OME / fullC /code /omol_store.py
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"""Zarr v3 shard writer for Pass A.
Layout
------
Each worker writes self-contained *shards*, so there is no write contention and no resize logic:
store/p1/<dataset>/shard_<nnnn>_<nn>.zarr scalars + per-atom + per-pair
store/p2/<dataset>/shard_<nnnn>_<nn>.zarr the same, plus fock/, eps/, occ/
p2 duplicates the p1 arrays on purpose: the tables are tiny next to the matrices (<0.2 TB for the
whole collection) and it keeps p1 independently usable without the 6 TB matrix store.
Columns are *packed*: all float scalars live in one (n_calc, n_col) array, all per-atom floats in
one (n_atom_total, n_col) array, and so on, with the column names recorded in group attrs. Writing
one array per column meant ~80 Zarr arrays per shard, and zarr-python's sync wrapper costs enough
per array that shard writes dominated the run; packing cuts that to ~15 arrays.
Ragged quantities are a concatenated array plus an int64 offsets array of length n_calc+1, so
calculation i occupies [off[i], off[i+1]).
Codecs follow the benchmark: Blosc zstd 9 + bit-shuffle for the int32 Fock triangles (4.5x), Blosc
zstd 5 + byte-shuffle elsewhere.
"""
from __future__ import annotations
import os
import numpy as np
import zarr
from zarr.codecs import BloscCodec
SHELLS = ("s", "p", "d", "f", "g")
FOCK_CODEC = [BloscCodec(cname="zstd", clevel=9, shuffle="bitshuffle")]
DATA_CODEC = [BloscCodec(cname="zstd", clevel=5, shuffle="shuffle")]
SCALARS_F8 = (
"e_total", "e_total_engrad", "e_nuc_rep", "e_one_elec", "e_two_elec", "e_kinetic",
"virial_ratio", "e_xc", "e_nl", "e_exchange", "n_alpha_int", "n_beta_int",
"s2", "s2_ideal", "s2_dev", "conv_denergy", "conv_maxdp", "conv_rmsdp", "conv_diiserr",
"smallest_ovlp_eig", "grad_norm", "grad_rms", "grad_max", "run_time_s",
"dipole_au", "dipole_debye", "quad_iso", "npa_core", "npa_valence", "npa_rydberg",
"nbo_lewis", "nbo_nonlewis", "homo_a", "lumo_a", "gap_a", "homo_b", "lumo_b", "gap_b",
)
SCALARS_I = ("charge", "mult", "nelec", "nbas", "naux", "n_lindep", "scf_cycles", "n_atoms")
FLAGS = ("scf_converged", "terminated_normally", "nbo_available", "npa_available",
"is_uhf", "has_fock")
VEC = (("dipole_elec", 3), ("dipole_nuc", 3), ("dipole_total", 3), ("rot_const_cm", 3),
("rot_const_mhz", 3), ("quad_diag", 3), ("quad_nuc", 6), ("quad_elec", 6),
("quad_total", 6))
ATOM_1D = ("mulliken_q", "mulliken_s", "loewdin_q", "loewdin_s",
"mayer_NA", "mayer_ZA", "mayer_QA", "mayer_VA", "mayer_BVA", "mayer_FA",
"npa_q", "npa_atom_core", "npa_atom_val", "npa_atom_ryd", "npa_spin")
ATOM_VEC3 = ("coords", "forces")
ATOM_SHELL = ("mulliken_shell_q", "mulliken_shell_s", "loewdin_shell_q", "loewdin_shell_s",
"natural_config")
PAIRS = ("mayer_bo", "loewdin_bo", "mulliken_ovlp")
ATOM_F8_COLS = [f"{k}_{ax}" for k in ATOM_VEC3 for ax in "xyz"] + list(ATOM_1D)
VEC_COLS = [f"{name}_{i}" for name, w in VEC for i in range(w)]
SHELL_COLS = [f"{k}_{sh}" for k in ATOM_SHELL for sh in SHELLS]
def frontier(eps, occ):
"""HOMO, LUMO and gap in Eh. Orbitals removed for linear dependence print as exactly 0.0."""
if eps is None or occ is None or len(eps) == 0:
return np.nan, np.nan, np.nan
occupied = np.flatnonzero(occ > 0)
if occupied.size == 0:
return np.nan, np.nan, np.nan
h = int(occupied[-1])
homo = float(eps[h])
lumo = np.nan
for k in range(h + 1, len(eps)):
if eps[k] != 0.0:
lumo = float(eps[k])
break
return homo, lumo, (lumo - homo if lumo == lumo else np.nan)
def _fock_chunk_elems(median_nbas):
if median_nbas < 600:
return 65_536
if median_nbas <= 2000:
return 1_000_000
return 4_194_304
CHUNKS_PER_SHARD = 256
def put_array(g, name, data, codec=DATA_CODEC, chunks=None, overwrite=False):
"""Create array `name` in group `g` holding `data`, using Zarr's sharding codec.
