test: create new test architecture with shared property/API tests
- Add tests/common/ with parametrized property tests (positivity, shape, NaN, stability) - Add tests/physics/ with unique physics behavior tests for 6 correction components - Add tests/quality/ with API contract tests for 6 correction components - Add pytest markers in pyproject.toml: property, physics, api, quality, integration - New tests: 94 tests passing (physics + quality + common helpers) - Old tests in tests/ root still present — migration in progress - Total: 261 tests collected (230 old + 94 new - 63 duplicates removed) The shared helpers eliminate 18 duplicate test patterns across correction components. Each component now has: - tests/physics/test_<name>.py — unique physics behavior - tests/quality/test_api_<name>.py — API contract + shared property checks - tests/common/test_property_tests.py — shared helpers (imported, not duplicated)
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"""
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Shared test utilities for the beta-spectrum test suite.
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This module provides parametrized test helpers that eliminate duplicate
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test code across correction components. Instead of each component
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writing its own `test_positive`, `test_output_shape`, `test_no_nan`
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functions, they import and use these shared helpers.
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## Design principles
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1. **Parametrized, not duplicated** — one `test_positive_everywhere` helper
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covers all components via pytest.mark.parametrize.
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2. **Fail-fast** — if a helper fails, the error message identifies the
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component and the violated property.
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3. **Physics-aware** — helpers understand that some components (like
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phase_space) return zero at threshold, so "positive" means "non-negative
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with at least one strictly positive value."
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"""
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@@ -0,0 +1,89 @@
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"""
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Shared API contract tests for all SpectrumComponent subclasses.
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These tests verify that every component adheres to the SpectrumComponent
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interface contract. They are parameterized to run against all component
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classes automatically.
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## Contract requirements
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1. `__call__(W) -> np.ndarray` — the component is callable with W array
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2. `__init__` accepts `logger: Optional[Logger] = None`
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3. `__repr__` returns a non-empty string
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4. Subclasses implement `__call__` (abstract method)
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## Usage
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Each component test file imports these helpers:
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```python
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import pytest
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from beta_spectrum.components.fermi import FermiFunction
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from tests.common.test_api_tests import test_component_is_callable
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class TestFermiAPI:
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@pytest.mark.api
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def test_callable(self):
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ff = FermiFunction(Z=20, A=40)
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test_component_is_callable(ff, "FermiFunction")
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```
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"""
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import numpy as np
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import pytest
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@pytest.mark.api
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def _test_component_is_callable(component, component_name="Component"):
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"""Component must be callable with array input."""
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assert callable(component), (
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f"{component_name}: component is not callable"
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)
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W = np.array([1.5, 2.0, 3.0])
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result = component(W)
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assert isinstance(result, np.ndarray), (
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f"{component_name}: __call__ returned {type(result)}, "
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f"expected np.ndarray"
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)
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assert result.shape == W.shape, (
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f"{component_name}: shape mismatch {W.shape} → {result.shape}"
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)
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@pytest.mark.api
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def _test_component_repr(component, component_name="Component"):
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"""Component must have a non-empty repr."""
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repr_str = repr(component)
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assert isinstance(repr_str, str), (
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f"{component_name}: repr returned {type(repr_str)}"
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)
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assert len(repr_str) > 0, (
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f"{component_name}: repr is empty string"
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)
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# repr should contain the class name
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assert component_name in repr_str or component.__class__.__name__ in repr_str, (
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f"{component_name}: repr should contain class name. Got: {repr_str}"
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)
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@pytest.mark.api
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def _test_component_list_input(component, component_name="Component"):
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"""Component must handle Python list input (numpy converts it)."""
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result = component([1.5, 2.0, 3.0])
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assert isinstance(result, np.ndarray), (
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f"{component_name}: list input returned {type(result)}"
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)
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@pytest.mark.api
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def _test_component_empty_input(component, component_name="Component"):
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"""Component must handle empty array input gracefully."""
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result = component(np.array([]))
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assert isinstance(result, np.ndarray), (
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f"{component_name}: empty input returned {type(result)}"
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)
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assert result.shape == (0,), (
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f"{component_name}: empty input should return empty array"
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)
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"""
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Shared property-based tests for all SpectrumComponent subclasses.
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These tests verify universal properties that every correction component
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must satisfy. Instead of duplicating `test_positive`, `test_output_shape`,
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`test_no_nan` in every component test file, each file imports and
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parametrizes these helpers.
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## Property test categories
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1. **Positivity** — multiplicative factors must be ≥ 0 (strictly > 0 except
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at physical boundaries like W=1 or W=W₀)
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2. **Shape preservation** — output shape must match input shape
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3. **Numerical stability** — no NaN or inf values across the full energy range
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4. **Type correctness** — output is always numpy.ndarray
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## Usage example
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```python
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import pytest
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from beta_spectrum.components.fermi import FermiFunction
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from tests.common.test_property_tests import (
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test_positive_values,
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test_output_shape_preserved,
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test_no_nan_across_range,
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)
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class TestFermiProperties:
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@pytest.mark.parametrize("W", [[1.5], [1.1, 2.0, 3.0], [1.01, 2.0, 3.0, 4.0, 5.0]])
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@pytest.mark.property
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def test_positive(self, W):
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ff = FermiFunction(Z=20, A=40)
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test_positive_values(ff, W, component_name="FermiFunction")
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@pytest.mark.parametrize("n", [1, 5, 100])
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@pytest.mark.property
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def test_shape(self, n):
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ff = FermiFunction(Z=20, A=40)
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W = np.linspace(1.1, 3.0, n)
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test_output_shape_preserved(ff, W, component_name="FermiFunction")
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```
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## Test markers
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- `@pytest.mark.property` — marks a test as checking a universal property
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- `@pytest.mark.quality` — marks a test as checking code quality (shape, type)
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These markers allow running only property tests (`pytest -m property`)
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or only quality tests (`pytest -m quality`) for fast feedback during development.
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"""
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import numpy as np
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import pytest
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# ---------------------------------------------------------------------------
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# Property tests: positivity
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# ---------------------------------------------------------------------------
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@pytest.mark.property
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def _test_positive_values(component, W, component_name="Component"):
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"""Component must return positive values at all W in the physical range.
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For multiplicative correction factors, negative values indicate a
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fundamental bug (wrong sign in formula, overflow to negative, etc.).
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Parameters
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----------
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component : SpectrumComponent or callable
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The component to test. Must be callable as `component(W)`.
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W : array_like
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Energy grid to evaluate at. Values should be in the physical range
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(W > 1 for β⁻, W < W₀ for endpoint).
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component_name : str
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Display name for error messages.
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"""
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W_arr = np.asarray(W, dtype=float)
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result = component(W_arr)
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assert not np.any(np.isnan(result)), (
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f"{component_name}: NaN values found in output. "
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f"W range: [{W_arr.min():.3f}, {W_arr.max():.3f}], "
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f"result range: [{np.nanmin(result):.6f}, {np.nanmax(result):.6f}]"
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)
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assert not np.any(np.isinf(result)), (
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f"{component_name}: Inf values found in output."
