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NSR database version of April 11, 2024.

Search: Author = R.Alarcon

Found 52 matches.

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2016BA29      Phys.Rev.Lett. 116, 242501 (2016)

M.J.Bales, R.Alarcon, C.D.Bass, E.J.Beise, H.Breuer, J.Byrne, T.E.Chupp, K.J.Coakley, R.L.Cooper, M.S.Dewey, S.Gardner, T.R.Gentile, D.He, H.P.Mumm, J.S.Nico, B.O'Neill, A.K.Thompson, F.E.Wietfeldt, for the RDK II Collaboration

Precision Measurement of the Radiative β Decay of the Free Neutron

RADIOACTIVITY 1NN(β-); measured decay products, Eγ, Iγ, Eβ, Iβ, Ep, Ip; deduced photon energy spectrum from neutron radiative decay branching ratio and its uncertainties. Comparison with theoretical calculations.

doi: 10.1103/PhysRevLett.116.242501
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2015GR20      Phys.Rev. B 91, 180301 (2015)

K.B.Grammer, R.Alarcon, L.Barron-Palos, D.Blyth, J.D.Bowman, J.Calarco, C.Crawford, K.Craycraft, D.Evans, N.Fomin, J.Fry, M.Gericke, R.C.Gillis, G.L.Greene, J.Hamblen, C.Hayes, S.Kucuker, R.Mahurin, M.Maldonado-Velazquez, E.Martin, M.McCrea, P.E.Mueller, M.Musgrave, H.Nann, S.I.Penttila, W.M.Snow, Z.Tang, W.S.Wilburn

Measurement of the scattering cross section of slow neutrons on liquid parahydrogen from neutron transmission

NUCLEAR REACTIONS H(n, X), E=0.0.000433313-0.0161166 eV; measured reaction products; deduced total and scattering σ.

doi: 10.1103/PhysRevB.91.180301
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14566.


2011BO21      Phys.Rev. C 84, 035206 (2011)

P.Bourgeois, Y.Sato, J.Shaw, R.Alarcon, A.M.Bernstein, W.Bertozzi, T.Botto, J.Calarco, F.Casagrande, M.O.Distler, K.Dow, M.Farkondeh, S.Georgakopoulos, S.Gilad, R.Hicks, M.Holtrop, A.Hotta, X.Jiang, A.Karabarbounis, J.Kirkpatrick, S.Kowalski, R.Milner, R.Miskimen, I.Nakagawa, C.N.Papanicolas, A.J.Sarty, S.Sirca, E.Six, N.F.Sparveris, S.Stave, E.Stiliaris, T.Tamae, G.Tsentalovich, C.Tschalaer, W.Turchinetz, Z.-L.Zhou, T.Zwart

Measurements of the generalized electric and magnetic polarizabilities of the proton at low Q2 using the virtual Compton scattering reaction

doi: 10.1103/PhysRevC.84.035206
Citations: PlumX Metrics


2011KI19      Phys.Rev. C 84, 028201 (2011)

J.M.Kirkpatrick, N.F.Sparveris, I.Nakagawa, A.M.Bernstein, R.Alarcon, W.Bertozzi, T.Botto, P.Bourgeois, J.Calarco, F.Casagrande, M.O.Distler, K.Dow, M.Farkhondeh, S.Georgakopoulos, S.Gilad, R.Hicks, A.Holtrop, A.Hotta, X.Jiang, A.Karabarbounis, S.Kowalski, R.Milner, R.Miskimen, C.N.Papanicolas, A.J.Sarty, Y.Sato, S.Sirca, J.Shaw, E.Six, S.Stave, E.Stiliaris, T.Tamae, G.Tsentalovich, C.Tschalaer, W.Turchinetz, Z.-L.Zhou, T.Zwart

Measurement of the partial cross sections σTT , σLT, and (σT + ϵσL) of the 1H(e, e'π+)n reaction in the Δ(1232) resonance

NUCLEAR REACTIONS 1H(e, e'π+) at Q2=0.127 GeV/c2; measured electron spectra using OHIPS spectrometer at MIT-Bates facility; deduced differential cross sections for Δ(1232) resonance. Comparison with predictions of MAID, DMT, Sato-Lee, and chiral EFT models.

doi: 10.1103/PhysRevC.84.028201
Citations: PlumX Metrics


2010CR03      Phys.Rev. C 82, 045211 (2010)

C.Crawford, T.Akdogan, R.Alarcon, W.Bertozzi, E.Booth, T.Botto, J.R.Calarco, B.Clasie, A.DeGrush, T.W.Donnelly, K.Dow, M.Farkhondeh, R.Fatemi, O.Filoti, W.Franklin, H.Gao, E.Geis, S.Gilad, D.Hasell, P.Karpius, M.Kohl, H.Kolster, T.Lee, E.Lomon, A.Maschinot, J.Matthews, K.McIlhany, N.Meitanis, R.Milner, J.Rapaport, R.Redwine, J.Seely, A.Shinozaki, A.Sindile, S.Sirca, E.Six, T.Smith, B.Tonguc, C.Tschalaer, E.Tsentalovich, W.Turchinetz, Y.Xiao, W.Xu, C.Zhang, Z.Zhou, V.Ziskin, T.Zwart

