Python SDK requires an API key. Create one in Settings → API Keys, then set OURO_API_KEY.
import os
from ouro import Ouro
# Set OURO_API_KEY in your environment or replace os.environ.get("OURO_API_KEY")
ouro = Ouro(api_key=os.environ.get("OURO_API_KEY"))
file_id = "ad25fb0e-72f2-468b-8712-2d75ea407345"
# Retrieve file metadata and signed URL
f = ouro.files.retrieve(file_id)
print(f.name, f.visibility)
data = f.read_data() # fetches signed URL
print(data.url)Fe15Ir (Pm-3m)
Fe15Ir (space group: Pm-3m #221, crystal system: cubic, point group: m-3m)
Fe15Ir (Pm-3m) - phonon dispersion
Image filePhonon band structure (supercell [2, 2, 2], Δ=0.01 Å); no imaginary modes; min freq = 0.00 THz
4moFe15Ir phase diagram
.html filePhase diagram of Fe15Ir; e_above_hull: 0.000000 eV/atom; predicted_stable: True
4moFe15Ir (Pm-3m) - relaxed
.cif fileRelaxed with Orb v3; 0.03 eV/Å threshold; final energy = -135.7751 eV; energy change = -0.0058 eV; symmetry: Pm-3m → Pm-3m
4mois a post describing the next steps after an initial pipeline run. The goal is to find materials with strong magnetocrystalline anisotropy energy (MAE) to validate candidates further. The text notes a model that predicts FePt around 3.07 meV and literature values for Nd2Fe14B near 2.9 meV per unit cell, suggesting values above about 2.5 meV are promising, since most materials have MAE below 0.1 meV. Several candidate results are shared, The notes mention exploring MnBi as a non-rare alternative and plan more testing later.
4mo