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2016VO11      Phys.Part. and Nucl.Lett. 13, 729 (2016)

V.V.Volkov, E.A.Cherepanov

Interpretation of the mechanism of spontaneous fission of heavy nuclei in the framework of dinuclear system conception

RADIOACTIVITY 238U, 242Pu, 246Cm, 252Cf(42S), (30Ne), (34Mg), (28Si); calculated energy release, nucleus-nucleus potential, spectroscopic factors. Comparison with available data.

doi: 10.1134/S1547477116060108
Citations: PlumX Metrics


2004VO11      Fiz.Elem.Chastits At.Yadra 35, 797 (2004); Physics of Part.and Nuclei 35, 425 (2004)

V.V.Volkov

Process of Complete Fusion of Nuclei. Nuclear Fusion within the Dinuclear-System Concept


2004VO14      Acta Phys.Hung.N.S. 19, 67 (2004)

V.V.Volkov

What is the Most Realistic Mechanism of the Compound Nucleus Formation in the Complete Fusion of Two Massive Nuclei?

NUCLEAR REACTIONS 197Au(40Ar, X), E=290, 340 MeV; Ag(40Ar, X), E=285 MeV; analyzed α-particle and intermediate mass fragment yields; deduced cluster effects, compound nucleus formation mechanism. Dinuclear system approach.

doi: 10.1556/APH.19.2004.1-2.10
Citations: PlumX Metrics


2003CH48      Yad.Fiz. 66, 1604 (2003); Phys.Atomic Nuclei 66, 1561 (2003)

E.A.Cherepanov, V.V.Volkov

Manifestation of Shell Effects in Quasifission Reactions

NUCLEAR REACTIONS 238U(32S, X), 208Pb(56Fe, X), 232Th(40Ar, X), 244Pu, 238U(48Ca, X), E ≈ 4-6 MeV/nucleon; analyzed fragment mass distributions; deduced shell effects. Di-nuclear system concept.

doi: 10.1134/1.1601766
Citations: PlumX Metrics


2003VO13      Yad.Fiz. 66, 1101 (2003); Phys.Atomic Nuclei 66, 1065 (2003)

V.V.Volkov

The Mechanism of Compound Nucleus Formation in Complete Fusion of Two Massive Nuclei

doi: 10.1134/1.1586419
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2003VO22      Acta Phys.Pol. B34, 1881 (2003)

V.V.Volkov

Analysis of nuclear reactions used for the synthesis of heavy and superheavy elements in the framework of the dinuclear system concept


2002VO18      Bull.Rus.Acad.Sci.Phys. 66, 704 (2002)

V.V.Volkov, E.A.Cherepanov

Quasifission in Reactions of Synthesis of Superheavy Elements. Shell Effects in Quasifission

NUCLEAR REACTIONS 208Pb(86Kr, xn), 244Pu, 248Cm(48Ca, xn), E* ≈ 10-80 MeV; analyzed fusion-evaporation σ, role of quasifission, shell effects.


2001AD29      Acta Phys.Hung.N.S. 14, 3 (2001)

G.G.Adamian, N.V.Antonenko, A.Diaz-Torres, S.P.Ivanova, W.Scheid, V.V.Volkov

Fusion to Superheavy Nuclei and Quasifission

doi: 10.1556/APH.14.2001.1-4.2
Citations: PlumX Metrics


2001VO17      Yad.Fiz. 64, No 6, 1191 (2001); Phys.Atomic Nuclei 64, 1116 (2001)

V.V.Volkov, G.G.Adamian, N.V.Antonenko, E.A.Cherepanov, W.Scheid

Synthesis of Superheavy Elements and the Process of Complete Fusion of Massive Nuclei

NUCLEAR REACTIONS 244Pu, 248Cm(48Ca, n), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E*=10-80 MeV; calculated σ. Dinuclear system concept, other reactions discussed.

doi: 10.1134/1.1383627
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1999AD22      Bull.Rus.Acad.Sci.Phys. 63, 693 (1999)

G.G.Adamian, N.V.Antonenko, V.V.Volkov, E.A.Cherepanov, W.Scheid

Some Aspects of Synthesis of Superheavy Elements

NUCLEAR REACTIONS 208Pb(50Ti, X), (54Cr, X), (62Ni, X), (64Ni, X), (66Zn, X), (68Zn, X), (70Zn, X), (70Ge, X), (72Ge, X), (74Ge, X), 209Bi(50Ti, X), (54Cr, X), (64Ni, X), (66Zn, X), (68Zn, X), (70Zn, X), E=low; calculated compound nucleus formation probability, compound nucleus excitation energy; 232Th, 238U, 244Pu(48Ca, X), E=low; calculated compound nucleus formation probability vs excitation energy. Dinuclear system model, comparison with experimental values and other theoretical calculations.


