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Search: Author = I.S.Gulkarov

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1998GU14      Int.J.Mod.Phys. E7, 367 (1998)

I.S.Gulkarov, B.P.Nigam

Charge Densities of the Nuclei ²⁰⁵Tl, ^{206, 208}Pb and the Occupancies of the Shell States

NUCLEAR STRUCTURE ²⁰⁵Tl, ^206,208Pb; calculated charge densities; deduced shell occupation numbers, nucleon-nucleon correlations role. Modified shell model.

doi: 10.1142/S0218301398000166
Citations: PlumX Metrics

1997GU12      Yad.Fiz. 60, No 6, 995 (1997); Phys.Atomic Nuclei 60, 890 (1997)

I.S.Gulkarov, B.P.Nigam

Charge Densities in ^142,146,150Nd Isotopes and Occupation Numbers for 2s and 2p Shell States

NUCLEAR STRUCTURE ^142,146,150Nd; calculated charge densities, isoscalar dipole state features, 2s-, 2p-states occupation numbers. Modified shell model.

1995GU09      Phys.Rev. C52, 663 (1995)

I.S.Gulkarov, B.P.Nigam

Charge Densities of the Nuclei ⁸⁶Sr, ⁸⁹Y, ⁹²Mo, ¹¹⁸Sn, and ¹⁵²Sm and the Proton Occupancies of the Shells 2s, 2p, 1g, and 1h

NUCLEAR STRUCTURE ⁸⁶Sr, ⁸⁹Y, ⁹²Mo, ¹¹⁸Sn, ¹⁵²Sm; calculated charge densities, proton configurations, occupation probabilities, rms radii. Modified shell model basis, eroding, gaining shells.

doi: 10.1103/PhysRevC.52.663
Citations: PlumX Metrics

1994GU15      Yad.Fiz. 57, No 6, 984 (1994); Phys.Atomic Nuclei 57, 923 (1994)

I.S.Gulkarov, B.P.Nigam

Charged Densities and Occupation Numbers of Shell States of ^142,146,150Nd Isotopes Near the Fermi Surface

NUCLEAR STRUCTURE ^142,146,150Nd; calculated charge density, B(λ). Modified shell model, fractional occupation numbers of states near Fermi surface.

1994GU22      Int.J.Mod.Phys. E3, 933 (1994)

I.S.Gulkarov, B.P.Nigam

Microscopic Description of the Charge Densities of the Isotopes ^146,150Nd

NUCLEAR STRUCTURE ^146,150Nd; calculated charge density distribution. Collective model.

doi: 10.1142/S0218301394000280
Citations: PlumX Metrics

1992GU11      Yad.Fiz. 55, 2024 (1992); Sov.J.Nucl.Phys. 55, 1123 (1992)

I.S.Gulkarov

Dipole Isospin-Forbidden Resonances and Polarizability of the ¹⁸O Nucleus

NUCLEAR STRUCTURE ¹⁸O; calculated transition charge densities, polarizability. Modified Steinwedel-Jensen model.

NUCLEAR REACTIONS ¹⁸O(e, e'), E not given; calculated T=0 states form factors. Modified Steinwedel-Jensen model based transition charge densities.

1992GU16      Bull.Rus.Acad.Sci.Phys. 56, 759 (1992)

I.S.Gulkarov, M.G.Karimov, M.M.Mansurov

Root-Mean-Square Radii of sd-Shell Nuclei

NUCLEAR STRUCTURE A=16-40; calculated rms radii. Harmonic oscillator model.

1990AM06      Yad.Fiz. 52, 1252 (1990); Sov.J.Nucl.Phys. 52, 796 (1990)

M.Ya.Amusya, I.S.Gulkarov, M.M.Mansurov

Sum Rules and Transition Densities of Isoscalar Dipole Resonances

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ²⁰⁸Pb; calculated form factors, charge transition densities, B(λ), rms radii. Sum rules.

1990GU10      Yad.Fiz. 51, 97 (1990); Sov.J.Nucl.Phys. 51, 61 (1990)

I.S.Gulkarov

Charge Densities of sp- and sd-Shell Nuclei and Occupation Number of 2s States

NUCLEAR STRUCTURE ¹⁶O, ¹⁵N, ^34,32S, ⁴⁰Ca, ⁴⁰Ar, ²⁸Si, ^24,26Mg; calculated charge density differences. ¹²C, ^14,15N, ^16,18O, ¹⁹F, ^20,22Ne, ²³Na, ^24,26Mg, ²⁷Al; calculated rms radii. Partial occupancy assumption.

