  We establish the Berry-phase formulas for the angular momentum (AM) and the
Hall viscosity (HV) to investigate chiral superconductors (SCs) in two and
three dimensions. The AM is defined by the temporal integral of the
anti-symmetric momentum current induced by an adiabatic deformation, while the
HV is defined by the symmetric momentum current induced by the symmetric
torsional electric field. Without suffering from the system size or geometry,
we obtain the macroscopic AM $L_z = \hbar m N_0/2$ at zero temperature in
full-gap chiral SCs, where $m$ is the magnetic quantum number and $N_0$ is the
total number of electrons. We also find that the HV is equal to half the AM at
zero temperature not only in full-gap chiral SCs as is well-known but also in
nodal ones, but its behavior at finite temperature is different in the two
cases.
