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NSR database version of April 11, 2024.

Search: Author = P.N.Tandon

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1996PA45      Phys.Rev. A54, 3014 (1996)

H.C.Padhi, B.B.Dhal, V.Nanal, K.G.Prasad, P.N.Tandon, D.Trautmann

L-Subshell Ionization Studies in Au and Bi for 19F and 28Si Large-Ion Bombardment

NUCLEAR REACTIONS 197Au, 209Bi(19F, X), E=30-57 MeV; 197Au, 209Bi(28Si, X), E=36-84 MeV; measured L-subshell X-ray production, subshell ionization σ.

ATOMIC PHYSICS 197Au, 209Bi(19F, X), E=30-57 MeV; 197Au, 209Bi(28Si, X), E=36-84 MeV; measured L-subshell X-ray production, subshell ionization σ.

doi: 10.1103/PhysRevA.54.3014
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1994TR06      Phys.Rev. A49, 1015 (1994)

L.C.Tribedi, K.G.Prasad, P.N.Tandon, Z.Chen, C.D.Lin

Single and Double K-Shell Ionization and Electron-Transfer Cross Sections for Fe and Ni Bombarded by S Ions and Fe by Si Ions at 1.25-4.70 MeV/amu

NUCLEAR REACTIONS Fe, Ni(28Si, X), (32S, X), E=1.25-4.7 MeV/nucleon; measured X-ray spectra; deduced fluorescence yield, single, double K-shell vacancy production σ(E), electron transfer σ.

ATOMIC PHYSICS Fe, Ni(28Si, X), (32S, X), E=1.25-4.7 MeV/nucleon; measured X-ray spectra; deduced fluorescence yield, single, double K-shell vacancy production σ(E), electron transfer σ.

doi: 10.1103/PhysRevA.49.1015
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1993TR05      Phys.Rev. A47, 3739 (1993)

L.C.Tribedi, K.G.Prasad, P.N.Tandon

K-K-Electron Transfer and K-Shell-Vacancy Production Cross Sections for Ti Bombarded by 28Si and 32S Beams at 1.25-4.70 MeV/amu

NUCLEAR REACTIONS Ti(28Si, X), (32S, X), E=1.25-4.7 MeV/nucleon; measured K-shell vacancy production σ; deduced average fluorescence yield. Model comparison.

ATOMIC PHYSICS Ti(28Si, X), (32S, X), E=1.25-4.7 MeV/nucleon; measured K-shell vacancy production σ; deduced average fluorescence yield. Model comparison.

doi: 10.1103/PhysRevA.47.3739
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1993TR14      Z.Phys. D27, 143 (1993)

L.C.Tribedi, K.G.Prasad, P.N.Tandon

Measurement of K-Shell Population of Swift Sulphur Ions Penetrating Fe and Ni Foils Using the Probe Layer Technique

NUCLEAR REACTIONS Fe, Ni(32S, X), E=40-150 MeV; measured S-ion degree of polarization, single, double K-vacancy fractions in Fe, Ni.

ATOMIC PHYSICS Fe, Ni(32S, X), E=40-150 MeV; measured S-ion degree of polarization, single, double K-vacancy fractions in Fe, Ni.

doi: 10.1007/BF01426761
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1992TR06      Phys.Rev. A45, 7860 (1992)

L.C.Tribedi, P.N.Tandon

K-Shell-Ionization Cross Sections for Low-Z Elements (11 ≤ Z ≤ 22) by Protons in the Energy Range 0.5-2.5 MeV

NUCLEAR REACTIONS 23Na, Mg, 27Al, Si, Cl, K, Ca, Ti(p, X), E=0.5-2.5 MeV; Fe, Ni, Cu(p, X), E < 2.5 MeV; measured K-shell ionization σ. Thin targets. Perturbed stationary state approach, Coulomb deflection, energy loss, relativistic corrections.

ATOMIC PHYSICS 23Na, Mg, 27Al, Si, Cl, K, Ca, Ti(p, X), E=0.5-2.5 MeV; Fe, Ni, Cu(p, X), E < 2.5 MeV; measured K-shell ionization σ. Thin targets. Perturbed stationary state approach, Coulomb deflection, energy loss, relativistic corrections.

doi: 10.1103/PhysRevA.45.7860
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1992TR07      Nucl.Instrum.Methods Phys.Res. B69, 178 (1992)

L.C.Tribedi, P.N.Tandon

Efficiency Determination of a Si(Li) X-Ray Detector in the Energy Range 1-20 keV

RADIOACTIVITY 57Co(EC); 54Mn(EC); 241Am(α); measured detector efficiency.

