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Search: Author = Y.K.Agarwal

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2004MA14      Nucl.Phys. A731, 146 (2004)

I.Mazumdar, Y.K.Agarwal, D.A.Gothe, U.Kadhane

Phase space selected GDR gamma rays from hot rotating 194Au

NUCLEAR REACTIONS Ta(13C, X), E=65, 84 MeV; Ta(12C, X), E=75 MeV; measured Eγ, Iγ(θ) from compound nucleus decay. 194Au deduced GDR parameters.

doi: 10.1016/j.nuclphysa.2003.11.027
Citations: PlumX Metrics

1999CH24      Phys.Rev. C60, 024606 (1999)

D.R.Chakrabarty, V.M.Datar, Y.K.Agarwal, C.V.K.Baba, M.S.Samant, I.Mazumdar, A.K.Sinha, P.Sugathan

Hard Photon Production in p + 197Au Reaction at Ep = 27 MeV

NUCLEAR REACTIONS 197Au(p, γ), E=27 MeV; measured Eγ, Iγ, σ(θ). 198Hg deduced single-particle levels, resonance widths. 12C(p, p'γ), E=27 MeV; measured Eγ, Iγ. NaI, BaF2 detectors.

doi: 10.1103/PhysRevC.60.024606
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1997KA48      Phys.Rev. C56, 1902 (1997)

D.O.Kataria, A.K.Sinha, J.J.Das, N.Madhavan, P.Sugathan, L.T.Baby, I.Mazumdar, R.Singh, C.V.K.Baba, Y.K.Agarwal, A.M.Vinodkumar, K.M.Varier

One- and Two-Nucleon Transfer in the 28Si + 68Zn System at Energies Below the Coulomb Barrier

NUCLEAR REACTIONS, ICPND 68Zn(28Si, 29Si), (28Si, 30Si), (28Si, 27Al), (28Si, 26Mg), E=65-83 MeV; measured target-like fragment mass, E, yield; deduced two-nucleon transfer related features. 68Zn(28Si, X), E=50-70 MeV; calculated fusion σ(E). 28Si, 68Zn levels deduced β2, β3. Recoil mass separator. Semiclassical theory, coupled-channels calculations.

doi: 10.1103/PhysRevC.56.1902
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1996CH13      Phys.Rev. C53, 2739 (1996)

D.R.Chakrabarty, V.M.Datar, R.K.Choudhury, B.K.Nayak, Y.K.Agarwal, C.V.K.Baba, M.K.Sharan

Study of Nuclear Shapes in Tl Isotopes Via Excited State Giant Dipole Resonance Studies in the Reaction 16O + 181Ta

NUCLEAR REACTIONS 181Ta(16O, X), E=84-107 MeV; measured Eγ, Iγ, γ-anisotropy; deduced Tl isotopes shape features, GDR parameters.

doi: 10.1103/PhysRevC.53.2739
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1996SA19      Nucl.Phys. A601, 251 (1996)

S.Saha, Y.K.Agarwal

Experimental Investigation on the Connection between Nucleon Transfer Channels and Near-Barrier Fusion in 32S + 64Ni and 28Si + 68Zn Systems

NUCLEAR REACTIONS 64Ni(32S, 31P), (32S, 30Si), 68Zn(28Si, 27Al), (28Si, 26Mg), E=80-120 MeV; measured (particle)γ-coin; deduced transfer probabilities for ground state, coupling strengths. Coupled channel fusion calculation, semi-classical theory.

doi: 10.1016/0375-9474(96)00038-3
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1994SA14      Phys.Rev. C49, 2578 (1994)

S.Saha, Y.K.Agarwal, C.V.K.Baba

One- and Two-Proton Transfer Reactions in 32S + 64Ni and 28Si + 68Zn at Near-Barrier Energies

NUCLEAR REACTIONS 64Ni(32S, X), 68Zn(28Si, X), E=80-115 MeV; measured (fragment)γ-coin, σ(fragment, θ); deduced one-, two-proton stripping probabilities vs distance of closest approach.

doi: 10.1103/PhysRevC.49.2578
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1993CH03      Phys.Rev. C47, R1 (1993)