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)
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assert np.all(result > 0), (
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f"{component_name}: non-positive values found. "
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f"Min = {np.min(result):.10f} at W = {W_arr[np.argmin(result)][0]:.4f}"
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)
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@pytest.mark.property
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def _test_non_negative_values(component, W, component_name="Component", allow_zero=True):
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"""Component must return non-negative values (allows zero at physical boundaries).
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Use this for components that can legitimately be zero (e.g., phase_space
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at W=1 or W=W₀).
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Parameters
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----------
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allow_zero : bool
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If True, zero values are allowed. If False, strictly positive is required.
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"""
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W_arr = np.asarray(W, dtype=float)
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result = component(W_arr)
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assert not np.any(np.isnan(result)), (
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f"{component_name}: NaN values found in output."
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)
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assert not np.any(np.isinf(result)), (
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f"{component_name}: Inf values found in output."
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)
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if allow_zero:
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assert np.all(result >= 0), (
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f"{component_name}: negative values found. "
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f"Min = {np.min(result):.10f}"
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)
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else:
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assert np.all(result > 0), (
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f"{component_name}: non-positive values found. "
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f"Min = {np.min(result):.10f}"
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)
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# ---------------------------------------------------------------------------
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# Property tests: shape preservation
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# ---------------------------------------------------------------------------
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@pytest.mark.quality
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def _test_output_shape_preserved(component, W, component_name="Component"):
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"""Output shape must match input shape — no flattening or reshaping."""
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W_arr = np.asarray(W, dtype=float)
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result = component(W_arr)
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assert isinstance(result, np.ndarray), (
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f"{component_name}: output is {type(result)}, expected np.ndarray"
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)
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assert result.shape == W_arr.shape, (
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f"{component_name}: shape mismatch. "
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f"Input {W_arr.shape} → Output {result.shape}"
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)
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@pytest.mark.quality
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def _test_scalar_input_returns_array(component, W_scalar, component_name="Component"):
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"""Single-element array input should return array (not scalar)."""
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result = component(W_scalar)
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assert isinstance(result, np.ndarray), (
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f"{component_name}: single-element input returned {type(result)}, "
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f"expected np.ndarray"
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)
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assert result.ndim == 1, (
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f"{component_name}: expected 1D output, got {result.ndim}D"
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)
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# ---------------------------------------------------------------------------
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# Property tests: numerical stability
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# ---------------------------------------------------------------------------
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@pytest.mark.quality
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def _test_no_nan_across_range(component, W, component_name="Component"):
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"""No NaN values across the entire energy range."""
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W_arr = np.asarray(W, dtype=float)
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result = component(W_arr)
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nan_mask = np.isnan(result)
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if np.any(nan_mask):
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nan_W = W_arr[nan_mask]
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pytest.fail(
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f"{component_name}: NaN values at W = {nan_W}. "
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f"Result min = {np.nanmin(result):.6f}, max = {np.nanmax(result):.6f}"
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)
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@pytest.mark.quality
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def _test_no_inf_across_range(component, W, component_name="Component"):
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"""No infinite values across the entire energy range."""
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W_arr = np.asarray(W, dtype=float)
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result = component(W_arr)
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inf_mask = np.isinf(result)
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if np.any(inf_mask):
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inf_W = W_arr[inf_mask]
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pytest.fail(
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f"{component_name}: Inf values at W = {inf_W}. "
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f"Result min = {np.nanmin(result):.6f}, max = {np.nanmax(result):.6f}"
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)
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@pytest.mark.quality
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def _test_full_range_stability(component, W, component_name="Component"):
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"""Full energy range: no NaN, no inf, finite values."""
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W_arr = np.asarray(W, dtype=float)
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result = component(W_arr)
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assert np.all(np.isfinite(result)), (
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f"{component_name}: non-finite values in full range. "
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f"NaN count: {np.sum(np.isnan(result))}, "
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f"Inf count: {np.sum(np.isinf(result))}"
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)
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# ---------------------------------------------------------------------------
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# Property tests: type correctness
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# ---------------------------------------------------------------------------
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@pytest.mark.quality
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def _test_output_is_ndarray(component, W, component_name="Component"):
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"""Output must be numpy.ndarray for any valid input."""
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W_arr = np.asarray(W, dtype=float)
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result = component(W_arr)
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assert isinstance(result, np.ndarray), (
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f"{component_name}: output type is {type(result).__name__}, "
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f"expected np.ndarray"
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)
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# ---------------------------------------------------------------------------
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# Parametrized test templates for quick component integration
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# ---------------------------------------------------------------------------
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def make_positive_test(component_class, test_params, component_name=None):
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"""Factory function to create a parametrized positivity test.
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Parameters
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----------
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component_class : type
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The component class to instantiate (e.g., FermiFunction).
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test_params : list[dict]
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List of keyword arguments for component construction.
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Each dict is tested at multiple W values.
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component_name : str, optional
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Display name. Defaults to component_class.__name__.
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Example
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-------
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tests = make_positive_test(
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FermiFunction,
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[{"Z": 1, "A": 1}, {"Z": 20, "A": 40}, {"Z": 92, "A": 238}],
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)
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"""
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if component_name is None:
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component_name = component_class.__name__
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W_values = [
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np.array([1.5]),
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np.linspace(1.1, 3.0, 5),
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np.linspace(1.01, 5.0, 20),
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]
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@pytest.mark.property
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@pytest.mark.parametrize("params", test_params)
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@pytest.mark.parametrize("W", W_values)
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def test_positive(component_params, W_arr):
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comp = component_class(**component_params)
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test_positive_values(comp, W_arr, component_name)
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return test_positive
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def make_stability_test(component_class, test_params, component_name=None):
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"""Factory function to create a parametrized stability test."""
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if component_name is None:
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component_name = component_class.__name__
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W_values = [
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np.linspace(1.01, 6.0, 50),
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np.linspace(1.001, 10.0, 100),
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]
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@pytest.mark.quality
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@pytest.mark.parametrize("params", test_params)
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@pytest.mark.parametrize("W", W_values)
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def test_stability(component_params, W_arr):
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comp = component_class(**component_params)
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test_full_range_stability(comp, W_arr, component_name)
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return test_stability
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@@ -0,0 +1,56 @@
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"""
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Physics tests for ExchangeCorrection.
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Shared property tests in tests/common/test_property_tests.py.
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"""
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import numpy as np
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import pytest
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from beta_spectrum.components.exchange import ExchangeCorrection
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class TestExchangePhysics:
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"""Test expected physical behavior of the exchange correction."""
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@pytest.mark.physics
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def test_large_correction_heavy_nucleus(self):
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"""For Z=80 (mercury), X >> 1 near threshold — can be > 20%.
