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NSR database version of May 8, 2024.

Search: Author = L.Smith

Found 45 matches.

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2016KO46      Sci. Rep. 6, 37321 (2016)

O.Kock, W.He, D.Swierad, L.Smith, J.Hughes, K.Bongs, Y.Singh

Laser controlled atom source for optical clocks

ATOMIC PHYSICS ^87,88Sr; measured frequencies; deduced an atom source for a strontium optical lattice clock with simple setups and sensitivity to thermal radiation, millions of strontium atoms from the vapour can be captured in a magneto-optical trap (MOT).

doi: 10.1038/srep37321
Citations: PlumX Metrics

2008JU04      Phys.Rev. C 77, 045205 (2008)

B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato, L.C.Smith

Dynamical coupled-channels effects on pion photoproduction

NUCLEAR REACTIONS p(γ, p)π⁰, E=1154-1632 MeV; calculated cross sections, angular distributions using dynamical coupled-channel model. Comparison with experimental data.

doi: 10.1103/PhysRevC.77.045205
Citations: PlumX Metrics

2007JU01      Phys.Rev. C 75, 015205 (2007)

B.Julia-Diaz, T.-S.H.Lee, T.Sato, L.C.Smith

Extraction and interpretation of γN → Δ form factors within a dynamical model

NUCLEAR REACTIONS ¹H(e, e'π⁰), E=high; analyzed σ(θ), related data; deduced form factors.

doi: 10.1103/PhysRevC.75.015205
Citations: PlumX Metrics

2007LE17      J.Phys.(London) G34, S83 (2007)

T.-S.H.Lee, L.C.Smith

Study of nucleon resonances with electromagnetic interactions

doi: 10.1088/0954-3899/34/7/S05
Citations: PlumX Metrics

2006WA13      Nucl.Instrum.Methods Phys.Res. A560, 360 (2006)

G.A.Warren, L.E.Smith, C.E.Aalseth, E.Ellis, T.W.Hossbach, A.B.Valsan

Determining activities of radionuclides from coincidence signatures

RADIOACTIVITY ⁹⁹Mo, ¹⁴⁰La; calculated γγ-coin intensities.

doi: 10.1016/j.nima.2005.12.236
Citations: PlumX Metrics

2005AZ01      Phys.Rev. C 71, 015201 (2005)

I.G.Aznauryan, V.D.Burkert, H.Egiyan, K.Joo, R.Minehart, L.C.Smith

Electroexcitation of the P₃₃(1232), P₁₁(1440), D₁₃(1520), and S₁₁(1535) at Q² = 0.4 and 0.65 (GeV/c)²

NUCLEAR REACTIONS ¹H(e, e'π⁺), (e, e'π⁰), E=high; analyzed data; deduced resonance contributions. Dispersion relation and isobar model approaches.

doi: 10.1103/PhysRevC.71.015201
Citations: PlumX Metrics

2000HI06      Phys.Rev. C61, 054609 (2000)

K.Hicks, V.Gladyshev, H.Baghaei, A.Caracappa, A.Cichocki, R.Deininger, R.Finlay, T.Gresko, S.Hoblit, M.Khandaker, O.Kistner, F.X.Li, R.Lindgren, M.Lucas, L.Miceli, B.Norum, J.Rapaport, A.Sandorfi, R.Sealock, L.C.Smith, C.Thorn, S.Thornton, C.S.Whisnant, D.Willits, L.E.Wright

The ¹⁶O(γ(pol), π^-p) Reaction at E_γ ≈ 300 MeV

NUCLEAR REACTIONS ¹⁶O(polarized γ, π^-p), E=290-325 MeV; measured σ(E, θ₁, θ₂), spin asymmetries. Comparison with DWIA results.

doi: 10.1103/PhysRevC.61.054609
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1999SM12      Fizika(Zagreb) B8, 1 (1999)

L.C.Smith

First Results from CLAS

1998FR07      Phys.Rev. C57, 3144 (1998)

E.Frlez, D.Pocanic, K.A.Assamagan, J.P.Chen, K.J.Keeter, R.M.Marshall, R.C.Minehart, L.C.Smith, G.E.Dodge, S.S.Hanna, B.H.King, J.N.Knudson

Differential Cross Sections for Pion Charge Exchange on the Proton at 27.5 MeV

NUCLEAR REACTIONS ¹H(π^-, π⁰), E=27.5 MeV; measured σ(θ).

doi: 10.1103/PhysRevC.57.3144
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1998GE11      Phys.Rev. C58, 3742 (1998)

M.Geso, D.Adams, J.Bystricky, G.Igo, A.Ling, C.Whitten, M.Nasser, L.C.Smith, R.W.Whitney

Measurements of Spin Observables for the p(pol)-⁴He Elastic Scattering at 800 MeV

NUCLEAR REACTIONS ⁴He(p, p), (polarized p, p), E=800 MeV; measured spin transfer observables vs momentum transfer.

doi: 10.1103/PhysRevC.58.3742
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0611.

