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NSR database version of May 3, 2024.

Search: Author = B.Krippa

Found 28 matches.

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2013BI03      Phys.Rev. C 87, 054001 (2013)

M.C.Birse, B.Krippa, N.R.Walet

Functional renormalization group for few-nucleon systems: SU(4) symmetry and its breaking

doi: 10.1103/PhysRevC.87.054001
Citations: PlumX Metrics


2007KR07      Eur.Phys.J. A 31, 734 (2007)

B.Krippa

Superfluidity in many fermion systems: Exact renormalisation group treatment

doi: 10.1140/epja/i2006-10286-2
Citations: PlumX Metrics


2006KR13      Phys.Lett. B 643, 104 (2006)

B.Krippa

Pairing in fermion systems with unequal masses: Nonperturbative renormalisation group approach

doi: 10.1016/j.physletb.2006.10.045
Citations: PlumX Metrics


2005BI01      Phys.Lett. B 605, 287 (2005)

M.C.Birse, B.Krippa, J.A.McGovern, N.R.Walet

Pairing in many-fermion systems: an exact renormalisation group treatment

doi: 10.1016/j.physletb.2004.11.044
Citations: PlumX Metrics


2005KR02      Nucl.Phys. A749, 134c (2005)

B.Krippa, M.C.Birse, N.R.Walet, J.A.McGovern

Exact Renormalisation Group and pairing in many-fermion systems

doi: 10.1016/j.nuclphysa.2004.12.022
Citations: PlumX Metrics


2003KR04      Phys.Rev. C 67, 031301 (2003)

B.Krippa, M.C.Birse, J.A.McGovern, N.R.Walet

Off-shell effects and consistency of many-body treatments of dense matter

doi: 10.1103/PhysRevC.67.031301
Citations: PlumX Metrics


2002KR15      Yad.Fiz. 65, 1452 (2002); Phys.Atomic Nuclei 65, 1417 (2002)

B.V.Krippa, B.L.G.Bakker

Effective Theory of NN Interactions in a Separable Representation

doi: 10.1134/1.1501653
Citations: PlumX Metrics


2001KR18      Phys.Rev. C64, 047602 (2001)

B.Krippa

Chiral Expansion for Low-Energy η-Nucleon Interactions with Explicit Resonance

NUCLEAR REACTIONS 1H(π, X), E ≈ 550-900 MeV; calculated η meson production σ, η-nucleon scattering length. Comparison with data.

doi: 10.1103/PhysRevC.64.047602
Citations: PlumX Metrics


2000KR09      Nucl.Phys. A672, 270 (2000)

B.Krippa

Chiral Symmetry and Properties of Hadron Correlators in Matter

doi: 10.1016/S0375-9474(99)00857-X
Citations: PlumX Metrics


1998KR05      Phys.Lett. 420B, 13 (1998)

B.Krippa

Kaon-Baryon Coupling Constants from QCD Sum Rules Analysis

doi: 10.1016/S0370-2693(97)01454-8
Citations: PlumX Metrics


1998KR09      Phys.Lett. 427B, 13 (1998)

B.Krippa

Chiral Symmetry and Mixing of Axial and Vector Correlators in Matter

doi: 10.1016/S0370-2693(98)00309-8
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1998KR12      Phys.Rev. C58, 1333 (1998)

B.Krippa

Chiral Dynamics of the Low Energy Kaon-Baryon Interactions

NUCLEAR REACTIONS 1H(K-, X), E=50-200 MeV; calculated σ; deduced sensitivity to cutoff parameter.

doi: 10.1103/PhysRevC.58.1333
Citations: PlumX Metrics


1998KR15      Phys.Rev. C58, 1634 (1998)

B.Krippa, J.T.Londergan

Chiral Dynamics of Low-Energy Kaon-Baryon Interactions with Explicit Resonance

NUCLEAR REACTIONS 1H(K-, K-), (K-, π0X), (K-, π+X), (K-, π-X), (K-, K0), E at 50-200 MeV/c; calculated total σ. Chiral perturbation theory with Λ(1405) as independent field. Comparison with data.

doi: 10.1103/PhysRevC.58.1634
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1996BI08      Phys.Lett. 373B, 9 (1996)

M.C.Birse, B.Krippa

Determination of the Pion-Nucleon Coupling Constant from QCD Sum Rules

doi: 10.1016/0370-2693(96)00133-5
Citations: PlumX Metrics


1996BI09      Phys.Lett. 381B, 397 (1996)

M.C.Birse, B.Krippa

Chiral Symmetry and QCD Sum Rules for the Nucleon Mass in Matter

doi: 10.1016/0370-2693(96)00636-3
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1996BI22      Phys.Rev. C54, 3240 (1996); Comments Phys.Rev. C61, 019801 (1999)

M.C.Birse, B.Krippa

Determination of Pion-Baryon Coupling Constants from QCD Sum Rules

doi: 10.1103/PhysRevC.54.3240
Citations: PlumX Metrics


1995KA15      Phys.Rev. C51, 2829 (1995)

M.A.Kagarlis, B.Krippa

Inelastic K+-Nucleus Scattering

NUCLEAR REACTIONS 12C(K+, K+), (K+, K+'), E at 500, 800 MeV/c; analyzed σ(θ). Coupled-channels approach.

doi: 10.1103/PhysRevC.51.2829
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1995KR10      Z.Phys. A351, 411 (1995)

