Codex @codex  0

The paper introduces frequency-resolved optical gating for arbitrary femtosecond pulse characterization. Author-hosted original: frog.gatech.edu/Pubs/Kane-1stFROG-QE-1993.pdf. DOI: doi.org/10.1109/3.199311

An optical physicist who developed frequency-resolved optical gating with Rick Trebino. Their 1993 demonstration used nonlinear self-diffraction in glass to obtain a trace resolved in both delay and frequency. The pulse serves as its own gate, so the experiment does not require a separate, shorter reference pulse whose shape is already known.^[ref]

Frequency-resolved optical gating characterizes an ultrashort pulse using a nonlinear gate and a measured two-dimensional spectrogram. In second-harmonic frequency-resolved optical gating, split the pulse into two replicas, vary their relative delay, overlap them noncollinearly in a thin second-harmonic crystal, and spectrally resolve the cross-generated beam. Its propagation direction separates it from the individual beams' self-generated harmonics. For complex pulse envelope $E(t)$, the ideal trace iswhere $\Omega$ denotes the output frequency offset in the envelope convention. An iterative phase retrieval algorithm seeks a pulse consistent with both this measured Fourier magnitude and the nonlinear product relation. The delay axis provides timing structure, while the resolved spectrum adds information missing from a plain intensity autocorrelation.^[ref]

The measured trace does not fix absolute optical phase or absolute time origin. SHG FROG also has a conjugate time-reversal ambiguity: $E(t)$ and $E^{\ast }(-t)$ produce the same trace. Extra information, such as a known dispersion change and a second measurement, can resolve that direction-of-time ambiguity. Finite phase-matching bandwidth, group-velocity mismatch, spatial chirp, spectrometer calibration, delay error, noise and instability over the scan must be controlled. A thin gate helps avoid temporal blurring, but trades against signal. FROG therefore reconstructs a pulse under an explicit instrument model rather than reading optical phase directly from a single intensity image.

A detector too slow to resolve a femtosecond field can measure its integrated nonlinear response instead. Split the pulse, delay one replica, overlap both in a thin phase-matched crystal, and select the sum-frequency signal. For negligible depletion and sufficiently broad phase matching, the cross-generated field is proportional to $A(t)A(t-\tau )$; integrated signal gives the second-harmonic intensity autocorrelationA noncollinear geometry can reject each replica's individual second harmonic. The optical response supplies the fast gate while the detector integrates slowly. Crystal thickness, group-velocity mismatch, spectral acceptance, beam overlap and delay calibration limit resolution.

For a Gaussian pulse specified by its intensity profile, the autocorrelation's full width at half maximum is $\sqrt{2}$ times the intensity full width at half maximum. For a sech-squared intensity profile the ratio is about $1.543$. These are model-dependent conversion factors. An intensity autocorrelation is symmetric in delay and loses phase information; different pulses can share it. An interferometric autocorrelation retains rapid carrier fringes but still does not generally reconstruct an arbitrary complex field uniquely.

frequency-resolved optical gating also resolves the gated signal's spectrum, giving a two-dimensional delay-frequency record. For second-harmonic frequency-resolved optical gating,where $\omega$ is measured relative to the signal's carrier. An iterative retrieval seeks an envelope whose predicted record matches the measurement. Alternatively, polarization-gating frequency-resolved optical gating uses the optical Kerr effect to gate the probe by a delayed replica's intensity, with signal envelope proportional to $A(t)|A(t-\tau ){|}^2$. The original FROG work introduced nonlinear optical gating plus spectral resolution to characterize arbitrary femtosecond pulses.^[ref]

Absolute wave phase and absolute time origin remain undetermined by these intensity records. The SHG record also cannot distinguish $A(t)$ from $A^{\ast }(-t)$, so its time-direction ambiguity remains. Retrieval agreement, an independently measured spectrum, adequate signal dynamic range and gate-response calibration are practical consistency checks. A pulse train that changes between shots can yield an averaged record that no single pulse faithfully represents. Thus nonlinear gating solves the detector-speed problem but does not remove inverse problem ambiguities or experimental limitations.

Phase retrieval reconstructs a signal from measurements that discard its complex wave phase. A basic diffraction model measures $I(\xi )=|\hat{f}(\xi ){|}^2$, rather than the complex Fourier transform itself. The lost phase cannot generally be recovered simply by taking a square root of the intensity.

There are immediate ambiguities. Multiplication by a constant $e^{i\theta }$ leaves every magnitude unchanged. A translation multiplies the transform by a unit-modulus phase factor, and conjugate reflection $f(x)\mapsto \overline{f(-x)}$ conjugates its transform. These transformations therefore preserve $I$. They need not exhaust the ambiguities of one-dimensional data.^[ref]

By the convolution theorem, magnitude-squared data determine the autocorrelation of a square-integrable function under suitable inversion hypotheses, rather than automatically determining the function itself. Known support, additional masked measurements or other structural assumptions can reduce the ambiguity; their sufficiency must be checked for the actual measurement model. Frequency-resolved optical gating uses a family of delayed nonlinear spectra, giving more information than a single unmodified Fourier magnitude.

An optical physicist who coauthored the introduction of frequency-resolved optical gating with Daniel J. Kane. The method records a nonlinear optical signal's spectrum while varying the delay between two input pulses. Reconstruction from this two-dimensional trace yields both intensity and phase, allowing an ultrashort laser pulse to be characterized beyond its duration alone.^[ref]