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Titlebook: Oxygen Transport to Tissue XXIX; Kyung A. Kang,David K. Harrison,Duane F. Bruley Conference proceedings 2008 The Editor(s) (if applicable)

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Mahmood Khan,Vijay Kumar Kutala,Sheik Wisel,Simi M. Chacko,M. Lakshmi Kuppusamy,Pawel Kwiatkowski,Pelectronic dynamics on atomic length scales tends to unfold within tens to thousands of attoseconds (1 as = 10. s). Recent breakthroughs in laser science are now opening the door to watching and controlling these hitherto inaccessible microscopic dynamics. The key to accessing the attosecond time dom
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David F. Wilson,William M.F. Lee,Sosina Makonnen,Sophia Apreleva,Sergei A. Vinogradovodologies presented.Invited chapters by leading research exptransconductance e?ciency of all critical devices in order to reduce the n- essary bias current. However, reducing the current density also results in a severely decreased device f . An optimization of the current density is re- T quired to
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a severely decreased device f . An optimization of the current density is re- T quired to provide the correct balance between transconductance e?ciency and bandwidth. Plots such as Figure 2. 1 are useful tools for designers when choosing appropriate transistor bias points. Technology scaling allows
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Ganesh R. Sharma,Bruce Gerlitz,David T. Berg,Martin S. Cramer,Joseph A. Jakubowski,Elizabeth J. Galb a severely decreased device f . An optimization of the current density is re- T quired to provide the correct balance between transconductance e?ciency and bandwidth. Plots such as Figure 2. 1 are useful tools for designers when choosing appropriate transistor bias points. Technology scaling allows
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Samim Rezania,Kyung A. Kang a severely decreased device f . An optimization of the current density is re- T quired to provide the correct balance between transconductance e?ciency and bandwidth. Plots such as Figure 2. 1 are useful tools for designers when choosing appropriate transistor bias points. Technology scaling allows
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