Layered materials have recently emerged as a promising class of materials for optoelectronics . These materials possess different band gaps leading to a large range of conductivities and the ability to emit and detect light at different wavelength ranges . For example, graphene has no band gap and behaves like a metal; semiconducting transition metal dichalcogenides (TMDCs), such as WS2, MoS2, MoSe2 and WSe2, and black phosphorous have band gaps on the order of 1–2.5 eV, and with its very wide band gap (~6 eV) hexagonal boron nitride (h-BN) is an excellent insulator. Going beyond usual conductivity, exotic properties like superconductivity (TaS2, NbSe2) , , ferroelectricity (CuInP2S6) , and ferromagnetism (Cr2Ge2Te6, CrI3) , ,  have been recently reported in these atomically thin materials. Figure 1A and B show the schematic of the atomic structure for a typical TMDC and graphene. While the bulk of the research in these materials has focused on material characterization, optical spectroscopy and electrical transport measurements, integration of these materials with nanophotonic and nanoelectronic devices is gaining attention. Such integration efforts are primarily motivated by the ease of transferring these extremely thin materials on any substrate without needing explicit lattice matching. Unlike many other quantum confined structures, such as III-V quantum wells or self-assembled quantum dots, these materials stick to the substrate via van der Waals force, and do not require expensive molecular beam epitaxy processes, or wafer bonding. This provides a unique opportunity to develop hybrid photonic platforms where the fabrication processes of the active and passive devices can be completely decoupled. Large-scale, passive photonic integrated circuits will be fabricated using existing foundry systems , and subsequently layered materials will be transferred on the pre-fabricated photonic chip to build the active devices, including modulators, detectors, light sources (lasers or light-emitting diodes) and nonlinear optical switches.
Over the last decade, the growth and extensive characterization of these materials have revealed their potential for various electronic and optoelectronic applications. Graphene, inarguably the most studied layered material , has found applications in building transistors , radio-frequency devices , and electronic sensors . In the optoelectronics community, the large electro-optic tunability ,  and strong photo-absorption  of graphene generated great interest. However, the extreme thinness of the material, the source of the unusual properties and unprecedented material compatibility of these layered materials also limits the effective light-matter interaction for optoelectronic device applications. To solve this problem, optical device engineers have used various nanophotonic devices integrated with graphene to enhance the light-matter interaction. For example, using nanophotonic waveguides integrated with graphene, the effective light-matter interaction can be increased to build an electro-optic modulator , , or a photo-detector with high efficiency , , . Further light-matter enhancement and reduction in the size of the device is possible using optical resonators, including photonic crystals , , ring resonators  and plasmonic resonators , , . Optical resonators enhance the light-matter interaction by confining the light both temporally and spatially. For a cavity, the extents of the temporal and spatial confinement are quantitatively given by the quality factor (Q) and mode volume (V), respectively . This trend of integrating graphene with nanophotonic devices continued with TMDCs , , . Cavity integrated TMDCs have been used to demonstrate optically pumped lasing , , , cavity-enhanced electroluminescence  and strongly coupled exciton-polaritons , . In all these devices, the enhancement due to the cavity depends on the Purcell factor Fp~Q/V , .
The success of optical resonators to enhance the light-matter interaction in layered materials motivated researchers to study cavity nonlinear optics using these materials. Due to their bosonic and chargeless nature, the interaction strength between photons is very weak and nonlinear optical effects appear only at very high power. This remains an outstanding challenge to be overcome for optics to be used for any compute applications. However, the required power can be lowered using optical resonators. For a cavity-enhanced second-order χ(2) (third-order χ(3)) nonlinear switch, the threshold power is proportional to V/Q3 (V/Q2) . The ability of nano-cavities to spatially confine light of wavelength λ to an extremely small mode volume [V~(λ/n)3 where n is the refractive index of the cavity material], and store light for a few nanoseconds (τph=Qλ/2πc) provides an opportunity to realize optical nonlinearity at the few photon level. Thus, cavities can significantly enhance the intrinsic optical nonlinearity of the layered materials. In this paper, we review the recent progress in the field of cavity nonlinear optics with layered materials. We note that the nonlinearity of layered materials is comparable to that achievable of existing material systems, including quantum confined structures and bulk materials. However, the ability to integrate these materials with any material systems provides an excellent opportunity to build hybrid integrated nonlinear photonic systems. Apart from the cavity-enhanced second-order and third-order nonlinear optics, the layered materials exhibit saturable absorption and nonlinear polariton-polariton interaction. Finally, the layered materials host defect centers, which are essentially two-level systems, and will provide a route to obtain single photon nonlinearity. Along with reviewing the existing works, we will lay out the outstanding challenges and several future directions of the cavity nonlinear optics with these emerging layered material systems.
