

NUCLEAR REACTIONS ³⁴S, ³⁵Cl(p, t), E=40 MeV; measured σ(Et, θ). ³²S, ³³Cl levels deduced L, S.

doi: 10.1103/PhysRevLett.35.609
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1975SE08 Phys.Rev. C11, 2087 (1975)

K.K.Seth, K.A.Buzard, J.Picard, G.Bassani

Comment on the ⁸⁷Sr(d, p) Reaction

NUCLEAR REACTIONS ⁸⁷Sr(d, p), E=12 MeV; analyzed data. ⁸⁸Sr levels deduced revised two-body matrix elements.

doi: 10.1103/PhysRevC.11.2087
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1975SE17 Phys.Lett. 59B, 333 (1975)

K.K.Seth, A.Saha, H.Nann, B.H.Wildenthal

Structure of Positive Parity States in ²⁹P and Two-Step Processes in (p, t) Reactions

NUCLEAR REACTIONS ³⁰Si, ³¹P(p, t), E=40 MeV; measured σ(Et, θ). ²⁹P, ²⁸Si deduced levels, L.

doi: 10.1016/0370-2693(75)90085-4
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1974MI16 Nucl.Phys. A231, 316 (1974)

W.Mittig, Y.Cassagnou, N.Cindro, L.Papineau, K.K.Seth

Spectroscopy of ⁴¹Sc by Resonant Scattering of Protons: Observation of An Intermediate Structure

NUCLEAR REACTIONS ⁴⁰Ca(p, p), (p, p'), E=4.8-8.2 MeV; measured σ(E, Ep', θ). ⁴¹Sc resonances deduced J, π, p-width, S, intermediate structure. Enriched target.

doi: 10.1016/0375-9474(74)90524-7
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1974PI09 Ann.Phys.(New York) 84, 165 (1974)

W.F.E.Pineo, M.Divadeenam, E.G.Bilpuch, K.K.Seth, H.W.Newson

Neutron Strength Functions and Average Total Cross Sections. II. The Behavior of the Average Cross Sections and the S-Wave Scattering Lengths

NUCLEAR REACTIONS Se, V, Mn, Co, Cu, Zn, As, Se, Ce, Nd, ^144,146,148Nd, Sm, ^149,152Sm, Gd, Tb, Dy, Ho, Hg(n, X), E=100-650 keV; measured σ(E), also for compounds KCl, RbBr, CsI.

doi: 10.1016/0003-4916(74)90298-X
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1974SE04 Phys.Lett. 49B, 157 (1974)

K.K.Seth, A.Saha, W.Stewart, W.Benenson, W.A.Lanford, H.Nann, B.H.Wildenthal

(p, t) Reactions on Odd-A Nuclei and the Weak-Coupling Core-Excitation Model

NUCLEAR REACTIONS ⁴³Ca(p, t), E=42 MeV; ⁴²Ca, ⁵⁹Co, ⁶⁰Ni(p, t), E=40 MeV; measured reaction products. ^40,41Ca, ⁵⁷Co, ⁵⁸Ni; deduced σ(θ), levels, negative-parity states, L, weak-coupling. The Michigan State University cyclotron and an Enge split-pole spectrograph equipped with a single-wire proportional counter.

doi: 10.1016/0370-2693(74)90497-3
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1974SE05 Phys.Rev.Lett. 33, 233 (1974)

K.K.Seth, A.Saha, W.Benenson, W.A.Lanford, H.Nann, B.H.Wildenthal

Discovery of the Missing Two-Particle, Two-Hole 0⁺ States in ⁴⁰Ca

NUCLEAR REACTIONS ⁴²Ca(p, t), E=40.27 MeV; measured Q, σ(E(t), θ). ⁴⁰Ca deduced levels, J, π.

doi: 10.1103/PhysRevLett.33.233
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1974SE10 Phys.Rev. C10, 1928 (1974)

K.K.Seth, K.A.Buzard, J.Picard, G.Bassani

⁸⁷Sr(d, p)⁸⁸Sr Reaction

NUCLEAR REACTIONS ⁸⁷Sr(d, p), E=12 MeV; measured σ(Ep, θ). ⁸⁸Sr deduced levels, J, π.

