High Energy Frontier - Recent Results from the LHCschoning/... · 2012. 11. 8. · The Higgs mass...
Transcript of High Energy Frontier - Recent Results from the LHCschoning/... · 2012. 11. 8. · The Higgs mass...
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A.Schöning 1 LHC Recent Results, Searches WS 2012/13
Lecture 3
LHC-Searches II
High Energy Frontier - Recent Results from the LHC
University of Heidelberg WS 2012/13
Supersymmetry
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A.Schöning 2 LHC Recent Results, Searches WS 2012/13
Please Register!
https://uebungen.physik.uni-heidelberg.de/v/339
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A.Schöning 3 LHC Recent Results, Searches WS 2012/13
Searches for New Symmetries at LHC
Fourth generation quarks (extension of the three generations)
Heavy new vector bosons (W´, Z´) → Left-Right Symmetric Models
Search for large extra dimensions (extension of 3D+1 space-time)
Search for supersymmetry: → fermion-boson symmetry
and many more models (symmetries) …
and many variants ...
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A.Schöning 4 LHC Recent Results, Searches WS 2012/13
Theory Arguments for New Physics (Too) many parameters (25)!
Why three generations?
Why so different masses (Yukawa couplings)
Grand Unification (GUT) → couplings?
Fine Tuning and Naturalness Problem of the Higgs Mass (M
H < M
planck)
Ultraviolet catastrophe at high energies
Unification with Gravitation?
Mechanism of CP violation?
electromagnetic (γ) α1~1/137
weak IA (W, Z) α2~1/29
strong IA (gluon) α3~1/10
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A.Schöning 5 LHC Recent Results, Searches WS 2012/13
Overview
● Preface– Standard Model extensions
– SU(5)
● Supersymmetry– Theory
– Phenomenology
● Experimental Searches for Supersymmetry
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A.Schöning 6 LHC Recent Results, Searches WS 2012/13
Beyond the Standard Model
SM Gauge Group (unbroken):
SU(3)QCD
x SU(2)L x U(1)
Y
Fermions have the following transformation properties:
U a= (ud ) = (3, 2, 1 /6)
u = (3 , 1, −2/3)
d = (3 , 1, 1/3)
La = (νe
e ) = (1, 2, −1/2)
e = (1 , 1, 1)
Q = T3 + Yrelation to electric charge:
Comments:
SM is a real gauge theory (renormalizable)
renormalizability requires: same number of quark and lepton families conservation of baryon and lepton number
Absence of gauge anomalies requires quantized hypercharges (electric charges)
Gauge couplings g1, g
2 and g
3 are different!
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A.Schöning 7 LHC Recent Results, Searches WS 2012/13
Grand UnificationIdea: unify couplings
Complete fermion family fits into a SU(5) group representation
SU(5) with SU(3) x SU(2) embedding of left-handed (chiral) particles
{5} {10}_
Remark: anti-neutrino can be embedded in SO(10)
0
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A.Schöning 8 LHC Recent Results, Searches WS 2012/13
SU(5) Gauge Boson matrix
V8 corresponds to the gluon fields
W corresponds to the W field
V24
corresponds to the hypercharge field
X,Y correspond to Leptoquarks: X,Y → l q and Diquarks: X → uu, Y→ du
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A.Schöning 9 LHC Recent Results, Searches WS 2012/13
SU(5) Fermion matricesNew X,Y bosons
gluons
W+,W0, W-
B-field
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A.Schöning 10 LHC Recent Results, Searches WS 2012/13
Baryon/Lepton Number Violation in SU(5)
0
u1= ψ
14uc
3 = ψ
12
X24
d2 = ψ
25e+ = ψ
45
Proton Decay
Proton Lifetime >> 1030 years mX > 1015 GeV
Lifetime ~ 1/MX
4
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A.Schöning 11 LHC Recent Results, Searches WS 2012/13
Running of Couplings:Evolve couplings from renormalization group equations:
1αi(μ)
=1
αi(m)+
bi
2πlog (
mμ )
with bi =−113
C +43
N f l f +13
N s ls
Nf = number of fermions
Ns = number of scalars (Higgs)
C, lf, and l
s are quadratic Casimir element
of representation
For SU(5) model
b1 =−11+43
N G
b2 =−22 /3+43
N G+16
H
b3 =43
N G+110
H
generations
Higgs doublets
PLOT
unification scale below proton lifetime bound !
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A.Schöning 12 LHC Recent Results, Searches WS 2012/13
Lessons from SU(5) Unification of coupling possible if right amount of Higgs doublets
Weinberg angle is more or less correctly predicted sin2 θ = 3/8 (at unification scale)
New bosons are predicted with masses MX~1015 GeV
Proton is unstable due to new interactions X
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A.Schöning 13 LHC Recent Results, Searches WS 2012/13
The Hierarchy Problem in the SMSM Fine Tuning Problem
The Higgs mass acquires large radiative corrections
In SUSY the quadratic divergences from fermion loops are compensated by scalars. Only “usual” logarithmic divergences remain.