2 Nonlinear processes in layered materials
In recent years, several experiments with stand-alone layered materials measured their nonlinear optical coefficients. Table 1 summarizes the measured χ(2) and χ(3) coefficients for different layered materials. The large χ(2) values near ~800 nm originate from the energetic proximity of the excitons in TMDCs, and thus generally come with large losses , , , , . These experiments also clearly showed that the second-order nonlinearity in TMDCs is the strongest at the single layer limit. With an even number of layers, this nonlinearity disappears, as the material becomes centrosymmetric. Thus, the nonlinear signal works as a convenient microscopy tool for probing the number of layers in the TMDC crystal. Additionally, a six-fold polarization pattern is found in the second harmonic signal reflecting the hexagonal crystal structure of the TMDCs (Figure 1C and D). Thus, nonlinear spectroscopy of the layered materials has become an indispensable tool to determine the crystalline orientation, thickness uniformity, layer stacking, and single-crystal domain size of atomically thin films , , , . In fact, this technique is critical for creating the heterostructures of TMDC layers, as the relative crystal orientation determines the heterostructure’s electronic band structure . Researchers have also demonstrated that the centrosymmetry of bilayer MoS2 can be broken with a static electric field, enabling second harmonic generation (SHG) . Note that this electric field-induced SHG can potentially create opportunities for electro-optic switching applications. Another way to break the symmetry will be via straining the bilayers. Straining monolayers and bilayers of MoS2, researchers have already demonstrated band gap engineering and photoluminescence (PL) control , , . However, strain induced nonlinear optics with layered matierlas have yet to be reported. In addition to experimental measurements, several research groups have reported atomistic simulation studies to estimate the nonlinear coefficients for different layered materials , , , and have also analyzed the effect of substrates . This work models the nonlinearity of layered materials as zero-thickness interfaces, and showed that without careful theoretical modelling, the extracted value of the nonlinear coefficient can be largely exaggerated.
Most studies with TMDCs have focused on pumping near the exciton resonance (~800 nm) and creating a second harmonic above the band gap at ~400 nm. A more interesting regime from an application point of view is to pump near 1550 nm and create a second harmonic signal at 775 nm. This wavelength range is particularly important for interfacing with telecommunication technologies. Such nonlinear devices could be utilized for optical bistability for a telecommunication wavelength laser . In this wavelength range, the absorptive loss at the fundamental frequency is also minimal. Researchers have demonstrated SHG under pump near 1550 nm in stand-alone, monolayer WSe2  and in GaSe . In WSe2, researchers also demonstrated electric field controlled SHG showing the nonlinear optical effect far from the excitonic frequency is strongest at twice the exciton frequency. Thus, by changing the exciton frequency, one can change the effective nonlinearity. The reported χ(2) values for WSe2 are around 60 pm/V at 1550 nm and for GaSe, the χ(2) value is estimated to be at least one order of magnitude larger (Table 1).
In addition to second-order nonlinear processes, third-order nonlinear processes have also been studied using layered materials. Being centrosymmetric, graphene does not possess intrinsic second-order nonlinearity, and hence graphene is primarily studied for third-order nonlinear processes. Several research papers explore third harmonic generation , cascaded third harmonic generation , and four wave mixing . Layer-dependent third harmonic generation is also recently reported in black phosphorous . In TMDCs, researchers have demonstrated intensity-dependent refractive index by exploiting the third-order nonlinearity .
We note that, the measured values of the nonlinear coefficients in infrared wavelengths (~1500 nm) are comparable to the χ(3) of bulk silicon (~10−19 m2/V2) or the χ(2) of bulk III–V materials, such as GaAs or GaP (~100×10−12 m/V), as a research article has pointed out in the past . Thus, the utility of nonlinear layered materials does not necessarily originate from a large nonlinearity per se, but rather from their tunable optical nonlinearity, their ease of integration onto arbitrary substrates, ease of patterning, and the possibility of creating a hybrid platform. For example, complementary metal-oxide-semiconductor (CMOS)-compatible materials, such as silicon and silicon nitride, lack second-order optical nonlinearity. By integrating layered materials on top of them, we can realize second-order nonlinearity in a CMOS compatible way. Thus, in our opinion, the true benefit of layered materials lies in creating hybrid, active photonic systems.
