TUNABLE VERNIER EFFECT LASER EMISSION DEVICE

Abstract

The invention relates to a wavelength-tunable laser emission device (1), comprising a cavity (CA) delimited by a first and a second Sagnac mirror (M1, M2). The cavity comprises an amplifying medium (MA) and a tunable spectral filter using the Vernier effect (F). This filter comprises at least three resonant rings (R.sub.1, R.sub.2, R.sub.N-1, R.sub.N) arranged in cascade, each resonant ring integrating a loop mirror with wavelength tunable reflectivity.

Claims

1. A wavelength tunable laser emission device, comprising: a first and a second Sagnac mirror; a cavity delimited by the first and second Sagnac mirrors, the cavity comprising an amplifying medium and a tunable spectral filter using the Vernier effect, wherein said tunable spectral filter comprises at least three resonant rings arranged in cascade and wherein each resonant ring of the at least three resonant rings integrates a loop mirror with tunable wavelength reflectivity.

2. The device according to claim 1, wherein each resonant ring of the at least three resonant rings comprises a Mach-Zehnder interferometric section.

3. The device according to claim 1, wherein each of the first and second Sagnac mirrors is comprised of an adiabatic directional coupler fed back through a waveguide.

4. The device according to claim 1, wherein the cavity further comprises a phase shift section.

5. The device according to claim 1, wherein one of the first and second Sagnac mirrors is partially reflective.

6. The device according to claim 5, further comprising, outside the cavity on the side of that one of the first and second Sagnac mirrors which is partially reflective, a tilted grating coupler to/from a single-mode optical fibre.

7. The device according to claim 1, wherein the amplifying medium comprises a III-V heterostructure.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0023] Other aspects, purposes, advantages and characteristics of the invention will become clearer upon reading the following detailed description of the preferred embodiments of the invention, given as a non-limitative example, and made with reference to the appended drawings in which:

[0024] FIG. 1 is a diagram representing a possible architecture of a laser emission device in accordance with the invention;

[0025] FIG. 2 is a diagram of a resonant ring provided with a loop mirror with wavelength tunable reflectivity;

[0026] FIG. 3 illustrates coincidence at 1261 nm of the emission peaks of each of five resonant rings of a spectral filter that can be used in the device according to the invention, in the absence of a phase shift applied to the rings;

[0027] FIG. 4 represents the emission peaks, around 1361 nm, of each of the resonant rings of the five-ring spectral filter, in the absence of a phase shift applied to the rings;

[0028] FIG. 5 represents coincidence at 1361 nm of the emission peaks of each of the resonant rings of the five-ring spectral filter, in the presence of a phase shift applied to the rings;

[0029] FIG. 6 represents the transmission spectrum of the five-ring filter respectively in the absence of a phase shift applied to the rings (coincidence of the individual resonances at 1231 nm) and in the presence of a phase shift applied to the rings to achieve a coincidence of the individual resonances at 1361 nm.

DETAILED DISCLOSURE OF PARTICULAR EMBODIMENTS

[0030] With reference to FIG. 2, one object of the invention is a wavelength tunable laser emission device 1. This device comprises: [0031] a first and a second Sagnac mirror M1, M2; [0032] a cavity CA delimited by the first and second Sagnac mirrors M1, M2, the cavity comprising an amplifying medium MA and a tunable spectral filter using the Vernier effect F.

[0033] In a favoured embodiment of the invention, the amplifying medium comprises a III-V heterostructure. By III-V type heterostructure, it is intended the use of binary, ternary, quaternary materials, which may be chosen from the following non-exhaustive list: InP, GaAs, InGaAlAs, InGaAsP, AlGaAs, InAsP, AlInAs. The heterostructure of such an amplifying medium, also called a gain medium, may include a stack of various layers, such as a stack of layers forming quantum wells sandwiched between a first doped, preferably N-doped, layer, and a second doped, preferably P-doped, layer.

[0034] This favoured mode is thus based on the technology of heterogeneous integration of III-V materials with silicon, which enables photonic circuits associating III-V optical sources with silicon-based components to be made. III-V heterogeneous on silicon integration can especially consist in bonding a portion of III-V active material capable of emitting light to a “passive” circuit etched on the surface of a silicon-on-insulator (SOI) substrate. A photonic circuit with an active III-V hybrid on silicon section thus generally comprises: [0035] an SOI substrate carrying a silicon waveguide, [0036] a gain structure that includes at least one III-V heterostructure optical amplifying medium, transferred by bonding to the SOI substrate, [0037] a thin oxide layer serving as a connecting layer and which separates the gain structure from the silicon waveguide.

