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Using Comparison Evidence ​

This page is a compact guide for technical discussion of NeoMC results.

State The Calculation ​

Always name:

  • source particle, energy/time distribution and normalization;
  • geometry and material state;
  • data library, version and processing assumptions;
  • enabled processes and explicit approximations;
  • observable definition, bins and units;
  • source histories and statistical uncertainty.

State The Reference ​

Classify it as one of:

ReferenceWhat agreement can establish
same-observable experimentbounded physical capability when the full model and uncertainty support it
evaluated tabledata import, interpolation or microscopic response
trusted processornuclear-data processing semantics
another transport codeimplementation diagnosis under matched inputs
analytic resulta limiting case or invariant

Do not label all five as validation.

Present Results ​

For scalar observables, report calculated value, Monte Carlo standard error, reference value, reference uncertainty and residual. For spectra, retain all bins and predeclared coarse summaries; one integrated ratio can hide a shape error.

Keep uncertainty sources separate:

  • Monte Carlo sampling uncertainty;
  • experimental uncertainty;
  • deterministic processing difference;
  • model-to-experiment residual.

Current Discussion Examples ​

  • The Cu K-shell result is a strong example of a microscopic response with incident-energy uncertainty included.
  • The TIARA result shows why a high-energy closed band and a lower-energy unresolved model discrepancy can coexist.
  • The O-16 result shows reaction competition where a channel with zero neutron yield still affects the analog photon collision rate.
  • The light-water result shows a compound observable assembled from bound and free constituents with covariance retained inside each history.

Exact values and source reports are listed in Current evidence status.

NeoMC user documentation.