SlideShare a Scribd company logo
1 of 37
1Eckhard von Toerne, Bonn ATLAS Higgs Measurements
Talk at BW 2013 – Beyond the Standard Models
25 – 29 April, 2013, Vrnjačka Banja, Serbia
Overview of the
ATLAS Higgs
Measurements
Eckhard von Toerne
University of Bonn
on behalf of the
ATLAS Collaboration
2Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• “Observation of a new particle”
in July 2012
• Overview of properties: mass,
spin/parity, (couplings)
• A Note:
While existence of new boson at mass of
~125 GeV is undisputed, its nature is
under active study.
Boson exhibits Higgs-like properties.
For brevity the term “Higgs-like boson” is
shortened to Higgs boson or Higgs
(working hypothesis).
PLB 716(2012) 1-29,
http://arxiv.org/abs/1207.7214
Introduction
See also: ATLAS Coll., Science 338, 1576 (2012)
3Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• x
Production of SM Higgs @ LHC
Cross sections at 8 TeV [pb]
ggH 19.4
VB Fusion 1.6
WH+ZH 1.1
ttH 0.1
mH = 125.5 GeV
4Eckhard von Toerne, Bonn ATLAS Higgs Measurements
Decay of SM Higgs
56.9 % bb
22.3 % WW
6.2 %
2.8 % ZZ
0.23 % γγ
@ mH=125.5 GeV
5Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• x
LHC runs in 2011 + 2012
Z→μμ event with
25 reconstructed vertices
6Eckhard von Toerne, Bonn ATLAS Higgs Measurements
ATLAS detector
7Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• Two isolated high-pt
photons (ET>40, 30 GeV)
• Mass peak with
resolution 1.77 GeV
above large backgr.
(S/B=3%).
• Reducible backgr. j, jj
(~25%)
• Irreducible bgd from
QED reaction qq
(~75%)
• Example event with
m =126.6 GeV
H
8Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• Two isolated high-pt
photons (ET>40, 30 GeV)
• Mass peak with
resolution 1.77 GeV
above large backgr.
(S/B=3%).
• Reducible backgr. j, jj
(~25%)
• Irreducible bgd from
QED reaction qq
(~75%)
• Example event with
m =126.6 GeV
H
Zoom into
Calorimeter cluster
• Layered
Calorimeter 
• Photon direction
• Selection of vertex
9Eckhard von Toerne, Bonn ATLAS Higgs Measurements
local significance:
- observed: 7.4σ
-expected
-(SM Higgs): 4.1σ
Best fit mass: 126.8 ± 0.2 (stat) ± 0.7 (syst) GeV
Signal Strength µ = obs/ SM = 1.65 ± 0.24(stat) ± 0.22(syst)
H
Prob. of a background
fluctuation to be more signal-
like than observed signal.
10Eckhard von Toerne, Bonn ATLAS Higgs Measurements
H
• 2.0 excess for VBF
production over bgd.
• 14 categories to optimize
sensitivity (different S/B ratios)
• and to categorize ggF, VBF, VH
11Eckhard von Toerne, Bonn ATLAS Higgs Measurements
HZZ(*)
ATLAS-CONF-2013-013
mH = 124.3 ± 0.6 (stat) ± 0.4 (syst) GeV
μ (124.3 GeV) = 1.7 ± 0.4
Need to reconstruct low pt leptons
12Eckhard von Toerne, Bonn ATLAS Higgs Measurements
HZZ(*)
ATLAS-CONF-2013-013
mH = 124.3 ± 0.6 (stat) ± 0.4 (syst) GeV
μ (124.3 GeV) = 1.7 ± 0.4
13Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• x
H  ZZ(*)  4 µ
m12=86.3 GeV, m34=31.6 GeV, m4μ = 125.1 GeV, ATLAS-CONF-2012-169
14Eckhard von Toerne, Bonn ATLAS Higgs Measurements
Higgs mass combination
Combined ATLAS result
Difference reduced by
700 MeV compared to
December result
Considering all
systematics and their
correlations, compatibility
of both results is at 1.5%
(2.4σ level)
With alternative
treatment of systematics,
compatibility rises to 8%
Main systematics:
energy scale
mH = 125.5 ± 0.2 (stat) ± 0.6 (syst) GeV
15Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• limited mass sensitivity due to neutrino contribution
• Transverse mass
• S/B ~ 15%
HWW
16Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• Observed significance (125 GeV) 3.8σ (3.7σ expected)
• Signal strength at 125 GeV μ = 1.01 ± 0.21(stat) ± 0.23(syst)
[ 0.21(stat) ± 0.19(theo) ± 0.12(exp) ± 0.04(lumi) ]
HWW
17Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• x
Hbb
• Limits derived from Mbb distribution (~16% mass resolution)
• 95%CL limit at 125 GeV: 1.8 x SM (expected limit 1.9)
• μ(125) = -0.4 ± 0.7(stat) ± 0.8(syst),
• Analysis still in flux and not all of 2012 data used
• Main benchmark analysis yields 4.0σ observation of boson
pairs WZ(bb)/ZZ(bb)
Combination of search channel WH, Wl / ZH, Zll / ZH, Z
18Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• x
Hbb candidate
19Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• x
H candidate
20Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• Global compatibility
between presented
channels and the SM
expectation is 8%
• Dependence of signal
strength on mass is
weak
ATLAS combined signal strength
ATLAS-CONF-2013-034
21Eckhard von Toerne, Bonn ATLAS Higgs Measurements
ATLAS combined Higgs signal significance
Moriond 2013 status, ATLAS-CONF-2013-034
• Combination of all
channels
• Local p0 = 10-23
•  ~10 excess
around 125 GeV
22Eckhard von Toerne, Bonn ATLAS Higgs Measurements
Spin and Parity
• SM predicts JP=0+
• Spin studies in three different modes
• H : sensitivity decay angle in Higgs rest frame *
• HWW decy angles no directly reconstructable due to
neutrinos, however other kinematic vars. quite sensitive
due to V-A nature of W decays.
• HZZ fully reconstructed, decay plane is sensitive
• Spin 1 disfavored by Landau-Yang
theorem and H decay
• Spin 2 case may be quite evolved
• Here: tensor with minimal
couplings to SM particles (2+
m model)
• Dependency on 2+
m production mode.
 free parameter fqq, fqq+fgg=1
23Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• Spin information from cosθ* shape, not sensitive to parity
• Minimize correlation between cosθ* and mass for bgd by
applying absolute pt cuts
• control the background cosθ* shape via mass sidebands
• Largest sensitivity if 2+
m is created by 100% gg fusion
Spin and Parity: H
24Eckhard von Toerne, Bonn ATLAS Higgs Measurements
Spin and Parity: HZZ(*)
Combine all kinematic variables in a Boosted Decision
Tree to optimize sensitivity
sensitive to parity
25Eckhard von Toerne, Bonn ATLAS Higgs Measurements
Spin and Parity: HWW
ATLAS-CONF-2013-031
0+ Hyp. 2+ Hyp.
BDT to combine all sensitive variables, most sensitive: fqq=100%
26Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• the 3 channels combined exclude 2+
m scenario at 99.9% CL
• ZZ analysis excludes the 0-, 1+ and (1-) hypotheses at the
>95% (94%) CL
Spin and Parity: combined
ATLAS-CONF-2013-040
27Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• Overwhelming evidence for a new boson at
• M = 125.5 ± 0.2 (stat) ± 0.6 (syst) GeV
• Measurements of signal strength and spin/parity in
agreement with SM hypothesis.
• Not covered in this talk: Meas. of couplings also in good
agreement.
• Improved measurements of pre-shutdown data and after
shutdown will further investigate this particle.
• Search for rare decays
• Search for additional states
• Moving towards precision Higgs Physics
• …if something walks like a duck and quacks like a duck,
it is probably a duck. This particle is looking more and
more like a Higgs boson.
Conclusion and Outlook
28Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• x
https://twiki.cern.ch/twiki/bin/view/AtlasPublic/HiggsPublicResults
29Eckhard von Toerne, Bonn ATLAS Higgs Measurements
Additional Slides
30Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• x
Higgs Mass
31Eckhard von Toerne, Bonn ATLAS Higgs Measurements
32Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• ATLAS-CONF-2012-101
ATLAS ET-mis Performance
33Eckhard von Toerne, Bonn ATLAS Higgs Measurements
Higgs couplings Overview
Good agreement with SM prediction
If µVBF tested alone  3.1 evidence for VBF production
34Eckhard von Toerne, Bonn ATLAS Higgs Measurements
Fermion vs. vector couplings
2-parameter model, group fermion and vector couplings together
κV = κZ = κW ; κF = κt = κb = κ = κg = κ
We assume only SM-loop contributions to kg and k
One overall un-observable sign, chose kV>0
Sign sensitivity mostly from interference in Hgg (t vs W in loop)
Only slight preference for kF>0  no conclusions yet
2D compatibility with SM 8%
35Eckhard von Toerne, Bonn ATLAS Higgs Measurements
• Custodial symmetry protects ratio of W, Z couplings (λWZ).
W vs Z couplings
λWZ = 0.80 ± 0.15 in agreement with SM prediction
36Eckhard von Toerne, Bonn ATLAS Higgs Measurements
HZZ(*) spin variables,
example: decay plane phi
37Eckhard von Toerne, Bonn ATLAS Higgs Measurements
HWW spin variables, example: deltaPhi