Role of mesons in the electromagnetic form factors of the nucleon

doi: 10.1103/PhysRevC.82.045211
Citations: PlumX Metrics


2007AL22      Eur.Phys.J. A 31, 588 (2007)

R.Alarcon, and the BLAST Collaboration

Nucleon form factors and the BLAST experiment

NUCLEAR REACTIONS 1,2H(polarized e, e'), (polarized e, e'p), (polarized e, e'n), (polarized e, e'π), E=850 MeV; measured particle spectra, asymmetries. 1n, 1H; deduced electric and magnetic form factors. Polarized targets.

doi: 10.1140/epja/i2006-10268-4
Citations: PlumX Metrics


2007AL48      Eur.Phys.J. A 32, 477 (2007)

R.Alarcon, and the BLAST Collaboration

Nucleon form factors and the BLAST experiment

doi: 10.1140/epja/i2006-10395-x
Citations: PlumX Metrics


2007CR01      Phys.Rev.Lett. 98, 052301 (2007)

C.B.Crawford, A.Sindile, T.Akdogan, R.Alarcon, W.Bertozzi, E.Booth, T.Botto, J.Calarco, B.Clasie, A.DeGrush, T.W.Donnelly, K.Dow, D.Dutta, M.Farkhondeh, R.Fatemi, O.Filoti, W.Franklin, H.Gao, E.Geis, S.Gilad, W.Haeberli, D.Hasell, W.Hersman, M.Holtrop, P.Karpius, M.Kohl, H.Kolster, T.Lee, A.Maschinot, J.Matthews, K.McIlhany, N.Meitanis, R.G.Milner, R.P.Redwine, J.Seely, A.Shinozaki, S.Sirca, E.Six, T.Smith, B.Tonguc, C.Tschalaer, E.Tsentalovich, W.Turchinetz, J.F.J.van den Brand, J.van der Laan, F.Wang, T.Wise, Y.Xiao, W.Xu, C.Zhang, Z.Zhou, V.Ziskin, T.Zwart

Measurement of the Proton's Electric to Magnetic Form Factor Ratio from 1H(pol)(e(pol), e'p)

NUCLEAR REACTIONS 1H(polarized e, e'p), E=high; measured asymmetries. 1H deduced electric to magnetic form factor ratios. Polarized target.

doi: 10.1103/PhysRevLett.98.052301
Citations: PlumX Metrics


2006BO29      Phys.Rev.Lett. 97, 212001 (2006)

P.Bourgeois, Y.Sato, J.Shaw, R.Alarcon, A.M.Bernstein, W.Bertozzi, T.Botto, J.Calarco, F.Casagrande, M.O.Distler, K.Dow, M.Farkhondeh, S.Georgakopoulos, S.Gilad, R.Hicks, M.Holtrop, A.Hotta, X.Jiang, A.Karabarbounis, J.Kirkpatrick, S.Kowalski, R.Milner, R.Miskimen, I.Nakagawa, C.N.Papanicolas, A.J.Sarty, S.Sirca, E.Six, N.F.Sparveris, S.Stave, E.Stiliaris, T.Tamae, G.Tsentalovich, C.Tschalaer, W.Turchinetz, Z.-L.Zhou, T.Zwart

Measurements of the Generalized Electric and Magnetic Polarizabilities of the Proton at Low Q2 Using the Virtual-Compton-Scattering Reaction

NUCLEAR REACTIONS 1H(e, e'), E=570-670 MeV; measured σ(E, θ), response functions. 1H deduced polarizability radii. Virtual Compton scattering.

doi: 10.1103/PhysRevLett.97.212001
Citations: PlumX Metrics


2005SP01      Phys.Rev.Lett. 94, 022003 (2005)

N.F.Sparveris, R.Alarcon, A.M.Bernstein, W.Bertozzi, T.Botto, P.Bourgeois, J.Calarco, F.Casagrande, M.O.Distler, K.Dow, M.Farkhondeh, S.Georgakopoulos, S.Gilad, R.Hicks, M.Holtrop, A.Hotta, X.Jiang, A.Karabarbounis, J.Kirkpatrick, S.Kowalski, R.Milner, R.Miskimen, I.Nakagawa, C.N.Papanicolas, A.J.Sarty, Y.Sato, S.Sirca, J.Shaw, E.Six, S.Stave, E.Stiliaris, T.Tamae, G.Tsentalovich, C.Tschalaer, W.Turchinetz, Z.-L.Zhou, T.Zwart

Investigation of the Conjectured Nucleon Deformation at Low Momentum Transfer

NUCLEAR REACTIONS 1H(e, e'π0), E=950 MeV; measured Ep, σ(θ). 1H deduced quadrupole to dipole amplitude ratios.

doi: 10.1103/PhysRevLett.94.022003
Citations: PlumX Metrics


2003AL32      Nucl.Phys. A721, 1075c (2003)

R.Alarcon

The MIT-Bates Large Acceptance Spectrometer Toroid

doi: 10.1016/S0375-9474(03)01288-0
Citations: PlumX Metrics


2003SP01      Phys.Rev. C 67, 058201 (2003)

