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name: Python package | ||
on: | ||
push: | ||
tags: | ||
- "v*.*.*" | ||
jobs: | ||
build: | ||
runs-on: ubuntu-latest | ||
steps: | ||
- uses: actions/checkout@v3 | ||
- name: Set up Python 3.11 | ||
uses: actions/setup-python@v4 | ||
with: | ||
python-version: 3.11 | ||
- name: Install python dependencies | ||
run: | | ||
pip install poetry | ||
poetry install | ||
poetry remove torch | ||
poetry run pip install torch --index-url https://download.pytorch.org/whl/cpu | ||
- name: Build package | ||
run: | | ||
poetry build | ||
- name: Publish package | ||
env: | ||
PYPI_TOKEN: ${{ secrets.PYPI_TOKEN }} | ||
run: | | ||
poetry config pypi-token.pypi "$PYPI_TOKEN" | ||
poetry publish |
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name: Integration test | ||
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on: [push] | ||
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env: | ||
TORCH_DEVICE: "cpu" | ||
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jobs: | ||
build: | ||
runs-on: ubuntu-latest | ||
steps: | ||
- uses: actions/checkout@v3 | ||
- name: Set up Python 3.11 | ||
uses: actions/setup-python@v4 | ||
with: | ||
python-version: 3.11 | ||
- name: Install python dependencies | ||
run: | | ||
pip install poetry | ||
poetry install | ||
poetry remove torch | ||
poetry run pip install torch --index-url https://download.pytorch.org/whl/cpu | ||
- name: Download benchmark data | ||
run: | | ||
wget -O benchmark_data.zip "https://drive.google.com/uc?export=download&id=1dbY0kBq2SUa885gmbLPUWSRzy5K7O5XJ" | ||
unzip benchmark_data.zip | ||
mv bench_data.json data/bench_data.json | ||
- name: Run benchmark test | ||
run: | | ||
poetry run texify_benchmark --max 16 | ||
poetry run python scripts/verify_benchmark_scores.py data/bench_results.json | ||
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* | ||
!.gitignore | ||
!examples | ||
!images | ||
!examples/* | ||
!images | ||
!images/* |
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The potential $V_{i}$ of cell $\mathcal{C}_ {j}$ centred at position $\mathbf{r}_ {i}$ is related to the surface charge densities $\sigma_ {j}$ of cells $\mathcal{E}_ {j}$ $j\in[1,N]$ through the superposition principle as: | ||
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$$V_ {i}\,=\,\sum_ {j=0}^{N}\,\frac{\sigma_ {j}}{4\pi\varepsilon_ {0}}\,\int_{\mathcal{E}_ {j}}\frac{1}{\left|\mathbf{r}_ {i}-\mathbf{r}^{\prime}\right|}\,\mathrm{d}^{2}\mathbf{r}^{\prime}\,=\,\sum_{j=0}^{N}\,Q_ {ij}\,\sigma_{j},$$ | ||
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where the integral over the surface of cell $\mathcal{C}_ {j}$ only depends on $\mathcal{C}{j}$ shape and on the relative position of the target point $\mathbf{r}_ {i}$ with respect to $\mathcal{C}_ {j}$ location, as $\sigma_ {j}$ is assumed constant over the whole surface of cell $\mathcal{C}_ {j}$. |
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Following , the minimal energy fraction the muon receives in the pion's rest frame is $r_ {\pi}=(m_ {\mu}/m_ {\pi})^2\approx0.57$, when it is emitted against the direction of movement, or 1 when it coincides with the pion's direction. |
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$$\mid\frac{1}{x}=\frac{1}{c}\mid=\mid\frac{c-x}{xc}\mid=\frac{1}{\left\vert x\right\vert}\cdot\frac{1}{\left\vert c\right\vert}\cdot\left\vert x-c\right\vert$$ | ||
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The factor $$\frac{1}{\left\vert x\right\vert}$$ is not good if its near 0. |
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Then the results are that afterward: | ||
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For every value of $\lambda$, there is a probability of $|\langle\Psi|\Psi_\lambda\rangle|^2$ that the system is in state $|\Psi_\lambda\rangle$ | ||
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This is captured by the density matrix formalism as the transition | ||
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$|\Psi\rangle\langle\Psi|\Rightarrow\sum_\lambda|\langle\Psi|\Psi_\lambda\rangle|^2|\Psi_\lambda\rangle\langle\Psi_\lambda|$ | ||
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atyy I guess thinking about it classically, Demystifier's argument must be right. |
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