SEARCH FOR LONG-LIVED PARTICLES IN THE ATLAS HADRONIC CALORIMETER IN ASSOCIATION WITH
LEPTONS OR JETS
Victoria Sánchez Sebastián
on behalf of the CalRatio analysis team
INTRODUCTION
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We are performing a search for neutral LLPs decaying hadronically in the calorimeter produced in association with leptons or jets, three channels:
➤ Displaced jet (DJ) + 2 jets
➤ DJ + leptons:
• DJ + W ( or )
• DJ + Z ( or )
All these channels use the NN displaced jet tagger from the two CalRatio jets analysis to identify LLPs [ref]
Signature-driven search using several benchmark models Main backgrounds: SM multijets, non-collision
backgrounds, W/Z+jets, single and pair production of top quarks
→ eν μν
→ ee μμ
ggF: Φ( → SS)
LLP
INTRODUCTION
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ggF: Φ( → SS)
DJ+2jets
We are performing a search for neutral LLPs decaying hadronically in the calorimeter produced in association with leptons or jets, three channels:
➤ Displaced jet (DJ) + 2 jets
➤ DJ + leptons:
• DJ + W ( or )
• DJ + Z ( or )
All these channels use the NN displaced jet tagger from the two CalRatio jets analysis to identify LLPs [ref]
Signature-driven search using several benchmark models Main backgrounds: SM multijets, non-collision
backgrounds, W/Z+jets, single and pair production of top quarks
→ eν μν
→ ee μμ
INTRODUCTION
2
CalRatio+X EB request - date V. Sánchez Sebastián
DJ+leptons
We are performing a search for neutral LLPs decaying hadronically in the calorimeter produced in association with leptons or jets, three channels:
➤ Displaced jet (DJ) + 2 jets
➤ DJ + leptons:
• DJ + W ( or )
• DJ + Z ( or )
All these channels use the NN displaced jet tagger from the two CalRatio jets analysis to identify LLPs [ref]
Signature-driven search using several benchmark models Main backgrounds: SM multijets, non-collision
backgrounds, W/Z+jets, single and pair production of top quarks
→ eν μν
→ ee μμ
We are performing
INTRODUCTION
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DISPLACED JET + LEPTONS CHANNELS
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Signature is at least one displaced jet in the Calorimeter + prompt Z/W boson, benefits from:
➤ Single displaced object search
➤ Use SM lepton triggers: high efficiency, no need of specific trigger
➤ Use same framework and tools (e.g. previous analysis’ per-jet NN) developed for two CalRatio jets analysis
Main backgrounds are:
➤ DJ+Z: Z+jets
➤ DJ+W: Z+jets, W+jets, ttbar and Wt
ANALYSIS OVERVIEW
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Lepton triggers
DJ+W: single lepton DJ+Z: single OR di-lepton
BDT
Separates signal & bkg Multiple trainings
depending on boost and kinematics
Preselection
&
Event Cleaning
Final selection
Signal
significance
&
limit-setting
ABCD method
(data-driven bkg estimation)
key: Filtering, Calculation
LEPTON TRIGGERS
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Lowest unprescaled single and dilepton triggers for each year used: only triggers that were fully active and
unprescaled during the full year are considered (full list in backup). In MC16a, different trigger requirement in 2015 and 2016 accounted for using “RandomRunNumber” obtained after PRW.
