Price & McEwen#
- s2fft.recursions.price_mcewen.compute_all_slices(beta: ndarray, L: int, spin: int, precomps=None) ndarray #
Compute a particular slice \(m^{\prime}\), denoted mm, of the complete Wigner-d matrix for all sampled polar angles \(\beta\) and all \(\ell\) using Price & McEwen recursion.
The Wigner-d slice for all \(\ell\) (el) and \(\beta\) is computed recursively over \(m\) labelled ‘m’ at a specific \(m^{\prime}\). The Price & McEwen recursion is analytically correct from \(-\ell < m < \ell\) however numerically it can become unstable for \(m > 0\). To avoid this we compute \(d_{m, m^{\prime}}^{\ell}(\beta)\) for negative \(m\) and then evaluate \(d_{m, -m^{\prime}}^{\ell}(\beta) = (-1)^{m-m^{\prime}} d_{-m, m^{\prime}}^{\ell}(\beta)\) which we can again evaluate using the same recursion.
On-the-fly renormalisation is implemented to avoid potential over/under-flows, within any given iteration of the recursion the iterants are \(\sim \mathcal{O}(1)\).
The Wigner-d slice \(d^\ell_{m, m^{\prime}}(\beta)\) is indexed for \(-L < m < L\) by dl[L - 1 - m, beta, ell]. This implementation has computational scaling \(\mathcal{O}(L)\) and typically requires \(\sim 2L\) operations.
- Parameters:
beta (np.ndarray) – Array of polar angles in radians.
L (int) – Harmonic band-limit.
spin (int, optional) – Harmonic spin. Defaults to 0.
precomps (List[np.ndarray]) – Precomputed recursion coefficients with memory overhead \(\mathcal{O}(L^2)\), which is minimal.
- Returns:
Wigner-d matrix mm slice of dimension \([2L-1, n_{\theta}, n_{\ell}]\).
- Return type:
np.ndarray
- s2fft.recursions.price_mcewen.compute_all_slices_jax(beta: Array, L: int, spin: int, sampling: str = 'mw', forward: bool = False, nside: int = None, precomps=None) Array #
Compute a particular slice \(m^{\prime}\), denoted mm, of the complete Wigner-d matrix for all sampled polar angles \(\beta\) and all \(\ell\) using Price & McEwen recursion.
The Wigner-d slice for all \(\ell\) (el) and \(\beta\) is computed recursively over \(m\) labelled ‘m’ at a specific \(m^{\prime}\). The Price & McEwen recursion is analytically correct from \(-\ell < m < \ell\) however numerically it can become unstable for \(m > 0\). To avoid this we compute \(d_{m, m^{\prime}}^{\ell}(\beta)\) for negative \(m\) and then evaluate \(d_{m, -m^{\prime}}^{\ell}(\beta) = (-1)^{m-m^{\prime}} d_{-m, m^{\prime}}^{\ell}(\beta)\) which we can again evaluate using the same recursion.
On-the-fly renormalisation is implemented to avoid potential over/under-flows, within any given iteration of the recursion the iterants are \(\sim \mathcal{O}(1)\).
The Wigner-d slice \(d^\ell_{m, m^{\prime}}(\beta)\) is indexed for \(-L < m < L\) by dl[L - 1 - m, beta, ell]. This implementation has computational scaling \(\mathcal{O}(L)\) and typically requires \(\sim 2L\) operations.
- Parameters:
beta (jnp.ndarray) – Array of polar angles in radians.
L (int) – Harmonic band-limit.
spin (int, optional) – Harmonic spin. Defaults to 0.
precomps (List[np.ndarray]) – Precomputed recursion coefficients with memory overhead \(\mathcal{O}(L^2)\), which is minimal.
- Returns:
Wigner-d matrix mm slice of dimension \([2L-1, n_{\theta}, n_{\ell}]\).
- Return type:
jnp.ndarray
- s2fft.recursions.price_mcewen.generate_precomputes(L: int, spin: int = 0, sampling: str = 'mw', nside: int | None = None, forward: bool = False, L_lower: int = 0) List[ndarray] #
Compute recursion coefficients with \(\mathcal{O}(L^2)\) memory overhead. In practice one could compute these on-the-fly but the memory overhead is negligible and well worth the acceleration.
- Parameters:
L (int) – Harmonic band-limit.
spin (int, optional) – Harmonic spin. Defaults to 0.
sampling (str, optional) – Sampling scheme. Supported sampling schemes include {“mw”, “mwss”, “dh”, “healpix”}. Defaults to “mw”.
nside (int, optional) – HEALPix Nside resolution parameter. Only required if sampling=”healpix”. Defaults to None.
forward (bool, optional) – Whether to provide forward or inverse shift. Defaults to False.
