Computation times#
05:42.966 total execution time for 55 files from all galleries:
Example |
Time |
Mem (MB) |
|---|---|---|
Two crossing beams in Cartesian free space ( |
01:33.079 |
0.0 |
A frequency-dependent Kerr response ( |
00:34.638 |
0.0 |
A radial filament in argon ( |
00:33.322 |
0.0 |
Resonant dispersive-wave propagation ( |
00:23.156 |
0.0 |
A four-wave-mixing delay scan through one backend ( |
00:23.103 |
0.0 |
Far-field spectra through apertures ( |
00:19.938 |
0.0 |
Explore exact step-index fibres and hollow rectangular guides ( |
00:17.183 |
0.0 |
Separate nitrogen and oxygen ionisation in an air-filled capillary ( |
00:10.902 |
0.0 |
An interactive session: design, run, compress ( |
00:09.616 |
0.0 |
Fewer source calls: the two integrators ( |
00:09.327 |
0.0 |
Nonlinear beam preparation and coupling into a capillary ( |
00:08.435 |
0.0 |
Mode conversion and loss in a taper with a coherent wall ( |
00:08.089 |
0.0 |
The vector wall: two impedances, two families, one conversion ( |
00:06.291 |
0.0 |
A line beam: diffraction and the (1+1)-D Kerr soliton ( |
00:05.236 |
0.0 |
Self-imaging in a graded-index guide, and a launch declared as a field ( |
00:04.282 |
0.0 |
GNLSE propagation: an N = 3 soliton ( |
00:04.112 |
0.0 |
A declared basis of a split pair: two bases, one answer ( |
00:04.062 |
0.0 |
Package overview ( |
00:03.625 |
0.0 |
A planar guide resolved in y ( |
00:02.1000 |
0.0 |
Use tabulated hollow and solid-core modes ( |
00:02.550 |
0.0 |
A Cartesian beam in argon ( |
00:02.325 |
0.0 |
Compare material choices ( |
00:02.209 |
0.0 |
Calibrating a weak band with the low-storage march ( |
00:02.203 |
0.0 |
Propagate through a single-ring antiresonant fibre ( |
00:01.774 |
0.0 |
Scan helium pressure and pulse energy ( |
00:01.711 |
0.0 |
Propagate a vector fibre mode, and check it against the GNLSE ( |
00:01.695 |
0.0 |
Compare a carrier-resolved pulse with envelope plasma ( |
00:01.592 |
0.0 |
A hollow planar waveguide, per unit width ( |
00:01.508 |
0.0 |
The coherent wall of a capillary, against the incoherent one ( |
00:01.091 |
0.0 |
Radial diffraction and a separate self-focusing diagnostic ( |
00:00.928 |
0.0 |
Analysing a saved run ( |
00:00.916 |
0.0 |
Gas flow in a hollow fibre: tapers, choked ends and the flow regime ( |
00:00.236 |
0.0 |
Follow vector Raman coherence with a delayed probe ( |
00:00.220 |
0.0 |
Grating spacing and prism insertion ( |
00:00.217 |
0.0 |
A pulse on both grids ( |
00:00.203 |
0.0 |
Inspect step-index and graded-index electric fields ( |
00:00.194 |
0.0 |
Vacuum-ultraviolet dispersive-wave emission in a gas-filled capillary ( |
00:00.000 |
0.0 |
Self-phase modulation and post-compression ( |
00:00.000 |
0.0 |
Soliton self-compression and ultraviolet dispersive-wave emission ( |
00:00.000 |
0.0 |
Four-wave mixing into the vacuum ultraviolet ( |
00:00.000 |
0.0 |
Cross-phase modulation in the deep ultraviolet ( |
00:00.000 |
0.0 |
Raman soliton self-frequency shift in hydrogen ( |
00:00.000 |
0.0 |
Photoionisation-induced soliton blue-shift ( |
00:00.000 |
0.0 |
The vacuum-ultraviolet dispersive wave under a frequency-dependent Kerr response ( |
00:00.000 |
0.0 |
Deep-ultraviolet four-wave mixing in argon under a frequency-dependent Kerr response ( |
00:00.000 |
0.0 |
Supercontinuum by self-phase modulation ( |
00:00.000 |
0.0 |
Supercontinuum by soliton self-compression, reaching the vacuum ultraviolet ( |
00:00.000 |
0.0 |
Supercontinuum by modulational instability ( |
00:00.000 |
0.0 |
Comb-to-continuum broadening in hydrogen ( |
00:00.000 |
0.0 |
A pressure-gradient soliton compressor ( |
00:00.000 |
0.0 |
A tapered capillary: compression, a dispersive wave and mode conversion ( |
00:00.000 |
0.0 |
Radially and azimuthally polarised pulses: the vector wall over a metre ( |
00:00.000 |
0.0 |
Spatiotemporal propagation in a graded-index multimode fibre ( |
00:00.000 |
0.0 |
A tapered graded-index fibre: adiabatic and abrupt mode conversion ( |
00:00.000 |
0.0 |
A planar hollow-waveguide compressor ( |
00:00.000 |
0.0 |