More Related Content

What's hot

IB Chemistry on Energetics, Enthalpy Change and
IB Chemistry on Energetics, Enthalpy Change and IB Chemistry on Energetics, Enthalpy Change and
IB Chemistry on Energetics, Enthalpy Change and Lawrence kok
 
Thermodynamics -Basic concepts
 Thermodynamics -Basic concepts Thermodynamics -Basic concepts
Thermodynamics -Basic conceptsselvakumar948
 
Simulated Annealing
Simulated AnnealingSimulated Annealing
Simulated Annealingguestead520
 
Unit 3 transient heat condution
Unit 3 transient heat condutionUnit 3 transient heat condution
Unit 3 transient heat condutionYashawantha K M
 
IB Chemistry on Energetics experiment, Thermodynamics and Hess's Law
IB Chemistry on Energetics experiment, Thermodynamics and Hess's LawIB Chemistry on Energetics experiment, Thermodynamics and Hess's Law
IB Chemistry on Energetics experiment, Thermodynamics and Hess's LawLawrence kok
 
One dim, steady-state, heat conduction_with_heat_generation
One dim, steady-state, heat conduction_with_heat_generationOne dim, steady-state, heat conduction_with_heat_generation
One dim, steady-state, heat conduction_with_heat_generationtmuliya
 
Latent heat practical
Latent heat practicalLatent heat practical
Latent heat practicalJosiahSpears
 
Lab 4 (specific latent heat)
Lab 4 (specific latent heat)Lab 4 (specific latent heat)
Lab 4 (specific latent heat)Alex Paradissis
 
Fins equation & lumped heat capacity system
Fins equation & lumped heat capacity systemFins equation & lumped heat capacity system
Fins equation & lumped heat capacity systemN/A
 
J. Milošević, Measurement of Two- and Four-particle Correlations in pPb and P...
J. Milošević, Measurement of Two- and Four-particle Correlations in pPb and P...J. Milošević, Measurement of Two- and Four-particle Correlations in pPb and P...
J. Milošević, Measurement of Two- and Four-particle Correlations in pPb and P...SEENET-MTP
 
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 01 Solutions
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 01 SolutionsCH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 01 Solutions
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 01 Solutionssemihypocrite
 
"When the top is not single: a theory overview from monotop to multitops" to...
"When the top is not single: a theory overview from monotop to multitops"  to..."When the top is not single: a theory overview from monotop to multitops"  to...
"When the top is not single: a theory overview from monotop to multitops" to...Rene Kotze
 

What's hot (20)

IB Chemistry on Energetics, Enthalpy Change and
IB Chemistry on Energetics, Enthalpy Change and IB Chemistry on Energetics, Enthalpy Change and
IB Chemistry on Energetics, Enthalpy Change and
 
One dimensional heat conduction equation
One dimensional heat conduction equationOne dimensional heat conduction equation
One dimensional heat conduction equation
 
Crocus Melting on Mars
Crocus Melting on MarsCrocus Melting on Mars
Crocus Melting on Mars
 
Thermodynamics -Basic concepts
 Thermodynamics -Basic concepts Thermodynamics -Basic concepts
Thermodynamics -Basic concepts
 
Simulated Annealing
Simulated AnnealingSimulated Annealing
Simulated Annealing
 
Unit 3 transient heat condution
Unit 3 transient heat condutionUnit 3 transient heat condution
Unit 3 transient heat condution
 
QM2015Talk_v2
QM2015Talk_v2QM2015Talk_v2
QM2015Talk_v2
 
IB Chemistry on Energetics experiment, Thermodynamics and Hess's Law
IB Chemistry on Energetics experiment, Thermodynamics and Hess's LawIB Chemistry on Energetics experiment, Thermodynamics and Hess's Law
IB Chemistry on Energetics experiment, Thermodynamics and Hess's Law
 