N.F.Sparveris, R.Alarcon, D.Barkhuff, A.Bernstein, W.Bertozzi, J.Calarco, F.Casagrande, J.Chen, J.Comfort, M.O.Distler, G.Dodson, S.Dolfini, A.Dooley, K.Dow, M.Farkhondeh, S.Gilad, R.Hicks, M.Holtrop, A.Hotta, X.Jiang, N.Kaloskamis, A.Karabarbounis, S.Kowalski, C.Kunz, D.Margaziotis, C.Mertz, R.Milner, R.Miskimen, I.Nakagawa, C.N.Papanicolas, M.M.Pavan, G.Peterson, A.Ramirez, D.Rowntree, A.J.Sarty, J.Shaw, E.Six, S.Soong, E.Stiliaris, D.Tieger, C.Tschalaer, W.Turchinetz, C.Vellidis, G.A.Warren, A.Young, J.Zhao, Z.-L.Zhou, T.Zwart

Measurement of the RLT response function for π0 electroproduction at Q2=0.070 (GeV/c)2 in the N → Δ transition

NUCLEAR REACTIONS 1H(e, e'π0), E=0.82 GeV; measured response functions. Out-of-plane detection technique.

doi: 10.1103/PhysRevC.67.058201
Citations: PlumX Metrics


2002AL06      Nucl.Phys. A699, 376c (2002)

R.Alarcon

The South Hall Ring and the BLAST Detector

doi: 10.1016/S0375-9474(01)01523-8
Citations: PlumX Metrics


2002PA13      Phys.Rev.Lett. 88, 102302 (2002)

I.Passchier, L.D.van Buuren, D.Szczerba, R.Alarcon, Th.S.Bauer, D.J.Boersma, J.F.J.van den Brand, H.J.Bulten, R.Ent, M.Ferro-Luzzi, M.Harvey, P.Heimberg, D.W.Higinbotham, S.Klous, H.Kolster, J.Lang, B.L.Militsyn, D.Nikolenko, G.J.L.Nooren, B.E.Norum, H.R.Poolman, I.Rachek, M.C.Simani, E.Six, H.de Vries, K.Wang, Z.-L.Zhou

Spin-Momentum Correlations in Quasielastic Electron Scattering from Deuterium

NUCLEAR REACTIONS 2H(polarized e, e'p), E=720 MeV; measured proton, electron energy spectrum, (proton)(electron)-coin, spin correlation parameter vs missing momentum. Polarized target, comparison with theoretical results including different nucleon-nucleon potentials and S, D states.

doi: 10.1103/PhysRevLett.88.102302
Citations: PlumX Metrics


2002VA11      Phys.Rev.Lett. 89, 012001 (2002)

L.D.Van Buuren, D.Szczerba, R.Alarcon, D.J.Boersma, J.F.J.van den Brand, H.J.Bulten, R.Ent, M.Ferro-Luzzi, M.Harvey, P.Heimberg, D.W.Higinbotham, S.Klous, H.Kolster, J.Lang, B.L.Militsyn, D.Nikolenko, B.E.Norum, I.Passchier, H.R.Poolman, I.Rachek, M.C.Simani, E.Six, H.de Vries, Z.-L.Zhou

Spin-Dependent Electron-Proton Scattering in the Δ-Excitation Region

NUCLEAR REACTIONS 1H(polarized e, e'), E=720 MeV; measured σ(E, θ), spin correlation parameters. Polarized target, comparison with model predictions.

doi: 10.1103/PhysRevLett.89.012001
Citations: PlumX Metrics


2001ME08      Phys.Rev.Lett. 86, 2963 (2001)

C.Mertz, C.E.Vellidis, R.Alarcon, D.H.Barkhuff, A.M.Bernstein, W.Bertozzi, V.Burkert, J.Chen, J.R.Comfort, G.Dodson, S.Dolfini, K.Dow, M.Farkhondeh, J.M.Finn, S.Gilad, R.W.Gothe, X.Jiang, K.Joo, N.I.Kaloskamis, A.Karabarbounis, J.J.Kelly, S.Kowalski, C.Kunz, R.W.Lourie, J.I.McIntyre, B.D.Milbrath, R.Miskimen, J.H.Mitchell, C.N.Papanicolas, C.F.Perdrisat, A.J.Sarty, J.Shaw, S.-B.Soong, D.Tieger, C.Tschalaer, W.Turchinetz, P.E.Ulmer, S.Van Verst, G.A.Warren, L.B.Weinstein, S.Williamson, R.J.Woo, A.Young

Search for Quadrupole Strength in the Electroexcitation of the Δ+(1232)

NUCLEAR REACTIONS 1H(e, e'π0), E=719, 799 MeV; measured recoil protons σ(φ), longitudinal-transverse asymmetry and response; deduced quadrupole strength in Δ resonance excitation.

doi: 10.1103/PhysRevLett.86.2963
Citations: PlumX Metrics


2000AL19      Nucl.Phys. A663-664, 1111c (2000)

