[Paper Review] Generation of spatiotemporal optical vortices with partial temporal coherence
This paper demonstrates the generation of spatiotemporal optical vortices (STOVs) with transverse orbital angular momentum using partially coherent light sources, such as amplified spontaneous emission (ASE) or noise-like pulses, instead of expensive mode-locked lasers. By applying a spiral phase to broadband, temporally incoherent pulses via a spatial light modulator, the authors experimentally verify STOVs with topological charges l = ±1 and l = +2 through interference-based phase transition measurements, proving that partial temporal coherence enables stable, low-cost STOV generation.
Recently, a spatiotemporal optical vortex (STOV) with a transverse orbital angular momentum (OAM) has been generated from coherent ultrafast pulses using mode-locked lasers. In contrast, we demonstrate theoretically and experimentally that a STOV can be generated from a light source with partial temporal coherence with fluctuating temporal phase. By eliminating the need of mode-locked laser sources, the partially coherent STOV will serve as a convenient and cost-effective transverse OAM source.
Motivation & Objective
- To develop a low-cost alternative to mode-locked lasers for generating spatiotemporal optical vortices (STOVs) with transverse orbital angular momentum (OAM).
- To investigate whether STOVs can be generated from partially coherent temporal sources such as ASE or noise-like pulses (NLPs), which lack stable phase relationships.
- To experimentally verify the existence of phase singularities and topological charge in partially coherent STOVs using interference-based detection with a time-delayed reference beam.
- To demonstrate that higher-order STOVs (l > 1) spontaneously split into multiple fundamental vortices due to random phase fluctuations, even without propagation.
Proposed method
- Modeling partially coherent pulses using a Gaussian spectrum with randomly distributed spectral phase, where the variance σ² controls the degree of temporal incoherence.
- Applying a spiral phase 𝑒𝑖𝑙𝜙 in the spatial-frequency domain via a 2D spatial light modulator (SLM) to generate STOVs from broadband, partially coherent sources.
- Numerically simulating STOVs using a 2D Fourier transform of the pulse envelope with random spectral phase, using equation 𝐴(𝑡) = 𝐹𝑇{𝑒−𝜔²/𝑟² 𝑒^{𝑗𝜙𝑟𝑎𝑛𝑑(𝜔)}}, where 𝜙𝑟𝑎𝑛𝑑(𝜔) ~ 𝑁(𝜇, 𝜎²).
- Measuring phase singularities via interference fringes between a reference beam and the object STOV, using a time-delayed reference beam and CCD detection, as described by the interference integral in equation (3).
- Using the time-averaged Poynting vector <𝑺> ∝ 𝑖(𝑢∇𝑢∗ − 𝑢∗∇𝑢)/2 + 𝑘|𝑢|²𝒛 to visualize vortex structures and singularities in the spatiotemporal domain.
- Experimentally generating STOVs using ASE from a Yb-doped fiber laser operated below threshold and from a noise-like pulse (NLP) state, both exhibiting high spatial and partial temporal coherence.
Experimental results
Research questions
- RQ1Can spatiotemporal optical vortices (STOVs) be generated using partially coherent light sources instead of mode-locked lasers?
- RQ2How does random temporal phase fluctuation affect the stability and structure of STOVs with topological charge l > 1?
- RQ3Can phase singularities in partially coherent STOVs be experimentally verified using interference-based detection with a time-delayed reference beam?
- RQ4What is the impact of increasing temporal incoherence (σ²) on the formation and morphology of STOVs?
- RQ5Can STOVs with topological charge l = 2 be generated and resolved into multiple fundamental vortices due to intrinsic phase randomness?
Key findings
- Partially coherent STOVs with topological charge l = 1 were successfully generated and experimentally verified using ASE and NLP sources, with clear phase transitions observed in interference patterns.
- For l = 1, a single π phase transition was observed in interference fringes, confirming the presence of a single phase singularity, with coherent time ~450 fs based on 8 nm bandwidth.
- For l = 2, two distinct π phase transitions were observed in the interference pattern, confirming the splitting of the high-order vortex into two fundamental vortices due to random phase fluctuations.
- Numerical simulations showed that increasing σ² from 0.2π² to π² severely distorts the ring-shaped STOV profile, introducing multiple amplitude peaks and singularities across the temporal domain.
- The experimental phase transition patterns for l = +1 and l = +2 matched theoretical predictions, with time delays of -68 fs, 0 fs, and 32 fs (l = +1), and multiple delays spanning -216 fs to 180 fs (l = +2), confirming vortex order.
- The method enables low-cost STOV generation using broadband sources like LEDs or fiber laser ASE, eliminating the need for expensive mode-locked lasers.
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This review was created by AI and reviewed by human editors.