1999VO15      Yad.Fiz. 62, No 7, 1159 (1999); Phys.Atomic Nuclei 62, 1086 (1999)

V.V.Volkov

Role of Dinuclear Systems in Nuclear Fusion, Quasifission, Fission, and Cluster Formation

NUCLEAR REACTIONS 110Pd(110Pd, X), E(cm)=220-300 MeV; calculated evaporation residue formation σ. 206Pb(40Ar, X), 170Er(76Ge, X), 160Gd(86Kr, X), 136Xe(110Pd, X), E not given; calculated compound nucleus formation probability vs orbital angular momentum. 232Th, 238U, 244Pu(48Ca, xn), E*=15-55 MeV; calculated compound nucleus formation probability. Dinuclear system approach.


1999VO16      Acta Phys.Pol. B30, 1517 (1999)

V.V.Volkov

From Deep Inelastic Transfer Reactions to Complete Fusion of Nuclei


1998AD06      Nucl.Phys. A633, 409 (1998)

G.G.Adamian, N.V.Antonenko, W.Scheid, V.V.Volkov

Fusion Cross Sections for Superheavy Nuclei in the Dinuclear System Concept

NUCLEAR REACTIONS 208Pb(50Ti, n), (54Cr, n), (58Fe, n), (62Ni, n), (64Ni, n), (70Zn, n), 209Bi(68Zn, n), (70Zn, n), E not given; calculated fusion probability, evaporation residue σ; deduced quasifission role. Dinuclear system concept. Comparison with data.

doi: 10.1016/S0375-9474(98)00124-9
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1997AD24      Nucl.Phys. A627, 361 (1997)

G.G.Adamian, N.V.Antonenko, W.Scheid, V.V.Volkov

Treatment of Competition between Complete Fusion and Quasifission in Collisions of Heavy Nuclei

NUCLEAR REACTIONS 90Zr(90Zr, X), 100Mo(100Mo, X), 110Pd(110Pd, X), 136Xe(86Kr, X), (110Pd, X), (136Xe, X), 208Pb(62Ni, X), (70Zn, X), (82Se, X), 244Pu(48Ca, X), E not given; calculated fusion probabilities; deduced quasifission role, friction parameter dependence. Dinuclear system evolution.

doi: 10.1016/S0375-9474(97)00605-2
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1997AN29      Nuovo Cim. 110A, 1143 (1997)

N.V.Antonenko, G.G.Adamian, W.Scheid, V.V.Volkov

Competition between Complete Fusion and Quasi-Fission in Dinuclear System

NUCLEAR REACTIONS 90Zr(90Zr, X), 100Mo(100Mo, X), 110Pd(110Pd, X), 86Kr, 110Pd, 136Xe(136Xe, X), E not given; calculated fusion probabilities; deduced friction parameter effect. 208Pb(50Ti, X), (54Cr, X), (58Fe, X), (64Ni, X), (70Zn, X), 209Bi(70Zn, X), E not given; calculated fusion probabilities, evaporation residue σ. Dinuclear system concept.

doi: 10.1007/BF03035956
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1997CH54      Bull.Rus.Acad.Sci.Phys. 61, 1740 (1997)

E.A.Cherepanov, G.G.Adamyan, N.V.Antonenko, V.V.Volkov, A.K.Nasirov

Concept of a Double Nuclear System in Conditions for Synthesis of Superheavy Elements

NUCLEAR REACTIONS 208Pb(62Ni, X), (70Zn, X), (82Se, X), 244Pu(48Ca, X), 136Xe(136Xe, X), E not given; calculated entrance potential, double-nuclear-system potential energy; deduced superheavy element formation features.


1997VO18      Nuovo Cim. 110A, 1127 (1997)

V.V.Volkov, G.G.Adamian, N.V.Antonenko, E.A.Cherepanov, A.K.Nasirov

Process of Complete Fusion of Nuclei within the Framework of Dinuclear System Concept

doi: 10.1007/BF03035954
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1996AN20      Bull.Rus.Acad.Sci.Phys. 60, 85 (1996)

N.V.Antonenko, V.V.Volkov, A.K.Nasirov, E.A.Cherepanov

Fusion of Massive Nuclei within a Concept of Double Nuclear System and Macroscopic Dynamic Model

NUCLEAR REACTIONS, ICPND 110Pd(110Pd, X), E(cm) ≈ 240-300 MeV; calculated evaporation residue production, compound nucleus formation σ vs E. 180Hf(40Ar, X), 96Zr(124Sn, X), E(cm) ≈ 205-250 MeV; calculated fusion probability vs E. 208Pb(62Ni, X), E not given; calculated dinuclear system potential vs Z. Macroscopic dynamical model, double nuclear systems concepts.