Heat conduction through a plane wall
Heat conduction through a plane wallHeat conduction through a plane wall
Heat conduction through a plane wall
 
conduction
conductionconduction
conduction
 
One dim, steady-state, heat conduction_with_heat_generation
One dim, steady-state, heat conduction_with_heat_generationOne dim, steady-state, heat conduction_with_heat_generation
One dim, steady-state, heat conduction_with_heat_generation
 
Latent heat practical
Latent heat practicalLatent heat practical
Latent heat practical
 
Analysis of solids
Analysis of solidsAnalysis of solids
Analysis of solids
 
Lab 4 (specific latent heat)
Lab 4 (specific latent heat)Lab 4 (specific latent heat)
Lab 4 (specific latent heat)
 
Fins equation & lumped heat capacity system
Fins equation & lumped heat capacity systemFins equation & lumped heat capacity system
Fins equation & lumped heat capacity system
 
J. Milošević, Measurement of Two- and Four-particle Correlations in pPb and P...
J. Milošević, Measurement of Two- and Four-particle Correlations in pPb and P...J. Milošević, Measurement of Two- and Four-particle Correlations in pPb and P...
J. Milošević, Measurement of Two- and Four-particle Correlations in pPb and P...
 
Gravitational Waves and Binary Systems (2) - Thibault Damour
Gravitational Waves and Binary Systems (2) - Thibault DamourGravitational Waves and Binary Systems (2) - Thibault Damour
Gravitational Waves and Binary Systems (2) - Thibault Damour
 
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 01 Solutions
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 01 SolutionsCH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 01 Solutions
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 01 Solutions
 
HEAT (KALOR)
HEAT (KALOR)HEAT (KALOR)
HEAT (KALOR)
 
"When the top is not single: a theory overview from monotop to multitops" to...
"When the top is not single: a theory overview from monotop to multitops"  to..."When the top is not single: a theory overview from monotop to multitops"  to...
"When the top is not single: a theory overview from monotop to multitops" to...
 

Similar to E. von Törne, Overview of the ATLAS Higgs Measurements

Epidemiology Meets Quantum: Statistics, Causality, and Bell's Theorem
Epidemiology Meets Quantum: Statistics, Causality, and Bell's TheoremEpidemiology Meets Quantum: Statistics, Causality, and Bell's Theorem
Epidemiology Meets Quantum: Statistics, Causality, and Bell's TheoremRichard Gill
 
Predrag Milenović "Physics potential of HE/HL-LHC and future circular"
Predrag Milenović "Physics potential of HE/HL-LHC and future circular"Predrag Milenović "Physics potential of HE/HL-LHC and future circular"
Predrag Milenović "Physics potential of HE/HL-LHC and future circular"SEENET-MTP
 
Dragoljub Dimitrijević "Tachyon Inflation in the RSII Framework"
Dragoljub Dimitrijević "Tachyon Inflation in the RSII Framework"Dragoljub Dimitrijević "Tachyon Inflation in the RSII Framework"
Dragoljub Dimitrijević "Tachyon Inflation in the RSII Framework"SEENET-MTP
 
Mass Resconstruction with HEP detectors
Mass Resconstruction with HEP detectorsMass Resconstruction with HEP detectors
Mass Resconstruction with HEP detectorsYuan CHAO
 
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...Lake Como School of Advanced Studies
 
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...Lake Como School of Advanced Studies
 
Pairing and Symmetries in Nuclear Matter
Pairing and Symmetries in Nuclear MatterPairing and Symmetries in Nuclear Matter
Pairing and Symmetries in Nuclear MatterAlex Quadros
 
972 B3102005 Xray3
972 B3102005 Xray3972 B3102005 Xray3
972 B3102005 Xray3praying1
 
Hyperon and charm baryons masses from twisted mass Lattice QCD
Hyperon and charm baryons masses from twisted mass Lattice QCDHyperon and charm baryons masses from twisted mass Lattice QCD
Hyperon and charm baryons masses from twisted mass Lattice QCDChristos Kallidonis
 
optimizedBell.pptx
optimizedBell.pptxoptimizedBell.pptx
optimizedBell.pptxRichard Gill
 
Tachyon inflation in DBI and RSII context
Tachyon inflation in DBI and RSII contextTachyon inflation in DBI and RSII context
Tachyon inflation in DBI and RSII contextMilan Milošević
 
X-ray_Diffraction.ppt
X-ray_Diffraction.pptX-ray_Diffraction.ppt
X-ray_Diffraction.pptSaroseThapa1
 
Results from WZ, Higgs and Top for the Summer Conferences
Results from WZ, Higgs and Top for the Summer ConferencesResults from WZ, Higgs and Top for the Summer Conferences
Results from WZ, Higgs and Top for the Summer ConferencesMedicineAndHealthNeurolog
 

Similar to E. von Törne, Overview of the ATLAS Higgs Measurements (20)

Epidemiology Meets Quantum: Statistics, Causality, and Bell's Theorem
Epidemiology Meets Quantum: Statistics, Causality, and Bell's TheoremEpidemiology Meets Quantum: Statistics, Causality, and Bell's Theorem
Epidemiology Meets Quantum: Statistics, Causality, and Bell's Theorem
 
Predrag Milenović "Physics potential of HE/HL-LHC and future circular"
Predrag Milenović "Physics potential of HE/HL-LHC and future circular"Predrag Milenović "Physics potential of HE/HL-LHC and future circular"
Predrag Milenović "Physics potential of HE/HL-LHC and future circular"
 
MyPaperNMSSMHiggs
MyPaperNMSSMHiggsMyPaperNMSSMHiggs
MyPaperNMSSMHiggs
 
Aalonso_h_to_fermions
Aalonso_h_to_fermionsAalonso_h_to_fermions
Aalonso_h_to_fermions
 
Dragoljub Dimitrijević "Tachyon Inflation in the RSII Framework"
Dragoljub Dimitrijević "Tachyon Inflation in the RSII Framework"Dragoljub Dimitrijević "Tachyon Inflation in the RSII Framework"
Dragoljub Dimitrijević "Tachyon Inflation in the RSII Framework"
 
UCI Seminar
UCI SeminarUCI Seminar
UCI Seminar
 
Mass Resconstruction with HEP detectors
Mass Resconstruction with HEP detectorsMass Resconstruction with HEP detectors
Mass Resconstruction with HEP detectors
 
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...
 
Lecture johnson
Lecture johnsonLecture johnson
Lecture johnson
 
CLIM Fall 2017 Course: Statistics for Climate Research, Guest lecture: Data F...
CLIM Fall 2017 Course: Statistics for Climate Research, Guest lecture: Data F...CLIM Fall 2017 Course: Statistics for Climate Research, Guest lecture: Data F...
CLIM Fall 2017 Course: Statistics for Climate Research, Guest lecture: Data F...
 
