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FDTD simulations of THz pulse control via moving fronts | Communications Physics 4, 162 (2021) | SLIPSTREAM platform

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THz Wave Control via Moving Dielectric Fronts - SLIPSTREAM Platform

2D Finite-Difference Time-Domain (FDTD) simulations of terahertz (THz) wave manipulation using relativistic moving fronts in semiconductor-filled waveguides. This work demonstrates temporal stretching and time-reversal of THz pulses through spatiotemporal control of photoexcited carrier density.

🔬 Overview

This repository contains the FDTD simulation code used to generate Figure 2 in our Nature Communications Physics publication on the SLIPSTREAM (Spacetime Light-Induced Photonic STRucturEs for Advanced Manipulation) platform.

The work explores how moving dielectric perturbations - created by photoexciting mobile charge carriers in a semiconductor waveguide - can manipulate THz light in exotic ways including temporal pulse stretching and time-reversal operations.

Paper: Front-induced transitions control THz waves
A.W. Schiff-Kearn, L. Gingras, S. Bernier, J.-M. Ménard, and D.G. Cooke
Communications Physics 4, 162 (2021)


🎯 Physical Concept

The SLIPSTREAM Platform

Key Innovation: By tilting the pulse front of a near-infrared pump laser, we create a moving front of photoexcited carriers in a silicon-filled parallel plate waveguide. This front travels at a controllable velocity vf relative to the THz wave velocity c/nSi.

Three Regimes:

  1. Subluminal (vf < c/nSi) - THz pulse stretching with quasi-static plateaus
  2. Luminal (vf ≈ c/nSi) - Optimal phase-matched emission
  3. Superluminal (vf > c/nSi) - Time-reversal via front-induced transitions

Physical Mechanism

  • THz Generation: Built-in Schottky fields at metal-semiconductor interfaces
  • Pulse Shaping: Spatiotemporal modulation via moving photoexcitation front
  • Control Parameter: Front velocity tuned by optical pump tilt angle
  • Applications: Sub-cycle THz control, dispersion compensation, pulse engineering

💻 My Contributions - Simulation Work

What I Did (Subluminal Regime Simulations) ✅

I developed and executed 2D-FDTD simulations for the subluminal regime that successfully:

  • Modeled the parallel plate waveguide geometry with silicon and conducting boundaries
  • Implemented Schottky field emission at top and bottom metal-semiconductor interfaces
  • Incorporated Drude dispersion model for photoexcited silicon with realistic carrier densities (~10¹⁷ cm⁻³)
  • Simulated moving carrier density fronts with velocity vf = 0.86 c/nSi
  • Reproduced experimental THz waveforms showing temporal pulse stretching
  • Validated the quasi-static plateau formation mechanism

Key Achievement: The simulations in Figure 2 of the paper quantitatively matched experimental data for various beam clipping configurations, confirming our physical understanding of the subluminal pulse stretching mechanism.

Technical Implementation

FDTD Algorithm Details:

  • 2D spatial grid with perfectly conducting boundaries
  • Time-stepping with Courant stability condition
  • Drude model: carrier scattering time τ = 0.1 ps
  • Schottky field depth: ~1 μm (Debye length)
  • TEM mode extraction at fixed position
  • Post-processing filter for detection response

🚧 Challenges and Limitations

Superluminal Regime - Numerical Difficulties

The Challenge: While the subluminal simulations worked excellently, I encountered significant numerical challenges when attempting to simulate the superluminal regime (vf ≥ c/nSi).

Technical Issues:

  • Standard FDTD algorithms become unstable near or beyond the phase velocity
  • Numerical dispersion errors accumulate for relativistic front velocities
  • Courant condition violations for fast-moving dielectric perturbations
  • Difficulty capturing front-induced transitions at phase-matched conditions

What Was Needed:

  • Modified FDTD schemes with moving reference frames
  • Specialized boundary conditions for superluminal fronts
  • Enhanced numerical stability for relativistic regime
  • Time-domain formulation of frequency-shifting processes

Personal Context

Unfortunately, I became seriously ill (cancer diagnosis and treatment) before I could develop and implement the modified FDTD algorithm necessary for the superluminal regime simulations. The paper was published during my recovery period.