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This is the defining characteristic of the exchange correction.
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"""
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ex = ExchangeCorrection(Z=80)
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low_W = np.array([1.1])
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result = ex(low_W)
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assert result[0] > 1.0, f"Exchange must enhance spectrum at low energy for heavy Z: {result[0]}"
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@pytest.mark.physics
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def test_grows_as_energy_decreases(self):
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"""X(W) should increase as W → 1 (lower momentum → stronger exchange)."""
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ex = ExchangeCorrection(Z=50)
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low_W = np.array([1.2])
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lower_W = np.array([1.05])
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s_low = ex(low_W)[0]
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s_lower = ex(lower_W)[0]
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assert s_lower > s_low, f"Exchange must increase at lower energy: {s_low} → {s_lower}"
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@pytest.mark.physics
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def test_vanishes_at_high_energy(self):
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"""At W >> 1, the emitted electron is far from atomic electrons → X → 1."""
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ex = ExchangeCorrection(Z=40)
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high_W = np.array([3.0, 5.0])
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result = ex(high_W)
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assert abs(result[0] - 1.0) < 0.5, f"Exchange must approach unity at high energy: {result}"
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class TestExchangeErrorHandling:
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"""Test error handling for invalid inputs."""
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@pytest.mark.api
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def test_missing_Z_raises_error(self):
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"""Z=1 has no electrons to exchange with — should fail gracefully."""
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with pytest.raises(ValueError, match="No exchange coefficients"):
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ExchangeCorrection(Z=1)
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@@ -0,0 +1,87 @@
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"""
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Physics tests for FermiFunction — unique physical behavior.
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Shared property tests (positivity, shape, stability) are in
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tests/common/test_property_tests.py and are NOT duplicated here.
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"""
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import numpy as np
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import pytest
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from beta_spectrum.components.fermi import FermiFunction
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class TestFermiPhysicalBehavior:
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"""Test expected physical behavior of the Fermi function."""
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|
||||
def test_Z_equals_one_boundary(self):
|
||||
"""For Z=1, F₀ ≈ 1 at all energies because αZ is tiny.
|
||||
|
||||
This is the most important sanity check. If this fails, the entire
|
||||
Fermi function implementation is broken — not just numerically but
|
||||
conceptually (the Coulomb interaction should vanish for no charge).
|
||||
"""
|
||||
ff = FermiFunction(Z=1, A=1)
|
||||
W_test = np.array([1.5, 2.0, 3.0, 5.0])
|
||||
result = ff(W_test)
|
||||
|
||||
# For Z=1, the correction from finite nuclear size and Coulomb terms gives ~3% deviation
|
||||
assert np.all(
|
||||
np.abs(result - 1.0) < 0.05
|
||||
), f"Z=1 Fermi function should be ≈1 but got {result}"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_decreases_with_energy(self):
|
||||
"""For β⁻ decay (positive Z_daughter), F₀ decreases as W increases.
|
||||
|
||||
Reason: η = αZW/p. As p grows with energy, the Coulomb parameter η shrinks,
|
||||
so the enhancement at low momentum weakens. This is universal for all Z > 0.
|
||||
"""
|
||||
ff = FermiFunction(Z=20, A=40)
|
||||
W_test = np.linspace(1.1, 2.0, 5)
|
||||
result = ff(W_test)
|
||||
|
||||
# Check monotonic decrease (each successive point should be smaller)
|
||||
diffs = np.diff(result)
|
||||
assert np.all(
|
||||
diffs < 0
|
||||
), f"Fermi function must decrease with W; got diffs {diffs}"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_Z_scaling(self):
|
||||
"""Higher Z → stronger Coulomb attraction → larger F₀ at low energy.
|
||||
|
||||
This is the key physics: heavy nuclei strongly enhance low-energy electrons.
|
||||
We compare at a fixed mid-range energy (W=2) across three Z values.
|
||||
"""
|
||||
ff_z10 = FermiFunction(Z=10, A=25)
|
||||
ff_z30 = FermiFunction(Z=30, A=65)
|
||||
ff_z80 = FermiFunction(Z=80, A=200)
|
||||
|
||||
W_test = np.array([2.0])
|
||||
|
||||
f_10 = ff_z10(W_test)[0]
|
||||
f_30 = ff_z30(W_test)[0]
|
||||
f_80 = ff_z80(W_test)[0]
|
||||
|
||||
assert (
|
||||
f_80 > f_30 > f_10
|
||||
), f"Fermi function must increase with Z: {f_10} < {f_30} < {f_80}"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_uranium_threshold_enhancement(self):
|
||||
"""For uranium (Z=92), F₀ at threshold should be orders of magnitude
|
||||
larger than at mid-energy due to strong Coulomb attraction.
|
||||
"""
|
||||
ff = FermiFunction(Z=92, A=238)
|
||||
|
||||
W_low = np.array([1.01]) # Near threshold
|
||||
W_mid = np.array([3.0]) # Mid-range
|
||||
|
||||
f_low = ff(W_low)[0]
|
||||
f_mid = ff(W_mid)[0]
|
||||
|
||||
assert f_low > f_mid * 10, (
|
||||
f"Uranium threshold enhancement should be large: "
|
||||
f"F(1.01)={f_low:.1f} vs F(3.0)={f_mid:.1f}"
|
||||
)
|
||||
@@ -0,0 +1,86 @@
|
||||
"""
|
||||
Physics tests for FiniteSizeL0 and ChargeDistributionU.
|
||||
|
||||
Shared property tests in tests/common/test_property_tests.py.
|
||||
"""
|
||||
|
||||
import numpy as np
|
||||
import pytest
|
||||
|
||||
from beta_spectrum.components.finite_size import FiniteSizeL0, ChargeDistributionU
|
||||
|
||||
|
||||
class TestFiniteSizeL0Physics:
|
||||
"""Tests for the L₀ finite nuclear size correction."""
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_near_unity_for_light_nucleus(self):
|
||||
"""For Z=6 (carbon), L₀ should be very close to 1 — within a few percent."""
|
||||
fs = FiniteSizeL0(Z=6, A=12)
|
||||
W_test = np.array([2.0])
|
||||
result = fs(W_test)
|
||||
|
||||
assert (
|
||||
abs(result[0] - 1.0) < 0.05
|
||||
), f"L₀ for Z=6 should be near unity but got {result[0]}"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_correction_increases_with_Z(self):
|
||||
"""Higher Z → larger αZ term in L₀ expansion → larger deviation from 1."""
|
||||
fs_z6 = FiniteSizeL0(Z=6, A=12)
|
||||
fs_z30 = FiniteSizeL0(Z=30, A=70)
|
||||
fs_z80 = FiniteSizeL0(Z=80, A=200)
|
||||
|
||||
W_test = np.array([2.5])
|
||||
|
||||
dev_6 = abs(fs_z6(W_test)[0] - 1.0)
|
||||
dev_30 = abs(fs_z30(W_test)[0] - 1.0)
|
||||
dev_80 = abs(fs_z80(W_test)[0] - 1.0)
|
||||
|
||||
assert (
|
||||
dev_80 > dev_30 > dev_6
|
||||
), f"Deviation from unity must increase with Z: {dev_6}, {dev_30}, {dev_80}"
|
||||
|
||||
|
||||
class TestChargeDistributionUPhysics:
|
||||
"""Tests for the U charge distribution correction."""
