NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = L.Blokhintsev Found 85 matches. 2023BL01 Eur.Phys.J. A 59, 162 (2023) L.D.Blokhintsev, A.S.Kadyrov, A.M.Mukhamedzhanov, D.A.Savin Determination of asymptotic normalization coefficients for the channel 16O → α+12C. II. Excited states 16O(3-, 2+, 1- RADIOACTIVITY 16O(α); analyzed available data; deduced asymptotic normalization coefficients (ANC) for a virtual decay, the overall normalization of σ of peripheral radiative capture reactions.
doi: 10.1140/epja/s10050-023-01079-4
2022BL04 Phys.Atomic Nuclei 85, 154 (2022), Erratum Phys.Atomic Nuclei 85, 306 (2022) Determination of Asymptotic Normalization Coefficients by Analytic Continuation of Differential Cross Sections NUCLEAR REACTIONS 12C(d, p)13C, E=3.7, 5.03, 9, 12, 30 MeV; analyzed available data; deduced the asymptotic normalization coefficients (ANC) using the analytic continuation of experimental differential cross sections for nuclear transfer reactions to the pole point of the reaction amplitude.
doi: 10.1134/S106377882202003X
2022BL07 Eur.Phys.J. A 58, 257 (2022) L.D.Blokhintsev, A.S.Kadyrov, A.M.Mukhamedzhanov, D.A.Savin Determination of asymptotic normalization coefficients for the channel 16O → α+12C: excited state 16O(0+; 6.05. MeV RADIOACTIVITY 16O(α); calculated asymptotic normalization coefficients (ANC) for for the virtual decay by approximating scattering data by the sum of polynomials in energy in the physical region and then extrapolated to the pole, and by solving the Schrodinger equation for the two-body α12 C potential, the parameters of which are selected from the requirement of the best description of the phase-shift analysis data at a fixed experimental binding energy.
doi: 10.1140/epja/s10050-022-00909-1
2022MU07 Eur.Phys.J. A 58, 29 (2022) A.M.Mukhamedzhanov, L.D.Blokhintsev Asymptotic normalization coefficients in nuclear reactions and nuclear astrophysics NUCLEAR REACTIONS 14C, 58Ni(d, p), E<60 MeV; 12,15N(p, γ), E(cm)<2 MeV; 2H(α, γ), E<1 MeV; analyzed available data; deduced asymptotic normalization coefficient (ANC), S-factors, astrophysical reaction rates.
doi: 10.1140/epja/s10050-021-00651-0
2021TU04 Phys.Rev. C 104, 045806 (2021) E.M.Tursunov, S.A.Turakulov, A.S.Kadyrov, L.D.Blokhintsev Astrophysical S factor and rate of 7Be (p, γ)8B direct capture reaction in a potential model NUCLEAR REACTIONS 7Be(p, γ)8B, E(cm)<13 MeV; calculated s-wave-scattering length, phase shift, astrophysical S factor, partial E1, E2, and M1 components of astrophysical S factor. 7Be(p, γ)8B, T9=0.001-10.0; calculated capture reaction rates. Comparison of astrophysical S factor with experimental data, and reaction rates with the results of the NACRE II Collaboration. Two-body potential model using single-channel approximation, with a modified potential.
doi: 10.1103/PhysRevC.104.045806
2020BL04 Phys.Atomic Nuclei 83, 573 (2020) Analytic Continuation of Scattering Data, Asymptotic Normalization Coefficients, and Astrophysics
doi: 10.1134/S1063778820040067
2019BL07 Phys.Rev. C 100, 024627 (2019) L.D.Blokhintsev, A.S.Kadyrov, A.M.Mukhamedzhanov, D.A.Savin New method of analytic continuation of elastic-scattering data to the negative-energy region, and asymptotic normalization coefficients for 17O and 13C NUCLEAR REACTIONS 12C(n, n), E=0.050, 0.100, 0.157, 0.207, 0.257, 0.307, 0.357, 0.407, 0.457, 0.507, 0.530, 0.630, 0.730, 0.830, 0.930, 1.040 MeV; 16O(n, n), E=0.20, 0.30, 0.40, 0.51, 0.60, 0.698, 0.73, 1.00, 1.21, 1.50, 1.75, 1.833, 2.15, 2.250, 2.353, 3.000 MeV; calculated asymptotic normalization coefficients (ANC) for excited s-states in 13C and 17O populated by elastic n-scattering using a new method based on analytic approximation of the modulus-squared of the partial-wave scattering amplitude. Comparison with theoretical results from traditional effective-range function approach.
doi: 10.1103/PhysRevC.100.024627
2018BL01 Phys.Rev. C 97, 024602 (2018) L.D.Blokhintsev, A.S.Kadyrov, A.M.Mukhamedzhanov, D.A.Savin Extrapolation of scattering data to the negative-energy region. II. Applicability of effective range functions within an exactly solvable model NUCLEAR REACTIONS 2H, 12C(α, α'), E not given; investigated the applicability of the effective range function (ERF) and the Δ function for scattering data to the negative-energy region in order to determine asymptotic normalization coefficients (ANCs); search for the parameters of the excited 0+ state in α+12C system using exactly solvable model.