1995AN12      Phys.Rev. C51, 2635 (1995)

N.V.Antonenko, E.A.Cherepanov, A.K.Nasirov, V.P.Permyakov, V.V.Volkov

Compound Nucleus Formation in Reactions between Massive Nuclei: Fusion barrier

NUCLEAR REACTIONS, ICPND 100Mo(100Mo, X), 110Pd(110Pd, X), E(cm)=180-300 MeV; measured evaporation, compound nucleus formation σ(E), fusion barrier dependence on the angular momentum. 180Hf(40Ar, X), 96Zr(124Sn, X), E(cm)=200-250 MeV; calculated compound nucleus formation probability vs E.

doi: 10.1103/PhysRevC.51.2635
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1995CH15      Nucl.Phys. A583, 165c (1995)

E.A.Cherepanov, V.V.Volkov, N.V.Antonenko, V.P.Permyakov, A.K.Nasirov

Model of Competition between Complete Fusion and Quasi-Fission in Reactions with Massive Nuclei

NUCLEAR REACTIONS, ICPND 110Pd(110Pd, X), E(cm)=220-300 MeV; 100Mo(100Mo, X), E(cm)=180-260 MeV; calculated fusion σ(E), fusion, quasifission barrier vs angular momentum. Massive symmetric dinuclear system.

doi: 10.1016/0375-9474(94)00654-6
Citations: PlumX Metrics


1994AN26      Bull.Rus.Acad.Sci.Phys. 58, 55 (1994)

N.V.Antonenko, V.V.Volkov, A.K.Nasirov, V.P.Permyakov, E.A.Cherepanov

Reactions with Complete Fusion of Massive Nuclei: Competition between complete fusion and quasifission

NUCLEAR REACTIONS, ICPND 100Mo(100Mo, X), E(cm)=180-240 MeV; 110Pd(110Pd, X), E(cm)=220-300 MeV; calculated fusion, evaporation residue production σ(E). Double nuclear system approach.


1993AN20      Phys.Lett. 319B, 425 (1993)

N.V.Antonenko, E.A.Cherepanov, A.K.Nasirov, V.P.Permjakov, V.V.Volkov

Competition between Complete Fusion and Quasi-Fission in Reactions between Massive Nuclei. The Fusion Barrier

NUCLEAR REACTIONS, ICPND 100Mo(100Mo, X), E(cm) ≈ 180-250 MeV; 110Pd(110Pd, X), E(cm)=220-300 MeV; calculated compound nucleus formation, evaporation residue production σ vs E; deduced new type of fusion barrier. Complete, quasifusion channels competition model.

doi: 10.1016/0370-2693(93)91746-A
Citations: PlumX Metrics


1993AN21      Bull.Rus.Acad.Sci.Phys. 57, 1261 (1993)

N.V.Antonenko, V.V.Volkov, A.K.Nasirov, V.P.Permyakov, E.A.Cherepanov

Compound Nucleus Formation and Analysis of Complete Fusion of Massive Nuclei. Fusion Barrier

NUCLEAR REACTIONS, ICPND 100Mo(100Mo, X), E(cm)=190-250 MeV; 110Pd(110Pd, X), E(cm) ≈ 230-300 MeV; analyzed compound nucleus, evaporation residue production σ(E); deduced reaction mechanism. Conventional models.


1988ME15      Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 2180 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.11, 99 (1988)

A.N.Mezentsev, A.G.Artyukh, V.V.Volkov, G.F.Gridnev, W.Karcz, S.Kliczewsky, M.Madeja, Ja.Szmider

Cluster Emission in Reactions with Heavy Ions

NUCLEAR REACTIONS 197Au, 232Th(12C, X), E=180 MeV; 181Ta(52Cr, X), E=380 MeV; measured σ(fragment θ); deduced light element formation σ.


1988PE18      Rev.Roum.Phys. 33, 811 (1988)

M.Petrascu, I.Brancus, A.Buta, I.Mihai, V.Simion, V.V.Volkov, A.G.Artukh, A.N.Mezentsev

Large Angle Emission of 4 ≤ Z ≤ 9 Products from the Reaction 40Ar (334 MeV) + 232Th

NUCLEAR REACTIONS 232Th(40Ar, X), E=334 MeV; measured σ(fragment θ, E) for X=Be-F; deduced energy, angle integrated σ.


1987VO09      Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 2049 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.11, 160 (1987)

V.V.Volkov, S.N.Ershov, S.P.Ivanova

Yield of Evaporation α-Particles in Reactions with Heavy Ions

NUCLEAR REACTIONS, MECPD 197Au, 209Bi(12C, αX), E=126 MeV; 197Au, 209Bi(16O, αX), E=168 MeV; 109Ag, 197Au, 232Th(40Ar, αX), E=240-340 MeV; calculated fusion, fission, evaporation α-particle σ.


1986VO04      Yad.Fiz. 43, 874 (1986)

V.V.Volkov, S.N.Ershov, S.P.Ivanova

On High Yield of Evaporated α Particles in Heavy-Ion Reactions

NUCLEAR REACTIONS 232Th(40Ar, xα), E=240 MeV; calculated evaporation α-particle yield; deduced fusion mechanism.


