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Shape Factor C(W, g_A)

Overview

The g_A-dependent nuclear shape factor C(W, g_A) is the key nuclear structure quantity that encodes the energy-dependent modification of the β decay spectrum due to forbidden nonunique transitions. For ⁹⁹Tc (second-forbidden nonunique, 9/2₁⁺ → 5/2₁⁺, Q ≈ 296 keV), the shape factor decomposes as:

C(W; g_A) = g_V² · C_V(W) + g_A² · C_A(W) + g_V · g_A · C_VA(W)

with g_V = 1.0 fixed by CVC.

Components

Component Description Sign for ⁹⁹Tc Magnitude
C_V(W) Vector contribution + 2.240 × 10⁻⁹ (integrated)
C_A(W) Axial-vector contribution + 2.130 × 10⁻⁹ (integrated)
C_VA(W) Vector-axial interference − −4.361 × 10⁻⁹ (integrated)

Key insight: C_VA is negative and twice as large as C_V or C_A. The total integrated shape factor is two orders of magnitude smaller due to destructive interference.

g_A Dependence

The spectral shape is most sensitive to g_A in the 0–100 keV range (low-energy region). Figure 9 from Paulsen et al. (2024) shows:

  • Small g_A (0.5–1.0): Bell-shaped spectrum with low-energy enhancement
  • Large g_A (1.4–2.0): Flattened spectrum with low-energy suppression
  • Crossover point: All spectra intersect around 100 keV

Table Data Sources

Source Method Coverage Availability
Kostensalo & Suhonen (2017) PRC 96, 024317 MQPM 26 forbidden decays Supplementary material (not public)
Ramalho & Suhonen (2024) NSM (NUSHELLX) ⁹⁹Tc-specific Supplementary material (not public)
Song et al. (2025) arXiv:2506.17544 ESSM + NSM/MQPM ⁹⁹Tc Integrated values only

Implementation

The ShapeFactorGA component should:

  1. Load C_V(W), C_A(W), C_VA(W) tables from CSV files
  2. Interpolate using cubic spline (scipy.interpolate.CubicSpline)
  3. Compute C(W; g_A) = C_V + g_A²·C_A + g_A·C_VA
  4. Return the shape factor for the full spectrum calculation

References