[0038] The III-V heterostructure is arranged to overlie a section of the silicon waveguide to form a hybrid waveguide section with the same. At this hybrid waveguide section, the vertical proximity of the III-V and silicon guides causes a coupled optical mode to occur, resulting from the hybridization between the fundamental eigenmodes of each of these guides. This coupled mode is transferred from the active III-V/Silicon hybrid active section to passive pure silicon light propagation sections arranged on either side of the hybrid waveguide section. For this purpose, the silicon waveguide is structured to have a modal transition section (taper) between the hybrid active section and the propagation sections.

[0039] The propagation sections and hybrid section are delimited by the Sagnac mirrors M1, M2 which thus make up an optical feedback structure capable of forming a resonant cavity CA for the amplifying medium MA. One of the mirrors, here M1, is a high reflectivity mirror which has for example a reflectivity greater than 90%, while the other mirror, here M2, is a low reflectivity mirror (partially reflecting mirror) which has for example a reflectivity less than 50%, typically between 35 and 10%. The low-reflectivity mirror thus forms the optical output of the laser emission device 1. This optical output can be equipped with a grating coupler CI to/from a single-mode optical fibre. This grating coupler is preferably a tilted grating which has the advantage of a reduced reflectivity. The principle of such a tilted grating is for example described in the publication by Yanlu Li et al, “Tilted silicon-on-insulator grating coupler with improved fibre coupling efficiency and low back reflection based on a silicon overlay”, IEEE Photonics Technology Letters, vol. 25, no. 13, pp. 1195-1198, July 2013.

[0040] In comparison with a diffraction-based DBR mirror, a Sagnac mirror is comprised of a directional coupler fed back through a waveguide and only works by constructive/destructive interference between two guides, which simplifies manufacture thereof since there is no sub-wavelength grating to make. The advantageous Sagnac loop concept has been widely used in the field of optical fibres, a field where silica guides show very low chromatic dispersion, so that Sagnac fibre loops are considered as achromatic. However, this property is no longer valid in integrated optics because when using a directional coupler based on silicon microguides, the coupling rate is wavelength-dependent. Nevertheless, in a favoured embodiment of the invention, each of the first and second Sagnac mirrors M1, M2 uses an adiabatic directional coupler. The adiabatic directional coupler exhibits near-perfect relative coupling ratios over 100 nm of bandwidth, typically relative coupling ratios between 0.45 and 0.55 over the entire bandwidth, for example over a band between 1260 nm and 1360 nm. An example of the development of such an adiabatic coupler is given, for example, in the publication by Karim Hassan et al, “Robust silicon-on-insulator adiabatic splitter optimized by metamodeling”, Applied Optics 56(8) 2017.

[0041] In addition to the amplifying medium MA, the cavity CA may include a phase control section P capable of tuning the modes of the Fabry-Perot cavity CA, by being thermally controlled by means of a heater placed above the section P.

[0042] The cavity CA additionally includes a tunable spectral filter using the Vernier effect F. This filter is a multi-ring resonator comprising several resonant rings arranged in cascade. As represented in FIG. 2, each resonant ring A integrates a loop mirror with wavelength tunable reflectivity MBR. As seen previously, such rings have a low reflectivity due to the addition of the tunable reflectivity loop mirror, which enables back propagation modes generated by light backscattering to be removed. In a favoured embodiment represented in FIG. 2, each resonant ring A integrates a loop mirror LM and an adjustable phase section. The adjustable phase section is typically a Mach-Zehnder interferometric section MZI comprising two arms able to be phase-shifted from each other by means of a thermo-optical phase-shifting element PS acting on one of the arms.

[0043] The addition to each resonant ring of the adjustable reflectivity mirror significantly increases the effective length of each resonator. As seen previously, this increase reduces the free spectral range, which is not desirable for high tunability. Anyway, in order to take advantage of this type of low reflectivity resonator while at the same time benefiting from a Vernier effect offering a wide tunability, the filter of the device according to the invention is not provided by two rings as is the case in the state of the art but by a larger number of rings, namely at least three resonant rings R1, R2, R.sub.N-1, R.sub.N as represented in FIG. 1.

[0044] An advantage of such a number of rings is that the overall FSR of the ring systems is no longer restrictive: two resonances can coincide, if the third or fourth resonance does not coincide, there will be no overall resonance of the system. This means that unlike the case with two rings, the difference in order between the resonators can be greater than 1. So there is no need to select the lowest possible ΔFSR since the tunability is no longer limited by

[00003]$S{R}_t=\frac{FSR1\times FS{R}_2}{FS{R}_2-FS{R}_1}.$

So both high tunability and good SMSR can be achieved.

[0045] An example of dimensioning the at least three rings of the filter is given below, in connection with an exemplary embodiment where the filter consists of five rings.

