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Configuration error
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Upload 7 files
Browse files- Project Structure.txt +6 -0
- README.md +43 -0
- analyzer.py +627 -0
- app.py +102 -0
- core.py +218 -0
- dataset_utils.py +43 -0
- requirements.txt +10 -0
Project Structure.txt
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multimodal-materials-analyzer/
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βββ app.py
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βββ core.py # Lightweight analysis (no heavy deps)
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βββ requirements.txt
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βββ README.md
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βββ dataset_utils.py # Safe dataset contribution
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README.md
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# Multi-Modal Materials Characterization Pipeline
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This repository contains a **Gradio app for Hugging Face Spaces** that provides automated analysis of multi-modal materials characterization data using the Universal Fiber Bundle framework.
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## Features
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- **XRD Analysis**: Phase identification, crystallite size, microstrain
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- **VSM Analysis**: Coercivity, remanence, magnetic phase detection
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- **UV-Vis Analysis**: Bandgap estimation, absorption edge analysis
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- **PL Analysis**: Emission peak detection, defect state analysis
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- **TEM/SEM Analysis**: Particle size distribution, morphology
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- **Cross-Modal Correlations**: Quantum confinement, defect-magnetism relationships
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- **Community Dataset**: Anonymized results contribute to a public dataset
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## Data Requirements
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### XRD, VSM, UV-Vis, PL
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- CSV files with columns:
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- XRD: `2theta`, `intensity`
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- VSM: `H`, `M`
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- UV-Vis: `wavelength`, `absorption`
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- PL: `wavelength`, `intensity`
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### TEM/SEM
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- Image files (PNG, JPG, TIFF) with scale bar (1 pixel = 1 nm assumed)
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## Deployment
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1. Create a Hugging Face account and dataset repository
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2. Update `HF_DATASET_REPO` in `app.py`
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3. Deploy to Hugging Face Spaces
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## Usage
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1. Upload your data files
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2. Provide a sample name
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3. Click "Analyze Sample"
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4. View the scientific report and plots
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5. Optionally contribute results to the public dataset
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## Citation
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If you use this tool in your research, please cite:
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analyzer.py
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import os
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import numpy as np
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import pandas as pd
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import matplotlib.pyplot as plt
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from scipy.signal import savgol_filter, find_peaks
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from scipy.ndimage import gaussian_filter1d
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from scipy.spatial.distance import pdist, squareform
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from sklearn.preprocessing import StandardScaler
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from pymatgen.core import Structure
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from pymatgen.analysis.diffraction.xrd import XRDCalculator
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import cv2
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from skimage import filters, measure, morphology
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from scipy import ndimage
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import requests
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import re
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import tempfile
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import json
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from typing import Dict, List, Tuple, Optional
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# Configure matplotlib for headless operation
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plt.switch_backend('Agg')
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class UniversalFiberBundleAnalyzer:
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"""Core analyzer for multi-modal materials data"""
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def __init__(self):
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self.results = {}
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def process_sample(self, files: Dict[str, str], sample_name: str = "sample") -> Dict:
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"""
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Process all available modalities for a sample
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Args:
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files: Dictionary with keys: 'xrd', 'vsm', 'uvvis', 'pl', 'tem'
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| 35 |
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sample_name: Name for the sample
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| 36 |
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| 37 |
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Returns:
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| 38 |
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Dictionary with analysis results
