| Sample search results for: aart-jriado jri lehtsaar |
| 1 | Our research Mechanical Engineering at Heriot-Watt University is one of the largest departments devoted to this subject in Scotland, and | ||
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Summary: ) in Engineering, which has provided an investment of£13M across the 3 ERP Joint Research Institutes (JRI) that we... : l JRI in Signal and Image Processing l JRI in Integrated Systems l JRI in Energy and l the James |
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Source: Greenaway, Alan - Department of Physics, Heriot-Watt University |
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Collection: Engineering ; Physics |
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| 2 | Copyright 2009 by the Genetics Society of America DOI: 10.1534/genetics.108.099663 | ||
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Summary: sequenced to confirm the point mutation and transformed into the sir1TLEU2 strain (JRY4621). S. cerevisiae... . cerevisiae sir1 strain (JRY4621) was transformed with pRS316 with S. cerevisiae SIR1-HA (pJR2793- 7... ) Genotype JRY4621 S. cerevisiae MATa sir1TLEU2 can1-100, his3-111 leu2-3,112, lys2D, trp1-1, ura3-1 CBS7001 |
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Source: Wolfe, Kenneth H. - Genetics Department, Trinity College, University of Dublin |
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Collection: Biotechnology ; Environmental Sciences and Ecology |
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| 3 | Vol. 9, No. 12MOLECULAR AND CELLULAR BIOLOGY, Dec. 1989, p. 5702-5712 0270-7306/89/125702-11$02.00/0 | ||
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Summary: disruption mutation into JRY438 by one-step gene disruption methods (46). The predicted structure... of the disrupted HEM) locus in the resulting strain, JRY1236, was confirmed after disruption by a gel transfer... ;TRANSCRIPTIONAL CONTROL BY HEME 5703 TABLE 1. Strains used Straina Genotype lacZ fusionb JRY438 a his4-519 leu2 |
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Source: Schafer, William R. - Laboratory of Molecular Biology, MRC |
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Collection: Biology and Medicine |
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| 4 | Vol. 9, No. 12MOLECULAR AND CELLULAR BIOLOGY, Dec. 1989, p. 5702-5712 0270-7306/89/125702-11$02.00/0 | ||
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Summary: disruption mutation into JRY438 by one-step gene disruption methods (46). The predicted structure... of the disrupted HEM) locus in the resulting strain, JRY1236, was confirmed after disruption by a gel transfer... lacZ fusionb JRY438 a his4-519 leu2-3,112 ura3-52 None JRY527 a his3A200 lys2-801 ade2-101 met ... |
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Source: Schafer, William R. - Laboratory of Molecular Biology, MRC |
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Collection: Biology and Medicine |
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| 5 | | Proc. of the VII Conf. on Diff. Geom and A* | Brno (1998), 469-480; EMS server http://www.e* | ||
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Summary: : Y ! X , with dim X = n and dim Y = n +* * m. For r 0 we are concerned with the r-jet space JrY... ; in particular, we set * *J0Y Y . We recall the natural fiberings ssrs: JrY ! JsY , r s, ssr : JrY ! X... for multi* *-indices. The charts induced on JrY are denoted by (x~, yiff), with ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 6 | Proc. of the VII Conf. on Diff. Geom and Appl., Brno (1998), 469480; EMS server http://www.emis.de. | ||
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Summary: with the rjet space JrY ; in particular, we set J0Y Y . We recall the natural fiberings r s : JrY JsY , r... s, r : JrY X, and, among these, the affine fiberings r r-1. We denote with V Y the vector subbundle... convention will be adopted also for multiindices. The charts induced on JrY are denoted ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 7 | 02 March 201002 March 2010 School of EngineeringSchool of Engineering | ||
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Summary: of sensorssensors #12;02 March 201002 March 2010 School of EngineeringSchool of Engineering 99 JRI EPSRC Project:JRI... EPSRC Project: Adaptive Hardware SystemsAdaptive Hardware Systems EPSRC project involving SIP JRI, plus... other researchers fromEPSRC project involving SIP JRI, plus other researchers from ... |
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Source: Edinburgh, University of - Division of Informatics, Institute for Adaptive and Neural Computation |
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Collection: Computer Technologies and Information Sciences |
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| 8 | Graduate School in Information and Communication Technologies. Experiences at Tallinn University of Technology | ||
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Summary: to Strengthen Doc- toral Studies in Estonia." V. Puura, T. Lehtsaar, A. Kärner (Eds.), Tartu Uni- versity, 2004 |
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Source: Kruus, Margus - Faculty of Information Technology, Tallinn University of Technology |
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Collection: Computer Technologies and Information Sciences |
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| 9 | Perron-Frobenius theorem for nonnegative multilinear forms and extensions | ||
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Summary: . Illinois at Chicago JRI workshop on eigenvalues of nonnegative tensors 18 December, 2010, Hong-Kong Shmuel... and extensions JRI workshop on eigenvalues of nonnegative t / 22 #12;Overview 1 Perron-Frobenius theorem... and extensions JRI workshop on eigenvalues of nonnegative t / 22 #12;Nonnegative irreducible and primitive |
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Source: Friedland, Shmuel - Department of Mathematics, Statistics, and Computer Science, University of Illinois at Chicago |
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Collection: Mathematics |
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| 10 | To appear in Math. Proc. Cambridge Philos. Soc.. | ||
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Summary: are concerned with the rjet space JrY ; in particular, we set J0Y = Y . We recall the canonical fibrings r... s : JrY JsY , s r, r : JrY X. We denote multi- indices of range m by Greek letters such as = (1... +· · ·+m and ! := 1! . . . m!. The induced charts on JrY are denoted by (xi , yp ), with 0 ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 11 | The University of Oklahoma Hourly Time Record. The time category codes are ordered alphabetically from left to right. (updated 01/05/06) Last Name: First Name: MI: EMPLID: FTE: Student | ||
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Summary: . CPT Comp. Time Taken ESL Extended Sick Leave FML FMLA W/ Pay FMN FMLA W/O Pay HOL Holiday Hours JRY... Extended Sick Leave FML FMLA W/ Pay FMN FMLA W/O Pay HOL Holiday Hours JRY Jury Leave MIL Military Leave |
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Source: Xue, Ming - School of Meteorology, University of Oklahoma |
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Collection: Geosciences |
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| 12 | Yeast PAS kinase coordinates glucose partitioning in response to metabolic and cell integrity | ||
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Summary: in fractions of crude yeast extracts separated by MonoQ. Wild-type cells (JRY 245) were treated... to activate PAS kinase. The wild-type strain (JRY245) containing either pRS426 (vector) or pRS426-WSC1 (WSC1... lacking uracil, and incubated at 371C for 3 days. The strains used were JRY245 (wild type þ pRS416), ... |
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Source: Rutter, Jared - Department of Biochemistry, University of Utah |
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Collection: Biology and Medicine |
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| 13 | Published in Arch. Math. (Brno), | ||
