long lived particle decay searches @ lhc · (r-hadron cloud model) expected observed status:...

Long lived particle decay searches @ LHC

Simone Gennai on behalf of the

ATLAS, CMS and LHCb Collaborations

La Thuile 2018 Simone.Gennai@cern.ch

Why searching for LLP?2

Standard Model includes quite few LLP it is natural to assume they can populate BSM theories as well

we cannot exclude we have not seen susy because we were concentrating on prompt particle decays!

There are several models that can predict LLP Split susy

Stealth susy

RPV susy

Hidden valley (HV), dark bosons, etc. etc.

From the experimental point of view they give raise to different signatures depending on the number of particles in the final state, and their spectrum in pT

A non zero lifetime adds a further dimension in the sea of possible topologies to consider

this poses yet another challenge for those final states that requires ad hoc reconstruction techniques

Excellent review in October 2017: https://indico.cern.ch/event/649760/timetable/

Data analyzed

LHC performed very well in Run2! more than 40/fb collected in 2015 and 2016

I will concentrate mostly on analysis using this data sample

I will deal with decaying particles i.e. no HSCP will be discussed

anyway you can find them in the back up …

Disclaimer 4

Particles with a similar lifetime may leave different signals in different experiments

on the other hand different phenomenological models can give similar signature

I will try to group similar signatures together even if different experiments may have considered different models and the results may not always be directly comparable

1m 2m 3m 4m

Reconstructing displaced particles 5

Reconstructing displaced particles 6

Efficiency usually depends on: decay distance, time distribution, speed

Acceptance may change as a function of the mother particle mass due to the boost

Excellent knowledge of the detector material is required

Re-interpretation of prompt searches

"Poor man" approach do not need any special reconstruction

consider loss in acceptance due to non zero lifetime

or category migration due to the presence of more b-like tagged particles

Impact measured in terms of exclusion limits an example from CMS: search for split supersymmetry

SUS-16-038

Displaced signal topologies 8

HSCPDisplaced Di-leptons

Displaced leptons

Disappearing Tracks

Displaced Jets

Displaced Photons

Displaced Conversions

Graphic Credit: Jamie Antonelli

Different signatures may requires special triggers and offline reconstruction

narrow jets, displaced and delayed calorimeter/muon reconstruction

Large impact parameter tracks

In many cases non “standard" background from cosmic rays, beam induced events,detector material interactions

Displacedvertex

Displaced leptons

Disappearing Tracks

Displaced Jets

Displaced Photons

Disappearing tracks 9

Displacedvertex

N.B. 1 ns corresponds to 30 cm

ATLAS and CMS Disappearing tracks 10

CERN-EP-2017-179

EXO-16-044

Chargino and neutralino production plus one or more jets triggering on the rest of the events

Very few events expected, almost background free…

Displaced leptons

Disappearing Tracks

Displaced Jets

Displaced Photons

Displaced vertices 11

Displacedvertex

Broad class of signatures Massive particles decaying with displaced vertices associated to large number of track based invariant mass

ATALS looks for long lived gluinos in split susy

CMS aims to a model independent search and interprets the results in a coupleof benchmark scenarios one being stop production in RPV decays to b-quarks+leptons

makes use of an ad hoc trigger to select jets associated to displaced tracks

One of the main background coming from interactions with the detector material.

detailed maps with the material descriptions are used to compute the interaction probability

ATLAS and CMS Displaced vertices and appearing jets 12

CERN-EP-2017-202

EXO-16-003

ATLAS Displaced Jets (from Run I)13

PHYSICAL REVIEW D 92, 012010 (2015)

Different models considered with a variable number of jets in the final state (looking for longer lifetime wrt the previous slide)

Hidden valley scalar and large mass mediator

Stealth susy

Differently from Run 2 analysis, this also exploits the presence of secondary vertices reconstructed in the muon system (larger lifetimes considered) Trigger based on:

clustered tracks in the muon spectrometer

or presence of jet and missing energy

Hidden valley signatures LHCb looks for a b-jet pair from a hidden valley pion

Sensitivity depends on the position of the displaced vertex fit performed on the diet invariant mass in bins of the distance from the origin of the displaced vertex

