NSR Query Results


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NSR database version of April 27, 2024.

Search: Author = M.Lahanas

Found 5 matches.

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1998AN15      Phys.Lett. 432B, 8 (1998); Erratum Phys.Lett. 444B, 583 (1998)

N.G.Antoniou, F.K.Diakonos, C.N.Ktorides, M.Lahanas

Critical Events and Intermittency in Nuclear Collisions

doi: 10.1016/S0370-2693(98)00629-7
Citations: PlumX Metrics


1997AN22      J.Phys.(London) G23, 1953 (1997)

N.G.Antoniou, Y.F.Contoyiannis, F.K.Diakonos, C.N.Ktorides, M.Lahanas

Strangeness in Chiral QCD Phase Transition

doi: 10.1088/0954-3899/23/12/020
Citations: PlumX Metrics


1987RY01      Z.Phys. A326, 455 (1987)

D.Rychel, R.Gyufko, B.van Kruchten, M.Lahanas, P.Singh, C.A.Wiedner

Isospin Decomposition of 0+ → 2+ and 0+ → 3- Transition Matrix Elements by Coulomb Nuclear Interference Observed in Inelastic α-Scattering from the Even Zr Isotopes

NUCLEAR REACTIONS 90,92,94,96Zr(α, α), (α, α'), E=35.4 MeV; measured σ(θ). 90,92,94,96Zr levels deduced B(E2), neutron, proton transition matrix elements ratios. Spectrograph. DWBA analyses.


1986LA18      Nucl.Phys. A455, 399 (1986)

M.Lahanas, D.Rychel, P.Singh, R.Gyufko, D.Kolbert, B.Van Kruchten, E.Madadakis, C.A.Wiedner

Inelastic α-Scattering from 90Zr and 96Zr

NUCLEAR REACTIONS 90,96Zr(α, α'), E=35.4 MeV; measured σ(θ). 90,96Zr deduced levels, J, π, L, isoscalar transition rates, deformation lengths. Enriched targets. DWBA calculations.

doi: 10.1016/0375-9474(86)90314-3
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0847.


1986SI17      Nucl.Phys. A458, 1 (1986)

P.Singh, D.Rychel, R.Gyufko, B.van Kruchten, M.Lahanas, C.A.Wiedner

Alpha Scattering from 92Zr and 94Zr

NUCLEAR REACTIONS 92,94Zr(α, α'), E=35.4 MeV; measured σ(θ). 92,94Zr levels deduced J, π, deformation lengths, isoscalar transition rates. Enriched targets.

doi: 10.1016/0375-9474(86)90279-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0081.


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