doi: 10.1103/PhysRevC.97.024602
2018BL06 Phys.Rev. C 98, 064610 (2018) L.D.Blokhintsev, A.S.Kadyrov, A.M.Mukhamedzhanov, D.A.Savin Extrapolation of scattering data to the negative-energy region. III. Application to the p - 16O system NUCLEAR REACTIONS 16O(p, p)17F, E(cm)=0-2 MeV; calculated asymptotic normalization coefficients (ANCs) for g.s. and excited state of 17F, polynomial approximation of Κ0(E), Κ2(E), Δ0(E), and Δ2(E) functions using the effective-range function (ERF) and the Δ methods. Comparison with experimental data.
doi: 10.1103/PhysRevC.98.064610
2018SH33 Phys.Rev. C 98, 044624 (2018) A.M.Shirokov, A.I.Mazur, I.A.Mazur, E.A.Mazur, I.J.Shin, Y.Kim, L.D.Blokhintsev, J.P.Vary Nucleon-α scattering and resonances in 5He and 5Li with JISP16 and Daejeon16 NN interactions NUCLEAR REACTIONS 4He(p, X)5Li, E*=0-15 MeV; 4He(n, X)5He, E*=0-17 MeV; calculated eigenenergies, widths, and phase shifts of resonances in pα and nα scattering in non-resonant and resonant 3/2- and 1/2- states using extension of the ab initio no-core shell model single state harmonic oscillator representation of scattering equations (NCSM-SS-HORSE) with JISP16 and Daejeon16 nucleon-nucleon interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.98.044624
2017BL04 Phys.Rev. C 95, 044618 (2017) L.D.Blokhintsev, A.S.Kadyrov, A.M.Mukhamedzhanov, D.A.Savin Extrapolation of scattering data to the negative-energy region
doi: 10.1103/PhysRevC.95.044618
2017BL06 Phys.Atomic Nuclei 80, 226 (2017); Yad.Fiz. 80, 102 (2017) L.D.Blokhintsev, A.I.Mazur, I.A.Mazur, D.A.Savin, A.M.Shirokov SS-HORSE method for studying resonances
doi: 10.1134/S1063778817020077
2017BL11 Phys.Atomic Nuclei 80, 1093 (2017) L.D.Blokhintsev, A.I.MazurI.A.Mazur, D.A.Savin, A.M.Shirokov SS-HORSE Method for Analysis of Resonances: Charged-Particle Scattering
doi: 10.1134/S1063778817060072
2016BL08 Phys.Atomic Nuclei 79, 358 (2016) Analytic continuation of scattering data to the region of negative energies for systems that have one and two bound states NUCLEAR REACTIONS 2H, 12C(α, x), E not given; calculated binding energy, mass excess, asymptotic normalization coefficient using exactly solvable model for three versions of expansion and various powers of polynomial approximation of the energy function within three steming from data on continuous states. Compared with data.
doi: 10.1134/S1063778816030066
2014BL02 Phys.Atomic Nuclei 77, 351 (2014); Yad.Fiz. 77, 376 (2014) Analytic continuation of the effective-range expansion as a method for determining the features of bound states: Application to the 6Li nucleus NUCLEAR REACTIONS 4He(d, X)6Li, E<10 MeV; calculated scattering phase shifts using Faddeev equations. Comparison with experimental data.
doi: 10.1134/S1063778814030041
2014BL10 Few-Body Systems 55, 1009 (2014) L.D.Blokhintsev, L.I.Nikitina, Yu.V.Orlov, D.A.Savin Characteristics of d + α Bound and Resonant States from Analytic Continuation of the Effective-Range Expansion NUCLEAR REACTIONS 2H(α, X)6Li, E not given; calculated asymptotic normalization coefficients, resonance width, J, π. Comparison with available data.
doi: 10.1007/s00601-013-0755-5
2014PI08 Few-Body Systems 55, 1001 (2014) R.G.Pizzone, C.Spitaleri, M.L.Sergi, L.Lamia, A.Tumino, C.A.Bertulani, L.Blokhintsev, V.Burjan, V.Kroha, M.La Cognata, J.Mrazek, A.M.Mukhamedzhanov, R.Sparta Trojan Horse Particle Invariance: An Extensive Study
doi: 10.1007/s00601-014-0829-z
2013BL08 Eur.Phys.J. A 49, 108 (2013) L.D.Blokhintsev, A.M.Mukhamedzhanov, R.Yarmukhamedov Anomalous asymptotics of radial overlap functions for bound systems of three or more particles NUCLEAR STRUCTURE 9Be, 16O, 20Ne; calculated radial overlaps of bound states nuclear wave functions treated as a system of three parts.
doi: 10.1140/epja/i2013-13108-6
2013PI03 Phys.Rev. C 87, 025805 (2013) R.G.Pizzone, C.Spitaleri, C.A.Bertulani, A.M.Mukhamedzhanov, L.Blokhintsev, M.La Cognata, L.Lamia, A.Rinollo, R.Sparta, A.Tumino Updated evidence of the Trojan horse particle invariance for the 2H(d, p)3H reaction NUCLEAR REACTIONS 2H(6Li, pt)α, E=14 MeV; measured proton and triton spectra by energy-loss method, momentum distribution, σ(θ) at INFN-LNS facility in Catania; deduced momentum distribution width, quasifree (QF) contribution, astrophysical S(E) factor for 2H(d, p) reaction via Trojan-horse method (THM) after 6Li breakup. 2H(3He, pt), E(cm)<0.9 MeV; analyzed averaged astrophysical S(E) factor for 2H(d, p) reaction measured via THM after 3He breakup. PWIA analysis. Comparison with previous experimental studies.
