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NSR database version of April 11, 2024.

Search: Author = K.Bharuth-Ram

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2012BH05      Hyperfine Interactions 207, 49 (2012)

K.Bharuth-Ram, H.Masenda, T.B.Doyle, S.Geburt, C.Ronning, H.P.Gunnlaugsson

A CEMS search for precipitate formation in ⁵⁷Fe implanted ZnO

ATOMIC PHYSICS ⁵⁷Fe; measured decay products, ce; deduced hyperfine parameters. Conversion electron Mossbauer spectroscopy (CEMS).

doi: 10.1007/s10751-011-0403-8
Citations: PlumX Metrics

2012MA11      Hyperfine Interactions 208, 71 (2012)

H.Masenda, K.Bharuth-Ram, D.Naidoo, H.P.Gunnlaugsson, T.E.Molholt

Mossbauer study of ¹¹⁹Sn in ¹¹⁹In^* implanted 3C-SiC

RADIOACTIVITY ¹¹⁹In(β^-) [from U(p, X)¹¹⁹In, E=1.4 GeV]; measured decay products, X-rays, Eγ, Iγ. ¹¹⁹Sn; deduced Mossbauer spectra, isomer shift, quadrupole splitting, lattice damage.

doi: 10.1007/s10751-011-0438-x
Citations: PlumX Metrics

2007BH09      Hyperfine Interactions 179, 17 (2007)

K.Bharuth-Ram, V.V.Naicker, D.Naidoo, H.P.Gunnlaugsson, R.Mantovan, G.Weyer, M.Dietrich, J.E.Butler, for the ISOLDE Collaboration

Mossbauer study of ⁵⁷Fe in CVD diamond following ⁵⁷Mn implantation

doi: 10.1007/s10751-008-9669-x
Citations: PlumX Metrics

1996NE05      Phys.Rev. C54, 1773 (1996); Erratum Phys.Rev. C55, 1605 (1997)

R.T.Newman, R.W.Fearick, S.M.Perez, D.G.Aschman, K.Bharuth-Ram, W.A.Richter, F.D.Smit, V.M.Tshivhase, T.S.Volkwyn

0f_7/2 Proton Transfer on ⁵⁵Mn

NUCLEAR REACTIONS ⁵⁵Mn(d, ³He), (d, d), E=46 MeV; measured σ(θ); deduced opptical model parameters. ⁵⁴Cr deduced levels, J, spectroscopic factors. ⁵⁵Mn(α, t), E not given; analyzed data. ⁵⁶Fe levels deduced spins, spectroscopic factors. Spectroscopic sum rules analysis.

doi: 10.1103/PhysRevC.54.1773
Citations: PlumX Metrics

1996QU03      Nucl.Instrum.Methods Phys.Res. B118, 72 (1996)

H.Quintel, K.Bharuth-Ram, H.Hofsass, M.Restle, C.Ronning

Emission Channeling Study of Annealing of Radiation Damage in Heavy-Ion Implanted Diamond

RADIOACTIVITY ¹¹¹In, ⁷³As(EC); measured I(ce)(θ); deduced diamond lattice annealing features.

doi: 10.1016/0168-583X(95)01195-1
Citations: PlumX Metrics

1994CO21      Nucl.Instrum.Methods Phys.Res. B85, 508 (1994)

S.H.Connell, E.Sideras-Haddad, K.Bharuth-Ram, C.G.Smallman, J.P.F.Sellschop, M.G.Bossenger

Perturbed Angular Distribution Studies in Natural, Synthetic CVD and HPHT Diamond

NUCLEAR REACTIONS ¹⁹F(p, p'), E=4.2 MeV; measured γ(θ, H, t); deduced usefulness as probe to determine hydrogen impurity. Natural, synthetic CVD, HPHT diamond.

doi: 10.1016/0168-583X(94)95873-4
Citations: PlumX Metrics

1993AL14      Phys.Lett. 314B, 173 (1993)

