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Trigger Anomaly Detection for New Physics at the Large Hadron Collider
This dataset is a mirror of the Zenodo record: https://doi.org/10.5281/zenodo.21787779
This dataset contains Level-1 Trigger objects from the CMS experiment at the CERN Large Hadron Collider, assembled for research on unsupervised anomaly detection in the trigger. The goal of unsupervised anomaly detection in this context is the discovery of new physics. This data set does not contain new physics. It is meant for research on anomaly detectors.
In the new physics search context, recording true anomalies or simulating them is impossible, compared to other settings (e.g. industrial applications of anomaly detection) where this is commonly done. Anomaly simulation data sets are provided, but they should be used with the aforementioned caveat in mind. Aside from its high statistics, this data set uniquely provides simulations of the normal data.
normal data: zero-bias events recorded during 2025 proton–proton running (runs 396102, 398183); these events are chosen at random from all the proton-proton collisions that happen inside the CMS detector and are recorded by it.
anomaly simulations: 20 simulated signal data sets covering Higgs, multi-Higgs, SUSY and exotic scenarios from the CMS Run 3 Winter25 campaign.
normal data simulation: one simulated zero-bias-like background sample (SingleNeutrino).
The normal data has 20,887,636 events. The normal data simulation has 2,000,000 events. The 20 anomaly simulations amount to 13,012,931 events.
Each event provides particle level and event information, as recorded by the trigger. The data is published pre-partitioned into training, validation and test splits: the zero-bias data 60/20/20, the simulated samples 60/40 between validation and test. All the feature values are in the trigger-native format of hardware integers.
Specific technical data can be found in the github repo that was used to produce this data: https://github.com/bb511/adl1t_datamaker
Comparison with other algorithms
The level-1 trigger contains around 180 algorithms that take data like the one in this
record and output a decision. These algorithms were applied to every event in the
presented data sets as well. Their results are in the -seeds configs and can be used
to do comparative studies with other live algorithms currently running in the CMS
trigger. Skip them if you want kinematics alone and do not want to compare your anomaly
detector with the rest of the algorithms.
Row i of <data set>-seeds is row i of <data set>, which is the correspondence
that always holds. Neither column is a key on its own: every event the standard
preprocessing dropped carries order = -1, and event cycles over a hundred values in
ggH-suep-decay, haa-4b-ma15 and smj-case-A. Among the rows with order >= 0 it is
unique within a split, so a filter or a shuffle can be undone by joining on order once
those rows are set aside.
Loading
Every data set is a configuration of its own, and every one of them has a -seeds twin
holding the other algorithm decisions for the same events in the same order.
from datasets import load_dataset
normal = load_dataset("podagiu/anomaly_detection_cmsl1t", "ZB_run396102", split="train")
signal = load_dataset("podagiu/anomaly_detection_cmsl1t", "WtoTauto3Mu", split="validation")
menu = load_dataset("podagiu/anomaly_detection_cmsl1t", "WtoTauto3Mu-seeds", split="validation")
HuggingFace calls the middle split validation while our files call it 'valid'. We also
include a dataloader that we used for performing anomaly detection trigger development
on this data. It reads the data, applies our cuts and normalisation, and stacks the
collections into pytorch tensors that can be directly fed into models.
import sys
from huggingface_hub import snapshot_download
from hydra import compose, initialize_config_dir
from hydra.utils import instantiate
record = snapshot_download("podagiu/anomaly_detection_cmsl1t", repo_type="dataset")
sys.path.insert(0, record) # the configs name loader.*, so the record has to be importable
with initialize_config_dir(config_dir=record + "/configs", version_base=None):
cfg = compose("config", overrides=["paths.root_dir=" + record])
data = instantiate(cfg.data)
data.prepare()
train = data.load("train")
prepare reads the whole record and caches each stage under ./cache, which the
ADL1T_CACHE environment variable moves elsewhere; allow it a few times the record's
size on disk. train then has x, the model input, of shape (events, 39, 3) under the
basis configuration, its padding mask, whether the event passed ANY other algorithm
in the trigger l1bit and the label y (0 for zerobias, > 0 for anomalies, < 0 for
zerobias simulation). data.load_aux("valid") returns the same for every simulated
sample. The pipeline needs python 3.10 or newer with awkward, pyarrow, numpy,
torch, omegaconf and hydra-core, which pip install -r requirements.txt at the
record's root installs. If you would just rather read the raw data, you need none of
the above dependencies. Just call load_dataset.