Impact: The experimental results for time-reversal (superluminal regime) were not independently confirmed numerically in the publication. While the physics is well-supported by theory and experimental data, full numerical validation would have strengthened the complete picture.


📂 Repository Contents

This repository contains the working FDTD code for subluminal simulations that successfully generated Figure 2 of the paper.

Included:

  • 2D-FDTD solver for THz propagation
  • Moving front carrier density profiles
  • Schottky field implementation
  • Drude dispersion for photoexcited silicon
  • Post-processing and filtering

Not Included:

  • Superluminal regime solver (requires algorithmic modifications)
  • Time-reversal simulations
  • Full 3D field distributions

🔗 Broader Context - Moving Front Research

This experimental work on THz optics connects to my subsequent computational studies on quantum systems:

Common Thread: Spatiotemporal quenches and moving fronts

  • This work (2021): THz photonics with moving dielectric fronts
  • Long-range paper (2023): Quantum quenches in Ising models with power-law interactions
  • 2D paper (2025): Efficient ground state preparation via moving parameter fronts

Insight: The concept of using moving fronts to control systems - whether electromagnetic waves or quantum wavefunctions - proved to be a powerful unifying theme across my research.


📄 Publication

Front-induced transitions control THz waves
A.W. Schiff-Kearn, L. Gingras, S. Bernier, J.-M. Ménard, and D.G. Cooke
Communications Physics 4, 162 (2021)
Open Access - Nature Publishing Group

My Role

Simulation contributor - Developed FDTD simulations for subluminal regime (Figure 2), validating experimental pulse stretching mechanism and demonstrating quantitative agreement between theory and experiment.


Software

  • MATLAB implementation (this repository)
  • Custom 2D-FDTD solver
  • Drude dispersion integration
  • Spatiotemporal source modeling

💡 Lessons and Future Work

What I Learned

✓ FDTD is powerful for electromagnetic problems but requires care near phase transitions
✓ Subluminal regime is more numerically stable than superluminal
✓ Good agreement between simulation and experiment validates physical models
✗ Superluminal regime needs specialized numerical methods
✗ Standard FDTD breaks down for relativistic moving boundaries


🔗 Dependencies

  • MATLAB (any recent version)
  • Standard numerical libraries
  • No special toolboxes required

📧 Contact

Simon Bernier


📝 Citation

If you use this code or build upon this work, please cite:

@article{schiffkearn2021front,
  title={Front-induced transitions control THz waves},
  author={Schiff-Kearn, A.W. and Gingras, L. and Bernier, S. and M{\'e}nard, J.-M. and Cooke, D.G.},
  journal={Communications Physics},
  volume={4},
  pages={162},
  year={2021},
  publisher={Nature Publishing Group},
  doi={10.1038/s42005-021-00667-4}
}

🎯 Bottom Line

What worked: FDTD simulations successfully validated the subluminal THz pulse stretching mechanism, providing quantitative agreement with experimental observations.

What didn't: Superluminal regime simulations required algorithmic modifications I couldn't complete due to illness.

Why it matters anyway: The successful subluminal simulations confirmed our physical understanding and enabled publication of a complete experimental story. Sometimes research challenges come from unexpected places, but the work that did get done contributed meaningfully to advancing THz photonics.


This project demonstrates: electromagnetic simulation, FDTD methods, ultrafast optics, THz photonics, spatiotemporal control, and the reality that research doesn't always go according to plan - but valuable contributions can still be made.

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FDTD simulations of THz pulse control via moving fronts | Communications Physics 4, 162 (2021) | SLIPSTREAM platform

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