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Summary: . Moreover, for 0 r, we are concerned with the rth jet space JrY ; in particular, we set J0Y Y . We recall... the natural fibrings r s : JrY JsY and r : JrY X for 0 s r. A detailed account of the theory of jets can... and µ = 0 if µ = . We also set |p| := p1 + · · · + pn and p! := p1! . . . pn!. The charts induced ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 14 | | Published in * | Arch. Math. (Brno), * | ||
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Summary: ! Y . Moreover, for 0 r, we are concerned with the r-th jet space JrY ; in part* *icular, we set J... 0Y Y . We recall the natural fibrings ssrs: JrY ! JsY and ssr : Jr* *Y ! X for 0 s r... on JrY are denoted by (x0; yip_), with 0 |p_| r; in particular, if |p_| = 0, then * *we set yi0 |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 15 | Diff. Geom. Appl. 22, n. 1 (2005), 105120 | ||
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Summary: . 2.1 Jet spaces For r 0 we are concerned with the rjet space JrY . This space is defined as the set... projections r s : JrY JsY , r s, sending r-th equivalent sections into s-th equivalent sections. Moreover... , there are obvious natural projections r : JrY X. The spaces JrY are endowed with a ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 16 | | Published in | | Math. Proc. Cambridge Philos. Soc.* | ||
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Summary: -jet space JrY ; in particular, we set J0Y Y . We recall the natural fibrings ssrs: JrY ! JsY , ssr : JrY... set |p_| := p1 + . .+.pn and p_! := p1! . .p.n!. The charts induced on JrY are denoted by (x0... to a section jrs : X ! JrY , with coordinate expression (jrs)ip_= ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 17 | Published in Math. Proc. Cambridge Philos. Soc., | ||
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Summary: jet space JrY ; in particular, we set J0Y Y . We recall the natural fibrings r s : JrY JsY , r : JrY X... !. The charts induced on JrY are denoted by (x0 , yi p), with 0 |p| r; in particular, we set yi 0 yi... . A section s : X Y can be prolonged to a section jrs : X JrY , with ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 18 | | Proc. VI Int. Conf. Diff. Geom* | Brno (1995), 487-494; * | ||
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Summary: by an adapted char* *t. The fibred manifold Y ! X yields in a natural way the jet manifolds JrY... . Let us set J0Y := Y , and r; s 2 N; r ~ s. We have the* * fibrings ssrs: JrY ! JsY and ssr : JrY... ; : :.:We have the adapted charts (x0; yip_) on JrY , with p_~ r (we have set * *yi0_:=yi |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 19 | Proc. VI Int. Conf. Diff. Geom. Appl., Brno (1995), 487494; | ||
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Summary: manifold Y X yields in a natural way the jet manifolds JrY . A detailed account of the theory of jets can... , and r, s N, r s. We have the fibrings r s : JrY JsY and r : JrY X. Onedimensional multi... indexes will be denoted by underlined latin letters p N, q N, . . . . We have the adapted charts (x0 , yi p) on ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 20 | followed by an additional 10 hours with a 120-s switch interval at 2C. | ||
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Summary: such that in vivo recombination would restore plas- mid-borne copies of ORC5. In one screen, an orc5-1 strain (JRY... by directly transforming the orc5 strain (JRY4154) with the mutagenic PCR reaction and the gapped plasmid... . Dillin and J. Rine, Genetics 147, 1053 (1997). 35. Strains used were as follows: JRY2334 (MATa ade2-1 ... |
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Source: Spies, Thomas - Basic Sciences Division, Fred Hutchinson Cancer Research Center |
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Collection: Biology and Medicine |
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| 21 | | Diff. Geom. Appl. * | 22, n. 1 (2005), 105-12* | ||
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Summary: . 2.1 Jet spaces For r 0 we are concerned with the r-jet space JrY . This space is defined... sections into s-th equivalent sections. Moreover, there are obvious natural pro* *jections ssr: JrY ! X... . The spaces JrY are endowed with a differentiable structure mak* *ing ssrs fiber bundles. Among these |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 22 | | To appear in * | Math. Proc. Cambridge Philos. * | ||
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Summary: are concerned with the r-jet space JrY ; in particular, we set* * J0Y = Y . We recall the canonical fibrings... ssrs:JrY ! JsY , s ~ r, ssr: JrY ! X. We denot* *e multi- indices of range m by Greek letters... otherwise. We set jffj :=ff1+ + * *ffm and ff! :=ff1! . .f.fm !. The induced charts on JrY are denoted |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 23 | Quantum Lower Bounds for Fanout M. Fang S. Fenner y F. Green z S. Homer Y. Zhang y | ||
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Summary: 2 k bits such that for any state jRi in the quotient space of B n complementary to j k i, the state... L 1 L 2 #1; #1; #1; L k (jRi j k i) has a 0 in the target position of C. Proof: The proof... 0 1 acts on the quotient space R complementary to j 1 i. No matter what state jRi 2 R we choose |
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Source: Boston University, Department of Computer Science |
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Collection: Computer Technologies and Information Sciences |
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| 24 | | Published in | | Rend. Circ. Mat. Palermo (2) Supp* | ||
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Summary: results on the geometry of spaces * *of jets JrY of a fibration Y ! X . We recall that the tangent... space T JrY has a nat* *ural splitting when pulled back to the higher order jet space Jr+1Y . Namely... * *rphic to T X . Then, we introduce horizontalization as the projection of forms on JrY , * *or r |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 25 | Published in Czechoslovak Math. J. | ||
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Summary: and dim Y = n + m. For r 0 we are concerned with the rjet space JrY ; in particular, we set J0Y Y . We... recall the natural fiberings r s : JrY JsY , r s, r : JrY X, and, among #12;M. Francaviglia, M. Palese... on JrY are denoted by (x , yi ), with 0 || r; in partic- ular, we set yi 0 yi . The ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 26 | | Published in * | Differential Geom. Ap* | ||
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Summary: and the vertical bundle V Y := kerT ss ! Y . Moreover, for 0 r, we are concerned with the r-th jet space JrY... ; in parti* *cular, we set J0Y Y . We recall the natural fibrings ssrs: JrY ! Js... Y , ssr : JrY ! X , and the affine bundle ssrr 1: ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 27 | Published in Differential Geom. Appl., | ||
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Summary: space JrY ; in particular, we set J0Y Y . We recall the natural fibrings r s : JrY JsY , r : JrY X... , and the affine bundle r r-1 : JrY Jr-1Y associated with the vector bundle r T X Jr-1Y V Y Jr-1Y , for 0 s r... |p| := p1 + · · · + pn and p! := p1! . . . pn!. The charts induced on ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 28 | Published in Rend. Circ. Mat. Palermo (2) Suppl., | ||
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Summary: of jets JrY of a fibration Y X. We recall that the tangent space TJrY has a natural splitting when pulled... as the projection of forms on JrY , or rth order forms, on forms on Jr+1Y having the highest exterior factor k T X... sequence on JrY is produced by taking the quotient of de Rham sequence on JrY ... |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 29 | Control and Estimation of the Boundary Heat Transfer Function in Stefan Problems | ||
