NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = D.R.Phillips Found 93 matches. 2024PA09 Phys.Rev. C 109, 015802 (2024) S.N.Paneru, C.R.Brune, D.Connolly, D.Odell, M.Poudel, D.R.Phillips, J.Karpesky, B.Davids, C.Ruiz, A.Lennarz, U.Greife, M.Alcorta, R.Giri, M.Lovely, M.Bowry, M.Delgado, N.E.Esker, A.B.Garnsworthy, C.Seeman, P.Machule, J.Fallis, A.A.Chen, F.Laddaran, A.Firmino, C.Weinerman Elastic scattering of 3He+4He with the SONIK scattering chamber
doi: 10.1103/PhysRevC.109.015802
2023CA17 Eur.Phys.J. A 59, 273 (2023) P.Capel, D.R.Phillips, A.Andis, M.Bagnarol, B.Behzadmoghaddam, F.Bonaiti, R.Bubna, Y.Capitani, P.-Y.Duerinck, V.Durant, N.Dopper, A.El Boustani, R.Farrell, M.Geiger, M.Gennari, N.Goldberg, J.Herko, T.Kirchner, L.-P.Kubushishi, Z.Li, S.S.Li Muli, A.Long, B.Martin, K.Mohseni, I.Moumene, N.Paracone, E.Parnes, B.Romeo, V.Springer, I.Svensson, O.Thim, N.Yapa Effective field theory analysis of the Coulomb breakup of the one-neutron halo nucleus 19C NUCLEAR REACTIONS 208Pb(19C, X)18C, E=67 MeV/nucleon; analyzed available data; deduced σ(θ), σ(E) using NLO Halo-EFT 18C-n potentials. A Halo-EFT description of the projectile within the Coulomb Corrected Eikonal approximation (CCE).
doi: 10.1140/epja/s10050-023-01181-7
2023GO01 Phys.Rev. C 107, 014617 (2023) M.Gobel, B.Acharya, H.-W.Hammer, D.R.Phillips Final-state interactions and spin structure in E1 breakup of 11Li in halo effective field theory NUCLEAR STRUCTURE 11Li; charge radii, mean-square neutron charge radius, calculated E1 strength distribution with inclusion of final state interactions in neutron-neutron and neutron-core channels, cumulative B(E1). Halo effective field theory (Halo EFT) at leading order treating 11Li as three-body system 9Li+n+n. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.014617
2022CA01 Phys.Lett. B 825, 136847 (2022) P.Capel, D.R.Phillips, H.-W.Hammer Simulating core excitation in breakup reactions of halo nuclei using an effective three-body force NUCLEAR REACTIONS 12C(11Be, X)10Be, E=67 MeV/nucleon; analyzed available data; deduced breakup σ(E), σ(θ), resonances using Halo Effective Field Theory and the Dynamical Eikonal Approximation to include an effective 10Be-n-target force.
doi: 10.1016/j.physletb.2021.136847
2022CI08 J.Phys.(London) G49, 120502 (2022) V.Cirigliano, Z.Davoudi, J.Engel, R.J.Furnstahl, G.Hagen, U.Heinz, H.Hergert, M.Horoi, C.W.Johnson, A.Lovato, E.Mereghetti, W.Nazarewicz, A.Nicholson, T.Papenbrock, S.Pastore, M.Plumlee, D.R.Phillips, P.E.Shanahan, S.R.Stroberg, F.Viens, A.Walker-Loud, K.A.Wendt, S.M.Wild Towards precise and accurate calculations of neutrinoless double-beta decay RADIOACTIVITY 48Ca(2β-); calculated neutrinoless nuclear matrix elements using chiral-EFT interactions, EDF, IBM, QRPA, SM-pf, SM-sdpf, SM-MBPT, RSM, QMC+SM, IM-GCM, VS-IMSRG, CCSD, CCSD-T1.
doi: 10.1088/1361-6471/aca03e
2022HO01 J.Phys.(London) G49, 010502 (2022) C.R.Howell, M.W.Ahmed, A.Afanasev, D.Alesini, J.R.M.Annand, A.Aprahamian, D.L.Balabanski, S.V.Benson, A.Bernstein, C.R.Brune, J.Byrd, B.E.Carlsten, A.E.Champagne, S.Chattopadhyay, D.Davis, E.J.Downie, J.M.Durham, G.Feldman, H.Gao, C.G.R.Geddes, H.W.Griesshammer, R.Hajima, H.Hao, D.Hornidge, J.Isaak, R.V.F.Janssens, D.P.Kendellen, M.Kovash, P.P.Martel, U.-G.Meissner, R.Miskimen, B.Pasquini, D.R.Phillips, N.Pietralla, D.Savran, M.R.Schindler, M.H.Sikora, W.M.Snow, R.P.Springer, C.Sun, C.Tang, B.Tiburzi, A.P.Tonchev, W.Tornow, C.A.Ur, D.Wang, H.R.Weller, V.Werner, Y.K.Wu, J.Yan, Z.Zhao, A.Zilges, F.Z.Zomer International workshop on next generation gamma-ray source
doi: 10.1088/1361-6471/ac2827
2022OD01 Phys.Rev. C 105, 014625 (2022) D.Odell, C.R.Brune, D.R.Phillips How Bayesian methods can improve R-matrix analyses of data: The example of the dt reaction NUCLEAR REACTIONS 3H(d, n)4He, E=5-47, 9-70, 12-214, 46-264, 48-70 keV; analyzed five sets of experimental σ(E) data using Bayesian statistics with Markov chain Monte Carlo sampling to evaluate one- and two-level R-matrix-plus-statistical model; deduced common-mode and additional point-to-point uncertainties. Discussed possible paths to reduction of uncertainty in the S-factor.