doi: 10.1103/PhysRevC.87.025805
2012AF02 Bull.Rus.Acad.Sci.Phys. 76, 433 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 489 (2012) N.V.Afanaseva, N.A.Burkova, L.D.Blokhintsev The construction of wave functions in the 7Li → d + 5He channel by the projection method NUCLEAR STRUCTURE 7Li; calculated relative motion wave functions, Whittaker functions, virtual disintegration channels; 2H, 5He.
doi: 10.3103/S1062873812040041
2012AF03 Bull.Rus.Acad.Sci.Phys. 76, 444 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 501 (2012) N.V.Afanaseva, N.A.Burkova, K.A.Zhaksybekova, L.D.Blokhintsev Spectroscopic factors in the 7Li → d + 5He(α) fragmentation channel RADIOACTIVITY 7Li(d); calculated spectroscopic factors. Shell model, comparison with other data.
doi: 10.3103/S1062873812040053
2012BL04 Bull.Rus.Acad.Sci.Phys. 76, 425 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 481 (2012) Allowing for Coulomb effects in the effective range expansion for two coupled channels
doi: 10.3103/S1062873812040089
2012BL05 Bull.Rus.Acad.Sci.Phys. 76, 438 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 494 (2012) L.D.Blokhintsev, V.O.Eremenko, D.A.Savin The possibility of using screened coulomb potentials in calculating asymptotic normalization coefficients
doi: 10.3103/S1062873812040090
2012BL08 Bull.Rus.Acad.Sci.Phys. 76, 909 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 1012 (2012) L.D.Blokhintsev, V.O.Eremenko, Yu.V.Orlov, D.A.Savin Studying the general properties of potentials by means of dimensionless scaling variables
doi: 10.3103/S1062873812080072
2011BL05 Bull.Rus.Acad.Sci.Phys. 75, 490 (2011); Izv.Akad.Nauk RAS, Ser.Fiz 75, 526 (2011) L.D.Blokhintsev, V.I.Kukulin, V.N.Pomerantsev, D.A.Savin Exchange mechanism of dα interaction and vertex constants of 6Li NUCLEAR STRUCTURE 6Li; calculated wave functions of dα interaction, orbital angular momenta.
doi: 10.3103/S1062873811040083
2011BL06 Bull.Rus.Acad.Sci.Phys. 75, 505 (2011); Izv.Akad.Nauk RAS, Ser.Fiz 75, 541 (2011) L.D.Blokhintsev, V.O.Eremenko, B.F.Irgaziev, Yu.V.Orlov Calculating the characteristics of neutron-deuteron and proton-deuteron systems in a two-body potential model NUCLEAR STRUCTURE 3H, 3He; calculated binding energy, asymptotic normalization coefficients. Two-body potential model.
doi: 10.3103/S1062873811040095
2011IR01 Bull.Rus.Acad.Sci.Phys. 75, 511 (2011); Izv.Akad.Nauk RAS, Ser.Fiz 75, 547 (2011) B.F.Irgaziev, A.M.Mukhamedzhanov, Yu.V.Orlov, L.D.Blokhintsev Extracting the complex energy of broad resonances by the S-matrix pole method NUCLEAR REACTIONS 12C(α, α), 26Mg(n, n), E not given; calculated energies and width for p-wave resonances, phase shifts. R-matrix and S-matrix pole fitting methods.
doi: 10.3103/S1062873811040204
2011MU08 Phys.Rev. C 83, 055805 (2011) A.M.Mukhamedzhanov, L.D.Blokhintsev, B.F.Irgaziev Reexamination of the astrophysical S factor for the α+d → 6Li+γ reaction NUCLEAR REACTIONS 2H(α, 6Li); analyzed α-d elastic scattering phase shift; deduced asymptotic normalization coefficient (ANC) for the decay of 6Li into α+d, reaction rates and astrophysical factor S24(E) for the radiative capture process of α+d to 6Li+γ using α-d potential model.
doi: 10.1103/PhysRevC.83.055805
2011PI04 Phys.Rev. C 83, 045801 (2011) R.G.Pizzone, C.Spitaleri, L.Lamia, C.Bertulani, A.Mukhamedzhanov, L.Blokhintsev, V.Burjan, S.Cherubini, Z.Hons, G.G.Kiss, V.Kroha, M.La Cognata, C.Li, J.Mrazek, S.Piskor, S.M.R.Puglia, G.G.Rapisarda, S.Romano, M.L.Sergi, A.Tumino Trojan horse particle invariance studied with the 6Li(d, α)4He and 7Li( p, α)4He reactions NUCLEAR REACTIONS 6Li(3He, 2α), E=17.5 MeV; measured Eα, Iα, angular distribution; deduced momentum distribution, Q value, quasifree (QF) contribution. 6Li(d, α), E(cm)=0-5 MeV; 7Li(p, α), E(cm)=0-7 MeV; 7Li(3He, 2α), E not given; analyzed excitation functions, σ, differential σ. Trojan horse method (THM) in the framework of the plane wave approximation.
