import jax import jax.numpy as jnp import jax_cosmo as jc from jaxpm.growth import dGfa, growth_factor, growth_rate from jaxpm.kernels import (PGD_kernel, fftk, gradient_kernel, laplace_kernel, longrange_kernel) from jaxpm.painting import cic_paint, cic_read def pm_forces(positions, mesh_shape=None, delta=None, r_split=0): """ Computes gravitational forces on particles using a PM scheme """ if mesh_shape is None: mesh_shape = delta.shape kvec = fftk(mesh_shape) if delta is None: delta_k = jnp.fft.rfftn(cic_paint(jnp.zeros(mesh_shape), positions)) else: delta_k = jnp.fft.rfftn(delta) # Computes gravitational potential pot_k = delta_k * laplace_kernel(kvec) * longrange_kernel(kvec, r_split=r_split) # Computes gravitational forces return jnp.stack([ cic_read(jnp.fft.irfftn(gradient_kernel(kvec, i) * pot_k), positions) for i in range(3) ], axis=-1) def lpt(cosmo, initial_conditions, positions, a): """ Computes first order LPT displacement """ initial_force = pm_forces(positions, delta=initial_conditions) a = jnp.atleast_1d(a) dx = growth_factor(cosmo, a) * initial_force p = a**2 * growth_rate(cosmo, a) * jnp.sqrt(jc.background.Esqr(cosmo, a)) * dx f = a**2 * jnp.sqrt(jc.background.Esqr(cosmo, a)) * dGfa(cosmo, a) * initial_force return dx, p, f def linear_field(mesh_shape, box_size, pk, seed): """ Generate initial conditions. """ kvec = fftk(mesh_shape) kmesh = sum((kk / box_size[i] * mesh_shape[i])**2 for i, kk in enumerate(kvec))**0.5 pkmesh = pk(kmesh) * (mesh_shape[0] * mesh_shape[1] * mesh_shape[2]) / ( box_size[0] * box_size[1] * box_size[2]) field = jax.random.normal(seed, mesh_shape) field = jnp.fft.rfftn(field) * pkmesh**0.5 field = jnp.fft.irfftn(field) return field def make_ode_fn(mesh_shape): def nbody_ode(state, a, cosmo): """ state is a tuple (position, velocities) """ pos, vel = state forces = pm_forces(pos, mesh_shape=mesh_shape) * 1.5 * cosmo.Omega_m # Computes the update of position (drift) dpos = 1. / (a**3 * jnp.sqrt(jc.background.Esqr(cosmo, a))) * vel # Computes the update of velocity (kick) dvel = 1. / (a**2 * jnp.sqrt(jc.background.Esqr(cosmo, a))) * forces return dpos, dvel return nbody_ode def pgd_correction(pos, mesh_shape, params): """ improve the short-range interactions of PM-Nbody simulations with potential gradient descent method, based on https://arxiv.org/abs/1804.00671 args: pos: particle positions [npart, 3] params: [alpha, kl, ks] pgd parameters """ kvec = fftk(mesh_shape) delta = cic_paint(jnp.zeros(mesh_shape), pos) alpha, kl, ks = params delta_k = jnp.fft.rfftn(delta) PGD_range=PGD_kernel(kvec, kl, ks) pot_k_pgd=(delta_k * laplace_kernel(kvec))*PGD_range forces_pgd= jnp.stack([cic_read(jnp.fft.irfftn(gradient_kernel(kvec, i)*pot_k_pgd), pos) for i in range(3)],axis=-1) dpos_pgd = forces_pgd*alpha return dpos_pgd def make_neural_ode_fn(model, mesh_shape): def neural_nbody_ode(state, a, cosmo, params): """ state is a tuple (position, velocities) """ pos, vel = state kvec = fftk(mesh_shape) delta = cic_paint(jnp.zeros(mesh_shape), pos) delta_k = jnp.fft.rfftn(delta) # Computes gravitational potential pot_k = delta_k * laplace_kernel(kvec) * longrange_kernel(kvec, r_split=0) # Apply a correction filter kk = jnp.sqrt(sum((ki/jnp.pi)**2 for ki in kvec)) pot_k = pot_k *(1. + model.apply(params, kk, jnp.atleast_1d(a))) # Computes gravitational forces forces = jnp.stack([cic_read(jnp.fft.irfftn(gradient_kernel(kvec, i)*pot_k), pos) for i in range(3)],axis=-1) forces = forces * 1.5 * cosmo.Omega_m # Computes the update of position (drift) dpos = 1. / (a**3 * jnp.sqrt(jc.background.Esqr(cosmo, a))) * vel # Computes the update of velocity (kick) dvel = 1. / (a**2 * jnp.sqrt(jc.background.Esqr(cosmo, a))) * forces return dpos, dvel return neural_nbody_ode