Layout
data/<data set>/<split>-NNNNN-of-NNNNN.parquet
data/<data set>/seeds/<split>-NNNNN-of-NNNNN.parquet
loader/
configs/
requirements.txt
One row is one event. The four object collections are jagged, holding one entry per in-time object up to the global trigger's capacity of 8 muons, 12 jets, 12 e-gammas and 12 taus, with no padding and no truncation. The energy sums are collections too, of one entry each. The event information, the trigger's verdict and every seed are plain values.
Columns
| column | holds |
|---|---|
<collection>_<branch> |
one collection's features, e.g. muons_muonIEt or jets_jetIEta. The collections are muons, jets, egammas, taus and the energy sums ET, HT, MET, MHT, FET, FHT, and the branch names are the trigger's own |
run, lumi, event, bx, orbit, time, nPV_True |
event information, carried without a prefix |
split, order |
the published partition and the position within it, described below |
L1bit |
whether the trigger menu accepted the event, i.e. the OR over its algorithms |
dataset |
the data set the row came from, so that a concatenation stays self-describing |
label |
0 for zero bias, negative for a simulated background, positive for a signal |
A column prefixed by a collection is a list, and every other column is a plain
value. The collections have one entry per object in the event. The energy sums have a
single entry (list with one value). Everything else holds one value: row["L1bit"] is
True, row["event"] is an integer, and ds.filter(lambda r: r["L1bit"]) selects the
events the trigger accepted. A -seeds config has one boolean column per trigger
algorithm and four other columns: L1bit, dataset, event and order.
Data sets
| config | label | train | valid | test |
|---|---|---|---|---|
GluGluHTo2B_Par-MH-125 |
1 | 293,231 | 195,736 | |
GluGluHto2G_Par-MH-125 |
2 | 598,666 | 399,132 | |
GluGluHto2G_Par-MH-90 |
3 | 443,336 | 295,444 | |
GluGluHto2Tau_Par-MH-125 |
4 | 35,706 | 23,805 | |
GluGlutoHHto2B2WtoLNu2Q_Par-c2-0-kl-1-kt-1 |
5 | 179,378 | 119,714 | |
HHHto4B2Tau_Par-c3-0-d4-0 |
6 | 1,200,063 | 800,123 | |
HHHto6B_Par-c3-0-d4-0 |
7 | 383,502 | 255,858 | |
SUSYGluGluToBBHTo2B_Par-M-1200 |
8 | 29,588 | 19,676 | |
SUSYGluGluToBBHToBB_Par-M-120 |
9 | 299,996 | 200,004 | |
SUSYGluGluToBBHToBB_Par-M-350 |
10 | 119,971 | 80,029 | |
SUSYGluGluToBBHToBB_Par-M-600 |
11 | 30,000 | 20,000 | |
SingleNeutrino_E-10-gun |
-1 | 1,200,002 | 799,998 | |
TTHTo2C_Par-MH-125 |
12 | 1,199,636 | 800,464 | |
TTHto2B_Par-MH-125 |
13 | 1,200,165 | 800,225 | |
VBFHTo2C_Par-MH-125 |
14 | 299,566 | 199,720 | |
VBFHto2B_Par-MH-125 |
15 | 299,564 | 199,733 | |
VBFHto2Tau_Par-MH-125 |
16 | 955,535 | 636,965 | |
WtoTauto3Mu |
17 | 60,002 | 39,998 | |
ZB_run396102 |
0 | 6,220,470 | 2,071,292 | 2,072,007 |
ZB_run398183 |
0 | 6,312,116 | 2,106,228 | 2,105,523 |
ggH-suep-decay |
18 | 59,640 | 39,760 | |
haa-4b-ma15 |
19 | 59,942 | 39,958 | |
smj-case-A |
20 | 59,458 | 39,642 |
Units
Each feature of each object has values that are integer hardware units, as the trigger produces them. Nothing in the files is scaled. Multiply by the following to get GeV, radians and pseudorapidity:
| collection | Et | eta | phi |
|---|---|---|---|
| muons | 0.5 GeV | 0.010875 | 0.0109083 rad |
| jets | 0.5 GeV | 0.0435 | 0.0436332 rad |
| e-gammas | 0.5 GeV | 0.0435 | 0.0436332 rad |
| taus | 0.5 GeV | 0.0435 | 0.0436332 rad |
| ET, HT | 0.5 GeV | ||
| MET, MHT, FET, FHT | 0.5 GeV | 0.0436332 rad |
The decimals are rounded. The steps are exact fractions: calorimeter eta is 0.0870/2,
muon eta is 0.0870/8, calorimeter phi is 2pi/144, and muon phi is 2pi/576.
