Ara
Toplam kayıt 295, listelenen: 221-240
Di-Μ-Nicotinamide-Κ2 N 1:O;Κ2 O:N 1-Bis[AquaBis(3-ChloroBenzoato-Κ2 O,O′)Cadmium]
(2013)
In the centrosymmetric dinuclear title compound, [Cd2(C7H4ClO2)4(C6H6N2O)2(H2O)2], the CdII atom is coordinated by one N atom from one bridging nicotinamide ligand and one O atom from another symmetry-related bridging ...
Di-Μ-Nicotinamide-Κ2O:N1;Κ2N 1:O-Bis[AquaBis(4-MethOxyBenzoato-Κo)Copper(Ii)]
(2010)
The asymmetric unit of the centrosymmetric dinuclear title compound, [Cu2(C8H7O3)4(C6H6N2O)2(H2O)2], contains one half of the complex molecule. Each CuII atom is five-coordinated by one N atom from one bridging nicotinamide ...
Dimethyl 6-Iodo-2-Methyl-1,2-DiHydroQuinoline-2,4-DiCarboxylAte
(2013)
In the title compound, C14H14INO4, the dihydropyridine ring adopts a twist conformation. In the crystal, pairs of N—H⋯O and C—H⋯O hydrogen bonds link the molecules into inversion R 2 2(10) and R 2 2(18) dimers, forming ...
Dimethyl 6-Bromo-2-Methyl-1,2-DiHydroQuinoline-2,4-DicarboxylAte
(2012)
In the title compound, C14H14BrNO4, the dihydropyridine ring adopts a screw-boat conformation. In the crystal, pairs of N—H⋯O hydrogen bonds link the molecules into inversion R 2 2(10) dimers.
Ethyl 4-HydrOxy-9-Tosyl-9H-Carbazole-3-CarboxylAte
(2009)
In the title compound, C22H19NO5S, the carbazole skeleton is nearly planar [maximum deviation = 0.043 (1) Å] with the pyrrole ring oriented at dihedral angles of 2.32 (6) and 1.77 (6)° with respect to the adjacent benzene ...
Ethyl 4,9-Dimethyl-9H-Carbazole-3-CarboxylAte
(2014)
In the title compound, C17H17NO2, the carbazole skeleton includes an ethoxycarbonyl group at the 3-position. The indole three-ring system is almost planar [maximum deviation = 0.065 (2) Å], and the ethyl ester group is ...
Ethyl 9H-1,2,3,4-Tetrahydrocarbazole-3-Carboxylate
(Blackwell Munksgaard, 2002)
Macroscopic Anomalies Before the September 2010 M=7.1 Earthquake in Christchurch, New Zealand
(Copernicus Gesellschaft Mbh, 2013)
Previous published work after the Kobe and A degrees zmit earthquakes (1995 and 1999, respectively) demonstrated some reported meteorological and animal behaviour precursors were valid. Predictions were freshly tested for ...
Measurement and Qcd Analysis of Double-Differential Inclusive Jet Cross Sections in Pp Collisions at Root S=8 Tev and Cross Section Ratios to 2.76 and 7 Tev
(Springer, 2017)
A measurement of the double-differential inclusive jet cross section as a function of the jet transverse momentum p(T) and the absolute jet rapidity |y| is presented. Data from LHC proton-proton collisions at root s = 8 ...
Limits on the Higgs Boson Lifetime and Width from Its Decay to Four Charged Leptons
(Amer Physical Soc, 2015)
Constraints on the lifetime and width of the Higgs boson are obtained from H -> ZZ -> 4l events using data recorded by the CMS experiment during the LHC run 1 with an integrated luminosity of 5.1 and 19.7 fb(-1) at a ...
Lattice Dynamics and Elastic Properties of Lanthanum Monopnictides
(Pergamon-Elsevier Science Ltd, 2008)
In this study, first principles calculation results of the second order elastic constants and lattice dynamics of two lanthanum monopnictides, LaN and LaBi, which crystallize in rock-salt Structure (B1 phase), are presented. ...
Measurement of Charged Pion, Kaon, and Proton Production in Proton-Proton Collisions at Root S=13 Tev
(Amer Physical Soc, 2017)
Transverse momentum spectra of charged pions, kaons, and protons are measured in proton-proton collisions at root s = 13 TeV with the CMS detector at the LHC. The particles, identified via their energy loss in the silicon ...
Measurement of Charged Particle Spectra in Minimum-Bias Events from Proton-Proton Collisions at Root S =13 Tev
(Springer, 2018)
Pseudorapidity, transverse momentum, and multiplicity distributions are measured in the pseudorapidity range vertical bar eta vertical bar < 2.4 for charged particles with transverse momenta satisfying pT > 0.5 GeV in ...
Lhc Forward Physics
(Iop Publishing Ltd, 2016)
Measurement Of The Z Gamma -> Nu(Nu)Over-Bar Gamma Production Cross Section In Pp Collisions At Root S=8 Tev And Limits On Anomalous Zz Gamma And Z Gamma Gamma Trilinear Gauge Boson Couplings
(Elsevier, 2016)
An inclusive measurement of the Z gamma -> nu(nu) over bar gamma production cross section in pp collisions at root s = 8 TeV is presented, using data corresponding to an integrated luminosity of 19.6fb(-1) collected with ...
Measurement Of The Zz Production Cross Section And Z -> L(+)L(-)L '(+)L '(-) Branching Fraction In Pp Collisions At Root S=13Tev
(Elsevier, 2016)
Four-lepton production in proton-proton collisions, pp -> (Z/gamma*)(Z/gamma*)-> l(+)l(-)l '(+)l '(-), where l,l '(-) = e or mu, is studied at a center-of-mass energy of 13 TeV with the CMS detector at the LHC. The data ...
Measurement of the W+W- Cross Section in Pp Collisions at Root S=8 Tev and Limits on Anomalous Gauge Couplings
(Springer, 2016)
A measurement of the W boson pair production cross section in proton-proton collisions at root s = 8TeV is presented. The data collected with the CMS detector at the LHC correspond to an integrated luminosity of 19.4 fb(-1). ...
Measurements Of Differential Cross Sections For Associated Production Of A W Boson And Jets In Proton-Proton Collisions At Root S=8 Tev
(Amer Physical Soc, 2017)
Differential cross sections for a W boson produced in association with jets are measured in a data sample of proton-proton collisions at a center-of-mass energy of 8 TeV recorded with the CMS detector and corresponding to ...
Measurement Of The Wz Production Cross Section In Pp Collisions At Root S=7 And 8 Tev And Search For Anomalous Triple Gauge Couplings At Root S=8 Tev
(Springer, 2017)
The WZ production cross section is measured by the CMS experiment at the CERN LHC in proton proton collision data samples corresponding to integrated luminosities of 4.9 fb(-1) collected at root s = 7 TeV, and 19.6fb(-1) ...
Measurement Of The Weak Mixing Angle Using The Forward-Backward Asymmetry Of Drell-Yan Events In Pp Collisions At 8 Tev
(Springer, 2018)
A measurement is presented of the effective leptonic weak mixing angle (sin(2) theta(effl))using the forward- backward asymmetry of Drell-Yan lepton pairs (mu mu and ee) produced in proton-proton collisions at N root s = ...