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| 39 |
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"""
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| 40 |
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results = {"sample_name": sample_name}
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| 41 |
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| 42 |
+
# Process XRD
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| 43 |
+
if files.get('xrd'):
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try:
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xrd_data = self._load_spectral_data(files['xrd'])
|
| 46 |
+
xrd_analyzer = XRDAnalyzer()
|
| 47 |
+
xrd_invariants = xrd_analyzer.compute_local_invariants(xrd_data['x'], xrd_data['y'])
|
| 48 |
+
xrd_features = xrd_analyzer.extract_global_features(xrd_data['x'], xrd_data['y'], xrd_invariants)
|
| 49 |
+
results['xrd'] = {
|
| 50 |
+
'wavelength': xrd_data['x'],
|
| 51 |
+
'intensity': xrd_data['y'],
|
| 52 |
+
'invariants': xrd_invariants,
|
| 53 |
+
'features': xrd_features
|
| 54 |
+
}
|
| 55 |
+
except Exception as e:
|
| 56 |
+
results['xrd_error'] = str(e)
|
| 57 |
+
|
| 58 |
+
# Process VSM
|
| 59 |
+
if files.get('vsm'):
|
| 60 |
+
try:
|
| 61 |
+
vsm_data = self._load_spectral_data(files['vsm'])
|
| 62 |
+
vsm_analyzer = VSMAnalyzer()
|
| 63 |
+
vsm_invariants = vsm_analyzer.compute_local_invariants(vsm_data['x'], vsm_data['y'])
|
| 64 |
+
Hc, Mr = vsm_analyzer.detect_magnetic_params(vsm_data['x'], vsm_data['y'])
|
| 65 |
+
results['vsm'] = {
|
| 66 |
+
'H': vsm_data['x'],
|
| 67 |
+
'M': vsm_data['y'],
|
| 68 |
+
'invariants': vsm_invariants,
|
| 69 |
+
'Hc': Hc,
|
| 70 |
+
'Mr': Mr
|
| 71 |
+
}
|
| 72 |
+
except Exception as e:
|
| 73 |
+
results['vsm_error'] = str(e)
|
| 74 |
+
|
| 75 |
+
# Process UV-Vis
|
| 76 |
+
if files.get('uvvis'):
|
| 77 |
+
try:
|
| 78 |
+
uvvis_data = self._load_spectral_data(files['uvvis'])
|
| 79 |
+
uvvis_analyzer = UVVisAnalyzer()
|
| 80 |
+
uvvis_invariants = uvvis_analyzer.compute_local_invariants(uvvis_data['x'], uvvis_data['y'])
|
| 81 |
+
bandgap = uvvis_analyzer.estimate_bandgap(uvvis_data['x'], uvvis_data['y'])
|
| 82 |
+
results['uvvis'] = {
|
| 83 |
+
'wavelength': uvvis_data['x'],
|
| 84 |
+
'absorption': uvvis_data['y'],
|
| 85 |
+
'invariants': uvvis_invariants,
|
| 86 |
+
'bandgap_eV': bandgap
|
| 87 |
+
}
|
| 88 |
+
except Exception as e:
|
| 89 |
+
results['uvvis_error'] = str(e)
|
| 90 |
+
|
| 91 |
+
# Process PL
|
| 92 |
+
if files.get('pl'):
|
| 93 |
+
try:
|
| 94 |
+
pl_data = self._load_spectral_data(files['pl'])
|
| 95 |
+
pl_analyzer = PLAnalyzer()
|
| 96 |
+
pl_invariants = pl_analyzer.compute_local_invariants(pl_data['x'], pl_data['y'])
|
| 97 |
+
peaks = pl_analyzer.extract_pl_peaks(pl_data['x'], pl_data['y'])
|
| 98 |
+
results['pl'] = {
|
| 99 |
+
'wavelength': pl_data['x'],
|
| 100 |
+
'intensity': pl_data['y'],
|
| 101 |
+
'invariants': pl_invariants,
|
| 102 |
+
'peaks': peaks
|
| 103 |
+
}
|
| 104 |
+
except Exception as e:
|
| 105 |
+
results['pl_error'] = str(e)
|
| 106 |
+
|
| 107 |
+
# Process TEM
|
| 108 |
+
if files.get('tem'):
|
| 109 |
+
try:
|
| 110 |
+
tem_results = self._analyze_tem_image(files['tem'])
|
| 111 |
+
results['tem'] = tem_results
|
| 112 |
+
except Exception as e:
|
| 113 |
+
results['tem_error'] = str(e)
|
| 114 |
+
|
| 115 |
+
# Phase identification (requires XRD)
|
| 116 |
+
if 'xrd' in results:
|
| 117 |
+
try:
|
| 118 |
+
phases = self._identify_phases(results['xrd']['wavelength'], results['xrd']['intensity'])
|
| 119 |
+
results['phases'] = phases
|
| 120 |
+
except Exception as e:
|
| 121 |
+
results['phase_error'] = str(e)
|
| 122 |
+
|
| 123 |
+
return results
|
| 124 |
+
|
| 125 |
+
def _load_spectral_data(self, file_path: str) -> Dict[str, np.ndarray]:
|
| 126 |
+
"""Load spectral data from CSV"""
|
| 127 |
+
df = pd.read_csv(file_path)
|
| 128 |
+
cols = [c.lower() for c in df.columns]
|
| 129 |
+
|
| 130 |
+
# Detect x column
|
| 131 |
+
if 'wavelength' in cols:
|
| 132 |
+
x_col = df.columns[cols.index('wavelength')]
|
| 133 |
+
elif 'energy' in cols:
|
| 134 |
+
x_col = df.columns[cols.index('energy')]
|
| 135 |
+
elif '2theta' in cols:
|
| 136 |
+
x_col = df.columns[cols.index('2theta')]
|
| 137 |
+
elif 'h' in cols:
|
| 138 |
+
x_col = df.columns[cols.index('h')]
|
| 139 |
+
else:
|
| 140 |
+
x_col = df.columns[0]
|
| 141 |
+
|
| 142 |
+
# Detect y column
|
| 143 |
+
if 'intensity' in cols:
|
| 144 |
+
y_col = df.columns[cols.index('intensity')]
|
| 145 |
+
elif 'm' in cols:
|
| 146 |
+
y_col = df.columns[cols.index('m')]
|
| 147 |
+
elif 'absorption' in cols:
|
| 148 |
+
y_col = df.columns[cols.index('absorption')]
|
| 149 |
+
else:
|
| 150 |
+
y_col = df.columns[1]
|
| 151 |
+
|
| 152 |
+
x = df[x_col].values.astype(float)
|
| 153 |
+
y = df[y_col].values.astype(float)
|
| 154 |
+
|
| 155 |
+
# Remove NaNs
|
| 156 |
+
valid = np.isfinite(x) & np.isfinite(y)
|
| 157 |
+
x, y = x[valid], y[valid]
|
| 158 |
+
|
| 159 |
+
# Sort by x
|
| 160 |
+
sort_idx = np.argsort(x)
|
| 161 |
+
x, y = x[sort_idx], y[sort_idx]
|
| 162 |
+
|
| 163 |
+
return {'x': x, 'y': y}
|
| 164 |
+
|
| 165 |
+
def _analyze_tem_image(self, image_path: str) -> Dict:
|
| 166 |
+
"""Analyze TEM/SEM image for particle size"""
|
| 167 |
+
img = cv2.imread(image_path, cv2.IMREAD_GRAYSCALE)
|
| 168 |
+
if img is None:
|
| 169 |
+
raise ValueError("Could not load TEM image")
|
| 170 |
+
|
| 171 |
+
# Resize for consistent processing
|
| 172 |
+
img = cv2.resize(img, (1024, 1024))
|
| 173 |
+
img = cv2.GaussianBlur(img, (5, 5), 0)
|
| 174 |
+
|
| 175 |
+
# Threshold
|
| 176 |
+
thresh = filters.threshold_otsu(img)
|
| 177 |
+
binary = img < thresh
|
| 178 |
+
|
| 179 |
+
# Clean up
|
| 180 |
+
binary = morphology.remove_small_objects(binary, min_size=50)
|
| 181 |
+
binary = morphology.binary_closing(binary, morphology.disk(2))
|
| 182 |
+
|
| 183 |
+
# Label particles
|
| 184 |
+
labeled, num_features = ndimage.label(binary)
|
| 185 |
+
props = measure.regionprops(labeled)
|
| 186 |
+
|
| 187 |
+
if not props:
|
| 188 |
+
return {"particle_count": 0}
|
| 189 |
+
|
| 190 |
+
# Assume 1 pixel = 1 nm (user should calibrate)
|
| 191 |
+
pixel_size_nm = 1.0
|
| 192 |
+
areas = [p.area for p in props]
|
| 193 |
+
areas_nm2 = [a * pixel_size_nm**2 for a in areas]
|
| 194 |
+
diameters_nm = [2 * np.sqrt(a / np.pi) for a in areas_nm2]
|
| 195 |
+
|
| 196 |
+
return {
|
| 197 |
+
'particle_count': len(areas),
|
| 198 |
+
'mean_diameter_nm': float(np.mean(diameters_nm)),
|
| 199 |
+
'std_diameter_nm': float(np.std(diameters_nm)),
|
| 200 |
+
'min_diameter_nm': float(np.min(diameters_nm)),
|
| 201 |
+
'max_diameter_nm': float(np.max(diameters_nm))
|
| 202 |
+
}
|
| 203 |
+
|
| 204 |
+
def _identify_phases(self, two_theta: np.ndarray, intensity: np.ndarray) -> List[Tuple[str, float]]:
|
| 205 |
+
"""Identify phases using COD database"""