doi: 10.1103/PhysRevC.105.014625
2022PO08 J.Phys.(London) G49, 045102 (2022) Effective field theory analysis of 3He-α scattering data NUCLEAR REACTIONS 4He(3He, 3He), E(cm)=0.38-3.12 MeV; analyzed available data from the scattering of nuclei in inverse kinematics (SONIK) gas target at TRIUMF; deduced σ(θ), analyzing power, phase shifts using a likelihood function that incorporates the theoretical uncertainty due to truncation of the effective field theory (EFT) and use Markov chain Monte Carlo sampling to obtain the resulting posterior probability distribution.
doi: 10.1088/1361-6471/ac4da6
2022SE11 Phys.Rev. C 106, 044002 (2022) A.C.Semposki, R.J.Furnstahl, D.R.Phillips Interpolating between small- and large-g expansions using Bayesian model mixing
doi: 10.1103/PhysRevC.106.044002
2022TE06 Few-Body Systems 63, 67 (2022) I.Tews, Z.Davoudi, A.Ekstrom, J.D.Holt, K.Becker, R.Briceno, D.J.Dean, W.Detmold, C.Drischler, T.Duguet, E.Epelbaum, A.Gasparyan, J.Gegelia, J.R.Green, H.W.Griesshammer, A.D.Hanlon, M.Heinz, H.Hergert, M.Hoferichter, M.Illa, D.Kekejian, A.Kievsky, S.Konig, H.Krebs, K.D.Launey, D.Lee, P.Navratil, A.Nicholson, A.Parreno, D.R.Phillips, M.Ploszajczak, X.-L.Ren, T.R.Richardson, C.Robin, G.H.Sargsyan, M.J.Savage, M.R.Schindler, P.E.Shanahan, R.P.Springer, A.Tichai, U.van Kolck, M.L.Wagman, A.Walker-Loud, C.-J.Yang, X.Zhang Nuclear Forces for Precision Nuclear Physics: A Collection of Perspectives
doi: 10.1007/s00601-022-01749-x
2021AL30 Phys.Rev. C 104, 064311 (2021) I.K.Alnamlah, E.A.Coello Perez, D.R.Phillips Effective field theory approach to rotational bands in odd-mass nuclei NUCLEAR STRUCTURE 99Tc, 159Dy, 167,169Er, 167,169Tm, 183W, 235U, 239Pu; calculated rotational bandhead energies, J, π, energy scales, relative correction to energies in bands at each order, low-energy constants (LECs) at each order for K=1/2 bands, for K=3/2 bands in 167Er and 159Dy, for K=5/2, 7/2 bands in 167Er and 235U. 169Er, 167,169Tm, 239Pu, 159Dy, 99Tc, 183W; calculated energies and energy residuals for ground-state and excited-state rotational bands at LO, NLO, N2LO, N3LO, and N4LO orders as follows: 1/2- g.s. band up to 35/2- for 169Er, 1/2+ g.s. band up to 31/2+ for 167Tm, 1/2+ excited band up to 19/2+ for 169Tm, 1/2+ g.s. band up to 53/2+ for 239Pu, 3/2- g.s. band up to 29/2- for 159Dy; 1/2- excited band up to 31/2- in 99Tc, and 1/2- g.s. band up to 35/2 in 183W. 167Er, 235U; calculated energy residuals for 1/2-, 5/2-, and 7/2+ rotational bands in 167Er, and for the 1/2+, 5/2+, and 7/2- rotational bands in 235U at LO, NLO, N2LO, N3LO, and N4LO orders; extracted breakdown scale in different systems. Extension of effective field theory up to fourth order in the angular velocity to describe rotational bands in even-even nuclei to the odd-mass case, and possibility of application of this EFT to halo nuclei in which low-lying rotational states of the core play a prominent role, such as in 11Be and 31Ne nuclei. Comparison with experimental band structures, data taken from ENSDF database and publications in Nuclear Data Sheets.
doi: 10.1103/PhysRevC.104.064311
2021GO20 Phys.Rev. C 104, 024001 (2021) M.Gobel, T.Aumann, C.A.Bertulani, T.Frederico, H.-W.Hammer, D.R.Phillips Neutron-neutron scattering length from the 6He (p, pα) nn reaction NUCLEAR REACTIONS 2H(π-, γ), (n, p), (d, 2He)2n, E not given; compiled experimental data for neutron-neutron scattering lengths reported between 1998 and 2008. 1H(6He, pα)2n, E=few MeV/nucleon; calculated ground-state nn relative-energy distributions for different nn scattering lengths using halo effective field theory (EFT), s-wave scattering length using a method based on the final-state interaction (FSI) between the neutrons after the sudden knockout of the α particle. Comparison with model calculations using the computer code FaCE. Proposed a novel method to measure the neutron-neutron scattering length in inverse kinematics. Relevance to precise determination of the nn scattering length using data from the approved experiment at RIKEN using the 1H(6He, pα)nn reaction.
