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Black Hole

Lensing of space time around a black hole. At Oxford we study black holes observationally and theoretically on all size and time scales - it is some of our core work.

Credit: ALAIN RIAZUELO, IAP/UPMC/CNRS. CLICK HERE TO VIEW MORE IMAGES.

Jirina Stone

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  • Astrophysics
jirina.stone@physics.ox.ac.uk
Telephone: 01865 (2)73306
Denys Wilkinson Building, room 704
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ONLINE NUCLEAR ORIENTATION OF I-118 AND THE IDENTIFICATION OF THE G9/2 INTRUDER ORBITAL

PHYSICS LETTERS B 153:4-5 (1985) 221-225

Authors:

TL SHAW, VR GREEN, NJ STONE, J RIKOVSKA, PM WALKER, S COLLINS, SA HAMADA, WD HAMILTON, IS GRANT
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Gamma-ray linear polarization and nuclear orientation experiments on oriented192, 194Ir Fe

Hyperfine Interactions 15:1-4 (1983) 41-42

Authors:

J Rikovska, D Novakova, J Ferencei

Abstract:

The combined technique of gamma-ray linear polarization and directional distribution measurement from oriented nuclei (LPγON) has been applied to192Ir Fe. New polarization data are used to deduce values of mixing ratios in Β and γ transitions. © 1983 J.C. Baltzer Scientific Publishing Company.
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Linear polarization and directional distribution of gamma-rays from oriented172Lu

Czechoslovak Journal of Physics 33:10 (1983) 1070-1083

Authors:

D Nováková, J Říkovská, A Jankech, J Ferencei, VN Pavlov, M Finger

Abstract:

The gamma-ray linear polarization data in combination with the results of the directional distribution measurements were used to determine precise values of the multipole mixing ratios of the gamma-transitions in the172Yb nucleus. A detailed analysis of the deduced mixing ratios, supplemented by previous data, lends support to the following description of the two-quasiparticle excitations of192Yb (see also tab. 6): 2073 keV Kπ = (4+) {p 4041 ↓ + p 411 ↓} + {n 514↓ - n 521↓} 1663 keV Kπ = (3+) {n 514↓ - n 521↓} + {n 512↑ - n 521↓} 1172 keV Kπ = 3+ {n 512↑ + n 521↓} + {p404↓ - P 411↓} A supporting evidence has also been given to the spin-parity assignments of the 1640 keV (Iπ = 4-) and 1706 keV (Iπ = 5-) members of the Kπ = 4- band. © 1983 Academia, Publishing House of the Czechoslovak Academy of Sciences.
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Nuclear magnetic moment of161Tb

Hyperfine Interactions 15:1-4 (1983) 83-84

Authors:

J Rikovska, A Machova, D Novakova, J Ferencei, M Finger

Abstract:

Nuclear orientation measurements on dilute Tb Gd are analysed to yield the magnetic dipole and electric quadrupole moments of161Tb g.s. and multipole mixing ratios of transitions in161Dy. © 1983 J.C. Baltzer Scientific Publishing Company.
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Nuclear orientation of152,154Tb in gadolinium

Czechoslovak Journal of Physics 31:5 (1981) 511-521

Authors:

J Ferencei, M Finger, J Dupák, A Jankech, J Koníček, FA Schus, J Říkovská, A Machová, DW Hamilton

Abstract:

The anisotropy in the directional distribution of gamma-rays from the decay of152,154Tb oriented in a gadolinium matrix at low temperatures, has been measured at the angles of 0 and π/2 with respect to the applied magnetic field direction at temperature of (15±1) mK. Unambiguous values of spin have been deduced for several levels in152Gd. Multipole mixing ratios of many gamma-ray transitions occurring in152Gd have been found and results are compared with the similar transitions in150,154,156Gd and they are discussed in terms of the rotational-vibrational model and dynamic deformation theory based on the Strutinsky method. Our results confirm the spin value of 0 for 21·4 h isomer in154Tb and they establish the spin value of 3 for the 2277·0 and 2336·1 keV levels and the spin value of 4 for the 2416·3 keV level in154Gd. © 1981 Academia, Publishing House of the Czechoslovak Academy of Sciences.
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