1990GU35      Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 2207 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, No.11, 120 (1990)

I.S.Gulkarov, V.I.Kuprikov, V.N.Tarasov, M.M.Mansurov

Calculations of the Charge Density Distributions in sd-Nuclei using the Hartree-Fock Method and the Harmonic Oscillator Model

NUCLEAR STRUCTURE ^20,22Ne, ^24,26Mg, ^28,30Si, ^36,40Ar; calculated charge density distributions. Hartree-Fock method, spherical, deformed basis.

1989GU06      Yad.Fiz. 49, 33 (1989)

I.S.Gulkarov, V.I.Kuprikov

Hartree-Fock and Shell Charge Densities of the Isotope Nuclei ^16,18O, ^32,34S, and ^40,48Ca

NUCLEAR STRUCTURE ^16,18O, ^32,34S, ^40,48Ca; calculated charge densities. Hartree-Fock method, Skyrme forces.

1989GU26      Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 2433 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.12, 156 (1989)

I.S.Gulkarov

Population of Shell States as a Function of Nucleon Number

NUCLEAR STRUCTURE ^14,15N, ¹⁶O, ^24,26Mg, ²⁸Si; calculated charge density distributions. Harmonic oscillator basis, shell model.

1988GU03      Yad.Fiz. 47, 42 (1988)

I.S.Gulkarov, M.M.Mansurov, A.A.Khomich

Charge Density Distribution for 1s - 1p- and 1d - 2s-Shell Nuclei and Occupation Numbers

NUCLEAR STRUCTURE ¹²C, ^16,18O, ²⁴Mg, ²⁸Si, ^32,34S, ^40,48Ca; calculated charge density distributions.

1988GU12      Fiz.Elem.Chastits At.Yadra 19, 345 (1988); Sov.J.Part.Nucl 19, 149 (1988)

I.S.Gulkarov

Electron Scattering by Nuclei and Transition Charge Densities

NUCLEAR REACTIONS ^16,18O, ^32,34S, ^40,48Ca, ²⁴Mg, ¹²C, ²⁰Ne, ²⁸Si, ⁴⁰Ar(e, e'), E not given; calculated multipole form factor, transition radii, charge densities.

1988GU14      Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 878 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.5, 42 (1988)

I.S.Gulkarov, M.M.Mansurov

Nuclear Models and Inelastic Electron Scattering by ¹⁶O

NUCLEAR REACTIONS ¹⁶O(e, e'), E not given; calculated form factors.

1988GU16      Yad.Fiz. 48, 1283 (1988)

I.S.Gulkarov, M.M.Mansurov

Transition Charge Densities and Occupation Numbers of Shell States

NUCLEAR STRUCTURE ³²S, ^40,48Ca; calculated octupole form factors, static, transition charge densities.

1987GU20      Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 911 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.5, 73 (1987)

I.S.Gulkarov, L.D.Pinkus

Model-Independent and Microscopically Calculated Electric Transition Densities in ⁴⁰Ca and ⁴⁸Ca

NUCLEAR STRUCTURE ^40,48Ca; calculated levels, J, π, electric transition densities, rms radii, form factors.

1987GU24      Ukr.Fiz.Zh. 32, 1643 (1987)

I.S.Gulkarov, M.M.Mansurov

Transition Densities and Form Factors of Isoscalar and Isovector Excitations of Nuclei in the Modified Steinwedel-Jensen Model

NUCLEAR REACTIONS ⁴⁰Ca(e, e'), E not given; calculated transition densities, form factors. Steinwedel-Jensen model.

1986GU05      Yad.Fiz. 43, 809 (1986)

I.S.Gulkarov, R.Kh.Vakil

Formfactors and Transition Densities of Charge of ¹⁶O and ¹⁸O Nuclei

NUCLEAR STRUCTURE ^16,18O; calculated transition charge density. Helm model.