1997HI01      Phys.Rev. C55, R12 (1997)

K.Hicks, H.Baghaei, A.Caracappa, A.Cichocki, G.Davenport, R.Finlay, V.Gladyshev, T.Gresko, S.Hoblit, M.Khandaker, O.Kistner, F.X.Lee, R.Lindgren, M.Lucas, L.Miceli, B.Norum, J.Rapaport, A.Sandorfi, R.Sealock, L.C.Smith, C.Thorn, S.Thornton, C.S.Whisnant, L.E.Wright

Spin Asymmetries from ¹⁶O(γ(pol), pπ^-) Near Δ Resonance Energies

NUCLEAR REACTIONS ¹⁶O(polarized γ, pπ^-), E=293 MeV; measured spin asymmetry vs θp, θ(π); deduced Δ-nucleus potential, δ lifetime dependences.

doi: 10.1103/PhysRevC.55.R12
Citations: PlumX Metrics

1997PE16      Nucl.Phys. A621, 566c (1997)

M.Pettini, D.L.King, L.J.Smith, R.W.Hunstead

The Emergence of Metals and Dust in Galaxies at High Redshifts

doi: 10.1016/S0375-9474(97)00304-7
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1996AB02      Phys.Rev.Lett. 76, 587 (1996)

K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration

Measurements of the Proton and Deuteron Spin Structure Function g₂ and Asymmetry A₂

NUCLEAR STRUCTURE ^1,2H; analyzed data; deduced spin structure function, asymmetry data. Polarized ammonia targets, (polarized e, e') reaction.

NUCLEAR REACTIONS ^1,2H(polarized e, e'), E=29.1 GeV; measured spin asymmetries. ^1,2H deduced spin structure functions. Polarized ammonia targets.

doi: 10.1103/PhysRevLett.76.587
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1995AB02      Phys.Rev.Lett. 74, 346 (1995)

K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration

Precision Measurement of the Proton Spin Structure Function g₁(p)

NUCLEAR REACTIONS ¹H(polarized e, e'), E=9.7-29.1 GeV; measured asymmetry. ¹H deduced spin structure function g₁(p). Polarized ¹⁵NH₃ target.

doi: 10.1103/PhysRevLett.74.346
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1995AD01      Phys.Rev. C51, 17 (1995)

G.S.Adams, H.Baghaei, A.Caracappa, W.Clayton, A.D'Angelo, S.Hoblit, M.Khandaker, O.C.Kistner, T.Kobayashi, R.Lindgren, L.Miceli, C.Ruth, A.M.Sandorfi, C.Schaerf, R.M.Sealock, L.C.Smith, P.Stoler, D.J.Tedeschi, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, E.J.Winhold

Measurement of γ(pol)d → pnπ⁰ at Large Nucleon Momenta

NUCLEAR REACTIONS ²H(polarized γ, nπ⁰), E=290 MeV; measured σ(θn, θp) vs neutron momentum; deduced beam asymmetries. Cascade Monte Carlo calculation.

doi: 10.1103/PhysRevC.51.17
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1995DO07      Phys.Lett. 344B, 91 (1995)

M.L.Dowell, S.Gilad, E.Piasetzky, S.Hoibraten, H.W.Baer, E.J.Beise, J.D.Bowman, G.W.Dodson, F.Irom, J.N.Knudson, G.S.Kyle, M.J.Leitch, L.D.Pham, R.P.Redwine, S.H.Rokni, L.C.Smith, D.R.Tieger, S.A.Wood

Measurements of Quasi-Elastic Pion Single Charge Exchange on ³He at T(π) = 245 MeV

NUCLEAR REACTIONS ³He(π⁺, π⁰), (π^-, π⁰), (π⁺, π⁰p), (π^-, π^-p), E=245 MeV; measured σ(θ(π), E(π)), σ(θ(π), θ(p)); deduced integral σ; deduced quasifree mechanism evidence.

