Computation times#
01:23.767 total execution time for 54 files from all galleries:
Example |
Time |
Mem (MB) |
|---|---|---|
Ionisation: the measured yields of argon, krypton and xenon ( |
00:10.074 |
0.0 |
Ionisation: the measured yields of N2 and O2 ( |
00:07.414 |
0.0 |
Dispersion uncertainty and sensitivity to dataset selection ( |
00:04.636 |
0.0 |
Cross-checks: phase-matching ratios and group-delay dispersion ( |
00:03.563 |
0.0 |
The compact models against their parents ( |
00:03.189 |
0.0 |
Wavelength coverage of the curated data ( |
00:02.736 |
0.0 |
Robustness: leaving one dataset out ( |
00:02.427 |
0.0 |
Group-velocity dispersion: the fits against the formulas in use ( |
00:02.313 |
0.0 |
Ionisation: the rates of molecules ( |
00:02.193 |
0.0 |
Ionisation: the Coulomb factor against Schrödinger calculations ( |
00:01.826 |
0.0 |
CO2 from the ultraviolet to its infrared windows ( |
00:01.823 |
0.0 |
Third-order uncertainty: statistical and working estimates ( |
00:01.676 |
0.0 |
Ionisation: the static rates of helium, neon and argon ( |
00:01.668 |
0.0 |
The second hyperpolarizability: every process on one curve ( |
00:01.568 |
0.0 |
Neon, argon, krypton and xenon in the extreme ultraviolet ( |
00:01.502 |
0.0 |
Carbon dioxide: the fitted model ( |
00:01.494 |
0.0 |
Argon: the curated data ( |
00:01.422 |
0.0 |
Argon: the fitted model ( |
00:01.411 |
0.0 |
Capillary zero-dispersion wavelength ( |
00:01.391 |
0.0 |
Ozone: the fitted model ( |
00:01.333 |
0.0 |
Helium: the fitted model ( |
00:01.301 |
0.0 |
Helium: the curated data ( |
00:01.236 |
0.0 |
Nitrogen: the fitted model ( |
00:01.140 |
0.0 |
Ionisation: the rates of the noble gases ( |
00:01.136 |
0.0 |
Nitrogen: the curated data ( |
00:01.083 |
0.0 |
Neon: the fitted model ( |
00:01.053 |
0.0 |
Krypton: the fitted model ( |
00:01.034 |
0.0 |
Neon: the curated data ( |
00:01.017 |
0.0 |
Xenon: the fitted model ( |
00:01.001 |
0.0 |
Carbon dioxide: the curated data ( |
00:00.983 |
0.0 |
Krypton: the curated data ( |
00:00.959 |
0.0 |
Ionisation: optmat’s rate of molecules ( |
00:00.943 |
0.0 |
Hydrogen: the fitted model ( |
00:00.936 |
0.0 |
Nitrous oxide: the fitted model ( |
00:00.898 |
0.0 |
Xenon: the curated data ( |
00:00.862 |
0.0 |
Oxygen: the fitted model ( |
00:00.853 |
0.0 |
Methane: the fitted model ( |
00:00.841 |
0.0 |
Hydrogen: the curated data ( |
00:00.835 |
0.0 |
Raman: the response functions of the gases ( |
00:00.833 |
0.0 |
Sulphur hexafluoride: the fitted model ( |
00:00.801 |
0.0 |
Oxygen: the curated data ( |
00:00.756 |
0.0 |
Carbon monoxide: the fitted model ( |
00:00.744 |
0.0 |
Methane: the curated data ( |
00:00.689 |
0.0 |
Ionisation: the noble gases against all-electron rates at 390 nm ( |
00:00.687 |
0.0 |
Two-photon ionisation of the noble gases ( |
00:00.686 |
0.0 |
Sulphur hexafluoride: the curated data ( |
00:00.658 |
0.0 |
Deuterium: the fitted model ( |
00:00.641 |
0.0 |
The dispersion of a helium-argon fill against pressure ( |
00:00.585 |
0.0 |
Nitrous oxide: the curated data ( |
00:00.566 |
0.0 |
Raman: fused silica’s response ( |
00:00.552 |
0.0 |
Fused silica: the complex index and n2 ( |
00:00.530 |
0.0 |
Helium in the extreme ultraviolet ( |
00:00.494 |
0.0 |
Linear density scaling against Lorentz-Lorenz ( |
00:00.421 |
0.0 |
Deuterium: the curated data ( |
00:00.355 |
0.0 |