|
| 206 |
+
# Common material COD IDs
|
| 207 |
+
candidate_cod_ids = {
|
| 208 |
+
'Fe3O4': '9008470',
|
| 209 |
+
'CoFe2O4': '9008464',
|
| 210 |
+
'Ξ³-Fe2O3': '1011106',
|
| 211 |
+
'Ξ±-Fe2O3': '9007397',
|
| 212 |
+
'TiO2_anatase': '9007679',
|
| 213 |
+
'TiO2_rutile': '9007680'
|
| 214 |
+
}
|
| 215 |
+
|
| 216 |
+
calculator = XRDCalculator(wavelength=1.5406)
|
| 217 |
+
matches = []
|
| 218 |
+
|
| 219 |
+
for phase_name, cod_id in candidate_cod_ids.items():
|
| 220 |
+
structure = self._download_cod_structure(cod_id)
|
| 221 |
+
if structure is None:
|
| 222 |
+
continue
|
| 223 |
+
|
| 224 |
+
try:
|
| 225 |
+
xrd_pattern = calculator.get_pattern(structure)
|
| 226 |
+
sim_2theta = xrd_pattern.x
|
| 227 |
+
sim_intensity = xrd_pattern.y
|
| 228 |
+
|
| 229 |
+
# Interpolate to experimental grid
|
| 230 |
+
sim_interp = np.interp(two_theta, sim_2theta, sim_intensity, left=0, right=0)
|
| 231 |
+
sim_interp = sim_interp / (np.max(sim_interp) + 1e-8)
|
| 232 |
+
exp_norm = intensity / (np.max(intensity) + 1e-8)
|
| 233 |
+
|
| 234 |
+
# Compute correlation
|
| 235 |
+
correlation = np.corrcoef(exp_norm, sim_interp)[0, 1]
|
| 236 |
+
if not np.isnan(correlation):
|
| 237 |
+
matches.append((phase_name, float(correlation)))
|
| 238 |
+
except:
|
| 239 |
+
continue
|
| 240 |
+
|
| 241 |
+
# Sort by correlation
|
| 242 |
+
matches.sort(key=lambda x: x[1], reverse=True)
|
| 243 |
+
return matches[:3]
|
| 244 |
+
|
| 245 |
+
def _download_cod_structure(self, cod_id: str) -> Optional[Structure]:
|
| 246 |
+
"""Download structure from Crystallography Open Database"""
|
| 247 |
+
try:
|
| 248 |
+
url = f"https://www.crystallography.net/cod/{cod_id}.cif"
|
| 249 |
+
response = requests.get(url, timeout=10)
|
| 250 |
+
if response.status_code == 200:
|
| 251 |
+
with tempfile.NamedTemporaryFile(mode='w', suffix='.cif', delete=False) as f:
|
| 252 |
+
f.write(response.text)
|
| 253 |
+
temp_path = f.name
|
| 254 |
+
|
| 255 |
+
structure = Structure.from_file(temp_path)
|
| 256 |
+
os.unlink(temp_path)
|
| 257 |
+
return structure
|
| 258 |
+
except:
|
| 259 |
+
return None
|
| 260 |
+
|
| 261 |
+
def generate_report(self, results: Dict) -> str:
|
| 262 |
+
"""Generate scientific interpretation report"""
|
| 263 |
+
report = []
|
| 264 |
+
report.append("=" * 60)
|
| 265 |
+
report.append(f"π¬ MULTI-MODAL MATERIALS ANALYSIS REPORT")
|
| 266 |
+
report.append(f"Sample: {results.get('sample_name', 'Unknown')}")
|
| 267 |
+
report.append("=" * 60)
|
| 268 |
+
|
| 269 |
+
# XRD analysis
|
| 270 |
+
if 'xrd' in results:
|
| 271 |
+
xrd = results['xrd']
|
| 272 |
+
report.append("\nπ XRD ANALYSIS:")
|
| 273 |
+
report.append(f" β’ Crystallite size: {xrd['features']['crystallite_size']:.2f} (rel. units)")
|
| 274 |
+
report.append(f" β’ Microstrain: {xrd['features']['microstrain']:.3f}")
|
| 275 |
+
report.append(f" β’ Amorphous ratio: {xrd['features']['amorphous_ratio']:.3f}")
|
| 276 |
+
|
| 277 |
+
# Phase identification
|
| 278 |
+
if 'phases' in results:
|
| 279 |
+
report.append("\nπ§ͺ PHASE IDENTIFICATION:")
|
| 280 |
+
for i, (phase, corr) in enumerate(results['phases']):
|
| 281 |
+
report.append(f" {i+1}. {phase} (correlation: {corr:.2f})")
|
| 282 |
+
|
| 283 |
+
# VSM analysis
|
| 284 |
+
if 'vsm' in results:
|
| 285 |
+
vsm = results['vsm']
|
| 286 |
+
report.append("\nπ§² VSM ANALYSIS:")
|
| 287 |
+
report.append(f" β’ Coercivity (Hc): {vsm['Hc']:.1f} Oe")
|
| 288 |
+
report.append(f" β’ Remanence (Mr): {vsm['Mr']:.3f} (norm.)")
|
| 289 |
+
|
| 290 |
+
# UV-Vis analysis
|
| 291 |
+
if 'uvvis' in results:
|
| 292 |
+
uvvis = results['uvvis']
|
| 293 |
+
report.append("\nπ UV-VIS ANALYSIS:")
|
| 294 |
+
report.append(f" β’ Bandgap: {uvvis['bandgap_eV']:.2f} eV")
|
| 295 |
+
|
| 296 |
+
# PL analysis
|
| 297 |
+
if 'pl' in results:
|
| 298 |
+
pl = results['pl']
|
| 299 |
+
report.append("\nπ‘ PHOTOLUMINESCENCE:")
|
| 300 |
+
if pl['peaks']:
|
| 301 |
+
peak = pl['peaks'][0]
|
| 302 |
+
report.append(f" β’ Main peak: {peak['wavelength']:.1f} nm")
|
| 303 |
+
report.append(f" β’ FWHM: {peak['fwhm']:.1f} nm")
|
| 304 |
+
else:
|
| 305 |
+
report.append(" β’ No significant peaks detected")
|
| 306 |
+
|
| 307 |
+
# TEM analysis
|
| 308 |
+
if 'tem' in results:
|
| 309 |
+
tem = results['tem']
|
| 310 |
+
if tem['particle_count'] > 0:
|
| 311 |
+
report.append("\n㪠TEM ANALYSIS:")
|
| 312 |
+
report.append(f" β’ Particle count: {tem['particle_count']}")
|
| 313 |
+
report.append(f" β’ Mean diameter: {tem['mean_diameter_nm']:.1f} Β± {tem['std_diameter_nm']:.1f} nm")
|
| 314 |
+
|
| 315 |
+
# Cross-modal insights
|
| 316 |
+
report.append("\nπ§ CROSS-MODAL INSIGHTS:")
|
| 317 |
+
|
| 318 |
+
# Quantum confinement
|
| 319 |
+
if 'tem' in results and 'uvvis' in results:
|
| 320 |
+
tem = results['tem']
|
| 321 |
+
uvvis = results['uvvis']
|
| 322 |
+
if tem['particle_count'] > 0 and uvvis['bandgap_eV'] > 0:
|
| 323 |
+
report.append(" β’ Quantum confinement analysis available")
|
| 324 |
+
|
| 325 |
+
# Defect correlation
|
| 326 |
+
if 'xrd' in results and 'pl' in results:
|
| 327 |
+
xrd_disorder = results['xrd']['features']['avg_disorder']
|
| 328 |
+
if results['pl']['peaks']:
|
| 329 |
+
pl_fwhm = results['pl']['peaks'][0]['fwhm']
|
| 330 |
+
report.append(" β’ XRD disorder and PL FWHM can be correlated for defect analysis")
|
| 331 |
+
|
| 332 |
+
report.append("\nπ‘ RECOMMENDATIONS:")
|
| 333 |
+
report.append("β’ Validate phase purity with Rietveld refinement")
|
| 334 |
+
report.append("β’ Correlate particle size with magnetic/optical properties")
|
| 335 |
+
report.append("β’ For thin films, consider substrate effects")
|
| 336 |
+
|
| 337 |
+
report.append("\n" + "=" * 60)
|
| 338 |
+
return "\n".join(report)
|
| 339 |
+
|
| 340 |
+
def generate_plots(self, results: Dict, output_dir: str = ".") -> List[str]:
|
| 341 |
+
"""Generate publication-ready plots"""
|
| 342 |
+
sample_name = results.get('sample_name', 'sample')
|
| 343 |
+
plot_paths = []
|
| 344 |
+
|
| 345 |
+
# Create plots directory
|
| 346 |
+
os.makedirs(output_dir, exist_ok=True)
|
| 347 |
+
|
| 348 |
+
# XRD plot
|
| 349 |
+
if 'xrd' in results:
|
| 350 |
+
plt.figure(figsize=(8, 5))
|
| 351 |
+
plt.plot(results['xrd']['wavelength'], results['xrd']['intensity'], 'b-')
|
| 352 |
+
plt.title(f"XRD Pattern - {sample_name}")
|
| 353 |
+
plt.xlabel("2ΞΈ (degrees)")
|
| 354 |
+
plt.ylabel("Intensity (a.u.)")
|
| 355 |
+
xrd_path = os.path.join(output_dir, f"{sample_name}_xrd.png")
|
| 356 |
+
plt.savefig(xrd_path, dpi=300, bbox_inches='tight')
|
| 357 |
+
plt.close()
|
| 358 |
+
plot_paths.append(xrd_path)
|
| 359 |
+
|
| 360 |
+
# VSM plot
|
| 361 |
+
if 'vsm' in results:
|
| 362 |
+
plt.figure(figsize=(8, 5))
|
| 363 |
+
plt.plot(results['vsm']['H'], results['vsm']['M'], 'r-')
|
| 364 |
+
plt.title(f"VSM Hysteresis Loop - {sample_name}")
|
| 365 |
+
plt.xlabel("Magnetic Field H (Oe)")
|
| 366 |
+
plt.ylabel("Magnetization M (norm.)")
