Computed runs from the public BEC Ground State example. Explore scientific results, code changes, and provenance.
View source ↗--- a/experiments/harmonic-reference.json
+++ b/experiments/harmonic-interacting.json
@@ -1 +1 @@
-{"experiment":"harmonic-ground-state","method":"split-step","g":0,"dt":0.01,"nx":256,"xmax":8,"trap":"harmonic"}+{"experiment":"harmonic-ground-state","method":"split-step","g":1,"dt":0.01,"nx":256,"xmax":8,"trap":"harmonic"}At fixed harmonic trap, dt, and grid, increasing g from 0 to 1 changes E from 0.499877011 to 0.689403720 ℏω and μ from 0.499877011 to 0.869941623 ℏω. This is the computed repulsive-interaction case; the differences are relative to the non-interacting reference, not a convergence estimate.
Computed with the 1D Gross-Pitaevskii solver (split-step, g=1, dt=0.01).
| Fact | Value | Source |
|---|---|---|
Ground-state energy★ Uncategorised / solver.energy | 0.6894037 ℏω | results/harmonic-interacting/summary.json#/energy |
Grid half-width Uncategorised / grid.half_width | 8 aₕₒ | command |
Grid points Uncategorised / grid.points | 256 | command |
Chemical potential Uncategorised / solver.chemical_potential | 0.8699416 ℏω | results/harmonic-interacting/summary.json#/chemical_potential |
Imaginary-time step Uncategorised / solver.imaginary_time_step | 0.01 ω⁻¹ | command |
Interaction strength g Uncategorised / solver.interaction_strength | 1 dimensionless | command |
Iterations Uncategorised / solver.iterations | 444 | results/harmonic-interacting/summary.json#/iterations |
Imaginary-time method Uncategorised / solver.method | split-step | command |
Normalization error Uncategorised / solver.normalization_error | 0 | results/harmonic-interacting/summary.json#/normalization_error |
Stationary-equation residual Uncategorised / solver.stationary_residual | 0.0005514652 | results/harmonic-interacting/summary.json#/residual |
Trap potential Uncategorised / trap.type | harmonic | command |
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