author_facet Thakur, P.
Behra, M. S.
Dogra, R.
Bhati, A.K.
Bedi, S. C.
Thakur, P.
Behra, M. S.
Dogra, R.
Bhati, A.K.
Bedi, S. C.
author Thakur, P.
Behra, M. S.
Dogra, R.
Bhati, A.K.
Bedi, S. C.
spellingShingle Thakur, P.
Behra, M. S.
Dogra, R.
Bhati, A.K.
Bedi, S. C.
Zeitschrift für Naturforschung A
Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
Physical and Theoretical Chemistry
General Physics and Astronomy
Mathematical Physics
author_sort thakur, p.
spelling Thakur, P. Behra, M. S. Dogra, R. Bhati, A.K. Bedi, S. C. 1865-7109 0932-0784 Walter de Gruyter GmbH Physical and Theoretical Chemistry General Physics and Astronomy Mathematical Physics http://dx.doi.org/10.1515/zna-2002-6-754 <jats:p>The time differential perturbed angular correlation (TDPAC) technique has been used to study the nuclear quadrupole interactions of the first excited state of ground state rotational band (2<jats:sup>+</jats:sup>, 80 keV, T<jats:sub>1/2</jats:sub> = 1.88 ns) and the band head of the = 4<jats:sub>1</jats:sub> <jats:sup>-</jats:sup> band (4<jats:sub>1</jats:sub> <jats:sup>-</jats:sup>,1094 keV, T<jats:sub>1/2</jats:sub> = 120 ns) in the <jats:sup>168</jats:sup>Er nucleus of a polycrystalline Er host. At room temperature we obtained the electric quadrupole interaction frequencies ω<jats:sub>0</jats:sub>(K= 0) = 457(15) Mrad/s and ω<jats:sub>0</jats:sub>(K= 4) = 69(2) Mrad/s, respectively, for the 2<jats:sup>+</jats:sup> and 4<jats:sup>-</jats:sup> isomeric states of <jats:sup>168</jats:sup>Er. The ratio of the spectroscopic quadrupole moments, i. e. Q<jats:sub>s</jats:sub> (K= 4)/Q<jats:sub>s</jats:sub> (K= 0) = 0.69(3), is independent of any model approximation and the electric field gradient at <jats:sup>168</jats:sup>Er in the host metal</jats:p> Static Electric Quadrupole Moments in the Ground State and K = 4<sup>–</sup> <sub>1</sub> Bands in <sup>168</sup>Er Zeitschrift für Naturforschung A
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series Zeitschrift für Naturforschung A
source_id 49
title Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
title_unstemmed Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
title_full Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
title_fullStr Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
title_full_unstemmed Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
title_short Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
title_sort static electric quadrupole moments in the ground state and k = 4<sup>–</sup> <sub>1</sub> bands in <sup>168</sup>er
topic Physical and Theoretical Chemistry
General Physics and Astronomy
Mathematical Physics
url http://dx.doi.org/10.1515/zna-2002-6-754
publishDate 2002
physical 591-594
description <jats:p>The time differential perturbed angular correlation (TDPAC) technique has been used to study the nuclear quadrupole interactions of the first excited state of ground state rotational band (2<jats:sup>+</jats:sup>, 80 keV, T<jats:sub>1/2</jats:sub> = 1.88 ns) and the band head of the = 4<jats:sub>1</jats:sub> <jats:sup>-</jats:sup> band (4<jats:sub>1</jats:sub> <jats:sup>-</jats:sup>,1094 keV, T<jats:sub>1/2</jats:sub> = 120 ns) in the <jats:sup>168</jats:sup>Er nucleus of a polycrystalline Er host. At room temperature we obtained the electric quadrupole interaction frequencies ω<jats:sub>0</jats:sub>(K= 0) = 457(15) Mrad/s and ω<jats:sub>0</jats:sub>(K= 4) = 69(2) Mrad/s, respectively, for the 2<jats:sup>+</jats:sup> and 4<jats:sup>-</jats:sup> isomeric states of <jats:sup>168</jats:sup>Er. The ratio of the spectroscopic quadrupole moments, i. e. Q<jats:sub>s</jats:sub> (K= 4)/Q<jats:sub>s</jats:sub> (K= 0) = 0.69(3), is independent of any model approximation and the electric field gradient at <jats:sup>168</jats:sup>Er in the host metal</jats:p>
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author Thakur, P., Behra, M. S., Dogra, R., Bhati, A.K., Bedi, S. C.
author_facet Thakur, P., Behra, M. S., Dogra, R., Bhati, A.K., Bedi, S. C., Thakur, P., Behra, M. S., Dogra, R., Bhati, A.K., Bedi, S. C.