doi: 10.1103/PhysRevC.10.1928
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1974SE12 Phys.Lett. 53B, 171 (1974)

K.K.Seth, S.G.Iversen

Identification of the Missing 3/2^- State in ⁴¹Ca

NUCLEAR REACTIONS ⁴⁰Ca(d, p), E=11 MeV; measured σ(Ep, θ). ⁴¹Ca deduced level, J, π, L.

doi: 10.1016/0370-2693(74)90523-1
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1974WI04 Phys.Rev.Lett. 32, 794 (1974)

B.H.Wildenthal, H.Nann, K.K.Seth

Prediction of Weak-Coupling Structure from a Shell-Model Basis

NUCLEAR REACTIONS ³⁰Si, ³¹P, ³⁴S, ³⁵Cl(p, t); measured nothing, calculated σ(θ). ²⁸Si, ²⁹P, ³²S, ³³Cl calculated S. ³²S(d, n); measured nothing. ³³Cl calculated S.

doi: 10.1103/PhysRevLett.32.794
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1973SE01 Phys.Rev.Lett. 30, 132 (1973); Erratum Phys.Rev.Lett. 30, 250 (1973)

K.K.Seth, H.Ohnuma, T.Suehiro, S.Yamada, S.Takeda

(p, t) Reactions on ⁴⁵Sc and ⁴⁴Ca and the Weak-Coupling Core-Excitation Model

NUCLEAR REACTIONS ⁴⁴Ca, ⁴⁵Sc(p, t), E=52 MeV; measured σ(Et, θ). ⁴²Ca, ⁴³Sc deduced levels, J, π, L.

doi: 10.1103/PhysRevLett.30.132
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1973SE09 Phys.Rev.Lett. 31, 552 (1973)

K.K.Seth, A.Saha, L.Greenwood

High-Spin States in ⁴¹Ca; K = 3/2⁺ and K = 3/2^- Rotational Bands (Question)

NUCLEAR REACTIONS ⁴⁰Ca(d, p), E=11 MeV; measured σ(Ep, θ). ⁴¹Ca levels deduced J, π, L, S.

doi: 10.1103/PhysRevLett.31.552
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1972LE01 Phys.Rev. C5, 328 (1972)

M.-C.Lemaire, M.C.Mermaz, K.K.Seth

Study of the 2p-1h Structure of ¹⁷O via the ¹⁵N(³He, p) Reaction

NUCLEAR REACTIONS ¹⁵N(³He, p), E=18 MeV; measured σ(θ). ¹⁷O deduced levels, J, π, L.

doi: 10.1103/PhysRevC.5.328
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1972SE27 Nucl.Data Sheets B7, 161 (1972)

K.K.Seth

Nuclear Data Sheets for A = 206

doi: 10.1016/S0090-3752(72)80057-7
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1971BO04 Nucl.Phys. A160, 577 (1971)

J.Bommer, K.Grabisch, H.Kluge, G.Roschert, H.Fuchs, U.Lynen, K.K.Seth

Study of ⁴³Sc States with Proton Transfer Reactions on ⁴²Ca

NUCLEAR REACTIONS ⁴²Ca(d, n), E=5.0-6.05 MeV;⁴²Ca(³He, d), E=18 MeV; measured σ(E, θ). ⁴³Sc deduced levels, isobaric analogs, L, J, π, S. Enriched ⁴²Ca targets.

doi: 10.1016/0375-9474(71)90099-6
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1971SE07 Priv.Comm. (1971)

K.K.Seth, P.D.Miller

1970BE20 Nucl.Phys. A147, 326 (1970)

O.Beer, A.El Behay, P.Lopato, Y.Terrien, G.Vallois, K.K.Seth

Spectroscopy of Even Tin Isotopes by Inelastic Scattering of 24.5 MeV Protons

NUCLEAR REACTIONS ^{116,118,120,122,124}Sn(p, p'), Ep=24.5 MeV; measured σ(Ep', θ). ^{116,118,120,122,124}Sn deduced J, π, β(L). Enriched targets.

