Enhanced Third-Harmonic Generation in Diamond Photonic Crystal Slabs via Doubly Resonant Quasi-Bound States in the Continuum
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Introduction to the show: ident: Quantum Radio. Generated commentary on the latest quantum physics and condensed matter papers.
Kai: I'm Kai.
Mira: And I'm Mira, here with Lev.
Kai: Today's paper: "Enhanced Third-Harmonic Generation in Diamond Photonic Crystal Slabs via Doubly Resonant Quasi-Bound States in the Continuum".
Mira: The gist: The authors propose and numerically demonstrate doubly resonant third-harmonic generation in a diamond photonic crystal (PhC) slab,
Kai: First, who's behind it and why it matters.
Paper summary: Kai: To dive deeper into the paper "Enhanced Third-Harmonic Generation in Diamond Photonic Crystal Slabs via Doubly Resonant Quasi-Bound States in the Continuum," we need to understand exactly what they are proposing with this geometry.
Mira: Essentially, it boils down to them showing how they can get both fundamental and third harmonic modes resonating at the same time inside a diamond photonic crystal slab.
Lev: They achieved this by breaking the symmetry of the holes, which lets them create that nonlinear coupling that normally wouldn't happen in a centrosymmetric material like diamond.
Kai: That symmetry breaking is what makes it all work; it turns a weak interaction into something measurable and controllable within a realistic slab thickness.
Mira: They use coupled-mode theory to set up a figure of merit—that equation that tells you how good the design is—and they optimized it using material properties from single-crystal diamond.
Lev: So, what this means for us in terms of actual hardware is that we need high quality factors for both those resonant modes and a big nonlinear coupling coefficient to get a meaningful power conversion.
Kai: If we can manage those quality factors, this structure gives us a solid way to do on-chip frequency conversion using just diamond platforms.
Mira: It’s not just about one specific wavelength either; because the geometry is defined by the lattice constant, you can map this whole design across different wavelengths.
Lev: The real hurdle is that every time you want to apply this idea to a new nonlinear process or a different material, you have to redo all that optimization work.
Kai: So the big picture here is using symmetry breaking in diamond photonic crystals to enable efficient frequency tripling through simultaneous resonance of fundamental and third harmonic modes.
Mira: It sets up a general and scalable route toward monolithic frequency conversion in an all-diamond platform for quantum and nonlinear photonics.
Conclusion: Kai: So we're wrapping up our look at the paper "Enhanced Third-Harmonic Generation in Diamond Photonic Crystal Slabs via Doubly Resonant Quasi-Bound States in the Continuum."
Mira: It really boils down to them showing how they can get both fundamental and third harmonic modes resonating at the same time inside a diamond photonic crystal slab.
Lev: They achieved this by breaking the symmetry of the holes, which lets them create that nonlinear coupling that normally wouldn't happen.
Kai: That symmetry breaking is what makes it all work; it turns a weak interaction into something measurable and controllable within a realistic slab thickness.
Mira: They used coupled-mode theory to set up a figure of merit—that equation that tells you how good the design is—and they optimized it using material properties from single-crystal diamond.
Lev: So, what this means for us in terms of actual hardware is that we need high quality factors for both those resonant modes and a big nonlinear coupling coefficient to get a meaningful power conversion.
Kai: If we can manage those quality factors, this structure gives us a solid way to do on-chip frequency conversion using just diamond platforms.
Mira: It’s not just about one specific wavelength either; because the geometry is defined by the lattice constant, you can map this whole design across different wavelengths.
Lev: The real hurdle is that every time you want to apply this idea to a new nonlinear process or a different material, you have to redo all that optimization work.
Kai: So the big picture here is using symmetry breaking in diamond photonic crystals to enable efficient frequency tripling through simultaneous resonance of fundamental and third harmonic modes.
Mira: It sets up a general and scalable route toward monolithic frequency conversion in an all-diamond platform for quantum and nonlinear photonics.
Lev: And next, we need to see how this kind of integrated on-chip conversion stacks up against the error correction overhead we deal with in superconducting qubits.
Sangmin Ji, Satoshi Iwamoto, Hideki Gotoh
Research Institute for Semiconductor Engineering, Hiroshima University · Research Center for Advanced Science and Technology, The University of Tokyo
physics.optics, cond-mat.mes-hall
Submitted: 2026-07-17
Updated: 2026-07-17
DOI: 10.1016/j.cap.2026.10.004
License: http://creativecommons.org/licenses/by/4.0/
Importance score: 76/100
The gist: The gist: The authors propose and numerically demonstrate doubly resonant third-harmonic generation in a diamond photonic crystal (PhC) slab, in which the fundamental harmonic (FH) and the third
Key concepts
- Doubly Resonant THG
- This technique involves making both the fundamental light (first harmonic) and the third harmonic light (third harmonic) oscillate strongly at the exact same time within a photonic crystal structure. This simultaneous resonance dramatically enhances how efficiently light is converted from one frequency to another, similar to tuning two musical notes perfectly together.