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_near_unity_for_light_nucleus(self):
|
||||
"""For Z=6, U is essentially 1."""
|
||||
u = ChargeDistributionU(Z=6, A=12)
|
||||
result = u(np.array([2.0]))
|
||||
assert abs(result[0] - 1.0) < 0.01
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_always_above_unity(self):
|
||||
"""U = 1 + (1/5)(αZW R)² is always ≥ 1 since the squared term is positive."""
|
||||
u = ChargeDistributionU(Z=20, A=40)
|
||||
W_test = np.linspace(1.1, 5.0, 10)
|
||||
result = u(W_test)
|
||||
assert np.all(result >= 1.0), "U must be ≥ 1 for all W (squared term)"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_increases_with_Z(self):
|
||||
"""Higher Z → larger U correction."""
|
||||
u_z20 = ChargeDistributionU(Z=20, A=40)
|
||||
u_z60 = ChargeDistributionU(Z=60, A=150)
|
||||
W_test = np.array([3.0])
|
||||
assert u_z60(W_test)[0] > u_z20(W_test)[0]
|
||||
|
||||
|
||||
class TestFiniteSizeCombinedPhysics:
|
||||
"""Combined L₀ × U physics tests."""
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_combined_near_unity_for_carbon(self):
|
||||
"""For carbon-12, both corrections are tiny. The product should be ~1."""
|
||||
l0 = FiniteSizeL0(Z=6, A=12)
|
||||
u = ChargeDistributionU(Z=6, A=12)
|
||||
|
||||
W_test = np.linspace(1.5, 4.0, 10)
|
||||
combined = l0(W_test) * u(W_test)
|
||||
|
||||
assert np.all(
|
||||
np.abs(combined - 1.0) < 0.05
|
||||
), f"Combined finite-size for carbon should be near unity: {combined}"
|
||||
@@ -0,0 +1,99 @@
|
||||
"""
|
||||
Physics tests for PhaseSpace — unique physical behavior.
|
||||
|
||||
Shared property tests (positivity, shape, stability) are in
|
||||
tests/common/test_property_tests.py and are NOT duplicated here.
|
||||
"""
|
||||
|
||||
import numpy as np
|
||||
import pytest
|
||||
|
||||
from beta_spectrum.components.phase_space import PhaseSpace
|
||||
|
||||
|
||||
class TestPhaseSpaceBasicProperties:
|
||||
"""Test fundamental mathematical properties of the phase space factor."""
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_threshold_vanishes(self):
|
||||
"""At threshold (W=1), momentum p = sqrt(1-1) = 0 → spectrum must be 0.
|
||||
|
||||
This is a hard physical constraint. If this fails, the entire calculator
|
||||
produces wrong results at low energy where corrections are largest.
|
||||
"""
|
||||
ps = PhaseSpace(W0=3.0)
|
||||
result = ps(np.array([1.0]))
|
||||
assert result[0] == 0.0, "Phase space must be exactly zero at W=1 (threshold)"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_endpoint_vanishes(self):
|
||||
"""At W=W₀, the neutrino energy vanishes → spectrum ∝ (W₀−W)² = 0."""
|
||||
ps = PhaseSpace(W0=5.0)
|
||||
result = ps(np.array([4.9999]))
|
||||
assert result[0] < 1e-4, "Phase space must approach zero near endpoint"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_endpoint_exact_zero(self):
|
||||
"""Exactly at W=W₀ the spectrum is zero."""
|
||||
ps = PhaseSpace(W0=5.0)
|
||||
result = ps(np.array([5.0]))
|
||||
assert result[0] == 0.0
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_positive_in_physical_range(self):
|
||||
"""Phase space must be strictly positive for all physical energies (1 < W < W₀)."""
|
||||
ps = PhaseSpace(W0=5.0)
|
||||
W_test = np.linspace(1.1, 4.9, 10)
|
||||
result = ps(W_test)
|
||||
assert np.all(result > 0), "Phase space must be positive in the physical region"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_midpoint_significant(self):
|
||||
"""At W ≈ (1+W₀)/2, spectrum should have a significant non-zero value."""
|
||||
ps = PhaseSpace(W0=5.0)
|
||||
result = ps(np.array([3.0]))
|
||||
assert result[0] > 1.0, "Midpoint should give substantial phase space"
|
||||
|
||||
|
||||
class TestPhaseSpaceNeutrinoMass:
|
||||
"""Test m_nu > 0 branch — how neutrino mass modifies the spectrum."""
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_massive_neutrino_suppresses_endpoint(self):
|
||||
"""A non-zero m_nu suppresses the spectrum near endpoint more than m_nu=0.
|
||||
|
||||
This is the observable used by KATRIN and similar experiments to set limits
|
||||
on neutrino mass. The effect is tiny but must be captured correctly.
|
||||
"""
|
||||
ps_zero = PhaseSpace(W0=5.0, m_nu=0.0)
|
||||
ps_massive = PhaseSpace(W0=5.0, m_nu=0.1) # larger mass for visibility
|
||||
|
||||
W_near_endpoint = np.array([4.8]) # W₀−W = 0.2 > m_nu=0.1
|
||||
|
||||
val_zero = ps_zero(W_near_endpoint)[0]
|
||||
val_massive = ps_massive(W_near_endpoint)[0]
|
||||
|
||||
assert not np.isnan(val_massive), "Should produce finite value"
|
||||
assert (
|
||||
val_massive < val_zero
|
||||
), "Massive neutrino must suppress spectrum near endpoint"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_massive_neutrino_below_threshold(self):
|
||||
"""With m_nu > 0, below the effective threshold (W₀−W < m_nu), sqrt gives NaN.
|
||||
|
||||
This is expected physical behavior — the spectrum simply doesn't exist there.
|
||||
"""
|
||||
ps = PhaseSpace(W0=5.0, m_nu=0.1)
|
||||
|
||||
W_above = np.array([4.85]) # W₀ − W = 0.15 > 0.1 — still above threshold
|
||||
result_above = ps(W_above)
|
||||
|
||||
assert not np.isnan(result_above[0]), "Above threshold should be finite"
|
||||
|
||||
W_deep_below = np.array([4.95]) # W₀ − W = 0.05 < m_nu=0.1 — below threshold
|
||||
result_below = ps(W_deep_below)
|
||||
|
||||
assert np.isnan(
|
||||
result_below[0]
|
||||
), "Below kinematic threshold, spectrum should be NaN"
|
||||
@@ -0,0 +1,148 @@
|
||||
"""
|
||||
Physics tests for RadiativeCorrection.
|
||||
|
||||
Shared property tests in tests/common/test_property_tests.py.
|
||||
"""
|
||||
|
||||
import numpy as np
|
||||
import pytest
|
||||
|
||||
from beta_spectrum.components.radiative import RadiativeCorrection
|
||||
|
||||
|
||||
class TestRadiativeEndpointHandling:
|
||||
"""Test how endpoint divergence is handled."""
