“…The 2 × 2 optical coupler (OC) divides the input optical field into two beams, which propagate in forward (E (1) f ) and backward (E (1) b ) directions, respectively. The optical fields after the HNLF, E (2) f and E (2) b , interfere at a 2 × 2 optical coupler, resulting into the optical transmitted field E out and the reflected field E r . In the HNLF, the SPM and cross-phase modulation (XPM) effects occur contributing to the nonlinear phase shift of the counter-propagating fields [14,15], and the former effect is involved in the following discussion, performing the SPM-NOLM.…”