S.Chattopadhyay, H.C.Jain, J.A.Sheikh, Y.K.Agarwal, M.L.Jhingan

Rotational Structure and Signature Inversion in Odd-Odd 84Y

NUCLEAR REACTIONS 59Co(28Si, n2p), E=98 MeV; measured γγ-coin. 84Y deduced levels, J, π, band structure, B(λ). Particle-rotor model.

doi: 10.1103/PhysRevC.47.R1
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1993SA42      Nucl.Instrum.Methods Phys.Res. A335, 165 (1993)

S.Saha, Y.K.Agarwal, M.D.Deshpande, A.Roy

A Method to Study Heavy Ion Reactions using Position Sensitive and Bragg Curve Spectroscopy Detectors

NUCLEAR REACTIONS 68Zn(28Si, X), E=115 MeV; measured γγ-coin. Position sensitive parallel grid avalanche counter, large area Bragg curve spectroscopy detector.

doi: 10.1016/0168-9002(93)90269-N
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1993SH28      Phys.Rev. C48, 2845 (1993)

M.K.Sharan, Y.K.Agarwal, C.V.K.Baba, D.R.Chakrabarty, V.M.Datar

Ultradipole Photon Production in 40 and 50 MeV α-Nucleus Collisions

NUCLEAR REACTIONS, ICPND 159Tb, 197Au(α, X), E=40 MeV; 197Au, 116Sn, Ag, 59Co(α, X), E=50 MeV; measured γ yields, γ(θ), σ(Eγ, θ); deduced nonstatistical component production mechanism. Statistical model, potential, incoherent nucleon-nucleon bremsstrahlung processes.

doi: 10.1103/PhysRevC.48.2845
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1992DA04      Nucl.Phys. A539, 351 (1992)

M.Dasgupta, A.Navin, Y.K.Agarwal, C.V.K.Baba, H.C.Jain, M.L.Jhingan, A.Roy

Fusion of 28Si + 68Zn, 32S + 64Ni, 37Cl + 59Co and 45Sc + 51V in the Vicintiy of the Coulomb Barrier

NUCLEAR REACTIONS 68Zn(28Si, X), E=50.7-70.7 MeV; 64Ni(32S, X), E=52.4-73.1 MeV; 59Co(37Cl, X), E=55.4-70.6 MeV; 51V(45Sc, X), E=58.3-71.1 MeV; measured evaporation residue σ; deduced fusion σ, average angular momentum. Enriched targets.

doi: 10.1016/0375-9474(92)90274-N
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6113.

1992DA11      Pramana 38, 291 (1992)

M.Dasgupta, A.Navin, Y.K.Agarwal, C.V.K.Baba, H.C.Jain, M.L.Jhingan, A.Roy

Yields of Evaporation Residues and Average Angular Momentum in Heavy Ion Induced Fusion Reactions Leading to Compound Nucleus 96Ru

NUCLEAR REACTIONS 68Zn(28Si, X), E=70-100 MeV;; 64Ni(32S, X), E=78-100 MeV; 59Co(37Cl, X), E=88-115 MeV; 51V(45Sc, X), E=110-134 MeV; measured evaporation residue production σ for X=90-93 from γ yields. Statistical model analyses.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6247.

1991DA09      Phys.Rev.Lett. 66, 1414 (1991)

M.Dasgupta, A.Navin, Y.K.Agarwal, C.V.K.Baba, H.C.Jain, M.L.Jhingan, A.Roy

Consistency of Angular Momentum and Cross Section in Near-Barrier Fusion of 28Si + 68Zn, 32S + 64Ni, and 37Cl + 59Co

NUCLEAR REACTIONS, ICPND 68Zn(28Si, X), 64Ni(32S, X), 59Co(37Cl, X), E(cm) ≈ 50-70 MeV; measured partial σ(E), evaporation following fusion; deduced <l>.

doi: 10.1103/PhysRevLett.66.1414
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6141.

