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NSR database version of April 11, 2024.

Search: Author = H.J.Karwowski

Found 91 matches.

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2022LI18      Phys.Rev.Lett. 128, 132502 (2022)

X.Li, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, M.Emamian, G.Feldman, H.Gao, D.Godagama, H.W.Griesshammer, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, K.K.H.Leung, D.M.Markoff, J.A.McGovern, S.Mikhailov, R.E.Pywell, M.H.Sikora, J.A.Silano, R.S.Sosa, M.C.Spraker, G.Swift, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, Z.W.Zhao

Proton Compton Scattering from Linearly Polarized Gamma Rays

NUCLEAR REACTIONS 1H(polarized γ, γ'), E=83.4 MeV; measured reaction products, Eγ, Iγ; deduced σ(θ), electromagnetic dipole polarizabilities of the proton. The High Intensity Gamma-Ray Source facility at the Triangle Universities Nuclear Laboratory.

doi: 10.1103/PhysRevLett.128.132502
Citations: PlumX Metrics


2021LA03      Phys.Rev. C 103, 034311 (2021)

G.Laskaris, W.Ji, X.Yan, J.Zhou, W.R.Zimmerman, M.W.Ahmed, T.Averett, A.Deltuva, A.C.Fonseca, H.Gao, J.Golak, A.Kafkarkou, H.J.Karwowski, B.Lalremruata, J.Manfredi, J.M.Mueller, P.U.Sauer, R.Skibinski, A.P.Smith, M.B.Tsang, H.R.Weller, H.Witala, Y.K.Wu, Z.W.Zhao

First measurement of the asymmetry and the Gerasimov-Drell-Hearn integrand from the 3He((pol)(γ(pol), p)2H reaction at an incident photon energy of 29 MeV

NUCLEAR REACTIONS 3He(polarized γ, p)2H, E=29 MeV; measured Ep, Ip, p(θ), time-of-flight, spin-dependent asymmetry and total σ using a circularly polarized, monoenergetic γ-ray beam and a longitudinally polarized 3He target, and an array of depleted silicon surface barrier detectors at the High Intensity γ-ray Source (HIγS) facility at TUNL; deduced contribution from the two-body photo-disintegration to the 3He Gerasimov-Drell-Hearn (GDH) integrands, and compared with the state-of-the art three-nucleon system calculations.

doi: 10.1103/PhysRevC.103.034311
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0271.


2020LI10      Phys.Rev. C 101, 034618 (2020)

X.Li, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, M.Emamian, G.Feldman, H.Gao, D.Godagama, H.W.Griesshammer, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, K.K.H.Leung, D.Markoff, S.Mikhailov, R.E.Pywell, M.H.Sikora, J.A.Silano, R.S.Sosa, M.C.Spraker, G.Swift, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, Z.W.Zhao

Compton scattering from 4He at the TUNL HIγS facility

NUCLEAR REACTIONS 4He(polarized γ, γ), E=81.3 MeV, 100% circularly and linearly polarized γ-ray beam via Compton backscattering from HiγS at TUNL; measured Compton scattered photons at different angles, time-of-flight spectra using an array of large NaI(Tl) detectors; deduced differential σ(θ). Comparison with previous experimental data from Lund at Eγ=87 MeV.

doi: 10.1103/PhysRevC.101.034618
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0259.


2020MU07      Phys.Rev. C 101, 055801 (2020)

M.Munch, C.Matei, S.D.Pain, M.T.Febbraro, K.A.Chipps, H.J.Karwowski, C.Aa.Diget, A.Pappalardo, S.Chesnevskaya, G.L.Guardo, D.Walter, D.L.Balabanski, F.D.Becchetti, C.R.Brune, K.Y.Chae, J.Frost-Schenk, M.J.Kim, M.S.Kwag, M.La Cognata, D.Lattuada, R.G.Pizzone, G.G.Rapisarda, G.V.Turturica, C.A.Ur, Y.Xu

Measurement of the 7Li(γ, t)4He ground-state cross section between Eγ = 4.4. and 10 MeV

NUCLEAR REACTIONS 7Li(γ, t), E=4.4-10 MeV from High Intensity Gamma-ray Source (HIγS) at TUNL; measured E(t), I(t), Eα, Iα, Eγ and Iγ, αt-coin, ground state σ(E) using the SIDAR silicon detector array. 3H(α, γ), E(cm)=0-7 MeV; deduced astrophysical S-factor from R-matrix analysis. Comparison with model predictions, and with previous experimental results. Relevance to primordial Li problem and the mirror α-capture reactions.

doi: 10.1103/PhysRevC.101.055801
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0260. Data from this article have been entered in the XUNDL database. For more information, click here.


2019BA10      Phys.Rev. C 99, 025802 (2019)

A.Banu, E.G.Meekins, J.A.Silano, H.J.Karwowski, S.Goriely

Photoneutron reaction cross section measurements on 94Mo and 90Zr relevant to the p-process nucleosynthesis

NUCLEAR REACTIONS 90Zr(γ, n), E=12-13.5 MeV; 94Mo(γ, n), E=9.5-13.5 MeV; measured Eγ, Iγ, E(n), I(n), and σ(E) using quasi-monochromatic, circularly polarized (aka unpolarized) high-intensity photon beam from HIγS-TUNL facility, 3He proportional counter array INVS for neutron detection, HPGe detector and thin plastic scintillator for γ detection; deduced γ-ray strength functions (γSF), and stellar reaction rates. Comparison with previous experimental results, and with Hauser-Feshbach statistical model calculations with D1M+QRPA E1 and M1 strengths, and with the GLO model. Relevance to p-process nucleosynthesis and impact on the photoneutron stellar reaction rates.

doi: 10.1103/PhysRevC.99.025802
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0248.


2019GA11      Phys.Rev.Lett. 122, 192501 (2019)

A.Gando, Y.Gando, T.Hachiya, M.Ha Minh, S.Hayashida, Y.Honda, K.Hosokawa, H.Ikeda, K.Inoue, K.Ishidoshiro, Y.Kamei, K.Kamizawa, T.Kinoshita, M.Koga, S.Matsuda, T.Mitsui, K.Nakamura, A.Ono, N.Ota, S.Otsuka, H.Ozaki, Y.Shibukawa, I.Shimizu, Y.Shirahata, J.Shirai, T.Sato, K.Soma, A.Suzuki, A.Takeuchi, K.Tamae, K.Ueshima, H.Watanabe, D.Chernyak, A.Kozlov, S.Obara, S.Yoshida, Y.Takemoto, S.Umehara, K.Fushimi, S.Hirata, B.E.Berger, B.K.Fujikawa, J.G.Learned, J.Maricic, L.A.Winslow, Y.Efremenko, H.J.Karwowski, D.M.Markoff, W.Tornow, T.O'Donnell, J.A.Detwiler, S.Enomoto, M.P.Decowski, J.Menendez, R.Dvornicky, F.Simkovic

Precision Analysis of the 136Xe Two-Neutrino ββ Spectrum in KamLAND-Zen and Its Impact on the Quenching of Nuclear Matrix Elements

RADIOACTIVITY 136Xe(2β-); measured decay products, Eβ, Iβ; deduced nuclear matrix elements.

doi: 10.1103/PhysRevLett.122.192501
Citations: PlumX Metrics

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


2018SI29      Phys.Rev. C 98, 054609 (2018)

J.A.Silano, H.J.Karwowski

Near-barrier photofission in 232Th and 238U

NUCLEAR REACTIONS 232Th, 238U, Pb, 2H(polarized γ, F), E=4.3-6.0 MeV; measured neutron and γ spectra, photofission neutron angular distributions and polarization asymmetries, photofission neutron multiplicities, and photofission σ(E) using 3He proportional counters for neutron detection at HIγS-TUNL facility. Comparison with previous experimental σ(E) data, ENDF/B-VIII.0 evaluation and several model predictions.

doi: 10.1103/PhysRevC.98.054609
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0239.


2017SI26      Phys.Rev. C 96, 055209 (2017)

M.H.Sikora, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, G.Feldman, H.Gao, H.W.Griesshammer, H.Hao, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, X.Li, D.M.Markoff, S.Mikhailov, V.Popov, R.E.Pywell, J.A.Silano, M.C.Spraker, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, W.Xiong, X.Yan, Z.W.Zhao

Compton scattering from 4He at 61 MeV

NUCLEAR REACTIONS 4He(γ, γ'), E=61 MeV; measured Eγ, Iγ, Compton scattering differential σ(θ) using NaI(Tl) detectors and liquid 4He target at HIγS facility at TUNL. Data interpreted using phenomenological model sensitive to the dipole isoscalar electromagnetic polarizabilities of the nucleon. Comparison with previous experimental data. Benchmarks for future calculations from effective field theories and lattice quantum chromodynamics.

doi: 10.1103/PhysRevC.96.055209
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0232.


