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Beta Spectrum Calculator — Knowledge Base 2026-04-26
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Beta Spectrum Calculator — Knowledge Base

This Obsidian vault serves as the scientific reference and development workspace for the beta-spectrum calculator project (beta_shape_pnpi).

Purpose

Organize the physics theory behind β-decay spectrum calculations into structured, interconnected notes that inform the implementation of correction components in the codebase.

Source Material

Reference Type Location
Hayen et al., Rev. Mod. Phys. 90, 015008 (2017) Review article refs/electromagnetic/2017_Hayen_analytical_beta_shape/summary

Directory Structure

docs/
├── README.md                          ← You are here
├── 00-beta-spectrum-overview.md       ← Master equation & full correction list
├── 02-phase-space.md                  ← Baseline spectral shape
├── corrections/                       ← All correction components
│   ├── 01-fermi-function.md           ← Fermi function F₀(Z,W)
│   ├── 02-finite-size.md              ← Nuclear size: L₀, U, DFS
│   ├── 03-screening.md                ← Atomic screening S(Z,W)
│   ├── 04-exchange.md                 ← Atomic exchange X(Z,W)
│   ├── 05-radiative.md                ← Outer radiative R(W,W₀)
│   ├── 06-recoil.md                   ← Recoil: R_N, Q, weak magnetism
│   ├── 07-detector-response.md        ← Detector convolution
│   ├── 08-atomic-overlap.md           ← Atomic mismatch r(Z,W)
│   └── 09-chemical-effects.md         ← Molecular environment
├── nuclear-structure/                 ← Nuclear theory
│   ├── index.md                       ← Overview
│   └── 01-shape-factors.md            ← C(Z,W), NMEs, impulse approximation
├── gA-extraction/                     ← gA extraction (new, in development)
│   ├── 01-ssm-algorithm.md            ← SSM step-by-step algorithm
│   ├── 02-ssnme.md                    ← sNME and ESSM formalism
│   ├── 03-tc99-case-study.md          ← 99Tc literature results
│   └── 04-implementation-todo.md      ← Implementation TODO list
└── refs/                              ← Paper summaries
    ├── electromagnetic/               ← CVC, radiative corrections
    ├── forbidden-decay/               ← Forbidden decay studies
    └── (organized by topic)

Calculator Architecture

SpectrumComponent (ABC, base.py)
 ├── PhaseSpace              → 02-phase-space.md
 ├── FermiFunction           → corrections/01-fermi-function.md
 ├── FiniteSizeL0            → corrections/02-finite-size.md
 ├── ChargeDistributionU     → corrections/02-finite-size.md
 ├── ScreeningCorrection     → corrections/03-screening.md
 ├── ExchangeCorrection      → corrections/04-exchange.md
 ├── RadiativeCorrection     → corrections/05-radiative.md
 └── (recoil.py)             → corrections/06-recoil.md (not yet implemented)

BetaSpectrum (spectrum.py) — multiplicative composition + from_config()
BetaSpectrumAnalyzer (spectrum.py) — plotting, CSV export

Correction Implementation Status

# Correction Module Note Status
1 Phase space phase_space.py Baseline ✓ implemented
2 Fermi function fermi.py Coulomb interaction ✓ implemented
3 Finite size finite_size.py L₀, U, DFS ✓ implemented
4 Screening screening.py Atomic screening ✓ implemented
5 Exchange exchange.py Atomic exchange ✓ implemented
6 Radiative radiative.py Outer RC ✓ implemented
7 Recoil recoil.py R_N, Q, weak magnetism ✗ not yet implemented
8 Shape factor shape_factor_gA.py C(Z,W) for forbidden — planned
9 Detector detector_response.py Convolution — planned

gA Extraction (New)

For forbidden nonunique decays (e.g., ^{99}\text{Tc}), the shape factor depends on g_A in a measurable way. See:

Key Variables and Units

  • W — total electron energy in units of m_e c^2 (natural units, m_e = 1)
  • T or E_{\text{kin}} — kinetic energy (keV or MeV)
  • W_0 — endpoint total energy
  • Z_{\text{parent}}, Z_{\text{daughter}} — atomic numbers
  • \alpha \approx 1/137.036 — fine structure constant
  • \gamma = \sqrt{1 - (\alpha Z)^2}

Conversion: W = 1 + T / m_e c^2, with m_e c^2 = 510.998950 keV.

Precision Goal

The calculator aims for accurate to a few parts in 10^{-4} down to 1 keV for low-to-medium Z nuclei, following the approach of Hayen et al. (2017).