R.Alarcon, and the BLAST Collaboration

BLAST: A new tool for intermediate energy nuclear physics

doi: 10.1016/S0375-9474(99)00789-7
Citations: PlumX Metrics


2000HI09      Nucl.Instrum.Methods Phys.Res. A444, 557 (2000)

D.W.Higinbotham, R.Alarcon, Th.Bauer, D.J.Boersma, J.F.J.van den Brand, H.J.Bulten, L.D.van Buuren, R.Ent, M.Ferro-Luzzi, D.Geurts, M.Harvey, P.Heimberg, B.E.Norum, I.Passchier, H.R.Poolman, E.Six, M.F.M.Steenbakkers, D.Szczerba, H.de Vries

Recoil Detection with a Polarized 3He Target

NUCLEAR REACTIONS 3He(polarized e, e'), E=720 MeV; measured electron spectra, σ(Q2), asymmetry. 3He(polarized e, e'π0), (polarized e, e'π+)E=720 MeV; measured missing mass spectrum. 3He(e, e'd), (e, e'pd), (e, e'p), (e, e'2p), E=720 MeV; measured coincident scattered electron spectra. Polarized target.

doi: 10.1016/S0168-9002(99)01176-6
Citations: PlumX Metrics


2000PA22      Nucl.Phys. A663-664, 421c (2000)

I.Passchier, L.D.van Buuren, D.Szczerba, R.Alarcon, Th.S.Bauer, D.Boersma, J.F.J.van den Brand, H.J.Bulten, M.Ferro-Luzzi, D.W.Higinbotham, C.W.de Jager, S.Klous, H.Kolster, J.Lang, D.Nikolenko, G.J.Nooren, B.E.Norum, H.R.Poolman, I.Rachek, M.C.Simani, E.Six, H.de Vries, K.Wang, Z.-L.Zhou

The Charge Form Factor of the Neutron from 2H(pol)(e(pol), e'n)p

NUCLEAR REACTIONS 2H(polarized e, e'n), (polarized e, e'p), E=720 MeV; measured (particle)(electron)-coin, sideways spin-correlation parameter. 1n deduced charge form factor. Polarized target.

doi: 10.1016/S0375-9474(99)00673-9
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1999BO12      Phys.Rev.Lett. 82, 3755 (1999)

M.Bouwhuis, R.Alarcon, T.Botto, J.F.J.van den Brand, H.J.Bulten, S.Dolfini, R.Ent, M.Ferro-Luzzi, D.W.Higinbotham, C.W.de Jager, J.Lang, D.J.J.de Lange, N.Papadakis, I.Passchier, H.R.Poolman, E.Six, J.J.M.Steijger, N.Vodinas, H.de Vries, Z.-L.Zhou

Measurement of T20 in Elastic Electron-Deuteron Scattering

NUCLEAR REACTIONS 2H(e, e), E=704 MeV; measured T20 vs momentum transfer. Polarized target. Comparison with nonrelativistic calculation.

doi: 10.1103/PhysRevLett.82.3755
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1999DO30      Phys.Rev. C60, 064622 (1999)

S.M.Dolfini, R.O.Alarcon, H.Arenhovel, R.Beck, A.M.Bernstein, W.Bertozzi, W.Boeglin, S.Boffi, J.R.Comfort, D.Dale, G.Dodson, K.Dow, M.B.Epstein, M.Farkhondeh, S.Gilad, J.Gorgen, M.Holtrop, D.Jordan, W.Kim, S.Kowalski, R.Laszewski, J.Mandeville, D.J.Margaziotis, D.Martinez, T.McIlvain, R.Miskimen, C.Papanicolas, M.Radici, D.Tieger, W.Turchinetz, C.E.Vellidis, L.Weinstein, S.Williamson

Out-of-Plane Measurements of the Fifth Response Function of the Exclusive Electronuclear Response

NUCLEAR REACTIONS 2H, 12C(polarized e, e'p), E=560 MeV; measured coincidence yields, σ(θ), beam asymmetry; deduced unpolarized σ, fifth response function f'(LT). Magnetic spectrometers, out-of-plane measurements. DWIA calculations.

doi: 10.1103/PhysRevC.60.064622
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1999FE14      Nucl.Phys. (Supplement) A654, 1009c (1999)

M.Ferro-Luzzi, R.Alarcon, N.van Bakel, T.Bauer, D.Boersma, T.Botto, M.Bouwhuis, J.F.J.van den Brand, L.van Buuren, H.-J.Bulten, R.Ent, D.Geurts, M.Harvey, P.Heimberg, D.W.Higinbotham, C.W.de Jager, S.Klous, H.Kolster, J.Lang, B.Militsyn, B.E.Norum, I.Passchier, H.R.Poolman, M.C.Simani, E.Six, J.J.M.Steijger, D.Szczerba, H.de Vries, Z.L.Zhou

Electron Scattering at NIKHEF with Polarized Beam and Targets

NUCLEAR REACTIONS 2H(e, e'), E=900 MeV; measured tensor analyzing powers. 3He(polarized e, e'n), (polarized e, e'p), E=900 MeV; measured spin correlation parameters. Polarized targets, comparisons with model predictions.

doi: 10.1016/S0375-9474(00)88589-9
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1999PA23      Phys.Rev.Lett. 82, 4988 (1999)