3 Cavity-enhanced second harmonic generation
While there is significant research progress in the nonlinear optics of layered materials, the extreme thinness of the material poses a serious problem for practical applications. This problem can be ameliorated by using an optical resonator to enhance the effective nonlinearity. While the effective nonlinearity in a layered material clad cavity is proportional to the material nonlinearity, the material interacts only with a small portion of the field on the surface. Hence it is important to estimate the effective nonlinearity in the presence of an optical resonator.
3.1 Modeling of the nonlinear cavity
In a recent work, Majumdar et al.  analyzed the effective nonlinearity of a layered material clad nano-cavity for second-order nonlinear optics. They assume that the optical cavity is formed in a dielectric slab with the field profile varying sinusoidally inside the slab, and decaying exponentially outside (Figure 2A). While such a model is a simplification, and neglects the actual mode profiles of the cavity, it allows the authors to obtain a closed form analytical expression, which provides an intuitive understanding of the effective nonlinearity. They find that the nonlinear interaction strength gnl is given by :
where ħ is the reduced Planck’s constant, ωo is the fundamental angular frequency, χ(2) is the value of the second-order nonlinear coefficient, d is the thickness of the layered materials, ε is the dielectric constant of the layered material, S signifies the ratio of the field strength at the surface and center of the slab, and σx and σy are the confinement length of the optical field inside the resonator along x and y directions. Note that, a stronger localization within the nonlinear material will increase the nonlinear interaction strength. A cavity helps to confine light and thus reduces both σx and σy. They also find that the interaction strength depends on the product of the nonlinear coefficient and the material thickness, as one would expect. Thus, the small thickness of the layered materials indeed limits the interaction strength. However, the analytical expression also shows that by enhancing the field on the surface, i.e. by increasing the value of S, the effective nonlinearity can be significantly enhanced. This criterion necessitates rethinking the design of the dielectric optical cavities, where the field is generally minimized on the surface to reduce the loss. In a more recent paper, the authors have also shown that layered materials provide a novel way to satisfy phase-matching condition in second-order nonlinear optics as elaborated below.
In deriving the analytical expression of the nonlinear interaction strength, it was previously assumed that the phase-matching condition is fully satisfied. In second-order nonlinear optics, the phase-matching condition is equivalent to satisfying the momentum conservation of the interacting waves . In a nano-cavity, satisfying this condition amounts to having a good modal overlap between the fundamental and the second harmonic modes. Moreover, for high efficiency, the cavity needs to support modes at both frequencies. Satisfying both of these requirements is difficult, and to date, the proposed designs require stringent fabrication tolerance, and often involve significant computational resources . A single monolayer does not significantly change the confined mode profiles in the cavities as the interaction is evanescent in nature, and due to the extreme thinness of the material, only slightly perturbs the cavity mode. Thus, 2D materials provide an excellent opportunity to decouple the cavity design and nonlinear material design. Starting with any cavity, and intelligently patterning 2D materials on top of it, the phase-matching condition can be satisfied. A schematic of a nano-resonator with patterned 2D material on top is shown in Figure 2B. Our theoretical analysis shows that such patterning can maintain a good overlap integral, and thus retain significant effective nonlinearity, even when the modes are largely mismatched .
The model described above primarily works for a dielectric optical resonator, and currently most of the reported results on cavity nonlinear optics with layered materials involve dielectric resonators. However, plasmonic resonators already are being used to enhance the linear properties of the layered materials , including light emission , , electro-optic modulation  and photo-detection . Recently, evidence of polariton formation has also been observed in plasmonic cavities . Plasmonic resonators can also be engineered to have multiple resonances , and thus can be ideal for second and third harmonic generation. While the quality factors of plasmonic resonances are significantly lower compared to dielectric resonators due to metallic losses, they provide an extremely small mode volume to which significantly enhances the light-matter interaction. Additionally, plasmonic effects can be exploited to confine light to lie in a single plane, where the layered material can be placed. Thus, plasmonic resonators are expected to play an important role in enhancing nonlinear optical effects in layered materials. Another important research direction could be to develop hybrid plasmonic-dielectric resonators to realize both high Q as is characteristic of dielectric cavities, with the low V that is characteristic of plasmonic cavities.
