• Photonics Research
  • Vol. 10, Issue 4, 1134 (2022)
Stefano Biasi†、*, Riccardo Franchi1、†, Filippo Mione, and Lorenzo Pavesi
Author Affiliations
  • Nanoscience Laboratory, Dipartimento di Fisica, Università di Trento, 38123 Trento, Italy
  • show less
    DOI: 10.1364/PRJ.450402 Cite this Article Set citation alerts
    Stefano Biasi, Riccardo Franchi, Filippo Mione, Lorenzo Pavesi. Interferometric method to estimate the eigenvalues of a non-Hermitian two-level optical system[J]. Photonics Research, 2022, 10(4): 1134 Copy Citation Text show less

    Abstract

    Non-Hermitian physics has found a fertile ground in optics. Recently, the study of mode coalescence, i.e., exceptional points, has led to the discovery of intriguing and counterintuitive phenomena. Degeneracies are typically modeled through the coupled mode theory to determine the behavior of eigenstates and eigenvalues. However, the complex nature of the eigenvalues makes their characterization from the response spectrum difficult. Here, we demonstrate that a coherent interferometric excitation allows estimation of both the real and imaginary parts of the eigenvalues. We study the clockwise and counter-clockwise modes in optical microresonators both in the case of Hermitian and non-Hermitian intermodal coupling. We show the conditions by which a resonant doublet, due to the dissipative coupling of counter-propagating modes caused by surface roughness backscattering, merges to a single Lorentzian. This permits us to estimate the optimal quality factor of the microresonator in the absence of modal coupling caused by backscattering. Furthermore, we demonstrate that a taiji microresonator working at an exceptional point shows a degeneracy splitting only in one propagation direction and not in the other. This follows from the strongly non-Hermitian intermodal coupling caused by the inner S-shaped waveguide.
    iddt(αCCWαCW)=(ω0i(γ+Γ)iβ12iβ21ω0i(γ+Γ))(αCCWαCW)2Γ(Ein,LEin,R),

    View in Article

    (Eout,REout,L)=(Ein,LEin,R)+i2Γ(αCCWαCW),

    View in Article

    εout,R=(12Γ(iΔω+γ+Γ)(iΔω+γ+Γ)2β12β21)εin,L+(2Γβ12(iΔω+γ+Γ)2β12β21)eiϕεin,R,

    View in Article

    εout,L=(12Γ(iΔω+γ+Γ)(iΔω+γ+Γ)2β12β21)eiϕεin,R+(2Γβ21(iΔω+γ+Γ)2β12β21)εin,L,

    View in Article

    ω(b1b2)=(ω0i(γ+Γ+g1)ig2ig2ω0i(γ+Γg1))(b1b2)2Γ(εin,L+εin,R2εin,Lεin,R2),

    View in Article

    λ1,2=ω0±β12β21i(γ+Γ),

    View in Article

    v1,2=11+|g1g12g22g2|2(g1g12g22g21)

    View in Article

    h:=iβ12β21*2,n:=β12+β21*2.

    View in Article

    v1,2=11+|sin[θh]1cos[θh]|2(isin[θh]1cos[θh]1),

    View in Article

    λ1,2=ω0±|β|i(γ+Γ),

    View in Article

    |εout,R|2=|εout,L|2=(14γΓ(Δω|β|)2+(γ+Γ)2)|ε0|2.

    View in Article

    λ1,2=ω0|β12||β21|sin[φ12+φ212]i(Γ+γ|β12||β21|cos[φ12+φ212]).

    View in Article

    εin,R=|β21||β12|εin,Landθ=±π2+2πm,

    View in Article

    (|εout,R|2|εout,L|2)=(14(γγ˜)Γ(Δωβ˜)2+(γγ˜+Γ)2)(|εin,L|2|εin,R|2),β˜:=|β12||β21|sin[(φ12+φ21)/2],γ˜:=|β12||β21|cos[(φ12+φ21)/2].

    View in Article

    K=(0iβ12iβ210).(A1)

    View in Article

    β12=β21*=:β.(A2)

    View in Article

    g1=i|β|sin[θ]R[g1]=0,(A3)

    View in Article

    g2=|β|cos[θ]I[g2]=0,(A4)

    View in Article

    v1,2=11+|sin[θ]1cos[θ]|2(isin[θ]1cos[θ]1).(A5)

    View in Article

    Stefano Biasi, Riccardo Franchi, Filippo Mione, Lorenzo Pavesi. Interferometric method to estimate the eigenvalues of a non-Hermitian two-level optical system[J]. Photonics Research, 2022, 10(4): 1134
    Download Citation