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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 E_p = 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 T_1/2. 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, T_1/2. ^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 T_1/2. 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, T_1/2, 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, T_1/2. ²⁵⁸Rf(SF) [from ²⁵⁸Db(EC-decay)]; measured T_1/2, 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 T_1/2; deduced SF(T_1/2) limit, branching ratio. ²⁵⁶Rf(SF) [from ²⁶⁰Sg(α-decay)]; measured T_1/2. 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 (νi²_13/2)(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). ^{190,192,194,196}Hg 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 νi²_13/2 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 T_1/2, 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), T_1/2. 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, T_1/2, 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, T_1/2, 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 T_1/2, 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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