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...
The Analytical/Numerical Relativity Interface behind Gravitational Waves: Lec...
 
Bell lund-2
Bell lund-2Bell lund-2
Bell lund-2
 
Pairing and Symmetries in Nuclear Matter
Pairing and Symmetries in Nuclear MatterPairing and Symmetries in Nuclear Matter
Pairing and Symmetries in Nuclear Matter
 
Sgra235
Sgra235Sgra235
Sgra235
 
972 B3102005 Xray3
972 B3102005 Xray3972 B3102005 Xray3
972 B3102005 Xray3
 
Hyperon and charm baryons masses from twisted mass Lattice QCD
Hyperon and charm baryons masses from twisted mass Lattice QCDHyperon and charm baryons masses from twisted mass Lattice QCD
Hyperon and charm baryons masses from twisted mass Lattice QCD
 
optimizedBell.pptx
optimizedBell.pptxoptimizedBell.pptx
optimizedBell.pptx
 
Tachyon inflation in DBI and RSII context
Tachyon inflation in DBI and RSII contextTachyon inflation in DBI and RSII context
Tachyon inflation in DBI and RSII context
 
X-ray_Diffraction.ppt
X-ray_Diffraction.pptX-ray_Diffraction.ppt
X-ray_Diffraction.ppt
 
Results from WZ, Higgs and Top for the Summer Conferences
Results from WZ, Higgs and Top for the Summer ConferencesResults from WZ, Higgs and Top for the Summer Conferences
Results from WZ, Higgs and Top for the Summer Conferences
 

More from SEENET-MTP

SEENET-MTP Booklet - 15 years
SEENET-MTP Booklet - 15 yearsSEENET-MTP Booklet - 15 years
SEENET-MTP Booklet - 15 yearsSEENET-MTP
 
Milan Milošević "The shape of Fe Kα line emitted from relativistic accretion ...
Milan Milošević "The shape of Fe Kα line emitted from relativistic accretion ...Milan Milošević "The shape of Fe Kα line emitted from relativistic accretion ...
Milan Milošević "The shape of Fe Kα line emitted from relativistic accretion ...SEENET-MTP
 
Ivan Dimitrijević "Nonlocal cosmology"
Ivan Dimitrijević "Nonlocal cosmology"Ivan Dimitrijević "Nonlocal cosmology"
Ivan Dimitrijević "Nonlocal cosmology"SEENET-MTP
 
Vesna Borka Jovanović "Constraining Scalar-Tensor gravity models by S2 star o...
Vesna Borka Jovanović "Constraining Scalar-Tensor gravity models by S2 star o...Vesna Borka Jovanović "Constraining Scalar-Tensor gravity models by S2 star o...
Vesna Borka Jovanović "Constraining Scalar-Tensor gravity models by S2 star o...SEENET-MTP
 
Elena Mirela Babalic "Generalized alpha-attractor models for hyperbolic surfa...
Elena Mirela Babalic "Generalized alpha-attractor models for hyperbolic surfa...Elena Mirela Babalic "Generalized alpha-attractor models for hyperbolic surfa...
Elena Mirela Babalic "Generalized alpha-attractor models for hyperbolic surfa...SEENET-MTP
 
Dragan Huterer "Novi pogledi na svemir"
Dragan Huterer "Novi pogledi na svemir"Dragan Huterer "Novi pogledi na svemir"
Dragan Huterer "Novi pogledi na svemir"SEENET-MTP
 
Mihai Visinescu "Action-angle variables for geodesic motion on resolved metri...
Mihai Visinescu "Action-angle variables for geodesic motion on resolved metri...Mihai Visinescu "Action-angle variables for geodesic motion on resolved metri...
Mihai Visinescu "Action-angle variables for geodesic motion on resolved metri...SEENET-MTP
 
Sabin Stoica "Double beta decay and neutrino properties"
Sabin Stoica "Double beta decay and neutrino properties"Sabin Stoica "Double beta decay and neutrino properties"
Sabin Stoica "Double beta decay and neutrino properties"SEENET-MTP
 
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...SEENET-MTP
 
Marija Dimitrijević Ćirić "Matter Fields in SO(2,3)⋆ Model of Noncommutative ...
Marija Dimitrijević Ćirić "Matter Fields in SO(2,3)⋆ Model of Noncommutative ...Marija Dimitrijević Ćirić "Matter Fields in SO(2,3)⋆ Model of Noncommutative ...
Marija Dimitrijević Ćirić "Matter Fields in SO(2,3)⋆ Model of Noncommutative ...SEENET-MTP
 
Zvonimir Vlah "Lagrangian perturbation theory for large scale structure forma...
Zvonimir Vlah "Lagrangian perturbation theory for large scale structure forma...Zvonimir Vlah "Lagrangian perturbation theory for large scale structure forma...
Zvonimir Vlah "Lagrangian perturbation theory for large scale structure forma...SEENET-MTP
 
Vitaly Vanchurin "General relativity from non-equilibrium thermodynamics of q...
Vitaly Vanchurin "General relativity from non-equilibrium thermodynamics of q...Vitaly Vanchurin "General relativity from non-equilibrium thermodynamics of q...
Vitaly Vanchurin "General relativity from non-equilibrium thermodynamics of q...SEENET-MTP
 
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...SEENET-MTP
 
Radoslav Rashkov "Integrable structures in low-dimensional holography and cos...
Radoslav Rashkov "Integrable structures in low-dimensional holography and cos...Radoslav Rashkov "Integrable structures in low-dimensional holography and cos...
Radoslav Rashkov "Integrable structures in low-dimensional holography and cos...SEENET-MTP
 
Nikola Godinović "The very high energy gamma ray astronomy"
Nikola Godinović "The very high energy gamma ray astronomy"Nikola Godinović "The very high energy gamma ray astronomy"
Nikola Godinović "The very high energy gamma ray astronomy"SEENET-MTP
 
Miroljub Dugić "The concept of Local Time. Quantum-mechanical and cosmologica...
Miroljub Dugić "The concept of Local Time. Quantum-mechanical and cosmologica...Miroljub Dugić "The concept of Local Time. Quantum-mechanical and cosmologica...
Miroljub Dugić "The concept of Local Time. Quantum-mechanical and cosmologica...SEENET-MTP
 
Cemsinan Deliduman "Astrophysics with Weyl Gravity"
Cemsinan Deliduman "Astrophysics with Weyl Gravity"Cemsinan Deliduman "Astrophysics with Weyl Gravity"
Cemsinan Deliduman "Astrophysics with Weyl Gravity"SEENET-MTP
 
