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NSR database version of May 24, 2024.

Search: Author = B.S.Sandhu

Found 9 matches.

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2020KA20      Phys.Rev. C 101, 034614 (2020)

R.Kaur, S.Kaur, B.B.Singh, B.S.Sandhu, S.K.Patra

Clustering effects in the exit channels of 13, 12C + 12C reactions within the collective clusterization mechanism of the dynamical cluster decay model

NUCLEAR REACTIONS 12C(12C, X)24Mg*, (12C, 6Li), (12C, 7Li), (12C, 7Be), (12C, 8Be), (12C, 9Be), (12C, X)25Mg*, (13C, 6Li), (13C, 7Li), (13C, 7Be), (13C, 8Be), (13C, 9Be), E*=53.9 MeV; calculated fragmentation potential, fragment preformation probability, l-summed preformation probability, scattering potential, barrier potential, penetration probability, and σ(25Mg*)/σ(24Mg*). Dynamical cluster decay model (DCM). Comparison with experimental data, and with other theoretical predictions. Discussed role of α-clustering in heavy-ion reactions.

doi: 10.1103/PhysRevC.101.034614
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2020KA26      Phys.Rev. C 101, 044605 (2020)

R.Kaur, M.Kaur, V.Singh, M.Kaur, B.B.Singh, B.S.Sandhu

Dynamical aspects od 48Ti + 58Fe, 58Ni → 106Cd*, 106Sn reactions at energies near the Coulomb barrier

NUCLEAR REACTIONS 58Fe(48Ti, X)106Cd*,58Ni(48Ti, X)106Sn*, E=118.06-165.8 MeV; calculated fragmentation and scattering potentials, barrier lowering and neck-length parameters, preformation probabilities, σ(E) as function of light and heavy fragments of the compound nuclei. Dynamical cluster decay model (DCM).

doi: 10.1103/PhysRevC.101.044605
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2018KA53      Phys.Rev. C 98, 064612 (2018)

R.Kaur, M.Kaur, V.Singh, S.Kaur, B.B.Singh, B.S.Sandhu

Investigating the fusion enhancement for neutron-rich mid-mass nuclei using the dynamical cluster-decay model

NUCLEAR REACTIONS 28Si(39K, X)67As*,28Si(40K, X)68As*,28Si(41K, X)69As*,28Si(45K, X)73As*,28Si(46K, X)74As*,28Si(47K, X)75As*, E(cm)=36.8-42.6 MeV; calculated fragment potentials and l-summed preformation probability as a function of fragment mass number, scattering potentials for the compound nuclei decaying through one-proton and one-neutron channels, barrier lowering as function of incident energy, summed penetration probabilities, fusion σ(E), -summed fragment cross sections using dynamical cluster-decay model (DCM). Comparison with available experimental data.

doi: 10.1103/PhysRevC.98.064612
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2007SI12      Radiat.Meas. 42, 420 (2007)

M.Singh, G.Singh, B.S.Sandhu, B.Singh

Angular distribution of 662 keV multiply-Compton scattered gamma rays in copper

NUCLEAR REACTIONS Cu(γ, γ'), E=662 keV; measured angular distribution and saturation depth in copper of multiply-Compton scattered γ rays.

doi: 10.1016/j.radmeas.2007.01.037
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2005DE19      Ann.Nucl.Energy 32, 1008 (2005)

R.Dewan, M.B.Saddi, B.S.Sandhu, B.Singh, B.S.Ghumman

Collision, scattering and absorption differential cross-sections in double-photon Compton scattering

NUCLEAR REACTIONS Al(γ, γ), E=662 keV; measured Eγ, γγ-coin, σ(E, θ) for double-photon Compton scattering.

doi: 10.1016/j.anucene.2005.02.001
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2004SH40      Nucl.Sci.Eng. 148, 445 (2004)

A.Sharma, M.B.Saddi, B.Singh, B.S.Sandhu

Collision Integral Cross Sections in Double Photon Compton Scattering and a Possible Method for Their Measurement

doi: 10.13182/NSE04-A2470
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2002DE22      Nucl.Sci.Eng. 141, 165 (2002)

R.Dewan, M.B.Saddi, B.S.Sandhu, B.Singh, B.S.Ghumman

Experimental Study of Energy Distribution in Double Photon Compton Scattering

NUCLEAR REACTIONS Al(γ, γ'), E=0.662 MeV; measured Eγ, Iγ, γγ-coin. Comparison with theory.

doi: 10.13182/NSE02-A2275
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1993SA40      Appl.Radiat.Isot. 44, 1367 (1993)

B.S.Sandhu, B.Singh, B.S.Ghumman

Experimental Measurement of Intensity Distribution in Two-Photon Compton Scattering

NUCLEAR REACTIONS 27Al(γ, γ), E=0.662 MeV; measured two photon Compton scattering σ(θ1, θ2, φ2); deduced weak process features. Model comparison.

doi: 10.1016/0969-8043(93)90087-Q
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1988SE12      Nuovo Cim. 100A, 789 (1988)

G.S.Sekhon, B.S.Sandhu, B.Singh, B.S.Ghumman

Double-Photon Compton Scattering of 662 keV Gamma-Rays

NUCLEAR REACTIONS 27Al, 45Sc, 137Cs(γ, γ), E=0.662 MeV; measured double photon Compton σ(θ1, θ2).

doi: 10.1007/BF02813325
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