1991JA11      Pramana 37, 269 (1991)

H.C.Jain, S.Chattopadhyay, Y.K.Agarwal, M.L.Jhingan, S.K.Mitra, H.V.Panchal, A.Roy

A Plunger Set-Up for Measuring Picosecond Nuclear Half-Lives

NUCLEAR REACTIONS 27Al(16O, xnypzα), E=60 MeV; measured Eγ, Iγ, recoil distance. 35Cl, 37,38Ar, 40K levels deduced T1/2. Plunger technique.

doi: 10.1007/BF02847481
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1991ME06      Z.Phys. A339, 317 (1991)

D.Mehta, Y.K.Agarwal, K.P.Blume, S.Heppner, H.Hubel, M.Murzel, K.Theine, W.Gast, G.Hebbinghaus, R.M.Lieder, W.Urban

Spectroscopy of 195Hg and 196Hg

NUCLEAR REACTIONS 198Pt(α, xn), E=78 MeV; measured γγ-coin, Eγ, Iγ, DCO ratios. 195,196Hg deduced levels, J, π, band structure.

doi: 10.1007/BF01560632
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1990AG07      Pramana 35, 49 (1990)

Y.K.Agarwal, C.V.K.Baba, D.R.Chakrabarty, V.M.Datar, D.A.Gothe, H.C.Jain, A.Roy, M.K.Sharan

A Multi NaI(Tl) Detector Array for Medium Energy γ-Ray Spectroscopy

NUCLEAR REACTIONS 197Au(α, X), E=50 MeV; Ta(16O, X), E=85 MeV; measured γ-spectra. Hexagonal NaI(Tl) detector array, tof, pile up.

doi: 10.1007/BF02846641
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1986HE28      J.Less-Common Met. 122, 445 (1986)

F.P.Hessberger, G.Munzenberg, S.Hofmann, P.Armbruster, Y.K.Agarwal, W.Reisdorf, K.Poppensieker, K.-H.Schmidt, J.R.H.Schneider, W.F.W.Schneider, H.J.Schott, C.-C.Sahm, D.Vermeulen, B.Thuma

Experiments on the Synthesis of Neutron-Deficient Isotopes with Atomic Numbers in the Region from Z = 102 to Z = 105

RADIOACTIVITY 258,257Db, 256,255Rf, 254,253Lr(α) [from 206,208Pb(48Ca, xn), E ≈ 15-30 MeV/nucleon; 207,208Pb, 209Bi(50Ti, xn), E=20-35 MeV/nucleon]; measured Eα, T1/2. 256,255Rf(SF); measured total kinetic energy release.

NUCLEAR REACTIONS 206,208Pb(48Ca, xn), E ≈ 15-30 MeV/nucleon; 207,208Pb, 209Bi(50Ti, xn)258Db/257Db/255Rf/256Rf/254Lr/253Lr, E ≈ 20-35 MeV/nucleon; measured evaporation residue, Z=104, 105, Lr isotope production σ(E).

doi: 10.1016/0022-5088(86)90440-6
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1986SC18      Phys.Lett. 174B, 241 (1986)

P.Schuler, Ch.Lauterbach, Y.K.Agarwal, J.De Boer, K.P.Blume, P.A.Butler, K.Euler, Ch.Fleischmann, C.Gunther, E.Hauber, H.J.Maier, M.Marten-Tolle, Ch.Schandera, R.S.Simon, R.Tolle, P.Zeyen

High-Spin States in 224,226,228Th and the Systematics of Octupole Effects in Even Th Isotopes

NUCLEAR REACTIONS 226Ra(α, 4n), (α, 2n), E=42 MeV; 226Ra(α, 6n), E=55 MeV; measured Eγ, Iγ, I(ce), γγ-coin, (ce)(ce)-coin. 220,222,230Th deduced B(E1)/B(E2) ratios, induced electric dipole to quadrupole moment ratio. 224,226,228Th deduced levels, J, π, γ-branching, B(E1)/B(E2) ratios, induced electric dipole to quadrupole moment ratio. Other data input.

doi: 10.1016/0370-2693(86)91091-9
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1985AG01      Z.Phys. A320, 295 (1985)

Y.K.Agarwal, C.Gunther, K.Hardt, P.Schuler, J.Stachel, H.J.Wollersheim, H.Emling, E.Grosse, R.Kulessa, W.Spreng