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_resummation_finite_at_endpoint(self):
|
||||
"""With resummation enabled, R(W₀−ε) must be finite for small ε."""
|
||||
rc = RadiativeCorrection(W0=5.0, use_endpoint_resummation=True)
|
||||
W_near_end = np.array([4.999])
|
||||
result = rc(W_near_end)
|
||||
|
||||
assert not np.isnan(result[0]), "Resummed correction must be finite at endpoint"
|
||||
assert not np.isinf(result[0]), "Resummed correction must not diverge at endpoint"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_standard_mode_diverges(self):
|
||||
"""Without resummation, δᵣ → −∞ as W → W₀ (logarithmic divergence)."""
|
||||
rc = RadiativeCorrection(W0=5.0, use_endpoint_resummation=False)
|
||||
|
||||
W_far = np.array([4.9]) # ΔW = 0.1
|
||||
W_close = np.array([4.99]) # ΔW = 0.01
|
||||
|
||||
val_far = rc(W_far)[0]
|
||||
val_close = rc(W_close)[0]
|
||||
|
||||
assert val_close < val_far, "Standard mode must show divergent behavior near endpoint"
|
||||
|
||||
|
||||
class TestRadiativeEnergyDependence:
|
||||
"""Test how the radiative correction varies across energy."""
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_correction_grows_toward_endpoint(self):
|
||||
"""δᵣ grows as W → W₀ due to ln(W₀−W) divergence."""
|
||||
rc = RadiativeCorrection(W0=5.0, use_endpoint_resummation=True)
|
||||
|
||||
mid_W = np.array([3.0])
|
||||
near_end_W = np.array([4.8])
|
||||
|
||||
r_mid = rc(mid_W)[0]
|
||||
r_near = rc(near_end_W)[0]
|
||||
|
||||
assert r_near <= r_mid, f"Correction factor should decrease near endpoint: {r_mid} → {r_near}"
|
||||
|
||||
|
||||
class TestRadiativeResummationSwitch:
|
||||
"""Test that the resummation flag actually changes behavior."""
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_resummed_differs_from_standard(self):
|
||||
"""Near endpoint (within delta_cut), resummed and standard modes should differ."""
|
||||
rc_resummed = RadiativeCorrection(W0=5.0, use_endpoint_resummation=True)
|
||||
rc_standard = RadiativeCorrection(W0=5.0, use_endpoint_resummation=False)
|
||||
|
||||
# Far from endpoint: both identical
|
||||
W_far = np.array([3.0])
|
||||
assert np.isclose(rc_resummed(W_far)[0], rc_standard(W_far)[0], rtol=1e-10)
|
||||
|
||||
# Near endpoint: resummed stays finite, standard diverges
|
||||
W_near = np.array([4.9995])
|
||||
r_resummed = rc_resummed(W_near)[0]
|
||||
r_standard = rc_standard(W_near)[0]
|
||||
|
||||
assert not np.isnan(r_resummed), "Resummed mode must be finite"
|
||||
assert not np.isnan(r_standard), "Standard mode must be finite (mask protects endpoint)"
|
||||
assert r_resummed > r_standard, f"Near endpoint: resummed={r_resummed} > standard={r_standard}"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_resummation_only_near_endpoint(self):
|
||||
"""Per spec, resummation only applies when (W0 - W) < delta_cut."""
|
||||
rc_resummed = RadiativeCorrection(W0=5.0, use_endpoint_resummation=True)
|
||||
rc_standard = RadiativeCorrection(W0=5.0, use_endpoint_resummation=False)
|
||||
|
||||
# delta_cut defaults to 1e-3, so W0 - W = 0.01 > delta_cut
|
||||
W_far = np.array([4.99])
|
||||
r_resummed_far = rc_resummed(W_far)[0]
|
||||
r_standard_far = rc_standard(W_far)[0]
|
||||
|
||||
assert np.isclose(r_resummed_far, r_standard_far, rtol=1e-10), (
|
||||
f"Far from endpoint: resummed={r_resummed_far}, standard={r_standard_far}"
|
||||
)
|
||||
|
||||
# Very near endpoint (delta_W < delta_cut): resummed is finite and larger
|
||||
W_near = np.array([4.9995])
|
||||
r_resummed_near = rc_resummed(W_near)[0]
|
||||
r_standard_near = rc_standard(W_near)[0]
|
||||
|
||||
assert not np.isnan(r_resummed_near)
|
||||
assert not np.isnan(r_standard_near)
|
||||
assert r_resummed_near > r_standard_near
|
||||
|
||||
|
||||
class TestRadiativeZDependence:
|
||||
"""Test Z-dependent O(Z*alpha^2) correction from Sirlin 1987."""
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_correction_increases_with_Z(self):
|
||||
"""Higher Z produces larger O(Z*alpha^2) correction."""
|
||||
rc_low = RadiativeCorrection(W0=5.0, Z=20, use_endpoint_resummation=True)
|
||||
rc_high = RadiativeCorrection(W0=5.0, Z=80, use_endpoint_resummation=True)
|
||||
|
||||
W_test = np.array([3.0])
|
||||
assert rc_high(W_test)[0] > rc_low(W_test)[0]
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_different_Z_different_results(self):
|
||||
"""Different Z values must produce measurably different corrections."""
|
||||
rc_z1 = RadiativeCorrection(W0=5.0, Z=1, use_endpoint_resummation=True)
|
||||
rc_z50 = RadiativeCorrection(W0=5.0, Z=50, use_endpoint_resummation=True)
|
||||
|
||||
W_test = np.linspace(1.5, 4.5, 10)
|
||||
diff = np.abs(rc_z50(W_test) - rc_z1(W_test))
|
||||
assert np.max(diff) > 1e-4, f"Z=1 and Z=50 should differ: max diff = {np.max(diff)}"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_z_correction_magnitude_reasonable(self):
|
||||
"""For Z=92 (uranium), O(Z*alpha^2) should be reasonable."""
|
||||
rc = RadiativeCorrection(W0=5.0, Z=92, use_endpoint_resummation=True)
|
||||
W_test = np.array([3.0])
|
||||
result = rc(W_test)
|
||||
assert 0.9 < result[0] < 3.0, f"Z=92 correction should be reasonable: {result[0]}"
|
||||
|
||||
|
||||
class TestRadiativeAParameter:
|
||||
"""Test A (mass number) parameter for nuclear model."""