Radu Constantinescu "Scientific research: Excellence in International context"
Radu Constantinescu "Scientific research: Excellence in International context"Radu Constantinescu "Scientific research: Excellence in International context"
Radu Constantinescu "Scientific research: Excellence in International context"SEENET-MTP
 
Loriano Bonora "HS theories from effective actions"
Loriano Bonora "HS theories from effective actions"Loriano Bonora "HS theories from effective actions"
Loriano Bonora "HS theories from effective actions"SEENET-MTP
 
Borut Bajc "Asymptotic safety"
Borut Bajc "Asymptotic safety"Borut Bajc "Asymptotic safety"
Borut Bajc "Asymptotic safety"SEENET-MTP
 

More from SEENET-MTP (20)

SEENET-MTP Booklet - 15 years
SEENET-MTP Booklet - 15 yearsSEENET-MTP Booklet - 15 years
SEENET-MTP Booklet - 15 years
 
Milan Milošević "The shape of Fe Kα line emitted from relativistic accretion ...
Milan Milošević "The shape of Fe Kα line emitted from relativistic accretion ...Milan Milošević "The shape of Fe Kα line emitted from relativistic accretion ...
Milan Milošević "The shape of Fe Kα line emitted from relativistic accretion ...
 
Ivan Dimitrijević "Nonlocal cosmology"
Ivan Dimitrijević "Nonlocal cosmology"Ivan Dimitrijević "Nonlocal cosmology"
Ivan Dimitrijević "Nonlocal cosmology"
 
Vesna Borka Jovanović "Constraining Scalar-Tensor gravity models by S2 star o...
Vesna Borka Jovanović "Constraining Scalar-Tensor gravity models by S2 star o...Vesna Borka Jovanović "Constraining Scalar-Tensor gravity models by S2 star o...
Vesna Borka Jovanović "Constraining Scalar-Tensor gravity models by S2 star o...
 
Elena Mirela Babalic "Generalized alpha-attractor models for hyperbolic surfa...
Elena Mirela Babalic "Generalized alpha-attractor models for hyperbolic surfa...Elena Mirela Babalic "Generalized alpha-attractor models for hyperbolic surfa...
Elena Mirela Babalic "Generalized alpha-attractor models for hyperbolic surfa...
 
Dragan Huterer "Novi pogledi na svemir"
Dragan Huterer "Novi pogledi na svemir"Dragan Huterer "Novi pogledi na svemir"
Dragan Huterer "Novi pogledi na svemir"
 
Mihai Visinescu "Action-angle variables for geodesic motion on resolved metri...
Mihai Visinescu "Action-angle variables for geodesic motion on resolved metri...Mihai Visinescu "Action-angle variables for geodesic motion on resolved metri...
Mihai Visinescu "Action-angle variables for geodesic motion on resolved metri...
 
Sabin Stoica "Double beta decay and neutrino properties"
Sabin Stoica "Double beta decay and neutrino properties"Sabin Stoica "Double beta decay and neutrino properties"
Sabin Stoica "Double beta decay and neutrino properties"
 
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...
 
Marija Dimitrijević Ćirić "Matter Fields in SO(2,3)⋆ Model of Noncommutative ...
Marija Dimitrijević Ćirić "Matter Fields in SO(2,3)⋆ Model of Noncommutative ...Marija Dimitrijević Ćirić "Matter Fields in SO(2,3)⋆ Model of Noncommutative ...
Marija Dimitrijević Ćirić "Matter Fields in SO(2,3)⋆ Model of Noncommutative ...
 
Zvonimir Vlah "Lagrangian perturbation theory for large scale structure forma...
Zvonimir Vlah "Lagrangian perturbation theory for large scale structure forma...Zvonimir Vlah "Lagrangian perturbation theory for large scale structure forma...
Zvonimir Vlah "Lagrangian perturbation theory for large scale structure forma...
 
Vitaly Vanchurin "General relativity from non-equilibrium thermodynamics of q...
Vitaly Vanchurin "General relativity from non-equilibrium thermodynamics of q...Vitaly Vanchurin "General relativity from non-equilibrium thermodynamics of q...
Vitaly Vanchurin "General relativity from non-equilibrium thermodynamics of q...
 
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...
 
Radoslav Rashkov "Integrable structures in low-dimensional holography and cos...
Radoslav Rashkov "Integrable structures in low-dimensional holography and cos...Radoslav Rashkov "Integrable structures in low-dimensional holography and cos...
Radoslav Rashkov "Integrable structures in low-dimensional holography and cos...
 
Nikola Godinović "The very high energy gamma ray astronomy"
Nikola Godinović "The very high energy gamma ray astronomy"Nikola Godinović "The very high energy gamma ray astronomy"
Nikola Godinović "The very high energy gamma ray astronomy"
 
Miroljub Dugić "The concept of Local Time. Quantum-mechanical and cosmologica...
Miroljub Dugić "The concept of Local Time. Quantum-mechanical and cosmologica...Miroljub Dugić "The concept of Local Time. Quantum-mechanical and cosmologica...
Miroljub Dugić "The concept of Local Time. Quantum-mechanical and cosmologica...
 
Cemsinan Deliduman "Astrophysics with Weyl Gravity"
Cemsinan Deliduman "Astrophysics with Weyl Gravity"Cemsinan Deliduman "Astrophysics with Weyl Gravity"
Cemsinan Deliduman "Astrophysics with Weyl Gravity"
 
Radu Constantinescu "Scientific research: Excellence in International context"
Radu Constantinescu "Scientific research: Excellence in International context"Radu Constantinescu "Scientific research: Excellence in International context"
Radu Constantinescu "Scientific research: Excellence in International context"
 
Loriano Bonora "HS theories from effective actions"
Loriano Bonora "HS theories from effective actions"Loriano Bonora "HS theories from effective actions"
Loriano Bonora "HS theories from effective actions"
 
Borut Bajc "Asymptotic safety"
Borut Bajc "Asymptotic safety"Borut Bajc "Asymptotic safety"
Borut Bajc "Asymptotic safety"
 

Recently uploaded

Beyond the EU: DORA and NIS 2 Directive's Global Impact
Beyond the EU: DORA and NIS 2 Directive's Global ImpactBeyond the EU: DORA and NIS 2 Directive's Global Impact
Beyond the EU: DORA and NIS 2 Directive's Global ImpactPECB
 
18-04-UA_REPORT_MEDIALITERAСY_INDEX-DM_23-1-final-eng.pdf
18-04-UA_REPORT_MEDIALITERAСY_INDEX-DM_23-1-final-eng.pdf18-04-UA_REPORT_MEDIALITERAСY_INDEX-DM_23-1-final-eng.pdf
18-04-UA_REPORT_MEDIALITERAСY_INDEX-DM_23-1-final-eng.pdfssuser54595a
 
Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...
Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...
Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...EduSkills OECD
 
Introduction to ArtificiaI Intelligence in Higher Education
Introduction to ArtificiaI Intelligence in Higher EducationIntroduction to ArtificiaI Intelligence in Higher Education
Introduction to ArtificiaI Intelligence in Higher Educationpboyjonauth
 
Employee wellbeing at the workplace.pptx
Employee wellbeing at the workplace.pptxEmployee wellbeing at the workplace.pptx
Employee wellbeing at the workplace.pptxNirmalaLoungPoorunde1
 
Activity 01 - Artificial Culture (1).pdf
Activity 01 - Artificial Culture (1).pdfActivity 01 - Artificial Culture (1).pdf
Activity 01 - Artificial Culture (1).pdfciinovamais
 
Hybridoma Technology ( Production , Purification , and Application )
Hybridoma Technology  ( Production , Purification , and Application  ) Hybridoma Technology  ( Production , Purification , and Application  )
Hybridoma Technology ( Production , Purification , and Application ) Sakshi Ghasle
 
CARE OF CHILD IN INCUBATOR..........pptx
CARE OF CHILD IN INCUBATOR..........pptxCARE OF CHILD IN INCUBATOR..........pptx
CARE OF CHILD IN INCUBATOR..........pptxGaneshChakor2
 
Separation of Lanthanides/ Lanthanides and Actinides
Separation of Lanthanides/ Lanthanides and ActinidesSeparation of Lanthanides/ Lanthanides and Actinides
Separation of Lanthanides/ Lanthanides and ActinidesFatimaKhan178732
 
Mastering the Unannounced Regulatory Inspection
Mastering the Unannounced Regulatory InspectionMastering the Unannounced Regulatory Inspection
Mastering the Unannounced Regulatory InspectionSafetyChain Software
 
Industrial Policy - 1948, 1956, 1973, 1977, 1980, 1991
Industrial Policy - 1948, 1956, 1973, 1977, 1980, 1991Industrial Policy - 1948, 1956, 1973, 1977, 1980, 1991
Industrial Policy - 1948, 1956, 1973, 1977, 1980, 1991RKavithamani
 
microwave assisted reaction. General introduction
microwave assisted reaction. General introductionmicrowave assisted reaction. General introduction
microwave assisted reaction. General introductionMaksud Ahmed
 
mini mental status format.docx
mini    mental       status     format.docxmini    mental       status     format.docx
mini mental status format.docxPoojaSen20
 
Nutritional Needs Presentation - HLTH 104
Nutritional Needs Presentation - HLTH 104Nutritional Needs Presentation - HLTH 104
Nutritional Needs Presentation - HLTH 104misteraugie
 
1029 - Danh muc Sach Giao Khoa 10 . pdf
1029 -  Danh muc Sach Giao Khoa 10 . pdf1029 -  Danh muc Sach Giao Khoa 10 . pdf
1029 - Danh muc Sach Giao Khoa 10 . pdfQucHHunhnh
 
Call Girls in Dwarka Mor Delhi Contact Us 9654467111
Call Girls in Dwarka Mor Delhi Contact Us 9654467111Call Girls in Dwarka Mor Delhi Contact Us 9654467111
Call Girls in Dwarka Mor Delhi Contact Us 9654467111Sapana Sha
 
Kisan Call Centre - To harness potential of ICT in Agriculture by answer farm...
Kisan Call Centre - To harness potential of ICT in Agriculture by answer farm...Kisan Call Centre - To harness potential of ICT in Agriculture by answer farm...
Kisan Call Centre - To harness potential of ICT in Agriculture by answer farm...Krashi Coaching
 
Grant Readiness 101 TechSoup and Remy Consulting
Grant Readiness 101 TechSoup and Remy ConsultingGrant Readiness 101 TechSoup and Remy Consulting
Grant Readiness 101 TechSoup and Remy ConsultingTechSoup
 
Contemporary philippine arts from the regions_PPT_Module_12 [Autosaved] (1).pptx
Contemporary philippine arts from the regions_PPT_Module_12 [Autosaved] (1).pptxContemporary philippine arts from the regions_PPT_Module_12 [Autosaved] (1).pptx
Contemporary philippine arts from the regions_PPT_Module_12 [Autosaved] (1).pptxRoyAbrique
 

Recently uploaded (20)

TataKelola dan KamSiber Kecerdasan Buatan v022.pdf
TataKelola dan KamSiber Kecerdasan Buatan v022.pdfTataKelola dan KamSiber Kecerdasan Buatan v022.pdf
TataKelola dan KamSiber Kecerdasan Buatan v022.pdf
 
Beyond the EU: DORA and NIS 2 Directive's Global Impact
Beyond the EU: DORA and NIS 2 Directive's Global ImpactBeyond the EU: DORA and NIS 2 Directive's Global Impact
Beyond the EU: DORA and NIS 2 Directive's Global Impact
 
18-04-UA_REPORT_MEDIALITERAСY_INDEX-DM_23-1-final-eng.pdf
18-04-UA_REPORT_MEDIALITERAСY_INDEX-DM_23-1-final-eng.pdf18-04-UA_REPORT_MEDIALITERAСY_INDEX-DM_23-1-final-eng.pdf
18-04-UA_REPORT_MEDIALITERAСY_INDEX-DM_23-1-final-eng.pdf
 
Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...
Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...
Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...
 
Introduction to ArtificiaI Intelligence in Higher Education
Introduction to ArtificiaI Intelligence in Higher EducationIntroduction to ArtificiaI Intelligence in Higher Education
Introduction to ArtificiaI Intelligence in Higher Education
 
Employee wellbeing at the workplace.pptx
Employee wellbeing at the workplace.pptxEmployee wellbeing at the workplace.pptx
Employee wellbeing at the workplace.pptx
 
Activity 01 - Artificial Culture (1).pdf
Activity 01 - Artificial Culture (1).pdfActivity 01 - Artificial Culture (1).pdf
Activity 01 - Artificial Culture (1).pdf
 
Hybridoma Technology ( Production , Purification , and Application )
Hybridoma Technology  ( Production , Purification , and Application  ) Hybridoma Technology  ( Production , Purification , and Application  )
Hybridoma Technology ( Production , Purification , and Application )
 
CARE OF CHILD IN INCUBATOR..........pptx
CARE OF CHILD IN INCUBATOR..........pptxCARE OF CHILD IN INCUBATOR..........pptx
CARE OF CHILD IN INCUBATOR..........pptx
 
Separation of Lanthanides/ Lanthanides and Actinides
Separation of Lanthanides/ Lanthanides and ActinidesSeparation of Lanthanides/ Lanthanides and Actinides
Separation of Lanthanides/ Lanthanides and Actinides
 