doi: 10.1103/PhysRevC.83.045801
2009PI12 Phys.Rev. C 80, 025807 (2009) R.G.Pizzone, C.Spitaleri, A.M.Mukhamedzhanov, L.D.Blokhintsev, C.A.Bertulani, B.F.Irgaziev, M.La Cognata, L.Lamia, S.Romano Effects of distortion of the intercluster motion in 2H, 3He, 3H, 6Li, and 9Be on Trojan horse applications NUCLEAR REACTIONS 2H(p, 2p), E=5, 6 MeV; 2H(t, pt), E=35.5 MeV; 2H(3He, p3He), E=17 MeV; 2H(6Li, 3Heα), E=25 MeV; 2H(9Be, α6Li), E=22 MeV; 2H(10B, α7Be), (11B, α8Be), E=27 MeV; 2H(7Li, 2α), E=20 MeV; 2H(15N, α12C), E=60 MeV; 2H(18O, α15N), E=54 MeV; 3H(3He, d3He), (3He, p3He), E=65 MeV; 3H(3He, 2d), E=50, 65, 78 MeV; 3H(3He, pt), E=78 MeV; 3H(d, 2d), E=35 MeV; 3H(p, 2p), (p, pd), E=45.6 MeV; 3He(p, pd), E=65, 85, 100, 590 MeV; 3He(d, pt), E=17, 35, 52 MeV; 3He(d, p3He), E=18 MeV; 6Li(6Li, 2α)4He, E=2.1-44 MeV; 7Li(3He, 2α), E=11, 12, 33 MeV; 9Be(p, pα)5He, E=47, 55, 57, 160 MeV; 9Be(3He, 2α)4He, E=2.8, 3, 4 MeV; 9Be(p, dα), E=30 MeV; 9Be(7Li, α7Li), E=52 MeV; 9Be(α, 2α), E=140 MeV; calculated widths (FWHM) of momentum distributions of the spectator particles using the Trojan Horse method and compared with the experimental data.
doi: 10.1103/PhysRevC.80.025807
2008BL07 Bull.Rus.Acad.Sci.Phys. 72, 295 (2008); Izv.Akad.Nauk RAS, Ser.Fiz. 72, 321 (2008) L.D.Blokhintsev, B.F.Irgaziev, A.M.Mukhamedzhanov, A.N.Safronov, A.A.Safronov Determination of the nuclear vertex constants for the 7Be <-> 3He4He vertex using the N/D equations and calculation of the astrophysical S factor for the 4He(3He, γ)7Be reaction
doi: 10.3103/S1062873808030064
2008BL10 Phys.Atomic Nuclei 71, 1219 (2008); Yad.Fiz. 71, 1247 (2008) L.D.Blokhintsev, V.O.Yeremenko Nuclear vertex constants and asymptotic normalization coefficients
doi: 10.1134/S1063778808070144
2008BL11 Bull.Rus.Acad.Sci.Phys. 72, 811 (2008) L.D.Blokhintsev, V.O.Eremenko, B.F.Irgaziev, Yu.V.Orlov Characteristics of scattering of Λ hyperons from nuclei within the potential model NUCLEAR STRUCTURE 7He, 6,7,8,9Be, 6,7,8Li, 11C, 14N, 15O, 39Ca, 88Zr, 207Pb; calculated scattering lengths, phase shifts, and effective radii for low energy Λ scattering using Woods-Saxon, Hulthen, and Yukawa potentials.
doi: 10.3103/S106287380806021X
2008MU07 J.Phys.(London) G35, 014016 (2008) A.M.Mukhamedzhanov, L.D.Blokhintsev, B.F.Irgaziev, A.S.Kadyrov, M.La Cognata, C.Spitaleri, R.E.Tribble Trojan Horse as an indirect technique in nuclear astrophysics NUCLEAR REACTIONS 15N(p, α), E=0-0.85 MeV; calculated astrophysical S-factor. Comparisons with experimental data. Trojan Horse Method.
doi: 10.1088/0954-3899/35/1/014016
2007AL28 Phys.Rev. C 75, 054003 (2007) E.O.Alt, L.D.Blokhintsev, A.M.Mukhamedzhanov, A.I.Sattarov Deuteron elastic scattering and stripping processes off 12C as a three-body problem NUCLEAR REACTIONS 12C(d, d), (d, p), E=4.66, 15, 56 MeV; calculated σ and analyzing powers within the framework of few body integral equations theory. Compared results to data.
doi: 10.1103/PhysRevC.75.054003
2007BL11 Bull.Rus.Acad.Sci.Phys. 71, 408 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 423 (2007) L.D.Blokhintsev, V.O.Eremenko, B.F.Irgaziev, Yu.V.Orlov Vertex Constants (Asymptotic Normalization Coefficients) and Mean-Square Radii, of Hypernuclei in the Potential Model NUCLEAR STRUCTURE A=7-208; calculated vertex constants, asymptotic normalization coefficients and mean-square radii for a number of hypernuclei using the potential approach.
doi: 10.3103/S1062873807030215
2007BL13 Nucl.Phys. A790, 241c (2007) L.D.Blokhintsev, A.N.Safronov, A.A.Safronov An analytic approach to constructing effective local interactions in few-body systems and its application to N4He, N3H, N3He, and 3He4He scattering NUCLEAR REACTIONS 3H(n, X), 3He(p, X), 4He(n, X), (p, X), (3He, X), E≈0-15 MeV; calculated phase-shifts. Comparison with data.