14LHCb Displaced vertices and appearing jets

LHCb-PAPER-2016-065

LHCb explores few different scenarios RPV neutralino decays and production of intermediate particles from Higgs boson decay

looking for a displaced vertex with a reconstructed muon plus jet

15LHCb Displaced vertices and leptons

LHCb-PAPER-2016-047

Displaced leptons

Disappearing Tracks

Displaced Jets

Displaced Photons

Displaced Leptons 16

Displacedvertex

ATLAS looking for the presence of leptons associated to a displaced multitrack secondary vertex

associated to split susy models

CMS in the most recent analysis looks for electron-muon final state from stop decays

associated to RPV susy models

lower limit on the m_stop with respect to slide 12

17Displaced leptons ATLAS and CMS

CERN-EP-2015-065

EXO-16-022

ATLAS displaced di-leptonsMain production mechanism is through Higgs decay to hidden fermions which decays to dark photons

two different signal benchmarks considered with 2 or 4 dark photons

Events categorized depending on the number of reconstructedmuon pairs

N.B. due to large boost, events with 4 dark photons are still reconstructed as two lepton-jet objects

ATLAS-CONF-2016-042

CMS displaced di-leptons 19

HIG-16-035

EXO-14-012

Two different analysis one with RunI data and one with 2015 data EXO-14-012 is looking for a dark-photon like signature as well as displaced muons from long lived neutralinos in RPV models

HIG-16-035 specifically deals with dark-photons models, even if with limited lifetime reach

HIG-16-035

EXO-14-012

LHCb displaced di-leptons 20

LHCb-PAPER-2017-038

PRD 95 (2017), 071101 (R)

LHCb can probe much lower mass regions than ATLAS and CMS several benchmark models considered

Axions, inflaton and dark photons

Displaced leptons

Disappearing Tracks

Displaced Jets

Displaced Photons

Displaced photons and jets 21

Displacedvertex

ATLAS Non-pointing/Delayed photons22

CERN-EP-2014-215

Neutral LLP decaying to photons that do not point to the primary vertex or delayed wrt the bunch crossing

Assuming GMSB susy scenario

presence of photons and MET

CMS Non-pointing/Delayed photons

Similar GMSB model as in ATLAS This allows an apple-to-apple comparison

Analysis mostly relying on the ecal time measurement

EXO-12-035

ATLAS "appearing" Jets in the calorimeters24

ATLAS-CONF-2016-103

Looking for showers initiated in the hadronic calorimeter special jet reconstructions, to cope with the shower initiatedlater than usual

basically looking for narrower than usual jets, low electromagnetic fraction energy and no tracks associated

Similar model as one already discussed in slide 13

Displaced leptons

Disappearing Tracks

Displaced Jets

Displaced Photons

Stopped Particles 25

Displacedvertex

ATLAS Stopped ParticlesLooking for R-hadrons stopped in the calorimeter

triggering on empty bunch crossings, low pT jet and ET-missing

several models considered in the results interpretation

PRD 88 (2013) 112003

CMS Stopped particlesR-hadrons which travel up to the calorimeter and then decay

analysis consider both hadronic decays in the calorimeters and decays into muons in the muon chambers

events recorded with special triggers focusing on out of bunch crossings activity

CERN-EP-2017-330

Summary plots 28

[ns]τ2−10 1−10 1 10 210 310 410

3000ExpectedObserved

)-1=13 TeV, 36 fbs (arXiv:1712.02332 missTJets+E

))-1=13 TeV, 33 fbs (arXiv:1710.04901Displaced vertices )-1=13 TeV, 3.2 fbs (arXiv:1604.04520Pixel dE/dx

)-1=13 TeV, 3.2 fbs (arXiv:1606.05129Stable charged )-1=7,8 TeV, 5.0,23 fbs (arXiv:1310.6584Stopped gluino

95% CL limits not includedtheory

SUSYσ

PreliminaryATLAS Status: December 2017 = 100 GeV

0χ∼ ; m

10χ∼ qq → (R-hadron) g~

=1)γβ=0, η(r for Beampipe Inner Detector Calo MS

[m]τc

3−10 2−10 1−10 1 10 210 310 410

[ns]τ

1−10 1 10

]1± χ∼

1000Expected limitsObserved limits

arXiv:1712.02118Disappearing track (pixel-only)

arXiv:1506.05332Pixel dE/dx arXiv:1411.6795Stable charged

arXiv:1310.3675Disappearing track

95% CL limits. not includedtheory

SUSYσ

=13 TeVs, -136 fb

=8 TeVs, -118.4-20.3 fb

PreliminaryATLAS

Status: December 2017]0W~[~10χ∼ ±π → ]±W~[~1

±χ∼

=1)γβ=0, η(r for Inner Detector Calo MSSt

[m]τc2−10 1−10 1 10

10�6 10�4 10�2 100 102 104 106 108 1010 1012 1014

c⌧ [m]