doi: 10.1016/0370-2693(94)01539-O
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1994PO01      Phys.Rev.Lett. 72, 1156 (1994)

D.Pocanic, E.Frlez, K.A.Assamagan, J.P.Chen, K.J.Keeter, R.M.Marshall, R.C.Minehart, L.C.Smith, G.E.Dodge, S.S.Hanna, B.H.King, J.N.Knudson

Reaction π⁺p → π⁺π⁰p Near Threshold and Chiral Symmetry Breaking

NUCLEAR REACTIONS ¹H(π⁺, π⁺π⁰), E=190-260 MeV; measured invariant mass spectra, π⁰π⁺-, π⁰p-coin; deduced total σ(E).

doi: 10.1103/PhysRevLett.72.1156
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1994RU04      Phys.Rev.Lett. 72, 617 (1994)

C.Ruth, G.S.Adams, H.Baghaei, A.Caracappa, W.B.Clayton, A.D'Angelo, M.-A.Duval, G.Giordano, S.Hoblit, O.C.Kistner, J.M.Laget, R.Lindgren, G.Matone, L.Miceli, W.K.Mize, M.A.Moinester, A.M.Sandorfi, C.Schaerf, R.M.Sealock, L.C.Smith, P.Stoler, D.J.Tedeschi, P.K.Teng, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, E.J.Winhold

First Measurement of the Reaction ³He(γ(pol), p)X with Polarized Photons

NUCLEAR REACTIONS ³He(polarized γ, p), E=195-304 MeV; measured σ(θ), photon asymmetry vs proton momentum; deduced three-nucleon absorption evidence. Linear beam polarization.

doi: 10.1103/PhysRevLett.72.617
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1994TE07      Phys.Rev.Lett. 73, 408 (1994)

D.J.Tedeschi, G.S.Adams, G.Audit, H.Baghaei, A.Caracappa, W.B.Clayton, A.D'Angelo, M.A.Duval, G.Giordano, S.Hoblit, O.C.Kistner, J.M.Laget, R.Lindgren, G.Matone, L.Miceli, W.K.Mize, M.Moinester, C.Ruth, A.Sandorfi, C.Schaerf, R.M.Sealock, L.C.Smith, P.Stoler, P.K.Teng, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, E.J.Winhold

Exclusive Photodisintegration of ³He with Polarized Photons

NUCLEAR REACTIONS ³He(polarized γ, np), (polarized γ, 2p), E=235-305 MeV; measured σ(θ₁, θ₂, p₁), asymmetry; deduced reaction mechanism.

doi: 10.1103/PhysRevLett.73.408
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1993ME01      Nucl.Phys. A553, 701c (1993)

Z.-E.Meziani, J.P.Chen, D.Beck, G.Boyd, L.M.Chinitz, D.B.Day, L.C.Dennis, G.E.Dodge, B.W.Filippone, K.L.Giovanetti, J.Jourdan, K.W.Kemper, T.Koh, W.Lorenzon, J.S.McCarthy, R.D.McKeown, R.G.Milner, R.C.Minehart, J.Morgenstern, J.Mougey, D.H.Potterveld, O.A.Rondon-Aramayo, R.M.Sealock, I.Sick, L.C.Smith, S.T.Thornton, R.C.Walker, C.Woodward

High Momentum Transfer R(T, L) Response Functions for ^3,4He

NUCLEAR REACTIONS ^3,4He(e, e'X), E=0.9-4.3 GeV; measured inclusive σ; deduced longitudinal, transverse response functions, Coulomb sum rule saturation.

doi: 10.1016/0375-9474(93)90683-O
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1993RI01      Phys.Rev. C47, 21 (1993)

B.G.Ritchie, T.D.Averett, D.Rothenberger, J.R.Tinsley, R.C.Minehart, K.Giovanetti, L.C.Smith, G.S.Blanpied, B.M.Preedom

π⁺ + d → p + p Below 21 MeV

NUCLEAR REACTIONS ²H(π⁺, p), E=3.7-20.5 MeV; measured absolute σ, σ(θ); deduced p-wave strength evidence.

doi: 10.1103/PhysRevC.47.21
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1993SM05      Phys.Rev. C48, R485 (1993)

L.C.Smith, R.C.Minehart, O.K.Baker, D.B.Day, K.L.Giovanetti, R.Lourie, R.M.Marshall, B.Milbrath, B.G.Ritchie, R.M.Sealock, D.Tedeschi, S.T.Thornton