1986VO15      Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 1879 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.10, 6 (1986)

V.V.Volkov

Some Information on Total Fusion Process of Nuclear Interaction from Products Investigated in Deep Inelastic Transfer

NUCLEAR REACTIONS 108Ag(20Ne, X), E=252 MeV; 108Ag(40Ar, X), E=288 MeV; 108Ag, 197Au(86Kr, X), E=620 MeV; calculated double nuclear system potential energies; 107,109Ag(40Ar, X), E=285 MeV; analyzed data; deduced fragment differential σ systematics; 159Tb(11B, X), E=115 MeV; 158Gd(12C, X), E=126 MeV; 154Sm(16O, X), E=137 MeV; 107,109Ag(40Ar, X), E=169-337 MeV; analyzed data; deduced critical, orbital angular moments systematics.


1985MI18      Yad.Fiz. 42, 295 (1985)

V.L.Mikheev, A.G.Artukh, V.V.Volkov, G.F.Gridnev, M.Gruszecki, W.Karcz, A.N.Mezentsev, V.M.Morozov, L.Pomorski

Nucleon Transfer Reactions and Nuclear Fission in the System 232Th + 40Ar

NUCLEAR REACTIONS 232Th(40Ar, F), E=300, 390 MeV; measured light, fission fragments-coin, σ(θ1, θ2); deduced ternary fission effect. 236U, 228Ra, 231Ac, 232Th, 233Pa deduced fission probability vs excitation energy.


1984AR08      Rev.Roum.Phys. 29, 139 (1984)

A.G.Artukh, G.F.Gridnev, M.Gruszecki, W.Karcz, A.N.Mezentsev, V.L.Mikheev, L.Pomorski, A.Popescu, D.G.Popescu, V.V.Volkov

The Formation of Alpha Particles in the System (nat)Ag + 40Ar (285 MeV)

NUCLEAR REACTIONS Ag(40Ar, pX), (40Ar, dX), (40Ar, tX), (40Ar, αX), E=285 MeV; measured αα-coin, inclusive σ(θ, Ep), σ(θ, Ed), σ(θ, Et), σ(θ, Eα), σ(light fragment θ). Ag(40Ar, BX), (40Ar, CX), (40Ar, BeX), E=285 MeV; measured σ(light fragment θ).


1983AR20      Yad.Fiz. 38, 549 (1983)

A.G.Artyukh, V.V.Avdeichikov, G.F.Gridnev, M.Gruszecki, W.Karcz, A.N.Mezentsev, V.L.Mikheev, V.M.Morozov, L.Pomorski, A.Popescu, D.G.Popescu, V.V.Volkov

Two-α-Particle Correlations in 40Ar + (nat)Ag Interaction at 285 MeV

NUCLEAR REACTIONS Ag(40Ar, 2α), E=285 MeV; measured αα-coin, σ(θα1, θα2); deduced α-production, massive nuclear transfer mechanisms.


1981AR20      Z.Phys. A303, 41 (1981)

A.G.Artukh, G.F.Gridnev, M.Gruszecki, W.Karcz, A.N.Mezentsev, V.L.Mikheev, L.Pomorski, A.Popescu, D.G.Popescu, V.V.Volkov

Multi-Nucleon Transfer Reactions and the Formation of Light Charged Particles in the System Ag(nat) + 40Ar (285 MeV)

NUCLEAR REACTIONS Ag(40Ar, X), (40Ar, p), (40Ar, d), (40Ar, t), (40Ar, α), E=300 MeV; measured σ(θ, Ep), σ(θ, Ed), σ(θ, Et), σ(θ, Eα), σ(θ, fragment E) for Li, C, Na, Si, Cl, Be, B; deduced multinucleon transfer contribution, two-body (Q) systematics.

doi: 10.1007/BF01420009
Citations: PlumX Metrics


1981VO10      Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 1810 (1981)

V.V.Volkov

Formation of Light Charged Particles in Heavy Ion Reactions

NUCLEAR REACTIONS 197Au(40Ar, α), E=290 MeV; measured αγ(θ), α(fragment)(θ), α(fragment)(fragment)(θ); deduced reaction mechanism.


1980VO11      Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 2226 (1980)

V.V.Volkov, A.G.Artyukh, G.F.Gridnev, M.Grushetski, W.Karcz, A.N.Mezentsev, V.L.Mikheev, L.Pomorski, A.Popescu, D.G.Popescu

Dominance of α-Particle Emission Channels in Deep Inelastic Transfer Reactions with 40Ar Ions.

NUCLEAR REACTIONS 107,109Ag(40Ar, X), E=285 MeV; measured σ(fragment θ) vs total kinetic energy for fragment Z=2-7; deduced α production dominance. Deep inelastic transfer reactions.


1978AR02      Yad.Fiz. 27, 29 (1978); Sov.J.Nucl.Phys. 27, 14 (1978)

A.G.Artukh, V.V.Volkov, E.Gerlik, R.Gerstenberger, G.F.Gridnev, V.B.Zlokazov, A.N.Mezentsev, V.L.Mikheev, T.S.Salamatina

Nucleon Transfer Reactions in Interaction of 220-MeV 40Ar Ions with 197Au

NUCLEAR REACTIONS 197Au(40Ar, X), E=220 MeV; measured σ(Z, θ), Z=11-35.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0023.


