how to tell apart non-standard ewsb mechanisms · bosonic goldstone since susy may not be there to...
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![Page 1: How to tell apart non-standard EWSB mechanisms · Bosonic Goldstone since SUSY may not be there to save the day Higgs as a PGB like the pion of QCD composite Higgs Composite Scalar](https://reader033.vdocument.in/reader033/viewer/2022060610/60615187c73b4a2e6b6702f8/html5/thumbnails/1.jpg)
How to tell apart non-standard
EWSB mechanisms
Veronica SanzCERN and YORK
Moriond 2012
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What is standard?
EWSB by elementary scalar(s)
includes SM and SUSY
What is non-standard?
EWSB by-composite scalar- no scalar at all
includes Little Higgs, Extra-Dimensions and Technicolor
In th
is tal
k
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What if there is a Higgs? Light scalarNeed stabilization mechanism
(or we have no clue about QFT)
SymmetriesFermionic SUSY
Bosonic Goldstone
since SUSY may not be there to save the day
Higgs as a PGB like the pion of QCD
composite Higgs
Composite Scalar - Motivation
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Composite Higgs is realized in Little Higgs, Extra-Dimensions and Technicolor
symmetry PGB -Little Higgs, TC: new 4D symmetry
-Extra-dimensions: SM 5D gauge= 4D gauge+GB
Composite Scalar - Realizations
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scalar resonance WW unitarizationnon-SM scalar: deviations
generic features are too SM-like
Giudice, Grojean, Pomarol and Rattazzi ʻ07! =
v2
f2 degree of fine-tuning
composite Higgsalready unitarize WW
Theory study 300 ifb @ 14 TeV for ! > 0.2
! ! 0 SM-like
Composite Scalar-Generic features
v
f
4!f
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Composite Scalar-Common features
s=1not crucial for WW scattering
ex. Z’, , !TC ZKK
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Composite Scalar-Common features
s=1not crucial for WW scattering
new gauge symms?
ex. Z’, , !TC ZKK
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Composite Scalar-Common features
s=1not crucial for WW scattering
new gauge symms?
Extra-Dimensions and TC-type
GKK fTC2,ex.s=2
see next
ex. Z’, , ZKK!TC
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Composite Scalar-Common features
s=1not crucial for WW scattering
new gauge symms?
ex. Z’, , !TC ZKK
Extra-Dimensions and TC-type
GKK fTC2,ex.s=2
s=1/2
New heavy quarks mix with SM quarks
QKKex. T, , techni-baryons
see next
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Composite Scalar-Common features
s=1not crucial for WW scattering
new gauge symms?
ex. Z’, , !TC ZKK
Extra-Dimensions and TC-type
GKK fTC2,ex.s=2
s=1/2
New heavy quarks mix with SM quarks
QKKex. T, , techni-baryons
3rd gen
light quarks
see next
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Composite Scalar-Common features
s=1not crucial for WW scattering
new gauge symms?
ex. Z’, , !TC ZKK
Extra-Dimensions and TC-type
GKK fTC2,ex.s=2
s=1/2
New heavy quarks mix with SM quarks
QKKex. T, , techni-baryons
3rd gen
light quarks
see next
see next
4th gen?
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparation
i.e. massive spin-2 resonance = smoking gun of extra-dimensions?
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparation
G G
i.e. massive spin-2 resonance = smoking gun of extra-dimensions?
KK-graviton TC-type impostor
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparation
G G
i.e. massive spin-2 resonance = smoking gun of extra-dimensions?
KK-graviton TC-type impostor
propagation
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparation
G G
i.e. massive spin-2 resonance = smoking gun of extra-dimensions?
KK-graviton TC-type impostor
propagation Pauli-Fierz Pauli-Fierz
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparation
G G
i.e. massive spin-2 resonance = smoking gun of extra-dimensions?
KK-graviton TC-type impostor
propagation Pauli-Fierz Pauli-Fierz
interactions
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparation
G G
i.e. massive spin-2 resonance = smoking gun of extra-dimensions?
KK-graviton TC-type impostor
ci
MGµ!Tµ!
i,SM
propagation Pauli-Fierz Pauli-Fierz
interactions
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparation
G G
i.e. massive spin-2 resonance = smoking gun of extra-dimensions?
KK-graviton TC-type impostor
ci
MGµ!Tµ!
i,SM
propagation Pauli-Fierz Pauli-Fierz
interactions
ci M ! TeVoverlap G with fields i and
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparation
G G
i.e. massive spin-2 resonance = smoking gun of extra-dimensions?
KK-graviton TC-type impostor
ci
MGµ!Tµ!
i,SM
propagation Pauli-Fierz Pauli-Fierz
interactions ?ci M ! TeVoverlap G with fields i and
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparationG couplings?
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparationG
Lorentz and gauge
couplings?
no dimension-4
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparationG
Lorentz and gauge
couplings?
dimension-5 same as in
Tµ!
flavor and CP invariant
no dimension-4
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparationG
Lorentz and gauge
couplings?
dimension-5 same as in
Tµ!
G G couples like
same spin determination
How do we distinguish them?
flavor and CP invariant
no dimension-4
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How to tell apart a graviton from an impostor?Guimaraes, Fok, Lewis, VS
in preparation
In any extra-dimension of the type
ds2 = w(z)2 (!µ!dxµdx! ! dz2)
example UED,RS
Rg/! =Br(! gg)Br(! !!)
=8c2
g
c2!