NUCLEAR REACTIONS ^16,18O(e, e'), E not given; analyzed form factor data. ^16,18O levels deduced β(L), B(λ). Helm model charge densities.

1986GU15      Yad.Fiz. 44, 330 (1986)

I.S.Gulkarov, L.D.Pinkus

Charge Densities and Octupole Form Factor of ³²S Nucleus

NUCLEAR STRUCTURE ³²S; calculated charge density distribution, octupole form factor. Harmonic oscillator model.

1984AM09      Yad.Fiz. 40, 1321 (1984); Sov.J.Nucl.Phys. 40, 839 (1984)

M.Ya.Amusya, I.S.Gulkarov, M.B.Zhalov, T.M.Potapova

Influence of Nuclear Structure on the Bremsstrahlung Spectra of Fast Nucleons

NUCLEAR REACTIONS ⁴⁰Ca(n, γ), (p, γ), E=1 GeV; calculated bremsstrahlung σ(θ).

1982GU23      Izv.Akad.Nauk SSSR, Ser.Fiz. 46, 2125 (1982); Bull.Acad.Sci.USSR, Phys.Ser. 46, No.11, 61 (1982)

I.S.Gulkarov, R.Kh.Vakil, M.G.Karimov

The Sum Rules and the Modified Shteinwedel-Jensen Model

NUCLEAR STRUCTURE ⁴⁰Ca; calculated octupole form factor, charge density distribution. Sum rule techniques.

1979GU04      Yad.Fiz. 29, 57 (1979); Sov.J.Nucl.Phys. 29, 28 (1979)

I.S.Gulkarov

On Sum Rules for the Transition Charge Density

NUCLEAR STRUCTURE ¹²C; calculated form factors, charge-transition density.

1978GU13      Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 159 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.1, 137 (1978)

I.S.Gulkarov, R.K.Vakil

Transition Densities and Form Factors of the Nuclides ¹²C, ²⁰Ne, ²⁴Mg, ²⁸Si, and ³²S

NUCLEAR STRUCTURE ¹²C, ²⁰Ne, ²⁴Mg, ²⁸Si, ³²S; calculated quadrupole form factors, B(λ).

1976GU11      Yad.Fiz. 23, 574 (1976); Sov.J.Nucl.Phys. 23, 301 (1976)

I.S.Gulkarov, R.K.Vakil

On the Choice of the Transition Density in Electron Inelastic Scattering from Nuclei

NUCLEAR REACTIONS ¹²C(e, e'); calculated form factors to levels in ¹²C.

1974GU16      Yad.Fiz. 20, 17 (1974); Sov.J.Nucl.Phys. 20, 9 (1975)

I.S.Gulkarov

Giant Quadrupole Resonances

NUCLEAR REACTIONS ^58,60,64Ni(e, e'), E=150-200 MeV; measured σ(Ee'). ^58,60,64Ni deduced giant resonances.

1974GU29      Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2642 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.12, 157 (1974)

I.S.Gulkarov

Giant Isoscalar Quadrupole Resonances

NUCLEAR REACTIONS ^58,60,64Ni(e, e'), E approx 200 MeV; analyzed data. ^58,60,64Ni analyzed GQR, parameters.

1974VA29      Izv.Akad.Nauk Uzb.SSR, Ser.Fiz.-Mat.Nauk No.3, 76 (1974)

R.K.Vakil, I.S.Gulkarov

Quadrupole Form Factor of ¹⁵N

NUCLEAR REACTIONS ¹⁵N(e, e'), E=250, 400 MeV; calculated ¹⁵N form factor.

1973GU22      Yad.Fiz. 18, 519 (1973); Sov.J.Nucl.Phys. 18, 267 (1974)

I.S.Gulkarov

Excitation of Giant Quadrupole Resonance in Ni⁶⁰ by Electron Scattering

NUCLEAR REACTIONS ⁶⁰Ni(e, e'); measured σ. ⁶⁰Ni deduced resonances, level-width, B(EL).

1972GU24      Izv.Akad.Nauk Uzb.SSR, Ser.Fiz.-Mat.Nauk No.4, 55 (1972)

I.S.Gulkarov, T.F.Masagutov, G.Y.Umarov

Formfactor of the 4.43 MeV Level in ¹²C

NUCLEAR REACTIONS ¹²C(e, e'), E not given; measured nothing; analyzed other data. ¹²C deduced form factor, B(E2) for 4.43-MeV level.