2016AS01      Nucl.Phys. A946, 171 (2016)

K.Asakura, A.Gando, Y.Gando, T.Hachiya, S.Hayashida, H.Ikeda, K.Inoue, K.Ishidoshiro, T.Ishikawa, S.Ishio, M.Koga, S.Matsuda, T.Mitsui, D.Motoki, K.Nakamura, S.Obara, M.Otani, T.Oura, I.Shimizu, Y.Shirahata, J.Shirai, A.Suzuki, H.Tachibana, K.Tamae, K.Ueshima, H.Watanabe, B.D.Xu, H.Yoshida, A.Kozlov, Y.Takemoto, S.Yoshida, K.Fushimi, T.I.Banks, B.E.Berger, B.K.Fujikawa, T.O'Donnell, L.A.Winslow, Y.Efremenko, H.J.Karwowski, D.M.Markoff, W.Tornow, J.A.Detwiler, S.Enomoto, M.P.Decowski

Search for double-beta decay of 136Xe to excited states of 136Ba with the KamLAND-Zen experiment

doi: 10.1016/j.nuclphysa.2015.11.011
Citations: PlumX Metrics

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


2016GA30      Phys.Rev.Lett. 117, 082503 (2016)

A.Gando, Y.Gando, T.Hachiya, A.Hayashi, S.Hayashida, H.Iked a, K.Inoue, K.Ishidoshiro, Y.Karino, M.Koga, S.Matsuda, T.Mitsui, K.Nakamura, S.Obara, T.Oura, H.Ozaki, I.Shimizu, Y.Shirahata, J.Shirai, A.Suzuki, T.Takai, K.Tamae, Y.Teraoka, K.Ueshima, H.Watanabe, A.Kozlov, Y.Takemoto, S.Yoshida, K.Fushimi, T.I.Banks, B.E.Berger, B.K.Fujikawa, T.O'Donnell, L.A.Winslow, Y.Efremenko, H.J.Karwowski, D.M.Markoff, W.Tornow, J.A.Detwiler, S.Enomoto, M.P.Decowski

Search for Majorana Neutrinos Near the Inverted Mass Hierarchy Region with KamLAND-Zen

RADIOACTIVITY 136Xe(2β-); measured decay products, Eγ, Iγ, Eβ, Iβ; deduced neutrinoless decay T1/2 limit. Comparison with available data.

doi: 10.1103/PhysRevLett.117.082503
Citations: PlumX Metrics

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


2015LA22      Phys.Lett. B 750, 547 (2015)

G.Laskaris, X.Yan, J.M.Mueller, W.R.Zimmerman, W.Xiong, M.W.Ahmed, T.Averett, P.-H.Chu, A.Deltuva, C.Flower, A.C.Fonseca, H.Gao, J.Golak, J.N.Heideman, H.J.Karwowski, M.Meziane, P.U.Sauer, R.Skibinski, I.I.Strakovsky, H.R.Weller, H.Witala, Y.K.Wu

Measurement of the doubly-polarized 3He(pol)(γ(pol), n)pp reaction at 16.5 MeV and its implications for the GDH sum rule

NUCLEAR REACTIONS 3He(polarized γ, n), E=12.8, 14.7 MeV; measured reaction products, Eγ, Iγ, En, In; deduced σ(θ, E), σ, contribution from the three-body channel to the Gerasimov-Drell-Hearn (GDH) integrand. Comparison with available data, Monte Carlo simulations using GEANT4.

doi: 10.1016/j.physletb.2015.09.065
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0212.


2015MU09      Phys.Rev. C 92, 034604 (2015)

J.M.Mueller, M.W.Ahmed, B.J.Davis, H.J.Karwowski, D.M.Markoff, L.S.Myers, M.C.Spraker, S.Stave, J.R.Tompkins, H.R.Weller, W.R.Zimmerman

Polarization asymmetries in the 9Be (γ, n0)reaction

NUCLEAR REACTIONS 9Be(polarized γ, n), E=5.5-15.5 MeV from High Intensity γ-ray Source (HIγS) at Duke University and TUNL; measure neutron spectra, time-of-flight spectrum, neutron yields parallel and perpendicular to the plane of beam polarization, polarization asymmetries using nearly 100% linearly polarized and monoenergetic γ-ray beam. Comparison with direct capture calculations using only E1 contributions. Relevance to new method of assaying special nuclear materials (SNM).

doi: 10.1103/PhysRevC.92.034604
Citations: PlumX Metrics


2014AN13      Phys.Rev. C 90, 054315 (2014)

C.T.Angell, R.Hajima, T.Hayakawa, T.Shizuma, H.J.Karwowski, J.Silano

Validating resonance properties using nuclear resonance fluorescence

NUCLEAR REACTIONS 27Al(polarized γ, γ'), E=2.6-3.2 MeV; measured Eγ, Iγ, integrated cross section for the 3.004-MeV level in 27Al at HIγS-TUNL facility; 27Al; deduced level spin, validation procedure of spectroscopic properties of a resonance.

doi: 10.1103/PhysRevC.90.054315
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0198. Data from this article have been entered in the XUNDL database. For more information, click here.


2014LA04      Phys.Rev. C 89, 024002 (2014)

G.Laskaris, Q.Ye, B.Lalremruata, Q.J.Ye, M.W.Ahmed, T.Averett, A.Deltuva, D.Dutta, A.C.Fonseca, H.Gao, J.Golak, M.Huang, H.J.Karwowski, J.M.Mueller, L.S.Myers, C.Peng, B.A.Perdue, X.Qian, P.U.Sauer, R.Skibinski, S.Stave, J.R.Tompkins, H.R.Weller, H.Witala, Y.K.Wu, Y.Zhang, W.Zheng

Spin-dependent cross sections from the three-body photodisintegration of 3He at incident energies of 12.8 and 14.7 MeV

NUCLEAR REACTIONS 3He(polarized γ, n), E=12.8, 14.7 MeV; measured time-of-flight spectra, γ spectra, and neutron spectra from three-body breakup of 3He using 16 liquid scintillator detectors, spin-dependent double-differential σ(E, θ) at HiγS-TUNL facility. Monoenergetic circularly polarized γ beam, and longitudinally polarized 3He target. Comparison with previous experimental results, and with theoretical calculations.

doi: 10.1103/PhysRevC.89.024002
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0181.


2014MU01      Phys.Rev. C 89, 034615 (2014)

J.M.Mueller, M.W.Ahmed, R.H.France, M.S.Johnson, H.J.Karwowski, L.S.Myers, J.Randrup, M.H.Sikora, M.C.Spraker, S.Stave, J.R.Tompkins, R.Vogt, H.R.Weller, C.S.Whisnant, W.R.Zimmerman

Prompt neutron polarization asymmetries in photofission of 232Th, 233, 235, 238U, 237Np, and 239, 240Pu

NUCLEAR REACTIONS 232Th, 233,235,238U, 237Np, 239,240Pu(polarized γ, F), E=5.3-7.6 MeV; measured E(n), I(n), time-of flight spectrum, angular distribution, and polarization asymmetry of prompt neutrons generated by fission, θ(fragment) at HIγS-TUNL facility; deduced angular distribution coefficients b and c, and compared with predicted values from FREYA computer code of event-by-event Monte Carlo prompt neutron+γ-ray emission calculation. Discussed differences in polarization asymmetries between the even-even actinides and odd-A actinides.

doi: 10.1103/PhysRevC.89.034615
Citations: PlumX Metrics


2013CS01      Acta Phys.Pol. B44, 643 (2013)

L.Csige, D.M.Filipescu, J.Gulyas, M.Gunther, D.Habs, H.J.Karwowski, A.Krasznahorkay, G.C.Rich, P.G.Thirolf

Photofission of 238U Induced by a Quasi-monochromatic, Compton Backscattered γ Beam

NUCLEAR REACTIONS 238U(γ, F), E=4.7-6 MeV; measured fission products; deduced σ. Comparison with EMPIRE 3.1 calculations, available data.

doi: 10.5506/APhysPolB.44.643
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0179.