doi: 10.1103/PhysRevC.104.024001
2021ME07 Eur.Phys.J. A 57, 81 (2021) J.A.Melendez, R.J.Furnstahl, H.W.Griesshammer, J.A.McGovern, D.R.Phillips, M.T.Pratola Designing optimal experiments: an application to proton Compton scattering
doi: 10.1140/epja/s10050-021-00382-2
2021PH05 J.Phys.(London) G48, 072001 (2021) D.R.Phillips, R.J.Furnstahl, U.Heinz, T.Maiti, W.Nazarewicz, F.M.Nunes, M.Plumlee, M.T.Pratola, S.Pratt, F.G.Viens, S.M.Wild Get on the BAND Wagon: a Bayesian framework for quantifying model uncertainties in nuclear dynamics NUCLEAR REACTIONS 208Pb(p, p), E=30 MeV; calculated σ. Comparison with available data.
doi: 10.1088/1361-6471/abf1df
2021WE14 Phys.Rev. C 104, 064001 (2021) S.Wesolowski, I.Svensson, A.Ekstrom, C.Forssen, R.J.Furnstahl, J.A.Melendez, D.R.Phillips Rigorous constraints on three-nucleon forces in chiral effective field theory from fast and accurate calculations of few-body observables NUCLEAR STRUCTURE 3H, 4He; calculated binding energies, rms point-proton radius of 4He, T1/2 of 3H β decay in the LO, NLO, and NNLO orders using three-nucleon force (3NF) of chiral effective field theory (χEFT), and compared with experimental values; evaluated Bayesian statistical methods for effective field theories of nuclei by using eigenvector continuation (EC) emulator.
doi: 10.1103/PhysRevC.104.064001
2020DR04 Phys.Rev.Lett. 125, 202702 (2020) C.Drischler, R.J.Furnstahl, J.A.Melendez, D.R.Phillips How Well Do We Know the Neutron-Matter Equation of State at the Densities Inside Neutron Stars? A Bayesian Approach with Correlated Uncertainties
doi: 10.1103/PhysRevLett.125.202702
2020DR05 Phys.Rev. C 102, 054315 (2020) C.Drischler, J.A.Melendez, R.J.Furnstahl, D.R.Phillips Quantifying uncertainties and correlations in the nuclear-matter equation of state
doi: 10.1103/PhysRevC.102.054315
2020GR16 Few-Body Systems 61, 48 (2020) H.W.Griesshammer, J.A.McGovern, A.Nogga, D.R.Phillips Scattering Observables from One- and Two-body Densities: Formalism and Application to γ 3He Scattering
doi: 10.1007/s00601-020-01578-w
2020RY02 Eur.Phys.J. A 56, 7 (2020) E.Ryberg, C.Forssen, D.R.Phillips, U.van Kolck Finite-size effects in heavy halo nuclei from effective field theory
doi: 10.1140/epja/s10050-019-00001-1
2019ME05 Phys.Rev. C 100, 044001 (2019) J.A.Melendez, R.J.Furnstahl, D.R.Phillips, M.T.Pratola, S.Wesolowski Quantifying correlated truncation errors in effective field theory
doi: 10.1103/PhysRevC.100.044001
2019WE07 J.Phys.(London) G46, 045102 (2019) S.Wesolowski, R.J.Furnstahl, J.A.Melendez, D.R.Phillips Exploring Bayesian parameter estimation for chiral effective field theory using nucleon-nucleon phase shifts
doi: 10.1088/1361-6471/aaf5fc
2018CA23 Phys.Rev. C 98, 034610 (2018) Erratum Phys.Rev. C 105, 019901 (2022) P.Capel, D.R.Phillips, H.-W.Hammer Dissecting reaction calculations using halo effective field theory and ab initio input NUCLEAR REACTIONS 208Pb, 12C(11Be, n), E=67, 69 MeV/nucleon; calculated radial wave functions of 11Be g.s. and 1/2- excited state, 11Be projectile partial wave phase shifts, and break-up σ(E) with contributions from the p3/2, s1/2, p1/2, and d partial waves of 11Be. No-core shell model with continuum (NCSMC) for structure calculations of 11Be. Dynamical eikonal approximation with halo effective field theory (EFT) and ab initio input for reaction mechanism. Comparison with experimental values.
doi: 10.1103/PhysRevC.98.034610
2018GR05 Eur.Phys.J. A 54, 37 (2018) H.W.Griesshammer, J.A.McGovern, D.R.Phillips Comprehensive study of observables in Compton scattering on the nucleon NUCLEAR REACTIONS 1H(γ, γ'), E=0-E(Δ(1232)); calculated, analyzed σ, asymmetry, polarized beams or targets using ChEFT (Chiral Effective Field Theory) (complete at N4LO at photon energies close to pion mass, in the resonance region complete at NLO); deduced asymmetry sensitivity to ill-determined combinations of proton spin polarizabilities.