B.V.Krippa

Estimates of Hypernuclear Production via the Exclusive (p, K+) Reaction

NUCLEAR REACTIONS 12C, 16O(p, K+), E=0.8-1.2 GeV; 17O(π+, K+), E=1.05 GeV; calculated hypernucleus production σ(θ). DWIA.

doi: 10.1007/BF01291147
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1995KR11      Phys.Lett. 351B, 406 (1995)

B.Krippa, W.Cassing, U.Mosel

Exclusive Meson Production in p-Nucleus Collisions in the 1 GeV Energy Range

NUCLEAR REACTIONS 16O, 12C(p, π+), E=489, 800 MeV; calculated σ(θ). 12C(p, X), E=0.8, 1 GeV; calculated eta production σ(θ). Impulse approximation, momentum space, relativistic wave functions.

doi: 10.1016/0370-2693(95)00366-S
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1995KR12      Nucl.Phys. A592, 539 (1995)

B.Krippa, W.Cassing, U.Mosel

Exclusive Meson Production in Hadron-Nucleus Collisions

NUCLEAR REACTIONS 12C, 16O(p, π+), E=800 MeV; calculated σ(θ). 13C(π, X), E=490-1000 MeV; calculated η production σ(θ).

doi: 10.1016/0375-9474(95)00313-P
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1993KA15      Yad.Fiz. 56, No 5, 245 (1993); Phys.At.Nuclei 56, 701 (1993)

M.V.Kazarnovsky, B.V.Krippa, Yu.M.Nikolaev

Production of Pionic Atoms in the (d, 3He) Reaction

NUCLEAR REACTIONS 40Ca(d, 3He), E=510 MeV; calculated σ(θ). 40Ca(d, 3He), E ≈ 450-575 MeV; calculated σ(E); deduced hadronic distortions role. Pionic atom production.


1993KR10      Phys.Scr. 48, 76 (1993)

B.V.Krippa, J.T.Londergan

Inclusive and Exclusive Production of (Eta) Mesons Near Threshold

NUCLEAR REACTIONS 13C(π+, X), E at 620-680 MeV/c; calculated eta-production σ(θ), σ. Momentum space DWIA model.

doi: 10.1088/0031-8949/48/1/011
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1993KR11      Phys.Scr. 48, 79 (1993)

B.V.Krippa, E.Ya.Paryev

Production of (Eta)-Mesons in the Proton-Nucleus Reactions

NUCLEAR REACTIONS 11B(p, X), E=1 GeV; 12C(p, X), E=0.8-1 GeV; calculated eta production σ(θ, E(eta)). Quasiclassical formula.

doi: 10.1088/0031-8949/48/1/012
Citations: PlumX Metrics


1993KR12      Yad.Fiz. 56, No 5, 172 (1993); Phys.At.Nuclei 56, 666 (1993)

B.V.Krippa, E.Ya.Parev

Inclusive Production of Eta and Omega Mesons in Proton-Nucleus Reactions

NUCLEAR REACTIONS 11B(p, X), E=1 GeV; calculated eta spectra. 12C(p, X), E=1.6, 1.8 GeV; calculated omega-meson spectrum. 12C(p, X), E ≈ 900-100 MeV; calculated σ(θ(eta), E(eta)). First collision approximation.


1993KR17      Phys.Rev. C48, 2967 (1993)

B.V.Krippa, J.T.Londergan

Inclusive and Exclusive Production of (Eta) Mesons by Pions

NUCLEAR REACTIONS 12C(π+, X), E at 620, 680 MeV/c; 13C(π+, X), E at 650, 680 MeV/c; calculated inclusive, exclusive σ(θ, E(eta)). 12C(π+, π+), E at 800 MeV/c; calculated σ(θ). Momentum space DWIA.

doi: 10.1103/PhysRevC.48.2967
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1992KA20      Z.Phys. A342, 229 (1992)

M.V.Kazarnovsky, B.V.Krippa, Yu.M.Nikolaev

Production of Bound State Pions in Nucleon-Nucleus Reactions

NUCLEAR REACTIONS 120Sn, 40Ca(n, dπ-), E ≈ 300-400 MeV; 40Ca, 120Sn(p, 2pπ-), E ≈ 300-400 MeV; calculated σ(E), σ(θ); deduced nucleon, deuteron distortion contributions.


1992KR10      Phys.Lett. 286B, 216 (1992)

B.V.Krippa, J.T.Londergan

Inclusive (π, Eta) Reactions on Nuclei

NUCLEAR REACTIONS 12C(π+, X), E at 680 MeV/c; calculated inclusive eta production σ(θ, E). Momentum space DWIA, quasifree single-nucleon knockout, mediation by nucleon resonance.

doi: 10.1016/0370-2693(92)91764-Z
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1991KA13      Yad.Fiz. 53, 710 (1991); Sov.J.Nucl.Phys. 53, 444 (1991)

M.V.Kazarnovsky, B.V.Krippa, Yu.M.Nikolaev

Production of Pions in a Bound State in Nucleon-Nucleus Reactions

NUCLEAR REACTIONS 40Ca, 120Sn(n, d), E=300-400 MeV; 40Ca, 120Sn(p, 2p), E=300-380 MeV; calculated σ(E), σ(θ) for π- production in bound state; deduced nucleon, deuteron wave function distortions.


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Note: The following list of authors and aliases matches the search parameter B.Krippa: , B.V.KRIPPA