Multiple Coulomb Excitation of 202Hg and 204Hg

NUCLEAR REACTIONS 202,204Hg(208Pb, 208Pb'), E=5 MeV/nucleon; measured Eγ, Iγ, γ yields following Coulomb excitation. 202,204Hg deduced levels, relative γ yield, B(E2).

doi: 10.1007/BF01881278
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1985AR02      Phys.Rev.Lett. 54, 406 (1985)

P.Armbruster, Y.K.Agarwal, W.Bruchle, M.Brugger, J.P.Dufour, H.Gaggeler, F.P.Hessberger, S.Hofmann, P.Lemmertz, G.Munzenberg, K.Poppensieker, W.Reisdorf, M.Schadel, K.-H.Schmidt, J.H.R.Schneider, W.F.W.Schneider, K.Summerer, D.Vermeulen, G.Wirth, A.Ghiorso, K.E.Gregorich, D.Lee, M.Leino, K.J.Moody, G.T.Seaborg, R.B.Welch, P.Wilmarth, S.Yashita, C.Frink, N.Greulich, G.Herrmann, U.Hickmann, N.Hildebrand, J.V.Kratz, N.Trautmann, M.M.Fowler, D.C.Hoffman, W.R.Daniels, H.R.von Gunten, H.Dornhofer

Attempts to Produce Superheavy Elements by Fusion of 48Ca with 248Cm in the Bombarding Energy Range of 4.5-5.2 MeV/u

NUCLEAR REACTIONS 248Cm(48Ca, X), E=4.5-5.2 MeV/nucleon; measured superheavy production σ upper limits vs T1/2. Different separation techniques.

doi: 10.1103/PhysRevLett.54.406
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1985DE14      Nucl.Phys. A436, 311 (1985)

D.J.Decman, H.Grawe, H.Kluge, K.H.Maier, A.Maj, N.Roy, Y.K.Agarwal, K.P.Blume, M.Guttormsen, H.Hubel, J.Recht

Decay of the Ground State and the (29/2)+ Isomer in 217Ac and g-Factor Measurements from Perturbed α-Particle Angular Distributions

NUCLEAR REACTIONS 205Tl(16O, 4n), E=96 MeV; 206Pb(15N, 4n), E=80, 84, 87 MeV; 209Bi(12C, 4n), E=75 MeV; measured αγ-, γγ-, α(ce)-, (ce)(ce)-coin, α(θ, H, t), γ(θ, H, T). 217Ac deduced levels, J, π, T1/2, g, γ multipolarity, γ-branching, γα. Shell model.

doi: 10.1016/0375-9474(85)90201-5
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1985HE22      Z.Phys. A322, 557 (1985)

F.P.Hessberger, G.Munzenberg, S.Hofmann, Y.K.Agarwal, K.Poppensieker, W.Reisdorf, K.-H.Schmidt, J.R.H.Schneider, W.F.W.Schneider, H.J.Schott, P.Armbruster, B.Thuma, C.-C.Sahm, D.Vermeulen

The New Isotopes 258105, 257105, 254Lr and 253Lr

RADIOACTIVITY 258Db, 257Db, 253,254Lr(α) [from 209Bi(50Ti, X), E=4.65-4.95 MeV/nucleon]; measured Eα, Iα, T1/2. 258Rf(SF) [from 258Db(EC-decay)]; measured T1/2, fission fragment total kinetic energy.

NUCLEAR REACTIONS 209Bi(50Ti, X), E=4.65-4.95 MeV/nucleon; measured Eα, Iα, evaporation residue σ(E) for one-, two-neutron emission; deduced evidence for 258Db, 257Db, 253,254Lr.

1985HO29      Nucl.Phys. A447, 335c (1985)

S.Hofmann, P.Armbruster, G.Munzenberg, W.Reisdorf, K.-H.Schmidt, H.G.Burkhard, F.P.Hessberger, H.-J.Schott, Y.K.Agarwal, G.Berthes, U.Gollerthan, H.Folger, R.Hingmann, J.G.Keller, M.E.Leino, P.Lemmertz, M.Montoya, K.Poppensieker, B.Quint, I.Zychor

The Influence of the Surprising Decay Properties of Element 108 on Search Experiments for New Elements