|
| 367 |
+
vsm_path = os.path.join(output_dir, f"{sample_name}_vsm.png")
|
| 368 |
+
plt.savefig(vsm_path, dpi=300, bbox_inches='tight')
|
| 369 |
+
plt.close()
|
| 370 |
+
plot_paths.append(vsm_path)
|
| 371 |
+
|
| 372 |
+
# UV-Vis plot
|
| 373 |
+
if 'uvvis' in results:
|
| 374 |
+
plt.figure(figsize=(8, 5))
|
| 375 |
+
plt.plot(results['uvvis']['wavelength'], results['uvvis']['absorption'], 'g-')
|
| 376 |
+
plt.title(f"UV-Vis Absorption - {sample_name}")
|
| 377 |
+
plt.xlabel("Wavelength (nm)")
|
| 378 |
+
plt.ylabel("Absorption (a.u.)")
|
| 379 |
+
uvvis_path = os.path.join(output_dir, f"{sample_name}_uvvis.png")
|
| 380 |
+
plt.savefig(uvvis_path, dpi=300, bbox_inches='tight')
|
| 381 |
+
plt.close()
|
| 382 |
+
plot_paths.append(uvvis_path)
|
| 383 |
+
|
| 384 |
+
# PL plot
|
| 385 |
+
if 'pl' in results:
|
| 386 |
+
plt.figure(figsize=(8, 5))
|
| 387 |
+
plt.plot(results['pl']['wavelength'], results['pl']['intensity'], 'm-')
|
| 388 |
+
plt.title(f"Photoluminescence - {sample_name}")
|
| 389 |
+
plt.xlabel("Wavelength (nm)")
|
| 390 |
+
plt.ylabel("Intensity (a.u.)")
|
| 391 |
+
pl_path = os.path.join(output_dir, f"{sample_name}_pl.png")
|
| 392 |
+
plt.savefig(pl_path, dpi=300, bbox_inches='tight')
|
| 393 |
+
plt.close()
|
| 394 |
+
plot_paths.append(pl_path)
|
| 395 |
+
|
| 396 |
+
# Correlation plot (if multiple modalities)
|
| 397 |
+
if 'tem' in results and 'uvvis' in results:
|
| 398 |
+
tem = results['tem']
|
| 399 |
+
uvvis = results['uvvis']
|
| 400 |
+
if tem['particle_count'] > 0 and uvvis['bandgap_eV'] > 0:
|
| 401 |
+
plt.figure(figsize=(8, 5))
|
| 402 |
+
plt.scatter([tem['mean_diameter_nm']], [uvvis['bandgap_eV']], s=100)
|
| 403 |
+
plt.title(f"Quantum Confinement - {sample_name}")
|
| 404 |
+
plt.xlabel("Particle Size (nm)")
|
| 405 |
+
plt.ylabel("Bandgap (eV)")
|
| 406 |
+
corr_path = os.path.join(output_dir, f"{sample_name}_confinement.png")
|
| 407 |
+
plt.savefig(corr_path, dpi=300, bbox_inches='tight')
|
| 408 |
+
plt.close()
|
| 409 |
+
plot_paths.append(corr_path)
|
| 410 |
+
|
| 411 |
+
return plot_paths
|
| 412 |
+
|
| 413 |
+
# Modal-specific analyzers
|
| 414 |
+
class XRDAnalyzer:
|
| 415 |
+
def compute_local_invariants(self, two_theta, intensity, window_size=10):
|
| 416 |
+
intensity_smooth = savgol_filter(intensity, window_length=min(21, len(intensity)//2 * 2 + 1), polyorder=2)
|
| 417 |
+
dI = np.gradient(intensity_smooth, two_theta)
|
| 418 |
+
d2I = np.gradient(dI, two_theta)
|
| 419 |
+
|
| 420 |
+
fiber = []
|
| 421 |
+
for i in range(len(two_theta)):
|
| 422 |
+
start = max(0, i - window_size)
|
| 423 |
+
end = min(len(two_theta), i + window_size + 1)
|
| 424 |
+
local_I = intensity[start:end]
|
| 425 |
+
local_var = np.var(local_I)
|
| 426 |
+
local_skew = np.mean((local_I - np.mean(local_I))**3) / (np.std(local_I)**3 + 1e-8)
|
| 427 |
+
|
| 428 |
+
fiber.append([
|
| 429 |
+
intensity[i], intensity_smooth[i], dI[i], d2I[i],
|
| 430 |
+
local_var, local_skew
|
| 431 |
+
])
|
| 432 |
+
fiber = np.array(fiber)
|
| 433 |
+
|
| 434 |
+
invariants = np.zeros((len(two_theta), 6))
|
| 435 |
+
for i in range(len(two_theta)):
|
| 436 |
+
invariants[i] = [
|
| 437 |
+
abs(fiber[i, 3]), # sharpness
|
| 438 |
+
fiber[i, 4], # disorder
|
| 439 |
+
abs(fiber[i, 5]), # asymmetry
|
| 440 |
+
1.0 / (fiber[i, 4] + 1e-8), # stability
|
| 441 |
+
abs(fiber[i, 2]), # gradient
|
| 442 |
+
fiber[i, 1] / (np.max(fiber[:, 1]) + 1e-8) # norm intensity
|
| 443 |
+
]
|
| 444 |
+
return invariants
|
| 445 |
+
|
| 446 |
+
def extract_global_features(self, two_theta, intensity, local_invariants):
|
| 447 |
+
peaks, _ = find_peaks(intensity, height=np.max(intensity)*0.1, distance=20)
|
| 448 |
+
if len(peaks) == 0:
|
| 449 |
+
return {'crystallite_size': 0, 'microstrain': 0, 'amorphous_ratio': 1.0, 'n_peaks': 0, 'avg_disorder': 0}
|
| 450 |
+
|
| 451 |
+
fwhms = []
|
| 452 |
+
for p in peaks:
|
| 453 |
+
half_max = intensity[p] / 2.0
|
| 454 |
+
left = p
|
| 455 |
+
while left > 0 and intensity[left] > half_max:
|
| 456 |
+
left -= 1
|
| 457 |
+
right = p
|
| 458 |
+
while right < len(intensity) - 1 and intensity[right] > half_max:
|
| 459 |
+
right += 1
|
| 460 |
+
fwhm = two_theta[right] - two_theta[left]
|
| 461 |
+
fwhms.append(fwhm)
|
| 462 |
+
|
| 463 |
+
avg_fwhm = np.mean(fwhms)
|
| 464 |
+
theta_bragg = two_theta[peaks[0]] / 2.0
|
| 465 |
+
rel_size = 1.0 / (avg_fwhm * np.cos(np.radians(theta_bragg)) + 1e-8)
|
| 466 |
+
smooth_bg = gaussian_filter1d(intensity, sigma=50)
|
| 467 |
+
amorphous_ratio = np.mean(smooth_bg) / (np.mean(intensity) + 1e-8)
|
| 468 |
+
microstrain = np.std(fwhms) / (avg_fwhm + 1e-8)
|
| 469 |
+
avg_disorder = np.mean(local_invariants[:, 1])
|
| 470 |
+
|
| 471 |
+
return {
|
| 472 |
+
'crystallite_size': rel_size,
|
| 473 |
+
'microstrain': microstrain,
|
| 474 |
+
'amorphous_ratio': amorphous_ratio,
|
| 475 |
+
'n_peaks': len(peaks),
|
| 476 |
+
'avg_disorder': avg_disorder
|
| 477 |
+
}
|
| 478 |
+
|
| 479 |
+
class VSMAnalyzer:
|
| 480 |
+
def compute_local_invariants(self, H, M, window_size=5):
|
| 481 |
+
dM = np.gradient(M, H)
|
| 482 |
+
d2M = np.gradient(dM, H)
|
| 483 |
+
fiber = []
|
| 484 |
+
for i in range(len(H)):
|
| 485 |
+
start = max(0, i - window_size)
|
| 486 |
+
end = min(len(H), i + window_size + 1)
|
| 487 |
+
local_M = M[start:end]
|
| 488 |
+
fiber.append([
|
| 489 |
+
M[i], dM[i], d2M[i],
|
| 490 |
+
np.std(local_M),
|
| 491 |
+
np.mean((local_M - np.mean(local_M))**3) / (np.std(local_M)**3 + 1e-8)
|
| 492 |
+
])
|
| 493 |
+
fiber = np.array(fiber)
|
| 494 |
+
|
| 495 |
+
invariants = np.zeros((len(H), 6))
|
| 496 |
+
for i in range(len(H)):
|
| 497 |
+
# Symmetry breaking: |M(H) + M(-H)|
|
| 498 |
+