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Summary: \Deltayj 2 )dx dt + Z \Omega T n\Omega 0 jry(x; oe(x))j 2 dx + Z \Omega T ( 1 2 y 2 t (x; T ) + jry(x; T )j 2... )dx + 2 Z \Gamma j(y(x; T ))doe x + Z \Sigma j(y)doe x dt (2.3) Z \Omega T ( 1 2 y 2 0 (x) + jry 0... ], Section 3. If one takes z = y '' \Gamma (y '' ) + in (2.5) one obtains ''j((y '' ) + ) t j 2 L 2 (Q) + ... |
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Source: Ring, Wolfgang - Institut für Mathematik und Wissenschaftliches Rechnen, Karl-Franzens-Universität Graz |
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Collection: Mathematics |
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| 30 | October 14, 2011(j~] Math 108 -Practice Quiz 18 | ||
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Summary: -d (f) f (,): _'-.r: 1 J I r · ':' .r,,? ::L) G"'~ 2.. T -r (ir)::. ~('(~~",JI-It- J-rY,~" ~{ . (IV |
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Source: Singman, David - Department of Mathematical Sciences, George Mason University |
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Collection: Mathematics |
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| 31 | B. Klshammer Ausgabe: 24.05.06 M. Mller Abgabe: 30.05.06 | ||
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Summary: Nullelement). (ii) Für jede Familie (Ri)iI von Ringen ist J( iI Ri) = iI J(Ri). (iii) Es gibt einen Ring R |
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Source: Friedrich-Schiller-Universität Jena, Mathematisches Institut, Lehrstuhl für Algebra und Zahlentheorie |
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Collection: Mathematics |
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| 32 | Continuing Dental Education, School of Dentistry Faculty of Medicine and Dentistry | ||
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Summary: . Director, Continuing Dental Education JRY/jw #12; |
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Source: MacMillan, Andrew - Department of Biochemistry, University of Alberta |
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Collection: Chemistry ; Biology and Medicine |
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| 33 | March 1, 2006 Dear Dental Staff | ||
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Summary: James R. Yacyshyn, BSc, DDS, MASc Director, Continuing Dental Education JRY/dg #12; |
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Source: MacMillan, Andrew - Department of Biochemistry, University of Alberta |
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Collection: Chemistry ; Biology and Medicine |
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| 34 | Image Registration, Optical Flow and Local Rigidity | ||
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Summary: ) if Jac(f \Lambda ) is symmetric, then (9) means that if jrI 1 j 6= 0, ffl direction j = rI 1 jrI 1 j... is eigenvector ( = det(Jac(f) is an eigenvalue); ffl direction ¸ = rI ? 1 jrI 1 j is ``rigid'' ( = 1... ), then we have: k\Pi oe (I 1 \Gamma I 2 ) \Gamma P I1 oe (h \Lambda )k L 2 ß 2 oe d+2 kh \Lambda ... |
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Source: Cohen, Laurent - Centre De Recherche en Mathématiques de la Décision, Université Paris-Dauphine |
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Collection: Mathematics |
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| 35 | UNCORRECTEDPROOF 2 Multilevel summation and Monte Carlo simulations | ||
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Summary: -range interaction 8 9 The energy U of a system of N point particles is given by UN ¼ 1 2 XN ipj qid G jri -rj j À... the location of the i-th particle. The interparticle interactions are 13 defined by the kernel G jri -rj j À... is defined by Uloc ¼ 1 2 XN ipj qid Gloc jri -rj j À Á d qj: ð6Þ 373839If rcut is ... |
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Source: |
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Collection: Computer Technologies and Information Sciences |
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| 36 | Control and Estimation of the Boundary Heat Transfer Function in Stefan Problems | ||
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Summary: T n 0 jryx; xj2dx + Z T 1 2y2 t x;T+ jryx;Tj2dx + 2 Z , jyx;Td x + Z jyd xdt 2.3 Z T 1 2y2 0x+ jry0... .5 one obtains "jy"+tj2 L2Q + jry"+j2 L2Q + 1 2jy"+;Tj2 L2 T + 1 2jy"+;0j2 L2 0 , Z 0 y0 y"+x;0dx + Z... . Next, for z = 0 in 2.5 we obtain 7 #12;"jy" tj2 L2Q + jry"j2 L2Q + 1 2jy";Tj2 L2 T + Z jy"d xdt 1 2 |
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Source: Ring, Wolfgang - Institut für Mathematik und Wissenschaftliches Rechnen, Karl-Franzens-Universität Graz |
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Collection: Mathematics |
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| 37 | Molecular Cell Regulation of Glucose Partitioning | ||
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Summary: . The Psk Proteins Phosphorylate Ugp1 at Ser11 In Vivo (A) BHY10 (PSK1 PSK2) and JRY40 (psk1 psk2) strains... antibody (bottom panel). (B) BHY10, JRY40, JRY232, and JRY234 (genotypes as indicated) were grown... - ity was then assayed as described (n = 3). (B) BHY10, JRY40, ... |
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Source: Rutter, Jared - Department of Biochemistry, University of Utah |
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Collection: Biology and Medicine |
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| 38 | Image Registration, Optical Flow and Local Martin Lef'ebure 1 and Laurent D. Cohen 2 | ||
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Summary: if dimension d is 1; 2. suppose d = 2: then, 3. if Jac(f \Lambda ) is symmetric, then (6) means that if jrI 1 j... 6= 0, -- direction j = rI1 jrI1 j is eigenvector ( = det(Jac(f) is an eigenvalue); -- direction... ¸ = rI ? 1 jrI1 j is ``rigid'' ( = 1 is an eigenvalue); then for all x 2 D where I 1 is not locally |
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Source: Cohen, Laurent - Centre De Recherche en Mathématiques de la Décision, Université Paris-Dauphine |
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Collection: Mathematics |
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| 39 | ESI The Erwin Schrodinger International Boltzmanngasse 9 Institute for Mathematical Physics A-1090 Wien, Austria | ||
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Summary: , is called a (nonlinear) resolvent of f. It is clearly nonexpansive, that is, 1-Lipschitz: |Jrx - Jry| |x... - y|, x, y C. (1.8) As a matter of fact, this resolvent is even firmly nonexpansive: |Jrx - Jry| Jrx... - Jry + s x - Jrx - (y - Jry) (1.9) for all x and y in C and for all positive s. 2 #12;This ... |
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Source: Pottmann, Helmut - Institut für Diskrete Mathematik und Geometrie, Technische Universität Wien |
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Collection: Mathematics |
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| 40 | | Published in * | Czechoslovak Math* | ||
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Summary: Y * * = n + m. For r ~ 0 we are concerned with the r-jet space JrY ; in particular, we set... * *J0Y j Y . We recall the natural fiberings ssrs: JrY ! JsY , r ~ s, ssr : JrY ! X , and... ! :=ff1! . .f.fn!. The charts induced on JrY are denoted by (x~, yiff), with 0 ~ jffj ~ r |
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Source: Vitolo, Raffaele - Dipartimento di Matematica, Università di Lecce |
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Collection: Mathematics |
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| 41 | Please cite this article in press as: Lampton, P.W., et al., The role of tapasin in MHC class I protein trafficking in embryos and T cells, J. Reprod. Immunol. (2007), doi:10.1016/j.jri.2007.10.003 | ||
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Summary: protein trafficking in embryos and T cells, J. Reprod. Immunol. (2007), doi:10.1016/j.jri.2007... .10.003 ARTICLE IN PRESS+Model JRI-1744; No.of Pages12 Journal of Reproductive Immunology xxx (2007) xxx... Elsevier Ireland Ltd. All rights reserved. doi:10.1016/j.jri.2007.10.003 #12;Please cite this article |
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Source: Warner, Carol M. - Department of Biology, Northeastern University |