2013CS03      Phys.Rev. C 87, 044321 (2013)

L.Csige, D.M.Filipescu, T.Glodariu, J.Gulyas, M.M.Gunther, D.Habs, H.J.Karwowski, A.Krasznahorkay, G.C.Rich, M.Sin, L.Stroe, O.Tesileanu, P.G.Thirolf

Exploring the multihumped fission barrier of 238U via sub-barrier photofission

NUCLEAR REACTIONS 238U(γ, F), E=4.7-6.0 MeV; measured Eγ, Iγ, photofission σ(E) at the HIγS facility. 238U; deduced triple-humped fission barrier parameters using EMPIRE-3.1 computer code calculations. Comparison with previous experimental studies.

doi: 10.1103/PhysRevC.87.044321
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0179.


2013KA48      Nucl.Instrum.Methods Phys.Res. B316, 48 (2013)

A.Kafkarkou, M.W.Ahmed, P.H.Chu, R.H.France, H.J.Karwowski, D.P.Kendellen, G.Laskaris, I.Mazumdar, J.M.Mueller, L.S.Myers, R.M.Prior, M.H.Sikora, M.C.Spraker, H.R.Weller, W.R.Zimmerman

Study of the 10B(p, α) reaction between 2.1 and 6.0 MeV

NUCLEAR REACTIONS 10B(p, α), E=2.1-6 MeV; measured reaction products, Eα, Iα; deduced σ(θ), S-factors and their uncertainties. Comparison with available data.

doi: 10.1016/j.nimb.2013.08.029
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2072.


2013LA14      Phys.Rev.Lett. 110, 202501 (2013)

G.Laskaris, Q.Ye, B.Lalremruata, Q.J.Ye, M.W.Ahmed, T.Averett, A.Deltuva, D.Dutta, A.C.Fonseca, H.Gao, J.Golak, M.Huang, H.J.Karwowski, J.M.Mueller, L.S.Myers, C.Peng, B.A.Perdue, X.Qian, P.U.Sauer, R.Skibinski, S.Stave, J.R.Tompkins, H.R.Weller, H.Witala, Y.K.Wu, Y.Zhang, W.Zheng

First Measurements of Spin-Dependent Double-Differential Cross Sections and the Gerasimov-Drell-Hearn Integrand from 3He(pol) (γ(pol), n)pp at Incident Photon Energies of 12.8 and 14.7 MeV

NUCLEAR REACTIONS 3He(polarized γ, n), E=12.8, 14.7 MeV; measured reaction products, En, In; deduced σ, σ(θ, E) and their uncertainties, contributions from the three-body photodisintegration to the 3He Gerasimov-Drell-Hearn integrand. Comparison with available data.

doi: 10.1103/PhysRevLett.110.202501
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0181.


2012AN13      Phys.Rev. C 86, 051302 (2012); Erratum Phys.Rev. C 91, 039901 (2015)

C.T.Angell, S.L.Hammond, H.J.Karwowski, J.H.Kelley, M.Krticka, E.Kwan, A.Makinaga, G.Rusev

Evidence for radiative coupling of the pygmy dipole resonance to excited states

NUCLEAR REACTIONS 142Nd(γ, n), E=9.86-13.3 MeV; 142Nd(polarized γ, γ'), E=4.2-9.7 MeV; measured Eγ, Iγ, branching ratio, σ(E) using High Intensity γ-ray Source (HIγS) at TUNL for (γ, γ'), and quasimonoenergetic γ-ray source at Tsukuba; deduced two distinct PDR peaks. Comparison with statistical-model calculations. Violation of Brink hypothesis.

doi: 10.1103/PhysRevC.86.051302
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2403.


2012AR01      Phys.Rev. C 85, 044605 (2012)

C.W.Arnold, T.B.Clegg, C.Iliadis, H.J.Karwowski, G.C.Rich, J.R.Tompkins, C.R.Howell

Cross-section measurement of 9Be(γ, n)8Be and implications for α+α+n → 9Be in the r process

NUCLEAR REACTIONS 9Be(γ, n)8Be, E=1.5-5.2 MeV; measured neutron spectra, Eγ, σ(E) using HIγS facility at TUNL. 9Be; deduced resonance energies, neutron and gamma widths, B(E1), B(M1), neutron branching ratios. Deduced astrophysical reaction rate for 4He(αn, γ)9Be reaction for r-process nucleosynthesis sites. Comparison with previous studies using (γ, n) and (e, e') reactions.

doi: 10.1103/PhysRevC.85.044605
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0171. Data from this article have been entered in the XUNDL database. For more information, click here.


2012HA12      Phys.Rev. C 85, 044302 (2012)

S.L.Hammond, A.S.Adekola, C.T.Angell, H.J.Karwowski, E.Kwan, G.Rusev, A.P.Tonchev, W.Tornow, C.R.Howell, J.H.Kelley

Dipole response of 238U to polarized photons below the neutron separation energy

NUCLEAR REACTIONS 238U(polarized γ, γ'), E=2.0-6.2 MeV; measured Eγ, Iγ, γ(θ), γ(linear pol), integrated cross sections using HIγS facility at TUNL. 238U; deduced levels, J, π, multipolarity, widths, branching ratios, B(M1), B(E1), total γ-ray interaction cross section for E1. Systematics of E1 and M1 strengths for 232Th, 236,238U. Comparison with QRPA calculations.

doi: 10.1103/PhysRevC.85.044302
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0170. Data from this article have been entered in the XUNDL database. For more information, click here.


2012MU01      Phys.Rev. C 85, 014605 (2012)

J.M.Mueller, M.W.Ahmed, B.Davis, J.M.Hall, S.S.Henshaw, M.S.Johnson, H.J.Karwowski, D.Markoff, L.S.Myers, B.A.Perdue, S.Stave, J.R.Tompkins, M.J.Tuffley, H.R.Weller

Measurement of prompt neutron polarization asymmetries in photofission of 235, 238U, 239Pu, and 232Th

NUCLEAR REACTIONS 232Th, 235,238U, 239Pu(polarized γ, F), E=5.6-7.3 MeV; measured neutron spectra, prompt fission neutron angular distributions polarization asymmetries using High Intensity γ-ray Source (HIγS). Comparison with simplified model of photofission.

doi: 10.1103/PhysRevC.85.014605
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0166.


2011AD02      Phys.Rev. C 83, 034615 (2011)

A.S.Adekola, C.T.Angell, S.L.Hammond, A.Hill, C.R.Howell, H.J.Karwowski, J.H.Kelley, E.Kwan

Discovery of low-lying E1 and M1 strengths in 232Th

NUCLEAR REACTIONS 232Th(γ, γ'), E=2-4 MeV; measured Eγ, Iγ, γγ(θ), integrated σ using HIγS facility; deduced widths. 232Th; deduced levels, J, π, multipolarity, B(M1), B(E1), branching ratios. Comparison of scissors mode summed B(M1) strengths with those in 232Th, 235,236,238U, and with predictions of quasiparticle random-phase approximation (QRPA).

doi: 10.1103/PhysRevC.83.034615
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0159. Data from this article have been entered in the XUNDL database. For more information, click here.


2011KW01      Phys.Rev. C 83, 041601 (2011)

E.Kwan, G.Rusev, A.S.Adekola, F.Donau, S.L.Hammond, C.R.Howell, H.J.Karwowski, J.H.Kelley, R.S.Pedroni, R.Raut, A.P.Tonchev, W.Tornow

Discrete deexcitations in 235U below 3 MeV from nuclear resonance fluorescence

NUCLEAR REACTIONS 235U(γ, γ'), E=1.6-3.0 MeV; measured Eγ, Iγ, γγ-coin, integrated cross sections, and widths using HIγS facility. 235U; deduced levels, J, π, branching ratios. Comparison with quasiparticle random-phase approximation in deformed basis for dipole transitions.

doi: 10.1103/PhysRevC.83.041601
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0161. Data from this article have been entered in the XUNDL database. For more information, click here.


