mirror of
https://github.com/allaunthefox/Research-Stack.git
synced 2026-07-31 03:05:21 +00:00
Add Plasma Chiral Drag Witness Gate documentation
This commit is contained in:
parent
a2520eb4bf
commit
b95f1d9678
1 changed files with 196 additions and 0 deletions
196
6-Documentation/famm/PLASMA_CHIRAL_DRAG_WITNESS_GATE.md
Normal file
196
6-Documentation/famm/PLASMA_CHIRAL_DRAG_WITNESS_GATE.md
Normal file
|
|
@ -0,0 +1,196 @@
|
|||
# Plasma Chiral Drag Witness Gate
|
||||
|
||||
## Purpose
|
||||
|
||||
Add Alfvén-wave image rotation in rotating magnetized plasma as a physical witness model for torsion/chirality receipts.
|
||||
|
||||
The external source is Gueroult et al., **Image rotation in plasmas**, arXiv:2505.18062. The paper reports observation of image rotation: dragging of a wave's transverse structure by a moving medium, using Alfvén waves in plasma where the group velocity is slow enough for the drag to be measurable.
|
||||
|
||||
Project translation:
|
||||
|
||||
```text
|
||||
hidden rotating plasma medium
|
||||
→ Alfvén wave transverse image rotation
|
||||
→ signed chirality / torsion witness
|
||||
→ residual receipt
|
||||
→ FAMM scar or pass
|
||||
```
|
||||
|
||||
## Citeable equation
|
||||
|
||||
Image-rotation rate per unit length:
|
||||
|
||||
```math
|
||||
\phi
|
||||
=
|
||||
\frac{1}{2}\frac{\Omega}{\omega}k_{\parallel}
|
||||
\sim
|
||||
\frac{1}{2}\frac{\Omega}{v_A}
|
||||
```
|
||||
|
||||
Total image rotation over path length `L`:
|
||||
|
||||
```math
|
||||
\Delta\Theta_{\mathrm{img}}
|
||||
\approx
|
||||
L\phi
|
||||
\approx
|
||||
\frac{L\Omega}{2v_A}
|
||||
```
|
||||
|
||||
Plasma rotation from radial electric potential in a magnetized plasma:
|
||||
|
||||
```math
|
||||
\Omega
|
||||
=
|
||||
\frac{1}{rB_0}\frac{\partial \varphi}{\partial r}
|
||||
```
|
||||
|
||||
Combined project-use form:
|
||||
|
||||
```math
|
||||
\Delta\Theta_{\mathrm{img}}
|
||||
\approx
|
||||
\frac{L}{2v_A}
|
||||
\left(
|
||||
\frac{1}{rB_0}\frac{\partial\varphi}{\partial r}
|
||||
\right)
|
||||
```
|
||||
|
||||
## Residual receipt
|
||||
|
||||
```math
|
||||
R_{\mathrm{chiral\ drag}}
|
||||
=
|
||||
\left|
|
||||
\Delta\Theta_{\mathrm{obs}}
|
||||
-
|
||||
\frac{L\Omega}{2v_A}
|
||||
\right|
|
||||
```
|
||||
|
||||
Pass condition:
|
||||
|
||||
```math
|
||||
R_{\mathrm{chiral\ drag}}\le \Theta_{\mathrm{tol}}
|
||||
```
|
||||
|
||||
Scar condition:
|
||||
|
||||
```math
|
||||
R_{\mathrm{chiral\ drag}}>\Theta_{\mathrm{tol}}
|
||||
```
|
||||
|
||||
## Universal shortcut packet
|
||||
|
||||
```math
|
||||
\Gamma_{\mathrm{plasma\ drag}}
|
||||
=
|
||||
(
|
||||
X_{\mathrm{plasma}},
|
||||
\pi_{\mathrm{wave}},
|
||||
W_{\Delta\Theta},
|
||||
R_{\Omega},
|
||||
I_{\mathrm{angular}},
|
||||
G_{\mathrm{Alfven}},
|
||||
K,
|
||||
\epsilon
|
||||
)
|
||||
```
|
||||
|
||||
Meaning:
|
||||
|
||||
| Packet term | Meaning |
|
||||
|---|---|
|
||||
| `X_plasma` | hidden rotating magnetized plasma state |
|
||||
| `π_wave` | projection through Alfvén-wave propagation |
|
||||
| `W_ΔΘ` | observed image-rotation witness |
|
||||
| `R_Ω` | reconstruction/estimate of plasma rotation |
|
||||
| `I_angular` | angular/torsion/chirality invariant |
|
||||
| `G_Alfven` | guard: Alfvén wave, magnetized plasma, slow group velocity, known path geometry |
|
||||
| `K` | cost of measuring wave image versus direct medium state |
|
||||
| `ε` | residual between observed and predicted twist |
|
||||
|
||||
## BraidStorm crossing receipt
|
||||
|
||||
A braid crossing may now carry chiral drag:
|
||||
|
||||
```math
|
||||
\beta_{ij}:
|
||||
(s_i,s_j)
|
||||
\to
|
||||
(s_i',s_j',r_{ij},\epsilon_{ij},\Omega_{ij},\Delta\Theta_{ij})
|
||||
```
|
||||
|
||||
where `DeltaTheta_ij` is the signed wave/image twist witness for the crossing environment.