RADIOACTIVITY 260Sg(α) [from 208Pb(54Cr, 2n), E=4.92 MeV/nucleon]; measured T1/2; deduced SF(T1/2) limit, branching ratio. 256Rf(SF) [from 260Sg(α-decay)]; measured T1/2. 260Sg, 256Rf deduced mass excess.

doi: 10.1016/0375-9474(86)90615-9
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1985RE06      Nucl.Phys. A440, 366 (1985)

J.Recht, Y.K.Agarwal, K.P.Blume, M.Guttormsen, H.Hubel, H.Kluge, K.H.Maier, A.Maj, N.Roy, D.J.Decman, J.Dudek, W.Nazarewicz

High-Spin Structure in 169W and 170W

NUCLEAR REACTIONS 154Gd(20Ne, xn), E=105-125 MeV; measured E(γ), I(γ), γγ-coin, γ(θ), linear polarization. 169,170W deduced levels, J, π. Ge, Ge(Li), NaI detectors, Bismuth germanate anti-Compton shield, enriched targets. Pairing self-consistent cranking calculations, particle number projections.

doi: 10.1016/0375-9474(85)90345-8
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1984GU29      Nucl.Instrum.Methods 227, 489 (1984)

M.Guttormsen, H.Hubel, A.v.Grumbkow, Y.K.Agarwal, J.Recht, K.H.Maier, H.Kluge, A.Maj, M.Menningen, N.Roy

A Superconducting Electron Spectrometer

NUCLEAR REACTIONS 194Pt(α, 4n), E not given; measured (ce)(ce)-coin. Superconducting electron spectrometer.

RADIOACTIVITY 213Ra(α), (β+), (EC) [from 204Pb(13C, 4n)]; measured (ce)(X-ray)-coin. 217Ac(α) [from 209Bi(12C, 4n)]; measured (ce)α-coin. Superconducting electron spectrometer.

doi: 10.1016/0168-9002(84)90206-7
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1984KE03      Phys.Rev. C29, 1569 (1984)

J.G.Keller, K.-H.Schmidt, H.Stelzer, W.Reisdorf, Y.K.Agarwal, F.P.Hessberger, G.Munzenberg, H.-G.Clerc, C.-C.Sahm

Fusion of the System 90Zr + 90Zr

NUCLEAR REACTIONS, ICPND 90Zr(90Zr, X), E(cm) ≈ 172-195 MeV; measured compound residue σ(E); deduced fusion barrier, fluctuations.

doi: 10.1103/PhysRevC.29.1569
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1984MU07      Z.Phys. A315, 145 (1984)

G.Munzenberg, W.Reisdorf, S.Hofmann, Y.K.Agarwal, F.P.Hessberger, K.Poppensieker, J.R.H.Schneider, W.F.W.Schneider, K.-H.Schmidt, H.-J.Schott, P.Armbruster, C.-C.Sahm, D.Vermeulen

Evidence for Element 109 from One Correlated Decay Sequence following the Fusion of 58Fe with 209Bi

RADIOACTIVITY 266Mt(SF) [from 209Bi(58Fe, X), E=5.15 MeV/nucleon]; measured Eα, Iα, αα-coin, SF-decay.

NUCLEAR REACTIONS 209Bi(58Fe, X), E=4.95, 5.05, 5.15 MeV/nucleon; measured σ(fragment) vs mass, Eα, Iα, SF-decay; deduced evidence for compound nucleus 266Mt.

1983AG01      Nucl.Phys. A399, 199 (1983)

Y.K.Agarwal, J.Recht, H.Hubel, M.Guttormsen, D.J.Decman, H.Kluge, K.H.Maier, J.Dudek, W.Nazarewicz

High-Spin Rotational Bands and Pairing Reduction in 166Hf

NUCLEAR REACTIONS 150Sm(20Ne, 4n), E=105 MeV; measured Eγ, Iγ, γγ(θ), γγ-coin. 166Hf deduced levels, J, π. Cranking model.

doi: 10.1016/0375-9474(83)90603-6
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1983GU05      Nucl.Phys. A398, 119 (1983)

M.Guttormsen, A.V.Grumbkow, Y.K.Agarwal, K.P.Blume, K.Hardt, H.Hubel, J.Recht, P.Schuler, H.Kluge, K.H.Maier, A.Maj, N.Roy

