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jaxdecomp proto (#21)
* adding example of distributed solution * put back old functgion * update formatting * add halo exchange and slice pad * apply formatting * implement distributed optimized cic_paint * Use new cic_paint with halo * Fix seed for distributed normal * Wrap interpolation function to avoid all gather * Return normal order frequencies for single GPU * add example * format * add optimised bench script * times in ms * add lpt2 * update benchmark and add slurm * Visualize only final field * Update scripts/distributed_pm.py Co-authored-by: Francois Lanusse <EiffL@users.noreply.github.com> * Adjust pencil type for frequencies * fix painting issue with slabs * Shared operation in fourrier space now take inverted sharding axis for slabs * add assert to make pyright happy * adjust test for hpc-plotter * add PMWD test * bench * format * added github workflow * fix formatting from main * Update for jaxDecomp pure JAX * revert single halo extent change * update for latest jaxDecomp * remove fourrier_space in autoshmap * make normal_field work with single controller * format * make distributed pm work in single controller * merge bench_pm * update to leapfrog * add a strict dependency on jaxdecomp * global mesh no longer needed * kernels.py no longer uses global mesh * quick fix in distributed * pm.py no longer uses global mesh * painting.py no longer uses global mesh * update demo script * quick fix in kernels * quick fix in distributed * update demo * merge hugos LPT2 code * format * Small fix * format * remove duplicate get_ode_fn * update visualizer * update compensate CIC * By default check_rep is false for shard_map * remove experimental distributed code * update PGDCorrection and neural ode to use new fft3d * jaxDecomp pfft3d promotes to complex automatically * remove deprecated stuff * fix painting issue with read_cic * use jnp interp instead of jc interp * delete old slurms * add notebook examples * apply formatting * add distributed zeros * fix code in LPT2 * jit cic_paint * update notebooks * apply formating * get local shape and zeros can be used by users * add a user facing function to create uniform particle grid * use jax interp instead of jax_cosmo * use float64 for enmeshing * Allow applying weights with relative cic paint * Weights can be traced * remove script folder * update example notebooks * delete outdated design file * add readme for tutorials * update readme * fix small error * forgot particles in multi host * clarifying why cic_paint_dx is slower * clarifying the halo size dependence on the box size * ability to choose snapshots number with MultiHost script * Adding animation notebook * Put plotting in package * Add finite difference laplace kernel + powerspec functions from Hugo Co-authored-by: Hugo Simonfroy <hugo.simonfroy@gmail.com> * Put plotting utils in package * By default use absoulute painting with * update code * update notebooks * add tests * Upgrade setup.py to pyproject * Format * format tests * update test dependencies * add test workflow * fix deprecated FftType in jaxpm.kernels * Add aboucaud comments * JAX version is 0.4.35 until Diffrax new release * add numpy explicitly as dependency for tests * fix install order for tests * add numpy to be installed * enforce no build isolation for fastpm * pip install jaxpm test without build isolation * bump jaxdecomp version * revert test workflow * remove outdated tests --------- Co-authored-by: EiffL <fr.eiffel@gmail.com> Co-authored-by: Francois Lanusse <EiffL@users.noreply.github.com> Co-authored-by: Wassim KABALAN <wassim@apc.in2p3.fr> Co-authored-by: Hugo Simonfroy <hugo.simonfroy@gmail.com> Former-commit-id: 8c2e823d4669eac712089bf7f85ffb7912e8232d
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26 changed files with 1871 additions and 434 deletions
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@ -1,30 +1,46 @@
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import jax.numpy as jnp
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import numpy as np
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from jax.lax import FftType
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from jax.sharding import PartitionSpec as P
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from jaxdecomp import fftfreq3d, get_output_specs
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from jaxpm.distributed import autoshmap
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def fftk(shape, symmetric=True, finite=False, dtype=np.float32):
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"""
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Return wave-vectors for a given shape
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def fftk(k_array):
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"""
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k = []
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for d in range(len(shape)):
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kd = np.fft.fftfreq(shape[d])
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kd *= 2 * np.pi
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kdshape = np.ones(len(shape), dtype='int')
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if symmetric and d == len(shape) - 1:
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kd = kd[:shape[d] // 2 + 1]
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kdshape[d] = len(kd)
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kd = kd.reshape(kdshape)
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Generate Fourier transform wave numbers for a given mesh.
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k.append(kd.astype(dtype))
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del kd, kdshape
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return k
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Args:
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nc (int): Shape of the mesh grid.
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Returns:
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list: List of wave number arrays for each dimension in
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the order [kx, ky, kz].
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"""
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kx, ky, kz = fftfreq3d(k_array)
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# to the order of dimensions in the transposed FFT
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return kx, ky, kz
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def interpolate_power_spectrum(input, k, pk, sharding=None):
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pk_fn = lambda x: jnp.interp(x.reshape(-1), k, pk).reshape(x.shape)
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gpu_mesh = sharding.mesh if sharding is not None else None
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specs = sharding.spec if sharding is not None else P()
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out_specs = P(*get_output_specs(
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FftType.FFT, specs, mesh=gpu_mesh)) if gpu_mesh is not None else P()
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return autoshmap(pk_fn,
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gpu_mesh=gpu_mesh,
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in_specs=out_specs,
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out_specs=out_specs)(input)
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def gradient_kernel(kvec, direction, order=1):
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"""
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Computes the gradient kernel in the requested direction
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Parameters
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-----------
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kvec: list
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@ -50,23 +66,30 @@ def gradient_kernel(kvec, direction, order=1):
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return wts
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def invlaplace_kernel(kvec):
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def invlaplace_kernel(kvec, fd=False):
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"""
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Compute the inverse Laplace kernel
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Compute the inverse Laplace kernel.
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cf. [Feng+2016](https://arxiv.org/pdf/1603.00476)
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Parameters
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-----------
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kvec: list
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List of wave-vectors
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fd: bool
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Finite difference kernel
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Returns
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--------
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wts: array
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Complex kernel values
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"""
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kk = sum(ki**2 for ki in kvec)
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kk_nozeros = jnp.where(kk==0, 1, kk)
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return - jnp.where(kk==0, 0, 1 / kk_nozeros)
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if fd:
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kk = sum((ki * jnp.sinc(ki / (2 * jnp.pi)))**2 for ki in kvec)
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else:
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kk = sum(ki**2 for ki in kvec)
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kk_nozeros = jnp.where(kk == 0, 1, kk)
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return -jnp.where(kk == 0, 0, 1 / kk_nozeros)
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def longrange_kernel(kvec, r_split):
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List of wave-vectors
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r_split: float
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Splitting radius
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Returns
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--------
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wts: array
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Complex kernel values
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TODO: @modichirag add documentation
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"""
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if r_split != 0:
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-----------
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kvec: list
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List of wave-vectors
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Returns:
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--------
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wts: array
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Complex kernel values
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"""
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kwts = [np.sinc(kvec[i] / (2 * np.pi)) for i in range(3)]
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kwts = [jnp.sinc(kvec[i] / (2 * np.pi)) for i in range(3)]
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wts = (kwts[0] * kwts[1] * kwts[2])**(-2)
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return wts
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