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1.
H. P. Gunnlaugsson K. Bharuth-Ram M. Dietrich M. Fanciulli H. O. U. Fynbo G. Weyer 《Hyperfine Interactions》2006,169(1-3):1315-1318
We report on the detection of Fe i –B pairs in heavily B doped silicon using 57Fe emission Mössbauer spectroscopy following implantation of radioactive 57Mn+ parent ions (T 1/2?=?1.5 min) at elevated temperatures >?850 K. The Fe i –B pairs are formed upon the dissociation of Fe i –V pairs during the lifetime of the Mössbauer state (T 1/2?=?100 ns). The resulting free interstitial Fei diffuses over sufficiently large distances during the lifetime of the Mössbauer state to encounter a substitutional B impurity atom, forming Fe i –B pairs, which are stable up to ~1,050 K on that time scale. 相似文献
2.
Hyperfine Interactions - Conversion electron Mössbauer spectroscopy measurements have been made on a diamond sample synthesized by chemical vapour deposition. The sample was implanted with 70... 相似文献
3.
K. Bharuth-Ram 《Hyperfine Interactions》2013,214(1-3):127-132
A brief review is given of the Hyperfine Interactions Conference series and, in particular, of the Joint meetings of the Hyperfine Interactions and Nuclear Quadrupole Interaction (HFI/NQI) Conferences, with respect to number of participants, contributed papers and participant countries. Trends are traced and recommendations are offered to attract a wider participation at future HFI/NQI conferences. 相似文献
4.
K. Bharuth-Ram J. Billowes J. Heese C. J. Gross K. P. Lieb N. Martin S. Skoda J. Eberth 《Hyperfine Interactions》1990,59(1-4):109-112
The IMPAD technique has been used to determine the Larmor precessions of the83Y 595 keV 13/2+ and 145 keV 7/2+ states in iron. The net precessions found are ωτ(13/2+)=−9(2) mrad and ωτ(7/2+)=−92(5) mrad, leading to g-factors, g(13/2+)=+1.3(4) and g(7/2+)=+0.61(18). These results are discussed in terms of a partially decoupled [422]5/2+ Nilsson band. 相似文献
5.
S. Connell K. Bharuth-Ram H. Appel J. P. F. Sellschop M. Stemmet 《Hyperfine Interactions》1987,36(3-4):185-200
19F has been used to probe the structure of the diamond lattice. The measurements were performed via the time differential perturbed
angular distribution (TDPAD) technique applied to the 197 keV state (τ=128 ns,Q=0.10 b) of19F. The nuclei were excited and recoil implanted into an oriented diamond using a (p,p′γ) reaction initiated by a pulsed 4
MeV proton beam. Model functions simulating a variety of residence sites for the probe ions in a single crystal were developed
for the analysis of the data. The data implies the formation of two molecular types, or sites within the lattice, with possibly
a third radiation damage component. 相似文献
6.
Hyperfine Interactions - 相似文献
7.
W. Fieber K. Bharuth-Ram J. Heese F. Cristancho C. J. Gross K. P. Lieb S. Skoda J. Eberth 《Zeitschrift für Physik A Hadrons and Nuclei》1989,332(4):363-370
Deformation parameters of the positive parity yrast band and negative parity bands in83Zr are deduced from lifetimes andE2/M1 mixing ratios. Lifetimes of high spin states have been determined from recoil distance Doppler shift and Doppler shift attenuation measurements using the54Fe(32S,2pnγ) 83Zr reaction. Ten lifetimes and five lifetimes limits were determined. The positive parity band, built on theg 9/2 K=5/2 orbital has an average deformation ¦β 2¦=0.28(2), and shows a reduction ofE2 transition strengths in the observed backbend region at Iπ≈21/2+. In contrast, theE2 strengths in the negative parity states show a steady increase up to Iπ≈=15/2?. These states are more strongly deformed than the positive parity states (¦β 2¦=0.33(3)). TheE2/M1 mixing ratios show that the negative parity band hasK=3/2 and is prolate, and favour oblate deformation for the positive parity yrast band. In theK=1/2? band theE2 strength of the 7/2?→3/2? transition yields a deformation ¦β 2¦=0.26(5). The band structure is compared with calculations within the Hartree-Fock Bogoliubov cranking model. 相似文献
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9.
H. Masenda S. Geburt K. Bharuth-Ram D. Naidoo H. P. Gunnlaugsson K. Johnston R. Mantovan T. E. Mølholt M. Ncube S. Shayestehaminzadeh H. P. Gislason G. Langouche S. Ólafsson C. Ronning ISOLDE Collaboration 《Hyperfine Interactions》2016,237(1):40
Emission Mössbauer Spectroscopy following the implantation of radioactive precursor isotope 57Mn+ (T 1/2= 1.5 min) into ZnO single crystals at ISOLDE/CERN shows that a large fraction of 57Fe atoms produced in the 57Mn beta decay is created as paramagnetic Fe3+ with relatively long spin-lattice relaxation times. Here we report on ZnO pre-implanted with 56Fe to fluences of 2×1013, 5×10 13 and 8 × 1013 ions/cm2 in order to investigate the dependence of the paramagnetic relaxation rate of Fe3+ on fluence. The spectra are dominated by magnetic features displaying paramagnetic relaxation effects. The extracted spin-lattice relaxation rates show a slight increase with increasing ion fluence at corresponding temperatures and the area fraction of Fe3+ at room temperature reaches a maximum contribution of 80(3)% in the studied fluence range. 相似文献
10.
K. Bharuth-Ram G. Lo Bianco P. Paruzzi A. Dewald J. Wrzesinski K.O. Zell P. Von Brentano 《Nuclear Physics A》1984,427(3):451-459
The lifetime of the 206Tl 2? state at 266 keV has been measured by the delayed coincidence technique. The state was populated via the γ-decay of high-lying states excited in the 205Tl (d, p)206Tl reaction at Ed = 9.0 MeV. Delayed coincidences between a Si surface-barrier detector and a Ge(Li) detector resulted in a mean life for the 266 keV level of τ = 3.3(2) ns. The deduced B(E2) value of 171 (11) e2 · fm4 indicates strong configuration mixing of two-hole states in this level. 相似文献