NUCLEAR REACTIONS 23Na, Cl, Mg, 27Al, Si, In, 31P, 41K, Ca, 19F, Ti, Fe, Cu(p, X), E=1 MeV; measured X-ray spectra; deduced detector efficiency. High purity thin targets, Si(Li) X-ray detector.

doi: 10.1016/0168-583X(92)96008-M
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1992TR09      Z.Phys. D24, 215 (1992)

L.C.Tribedi, K.G.Prasad, P.N.Tandon

K-Shell Vacancies at Swift Sulphur Ions in Gd Host

NUCLEAR REACTIONS Gd(32S, X), E=40-150 MeV; measured X-ray spectra, average Ti probe σ; deduced single-, double K-vacancy fractions at S ions in Gd host, polarization transfer mechanism features.

doi: 10.1007/BF01425745
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1989RE08      Phys.Lett. 230B, 16 (1989)

U.Reuter, F.Hagelberg, S.Kremeyer, H.-J.Simonis, K.-H.Speidel, M.Knopp, W.Karle, J.Cub, P.N.Tandon, J.Gerber

Large Transient Magnetic Fields for Single Electron O Ions on a 10 fs Time Scale

NUCLEAR REACTIONS 4He(16O, α), E=44 MeV; measured σ(E(16O)), αγ(θ); deduced O-ion transient magnetic field passing through thin magnetized Gd layers.

doi: 10.1016/0370-2693(89)91645-6
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1989SP02      Phys.Lett. 227B, 16 (1989)

K.-H.Speidel, M.Knopp, W.Karle, M.-L.Dong, J.Cub, U.Reuter, H.-J.Simonis, P.N.Tandon, J.Gerber

Heavy Ion Beam Induced Attenuations of Transient Magnetic Fields

NUCLEAR REACTIONS Ag(28Si, 28Si'), E=130 MeV; Si(62Ni, 62Ni'), E=160 MeV; measured transient magnetic fields, Coulomb excitation ion recoil in Fe(Gd) host; deduced heavy ion beam induced attenuations.

doi: 10.1016/0370-2693(89)91276-8
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1987KN01      Z.Phys. D4, 329 (1987)

M.Knopp, K.-H.Speidel, F.Hagelberg, H.-J.Simonis, P.N.Tandon, J.Gerber

Attenuations and Atomic Spin Precessions of γ-Angular Correlations for Coulomb Excited 19F Nuclei in Single-Electron Ions

NUCLEAR REACTIONS 197Au(19F, 19F'γ), E=75 MeV; measured γγ(θ) following Coulomb excitation, atomic spin precessions. Si, Ge(Li) detectors. Simple electron configurations, statistical model.

doi: 10.1007/BF01384884
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1987KN06      Hyperfine Interactions 34, 183 (1987)

M.Knopp, K.-H.Speidel, F.Hagelberg, H.-J.Simonis, J.Gerber, P.N.Tandon

Experimental Tests for detecting Spin Polarization Pick-Up of Single-Electron 19F-Ions on Emergence from Magnetized Iron

NUCLEAR REACTIONS 197Au(19F, 19F'), E=75 MeV; measured γγ(θ, H) following projectile Coulomb excitation.

doi: 10.1007/BF02072699
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1987MA25      Z.Phys. A327, 157 (1987)

M.Mayr, K.-H.Speidel, M.Knopp, W.Karle, T.Faestermann, F.Hagelberg, H.-J.Simonis, P.N.Tandon, J.Gerber

Measurements of the g-Factor Ratio of the First 3- and 5- States in 40Ca and the Lifetime of the 5- State

NUCLEAR REACTIONS 40Ca(α, α'), E=13.62 MeV; measured Eγ, Iγ, αγ(θ). 40Ca levels deduced g-factor ratio, T1/2.