1972GU25      Yad.Fiz. 16, 689 (1972); Sov.J.Nucl.Phys. 16, 386 (1973)

I.S.Gulkarov

Form Factors and Transition Densities of the Quadrupole and Octupole Vibrations of the C¹² Nucleus

NUCLEAR STRUCTURE ¹²C; calculated level form factors.

1971GU10      Yad.Fiz. 13, 321 (1971); Sov.J.Nucl.Phys. 13, 178 (1971)

I.S.Gulkarov

Integral Characteristics of the Giant Resonance and Transition Radii of Nuclei with A < 60

NUCLEAR REACTIONS ¹²C, ²⁸Si, ³²S, ⁶⁰Ni(γ, X), E not given; calculated giant resonance form factors, transition radii.

1970GU12      Yad.Fiz. 12, 694 (1970); Sov.J.Nucl.Phys. 12, 376 (1971)

I.S.Gulkarov

Form Factors and Fine Structure of the Giant Resonance in C¹²

NUCLEAR REACTIONS ¹²C(e, e'), E=200 MeV; measured σ(Ee', θ); deduced form factors. ¹²C deduced giant resonance structure.

1970KH02      Nucl.Phys. A146, 15 (1970)

V.M.Khvastunov, N.G.Afanasyev, V.D.Afanasyev, I.S.Gulkarov, A.S.Omelaenko, G.A.Savitsky, A.A.Khomich, N.G.Shevchenko, V.S.Romanov, N.V.Rusanova

Elastic Electron Scattering on ^58,60,64Ni and ^112,118Sn Isotopes

NUCLEAR REACTIONS ^58,60,64Ni(e, e), ^112,118Sn(e, e), E=225 MeV; measured σ(θ). ^58,60,64Ni, ^112,118Sn deduced nuclear charge distribution parameters, isotopic charge radius changes. Enriched targets.

doi: 10.1016/0375-9474(70)91083-3
Citations: PlumX Metrics

1970KH05      Yad.Fiz. 12, 9 (1970); Sov.J.Nucl.Phys. 12, 5 (1971)

V.M.Khvastunov, N.G.Afanasev, V.D.Afanasev, E.V.Bondarenko, I.S.Gulkarov, G.A.Savitskii, N.G.Shevchenko

Scattering of High-Energy Electrons by the Isotopes Mg²⁴ and Mg²⁶

NUCLEAR REACTIONS ^24,26Mg(e, e), (e, e'), E=25 MeV; measured σ(Ee'); deduced form factors. ^24,26Mg deduced quadrupole moment, nuclear radius shifts, B(E2).

1969AF01      Yadern.Fiz. 10, 33 (1969); Soviet J.Nucl.Phys. 10, 18 (1970)

V.D.Afanasev, N.G.Afanasev, I.S.Gulkarov, G.A.Savitskii, V.M.Khvastunov, N.G.Shevchenko, A.A.Khomich

Electroexcitation of Low Lying Collective States in the Isotopes Ni^58,60,64

NUCLEAR REACTIONS ^58,60,64Ni(e, e), (e, e'), E=150, 225 MeV; measured σ(Ee', θ); deduced elastic, inelastic form factors. ^58,60,64Ni deduced B(E2), B(E3), transition radii, charge distributions.

1969GU05      Yadern.Fiz. 9, 1138 (1969); Soviet J.Nucl.Phys. 9, 666 (1969)

I.S.Gulkarov, N.G.Afanasev, A.A.Khomich, V.D.Afanasev, V.M.Khvastunov, G.A.Savitskii, N.G.Shevchenko

Inelastic Scattering of Electrons by Carbon

NUCLEAR REACTIONS ¹²C(e, e'), E=115, 200 MeV; measured σ(Ee'). ¹²C deduced form factor for giant resonance, B(E2), transition radii, oscillation parameters.

1969GU06      Yadern.Fiz. 9, 478 (1969); Soviet J.Nucl.Phys. 9, 274 (1969)

I.S.Gulkarov, N.G.Afanasev, V.M.Khvastunov, N.G.Shevchenko, V.D.Afanasev, G.A.Savitskii, A.A.Khomich

Excitation of the Giant Resonance in Nickel Isotopes by High-Energy Electrons

NUCLEAR REACTIONS ^58,60,64Ni(e, e'), E=150-200 MeV; measured σ(E;Ee') . ^58,60,64Ni deduced giant resonance form factors.