1978AR14      Yad.Fiz. 28, 611 (1978); Sov.J.Nucl.Phys. 28, 313 (1978)

A.G.Artyukh, V.V.Volkov, E.Gierlik, G.F.Gridnev, A.N.Mezentsev, V.L.Mikheev

Energy Spectra of Products with Z ≤ 38 in the System 232Th + 40Ar (390 MeV)

NUCLEAR REACTIONS 232Th(40Ar, X), E=390 MeV; measured σ(E(X), Z(X)), Z=5-38; deduced evidence for deep inelastic nucleon transfers.


1978AR20      Yad.Fiz. 28, 1154 (1978); Sov.J.Nucl.Phys. 28, 594 (1978)

A.G.Artyukh, V.V.Volkov, G.F.Gridnev, A.N.Mezentsev, V.L.Mikheev, A.Popescu, D.Popescu

Nucleon Transfer Reactions in the System 197Au + 20Ne (110 MeV)

NUCLEAR REACTIONS 197Au(20Ne, X), E=110 MeV; measured σ(θ), σ(E(12C), E(14N), E(16O)); deduced reaction mechanism.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0046.


1978VO10      Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 2234 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.11, 14 (1978)

V.V.Volkov, A.G.Artyukh, G.F.Gridnev, A.N.Mezentsev, V.L.Mikheev, A.Popescu, D.G.Popescu, A.M.Sukhov, L.P.Chelnokov

Some Laws Governing the Decay of a Binary Nuclear System Produced in Deep-Inelastic Collisions of Complex Nuclei

NUCLEAR REACTIONS 107,109Ag(40Ar, X), E=285 MeV; 107,109Ag(11B, X), E=86 MeV; measured production σ for more than 100 nuclides. 181Ta(40Ar, X), E=290 MeV; 181Ta(136Xe, X), E=840 MeV; 181Ta(86Kr, X), E=550 MeV; calculated production σ for Au isotopes. Two-body ground state Q systematics, neutron evaporation.


1977AR06      Nucl.Phys. A283, 350 (1977)

A.G.Artukh, G.F.Gridnev, V.L.Mikheev, V.V.Volkov

Some Regularities in the Production of Isotopes with 4 ≤ Z ≤ 9 in the Interaction of 22Ne with 232Th

NUCLEAR REACTIONS 232Th(22Ne, X), E=172 MeV; measured reaction products. 7,9,10,11,12Be, 10,11,12,13,14,15B, 10,11,12,13,14,15,16,17,18C, 13,14,15,16,17,18,19,20,21N, 15,16,17,18,19,20,21,22O, 17,18,19,20,21,22,23F deduced σ(θ), θ=12°. Natural target.

doi: 10.1016/0375-9474(77)90436-5
Citations: PlumX Metrics


1977MI04      Yad.Fiz. 25, 255 (1977); Sov.J.Nucl.Phys. 25, 139 (1977)

V.L.Mikheev, A.G.Artyukh, V.V.Volkov, G.F.Gridnev

Many-Nucleon-Transfer Reactions in the System 94Zr + 22Ne

NUCLEAR REACTIONS 94Zr(22Ne, X), E=174 MeV; measured production σ for Be, B, C, N, O; deduced σ systematics.


1976AR03      Yad.Fiz. 23, 261 (1976); Sov.J.Nucl.Phys. 23, 136 (1976)

A.G.Artyukh, V.V.Volkov, G.F.Gridnev, V.L.Mikheev

Proton Pickup in the Interaction of 40Ar with 232Th

NUCLEAR REACTIONS 232Th(40Ar, X), E=388 MeV; measured σ(A); deduced reaction mechanism.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0015.


1975AR14      Izv.Akad.Nauk SSSR, Ser.Fiz. 39, 2 (1975); Bull.Acad.Sci.USSR, Phys.Ser. 39, No.1, 1 (1975)

A.G.Artyukh, V.V.Volkov, G.F.Gridnev, V.L.Mikheev

Transfer Reactions on Heavy Ions (Peculiarities of Transfer Reactions for Deeply Inelastic Collisions between Two Nuclei)

NUCLEAR REACTIONS 27Al(14N, X), E=71 MeV; 27Al(16O, X), E=86 MeV; 51V(16O, X), E=101 MeV; 93Nb(16O, X), E=111 MeV; 232Th(22Ne, X), E=159, 331 MeV; 232Th(40Ar, X), E=253 MeV; 197Au(16O, X), E=127 MeV; 232Th(16O, X), E=128 MeV; 232Th(22Ne, X), E=159 MeV; 94Zr(22Ne, X), E=141 MeV; calculated σ(E(fragment mass)).


