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Crystal Structure And Hirshfeld Surface Analysis Of 1-{[2-Oxo-3-(Prop-1-En-2-Yl)-2,3-DiHydro-1H-1,3-BenzoDiazol-1-Yl]MethYl}-3-(Prop-1-En-2-Yl)-2,3-DiHydro-1H-1,3-BenzoDiazol-2-One
(2018)
In the title compound, the benzodiazolone moieties are planar to within 0.017 (1) and 0.026 (1) Å, and oriented at a dihedral angle of 57.35 (3)°. In the crystal, two sets of intermolecular C—H⋯O hydrogen bonds generate ...
Crystal Structure And Hirshfeld Surface Analysis Of (4Z)-1-Butyl-4-(2-OxoPropylIdene)-2,3,4,5-TetraHydro-1H-1,5-Benzodiazepin-2-One
(2018)
The asymmetric unit of the title compound consists of two independent molecules differing slightly in the conformations of the seven-membered rings and the butyl substituents., The asymmetric unit of the title compound, ...
Crystal Structure And Hirshfeld Surface Analysis Of AquaBis(Nicotinamide-Κn)Bis(4-Sulfamoylbenzoato-Κo 1)Copper(Ii)
(2018)
The CuII cation, located on a twofold rotation axis, is coordinated by two 4-sulfamoylbenzoate anions, two nicotinamide (NA) molecules and one water molecule in a slightly distorted square-pyramidal geometry., In the ...
Crystal Structure and Hirshfeld Surface Analysis of 5-Methyl-1,2,4-Triazolo[1,5-A]Pyrimidine
(2018)
The nine-membered ring system of the title compound is essentially planar. In the crystal, molecules are linked via C—HTrz⋯NTrz and C—HPyrm⋯NTrz (Trz = triazole and Pyrm = pyrimidine) hydrogen bonds together with weaker ...
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 ...
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 = ...
Observation Of The Chi(B1)(3P) And Chi(B2)(3P) And Measurement Of Their Masses
(Amer Physical Soc, 2018)
The chi(b1)(3P) and chi(b2)(3P) states are observed through their gamma(3S)(gamma) decays, using an event sample of proton-proton collisions collected by the CMS experiment at the CERN LHC. The data were collected at a ...
Performance of Reconstruction and Identification of Tau Leptons Decaying to Hadrons And Nu(Tau) in Pp Collisions at Root S=13 Tev
(Iop Publishing Ltd, 2018)
The algorithm developed by the CMS Collaboration to reconstruct and identify tau leptons produced in proton-proton collisions at root s = 7 and 8 TeV, via their decays to hadrons and a neutrino, has been significantly ...
Observation Of Higgs Boson Decay To Bottom Quarks
(Amer Physical Soc, 2018)
The observation of the standard model (SM) Higgs boson decay to a pair of bottom quarks is presented. The main contribution to this result is from processes in which Higgs bosons arc produced in association with a W or Z ...
Observation Of The Z -> Psi L(+)L(-) Decay In Pp Collisions At Root S=13 Tev
(Amer Physical Soc, 2018)
This Letter presents the observation of the rare Z boson decay Z -> psi l(+)l(-). Here, psi represents contributions from direct J/psi and psi(2S) -> J/psi X, l(+)l(-) is a pair of electrons or muons, and the J/psi meson ...