M.S.Allie, F.D.Brooks, D.G.Aschman, A.Buffler, W.A.Cilliers, R.W.Fearick, C.G.L.Henderson, M.J.Oliver, M.R.Nchodu, S.M.Perez, D.Steyn, W.R.McMurray, B.R.S.Simpson, F.D.Smit, H.G.Miller, K.Bharuth-Ram, I.J.van Heerden

Differential Cross Section for n-p Radiative Capture at E(n) = 63.4 MeV

NUCLEAR REACTIONS ¹H(n, γ), E=63.4 MeV; measured Iγ(θ); deduced σ(θ) for ²H(γ, p), E ≈ 34 MeV. Legendre polymonial fits.

doi: 10.1016/0370-2693(93)90445-N
Citations: PlumX Metrics

1993MC06      Nucl.Instrum.Methods Phys.Res. A329, 217 (1993)

W.R.McMurray, D.G.Aschman, K.Bharuth-Ram, R.W.Fearick

The Faure Cylotron Neutron Source and a Particle Spectrometer for Neutron Induced Emission of Charged Particles at Energies between 60 and 200 MeV

NUCLEAR REACTIONS ¹²C(n, p), (n, d), E=64 MeV; measured p-, d-spectra; deduced system particle identification capabilities. Faure cyclotron neutron source, particle spectrometer.

doi: 10.1016/0168-9002(93)90939-F
Citations: PlumX Metrics

1993SI22      Hyperfine Interactions 79, 793 (1993)

E.Sideras-Haddad, S.H.Connell, J.P.F.Sellschop, M.C.Stemmet, K.Bharuth-Ram

Hydrogen-Related Molecular Structures Observed in ¹⁹F-TDPAD Studies in Diamond

NUCLEAR REACTIONS ¹⁹F(p, p'), E not given; measured γ(θ, H, t), recoil ¹⁹F implantation in diamond; deduced diamond lattice sites populated by ¹⁹F.

doi: 10.1007/BF00567610
Citations: PlumX Metrics

1990BH03      Hyperfine Interactions 59, 109 (1990)

K.Bharuth-Ram, J.Billowes, J.Heese, C.J.Gross, K.P.Lieb, N.Martin, S.Skoda, J.Eberth

IMPAD g-Factor Measurements in ⁸³Y

NUCLEAR REACTIONS ⁵⁴Fe(³²S, 3p), E=107 MeV; ⁵⁸Ni(²⁸Si, 3p), E=90 MeV; measured γ(θ, H). ⁸³Y levels deduced g. Model analysis.

doi: 10.1007/BF02401201
Citations: PlumX Metrics

1990BH06      Phys.Lett. 252B, 540 (1990)

K.Bharuth-Ram, J.Billowes, C.J.Gross, J.Heese, K.P.Lieb, J.Eberth, S.Skoda

Nature of the Three-Quasiparticle ((17/2)^-)₂ State in ⁸³Y

RADIOACTIVITY ⁸³Y; measured level g-factor; deduced level configuration. Time-integral IMPAD technique.

doi: 10.1016/0370-2693(90)90479-P
Citations: PlumX Metrics

1990MC04      Nucl.Instrum.Methods Phys.Res. A288, 421 (1990)

W.R.McMurray, K.Bharuth-Ram, D.G.Aschman

A Particle Spectrometer for Angular Distribution Measurements from (n, p) and (n, d) Reactions at 22 MeV

NUCLEAR REACTIONS ⁵¹V(n, d), E=21.6 MeV; measured σ(Ed). New type of particle spectrometer.

doi: 10.1016/0168-9002(90)90133-Q
Citations: PlumX Metrics

1990NA16      Z.Phys. A336, 203 (1990)

R.Y.Naidoo, K.Bharuth-Ram, W.R.McMurray

The ²⁷Al(n, d)²⁶Mg Reaction at 22 MeV

NUCLEAR REACTIONS ²⁷Al(n, d), E=21.6 MeV; measured σ(θ); deduced model parameters. ²⁶Mg levels deduced S. DWBA analysis.