1975VO09      Fiz.Elem.Chastits At.Yadra 6, 1040 (1975);Sov.J.Particles Nucl. 6, 420 (1976)

V.V.Volkov

Transfer Reactions Induced by Heavy Ions


1974AR06      Yad.Fiz. 19, 54 (1974); Sov.J.Nucl.Phys. 19, 28 (1974)

A.G.Artyukh, V.V.Volkov, G.F.Gridnev, A.S.Ilinov, V.L.Mikheev

Possibility of Synthesis of Isotopes of Transuranium Elements in Incomplete Fusion Reactions Induced by Heavy Ions

NUCLEAR REACTIONS 238U(22Ne, X), E=172 MeV; 238U(40Ar, X), E=288, 379 MeV; calculated σ for production of elements with 94 < Z < 100.


1973AR08      Nucl.Phys. A211, 299 (1973)

A.G.Artukh, G.F.Gridnev, V.L.Mikheev, V.V.Volkov, J.Wilczynski

Multinucleon Transfer Reactions in the 232Th + 22Ne System

NUCLEAR REACTIONS 232Th(22Ne, X), E=174 MeV; measured σ(E(X), 40°) for X = 6,7,8,9Li, 7,9,10,11,12Be, 10,11,12,13,14B, 12,13,14,15,16,17,18C, 14,15,16,17,18,19,20N, 15,16,17,18,19,20,21,22O, 18,19,20,21,22,23F, 20,21,22,23,24,25Ne, 22,23,24,25,26,27Na, 24,25,26,27Mg. Natural target.

doi: 10.1016/0375-9474(73)90721-5
Citations: PlumX Metrics


1973AR09      Yad.Fiz. 17, 1126 (1973); Sov.J.Nucl.Phys. 17, 586 (1974)

A.G.Artyukh, J.Wilczynski, V.V.Volkov, G.F.Gridnev, V.L.Mikheev

Direct Reactions in the Interaction of Ne22 with Th232

NUCLEAR REACTIONS 232Th(22Ne, X), E=174 MeV; measured σ(E;θ), production σ for 2 < Z < 13.


1973AR17      Nucl.Phys. A215, 91 (1973)

A.G.Artukh, G.F.Gridnev, V.L.Mikheev, V.V.Volkov, J.Wilczynski

Transfer Reactionsin the Interaction of 40Ar with 232Th

NUCLEAR REACTIONS 232Th(40Ar, X), E=297, 388 MeV; measured σ(E(X-ray), ) for X=B, C, N, O, F, Ne, Na, Mg, Al, Si, P, S, Cl, Ar, K, Ca. Natural target.

doi: 10.1016/0375-9474(73)90104-8
Citations: PlumX Metrics


1972AR05      Nucl.Phys. A192, 170 (1972)

A.G.Artukh, G.F.Gridnev, V.L.Mikheev, V.V.Volkov, J.Wilczynski

Mass Measurements of 21O and 22O

doi: 10.1016/0375-9474(72)90012-7
Citations: PlumX Metrics


1972AR30      JINR-E7-6764 (1972)

A.G.Artukh, G.F.Gridnev, V.L.Mikheev, V.V.Volkov, J.Wilczynski

Multinucleon Transfer Reactions in the 232Th + 22Ne System

NUCLEAR REACTIONS 232Th(22Ne, 22Ne), (22Ne, X), E=174 MeV; measured σ, particle energy spectra. Multinucleon transfer reactions.


1972AR35      Yad.Fiz. 16, 905 (1972); Sov.J.Nucl.Phys. 16, 499 (1973)

A.G.Artyukh, V.V.Volkov, L.Pomorski, J.Tys

Angular Distribution and Excitation Functions of the Reactions (N15, N16), (N14, N16), (N15, N17), (N14, N17)

NUCLEAR REACTIONS 181Ta(14N, 17N), (15N, 16N), (15N, 17N), 197Au(14N, 16N), (14N, 17N), (15N, 16N), (15N, 17N), E=90-103 MeV; measured σ(E, θ), deduced reaction mechanism.


1971AR02      Nucl.Phys. A160, 511 (1971)

A.G.Artukh, V.V.Avdeichikov, J.Ero, G.F.Gridnev, V.L.Mikheev, V.V.Volkov, J.Wilczynski

On Some Regularities in Multinucleon Transfer Reactions with Heavy Ions

NUCLEAR REACTIONS 197Au, 232Th(16O, X), E=137 MeV; measured σ(E(X-ray), θ=40°) for X= 7,9,12Be, 10,15B, 10,17C, 13,18N, 15,21O, 17,22F, 20,24Ne. Natural targets.

doi: 10.1016/0375-9474(71)90093-5
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1971AR15      Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 2 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 3 (1972)

A.G.Artyukh, V.V.Avdeichikov, J.Wilczynski, V.V.Volkov, G.F.Gridnev, V.L.Mikheev, J.Ero, A.A.Vorobev, V.T.Grachev, Y.K.Zalite, I.A.Kondurov, A.M.Nikitin, D.M.Seliverstov

Nuclei of Light Nuclei Elements with Large Neutron Excess

NUCLEAR REACTIONS 232Th(11B, X), E=97 MeV; measured He spectra. 235U(n, F), E=thermal; measured He, Li spectra, yields. 10He deduced particle instability.