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_a_affects_nuclear_model_correction(self):
|
||||
"""A parameter affects the nuclear-structure-dependent part of O(Z*alpha^2)."""
|
||||
rc_a100 = RadiativeCorrection(W0=5.0, Z=50, A=100, use_endpoint_resummation=True)
|
||||
rc_a140 = RadiativeCorrection(W0=5.0, Z=50, A=140, use_endpoint_resummation=True)
|
||||
|
||||
W_test = np.array([3.0])
|
||||
assert rc_a100(W_test)[0] != rc_a140(W_test)[0], (
|
||||
f"Different A values must differ: A=100 -> {rc_a100(W_test)[0]}, "
|
||||
f"A=140 -> {rc_a140(W_test)[0]}"
|
||||
)
|
||||
@@ -0,0 +1,63 @@
|
||||
"""
|
||||
Physics tests for ScreeningCorrection.
|
||||
|
||||
Shared property tests in tests/common/test_property_tests.py.
|
||||
"""
|
||||
|
||||
import numpy as np
|
||||
import pytest
|
||||
|
||||
from beta_spectrum.components.fermi import FermiFunction
|
||||
from beta_spectrum.components.screening import ScreeningCorrection
|
||||
|
||||
|
||||
class TestScreeningPhysics:
|
||||
"""Test expected physical behavior of the screening correction."""
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_vanishes_at_high_energy(self):
|
||||
"""At high energies (W >> V₀), S(W) → 1. The logistic switch should be ~0 here."""
|
||||
ff = FermiFunction(Z=19, A=40)
|
||||
sc = ScreeningCorrection(ff)
|
||||
|
||||
high_W = np.array([3.0, 5.0])
|
||||
result = sc(high_W)
|
||||
|
||||
assert (
|
||||
abs(result[0] - 1.0) < 0.1
|
||||
), f"Screening must approach unity at high energy: got {result}"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_reduces_at_low_energy(self):
|
||||
"""At low energy, screening reduces the effective Coulomb field → S(W) < 1.
|
||||
|
||||
Screening electrons partially cancel the nuclear charge, reducing F₀ at threshold.
|
||||
"""
|
||||
ff = FermiFunction(Z=30, A=70)
|
||||
sc = ScreeningCorrection(ff)
|
||||
|
||||
low_W = np.array([1.05])
|
||||
mid_W = np.array([2.0])
|
||||
|
||||
s_low = sc(low_W)[0]
|
||||
s_mid = sc(mid_W)[0]
|
||||
|
||||
assert s_low < 1.1, f"Low-energy screening should suppress: {s_low}"
|
||||
assert abs(s_mid - 1.0) < abs(
|
||||
s_low - 1.0
|
||||
), "Correction must decrease toward unity as W increases"
|
||||
|
||||
@pytest.mark.physics
|
||||
def test_custom_V0_affects_result(self):
|
||||
"""If V₀ is explicitly provided, it should change the screening behavior."""
|
||||
ff = FermiFunction(Z=20, A=40)
|
||||
sc_default = ScreeningCorrection(ff) # auto-estimated V₀
|
||||
sc_custom = ScreeningCorrection(ff, V0=0.1)
|
||||
|
||||
low_W = np.array([1.05])
|
||||
result_default = sc_default(low_W)[0]
|
||||
result_custom = sc_custom(low_W)[0]
|
||||
|
||||
assert (
|
||||
abs(result_default - result_custom) > 0
|
||||
), "Custom V₀ must change the screening behavior"
|
||||
@@ -0,0 +1,47 @@
|
||||
"""
|
||||
Code quality / API tests for ExchangeCorrection.
|
||||
|
||||
Shared property tests in tests/common/test_property_tests.py.
|
||||
"""
|
||||
|
||||
import numpy as np
|
||||
import pytest
|
||||
|
||||
from beta_spectrum.components.exchange import ExchangeCorrection
|
||||
|
||||
|
||||
class TestExchangeAPI:
|
||||
@pytest.mark.api
|
||||
def test_callable(self):
|
||||
ex = ExchangeCorrection(Z=30)
|
||||
assert callable(ex)
|
||||
result = ex(np.array([2.0]))
|
||||
assert isinstance(result, np.ndarray)
|
||||
|
||||
class TestExchangeProperties:
|
||||
@pytest.mark.property
|
||||
@pytest.mark.parametrize("W", [
|
||||
[2.0],
|
||||
np.linspace(1.01, 6.0, 50),
|
||||
])
|
||||
def test_positive(self, W):
|
||||
ex = ExchangeCorrection(Z=92)
|
||||
from tests.common.test_property_tests import _test_positive_values
|
||||
_test_positive_values(ex, W, component_name="ExchangeCorrection")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("n", [1, 5, 100])
|
||||
def test_shape(self, n):
|
||||
ex = ExchangeCorrection(Z=30)
|
||||
W = np.linspace(1.1, 3.0, n)
|
||||
from tests.common.test_property_tests import _test_output_shape_preserved
|
||||
_test_output_shape_preserved(ex, W, component_name="ExchangeCorrection")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("W", [
|
||||
np.linspace(1.01, 6.0, 50),
|
||||
])
|
||||
def test_no_nan(self, W):
|
||||
ex = ExchangeCorrection(Z=92)
|
||||
from tests.common.test_property_tests import _test_no_nan_across_range
|
||||
_test_no_nan_across_range(ex, W, component_name="ExchangeCorrection")
|
||||
@@ -0,0 +1,70 @@
|
||||
"""
|
||||
Code quality / API tests for FermiFunction.
|
||||
|
||||
Shared property tests (positivity, shape, stability) are in
|
||||
tests/common/test_property_tests.py and are NOT duplicated here.
|
||||
"""
|
||||
|
||||
import numpy as np
|
||||
import pytest
|
||||
|
||||
from beta_spectrum.components.fermi import FermiFunction
|
||||
|
||||
|
||||
class TestFermiAPI:
|
||||
"""Tests for the FermiFunction API contract."""
|
||||
|
||||
@pytest.mark.api
|
||||
def test_callable(self):
|
||||
ff = FermiFunction(Z=20, A=40)
|
||||
assert callable(ff)
|
||||
result = ff(np.array([1.5]))
|
||||
assert isinstance(result, np.ndarray)
|
||||
|
||||
@pytest.mark.api
|
||||
def test_repr(self):
|
||||
ff = FermiFunction(Z=20, A=40)
|
||||
assert "FermiFunction" in repr(ff)
|
||||
|
||||
class TestFermiProperties:
|
||||
"""Shared property tests for FermiFunction."""
|
||||
|
||||
@pytest.mark.property
|
||||
@pytest.mark.parametrize("W", [
|
||||
[1.5],
|
||||
[1.1, 2.0, 3.0],
|
||||
np.linspace(1.01, 5.0, 20),
|
||||
])
|
||||
def test_positive(self, W):
|
||||
"""F₀ must be positive everywhere — it's a probability enhancement factor."""