In the SM divergences corresponding to physical objects are renormalized.However, the ratio of bare Higgs mass to the observed Higgs mass of M
Higgs /M
Planck = 10-17
is considered to be unnatural → fine tuning problem
scalar bosonfermion
δM H2 = M H ,bare
2 + δM H2
M Hf2 =
∣g f2∣
162 [−22 6m f2 log /m f ]M Hs
2 =∣s
2∣162 [ 2 2ms
2 log /ms ]note factor 2
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A.Schöning 14 LHC Recent Results, Searches WS 2012/13
The Hierarchy Problem in the SMSM Fine Tuning Problem
The Higgs mass acquires large radiative corrections
scalar bosonfermion
M Hf2 =
∣g f2∣
162 [−22 6m f2 log /m f ]M Hs
2 =∣s
2∣162 [ 2 2ms
2 log /ms ]note factor 2
An exact cancellation happens if the number of scalars is twicethe number of fermions
invent symmetry: 2 x # scalars ↔ # fermions
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A.Schöning 15 LHC Recent Results, Searches WS 2012/13
Superpartners Supersymmetry (SUSY) connects SM particles with SUSY partners
SUSY partners are different from SM particles only in spin by -1/2.All other quantum numbers are identical
SUSY is broken because we haven't seen SUSY particles yet (different mass of SM and SUSY particles)
SUSY particles are SM partners with respect to the SM chiral particlesand denoted in the following way:
eL→ eLeR→ eR
To each SM fermion correspond two SUSY particles!
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A.Schöning 16 LHC Recent Results, Searches WS 2012/13
Superpartners
actually, there are two Higgs doublets → 4 Higgs states!
SUSY partners not seen (heavy) → SUSY is broken
SUSY Breaking Scale should be ~ 1 TeV otherwise hierarchy problem reappears
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A.Schöning 17 LHC Recent Results, Searches WS 2012/13
Superpartners
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A.Schöning 18 LHC Recent Results, Searches WS 2012/13
SUSY Gauge Coupling Unificationlogarithmic slopes:
SM:
SUSY:
bSM = (41/10,−19/6, −7)
bSM = (33/5, 1, −3)
coupling unification in SUSY
M unification≈1016 GeV
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A.Schöning 19 LHC Recent Results, Searches WS 2012/13
Problems solved by SUSY? (Too) many parameters (25)!
Why three generations?
Why so different masses (Yukawa couplings)
Grand Unification (GUT) → couplings?
Fine Tuning and Naturalness Problem of the Higgs Mass (M
H < M
planck)
Ultraviolet catastrophe at high energies
Unification with Gravitation?
Mechanism of CP violation?
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A.Schöning 20 LHC Recent Results, Searches WS 2012/13
What breaks SUSY?
Different models developed:
SuperGravity SUSY-Breaking (SUGRA)
Gauge Mediated SUSY-Breaking (GMSB)
Anamolous Mediated Gravity SUSY-Breaking (AMSB)
….
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A.Schöning 21 LHC Recent Results, Searches WS 2012/13
too many!
124 parameters in Minimal SUSY Model (MSSM)
Simplified models often used:
constrained MSSM
Supergravity models (mSUGRA)
...
How man Parameters in SUSY?
SUSY breaking and the large number of parameters are concerns!
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A.Schöning 22 LHC Recent Results, Searches WS 2012/13
MSSM Parameters Coulings: g
s, g, g' corresponding to the SU(3) x SU(2) x U(1) gauge groups
Masses:
gaugino masses M3 , M
2 , M
1 associated to SU(3) x SU(2) x U(1)
scalar squared mass parameters
SUSY breaking parameters:
Higgsino mass parameter μ
Higgs-Fermion Yukawa coupling yu, yd, ye (fermion-Higgs, sfermion-Higgsino)
M Q2 , M U
2 , M D2 , M L
2 , M E2 u ,d L , uL
c , d Lc , , e− L , eL
ccorresponding to
trilinear Higgs-sfermion-sfermion couplings: Au, Ad, Ae
scalar Higgs mass parameters: m12+μ2 , m2
2+μ2 , m122 =Bμ
can also be re-expressed by: tan =vu /vd vu2vd
2 = 246GeV 2
In total 124 parameters in MSSM
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A.Schöning 23 LHC Recent Results, Searches WS 2012/13
SUSY Phenomenology
particle spectrum is rich and complicated several particles can mix!
