paulgessinger's picture
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metadata
license: cc-by-4.0
task_categories:
  - other
tags:
  - physics
  - high-energy-physics
  - particle-physics
  - tracking
  - calorimetry
  - machine-learning
  - simulation
pretty_name: ColliderML Top-Quark Pair Production (No Pileup)
size_categories:
  - 10K<n<100K
configs:
  - config_name: particles
    data_files:
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  - config_name: tracker_hits
    data_files:
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events30000-30999.parquet
      - >-
        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events31000-31999.parquet
      - >-
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events33000-33999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events41000-41999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events44000-44999.parquet
      - >-
        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events45000-45999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events46000-46999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events47000-47999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events5000-5999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events51000-51999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events52000-52999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events53000-53999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events55000-55999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events56000-56999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events57000-57999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events58000-58999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events59000-59999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events6000-6999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events60000-60999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events61000-61999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events62000-62999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events63000-63999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events64000-64999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events65000-65999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events66000-66999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events67000-67999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events68000-68999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events69000-69999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events7000-7999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events74000-74999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events75000-75999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events81000-81999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events82000-82999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events83000-83999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events84000-84999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events96000-96999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events97000-97999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/tracker_hits/hard_scatter.ttbar.v1.reco.tracker_hits.events99000-99999.parquet
  - config_name: calo_hits
    data_files:
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/calo_hits/hard_scatter.ttbar.v1.reco.calo_hits.events22000-22999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/calo_hits/hard_scatter.ttbar.v1.reco.calo_hits.events24000-24999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/calo_hits/hard_scatter.ttbar.v1.reco.calo_hits.events26000-26999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/calo_hits/hard_scatter.ttbar.v1.reco.calo_hits.events34000-34999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/calo_hits/hard_scatter.ttbar.v1.reco.calo_hits.events4000-4999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/calo_hits/hard_scatter.ttbar.v1.reco.calo_hits.events40000-40999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/calo_hits/hard_scatter.ttbar.v1.reco.calo_hits.events41000-41999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/calo_hits/hard_scatter.ttbar.v1.reco.calo_hits.events42000-42999.parquet
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        https://actseos.web.cern.ch/colliderml/v0/ttbar_p0/calo_hits/hard_scatter.ttbar.v1.reco.calo_hits.events43000-43999.parquet
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ColliderML: ColliderML Top-Quark Pair Production (No Pileup)

Dataset Description

This dataset contains simulated high-energy physics collision events for top-quark pair (ttbar) production with no pileup (single interaction per event) generated using the Open Data Detector (ODD) geometry within the Key4hep and ACTS (A Common Tracking Software) frameworks, representing a generic collider detector similar to those at the HL-LHC.

Dataset Summary

  • Campaign: hard_scatter
  • Process: Top-quark pair (ttbar) production
  • Version: v1
  • Number of Events: ~100000 events
  • Pileup: 0 (no additional interactions)
  • Detector: Open Data Detector (ODD)
  • Format: Apache Parquet with list columns for variable-length data
  • License: cc-by-4.0

Supported Tasks

This dataset is designed for machine learning tasks in high-energy physics, including:

  • Particle tracking: Reconstruct charged particle trajectories from detector hits
  • Track-to-particle matching: Associate reconstructed tracks with truth particles
  • Jet tagging: Identify jets originating from top quarks, b-quarks, or light quarks
  • Energy reconstruction: Predict particle energies from calorimeter deposits
  • Physics analysis: Event classification (signal vs. background discrimination)
  • Representation learning: Study hierarchical information at different detector levels

Languages

N/A (Physics data)

Quick Start

Installation

pip install datasets pyarrow

Load First 100 Events (All Objects)

from datasets import load_dataset

# Load first 100 rows of each configuration
particles = load_dataset("OpenDataDetector/ColliderML_ttbar_pu0", "particles", split="train[:100]")
tracker_hits = load_dataset("OpenDataDetector/ColliderML_ttbar_pu0", "tracker_hits", split="train[:100]")
calo_hits = load_dataset("OpenDataDetector/ColliderML_ttbar_pu0", "calo_hits", split="train[:100]")
tracks = load_dataset("OpenDataDetector/ColliderML_ttbar_pu0", "tracks", split="train[:100]")

print(f"Loaded {len(particles)} particle events")
print(f"Loaded {len(tracker_hits)} tracker hit events")
print(f"Loaded {len(calo_hits)} calo hit events")
print(f"Loaded {len(tracks)} track events")

Load Specific Columns from First 100 Events

from datasets import load_dataset
import numpy as np

# Load only specific columns from particles
particles = load_dataset(
    "OpenDataDetector/ColliderML_ttbar_pu0",
    "particles",
    split="train[:100]",
    columns=["event_id", "px", "py", "pz", "energy", "pdg_id"]
)

# Access data
for event in particles:
    event_id = event['event_id']

    # Convert to numpy arrays
    px = np.array(event['px'])
    py = np.array(event['py'])
    pz = np.array(event['pz'])

    # Calculate transverse momentum
    pt = np.sqrt(px**2 + py**2)

    print(f"Event {event_id}: {len(px)} particles, mean pt = {pt.mean():.2f} GeV")