2011TO06      Phys.Lett. B 702, 121 (2011)

W.Tornow, H.J.Karwowski, J.H.Kelley, R.Raut, G.Rusev, S.C.Stave, A.P.Tonchev, A.Deltuva, A.C.Fonseca, L.E.Marcucci, M.Viviani, A.Kievsky, J.Golak, R.Skibinski, H.Witala, R.Schiavilla

Two-body photodisintegration of 3He between 7 and 16 MeV

NUCLEAR REACTIONS 3He(γ, p), E=7-16 MeV; measured reaction products, Ep, Ip; deduced σ. Comparison with theoretical calculations and experimental data.

doi: 10.1016/j.physletb.2011.06.080
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2011TO10      Phys.Rev. C 84, 044331 (2011)

J.R.Tompkins, C.W.Arnold, H.J.Karwowski, G.C.Rich, L.G.Sobotka, C.R.Howell

Measurements of the 48Ca(γ, n) reaction

NUCLEAR REACTIONS 48Ca(polarized γ, n), E=9.5-15.3 MeV; measured E(n), I(n), Eγ, excitation functions, cross section; deduced B(M1) for 10.23 MeV resonance. High-intensity γ-ray source at TUNL. Comparison with previous studies, and with extended random-phase approximation calculations.

doi: 10.1103/PhysRevC.84.044331
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2010DA18      Phys.Rev. C 82, 034002 (2010)

T.V.Daniels, C.W.Arnold, J.M.Cesaratto, T.B.Clegg, A.H.Couture, H.J.Karwowski, T.Katabuchi

Spin-correlation coefficients and phase-shift analysis for p+3He elastic scattering

NUCLEAR REACTIONS 3He(polarized p, p), E=2-6 MeV; measured Ep, Ip, analyzing powers; deduced phase shifts, spin-correlation coefficients using polarized 3He target. Comparison with theoretical calculations using realistic nucleon-nucleon potential models.

doi: 10.1103/PhysRevC.82.034002
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2009HU09      Phys.Rev. C 80, 014603 (2009)

A.Hutcheson, C.Angell, J.A.Becker, A.S.Crowell, D.Dashdorj, B.Fallin, N.Fotiades, C.R.Howell, H.J.Karwowski, T.Kawano, J.H.Kelley, E.Kwan, R.A.Macri, R.O.Nelson, R.S.Pedroni, A.P.Tonchev, W.Tornow

Cross sections for 238U(n, n'γ) and 238U(n, 2nγ) reactions at incident neutron energies between 5 and 14 MeV

NUCLEAR REACTIONS 238U(n, n'γ), (n, 2nγ), E=5-14 MeV; measured Eγ, yields, σ and excitation functions. Comparison with existing data and calculations using the GNASH and TALYS Hauser-Feshbach statistical-model codes.

doi: 10.1103/PhysRevC.80.014603
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2008EL09      Phys.Rev. C 78, 064303 (2008); Erratum Phys.Rev. C 88, 029903 (2013)

E.Elhami, J.N.Orce, M.Scheck, S.Mukhopadhyay, S.N.Choudry, M.T.McEllistrem, S.W.Yates, C.Angell, M.Boswell, B.Fallin, C.R.Howell, A.Hutcheson, H.J.Karwowski, J.H.Kelley, Y.Parpottas, A.P.Tonchev, W.Tornow

Experimental study of the low-lying structure of 94Zr with the (n, n'γ) reaction

NUCLEAR REACTIONS 94Zr(n, n'γ), E=2.5-4.0 MeV; measured Eγ, Iγ, γγ-coin, angular distributions, half-lives by Doppler shift attenuation; deduced levels, J, π, multipolarities, mixing ratios, B(M1), B(E2).90,92,96,98,100,102Zr, 96Ru, 94,96Mo; systematics. Comparison with IBA and shell model calculations.

doi: 10.1103/PhysRevC.78.064303
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2008TO06      Phys.Rev. C 77, 054610 (2008)

A.P.Tonchev, C.T.Angell, M.Boswell, A.S.Crowell, B.Fallin, S.Hammond, C.R.Howell, A.Hutcheson, H.J.Karwowski, J.H.Kelley, R.S.Pedroni, W.Tornow, J.A.Becker, D.Dashdorj, J.Kenneally, R.A.Macri, M.A.Stoyer, C.Y.Wu, E.Bond, M.B.Chadwick, J.Fitzpatrick, T.Kawano, R.S.Rundberg, A.Slemmons, D.J.Vieira, J.B.Wilhelmy

Measurement of the 241Am(n, 2n) reaction cross section from 7.6 MeV to 14.5 MeV

NUCLEAR REACTIONS 241Am(n, 2n), E=7.6-14.5 MeV; measured Eγ, Iγ, neutron time-of-flight spectra, σ, excitation functions. Comparison with evaluated data in ENDF/B-VII and JENDL-3.3.

doi: 10.1103/PhysRevC.77.054610
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2006FI06      Phys.Rev. C 74, 034001 (2006)

B.M.Fisher, C.R.Brune, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, T.C.Black, M.Viviani, A.Kievsky, S.Rosati

Proton-3He elastic scattering at low energies

NUCLEAR REACTIONS 3He(p, p), (polarized p, p), E=0.99, 1.59, 2.24, 3.11, 4.02 MeV; measured σ(θ), Ay(θ). Four-body variational calculations with realistic two- and three-body interactions.

doi: 10.1103/PhysRevC.74.034001
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1467.


2006LE19      Phys.Rev. C 73, 045801 (2006)

D.S.Leonard, H.J.Karwowski, C.R.Brune, B.M.Fisher, E.J.Ludwig

Precision measurements of 2H(d, p)3H and 2H(d, n)3He total cross sections at Big Bang nucleosynthesis energies

NUCLEAR REACTIONS 2H(d, p), (d, n), E=120-650 keV; measured Ep, En, σ(E, θ); deduced integrated σ. Astrophysical implications discussed.

doi: 10.1103/PhysRevC.73.045801
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1499.


2004BR08      Phys.Rev. C 69, 024608 (2004)

B.Braizinha, C.R.Brune, A.M.Eiro, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, F.D.Santos, I.J.Thompson

Resonant and direct components in the 3He(d, p)4He reaction at low energies

NUCLEAR REACTIONS 3He(polarized d, p), E=0.52, 0.89, 1.49 MeV; measured σ(θ=0°), analyzing power; deduced scattering matrix elements.

doi: 10.1103/PhysRevC.69.024608
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2003KE05      Phys.Rev. C 67, 044604 (2003)

N.Keeley, T.L.Drummer, E.E.Bartosz, C.R.Brune, P.D.Cathers, M.Fauerbach, H.J.Karwowski, K.W.Kemper, B.Kozlowska, E.J.Ludwig, F.Marechal, A.J.Mendez, E.G.Myers, D.Robson, K.Rusek, K.D.Veal

Multistep processes in the 12C(6Li, d) stripping reaction

NUCLEAR REACTIONS 12C(polarized 6Li, d), E=34, 50 MeV; measured σ(E, θ), analyzing powers; deduced multistep transfer contributions. Coupled reaction channels calculations.

doi: 10.1103/PhysRevC.67.044604
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2002FL03      Phys.Rev. C 66, 057601 (2002)

K.A.Fletcher, C.R.Brune, B.M.Fisher, R.P.Fitzgerald, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, R.C.Runkle, M.H.Wood, W.H.Geist, K.D.Veal, G.M.Hale

Kyy'(O°) for 3He(d, p)4He near the Jπ=3/2+ resonance

NUCLEAR REACTIONS 3He(polarized d, p), E=520, 890, 1490 keV; measured polarization transfer coefficient. 5Li deduced resonance.

doi: 10.1103/PhysRevC.66.057601
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2002WO05      Phys.Rev. C65, 034002 (2002)

M.H.Wood, C.R.Brune, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, A.Kievsky, S.Rosati, M.Viviani

Low-Energy p-d Scattering: High-Precision data, comparisons with theory, and phase-shift analyses

NUCLEAR REACTIONS 2H(polarized p, p), 1H(polarized d, d), E(cm)=667 keV; measured σ(θ), Ay(θ), other analyzing powers; deduced phase shift parameters. Comparison with NN and 3N model predictions.

doi: 10.1103/PhysRevC.65.034002
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0891.