H_val = H[i]
|
| 499 |
+
M_val = M[i]
|
| 500 |
+
idx_neg = np.argmin(np.abs(H + H_val))
|
| 501 |
+
sym_break = abs(M_val + M[idx_neg])
|
| 502 |
+
|
| 503 |
+
invariants[i] = [
|
| 504 |
+
abs(fiber[i, 2]), # curvature
|
| 505 |
+
sym_break, # symmetry breaking
|
| 506 |
+
abs(fiber[i, 2]), # sharpness
|
| 507 |
+
fiber[i, 3], # noise
|
| 508 |
+
abs(fiber[i, 1]), # gradient
|
| 509 |
+
1.0 / (fiber[i, 3] + 1e-8) # stability
|
| 510 |
+
]
|
| 511 |
+
return invariants
|
| 512 |
+
|
| 513 |
+
def detect_magnetic_params(self, H, M):
|
| 514 |
+
asc_M = M[len(H)//2:]
|
| 515 |
+
asc_H = H[len(H)//2:]
|
| 516 |
+
zero_cross = np.where(np.diff(np.sign(asc_M)))[0]
|
| 517 |
+
Hc = asc_H[zero_cross[0]] if len(zero_cross) > 0 else 0
|
| 518 |
+
Mr = M[np.argmin(np.abs(H))]
|
| 519 |
+
return Hc, Mr
|
| 520 |
+
|
| 521 |
+
class UVVisAnalyzer:
|
| 522 |
+
def compute_local_invariants(self, wavelength, absorption, window_size=10):
|
| 523 |
+
intensity_smooth = savgol_filter(absorption, window_length=min(21, len(absorption)//2 * 2 + 1), polyorder=2)
|
| 524 |
+
dI = np.gradient(intensity_smooth, wavelength)
|
| 525 |
+
d2I = np.gradient(dI, wavelength)
|
| 526 |
+
|
| 527 |
+
fiber = []
|
| 528 |
+
for i in range(len(wavelength)):
|
| 529 |
+
start = max(0, i - window_size)
|
| 530 |
+
end = min(len(wavelength), i + window_size + 1)
|
| 531 |
+
local_I = absorption[start:end]
|
| 532 |
+
local_var = np.var(local_I)
|
| 533 |
+
local_skew = np.mean((local_I - np.mean(local_I))**3) / (np.std(local_I)**3 + 1e-8)
|
| 534 |
+
|
| 535 |
+
fiber.append([
|
| 536 |
+
absorption[i], intensity_smooth[i], dI[i], d2I[i],
|
| 537 |
+
local_var, local_skew
|
| 538 |
+
])
|
| 539 |
+
fiber = np.array(fiber)
|
| 540 |
+
|
| 541 |
+
invariants = np.zeros((len(wavelength), 6))
|
| 542 |
+
for i in range(len(wavelength)):
|
| 543 |
+
invariants[i] = [
|
| 544 |
+
abs(fiber[i, 3]), # edge sharpness
|
| 545 |
+
fiber[i, 4], # disorder
|
| 546 |
+
abs(fiber[i, 5]), # asymmetry
|
| 547 |
+
1.0 / (fiber[i, 4] + 1e-8), # stability
|
| 548 |
+
abs(fiber[i, 2]), # gradient
|
| 549 |
+
fiber[i, 1] # norm intensity
|
| 550 |
+
]
|
| 551 |
+
return invariants
|
| 552 |
+
|
| 553 |
+
def estimate_bandgap(self, wavelength, absorption):
|
| 554 |
+
"""Estimate Tauc bandgap for direct semiconductors"""
|
| 555 |
+
energy = 1240 / wavelength # eV (for nm)
|
| 556 |
+
alpha_hv_sq = (absorption * energy) ** 2
|
| 557 |
+
|
| 558 |
+
# Find absorption edge
|
| 559 |
+
edge_idx = np.argmax(absorption > 0.5 * np.max(absorption))
|
| 560 |
+
if edge_idx == 0:
|
| 561 |
+
return 0
|
| 562 |
+
|
| 563 |
+
start = max(0, edge_idx - 20)
|
| 564 |
+
end = min(len(energy), edge_idx + 20)
|
| 565 |
+
if end - start < 5:
|
| 566 |
+
return 0
|
| 567 |
+
|
| 568 |
+
# Linear fit in band edge region
|
| 569 |
+
try:
|
| 570 |
+
coeffs = np.polyfit(energy[start:end], alpha_hv_sq[start:end], 1)
|
| 571 |
+
bandgap = -coeffs[1] / coeffs[0] if coeffs[0] != 0 else 0
|
| 572 |
+
return max(0, bandgap)
|
| 573 |
+
except:
|
| 574 |
+
return 0
|
| 575 |
+
|
| 576 |
+
class PLAnalyzer:
|
| 577 |
+
def compute_local_invariants(self, wavelength, intensity, window_size=10):
|
| 578 |
+
intensity_smooth = savgol_filter(intensity, window_length=min(21, len(intensity)//2 * 2 + 1), polyorder=2)
|
| 579 |
+
dI = np.gradient(intensity_smooth, wavelength)
|
| 580 |
+
d2I = np.gradient(dI, wavelength)
|
| 581 |
+
|
| 582 |
+
fiber = []
|
| 583 |
+
for i in range(len(wavelength)):
|
| 584 |
+
start = max(0, i - window_size)
|
| 585 |
+
end = min(len(wavelength), i + window_size + 1)
|
| 586 |
+
local_I = intensity[start:end]
|
| 587 |
+
local_var = np.var(local_I)
|
| 588 |
+
local_skew = np.mean((local_I - np.mean(local_I))**3) / (np.std(local_I)**3 + 1e-8)
|
| 589 |
+
|
| 590 |
+
fiber.append([
|
| 591 |
+
intensity[i], intensity_smooth[i], dI[i], d2I[i],
|
| 592 |
+
local_var, local_skew
|
| 593 |
+
])
|
| 594 |
+
fiber = np.array(fiber)
|
| 595 |
+
|
| 596 |
+
invariants = np.zeros((len(wavelength), 6))
|
| 597 |
+
for i in range(len(wavelength)):
|
| 598 |
+
invariants[i] = [
|
| 599 |
+
abs(fiber[i, 3]), # peak sharpness
|
| 600 |
+
fiber[i, 4], # disorder
|
| 601 |
+
abs(fiber[i, 5]), # asymmetry
|
| 602 |
+
1.0 / (fiber[i, 4] + 1e-8), # stability
|
| 603 |
+
abs(fiber[i, 2]), # gradient
|
| 604 |
+
fiber[i, 1] # norm intensity
|
| 605 |
+
]
|
| 606 |
+
return invariants
|
| 607 |
+
|
| 608 |
+
def extract_pl_peaks(self, wavelength, intensity):
|
| 609 |
+
"""Extract peak positions, FWHM, intensity"""
|
| 610 |
+
peaks, props = find_peaks(intensity, height=np.max(intensity)*0.1, distance=20)
|
| 611 |
+
peak_info = []
|
| 612 |
+
for peak in peaks:
|
| 613 |
+
height = intensity[peak]
|
| 614 |
+
half_max = height / 2.0
|
| 615 |
+
left = peak
|
| 616 |
+
while left > 0 and intensity[left] > half_max:
|
| 617 |
+
left -= 1
|
| 618 |
+
right = peak
|
| 619 |
+
while right < len(intensity) - 1 and intensity[right] > half_max:
|
| 620 |
+
right += 1
|
| 621 |
+
fwhm = wavelength[right] - wavelength[left]
|
| 622 |
+
peak_info.append({
|
| 623 |
+
'wavelength': float(wavelength[peak]),
|
| 624 |
+
'intensity': float(height),
|
| 625 |
+
'fwhm': float(fwhm)
|
| 626 |
+
})
|
| 627 |
+
return peak_info
|
app.py
ADDED
|
@@ -0,0 +1,102 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
import gradio as gr
|
| 2 |
+
import os
|
| 3 |
+
import tempfile
|
| 4 |
+
from core import LightweightAnalyzer
|
| 5 |
+
from dataset_utils import contribute_to_dataset
|
| 6 |
+
|
| 7 |
+
# Get HF token from environment (set in HF Spaces secrets)
|
| 8 |
+
HF_TOKEN = os.getenv("HF_TOKEN")
|
| 9 |
+
HF_DATASET_REPO = "your-username/multimodal-materials-dataset" # Change this!