1969GU12      Yadern.Fiz. 10, 694 (1969); Soviet J.Nucl.Phys. 10, 400 (1970)

I.S.Gulkarov, N.G.Afanasev, A.A.Khomich, V.M.Khvastunov, V.D.Afanasev, G.A.Savitskii, N.G.Shevchenko

Excitation of Giant Resonance in S³² by Electron Scattering

NUCLEAR REACTIONS ³²S(e, e'), E=120-200 MeV; measured σ(Ee', θ). ³²S deduced giant resonance energy, width.

1969GU14      Ukr.Fiz.Zh. 14, 125 (1969)

I.S.Gulkarov, N.G.Afanasyev, G.A.Savitsky, V.M.Khvastunov, N.G.Shevchenko

Form Factor of the 17.5 MeV Level in Si²⁸

NUCLEAR REACTIONS ²⁸Si(e, e'), E=150-225 MeV; measured σ(E;Ee'). ²⁸Si deduced form factor of 17.5-MeV level.

1969KH07      Yadern.Fiz. 10, 217 (1969); Soviet J.Nucl.Phys. 10, 122 (1970)

V.M.Khvastunov, N.G.Afanasev, V.D.Afanasev, I.S.Gulkarov, A.S.Omelaenko, G.A.Savitskii, A.A.Khomich, N.G.Shevchenko, V.S.Romanov

Elastic Scattering of Electrons by the Isotopes Ni^58,60,64

NUCLEAR REACTIONS ^58,60,64Ni(e, e), E=225 MeV; measured σ(θ). ^58,60,64Ni deduced charge distribution.

1969SA14      Izv.Akad.Nauk SSSR, Ser.Fiz. 33, 53 (1969); Bull.Acad.Sci.USSR, Phys.Ser. 33, 50 (1970)

G.A.Savitskii, N.G.Afanasev, I.V.Andreeva, I.S.Gulkarov, L.M.Krugovaya, V.M.Khvastunov, A.A.Khomich, N.G.Shevchenko

Electron Scattering Study of Levels in ²⁴Mg

NUCLEAR REACTIONS ²⁴Mg(e, e'), E = 100-250 MeV; measured σ(E;Ee'); deduced inelastic form factors, charge distribution. ²⁴Mg deduced levels, B(λ), transition radii.

1969SA16      Izv.Akad.Nauk SSSR, Ser.Fiz. 33, 60 (1969); Bull.Acad.Sci.USSR, Phys.Ser. 33, 56 (1970)

G.A.Savitskii, N.G.Afanasev, I.S.Gulkarov, V.D.Kovalev, V.M.Khvastunov, N.G.Shevchenko, I.V.Andreeva

Elastic and Inelastic Scattering of High Energy Electrons by ²³Na and ³⁹K

NUCLEAR REACTIONS ²³Na, ³⁹K(e, e'), E = 100-230 MeV; measured σ(E;Ee', θ); deduced elastic, inelastic form factors. ²³Na, ³⁹K levels deduced B(EL), transition radii.

1968AF01      Yadern.Fiz. 7, 13(1968); Soviet J.Nucl.Phys. 7, 8(1968)

N.G.Afanasev, I.S.Gulkarov, G.A.Savitskii, V.M.Khvastunov, N.G.Shevchenko

Excitation of the Giant Resonance in Si²⁸ by Means of Inelastic Electron Scattering

NUCLEAR REACTIONS ²⁸Si(e, e'), E=150 MeV; measured σ(Ee', θ). ²⁸Si deduced levels, J, π, level-width.

1968AF02      Ukr.Fiz.Zh.(Ukr.Ed.) 13, 1919 (1968); Ukr.Phys.J. 13, 1369 (1969)

V.D.Afanasev, N.G.Afanasev, I.S.Gulkarov, G.A.Savitskii, V.M.Khvastunov, N.G.Shevchenko, A.A.Khomich

Inelastic Scattering of Electrons with Excitation of the First 2⁺ - States of Ni^58,64

NUCLEAR REACTIONS ^58,64Ni(e, e'), E=150, 225 MeV; measured σ(Ee'). ^58,64Ni transitions deduced B(E2).