2001BR12      Phys.Rev. C63, 044013 (2001)

C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, K.D.Veal, M.H.Wood, A.Kievsky, S.Rosati, M.Viviani

Proton-Deuteron Elastic Scattering at Low Energies

NUCLEAR REACTIONS 2H(polarized p, p), E=431.3-2000 keV; measured σ(θ), analyzing power vector and tensor components. Comparison with calculations using hyperspherical harmonic basis and different nuclear potentials.

doi: 10.1103/PhysRevC.63.044013
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2001BR22      Nucl.Phys. A688, 263c (2001)

C.R.Brune, J.Daly, R.Detwiler, B.Fisher, W.H.Geist, J.Gorres, H.J.Karwowski, R.W.Kavanagh, D.S.Leonard, P.Tischhauser, K.D.Veal, M.Wiescher

Using Sub-Coulomb α Transfer Reactions to Study the Low-Energy 12C(α, γ)16O S-Factor

NUCLEAR REACTIONS 12C(6Li, d), (7Li, t), E=2.7-7.0 MeV; measured Eγ, σ(θ), reduced α widths. 12C(α, γ), E=0-5 MeV; calculated E1 and E2 S-factors following R-matrix fits.

doi: 10.1016/S0375-9474(01)00711-4
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2001KI03      Phys.Rev. C63, 024005 (2001)

A.Kievsky, M.H.Wood, C.R.Brune, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, S.Rosati, M.Viviani

Evidence for Three Nucleon Force Effects in p-d Elastic Scattering

NUCLEAR REACTIONS 2H(p, p), E=1 MeV; measured σ(θ); deduced contribution from three-nucleon force. Comparisons with model predictions.

doi: 10.1103/PhysRevC.63.024005
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0891.


2001KI22      Nucl.Phys. A689, 349c (2001)

A.Kievsky, M.H.Wood, C.R.Brune, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, S.Rosati, M.Viviani

χ2 Analysis of p-d Differential Cross Sections at Low Energies

NUCLEAR REACTIONS 1H(d, d), E=1 MeV; measured σ(θ); deduced model parameters.

doi: 10.1016/S0375-9474(01)00852-1
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2001WO06      Nucl.Phys. A684, 549c (2001)

M.H.Wood, C.R.Brune, B.M.Fisher, H.J.Karwowski, A.Kievsky, D.S.Leonard, E.J.Ludwig, S.Rosati, M.Viviani

Low Energy P-D Elastic Scattering and the ' Ay Puzzle '

NUCLEAR REACTIONS 2H(polarized p, p), E(cm)=667 keV; measured σ(θ), Ay(θ), tensor analyzing powers. Comparisons with model predictions.

doi: 10.1016/S0375-9474(01)00390-6
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2000CR01      Phys.Rev. C61, 034006 (2000)

B.J.Crowe III, C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, K.D.Veal, A.C.Fonseca, G.M.Hale, K.A.Fletcher

Analyzing Powers for 2H(d(pol), d)2H at Deuteron Energies of 3.0, 4.75, and 6.0 MeV

NUCLEAR REACTIONS 2H(polarized d, d), E=3.0, 4.75, 6.0 MeV; measured tensor analyzing powers vs θ; deduced nucleon-nucleon p-wave contributions. R matrix parameterization, microscopic four-body calculations.

doi: 10.1103/PhysRevC.61.034006
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2000FL08      Nucl.Instrum.Methods Phys.Res. A455, 620 (2000)

K.A.Fletcher, W.H.Geist, C.R.Brune, B.M.Fisher, R.P.Fitzgerald, H.J.Karwowski, D.E.Kruse, D.S.Leonard, E.J.Ludwig, R.C.Runkle, K.D.Veal, M.H.Wood

A Proton Polarimeter for 3He(d, p)4He Polarization Transfer Studies

NUCLEAR REACTIONS 3He(d, p), E=430 keV; measured proton polarization, effective analyzing power vs Ep. Comparison with Monte Carlo simulation.

doi: 10.1016/S0168-9002(00)00569-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1348.


1999BL26      Phys.Lett. 471B, 103 (1999)

T.C.Black, H.J.Karwowski, E.J.Ludwig, A.Kievsky, S.Rosati, M.Viviani

Determination of Proton-Deuteron Scattering Lengths

NUCLEAR REACTIONS 2H(p, p), E(cm)=0.163-2 MeV; calculated σ(θ), doublet and quartet S-wave effective range function, phase shifts; deduced singularity in doublet S-wave effective range function. Three nucleon interaction.

doi: 10.1016/S0370-2693(99)01366-0
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1999GE19      Phys.Rev. C60, 054003 (1999); Erratum Phys.Rev. C67, 059904 (2003)

W.H.Geist, C.R.Brune, H.J.Karwowski, E.J.Ludwig, K.D.Veal, G.M.Hale

The 3He(d(pol), p)4He Reaction at Low Energies

NUCLEAR REACTIONS 3H(polarized d, p), E=60-641 keV; measured σ(E, θ), Ay(E, θ), Azz(E, θ), Ayy(E, θ), Axz(E, θ); deduced low-energy S-factor, electron screening potential. 5Li deduced levels, J, π. R-matrix analysis.

doi: 10.1103/PhysRevC.60.054003
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0594.


1999KA46      Acta Phys.Pol. B30, 1479 (1999)

H.J.Karwowski, C.R.Brune, W.H.Geist, E.J.Ludwig, K.D.Veal, M.H.Wood, A.Kievsky, S.Rosati, M.Viviani, T.C.Black

New Physics in p-d Elastic Scattering at Low Energies

NUCLEAR REACTIONS 2H(polarized p, p), E(cm)=0.163-2 MeV; 1H(polarized d, d), E(cm)=0.163-2 MeV; measured σ, vector and tensor analyzing powers; deduced NN potential features, role of 3-body force. Pair-Correlated Hyperspherical Harmonic Calculations.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0801.


1999VE11      Phys.Rev. C60, 064003 (1999)

K.D.Veal, C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, E.E.Bartosz, P.D.Cathers, T.L.Drummer, K.W.Kemper, A.M.Eiro, F.D.Santos, B.Kozlowska, H.J.Maier, I.J.Thompson

Determination of the Asymptotic D- to S-State Ratio for 6Li via (6Li(pol), d) Transfer Reactions

NUCLEAR REACTIONS 40Ca, 58Ni(polarized 6Li, d), E=34 MeV; measured deuteron spectra, σ(E, θ), Ay(θ), tensor analyzing powers. 6Li deduced asymptotic D- to S-state ratio. DWBA analysis.

doi: 10.1103/PhysRevC.60.064003
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1998BL05      Nucl.Phys. A631, 680c (1998)

T.-C.Black, H.-J.Karwowski, E.-J.Ludwig, A.Kievsky, S.Rosati, M.Viviani

An Energy-Dependent Phase Shift Analysis of Low-Energy Proton-Deuteron Elastic Scattering

doi: 10.1016/S0375-9474(98)00090-6
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1998BR10      Phys.Rev. C57, 3437 (1998)

C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, K.D.Veal

9Be(p(pol), d)8Be and 9Be(p(pol), α)6Li Reactions at Low Energies

NUCLEAR REACTIONS 9Be(polarized p, d), (polarized p, α), E=77-321 keV; measured σ(θ), A(y)(θ); deduced reaction mechanism. R-matrix, DWBA analyses. Implications for stellar reaction rates discussed.

doi: 10.1103/PhysRevC.57.3437
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1998BR11      Phys.Lett. 428B, 13 (1998)

C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, K.D.Veal, M.H.Wood, A.Kievsky, S.Rosati, M.Viviani

Possible Three-Nucleon Force Effects in D-P Scattering at Low Energies

NUCLEAR REACTIONS 2H(polarized p, p), E(cm)=432 keV; measured A(y)(θ), iT11(θ); deduced possible three-nucleon force effects.

doi: 10.1016/S0370-2693(98)00370-0
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1998VE03      Phys.Rev.Lett. 81, 1187 (1998)

K.D.Veal, C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, A.J.Mendez, E.E.Bartosz, P.D.Cathers, T.L.Drummer, K.W.Kemper, A.M.Eiro, F.D.Santos, B.Kozlowska, H.J.Maier, I.J.Thompson

Deformation Effects in 6Li

NUCLEAR REACTIONS 58Ni(polarized 6Li, d), E=34 MeV; analyzed σ(θ), A(y)(θ), A(zz)(θ), A(xz)(θ). 6Li deduced asymptototic D- to S-state ratio. DWBA analysis.

doi: 10.1103/PhysRevLett.81.1187
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1997BR37      Nucl.Instrum.Methods Phys.Res. A389, 421 (1997)

C.R.Brune, H.J.Karwowski, E.J.Ludwig

Determination of Low-Energy Proton Polarization Via the 6Li(p(pol), 3He)4He Reaction