doi: 10.1016/j.nuclphysa.2007.03.040
2007MU10 Nucl.Phys. A787, 321c (2007) A.M.Mukhamedzhanov, L.D.Blokhintsev, S.Brown, V.Burjan, S.Cherubini, V.Z.Goldberg, M.Gulino, B.F.Irgaziev, E.Johnson, K.Kemper, V.Kroha, M.La Cognata, L.Lamia, A.Momotyuk, R.G.Pizzone, B.Roeder, G.Rogachev, S.Romano, C.Spitaleri, R.E.Tribble, A.Tumino Indirect Techniques in Nuclear Astrophysics. Asymptotic Normalization Coefficient and Trojan Horse NUCLEAR REACTIONS 13C(α, n), E=0-0.9 MeV; calculated astrophysical S-factor. Asymptotic normalization coefficient method. Comparison with data. 6Li(d, α), 7Li(p, α), E=0-800 keV; calculated astrophysical S-factor. Trojan horse method.
doi: 10.1016/j.nuclphysa.2006.12.051
2006BL07 Phys.Atomic Nuclei 69, 433 (2006); Yad.Fiz. 69, 456 (2006) L.D.Blokhintsev, S.B.Igamov, M.M.Nishonov, R.Yarmukhamedov Calculation of the Nuclear Vertex Constant (Asymptotic Normalization Coefficient) for the Virtual Decay 6Li → α + d on the Basis of the Three-Body Model and Application of the Result in Describing the Astrophysical Nuclear Reaction d(α, γ)6Li at Ultralow Energies NUCLEAR REACTIONS 2H(α, γ), E=0-600 keV; calculated nuclear vertex constant, astrophysical S-factor. Three-body model.
doi: 10.1134/S1063778806030069
2006BL15 Bull.Rus.Acad.Sci.Phys. 70, 233 (2006) L.D.Blokhintsev, A.N.Safronov, A.A.Safronov Correlation between low-energy parameters of Nd and Nα scattering and vertex constants of virtual dissociation (Fusion) of 2H and 4He nuclei NUCLEAR REACTIONS 2H, 4He(n, X), (p, X), E=low; calculated scattering lengths, phase shifts, effective radii.
2006BL16 Bull.Rus.Acad.Sci.Phys. 70, 262 (2006) L.D.Blokhintsev, V.O.Eremenko, A.A.Sudarenko Square-with-diagonal diagram for nuclear processes NUCLEAR REACTIONS 2H(d, d), (d, n), 6Li(d, d), (d, p), (d, α), E not given; calculated singularity energies.
2006BL18 Bull.Rus.Acad.Sci.Phys. 70, 1869 (2006) L.D.Blokhintsev, A.N.Safronov, A.A.Safronov Analytical approach to construction of effective interaction operators for analysis of n3H, p3He, and 3He4He scattering in low-energy region NUCLEAR REACTIONS 3H(n, X), 3He(p, X), 4He(3He, X), E < 10 MeV; calculated S-wave scattering amplitudes using an analytical approach.
2006MU15 Eur.Phys.J. A 27, Supplement 1, 205 (2006) A.M.Mukhamedzhanov, L.D.Blokhintsev, B.A.Brown, V.Burjan, S.Cherubini, C.A.Gagliardi, B.F.Irgaziev, V.Kroha, F.M.Nunes, F.Pirlepesov, R.G.Pizzone, S.Romano, C.Spitaleri, X.D.Tang, L.Trache, R.E.Tribble, A.Tumino Indirect techniques in nuclear astrophysics: Asymptotic Normalization Coefficient and Trojan Horse NUCLEAR REACTIONS 14N(3He, d), E=26.3 MeV; measured σ(θ). 14N(p, γ), E ≈ 100-600 keV; deduced astrophysical S-factor. 11C, 13N(p, γ), E not given; analyzed resonant and nonresonant amplitudes. Asymptotic normalization coefficient and Trojan horse techniques discussed.
doi: 10.1140/epja/i2006-08-032-7
2005BL17 Yad.Fiz. 68, 1165 (2005); Phys.Atomic Nuclei 68, 1120 (2005) L.D.Blokhintsev, V.I.Kukulin, V.N.Pomerantsev Puzzle of the 6Li Quadrupole Moment: Steps toward Solving It NUCLEAR MOMENTS 6Li; calculated quadrupole moment; deduced role of three-deuteron configuration and negative exchange contribution.
doi: 10.1134/1.1992566
2005BL21 Yad.Fiz. 68, 1427 (2005); Phys.Atomic Nuclei 68, 1372 (2005) L.D.Blokhintsev, M.K.Ubaidullaeva, R.Yarmukhamedov Coordinate Asymptotic Behavior of the Radial Three-Particle Wave Function for a Bound State Involving Two Charged Particles NUCLEAR STRUCTURE 9Be; calculated three-particle wave functions.
doi: 10.1134/1.2011496
2005BL35 Bull.Rus.Acad.Sci.Phys. 69, 1743 (2005) L.D.Blokhintsev, A.N.Safronov, A.A.Safronov Analytical approach to construction of effective potentials between aggregates of strongly interaction particles taking into account Coulomb effects and its application to pd scattering NUCLEAR REACTIONS 2H(p, p), E=0-50 MeV; calculated effective local potential, phase shifts. Analytical approach.