1968GU03      Phys.Letters 27B, 417 (1968)

I.S.Gulkarov, N.G.Afanasyev, G.A.Savitsky, V.M.Khvastunov, N.G.Shevchenko

Giant Resonance Electroexcitation in ²⁸Si

NUCLEAR REACTIONS ²⁸Si(e, e'), E=150-225 MeV; measured σ(Ee').

doi: 10.1016/0370-2693(68)90223-2
Citations: PlumX Metrics

1968GU09      Izv.Akad.Nauk SSSR, Ser.Fiz. 32, 1763 (1968); Bull.Acad.Sci.USSR, Phys.Ser. 32, 1624 (1969)

I.S.Gulkarov, N.G.Afanasev, G.A.Savitskii, V.M.Khvastunov, N.G.Shevchenko

Electron Excitation of the Giant Resonance in ²⁸Si

NUCLEAR REACTIONS ²⁸Si(e, e'), E = 150-225 MeV; measured σ(E;Ee', θ); deduced form factors. ²⁸Si deduced giant resonance, B(E1), level-width.

1968SA18      Yadern.Fiz. 7, 1181 (1968); Soviet J.Nucl.Phys. 7, 705 (1968)

G.A.Savitskii, N.G.Afanasev, I.S.Gulkarov, V.M.Khvastunov, A.A.Khomich, N.G.Shevchenko

Scattering of High-Energy Electrons by Mg²⁴ and Si²⁸, and the α-Particle Model

NUCLEAR REACTIONS ²⁴Mg, ²⁸Si(e, e), (e, e'), E=100-260 MeV; measured elastic, inelastic form factors. ²⁴Mg, ²⁸Si deduced levels.

1968SA20      Yadern.Fiz, 8, 648 (1968); Soviet J.Nucl.Phys. 8, 376 (1969)

G.A.Savitskii, N.G.Afanasev, I.S.Gulkarov, V.D.Kovalev, A.S.Omelaenko, V.M.Khvastunov, N.G.Shevchenko

Elastic and Inelastic Scattering of High Energy Electrons by Si²⁸ Nuclei

NUCLEAR REACTIONS ²⁸Si(e, e), (e, e'), E=110-260 MeV; measured σ(E;θ), σ(E;Ee', θ). ²⁸Si deduced levels, J, π, reduced transition rates, quadrupole moment.

1968SA24      Urk.Fiz.Zh.(Ukr.Ed.) 13, 1647 (1968); Ukr.Phys.J. 13, 1174 (1969)

G.A.Savitskii, N.G.Afanasev, I.S.Gulkarov, V.D.Kovalev, I.V.Andreeva, V.M.Khvastunov, N.G.Shevchenko

High Energy Electron Scattering by Na²³

NUCLEAR REACTIONS ²³Na(e, e), (e, e'), E=100, 150, 225 MeV; measured σ(Ee', θ); deduced elastic, inelastic form factors. ²³Na deduced B(E2), γ-multipolarity, transition radius.

1967SA12      Yadern.Fiz. 6, 685 (1967);Soviet J.Nucl.Phys. 6, 499 (1968)

G.A.Savitskii, N.G.Afanasev, I.S.Gulkarov, V.D.Kovalev, A.S.Omelaenko, V.M.Khvastunov, N.G.Shevchenko

Determination of Transition Matrix Elements of Si²⁸ from Inelastic Electron Scattering Experiments

NUCLEAR REACTIONS ²⁸Si(e, e'), E=100-260 MeV; measured σ(E).

1967SH12      Yadern.Fiz. 5, 948 (1967); Soviet J.Nucl.Phys. 5, 676 (1967)

N.G.Shevchenko, N.G.Afanasev, G.A.Savitskii, V.M.Khvastunov, V.D.Kovalev, A.S.Omelaenko, I.S.Gulkarov

Scattering of 225-MeV Electrons by Y⁸⁹ and Nb⁹³

NUCLEAR STRUCTURE ⁹³Nb, ⁸⁹Y; measured not abstracted; deduced nuclear properties.