Andrew M. Weiner’s research while affiliated with Purdue University West Lafayette and other places

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Publications (1,000)


From broadband biphotons to frequency combs via spectral compression with time-varying cavities
  • Preprint

October 2024

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2 Reads

Karthik V. Myilswamy

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Jordan A. Gaines

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Jason D. McKinney

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[...]

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Andrew M. Weiner

Biphoton frequency combs are promising resources for quantum networking due in large part to their compatibility with the telecommunication infrastructure. In this work, we propose a method to periodically compress broadband frequency-entangled photons into biphoton frequency combs by utilizing time-varying linear cavities. Our approach hinges on rapid modulation of the input cavity coupling, yielding high spectral purity in each output comb line similar to that achieved with narrowband filters, but without the associated loss in flux. We examine the dependence of spectral purity and compression on coupling strength, cavity loss, and switching speed, finding realistic regimes supporting purities in excess of 0.999 and peak enhancement factors of 100 and beyond.


(a) Diagram of the experimental setup. CW: continuous-wave. PPLN: periodically poled lithium niobate. SiP: silicon photonic. FSR: free spectral range. SNSPD: superconducting nanowire single-photon detector. WSS: wavelength-selective switch.
(b) Conceptual illustration of high-dimensional frequency-bin states, depicting $d$ coherent superpositions of frequency-bin pairs and their corresponding temporal correlation functions. In this example, linear spectral phases are applied to both signal and idler bins, resulting in a temporal offset (gold) compared to the case with constant phase (gray). See text for details.
On-chip pulse shaping of entangled photons
  • Preprint
  • File available

September 2024

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43 Reads

We demonstrate spectral shaping of entangled photons with a six-channel microring-resonator-based silicon photonic pulse shaper. Through precise calibration of thermal phase shifters in a microresonator-based pulse shaper, we demonstrate line-by-line phase control on a 3~GHz grid for two frequency-bin-entangled qudits, corresponding to Hilbert spaces of up to 6×66\times 6 (3×33\times 3) dimensions for shared (independent) signal-idler filters. The pulse shaper's fine spectral resolution enables control of nanosecond-scale temporal features, which are observed by direct coincidence detection of biphoton correlation functions that show excellent agreement with theory. This work marks, to our knowledge, the first demonstration of biphoton pulse shaping using an integrated spectral shaper and holds significant promise for applications in quantum information processing.

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Silicon photonic spectral shaper
a Graphic illustration of a six-channel microresonator-based spectral shaper, and a conceptual illustration of line-by-line pulse shaping. An input optical frequency comb with random relative phases between comb lines generates a distorted waveform in the time domain. The spectral shaper chip can be programmed to align the phases and produce transform-limited pulses at the output. b Top-down microscope image of the fabricated system. c Zoomed-in schematic of a single resonator device used in our shaper.
Experimental configuration
High-level schematic diagram of experimental setups for a-i Multi-Heterodyne Spectroscopy (MHS), a-ii Dual-Comb Spectroscopy (DHS), for measuring the channel frequencies and phases, respectively, and a-iii the Waveform Monitor. Yellow and dashed black lines indicate optical and RF connections, respectively. Brown (solid and dashed) and green arrows in (a-i) follow directions of propagation for the MLFC and CW laser, respectively. Orange arrows in (a-ii) follow the signal comb. Arrows on the resonators within the SiP shaper follow the direction of propagation for each method. For clarity, the SiP shaper is drawn here with optical I/O on both sides of the chip; in the experiment, optical I/O is on a single side, as depicted in Fig. 1a. MHS and DCS measurements are run at the same time by adding circulators and DWDM filters. PD: Photodiode. b Flowchart of our shaper control scheme. c-i Transmission spectrum of the as-fabricated spectral shaper and c-ii with the shaper programmed to compress six lines from a 3 GHz EO comb. In both cases, the measurement is from a swept laser source and the two FSRs for MHS and DCS measurement are shown. Transmission is normalized to coupling loss to/from the chip, which we measure to be ~3.5 dB/facet.
Optical arbitrary waveform generation
a, b, c-i Ideal target waveforms in the time domain (green traces) and signal comb spectral phase (top) for the compressed, Talbot, and forked state, respectively. a, b, c-ii Measured waveforms (blue trace) and the ideal waveforms convolved with the measurement system impulse response (dashed orange traces) for the compressed, Talbot, and forked states, respectively. An additional waveform is shown in (a-ii) (black dotted trace) with an untuned phase and phase shifters driven to induce ~π phase. a, b, c-iii Target (gray dashed) and measured (blue scattered with error bars) signal comb spectral phase for the compressed, Talbot, and forked states, respectively. An additional measurement is shown in (a-iii) (black scattered with error bars) for the untuned phase state, with phase shifters driven to induce ~π phase. Figure legends in (a-i, ii, iii) are shared amongst subplots in a row, and the untuned state is only shown in (a-ii, iii). All theoretical waveforms take into account the optical power of each comb line as measured by OSA. Error bars (standard deviation) in the phase plots are difficult to see. These errors always <0.15 rad (see Methods and Supplementary Information note 6), and are on average ~0.05 rad. See Fig. 4a, b, c-iii for a clear example.
Pulse compression
a, b, c-i Waveforms acquired from a 30 GHz PD and 50 GHz sampling oscilloscope (blue traces) compared with the simulated target waveform after convolution with our measurement system impulse response (red dashed traces), for 3, 4, and 5 GHz channel spacing, respectively. a, b, c-ii OSA power spectral density of the EO comb lines coming out of the shaper after being programmed for compression on 3, 4, and 5 GHz grids, respectively. The power measured here for each spectral line is taken into account in the theoretical trace in (a, b, c-i). a, b, c-iii The difference between measured and target phase vectors with error bars (standard deviation) from the measured phases, after programming for 3, 4, and 5 GHz grids, respectively.
Silicon photonic microresonator-based high-resolution line-by-line pulse shaping