2005MU27 J.Phys.(London) G31, S1413 (2005) A.M.Mukhamedzhanov, E.O.Alt, L.D.Blokhintsev, S.Cherubini, B.F.Irgaziev, A.S.Kadyrov, D.Miljanic, A.Musumarra, M.G.Pellegriti, F.Pirlepesov, C.Rolfs, S.Romano, C.Spitaleri, N.K.Timofeyuk, R.E.Tribble, A.Tumino Few-body problems in nuclear astrophysics
doi: 10.1088/0954-3899/31/10/005
2003BL18 Bull.Rus.Acad.Sci.Phys. 67, 115 (2003) Generalized folded potential
2003TI10 Phys.Rev. C 68, 021601 (2003) N.K.Timofeyuk, L.D.Blokhintsev, J.A.Tostevin Pre-asymptotic behavior of single-particle overlap integrals of non-Borromean two-neutron halos NUCLEAR STRUCTURE 12Be, 15B, 9,16C; calculated single-particle overlap integrals, local effective potentials. NUCLEAR REACTIONS 9Be(12Be, 11BeX), E=80 MeV/nucleon; calculated σ, stripping and diffraction contributions, longitudinal momentum distribution, role of pre-asymptotic behavior.
doi: 10.1103/PhysRevC.68.021601
2001BL15 Bull.Rus.Acad.Sci.Phys. 65, 77 (2001) Asymptotics of Wave Functions for Many-Nucleon Nuclei in Two-Particle Channels
2000AV01 Yad.Fiz. 63, No 3, 519 (2000); Phys.Atomic Nuclei 63, 448 (2000) G.V.Avakov, L.D.Blokhintsev, E.N.Voronina Protonium Formation in Collisions of Antiprotons with Hydrogen Atoms ATOMIC PHYSICS 1H(p-bar, X), E=1-250 keV; calculated protonium formation σ(E), σ(θ).
doi: 10.1134/1.855653
1999BL19 Yad.Fiz. 62, No 8, 1368 (1999); Phys.Atomic Nuclei 62, 1289 (1999) L.D.Blokhintsev, M.K.Ubajdullaeva, R.Yarmukhamedov Coordinate Asymptotic Behavior of the Radial Three-Body Wave Function of a Bound State NUCLEAR STRUCTURE 6He; calculated three-body wave function, asymptotic behaviour.
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
1998BL17 Bull.Rus.Acad.Sci.Phys. 62, 64 (1998) L.D.Blokhintsev, L.I.Nikitina, Yu.V.Orlov Hypertriton in a Potential Model NUCLEAR STRUCTURE 3H; calculated hypernucleus virtual decay form factor, vertex constant. Two-body model, Hulthen and Yukawa potentials.
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
1995BL26 Bull.Rus.Acad.Sci.Phys. 59, 1916 (1995) L.D.Blokhintsev, O.Dias, A.M.Mukhamedzhanov, M.V.Poletaeva Asymptotics of Nuclear Wave Functions in Two-Particle Channels
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.
1993BL09 Phys.Rev. C48, 2390 (1993) L.D.Blokhintsev, V.I.Kukulin, A.A.Sakharuk, D.A.Savin, E.V.Kuznetsova Determination of the 6Li → α + d Vertex Constant (Asymptotic Coefficient) from the 4He + d Phase-Shift Analysis NUCLEAR STRUCTURE 6Li; analyzed reaction data; deduced nuclear vertex constant for α+d channel.
doi: 10.1103/PhysRevC.48.2390
1991BL04 Yad.Fiz. 53, 693 (1991); Sov.J.Nucl.Phys. 53, 433 (1991) L.D.Blokhintsev, V.I.Kukulin, D.A.Savin, A.A.Sakharuk Manifestation of Pauli-Forbidden States in Low-Energy d 4He Scattering NUCLEAR REACTIONS 4He(d, d), E < 12 MeV; calculated phase shift vs E; deduced Pauli-forbidden states role, nucleon-α interaction dependence.
1990BL13 Yad.Fiz. 51, 1289 (1990); Sov.J.Nucl.Phys. 51, 819 (1990) L.D.Blokhintsev, V.I.Kukulin, D.A.Savin Analysis of Higher Partial Waves of Elastic D + 4He Scattering within the Framework of the Three-Body Problem NUCLEAR REACTIONS 4He(d, d), E ≤ 16 MeV; calculated phase shift, inelasticity coefficients vs E. Faddeev formalism.
1990BL16 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 569 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, No.3, 190 (1990) L.D.Blokhintsev, A.M.Mukhamedzhanov, N.K.Timofeyuk, Yu.M.Chuvilsky Microscopic Approach to the Calculation of the Vertex Constants of Neutron Cleavage NUCLEAR STRUCTURE 13C, 9Be, 16O, 15,14N; calculated neutron cleavage vertex constant. Microscopic approach, translationally invariant shell model.
1988AV05 Yad.Fiz. 47, 1508 (1988) G.V.Avakov, S.N.Belolipetsky, L.D.Blokhintsev, G.S.Valiev, I.R.Gulamov, Yu.I.Denisov, T.Iskhakov, A.M.Mukhamedzhanov, E.A.Romanovsky, R.Yarmukhamedov Reaction 3He(p, d)pp and 3He → ppn On-Shell Vertex Function NUCLEAR REACTIONS 3He(p, 2p), E=18.6 MeV; measured σ(θd, Ed); deduced 3He-ppn on-shell vertex function.
