EQUATION REGISTRY

Conditional position distribution for a detection protocol

Nonzero total detection rate with stated efficiency, thickness and time window. For normal-flux sampling jn=vn|Ψ|²; normalized squared modulus also requires constant or cancelling vn across compared positions.

Theory · EFFECTIVE MODELEquation version 1.0.0

Based on the final manuscript · Chapter 5

ASD-WEB-QM-027
R(r,t)=ηD(r,t)∣Ψ∣2,RA=∫thicknessR dz,p(Y∣det)=∫TRA(Y,t)dt∫dA∫TRA(Y,t)dt\mathcal R(\mathbf r,t)=\eta_D(\mathbf r,t)|\Psi|^2,\quad\mathcal R_A=\int_{\rm thickness}\mathcal R\,dz,\quad p(Y\mid\mathrm{det})=\frac{\int_{\mathcal T}\mathcal R_A(Y,t)dt}{\int dA\int_{\mathcal T}\mathcal R_A(Y,t)dt}

Nonzero total detection rate with stated efficiency, thickness and time window. For normal-flux sampling jn=vn|Ψ|²; normalized squared modulus also requires constant or cancelling vn across compared positions.
Chapter reference: Ch. 5 (5.3.20)–(5.3.21) · ASD-BOOK-ddbade997b45

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Adopted source, conditions and previous versions

Ch. 5 (5.3.20)–(5.3.21)

Nonzero total detection rate with stated efficiency, thickness and time window. For normal-flux sampling jn=vn|Ψ|²; normalized squared modulus also requires constant or cancelling vn across compared positions.

Conditions retained in this adoption

  • Selected channel and stated initial/boundary conditions; action/energy matching retained
  • Continuum, slow-envelope and detector approximations kept at their respective levels

Specific unresolved source issues

  • QC-DETECTION-002: normal-velocity weighting in the Born reduction

Source locators: p1954 · p1959 · p1960 · p1962 · p2305

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

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QM-0accdcbe7725 · Ch. 5 (5.3.20)–(5.3.21)

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