NUCLEAR REACTIONS 6Li(polarized p, 3He), E=250-460 MeV; measured A(y)(θ). 4He(polarized p, p), E=6 MeV; measured A(y); deduced beam polarization.

doi: 10.1016/S0168-9002(97)00340-9
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1997KI17      Phys.Lett. 406B, 292 (1997)

A.Kievsky, S.Rosati, M.Viviani, C.R.Brune, H.J.Karwowski, E.J.Ludwig, M.H.Wood

The Three-Nucleon System Near the N-d Threshold

NUCLEAR REACTIONS 1H(polarized d, d), E(cm)=432 keV; measured tensor analyzing powers vs θ; deduced scattering wave functions, three-nucleon properties.

doi: 10.1016/S0370-2693(97)00691-6
Citations: PlumX Metrics

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1997MA08      Phys.Rev. C55, 588 (1997)

L.Ma, H.J.Karwowski, C.R.Brune, Z.Ayer, T.C.Black, J.C.Blackmon, E.J.Ludwig, M.Viviani, A.Kievsky, R.Schiavilla

Measurements of 1H(d(pol), γ)3He and 2H(p(pol), γ)3He at Very Low Energies

NUCLEAR REACTIONS 1H(polarized d, γ), E(cm)=40-110 keV; 2H(polarized p, γ), E(cm)=70-210 keV; measured σ(θ), analyzing powers vs θ; deduced thermonuclear reaction rate.

doi: 10.1103/PhysRevC.55.588
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1995AY03      Phys.Rev. C52, 2851 (1995)

Z.Ayer, H.J.Karwowski, B.Kozlowska, E.J.Ludwig

Determination of the Asymptotic D- to S-State Ratio for 3He via (d(pol), 3He) Reactions

NUCLEAR REACTIONS 93Nb(polarized d, 3He), E=12 MeV; 63Cu(polarized d, 3He), E=8 MeV; 89Y(polarized d, 3He), E=10.5 MeV; 93Nb(polarized d, d), E=12 MeV; measured σ(θ), tensor analyzing powers vs θ. 3He deduced D-state parameter. Finite-range DWBA analysis. Enriched targets.

doi: 10.1103/PhysRevC.52.2851
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1995GE16      Nucl.Instrum.Methods Phys.Res. A365, 36 (1995)

W.Geist, Z.Ayer, A.C.Hird, H.J.Karwowski, E.J.Ludwig

A Deuteron Tensor Polarimeter for Low-Energy Experiments

NUCLEAR REACTIONS 3He(polarized d, p), E=121-311 keV; measured tensor analyzing power vs θ; deduced polarimeter calibration.

doi: 10.1016/0168-9002(95)00456-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1429.


1994FL03      Phys.Rev. C49, 2305 (1994)

K.A.Fletcher, Z.Ayer, T.C.Black, R.K.Das, H.J.Karwowski, E.J.Ludwig, G.M.Hale

Tensor Analyzing Power for 2H(d, p)3H and 2H(d, n)3He at Deuteron Energies of 25, 40, 60, and 80 keV

NUCLEAR REACTIONS 2H(polarized d, p), (polarized d, n), E=25-80 keV; measured σ(θ), tensor analyzing power vs θ; deduced implications for neutron-lean fusion reaction, entrance channel quintent S-state role.

doi: 10.1103/PhysRevC.49.2305
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1994KO29      Phys.Rev. C50, 2695 (1994)

B.Kozlowska, Z.Ayer, R.K.Das, H.J.Karwowski, E.J.Ludwig

Determination of the Asymptotic D- to S-State Ratio of the Triton from Sub-Coulomb (d(pol), t) Reactions

NUCLEAR REACTIONS 119Sn(polarized d, t), E=5.25 MeV; 149Sm(polarized d, t), E=6 MeV; 206Pb(polarized d, t), E=10 MeV; measured tensor analyzing power vs θ. 3H deduced asymptotic D- to S-state ratio. Finite-range DWBA analysis.

doi: 10.1103/PhysRevC.50.2695
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1993FL06      Nucl.Instrum.Methods Phys.Res. A329, 197 (1993)

K.A.Fletcher, T.C.Black, H.J.Karwowski, E.J.Ludwig, Y.Tagishi

A Deuteron Tensor Polarimeter for Energies Below 90 keV

NUCLEAR REACTIONS 2H(polarized d, p), E=20-90 keV; measured analyzing power at θ=10°; deduced deuteron tensor polarimeter characteristics.

doi: 10.1016/0168-9002(93)90936-C
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1993PI14      Phys.Rev. C48, 2763 (1993)

M.A.Pickar, A.D.Bacher, M.Hugi, H.O.Meyer, R.E.Pollock, G.T.Emery, H.J.Karwowski, J.R.Hall, M.Fatyga

Near-Threshold Proton-Induced Neutral Pion Production from 12C

NUCLEAR REACTIONS 12C(polarized p, π0), E=146.87 MeV; measured σ(θ), analyzing power vs (θ), σ. 12C(p, π0), (p, π+), E ≤ 200 MeV; compiled σ; deduced p-wave strengths.

doi: 10.1103/PhysRevC.48.2763
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1992BO14      Phys.Rev. C45, 2824 (1992)

J.E.Bowsher, T.B.Clegg, H.J.Karwowski, E.J.Ludwig, W.J.Thompson, J.A.Tostevin

Effects of 6Li Excitation in 64Zn(d(pol), 6Li)60Ni at Low Energies

NUCLEAR REACTIONS 64Zn(polarized d, 6Li), E=16.4 MeV; measured σ(θ), analyzing power vs θ; deduced 6Li levels role in reaction mechanism, model parameters. Vector, tensor polarized beam. Finite-range, coupled-channel Born approximation analysis.

doi: 10.1103/PhysRevC.45.2824
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1992DA01      Phys.Rev.Lett. 68, 1112 (1992)

R.K.Das, T.B.Clegg, H.J.Karwowski, E.J.Ludwig

Precise Determination of Triton D-State Parameters Using Transfer Reactions at Sub-Coulomb Energies

NUCLEAR REACTIONS 95Mo(polarized d, t), E=7 MeV; 119Sn(polarized d, t), E=6.7 MeV; 149Sm(polarized d, t), E=8 MeV; measured σ(θ), tensor analyzing power vs θ. 3H deduced D-state parameters. Exact finite-range DWBA.

doi: 10.1103/PhysRevLett.68.1112
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1992LU04      Phys.Rev.Lett. 69, 2448 (1992)

E.J.Ludwig, R.K.Das, T.B.Clegg, H.J.Karwowski

Ludwig et al. Reply:

doi: 10.1103/PhysRevLett.69.2448
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1992WI13      Nucl.Phys. A549, 223 (1992)

J.F.Wilkerson, T.M.Mooney, R.E.Fauber, T.B.Clegg, H.J.Karwowski, E.J.Ludwig, W.J.Thompson

Isospin-Nonconserving Particle Decays in Light Nuclei

NUCLEAR REACTIONS 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar(polarized p, p), E ≈ resonance; 23Na, 31P(polarized p, p), (polarized p, α), 24Mg, 28Si(α, α), 20Ne(polarized p, p), E=6.4-7.7 MeV; measured σ(θ, E), analyzing power vs E, θ; deduced σ(E). 13N, 17F, 24Na, 25Al, 29P, 33S, 37K, 24Mg, 32S, 28Si deduced resonance parameters, isospin-nonconservation probabilities. Enriched targets, ion-implanted targets, polarized and unpolarized beams.

doi: 10.1016/0375-9474(92)90041-H
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1991BH02      Nucl.Phys. A526, 36 (1991)

C.M.Bhat, E.J.Ludwig, T.B.Clegg, H.J.Karwowski

A Determination of the Asymptotic D- to S-State Ratio for 3He

NUCLEAR REACTIONS 32S(polarized d, 3He), E=16 MeV; measured σ(θ), tensor analyzing power vs θ. 3He deduced D-state. Finite-range DWBA analysis.

doi: 10.1016/0375-9474(91)90296-I
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1990LU10      J.Phys.(Paris), Colloq.C-6, 439 (1990)

E.J.Ludwig, C.M.Bhat, T.B.Clegg, E.R.Crosson, H.J.Karwowski, G.Graw, P.Schiemenz, R.Hertenberger, H.Kader, D.Hofer, M.Bisenberger, A.M.Eiro, F.D.Santos

D-State Parameter Determinations for 3He and 4He

NUCLEAR REACTIONS 32S(polarized d, 3He), E=16 MeV; 58Ni(polarized d, α), E=22 MeV; measured σ(θ), analyzing power vs θ. 3,4He deduced asymptotic D- to S-state ratio, D2 parameter.