1989CR08      Nucl.Phys. A501, 118 (1989)

F.Cristancho, K.P.Lieb, J.Heese, C.J.Gross, W.Fieber, Th.Osipowicz, S.Ulbig, K.Bharuth-Ram, S.Skoda, J.Eberth, A.Dewald, P.von Brentano

Side-Feeding Times and Level Lifetimes Measured in the Reaction ⁵⁴Fe(³²S, 3p)⁸³Y

NUCLEAR REACTIONS ⁵⁴Fe(³²S, 3p), E=103-107 MeV; measured Doppler-broadened lineshapes, γγ-coin. ⁸³Y levels deduced T_1/2, side-feeding times, B(E2). Monte Carlo simulation of side feeding.

doi: 10.1016/0375-9474(89)90568-X
Citations: PlumX Metrics

1989FI06      Z.Phys. A332, 363 (1989)

W.Fieber, K.Bharuth-Ram, J.Heese, F.Cristancho, C.J.Gross, K.P.Lieb, S.Skoda, J.Eberth

On the Coexistence of Oblate and Prolate Deformed Bands in ⁸³Zr

NUCLEAR REACTIONS ⁵⁴Fe(³²S, n2p), E=103, 107 MeV; measured nγ-coin, DSA. ⁸³Zr deduced levels, J, π, band structure, B(λ), transition quadrupole moments, T_1/2, deformation parameters. Cranking model.

1988CO20      Hyperfine Interactions 39, 397 (1988)

S.Connell, K.Bharuth-Ram, J.P.F.Sellschop, M.C.Stemmet, H.Appel

Temperature Dependence Study of ¹⁹F Implants in Diamond by TDPAD

NUCLEAR REACTIONS ¹⁹F(p, p'), E=4 MeV; measured γ(θ, H, t). Target implanted in diamond.

doi: 10.1007/BF02397649
Citations: PlumX Metrics

1987BH05      Hyperfine Interactions 34, 189 (1987)

K.Bharuth-Ram, S.Connell, J.P.F.Sellschop, M.C.Stemmet, H.Appel, G.M.Then

TDPAD Studies on ¹⁹F Implanted into Diamond

NUCLEAR REACTIONS ¹⁹F(p, p'γ), E=4 MeV; measured γ(θ, H, t). Target implantation in diamond.

doi: 10.1007/BF02072700
Citations: PlumX Metrics

1987BH08      Phys.Rev. C36, 1749 (1987)

K.Bharuth-Ram, A.C.Bawa, W.R.McMurray

⁹⁰Zr(n, d)⁸⁹Y Reaction at 22 MeV

NUCLEAR REACTIONS ⁹⁰Zr(n, d), E=22 MeV; measured σ(Ed), σ(θ). ⁸⁹Y deduced levels, spectroscopic factors.

doi: 10.1103/PhysRevC.36.1749
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31683.

1987ZI04      Phys.Rev. A36, 5170 (1987)

M.Zielinski, W.Y.Baek, K.Bharuth-Ram, D.Gassen, W.Neuwirth

Enery Loss of ¹⁴N Ions in Ni, Ag, and Cu and the Lifetimes of the States at 2.3 and 3.9 MeV in ¹⁴N

NUCLEAR REACTIONS ¹²C(³He, pγ), E=6.23 MeV; measured σ(Ep), σ(Eγ), pγ-coin; deduced residue energy loss in Ni, Ag, Cu. ¹⁴N levels deduced T_1/2. Ge(Li), Si detectors.

doi: 10.1103/PhysRevA.36.5170
Citations: PlumX Metrics

1984BH06      Nucl.Phys. A427, 451 (1984)

K.Bharuth-Ram, G.Lo Bianco, P.Paruzzi, A.Dewald, J.Wrzesinski, K.O.Zell, P.Von Brentano

The Lifetime of the 266 keV Level in ²⁰⁶Tl

NUCLEAR REACTIONS ²⁰⁵Tl(d, p), E=9 MeV; measured pγ(t). ²⁰⁶Tl level deduced T_1/2, B(E2). Ge(Li), Si surface barrier detectors, enriched target.

doi: 10.1016/0375-9474(84)90224-0
Citations: PlumX Metrics

1984MC05      Z.Phys. A315, 189 (1984)

