High-γ Charge Field and EO Workbench
P3 · ASD-PRED-003. Compare recorded detector signals rather than ideal source fields. The Ota case remains open.
Registry and comparison planning; no new canonical physical result or closed quantitative discriminator.
Standard transverse field of a uniformly moving point charge, normalized to its ideal peak. A Gaussian response only demonstrates temporal resolution. Ota bunch, crystal, conductor boundaries and gain are omitted; this is neither an Ota reproduction nor an ASD curve.
γ = 69.4933 · b/(γβc) = 0.0960 ps
The linear response uses a unit-area kernel; its peak is not renormalized.
S_ASD(t), V_ASD(t), ΔS(t): not calculated. A normalized field cannot directly replace the EO differential readout.
01What the experiment records
Ota et al. (2022) studied spatiotemporal fields around a relativistic electron beam through optical modulation in electro-optic sampling. The paper specifies a 35 MeV beam and discusses possible instrumental causes of a measured peak below the calculation. That discrepancy is not ASD evidence.
The paper states that data and code are available from the corresponding author on reasonable request. No raw time series, calibration files or complete reproduction code have been acquired here; no author contact or fit is claimed.
02From source field to signal
An operational linear small-signal interface is
This defines a response integral, not a new ASD field equation. contains crystal, laser and sampling response; is independently calibrated gain and instrument parameters. Nonlinear, dispersive or nonstationary responses require appropriate extensions. Each theory supplies through the same apparatus chain before comparing . Theory-dependent calibration must also be propagated.
03Strict limits of the current baseline
The workbench computes only the standard normalized transverse field of a uniformly moving point charge, , followed by an assumed Gaussian temporal kernel. It omits the real 3D bunch, ZnTe dispersion, phase matching, reflections, conductor boundaries, irradiation and optical transfer. It checks how response changes a waveform; it is not an Ota reproduction.
04Required joint calculation
First reproduce the paper's standard source and recorded signal; then independently calculate the general ASD moving source and laboratory mapping. Freeze bunch inputs, time zero, gain and noise covariance, and compare full waveform, width, sign and spatial scans. Do not multiply an EO readout by a co-moving parallel-charge force ratio. Advance OP-EM-001 and OP-EM-004 separately.
Reference constants: PDG 2024 electron.
Position within the framework
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Revision history
Existing canonical module snapshots / 现有正式模块快照 · Predictions & Falsification v1.0 · review 2026-09-22
Download source and scope manifest
Based on versioned canonical modules and cited instrument literature. This experimental program adds operational templates, not new canonical field equations.
Knowledge scopeASD: High-γ Charge Field and EO Workbench. ASD-EM-HIGH-GAMMA-CHARGE-FIELD-EN. Version 1.0.0; 2026-09-22. https://asd-physics.org/en/tests/case-studies/high-gamma-charge-field. Predictions & Falsification v1.0 · review 2026-09-22. Source EXP-7ca61744dcd2.
Continue with the assumptions, equations and sources.
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