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NSR database version of April 27, 2024.

Search: Author = M.G.Huber

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2020HA02 Phys.Rev.Lett. 124, 012501 (2020)

R.Haun, F.E.Wietfeldt, M.Arif, M.G.Huber, T.C.Black, B.Heacock, D.A.Pushin, C.B.Shahi

Precision Measurement of the Neutron Scattering Length of ⁴He Using Neutron Interferometry

NUCLEAR REACTIONS ⁴He(n, n), E not given; measured reaction products, En, In; deduced the bound neutron scattering length of ⁴He using neutron interferometry.

doi: 10.1103/PhysRevLett.124.012501
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2019GE07 Phys.Rev. C 100, 034005 (2019)

T.R.Gentile, M.G.Huber, D.D.Koetke, M.Peshkin, M.Arif, T.Dombeck, D.S.Hussey, D.L.Jacobson, P.Nord, D.A.Pushin, R.Smither

Direct observation of neutron spin rotation in Bragg scattering due to the spin-orbit interaction in silicon

NUCLEAR MOMENTS ¹n; measured rotation of neutron spin, caused by interaction of a moving neutron's magnetic dipole moment (MDM) with the atomic electric field, using the technique of multiple Bragg reflections in silicon at the neutron guide NG-6A beam line at the NIST Center for Neutron Research (NCNR); deduced neutron spin-orbit interaction, or Schwinger scattering. Comparison with theoretical value.

doi: 10.1103/PhysRevC.100.034005
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2016MU05 Phys.Rev. C 93, 065502 (2016)

H.P.Mumm, M.G.Huber, W.Bauder, N.Abrams, C.M.Deibel, C.R.Huffer, P.R.Huffman, K.W.Schelhammer, R.Janssens, C.L.Jiang, R.H.Scott, R.C.Pardo, K.E.Rehm, R.Vondrasek, C.M.Swank, C.M.O'Shaughnessy, M.Paul, L.Yang

High-sensitivity measurement of ³He - ⁴He isotopic ratios for ultracold neutron experiments

ATOMIC MASSES ^3,4He; measured absolute isotopic ratio of ³He to ⁴He with a high sensitivity at ATLAS-ANL facility. Relevance to neutron half-life measurements using ultra-cold neutrons.

doi: 10.1103/PhysRevC.93.065502
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2014HU23 Phys.Rev. C 90, 064004 (2014)

M.G.Huber, M.Arif, W.C.Chen, T.R.Gentile, D.S.Hussey, T.C.Black, D.A.Pushin, C.B.Shahi, F.E.Wietfeldt, L.Yang

Neutron interferometric measurement of the scattering length difference between the triplet and singlet states of n-³He

NUCLEAR REACTIONS ³He(n, n), E=low; measured neutron polarization, spin-dependent scattering length between the triplet and singlet states of n-³He system using neutron interferometric technique at NIST reactor facility. Polarized ³He target.

doi: 10.1103/PhysRevC.90.064004
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2009HU14 Nucl.Instrum.Methods Phys.Res. A611, 235 (2009)

M.G.Huber, F.E.Wietfeldt, T.R.Gentile, W.C.Chen, M.Arif, D.A.Hussey, D.A.Pushin, L.Yang, T.Black

Precision measurement of the neutron-³He spin-dependent scattering length using neutron interferometry

NUCLEAR REACTIONS ³He(n, n), E=reactor spectrum; measured En, In, neutron spectra;deduced neutron polarization, spin-dependent scattering length.

doi: 10.1016/j.nima.2009.07.062
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1991HA22 Z.Phys. A340, 399 (1991)

L.Harzheim, M.G.Huber, B.C.Metsch

Pion Production in Nuclear Collisions

NUCLEAR REACTIONS ¹H(p, π⁺), E=295-810 MeV; ²H(p, π⁰), E=340-500 MeV; ³He(³He, π⁺), E=300-600 MeV; calculated σ(θ). Microscopic reaction model, nucleon resonance excitation role in channel coupling, other high energy data analysis included.

doi: 10.1007/BF01290328
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1990HU03 Z.Phys. C46, S37 (1990)

M.G.Huber, B.Ch.Metsch

KAON and COSY - Common Aspects in Hadron Physics

NUCLEAR REACTIONS ¹²C(π, π), E=260 MeV; calculated σ(θ), scattering amplitude.