W.R.McMurray, K.Bharuth-Ram, S.M.Perez

Excitation of the Analogue of the T( > ) Giant Dipole Resonance of ⁹⁰Zr via the (n, p) Reaction

NUCLEAR REACTIONS ⁹⁰Zr(n, p), E=21.8 MeV; measured σ(Ep, θ). ⁹⁰Zr deduced GDR T( > ) component, other resonance excitation. DWBA analysis, Lane potential.

doi: 10.1007/BF01419378
Citations: PlumX Metrics

1984SP03      Z.Phys. A315, 319 (1984)

K.-H.Speidel, V.Mertens, W.Trolenberg, M.Knopp, H.Neuburger, K.Bharuth-Ram, J.Gerber

g-Factor of the Second 4⁺ State in ²⁴Mg

NUCLEAR REACTIONS, ICPND ¹²C(¹⁶O, α), E=39-40 MeV; measured α yield vs E, (²⁴Mg)γ-, γ(particle)-coin, γ(particle)(θ), γ(θ, H, t). ²⁴Mg levels deduced g.

doi: 10.1007/BF01438456
Citations: PlumX Metrics

1983SP01      Nucl.Phys. A403, 421 (1983)

K.-H.Speidel, V.Mertens, W.Trolenberg, M.Knopp, H.Neuburger, J.Gerber, K.Bharuth-Ram

g-Factor Measurements of Excited States in ²⁴Mg

NUCLEAR REACTIONS ¹²C(¹⁶O, α), E=34.8-38.7 MeV; measured α-yield, (particle)γ-coin, DSA, γ(θ, H). ²⁴Mg levels deduced g, T_1/2.

doi: 10.1016/0375-9474(83)90235-X
Citations: PlumX Metrics

1983SP04      Hyperfine Interactions 15/16, 55 (1983)

K.-H.Speidel, V.Mertens, M.Knopp, W.Trolenberg, H.Neuburger, J.Gerber, K.Bharuth-Ram

Anomalous g-Factor Measurements using Transient Fields

NUCLEAR REACTIONS ¹²C(¹²C, α), (¹⁶O, α), E not given; measured αγ(θ, H) in Fe, Gd. ²⁰Ne, ²⁴Mg levels deduced g.

doi: 10.1007/BF02159714
Citations: PlumX Metrics

1981MI08      Z.Phys. A300, 97 (1981)

M.Miller, A.M.Kleinfeld, A.Bockisch, K.Bharuth-Ram

The Analysis of Elastic and Inelastic Scattering of Alpha Particles using a Folding Potential

NUCLEAR REACTIONS ^{110,112,114,116}Cd, ¹²⁴Te(α, α), (α, α'), E=10-17 MeV; measured σ(Eα, θ); deduced folding potential parameters. ^{110,112,114,116}Cd deduced rms radius. Effective α-nucleon interaction.

doi: 10.1007/BF01412620
Citations: PlumX Metrics

1979BO02      Z.Phys. A289, 231 (1979)

A.Bockisch, K.Bharuth-Ram, A.M.Kleinfeld, K.P.Lieb

Oblate Shapes of ^200,202,204Hg

NUCLEAR REACTIONS Hg(¹⁶O, ¹⁶O'), E=56-64 MeV; measured relative γ-yield following Coulomb excitation. ^200,202,204Hg deduced quadrupole moment, oblate shapes. ^{196,198,200,202,204}Hg levels deduced B(E2). Natural target.

doi: 10.1007/BF01435944
Citations: PlumX Metrics

1979BO16      Z.Phys. A291, 245 (1979)

A.Bockisch, K.Bharuth-Ram, A.M.Kleinfeld, K.P.Lieb

Reorientation Effect Measurements of Even Mercury Isotopes

NUCLEAR REACTIONS ¹⁹⁸Hg(α, α'), E=13, 15, 16 MeV; ¹⁹⁸Hg(¹⁶O, ¹⁶O'), E=56, 58, 60 MeV; Hg(α, α'), E=15 MeV; Hg(¹⁶O, ¹⁶O'), E=56-64 MeV; measured Eγ, Iγ, multiple Coulomb excitation, reorientation effects, particle spectra. ¹⁹⁸Hg deduced quadrupole moment. ^198,200,202Hg deduced B(E2), oblate shapes. Triaxial rotation, anharmonic vibration interpretation.