|
||||
ff = FermiFunction(Z=92, A=238) # Uranium — extreme case
|
||||
from tests.common.test_property_tests import _test_positive_values
|
||||
_test_positive_values(ff, W, component_name="FermiFunction")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("n", [1, 5, 100])
|
||||
def test_shape_preserved(self, n):
|
||||
"""Output shape must match input shape."""
|
||||
ff = FermiFunction(Z=20, A=40)
|
||||
W = np.linspace(1.1, 3.0, n)
|
||||
from tests.common.test_property_tests import _test_output_shape_preserved
|
||||
_test_output_shape_preserved(ff, W, component_name="FermiFunction")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("W", [
|
||||
np.linspace(1.01, 6.0, 50),
|
||||
np.linspace(1.001, 10.0, 100),
|
||||
])
|
||||
def test_no_nan(self, W):
|
||||
"""For very heavy nuclei, the loggamma implementation must not overflow."""
|
||||
ff = FermiFunction(Z=92, A=238)
|
||||
from tests.common.test_property_tests import _test_no_nan_across_range
|
||||
_test_no_nan_across_range(ff, W, component_name="FermiFunction")
|
||||
|
||||
@pytest.mark.quality
|
||||
def test_no_nan_at_threshold(self):
|
||||
"""At W→1, p→0 and η→∞. The implementation must handle this limit."""
|
||||
ff = FermiFunction(Z=50, A=120) # Tin — moderate heavy
|
||||
result = ff(np.array([1.001]))
|
||||
assert not np.isnan(result[0]), "Must handle threshold (W→1) without NaN"
|
||||
assert result[0] > 0, "Threshold value must be positive and finite"
|
||||
@@ -0,0 +1,77 @@
|
||||
"""
|
||||
Code quality / API tests for FiniteSizeL0 and ChargeDistributionU.
|
||||
|
||||
Shared property tests in tests/common/test_property_tests.py.
|
||||
"""
|
||||
|
||||
import numpy as np
|
||||
import pytest
|
||||
|
||||
from beta_spectrum.components.finite_size import FiniteSizeL0, ChargeDistributionU
|
||||
|
||||
|
||||
class TestFiniteSizeL0API:
|
||||
@pytest.mark.api
|
||||
def test_callable(self):
|
||||
fs = FiniteSizeL0(Z=20, A=40)
|
||||
assert callable(fs)
|
||||
result = fs(np.array([2.0]))
|
||||
assert isinstance(result, np.ndarray)
|
||||
|
||||
@pytest.mark.api
|
||||
def test_repr(self):
|
||||
fs = FiniteSizeL0(Z=20, A=40)
|
||||
assert "FiniteSizeL0" in repr(fs)
|
||||
|
||||
class TestFiniteSizeL0Properties:
|
||||
@pytest.mark.property
|
||||
@pytest.mark.parametrize("W", [
|
||||
[2.0],
|
||||
np.linspace(1.05, 6.0, 20),
|
||||
])
|
||||
def test_positive(self, W):
|
||||
fs = FiniteSizeL0(Z=92, A=238)
|
||||
from tests.common.test_property_tests import _test_positive_values
|
||||
_test_positive_values(fs, W, component_name="FiniteSizeL0")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("n", [1, 5, 100])
|
||||
def test_shape(self, n):
|
||||
fs = FiniteSizeL0(Z=20, A=40)
|
||||
W = np.linspace(1.1, 3.0, n)
|
||||
from tests.common.test_property_tests import _test_output_shape_preserved
|
||||
_test_output_shape_preserved(fs, W, component_name="FiniteSizeL0")
|
||||
|
||||
|
||||
class TestChargeDistributionUAPI:
|
||||
@pytest.mark.api
|
||||
def test_callable(self):
|
||||
u = ChargeDistributionU(Z=20, A=40)
|
||||
assert callable(u)
|
||||
result = u(np.array([2.0]))
|
||||
assert isinstance(result, np.ndarray)
|
||||
|
||||
@pytest.mark.api
|
||||
def test_repr(self):
|
||||
u = ChargeDistributionU(Z=20, A=40)
|
||||
assert "ChargeDistributionU" in repr(u)
|
||||
|
||||
|
||||
class TestChargeDistributionUProperties:
|
||||
@pytest.mark.property
|
||||
@pytest.mark.parametrize("W", [
|
||||
[2.0],
|
||||
np.linspace(1.1, 5.0, 10),
|
||||
])
|
||||
def test_non_negative(self, W):
|
||||
u = ChargeDistributionU(Z=20, A=40)
|
||||
from tests.common.test_property_tests import _test_non_negative_values
|
||||
_test_non_negative_values(u, W, component_name="ChargeDistributionU")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("n", [1, 5, 100])
|
||||
def test_shape(self, n):
|
||||
u = ChargeDistributionU(Z=20, A=40)
|
||||
W = np.linspace(1.1, 3.0, n)
|
||||
from tests.common.test_property_tests import _test_output_shape_preserved
|
||||
_test_output_shape_preserved(u, W, component_name="ChargeDistributionU")
|
||||
@@ -0,0 +1,57 @@
|
||||
"""
|
||||
Code quality / API tests for PhaseSpace.
|
||||
|
||||
Shared property tests (positivity, shape, stability) are in
|
||||
tests/common/test_property_tests.py and are NOT duplicated here.
|
||||
"""
|
||||
|
||||
import numpy as np
|
||||
import pytest
|
||||
|
||||
from beta_spectrum.components.phase_space import PhaseSpace
|
||||
|
||||
|
||||
class TestPhaseSpaceAPI:
|
||||
"""Tests for the PhaseSpace API contract."""
|
||||
|
||||
@pytest.mark.api
|
||||
def test_callable(self):
|
||||
ps = PhaseSpace(W0=5.0)
|
||||
assert callable(ps)
|
||||
result = ps(np.array([3.0]))
|
||||
assert isinstance(result, np.ndarray)
|
||||
|
||||
class TestPhaseSpaceProperties:
|
||||
"""Shared property tests for PhaseSpace."""
|
||||
|
||||
@pytest.mark.property
|
||||
@pytest.mark.parametrize("W", [
|
||||
[1.5],
|
||||
[1.1, 2.0, 3.0],
|
||||
np.linspace(1.01, 4.9, 20),
|
||||
])
|
||||
def test_non_negative(self, W):
|
||||
"""Phase space must be non-negative (zero at boundaries)."""
|
||||
ps = PhaseSpace(W0=5.0)
|
||||
from tests.common.test_property_tests import _test_non_negative_values
|
||||
_test_non_negative_values(ps, W, component_name="PhaseSpace")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("n", [1, 5, 100])
|
||||
def test_shape_preserved(self, n):
|
||||
"""Output shape must match input shape."""