With sharding an array is a handful of files no matter how many chunks it holds. Without it
each chunk is a file: the first full run produced 1.5 to 4.7 files per calculation, on course
to exhaust the 10 M-inode scratch quota. One shard file holds CHUNKS_PER_SHARD chunks (capped
at the array itself), and the shard length is always a multiple of the chunk length as Zarr
requires. `codec=None` stores the bytes uncompressed (for incompressible fp32 coefficients).
"""
data = np.ascontiguousarray(data)
if chunks is None:
if data.ndim == 1:
chunks = (max(1, min(data.shape[0], 1 << 22)),)
else:
chunks = (max(1, min(data.shape[0], 1 << 18)),) + data.shape[1:]
chunks = tuple(int(c) for c in chunks)
n_chunks = max(1, -(-data.shape[0] // chunks[0])) # ceil
shards = (chunks[0] * min(CHUNKS_PER_SHARD, n_chunks),) + tuple(data.shape[1:])
if overwrite and name in g:
del g[name]
z = g.create_array(name=name, shape=data.shape, chunks=chunks, shards=shards,
dtype=data.dtype, compressors=codec)
if data.size:
z[...] = data
return z
def write_shard(records, out_dir, shard_name, include_matrices):
"""Write one shard group. Records are parser outputs augmented with calc_id/rel_path/dataset."""
os.makedirs(out_dir, exist_ok=True)
path = os.path.join(out_dir, shard_name)
g = zarr.open_group(path, mode="w")
n = len(records)
natom = [r["n_atoms"] for r in records]
atom_off = np.cumsum([0] + natom).astype("i8")
def put(name, data, codec=DATA_CODEC, chunks=None):
put_array(g, name, data, codec=codec, chunks=chunks)
# ---- identity and column names live in attrs: JSON, portable, no bytes dtype
g.attrs.update({
"schema": "omol_elec/pass_a/2",
"n_calc": n,
"shells": list(SHELLS),
"scalar_f8_cols": list(SCALARS_F8),
"scalar_i_cols": list(SCALARS_I),
"flag_cols": list(FLAGS),
"vec_cols": VEC_COLS,
"atom_f8_cols": ATOM_F8_COLS,
"atom_shell_cols": SHELL_COLS,
"pair_names": list(PAIRS),
"calc_id": [r["calc_id"] for r in records],
"rel_path": [r["rel_path"] for r in records],
"dataset": records[0]["dataset"] if n else "",
"hftyp": [(r.get("hftyp") or "?") for r in records],
"has_matrices": bool(include_matrices),
})
# ---- packed scalars
sf = np.full((n, len(SCALARS_F8)), np.nan)
for i, r in enumerate(records):
for j, k in enumerate(SCALARS_F8):
v = r.get(k)
if v is not None:
sf[i, j] = v
put("scalar_f8", sf)
si = np.full((n, len(SCALARS_I)), -1, dtype="i8")
for i, r in enumerate(records):
for j, k in enumerate(SCALARS_I):
v = r.get(k)
if v is not None:
si[i, j] = v
put("scalar_i", si)
fl = np.zeros((n, len(FLAGS)), dtype="i1")
for i, r in enumerate(records):
for j, k in enumerate(FLAGS):
if k == "is_uhf":
fl[i, j] = bool(r.get("hftyp") == "UHF")
elif k == "has_fock":
fl[i, j] = r.get("fock_a") is not None
else:
fl[i, j] = bool(r.get(k))
put("flags", fl)
vv = np.full((n, len(VEC_COLS)), np.nan)