The (νi213/2)(8+, 10+, 12+) Triplets in 190-196Hg

NUCLEAR REACTIONS 181Ta(14N, 5n), E=100 MeV; 192,194,196Pt(α, 4n), E=50 MeV; measured (ce)(ce)(t). 190,192,194,196Hg deduced levels, J, π, M1/E2 mixing, γ-multipolarity, B(E2). Superconducting solenoid, Si(Li) detectors.

doi: 10.1016/0375-9474(83)90651-6
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1983GU12      Z.Phys. A312, 155 (1983)

M.Guttormsen, K.P.Blume, Y.K.Agarwal, A.v.Grumbkow, K.Hardt, H.Hubel, J.Recht, P.Schuler

Rotation Aligned Bands and Configuration Dependent Interaction in 189Hg

NUCLEAR REACTIONS 181Ta(14N, 6n), E=100 MeV: measured Eγ, Iγ, (ce)(ce)-, γγ-coin, γ(θ). 189Hg deduced levels, J, π. Ge(Li), NaI, Si-Li detectors.

doi: 10.1007/BF01412158
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1983HA15      Z.Phys. A312, 251 (1983)

K.Hardt, Y.K.Agarwal, C.Gunther, M.Guttormsen, R.Kroth, J.Recht, F.A.Beck, T.Byrski, J.C.Merdinger, A.Nourredine, D.C.Radford, J.P.Vivien, C.Bourgeois

Observation of the Weakly Deformed νi213/2 Band in 188Hg

NUCLEAR REACTIONS 168Er(24Mg, 4n), E=125 MeV; measured Eγ, Iγ, γγ-coin. 188Hg deduced levels, J, π, rotation aligned band structure, isomer T1/2, γ-branching, B(E2), configuration.

doi: 10.1007/BF01412168
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1983HU15      Z.Phys. A314, 89 (1983)

H.Hubel, M.Guttormsen, K.P.Blume, J.Recht, A.von Grumbkow, K.Hardt, P.Schuler, Y.K.Agarwal, A.Maj

Isomeric Transitions in 203Bi and 205Bi

NUCLEAR REACTIONS 203,205Tl(α, 4n), E=50 MeV; measured Eγ, Iγ, γ(θ), (ce)(ce)(t). 203,205Bi deduced levels, J, π, B(Eλ), T1/2. Electron spectrometers, Si(Li)-, Ge-detectors.

1983KE01      Z.Phys. A311, 243 (1983)

J.G.Keller, H.-G.Clerc, K.-H.Schmidt, Y.K.Agarwal, F.P.Hessberger, R.Hingmann, G.Munzenberg, W.Reisdorf, C.C.Sahm

Observation of Radiative Capture in the Reaction 90Zr + 90Zr

NUCLEAR REACTIONS 90Zr(90Zr, X), E=351, 360 MeV; measured Eα, Iα following evaporation residue decay; deduced heavy system radiative capture.

doi: 10.1007/BF01415109
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1983RE03      Phys.Lett. 122B, 207 (1983)

J.Recht, Y.K.Agarwal, M.Guttormsen, H.Hubel, D.J.Decman, H.Kluge, K.H.Maier, N.Roy, J.Dudek, W.Nazarewicz

Delayed Second Band Crossing in 170W

NUCLEAR REACTIONS 150Gd(20Ne, 4n), E=105, 110, 120 MeV; measured γγ-coin, I(ce), Eγ, Iγ. 170W deduced levels, J, π, γ-branching, band structure, γ-multipolarity, kinematic moment of inertia.

doi: 10.1016/0370-2693(83)90685-8
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1982GU10      Nucl.Phys. A383, 541 (1982)

M.Guttormsen, Y.K.Agarwal, C.Gunther, K.Hardt, H.Hubel, A.Kalbus, R.Kroth, G.Mikus, J.Recht, P.Schuler

Band Crossings in Weakly Deformed 190Hg

NUCLEAR REACTIONS 181Ta(14N, 5n), E=100 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 190Hg deduced levels, J, π, Natural targets, Ge(Li), NaI detectors. Cranking model calculations.