doi: 10.1140/epja/i2018-12467-8
2018LE16 Phys.Rev. C 98, 051001 (2018) J.Lei, L.Hlophe, Ch.Elster, A.Nogga, F.M.Nunes, D.R.Phillips Few-body universality in the deuteron-α system NUCLEAR STRUCTURE 6Li; calculated d-α S-wave scattering length and absolute value of the n-p-α three body separation energy using variety of phase-shift equivalent nucleon-nucleon and α-nucleon interactions; interpreted as a deuteron or two-nucleon halo nucleus from dα and 6Li correlation.
doi: 10.1103/PhysRevC.98.051001
2018MA42 Eur.Phys.J. A 54, 125 (2018) A.Margaryan, B.Strandberg, H.W.Griesshammer, J.A.McGovern, D.R.Phillips, D.Shukla Elastic Compton scattering from 3He and the role of the Delta NUCLEAR REACTIONS 3He(γ, γ), E=50-120 MeV; calculated elastic Compton scattering σ, σ(θ), beam asymmetry, double asymmetry resulting from circularly polarized photons and longitudinally or transversely polarized target using Chiral Effective Field Theory with explicit Δ(1232) degree of freedom; deduced corrections to N2LO results (without explicit Δ). Compared observables for p, n and d targets.
doi: 10.1140/epja/i2018-12554-x
2018ZH40 Phys.Rev. C 98, 034616 (2018) X.Zhang, K.M.Nollett, D.R.Phillips Models, measurements, and effective field theory: Proton capture on 7Be at next-to-leading order NUCLEAR REACTIONS 7Be(p, γ)8B, E(cm)=100-500 keV; analyzed asymptotic normalization coefficients (ANCs), S factor at astrophysically relevant energies, and reaction amplitudes using halo effective field theory (EFT) at leading-order (LO), and next-to-leading-order (NLO) for capture reactions. Comparison with experimental values. Discussed higher order effects from N2LO and N3LO.
doi: 10.1103/PhysRevC.98.034616
2017HA22 J.Phys.(London) G44, 103002 (2017) H.-W.Hammer, C.Ji, D.R.Phillips Effective field theory description of halo nuclei NUCLEAR STRUCTURE 2H, 4,5,6He, 8,11Li, 11,14Be, 15,19,22C; calculated halo, Efimov states, matter radii, one- and two-neutron separation energies. Effective field theory (EFT).
doi: 10.1088/1361-6471/aa83db
2017TH08 Eur.Phys.J. A 53, 206 (2017) The reactions ππ → ππ and γγ → ππ in x PT with an isosinglet scalar resonance
doi: 10.1140/epja/i2017-12401-8
2016GR05 Eur.Phys.J. A 52, 139 (2016) H.W.Griesshammer, J.A.McGovern, D.R.Phillips Nucleon polarisabilities at and beyond physical pion masses NUCLEAR STRUCTURE 1n, 1H; calculated nucleon polarizability vs pion mass using chiral effective field theory.
doi: 10.1140/epja/i2016-16139-5
2016SA33 Phys.Rev. C 94, 024001 (2016) D.Samart, C.Schat, M.R.Schindler, D.R.Phillips Time-reversal-invariance-violating nucleon-nucleon potential in the 1/Nc expansion
doi: 10.1103/PhysRevC.94.024001
2015FU10 Phys.Rev. C 92, 024005 (2015) R.J.Furnstahl, N.Klco, D.R.Phillips, S.Wesolowski Quantifying truncation errors in effective field theory
doi: 10.1103/PhysRevC.92.024005
2015PA12 Phys.Rev.Lett. 114, 082502 (2015) M.Pavon Valderrama, D.R.Phillips Power Counting of Contact-Range Currents in Effective Field Theory
doi: 10.1103/PhysRevLett.114.082502
2015PH01 Phys.Rev.Lett. 114, 062301 (2015) D.R.Phillips, D.Samart, C.Schat Parity-Violating Nucleon-Nucleon Force in the 1/Nc Expansion
doi: 10.1103/PhysRevLett.114.062301
2014JI12 Phys.Rev. C 90, 044004 (2014) 6He nucleus in halo effective field theory NUCLEAR STRUCTURE 6He; calculated S(2n), two-body amplitudes, properties of the ground state of Borromean halo nucleus 6He described as nnα three-body system in the framework of Halo effective field theory (EFT) built on cluster degrees of freedom. Faddeev formulation. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.044004
2014MY06 Phys.Rev.Lett. 113, 262506 (2014) L.S.Myers, J.R.M.Annand, J.Brudvik, G.Feldman, K.G.Fissum, H.W.Griesshammer, K.Hansen, S.S.Henshaw, L.Isaksson, R.Jebali, M.A.Kovash, M.Lundin, J.A.McGovern, D.G.Middleton, A.M.Nathan, D.R.Phillips, B.Schroder, S.C.Stave, for the COMPTON @ MAX-lab Collaboration Measurement of Compton Scattering from the Deuteron and an Improved Extraction of the Neutron Electromagnetic Polarizabilities NUCLEAR REACTIONS 2H(γ, γ), (γ, E), E=65-115 MeV; measured reaction products, Eγ, Iγ; deduced the isoscalar polarizabilities and reduced the statistical uncertainty on these quantities. Comparison with available data.