Pion Absorption in ⁴He Above the Delta Resonance

NUCLEAR REACTIONS ⁴He(π⁺, 2p), E=500 MeV; measured σ(θ, E); deduced quasifree two-nucleon, four-body absorption. PWIA analysis, isobar-isobar model.

doi: 10.1103/PhysRevC.48.R485
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1992ME08      Phys.Rev.Lett. 69, 41 (1992)

Z.-E.Meziani, J.P.Chen, D.Beck, G.Boyd, L.M.Chinitz, D.B.Day, L.C.Dennis, G.E.Dodge, B.W.Filippone, K.L.Giovanetti, J.Jourdan, K.W.Kemper, T.Koh, W.Lorenzon, J.S.McCarthy, R.D.McKeown, R.G.Milner, R.C.Minehart, J.Morgenstern, J.Mougey, D.H.Potterveld, O.A.Rondon-Aramayo, R.M.Sealock, I.Sick, L.C.Smith, S.T.Thornton, R.C.Walker, C.Woodward

High Momentum Transfer R(T, L) Inclusive Response Functions for ^3,4He

NUCLEAR REACTIONS ^3,4He(e, e'X), E=0.9-4.3 GeV; measured σ(θ, E(e')); deduced longitudinal, transverse response functions. ^3,4He deduced Coulomb sum rule.

doi: 10.1103/PhysRevLett.69.41
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1991CH15      Phys.Rev.Lett. 66, 1283 (1991)

J.P.Chen, Z.E.Meziani, D.Beck, G.Boyd, L.M.Chinitz, D.B.Day, L.C.Dennis, G.Dodge, B.W.Filippone, K.L.Giovanetti, J.Jourdan, K.W.Kemper, T.Koh, W.Lorenzon, J.S.McCarthy, R.D.McKeown, R.G.Milner, R.C.Minehart, J.Morgenstern, J.Mougey, D.H.Potterveld, O.A.Rondon-Aramayo, R.M.Sealock, L.C.Smith, S.T.Thornton, R.C.Walker, C.Woodward

Longitudinal and Transverse Response Functions in ⁵⁶Fe(e, e') at Momentum Transfer Near 1 GeV/c

NUCLEAR REACTIONS ⁵⁶Fe(e, e'), E=0.9-4.3 GeV; measured longitudinal, transverse response functions. Model comparison.

doi: 10.1103/PhysRevLett.66.1283
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1991MU01      Phys.Rev. C43, 957 (1991)

S.Mukhopadhyay, S.Levenson, R.E.Segel, G.Garino, D.Geesaman, J.P.Schiffer, G.Stephans, B.Zeidman, E.Ungricht, H.Jackson, R.Kowalczyk, D.Ashery, E.Piasetzky, M.Moinester, I.Navon, L.C.Smith, R.C.Minehart, G.S.Das, R.R.Whitney, R.Mckeown, B.Anderson, R.Madey, J.Watson

Pion Absorption by ³He at the Δ-Resonance Energy

NUCLEAR REACTIONS ³He(π⁺, X), (π^-, X), E=165 MeV; measured σ(θ₁, θ₂) vs momentum following pion absorption; deduced absorption mechanism.

doi: 10.1103/PhysRevC.43.957
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1989SM03      Phys.Rev. C40, 1347 (1989)

L.C.Smith, R.C.Minehart, D.Ashery, E.Piasetzky, M.Moinester, I.Navon, D.F.Geesaman, J.P.Schiffer, G.Stephens, B.Zeidman, S.Levinson, S.Mukhopadhyay, R.E.Segel, B.Anderson, R.Madey, J.Watson, R.R.Whitney

Reaction ³He(π⁺, pp)p at T(π) = 350 and 500 MeV

NUCLEAR REACTIONS ³He(π⁺, 2p), E=350, 500 MeV; measured pp-coin, pp(φ), σ(θp₁) vs p₃ momentum; deduced pion absorption mechanism. Kinematically complete experiment. Impulse approximation model.

doi: 10.1103/PhysRevC.40.1347
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1986RU09      Int.J.Appl.Radiat.Isotop. 37, 1029 (1986)

A.R.Rutledge, L.V.Smith, J.S.Merritt

The Half-Lives of ⁴¹Ar and ¹¹¹In

RADIOACTIVITY ⁴¹Ar(β^-), ¹¹¹In(EC); measured T_1/2. 4πγ ionization chamber.

