We analyzed the shapes of Galactic open clusters by the star counting
technique with the 2MASS star catalog database. Morphological parameters such
as the ellipticity and size have been derived via stellar density distribution,
weighed by clustering probability. We find that most star clusters are
elongated, even for the youngest star clusters of a few million years old,
which are located near to the Galactic disk. The shapes of young star clusters
must reflect the conditions in the parental molecular clouds and during the
cluster formation process. As an open cluster ages, stellar dynamics cause the
inner part of the cluster to circularize, but the overall radius gets larger
and the stellar density becomes sparser. We discuss how internal relaxation
process competes with Galactic external perturbation during cluster evolution.Comment: 13 pages; 10 pages; accepted Astronomical Journa
A search for heavy resonances decaying to a Higgs boson and a vector boson is presented. The analysis is performed using data samples collected in 2015 by the CMS experiment at the LHC in proton–proton collisions at a center-of-mass energy of 13 TeV, corresponding to integrated luminosities of 2.2–2.5 fb−1. The search is performed in channels in which the vector boson decays into leptonic final states (Z→ννZ→νν, W→ℓνW→ℓν, and Z→ℓℓZ→ℓℓ, with ℓ=e,μℓ=e,μ), while the Higgs boson decays to collimated b quark pairs detected as a single massive jet. The discriminating power of a jet mass requirement and a b jet tagging algorithm are exploited to suppress the standard model backgrounds. The event yields observed in data are consistent with the background expectation. In the context of a theoretical model with a heavy vector triplet, a resonance with mass less than 2 TeV is excluded at 95% confidence level. The results are also interpreted in terms of limits on the parameters of the model, improving on the reach of previous searches
Multi-wavelength B, V , R, I observations of the optical afterglow of GRB 050319 were performed by the 1.05-m telescope at Kiso Observatory and the 1.0-m telescope at Lulin Observatory from 1.31 hours to 9.92 hours after the burst. Our R band lightcurves, combined with other published data, can be described by the smooth broken power-law function, with α 1 = −0.84 ±0.02 to α 2 = −0.48±0.03, 0.04 days after the GRB. The optical lightcurves are characterized by shallow decays-as was also observed in the X-rays-which may have a similar origin, related to energy injection. However, our observations indicate that there is still a puzzle concerning the chromatic breaks in the R band lightcurve (at 0.04 days) and the X-ray lightcurve (at 0.004 days) that remains to be solved.
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