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NSR database version of April 29, 2024.

Search: Author = E.N.Gazis

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2000ST16      Nucl.Phys. A663-664, 1095c (2000)

E.Stiliaris, D.Baltadoros, M.Barbarosou, S.Cohen, D.Economou, T.A.Filippas, E.N.Gazis, N.Giokaris, H.Herminghaus, A.Karabarbounis, D.Maroulis, E.Meintanis, N.H.Papadakis, C.N.Papanicolas, P.Phinou, N.Sparveris, N.Uzunglou, A.Zolfaghari

The IASA RaceTrack Microtron Facility

doi: 10.1016/S0375-9474(99)00785-X
Citations: PlumX Metrics

1994GA06      Nucl.Phys. A569, 603 (1994)

E.N.Gazis, R.Vlastou, C.T.Papadopoulos, A.E.Aravantinos, E.Adamides, A.C.Xenoulis, U.Lenz, K.E.G.Lobner, K.Rudolph, S.J.Skorka, H.G.Thies

Investigation on Some ¹⁶O + ¹²C Resonances by the pn to d Competition Ratio Technique

NUCLEAR REACTIONS ¹²C(¹⁶O, np), (¹⁶O, d), E=26-31, 44-48 MeV; measured relative σ(E) for pn-, d-emission; calculated relative σ(E) for pn-, d-emission.

doi: 10.1016/0375-9474(94)90321-2
Citations: PlumX Metrics

1990XE01      Nucl.Phys. A516, 108 (1990)

A.C.Xenoulis, A.E.Aravantinos, G.P.Eleftheriades, C.T.Papadopoulos, E.N.Gazis, R.Vlastou

The Competition between p2n, dn and t Emission in Heavy-Ion Induced Nuclear Reactions

NUCLEAR REACTIONS ¹³C, ¹⁸O(¹⁶O, X), ¹²C, ¹⁸O, ¹⁹F(¹⁸O, X), ¹²C(¹⁹F, X), ³⁰Si(⁷Li, X), E=10-16 MeV; measured relative σ(E) for p2n, dn, t emission; calculated relative σ(E) for p2n, dn and t emission.

doi: 10.1016/0375-9474(90)90051-M
Citations: PlumX Metrics

1986AD04      Phys.Rev. C34, 791 (1986)

E.Adamides, J.Sinatkas, L.D.Skouras, A.C.Xenoulis, E.N.Gazis, C.T.Papadopoulos, R.Vlastou

Structure of ⁹⁶Ru

NUCLEAR REACTIONS ⁹⁶Ru(p, p'γ), E=7 MeV; measured Eγ, Iγ, γγ-coin, DSA, γ(θ), oriental nuclei. ⁹⁶Ru deduced levels, J, π, γ-branching, B(λ), δ(E2/M1).

doi: 10.1103/PhysRevC.34.791
Citations: PlumX Metrics

1986GA13      Phys.Rev. C34, 872 (1986)

E.N.Gazis, C.T.Papadopoulos, R.Vlastou, A.C.Xenoulis

pn to d and αpn to αd Emission Ratios in Heavy-Ion-Induced Reactions

NUCLEAR REACTIONS ¹²C(¹⁶O, np), (¹⁶O, d), E(cm)=11.6-16.1 MeV; ¹³C(¹⁶O, np), (¹⁶O, d), E(cm)=12.1-14.3 MeV; ¹⁶O(¹⁶O, np), (¹⁶O, d), E(cm)=15, 15.5 MeV; ²⁷Al(¹⁶O, np), (¹⁶O, d), E(cm)=18.8 MeV; ¹²C(¹⁸O, np), (¹⁸O, d), E(cm)=12.4 MeV; ¹⁶O(¹⁸O, np), (¹⁸O, d), E(cm)=13.8, 15.5 MeV; ¹⁹F(¹⁸O, np), (¹⁸O, d), E(cm)=15.4, 15.9 MeV; ²⁸Si(¹⁸O, np), (¹⁸O, d), E(cm)=16.7-20.7 MeV; ¹⁹F(¹²C, npα), (¹²C, dα), E(cm)=31.9 MeV; ¹⁶O(¹³C, npα), (¹³C, dα), E(cm)=18.2 MeV; ¹⁸O(¹⁸O, npα), (¹⁸O, dα), E(cm)=15.5 MeV; ¹⁹F(¹⁸O, npα), (¹⁸O, dα), E(cm)=15.4 MeV; ²⁸Si(¹⁸O, npα), (¹⁸O, dα), E(cm)=16.7 MeV; measured pγ-, dγ-coin; deduced σ(pn)/σ(d), σ(αpn)/σ(αd). ^30,29,28Si, ^34,32,36S, ⁴³K, ^31,37P, ⁴⁶Ca deduced multi-particle, light particle emission competition. Silicon surface barrier telescope, Ge(Li) detectors, enriched targets. Statistical model.

