Isotope Shift in the Dielectronic Recombination of Three-Electron ^ANd⁵⁷⁺

<p>Isotope shifts in dielectronic recombination spectra were studied for Li-like <sup style="margin: 0px; padding: 0px; border: 0px; font-size: 0.88em; vertical-align: 0.5em; line-height: 1em; color: rgb(50, 50, 50); font-family: arial, helvetica, sans-serif; text-align: justify; background-color: rgb(255, 255, 255);"><em>A</em></sup>Nd<sup style="margin: 0px; padding: 0px; border: 0px; font-size: 0.88em; vertical-align: 0.5em; line-height: 1em; color: rgb(50, 50, 50); font-family: arial, helvetica, sans-serif; text-align: justify; background-color: rgb(255, 255, 255);">57+</sup> ions with <em>A</em>=142 and <em>A</em>=150. From the displacement of resonance positions energy shifts <em>d</em><em>E</em><sup style="margin: 0px; padding: 0px; border: 0px; font-size: 0.88em; vertical-align: 0.5em; line-height: 1em; color: rgb(50, 50, 50); font-family: arial, helvetica, sans-serif; text-align: justify; background-color: rgb(255, 255, 255);">142?150</sup>(2<em>s</em>-2<em>p</em><sub style="margin: 0px; padding: 0px; border: 0px; color: rgb(50, 50, 50); font-family: arial, helvetica, sans-serif; line-height: 18px; text-align: justify; background-color: rgb(255, 255, 255);">1/2</sub>)=40.2(3)(6)??meV [(stat)(sys)] and <em>d</em><em>E</em><sup style="margin: 0px; padding: 0px; border: 0px; font-size: 0.88em; vertical-align: 0.5em; line-height: 1em; color: rgb(50, 50, 50); font-family: arial, helvetica, sans-serif; text-align: justify; background-color: rgb(255, 255, 255);">142?150</sup>(2<em>s</em>-2<em>p</em><sub style="margin: 0px; padding: 0px; border: 0px; color: rgb(50, 50, 50); font-family: arial, helvetica, sans-serif; line-height: 18px; text-align: justify; background-color: rgb(255, 255, 255);">3/2</sub>)=42.3(12)(20)??meV of 2<em>s</em>-2<em>p</em><sub style="margin: 0px; padding: 0px; border: 0px; color: rgb(50, 50, 50); font-family: arial, helvetica, sans-serif; line-height: 18px; text-align: justify; background-color: rgb(255, 255, 255);"><em>j</em></sub>transitions were deduced. An evaluation of these values within a full QED treatment yields a change in the mean-square charge radius of <sup style="margin: 0px; padding: 0px; border: 0px; font-size: 0.88em; vertical-align: 0.5em; line-height: 1em; color: rgb(50, 50, 50); font-family: arial, helvetica, sans-serif; text-align: justify; background-color: rgb(255, 255, 255);">142?150</sup><em>d</em>?<em>r</em><sup style="margin: 0px; padding: 0px; border: 0px; font-size: 0.88em; vertical-align: 0.5em; line-height: 1em; color: rgb(50, 50, 50); font-family: arial, helvetica, sans-serif; text-align: justify; background-color: rgb(255, 255, 255);">2</sup>?=-1.36(1)(3)??fm<sup style="margin: 0px; padding: 0px; border: 0px; font-size: 0.88em; vertical-align: 0.5em; line-height: 1em; color: rgb(50, 50, 50); font-family: arial, helvetica, sans-serif; text-align: justify; background-color: rgb(255, 255, 255);">2</sup>. The approach is conceptually new and combines the advantage of a simple atomic structure with high sensitivity to nuclear size.</p>

Thomson Scattering as a Diagnostic of Second-Harmonic Nd:YAG-Laser-Ablated Mg Plasma Plume

Thomson scattering is one of the most powerful diagnostic tools for plasma characterization, and it has been applied to a variety of plasmas. It is a nonintrusive technique, and the interpretation of the signal is relatively simple. However, this method has not been widely applied to low-temperature laser-ablated plasmas. Raman satellites have been observed in the scattering spectrum from a Mg laser-ablated plasma, giving this diagnostic the potential to be also used in density quantification of metastable states in plasmas.

High-gain x-ray lasing at 11.1 nm in sodiumlike copper driven by a 20-J, 2-ps Nd:glass laser

Evidence of high gain pumped by recombination has been observed in the 5g-4f transition at 11.1 nn in sodiumlike copper ions with use of a 20-J 2-ps Nd:glass laser system. The time- and space-integrated gain coefficient was 8.8 +/- 1.4 cm(-1), indicating a single-transit amplification of similar to 60 times. This experiment has shown that 2 ps is the optimum pulse duration to drive the sodiumlike copper recombination x-ray lasing at 11.1 nm. (C) 1996 Optical Society of America

Sr-Nd-Pb Isotope Evidence for Ice-Sheet Presence on Southern Greenland During the Last Interglacial

To ascertain the response of the southern Greenland Ice Sheet (GIS) to a boreal summer climate warmer than at present, we explored whether southern Greenland was deglaciated during the Last Interglacial (LIG), using the Sr-Nd-Pb isotope ratios of silt-sized sediment discharged from southern Greenland. Our isotope data indicate that no single southern Greenland geologic terrane was completely deglaciated during the LIG, similar to the Holocene. Differences in sediment sources during the LIG relative to the early Holocene denote, however, greater southern GIS retreat during the LIG. These results allow the evaluation of a suite of GIS models and are consistent with a GIS contribution of 1.6 to 2.2 meters to the =4-meter LIG sea-level highstand, requiring a significant sea-level contribution from the Antarctic Ice Sheet.

Book Review - <i>An Architecture of Parts: Architects, Building Workers and Industrialisation in Britain 1940–1970 </i>by Christine Wall <i>a</i>nd <i>Architecture and the Welfare State</i>, edited by Mark Swenarton, Tom Avermaete and Dirk van den Heuvel.

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