doi: 10.1103/PhysRevLett.113.262506
2014PH01 Few-Body Systems 55, 931 (2014) One- and Two-Neutron Halos in Effective Field Theory
doi: 10.1007/s00601-013-0769-z
2014ZH07 Phys.Rev. C 89, 024613 (2014) X.Zhang, K.M.Nollett, D.R.Phillips Combining ab initio calculations and low-energy effective field theory for halo nuclear systems: The case of 7Li + n → 8Li + γ NUCLEAR REACTIONS 7Li(n, γ), E<0.05 keV; calculated total and partial σ(E) in the radiative capture process in the framework of low-energy effective field theory (halo-EFT). The couplings in EFT fixed by calculating asymptotic normalization coefficients (ANCs)of the ground and first excited state in 8Li by ab initio variational Monte Carlo method. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.024613
2014ZH17 Phys.Rev. C 89, 051602 (2014) X.Zhang, K.M.Nollett, D.R.Phillips Combining ab initio calculations and low-energy effective field theory for halo nuclear systems: The case of7Be + p → 8B + γ NUCLEAR REACTIONS 7Be(p, γ)8B, E<0.5 MeV; calculated S(E), zero-energy S factor using Halo leading-order (LO) effective field theory (EFT) to radiative proton capture by treating 8B as shallow proton+7Be core and proton+7Be* (core excitation) p-wave bound state; discussed role of proton-7Be scattering parameters.
doi: 10.1103/PhysRevC.89.051602
2013AC02 Phys.Lett. B 723, 196 (2013) Implications of a matter-radius measurement for the structure of Carbon-22 NUCLEAR STRUCTURE 20,21,22C; calculated binding energies, excited Efimov states, rms matter radius of s-wave Borromean halo nuclei. Comparison with available data.
doi: 10.1016/j.physletb.2013.04.055
2013AC03 Nucl.Phys. A913, 103 (2013) 19C in halo EFT: Effective-range parameters from Coulomb dissociation experiments NUCLEAR REACTIONS 181Ta(19C, n18C), E=88 MeV/nucleon; calculated halo nucleus Coulomb dissociation σ(θ), σ(E), 1n separation energy, n-18C scattering length, longitudinal momentum distribution using EFT (effective field theory); deduced EFT parameters. Compared with available data.
doi: 10.1016/j.nuclphysa.2013.05.021
2013MC02 Eur.Phys.J. A 49, 12 (2013) J.A.McGovern, D.R.Phillips, H.W.Griesshammer Compton scattering from the proton in an effective field theory with explicit Delta degrees of freedom
doi: 10.1140/epja/i2013-13012-1
2013PH02 Phys.Rev. C 88, 034002 (2013) Three-nucleon forces in the 1/Nc expansion
doi: 10.1103/PhysRevC.88.034002
2013YA22 Eur.Phys.J. A 49, 122 (2013) The longitudinal response function of the deuteron in chiral effective field theory NUCLEAR STRUCTURE 2H; calculated wave function, longitudinal response function vs θ, phase shifts vs energy using chiral effective field theory.
doi: 10.1140/epja/i2013-13122-8
2012BA24 Eur.Phys.J. A 48, 69 (2012) V.Baru, E.Epelbaum, C.Hanhart, M.Hoferichter and A.E.Kudryavtsev, D.R.Phillips The multiple-scattering series in pion-deuteron scattering and the nucleon-nucleon potential: perspectives from effective field theory
doi: 10.1140/epja/i2012-12069-6
2012KO35 Phys.Rev. C 86, 047001 (2012) S.Kolling, E.Epelbaum, D.R.Phillips Magnetic form factor of the deuteron in chiral effective field theory
doi: 10.1103/PhysRevC.86.047001
2012LE14 Phys.Rev. C 86, 048201 (2012) V.Lensky, J.A.McGovern, D.R.Phillips, V.Pascalutsa Proton Compton scattering cross section in different variants of chiral effective field theory
doi: 10.1103/PhysRevC.86.048201
2011BA43 Nucl.Phys. A872, 69 (2011) V.Baru, C.Hanhart, M.Hoferichter, B.Kubis, A.Nogga, D.R.Phillips Precision calculation of threshold π-d scattering, πN scattering lengths, and the GMO sum rule NUCLEAR REACTIONS 2H(π-, π-), (π-, π-'), E≈threshold; calculated matrix elements, πN scattering lengths using chiral perturbation theory including isospin-violating corrections; deduced charged-pion-nucleon coupling constant from discussion of validity of Goldberger-Miyazawa-Oehme sum rule in the presence of isospin violation.
doi: 10.1016/j.nuclphysa.2011.09.015
2011HA41 Nucl.Phys. A865, 17 (2011) Electric properties of the Beryllium-11 system in Halo EFT NUCLEAR REACTIONS 11Be(γ, n), (γ, γ'), E=0.5-6.5 MeV; calculated formfactors, electric radius, neutron radius, B(E1), Coulomb excitation; deduced interaction parameters. Effective field theory with local, nonlocal interactions.