1987SP06      Z.Phys. D6, 43 (1987)

K.-H.Speidel, M.Knopp, W.Karle, M.Mayr, F.Hagelberg, H.-J.Simonis, J.Gerber, P.N.Tandon

Transient K-Shell Hyperfine Fields and Deduced Polarizations for Single-Electron C and O Ions in Different Ferromagnets

NUCLEAR REACTIONS 4He(12C, α), E=30.6 MeV; 4He(16O, α), E=14.4 MeV; measured Eα, Iα, αγ-coin, αγ(θ) in polarized Ni, Gd hosts; deduced transient K-shell hyperfine fields.

doi: 10.1007/BF01436996
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1986TR08      Nucl.Phys. A458, 95 (1986)

W.Trolenberg, F.Hagelberg, H.J.Simonis, P.N.Tandon, K.-H.Speidel, M.Knopp, J.Gerber

Transient Magnetic Fields at Ne Ions in Fe and Gd Hosts and a Critical Assessment of 20Ne(4+) g-Factor Measurements.

NUCLEAR REACTIONS 20Ne(α, α'), E=14.2 MeV; 12C(12C, α), E=34.7 MeV; measured γ(θ, H); deduced transient magnetic fields at Ne in Fe, Gd hosts. 20Ne level deduced g.

doi: 10.1016/0375-9474(86)90284-8
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1985KN02      Z.Phys. A320, 635 (1985)

M.Knopp, V.Mertens, F.Hagelberg, K.-H.Speidel, J.Gerber, H.Dekhissi, P.N.Tandon

Atomic Spin Precissions of Fluorine Ions Recoiling Through Vaccuum in Weak Transverse Magnetic Fields

NUCLEAR REACTIONS 19F(α, α'), E=5.5 MeV; measured σ(Eα'), γγ-coin, γγ(θ) for recoil in Ag; deduced multi-electron hyperfine interactions.

doi: 10.1007/BF01411864
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1983MI03      Phys.Lett. 94A, 317 (1983)

S.N.Mishra, R.G.Pillay, P.N.Tandon, H.G.Devare

Quadrupole Interactions at 111Cd Nuclei in Light Rare Earths

RADIOACTIVITY 111In(EC); measured γγ(θ, H, t); deduced quadrupole interaction at 111Cd in Pr, Nd hosts.

doi: 10.1016/0375-9601(83)90728-4
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1983MI31      Hyperfine Interactions 15/16, 701 (1983)

S.N.Mishra, R.G.Pillay, P.N.Tandon, H.G.Devare

Quadrupole Interaction at 111Cd in Rare-Earth Intermetallics

RADIOACTIVITY 111In(EC); measured γγ(θ, H, t); deduced 111Cd quadrupole interaction in rare earth intermetallics.

doi: 10.1007/BF02147346
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1982SP02      Nucl.Phys. A378, 130 (1982)

K.-H.Speidel, P.N.Tandon, V.Mertens, W.Trolenberg, G.J.Kumbartzki, N.Ayres de Campos, M.B.Goldberg, J.Gerber, M.Toulemonde

The g-Factor of the Yrast 4+ State in 20Ne from Transient-Field Precession Measurements

NUCLEAR REACTIONS 12C(12C, α), E=32.6, 33.5 MeV; measured σ(Eγ, θ), γ(θ, B), DSA. 20Ne level deduced g, T1/2.

doi: 10.1016/0375-9474(82)90386-4
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1981SP04      Phys.Lett. 102B, 6 (1981)

K.-H.Speidel, G.J.Kumbartzki, W.Knauer, M.Knopp, V.Mertens, P.N.Tandon, J.Gerber, R.M.Freeman

The g-Factor of the First Excited 2+ State in 26Mg from Transient Field Precession Measurements

NUCLEAR REACTIONS 24Mg(α, α'), E=7.08 MeV; 26Mg(α, α'), E=8.01 MeV; measured γ(θ, H) in Fe, αγ(θ); deduced K-shell ion polarization effects. 26Mg level deduced g.

doi: 10.1016/0370-2693(81)90200-8
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1980SP02      Phys.Lett. 92B, 289 (1980)

K.-H.Speidel, G.J.Kumbartzki, W.Knauer, V.Mertens, P.N.Tandon, N.Ayres de Campos, J.Gerber, M.B.Goldberg

The g-Factor of the First Excited 4+ State in Backbending 20Ne

NUCLEAR REACTIONS 12C(12C, α), E=32.6 MeV; measured γγ(θ, H) in Fe, γα-coin. 20Ne level deduced g.

doi: 10.1016/0370-2693(80)90266-X
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1976PA16      Phys.Rev. C14, 2027 (1976)