Mastering the Unannounced Regulatory Inspection
Mastering the Unannounced Regulatory InspectionMastering the Unannounced Regulatory Inspection
Mastering the Unannounced Regulatory Inspection
 
Industrial Policy - 1948, 1956, 1973, 1977, 1980, 1991
Industrial Policy - 1948, 1956, 1973, 1977, 1980, 1991Industrial Policy - 1948, 1956, 1973, 1977, 1980, 1991
Industrial Policy - 1948, 1956, 1973, 1977, 1980, 1991
 
microwave assisted reaction. General introduction
microwave assisted reaction. General introductionmicrowave assisted reaction. General introduction
microwave assisted reaction. General introduction
 
mini mental status format.docx
mini    mental       status     format.docxmini    mental       status     format.docx
mini mental status format.docx
 
Nutritional Needs Presentation - HLTH 104
Nutritional Needs Presentation - HLTH 104Nutritional Needs Presentation - HLTH 104
Nutritional Needs Presentation - HLTH 104
 
1029 - Danh muc Sach Giao Khoa 10 . pdf
1029 -  Danh muc Sach Giao Khoa 10 . pdf1029 -  Danh muc Sach Giao Khoa 10 . pdf
1029 - Danh muc Sach Giao Khoa 10 . pdf
 
Call Girls in Dwarka Mor Delhi Contact Us 9654467111
Call Girls in Dwarka Mor Delhi Contact Us 9654467111Call Girls in Dwarka Mor Delhi Contact Us 9654467111
Call Girls in Dwarka Mor Delhi Contact Us 9654467111
 
Kisan Call Centre - To harness potential of ICT in Agriculture by answer farm...
Kisan Call Centre - To harness potential of ICT in Agriculture by answer farm...Kisan Call Centre - To harness potential of ICT in Agriculture by answer farm...
Kisan Call Centre - To harness potential of ICT in Agriculture by answer farm...
 
Grant Readiness 101 TechSoup and Remy Consulting
Grant Readiness 101 TechSoup and Remy ConsultingGrant Readiness 101 TechSoup and Remy Consulting
Grant Readiness 101 TechSoup and Remy Consulting
 
Contemporary philippine arts from the regions_PPT_Module_12 [Autosaved] (1).pptx
Contemporary philippine arts from the regions_PPT_Module_12 [Autosaved] (1).pptxContemporary philippine arts from the regions_PPT_Module_12 [Autosaved] (1).pptx
Contemporary philippine arts from the regions_PPT_Module_12 [Autosaved] (1).pptx
 