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Collection: Biology and Medicine |
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| 42 | JSS Journal of Statistical Software MMMMMM YYYY, Volume VV, Issue II. http://www.jstatsoft.org/ | ||
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Summary: likelihood L() = m i=1 e xj(i) jRi exj #12;2 Fitting the Penalized Cox Model via Coordinate Descent where... /censoring time. We wish to find which maximizes L() = m i=1 e xj(i) jRi exj subject to our constraint: |i... likelihood, 2 n () = 2 n m i=1 xj(i) - log jRi exj We scale by a factor of 2/n for convenience |
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Source: Tibshirani, Robeert - Department of Statistics, Stanford University |
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Collection: Mathematics |
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| 43 | JSS Journal of Statistical Software March 2011, Volume 39, Issue 5. http://www.jstatsoft.org/ | ||
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Summary: likelihood L() = m i=1 e xj(i) jRi exj #12;2 Fitting the Penalized Cox Model via Coordinate Descent where... e xj(i) jRi exj subject to our constraint: |i| + (1 - ) 2 i c. Maximizing the partial likelihood... is equivalent to maximizing a scaled log partial likelihood, 2 n () = 2 n m i=1 xj(i) - log jRi exj We |
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Source: Hastie, Trevor - Department of Statistics, Stanford University |
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Collection: Mathematics |
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| 44 | On small perturbations of stable Markov operators: unbounded case | ||
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Summary: ; where Q j = r Y i=1 (I \Gamma flY jr+i Y T jr+i ): Note that jQ j j p = fi fi fi fi fi I \Gamma fl r X i... =1 Y jr+i Y T jr+i + ::: + (\Gamma1) r fl r r Y i=1 Y jr+i Y T jr+i fi fi fi fi fi p fi fi fi fi fi... I \Gamma fl r X i=1 Y jr+i Y T ... |
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Source: Delyon, Bernard - Institut de Recherche Mathématique de Rennes, Université de Rennes |
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Collection: Mathematics |
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| 45 | B. K"ulshammer 19.11* Ringtheorie | ||
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Summary: ). (ii)F"ur jede Familie (Ri)i2Ivon Ringen ist J( Ri) = J(Ri |
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Source: Friedrich-Schiller-Universität Jena, Mathematisches Institut, Lehrstuhl für Algebra und Zahlentheorie |
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Collection: Mathematics |
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| 46 | ESI The Erwin Schrodinger International Pasteurgasse 6/7 Institute for Mathematical Physics A-1090 Wien, Austria | ||
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Summary: ;ri A rn?i A ] + rn A ; ]; ]; (3.7) @tjrn A j2 jrn A j2 ?jrn+1 A j2 + Cjrn A j nX i=0 jri A jjrn?i A j... + 1) r @run + (n + 1)(n + 2) r2 un + Cj jun + C n?1X i=1 (ri+ 1 2 jri A j)(rn?i+ 1 2 jrn?i A j): Using... .16) where gn = C Pn?1 i=1 (ri+ 1 2 jri A j)(rn?i+ 1 2 jrn?i A j). For any 0 < " < R, let (r) be a non |
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Source: Pottmann, Helmut - Institut für Diskrete Mathematik und Geometrie, Technische Universität Wien |
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Collection: Mathematics |
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| 47 | Physics 0551 Lecture #10 Title: Lattice vibrations of a monoatomic lattice. | ||
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Summary: ). Using a Taylor series expansion: V (ri r0) = V (0) + dV dri jri=r0 (ri r0)1 2 d2 V dr2 i jri=r0(ri r0... r0)2 >> (ri r0)3 . Thus V (ri r0) V (0) + 1 2 d2 V dr2 i jri=r0(ri r0)2 Note: The absolute |
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Source: Winokur, Michael - Department of Physics, University of Wisconsin at Madison |
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Collection: Physics |
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| 48 | Atomic and Molecular Quantum Theory Course Number: C561 25 The Independent particle approximation: Slater determi- | ||
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Summary: )2(r2) · · · i(rj) · · · j(ri) · · ·] (25.4) where in the second term we have just interchanged... ,j = Pi,j {[1(r1)2(r2) · · · i(ri) · · · j(rj) · · ·] - [1(r1)2(r2) · · · i(rj) · · · j(ri) · · ·]} = [1(r... 1)2(r2) · · · i(rj) · · · j(ri) · · ·] - [1(r1)2(r2) · · · i(ri) · · · j(rj) · · ... |
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Source: Iyengar, Srinivasan S. - Department of Chemistry, Indiana University |
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Collection: Chemistry |
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| 49 | Coherent Quantum Optical Control with Subwavelength Resolution Alexey V. Gorshkov,1 | ||
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Summary: . Destructive interference of excitation pathways from jgi and jri up to jei ensures that the so-called dark... state jdarkxi cxjgi ÿ jri= 2 cx 2 p is decoupled from both optical fields [7]. It is the sharp... jei corresponds to a cycling transition (this is pos- sible either if jri is above jei |
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Source: Lukin, Mikhail - Department of Physics, Harvard University |
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Collection: Materials Science ; Physics |
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| 50 | Programming Research Group OBFUSCATING SET REPRESENTATIONS | ||
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Summary: j = jry j, we would obtain hly ++ rz ; ry ++ (tail lz )i aSp We cannot simplify this expression any... further. However, we can use the fact that the lists are unordered so that, as jly j = jry j, the sets... + jry j | so it has linear complexity. The de#12;nition of insert aSp is: insert aSp a hl ; ri a |
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Source: Oxford, University of - Computing Laboratory, Programming Tools Group |
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Collection: Computer Technologies and Information Sciences |
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| 51 | Entanglement of Two Individual Neutral Atoms Using Rydberg Blockade T. Wilk, A. Gaetan, C. Evellin, J. Wolters, Y. Miroshnychenko, P. Grangier, and A. Browaeys | ||
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Summary: they are in a Rydberg state jri, atoms a and b interact strongly if they are close enough, and the doubly excited state... state jri (with Rabi frequency "r) cannot excite both atoms at the same time, provided... "i to jri and from jri to j#i. PRL 104, 010502 (2010) P H Y S I C A L R E V I E W L E T T E R S ... |
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Source: Grangier, Philippe - Quantum Optics Group, Institut d'Optique, Orsay |
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Collection: Physics |
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| 52 | Distributed Optimization for Cooperative Agents: Application to Formation Flight | ||
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Summary: ||2 2 + N i=1 jR(i) ||C(xi - xj) - yij||2 2 Subject to xi Di, i = 1, . . . , N (P1) B. Decentralized... + jR(i) 2(dij -dji)T Cxi }. 3. Each vehicle i sends (resp. receives) its (resp. their) optimal... , we introduce slack variables ~xi Rni , i = 1, . . . , N, as follows: Minimize N i=1 Ji + N i=1 jR(i |
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Source: Boyd, Stephen P.- Department of Electrical Engineering, Stanford University; Tomlin, Claire - Department of Electrical Engineering and Computer Sciences, University of California at Berkeley |
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Collection: Engineering |
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| 53 | Cell, Vol. 111, 1728, October 4, 2002, Copyright 2002 by Cell Press Coordinate Regulation of Sugar Flux | ||