doi: 10.1016/0375-9474(82)90090-2
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1976LA10      Pramana 6, 209 (1976)

B.Lal, Y.K.Agarwal, C.V.K.Baba, S.M.Bharathi, S.K.Bhattacherjee

Levels in 74As from the 74Ge(p, nγe)74As Reaction

NUCLEAR REACTIONS 74Ge(p, nγ), E=3.5-5.0 MeV; measured σ(E, Eγ), γγ-coin, I(ce), γce(t), nce(t). 74As deduced levels, J, π, ICC, T1/2, λ, γ-branching.

doi: 10.1007/BF02875212
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1975BH02      Pramana 4, 25 (1975)

S.M.Bharathi, Y.K.Agarwal, B.Lal, C.V.K.Baba, M.G.Betigeri, N.G.Puttaswamy

Rotational Bands in 79Kr

NUCLEAR REACTIONS 79Br(p, nγ), E=1.7-5.0 MeV; measured Eγ, Iγ, I(ce), σ(E, Eγ, θ), γγ-γce-coin. 79Kr deduced levels, J, π, ICC, β, γ-branching.

doi: 10.1007/BF02852262
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1974AG03      Phys.Lett. 47A, 161 (1974)

Y.K.Agarwal, H.Bertschat, H.Haas, F.Pleiter, E.Recknagel, E.Schlodder, B.Spellmeyer

Magnetic Hyperfine Field for Zinc in Iron

NUCLEAR REACTIONS 64Ni(α, nγ); measured σ(Eγ, θ, H, t). 67Zn deduced hyperfine field in Fe.

doi: 10.1016/0375-9601(74)90393-4
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1974AG05      Pramana 3, 243 (1974)

Y.K.Agarwal, C.V.K.Baba, S.M.Bharathi, S.K.Bhattacherjee, B.Lal, B.Sahai

In-Beam Gamma-Ray and Electron Spectroscopy Following the 75As(p, n)75Se Reaction

NUCLEAR REACTIONS 75As(p, nγ), E=1.5-5.0 MeV; measured Eγ, Iγ, I(ce), γγ-, γce-coin, γ(θ), γ(t); deduced ICC. 75Se deduced levels, J, π, T1/2, B(λ).

doi: 10.1007/BF02872243
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1971AG04      Nucl.Phys. A176, 142 (1971)

Y.K.Agarwal, S.Hofmann, K.Wien

Untersuchung des Zerfalls von 56Co durch γγ-Winkelkorrelationsmessungen

RADIOACTIVITY 56Co[from 56Fe(p, n)]; measured γγ(θ). 56Fe levels deduced J, γ-mixing. Ge(Li), NaI(Tl) detectors.

doi: 10.1016/0375-9474(71)90736-6
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1969AG01      Nucl.Phys. A127, 652 (1969)

Y.K.Agarwal, C.V.K.Baba, S.K.Mitra

Nuclear Matrix Elements in the 2.14 MeV Beta Group in 139Ba

RADIOACTIVITY 139Ba [from 138Ba(n, γ)]; measured β-spectrum shape factor, βγ(θ); deduced β-decay matrix elements.

doi: 10.1016/0375-9474(69)91036-7
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1969AG02      Nucl.Phys. A127, 661 (1969)

Y.K.Agarwal, C.V.K.Baba, N.C.Mukhopadhyay

Particle Parameters for Conversion Electrons in 152Sm, 152Gd and 160Dy

RADIOACTIVITY 152Eu [from 151Eu(n, γ)]; 160Tb [from 159Tb(n, γ)]; measured γγ(θ), ceγ(θ). 152Sm, 152Gd, 160Dy deduced conversion electron particle parameters.

doi: 10.1016/0375-9474(69)91037-9
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1969IN07      Phys.Rev. 188, 605 (1969)

P.Inia, Y.K.Agarwal, H.de Waard

Hyperfine Fields of Technetium and Zinc Impurities in Iron

RADIOACTIVITY 99Mo, 67Ga; measured γγ(θ, H) in Fe; deduced hyperfine fields. 99Tc, 67Zn levels deduced g.

doi: 10.1103/PhysRev.188.605
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1967AG03      Nucl.Phys. A99, 457 (1967); Y.K.Agarwal - Priv.Comm. (April 1972)