doi: 10.1016/0375-9474(70)90271-X
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1970CO17 Phys.Rev. C2, 149 (1970)

R.G.Couch, J.A.Biggerstaff, F.G.Perey, S.Raman, K.K.Seth

Spectroscopy of ^65,67,69Ga by (d, n) Reaction

NUCLEAR REACTIONS ^64,66,68Zn(d, n), E=10 MeV; measured σ(En, θ). ^65,67,69Ga deduced levels, L(p), J, π, S.

doi: 10.1103/PhysRevC.2.149
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1970GO19 Priv.Comm. (1970)

W.Good, J.H.Gibbons, J.A.Biggerstaff, K.K.Seth

Neutron Total Cross Sections of ²⁰³Tl and ²⁰⁵Tl

1970SE01 Nucl.Phys. A140, 577 (1970)

K.K.Seth, J.Picard, G.R.Satchler

A Study of the ⁴⁰Ca(d, p)⁴¹Ca Reaction (I). The Single-Particle States

NUCLEAR REACTIONS ⁴⁰Ca(d, p), E=9.8-12.12 MeV; measured σ(E;Ep, θ). ⁴⁰Ca(d, d), E=11, 12 MeV; measured σ(θ). ⁴¹Ca levels deduced S. Enriched target.

doi: 10.1016/0375-9474(70)90581-6
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1969CO10 Phys.Letters 29B, 657 (1969)

T.G.Couch, F.G.Perey, J.A.Biggerstaff, K.K.Seth

Isobaric Spin Dependence in Proton Transfer Reactions

NUCLEAR REACTIONS ⁵⁴Fe(d, n), E=10 MeV; measured σ(En, θ). ⁵⁵Co deduced levels, J, π, L(p), S, t. Enriched ⁵⁴Fe target.

doi: 10.1016/0370-2693(69)90102-6
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1968CA24 Izv.Akad.Nauk SSSR, Ser.Fiz. 32, 1650 (1968); Bull.Acad.Sci.USSR, Phys.Ser. 32, 1531 (1969)

Y.Cassagnou, E.Cotton, W.Mittig, L.Papineau, K.K.Seth, N.Cindro

Search for Two-Particle - One-Hole States in ⁴¹Sc

NUCLEAR REACTIONS ⁴⁰Ca(p, p'), E = 4.8 -6.1 MeV; measured σ(E;Ep', θ). ⁴¹Sc deduced resonances.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1012.

1967BI07 Phys.Letters 25B, 273 (1967)

J.A.Biggerstaff, C.Bingham, P.D.Miller, J.Solomon, K.K.Seth

Proton Particle-Hole States in ¹¹⁶Sn

NUCLEAR STRUCTURE ¹¹⁶Sn; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90011-1
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1967SE10 Phys.Rev. 164, 1450 (1967)

K.K.Seth, J.A.Biggerstaff, P.D.Miller, G.R.Satchler

Study of Proton Particle-Hole States in ⁴⁰Ca by the ³⁹K(³He, D)⁴⁰Ca Reaction

NUCLEAR STRUCTURE ⁴⁰Ca; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.164.1450
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1966SE08 Phys.Rev.Letters 17, 1294 (1966)

K.K.Seth, R.G.Couch, J.A.Biggerstaff, P.D.Miller

Reaction ³⁹K(³He, P)⁴¹Ca and Two-Particle, One-Hole States

NUCLEAR STRUCTURE ⁴¹Ca; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.17.1294
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1965SE01 Bull.Am.Phys.Soc. 10, No.1, 10, AC8 (1965)

K.K.Seth, G.Walter, P.D.Miller, J.A.Biggerstaff

¹⁵N(³He, p) Reaction and Intermediate States

NUCLEAR STRUCTURE ¹⁵N; measured not abstracted; deduced nuclear properties.