muons_muonIEtaAtVtx and muons_muonIPhiAtVtx take the same scales as muon eta and
phi. Two energies are missing from the table: muons_muonIEtUnconstrained is 1 GeV per
unit rather than 0.5, and jets_jetRawEt has no documented scale. Quality, charge,
isolation, index and tower-count fields are already integers and unscaled, as is every
event information field and every seed.
Caveats
Ordering. Objects arrive in the trigger's readout order, which is ET-descending for the calorimeter objects and not for the muons. The shipped loader sorts objects by ET before processing them.
The menu differs between data and simulation. Zero bias data has 183 algorithm columns and the simulations have 161, of which 147 are shared. Additionally, the order of the other trigger algorithm decisions is not the same between zerobias and simulations.
nPV_True has two types. It is float32 in zero bias and int32 in simulation.
Simulation carries no beam coordinates. Every simulated sample has run of 1, bx
of 4294967295 and orbit of 18446744073709551615, the all-ones codes of their types, in
place of the values a collision would have. Only the zero bias has non-trivial values in
these fields.
jetRawEt is zero throughout the zero-bias data. The branch is unfilled in original
data ntuples, though it has real values in simulation.
Standard preprocessing
Multiple studies were done internally at CERN on this data set. A number of conventional
preprocessing steps were applied in each of these studies. Therefore the record contains
two columns that the raw data does not: split, so a file separated from its directory
is still self-describing, and order, the position in that ordering, which is -1 for
the events that the conventional preprocessing removed. Links to the papers detailing
these studies will be attached here once these studies become public.
The split was drawn once with NumPy's PCG64 generator seeded with 42, over the two
zero-bias runs concatenated in the order ZB_run396102 then ZB_run398183.
A split can span two configs. The two zero-bias runs were permuted together. Their
training rows interleave and order counts across the whole split rather than within
one run. To rebuild the same order as in previous studies, read both zero-bias configs,
concatenate them, then stable-sort by order with the -1 rows left at the end.
Concatenating one run after the other gives the right rows in the wrong order.
The pipeline in loader/ goes through the standard preprocessing steps. In the four
stages the studies used: read the tables into one array per collection, drop the events
saturated in ET and mask the objects above a cut, fit the normalisation on the training
split alone and apply it to every other split, then pad each collection to a fixed
number of constituents and stack them into one tensor. That object cut is Et < 511 for
muons, e-gammas, jets and taus; 511 is the all-ones code of the 9-bit muon, e-gamma and
tau energies, so this cut removes saturated objects. For the jet energy, the full bit
width is 11, which would saturate at 2047. The loader cuts any jets above 255.5 GeV, and
not at the hardware limit. The events cut by this pipeline have the order set to -1:
run over the zero bias it removes the 457 events marked -1, 0.0022% of them.
Provenance
Zero-bias data: CMS, 2025, runs 396102, 398183. Simulated samples: CMS Run 3 Winter25 campaign. The values are the Level-1 trigger's own reconstructed objects rather than offline reconstruction.
Citation
Cite the Zenodo record that this dataset mirrors. The data descriptor is not published yet; its citation will be added here once it is.
@dataset{cms_l1t_anomaly_2026,
author = {{CMS Collaboration}},
title = {Trigger Anomaly Detection for New Physics at the Large Hadron Collider},
year = {2026},
publisher = {Zenodo},
version = {1.0},
doi = {10.5281/zenodo.21787779},
url = {https://doi.org/10.5281/zenodo.21787779}
}
Licence
CC0 1.0, a public domain dedication with no restrictions on reuse. See LICENSE.
Citation by DOI is requested as a courtesy, not required.
Contact
Questions and problems are welcome as a discussion on this dataset's page, or as an issue on the repository that produced it: https://github.com/bb511/adl1t_datamaker.
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