Rg/! = 8
G
G
can produce any other ratio
:
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How to tell apart 1st generation RH or LH compositeness? Martin and VS
JHEP (2010)Redi,VS, Weiler
in preparationComposite baryons and elementary quarks mix
Lmixing = !uL,R uL,RUL + (u! d) y ! !L!R
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How to tell apart 1st generation RH or LH compositeness? Martin and VS
JHEP (2010)Redi,VS, Weiler
in preparationComposite baryons and elementary quarks mix
1st generation compositeness! Flavor?
Lmixing = !uL,R uL,RUL + (u! d) y ! !L!R
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How to tell apart 1st generation RH or LH compositeness? Martin and VS
JHEP (2010)Redi,VS, Weiler
in preparationComposite baryons and elementary quarks mix
1st generation compositeness! Flavor?MFV if composite sector flavor invariant
Lmixing = !uL,R uL,RUL + (u! d)
• Left-handed compositeness: !Lu ! Id , !Ld ! Id
!Ru ! yu , !Rd ! yd
• Right-handed compositeness: !Lu ! yu , !Ld ! yd
!Ru ! Id , !Rd ! Id
y ! !L!R
Redi, Weiler ‘11
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How to tell apart 1st generation RH or LH compositeness? Martin and VS
JHEP (2010)Redi,VS, Weiler
in preparationComposite baryons and elementary quarks mix
Lmixing = !uL,R uL,RUL + (u! d) y ! !L!R
Redi, Weiler ‘11
MFV half of the proton could be composite
1st generation compositeness! Flavor?MFV if composite sector flavor invariant
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How to tell apart 1st generation RH or LH compositeness?
LH compositeness RH compositeness
Signature: single production heavy quarkq Q
!
Q
q
W,Z
Q
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How to tell apart 1st generation RH or LH compositeness?
LH compositeness
Q
q
W,ZMartin and VSJHEP (2010)
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How to tell apart 1st generation RH or LH compositeness?
LH compositeness
Q
q
W,ZMartin and VSJHEP (2010)
ATLAS-PH-EP-2011-193. Lepton channel w/ 1 ifb.
EW production
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How to tell apart 1st generation RH or LH compositeness?
Redi,VS, Weilerin preparation
RH compositeness
Q
500 1000 1500 2000
1
2
3
4
mQ (GeV )
mG = 4 TeV
mG = 3 TeV
mG = 2 TeV
Log10(!(fb))
BGs: multijet, W+jets, Z+jets, top pair and single top
Rejection: exclude dijet near W or Z and veto b-tagging, cut on leading jet
ATLAS-PH-EP-2011-154
QCD generated with ALPGEN -> PYTHIA signal xsecs mQ=1 TeV, mG=2 TeV
Looking at current bounds and discovery prospects
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How to tell apart 1st generation RH or LH compositeness?
Redi,VS, Weilerin preparationRH compositeness
We use two methods: deltaR and leading jetoptimized for high-low mQ
(GeV)3jm0 500 1000 1500 2000 2500 3000 3500 4000
-1N
um
ber
of
Even
ts f
or
10 f
b
0
100
200
300
400
500
(GeV)3jm0 500 1000 1500 2000 2500 3000 3500 4000
-1N
um
ber
of
Even
ts f
or
10 f
b
0
100
200
300
400
500
QCD
Signal
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No Scalar-Generic features
s=1 resonances do unitarize WW scattering
Realized in warped extra-dimensions and TC-type
THE problem: S parametersolutions do not abound
Non-calculable, ignore TCSM
Mechanisms to cancel, warped models
Holographic TC Hirn,VSPhys. Rev. Lett. ‘06s=1 cancellation
Cured Higgsless Cacciapaglia et alPhys. Rev. D ‘05(s=1)-(s=1/2) cancellation
Eichten, LanePhys. Lett. B ‘89
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In dileptons...
How to tell apart scenarios of dynamical EWSB?Banerjee, Martin and VS
JHEP (2012)
1. Invariant mass
(GeV) - l
+l
m550 600 650 700 750 800 850 900
Arb
itary
Units
0
200
400
600
800
1000
1200TCSM
HTC
CHL
MG> PYTHIA> ATLFAST and DELPHES@7 TeV
(GeV)- l
+l
m0 200 400 600 800 1000 1200
Arb
ita
ry U
nits
1
10
210
310 CHL
ZKK2
ZKK1
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How to tell apart scenarios of dynamical EWSB?Banerjee, Martin and VS
JHEP (2012)2. Charge asymmetry
| -l!|-|+
l!|
-2.5 -2 -1.5 -1 -0.5 0 0.5 1 1.5 2 2.5
Arb
ita
ry U
nits
0
100
200
300
400
500
Vector (R=L)
Non-vector (R=(1/3)L)
Chiral (R=0) !
!
!
!
!
!
!
!
!
!
0.1 0.2 0.3 0.4
0.05
0.10
0.15
0.20
0.25
!A! V
A2 + V 2
"2
! "# $%&#
Acharge =N(!! > 0)!N(!! < 0)N(!! > 0) + N(!! < 0)
can tell V,A admixtureeta asym is a good measure
of chirality
A after simulation
!! = |!!+ |!| !!! |
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Conclusions✦ Non-standard EWSB ideas abound and have a
very rich phenomenology.
✦ May not be easy to discover by just looking at scalar EWSB sector. Need correlations with other signals.
✦ Tell apart Extra-Dimensions from TC-type: gravitons and its impostor
✦ Tell apart 1st gen RH or LH compositeness in multijets
✦ Tell apart different scenarios of DEWSB in dileptons
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Operators
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ratio to gluonsgluon-jet from quark-jet?
1. most models: G coupling to light quarks suppressed2. Angular correlations
3. Tag light jet using Galliccio-Schwartz techniques
d!
d cos "!(qq ! G) = 1 + c2
!!!1" 4s2
!!"
to fermions
= 1" c4!! to gluons ,