  The polarizations of Y(nS) (n=1,2,3) and prompt J/\psi and \psi(2S), as well
as the differential cross section of the Y(nS), are measured in proton-proton
collisions at sqrt(s) = 7 TeV, using a dimuon data sample collected by the CMS
experiment at the LHC, corresponding to an integrated luminosity of 4.9 fb-1.
The differential cross section is measured as a function of transverse momentum
of Y(nS). The data show a transition from exponential to power-law behavior in
the neighborhood of 20 GeV, and the power-law exponents for all three states
are consistent. The polarization parameters \lambda\theta, \lambda\phi, and
\lambda\theta\phi, as well as the frame-invariant quantity \lambda, are
measured from the dimuon decay angular distributions in three different
polarization frames. No evidence of large polarizations is seen in these
kinematic regions, which extend much beyond those previously explored.