Y.K.Agarwal, C.V.K.Baba, S.K.Bhattacherjee

Properties of Low-Lying Levels in 59Co

RADIOACTIVITY 59Fe; measured βγ-delay γγ(θ, H) 59Co level deduced T1/2, g, μ(1290 keV).

doi: 10.1016/0375-9474(67)90943-8
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1966AG01      Proc.Nucl.Phys. and Solid State Phys.Symp., Nucl.Phys., Bombay, p.181 (1966); CONF-660221; Y.K.Agarwal - Priv.Comm. (April 1972)

Y.K.Agarwal, C.V.K.Baba

Magnetic Moment of the 280 keV (5/2-) Level in As75

NUCLEAR STRUCTURE 75Se; measured not abstracted; deduced nuclear properties.

1966AG02      Nucl.Phys. 79, 437 (1966); Y.K.Agarwal - Priv.Comm. (April 1972)

Y.K.Agarwal, C.V.K.Baba, S.K.Bhattacherjee

Measurement of the g-Factors of 2+ States in Even Nuclei Utilizing Hyperfine Fields in Iron Lattice (I). The 316 keV State in 192Pt and 328 and 622 keV States in 194Pt

RADIOACTIVITY 192Ir, 194Ir; measured γγ(θ, H). 192Pt[316 keV state], 194Pt [328, 622 keV states] deduced g.

doi: 10.1016/0029-5582(66)90156-8
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1966HA15      Nucl.Phys. 76, 257 (1966)

P.G.Hansen, H.L.Nielsen, K.Wilsky, Y.K.Agarwal, C.V.K.Baba, S.K.Bhattacherjee

Spectral Shapes and a Beta-Gamma Directional Correlation in the Beta Decay of 172Tm (Jπ=2-)

RADIOACTIVITY 172Tm [from n-capture in 170Er, chem]; measured Eβ, Iβ, βγ-coin, shape factors, βγ-coin(θ); deduced log f1t'S, multipolarity of β. Enriched target.

doi: 10.1016/0029-5582(66)90022-8
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1965AG01      Nucl.Phys. 63, 685 (1965); Y.K.Agarwal - Priv.Comm. (April 1972)

Y.K.Agarwal, C.V.K.Baba, S.K.Bhattacherjee

Magnetic Moment of the 160 keV State in Cs133

RADIOACTIVITY 133Ba; measured γγ(θ, H). 133Cs [160 keV level] deduced J, g, μ.

doi: 10.1016/0029-5582(65)90755-8
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1965AG02      Phys.Letters 14, 214 (1965); Y.K.Agarwal - Priv.Comm. (April 1972)

Y.K.Agarwal, C.V.K.Baba, S.K.Bhattacherjee

Magnetic Properties of K = 1/2 Rotational Band in Tm171

NUCLEAR STRUCTURE 171Er; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)90595-0
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1965AG03      Phys.Letters 19, 578 (1965)

Y.K.Agarwal, C.V.K.Baba, S.K.Bhattacherjee, D.C.Ephraim

Magnetic Moment of the 405 keV (7/2-) Level in 211Bi

NUCLEAR STRUCTURE 211Bi, 211Pb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)90784-5
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1964AG01      Nucl. Phys. 58, 641 (1964)

Y.K.Agarwal, C.V.K.Baba, S.K.Bhattacherjee

Levels in La140 from the Beta Decay of Ba140

RADIOACTIVITY 140Ba [fission product]; measured Eγ, Iγ, βγ(θ), γγ(θ). 140La deduced levels, J, π, delta(E2/M1).

doi: 10.1016/0029-5582(64)90574-7
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1964AG02      Nucl.Phys. 58, 651 (1964); Y.K.Agarwal - Priv.Comm. (April 1972)

Y.K.Agarwal, C.V.K.Baba, S.K.Bhattacherjee

Measurement of Magnetic Moments of Excited States in Ta181 and Cs133

RADIOACTIVITY 133Ba, 181Hf; measured γγ(θ, H). 133Cs, 181Ta deduced μ, g.

doi: 10.1016/0029-5582(64)90575-9
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