Datasets:
Restore the analytic validation with the corrected sheath sign, measured signed
Browse files- README.md +16 -10
- figures/fig_analytic_validation.png +3 -0
README.md
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@@ -69,20 +69,26 @@ tracks each substrate's own internal-gradient variance, not the compression.
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## Is the physics right?
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Against an **exact** answer, not against another simulation. For an infinite coaxial hollow cylinder the
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| | measured | exact |
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| lumen field | **0.131%** of χ·B₀ | 0 |
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of χ·B₀ through the non-decaying dipole
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partial-volume occupancy suppresses it to
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## Susceptibility dephasing vs B₀ orientation
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## Is the physics right?
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Against an **exact** answer, not against another simulation. For an infinite coaxial hollow cylinder the
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answer is known in closed form, with no fitting freedom to hide an error in:
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* the field inside the lumen is **exactly zero** at every orientation;
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* inside the sheath at θ = 90°, `ΔB/B₀ = χ[−1/6 − ½(R_i²/r²)cos 2φ]`;
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* inside a *solid* cylinder the interior is uniform at `χ/6·(3cos²θ − 1)`.
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| | measured | exact |
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| lumen field | **0.131%** of χ·B₀ | 0 |
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| sheath amplitude | **0.9996×** analytic | 1 |
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| sheath structure, signed | **corr +0.9995, slope +0.999** | +1 |
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| solid-cylinder interior (θ=90°) | **−0.1649** χ·B₀ | −1/6 |
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All are permanent gates in the generator's test suite (`test_susceptibility_field_oracle.py`), not one-off
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checks, and the sheath comparison is **signed** — an inverted field fails it. The lumen null is the sharp
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one: a hard binary myelin source rings into the lumen at ~2.6% of χ·B₀ through the non-decaying dipole
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kernel, which would silently inflate intra-axonal dephasing; partial-volume occupancy suppresses it to
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~0.1%.
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## Susceptibility dephasing vs B₀ orientation
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figures/fig_analytic_validation.png
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Git LFS Details
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