We present a study of higher-order Raman ($\mathrm{\ensuremath{\Lambda}}, V$, and
S) transitions between Rydberg states involving the absorption and emission of at least three photons in the interaction of two-color corotating circularly polarized laser pulses with the hydrogen atom. Our analysis is based on results of numerical solutions of the corresponding time-dependent Schr\"odinger equation. The results for the interaction with ($\ensuremath{\omega},2\ensuremath{\omega}$) fields show that the simultaneous interaction with both fields results in an excited state distribution over a broad range of magnetic quantum numbers. Indications of the impact of the $\mathrm{\ensuremath{\Lambda}}, V$, and
S transitions are found via the analysis of final distributions resulting from the preparation of the atom in specific Rydberg states. Furthermore, we show that similar mechanisms for the redistribution of population between Rydberg states are present in two-color fields with larger differences in the central frequencies, i.e., ($\ensuremath{\omega},3\ensuremath{\omega}$) and ($\ensuremath{\omega},4\ensuremath{\omega}$) fields.
In this paper I calculate the leading transition amplitudes for a single-photon-double-excitation process which is dominated by long-range correlation effects. The process examined is an excitation of a Rydberg atom with the inner core in an
S state and the outer electron in essentially a hydrogenic state
n to another
S inner-core state and the outer electron in another hydrogenic state ${n}^{\ensuremath{'}}$. We find the leading contribution comes from terms in which the photon is received by the inner core. The excitation of the outer electron is done in intermediate states. The transition amplitude factors into a part entirely dependent on the inner core and a part which is a simple hydrogenic matrix element for the outer electron. The form of the amplitudes suggest that the coefficient to the hydrogenic matrix element be called a "transition polarizability."