1971AR21      Nucl.Phys. A168, 321 (1971)

A.G.Artukh, V.V.Avdeichikov, G.F.Gridnev, V.L.Mikheev, V.V.Volkov, J.Wilczynski

Evidence for Particle Instability of 10He

NUCLEAR REACTIONS 232Th(15N, X), E=145 MeV; measured σ(E(X-ray), 40°) for X: 13,14,15,16C, 11,12,13,14,15B, 9,10,11,12Be, 7,8,9,11Li, 6,8He. 10He not observed.

doi: 10.1016/0375-9474(71)90797-4
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1971AR32      Nucl.Phys. A176, 284 (1971)

A.G.Artukh, V.V.Avdeichikov, G.F.Gridnev, V.L.Mikheev, V.V.Volkov, J.Wilczynski

New Isotopes 29,30Mg, 31,32,33Al, 33,34,35,36Si, 35,36,37,38P, 39,40S and 41,42Cl Produced in Bombardment of a 232Th Target with 290 MeV 40Ar Ions

NUCLEAR REACTIONS 232Th(40Ar, X), E=290 MeV; measured fragments isotopic yields; deduced evidence for 27,28,29,30Mg, 29,30,31,32,33Al, 31,32,33,34,35,36Si, 33,34,35,36,37,38P, 36,37,38,39,40S, 37,38,39,40,41,42Cl, 39,40,41,42,43,44Ar.

doi: 10.1016/0375-9474(71)90270-3
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1970AR01      Phys.Lett. 31B 129 (1970)

A.G.Artukh, V.V.Avdeichikov, G.F.Gridnev, V.L.Mikheev, V.V.Volkov, J.Wilczynski

New Isotopes 23F, 24F, 25Ne and 26Ne, Produced in Nuclear Reactions with Heavy Ions

NUCLEAR REACTIONS 232Th(22Ne, X), E = 174 MeV; measured σ(E(23F), E(24F), E(25Ne), E(26Ne)). 23,24F, 25,26Ne deduced yields.

doi: 10.1016/0370-2693(70)90130-9
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1970AR09      Phys.Lett. 32B, 43 (1970)

A.G.Artukh, V.V.Avdeichikov, L.P.Chelnokov, G.F.Gridnev, V.L.Mikheev, V.I.Vakatov, V.V.Volkov, J.Wilczynski

New Isotopes 21N, 23O, 24O and 25F, Produced in Nuclear Reactions with Heavy Ions

NUCLEAR REACTIONS 232Th(22Ne, X), E=174 MeV; measured σ(E(21N), E(23O), E(24O), E(25F)). 21N, 23,24O, 25F deduced yields.

doi: 10.1016/0370-2693(70)90332-1
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1970AR27      Phys.Lett. 33B, 407 (1970)

A.G.Artukh, V.V.Avdeichikov, J.Ero, G.F.Gridnev, V.L.Mikheev, V.V.Volkov, J.Wilczynski

Evidence for Particle Instability of 13Be and 14Be

NUCLEAR REACTIONS 232Th(15N, X), E=145 MeV; measured σ(E(X)), X= 14,15,16C, 13,14,15B, 12Be. 13,14Be deduced paricle instability.

doi: 10.1016/0370-2693(70)90616-7
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1970GR06      Nucl.Phys. A142, 385 (1970)

G.F.Gridnev, V.V.Volkov, J.Wilczynski

Evidence for an Intermediate Mechanism in Interactions between Complex Nuclei

NUCLEAR REACTIONS 27Al(16O, F), 27Al(16O, Ne), 27Al(16O, Na), 27Al(16O, Mg), E=137 MeV; 51V(16O, F), 51V(16O, Ne), 51V(16O, Na), E=126 MeV; 93Nb(16O, F), 93Nb(16O, Ne), 93Nb(16O, Na), E=131 MeV; measured σ(E(F), E(Ne), E(Na), E(Mg), θ). Natural targets.

doi: 10.1016/0375-9474(70)90537-3
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1969AR13      Nucl.Phys. A137, 348(1969)

A.G.Artukh, G.F.Gridnev, V.L.Mikheev, V.V.Volkov

New Isotopes 22O, 20N and 18C Produced in Transfer Reactions with Heavy ions

NUCLEAR REACTIONS 232Th(18O, X), E = 122 MeV; measured reaction products. 9,10,11,12Be, 12,13,14B, 14,15,16,17,18C, 17,18,19,20N, 18,19,20,21,22O deduced yields. Natural target.

doi: 10.1016/0375-9474(69)90114-6
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1969VO02      Nucl.Phys. A126, 1(1969)

V.V.Volkov, G.F.Gridnev, G.N.Zorin, L.P.Chelnokov

Nucleon and Nucleon-Group Transfer Reactions Induced in the Bombardment of 197Au and 232Th by 12C, 14N and 15N Projectiles