|
||||
ps = PhaseSpace(W0=5.0)
|
||||
W = np.linspace(1.1, 4.9, n)
|
||||
from tests.common.test_property_tests import _test_output_shape_preserved
|
||||
_test_output_shape_preserved(ps, W, component_name="PhaseSpace")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("W", [
|
||||
np.linspace(1.01, 4.99, 50),
|
||||
np.linspace(1.001, 4.999, 100),
|
||||
])
|
||||
def test_stability(self, W):
|
||||
"""Phase space must be stable across the full energy range."""
|
||||
ps = PhaseSpace(W0=5.0)
|
||||
from tests.common.test_property_tests import _test_full_range_stability
|
||||
_test_full_range_stability(ps, W, component_name="PhaseSpace")
|
||||
@@ -0,0 +1,86 @@
|
||||
"""
|
||||
Code quality / API tests for RadiativeCorrection.
|
||||
|
||||
Shared property tests in tests/common/test_property_tests.py.
|
||||
"""
|
||||
|
||||
import numpy as np
|
||||
import pytest
|
||||
|
||||
from beta_spectrum.components.radiative import RadiativeCorrection
|
||||
|
||||
|
||||
class TestRadiativeAPI:
|
||||
@pytest.mark.api
|
||||
def test_callable(self):
|
||||
rc = RadiativeCorrection(W0=5.0)
|
||||
assert callable(rc)
|
||||
result = rc(np.array([3.0]))
|
||||
assert isinstance(result, np.ndarray)
|
||||
|
||||
@pytest.mark.api
|
||||
def test_accepts_Z(self):
|
||||
"""RadiativeCorrection must accept Z parameter."""
|
||||
for Z in [1, 20, 50, 92]:
|
||||
rc = RadiativeCorrection(W0=5.0, Z=Z)
|
||||
assert rc.Z == Z
|
||||
|
||||
@pytest.mark.api
|
||||
def test_accepts_A(self):
|
||||
"""RadiativeCorrection must accept A parameter."""
|
||||
rc = RadiativeCorrection(W0=5.0, Z=50, A=120)
|
||||
assert rc.A == 120
|
||||
|
||||
@pytest.mark.api
|
||||
def test_default_A_is_none(self):
|
||||
rc = RadiativeCorrection(W0=5.0, Z=50)
|
||||
assert rc.A is None
|
||||
|
||||
|
||||
class TestRadiativeProperties:
|
||||
@pytest.mark.property
|
||||
@pytest.mark.parametrize("W", [
|
||||
[2.0],
|
||||
np.linspace(1.1, 4.9, 20),
|
||||
])
|
||||
def test_positive(self, W):
|
||||
rc = RadiativeCorrection(W0=5.0)
|
||||
from tests.common.test_property_tests import _test_positive_values
|
||||
_test_positive_values(rc, W, component_name="RadiativeCorrection")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("n", [1, 5, 100])
|
||||
def test_shape(self, n):
|
||||
rc = RadiativeCorrection(W0=5.0)
|
||||
W = np.linspace(1.1, 4.9, n)
|
||||
from tests.common.test_property_tests import _test_output_shape_preserved
|
||||
_test_output_shape_preserved(rc, W, component_name="RadiativeCorrection")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("W0", [2.0, 5.0, 10.0])
|
||||
def test_no_nan_various_W0(self, W0):
|
||||
"""Different endpoint energies should all produce valid output."""
|
||||
rc = RadiativeCorrection(W0=W0)
|
||||
W = np.linspace(1.1, min(9.9, W0 - 0.01), 20)
|
||||
from tests.common.test_property_tests import _test_no_nan_across_range
|
||||
_test_no_nan_across_range(rc, W, component_name=f"RadiativeCorrection(W0={W0})")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("W", [
|
||||
np.linspace(1.0001, 4.9999, 200),
|
||||
np.linspace(1.001, 9.99, 100),
|
||||
])
|
||||
def _test_full_range_stability(self, W):
|
||||
"""Entire energy range from threshold to endpoint must be free of NaN/inf."""
|
||||
rc = RadiativeCorrection(W0=5.0, Z=92, use_endpoint_resummation=True)
|
||||
from tests.common.test_property_tests import _test_full_range_stability
|
||||
_test_full_range_stability(rc, W, component_name="RadiativeCorrection(Z=92)")
|
||||
|
||||
@pytest.mark.quality
|
||||
def test_ultra_low_energy_stable(self):
|
||||
"""W = 1.00001 (beta ~ 0.014) — deep in small-beta regime."""
|
||||
rc = RadiativeCorrection(W0=5.0, Z=92, use_endpoint_resummation=True)
|
||||
W_ultra_low = np.array([1.00001])
|
||||
result = rc(W_ultra_low)
|
||||
assert not np.isnan(result[0])
|
||||
assert not np.isinf(result[0])
|
||||
@@ -0,0 +1,48 @@
|
||||
"""
|
||||
Code quality / API tests for ScreeningCorrection.
|
||||
|
||||
Shared property tests in tests/common/test_property_tests.py.
|
||||
"""
|
||||
|
||||
import numpy as np
|
||||
import pytest
|
||||
|
||||
from beta_spectrum.components.fermi import FermiFunction
|
||||
from beta_spectrum.components.screening import ScreeningCorrection
|
||||
|
||||
|
||||
class TestScreeningAPI:
|
||||
@pytest.mark.api
|
||||
def test_callable(self):
|
||||
ff = FermiFunction(Z=20, A=40)
|
||||
sc = ScreeningCorrection(ff)
|
||||
assert callable(sc)
|
||||
result = sc(np.array([2.0]))
|
||||
assert isinstance(result, np.ndarray)
|
||||
|
||||
@pytest.mark.api
|
||||
def test_repr(self):
|
||||
ff = FermiFunction(Z=20, A=40)
|
||||
sc = ScreeningCorrection(ff)
|
||||
assert "Screening" in repr(sc)
|
||||
|
||||
class TestScreeningProperties:
|
||||
@pytest.mark.property
|
||||
@pytest.mark.parametrize("W", [
|
||||
[2.0],
|
||||
np.linspace(1.02, 3.0, 20),
|
||||
])
|
||||
def test_positive(self, W):
|
||||
ff = FermiFunction(Z=40, A=95)
|
||||
sc = ScreeningCorrection(ff)
|
||||
from tests.common.test_property_tests import _test_positive_values
|
||||
_test_positive_values(sc, W, component_name="ScreeningCorrection")
|
||||
|
||||
@pytest.mark.quality
|
||||
@pytest.mark.parametrize("n", [1, 5, 100])
|
||||
def test_shape(self, n):
|
||||
ff = FermiFunction(Z=20, A=40)
|
||||
sc = ScreeningCorrection(ff)
|
||||
W = np.linspace(1.1, 3.0, n)
|
||||
from tests.common.test_property_tests import _test_output_shape_preserved
|
||||
_test_output_shape_preserved(sc, W, component_name="ScreeningCorrection")
|
||||
Reference in New Issue
Block a user