I.Passchier, R.Alarcon, Th.S.Bauer, D.Boersma, J.F.J.van den Brand, L.D.van Buuren, H.J.Bulten, M.Ferro-Luzzi, P.Heimberg, D.W.Higinbotham, C.W.de Jager, S.Klous, H.Kolster, J.Lang, B.L.Militsyn, D.Nikolenko, G.J.L.Nooren, B.E.Norum, H.R.Poolman, I.Rachek, M.C.Simani, E.Six, D.Szczerba, H.de Vries, K.Wang, Z.-L.Zhou

Charge Form Factor of the Neutron from the Reaction 2H(pol)(e(pol), e'n)p

NUCLEAR REACTIONS 2H(polarized e, e'n), E=720 MeV; measured asymmetry, spin correlation parameter. 1n deduced charge form factor. Polarized gas target.

doi: 10.1103/PhysRevLett.82.4988
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1999ZH03      Phys.Rev.Lett. 82, 687 (1999)

Z.-L.Zhou, M.Bouwhuis, M.Ferro-Luzzi, E.Passchier, R.Alarcon, M.Anghinolfi, H.Arenhovel, R.van Bommel, T.Botto, J.F.J.van den Brand, H.J.Bulten, S.Choi, J.Comfort, S.M.Dolfini, R.Ent, C.Gaulard, D.W.Higinbotham, C.W.de Jager, E.Konstantinov, J.Lang, W.Leidemann, D.J.de Lange, M.A.Miller, D.Nikolenko, N.Papadakis, I.Passchier, H.R.Poolman, S.G.Popov, I.Rachek, M.Ripani, E.Six, J.J.M.Steijger, M.Taiuti, O.Unal, N.Vodinas, H.de Vries

Tensor Analyzing Powers for Quasielastic Electron Scattering from Deuterium

NUCLEAR REACTIONS 2H(e, e'p), E=565 MeV; measured missing momentum spectrum, tensor analyzing power vs θ. Comparison with model. Polarized target.

doi: 10.1103/PhysRevLett.82.687
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1998FE01      Nucl.Phys. A631, 190c (1998)

M.Ferro-Luzzi, R.Alarcon, T.Bauer, D.Boersma, T.Botto, M.Bouwhuis, J.F.J.van den Brand, H.J.Bulten, L.van Buuren, R.Ent, D.Geurts, M.Harvey, P.Heimberg, D.Higinbotham, C.W.de Jager, J.Lang, D.J.de Lange, B.Norum, I.Passchier, H.R.Poolman, M.van der Putte, E.Six, J.Steijger, D.Szczerba, O.Unal, H.de Vries, Z.-L.Zhou

Spin-Dependent Electromagnetic Response of Few-Body Systems

NUCLEAR REACTIONS 2H(e, e), (e, e'), E not given; measured tensor analyzing powers. Polarized targets.

doi: 10.1016/S0375-9474(98)00023-2
Citations: PlumX Metrics


1998HO20      Phys.Rev. C58, 3205 (1998)

M.Holtrop, D.Jordan, T.McIlvain, R.Alarcon, R.Beck, W.Bertozzi, V.Bhushan, W.Boeglin, J.P.Chen, D.Dale, G.Dodson, S.Dolfini, K.Dow, J.Dzengeleski, M.B.Epstein, M.Farkhondeh, S.Gilad, J.Gorgen, K.Joo, J.Kelsey, W.Kim, R.Laszewski, R.Lourie, J.Mandeville, D.J.Margaziotis, D.Martinez, R.Miskimen, C.Papanicolas, S.Penn, W.Sapp, A.J.Sarty, D.Tieger, C.Tschalaer, W.Turchinetz, G.Warren, L.Weinstein, S.Williamson

Measurement of the Interference Structure Function RLT for the 12C(e, e'p) Reaction in the Quasielastic Region

NUCLEAR REACTIONS 12C(e, e'p), E=576 MeV; measured ep-coin, σ(E, θ(e), θ(p)); deduced interference structure function R(LT) vs missing energy. HF-RPA calculations.

doi: 10.1103/PhysRevC.58.3205
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1998VA09      Nucl.Instrum.Methods Phys.Res. A402, 268 (1998)

J.F.J.van den Brand, R.Alarcon, Th.Bauer, D.Boersma, T.Botto, H.J.Bulten, L.van Buuren, R.Ent, M.Ferro-Luzzi, D.Geurts, M.Harvey, P.Heimberg, D.Higinbotham, C.W.de Jager, B.Norum, I.Passchier, H.R.Poolman, M.van der Putte, E.Six, J.Steijger, D.Szczerba, H.de Vries

Spin Effects in Medium-Energy Electron-3He Scattering

NUCLEAR REACTIONS 3He(polarized e, e'p), (polarized e, e'n), E not given; calculated asymmetry. Polarized target. Proposed experiment discussed.

doi: 10.1016/S0168-9002(97)00848-6
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1997VA08      Phys.Rev.Lett. 78, 1235 (1997)