S.B.Patel, P.N.Tandon, K.P.Gopinathan

g Factor of the 635.4 keV Level in 171Tm

RADIOACTIVITY 171Er [from 170Er(n, γ)]; measured γγ(θ), γγ(θ, H). 171Tm levels deduced g, μ. Enriched target.

doi: 10.1103/PhysRevC.14.2027
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1976PI18      Pramana 7, 190 (1976)

R.G.Pillay, S.H.Devare, P.N.Tandon

The g-Factor of the 659 keV Level in 117In

RADIOACTIVITY 117Cd; measured γγ(θ, H, t). 117In level deduced g, T1/2.

doi: 10.1007/BF02892176
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1975FO06      Phys.Rev. C11, 1976 (1975)

M.Forterre, J.Gerber, J.P.Vivien, M.B.Goldberg, K.-H.Speidel, P.N.Tandon

Transient Field at Nitrogen Nuclei Recoiling in Iron and the Magnetic Moment of the 15N First Excited State

NUCLEAR REACTIONS 13,14C(3He, pγ), E=2-4 MeV; measured pγ-coin, W(θ). 15,16N levels deduced g, transient field. Recoil in magnetized Fe.

doi: 10.1103/PhysRevC.11.1976
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1974CH31      Phys.Rev. C10, 774 (1974)

R.C.Chopra, P.N.Tandon

g Factor of the 632 keV (5/2+) Level in 77As

RADIOACTIVITY 77Ge; measured γγ(θ, H, t). 77As level deduced g.

doi: 10.1103/PhysRevC.10.774
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1974PA03      Phys.Rev. C9, 1515 (1974)

S.B.Patel, A.P.Agnihotry, P.N.Tandon, K.P.Gopinathan

Electromagnetic Properties of the Excited States in 239Pu

RADIOACTIVITY 239Np; measured βγ(t), γγ(t), γγ(θ), γγ(θ, H). 239Pu levels deduced T1/2, γ-mixing, B(M1), B(E2), g.

doi: 10.1103/PhysRevC.9.1515
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1973CH26      Nucl.Phys. A209, 461 (1973)

R.C.Chopra, P.N.Tandon, S.H.Devare, H.G.Devare

Half-Lives of Excited States in 77As, 97Tc and 192Os

RADIOACTIVITY 77Ge [from 76Ge(n, γ)], 97Ru [from 96Ru(n, γ)], 192Ir [from 191Ir(n, γ)]; measured βγ-, γγ-, γ-X delay. Levels in 77As, 97Tc, 192Os; deduced T1/2, B(M1), B(E2).

doi: 10.1016/0375-9474(73)90839-7
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1973CH42      Nucl.Phys. A217, 177 (1973)

R.C.Chopra, P.N.Tandon

The g-Factor of the 264 keV Level in 77As

RADIOACTIVITY 77Ge [from 76Ge(n, γ), natural target]; measured γγ(θ, H). 77As level deduced g.

doi: 10.1016/0375-9474(73)90630-1
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1973CH45      Pramana 1, 70 (1973)

R.C.Chopra, P.N.Tandon

Electromagnetic Properties of Low Lying Levels in 75As

RADIOACTIVITY 75Se; measured γγ(t). 75As levels deduced T1/2, g, B(M1), B(E2).

doi: 10.1007/BF02847180
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1972AV01      Nucl.Phys. A182, 359 (1972)

R.Avida, I.Ben-Zvi, G.Goldring, S.S.Hanna, P.N.Tandon, Y.Wolfson

Magnetic Moment of the First Excited State of 10B

NUCLEAR REACTIONS 9Be(p, γγ), E=1.084 MeV, H= 17.6 kG; measured γγ(θ, H). 10B deduced g-factor 1+ first excited state.

doi: 10.1016/0375-9474(72)90283-7
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1972BE66      Nucl.Phys. A196, 312 (1972)

Z.Berant, R.A.Eisenstein, Y.Horowitz, U.Smilansky, P.N.Tandon, J.S.Greenberg, A.M.Kleinfeld, H.G.Maggi

The Reorientation Effect in 110Cd and 114Cd

NUCLEAR REACTIONS 110,114Cd(α, α'), Eα=8-16 MeV; 110,114Cd(16O, 16O'), E(16O)=36-45 MeV; measured Coulomb excitation probability. 110,114Cd levels deduced B(E2), Q2+. Enriched targets.

doi: 10.1016/0375-9474(72)90967-0
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1972BR17      Phys.Lett. 39B, 185 (1972)

