a general search for new phenomenascaron/talks/heralhctalk.pdf · 2011-12-07 · a general search...

A general search A general search for new for new

phenomenaphenomenaHERAHERA-- LHC WORKSHOPLHC WORKSHOPOktoberOktober 20042004

Sascha Caron (NIKHEF)

o Idea and motivation o A general search at H1 (and the LHC?)o Important ingredients for a SM predictiono Summary

Searches

Sascha Caron (NIKHEF) at HERA-LHC workshop2

Why is this interesting for the Why is this interesting for the workshop?workshop?

• LHC physics may also profit from data analysis techniques used at HERA

• HERA data is well understood and could better be used for model tuning

• Do usual LO+PS Monte Carlos work within this approach?


Idea and MotivationIdea and MotivationQuestion: Are there any new phenomena hidden in the data?Are there any new phenomena hidden in the data?

Solutions:Check if the data is described by the SM prediction(or search for deviations between data and SM prediction)

• Test of (BSM) models by searching for deviations in many specific data sub-sets

• (Global) fits to the data to check if the picture is consistent

• Measure final states and compare with the SM expectation

• Search systematically for deviations, e.g. with a search algorithm


How can weoptimize thediscovery potential?

Do we know what we want to look for?

Are we sensitive to the unexpected?


In how many final states do we In how many final states do we search at the LHC?search at the LHC?

Number of final states per BSM model:(numbers are derived by counting on an afternoon and should not be taken too seriously)Excited Fermions: about 20, e.g. ph-j, j-j, e-ph-jet,4th generation and compositeness: about 10-15Leptoquarks: about 20W’ Z’, new gauge bosons etc. : 20-40 ?Heavy quarks and leptons: 10? e.g. e-e-e-e-e-e, l-l-j-j-j-jDynamical symmetry breaking: 50? e.g. W-W, ZZ, toptop, bbjj, lllv,bjll, Ztop, Wb, Htop, …Extra Dimensions and Black Holes: 20 + very high pt final states

+ many more + SUSY + …= approx 100-500 final states

We measure at about 10 particles (e±, μ±, τ±, jet, b-jet, photon, neutrino)

about 6000-40000 Final States!!(depends if you distinguish charge etc.)


A StrategyA StrategySearch for deviations in all final states (H1 General Search)

• They are all interesting Either as a background or as a signal

• Helps to find the origin of a deviation (experimental, Monte Carlo prediction or new physics?)

• Needs reliable prediction for all final states (or check if predictionsare globally consistent)

Need to explore more (sophisticated) data analysis techniques

• Why not do the search with a search algorithm ?(DØ Sleuth: Idea to automatise a search , H1 General Search: Develop a simple and powerful strategy)


General Search for new General Search for new phenomena at HERAphenomena at HERA

o HERA1 data (1994-2000, L = 117 pb-1)HERA2 analysis is used as a watchdog

o Investigate all final state topologies in epcollisions (in 1 coherent analysis)Data is classified into exclusive channels (e.g. e-j)

o Considered particles: electron, muon, photon, jet (inv KT), neutrino

o Common phase space for all particles: PT > 20 GeV and 10o< θ < 140o


What is the SM?What is the SM?•• The SM: The SM:

Set of leading order ME + Set of leading order ME + PartonParton shower Monte Carlos +shower Monte Carlos +assigned theoretical uncertainties + NLO K factorsassigned theoretical uncertainties + NLO K factors

Used are standard MC parameter settings (and pparp(64)=4)which are almost independent of the data• Photoproduction: Pythia6.1 (k=1.2 for > 1jet production) • NC DIS: Rapgap (k=1.2 for > 1jet production)• CC DIS: Django-Ariadne (k=1.2 for > 1jet production)• QED Compton: Wabgen• EW dilepton: Grape• W production: EPVEC (reweighted to NLO calculation)

Theoretical uncertainties assigned to the generator level process (e.g. 15% for photoproduction of jets and 10% for DIS)Additional uncertainty of 20% added for each jet produced by parton

showers (checked with low PT data)


A general Search for A general Search for new phenomenanew phenomena

• Event yields for HERA 1 data(all channels with SM exp.> 0.01 event)

• Good agreement for(almost) all channels

even Multi-jet channels


Search for deviationsSearch for deviationsSearch for deviations between data andSM prediction in 1 dim. Distributions (Mall and ΣPT)

Check all connected regions with a size ≥ resolution in a histogram, i.e. calculate the probability p that data agrees with the SM



Check all connected regions with a size ≥ resolution in a histogram, i.e. calculate the probability p that data agrees with the SMRegion of greatest interest is the one with the smallest p

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Check all connected regions with a size ≥ resolution in a histogram, i.e. calculate the probability p that data agrees with the SMRegion of greatest interest is the one with the smallest p

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DistributionsallH1 General Search - M

InvestigateMall and ΣPT distributions

Find in each channelthe region with thegreatest deviation


InvestigateMall and ΣPT distributions

Find in each channelthe region with thegreatest deviation

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H1 Data

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DistributionsT PΣH1 General Search -


Quantify the Quantify the deviationsdeviations

Derive for each event class the probability P to observea deviation anywhere in the spectrum as large as found inthe data

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min minnumber of pseudo H with p <p in dataˆnumber of pseudo H

P =

Dice pseudo Histograms H according to probability density functionof the expectations


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Quantify the Quantify the deviationsdeviations

Derive for each event class the probability P to observea deviation anywhere in the spectrum as large as found inthe data

Repeat the whole analysis with many MC (pseudo data) experiments each with the H1 luminosity

Smallest P found inµ-jet-ν, e-jet and e-echannels

About 3% (Σ PT) and 25% (Mall) ofMC experiments have a deviationlarger than that of µ-j-ν final state

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^


Does this make any sense?

Test sensitivity of the analysis by generating pseudo data usingBSM predictions

Dice a data set and run the algorithm

Signals are found where they shouldbe

(plots from M. Wessels Ph. D. thesis)


SensitivityMake BSM pseudo data sets andderive average P values

Found sensitivity comparable tothat of dedicated searches


SummarySummary

)o (φ

-150-100-50050100150

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A general search might bea good solution to exploit the discovery potential at LHC

Unexpected physics may be found

The analysis of many final states helps to find the origin of effects

A MC mixture can do a good job to representthe SM in this case

A H1 event found in the ejjjj channelwith a invariant mass of 260 GeVThe NC DIS expectation in thisregion is ≈ 9* 10-5. Rare SM processes(e.g. WW production) may dominatein this region and could not be considered.


ReferencesA general search for new phenomena, H1 Collaboration, A. Aktaset al. , accepted by Phys. Lett. B 08/04 (hep-ex 0408044),

M. Wessels (Aachen), M. Peez (Marseille) , G. Frising(Aachen) Ph.D. theses

Search for new physics in e mu X data using Sleuth: A quasi-modelIndendent search strategy for new physics, D0 Collaboration, Phys.Rev.D62, 2000.

a general search for new phenomenascaron/talks/heralhctalk.pdf · 2011-12-07 · a general search...

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