September 2024

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99 Reads

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5 Citations

Optical pulse shaping stands as a formidable technique in ultrafast optics, radio-frequency photonics, and quantum communications. While existing systems rely on bulk optics or integrated platforms with planar waveguide sections for spatial dispersion, they face limitations in achieving finer (few- or sub-GHz) spectrum control. These methods either demand considerable space or suffer from pronounced phase errors and optical losses when assembled to achieve fine resolution. Addressing these challenges, we present a foundry-fabricated six-channel silicon photonic shaper using microresonator filter banks with inline phase control and high spectral resolution. Leveraging existing comb-based spectroscopic techniques, we devise a system to mitigate thermal crosstalk and enable the versatile use of our on-chip shaper. Our results demonstrate the shaper’s ability to phase-compensate six comb lines at tunable channel spacings of 3, 4, and 5 GHz. Specifically, at a 3 GHz channel spacing, we showcase the generation of arbitrary waveforms in the time domain. This scalable design and control scheme holds promise in meeting future demands for high-precision spectral shaping capabilities.


Experimental setup including conceptual diagrams of the polarization-frequency states at various stages. TL, continuous-wave tunable laser; DWDM, dense wavelength-division multiplexer; PC, polarization controller; TE, transverse electric; TM, transverse magnetic; PSR, polarization splitter-rotator; MRR, microring resonator; SNSPD, superconducting nanowire single-photon detector.
Unidirectionally pumped JSIs measured for bins $k\in \{2,\ldots,117\}$ k ∈ { 2 , … , 117 } with a 1-ns coincidence window. (a) TE-polarized input for counterclockwise (CCW) pumping only. (b) TM-polarized input for clockwise (CW) pumping only. Strong correlations are observed in energy-matched resonances, while other combinations exhibit levels close to accidental coincidences. Excessive noise in the first 10 bin pairs is attributed to residual pump light.
Bayesian-estimated fidelities with respect to $|\Phi ^+\rangle$ | Φ + ⟩ for 116 energy-matched frequency bins, along with corresponding density matrices (real part) for select bins (i)–(iv). The magnitudes of all imaginary components are less than 0.01 and are omitted for clarity.
Experimentally measured density matrices (real part) for $\{1, 2, 4, 8, 16, 32, 64, 116\}$ { 1 , 2 , 4 , 8 , 16 , 32 , 64 , 116 } grouped frequency bins, their fidelity $\mathcal {F}$ F with respect to $|\Phi ^+\rangle$ | Φ + ⟩ , purity $\mathcal {P}$ P , and lower and upper bounds of distillable entanglement, all obtained from Bayesian QST. The imaginary components of all density matrices (not shown) are smaller than 0.03.
CMOS photonic integrated source of broadband polarization-entangled photons

August 2024

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26 Reads

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4 Citations

We showcase a fully on-chip CMOS-fabricated silicon photonic integrated circuit employing a bidirectionally pumped microring and polarization splitter-rotators tailored for the generation of broadband (>9 THz), high-fidelity (90–98%) polarization-entangled photons. Spanning the optical C+L-band and producing over 116 frequency-bin pairs on a 38.4-GHz-spaced grid, this source is ideal for flex-grid wavelength-multiplexed entanglement distribution in multiuser networks.