[0046] A reference ring with a free spectral range FSR.sub.0 is considered. The other rings of the filter have an FSR expressed as FSR.sub.i=α.sub.iFSR.sub.0. The free spectral range of the 2-ring subsystems 0 and i is given by

[00004]$FS{R}_{i-0}=\frac{{\alpha }_i}{1-{\alpha }_i}FS{R}_0$

while the tree spectral range of the N-ring system is given by

[00005]$.Math.\frac{{\alpha }_i}{1-{\alpha }_i}{\mathrm{FSR}}_0.$

[0047] For example, if four rings are considered such that FSR.sub.1=0.9*FSR.sub.0, FSR.sub.2=0.8*FSR.sub.0 and FSR.sub.3=0.7*FSR.sub.0, the overall free spectral range of the system is 0.9*0.8*0.7/(0.1*0.2*0.3)=84*FSR.sub.0, that is 126 nm if typical FSR0 of 1.5 nm is assumed. it is thus noticed that the free spectral range of an N-ring system increases with the number of rings, which makes a larger tuning range available.

[0048] Let a waveguide with an effective index n.sub.eff and a minimum resonant ring perimeter L.sub.0. The lowest wavelength to be reached in the system is selected: λ.sub.0=1.26 μm. The resonance order of the ring 0 is expressed according to

[00006]$m_0=\mathrm{int}\left(\frac{L_0{n}_{eff}}{{\lambda }_0}\right)$

where the int function is the integer part of the result (i.e. the value rounded down), and its free spectral range is

[00007]$FS{R}_0=\frac{L_0{n}_{\mathrm{eff}}}{m_0}-\frac{L_0{n}_{eff}}{m_0-1}.$

[0049] A tunability range is then selected, for example Δλ=100 nm, and the λ.sub.m=λ.sub.0+Δλ is noted. The resonance order shift for ring 0 to reach the maximum wavelength is expressed according to

[00008]$N=m_0-\frac{L_0{n}_{eff}}{{\lambda }_m}$

and the free spectral range of ring 0 at λ.sub.m according to

[00009]$FS{R}_m=\frac{L_0{n}_{eff}}{m_0-N}-\frac{L_0{n}_{eff}}{m_0-N-1}.$

[0050] The selection of the other rings in terms of free spectral range difference from the reference ring 0 (typically taking ΔFSR>FWHM) is as follows. The ring i should have a free spectral interval FSR.sub.i by imposing its resonance with the condition λ.sub.i=λ.sub.0. Hence

[00010]$m_i=1+int\left(\frac{{\lambda }_0}{FS{R}_i}\right)$$\mathrm{and}$$L_i=\frac{{\lambda }_0{m}_i}{n_{eff}}.$

This selection ensures coincidence at λ.sub.0 but is not restrictive on the geometry of the other rings. FIG. 3 illustrates the transmission spectrum T as a function of wavelength of a five-ring filter, with respective diameters 350, 368, 388, 411 and 437 μm, for which a resonance coincidence has been imposed at λ.sub.0=1261 nm.

[0051] Since the filter should be tunable in the range AA, a resonance of the ring system is sought at λ.sub.s such that λ.sub.0<λ.sub.s<λ.sub.m. For this, for each ring

[00011]$N_{i,s}=m_i-int\left(\frac{L_i{n}_{eff}}{{\lambda }_s}\right)$

is determined, that is the resonance order closest to λ.sub.s at

[00012]${\lambda }_{i,s}=\frac{n_{eff}{L}_i}{m_i-N_{i,s}}.$

The FSR of each ring is then calculated at λ.sub.s, FSR.sub.i,s. For a given λ.sub.s, and as represented by the window FS in FIG. 4, there is always a resonance of each ring at less than half FSR.

[0052] The rings are then attempted to be tuned to be coincident at λ.sub.s. The phase shift to be applied to each ring is written as Δϕ.sub.i=2π(λ.sub.s−λ.sub.i,s)/FSR.sub.i,s. This phase shift can be applied by means of a heater placed above each ring. The individual resonances of the rings at λ.sub.0+100 nm have been represented in FIG. 4, in the absence of a phase shift applied to the rings. A lack of overall resonance of the system is noticed. Additionally, the individual resonances of the rings at λ.sub.0+100 nm have been represented in FIG. 5, with the application of the phase shift Δϕ.sub.i. A coincidence of the individual resonances and thus an overall resonance of the system are noticed.

[0053] Additionally, the transmission spectrum T of the 5-ring filter has been represented in FIG. 6 without applying a phase shift (dotted lines; resonance at 1261 nm) and by applying Δϕ.sub.i (solid lines; resonance at 1361 nm). The phase shift applied is less than pi, that is the resonance of the rings is shifted by a maximum of half FSR. The filter is thus tunable over 100 nm with an SMSR of more than 60 dB

[0054] Ultimately, the laser emission device according to the invention can consist of a low-reflection grating coupler, Sagnac loop mirrors with improved bandwidth by using broadband adiabatic directional couplers, and in the core of the tunability mechanism a series of resonant rings with low reflectivity. The use of at least three rings makes them compatible with providing a Vernier effect offering wide tunability.