1983HU02 Nucl.Phys. A396, 191c (1983)

M.G.Huber, K.Klingenbeck, R.Hupke

Pionic Fusion - A Tool to Coherently Produce New Isotopes -

NUCLEAR REACTIONS ⁴He(³He, π⁺), E=268, 283 MeV; calculated σ(θ). ⁶Li(d, π^-), E=200-600 MeV; calculated σ(θ) vs E. Fusion model.

doi: 10.1016/0375-9474(83)90019-2
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1981KL01 Phys.Lett. B98, 15 (1981)

K.Klingenbeck, M.G.Huber

Excitation of A* Resonances in Deep Inelastic Electron Scattering

NUCLEAR REACTIONS ¹²C(e, e'), E=480, 500 MeV; calculated response function vs E, θ; deduced isobar-nucleon dynamics in nuclear medium. Deep inelastic scattering.

doi: 10.1016/0370-2693(81)90356-7
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1981KL07 Phys.Rev.Lett. 47, 1654 (1981)

K.Klingenbeck, M.Dillig, M.G.Huber

Pionic Fusion in Nucleus-Nucleus Collisions

NUCLEAR REACTIONS ³He(³He, π⁺), E=282, 268.5 MeV; calculated σ(θ). Microscopic model, complete fusion, two nucleon meson exchange.

doi: 10.1103/PhysRevLett.47.1654
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1980KL03 Phys.Rev. C22, 681 (1980)

K.Klingenbeck, M.G.Huber

Unified Description of Inelastic Pion Nucleus Reactions in the A* Model

NUCLEAR REACTIONS ¹²C(π, π'), (π⁺, π), (π⁺, γ), E=240-370 MeV; calculated σ(θ), total σ(E); deduced role of IAS excitation. T-matrix, single charge exchange, radiative pion capture in flight mechanisms.

doi: 10.1103/PhysRevC.22.681
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1980KL04 J.Phys.(London) G6, 961 (1980)

K.Klingenbeck, M.G.Huber

Pionic and Electromagnetic Excitation of A* Resonances

NUCLEAR REACTIONS ¹²C(γ, π⁰), E=10-180 MeV; calculated σ(θ); deduced nucleus-baryon resonances. DWIA, isobar doorway model.

doi: 10.1088/0305-4616/6/8/007
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1978HA06 Phys.Lett. 73B, 4 (1978)

R.Handel, M.Dillig, M.G.Huber

Pion-Deuteron Scattering in a D* Model

NUCLEAR REACTIONS ²H(π, π), E=87, 140, 180, 256, 300 MeV; calculated σ(θ), A(θ).

doi: 10.1016/0370-2693(78)90157-0
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1978KL06 Phys.Rev.Lett. 41, 387 (1978)

K.Klingenbeck, M.Dillig, M.G.Huber

Collective Resonances in Pion-Nucleus Scattering

NUCLEAR REACTIONS ¹²C(π^-, π^-), (π^-, π^-'), E=250-340 MeV; calculated σ(θ).

doi: 10.1103/PhysRevLett.41.387
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1977DI06 Lett.Nuovo Cim. 18, 487 (1977)

M.Dillig, C.Helwig, M.G.Huber

Investigation of Deuteron-Induced Pion Production Near Threshold

NUCLEAR REACTIONS ¹²C(d, π⁺), E=185 MeV; calculated σ(θ).

doi: 10.1007/BF02785065
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1977GR02 Phys.Rev. C15, 837 (1977)

E.Grecksch, W.Knupfer, M.G.Huber

Electroexcitation of Collective M1 Resonances in ¹²C

NUCLEAR STRUCTURE ¹²C; calculated electroexcited M1 resonances.

doi: 10.1103/PhysRevC.15.837
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1977GR24 Phys.Lett. 72B, 11 (1977)

E.Grecksch, M.Dillig, M.G.Huber

Virtual Isobar Admixtures in Complex Nuclei

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ²⁸Si, ⁴⁰Ca; calculated levels, B(λ).

doi: 10.1016/0370-2693(77)90050-8
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1977KL02 Phys.Rev. C15, 1483 (1977)

K.Klingenbeck, W.Knupfer, M.G.Huber, P.W.M.Glaudemans

Central and Noncentral Components of the Effective sd-Shell Interaction

NUCLEAR STRUCTURE ²⁸Si; calculated levels, tensor effects.

doi: 10.1103/PhysRevC.15.1483
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1977KN02 Phys.Lett. 66B, 305 (1977)

W.Knupfer, K.Knauss, M.G.Huber

Giant Multipole Resonances in an Excited Core Model

NUCLEAR STRUCTURE ^20,22Ne; calculated giant multipole resonances, parameters.

doi: 10.1016/0370-2693(77)90001-6
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1977KN03 Z.Phys. A280, 175 (1977)

W.Knupfer, E.Grecksch, M.G.Huber

Splitting of the Isovector Giant Quadrupole Resonances in ¹²C and ¹⁶O

NUCLEAR STRUCTURE ¹²C, ¹⁶O; calculated splitting of isovector GQR, B(λ).

