Variation of Pertechnetate Ion Adsorption on Some Active Carbons from Mineral Acid Solutions

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Estimate of LHCb's sensitivity to the CKM angle using B0→D0K∗0B^0 \to D^0 K^{*0} Decays

In this note an updated event selection of the B0 -> D0 K*0 decay, with the D0 decaying into Kpi, KK, pipi is presented. The selection efficiencies are used to estimate the statistical error for determining the CKM phase applying a combination of the GLW and ADS methods

Extraction of Technetium by Tri-n-octyl Amine Impregnated Resin

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Sorption of Technetium on Activated Carbon

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Optical vortices of slow light using tripod scheme

We consider propagation, storing and retrieval of slow light (probe beam) in a resonant atomic medium illuminated by two control laser beams of larger intensity. The probe and two control beams act on atoms in a tripod configuration of the light-matter coupling. The first control beam is allowed to have an orbital angular momentum (OAM). Application of the second vortex-free control laser ensures the adiabatic (lossles) propagation of the probe beam at the vortex core where the intensity of the first control laser goes to zero. Storing and release of the probe beam is accomplished by switching off and on the control laser beams leading to the transfer of the optical vortex from the first control beam to the regenerated probe field. A part of the stored probe beam remains frozen in the medium in the form of atomic spin excitations, the number of which increases with increasing the intensity of the second control laser. We analyse such losses in the regenerated probe beam and provide conditions for the optical vortex of the control beam to be transferred efficiently to the restored probe beam.Comment: 2 figure