The Hidden Valley and ATLAS Dan Ventura U.Washington Particle Theory Journal Club 01 June 2007.
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Transcript of The Hidden Valley and ATLAS Dan Ventura U.Washington Particle Theory Journal Club 01 June 2007.
The Hidden Valley and ATLAS
Dan Ventura
U.Washington Particle Theory Journal Club
01 June 2007
1 June 2007 U. Washington PTJC 2
1 June 2007 U. Washington PTJC 3
Outline
• Introduction to Hidden Valley models– Specialize to QCD-like Hidden Valley with 2 light
flavors
• Production of Hidden Valley particles– Via the Higgs and the Z´
– Experimental signatures & issues of Hidden Valley type models
1 June 2007 U. Washington PTJC 4
What is a Hidden Valley
• SM extended by a non-abelian gauge group Gv – SM → SM x Gv
• All SM particles are neutral under Gv
• There are new “light” particles (v-particles) charged under Gv and neutral under the SM
• Interactions between the v-particles and SM are mediated by new heavy communicators (Z´ or loop of heavy particles carrying both SM and Gv charges)
1 June 2007 U. Washington PTJC 5
Conceptual Diagram
• The heavy communicators that carry both SM and Gv charge were rarely produced at LEP and LEPII
Energy
Inaccessibility
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Hidden Valley
• Let Gv = U(1)´ x SU(nv)
• The U(1)´ is broken by a scalar expectation value giving a Z´ a mass of ~3 TeV
• The SU(nv) confines on a scale of
~100 GeV < v < 1 TeV
1 June 2007 U. Washington PTJC 7
QCD-like Hidden Valley
• Consider a Hidden Valley with 2 light flavors ( UV & CV )
• mU ~mC << V-QCD • Particle spectrum controlled by approximate v-
isospin symmetry • v-hadrons decay promptly to v-pions & v-nucleons• V-nucleons are stable• The SM neutral v
± are stable unless FCNC allows CV→UV
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v0 Decays
v0 has the wave function UU - CC and
can decay via QVQV→ Z´→ f f
v0 decays predominately to heavy flavor
( b b or for m < 2 mt)
Free Parameters
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v Production via the Higgs
• The potential for the scalar fields is:– V= -2 |H|2 - ||2 + |H|4 + ||4 + ||2 |H|2
• After SSB, H and fields mix– The produced higgs state is: cos|h> + sin|>– Then the SM higgs can decay into the HV through
the
ˆ
v0
Mixing
h hv
v0
g
g
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Hidden Valley in ATLAS
Rome La SapienzaGuido Ciapetti Carlo DionisiStefano Giagu Daniele DePedisMarco ResignoLucia Zanello
Barbara Mele*
U. WashingtonHenry LubattiGiuseppe SalamannaLaura BodineDan Ventura
Matt Strassler*
Rome1 - Seattle Collaboration
*Theoretical consultants (not ATLAS members)
• Rome1-Seattle working group formed in Sept. 2006
• All work presented is property of the ATLAS collaboration and was preformed by members of the Rome1-Seattle WG
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Parameters
• Parameters used in the current study: – mh = 140 GeV mZ´ = 3 TeV
– m = 40 GeV
250 mm -- for v from higgs decays
100 mm -- for v from Z´ decays
Lifetimes were chosen to give a distribution of decay positions throughout the inner detector
{c =
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Event Signatures
Pixel Layers
Silicon Layers
TRT
Radial Position of “truth” vertices
For gluon fusion:• Highly displaced vertices O(10 cm - 1m)– Jets with few tracks
• SM Backgrounds: Interaction of neutrals with detector material
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Jets from HV decaysgg→h→v v
Number of reconstructed jets per eventNumber of reconstructed tracks per jet
nTracks
Jet cut: ET > 35 GeV
• Final state has 4 b quarks -- not 4 b jets• Number of jets depends on the boost and
decay position of v
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gg→h→v v
Pixel detector
Silicon tracker
TRT
50 - 120 mm
300 - 520 mm
640 - 1030 mm
White tracks are MC “truth” tracks Green tracks are reconstructed
v decay ~ 50 cm from the interaction point (IP)
v decay ~ 5 cm from IP with associated tracks
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Jet
2nd v does not produce a jet -- the decay products are not energetic enough and are too spread out to form a jet
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Muons from HV decays
• Muons are produced from the semi-leptonic decays of B-mesons (or decays)
• Produced at large distances from the IP
• Backgrounds: SM ± and K decays in flight
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Muons from displaced verticesLongitudinal Impact Parameter
Reconstructed Muon track
v decay vertex
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Muon Impact Parameters
Reconstructed longitudinal impact parameter -- Distance from the IP
Reconstructed radial impact parameter
1.5 m
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Triggering on muons from HV decays
7.5 m
2.5 m
Level 1 triggers
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Triggering on muons from HV decaysLevel 2 triggers
• Full granularity of data is available within region of interest (RoI) around the “infinite momentum path” as defined by level 1
• Refined PT measurement preformed• Outside-in tracking is preformed to match the
muon spectrometer track to an inner detector track
• If PT < threshold or if no matching track is found, the trigger fails
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Muon Trigger results
≥ 6 GeV~17% of events
≥ 10 GeV~13% of events ≥ 20 GeV
~6% of events
Level 1 muon triggers
Level 2 muon triggers
≥ 2 GeV“loose” trigger ≥ 6 GeV
≥ 20 GeV
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Other higgs production mechanisms
• Vector Boson Fusion
– Higgs produced with 2 forward jets
• Higgsstrahlung
– Higgs recoils against the W
h0
W/Z
W/Zq
q
q1
q2
q3
q4
h0W/Z
W/Z
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Longer lifetimes or boosted v
W decayv decays inside ID
2nd v decays at the end of the HCal Hadronic shower occurs inside the Muon Spectrometer
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For a particular model. Others may differ by ~ factor of 10
100 events/year
Z’Z’
v production via the Z´
Many v-hadrons are formed. ±
v and v-nucleons are stable -- give MET
0v decay to bb ()
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Z´ decay to v
Pixel detector ~12 cm
EM Cal ~1.1 m
v decays inside the HCal -- will cause punch through
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Trigger Rates
• Jet triggers:– ~75% of events pass
Level 1 single jet triggers
– ~70% pass level 1 multi-jet triggers
• Muon triggers:– 80% of events pass
level 1 6 GeV muon trigger
– 8.2% pass level 2 muon trigger
• ~10% of these muon triggers are caused by punch through
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Work in progress …
• Level 1 triggers are hardware based– Cannot be changed at this point
• Level 2 triggers are software based– Still being written/implemented
• Can still be modified -- We are currently looking for a set of level 2 trigger objects that will keep our events without letting in SM backgrounds