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container_title Zeitschrift für Naturforschung A
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description <jats:p>The time differential perturbed angular correlation (TDPAC) technique has been used to study the nuclear quadrupole interactions of the first excited state of ground state rotational band (2<jats:sup>+</jats:sup>, 80 keV, T<jats:sub>1/2</jats:sub> = 1.88 ns) and the band head of the = 4<jats:sub>1</jats:sub> <jats:sup>-</jats:sup> band (4<jats:sub>1</jats:sub> <jats:sup>-</jats:sup>,1094 keV, T<jats:sub>1/2</jats:sub> = 120 ns) in the <jats:sup>168</jats:sup>Er nucleus of a polycrystalline Er host. At room temperature we obtained the electric quadrupole interaction frequencies ω<jats:sub>0</jats:sub>(K= 0) = 457(15) Mrad/s and ω<jats:sub>0</jats:sub>(K= 4) = 69(2) Mrad/s, respectively, for the 2<jats:sup>+</jats:sup> and 4<jats:sup>-</jats:sup> isomeric states of <jats:sup>168</jats:sup>Er. The ratio of the spectroscopic quadrupole moments, i. e. Q<jats:sub>s</jats:sub> (K= 4)/Q<jats:sub>s</jats:sub> (K= 0) = 0.69(3), is independent of any model approximation and the electric field gradient at <jats:sup>168</jats:sup>Er in the host metal</jats:p>
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spelling Thakur, P. Behra, M. S. Dogra, R. Bhati, A.K. Bedi, S. C. 1865-7109 0932-0784 Walter de Gruyter GmbH Physical and Theoretical Chemistry General Physics and Astronomy Mathematical Physics http://dx.doi.org/10.1515/zna-2002-6-754 <jats:p>The time differential perturbed angular correlation (TDPAC) technique has been used to study the nuclear quadrupole interactions of the first excited state of ground state rotational band (2<jats:sup>+</jats:sup>, 80 keV, T<jats:sub>1/2</jats:sub> = 1.88 ns) and the band head of the = 4<jats:sub>1</jats:sub> <jats:sup>-</jats:sup> band (4<jats:sub>1</jats:sub> <jats:sup>-</jats:sup>,1094 keV, T<jats:sub>1/2</jats:sub> = 120 ns) in the <jats:sup>168</jats:sup>Er nucleus of a polycrystalline Er host. At room temperature we obtained the electric quadrupole interaction frequencies ω<jats:sub>0</jats:sub>(K= 0) = 457(15) Mrad/s and ω<jats:sub>0</jats:sub>(K= 4) = 69(2) Mrad/s, respectively, for the 2<jats:sup>+</jats:sup> and 4<jats:sup>-</jats:sup> isomeric states of <jats:sup>168</jats:sup>Er. The ratio of the spectroscopic quadrupole moments, i. e. Q<jats:sub>s</jats:sub> (K= 4)/Q<jats:sub>s</jats:sub> (K= 0) = 0.69(3), is independent of any model approximation and the electric field gradient at <jats:sup>168</jats:sup>Er in the host metal</jats:p> Static Electric Quadrupole Moments in the Ground State and K = 4<sup>–</sup> <sub>1</sub> Bands in <sup>168</sup>Er Zeitschrift für Naturforschung A
spellingShingle Thakur, P., Behra, M. S., Dogra, R., Bhati, A.K., Bedi, S. C., Zeitschrift für Naturforschung A, Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er, Physical and Theoretical Chemistry, General Physics and Astronomy, Mathematical Physics
title Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
title_full Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
title_fullStr Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
title_full_unstemmed Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
title_short Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
title_sort static electric quadrupole moments in the ground state and k = 4<sup>–</sup> <sub>1</sub> bands in <sup>168</sup>er
title_unstemmed Static Electric Quadrupole Moments in the Ground State and K = 4– 1 Bands in 168Er
topic Physical and Theoretical Chemistry, General Physics and Astronomy, Mathematical Physics
url http://dx.doi.org/10.1515/zna-2002-6-754