NUCLEAR REACTIONS 197Au, 232Th(12C, 11B), (12C, 13C), (12C, 9Be), (12C, 14N)(12C, 16O), E=82 MeV; 197Au, 232Th(14N, 15N), (14N, 12C), (14N, 10B), (14N, 16O), (14N, 18F), E=110 MeV; 232Th(15N, 16N), (15N, 16O), E=98.5 MeV, measured σ(θ), energy spectra. Natural targets.

doi: 10.1016/0375-9474(69)90396-0
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1967VO01      Nucl.Phys. A92, 495 (1967)

V.V.Volkov, J.Wilczynski

On the Mechanism of Proton-Transfer Reactions

NUCLEAR REACTIONS 51V(12C, 13N), E = 81.0, 68.4, 53.3, 39.2 MeV; 93Nb(12C, 13N), E = 80.2, 67.4, 52.8 MeV; Ag(12C, 13N), E = 80.4 MeV; 181Ta(12C, 13N), E = 79.3 MeV; 181Ta(14N, 15O), E = 106.0 MeV; measured σ(θ). Natural targets.

doi: 10.1016/0375-9474(67)90628-8
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1967WI04      Nucl.Phys. A93, 133(1967)

J.Wilczynski, V.V.Volkov

Diffraction Effects in Proton Transfer Reactions

NUCLEAR REACTIONS 27Al(12C, 13N), E = 80.0, 70.3, 59.0, 38.1 MeV; 12C(12C, 13N), E = 81.0, 68.2 MeV; measured σ(E(13N), θ). 27Al(12C, 11C), E = 81.0 MeV; measured σ(θ). Natural targets.

doi: 10.1016/0375-9474(67)90175-3
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1967WI16      Yadern.Fiz. 5, 942 (1967); Soviet J.Nucl.Phys. 5, 672 (1967)

J.Wilczynski, V.V.Volkov, P.Decowski

Some Features of the Mechanism of Many-Nucleon-Transfer Reactions

NUCLEAR REACTIONS 27Al(14N, 18F), E=65, 79, 91, 107 MeV; 27Al(15N, 18F), E=96.5, 78.5 MeV; measured σ(E;E(18F), θ), σ(E(18F)); deduced reaction mechanisms.


1966AR17      Yadern.Fiz. 4, 1165 (1966); Soviet J.Nucl.Phys. 4, 839 (1967)

A.G.Artyukh, V.V.Volkov, T.Kwiecinksa

Study of Neutron Pickup in the Bombardment of Ta181, Au197, Th232, and U238 Isotopes by N15 Ions

NUCLEAR REACTIONS 181Ta, 197Au, 232Th, 238U(15N, 16N), E=70-103 MeV; measured sigam easured σ(E;E(16N), θ).


1966PO08      Phys.Letters 23, 369 (1966)

L.Pomorski, J.Tys, V.V.Volkov

Angular Distributions of 17N Nuclei from the Three-Neutron Transfer Reactions

NUCLEAR STRUCTURE 178Ta, 194Au; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90470-7
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1962VO01      Zhur.Eksptl.i Teoret.Fiz. 42, 635 (1962); Soviet Phys. JETP 15, 442 (1962)

V.V.Volkov, L.Pomorski, J.Tys, G.N.Flerov

NUCLEAR STRUCTURE C; measured not abstracted; deduced nuclear properties.


1960FL01      Zhur.Eksptl. I Teoret.Fiz. 38, 82 (1960); Soviet Phys.JETP 11, 61 (1960)

G.N.Flerov, S.M.Polikanov, A.S.Karamyan, A.S.Pasyuk, D.M.Parfanovich, N.I.Tarantin, V.A.Karnaukhov, V.A.Druin, V.V.Volkov, A.M.Semchinova, Yu.Ts.Oganesyan, V.I.Khalizev, G.I.Khlebnikov, B.F.Myasoedov, K.A.Gavrilov

Experiments on Production of 102-ND Element

NUCLEAR STRUCTURE 253No; measured not abstracted; deduced nuclear properties.


1959FL69      AEC-tr-3826 (1959)

G.N.Flerov, S.M.Polikanov, A.S.Karamian, A.S.Pasiuk, D.M.Parfanovich, N.I.Tarantin, V.A.Karnaukhov, V.A.Druin, V.V.Volkov, A.M.Semchinova, Y.T.Oganesian, V.I.Khalizev, G.I.Khlebnikov, B.F.Myasoedov, K.A.Gavrilov

Experiments in Obtaining the 102nd Element


1958FL42      Doklady Akad.Nauk SSSR 120, 73 (1958); Soviet Phys.Doklady 3, 546 (1958)

G.N.Flerov, S.M.Polikanov, A.S.Karamian, A.S.Pasiuk, D.M.Parfanovich, N.I.Tarantin, V.A.Karnaukhov, V.A.Druin, V.V.Volkov, A.M.Semchinova, Y.T.Oganesian, V.I.Khalizev, G.I.Khlebnikov

Experiments on the Production of the 102 d Element


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