(⌘ = 0, �� = 1)

CMS Preliminary 13–39 fb�1 (13 TeV)

eg ! qq�0 (BR=100%)(R-hadron cloud model)

Expected

Observed

Status: February 2018

Jets + pmissT , arXiv:1802.02110

m�0 = 100 GeV, charge suppressedJets + pmiss

T , arXiv:1802.02110meg � m�0 = 100 GeV, charge suppressed

Stopped gluino, arXiv:1801.00359meg � m�0 > 160 GeV, fegg = 0.1

HSCP, CMS-PAS-EXO-16-036fegg = 0.1

10�5 10�3 10�1 101 103 105 107 109 1011 1013 1015

⌧ [ns]

ConclusionsLong lived particle search is a tough problem since detector is optimized for prompt decays.

still, they are becoming more and more popular at LHC

different place space probed with different detectors in different experiments

very nice redundancy of studies in few cases

this also means that it is more difficult to compare results and sensitivity

We have enthusiastic dedicated (but small) team tackling it in creative ways

A lot of work on going in defining framework for easier recasting of results in different benchmark scenarios

Back up 30

Displaced leptons

Disappearing Tracks

Displaced Jets

Displaced Photons

Stopped Particles 31

Displacedvertex

La Thuile 2018 Simone.Gennai@cern.chLLP Workshop | Karri Folan DiPetrillo | 18.10.2017

Pixel + Tile Calorimeter 29

Make a mass estimate using ‣ Pixel dE/dx ‣ Tile time of flight

PLB 760 (2016) 647-66513 TeV 3.2 fb-1

ToF from Muon Spectrometer not yet used in Run 2!

JHEP 01 (2015) 0688 TeV 19.1 fb-1

Tile cell timing resolution: 1.3-2.5 ns after calibration ! resolution: $(!)~ 0.1

HSCP ATLAS 32

HSCP CMSAnalysis with 12.9/fb from Run2

looking for R-hadron-like as well as lepton-like models

two categories

tracker only analysis, using only dE/dX

tracker+muon analysis, using dE/dX and TOF

trigger used: both muon and ETM based triggers

EXO-16-036

MSCP LHCB 34

(shamelessly stolen from Martino’s talk at previous LLP workshop)

Carlos Vazquez Sierra 2nd LHC LLP Community Workshop (Trieste) October 18, 2017 35 / 29

Stable : can pass through the mu-stations

smaller dE/dX

Longer life time

Absence of Cherenkov signal

Models:

susy stau mGMB

long lived with m>100 GeV

Dark Photons LHCb future35

Future CMS 36

Reinterpretation 37

LLP Workshop | Karri Folan DiPetrillo | 18.10.2017

How do we trigger on these objects?

ATLAS trigger basics ‣ L1: calorimeter & muon information ‣ HLT: e/µ/"/#/jets/MET ‣ limited tracking info at HLT ‣ typically d0 requirements on e/µ

very hard

very easy

1. Design your owndisplaced lepton jets:

“narrow scan” and “cal ratio”

2. Be sneakydisplaced e: " trigger

displaced µ: Muon Spectrometer only trigger

3. Be luckyInner Detector displaced

vertices: multi-jet/MET

LLP Strategies

Is there room for improvement? Many HLT ideas limited by L1 constraints

LLP Workshop | Karri Folan DiPetrillo | 18.10.2017

How do we reconstruct these signatures?

Lots of work in non-standard reconstruction ‣ Pixel tracklets ‣ Large radius tracking ‣ Slow muons ‣ Secondary Vertex finding

These methods are difficult, but essential ‣ computationally expensive ‣ require running on raw data ‣ filter out events using special data streams ‣ so we can run our non-standard reconstruction a single time

long lived particle decay searches @ lhc · (r-hadron cloud model) expected observed status:...

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