for i, r in enumerate(records):
c = 0
for name, w in VEC:
v = r.get(name)
if v is not None and len(v) == w:
vv[i, c:c + w] = v
c += w
put("vec", vv)
# ---- per-atom, packed
put("atom_offsets", atom_off)
tot = int(atom_off[-1])
az = np.zeros(tot, dtype="i2")
af = np.full((tot, len(ATOM_F8_COLS)), np.nan)
ash = np.full((tot, len(SHELL_COLS)), np.nan, dtype="f4")
for i, r in enumerate(records):
a, b = int(atom_off[i]), int(atom_off[i + 1])
z = r.get("atomic_numbers")
if z is not None:
az[a:b] = np.asarray(z, dtype="i2")
c = 0
for k in ATOM_VEC3:
v = r.get(k)
if v is not None:
af[a:b, c:c + 3] = np.asarray(v, dtype="f8").reshape(-1, 3)
c += 3
for k in ATOM_1D:
v = r.get(k)
if v is not None:
af[a:b, c] = np.asarray(v, dtype="f8")
c += 1
c = 0
for k in ATOM_SHELL:
v = r.get(k)
if v is not None:
ash[a:b, c:c + len(SHELLS)] = np.asarray(v, dtype="f4").reshape(-1, len(SHELLS))
c += len(SHELLS)
put("atom_z", az)
put("atom_f8", af)
put("atom_shell", ash)
# ---- per-pair: one offsets/index/value triple per bond-order flavour
for key in PAIRS:
idx, val, offs = [], [], [0]
for r in records:
for i, j, v in (r.get(key) or []):
idx.append((i, j))
val.append(v)
offs.append(len(val))
put(f"pair_{key}_offsets", np.array(offs, dtype="i8"))
put(f"pair_{key}_index", np.array(idx, dtype="i4").reshape(-1, 2))
put(f"pair_{key}_value", np.array(val, dtype="f4"))
# ---- orbitals and matrices (p2 only)
if include_matrices:
med = int(np.median([r["nbas"] for r in records])) if n else 1000
fchunk = _fock_chunk_elems(med)
for spin in ("a", "b"):
eps_parts, occ_parts, offs = [], [], [0]
for r in records:
e, o = r.get(f"eps_{spin}"), r.get(f"occ_{spin}")
if e is None:
e, o = np.zeros(0), np.zeros(0)
eps_parts.append(np.asarray(e, dtype="f8"))
occ_parts.append(np.asarray(o, dtype="f8"))
offs.append(offs[-1] + len(e))
put(f"eps_{spin}_offsets", np.array(offs, dtype="i8"))
put(f"eps_{spin}", np.concatenate(eps_parts) if eps_parts else np.zeros(0))
put(f"occ_{spin}", np.concatenate(occ_parts) if occ_parts else np.zeros(0))
fparts, foffs = [], [0]
for r in records:
f = r.get(f"fock_{spin}")
f = np.zeros(0, dtype="i4") if f is None else np.asarray(f, dtype="i4")
fparts.append(f)
foffs.append(foffs[-1] + len(f))
flat = np.concatenate(fparts) if fparts else np.zeros(0, dtype="i4")
put(f"fock_{spin}_offsets", np.array(foffs, dtype="i8"))
put(f"fock_{spin}", flat, codec=FOCK_CODEC,
chunks=(max(1, min(len(flat), fchunk)),))
return path
def shard_bytes(rec):
"""Rough in-memory footprint, used to decide when to flush a shard."""
b = 0
for k in ("fock_a", "fock_b", "eps_a", "eps_b", "occ_a", "occ_b"):
v = rec.get(k)
if v is not None:
b += v.nbytes
return b + 4096
# ----------------------------------------------------------------------------- reading
def read_calc(g, i):
"""Unpack calculation i from an open shard group into a dict."""