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Summary: (JRY40 pRS416), psk2 single mutant (JRY10 pRS416), psk1 single mutant (JRY30 pRS416), double... a kinase- galactose (Boles et al., 1994; Masuda et al., 2001). In- inactivating mutation (JRY40 pRS416-PSK2... (JRY40 pRS416-PSK2 N792). JRY10 pRS416 phenotype by ... |
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Source: Rutter, Jared - Department of Biochemistry, University of Utah |
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Collection: Biology and Medicine |
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| 54 | Adhesion, Atomic Structure, and Bonding at theAdhesion, Atomic Structure, and Bonding at the ----AlAl22OO33(0001)/Al(111) Interface:(0001)/Al(111) Interface | ||
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Summary: r2 I ; 1 2 X i I ZI e2 jri ;RI j + 1 2 X i6=j e2 jri ;rj j + 1 2 X I6=J ZI ZJ e2 jRI ;RJ j #12 |
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Source: Adams, James B - Department of Chemical and Materials Engineering, Arizona State University |
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Collection: Materials Science |
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| 55 | Eects of columnar and point defects on magnetic hysteresis curves produced by three-dimensional vortices in | ||
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Summary: layer fvp i ) is given by fi;L XNv j1 f0K1 jri;L À rj;Lj k ^rij;L XNp;L k1 fp np jri;L À r p k... ;LjH np À jri;L À r p k;Lj k ! ^rik;L Aintf0jri;L À ri;LÀ1j^riid jri;L À ri;L1j^riiu: Fig. 1. A single... ±pinning unit vectors are, respectively, given by ^rij;L ri;L À rj;L ... |
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Source: Nori, Franco - Institute for Physical and Chemical Research, RIKEN &Department of Physics, University of Michigan |
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Collection: Physics ; Materials Science |
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| 56 | Advanced Statistical Mechanics: CHEM 646 Problem Set 3 | ||
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Summary: the molecules interact by pairwise additive poten- tials of the form: ui, j(ri, j, µi, µ j) , for ri, j |
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Source: Ronis, David M. - Department of Chemistry, McGill University |
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Collection: Physics |
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| 57 | M. Nielsen, P. Johansen, O.F. Olsen, J. Weickert (Eds.), Scale-Space Theories in Computer Vision, Lecture Notes in Computer Science, Springer, Berlin, Vol. 1682, | ||
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Summary: ) is a regularized projection matrix in the direction perpendicular of rI 1 : D (rI 1 ) = 1 jrI 1 j 2 + 2#21; 2 8... boundaries of I 1 where jrI 1 j >> #21;. This model, however, uses an optical ow constraint which... eigenvalues are given by #21; 1 (jrI 1 j) = #21; 2 jrI 1 j 2 + 2#21; 2 ; (9) #21; 2 ... |
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Source: Saarlandes, Universität des, Mathematical Image Analysis Group |
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Collection: Mathematics ; Computer Technologies and Information Sciences |
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| 58 | CMC 2003/04 School of Mathematics and Statistics | ||
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Summary: transformation. Given any two finite presentations hXjR(X) = 1i; hY jR(Y ) = 1i for a group G, prove that one can |
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Source: St Andrews, University of - School of Mathematics and Statistics, Centre for Interdisciplinary Research in Computational Algebra |
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Collection: Mathematics |
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| 59 | UNITED STATES DEPARTMENT OF COM"'ERCE Natlon_l Ocpnil; _nd Atrno:spn&ric Adm'nlatrlltlon | ||
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Summary: -.l rs lmplcmerlled inlcrim m~nagCm"l1( measures effcClil'c Jlll1l.1Jry I, 20Io. tlUl would benefit |
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Source: Southwest Fisheries Science Center, NOAA |
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Collection: Environmental Sciences and Ecology |
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| 60 | Dynamic Optimal Power Dispatch of Power Networks: from Game Theoretic Point of View | ||
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Summary: ,j (dj(k) - pj(k)) 2 (3) wD1,j J2 D = jD wD2,ju2 gj(k) (4) wD2,ij JR = iR JRi (5) JRi = wR,i ri... .1, . . . , ri} Ui (6) JRi i B ai Ai = {-li, 0, li} on-off Ui (8) JBi JBi bi b d r 1 G = (V , A, {Ui}iV , b, {Bi... = 0 i B #12;a = (a 1, . . . , a n) b (a , b ) G 2 Ri Bi JRi JBi J 4.2 i N ai, ai Ai Ui(ai, ... |
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Source: Fujita, Masayuki -- Department of Mechanical and Control Engineering, Tokyo Institute of Technology |
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Collection: Engineering |
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| 61 | IEEE JOURNAL OF SOLID-STATE CIRCUITS, VOL. 40, NO. 2, FEBRUARY 2005 559 Correspondence________________________________________________________________________ | ||
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Summary: " Jri Lee, Member, IEEE, and Behzad Razavi, Fellow, IEEE The first author of [1] has indicated |
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Source: Galton, Ian - Department of Electrical and Computer Engineering, University of California at San Diego |
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Collection: Engineering |
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| 62 | Online Submission ID: 134 Shape Matching based Real-time Simulation on Adaptive Lattice | ||
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Summary: , the following step is taken: · Evaluate mass center of the particles in Ri: ci = jRi {mjxj} jRi {mj} = jRi {mjxj... } Mi (2) · Calculate the best affine transform Ai: Ai = jRi mj(xj - cj)(x0 j - c0 j )T = jRi mjxjx0T j... - Micic0T i , (3) where c0 i = jRi mjx0 j ... |
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Source: Xuan, Dong - Department of Computer Science and Engineering, Ohio State University |
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Collection: Computer Technologies and Information Sciences |
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| 63 | Lifetime Data Anal (2007) 13:471480 DOI 10.1007/s10985-007-9048-y | ||
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Summary: ) jRi eT Z j (Ti ) i , 123 #12;Lifetime Data Anal (2007) 13:471480 473 where Ri = { j : Tj Ti... }. The corresponding score function is U() = n i=1 i Zi (Ti ) - jRi eT Z j (Ti ) Z j (Ti ) jRi eT Z j (Ti ) . (2... failure times, one can show that L(, 0) is maximized simultaneously at and 0(t) = n i=1 I (Ti t) i ... |
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Source: Lin, Danyu - Department of Biostatistics, University of North Carolina at Chapel Hill |
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Collection: Biology and Medicine |
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| 64 | Convergence of Dual Algorithm with Arbitrary Communication Richard J. La | ||
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Summary: d dt µl(t) = l iIl Di jri µj(t - (Tr i,j + Tf i,l)) - ql(µl(t)) l L . (23) The existence... (t))) iIl Di jri q-1 j (j(t - Tr i,j - Tf i,l)) - l(t) . (24) This can be put in the following matrix... + {}, is defined by Fl(~(t)) = iIl Di jri q-1 j (j(t - Tr i,j - Tf i,l)) , l L . (26) Note that Assumption 3 |
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Source: La, Richard J. - Institute for Systems Research & Department of Electrical and Computer Engineering, University of Maryland at College Park |
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Collection: Computer Technologies and Information Sciences |
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| 65 | Annu. Rev. Public Health. 1999. 20:14557 Copyright c 1999 by Annual Reviews. All rights reserved | ||
