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On the max coloring problem

by Leah Epstein, Asaf Levin - In Proc. of WAOA’07
"... We consider max coloring on hereditary graph classes. The problem is defined as follows. Given a graph G = (V, E) and positive node weights w: V → (0, ∞), the goal is to find a proper node coloring of G whose color classes C1, C2,..., Ck minimize k∑ maxv∈Ci w(v). We design a general framework which ..."
Abstract - Cited by 9 (0 self) - Add to MetaCart
We consider max coloring on hereditary graph classes. The problem is defined as follows. Given a graph G = (V, E) and positive node weights w: V → (0, ∞), the goal is to find a proper node coloring of G whose color classes C1, C2,..., Ck minimize k∑ maxv∈Ci w(v). We design a general framework which

T min = 0.291, T max = 0.493 Refinement

by Rui-jun Xu, Orthorhombic Pbca, Rigaku Scxmini Diffractometer , 2010
"... a = 12.290 (3) A ˚ b = 7.1302 (14) A ˚ c = 20.304 (4) A ˚ V = 1779.2 (6) A ˚ 3 ..."
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a = 12.290 (3) A ˚ b = 7.1302 (14) A ˚ c = 20.304 (4) A ˚ V = 1779.2 (6) A ˚ 3

Generating Hard Instances of Lattice Problems (Extended Abstract)

by M. Ajtai - In Proceedings of the Twenty-Eighth Annual ACM Symposium on the Theory of Computing , 1996
"... . We give a random class of lattices in Z n so that, if there is a probabilistic polynomial time algorithm which finds a short vector in a random lattice with a probability of at least 1 2 then there is also a probabilistic polynomial time algorithm which solves the following three lattice probl ..."
Abstract - Cited by 143 (0 self) - Add to MetaCart
in the sense that any other vector whose length is at most n c kvk is parallel to v, where c is a sufficiently large absolute constant. (3) Find a basis b 1 ; :::; b n in the n-dimensional lattice L whose length, defined as max n i=1 kb i k, is the smallest possible up to a polynomial factor. A large

T min = 0.548, T max = 0.712

by Ming-lin Guo, Long Liu, Cong-cong Lu, Mo K Radiation , 2010
"... Monoclinic, P21=c a = 6.7745 (14) A ˚ b = 14.220 (3) A ˚ c = 15.629 (3) A ˚ = 101.10 (3) ..."
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Monoclinic, P21=c a = 6.7745 (14) A ˚ b = 14.220 (3) A ˚ c = 15.629 (3) A ˚ = 101.10 (3)

U =2.1kV and B =6,24⋅10 Anode z,max-3

by O. Meusel, J. Pozimski, A. Jakob, C. Gabor, U. Ratzinger, Wdujhw Fkdpehu, T. Our Hitherto
"... Gabor lenses using a stable space charge cloud for focusing have several advantages. They provide strong cylinder symmetric focusing at drastically reduced magnetic and electrostatic field strength. In case of a positive ion beam the space charge of the confined electrons causes compensation of the ..."
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to 500 keV a new very powerful GPL will be installed behind the RFQ.,RQ VRXUFH /(%7 $FFHOHUDWRU

Symbol Parameter Conditions Min Typ Max Unit

by unknown authors , 2011
"... The TFF1014HN/N1 is an integrated downconverter for use in Low Noise Block (LNB) convertors in a 10.7 GHz to 12.75 GHz Ku band satellite receiver system. Low current consumption integrated pre-amplifier, mixer, buffer amplifier and PLL synthesizer Flat gain over frequency Single 5 V supply pin Low c ..."
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) 4. Quick reference data Table 1. Quick reference data VCC = 5 V; Tamb = 25 �C; fLO = 9.75 GHz or 10.6 GHz; fxtal = 25 MHz; Z0 = 50 � unless otherwise specified. Symbol Parameter Conditions Min Typ Max Unit VCC supply voltage 4.5 5 5.5 V ICC supply current RF input and IF output AC coupled- 52- m

on behalf of the CDF and D0 Collaborations Max-Planck-Institut für Physik,

by Federico Sforza
"... We present the study of the SM Higgs properties obtained from the combined analysis of the up-to 10 fb−1 dataset collected by the CDF and D0 experiments during the pp ̄ collision at√ s = 1.96 TeV of Tevatron Run II. The observed local significance for the SM Higgs boson signal is of 3.0σ at mH = 125 ..."
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H = 125 GeV/c 2. After a brief review of analysis channels contributing the most, where the Higgs boson decays to a pair of W bosons or to a pair of b-quarks jets, the signal production cross section and its couplings to fermions and vector bosons are analyzed. Other presented results are the recent study

A New Lower Bound on the Maximum Number of Satisfied Clauses in Max-SAT and its Algorithmic Applications

by Robert Crowston, Gregory Gutin, Mark Jones, Anders Yeo
"... In a formula F = (V, C) in conjunctive normal form (CNF), V is the set of variables and C is the multiset of clauses. We denote by sat(F) the maximum number of clauses of F that can be satisfied by a truth assignment. It is well-known that for every CNF formula F = (V, C), sat(F) ≥ |C|/2 and the bo ..."
Abstract - Cited by 5 (4 self) - Add to MetaCart
prove that for each UCF CNF formula F = (V, C) a subformula F ′ = (V ′ , C ′ ) can be found in polynomial time such that sat(F) ≥ ˆφ|C | + (1 − ˆφ)|C ′ | + (2 − 3 ˆφ)|Y |/2, where Y is the set of variables in C \ C ′. This improves the Lieberherr-Specker lower bound on sat(F). We show that our new

Effect of Integrated Nutrient Management and Mulching on Growth and Yield of Soybean [Glycine max (L.) Merrill] in Clay Loam Soil

by R C Jain , 2015
"... ABSTRACT The present experiment was laid out in a randomized block design consisted of 6 treatments. The experimental site having fairly uniform topography with normal fertility status.The effect of integrated nutrient management and mulching on plant height was noticed non significant. However , b ..."
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, branches per plant, Root length/ plant (cm), Dry weight/ plant (g), Pods/plant(no), Seed index(g), and Grain yield(kg/ha) were found to increase significantly due to the application of 50% RDF + ZnSO 4 @25 kg/ha+ V.C. 1.5t/ ha + B.F.+ A.M. + Mulching(T 6 ) followed by treatment T 4 and T 5

Technology development of 4H-SiC RF BJTs with 5GHz fMAX

by Bart Van Zeghbroeck, Ivan Perez, Feng Zhao, John Torvik
"... 4H-SiC RF BJTs were developed on a semi-insulating (>105 Ω-cm) substrate using an triple mesa-etch and interdigitated emitter-base finger design. The sheet conductance of the emitter layer was measured during the etch to accurately determine the location of the base-emitter interface. On-wafer sm ..."
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-emitter configuration at JE = 10.6 kA/cm2 and VCE = 20 V. The maximum available power gain (GMAX) is 18.6-dB at 500 MHz and 12.4-dB at 1 GHz, demonstrating the potential of 4H-SiC BJTs for both UHF and L-band applications. Small-periphery (4x150μm) devices were tested using on-wafer load pull measurements up to 1.5GHz
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