1976DI10 Lett.Nuovo Cim. 16, 293 (1976)

M.Dillig, M.G.Huber

Proton Induced π^- Production Near Threshold

NUCLEAR REACTIONS ⁹Be, ¹³C(p, π^-), E ≈ 185 MeV; calculated σ(θ).

doi: 10.1007/BF02747089
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1976DI11 Lett.Nuovo Cim. 16, 299 (1976)

M.Dillig, M.G.Huber

Nuclear Pion Production as a Direct Reaction

NUCLEAR REACTIONS ¹³C(p, π⁺), (p, π^-), E=185 MeV; calculated σ.

doi: 10.1007/BF02747090
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1976KN02 Z.Phys. A276, 99 (1976)

W.Knupfer, M.G.Huber

Splitting of the Isoscalar E0 and E2 Giant Multipole Resonances in ¹⁶O

NUCLEAR STRUCTURE ¹⁶O; calculated giant resonance excitation, B(E2).

1976KN06 Phys.Rev. C14, 2254 (1976)

W.Knupfer, M.G.Huber

Universal Relationship Connecting Various Two-Body Effective Residual Interactions

NUCLEAR STRUCTURE ¹⁶O; calculated levels, T=1 strength. ⁸⁸Sr; calculated B(E2), B(E3). ²⁰⁸Pb; calculated excitation, transition strengths. ^59,62Ni; calculated levels. ⁴⁸Ca, ⁵⁰Ti, ⁵²Cr, ⁵⁴Fe, ⁵⁶Ni; calculated quadrupole moment.effective residual interaction.

doi: 10.1103/PhysRevC.14.2254
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1976WE27 Phys.Lett. 65B, 189 (1976)

E.Weber, W.Knupfer, E.Grecksch, M.G.Huber

Electroexcitation of High Spin States in ²⁰⁸Pb

NUCLEAR STRUCTURE ²⁰⁸Pb; calculated electroexcitation form factors.

doi: 10.1016/0370-2693(76)90159-3
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1975GR33 Lett.Nuovo Cim. 14, 505 (1975)

E.Grecksch, W.Knupfer, M.G.Huber

Giant Multipole Resonances in ²⁰⁸Pb

NUCLEAR STRUCTURE ²⁰⁸Pb; calculated giant resonances, B(λ).

doi: 10.1007/BF02746044
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1974DI20 Lett.Nuovo Cim. 11, 728 (1974)

M.Dillig, M.G.Huber

Proton-Induced Production of Negative Pions on ⁹Be

NUCLEAR REACTIONS ⁹Be(p, π⁺), (p, π^-), E=185 MeV; calculated σ, correlation parameters.

doi: 10.1007/BF02762938
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1973DI08 Phys.Lett. 44B, 484 (1973)

M.Dillig, H.M.Hofmann, M.G.Huber

Microscopic Description of Nuclear π⁺ Production in ¹²C

NUCLEAR REACTIONS ¹²C(p, π⁺), E=185 MeV; calculated σ(Eπ+, θ).

doi: 10.1016/0370-2693(73)90003-8
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1971WE04 Nucl.Phys. A162, 330 (1971)

W.Weise, M.G.Huber

A Microscopic Analysis of the (γ, p) and (γ, n) Reactions at Medium Photon Energies

NUCLEAR REACTIONS ¹⁶O(γ, n), (γ, p), E=40-140 MeV; calculated σ(E).

doi: 10.1016/0375-9474(71)90988-2
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1970CH25 Phys.Lett. 32B, 536 (1970)

K.Chung, M.G.Huber, B.Blum, M.Danos

Pion Absorption in the Oxygen Isotopes

ATOMIC PHYSICS, Mesic-Atoms ¹⁶O, ¹⁸O; calculated π absorption rates. Independent-particle model, short-range N-N correlations.

doi: 10.1016/0370-2693(70)90536-8
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1970HU18 Ann.Phys.(Paris) 5, 239 (1970)

M.G.Huber

Short Range Correlations in Nuclei

NUCLEAR REACTIONS ¹⁶O(γ, n), (γ, p), (γ, pn), E=40-160 MeV; calculated σ(E). ¹⁶O(π^-, X), E approx o; calculated absorption rates. ⁴⁰Ca(e, e), E=758 MeV/c; calculated inelastic form factor. Independent particle model, short-range correlations.

1970WR01 Lett.Nuovo Cimento 3, 253 (1970)

L.E.Wright, S.-T.Tuan, M.G.Huber

Short-Range Correlations in ⁴⁰Ca

NUCLEAR REACTIONS ⁴⁰Ca(e, e), E=757.5 MeV/c; calculated σ(θ). ⁴⁰Ca calculated nuclear charge distribution.

doi: 10.1007/BF02755756
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1969TU01 Phys.Rev.Letters 23, 174 (1969)

S.T.Tuan, L.E.Wright, M.G.Huber

Short-Range Correlations and Elastic Electron Scattering

NUCLEAR REACTIONS ¹⁶O(e, e), E=100-900 MeV/c; calculated form factor; deduced short-range correlation effects.

doi: 10.1103/PhysRevLett.23.174
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1968CA05 Nucl.Phys. A109, 385 (1968)

P.H.Cannington, R.J.J.Stewart, B.M.Spicer, M.G.Huber