3.2 Second harmonic generation with single mode cavity
Current experimental efforts on SHG with layered materials are primarily focused on a single cavity mode coupled to exfoliated layered materials. Using a tungsten diselenide (WSe2) clad silicon photonic crystal cavity, Fryett et al.  showed enhanced SHG. In this work they used a pulsed laser operating within the telecommunication band (~1550 nm). Figure 3A shows the scanning electron micrograph of a WSe2 clad silicon photonic crystal cavity. The cavity modes are near 1490 nm. When the cavity is resonantly excited using a pulsed laser, they observed a strong second harmonic signal around 745 nm (Figure 3B). In the second harmonic signal, they observed a Gaussian background which comes from the doubling of the laser wavelengths, which are off-resonant from the cavity. In this background, they observed a Lorentzian peak at exactly the half-wavelength of the cavity resonance, signifying the cavity-enhanced SHG. The reported enhancement is only ~100, primarily because of the lack of a cavity mode at the second harmonic frequency and low Q-factor of the cavity (Q~100). Moreover, silicon absorbs a significant amount of second harmonic signal. A promising solution will be to make a doubly resonant cavity out of wide bandgap materials, such as silicon nitride  or silicon dioxide . Researchers also recently demonstrated continuous wave (CW) SHG using GaSe coupled with silicon photonic crystal cavity with a pump laser at ~1550 nm . The required optical power in this work is only microwatts, primarily due to the high Q-factor and small mode-volume of the photonic crystal cavities.
In another experiment, Day et al.  demonstrated SHG using MoS2 integrated inside a distributed Bragg reflector (DBR) cavity (Figure 3C and D). In this experiment, the DBR is formed by using alternating layers of silicon nitride and silicon dioxide to minimize the absorption of light. Here, the SHG is observed under pulsed excitation at 800 nm. The reported enhancement is ~10. The lower enhancement factor can be attributed to low Q-factor of ~20, and the large mode-volume of the DBR cavity. An open hemiconfocal cavity geometry  might be more suitable to reduce the mode volume and thus further enhance the nonlinearity.
3.3 Second harmonic generation with double mode cavity
The enhancement factor can be significantly increased by using cavity modes both at the fundamental and the second harmonic frequency. Such mode engineering is theoretically difficult at the nano-scale, but can be easily realized in a DBR-based Fabry-Perot cavity. However, inevitable fabrication errors prevent the cavity modes from appearing exactly at the desired resonance wavelengths. Yi et al.  solved this problem by creating a mechanically tunable Fabry-Perot cavity, where the bottom mirror is a DBR, and the top mirror is a capacitively actuated silver mirror (Figure 4A). The capacitive tuning enables changing the cavity length, and thus cavity resonances. Via mechanical tuning, it is possible to bring both the fundamental and the second harmonic modes to the desired frequencies. In this experiment, they used MoS2 as the nonlinear material, and despite their low cavity Q-factor, the reported enhancement is ~3000 (Figure 4B and C). This experiment used a pulsed excitation near 930 nm. Further improvement is possible by improving the cavity Q-factor, and reducing the mode-volume, which is often very large in Fabry-Perot cavities.
Phase-matched SHG was also recently reported in a silicon photonic waveguide using MoSe2 . By engineering the waveguide cross-section, the effective mode-indices of the fundamental and second harmonic modes are matched, which ensures the phase-matching of the light at the fundamental and second harmonic frequencies. Similar methods have been used for designing phase-matched ring resonators for cavity nonlinear optics using aluminum nitride . Such a phase-matched ring integrated with layered materials can enhance the efficiency of the second-order nonlinear processes.
All the existing experiments so far have reported significantly lower SHG efficiency, compared to the theoretical predictions. For a given power, the efficiency can be improved by increasing the quality factor and reducing the mode volume. Another limiting factor might be the transfer of the layered materials, which generally involves organic polymers, and might introduce excess loss coming from the polymer residues. Having the resonances at both the fundamental and the second harmonic frequencies will also increase the efficiency significantly. Along with innovating cavity structures, new layered materials with stronger nonlinear optical properties, such as multiferroics , can also improve the overall efficiency of SHG.