out = {}
sf = g["scalar_f8"][i]
for j, k in enumerate(g.attrs["scalar_f8_cols"]):
out[k] = float(sf[j])
si = g["scalar_i"][i]
for j, k in enumerate(g.attrs["scalar_i_cols"]):
out[k] = int(si[j])
fl = g["flags"][i]
for j, k in enumerate(g.attrs["flag_cols"]):
out[k] = bool(fl[j])
vv = g["vec"][i]
c = 0
for name, w in VEC:
out[name] = np.asarray(vv[c:c + w])
c += w
out["calc_id"] = g.attrs["calc_id"][i]
out["rel_path"] = g.attrs["rel_path"][i]
out["hftyp"] = g.attrs["hftyp"][i]
out["dataset"] = g.attrs["dataset"]
a, b = int(g["atom_offsets"][i]), int(g["atom_offsets"][i + 1])
out["atomic_numbers"] = np.asarray(g["atom_z"][a:b])
af = np.asarray(g["atom_f8"][a:b])
cols = g.attrs["atom_f8_cols"]
out["coords"] = af[:, [cols.index(f"coords_{x}") for x in "xyz"]]
out["forces"] = af[:, [cols.index(f"forces_{x}") for x in "xyz"]]
for k in ATOM_1D:
out[k] = af[:, cols.index(k)]
ash = np.asarray(g["atom_shell"][a:b])
for j, k in enumerate(ATOM_SHELL):
out[k] = ash[:, j * len(SHELLS):(j + 1) * len(SHELLS)]
for key in PAIRS:
p0 = int(g[f"pair_{key}_offsets"][i])
p1 = int(g[f"pair_{key}_offsets"][i + 1])
out[key] = (np.asarray(g[f"pair_{key}_index"][p0:p1]),
np.asarray(g[f"pair_{key}_value"][p0:p1]))
if g.attrs.get("has_matrices"):
for spin in ("a", "b"):
e0 = int(g[f"eps_{spin}_offsets"][i])
e1 = int(g[f"eps_{spin}_offsets"][i + 1])
out[f"eps_{spin}"] = np.asarray(g[f"eps_{spin}"][e0:e1])
out[f"occ_{spin}"] = np.asarray(g[f"occ_{spin}"][e0:e1])
f0 = int(g[f"fock_{spin}_offsets"][i])
f1 = int(g[f"fock_{spin}_offsets"][i + 1])
out[f"fock_{spin}"] = np.asarray(g[f"fock_{spin}"][f0:f1])
return out
def inflate_fock(tri, nbas):
"""int32 micro-Hartree upper triangle -> symmetric float64 matrix in Eh."""
M = np.zeros((nbas, nbas))
M[np.triu_indices(nbas)] = tri.astype(np.float64) * 1e-6
return M + M.T - np.diag(M.diagonal())
def read_mo(g, i, spin="a"):
"""MO coefficient matrix C[ao, mo] of calculation i for one spin channel (after Pass B1).
Stored MO-major (C^T) so the occupied block is a contiguous prefix; this returns the
(nbas, n_stored) matrix with columns = MOs in ORCA AO order: all nbas orbitals in a full-C
store, the nocc occupied ones in an occupied-only store (see attrs["mo_content"]). Empty
(nbas, 0) when the channel is absent (beta of an RHF run) or the gbw was not paired.
"""
nbas = int(g["scalar_i"][i][list(g.attrs["scalar_i_cols"]).index("nbas")])
o0, o1 = int(g[f"cmo_{spin}_offsets"][i]), int(g[f"cmo_{spin}_offsets"][i + 1])
if o1 == o0:
return np.zeros((nbas, 0), dtype=g[f"cmo_{spin}"].dtype)
# (nbas, nbas) in a full-C store, (nbas, nocc) in an occupied-only one (attrs["mo_content"])
return np.asarray(g[f"cmo_{spin}"][o0:o1]).reshape(-1, nbas).T
def read_cocc(g, i):
"""Occupied MO coefficients and gbw orbital data for calculation i (after Pass B1).
Returns C_a (nbas, nocc_a) and C_b (nbas, nocc_b) in ORCA AO order, the occupations of those
columns, the full gbw orbital energies and occupations, and the B1 flags. Empty arrays when the
gbw was not paired; check flags['mo_ok'] before trusting the pairing.
"""
out = {}
nbas = int(g["scalar_i"][i][list(g.attrs["scalar_i_cols"]).index("nbas")])
mi = g["mo_i"][i]
for j, k in enumerate(g.attrs["mo_i_cols"]):
out[k] = int(mi[j])
mf = g["mo_f8"][i]
for j, k in enumerate(g.attrs["mo_f8_cols"]):
out[k] = float(mf[j])
fl = g["mo_flags"][i]
out["flags"] = {k: bool(fl[j]) for j, k in enumerate(g.attrs["mo_flag_cols"])}
for s in "ab":
nocc = out[f"nocc_{s}"]
o0, o1 = int(g[f"cmo_{s}_offsets"][i]), int(g[f"cmo_{s}_offsets"][i + 1])
if o1 > o0 and nocc:
# first nocc rows of C^T, read without touching the virtual block
out[f"C_{s}"] = np.asarray(g[f"cmo_{s}"][o0:o0 + nocc * nbas]).reshape(nocc, nbas).T
else:
out[f"C_{s}"] = np.zeros((nbas, 0), dtype=g[f"cmo_{s}"].dtype)
for name in ("gbw_eps", "gbw_occ"):
a, b = int(g[f"{name}_{s}_offsets"][i]), int(g[f"{name}_{s}_offsets"][i + 1])
out[f"{name}_{s}"] = np.asarray(g[f"{name}_{s}"][a:b])
out[f"cocc_occ_{s}"] = out[f"gbw_occ_{s}"][:nocc]
return out