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Summary: score function U() = n i=1 i Zi (Xi ) - jRi e Z j (Xi ) Z j (Xi ) jRi e Z j (Xi ) , 2. where Ri... normal with covariance matrix I-1 ( ^), where I () = n i=1 i jRi e Z j (Xi ) Z j (Xi )Z j (Xi ) jRi e Z j... (Xi ) - jRi e Z j (Xi ) Z j (Xi ) jRi e Z j (Xi ) Z j (Xi ) ... |
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Source: Lin, Danyu - Department of Biostatistics, University of North Carolina at Chapel Hill |
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Collection: Biology and Medicine |
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| 66 | Generation of Hyperentangled Photon Pairs Julio T. Barreiro,1 | ||
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Summary: the horizontal (vertical) photon polarization; jli, jgi, and jri represent the paraxial spatial modes (Laguerre... into the orthogonal basis states (jli; jgi, and jri), as well as the superpositions jhi jli jri= 2 p and jvi jli ÿ... jri= 2 p ). The measured Bell parameters agreed (within 2) with ... |
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Source: Kwiat, Paul - Department of Physics, University of Illinois at Urbana-Champaign |
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Collection: Physics |
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| 67 | HOMELAND SECURITY @ Fall 2004ResearchHorizons12 and users were pleased with the | ||
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Summary: @ gtresearchnews.gatech.edu System (JRIES) if it joins this part- nership of law enforcement agencies. Through... JRIES, officials can request information on suspects and/or events. Pennywitt and his colleagues expect |
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Source: Sherrill, David - School of Chemistry and Biochemistry, Georgia Institute of Technology |
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Collection: Chemistry |
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| 68 | INVESTIGATION The Awesome Power of Yeast Evolutionary | ||
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Summary: @ gtresearchnews.gatech.edu System (JRIES) if it joins this part- nership of law enforcement agencies. Through... JRIES, officials can request information on suspects and/or events. Pennywitt and his colleagues expect |
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Source: Dunham, Maitreya - Department of Genome Sciences, University of Washington at Seattle; Rokas, Antonis - Department of Biological Sciences, Vanderbilt University |
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Collection: Biology and Medicine ; Biotechnology |
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| 69 | Mixture of the Riesz distribution with respect to the multivariate Poisson | ||
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Summary: - ))-1 = u r j=r-i+1 cj . (3.33) On the other hand, using (2.8), we can write for all i {1... -i+1 - r-iu2 r-i + 1 2 u r j=r-i+1 cj - 1 2 u r i=1 ci . This after a standard calculation, gives k... ) -1 + r i=1 r-i+1 er-i+1 (m) br-i+1(m) - r-i er-i(m) br-i(m) + 1 2 × P r j=r-i+1 1 bj(m) P r-j+1(m |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 70 | RESEARCHARTICLE Copyright 2006 American Scientific Publishers | ||
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Summary: is r = jSi Aji, and the number of packets to send is s = jRi Aij . Therefore, the energy consumption... of node i in this policy can be expressed as Eci Aij = P1 jSi Aji + jRi P2d2 ij Aij +P3Aij (3) 4... of the optimization model should be max Aij min iV i=Nn E0i -Eci Aij -w iV i=Nn Eci Aij Eci Aij = P1 jSi Aji + jRi P2d |
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Source: Chen, Min - School of Computer Science and Engineering, Seoul National University |
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Collection: Computer Technologies and Information Sciences |
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| 71 | Duality for Logics of Transition Systems Marcello M. Bonsangue 1? Alexander Kurz 2?? | ||
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Summary: ) algebraic theory 3 . Clearly, every presentation AhS jRi by generators S and relations R defines an algebra... frame to its underlying set is monadic. Hence the infinitary algebra FrmhS jRi presented by a set... of a presentation AhS jRi is a pair hB ; f :S ! UBi such that B 2 A and f y (e l ) = f y (e r ), where (e l ; e r |
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Source: Kurz, Alexander - Department of Computer Science, University of Leicester |
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Collection: Mathematics ; Computer Technologies and Information Sciences |
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| 72 | CNOT and Bell-state analysis in the weak-coupling cavity QED regime Cristian Bonato,1 | ||
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Summary: polarization (labels jLi and jRi) and by a superscript arrow to indicate their propaga- tion direction along... , the states jR#i and jL"i (sz ¼ À1) are reflected if the electron-spin state is j#i and are transmitted... bit the spin of the photon. Consider an incident photon in the polarization state jc phi ¼ jRi þ #12;j |
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Source: Exter, Martin van - Leiden Institute of Physics, Universiteit Leiden |
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Collection: Physics |
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| 73 | Hyperentangled Mixed Phased Dicke States: Optical Design and Detection A. Chiuri,1 | ||
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Summary: Vi polariza- tion or into right jri and left j`i path. Explicitly, we used the following correspondence... selects four optical modes (two for each photon), namely jriA, j`iA, jriB, and j`iB, within the emission... contribution 2jVVijr`i is determined by the first excitation of the pump beam: here the j`ri ... |
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Source: Roma "La Sapienza", Università di - Dipartimento di Fisica, Quantum Optics Group |
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Collection: Physics |
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| 74 | Quantum Computing with Collective Ensembles of Multilevel Systems E. Brion and K. Mlmer | ||
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Summary: be coupled coherently to the Rydberg state jri, or to different Rydberg states jri, jr0 i . . . via suitable... of the level population in jii to jri, (ii) a coherent coupling in the two-state system with zero and one atom... in jri, blocking further transfer of atoms to the Rydberg state and, finally, (iii) ... |
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Source: Saffman, Mark - Department of Physics, University of Wisconsin at Madison |
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Collection: Physics |
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| 75 | Strongly Correlated Gases of Rydberg-Dressed Atoms: Quantum and Classical Dynamics G. Pupillo,1 | ||
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Summary: couple with laser light the ground state jgi of each atom to a Stark-split Rydberg state jri with large... and jri are coupled by a laser with Rabi frequency and (blue) detuning Á. r is the spontaneous emission... from jri, with momentum @kR of the photon recoil. (b) Born- Oppenheimer potentials in the x |
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Source: Boninsegni, Massimo - Department of Physics, University of Alberta |
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Collection: Physics |
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| 76 | Coherent Manipulation of Electronic States in a Double Quantum Dot T. Hayashi,1 | ||
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Summary: dot (jLi) or the right dot (jRi) with electrochemical potentials EL and ER, respectively. In practice... bases of jLi and jRi. When EL and ER of the localized states are crossed by changing Vsd, for instance... state in each dot, jLi and jRi. The qubit parameters, " and , and tunneling rates, ÿL and ÿ |
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Source: Zumbühl, Dominik - Department für Physik und Astronomie, Universität Basel |