4 Third-order nonlinear processes
While most of the recent works on cavity nonlinear optics using layered materials primarily focused on second-order nonlinear optics, the first demonstration of cavity nonlinear optics was with third-order nonlinearity of graphene. Gu et al.  demonstrated optical bistability and regenerative oscillation using a graphene-clad silicon photonic crystal cavity. Figure 5A shows the fabricated photonic crystal cavity which is coupled to a waveguide. Graphene is transferred onto the cavity, and under ~1562 nm CW excitation optical bistability is observed (Figure 5B). The threshold power where the bistable behavior appears in graphene-silicon resonator is lower than that observed with a bare silicon photonic crystal cavity.
In the authors’ opinion, however, the third-order nonlinearity with 2D materials is not as attractive as second-order nonlinear optics from an application point of view. As most materials already possess strong third-order nonlinearity, and the measured values of nonlinearity for graphene and black phosphorous are almost the same order of magnitude as silicon, the application area of third-order nonlinear optics with layered material is debatable . However, for many applications, requiring high power operation, silicon is not ideal due to high two-photon absorption when operating at the telecommunication wavelength. In those applications, silicon nitride and silicon dioxide are gaining popularity due to their wide band gaps . The magnitude of the third-order nonlinear coefficient in layered materials is higher compared to that of the nitride (χ(3)~1×10−20 m2/V2)  or oxide (χ(3)~2.5×10−22 m2/V2) , and will play an important role in realizing low-power nonlinear optics.
5 Saturable absorption
Another promising nonlinear optical effect in layered materials is their saturable absorption. Due to the extreme thinness of layered materials, their photo-absorption can be easily saturated with low optical power. A common application of saturable absorption is the integration into optical cavities to generate pulsed laser sources, both in fiber and free space systems. Many recent papers on pulsed lasers have utilized layered 2D materials as the saturable absorption material of choice , , . Most of these works used graphene as the saturable absorber. One particularly appealing aspect of graphene is its broadband absorption due to its lack of a band gap, which allows mode-locking over a large wavelength range, including in the mid-infrared wavelengths. Figure 6A shows an experimental setup with a graphene saturable absorption mirror . In this work, stable mode-locked laser pulses as short as 729 fs were obtained with a repetition rate of 98.7 MHz and an average output power of 60.2 mW at ~2 μm (Figure 6B). In addition to the free-space setup, saturable absorption in graphene was used in a fiber laser to demonstrate mode-locking (Figure 6C) . In this work, they created a passively mode-locked erbium-doped fiber laser working at 1559 nm, with 460 fs pulse duration (Figure 6D). Recently, several works reported similar mode-locked laser systems with a variety of atomically thin materials including black phosphorous , MoS2  and WS2 . Additionally, researchers have used black phosphorous, WS2 and MoS2 solutions as saturable absorbers to construct passively Q-switched Nd:YVO4 lasers, with pulse durations of few nanoseconds .
6 Nonlinear exciton-polaritons
So far, most of the nonlinear optical effects we discussed are observed with light sources off-resonant from the exciton. Very near the exciton resonances, a large nonlinearity can be realized using the polaritonic system formed by strong coupling between the cavity-confined photons, and the excitons in the layered materials. Recent works reported observation of strongly coupled exciton-polaritons using layered materials, including MoS2 and bilayer MoSe2 , . Figure 7A shows the schematic of the open DBR cavity used to demonstrate strong coupling between the cavity mode and the exciton . The open cavity architecture allows tuning the cavity resonance by mechanically displacing one of the cavity mirrors. When the cavity mode is tuned across the excitonic resonance, anti-crossing between the cavity mode and the exciton is observed, signifying strong coupling and polariton formation. Figure 7B shows the upper and lower polaritons measured in PL.