C.Broude, P.Engelstein, M.Popp, P.N.Tandon

Dependence of the Doppler Shift Lifetime Method on Slowing Environment

NUCLEAR REACTIONS 19F(α, pγ), E=6 MeV; measured DSA; evaluated systematic analysis errors. 22Ne level deduced T1/2.

doi: 10.1016/0370-2693(72)90769-1
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1971BE36      Phys.Rev.Lett. 27, 110 (1971)

Z.Berant, R.A.Eisenstein, J.S.Greenberg, Y.Horowitz, U.Smilansky, P.N.Tandon, A.M.Kleinfeld, H.G.Maggi

Investigation of the Reorientation Effect in Cd110 and Cd114

NUCLEAR REACTIONS 110,114Cd(α, α'), E = 8-16 MeV; (16O, 16O'), E = 37-48 MeV; measured σ(E;Eα'), σ(E; E(16O')). 110,114Cd levels deduced B(E2), quadrupole moment.

doi: 10.1103/PhysRevLett.27.110
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1971BE45      Nucl.Phys. A173, 401 (1971)

Z.Berant, M.B.Goldberg, M.Popp, J.S.Sokolowski, P.N.Tandon, Y.Wolfson

Nuclear Spectroscopic Studies on 18O

NUCLEAR REACTIONS 18O(α, α'γ), E=13.5, 15.0, 16.0, 17.0 MeV; measured αγ(θ). 18O deduced levels, J, π, γ-mixing, branching ratios. Enriched targets.

doi: 10.1016/0375-9474(71)90353-8
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1971BE60      Nucl.Phys. A178, 155 (1971)

Z.Berant, M.B.Goldberg, G.Goldring, S.S.Hanna, H.M.Loebenstein, I.Plesser, M.Popp, J.S.Sokolowski, P.N.Tandon, Y.Wolfson

Hyperfine Interaction Studies of Light Nuclei in Highly Ionized Atoms Recoiling in Vacuum

NUCLEAR REACTIONS 19F(p, αγ), Ep=0.873 MeV; 12C(α, α'γ), Eα=10-17 MeV; 16O(α, α'γ), Eα=17.9 MeV; 18O(α, α'γ), Eα=18.0 MeV; 19F(α, α'γ), Eα=10.6, 12.3 MeV; 24Mg(α, α'γ), Eα=11.4 MeV; 12C(16O, αγ), E(16O)=28.0-30.5 MeV; 12C(18O, 18O'γ), E(18O)=33-35 MeV; measured σ(θ(γ)), recoils in vacuum, metals; deduced ionic fields. Natural, enriched targets.

doi: 10.1016/0375-9474(71)90195-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0272.


1969DE03      Nucl.Phys. A124, 655 (1969)

S.H.Devare, P.N.Tandon, H.G.Devare

Coulomb Excitation in 127I

NUCLEAR REACTIONS 127I(α, α'γ), 127I(p, p'γ), E=3.5-5 MeV; measured σ(Eγ). 127I γ-transitions deduced B(E2).

doi: 10.1016/0375-9474(69)90657-5
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1969HO42      Indian J.Pure Appl.Phys. 7, 604 (1969)

R.R.Hosangdi, P.N.Tandon, S.H.Devare

The Half-Lives of Excited Levels in 125Te and 132I

RADIOACTIVITY 125Sb; measured βγ-delay. 132Te; measured βγ-, γγ-delay. 125Te, 132I levels deduced T1/2.


1969SI05      Nucl.Phys. A131, 92 (1969)

V.Singh, P.N.Tandon, S.H.Devare, H.G.Devare

g-Factors of the 321 and 463 keV Levels in 125Te

RADIOACTIVITY 125Sb[from 124Sn(n, γ)]; measured γγ(θ), γγ(θ, H). 125Te levels deduced μ. Natural target.

doi: 10.1016/0375-9474(69)90811-2
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1969SI06      Nucl.Phys. A132, 221 (1969)

V.Singh, P.N.Tandon, S.H.Devare, H.G.Devare

Magnetic Moment of the 49.7 keV Level in 132I

RADIOACTIVITY 132Te [from fission]; measured γγ(θ), γγ(θ, H). 132I level deduced μ.

doi: 10.1016/0375-9474(69)90625-3
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1969SI13      Nucl.Phys. A137, 278 (1969)

V.Singh, P.N.Tandon, S.H.Devare, H.G.Devare

g-Factor of the 810.5 keV Level in 58Fe

RADIOACTIVITY 58Co [from 58Ni(n, p)]; measured γγ(θ), γγ(θ, H). 58Fe level, deduced μ, γ-mixing. Natural target.

doi: 10.1016/0375-9474(69)90109-2
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1969TA08      Indian J.Pure Appl.Phys. 7, 1 (1969)

P.N.Tandon, H.G.Devare

The g Factor of the 114 keV State in 149Pm

RADIOACTIVITY 149Nd [from 148Nd(n, γ)]; measured γγ(θ, H, t). 149Pm level deduced T1/2, g.


