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NSR database version of April 26, 2024.

Search: Author = A.V.Lado

Found 10 matches.

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1998BL08      Nucl.Instrum.Methods Phys.Res. A402, 386 (1998)

L.D.Blokhintsev, A.V.Lado, Yu.N.Uzikov

Backward Elastic p 3He Scattering at Energies 1-2 GeV

NUCLEAR REACTIONS 3He(p, p), E=0.2-1.7 GeV; calculated backward scattering σ(θ); deduced sequential transfer role.

doi: 10.1016/S0168-9002(97)00868-1
Citations: PlumX Metrics

1996BL01      Nucl.Phys. A597, 487 (1996)

L.D.Blokhintsev, A.V.Lado, Yu.N.Uzikov

np Pair Transfer Mechanism for Backward Elastic p 3He Scattering at Intermediate Energies

NUCLEAR REACTIONS 3He(p, p), E=0.5-1.7 GeV; analyzed σ(θ); deduced two-body transfer mechanism, rearrangement scattering related features.

doi: 10.1016/0375-9474(95)00411-4
Citations: PlumX Metrics

1996KO22      Yad.Fiz. 59, No 5, 842 (1996); Phys.Atomic Nuclei 59, 804 (1996)

V.I.Komarov, A.V.Lado, Yu.N.Uzikov

Mechanisms of the Reaction pd → 3H(Λ)K+

NUCLEAR REACTIONS 2H(p, X), E=threshold-3 GeV; analyzed K+-, η-production σ(θ); deduced K+ production mechanism related features. One-, two-step mechanisms included.

1995KO31      Yad.Fiz. 58, No 3, 525 (1995); Phys.Atomic Nuclei 58, 473 (1995)

L.A.Kondratyuk, A.V.Lado, Yu.N.Uzikov

Production of (Eta) Mesons Near the Threshold of the Reaction pD → 3He(Eta) and the Possibility of the Existence of a Quasi-Bound State in the (Eta)3He System

NUCLEAR REACTIONS 2H(p, X), E ≈ 1-2.5 GeV; calculated σ(θ) vs E for eta production; deduced sub-threshold (eta+3He) system quasibound state possibility, parameters. Two-step mechanism.

1995KO42      J.Phys.(London) G21, L69 (1995)

V.I.Komarov, A.V.Lado, Yu.N.Uzikov

The pd → 3H(Λ)K+ Reaction Cross Section

NUCLEAR REACTIONS 2H(p, K+), E=1.13-3 GeV; calculated hypernucleus production σ(θ) vs E, one-, two-step mechanisms.

doi: 10.1088/0954-3899/21/9/001
Citations: PlumX Metrics

1993BL07      Yad.Fiz. 56, No 7, 139 (1993); Phys.Atomic Nuclei 56, 933 (1993)

L.D.Blokhintsev, A.V.Lado, Yu.N.Uzikov

Mechanism of Breakward Elastic p3He Scattering at Energies 1-1.5 GeV

NUCLEAR REACTIONS 3He(p, p), E=0.9-1.7 GeV; calculated σ(θ); deduced np-pair transfer mechanism role.

1993LA20      Yad.Fiz. 56, No 9, 114 (1993); Phys.Atomic Nuclei 56, 1216 (1993)

A.V.Lado, Yu.N.Uzikov

Exchange of an np Pair in Elastic p3He Backward Scattering at Intermediate Energies

NUCLEAR REACTIONS 3He(p, p), E ≤ 1.6 GeV; calculated σ(θ); deduced dominant mechanism. Feynmann diagram approach, Faddeev five channel 3He wave function.

1993LA26      Bull.Rus.Acad.Sci.Phys. 57, 875 (1993)

A.V.Lado, Yu.N.Uzikov

d(*) + p-Structure of 3He Nucleus in Elastic p, 3He Backward Scattering at E(p) = 0.5-1.7 GeV

NUCLEAR REACTIONS 3He(p, p), E=0.5-1.7 GeV; calculated σ(θ); deduced role of singlet deuteron in 3He. Faddeev, cluster 3He wave functions.

1992LA06      Phys.Lett. 279B, 16 (1992)

A.V.Lado, Yu.N.Uzikov

The Mechanism of Two-Nucleon Transfer in Backward Elastic p3He Scattering at Intermediate Energies

NUCLEAR REACTIONS 3He(p, p), E ≈ 0.2-1.6 GeV; calculated σ(θ); deduced two-nucleon transfer mechanism. Glauber rescattering effects.

doi: 10.1016/0370-2693(92)91832-T
Citations: PlumX Metrics

1989LA26      Yad.Fiz. 50, 1309 (1989)

A.V.Lado, Yu.N.Uzikov

The Mechanism of Two-Nucleon Exchange in the Backward Elastic p3He Scattering

NUCLEAR REACTIONS 3He(p, p), (n, n), E=2 MeV; calculated σ(θ); deduced reaction mechanism. K-matrix approach.

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