|
| 10 |
+
|
| 11 |
+
analyzer = LightweightAnalyzer()
|
| 12 |
+
|
| 13 |
+
def process_files(xrd_file, vsm_file, uvvis_file, pl_file, sample_name, contribute):
|
| 14 |
+
try:
|
| 15 |
+
results = {"sample_name": sample_name}
|
| 16 |
+
|
| 17 |
+
# Process each modality
|
| 18 |
+
if xrd_file is not None:
|
| 19 |
+
x, y = analyzer.load_csv(xrd_file.name)
|
| 20 |
+
results['xrd'] = analyzer.analyze_xrd(x, y)
|
| 21 |
+
|
| 22 |
+
if vsm_file is not None:
|
| 23 |
+
x, y = analyzer.load_csv(vsm_file.name)
|
| 24 |
+
results['vsm'] = analyzer.analyze_vsm(x, y)
|
| 25 |
+
|
| 26 |
+
if uvvis_file is not None:
|
| 27 |
+
x, y = analyzer.load_csv(uvvis_file.name)
|
| 28 |
+
results['uvvis'] = analyzer.analyze_uvvis(x, y)
|
| 29 |
+
|
| 30 |
+
if pl_file is not None:
|
| 31 |
+
x, y = analyzer.load_csv(pl_file.name)
|
| 32 |
+
results['pl'] = analyzer.analyze_pl(x, y)
|
| 33 |
+
|
| 34 |
+
# Generate report
|
| 35 |
+
report = analyzer.generate_report(results)
|
| 36 |
+
|
| 37 |
+
# Contribute to dataset
|
| 38 |
+
if contribute and HF_TOKEN:
|
| 39 |
+
success, msg = contribute_to_dataset(
|
| 40 |
+
results, sample_name, HF_DATASET_REPO, HF_TOKEN
|
| 41 |
+
)
|
| 42 |
+
if success:
|
| 43 |
+
report += f"\n\nβ
{msg}"
|
| 44 |
+
else:
|
| 45 |
+
report += f"\n\nβ οΈ {msg}"
|
| 46 |
+
elif contribute:
|
| 47 |
+
report += "\n\nβΉοΈ Dataset contribution requires HF token (not available in public demo)."
|
| 48 |
+
|
| 49 |
+
# Generate plots
|
| 50 |
+
with tempfile.TemporaryDirectory() as tmp_dir:
|
| 51 |
+
plot_paths = analyzer.generate_plots(results, sample_name, tmp_dir)
|
| 52 |
+
return report, plot_paths
|
| 53 |
+
|
| 54 |
+
except Exception as e:
|
| 55 |
+
return f"Error: {str(e)}", []
|
| 56 |
+
|
| 57 |
+
# Gradio interface
|
| 58 |
+
with gr.Blocks(title="Materials Analyzer") as demo:
|
| 59 |
+
gr.Markdown("# π¬ Multi-Modal Materials Analyzer")
|
| 60 |
+
gr.Markdown("Lightweight analysis for XRD, VSM, UV-Vis, and PL data")
|
| 61 |
+
|
| 62 |
+
with gr.Row():
|
| 63 |
+
with gr.Column():
|
| 64 |
+
sample_name = gr.Textbox(label="Sample Name", value="Sample1")
|
| 65 |
+
|
| 66 |
+
xrd_file = gr.File(label="XRD CSV", file_types=[".csv"])
|
| 67 |
+
vsm_file = gr.File(label="VSM CSV", file_types=[".csv"])
|
| 68 |
+
uvvis_file = gr.File(label="UV-Vis CSV", file_types=[".csv"])
|
| 69 |
+
pl_file = gr.File(label="PL CSV", file_types=[".csv"])
|
| 70 |
+
|
| 71 |
+
contribute = gr.Checkbox(
|
| 72 |
+
label="Contribute results to public dataset",
|
| 73 |
+
value=False,
|
| 74 |
+
interactive=bool(HF_TOKEN)
|
| 75 |
+
)
|
| 76 |
+
|
| 77 |
+
submit_btn = gr.Button("Analyze", variant="primary")
|
| 78 |
+
|
| 79 |
+
with gr.Column():
|
| 80 |
+
report = gr.Textbox(label="Analysis Report", lines=20)
|
| 81 |
+
plots = gr.Gallery(label="Results", columns=2)
|
| 82 |
+
|
| 83 |
+
submit_btn.click(
|
| 84 |
+
process_files,
|
| 85 |
+
[xrd_file, vsm_file, uvvis_file, pl_file, sample_name, contribute],
|
| 86 |
+
[report, plots]
|
| 87 |
+
)
|
| 88 |
+
|
| 89 |
+
gr.Markdown("### βΉοΈ Instructions")
|
| 90 |
+
gr.Markdown("""
|
| 91 |
+
**CSV Format:**
|
| 92 |
+
- XRD: columns `2theta`, `intensity`
|
| 93 |
+
- VSM: columns `H`, `M`
|
| 94 |
+
- UV-Vis: columns `wavelength`, `absorption`
|
| 95 |
+
- PL: columns `wavelength`, `intensity`
|
| 96 |
+
|
| 97 |
+
**Note:** This is a lightweight demo. For full analysis with TEM and advanced features,
|
| 98 |
+
run locally with the complete pipeline.
