Luis Ledezma’s research while affiliated with California Institute of Technology and other places

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Publications (64)


Large-scale time-multiplexed nanophotonic parametric oscillators
  • Article

May 2025

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26 Reads

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Luis Ledezma

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Alireza Marandi


Figure 1: A diagram of the squeezer and measurement OPA circuit.
Ultrafast All-Optical Measurement of Squeezed Vacuum in a Lithium Niobate Nanophotonic Circuit
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  • File available

February 2025

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40 Reads

Squeezed vacuum, a fundamental resource for continuous-variable quantum information processing, has been used to demonstrate quantum advantages in sensing, communication, and computation. While most experiments use homodyne detection to characterize squeezing and are therefore limited to electronic bandwidths, recent experiments have shown optical parametric amplification (OPA) to be a viable measurement strategy. Here, we realize OPA-based quantum state tomography in integrated photonics and demonstrate the generation and all-optical Wigner tomography of squeezed vacuum in a nanophotonic circuit. We employ dispersion engineering to enable the distortion-free propagation of femtosecond pulses and achieve ultrabroad operation bandwidths, effectively lifting the speed restrictions imposed by traditional electronics on quantum measurements with a theoretical maximum clock speed of 6.5 THz. We implement our circuit on thin-film lithium niobate, a platform compatible with a wide variety of active and passive photonic components. Our results chart a course for realizing all-optical ultrafast quantum information processing in an integrated room-temperature platform.

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Figure 1: Two-color soliton pulse compression in nanophotonics. a, A pulse at the fundamental frequency (ω) is used to pump the dispersion-engineered nanophotonic waveguide designed for phase-mismatched second harmonic (2ω) generation. Co-propagating compressed pulses at the fundamental and second harmonic are achieved through the two-color soliton compression. b, Microscope image of the measured waveguide, showing back-and-forth conversion between harmonics. c, Simulated evolution of the fundamental (top) and second harmonic (bottom) as a function of normalized propagation distance, z, in the waveguide. d, Temporal profiles of the fundamental and second harmonic at labeled locations in the waveguide.
Figure 2: Scaling behaviors of two-color soliton pulse compression. a, Soliton solutions of the fundamental wave for varying α. b, Corresponding soliton solutions for the second harmonic. c, Optimum ζ for achieving compression. A fit is given by the dashed black line. d-f, Scaling behaviors for varying α of the d fundamental FWHM, e compression quality, and f fundamental peak power ratio at ζ opt . FWHM, full-width at half-maximum.
Figure 5: Towards integrated single-cycle pulse synthesizers. a, Proposed nanophotonic circuit architecture for single-cycle pulse synthesis. b, Simulated waveforms that may be achieved through manipulation of the input envelope phase, ∆ϕ ω . c, Simulated synthesized single-cycle waveform and d, corresponding electric field. e, Expected waveform from synthesis of experimentally measured pulses.
Two-optical-cycle pulses from nanophotonic two-color soliton compression

January 2025

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89 Reads

Few- and single-cycle optical pulses and their associated ultra-broadband spectra have been crucial in the progress of ultrafast science and technology. Multi-color waveforms composed of independently manipulable ultrashort pulses in distinct spectral bands offer unique advantages in pulse synthesis and high harmonic generation. However, the generation and control of ultrashort pulses has required bulky optical systems at the tabletop scale. Quadratic soliton compression theoretically offers a direct route to generation of few-cycle, two-color pulses but is fundamentally limited in bulk systems by the unavoidable presence of walk-off between the fundamental and second harmonic waves. Here, we show that the dispersion engineering capabilities of nanophotonics allow these limitations to be overcome, enabling extreme simultaneous pulse compression of the fundamental and second harmonic components and control over the resultant pulse shape. We experimentally demonstrate quadratic soliton pulse compression in dispersion-engineered nanophotonic lithium niobate waveguides and achieve two-optical-cycle pulses requiring pJ pump pulse energies. We further illustrate how the demonstrated compression scheme can be readily extended to on-chip single-cycle pulse synthesis. When integrated with femtosecond and picosecond sources in lithium niobate, our results provide a path towards realization of single-cycle ultrafast systems in nanophotonic circuits.