E. von Törne, Overview of the ATLAS Higgs Measurements

  • 1. 1Eckhard von Toerne, Bonn ATLAS Higgs Measurements Talk at BW 2013 – Beyond the Standard Models 25 – 29 April, 2013, Vrnjačka Banja, Serbia Overview of the ATLAS Higgs Measurements Eckhard von Toerne University of Bonn on behalf of the ATLAS Collaboration
  • 2. 2Eckhard von Toerne, Bonn ATLAS Higgs Measurements • “Observation of a new particle” in July 2012 • Overview of properties: mass, spin/parity, (couplings) • A Note: While existence of new boson at mass of ~125 GeV is undisputed, its nature is under active study. Boson exhibits Higgs-like properties. For brevity the term “Higgs-like boson” is shortened to Higgs boson or Higgs (working hypothesis). PLB 716(2012) 1-29, http://arxiv.org/abs/1207.7214 Introduction See also: ATLAS Coll., Science 338, 1576 (2012)
  • 3. 3Eckhard von Toerne, Bonn ATLAS Higgs Measurements • x Production of SM Higgs @ LHC Cross sections at 8 TeV [pb] ggH 19.4 VB Fusion 1.6 WH+ZH 1.1 ttH 0.1 mH = 125.5 GeV
  • 4. 4Eckhard von Toerne, Bonn ATLAS Higgs Measurements Decay of SM Higgs 56.9 % bb 22.3 % WW 6.2 % 2.8 % ZZ 0.23 % γγ @ mH=125.5 GeV
  • 5. 5Eckhard von Toerne, Bonn ATLAS Higgs Measurements • x LHC runs in 2011 + 2012 Z→μμ event with 25 reconstructed vertices
  • 6. 6Eckhard von Toerne, Bonn ATLAS Higgs Measurements ATLAS detector
  • 7. 7Eckhard von Toerne, Bonn ATLAS Higgs Measurements • Two isolated high-pt photons (ET>40, 30 GeV) • Mass peak with resolution 1.77 GeV above large backgr. (S/B=3%). • Reducible backgr. j, jj (~25%) • Irreducible bgd from QED reaction qq (~75%) • Example event with m =126.6 GeV H
  • 8. 8Eckhard von Toerne, Bonn ATLAS Higgs Measurements • Two isolated high-pt photons (ET>40, 30 GeV) • Mass peak with resolution 1.77 GeV above large backgr. (S/B=3%). • Reducible backgr. j, jj (~25%) • Irreducible bgd from QED reaction qq (~75%) • Example event with m =126.6 GeV H Zoom into Calorimeter cluster • Layered Calorimeter  • Photon direction • Selection of vertex
  • 9. 9Eckhard von Toerne, Bonn ATLAS Higgs Measurements local significance: - observed: 7.4σ -expected -(SM Higgs): 4.1σ Best fit mass: 126.8 ± 0.2 (stat) ± 0.7 (syst) GeV Signal Strength µ = obs/ SM = 1.65 ± 0.24(stat) ± 0.22(syst) H Prob. of a background fluctuation to be more signal- like than observed signal.
  • 10. 10Eckhard von Toerne, Bonn ATLAS Higgs Measurements H • 2.0 excess for VBF production over bgd. • 14 categories to optimize sensitivity (different S/B ratios) • and to categorize ggF, VBF, VH
  • 11. 11Eckhard von Toerne, Bonn ATLAS Higgs Measurements HZZ(*) ATLAS-CONF-2013-013 mH = 124.3 ± 0.6 (stat) ± 0.4 (syst) GeV μ (124.3 GeV) = 1.7 ± 0.4 Need to reconstruct low pt leptons
  • 12. 12Eckhard von Toerne, Bonn ATLAS Higgs Measurements HZZ(*) ATLAS-CONF-2013-013 mH = 124.3 ± 0.6 (stat) ± 0.4 (syst) GeV μ (124.3 GeV) = 1.7 ± 0.4
  • 13. 13Eckhard von Toerne, Bonn ATLAS Higgs Measurements • x H  ZZ(*)  4 µ m12=86.3 GeV, m34=31.6 GeV, m4μ = 125.1 GeV, ATLAS-CONF-2012-169
  • 14. 14Eckhard von Toerne, Bonn ATLAS Higgs Measurements Higgs mass combination Combined ATLAS result Difference reduced by 700 MeV compared to December result Considering all systematics and their correlations, compatibility of both results is at 1.5% (2.4σ level) With alternative treatment of systematics, compatibility rises to 8% Main systematics: energy scale mH = 125.5 ± 0.2 (stat) ± 0.6 (syst) GeV
  • 15. 15Eckhard von Toerne, Bonn ATLAS Higgs Measurements • limited mass sensitivity due to neutrino contribution • Transverse mass • S/B ~ 15% HWW
  • 16. 16Eckhard von Toerne, Bonn ATLAS Higgs Measurements • Observed significance (125 GeV) 3.8σ (3.7σ expected) • Signal strength at 125 GeV μ = 1.01 ± 0.21(stat) ± 0.23(syst) [ 0.21(stat) ± 0.19(theo) ± 0.12(exp) ± 0.04(lumi) ] HWW
  • 17. 17Eckhard von Toerne, Bonn ATLAS Higgs Measurements • x Hbb • Limits derived from Mbb distribution (~16% mass resolution) • 95%CL limit at 125 GeV: 1.8 x SM (expected limit 1.9) • μ(125) = -0.4 ± 0.7(stat) ± 0.8(syst), • Analysis still in flux and not all of 2012 data used • Main benchmark analysis yields 4.0σ observation of boson pairs WZ(bb)/ZZ(bb) Combination of search channel WH, Wl / ZH, Zll / ZH, Z
  • 18. 18Eckhard von Toerne, Bonn ATLAS Higgs Measurements • x Hbb candidate
  • 19. 19Eckhard von Toerne, Bonn ATLAS Higgs Measurements • x H candidate
  • 20. 20Eckhard von Toerne, Bonn ATLAS Higgs Measurements • Global compatibility between presented channels and the SM expectation is 8% • Dependence of signal strength on mass is weak ATLAS combined signal strength ATLAS-CONF-2013-034
  • 21. 21Eckhard von Toerne, Bonn ATLAS Higgs Measurements ATLAS combined Higgs signal significance Moriond 2013 status, ATLAS-CONF-2013-034 • Combination of all channels • Local p0 = 10-23 •  ~10 excess around 125 GeV
  • 22. 22Eckhard von Toerne, Bonn ATLAS Higgs Measurements Spin and Parity • SM predicts JP=0+ • Spin studies in three different modes • H : sensitivity decay angle in Higgs rest frame * • HWW decy angles no directly reconstructable due to neutrinos, however other kinematic vars. quite sensitive due to V-A nature of W decays. • HZZ fully reconstructed, decay plane is sensitive • Spin 1 disfavored by Landau-Yang theorem and H decay • Spin 2 case may be quite evolved • Here: tensor with minimal couplings to SM particles (2+ m model) • Dependency on 2+ m production mode.  free parameter fqq, fqq+fgg=1
  • 23. 23Eckhard von Toerne, Bonn ATLAS Higgs Measurements • Spin information from cosθ* shape, not sensitive to parity • Minimize correlation between cosθ* and mass for bgd by applying absolute pt cuts • control the background cosθ* shape via mass sidebands • Largest sensitivity if 2+ m is created by 100% gg fusion Spin and Parity: H
  • 24. 24Eckhard von Toerne, Bonn ATLAS Higgs Measurements Spin and Parity: HZZ(*) Combine all kinematic variables in a Boosted Decision Tree to optimize sensitivity sensitive to parity
  • 25. 25Eckhard von Toerne, Bonn ATLAS Higgs Measurements Spin and Parity: HWW ATLAS-CONF-2013-031 0+ Hyp. 2+ Hyp. BDT to combine all sensitive variables, most sensitive: fqq=100%
  • 26. 26Eckhard von Toerne, Bonn ATLAS Higgs Measurements • the 3 channels combined exclude 2+ m scenario at 99.9% CL • ZZ analysis excludes the 0-, 1+ and (1-) hypotheses at the >95% (94%) CL Spin and Parity: combined ATLAS-CONF-2013-040
  • 27. 27Eckhard von Toerne, Bonn ATLAS Higgs Measurements • Overwhelming evidence for a new boson at • M = 125.5 ± 0.2 (stat) ± 0.6 (syst) GeV • Measurements of signal strength and spin/parity in agreement with SM hypothesis. • Not covered in this talk: Meas. of couplings also in good agreement. • Improved measurements of pre-shutdown data and after shutdown will further investigate this particle. • Search for rare decays • Search for additional states • Moving towards precision Higgs Physics • …if something walks like a duck and quacks like a duck, it is probably a duck. This particle is looking more and more like a Higgs boson. Conclusion and Outlook
  • 28. 28Eckhard von Toerne, Bonn ATLAS Higgs Measurements • x https://twiki.cern.ch/twiki/bin/view/AtlasPublic/HiggsPublicResults
  • 29. 29Eckhard von Toerne, Bonn ATLAS Higgs Measurements Additional Slides
  • 30. 30Eckhard von Toerne, Bonn ATLAS Higgs Measurements • x Higgs Mass
  • 31. 31Eckhard von Toerne, Bonn ATLAS Higgs Measurements
  • 32. 32Eckhard von Toerne, Bonn ATLAS Higgs Measurements • ATLAS-CONF-2012-101 ATLAS ET-mis Performance
  • 33. 33Eckhard von Toerne, Bonn ATLAS Higgs Measurements Higgs couplings Overview Good agreement with SM prediction If µVBF tested alone  3.1 evidence for VBF production
  • 34. 34Eckhard von Toerne, Bonn ATLAS Higgs Measurements Fermion vs. vector couplings 2-parameter model, group fermion and vector couplings together κV = κZ = κW ; κF = κt = κb = κ = κg = κ We assume only SM-loop contributions to kg and k One overall un-observable sign, chose kV>0 Sign sensitivity mostly from interference in Hgg (t vs W in loop) Only slight preference for kF>0  no conclusions yet 2D compatibility with SM 8%
  • 35. 35Eckhard von Toerne, Bonn ATLAS Higgs Measurements • Custodial symmetry protects ratio of W, Z couplings (λWZ). W vs Z couplings λWZ = 0.80 ± 0.15 in agreement with SM prediction
  • 36. 36Eckhard von Toerne, Bonn ATLAS Higgs Measurements HZZ(*) spin variables, example: decay plane phi
  • 37. 37Eckhard von Toerne, Bonn ATLAS Higgs Measurements HWW spin variables, example: deltaPhi