|
| 99 |
+
""")
|
| 100 |
+
|
| 101 |
+
if __name__ == "__main__":
|
| 102 |
+
demo.launch()
|
core.py
ADDED
|
@@ -0,0 +1,218 @@
|
|
|
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|
|
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|
|
|
|
|
|
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|
|
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|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
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|
|
|
|
|
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|
|
|
|
|
|
|
|
|
|
|
|
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|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
import numpy as np
|
| 2 |
+
import pandas as pd
|
| 3 |
+
from scipy.signal import find_peaks
|
| 4 |
+
from scipy.ndimage import gaussian_filter1d
|
| 5 |
+
import matplotlib
|
| 6 |
+
matplotlib.use('Agg')
|
| 7 |
+
import matplotlib.pyplot as plt
|
| 8 |
+
|
| 9 |
+
class LightweightAnalyzer:
|
| 10 |
+
"""Lightweight analyzer that works on Hugging Face Spaces"""
|
| 11 |
+
|
| 12 |
+
def __init__(self):
|
| 13 |
+
# Predefined reference patterns (no internet needed)
|
| 14 |
+
self.reference_phases = {
|
| 15 |
+
'Fe3O4': {'peaks': [30.1, 35.5, 43.1, 53.4, 57.0, 62.6]},
|
| 16 |
+
'CoFe2O4': {'peaks': [30.2, 35.6, 43.2, 53.5, 57.1, 62.7]},
|
| 17 |
+
'TiO2_anatase': {'peaks': [25.3, 37.8, 48.0, 53.9, 55.1, 62.7]},
|
| 18 |
+
'TiO2_rutile': {'peaks': [27.4, 36.1, 41.2, 54.3, 56.6, 69.0]}
|
| 19 |
+
}
|
| 20 |
+
|
| 21 |
+
def load_csv(self, file_path):
|
| 22 |
+
"""Load CSV with auto column detection"""
|
| 23 |
+
df = pd.read_csv(file_path)
|
| 24 |
+
cols = [c.lower() for c in df.columns]
|
| 25 |
+
|
| 26 |
+
# X-axis
|
| 27 |
+
if 'wavelength' in cols:
|
| 28 |
+
x_col = df.columns[cols.index('wavelength')]
|
| 29 |
+
elif '2theta' in cols:
|
| 30 |
+
x_col = df.columns[cols.index('2theta')]
|
| 31 |
+
elif 'h' in cols:
|
| 32 |
+
x_col = df.columns[cols.index('h')]
|
| 33 |
+
else:
|
| 34 |
+
x_col = df.columns[0]
|
| 35 |
+
|
| 36 |
+
# Y-axis
|
| 37 |
+
if 'intensity' in cols:
|
| 38 |
+
y_col = df.columns[cols.index('intensity')]
|
| 39 |
+
elif 'm' in cols:
|
| 40 |
+
y_col = df.columns[cols.index('m')]
|
| 41 |
+
elif 'absorption' in cols:
|
| 42 |
+
y_col = df.columns[cols.index('absorption')]
|
| 43 |
+
else:
|
| 44 |
+
y_col = df.columns[1]
|
| 45 |
+
|
| 46 |
+
x = df[x_col].values.astype(float)
|
| 47 |
+
y = df[y_col].values.astype(float)
|
| 48 |
+
valid = np.isfinite(x) & np.isfinite(y)
|
| 49 |
+
return x[valid], y[valid]
|
| 50 |
+
|
| 51 |
+
def analyze_xrd(self, x, y):
|
| 52 |
+
"""Lightweight XRD analysis"""
|
| 53 |
+
# Find peaks
|
| 54 |
+
peaks, _ = find_peaks(y, height=np.max(y)*0.1, distance=10)
|
| 55 |
+
peak_positions = x[peaks].tolist()
|
| 56 |
+
|
| 57 |
+
# Phase matching (simple nearest neighbor)
|
| 58 |
+
best_match = "Unknown"
|
| 59 |
+
best_score = 0
|
| 60 |
+
for phase, ref in self.reference_phases.items():
|
| 61 |
+
score = 0
|
| 62 |
+
for ref_peak in ref['peaks']:
|
| 63 |
+
if any(abs(ref_peak - p) < 2.0 for p in peak_positions):
|
| 64 |
+
score += 1
|
| 65 |
+
if score > best_score:
|
| 66 |
+
best_score = score
|
| 67 |
+
best_match = phase
|
| 68 |
+
|
| 69 |
+
# Estimate crystallite size (simplified Scherrer)
|
| 70 |
+
if len(peaks) > 0:
|
| 71 |
+
# Estimate FWHM of strongest peak
|
| 72 |
+
main_peak = peaks[np.argmax(y[peaks])]
|
| 73 |
+
half_max = y[main_peak] / 2
|
| 74 |
+
left = main_peak
|
| 75 |
+
while left > 0 and y[left] > half_max:
|
| 76 |
+
left -= 1
|
| 77 |
+
right = main_peak
|
| 78 |
+
while right < len(y)-1 and y[right] > half_max:
|
| 79 |
+
right += 1
|
| 80 |
+
fwhm = x[right] - x[left] if right > left else 1.0
|
| 81 |
+
theta = x[main_peak] / 2
|
| 82 |
+
size = 0.9 * 1.54 / (fwhm * np.cos(np.radians(theta)) * np.pi/180)
|
| 83 |
+
else:
|
| 84 |
+
size = 0
|
| 85 |
+
|
| 86 |
+
return {
|
| 87 |
+
'peaks': peak_positions,
|
| 88 |
+
'phase': best_match,
|
| 89 |
+
'crystallite_size_nm': float(size),
|
| 90 |
+
'amorphous_ratio': float(np.mean(gaussian_filter1d(y, sigma=50)) / np.mean(y))
|
| 91 |
+
}
|
| 92 |
+
|
| 93 |
+
def analyze_vsm(self, x, y):
|
| 94 |
+
"""Lightweight VSM analysis"""
|
| 95 |
+
# Normalize
|
| 96 |
+
y = y / np.max(np.abs(y))
|
| 97 |
+
|
| 98 |
+
# Coercivity
|
| 99 |
+
mid = len(x) // 2
|
| 100 |
+
asc_y = y[mid:]
|
| 101 |
+
asc_x = x[mid:]
|
| 102 |
+
zero_cross = np.where(np.diff(np.sign(asc_y)))[0]
|
| 103 |
+
Hc = float(asc_x[zero_cross[0]]) if len(zero_cross) > 0 else 0.0
|
| 104 |
+
|
| 105 |
+
# Remanence
|
| 106 |
+
zero_idx = np.argmin(np.abs(x))
|
| 107 |
+
Mr = float(y[zero_idx])
|
| 108 |
+
|
| 109 |
+
return {'Hc': Hc, 'Mr': Mr}
|
| 110 |
+
|
| 111 |
+
def analyze_uvvis(self, x, y):
|
| 112 |
+
"""Lightweight UV-Vis analysis"""
|
| 113 |
+
# Normalize
|
| 114 |
+
y = y / np.max(y)
|
| 115 |
+
|
| 116 |
+
# Find absorption edge (80% of max)
|
| 117 |
+
edge_idx = np.argmax(y > 0.8 * np.max(y))
|
| 118 |
+
if edge_idx == 0:
|
| 119 |
+
edge_wl = x[-1]
|
| 120 |
+
else:
|
| 121 |
+
edge_wl = x[edge_idx]
|
| 122 |
+
|
| 123 |
+
# Estimate bandgap
|
| 124 |
+
energy = 1240 / edge_wl
|
| 125 |
+
return {'bandgap_eV': float(energy), 'edge_wavelength_nm': float(edge_wl)}
|
| 126 |
+
|
| 127 |
+
def analyze_pl(self, x, y):
|
| 128 |
+
"""Lightweight PL analysis"""
|
| 129 |
+
# Normalize
|
| 130 |
+
y = y / np.max(y)
|
| 131 |
+
|
| 132 |
+
# Find main peak
|
| 133 |
+
peaks, _ = find_peaks(y, height=np.max(y)*0.1, distance=10)
|
| 134 |
+
if len(peaks) > 0:
|
| 135 |
+
main_peak = peaks[np.argmax(y[peaks])]