# Load only specific columns from tracks
tracks = load_dataset(
    "OpenDataDetector/ColliderML_ttbar_pu0",
    "tracks",
    split="train[:100]",
    columns=["event_id", "qop", "theta", "phi"]
)

# Calculate derived quantities
for event in tracks:
    qop = np.array(event['qop'])
    theta = np.array(event['theta'])

    # Compute transverse momentum from track parameters
    pt = np.abs(1.0 / qop) * np.sin(theta)
    eta = -np.log(np.tan(theta / 2.0))

    print(f"Event {event['event_id']}: {len(qop)} tracks, pt range [{pt.min():.2f}, {pt.max():.2f}] GeV")

Dataset Structure

Data Instances

Each row in the Parquet files represents a single collision event. Variable-length quantities (e.g., lists of particles, hits, tracks) are stored as Parquet list columns.

Example event structure:

{
    'event_id': 42,
    'particle_id': [0, 1, 2, 3, ...],  # List of particle IDs
    'pdg_id': [11, -11, 211, ...],     # Particle type codes
    'px': [1.2, -0.5, 3.4, ...],       # Momentum components (GeV)
    'py': [0.8, 1.1, -0.3, ...],
    'pz': [5.2, -2.1, 10.5, ...],
    'energy': [5.5, 2.3, 11.2, ...],
    # ... additional fields
}

Data Fields

The dataset contains 4 data types organized by detector hierarchy:

1. particles (Truth-level)

Truth information about generated particles before detector simulation.

Field Type Description
event_id int64 Unique event identifier
particle_id list Unique particle ID within event
pdg_id list PDG particle code (e.g., 11=electron, 13=muon, 211=pion)
mass list Particle rest mass (GeV/c²)
energy list Particle total energy (GeV)
charge list Electric charge (in units of e)
px, py, pz list Momentum components (GeV/c)
vx, vy, vz list Vertex position (mm)
time list Production time (ns)
num_tracker_hits list Number of hits in tracker
num_calo_hits list Number of hits in calorimeter
vertex_primary list Primary vertex flag (1 = hard scatter, 2,...,N = pileup)
parent_id list ID of parent particle

Typical event: ~200-500 particles per event

2. tracker_hits (Detector-level)

Digitized spatial measurements from the tracking detector (silicon sensors).

Field Type Description
event_id int64 Unique event identifier
x, y, z list Measured hit position (mm)
true_x, true_y, true_z list True (simulated) hit position before digitization (mm)
time list Hit time (ns)
particle_id list Truth particle that created this hit
volume_id list Detector volume identifier
layer_id list Detector layer number
surface_id list Sensor surface identifier
cell_id list Cell/pixel identifier
detector list Detector subsystem code

Typical event: ~2,000-5,000 hits per event

3. calo_hits (Calorimeter-level)

Energy deposits in the calorimeter system (electromagnetic + hadronic).

Field Type Description
event_id int64 Unique event identifier
detector list Calorimeter subsystem name
cell_id list Calorimeter cell identifier
total_energy list Total energy deposited in cell (GeV)
x, y, z list Cell center position (mm)
contrib_particle_ids list<list> IDs of particles contributing to this cell
contrib_energies list<list> Energy contribution from each particle (GeV)
contrib_times list<list> Time of each contribution (ns)

Note: Nested lists for contributions (one cell can have multiple particle deposits).

Typical event: ~500-1,000 calorimeter cells with deposits

4. tracks (Reconstruction-level)

Reconstructed particle tracks from pattern recognition and track fitting algorithms.

Field Type Description
event_id int64 Unique event identifier
track_id list Unique track identifier within event
majority_particle_id list Truth particle with most hits on this track
d0 list Transverse impact parameter (mm)
z0 list Longitudinal impact parameter (mm)
phi list Azimuthal angle (radians)
theta list Polar angle (radians)
qop list Charge divided by momentum (e/GeV)
hit_ids list<list> List of tracker hit IDs assigned to this track

Track parameters: Standard ACTS track representation (perigee parameters at origin).

Derived quantities:

  • Transverse momentum: pt = abs(1/qop) * sin(theta)
  • Pseudorapidity: eta = -ln(tan(theta/2))
  • Total momentum: p = abs(1/qop)

Typical event: ~50-150 reconstructed tracks per event

Data Splits

Currently, the dataset does not have predefined train/validation/test splits. Users should implement their own splitting strategy based on their use case. Recommended approach:

from sklearn.model_selection import train_test_split

# Example: 70% train, 15% validation, 15% test
all_events = list(range(100000))
train_val, test = train_test_split(all_events, test_size=0.15, random_state=42)
train, val = train_test_split(train_val, test_size=0.176, random_state=42)  # 0.176 * 0.85 ≈ 0.15

Support

For questions, issues, or feature requests:

  • Email: [email protected]
  • You can also open a discussion in the HuggingFace community panel for this dataset.

Acknowledgments

This work was supported by:

  • NERSC computing resources
  • U.S. Department of Energy, Office of Science
  • Danish Data Science Academy (DDSA)

Last updated: October 2025 Dataset version: v0