1968JO18      Arkiv Fysik 37, 453 (1968)

K.Johansson, E.Karlsson, L.O.Norlin, P.N.Tandon, H.C.Jain

The Temperature Dependence of the Magnetic Hyperfine Field at Palladium in Iron

RADIOACTIVITY 106Rh [from 106Ru(β)]; measured γγ(θ, H, T); deduced temperature dependence of magnetic hyperfine field at palladium in iron.


1968TA12      Proc.Intern.Conf.Hyperfine Struct.Nucl.Radiations, Asilomar, Pacific Grove, Calif. (1967), E.Matthias, D.A.Shirley, Eds., North-Holland Publ.Co., Amsterdam, p.164 (1968)

P.N.Tandon, H.G.Devare

On the Ionic State of 143Pr from the Decay of 143Ce

RADIOACTIVITY 143Ce; measured γγ(θ, H). 143Pr level deduced g.


1967SV01      Nucl.Phys. A95, 653 (1967)

A.G.Svensson, R.W.Sommerfeldt, L.-O.Norlin, P.N.Tandon

Nuclear Magnetic Moments of the First and the Second Excited States in 127I

RADIOACTIVITY 127Xe [from 127I(p, n)]; 127mTe [from 126Te(n, γ)]; measured γγ(θ, H), γγ-delay. 127I levels deduced μ, T1/2. Enriched 126Te target.

doi: 10.1016/0375-9474(67)90858-5
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1967SV02      Arkiv Fysik 34, 113 (1967)

A.G.Svensson, L.-O.Norlin, P.N.Tandon

Influence of Positon Annihilation γ-γ Coincidence Measurements in the Decay of 118-Te and 119m-Te

NUCLEAR STRUCTURE 119Te, 118Te; measured not abstracted; deduced nuclear properties.


1967TA07      Nucl.Phys. A102, 203(1967)

P.N.Tandon, H.G.Devare

Measurement of the g-Factors of Two Levels of 131I

RADIOACTIVITY 131mTe[from 130Te(n, γ)]; measured γγ(θ, t), γγ(θ, H). 131I levels deduced μ. Enriched 130Te target.

doi: 10.1016/0375-9474(67)90331-4
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1967TA12      Contrib.Intern.Conf.Nucl.Struct., Tokyo, p.201 (1967)

P.N.Tandon, H.G.Devare

Magnetic Moment of the 114 keV State in 149Pm

RADIOACTIVITY 149Nd [from 148Nd(n, γ)]; measured γγ(θ, H). 149Pm level deduced g.


1964TA08      Nuovo Cimento 32, 388 (1964)

P.N.Tandon, H.G.Devare

On the Decay of the 4-Hour Activity of 71Zn

NUCLEAR STRUCTURE 71Zn; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF02733968
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1964TA09      Phys.Letters 10, 113 (1964)

P.N.Tandon, H.G.Devare

The Lifetime of the 820 keV State of In115

NUCLEAR STRUCTURE 115Cd; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90599-2
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1963DE10      Phys.Rev. 131, 1750 (1963)

S.H.Devare, P.N.Tandon, H.G.Devare

Decay of the 25-min Activity of Te131

NUCLEAR STRUCTURE 131Te; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.131.1750
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1963DE17      Proc.Nucl.Phys.Symp.Bombay, p.43 (1963)

S.H.Devare, P.N.Tandon, H.G.Devare

Decay of the 25 min Activity of Te131

NUCLEAR STRUCTURE 131Te; measured not abstracted; deduced nuclear properties.


1963TA11      Priv.Comm. (October 1963)

P.N.Tandon, H.G.Davers

On the Decay of the 4-Hour Activity of Zn71

NUCLEAR STRUCTURE 71Zn; measured not abstracted; deduced nuclear properties.


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