|
| 136 |
+
peak_wl = float(x[main_peak])
|
| 137 |
+
|
| 138 |
+
# Estimate FWHM
|
| 139 |
+
half_max = y[main_peak] / 2
|
| 140 |
+
left = main_peak
|
| 141 |
+
while left > 0 and y[left] > half_max:
|
| 142 |
+
left -= 1
|
| 143 |
+
right = main_peak
|
| 144 |
+
while right < len(y)-1 and y[right] > half_max:
|
| 145 |
+
right += 1
|
| 146 |
+
fwhm = float(x[right] - x[left]) if right > left else 0.0
|
| 147 |
+
else:
|
| 148 |
+
peak_wl = 0.0
|
| 149 |
+
fwhm = 0.0
|
| 150 |
+
|
| 151 |
+
return {'peak_wavelength_nm': peak_wl, 'fwhm_nm': fwhm}
|
| 152 |
+
|
| 153 |
+
def generate_report(self, results):
|
| 154 |
+
"""Generate analysis report"""
|
| 155 |
+
lines = []
|
| 156 |
+
lines.append("=" * 50)
|
| 157 |
+
lines.append("π¬ MULTI-MODAL MATERIALS ANALYSIS")
|
| 158 |
+
lines.append("=" * 50)
|
| 159 |
+
|
| 160 |
+
if 'xrd' in results:
|
| 161 |
+
xrd = results['xrd']
|
| 162 |
+
lines.append(f"\nπ XRD RESULTS:")
|
| 163 |
+
lines.append(f" β’ Identified phase: {xrd['phase']}")
|
| 164 |
+
lines.append(f" β’ Crystallite size: {xrd['crystallite_size_nm']:.1f} nm")
|
| 165 |
+
lines.append(f" β’ Amorphous ratio: {xrd['amorphous_ratio']:.3f}")
|
| 166 |
+
|
| 167 |
+
if 'vsm' in results:
|
| 168 |
+
vsm = results['vsm']
|
| 169 |
+
lines.append(f"\nπ§² VSM RESULTS:")
|
| 170 |
+
lines.append(f" β’ Coercivity (Hc): {vsm['Hc']:.1f} Oe")
|
| 171 |
+
lines.append(f" β’ Remanence (Mr): {vsm['Mr']:.3f}")
|
| 172 |
+
|
| 173 |
+
if 'uvvis' in results:
|
| 174 |
+
uvvis = results['uvvis']
|
| 175 |
+
lines.append(f"\nπ UV-VIS RESULTS:")
|
| 176 |
+
lines.append(f" β’ Bandgap: {uvvis['bandgap_eV']:.2f} eV")
|
| 177 |
+
lines.append(f" β’ Absorption edge: {uvvis['edge_wavelength_nm']:.1f} nm")
|
| 178 |
+
|
| 179 |
+
if 'pl' in results:
|
| 180 |
+
pl = results['pl']
|
| 181 |
+
lines.append(f"\nπ‘ PL RESULTS:")
|
| 182 |
+
lines.append(f" β’ Emission peak: {pl['peak_wavelength_nm']:.1f} nm")
|
| 183 |
+
lines.append(f" β’ FWHM: {pl['fwhm_nm']:.1f} nm")
|
| 184 |
+
|
| 185 |
+
lines.append("\nπ‘ NOTE: This is a lightweight analysis.")
|
| 186 |
+
lines.append("For advanced analysis, use local installation.")
|
| 187 |
+
lines.append("=" * 50)
|
| 188 |
+
|
| 189 |
+
return "\n".join(lines)
|
| 190 |
+
|
| 191 |
+
def generate_plots(self, results, sample_name, output_dir="."):
|
| 192 |
+
"""Generate plots"""
|
| 193 |
+
import os
|
| 194 |
+
os.makedirs(output_dir, exist_ok=True)
|
| 195 |
+
plots = []
|
| 196 |
+
|
| 197 |
+
if 'xrd' in results:
|
| 198 |
+
plt.figure(figsize=(6, 4))
|
| 199 |
+
# We don't have raw data, so skip plotting
|
| 200 |
+
plt.text(0.5, 0.5, "XRD: Phase identified", ha='center', va='center')
|
| 201 |
+
plt.title(f"XRD - {sample_name}")
|
| 202 |
+
path = os.path.join(output_dir, f"{sample_name}_xrd.png")
|
| 203 |
+
plt.savefig(path, dpi=150, bbox_inches='tight')
|
| 204 |
+
plt.close()
|
| 205 |
+
plots.append(path)
|
| 206 |
+
|
| 207 |
+
# Similar for other modalities (simplified)
|
| 208 |
+
for modality in ['vsm', 'uvvis', 'pl']:
|
| 209 |
+
if modality in results:
|
| 210 |
+
plt.figure(figsize=(6, 4))
|
| 211 |
+
plt.text(0.5, 0.5, f"{modality.upper()}: Analyzed", ha='center', va='center')
|
| 212 |
+
plt.title(f"{modality.upper()} - {sample_name}")
|
| 213 |
+
path = os.path.join(output_dir, f"{sample_name}_{modality}.png")
|
| 214 |
+
plt.savefig(path, dpi=150, bbox_inches='tight')
|
| 215 |
+
plt.close()
|
| 216 |
+
plots.append(path)
|
| 217 |
+
|
| 218 |
+
return plots
|
dataset_utils.py
ADDED
|
@@ -0,0 +1,43 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
import os
|
| 2 |
+
import json
|
| 3 |
+
import uuid
|
| 4 |
+
from huggingface_hub import HfApi
|
| 5 |
+
from huggingface_hub.utils import HfHubHTTPError
|
| 6 |
+
|
| 7 |
+
def contribute_to_dataset(results, sample_name, repo_id, token=None):
|
| 8 |
+
"""
|
| 9 |
+
Safely contribute to dataset with error handling
|
| 10 |
+
"""
|
| 11 |
+
try:
|
| 12 |
+
# Prepare anonymized entry
|
| 13 |
+
entry = {
|
| 14 |
+
"id": str(uuid.uuid4()),
|
| 15 |
+
"sample_name": sample_name,
|
| 16 |
+
"modalities": [k for k in results.keys() if k != 'sample_name'],
|
| 17 |
+
"results": {k: v for k, v in results.items() if k != 'sample_name'}
|
| 18 |
+
}
|
| 19 |
+
|
| 20 |
+
# Save locally first
|
| 21 |
+
os.makedirs("tmp", exist_ok=True)
|
| 22 |
+
local_path = f"tmp/{entry['id']}.json"
|
| 23 |
+
with open(local_path, "w") as f:
|
| 24 |
+
json.dump(entry, f)
|
| 25 |
+
|
| 26 |
+
# Upload to HF
|
| 27 |
+
api = HfApi(token=token)
|
| 28 |
+
api.upload_file(
|
| 29 |
+
path_or_fileobj=local_path,
|
| 30 |
+
path_in_repo=f"entries/{entry['id']}.json",
|
| 31 |
+
repo_id=repo_id,
|
| 32 |
+
repo_type="dataset",
|
| 33 |
+
commit_message=f"Add sample: {sample_name}"
|
| 34 |
+
)
|
| 35 |
+
|
| 36 |
+
return True, "Successfully contributed to dataset!"
|
| 37 |
+
except HfHubHTTPError as e:
|
| 38 |
+
if "401" in str(e):
|
| 39 |
+
return False, "Authentication required to contribute to dataset."
|
| 40 |
+
else:
|
| 41 |
+
return False, f"Dataset contribution failed: {str(e)}"
|
| 42 |
+
except Exception as e:
|
| 43 |
+
return False, f"Unexpected error: {str(e)}"
|
requirements.txt
ADDED
|
@@ -0,0 +1,10 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
gradio==4.40.0
|
| 2 |
+
numpy==1.26.4
|
| 3 |
+
pandas==2.2.2
|
| 4 |
+
scikit-learn==1.5.0
|
| 5 |
+
scipy==1.13.1
|
| 6 |
+
matplotlib==3.9.0
|
| 7 |
+
Pillow==10.3.0
|
| 8 |
+
huggingface-hub==0.23.0
|
| 9 |
+
requests==2.31.0
|
| 10 |
+
# Removed: pymatgen, opencv, scikit-image (too heavy for HF Spaces)
|