1988BA74 Yad.Fiz. 48, 1273 (1988) A.G.Baryshnikov, L.D.Blokhintsev, I.M.Narodetsky, D.A.Savin The Quark Compound Bag Method in the Four-Nucleon Problem NUCLEAR STRUCTURE 4He; calculated binding energy. Quark compound bag.
1986AV01 Yad.Fiz. 43, 824 (1986) G.V.Avakov, L.D.Blokhintsev, A.M.Mukhamedzhanov, R.Yarmukhamedov Three-Particle Coulomb Effects in Nuclear Reactions with Three Charged Particles NUCLEAR REACTIONS 27Al(3He, d), E=37.7 MeV; 6Li(d, d), (d, t), E=12 MeV; 9Be(3He, d), E=10, 30, 40 MeV; 6,7Li(d, 6He), E=8, 12 MeV; calculated σ(θ); deduced three-particle Coulomb effects role.
1986AV08 Yad.Fiz. 44, 1471 (1986) G.V.Avakov, L.D.Blokhintsev, T.D.Blokhintseva, V.P.Kurochkin, Zh.P.Pustylnik Calculation of the Cross Section of the Reaction π+7Li → e+e-p6Li NUCLEAR REACTIONS 7Li(π+, e+e-p), E=380 MeV; calculated σ(θ), spectra. Nuclear cluster, shell models.
1986BA15 Ukr.Fiz.Zh. 31, 16 (1986) A.G.Baryshnikov, L.D.Blokhintsev, S.P.Krekoten, A.N.Safronov Positive Kaon Scattering by 2H, 3He and 4He Nuclei NUCLEAR REACTIONS 2H, 3,4He(K+, K+), E=5-120 MeV; calculated σ(θ). K-matrix approach.
1986BA73 Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 1962 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.10, 90 (1986) A.G.Baryshnikov, L.D.Blokhintsev, R.Kapote, D.A.Savin Resonant Mechanism of the Reaction tt → αnn at very Low Incident Energy NUCLEAR REACTIONS 3H(t, nα), E=low; calculated σ(Eα), σ(En). 5He deduced resonance excitation mechanism.
1986BL15 Yad.Fiz. 44, 1167 (1986); Sov.J.Nucl.Phys. 44, No.5, 758 (1986) L.D.Blokhintsev, S.M.Rasulev, R.Yarmukhamedov Determination of Nuclear Vertex Constants (Asymptotic Coefficients) from Charged-Particle-Transfer Reactions NUCLEAR REACTIONS 2H(d, n), E=8.15 MeV; 3H(d, n), E=15 MeV; analyzed σ(θ). 3,4He deduced nuclear vertex constants.
1984BA17 Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 149 (1984); Bull.Acad.Sci.USSR, Phys.Ser. 48, No.1, 151 (1984) A.G.Baryshnikov, L.D.Blokhintsev, S.P.Kretkoren Inclusion of Triangle Diagrams in the Process N + T → N + T in K-Matrix Scattering and Reaction Calculations in Four Nucleon Systems NUCLEAR REACTIONS 3H(p, n), E=12.4, 21, 30 MeV; 3He(n, p), E=14.4 MeV; 2H(d, p), E=25.3, 83 MeV; calculated σ(θ). K-Matrix formalism, triangle diagram inclusion.
1984BL21 Fiz.Elem.Chastits At.Yadra 15, 1296 (1984); Sov.J.Part.Nucl 15, 580 (1984) L.D.Blokhintsev, A.M.Mukhamedzhanov, A.N.Safronov Coulomb Effects in Nuclear Reactions with Charged Particles NUCLEAR REACTIONS 4He(3He, 3He), E=1-14 MeV; 2H(p, p), E=0-14 MeV; 4He(n, n), (p, p), E=0-23 MeV; calculated S-, P-wave phase shifts. 12C(d, n), E=11.8, 15.25 MeV; 12C, 19F(3He, d), E=16 MeV; 27Al(d, p), E=10, 30 MeV; 12C(14N, 13N), E=70 MeV; 208Pb(16O, 17O), E=90, 150 MeV; 6Li(d, d), E=8, 10, 12, 14.7 MeV; 7Li(p, α), E=45.2 MeV; 7Li(d, 6Li), E=12 MeV; calculated σ(θ).
1983BL13 Yad.Fiz. 37, 312 (1983); Sov.J.Nucl.Phys. 37, 186 (1983) L.D.Blokhintsev, A.I.Veselov, I.M.Narodetsky Effects of Proton-Deuteron Rescattering in the Reaction tp → pnd at Intermediate Energies NUCLEAR REACTIONS 1H(t, np), E at 2.5 GeV/c; calculated reaction amplitude. Triangle diagrams, proton-deuteron rescattering.
1983BL15 Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 2168 (1983) Coulomb Interaction Effects in the N/D-Equations and the K-Matrix Approach to Nuclear Reaction Theories NUCLEAR REACTIONS 4He(3He, 3He), 2H, 3He(p, p), E ≈ 2-14 MeV; calculated phase shift vs E. K-matrix approach, Coulomb effects.