doi: 10.1007/BF01409190
Citations: PlumX Metrics

1977BH01      Nucl.Phys. A278, 285 (1977)

K.Bharuth-Ram, S.M.Perez, F.D.Brooks, S.A.R.Wynchank, W.R.McMurray

Excitation of the Analogue Dipole State in ²⁸Al via the Reaction ²⁸Si(n, p)²⁸Al

NUCLEAR REACTIONS ²⁸Si(n, p), E=21.6 MeV; measured σ(Ep, θ(p)). Natural target.

doi: 10.1016/0375-9474(77)90240-8
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30431.

1976BH03      Nucl.Phys. A269, 327 (1976)

K.Bharuth-Ram, K.P.Jackson, P.G.Lawson, N.A.Jelley, K.W.Allen

Electromagnetic Transitions in ¹⁹F

NUCLEAR REACTIONS ¹⁹F(p, p'γ), E=5-9 MeV; measured Eγ, Iγ, p'γ-coin, γ(θ), DSA. ¹⁹F deduced levels, J, π, T_1/2, Γ, Γγ, γ-branching. Ge(Li) detectors.

doi: 10.1016/0375-9474(76)90684-9
Citations: PlumX Metrics

1970BH02      Phys.Rev. C2, 1210 (1970)

K.Bharuth-Ram, R.D.Gill, K.P.Jackson, B.Povh, E.K.Warburton

Nuclear Lifetime of the Ne¹⁹ 275-keV Level

NUCLEAR REACTIONS ³He(²⁰Ne, αγ), E=31.2 MeV; measured σ(Eγ), Doppler shifts. ¹⁹Ne deduced levels, T_1/2. Recoil distance method.

doi: 10.1103/PhysRevC.2.1210
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1970GI09      Nucl.Phys. A152, 369 (1970)

R.D.Gill, K.Bharuth-Ram, K.P.Jackson, R.A.I.Bell, B.C.Robertson, J.L'Ecuyer, N.G.Chapman, H.J.Rose

Electromagnetic Transitions in ¹⁹Ne

NUCLEAR REACTIONS ¹⁹F(p, n), E=8.48-10.4 MeV; ¹⁶O(α, n), E=15-19 MeV; measured σ(E;En, Eγ, θ(nγ)), Doppler shift attenuation. ¹⁹Ne deduced levels, T_1/2, branching ratios, J, π, γ-mixing. Natural targets, Ge(Li) detectors.

doi: 10.1016/0375-9474(70)90837-7
Citations: PlumX Metrics

1969BH01      Nucl.Phys. A137, 262 (1969)

K.Bharuth-Ram, K.P.Jackson, K.W.Jones, E.K.Warburton

Nuclear Lifetimes from Bombardment of ^2,3H by ^20,22Ne

NUCLEAR REACTIONS ²H(²⁰Ne, p), ²H(²⁰Ne, n), ³H(²⁰Ne, α), ³H(²²Ne, p); E approx 30 MeV; measured Eγ, Doppler-shift attenuation; ¹⁹F, ²¹Ne, ²¹Na, ²⁴Ne deduced T_1/2. Ge(Li) detector.

doi: 10.1016/0375-9474(69)90107-9
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1969JA09      Phys.Letters 30B, 162 (1969)

K.P.Jackson, K.Bharuth Ram, P.G.Lawson, N.G.Chapman, K.W.Allen

High Spin States in ¹⁹F

NUCLEAR REACTIONS ¹⁹F(α, α'γ), E =12.7 MeV; measured Q, σ(Eα', Eγ, θ(γ)), Doppler shift attenuation. ¹⁹F deduced levels, J, π, T_1/2.

doi: 10.1016/0370-2693(69)90357-8
Citations: PlumX Metrics