FIG. 1. (a) Conceptual illustration of temporal modulation of frequency-entangled photons with distributed clocks. (b) Simulated JSI of frequency-bin-entangled states subjected to in-phase and out-of-phase modulation, with either synchronized (left) or uniformly drifting (right) RF signals. WDM, wavelength-division multiplexer; RFoF Rx/Tx, RF-over-fiber receiver/transmitter; Osc.,  oscillator.
FIG. 2. FIG. 2. (a) Experimental setup for classical modulation cancellation. This configuration captures the relative drifts between the
RF signals, which are reflected in the optical spectrum at the output via spectral interference. (b) Diagram of our home-built
RFoF system. (c) Measured optical spectra when (i) RF signals from a single oscillator are split to directly drive both EOPMs
and (ii) our home-built RFoF system is used to distribute the RF signals. The figure insets provide a zoomed-in view of
the optical spectra near the first-order sidebands. DWDM, dense wavelength-division multiplexer; EOPM, electro-optic phase
modulator; EOIM, electro-optic intensity modulator.
FIG. 3. Experimental setup for nonlocal modulation cancellation. Entangled photons and classical RFoF clock are represented by spheres and sinewaves, respectively.  The inset displays the passbands programmed on Pulse Shaper 1, and the spectral filters (or ``bins'') scanned on Pulse Shapers 2 and 3 for JSI measurements. PPLN, periodically poled lithium niobate waveguide; SNSPD, superconducting nanowire single-photon detector.
FIG. 4. Measured JSIs for three scenarios: (a) RF oscillator off and both EOPMs unmodulated, (b) EOPMs synchronously driven in phase, and (c) EOPMs synchronously driven 180◦ out of phase. Coincidences are integrated over 2 s per bin pair (shown in blue), with error bars assuming Poissonian statistics. The red stem plots represent theoretical predictions, scaled and vertically offset to match the data points via linear least squares. The reference laser remains on for all three scenarios.
Quantum nonlocal modulation cancellation with distributed clocks

July 2024

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99 Reads

We demonstrate nonlocal modulation of entangled photons with truly distributed RF clocks. Leveraging a custom radio-over-fiber (RFoF) system characterized via classical spectral interference, we validate its effectiveness for quantum networking by multiplexing the RFoF clock with one photon from a frequency-bin-entangled pair and distributing the coexisting quantum-classical signals over fiber. Phase modulation of the two photons reveals nonlocal correlations in excellent agreement with theory: in-phase modulation produces additional sidebands in the joint spectral intensity, while out-of-phase modulation is nonlocally canceled. Our simple, feedback-free design attains sub-picosecond synchronization -- namely, drift less than \sim0.5 ps in a 5.5 km fiber over 30 min (fractionally only \sim2×\times108^{-8} of the total fiber delay) -- and should facilitate frequency-encoded quantum networking protocols such as high-dimensional quantum key distribution and entanglement swapping, unlocking frequency-bin qubits for practical quantum communications in deployed metropolitan-scale networks.


Fine-Resolution Silicon Photonic Wavelength-Selective Switch Using Hybrid Multimode Racetrack Resonators

July 2024

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50 Reads

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3 Citations

Journal of Lightwave Technology

In this work, we describe a procedure for synthesizing racetrack resonators with large quality factors and apply it to realize a multi-channel wavelength-selective switch (WSS) on a silicon photonic chip. We first determine the contribution of each component primitive to propagation loss in a racetrack resonator and use this data to develop a model for the frequency response of arbitrary order, coupled-racetrack channel dropping filters. We design second-order racetrack filters based on this model and cascade multiple such filters to form a 1×7 WSS. We find good agreement between our model and device performance with second-order racetrack that have ≈ 1 dB of drop-port loss, ≈ 2 GHz FWHM linewidth, and low optical crosstalk due to the quick filter roll-off of ≈ 5.3 dB / GHz. Using a control algorithm, we show three-channel operation of our WSS with a channel spacing of only 10 GHz. Owing to the high quality factor and quick roll-off of our filter design, adjacent channel crosstalk is measured to be < - 25 dB for channels spaced on a 10 GHz grid. As a further demonstration, we use five of seven WSS channels to perform a demultiplexing operation on both an 8 GHz and a 10 GHz grid. These results suggest that a low-loss WSS with fine channel resolution can be realized in a scalable manner using the silicon photonics platform.






Citations (33)


... The bulky volume of these devices limits their use in subsequent applications that urgently require miniaturization and integration. Fortunately, a variety of innovative on-chip spectral shaping devices [90][91][92][93][94][95][96][97] have recently emerged, offering significant potential for miniaturization essential for compact device applications. For example, PICs composed of MZI coupler arrays and linearly incremental delay lines can be programmed to perform various signal processing functions as needed [90][91][92]. ...