Ultrafast single-photon detection using nanophotonic parametric amplifiers

October 2024

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88 Reads

Integrated photonic quantum information processing (QIP) has advanced rapidly due to progress in various nanophotonic platforms. Single photon detectors have been the subject of intense study due to their ubiquity in QIP systems, yet many state-of-the art detectors operate at cryogenic temperatures under vacuum and suffer from long dead times. We propose and demonstrate a single photon detection scheme based on optical parametric amplification in nanophotonic lithium niobate (LN) combined with a classical photodetector. We use quantum detector tomography and experimentally demonstrate an efficiency of 26.5% with a 2.2% dark count rate. We show that by improving the nonlinearity-to-loss ratio in nanophotonics and using homodyne detection on a squeezed pump, the detector can achieve 69% efficiency with 0.9% dark count rate. The detector operates at room temperature, has no intrinsic dead time, and is readily integrated in LN nanophotonics, in which many other components of photonic QIP are available. Our results represent a step towards all-optical ultrafast photon detection for scalable nanophotonic QIP.


Enhanced sensing using quadratic cavity simultons
a Schematic depiction of sensing in the simulton regime of a synchronously-pumped optical parametric oscillator at degeneracy. The bright soliton in the signal interacts with the sample every round trip, and the resulting competing nonlinear dynamics generate the measured signal response. b Specifically, stable simulton operation requires the simulton group advance, ΔT, to balance the round-trip group delay, ΔTRT, and the parametric gain to balance the sample loss, αsamp, and output coupling. c Schematic representation of linear absorption sensing governed by the Beer-Lambert Law for light interacting with a sample over a path length L. d Linear methods (light blue region) face limitations in the achievable sensitivity at high sample concentrations. In contrast, active cavity sensing with quadratic cavity (orange) can achieve high sensitivities at high sample concentrations. Trep, pump repetition period; Tcirc, pulse circulation time in the cavity; ΔT, simulton group advance; TRT, cold cavity round-trip time ΔTRT, round-trip group delay; χ⁽²⁾, second-order susceptibility; ω, angular frequency; αsamp, sample absorption coefficient; OC, output coupling; Pin, input power; Pout, output power; L, path length; ℏ, reduced Planck’s constant.
Quadratic cavity simulton enhancement mechanism
a Theoretical behavior of near-threshold sensing, wherein the addition of sample causes an increase in threshold, resulting in a decrease in signal power at the sensing point. b The corresponding signal enhancement grows asymptotically as threshold is approached. c Experimentally measured input-output power relationships for the simulton (orange) and conventional (pink) regimes show the extremely high slope efficiency and high threshold of the simulton, suggesting its potential for near-threshold sensing with high SNR. Solid lines capture the trends through linear fits of the experimental data while the orange, dashed line shows the corresponding simulton simulation.
Simulton dynamics responsible for sensing
a Experimental power spectral densities demonstrate reduced power across the entire simulton spectrum with the addition of sample despite the relatively narrow CO2 absorption feature. b In the far above threshold conventional regime, like other general multi-mode lasers, power in non-absorbing modes increases with the addition of sample, largely compensating the loss in the absorbing modes. c Schematic depiction of the temporal dynamics of cavity simulton formation which enable the sensing enhancement mechanism. Additional loss in the round trip limits the ability of the simulton to deplete the pump and accelerate, leading to a reduced gain for all modes at steady-state. d Simulated steady-state pulse position as a function of gas concentration (left). Comparison with the theoretical gain window (right) shows the simulton moving further towards the gain window edge as the sample concentration is increased, in accordance with (c).
Sensing behaviors of quadratic cavity solitons
a Measured output power as a function of CO2 concentration for different number of times above threshold, N. A high sensitivity of 4.1 mW/ppm is measured near threshold, emphasized using the solid trend lines. b Simulations of the simulton response to the addition of CO2 at various number of times above threshold exhibit good qualitative agreement with the experimental data. c Equivalent path-length enhancement calculated for neighboring points in the experiment, showing a measured enhancement as large as 6000. Solid lines show the expected asymptotic enhancement corresponding to the linear fits in (b), with dashed lines extending these fits to enable extrapolation of detector-limited enhancements for detection bandwidths of 1 MHz (x’s) and 1 Hz (stars). d Simulated change in output power as a function of CO2 concentration with a linear fit (dashed line) showing good linearity over a dynamic range of 10⁷. e Measured sensitivity as a function of CO2 concentration in direct comparison with linear sensing (light blue), demonstrating orders of magnitude sensitivity improvement over linear methods at high sample concentrations.
Quadratic-soliton-enhanced mid-IR molecular sensing