1965SE10 Phys.Letters 16, 306 (1965)

K.K.Seth

Neutron Total Cross Sections and Intermediate Resonances

doi: 10.1016/0031-9163(65)90863-2
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1965WI17 Nucl.Phys. 62, 511 (1965)

R.M.Wilenzick, K.K.Seth, P.R.Bevington, H.W.Lewis

Elastic And Inelastic Scattering Of 6 Mev Neutrons

NUCLEAR REACTIONS C(n, n), ¹²C(n, n), ¹²C(n, n'), Fe(n, n), Fe(n, n'), ⁸⁹Y(n, n), ⁸⁹Y(n, n'), Mo(n, n), Mo(n, n'), ¹⁰³Rh(n, n), ¹⁰³Rh(n, n'), Cd(n, n), Cd(n, n'), Sn(n, n), Sn(n, n'), ²⁰⁹Bi(n, n), ²⁰⁹Bi(n, n'), E=-1.0 eV-6 MeV; measured products, ¹²C, C, Fe, ⁸⁹Y, Mo, ¹⁰³Rh, Cd, Sn, ²⁰⁹Bi; deduced σ, σ(E), σ(θ). Data were imported from EXFOR entry 11287.

doi: 10.1016/0029-5582(65)90496-7
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1964SE03 Compt.Rend.Congr.Intern.Phys.Nucl., Paris, P.Gugenberger, Ed., Centre National de la Recherche Scientifique, Paris, Vol.II, p.916(1964)

K.K.Seth, R.H.Tabony, E.G.Bilpuch, H.W.Newson

S-, P-, and D-Wave Neutron Strength Functions and the Optical Model

1964SE12 Phys.Letters 13, 70 (1964)

K.K.Seth, R.H.Tabony, E.G.Bilpuch, H.W.Newson

s-, p-, and d- Wave Neutron Strength Functions

doi: 10.1016/0031-9163(64)90312-9
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1963CH01 Bull.Am.Phys.Soc. 8, No.1, 38 , J12 (1963)

R.Chalmers, R.S.Cox, K.K.Seth, E.N.Strait

Polarization of Protons Elastically Scattered from Deuterons

NUCLEAR STRUCTURE ²H; measured not abstracted; deduced nuclear properties.

1963SE13 Nucl.Phys. 47, 137 (1963)

K.K.Seth, E.G.Bilpuch, H.W.Newson

Total Neutron Cross Section of Carbon

NUCLEAR STRUCTURE ¹²C; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90860-5
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1962TA01 Bull.Am.Phys.Soc. 7, No.1, 23, F11(1962)

R.H.Tabony, K.K.Seth, E.G.Bilpuch, H.W.Newson

Average Total Neutron Cross Section and s-, p-, d-Wave Strength Functions

1962TA19 WASH-1034, p.10 (1962); Priv.Comm. (1966)

R.H.Tabony, K.K.Seth, E.G.Bilpuch, H.W.Newson

Average Total Neutron Cross Sections

1962WI01 Bull.Am.Phys.Soc. 7, No.1, 23, F8 (1962)

R.M.Wilenzick, K.K.Seth, P.R.Bevington, H.W.Lewis

Inelastic Neutron Scattering from Light and Medium Heavy Nuclei

NUCLEAR STRUCTURE ¹²C; measured not abstracted; deduced nuclear properties.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11287.

1961BI01 Bull.Am.Phys.Soc. 6, No.1, 69, X1 (1961)

E.G.Bilpuch, K.K.Seth, C.D.Bowman, H.W.Newson

Neutron Resonance Parameters in the keV Region

1961BI06 Ann.Phys.(N.Y.) 14, 387 (1961)

E.G.Bilpuch, K.K.Seth, C.D.Bowman, R.H.Tabony, R.C.Smith, H.W.Newson

s and p-Wave Neutron Spectroscopy Part VII. Widths of Neutron Resonances

NUCLEAR STRUCTURE ¹³¹Te, ¹³⁹Ba, ¹³⁷Ba, ²⁰⁹Pb, ²⁰⁸Pb, ²⁰⁷Pb, ⁸⁹Sr, ⁹⁰Y, ⁶¹Ni, ⁵⁷Fe, ⁵⁹Ni, ⁵⁸Fe, ⁴¹Ca, ⁵¹Cr, ⁵⁵Cr, ⁵⁵Fe, ⁵³Cr, ⁴⁵Ca, ⁴⁹Ti; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0003-4916(61)90063-X
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11599.

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