doi: 10.1016/j.nuclphysa.2011.06.028
2011KI30 Phys.Rev. C 84, 054004 (2011) Constraining the neutron-neutron scattering length using the effective field theory without explicit pions NUCLEAR STRUCTURE 3H, 3He; calculated splitting in binding energies between 3H and 3He, model-independent correlation between the difference of neutron-neutron and proton-proton scattering lengths; deduced neutron-neutron scattering length using experimental values for binding energies and proton-proton scattering length. Effective field theory without explicit pions.
doi: 10.1103/PhysRevC.84.054004
2009PH02 Nucl.Phys. A822, 1 (2009) D.R.Phillips, M.R.Schindler, R.P.Springer An effective-field-theory analysis of low-energy parity-violation in nucleon-nucleon scattering NUCLEAR REACTIONS 1H(polarized p, p), E=13.6, 45 MeV; 1n, 1H(polarized n, n), E not given; calculated longitudinal analyzing power using pionless effective field theory. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.02.011
2009PH03 J.Phys.(London) G36, 104004 (2009) The chiral structure of the neutron as revealed in electron and photon scattering
doi: 10.1088/0954-3899/36/10/104004
2009SH09 Nucl.Phys. A819, 98 (2009) D.Shukla, A.Nogga, D.R.Phillips Analyzing the effects of neutron polarizabilities in elastic Compton scattering off 3He NUCLEAR REACTIONS 3He(γ, γ), (polarized γ, γ), E(cm)=60, 80, 100, 120 MeV; calculated σ(θ), double-polarization observables; deduced sensitivity to neutron spin polarizabilities. Heavy-baryon chiral perturbation theory. Polarized target.
doi: 10.1016/j.nuclphysa.2009.01.003
2009YA14 Phys.Rev. C 80, 034002 (2009) C.-J.Yang, Ch.Elster, D.R.Phillips Subtractive renormalization of the chiral potentials up to next-to-next-to-leading order in higher NN partial waves
doi: 10.1103/PhysRevC.80.034002
2009YA16 Phys.Rev. C 80, 044002 (2009) C.-J.Yang, Ch.Elster, D.R.Phillips Subtractive renormalization of the NN interaction in chiral effective theory up to next-to-next-to-leading order: S waves
doi: 10.1103/PhysRevC.80.044002
2008PA19 Eur.Phys.J. A 36, 315 (2008) M.Pavon Valderrama, A.Nogga, E.Ruiz Arriola, D.R.Phillips Deuteron form factors in chiral effective theory: Regulator-independent results and the role of two-pion exchange NUCLEAR STRUCTURE 2H; calculated wave function, quadrupole moment, form factors, radius using effective field theory with one-pion and chiral two-pion exchange potentials.
doi: 10.1140/epja/i2007-10581-4
2008SH19 J.Phys.(London) G35, 115009 (2008) D.Shukla, D.R.Phillips, E.Mortenson Chiral potentials, perturbation theory and the 1S0 channel of NN scattering
doi: 10.1088/0954-3899/35/11/115009
2008YA02 Phys.Rev. C 77, 014002 (2008) C.-J.Yang, Ch.Elster, D.R.Phillips Subtractive renormalization of the NN scattering amplitude at leading order in chiral effective theory NUCLEAR REACTIONS p(p, X), E=0-80 keV; calculated phase shifts, wave functions.
doi: 10.1103/PhysRevC.77.014002
2007HA42 Eur.Phys.J. A 32, 335 (2007) H.-W.Hammer, D.R.Phillips, L.Platter Pion-mass dependence of three-nucleon observables NUCLEAR STRUCTURE 3H; calculated ground and excited state binding energies using effective field theory.
doi: 10.1140/epja/i2007-10380-y
2007PH01 J.Phys.(London) G34, 365 (2007) Chiral effective theory predictions for deuteron form factor ratios at low Q2 NUCLEAR STRUCTURE 2H; calculated quadrupole moment, form factor ratios, related features. Chiral effective theory.
doi: 10.1088/0954-3899/34/2/015
2006GA01 Phys.Rev. C 73, 014002 (2006) Using chiral perturbation theory to extract the neutron-neutron scattering length from π-d → nnγ NUCLEAR REACTIONS 2H(π-, nγ), E at rest; calculated neutron spectra, dependence on neutron-neutron scattering length. Chiral perturbation theory, theoretical uncertainties discussed.
doi: 10.1103/PhysRevC.73.014002
2006GA08 Phys.Rev. C 73, 024002 (2006) A.Gardestig, D.R.Phillips, Ch.Elster Near-threshold NN → dπ reaction in chiral perturbation theory NUCLEAR REACTIONS 1H(n, π0), E ≈ threshold; calculated σ. Chiral perturbation theory.
doi: 10.1103/PhysRevC.73.024002
2006GA20 Phys.Rev.Lett. 96, 232301 (2006) How Low-Energy Weak Reactions Can Constrain Three-Nucleon Forces and the Neutron-Neutron Scattering Length NUCLEAR REACTIONS 2H(π-, 2n), E not given; calculated Gamow-Teller matrix elements, neutron spectra; deduced neutron-neutron scattering length.