October 2024

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105 Reads

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2 Citations

Optical solitons have long been of interest both from a fundamental perspective and because of their application potential. Both cubic (Kerr) and quadratic nonlinearities can lead to soliton formation, but quadratic solitons can practically benefit from stronger nonlinearity and achieve substantial wavelength conversion. However, despite their rich physics, quadratic cavity solitons have been used only for broadband frequency comb generation, especially in the mid-infrared. Here, we show that the formation dynamics of mid-infrared quadratic cavity solitons, specifically temporal simultons in optical parametric oscillators, can be effectively leveraged to enhance molecular sensing. We demonstrate significant sensitivity enhancement while circumventing constraints of traditional cavity enhancement mechanisms. We perform experiments sensing CO2 using cavity simultons around 4 μm and achieve an enhancement of 6000. Additionally, we demonstrate large sensitivity at high concentrations of CO2, beyond what can be achieved using an equivalent high-finesse linear cavity by orders of magnitude. Our results highlight a path for utilizing quadratic cavity nonlinear dynamics and solitons for molecular sensing beyond what can be achieved using linear methods.


Ultrashort pulse biphoton source in lithium niobate nanophotonics at 2 μm

June 2024

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71 Reads

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9 Citations

Photonics offers unique capabilities for quantum information processing (QIP) such as room-temperature operation, the scalability of nanophotonics, and access to ultrabroad bandwidths and consequently ultrafast operation. Ultrashort pulse sources of quantum states in nanophotonics are an important building block for achieving scalable ultrafast QIP; however, their demonstrations so far have been sparse. Here, we demonstrate a femtosecond biphoton source in dispersion-engineered periodically poled lithium niobate nanophotonics. We measure 17 THz of bandwidth for the source centered at 2.09 µm, corresponding to a few optical cycles, with a brightness of 8.8 GHz/mW. Our results open new paths toward realization of ultrafast nanophotonic QIP.


Figure 1: Time-multiplexed nanophotonic OPOs. (A) Schematic of the device based on thin-film lithium niobate. N pulses in a long cavity are equivalent to (B) N independent timemultiplexed oscillators. (C) In the non-degenerate regime, the pump photons split into signal and idler photons at different frequencies. In this case, the phase of each is unconstrained, as shown in the signal phase space diagram. (D) In the degenerate regime, the pump photons split into indistinguishable signal photons at the half-harmonic of the pump, resulting in a binary phase for the signal.
Figure 2: Measurement of independent oscillators. (A) Schematic of the measurement setup. The nanophotonic chip is pumped by the output of an EO comb which provides ps pulses at GHz repetition rates. The output is passed through a fiber interferometer with an M-pulse delay for characterizing the relative phases of the output pulses. The inset shows microscope (left) and SEM (right) images of a segment of the spiral resonator. (B) Illustration of the pump pulse train, with 4-µs on-time. (C) Example signal pulse train at degeneracy, showing the binary phase of the output. Each OPO iteration contains a repeating 4-ns random pattern of |0⟩ and |π⟩. (D) Principle of the interferometric measurement of the OPO signal, illustrated with a 1-pulse delay. (E) Expected outputs for pulse-to-pulse (fast) and average (slow) measurements. EO, electro-optic; PD, photodetector.
Figure 3: Interference measurements for N = 40. (A-D) Fast detector measurements in the degenerate (A-B) and non-degenerate (C-D) regimes. Examples of the measured interference pulse trains are shown in (A) and (C). Histograms of the measured peak pulse intensities over 30 degenerate (B) and 25 non-degenerate (D) interference measurements show good agreement with theoretical expectations. (E-I) Slow detector measurements in the degenerate (E-G) and non-degenerate (H-I) regimes. Example data out of the slow detector is shown in (E) and (H). The reference trace (top) is sampled from the OPO output before the MZI and is used for intensity noise correction of the interference trace (bottom). Histograms of the resulting corrected traces are shown in (F) and (I). As expected theoretically, discrete peaks are observed in the degenerate case (F), whereas a continuous distribution is seen in the the non-degenerate case (I). The discrete peaks in the degenerate case are binned for comparison with theory (G), showing good agreement.
Figure 5: Time-multiplexed architecture for programmable all-to-all coupled nonlinear resonators. (A) The main resonator (bottom) with N time-multiplexed OPOs is coupled to a secondary memory cavity (top), designed to have N + 1 sites. Losses in the memory cavity are compensated by a secondary pump and poled region. EOMs in the coupling regions are used to program an MZI-based intensity modulator, which can be used to tune the strength of the coupled pulse. (B) Connectivity diagrams showing how arbitrary couplings are achieved over N roundtrips. EOM, electro-optic modulator; MZI, Mach-Zehnder interferometer.
Large-scale time-multiplexed nanophotonic parametric oscillators

