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Advisory Board Elon Eisenberg, MD Neurology Israel James R. Fricton, DDS, MS Dentistry, Orofacial Pain USA Maria Adele Giamberardino, MD Internal Medicine, Physiology Italy Cynthia R. Goh, MB BS, FRCP, PhD Palliative Medicine Singapore Alejandro R. Jadad, MD, PhD Anesthesiology, Evidence-Based Medicine and Consumer Issues Canada Andrzej W. Lipkowski, PhD, DSc Neuropharmacology and Peptide Chemi...
Sunday 2/13/05 15 24 60 29 64 24 –6.7% 16.7% Monday 2/14/05 18 65 80 78 78 88 2.5% –12.8% Tuesday 2/15/05 17 75 80 90 78 104 2.5% –15.6% Wednesday 2/16/05 15 82 60 98 68 112 –13.3% –13.8% Thursday 2/17/05 18 74 80 89 90 88 –12.5% 0.9% Friday 2/18/05 14 89 60 107 56 100 6.7% 6.4% Saturday 2/19/05 10 40 48 48 48 48 0.0% 0.0% Sunday 2/20/05 15 26 60 31 65 24 –8.3% 23.1% Monday 2/21/05 19 78 80 94 ...
2:30 p.m. 2:45 p.m. OF MICE, MEN AND PIGS: LOSS OF CFTR PRODUCES ABNORMAL TRACHEAL DEVELOPMENT D.K. Meyerholz, S. Ramachandran, D.A. Stoltz, M.J. Welsh, and P.B. McCray, Jr. Departments of Pathology, Pediatrics, Internal Medicine, Molecular Physiology and Biophysics, and Howard Hughes Medical Institute, Roy Carver College of Medicine, University of Iowa, Iowa City, IA Keyword: Respiratory Syste...
Resonant annihilation of ultra-high energy cosmic neutrinos (UHECν) on the cosmic neutrino background (CνB) into Z bosons—the Z-burst mechanism—and its associated absorption and emission phenomenology provide a unique, albeit indirect, probe of the CνB in its present state. In this paper, we examine the implications of gravitational clustering of the CνB in nearby galaxy clusters for the Z-burs...
The paper contains a proposal for an energy and time representation. We construct modes that correspond to fuzzy distributions around discrete values of energy or time. The modes form an orthogonal and complete set in the space of square integrable functions. Energy and time are self adjoint in the space spanned by the modes. The widths of the modes are analyzed as well as their energy-time unc...
Use qij to denote the (i; j)-entry of the matrix Q (i; j = 1; 2). Then (Q) reads as (Q) = 0(1 + p 05)r 0 2 0(2 0 p 05)r + (1 + p 05) 2r + (1 0 p 05) 0(1 + p 05)r 0 2 (2) where r = (01+ p 05)q 11 0(2+ p 05)q 12 +2q 21 + (01+ p 05)q 22 : (3) Because any stabilizing controller can be obtained from the (2, 1)-and (2, 2)-entries of (2), we are interested in the set of r's of (3), that is, the ideal ...
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