# 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.