doi: 10.1103/PhysRevLett.96.232301
2006PL10 Phys.Lett. B 641, 164 (2006) Deuteron matrix elements in chiral effective theory at leading order
doi: 10.1016/j.physletb.2006.08.053
2005BE08 Nucl.Phys. A747, 311 (2005) S.R.Beane, M.Malheiro, J.A.McGovern, D.R.Phillips, U.van Kolck Compton scattering on the proton, neutron, and deuteron in chiral perturbation theory to O(Q4) NUCLEAR REACTIONS 1n, 1,2H(γ, γ'), E ≈ 40-200 MeV; calculated σ(θ). Chiral perturbation theory, comparison with data.
doi: 10.1016/j.nuclphysa.2004.09.068
2005CH31 Phys.Rev. C 71, 044002 (2005) Predictions for polarized-beam and/or vector-polarized-target observables in elastic Compton scattering on the deuteron NUCLEAR REACTIONS 2H(polarized γ, γ), E=50-135 MeV; calculated polarization observables; deduced sensitivity to neutron polarizabilities. Heavy-baryon chiral perturbation theory.
doi: 10.1103/PhysRevC.71.044002
2005HI02 Nucl.Phys. A748, 573 (2005) R.P.Hildebrandt, H.W.Griesshammer, T.R.Hemmert, D.R.Phillips Explicit Δ(1232) degrees of freedom in Compton scattering off the deuteron NUCLEAR REACTIONS 2H(γ, γ), E=49, 69, 94.2 MeV; calculated Compton scattering σ(θ), resonance contribution. Comparison with data.
doi: 10.1016/j.nuclphysa.2004.11.017
2005PA34 Phys.Rev. C 71, 064002 (2005) V.R.Pandharipande, D.R.Phillips, U.van Kolck Δ effects in pion-nucleon scattering and the strength of the two-pion-exchange three-nucleon interaction
doi: 10.1103/PhysRevC.71.064002
2005PH01 Phys.Rev. C 72, 014006 (2005) D.R.Phillips, S.J.Wallace, N.K.Devine Electron-deuteron scattering in the equal-time formalism: Beyond the impulse approximation NUCLEAR REACTIONS 2H(e, e'X), E=high; calculated form factors, structure functions, polarization observables. Three-dimensional formalism, comparison with data.
doi: 10.1103/PhysRevC.72.014006
2005PH02 J.Phys.(London) G31, S1263 (2005) Chiral perturbation theory for electroweak reactions on deuterium NUCLEAR REACTIONS 2H(e, e), E not given; calculated charge and quadrupole form factors. 2H(γ, γ'), E ≈ 50-100 MeV; calculated σ(θ). Chiral perturbation theory, comparison with data.
doi: 10.1088/0954-3899/31/8/004
2004AF01 Phys.Rev. C 69, 034010 (2004) Three-body problem with short-range forces: Renormalized equations and regulator-independent results NUCLEAR REACTIONS 2H(n, n), E=low; calculated phase shifts. Effective field theory, comparison with data.
doi: 10.1103/PhysRevC.69.034010
2004PH03 Nucl.Phys. A737, 52 (2004) M.Poincare visits Jefferson Lab: Relativistic Models of Few-Nucleon Systems NUCLEAR REACTIONS 2H(e, e'X), E=high; calculated form factors, tensor analyzing power. Relativistic models.
doi: 10.1016/j.nuclphysa.2004.03.043
2003BE35 Nucl.Phys. A720, 399 (2003) S.R.Beane, V.Bernard, E.Epelbaum, Ulf-G.Meissner, D.R.Phillips The S-wave pion-nucleon scattering lengths from pionic atoms using effective field theory ATOMIC PHYSICS, Mesic-atoms 1,2H(π-, X), E at rest; analyzed pionic atoms decay data; deduced pion-nucleon scattering lengths.
doi: 10.1016/S0375-9474(03)01008-X
2003BE40 Phys.Lett. B 567, 200 (2003); Erratum Phy.Lett. B 607, 320 (2005) S.R.Beane, M.Malheiro, J.A.McGovern, D.R.Phillips, U.van Kolck Nucleon polarizabilities from low-energy Compton scattering NUCLEAR REACTIONS 1,2H(γ, γ), E ≈ 40-200 MeV; analyzed σ(θ). 1n, 1H deduced polarizabilities.
doi: 10.1016/j.physletb.2003.06.040
2003PA18 Phys.Rev. C 67, 055202 (2003) Effective theory of the Δ(1232) resonance in Compton scattering off the nucleon NUCLEAR REACTIONS 1H(γ, γ'), E ≈ 60-450 MeV; calculated σ(θ), spin-independent polarizabilities. Chiral effective-field theory, comparison with data.
doi: 10.1103/PhysRevC.67.055202
2003PA49 Phys.Rev. C 68, 055205 (2003) Model-independent effects of Δ excitation in nucleon polarizabilities NUCLEAR STRUCTURE 1n, 1H; calculated polarizabilities, Δ resonance contributions.
doi: 10.1103/PhysRevC.68.055205
2003PH01 Phys.Lett. B 567, 12 (2003) Higher-order calculations of electron-deuteron scattering in nuclear effective theory NUCLEAR STRUCTURE 2H; calculated electromagnetic form factors, radius, μ, quadrupole moment. Chiral perturbation theory. NUCLEAR REACTIONS 2H(e, e'X), E not given; calculated electromagnetic form factors. Chiral perturbation theory.