B , W 0 , H , h → χ10 , χ2
0 , χ30 , χ4
0
W ± , H ± → χ1± , χ2
±
neutralinos
charginos
Masses of states depend on SUSY-breaking scheme andparameters
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A.Schöning 24 LHC Recent Results, Searches WS 2012/13
SUSY Mass Phenomenology
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A.Schöning 25 LHC Recent Results, Searches WS 2012/13
SUSY Mass Phenomenology
comparison of two different parameters sets (“Snowmass Points”)
both are excluded in the meantime...
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A.Schöning 26 LHC Recent Results, Searches WS 2012/13
SUSY RP-Conserving Couplings
Gluino-squark-quark:
Neutralino-squark-quark:
Neutralino-Neutralino-Z-boson:
RP is a multiplicative quantum number
if conserved SUSY particles can only produced in pairs and “SUSYness” is conserved in decays
R∣SM ⟩ = 1 R∣SUSY ⟩ =−1
relation: R=(-1)3B+L+2S
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A.Schöning 27 LHC Recent Results, Searches WS 2012/13
SUSY Feynman Graphs
Neutralino Pair-Production:
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A.Schöning 28 LHC Recent Results, Searches WS 2012/13
SUSY Feynman GraphsSUSY production in hadron interactions (e.g. LHC)
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A.Schöning 29 LHC Recent Results, Searches WS 2012/13
R-Parity Violating CoulingsTrilinear RPV-Yukawa Couplings:
RPV sparticles decay: RPV =1
16 ijk
2 M q (but could be long-lived)
lightestSUSY particle(dark mattercandidate!)not stable
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A.Schöning 30 LHC Recent Results, Searches WS 2012/13
L,B Number Violation and R-Parity
L L=1 =12ijk Li L jek ' ijk LiQ j
dk i Li H u
L B=1 =12 ' ' ijkui
d jdk
if R-parity is violated with first generation couplings ΔL=1 and ΔB=1,the proton would undergo a catastrophic decay:
RP-Violating couplings are not excluded in general
but many combinations of non-zero terms are constrained!
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A.Schöning 31 LHC Recent Results, Searches WS 2012/13
Experimental Search Strategy at LHC Assumption: R
P is conserved
SUSY particles produced in pairs will decay in cascades
In many models the neutralino is the lightest SUSY particle and stable
The neutralino escapes detection and leads to missing energy in the detector
χ0χ0
MET
MET
leptons or quarks
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A.Schöning 32 LHC Recent Results, Searches WS 2012/13
ET
miss Performance
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A.Schöning 33 LHC Recent Results, Searches WS 2012/13
Same Charge Dilepton Sample
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A.Schöning 34 LHC Recent Results, Searches WS 2012/13
Search for SUSY in Top-Quark Final States with same charge Dileptons
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A.Schöning 35 LHC Recent Results, Searches WS 2012/13
Search for SUSY in Top-Quark Final States without Leptons
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A.Schöning 36 LHC Recent Results, Searches WS 2012/13
RP Violation (RPV) Searches
The neutralinodecays into SMparticles!
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A.Schöning 37 LHC Recent Results, Searches WS 2012/13
Search for GMSB-SUSY at LHC Assumption: R
P is conserved
In GMSB models the gravitino is the LSP (can be very light!)
The neutralino is the NLSP and decays to photon and gravitino
Search Topology: MET + photons
GG
MET
MET
gravitino = LSP
photons
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A.Schöning 38 LHC Recent Results, Searches WS 2012/13
CMS Two Photon Event
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A.Schöning 39 LHC Recent Results, Searches WS 2012/13
Di-Photon Missing Energy
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A.Schöning 40 LHC Recent Results, Searches WS 2012/13
CMS Results (GMSB)
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A.Schöning 41 LHC Recent Results, Searches WS 2012/13
Overview CMS Results (MSSM)
mass limits dependingon neutralino mass
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A.Schöning 42 LHC Recent Results, Searches WS 2012/13
Other SUSY Searches
Discussed: MSSM SUSY searches with neutralino in final state (missing E
T)
Searches with photons and gravitinos in final state (missing ET)
Searches with same-charge leptons and missing ET
Searches with R-parity violation
Not Discussed: Many more (complex) topologies exist and studied SUSY particles could be long-lived and massive (highly ionizing) SUSY particles could decay half way in the detector (kinks) SUSY particles could form R-hadrons (SUSY-hadrons) which
interact in the detector and, and, and ….
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A.Schöning 43 LHC Recent Results, Searches WS 2012/13
Summary
Despite the fact that the cross section for the productionof light SUSY particles is large at LHC, no sign of SUSYseen yet (in most simple models and analysis)
Searches will continue with larger datasets and at higherbeam energies (s1/2=14 TeV). More complex models willbe studied. Main problem is that the mechanism of SUSYbreaking is unknown.
SUSY cannot experimentally ruled at at LHC if the SUSYmass scale is large. However, than it would not solvethe fine tuning problem.
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A.Schöning 44 LHC Recent Results, Searches WS 2012/13