May 2024

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133 Reads

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1 Citation

Arrays of nonlinear resonators offer a fertile ground for a wide range of complex phenomena and opportunities for advanced photonic sensing and computing. Recently, significant attention has focused on studying coupled resonators in special-purpose configurations either on chips or in table-top experiments. However, a path to realizing a large-scale programmable network of nonlinear photonic resonators remains elusive because of the challenges associated with simultaneously achieving strong nonlinearity, independent operation of the resonators, and programmability of the couplings. In this work, we break these barriers by realizing large-scale, time-multiplexed optical parametric oscillators (OPOs) on a single lithium niobate nanophotonic chip. We show independent operation of 70 identical OPOs in an ultrafast nanophotonic circuit. The OPOs exhibit an ultra-low threshold of a few picojoules, substantially surpassing the strength of nonlinearity of other platforms. Using our ultrafast nanophotonic circuit, a network of N OPOs with programmable all-to-all couplings requires only a few additional components. The time-multiplexed nanophotonic OPOs can enable myriad applications, including ultrafast classical and quantum information processing.


Architecture of OPA-BFS.
Qualitative comparison between different schemes.
OPA-BFS for mock sample. (a) Intensity (absorbance) and phase of assumed 11 Lorentzian transitions. (b) FID field of the signal pulse and envelope of the pump pulse. (c)–(f) Spectral noise level (blue dotted curves) and ideal absorption signal (red solid curves) in different schemes. Note that we zoom into the central five transitions to show the details more clearly.
BFS and OPA-BFS for NH3 and CO2 around 143.4 THz.
Noise and LOD scaling with excitation power. (a) Detector noise (DN, blue dashed line), relative intensity noise (RIN, yellow dashed line) and total noise (red dotted curve) in DAS (left y-axis). Green curve (right y-axis) denotes the LOD of DAS. (b) LOD scaling with power of different schemes. The green solid curve for DAS is the same as that in (a).
Optical-parametric-amplification-enhanced background-free spectroscopy

Traditional absorption spectroscopy has a fundamental difficulty in resolving small absorbance from a strong background due to the instability of laser sources. Existing background-free methods in broadband vibrational spectroscopy help to alleviate this problem but face challenges in realizing either low extinction ratios or time-resolved field measurements. Here, we introduce optical-parametric-amplification-enhanced background-free spectroscopy, in which the excitation background is first suppressed by an interferometer, and then the free-induction decay that carries molecular signatures is selectively amplified. We show that this method can improve the limit of detection in linear interferometry by order(s) of magnitude without requiring lower extinction ratios or a time-resolved measurement, which can benefit sensing applications in detecting trace species.


Highly efficient visible and near-IR photon pair generation with thin-film lithium niobate

April 2024

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249 Reads

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11 Citations

Efficient on-chip entangled photon pair generation at telecom wavelengths is an integral aspect of emerging quantum optical technologies, particularly for quantum communication and computing. However, moving to shorter wavelengths enables the use of more accessible silicon detector technology, and opens up applications in imaging and spectroscopy. Here, we present high brightness ((1.6 ± 0.3) × 10⁹ pairs/s/mW/nm) visible–near-IR photon pair generation in a periodically poled lithium niobate nanophotonic waveguide. The degenerate spectrum of the photon pairs is centered at 811 nm with a bandwidth of 117 nm when pumped with a spectrally multimode laser diode. The measured on-chip source efficiency of (2.3 ± 0.5) × 10¹¹ pairs/s/mW is on par with source efficiencies at telecom wavelengths and is also orders of magnitude higher than the efficiencies of other visible sources implemented in bulk crystal or diffused waveguide-based technologies. Further improvements in the brightness and efficiencies are possible by pumping the device with a single-frequency laser, which would also shrink the pair bandwidth. These results represent the shortest wavelength of photon pairs generated in a nanophotonic waveguide reported to date by nearly an octave.


Citations (31)


... Existing single-shot [40] or few-shot [41] methods suffer from low frame update rates and/or require extensive postprocessing algorithms to extract the useful information. Additionally, our all-optical computing architecture can be realized as a feedback mechanism for controlling the soliton state generation and/or ultrafast sensing schemes based on similar soliton dynamics [42]. ...

