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805
On the max coloring problem
 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 ..."
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Cited by 9 (0 self)
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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
, 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)
 In Proceedings of the TwentyEighth 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 ..."
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Cited by 143 (0 self)
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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 ndimensional 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
, 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,max3
"... 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
, 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 preamplifier, 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 MaxPlanckInstitut für Physik,
"... We present the study of the SM Higgs properties obtained from the combined analysis of the upto 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 bquarks 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 MaxSAT and its Algorithmic Applications
"... 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 wellknown that for every CNF formula F = (V, C), sat(F) ≥ C/2 and the bo ..."
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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) ≥ ˆφC  + (1 − ˆφ)C ′  + (2 − 3 ˆφ)Y /2, where Y is the set of variables in C \ C ′. This improves the LieberherrSpecker 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
, 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 4HSiC RF BJTs with 5GHz fMAX
"... 4HSiC RF BJTs were developed on a semiinsulating (>105 Ωcm) substrate using an triple mesaetch and interdigitated emitterbase finger design. The sheet conductance of the emitter layer was measured during the etch to accurately determine the location of the baseemitter interface. Onwafer sm ..."
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emitter configuration at JE = 10.6 kA/cm2 and VCE = 20 V. The maximum available power gain (GMAX) is 18.6dB at 500 MHz and 12.4dB at 1 GHz, demonstrating the potential of 4HSiC BJTs for both UHF and Lband applications. Smallperiphery (4x150μm) devices were tested using onwafer load pull measurements up to 1.5GHz
Results 1  10
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805