J.F.J.van den Brand, H.J.Bulten, M.Ferro-Luzzi, Z.-L.Zhou, R.Alarcon, T.Botto, M.Bouwhuis, S.Dolfini, R.Ent, P.Heimberg, D.Higinbotham, C.W.de Jager, J.Lang, D.J.de Lange, G.J.Nooren, N.Papadakis, I.Passchier, H.R.Poolman, J.J.M.Steijger, O.Unal, N.Vodinas, H.de Vries

Evidence for Nuclear Tensor Polarization of Deuterium Molecules in Storage Cells

doi: 10.1103/PhysRevLett.78.1235
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1997ZW01      Nucl.Instrum.Methods Phys.Res. A384, 299 (1997)

T.Zwart, R.Alarcon, E.Booth, G.Dodson, S.Dolfini, K.Dow, M.Farkhondeh, K.Jacobs, K.Joo, S.Kowalski, S.Soong, J.Shaw, W.Turchinetz, E.Tsentalovich, B.Wojtsekhowski, A.Young

A Precise Electron Beam Energy Calibration for use in Nuclear Physics

doi: 10.1016/S0168-9002(96)00723-1
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1996FE03      Phys.Rev.Lett. 77, 2630 (1996)

M.Ferro-Luzzi, M.Bouwhuis, E.Passchier, Z.-L.Zhou, R.Alarcon, M.Anghinolfi, R.van Bommel, T.Botto, J.F.J.van den Brand, M.Buchholz, H.J.Bulten, S.Choi, J.Comfort, S.Dolfini, R.Ent, C.Gaulard, D.Higinbotham, C.W.de Jager, E.P.van Klaveren, E.Konstantinov, J.Lang, D.J.de Lange, M.A.Miller, D.Nikolenko, G.J.Nooren, N.Papadakis, I.Passchier, H.R.Poolman, S.G.Popov, I.Rachek, M.Ripani, E.Six, J.J.M.Steijger, M.Taiuti, O.Unal, N.Vodinas, H.de Vries

Measurement of Tensor Analyzing Powers for Elastic Electron Scattering from a Polarized 2H Target Internal to a Storage Ring

NUCLEAR REACTIONS 2H(e, e), E=565 MeV; measured absolute T20, T22 vs momentum transfer. Tensor polarized target.

doi: 10.1103/PhysRevLett.77.2630
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1996JO09      Phys.Rev.Lett. 76, 1579 (1996)

D.Jordan, T.McIlvain, R.Alarcon, R.Beck, W.Bertozzi, V.Bhushan, W.Boeglin, J.P.Chen, D.Dale, G.Dodson, S.Dolfini, K.Dow, J.Dzengeleski, M.B.Epstein, M.Farkhondeh, S.Gilad, J.Gorgen, M.Holtrop, K.Joo, J.Kelsey, W.Kim, R.Laszewski, R.Lourie, J.Mandeville, D.Margaziotis, D.Martinez, R.Miskimen, C.N.Papanicolas, S.Penn, W.Sapp, A.J.Sarty, D.Tieger, C.Tschalaer, W.Turchinetz, G.Warren, L.Weinstein, S.Williamson

Measurement of the Longitudinal, Transverse, and Longitudinal-Transverse Structure Functions in the 2H(e, e'p)n Reaction

NUCLEAR REACTIONS 2H(e, e'p), E=577, 292 MeV; measured σ(θ(e'), θ(np)) vs energy transfer; deduced longitudinal, transverse, longitudinal-transverse interference structure function.

doi: 10.1103/PhysRevLett.76.1579
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1995DO14      Phys.Rev. C51, 3479 (1995)

S.Dolfini, R.Alarcon, H.Arenhovel, R.Beck, A.Bernstein, W.Bertozzi, W.Boeglin, L.Cardman, J.Comfort, D.Dale, G.Dodson, K.Dow, M.Epstein, M.Farkhondeh, S.Gilad, J.Gorgen, M.Holtrop, D.Jordan, W.Kim, S.Kowalski, R.Laszewski, J.Mandeville, D.Margaziotis, D.Martinez, T.McIlvain, R.Miskimen, C.Papanicolas, D.Tieger, W.Turchinetz, L.Weinstein, S.Williamson

Out-of-Plane Quasielastic Scattering from Deuterium using Polarized Electrons

NUCLEAR REACTIONS 2H(polarized e, e'p), E=560 MeV; measured helicity independent coincidence σ(E, θ(e)) vs missing momentum, electron helicity asymmetry, A(e); deduced imaginary part of the longitudinal-transverse interference structure function f'(LT).

doi: 10.1103/PhysRevC.51.3479
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1994MA26      Phys.Rev.Lett. 72, 3325 (1994)

J.Mandeville, R.Alarcon, R.Beck, A.Bernstein, W.Bertozzi, W.Boeglin, S.Boffi, L.Cardman, J.Comfort, D.Dale, G.Dodson, S.Dolfini, K.Dow, M.Epstein, S.Gilad, J.Gorgen, M.Holtrop, D.Jordan, W.Kim, S.Kowalski, R.Laszewski, D.Margaziotis, D.Martinez, T.McIlvain, R.Miskimen, C.Papanicolas, M.Radici, D.Tieger, W.Turchinetz, L.Weinstein, S.Williamson

