“…The suppression is achieved by independently controlling the polarization of all pulses . The diagonal-suppressing sequence is encoded into the beam polarizations as {90, 60, 120, 0°} , or {60, 120, 0, 0°}, , where the first two pulses are pump pulses, the third is the probe, and the fourth is the local oscillator pulse. Suppressed signals include diagonal signals as well as off-diagonal signals arising from Stokes shifts and ultrafast solvation, as these processes typically do not strongly reorient the transition dipole.…”