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Collection: Physics |
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| 77 | BIAS EVALUATION IN THE PROPORTIONAL HAZARDS | ||
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Summary: of ties is written for the model (1) as l() = n i=1 i (Z i) - log jRi exp(Z j) , (2) 3 #12;where Ri... - Aik()] = 0, k = 1, . . . p, (3) where Aik() = jRi [zjk exp(Z j)] jRi exp(Z j) . The kl element... of the observed information matrix is given by - 2 l() kl = n i=1 i [Bikl() - Aik()Ail()] , (4) where Bikl() = ... |
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Source: Cruz, Frederico - Departamento de Estatística, Universidade Federal de Minas Gerais |
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Collection: Mathematics |
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| 78 | August 15, 1995 / Vol. 20, No. 16 / OPTICS LETTERS 1665 Enhanced backscattering from a volume-scattering | ||
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Summary: interparticle distance l ~ jri 2 rf j . Consequently a cone of en- hanced intensity with an angular width of l l... points of the time-reversed scattering sequences, jri 2 rf j , is determined by the transverse scattering... of placing a RPS in front of the VSM is an increase in the separation distance jri 2 rf j . The phase |
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Source: Boreman, Glenn D. - School of Optics (CREOLE), University of Central Florida |
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Collection: Physics |
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| 79 | Pattern Recognition 40 (2007) 32773291 www.elsevier.com/locate/pr | ||
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Summary: is a Gaussian white noise of variance 2, then jrI jx , jrI jy , rI #12;3282 I. Abraham et al. / Pattern... are given by jrI jx (u, v) = 1 b(r) Br x B(u + x, v + y) dx dy, jrI jy (u, v) = 1 b(r) Br y B(u + x, v + y... of B, they have the same law as jrI jx (0, 0) = 1 b(r) Br x B(x, y) dx ... |
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Source: Desolneux, Agnès - UFR de Mathématiques et Informatique, Université René Descartes |
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Collection: Mathematics ; Computer Technologies and Information Sciences |
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| 80 | Social Work and Social Welfare | ||
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Summary: Social Work and Social Welfare Journals from Routledge www.tandfonline.com SW&SW JRI 12-A4 20... , Norway www.tandfonline.com/rnsw Featured Journals SW&SW JRI 12-A4 20/10/2011 12:08 Page 2 #12... &SW JRI 12-A4 20/10/2011 12:08 Page 3 #12;4 Emotional and Behavioural Difficulties Official Journal |
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Source: Grant, James D.E. - Fakultät für Mathematik, Universität Wien |
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Collection: Mathematics |
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| 81 | Nonparametric MixedEffects | ||
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Summary: jRi j : The solutions are ^ #17; = (X T V 1 X) 1 X T V 1 y; ^ v = #22; DZ T V 1 (y X^ #17;); where... #17; Xivi) +log jDj+ v T i D 1 vi +log jRi j +#21;v R [v 00 i (t)] 2 dt +#21; R [#17; 00 (t)] 2 dt... T i D 1 vi +log jRi j +#21;vv T i Gvig+ #21;#17; T G#17;: Set ~ D = (D 1 +#21;vG) 1 , and ~ V i =Xi |
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Source: Zhang, Jin-Ting - Department of Statistics and Applied Probability, National University of Singapore |
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Collection: Mathematics |
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| 82 | Donald Siegel Department of Physics, University of Illinois at Urbana-Champaign | ||
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Summary: 1 MI r2 I ; 1 2 X i I ZI e2 jri ;RI j + 1 2 X i6=j e2 jri ;rj j + 1 2 X I6=J ZI ZJ e2 jRI ;RJ j |
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Source: Adams, James B - Department of Chemical and Materials Engineering, Arizona State University |
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Collection: Materials Science |
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| 83 | Donald Siegel Department of Physics, University of Illinois at Urbana-Champaign | ||
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Summary: 1 MI r2 I ; 1 2 X i I ZI e2 jri ;RI j + 1 2 X i6=j e2 jri ;rj j + 1 2 X I6=J ZI ZJ e2 jRI ;RJ j |
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Source: Adams, James B - Department of Chemical and Materials Engineering, Arizona State University |
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Collection: Materials Science |
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| 84 | Measurement of Screening Enhancement to Nuclear Reaction Rates using a Strongly Magnetized and Strongly Correlated Non-neutral Plasma | ||
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Summary: _kijt e2ri ÿ rj v?i ÿ v?j=jri ÿ rjj3 is the rate of change of the relative perpendicular kinetic... v2 ij e2 jri ÿ rjj ri; 0 rj; 0; (7) where H0 0 is the energy of a system of N ÿ 2 particles plus... where R ri rj=2 is the center of mass position. Then H H00 2R; 0 1 2v2 ij e2=jri ÿ rjj: (8) Noting |
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Source: Dubin, Daniel H.E. - Nonneutral Plasma Physics Group, Department of Physics, University of California at San Diego |
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Collection: Plasma Physics and Fusion |
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| 85 | Supersolid Droplet Crystal in a Dipole-Blockaded Gas M. Boninsegni,1 | ||
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Summary: dimensionless form): H ¼ À 1 2 XN i¼1 r2 i þ X i>j vðrijÞ (2) where rij ¼ jri À rjj is the distance between... the ground state jgi of each atom with an excited Rydberg state jri with a large dipole moment d, in the k... Debye range [11]. While several dressing schemes are possible [5,22], here we consider jri as the ... |
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Source: Boninsegni, Massimo - Department of Physics, University of Alberta |
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Collection: Physics |
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| 86 | Spatially anisotropic Heisenberg kagome antiferromagnet Andreas P. Schnyder,1 Oleg A. Starykh,2 and Leon Balents1 | ||
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Summary: dx JL,y · JL,y + JR,y · JR,y , 49 where u~ =cos qu is the modified spinon velocity. To the order we... ANISOTROPIC HEISENBERG KAGOME... PHYSICAL REVIEW B 78, 174420 2008 174420-9 #12;Hbs = y dxg~bsJL,y · JR,y, 50... - cos q y dx 2 u 3 JL,y x JL,y x + JR,y x JR,y x + gbsJR,y x JL,y x . ... |
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Source: Starykh, Oleg - Department of Physics and Astronomy, University of Utah |
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Collection: Physics |
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| 87 | VOLUME 85, NUMBER 5 P H Y S I C A L R E V I E W L E T T E R S 31 JULY 2000 Dynamics of Three-Tori in a Periodically Forced Navier-Stokes Flow | ||
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Summary: ) the pe- riod close to the bifurcation point would have the form TVLF c ln 1 jRi 2 Ricritj 1 d [13], while... in case (ii) TVLF c p jRi 2 Ricritj 1 d [12]. Our computed TVLF fits the logarithmic form very well... by TVLF l21 het ln 1 jRi 2 Rihetj 1 l21 hom ln 1 jRi 2 Rihomj 1 c . The logarithmic fits give ... |
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Source: Lopez, John M. - Department of Mathematics and Statistics, Arizona State University; Marques, Francisco - Departament de Física Aplicada, Universitat Politècnica de Catalunya |
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Collection: Engineering ; Mathematics ; Physics |
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| 88 | http://soc2010.inha.ac.kr 2 0 1 0 S o C C o n f e r e n c e | ||
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Summary: ) EDA , . [1] Jri Lee, "A 20Gb/s Adaptive Equalizer in 0.13 m CMOS Technology," IEEE J |