1989AB17      Nucl.Instrum.Methods Phys.Res. A284, 409 (1989)

D.J.Abbott, H.J.Karwowski, T.B.Clegg, E.J.Ludwig

A Deuteron Polarimeter for Polarization Transfer Experiments

NUCLEAR REACTIONS 3He(polarized d, p), E=5-12 MeV; measured vector, tensor analyzing powers vs E. Deuteron polarimeter calibration.

doi: 10.1016/0168-9002(89)90310-0
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1989PI06      Phys.Rev. C39, 1679 (1989)

W.K.Pitts, H.O.Meyer, L.C.Bland, J.D.Brown, R.C.Byrd, M.Hugi, H.J.Karwowski, P.Schwandt, A.Sinha, J.Sowinski, I.J.van Heerden

2H(d(pol), γ)4He Reaction at E(d) = 95 MeV

NUCLEAR REACTIONS 2H(polarized d, γ), E=95 MeV; measured σ(θ), vector, tensor analyzing power vs θ.

doi: 10.1103/PhysRevC.39.1679
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1989SK04      Phys.Rev. C40, 1279 (1989)

W.Skulski, M.Fatyga, H.J.Karwowski, K.Kwiatkowski, V.E.Viola, Jr., K.Hicks, R.Ristinen

Linear Momentum Transfer in the Reaction of 64-269 MeV 3He with 238U

NUCLEAR REACTIONS 238U(3He, F), E=64-269 MeV; measured fission (fragment)(light particle)-coin; deduced linear momentum transfer, missing momentum.

doi: 10.1103/PhysRevC.40.1279
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1988BH02      Phys.Rev. C37, 1358 (1988)

C.M.Bhat, T.B.Clegg, H.J.Karwowski, E.J.Ludwig

D-State Amplitudes of Three-Nucleon Systems using Single-Nucleon Transfer Reactions

NUCLEAR REACTIONS 31P(polarized d, 3He), 31P(polarized d, t), E ≈ 16 MeV; measured absolute σ(θ), tensor analyzing power vs θ. 3He, 3H deduced D-state amplitudes. Finite-range DWBA analysis. Enriched target.

doi: 10.1103/PhysRevC.37.1358
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1988BH09      Phys.Rev. C38, 1537 (1988)

C.M.Bhat, J.E.Bowsher, T.B.Clegg, H.J.Karwowski, E.J.Ludwig, B.A.Brown

Single-Nucleon Pickup Spectroscopic Factors for Levels in 30Si and 30P and the D State of Three-Nucleon Systems

NUCLEAR REACTIONS 31P(polarized d, 3He), (polarized d, t), (polarized d, d), E=16 MeV; measured σ(θ), vector, tensor analyzing powers vs θ; deduced model parameters. 30Si, 30P levels deduced spectroscopic factors.

doi: 10.1103/PhysRevC.38.1537
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1988PI01      Phys.Rev. C37, 1 (1988)

W.K.Pitts, H.O.Meyer, L.C.Bland, J.D.Brown, R.C.Byrd, M.Hugi, H.J.Karwowski, P.Schwandt, A.Sinha, J.Sowinski, I.J.van Heerden, A.Arriaga, F.D.Santos

1H(d(pol), γ)3He Reaction at E(d) = 95 MeV

NUCLEAR REACTIONS, MECPD 1H(polarized d, γ), E=95 MeV; measured σ(θ), analyzing power vs θ. 3He deduced D- to S- state asymptotic normalization ratio.

doi: 10.1103/PhysRevC.37.1
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1987FA01      Phys.Rev. C35, 568 (1987)

M.Fatyga, H.J.Karwowski, K.Kwiatkowski, L.Nowicki, V.E.Viola, K.Hicks

Linear Momentum Transfer and Light Particle Emission in the E/A = 25 MeV 6Li + 238U Reaction

NUCLEAR REACTIONS 238U(6Li, pF), (6Li, dF), (6Li, tF), (6Li, 3HeF), (6Li, αF), E=150 MeV; measured fission fragment(light particle)-coin, σ(fragment θ, mass) vs linear momentum transfer; deduced complete fussion σ upper limit. Position sensitive multi-wire chamber, surface barrier detector.

doi: 10.1103/PhysRevC.35.568
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1987FA03      Phys.Lett. 185B, 321 (1987)

M.Fatyga, R.C.Byrd, K.Kwiatkowski, W.G.Wilson, L.W.Woo, V.E.Viola, Jr., H.J.Karwowski, J.Jastrzebski, W.Skulski

Source Properties of Intermediate Mass Fragments Emitted in the 270 MeV 3He + 232Th Reaction

NUCLEAR REACTIONS 232Th(3He, X), (3He, F), E=270 MeV; measured fission probability following intermediate mass fragmentation; deduced reaction mechanism. ΔE-E telescopes.

doi: 10.1016/0370-2693(87)91007-0
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1987PI01      Phys.Rev. C35, 37 (1987)

M.A.Pickar, H.J.Karwowski, J.D.Brown, J.R.Hall, M.Hugi, R.E.Pollock, V.R.Cupps, M.Fatyga, A.D.Bacher

Proton Radiative Capture by Deuterium between 100 and 200 MeV

NUCLEAR REACTIONS, MECPD 2H(polarized p, γ), E=100-200 MeV; measured σ(θ), A(θ); deduced quasideuteron role. Coincidence measurement. Quasideuteron model calculations.

doi: 10.1103/PhysRevC.35.37
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1986JA09      Phys.Rev. C34, 60 (1986)

J.Jastrzebski, P.P.Singh, T.Mroz, S.E.Vigdor, M.Fatyga, H.J.Karwowski

Interaction of 5-50 MeV/Nucleon 3He and 4He with 59Co

NUCLEAR REACTIONS, ICPND 59Co(α, X)61Cu/60Cu/57Ni/62Cu/59Cu/62Ni/60Ni/59Ni/58Ni/61Co/60Co/58Co/58mCo/59Co/57Co/56Co/55Co/59Fe/58Fe/57Fe/56Fe/55Fe/54Fe/53Fe/52Fe/55Mn/54Mn/53Mn/52Mn/52mMn/51Mn/51Cr/52Cr/53Cr/54Cr/50Cr/49V/48V/50Ti/48Ti, E=20.1-198.9 MeV; 59Co(3He, X)61Cu/57Ni/58Co/58mCo/57Co/56Co/55Co/59Fe/52Fe/56Mn/54Mn/52Mn/51Cr/48V/48Sc/44Sc/44mSc, E=11-44.2 MeV; measured residual production σ, fragment mass, charge distributions, σ(fragment θ). In beam spectroscopy, activation techniques.

doi: 10.1103/PhysRevC.34.60
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1986VA02      Phys.Lett. 166B, 372 (1986)

S.Y.Van Der Werf, N.Blasi, M.N.Harakeh, G.Wenes, A.D.Bacher, G.T.Emery, C.W.Glover, W.P.Jones, H.J.Karwowski, H.Nann, C.Olmer, P.Den Heijer, C.W.De Jager, H.De Vries, J.Ryckebusch, M.Waroquier

High-Spin 1p-1h Configurations in 116Sn and Their Fragmentation as seen in the Reactions 116Sn(p(pol), p'), 116Sn(e, e'), 115In(He, d) and 115In(α, t)

NUCLEAR REACTIONS 116Sn(polarized p, p'), E=133.8 MeV; measured σ(θ), σ(Ep'), A(θ). 116Sn(e, e'), E=350 MeV; measured σ(E(e)), form factors. 115In(α, t), E=65 MeV; 115In(3He, d), E=50 MeV; measured σ(Et), σ(Ed). 116Sn deduced levels, J, π, L, stretched configuration fragmentation, transition amplitudes. DWBA analysis, shell model comparison.

doi: 10.1016/0370-2693(86)91582-0
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1985FA07      Phys.Rev. C32, 1496 (1985)