doi: 10.1103/PhysRevC.34.872
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1986PA10      Phys.Rev. C34, 196 (1986)

C.T.Papadopoulos, R.Vlastou, E.N.Gazis, P.A.Assimakopoulos, C.A.Kalfas, S.Kossionides, A.C.Xenoulis

Fusion Cross Section of the ¹⁶O + ¹³C Reaction

NUCLEAR REACTIONS, ICPND ¹³C(¹⁶O, X)²⁸Si/²⁷Si/²⁴Mg/²¹Ne/²⁴Na/²⁷Mg/²⁵Mg/²⁷Al, ¹³C(¹⁶O, 2n), (¹⁶O, nα), (¹⁶O, 2α), (¹⁶O, α), (¹⁶O, 2p), (¹⁶O, np), (¹⁶O, pα), E(cm)=7.8-14.6 MeV; measured Eγ, Iγ, residual production σ(E); deduced fusion σ(E). Statistical model analysis. Ge(Li) detector, enriched target.

doi: 10.1103/PhysRevC.34.196
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1638.

1981GA21      Phys.Rev. C24, 762 (1981)

E.N.Gazis, P.Kakanis, A.C.Xenoulis

Contribution of Unbound Deuteron Disintegration to the Reaction ¹²C(¹⁶O, pn)²⁶Al

NUCLEAR REACTIONS ¹²C(¹⁶O, np), E=30 MeV; measured pn-coin, Ep; deduced unbound deuteron emission contribution. Ge(Li), Si surface barrier, NE 213 scintillation detectors.

doi: 10.1103/PhysRevC.24.762
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1981PA17      Z.Phys. A302, 117 (1981)

A.D.Panagiotou, P.K.Kakanis, E.N.Gazis, M.Bernas, C.Detraz, M.Langevin, D.Guillemaud, E.Plagnol

A New Mass Measurement of ²⁹Mg. Observation of Excited States via the ¹³C(¹⁸O, 2p)²⁹Mg Reaction

NUCLEAR REACTIONS ¹³C(¹⁸O, 2p), E=32 MeV; measured pp-coin, σ(Ep₁, Ep₂, θ). ²⁹Mg deduced mass excess, levels. Silicon surface barrier detectors.

doi: 10.1007/BF01413040
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1980XE01      Phys.Lett. 90B, 224 (1980)

A.C.Xenoulis, E.N.Gazis, P.Kakanis, D.Bucurescu, A.D.Panagiotou

Competition between Exit Channels Leading to the Same Residual Nucleus in Heavy-Ion Reactions

NUCLEAR REACTIONS ¹³C, ¹²C(¹⁶O, np), (¹⁶O, d), (¹⁶O, 2np), (¹⁶O, nd), (¹⁶O, t), E=24-38 MeV; measured particle γ-coin. ²⁶Al level deduced exit channel competition. Hauser-Feshbach analysis.

doi: 10.1016/0370-2693(80)90728-5
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1977PA11      J.Phys.(London) G3, L85 (1977)

A.D.Panagiotou, P.Kakanis, E.N.Gazis, E.Kossionides, N.Xiromeritis

The (¹⁶O, 2p) Reaction on Light Nuclei

NUCLEAR REACTIONS ¹²C, ¹⁶O, ²⁷Al(¹⁶O, 2p), E ≈ 35 MeV; measured σ.

doi: 10.1088/0305-4616/3/4/005
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2113.