Age | Commit message (Collapse) | Author | |
---|---|---|---|
2025-04-21 | New way to adjust γ with simulation | Jaron Kent-Dobias | |
2025-04-20 | Removed singularity at τ₀ = 2 | Jaron Kent-Dobias | |
2025-04-20 | Change convention to fixed Γ₀, and changed behavior on NaN | Jaron Kent-Dobias | |
2025-04-20 | More information in energy output | Jaron Kent-Dobias | |
2025-04-20 | Removed unnecessary header. | Jaron Kent-Dobias | |
2025-04-20 | Standardized saving and loading of files | Jaron Kent-Dobias | |
2025-04-20 | Added support for loading data from previous runs | Jaron Kent-Dobias | |
2025-04-20 | Output full correlation files each step, and decrease γ on failure | Jaron Kent-Dobias | |
2025-04-20 | Another iteration tweak | Jaron Kent-Dobias | |
2025-04-20 | Adjust ε from the command line | Jaron Kent-Dobias | |
2025-04-20 | Reverting | Jaron Kent-Dobias | |
2025-04-20 | Testing alternate iterate | Jaron Kent-Dobias | |
2025-04-20 | Added singular solution | Jaron Kent-Dobias | |
2025-04-20 | Change to convention normalizing Γ₀ by τ₀ | Jaron Kent-Dobias | |
2025-04-20 | Un-debug the energy | Jaron Kent-Dobias | |
2025-04-20 | Fixed serious mistake in log inverse transform | Jaron Kent-Dobias | |
2025-04-19 | Removed external μ control | Jaron Kent-Dobias | |
2025-04-19 | Tweak | Jaron Kent-Dobias | |
2025-04-19 | Small tweak | Jaron Kent-Dobias | |
2025-04-19 | Fixed energy | Jaron Kent-Dobias | |
2025-04-19 | Use Simpson integrator for the regular fourier case too | Jaron Kent-Dobias | |
2025-04-19 | Many changes to the original integrator | Jaron Kent-Dobias | |
2025-04-19 | Smaller increase to μ after failure | Jaron Kent-Dobias | |
2025-04-19 | Changed iteration again | Jaron Kent-Dobias | |
2025-04-19 | Back to other iterate | Jaron Kent-Dobias | |
2025-04-19 | Tweaked iteration | Jaron Kent-Dobias | |
2025-04-19 | Faster approach to μ | Jaron Kent-Dobias | |
2025-04-19 | Back to other iterator | Jaron Kent-Dobias | |
2025-04-19 | Grow μ before trying agian. | Jaron Kent-Dobias | |
2025-04-19 | Disable γ for now | Jaron Kent-Dobias | |
2025-04-19 | More controls after failure | Jaron Kent-Dobias | |
2025-04-19 | More tweaks | Jaron Kent-Dobias | |
2025-04-19 | New way to regularize the factor | Jaron Kent-Dobias | |
2025-04-19 | More sqrts | Jaron Kent-Dobias | |
2025-04-19 | More tweaks | Jaron Kent-Dobias | |
2025-04-19 | Tweaks | Jaron Kent-Dobias | |
2025-04-19 | Trying new approach | Jaron Kent-Dobias | |
2025-04-19 | Fixed failsafe | Jaron Kent-Dobias | |
2025-04-19 | Tweaks | Jaron Kent-Dobias | |
2025-04-19 | Many tweaks | Jaron Kent-Dobias | |
2025-04-19 | Slower step-size build-up | Jaron Kent-Dobias | |
2025-04-19 | Faster step size build-up | Jaron Kent-Dobias | |
2025-04-19 | More straightforward adjustment of step size | Jaron Kent-Dobias | |
2025-04-19 | Start μ larger | Jaron Kent-Dobias | |
2025-04-19 | Iteration tweak | Jaron Kent-Dobias | |
2025-04-19 | Back to the old scheme | Jaron Kent-Dobias | |
2025-04-19 | Don't rely on past output for μ | Jaron Kent-Dobias | |
2025-04-19 | Softer quitting requirements for μ | Jaron Kent-Dobias | |
2025-04-19 | Start from β = 0 again | Jaron Kent-Dobias | |
2025-04-19 | Better setting of μ bounds | Jaron Kent-Dobias | |