M.Fatyga, K.Kwiatkowski, H.J.Karwowski, L.W.Woo, V.E.Viola

Linear Momentum Transfer in 40-150 MeV Proton-Induced Reactions with 238U

NUCLEAR REACTIONS 238U(p, F), E=40, 90, 150 MeV; measured fission (fragment)(fragment)(θ), σ(θ1, θ2); deduced linear momentum transfer distribution. Intranuclear cascade, precompound emission models.

doi: 10.1103/PhysRevC.32.1496
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1985ME03      Phys.Rev. C31, 309 (1985)

H.O.Meyer, J.R.Hall, M.Hugi, H.J.Karwowski, R.E.Pollock, P.Schwandt

Neutron-Proton Radiative Capture Cross Section at T(n) = 185 MeV

NUCLEAR REACTIONS 1H(n, γ), E=185 MeV; measured recoil σ(θd), θ=0°-65°; deduced charge density, relativistic corrections role.

doi: 10.1103/PhysRevC.31.309
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1984DA14      Phys.Rev. C30, 236 (1984)

J.M.D'Auria, M.Dombsky, G.Sheffer, T.E.Ward, H.J.Karwowski, A.I.Yavin, J.L.Clark

Inclusive Measurement of Quasifree (p, xn) Charge Exchange Reactions on Bismuth from 62 to 800 MeV

NUCLEAR REACTIONS, ICPND 209Bi(p, n), (p, 2n), (p, 4n), (p, 6n), E=62-800 MeV; measured residuals production σ(E), production σ relative to 208Po vs E. 209Bi(p, X), E=210-480 MeV; measured residuals production σ relative to 202o. Radiochemical activation techniques. Intranuclear cascade calculation.

doi: 10.1103/PhysRevC.30.236
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1984JA04      Phys.Lett. 136B, 153 (1984)

J.Jastrzebski, P.P.Singh, T.Mroz, H.J.Karwowski, S.E.Vigdor, M.Fatyga

Momentum Transfer in 30-200 MeV 4He Induced Reaction with 59Co

NUCLEAR REACTIONS 59Co(α, X), E=30-200 MeV; measured residual production σ, recoil range vs compound nucleus, residue mass difference; deduced momentum transfer average characteristics.

doi: 10.1016/0370-2693(84)91170-5
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1984KA03      Phys.Rev. C29, 872 (1984)

H.J.Karwowski, S.E.Vigdor

Calculations of High-Spin Fission for A ≈ 200

NUCLEAR REACTIONS, ICPND 181Ta(19F, F), E=95.7, 109.9 MeV; 170Er(30Si, F), E=134.7, 152.9 MeV; 197Au(6Li, F), E=84.4 MeV; calculated fission σ(E). 181Ta(19F, xα), E=80-120 MeV; calculated evaporation σ(E). 181Ta(19F, F), E=96 MeV; calculated fission fragment σ(θ). 170Er(30Si, 4n), (30Si, 5n), (30Si, 6n), E ≈ 120-170 MeV; calculated σ(E); deduced rotating liquid drop model validity. 200,203Pb deduced fission, evaporation decay characteristics.

doi: 10.1103/PhysRevC.29.872
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1984ME05      Phys.Rev.Lett. 52, 1759 (1984)

H.O.Meyer, J.R.Hall, M.Hugi, H.J.Karwowski, R.E.Pollock, P.Schwandt

Absolute Cross Section for Neutron-Proton Radiative Capture at T(n) = 185 MeV

NUCLEAR REACTIONS 1H(n, d), E=185 MeV; measured absolute σ(θ), radiative capture.

doi: 10.1103/PhysRevLett.52.1759
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1982KA05      Phys.Rev. C25, 1355 (1982)

H.J.Karwowski, S.E.Vigdor, W.W.Jacobs, S.Kailas, P.P.Singh, F.Soga, T.G.Throwe, T.E.Ward, D.L.Wark, J.Wiggins

Multiplicity of K X Rays and Collective Structure in the Transitional Nuclei with A ≈ 200

NUCLEAR REACTIONS 180Hf, 181Ta, 186W, 185,187Re, 194,198Pt, 197Au, 203,205Tl, 208Pb, 209Bi(6Li, xn), (7Li, xn), E=55-124 MeV; measured γ(X-ray)-, (X-ray)(X-ray)-coin, Eγ, Iγ, E(X-ray), I(X-ray); deduced σ(total), K X-ray multiplicity, production σ for K X-ray.

doi: 10.1103/PhysRevC.25.1355
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1982VI02      Phys.Rev. C26, 1035 (1982)

S.E.Vigdor, H.J.Karwowski, W.W.Jacobs, S.Kailas, P.P.Singh, F.Soga, T.G.Throwe

Decay of Hot, High-Spin Nuclei Produced in 6Li-Induced Fusion Reactions

NUCLEAR REACTIONS 181Ta, 194,198Pt, 197Au, 208Pb(6Li, pX), (6Li, dX), (6Li, tX), (6Li, αX), E=94.4, 74.8 MeV; measured inclusive σ(θ), particle spectra. 181Ta, 194,198Pt, 197Au, 208Pb(6Li, F), (6Li, X), E=74.8, 84.2, 94.4 MeV; measured σ(fragment θ), σ(fragment E), fission fragment anisotropy, σ(fusion). 181Ta, 194,198Pt, 197Au, 208Pb(6Li, xn), E=74.8, 84.2, 94.4 MeV; measured K X-ray multiplicities.

doi: 10.1103/PhysRevC.26.1035
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1982VI03      Phys.Rev. C26, 1068 (1982)

S.E.Vigdor, H.J.Karwowski

Influence of Deformed-Nucleus Level Densities on Statistical Model Calculations for High-Spin Fission

NUCLEAR REACTIONS 197Au(6Li, F), (6Li, xα), (6Li, X), E=84.2 MeV; calculated fission σ, α-production σ, fission fragment anisotropy, fission probability vs spin, chance. 203Pb deduced fission, evaporation competition. Statistical model.

doi: 10.1103/PhysRevC.26.1068
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1981KA34      Phys.Rev.Lett. 47, 1251 (1981)

H.J.Karwowski, S.E.Vigdor, W.W.Jacobs, T.G.Throwe, D.L.Wark, S.Kailas, P.P.Singh, F.Soga, T.E.Ward, J.Wiggins

Systematics of the K X-Ray Multiplicity for Transitional Nuclei with A ≈ 200

NUCLEAR REACTIONS 209Bi, 197Au, 203,205Tl, 185,187Re, 181Ta, 208Pb, 198,194Pt, 186W, 180Hf(6Li, xn), 197Au, 208Pb(7Li, xn), E=55-124 MeV; measured K X-ray multiplicities; deduced high-K rotational band role.

doi: 10.1103/PhysRevLett.47.1251
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1980JA14      Phys.Rev. C22, 1443 (1980)

J.Jastrzebski, H.J.Karwowski, M.Sadler, P.P.Singh

Recoil Ranges of Nuclei Produced in the Interaction of 80-164 MeV Protons with Ni

NUCLEAR REACTIONS 58Ni(p, X), 62Ni(p, X), E=80-164 MeV; measured Eγ, Iγ of radioactive products; deduced σ(X, E), recoil ranges, mass, charge distributions. Enriched targets, Ge(Li) counter.

doi: 10.1103/PhysRevC.22.1443
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1980VI02      Phys.Lett. 90B, 384 (1980)

S.E.Vigdor, H.J.Karwowski, W.W.Jacobs, S.Kailas, P.P.Singh, F.Soga, P.Yip

On the Anisotropy of Multi-Chance, High-Spin Fission

NUCLEAR REACTIONS 181Ta, 194,198Pt, 197Au, 208Pb(6Li, xn), (6Li, F), E=74.8-94.5 MeV; calculated σ(fragment θ), fission σ vs neutron number. Statistical model.

doi: 10.1016/0370-2693(80)90954-5
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1979KA12      Phys.Rev.Lett. 42, 1732 (1979)

H.J.Karwowski, S.E.Vigdor, W.W.Jacobs, S.Kailas, P.P.Singh, F.Soga, W.D.Ploughe

Multiplicity of K X Rays Emitted in (6Li, xn) Reactions

NUCLEAR REACTIONS 181Ta, 194,198Pt, 197Au, 208Pb(6Li, xn), E=75, 85, 95 MeV; measured (X-ray)(X-ray)-coin, γX-coin, Eγ, Iγ. 187Os, 200,204Tl, 203Pb, 214At deduced K X-ray multiplicities, absolute evaporation residue σ.

doi: 10.1103/PhysRevLett.42.1732
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