First Measurement of the Imaginary Part of the Transverse-Longitudinal Nuclear Response

NUCLEAR REACTIONS 12C(polarized e, e'p), E=560 MeV; measured asymmetry, differential σ, fifth structure function; deduced direct knockout, rescattering amplitudes interference.

doi: 10.1103/PhysRevLett.72.3325
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1994YE06      Phys.Rev. C50, 897 (1994)

Y.-F.Yen, B.Brinkmoller, D.Dehnhard, M.A.Franey, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.I.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti

Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance

NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=130-180 MeV; 13C(π+, π+), E=223 MeV; 13C(π-, π-), E=226 MeV; measured analyzing power A(y)(θ), σ(θ); deduced spin-flip transition quadrupole component role. Polarized, unpolarized target. DWIA calculations, optical, Δ-hole models.

doi: 10.1103/PhysRevC.50.897
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1993AL13      Phys.Rev. C48, 1431 (1993)

R.Alarcon, S.Choi, R.M.Laszewski, D.S.Dale

Isoscalar M1 Strength in Lead

NUCLEAR REACTIONS 206Pb(γ, γ), E=5.5-7 MeV; measured σ(Eγ). 206Pb deduced B(M1). Polarized photons.

doi: 10.1103/PhysRevC.48.1431
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1991AL10      Phys.Rev. C43, R2470 (1991)

R.Alarcon, P.L.Cole, D.S.Dale, P.T.Debevec, L.J.Morford

Statistical and Nonstatistical Neutron Decay of the Giant Electric Dipole Resonance of 208Pb

NUCLEAR REACTIONS 208Pb(γ, n), E=11.2-15.6 MeV; measured absolute σ(θn, En); deduced total σ, nonstatistical fraction. Hauser Feshbach model. Tagged photon, tof.

doi: 10.1103/PhysRevC.43.R2470
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1991YE01      Phys.Rev.Lett. 66, 1959 (1991)

Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti

Asymmetry Measurement of Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance

NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=132-226 MeV; measured analyzing power vs θ. Polarized target.

doi: 10.1103/PhysRevLett.66.1959
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1990YE06      J.Phys.(Paris), Colloq.C-6, 587 (1990)

Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.Gorgen, B.Ritchie, J.R.Tinsley, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, S.Hoibraten, M.Khandaker, S.Chakravarti

Pion Elastic Scattering from Polarized 13C in the Energy Region of the [3, 3] Resonance

NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=114-226 MeV; measured analyzing power vs θ. Polarized target. DWIA analyses.


1989AL01      Phys.Rev. C39, 324 (1989)

R.Alarcon, A.M.Nathan, S.F.LeBrun, S.D.Hoblit

Photon Scattering in the Giant Resonance Region of 24Mg, 28Si, and 32S

NUCLEAR REACTIONS 24Mg, 28Si, 32S(γ, γ'), E=17-28 MeV; measured σ(θ) vs E. 24Mg, 28Si, 32S deduced GDR properties.

doi: 10.1103/PhysRevC.39.324
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1989AL18      Phys.Rev. C40, R1097 (1989)

R.Alarcon, R.M.Laszewski, D.S.Dale

Giant M1 Resonance in 120Sn and the Quenching of the Nucleon Spin g Factors

NUCLEAR REACTIONS 120Sn(polarized γ, γ), E=7.3-9.3 MeV; measured σ(E), asymmetry; deduced nucleon spin g factors. 120Sn deduced B(M1). Tagged photon beam.

doi: 10.1103/PhysRevC.40.R1097
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1988IS03      Phys.In Med.Biol. 33, 315 (1988)

M.S.Islam, R.W.Finlay, J.S.Petler, J.Rapaport, R.Alarcon, J.Wierzbicki

Neutron Scattering Cross Sections and Partial Kerma Values for Oxygen, Nitrogen and Calcium at 18 < En < 60 MeV

NUCLEAR REACTIONS 14N, 16O, 40Ca(n, n), (n, n'), E=18-60 MeV; measured σ(θ); deduced optical model parameters, partial kerma factors. Previously acquired data included in analysis.


1988LA06      Phys.Rev.Lett. 60, 1202 (1988)

R.M.Laszewski, R.Alarcon

Laszewski and Alarcon Reply

NUCLEAR REACTIONS 90Zr(polarized γ, γ'), E not given; analyzed data, previous calculations. 90Zr deduced M1 transition strength distribution.

doi: 10.1103/PhysRevLett.60.1202
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1988LA23      Phys.Rev.Lett. 61, 1710 (1988)

R.M.Laszewski, R.Alarcon, D.S.Dale, S.D.Hoblit

Distribution of M1 Transitions in 208Pb

NUCLEAR REACTIONS 208Pb(polarized γ, γ'), E=5.8-7.6 MeV; measured σ(Eγ, E), asymmetry. 208Pb deduced B(M1) distribution. Linearly polarized tagged photon beam.

doi: 10.1103/PhysRevLett.61.1710
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1988MI07      Phys.Rev. C37, 1600 (1988)