- Quasi-BIC Mode
- This refers to a mode that is nearly bound (trapped) within the material structure but not perfectly confined. In this study, the third harmonic mode acts as a quasi-BIC because its symmetry prevents it from radiating into free space, allowing it to be highly localized and coupled effectively with other modes.
- Symmetry Breaking
- The original design used circular holes, which preserved a high degree of symmetry that prevented the fundamental and third harmonic modes from interacting nonlinearly. By changing the hole shape to equilateral triangles, the symmetry was broken. This change is crucial because it allows a previously weak nonlinear coupling between the two modes to become strong enough for efficient conversion.
- Figure of Merit (FOM)
- The FOM is a mathematical metric used to guide the design process. In this study, it quantifies how good the proposed unit cell geometry and cavity structure are at achieving high third-harmonic generation efficiency. Optimizing this value helps researchers find the best physical dimensions for the diamond slab before expensive fabrication.
Summary
The gist: The authors propose and numerically demonstrate doubly resonant third-harmonic generation in a diamond photonic crystal (PhC) slab, in which the fundamental harmonic (FH) and the third harmonic (TH) modes are simultaneously resonant within the same membrane. This design establishes a robust route toward efficient, monolithic on-chip frequency conversion in an all-diamond platform for quantum and nonlinear photonics.
Design Strategy for Doubly Resonant THG
The research focuses on overcoming the challenge of vanishing nonlinear coupling by performing band engineering that tailors the nonlinear overlap between FH and TH modes via the χ(3) tensor The design utilizes a hexagonal-lattice PhC slab where a K-point band-edge FH mode is used, which is readily confined in a PhC heterostructure cavity owing to the relatively large TE bandgap of the hexagonal lattice Candidates for the TH mode (ω3) are identified as nondegenerate modes at the Γ point, which are symmetry-protected BICs because their mode symmetry is incompatible with the radiation continuum The authors introduce asymmetry by continuously deforming the circular hole into an equilateral triangular hole while keeping the hole area constant, which transforms Mode II into Mode II(t), which acquires a nonzero β3 with the FH mode owing to the broken symmetry.
Coupled-Mode Theory and Figure of Merit
The THG efficiency is formulated using temporal coupled-mode theory (CMT) The normalized THG efficiency η is defined by the expression η = 16ω3/2β32τ1/6τ3/2τex1,3·L1(ω)3L3(ω). Under the doubly resonant condition (ω = ω1 and 3ω = ω3), the line shapes equal unity, so η ∝ Q13Q3β32. This expression, Equation (8), is defined as the figure of merit (FOM) that guides the optimization below. The nonlinear overlap β3 is defined by the integral involving the nonlinear polarization vector P(3)(3ω) and the field distributions.
Optimization of Unit Cell Geometry
The optimization process maximizes Q13Q3β32 over the three-dimensional unit-cell geometry. The material dispersion of single-crystal diamond is used, and the third-order susceptibility tensor is set to χ1111 = 3χ1122 = 2.1 × 10−21 m2V−2. The FOM Q3β32 is maximized at (d/√3)/a = 0.4375, 0.455, 0.4625, for t/a = 0.50, 0.55, and 0.60, respectively. The corresponding three-dimensional band diagram for the designed structure (t/a, d/a) = (0.55, 0.451√3) is shown in Fig. 3.
Cavity Design and Performance Verification
Three-dimensional finite difference time domain (3D-FDTD) simulations were performed to verify the design in realistic PhC heterostructure cavities The designed cavity comprises core, transition, and cladding layers with parameters (t, dcore, dtrans, dclad) = (0.55a, 0.46√3a, 0.44√3a, 0.4√3a). The FH mode quality factor Q1 increases exponentially with the number of cladding layers nclad. The calculated nonlinear overlap reaches β32 = 5.8 × 106 J−2. Inserting these values into Eq. (8) gives a normalized THG efficiency η = 2.7 × 10−7 W−2. This value of η corresponds to Q1 = 4000, obtained with nclad = 5.
Benchmarking and Scalability
The proposed design outperforms most previously reported structures, exceeding the record-high THG performance reported to date [22] by two orders of magnitude. The PhC cavity can be excited directly from free space, enabling much higher-power pumping and improved efficiency. The design is scalable via the lattice constant a, and the broad transparency of diamond allows a single geometry to be mapped onto fabricable wavelengths for a range of applications. The results establish a robust route toward efficient, monolithic on-chip frequency conversion in an all-diamond platform for quantum and nonlinear photonics.