➤ DJ+W: single lepton triggers
➤ DJ+Z: single OR di lepton triggers
Lepton triggers OR CalRatio triggers increase ~1% signal efficiency, decided not to use them
Preselection for DJ+leptons channels:
➤ Lepton triggers
➤ Z or W reconstruction (see box on the right): orthogonal selections + common preselection:
➤ At least one trackless (min ) un-calibrated jet in the event with GeV: condition required to store events that fire lepton triggers in EXOT15
➤ Event > 0.5 (calculated over clean jets)
➤ DJ preselection: clean jet with highest low-ET NN signal score ( ), require
• Trackless: min , and GeV
• Low-ET NN signal score > 0.4
• Jet cleaning cuts: logRatio > -1, -3 ns < time < 15 ns, not in Tile Calorimeter gap region
ΔR(jet, tracks) > 0.2 pT > 40
∑ ΔRmin(jet,tracks)
jsig1,l ΔR(jet, tracks) > 0.2 pT > 50
jsig1,l jsig1,l
PRESELECTION AND EVENT CLEANING
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DJ + W: reconstruction:
• Exactly one lepton
• > 50 GeV
• lepton GeV
• GeV
DJ + Z: reconstruction:
• 2 OSSF leptons
• >60 GeV
• Leading lepton > 25 GeV
• Subleading lepton > 10 GeV
W → lν MT(lepton,MET)
pT > 27 ETmiss > 30
Z → l+l−
M(l+, l−)
pT
pT
placeholder of two
preselection plots
A set of boosted decision trees are trained using XGBoost after preselection:
➤ Separate signal from background
➤ One of the two axis of ABCD plane Similar architecture and development:
➤ Input variables: combination of DJ, lepton and event level variables
➤ Training uses MC for signal and background:
• Odd-numbered events for signal, background all events included
• Signal and background input samples are randomly split into train (80%) and validation (20%) samples
• DJ+W: two trainings, signal W+ALP / low mass W+ , against combination of Z+jets, W+jets, Wt and (+ high mass selection, work-in-progress)
• DJ+Z: one training, Z+ and high mass combination, against Z+jets (+ 2 low mass selections, work-in-progress)
Φ → SS t t ¯
Φ → SS Φ → ZZ
dPER EVENT BDT
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Two trainings according to event topology and kinematics:
➤ W+ALP: all signal mass points
➤ Low mass W+ , GeV
Same input variables: differences due to particle boosts and model topology (full list in backup)
Φ( → SS ) m
Φ≤ 200
BDT: DJ+W CHANNEL
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blinded blinded
Example input variables BDT score distributions
Very similar performance test and training samples: no overfitting
Very different feature importance between two trainings due to different
behavior
…
BDT: DJ+Z CHANNEL
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High-ET training performed, includes combination of signal samples:
➤ Z+ ( GeV)
➤ ( GeV)
Φ → SS m
Φ≥ 400 Φ → ZZ
dm
Φ≥ 250
Mariia to provide a
few plots
FINAL SELECTION OPTIMIZATION
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Test additional cuts in ABCD plane to increase in
reg. A and reduce signal contamination in B, C & D
S/ B
Find optimal region A boundaries
Background in A taken
from ABCD method Control stats
error in A Maximize S/ B Control signal leakage
Example variations for W+HSS selection
Final selection marked in bold
Optimization performed using full Run 2 data
➤ For each selection, define ABCD plane with: BDT score vs , and test multiple cuts to define region A
➤ Calculate expected number of events in region A using ABCD method estimation from B, C & D
➤ Keep selections with: low stat error in A (<50%), more than 50% of signal in region A, and maximize
∑ ΔRmin(jet,tracks)
S/ B
blinded
∑jets
ΔRmin(tracks)
W+HSS BDT score
DJ+W preselection, Full Run 2
Correlation: -0.018
Correlation: -0.007 Construct ABCD plane with
2 uncorrelated variables
ABCD plane
FINAL SELECTIONS
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W+ALP selection: W+HSS selection: DJ+Z high-ET selection:
➤ Final selections for DJ+lepton channels (after preselection) obtained with the selection optimization procedure:
DJ+W channel:
As in previous CalRatio analyses, use the modified ABCD method for background estimation. Simulataneous S+B likelihood fit to all regions. Pair of uncorrelated variables used:
➤ BDT score
➤
ABCD method is tested in validation regions (VRs), orthogonal to signal region A. Checked that there is low signal contamination: reduced a factor of 10 between expected in region A and VRs.
∑ ΔRmin(jet,tracks)
S / B
ABCD METHOD VALIDATION
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VR-CD for W+ALP selection
Define region A’ boundaries
Move boundaries across VR and compare observed and expected number of events in
A’ using ABCD method
Agreement within statistical errors
Reg A cut in final selection
ABCD METHOD VALIDATION
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ABCD plane validation for DJ+W WHSS selection and DJ+Z high-ET selection:
VR-CD for W+HSS selection
VR-CD for DJ+Z high-ET selection
Non-closure in two extremes,
low stats
Reg A cut in final selection
Reg A cut in final selection
EXPECTED LIMITS: DJ + W
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Region A signal efficiency: First limits for this model!
Does not improve 2CR
FR2 limits Improve 2CR FR2 limit (but
different production mode)
EXPECTED LIMITS: DJ + Z, HIGH-ET SELECTION
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Region A signal efficiency:
Improve 2CR FR2 limit (but different production mode)
Generally, factor 10 improvement wrt previous CR+Z analysis limit for similar mass points (not exactly
the same in some cases)
(CR+Z analysis used 2015+2016 data)
BACKUP SLIDES
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LEPTON TRIGGERS
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