doi: 10.1016/0883-2889(86)90042-0
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1984BO02      Phys.Rev. C29, 182 (1984)

K.G.Boyer, W.J.Braithwaite, W.B.Cottingame, S.J.Greene, L.E.Smith, C.F.Moore, C.L.Morris, H.A.Thiessen, G.S.Blanpied, G.R.Burleson, J.F.Davis, J.S.McCarthy, R.C.Minehart, C.A.Goulding

Pion Elastic and Inelastic Scattering from ^40,42,44,48Ca and ⁵⁴Fe

NUCLEAR REACTIONS ^40,42,44,48Ca, ⁵⁴Fe(π⁺, π⁺'), (π^-, π^-'), E=116, 118, 292.5 MeV; measured σ(E(π)), σ(θ). ^40,42,44,48Ca, ⁵⁴Fe level deduced neutron density rms radii. DWIA analysis.

doi: 10.1103/PhysRevC.29.182
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1983RU04      Nucl.Instrum.Methods 206, 211 (1983)

A.R.Rutledge, L.V.Smith, J.S.Merritt

Experimental Study of Half-Life Determinations using ⁶⁰Co

RADIOACTIVITY ⁶⁰Co(β^-); measured T_1/2. 4π γ ionization chamber, 4π β-γ coincidence methods.

doi: 10.1016/0167-5087(83)91261-9
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1982ME04      Int.J.Appl.Radiat.Isotop. 33, 77 (1982)

J.S.Merritt, A.R.Rutledge, L.V.Smith

Measurement of the Probability for 909-keV γ-Ray Emission following the Decay of ⁸⁹Sr

RADIOACTIVITY ⁸⁹Sr; measured γ-emission probability following β-decay. 4π β counting.

doi: 10.1016/0020-708X(82)90210-1
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1981BO26      Phys.Rev. C24, 598 (1981)

K.G.Boyer, W.B.Cottingame, L.E.Smith, S.J.Greene, C.F.Moore, J.S.McCarthy, R.C.Minehart, J.F.Davis, G.R.Burleson, G.Blanpied, C.A.Goulding, H.A.Thiessen, C.L.Morris

Pion Inelastic Scattering to the Low-Lying States in ^42,44,48Ca: Determination of the neutron and proton multipole matrix elements

NUCLEAR REACTIONS ^42,44,48Ca(π⁺, π⁺), (π⁺, π⁺'), (π^-, π^-), (π^-, π^-'), E=180 MeV; measured σ(θ). ^40,42,48Ca levels deduced neutron, proton multipole matrix elements, M(E2), M(E3). DWIA analysis, collective, microscopic model from factors.

doi: 10.1103/PhysRevC.24.598
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1981SM02      Phys.Lett. 102B, 114 (1981)

L.G.Smith, E.Koets, A.H.Wapstra

The Mass-Difference ³T - ³He and the Neutrino Mass

ATOMIC PHYSICS ³H, ³He; measured mass difference. Discussed neutrino mass implications.

doi: 10.1016/0370-2693(81)91042-X
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1978MO01      Phys.Rev. C17, 227 (1978)

C.L.Morris, R.L.Boudrie, J.J.Kraushaar, R.J.Peterson, R.A.Ristinen, G.R.Smith, J.E.Bolger, W.J.Braithwaite, C.F.Moore, L.E.Smith

Pion-Induced Single-Nucleon Removal to Discrete Final States

NUCLEAR REACTIONS ⁷Li, ⁹Be, ^13,12C, ¹⁶O(π⁺, X), (π^-, X), E ≈ 180 MeV; measured σ(Eπ-)/σ(Eπ+).

doi: 10.1103/PhysRevC.17.227
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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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1978SM03      JOUR PYLBB 72B 176

G.R.Smith, R.L.Boudrie, J.J.Kraushaar, R.J.Peterson, R.A.Ristinen, C.L.Morris, J.E.Bolger, W.J.Braithwaite, C.F.Moore, L.E.Smith

Energy Dependence of π⁺ Induced Two- and Four-Nucleon Removal

NUCLEAR REACTIONS ¹²C, ¹⁶O(π⁺, X), E=75-290 MeV; measured σ(E), γ-yields.