Conclusion
In conclusion, we have proposed and numerically demonstrated doubly resonant third-harmonic generation in a centrosymmetric diamond photonic crystal slab Combining a K-point band-edge mode at the fundamental frequency with a Γ-point BIC at the third harmonic, and deforming the circular holes into equilateral triangles that break the lattice symmetry, we simultaneously activate a symmetry-forbidden nonlinear overlap for a realistic slab thickness. A closed-form expression for the coupled-mode-theory THG efficiency provided a material-independent figure of merit that guided both the unit-cell and the heterostructure-cavity design. Three-dimensional FDTD simulations of the designed cavity, which co-confines the fundamental and third-harmonic modes, yield η = 2.7 × 10−7 W−2, projected to reach 0.034 W−2 at the fabrication-limited quality factor. Because the scheme relies only on lattice symmetry and a material-independent figure of merit, it offers a general and scalable route to monolithic frequency conversion, which is readily transferable to other wavelengths, χ(3) processes, and material platforms for nonlinear-optical and colorcenter quantum applications in diamond.
CRediT authorship contribution statement Sangmin Ji: Conceptualization, Methodology, Software, Investigation, Formal analysis, Visualization, Writing – original draft. Satoshi Iwamoto: Supervision, Writing – review & editing. Hideki Gotoh: Supervision, Project administration, Writing – review & editing. Acknowledgements This work was supported by Iketani Science and Technology Foundation (0361158-A); Hirose Foundation (12th Research Grant); JSPS KAKENHI (23K19197, 24K17579). Disclosures The authors declare no conflicts of interest. Data availability Data underlying the results may be obtained from the authors upon reasonable request. Declaration of generative AI and AI-assisted technologies in the manuscript preparation process During the preparation of this work the authors used Claude AI and Gemini AI in order to review the grammar and the correspondence between figures and main text. After using this tool/service, the authors reviewed and edited the content as needed and take full responsibility for the content of the published article. References 1 M. D. Levenson and N. Bloembergen, Dispersion of the nonlinear optical susceptibility tensor in centrosymmetric media, Phys. Rev. B 10, 4447 (1974). https://doi.org/10.1103/PhysRevB.10.4447 2 R. P. Mildren and J. R. Rabeau, Optical engineering of diamond, Wiley (2013). DOI:10.1002/9783527648603 3 B. J. M. Hausmann, I. Bulu, V. Venkataraman, P. Deotare & M. Lončar, Diamond nonlinear photonics, Nat. Photon.
Improvements for AI systems
-
The AI system can perform automated band engineering optimization by using
a closed-form expression for THG efficiency derived from coupled-mode theory
as a figure of merit to optimize the unit cell geometry, ensuring scalability across various wavelengths. -
The system can predict the optimal slab thickness by combining
the hole size d that maximizes the FOM increases with t, while d satisfying the tripling condition ω3 = 3ω1 decreases with t,
allowing it to select the best physical configuration for a target frequency conversion wavelength. -
The AI can design and simulate complex heterostructure cavities using
three-dimensional finite difference time domain (3D-FDTD simulations
to determine mode properties, including eigenfrequencies and quality factors, for simultaneous FH and TH mode confinement. -
The system can calculate the expected performance benchmark by evaluating
the normalized THG efficiency η = 2.7 × 10−7 W−2
under fabrication-limited conditions (Q ≈ 200,000), providing a quantitative comparison against literature whereDiamond PhC cavity [This work, Q1 = 200,000] 3.4 × 10−2 W-2.
-
The system can identify the critical structural parameters for maximizing efficiency by locating the
optimum ncore = 6
as determined by simulations where "β32 peaks near ncore = 3–4 and decreases for ncore > 4."
Abstract
We propose and numerically demonstrate doubly resonant third-harmonic generation (THG) in a diamond photonic crystal (PhC) slab, in which the fundamental harmonic (FH) and the third harmonic (TH) modes are simultaneously resonant within the same membrane. A hexagonal-lattice slab with triangular air holes is designed so that a K-point band-edge FH mode and a Γ-point quasi-bound-state-in-the-continuum (quasi-BIC) TH mode satisfy the frequency-tripling condition 3ω 1 aboutω 3. Modifying the hole shape from circular to equilateral triangular breaks the in-plane symmetry that otherwise forces the nonlinear coupling to vanish, thereby converting a TH mode with negligible overlap into one with finite while simultaneously reducing the required slab thickness. Guided by a closed-form expression for THG efficiency derived from coupled-mode theory, we design the unit cell and a PhC heterostructure cavity. Three-dimensional simulations of the designed cavity yield a normalized THG efficiency η=2.7 times10-7 W-2 under moderate quality factors, which is projected to reach 0.034 W-2 at the fabrication-limited quality factor (Q = 200,000). Because the operating wavelength is set by the lattice constant, this design, combined with the ultra-wide transparency window of diamond, can map a single geometry across various fabricable wavelengths, spanning from telecommunication bands to color-center-resonant visible and deep-UV outputs. These results establish a robust route toward efficient, monolithic on-chip frequency conversion in an all-diamond platform for quantum and nonlinear photonics.
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