|
||||
|
||||
## FAMM object
|
||||
|
||||
```math
|
||||
\mathfrak C_{\mathrm{PlasmaChiralDrag}}
|
||||
=
|
||||
A_{16}(u_{\mathrm{plasma\_drag}})
|
||||
\otimes
|
||||
[
|
||||
\Sigma_{\mathrm{medium}}
|
||||
+
|
||||
\Sigma_{\Omega}
|
||||
+
|
||||
\Sigma_{B_0}
|
||||
+
|
||||
\Sigma_{v_A}
|
||||
+
|
||||
\Sigma_L
|
||||
+
|
||||
\Sigma_{\Delta\Theta}
|
||||
+
|
||||
\Sigma_{\chi}
|
||||
+
|
||||
\Sigma_{\epsilon}
|
||||
+
|
||||
\Sigma_{\mathrm{receipt}}
|
||||
]
|
||||
```
|
||||
|
||||
## Stack placement
|
||||
|
||||
```text
|
||||
PLASMA_CHIRAL_DRAG_WITNESS_GATE
|
||||
→ BraidStorm crossing receipt
|
||||
→ PIST torsional transition logic
|
||||
→ FAMM torsion/chirality scar ledger
|
||||
→ NUVMAP wave/medium address
|
||||
→ BJW Judge checks sign reversal and residual
|
||||
```
|
||||
|
||||
## Warden boundaries
|
||||
|
||||
Do not overclaim this gate as light in vacuum, universal wave twisting, or literal proof of every torsion model.
|
||||
|
||||
This gate is valid as a project primitive under the narrower condition:
|
||||
|
||||
```text
|
||||
rotating magnetized plasma + Alfvén wave transverse structure + measured image rotation
|
||||
```
|
||||
|
||||
The equation is a witness model, not a universal plasma theorem.
|
||||
|
||||
## Citation
|
||||
|
||||
Recommended short citation:
|
||||
|
||||
```bibtex
|
||||
@misc{gueroult2025image_rotation_plasmas,
|
||||
title = {Image rotation in plasmas},
|
||||
author = {Renaud Gueroult and Shreekrishna K. Tripathi and Jia Han and Patrick Pribyl and Jean-Marcel Rax and Nathaniel J. Fisch},
|
||||
year = {2025},
|
||||
eprint = {2505.18062},
|
||||
archivePrefix = {arXiv},
|
||||
primaryClass = {physics.plasm-ph},
|
||||
doi = {10.48550/arXiv.2505.18062}
|
||||
}
|
||||
```
|
||||
|
||||
## Project sentence
|
||||
|
||||
Plasma chiral drag can be modeled by `DeltaTheta_img ≈ L Omega/(2 v_A)`: a rotating magnetized plasma drags the transverse structure of an Alfvén wave, so observed image rotation becomes a signed torsion/chirality receipt for hidden medium rotation.
|
||||
Loading…
Add table
Reference in a new issue