L_lower (int, optional) – Harmonic lower-bound. Transform will only be computed for \(\texttt{L_lower} \leq \ell < \texttt{L}\). Defaults to 0.
- Returns:
List of precomputed coefficient arrays.
- Return type:
List[np.ndarray]
Note
TODO: this function should be optimised.
- s2fft.recursions.price_mcewen.generate_precomputes_jax(L: int, spin: int = 0, sampling: str = 'mw', nside: int = None, forward: bool = False, L_lower: int = 0, betas: Array = None) List[Array] #
Compute recursion coefficients with \(\mathcal{O}(L^2)\) memory overhead. In practice one could compute these on-the-fly but the memory overhead is negligible and well worth the acceleration. JAX implementation of
generate_precomputes()
.- Parameters:
L (int) – Harmonic band-limit.
spin (int, optional) – Harmonic spin. Defaults to 0.
sampling (str, optional) – Sampling scheme. Supported sampling schemes include {“mw”, “mwss”, “dh”, “healpix”}. Defaults to “mw”.
nside (int, optional) – HEALPix Nside resolution parameter. Only required if sampling=”healpix”. Defaults to None.
forward (bool, optional) – Whether to provide forward or inverse shift. Defaults to False.
L_lower (int, optional) – Harmonic lower-bound. Transform will only be computed for \(\texttt{L_lower} \leq \ell < \texttt{L}\). Defaults to 0.
beta (jnp.ndarray) – Array of polar angles in radians.
- Returns:
List of precomputed coefficient arrays.
- Return type:
List[jnp.ndarray]
- s2fft.recursions.price_mcewen.generate_precomputes_wigner(L: int, N: int, sampling: str = 'mw', nside: int | None = None, forward: bool = False, reality: bool = False, L_lower: int = 0) List[List[ndarray]] #
Compute recursion coefficients with \(\mathcal{O}(L^2)\) memory overhead. In practice one could compute these on-the-fly but the memory overhead is negligible and well worth the acceleration. This is a wrapped extension of
generate_precomputes()
for the case of multiple spins, i.e. the Wigner transform over SO(3).- Parameters:
L (int) – Harmonic band-limit.
N (int) – Azimuthal bandlimit
sampling (str, optional) – Sampling scheme. Supported sampling schemes include {“mw”, “mwss”, “dh”, “healpix”}. Defaults to “mw”.
nside (int, optional) – HEALPix Nside resolution parameter. Only required if sampling=”healpix”. Defaults to None.
forward (bool, optional) – Whether to provide forward or inverse shift. Defaults to False.
reality (bool, optional) – Whether the signal on the sphere is real. If so, conjugate symmetry is exploited to reduce computational costs. Defaults to False.
L_lower (int, optional) – Harmonic lower-bound. Transform will only be computed for \(\texttt{L_lower} \leq \ell < \texttt{L}\). Defaults to 0.
- Returns:
2N-1 length List of Lists of precomputed coefficient arrays.
- Return type:
List[List[np.ndarray]]
Note
TODO: this function should be optimised.
- s2fft.recursions.price_mcewen.generate_precomputes_wigner_jax(L: int, N: int, sampling: str = 'mw', nside: int = None, forward: bool = False, reality: bool = False, L_lower: int = 0) List[List[Array]] #
Compute recursion coefficients with \(\mathcal{O}(L^2)\) memory overhead. In practice one could compute these on-the-fly but the memory overhead is negligible and well worth the acceleration. This is a wrapped extension of
generate_precomputes()
for the case of multiple spins, i.e. the Wigner transform over SO(3). JAX implementation ofgenerate_precomputes_wigner()
.- Parameters:
L (int) – Harmonic band-limit.
N (int) – Azimuthal bandlimit
sampling (str, optional) – Sampling scheme. Supported sampling schemes include {“mw”, “mwss”, “dh”, “healpix”}. Defaults to “mw”.
nside (int, optional) – HEALPix Nside resolution parameter. Only required if sampling=”healpix”. Defaults to None.
forward (bool, optional) – Whether to provide forward or inverse shift. Defaults to False.
reality (bool, optional) – Whether the signal on the sphere is real. If so, conjugate symmetry is exploited to reduce computational costs. Defaults to False.
L_lower (int, optional) – Harmonic lower-bound. Transform will only be computed for \(\texttt{L_lower} \leq \ell < \texttt{L}\). Defaults to 0.
- Returns:
2N-1 length List of Lists of precomputed coefficient arrays.
- Return type:
List[List[jnp.ndarray]]