R.A.Miskimen, A.M.Bernstein, G.Bernhardt, C.F.Williamson, B.A.Brown, R.Alarcon

Transition Densities in 30Si Studied by Electron Scattering and Coupled-Channel Calculations of 650 MeV Proton Scattering

NUCLEAR REACTIONS 30Si(p, p'), E=650 MeV; 30Si(e, e'), E not given; analyzed data. 30Si deduced transition densities.

doi: 10.1103/PhysRevC.37.1600
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1987AL02      Nucl.Phys. A462, 413 (1987)

R.Alarcon, J.Rapaport, R.W.Finlay

Nucleon Elastic Scattering from 40Ca between 11 and 48 MeV

NUCLEAR REACTIONS Ca(n, n), E=19, 21.7, 25.5 MeV; measured σ(θ); 40Ca(n, n), (p, p), E=11-48 MeV; analyzed σ(θ). Optical model.

doi: 10.1016/0375-9474(87)90397-6
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1987AL03      Nucl.Phys. A462, 445 (1987)

R.Alarcon, J.Rapaport

Neutron Inelastic Scattering from 40Ca at 21.7 and 25.5 MeV

NUCLEAR REACTIONS Ca(n, n'), E=21.7, 25.5 MeV; measured σ(θ), σ(En). 40Ca levels deduced deformation parameters, octupole moments, B(λ). Natural target. Coupled-channels analysis.

doi: 10.1016/0375-9474(87)90398-8
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1987AL16      Phys.Rev. C36, 954 (1987)

R.Alarcon, R.M.Laszewski, A.M.Nathan, S.D.Hoblit

Photon Scattering from 90Zr below Neutron Emission Threshold

NUCLEAR REACTIONS 90Zr(γ, γ), (γ, γ'), E=8.1-10.5 MeV; measured elastic, inelastic σ(E); deduced total σ(E). 90Zr deduced B(E1), GDR dominance.

doi: 10.1103/PhysRevC.36.954
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1987BI15      Phys.Rev. C36, 1293 (1987)

Y.Birenbaum, R.Alarcon, S.D.Hoblit, R.M.Laszewski, A.M.Nathan

Photon Scattering on 238U and the Interpretation of Near-Threshold Photofission Resonances

NUCLEAR REACTIONS 238U(γ, γ), E=4.8-6.4 MeV; measured σ(E, θ=135°); deduced total σ(E). 238U deduced fission transmission factors.

doi: 10.1103/PhysRevC.36.1293
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1987LA19      Phys.Rev.Lett. 59, 431 (1987)

R.M.Laszewski, R.Alarcon, S.D.Hoblit

Giant M1 Resonance in 90Zr

NUCLEAR REACTIONS 90Zr(polarized γ, γ), E=8.1-10.5 MeV; measured σ(E), γ asymmetry vs E. 90Zr deduced giant M1 transition strength distribution.

doi: 10.1103/PhysRevLett.59.431
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1986AL21      Nucl.Phys. A458, 502 (1986)

R.Alarcon, J.Rapaport

Neutron Elastic and Inelastic Scattering from 28Si, 32S and 34S

NUCLEAR REACTIONS Si, S, 34S(n, n), (n, n'), E=21.7 MeV; 34S(n, n), (n, n'), E=25.5 MeV. 28Si levels deduced β2, β4, multipole moments, B(λ). 32,34S levels deduced β, B(λ). Coupled-channels analysis. Natural Si, S targets.

doi: 10.1016/0375-9474(86)90048-5
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1985AL03      Phys.Rev. C31, 697 (1985)

R.Alarcon, J.Rapaport, R.T.Kouzes, W.H.Moore, B.A.Brown

Nucleon Scattering from 34S and the Relative Sign of Neutron and Proton Transition Matrix Elements for the (0 → 2+2) Transition

NUCLEAR REACTIONS 34S(p, p'), E=29.8 MeV; measured σ(Ep), σ(θ). 34S(n, n'), E=21.7 MeV; measured σ(θ); deduced optical model parameters, absolute σ. 34S level deduced σ(θ), neutron to proton matrix element ratios. Coupled-channels analysis.

doi: 10.1103/PhysRevC.31.697
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1984RA15      Nucl.Phys. A427, 332 (1984)

J.Rapaport, R.Alarcon, B.A.Brown, C.Gaarde, J.Larsen, C.D.Goodman, C.C.Foster, D.Horen, T.Masterson, E.Sugarbaker, T.N.Taddeucci

The 51V(p, n)51Cr Reaction at E(p) = 160 MeV

NUCLEAR STRUCTURE 40,42,44,46,48Ca, 50Ti, 51V, 52Cr, 54Fe; calculated B(M1). 22O, 23F, 24Ne, 25Na, 26Mg, 27Al, 28Si; calculated Gamow-Teller transition strength. Shell model.

NUCLEAR REACTIONS 51V(p, n), E=159.4 MeV; measured σ(θ), σ(En). 51Cr deduced levels, analogs, Gamow-Teller transition strengths. 50Ti, 51V(p, p'), (e, e'), (p, n), E not given; calculated Gamow-Teller transition strengths. Shell model.

doi: 10.1016/0375-9474(84)90089-7
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