Reference:

A Review of Soliton Crystal Kerr Microcombs
Silicon photonic microresonator-based high-resolution line-by-line pulse shaping

... This will expand the number of channels accessible. [22,23,34] Finally, other degrees of freedom, such as the time-bins could be added to the setup. [35][36][37] Taken together, these modifications will dramatically increase the capacity for quantum information transfer within the network. ...

CMOS photonic integrated source of broadband polarization-entangled photons

... After the first PSR, the pump photons bidirectionally couple into a racetrack-shaped MRR with 500-nm-wide by 220-nmthick silicon single-mode waveguides throughout and adiabatic curves and directional couplers in the coupling sections [19]. The MRR was designed for a free spectral range of 38.4 GHz and intrinsic (loaded) Q factor of 3.7 × 10 5 (3.7 × 10 4 ) under the assumption of 2 dB cm −1 waveguide loss; experimentally we measured a loaded Q factor of ∼ 3.4 × 10 4 near the pump resonance. ...

Fine-Resolution Silicon Photonic Wavelength-Selective Switch Using Hybrid Multimode Racetrack Resonators
  • Citing Article
  • July 2024

Journal of Lightwave Technology

... The first experimental demonstration of a 36-dimensional quantum system entangled in polarisation, spatial mode and time-energy was done in [253], generating hyperentanglement. Hyperentangled photon pairs have since been generated in various configurations, including frequency-polarisation [254,255], polarisation-energy-time [164,225], path-frequency [198], polarisation-spatial modes [256], implemented on integrated platforms through the SPDC process. Hyperentanglement was also shown in Bragg reflection waveguides [257] and AlGaAs ridge waveguides [256]. ...

Tomography of ultrabroadband polarization-frequency hyperentangled photons
  • Citing Conference Paper
  • November 2023

... Frequency-bin states can be generated from compact sources, are easily manipulated using standard optical components, and the stability in their relative phase provides inherent resistance against mode mixing and phase noise in long-distance propagation. Furthermore, frequency-bin encoding has shown promise in overcoming challenges associated with solid state emitters, such as phonon dephasing and spectral diffusion, thus allowing for the generation of photonic cluster states [13,14] and facilitating scalable quantum information processing [15][16][17][18]. In particular, frequency-bins are compatible with spectrally heterogeneous matter qubits [5,19] and support dense spectral multiplexing making them prime candidates for quantum networking. ...

Frequency-bin photonic quantum information

... G.694.1) to numerous output fibers. For stabilization against the environmentally induced fluctuations in splitting ratio previously observed in [41], we tap 1% of the light in each direction to feedback the LCVR to maintain the pump splitting ratio [42]. In our setup we enable the WSSs to output a 100 GHz bin frequency-correlated channel. ...

Generation and characterization of ultrabroadband polarization–frequency hyperentangled photons

... Currently, microwave-to-optical links relying on spectrally-broadened microcombs [145] or multiple phaselocked microcombs are quite sophisticated [37,40,146]. This highlights the need for octave-spanning microcombs that can be easily self-referenced, simplifying the system and ensuring the detection of the carrier-envelope-offset frequency. ...

Vernier microcombs for high-frequency carrier envelope offset and repetition rate detection

... To date, dedicated devices have been developed and tailored for each application. The socalled quantum frequency processor [20,21], for instance, demonstrated mode-sorting of threedimensional frequency bins and their superpositions using a combination of phase modulators and pulse shapers. Similarly, interferometric setups based on beam splitters [22] or groupvelocity dispersion [23] have been used to decode time bins in up to four dimensions and two conjugate bases. ...

Characterization of Quantum Frequency Processors
  • Citing Article
  • November 2023

IEEE Journal of Selected Topics in Quantum Electronics

... Because the biphoton flux from our PPLN waveguide setup fluctuates significantly due to unstable coupling, we normalize all experimental correlation functions for ease of comparison. Specifically, histograms of the same qudit dimension d are scaled to conserve the total area under each curve-justified since the tested configurations differ only in spectral phase [39]. The peak across a given a family of scaled curves is then assigned a value of one for plotting in dimensionless units. ...

Time-Resolved Hanbury Brown–Twiss Interferometry of On-Chip Biphoton Frequency Combs Using Vernier Phase Modulation
  • Citing Article
  • March 2023

Physical Review Applied

... Resonators in our device (diagram in Fig. 1c) are designed using multimode waveguides. Operating these waveguides in the fundamental mode substantially diminishes the predominant loss mechanism of field-sidewall overlap in SiP waveguides, thereby ensuring lowloss performance 44,45 . The racetrack resonators include 200 μm-long straight waveguides, which have a width of 2 μm. ...

Low-loss, high finesse, add-drop resonators from a commercial silicon photonics foundry
  • Citing Conference Paper
  • November 2022