1982BL05 Czech.J.Phys. B32, 340 (1982) Scattering of Positive Kaons by Lightest Nuclei on the Basis of Dispersion Methods NUCLEAR REACTIONS 2H, 3,4He(K+, K+), E=5-20 MeV; calculated Coulomb-nuclear amplitudes, σ(θ). Inverse amplitude, K-matrix, N/D equation methods.
doi: 10.1007/BF01602083
1980BA55 Yad.Fiz. 32, 369 (1980); Sov.J.Nucl.Phys. 32, 191 (1980) A.G.Baryshnikov, V.B.Belyaev, L.D.Blokhintsev, B.F.Irgaziev, Yu.V.Orlov Scattering and Reactions in a 4-Nucleon System within the Framework of the K-Matrix Formalism NUCLEAR REACTIONS 3He(p, p), E=9.75, 19.48, 30.6 MeV; 3H(p, p), E=13.6, 19.48 MeV; calculated σ(θ); deduced nucleon-nucleon interaction dependence. Multi-channel K-matrix formalism.
1977BA46 Yad.Fiz. 25, 1167 (1977); Sov.J.Nucl.Phys. 25, 620 (1977) A.G.Baryshnikov, L.D.Blokhintsev, I.M.Narodetskii Microscopic K-Matrix Approach to the Continuous Spectrum in the Four-Nucleon Problem NUCLEAR REACTIONS 3He(p, p), E=9.75-156 MeV; 3H(p, n), E=13.6 MeV; 2H(d, p), E=8.1-83 MeV; 2H(d, d); calculated σ(E).
1977BL04 Yad.Fiz. 25, 315 (1977); Sov.J.Nucl.Phys. 25, 171 (1977) Elastic Scattering of K+ Mesons by Deuterons at Low Energies NUCLEAR REACTIONS 2H(K+, K+), E=low MeV; calculated σ.
1977BL11 Fiz.Elem.Chastits At.Yadra 8, 1189 (1977); Sov.J.Part.Nucl. 8, 485 (1977) L.D.Blokhintsev, I.Borbely, E.I.Dolinskii Nuclear Vertex Constants NUCLEAR STRUCTURE 2H, 3H, 3He, 4He, 6Li; reviewed properties of nuclear vertex constants, relation to nuclear wave functions.
1976BA51 Nucl.Phys. A272, 327 (1976) A.G.Baryshnikov, L.D.Blokhintsev, I.M.Narodetsky Application of the Method of Integral Equations for Calculating the Vertex Constants for an α-Particle NUCLEAR STRUCTURE 4He; calculated vertex constants.
doi: 10.1016/0375-9474(76)90335-3
1975BA38 J.Phys. (London) G1, L43 (1975) A.G.Baryshnikov, L.D.Blokhintsev Dispersion K-Matrix Approach to αt Scattering and Determination of the Vertex Constant for the Process α → t+p NUCLEAR REACTIONS 3H(α, α), E=8.249 MeV; calculated σ(θ).
doi: 10.1088/0305-4616/1/6/003
1975BA43 Yad.Fiz. 22, 104 (1975); Sov.J.Nucl.Phys. 22, 50 (1975) A.G.Baryshnikov, L.D.Blokhintsev Analysis of the Elastic Scattering of α Particles by 6Li Using the K-Matrix and Pade-Approximant Approaches and the Determination of the Coupling Constant for the Vertex 6Li → α + d NUCLEAR REACTIONS 6Li(α, α); analyzed reaction in framework of K-matrix approach.
1974BA34 Nucl.Phys. A224, 61 (1974) A.G.Baryshnickov, L.D.Blokhintsev, A.N.Safronov, V.V.Turovtsev Dispersion K-Matrix Approach to Nuclear Reactions and its Application to Nα Scattering NUCLEAR REACTIONS 4He(p, p), E=20.62 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(74)90162-6
1973BA27 Phys.Lett. 45B, 1 (1973) A.G.Baryshnickov, L.D.Blokhintsev, A.M.Mukhamedzhanov, V.V.Turovtsev Peripheral Model Approach to the Process of Radiative Proton Capture by Tritium NUCLEAR REACTIONS 3H(p, γ), E=156 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(73)90237-2
1972BB19 Pisma Zh.Eksp.Teor.Fiz. 16, 414 (1972); JETP Lett.(USSR) 16, 294 (1972) A.G.Baryshnikov, L.D.Blokhintsev, A.N.Safronov, V.V.Turovtsev Diagram K-Matrix Approach to pα Scattering
1971BA61 Phys.Lett. 36B, 205 (1971) A.G.Baryshnickov, L.D.Blokhintsev Vertex Constants for an Alpha Particle NUCLEAR REACTIONS 4He(p, p), E=49, 98 MeV; 12C(d, α), E=20 MeV; 12C(p, 3He), E=40 MeV; calculated σ(θ). Peripheral model.
doi: 10.1016/0370-2693(71)90069-4
1970AB17 Izv.Akad.Nauk SSSR, Ser.Fiz. 34, 2192 (1970); Bull.Acad.Sci.USSR, Phys.Ser. 34, 1956 (1971) Abdel Rida Al Khor, L.D.Blokhintsev, I.A.Schwarz The Polar Mechanism for the 3He(n, p)3H and 2H(d, p)3H Reactions NUCLEAR REACTIONS 3He(n, p), 2H(d, p), E=14.4 MeV, Ed=6.1, 13.8 MeV; calculated σ(θ). Feynman diagram formalism, pole diagrams.
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