  This memo contains a collection of formulas describing the electromagnetic
energy, momentum and spin distribution of an optical field formed in dielectric
media separated by a plane interface when an incident monochromatic plane wave
is totally reflected. The formulas are based on the Abraham momentum definition
and include the momentum decomposition into the orbital (canonical) and spin
parts as well as explicit dual-symmetric separation of the electric and
magnetic contributions. This material was prepared in February 2013 but it had
not been finalized and published because of the difficulties in physical
interpretation of singular terms in the spin and orbital momentum expressions
associated with the sharp interface. Meanwhile, it has become clear that the
"naive" Abraham approach is not correct for this problem and the
electromagnetic spin and momentum in inhomogeneous media are better
characterized by the more elaborated relations based on the Minkowski paradigm
[see, e.g., Phys. Rev. A 83, 013823 (2011); 86, 055802 (2012);
arXiv:1706.05493]. In application to the total-reflection situation this
Minkowski-based description was recently illustrated in arXiv:1706.06263, so
the present material is mainly of historical interest. However, it seems useful
to make it known for a wide audience, at least for comparison with the recent
improved approaches and for suitable references. The last section, treating the
ponderomotive action experienced by a Mie particle in the evanescent wave, is
independent of the Abraham - Minkowski controversy. The numerical calculations
preserve their validity, and association of the various force and torque
components with corresponding components of the optical momentum and spin
remains legal in the Minkowski pattern. The results of the last section were
partly used in other published works [e.g., Nature Commun. 5, 3300 (2014)].
