We demonstrate the formation of an exceptional point (EP) between distinct Hermite–Gaussian transverse modes in a Fabry–Perot cavity by combining tunable intracavity birefringence with controllable, polarization-dependent loss. By inserting two qu...
We demonstrate the formation of an exceptional point (EP) between distinct Hermite–Gaussian transverse modes in a Fabry–Perot cavity by combining tunable intracavity birefringence with controllable, polarization-dependent loss. By inserting two quarter-waveplates and a thin pellicle beamsplitter inside the cavity, we mix orthogonal polarization modes and introduce differential attenuation. Tuning the waveplate rotation angle as well as the beamsplitter’s loss drives the cavity’s round-trip Jones matrix to a non-Hermitian degeneracy, at which both the resonance frequencies and linewidths of two interacting modes coalesce. Experimentally, we excite either the fundamental (TEM00) and firstorder transverse modes (TEM10) or two orthogonally polarized TEM00 modes, and we probe their Stokes parameters and transmission spectra as the system approaches the EP. We observe that, at the critical tuning, the two modes merge into a single circularly polarized eigenstate, exhibiting identical frequency and linewidth. Our results agree quantitatively with the analytic Jones-matrix model, confirming that precise control of birefringence and loss in a standard Fabry–Perot cavity suffices to engineer non-Hermitian singularities. This work opens new avenues for exploring and enhanced sensing in precision photonics as well as EP physics in cavity quantum electrodynamics.