1977MO12      Phys.Rev.Lett. 39, 1455 (1977)

C.L.Morris, H.A.Thiessen, W.J.Braithwaite, C.F.Moore, J.E.Bolger, L.E.Smith, R.J.Peterson, R.L.Boudrie, J.J.Kraushaar, R.A.Ristinen, G.R.Smith

Definitive Test of Outgoing-Nucleon Analog Charge Exchange Using the Reactions ¹²C(π⁺, πN)¹²C (4.44 and 15.11 MeV)

NUCLEAR REACTIONS ¹²C(π⁺, π⁺n), (π^-, π^-n), E=60-300 MeV; measured reaction products, Eγ, Iγ. ¹²C; deduced σ, nucleon charge exchange (p-n or n-p reactions between analog states) cannot explain the difference between the σ(π^-)/σ(π⁺) ratio.

doi: 10.1103/PhysRevLett.39.1455
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1977SM06      Phys.Lett. 72B, 176 (1977)

G.R.Smith, R.L.Boudrie, J.J.Kraushaar, R.J.Peterson, R.A.Ristinen, C.L.Morris, J.E.Bolger, W.J.Braithwaite, C.F.Moore, L.E.Smith

Energy Dependence of π⁺ Induced Two- and Four-Nucleon Removal

NUCLEAR REACTIONS ¹²C, ¹⁶O(π⁺, X), E=75-290 MeV; measured σ(E), γ-yields.

doi: 10.1016/0370-2693(77)90695-5
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1976BO32      Phys.Rev.Lett. 37, 1206 (1976)

J.E.Bolger, W.J.Braithwaite, J.J.Kraushaar, J.McGill, C.F.Moore, C.L.Morris, R.J.Peterson, R.A.Ristinen, G.Smith, L.E.Smith, H.A.Thiessen, J.Whitenton

Comparison of Neutron Removal from ⁷Li by π± with Free Pion-Nucleon Results

NUCLEAR REACTIONS ⁷Li(π^-, π^-n), (π⁺, π⁺n), E=50-290 MeV; measured σ(E).

doi: 10.1103/PhysRevLett.37.1206
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1975SM02      Phys.Rev. C11, 1392 (1975)

L.G.Smith, A.H.Wapstra

Masses of Isotopes of H, He, C, N, O, and F

ATOMIC MASSES ³H, ³He, ^13,14C, ^14,15N, ¹⁶O, ¹⁹F; measured atomic mass.

NUCLEAR REACTIONS ²H, ³He, ^12,13C, ¹⁴N(n, γ); calculated quadrupole moment.

doi: 10.1103/PhysRevC.11.1392
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1971SM01      Phys.Rev. C4, 22 (1971)

L.G.Smith

Measurements of Six Light Masses

ATOMIC MASSES ^1,2H, ¹⁴N, ¹⁶O, ^35,37Cl; measured mass differences.

doi: 10.1103/PhysRevC.4.22
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1958FR50      Phys.Rev. 109, 2214 (1958)

L.Friedman, L.G.Smith

Mass Difference T - He³ and the Mass of the Neutrino

doi: 10.1103/PhysRev.109.2214
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1958SM10      Phys.Rev. 111, 1606 (1958)

L.G.Smith

Measurements of Light Masses with the Mass Synchrometer

doi: 10.1103/PhysRev.111.1606
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1955CO58      Phys.Rev. 98, 1369 (1955)

T.Coor, D.A.Hill, W.F.Hornyak, L.W.Smith, G.Snow

Nuclear Cross Sections For 1.4-Bev Neutrons

NUCLEAR REACTIONS ¹H, ⁹Be, C, ²⁷Al, Cu, Sn, Pb, ²⁰⁹Bi, U(n, x), E=1.4 GeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 11087.

doi: 10.1103/PhysRev.98.1369
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11087.

1951SM64      Phys.Rev. 84, 842 (1951)

L.A.Smith, R.N.H.Haslam, J.G.V.Taylor

The Decay of Co⁶¹

doi: 10.1103/PhysRev.84.842
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1951SM73      Phys.Rev. 83, 1137 (1951)

L.W.Smith, P.G.Kruger

Thick Target Yields from the (d, n) Reaction at 10 Mev

NUCLEAR REACTIONS ⁹Be, B, C, ²⁷Al, Ni, Cu, Mo, ¹⁸¹Ta, W, Pt, ¹⁹⁷Au(d, n), E=10 MeV; measured reaction products; deduced thick target yields.

doi: 10.1103/PhysRev.83.1137
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2846.

Note: The following list of authors and aliases matches the search parameter L.Smith: , L.A.SMITH, L.C.SMITH, L.E.SMITH, L.G.SMITH, L.J.SMITH, L.V.SMITH, L.W.SMITH