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Source: Choi, Woo-Young - School of Electrical and Electronics Engineering, Yonsei University |
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Collection: Engineering |
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| 89 | WEBINTEGRATING NETWORKCONSCIOUS IMAGE TRANSMISSION Armando L. Caro Jr. | ||
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Summary: ate a Java API that would call UTL functions using the Java Runtime Interface (JRI) d [11]. Rewrit... be generically used for all NC images; only the plu d JRI is a technology developed by Netscape which is very... and Java code. However, JRI may only be used with Netscape's Java Virtual Machine. #12; gin is image |
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Source: Delaware, University of - Protocol Engineering Laboratory |
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Collection: Computer Technologies and Information Sciences |
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| 90 | CSC320: Visual Computing Term Test 1 February 27, 2004 9:10-11:00 | ||
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Summary: rI . (b) De#12;ne jrI j. What does this have to do with edge detection? (c) De#12;ne the gradient |
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Source: Toronto, University of - Department of Computer Science, Dynamic Graphics Project |
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Collection: Computer Technologies and Information Sciences |
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| 91 | Robust Segmentation by Cutting Across a Stack of Gamma Transformed Images 3D view of hair cells | ||
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Summary: R(i,j) is strongest for nearby peaks; decreases as pixels approach minimum intensity mij: R(i, j)>R(i |
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Source: Plotkin, Joshua B. - Department of Biology, University of Pennsylvania; Yu, Stella X. - Computer Science Department, Boston College |
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Collection: Biology and Medicine ; Computer Technologies and Information Sciences |
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| 92 | Journal of Reproductive Immunology 62 (2004) 1718 | ||
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Summary: . doi:10.1016/j.jri.2003.08.002 #12;18 J.L. Strominger / Journal of Reproductive Immunology 62 (2004) 17 |
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Source: Strominger, Jack L. - Department of Molecular and Cellular Biology, Harvard University |
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Collection: Biology and Medicine |
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| 93 | Choice questions (2 points each) 1. What is the function of statocyst of an invertebrate? (A) vision (B) olfaction (C) reproduction (D) | ||
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Summary: Q&I& &hl&figlucocorticoidreceptor $kl&iE$@ (C) klf$hi&+mineralocorticoid |
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Source: Huang, Haimei - Department of Life Science, National Tsing Hua University |
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Collection: Biology and Medicine |
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| 94 | 1 (10%) The Capability Maturity Model for Sof'ware (CMM or SW-CMM) was successfully devel'oped by 'the Software Engineering Institute of Carnegie Mellon | ||
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Summary: is the maximum value for JRI? How many antisymmetric relations can have this size? 9 (11%) This problem is about |
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Source: Huang, Haimei - Department of Life Science, National Tsing Hua University |
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Collection: Biology and Medicine |
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| 95 | Dice: a Game Theoretic Framework for Wireless Multipath Network Coding | ||
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Summary: condition for collision free schedule is: X k Bk i [t] + X k X jR(i) Bk j [t] 1, i V k \Sk , (2) i... of node i is: X k bk i = lim T 1 T TX t=1 X k Bk i [t], (3) Apply (3) to (2), we have: X k bk i + X k X jR(i... ) subject to: X j xk ij - X j xk ji = (i, k), i V k (7) xk ij 0, (i, j) Ek (8) X k bk i + X k X jR(i) bk |
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Source: Li, Baochun - Department of Electrical and Computer Engineering, University of Toronto |
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Collection: Computer Technologies and Information Sciences |
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| 96 | Biometrics 62, 10531061 December 2006 | ||
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Summary: ; Kalbfleisch and Prentice, 2002): (k+1) 0 (t; , g) = i:Yit i jRi e Zj +g P (k) Gj + e Zj P(k) j - P (k) Gj... - log jRi e Zj +g P (k) Gj + e Zj P(k) j - P (k) Gj . (6) Then ~lp 2 is maximized to obtain updated... ) and is given by PL2(, g) = n i=1 exp( Zi + gGi) jRi j exp( Zj + gGj) i . (7) The PL2 in (7) can also |
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Source: Lu, Wenbin - Department of Statistics, North Carolina State University |
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Collection: Biology and Medicine ; Mathematics |
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| 97 | Scaling of the peak magnetic recconnection rate in the inviscid Taylor problem | ||
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Summary: ) across the reconnecting layer. The resistive-inertial regime holds for ^t 1. In this regime, J = Jri... occur at time t2 = 0.368 2 ^-3/5 , (12) and should scale as J2 = Jri(^t = 0.368 2) ^-2/5 . (13) V |
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Source: Fitzpatrick, Richard - Department of Physics, University of Texas at Austin |
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Collection: Plasma Physics and Fusion ; Physics |
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| 98 | Scaling of the peak magnetic reconnection rate in the inviscid Taylor problem | ||
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Summary: -inertial regime holds for t^ 1. In this regime, J = Jri ^ -2/5 F t^/ 2 , 8 where PHYSICS OF PLASMAS 15, 024503... reconnection rate should occur at time t2 = 0.368 2 ^ -3/5 , 12 and should scale as J2 = Jri t^ = 0.368 2 ^ -2 |
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Source: Fitzpatrick, Richard - Department of Physics, University of Texas at Austin |
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Collection: Plasma Physics and Fusion ; Physics |
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| 99 | Teor'ia KAM sin Coordenadas Acci'on--' | ||
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Summary: )--(2) Si tenemos: dethAi 6= 0 ! es diofantino hT ? ` JRi = 0 h\Deltai = 1 (2ß) n R T n \Delta d... R(\DeltaT ) +Rk = O 2 (kRk) Proposici'on: Siempre se verifica hT ? ` JRi = 0. 11 #12; Teorema (Kolmogorov |
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Source: Politècnica de Catalunya, Universitat - Departament de Matemàtica Aplicada I |
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Collection: Mathematics |
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| 100 | A sub-cubic time algorithm for computing the quartet distance between two general trees | ||
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Summary: =1 dv j=1 I [i, j] (9) R [i] = dv j=1 I[i, j](C[j] - I[i, j]) (10) C [j] = dv i=1 I[i, j](R[i] - I... the expression in Eq. (22) as I[i, j] (23) (M - R[i] - C[j] + I[i, j])(R[i] - I[i, j])(C[j] - I[i, j])+ (R[i] - I... [i, j])(I[i, j](R[i] - I[i, j]) - C [j])+ (C[j] - I[i, j])(I[i, j](C[j] - I[i, j]) - R [i])+ I1 [i, j |
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Source: Mailund, Thomas - Bioinformatics Research Center & Department of Computer Science, Aarhus Universitet |
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Collection: Environmental Sciences and Ecology ; Computer Technologies and Information Sciences |
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