Exciton-polaritons using quantum wells have been previously used to extensively study “quantum fluids of light” . At low excitation power, the exciton-polariton system behaves linearly as the exciton-exciton interaction is weak. Bose-Einstein condensation (BEC) of exciton-polaritons has also been observed by several groups , . The polaritons have much smaller effective mass compared to atoms due to their photonic components, and thus the BEC can be realized at a much higher temperature. Moreover, the extremely large binding energy (~0.2–0.8 eV) in TMDC excitons can potentially allow creation of polaritons and condensates at room temperature. Such condensation has not yet been observed in layered materials, but is theoretically predicted . Theory also predicts observation of topological polaritons  and exciton-mediated superconductivity using the TMDC exciton-polaritons . With higher excitation power, however, one cannot create an arbitrary number of excitons . Thus, the fermionic nature of the constituent electron and hole in the exciton-polariton becomes more prominent in high density exciton-polaritons, and strong polariton-polariton repulsion can be observed. When the exciton density reaches the Mott density, the exciton-polariton system can potentially exhibit BEC-BCS crossover . Thus, layered material based exciton-polaritons and their condensates can potentially provide a strongly nonlinear material platform.
Additionally, the extreme thinness of the layered materials allows for straightforward patterning by etching. Thus, one can easily pattern them to create small islands of layered materials, which should behave like quantum dots (Figure 8A). The size and position of these islands can be easily controlled by lithography . Performance of such quantum dot like structures has been theoretically analyzed . In TMDCs with excitonic Bohr radius of only 1 nm, theoretical analysis showed that when the radius of the patterned material reaches a few tens of nm, single photon nonlinear optics can be observed . Specifically, polaritonic blockade can be realized in these quantum dot like structures. The ability to deterministically position these structures via lithography can potentially create an array of interacting single photon nonlinear systems (Figure 8B). Researchers have already designed and fabricated an array of linear cavities , . The addition of the single photon nonlinearity in each of these cavities will create a testbed to study non-equilibrium quantum many body physics with correlated photons , , .
7 Single photon nonlinear optics
Several theoretical proposals explored the feasibility of reaching single photon nonlinear optics using the second-order and third-order optical nonlinear materials, coupled to optical resonators , . As layered materials can be integrated with high-Q silicon or silicon nitride cavities, it is indeed possible to reach single photon nonlinear optics using the off-resonant nonlinearity. However, the quality factor needed to reach the single photon nonlinear optical regime is generally very high, ~105–106, and it is not yet clear whether such a high Q can be reached with a polymer-based transfer process of layered materials. The creation of the quantum dot like structures by lithography is promising, but the effect of etching on the non-radiative excitonic decay rate is not clear.
A more straightforward route would be to exploit quantum emitters in layered materials. Recently several research groups have reported single quantum emitters in layered materials, particularly in TMDCs and in h-BN , , , . These single emitters originate from the localized defects in the crystals . Figure 9A shows the scanning PL data from a chemical vapor deposition-grown WSe2 flake, where the bright defects can be clearly identified. When such a bright spot is spatially separated, the measured spectrum shows narrow lines, indicative of single defects (Figure 9B). Via second-order autocorrelation measurements under both CW and pulsed excitation (Figure 9C and D), a g(2) (0)<0.5 is measured, which unambiguously proves single photon emission from these defects. Via coupling two-level quantum emitters, such as quantum dots, with an optical cavity, strong nonlinear optical effects, such as single photon switching , ,  and photon blockade , ,  have been observed. A similar performance is expected from the defects in layered materials as well. To this end, Tran et al.  have coupled the single defects in h-BN to plasmonic resonators. The plasmonic pillars enhanced the overall brightness of the emitters by a factor of two. These emitters are also recently excited by two-photon processes . Recently, enhancement of the quantum emitters in WSe2 was also observed using silver nanowires, where the emission was coupled to a surface plasmon polariton mode . Finally, very recently, scalable growth of defects in layered material has been demonstrated . In this work, monolayers of WSe2 and WS2 were transferred in a templated vertical silica nano-pillar, and with high probability the defects were localized near the pillar. The wavelength of the defect emission also can be controlled by the pillar diameter. Such capability of deterministic positioning and wavelength selection can solve the long-standing problem of stochastic positioning and large inhomogeneous broadening of quantum dots, which have largely limited the scalable operation of quantum dots, and other quantum emitters. The defects in layered materials thus can provide a scalable platform of single photon nonlinear devices.
The field of the cavity nonlinear optics with layered materials is in its infancy. The majority of researchers working with layered materials still primarily focus on the spectroscopy and material characterization, and the effort on integration with nanophotonic resonant structures is relatively recent. However, the unprecedented material compatibility, easy availability of the materials, and unique optoelectronic properties of the layered materials have very quickly generated strong interest in the nanophotonics community. Hence, we are hopeful that integration of layered materials with nanophotonic devices will enable more fundamentally new scientific studies, and novel low-power applications in the near future. As explained earlier, all the reported nonlinearities can be enhanced by improving the cavities (larger Q and smaller V), and this will surely drive future research on cavity nonlinear optics with layered material systems. In this section, we elaborate on some of the new and more speculative research directions involving cavity nonlinear optics with layered materials.