Reference:

All-optical computing with beyond 100-GHz clock rates
Quadratic-soliton-enhanced mid-IR molecular sensing

... The longest duration laser pulse width used in our experiments was ∼ 5 ps, which limits the maximum allowable clock rates since pulses will begin overlapping in time and suffering from undesirable cross-talk beyond ∼ 200 GHz clock rates. This issue can be overcome by using even shorter laser pulses, for example, few-cycle pulses generated using nonlinear optical pulse compression [51] in TFLN. Finally, implementing the main cavity in the AO-RNN using an integrated optical parametric oscillator [52][53][54] in TFLN could also drastically reduce the overall latency given by the light propagation time through the network. ...

Soliton Pulse Compression in Lithium Niobate Nanophotonics
  • Citing Conference Paper
  • January 2024

... More recent experiments have focused toward integrated photonics implementations, to increase scalability and lower the power consumption. Even though efforts have been made to realize photonic integrated Ising machines exploiting the χ 3 nonlinearity in the SiN platform with a spatial multiplexing scheme [10], and using the quadratic χ 2 nonlinearity of lithium niobate in a time-multiplexed configuration [11], the spatial coupling of OPOs leveraging the χ 2 nonlinearity has not been investigated. ...

Large-scale time-multiplexed nanophotonic parametric oscillators

... There are demonstrations of on-chip photon pair sources with integrated nonlinear photonic platforms such as LiNbO 3 , Si, and Si 3 N 4 (18)(19)(20)(21). With large scale integration of spatial and temporal multiplexing systems, near-deterministic entangled multi-photon states can be implemented. ...

Highly efficient visible and near-IR photon pair generation with thin-film lithium niobate

... Lithium niobate (LN) is a key material in integrated photonics, [1][2][3][4] owing to its strong electro-optic response and second-and third-order nonlinear optical properties, which makes it essential for high-speed modulation, 2,5-10 frequency comb generation, [11][12][13][14] and quantum photonic applications. [15][16][17][18][19][20] The development of thin-film lithium niobate (TFLN) has further expanded its potential by enabling low-loss, tightly confined optical modes, leading to improved nonlinear efficiency and denser photonic integration. ...

Visible-to-ultraviolet frequency comb generation in lithium niobate nanophotonic waveguides

Nature Photonics

... Harnessing SBS in the thin-film lithium niobate (TFLN) platform can elevate the SBS technology to a new level of readiness. Renowned for its exceptional scalability, low optical losses, and significant electro-optic (EO) coefficients (27,28), TFLN has unlocked a variety of novel applications with exceptional performances, including onchip EO modulators (29), optical frequency combs (30,31), MWP processors (32), and integrated lasers (33,34). Expanding the capabilities of TFLN to include SBS not only enables Brillouin-based applications on a more scalable platform, but also creates a synergistic interplay with its existing functionalities. ...

Ultrafast mode-locked laser in nanophotonic lithium niobate

Science

... Leveraging nonlinearity for frequency generation [1][2][3][4][5][6][7][8][9][10][11][12][13] has become a central focus in photonic science, enabling groundbreaking advances such as tunable frequency comb sources [14][15][16][17][18][19][20][21][22][23] , atomic clocks 24,25 , and sum frequency generation spectroscopies 26,27 , to mention a few. These innovations find numerous applications, in areas ranging from optical communications 28 and metrology 29,30 to imaging [31][32][33] and bio-photonics 34,35 . ...

Visible-to-mid-IR tunable frequency comb in nanophotonics

... To demonstrate the utility of this design approach we explore the optimization of an etched TFLN waveguide for maximized second harmonic generation (SHG) phase-matching bandwidth. We chose this design goal because broadband simultaneous phase matching of optical three-wave mixing in TFLN waveguides is of great interest for a wide range of applications [9,28,[46][47][48][49][50][51][52][53][54][55]. In this example the rib waveguide geometry is parameterized by core width, core thickness and normalized etch fraction. ...

Multi-Octave Frequency Comb from an Ultra-Low-Threshold Nanophotonic Parametric Oscillator

... Ultrafast switching [60], and ultrafast computation of nonlinear functions for machine learning have been achieved [61]. Combining these OPAs with resonators has allowed new regimes of nonlinearity to be studied which were previously impossible to achieve in bulk platforms [62]. ...

Multi-Octave Frequency Comb from a Nanophotonic Parametric Oscillator
  • Citing Conference Paper
  • January 2023