doi: 10.1016/S0370-2693(03)00867-0
2001HA06 Phys.Lett. 499B, 9 (2001) C.Hanhart, D.R.Phillips, S.Reddy Neutrino and Axion Emissivities of Neutron Stars from Nucleon-Nucleon Scattering Data
doi: 10.1016/S0370-2693(00)01382-4
2001PH01 Nucl.Phys. A680, 294c (2001) Probing the Effectiveness: Chiral perturbation theory calculations of low-energy reactions on the deuteron
doi: 10.1016/S0375-9474(00)00431-0
2000CO18 Phys.Rev. C61, 064005 (2000) J.R.Cooke, G.A.Miller, D.R.Phillips Restoration of Rotational Invariance of Bound States on the Light Front
doi: 10.1103/PhysRevC.61.064005
2000PH01 Phys.Lett. 473B, 209 (2000) D.R.Phillips, G.Rupak, M.J.Savage Improving the Convergence of NN Effective Field Theory NUCLEAR STRUCTURE 2H; calculated radius, quadrupole moment. Low-energy effective field theory.
doi: 10.1016/S0370-2693(99)01496-3
2000PH02 Nucl.Phys. A668, 45 (2000) Deuteron Electromagnetic Properties and the Viability of Effective Field Theory Methods in the Two-Nucleon System NUCLEAR REACTIONS 2H(e, e), E not given; analyzed T20(Q). 2H calculated electromagnetic form factors; deduced insensitivity to short-range potential. Effective field theory.
doi: 10.1016/S0375-9474(99)00422-4
2000PH03 Phys.Rev. C61, 044002 (2000) D.R.Phillips, I.R.Afnan, A.G.Henry-Edwards Numerical Renormalization using Dimensional Regularization: A simple test case in the Lippmann-Schwinger equation
doi: 10.1103/PhysRevC.61.044002
1999BE42 Nucl.Phys. A656, 367 (1999) S.R.Beane, M.Malheiro, D.R.Phillips, U.van Kolck Compton Scattering on the Deuteron in Baryon Chiral Perturbation Theory NUCLEAR REACTIONS 2H(γ, γ'), E=49, 69, 95 MeV; calculated Compton scattering σ(θ). Baryon chiral perturbation theory, comparisons with data.
doi: 10.1016/S0375-9474(99)00312-7
1998BE17 Nucl.Phys. A632, 445 (1998) S.R.Beane, T.D.Cohen, D.R.Phillips The Potential of Effective Field Theory in NN Scattering
doi: 10.1016/S0375-9474(98)00007-4
1998PH01 Nucl.Phys. A631, 447c (1998) D.R.Phillips, S.R.Beane, T.D.Cohen Regularization and Renormalization in Effective Theories of the Nucleon-Nucleon Interaction
doi: 10.1016/S0375-9474(98)00045-1
1998PH02 Phys.Rev. C58, 2261 (1998) D.R.Phillips, S.J.Wallace, N.K.Devine Electron-Deuteron Scattering in a Current-Conserving Description of Relativistic Bound States: Formalism and impulse approximation calculations NUCLEAR REACTIONS 2H(e, e), E not given; calculated deuteron form factor, tensor polarization. Equal-time formalism, conserved current. NUCLEAR STRUCTURE 2H; calculated form factor. Equal-time formalism, conserved current.
doi: 10.1103/PhysRevC.58.2261
1997PH01 Phys.Lett. 390B, 7 (1997) How Short is Too Short ( Question ) Constraining Zero-Range Interactions in Nucleon-Nucleon Scattering
doi: 10.1016/S0370-2693(96)01411-6
1997PH02 Phys.Rev. C55, 1937 (1997) D.R.Phillips, M.C.Birse, S.J.Wallace Low-Energy Interaction of Composite Spin-Half Systems with Scalar and Vector Fields
doi: 10.1103/PhysRevC.55.1937
1997SC16 Phys.Rev. C56, 679 (1997) K.A.Scaldeferri, D.R.Phillips, C.-W.Kao, T.D.Cohen Short-Range Interactions in an Effective Field Theory Approach for Nucleon-Nucleon Scattering
doi: 10.1103/PhysRevC.56.679
1996PH01 Phys.Rev. C54, 507 (1996) Relativistic Bound-State Equations in Three-Dimensions
doi: 10.1103/PhysRevC.54.507
1996PH02 Phys.Rev. C54, 1542 (1996); Erratum Phys.Rev. C55, 3178 (1997) Solving the Four-Dimensional NN-πNN Equations for Scalars below the Meson-Production Threshold
doi: 10.1103/PhysRevC.54.1542
1996PH04 Ann.Phys.(New York) 247, 19 (1996) Covariant Four-Dimensional Scattering Equations for the NN → πNN System
doi: 10.1006/aphy.1996.0037
1995JA20 J.Radioanal.Nucl.Chem. 195, 263 (1995) D.J.Jamriska, Sr., W.A.Taylor, M.A.Ott, R.C.Heaton, D.R.Phillips, M.M.Fowler Activation Rates and Chemical Recovery of 67Cu Produced with Low Energy Proton Irradiation of Enriched 70Zn Targets NUCLEAR REACTIONS 70Zn(p, α), E=18.1, 18.8 MeV; measured residual production rate.
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