8.1 Phase transition layered materials
Phase transition in layered materials, such as MoTe2 and WTe2 has been predicted , , . Bulk phase change materials, such as GeSbTe (GST), have recently generated a lot of interest in the field of integrated nanophotonics due to the large change in the refractive index associated with the structural change in GST , , . Coupled with an optical resonator, such large change in refractive index will enable optical bistability, where the output optical power is a strongly nonlinear function of the input optical power. One major problem of GST, however, is the large amount of loss in the visible and near-infrared frequency. The layered phase change materials have a wider band gap, and can provide a new way to realize a very large change in the refractive indices, while maintaining a low loss.
8.2 Heterostructure of layered materials
Several groups have reported fabrication and characterization of heterostructures of layered materials , . One particularly interesting aspect of the heterostructure is the observation of long-lived inter-layer excitons, where the electron and holes are separated into different layers. This prevents the recombination of the electron and hole pair, and thus long-lived exciton states can be realized. The implication of such long-lived excitons for nonlinear optics is not clear, and can potentially constitute a new research field. For example, what are the implications for exciton-polaritons and exciton-polaritons BEC with long-lived excitons? Furthermore, by separating different TMDC layers by h-BN, a multi-quantum well-like structure can be realized, where the thickness of the nonlinear material can be varied. Researchers have already demonstrated stronger exciton-photon coupling in bilayer MoSe2 separated by h-BN . With N layers, we expect the coupling strength to increase by a factor of
8.3 Valley exciton-polaritons
TMDCs exhibit unique spin-valley physics, which primarily stems from the combination of two features. First, the band gap is at the +K and –K “Dirac valleys”, not at the Brillouin zone center. This gives the electron states a “valley index” (or pseudospin) in addition to real spin , . Optical selection rules are such that right hand circularly polarized light (σ+) couples only to one valley and left hand circularly polarized light (σ−) couples to the other, providing the first solid-state system in which dynamic control of valley pseudospin is possible , , , , , , , . Second, the strong spin-orbit coupling locks the real spin at the band edges to the valley index . Spontaneous transitions between these spin-states are unlikely due to the large mismatch between momentum vectors. Several research groups have observed valley physics in the exciton-polariton system , , . Surprisingly, the results show that the hybridization with cavity photons makes it easier to observe the spin-valley physics at room temperature , and for materials, where the exciton does not ordinarily demonstrate strong spin-valley physics . However, the spin-valley physics remained largely ignored in the cavity nonlinear optics with monolayer materials. In III-V quantum well systems, researchers demonstrated a helicity dependent polariton-polariton interaction. Exploiting such an effect, multistability in helicity is observed in exciton-polariton systems , . Similar effects are expected with TMDC exciton-polaritons as well. The multistable devices can enable multi-state optical logic.
8.4 Hyperbolic metamaterial with layered materials
In all the nonlinear systems we have considered in this article so far, the layered materials only provide the required nonlinearity and the cavity is formed by another, linear material. However, it is possible to fabricate a whole photonic structure using layered materials. For example, using graphene and h-BN layered structures, researchers predicted that a hyperbolic metamaterial can be created , . Hyperbolic metamaterials are promising candidates for enhancing the nonlinear optical interaction . Thus, it is possible to build a nonlinear nanophotonic system solely made out of layered materials. This will open a completely new field of research.
The authors acknowledge useful discussion with Professor Vinod Menon, Professor Xiaodong Xu and Professor Feng Wang. This work is supported by the National Science Foundation under grant NSF-EFRI-1433496, and the Air Force Office of Scientific Research-Young Investigator Program under grant FA9550-15-1-0150.
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About the article
Published Online: 2017-12-04
Citation Information: Nanophotonics, Volume 7, Issue 2, Pages 355–370, ISSN (Online) 2192-8614, DOI: https://doi.org/10.1515/nanoph-2017-0069.
© 2017 Arka Majumdar et al., published by De Gruyter, Berlin/Boston. This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License. BY-NC-ND 4.0