m H = ± 0.24GeV

Similar documents
Electroweak baryogenesis as a probe of new physics

Higgs physics as a probe of electroweak baryogenesis

The Higgs boson. Marina Cobal University of Udine

Higgs boson(s) in the NMSSM

Decoupling and Alignment in Light of the Higgs Data. Howard E. Haber Pi Day, 2014 Bay Area ParCcle Physics Seminar San Francisco State Univ.

Properties of the Higgs Boson, and its interpretation in Supersymmetry

Kinematics in Higgs Fits

Can the Hbb coupling be equal in magnitude to its Standard Model value but opposite in sign? Howard E. Haber July 22, 2014

Junichi TANAKA ICEPP, the University of Tokyo. 13 Feb, 2013 in Japan

A Minimal Composite Goldstone Higgs model

Probing Higgs Self Coupling at the LHC and future Colliders. Jung Chang, KC, Jae Sik Lee, Chih-Ting Lu, ; in preparation.

Electroweak baryogenesis from a dark sector

LHC Higgs Signatures from Extended Electroweak Guage Symmetry

Search for Higgs in H WW lνlν

Little Higgs at the LHC: Status and Prospects

No-Bend Orthogonal Drawings of Subdivisions of Planar Triconnected Cubic Graphs

Search for di-higgs to 4b with the ATLAS detector. Tony(Baojia)Tong, Harvard University CLHCP, PKU, Dec. 18, 2016

A realistic model for DM interactions in the neutrino portal paradigm

Hidden two-higgs doublet model

Testing the Electroweak Baryogenesis at the LHC and CEPC

Precision tools and models to narrow in on the 750 GeV diphoton resonance

TLEP White Paper : Executive Summary

Higgs and Precision Electroweak Data

tth searches at ATLAS and CMS Thomas CALVET for the ATLAS and CMS collaborations Stony Brook University Apr 11 th, 2018

MSSM Higgs self-couplings at two-loop

LHC Run1 Higgs Results. Quentin Buat - Simon Fraser University On behalf of the ATLAS and CMS collaborations

Inert Doublet Model:

New opportunities on diboson

acclamation. sophomores, their roomer, George P. Burdell, who

ATLAS Preliminary. Signal strength (µ) Combined 0.3. = 126 GeV (*) (*) s = 7 TeV: Ldt = fb. s = 8 TeV: Ldt = 5.

Flavor in the scalar sector of Warped Extra Dimensions a. Manuel Toharia

The Inert Doublet Matter

Higgs Boson Couplings as a Probe of New Physics

D0 Higgs Results and Tevatron Higgs Combination

Higgs Couplings and Electroweak Phase Transition

"INDEPENDENT IN AI.L THINOS. NEUTRAI. IN NOTHINO' LOWELL, MICHIGAN, JAM AHV, 19, WHOLE NO. 290.

Electroweak phase transition with two Higgs doublets near the alignment limit

Higgs couplings. beyond the Standard Model. Giacomo Cacciapaglia (IPN Lyon, France) IHEP Beijing

Electroweak Baryogenesis after LHC8

ANSWER KEY. Page 1 Page 2 cake key pie boat glue cat sled pig fox sun dog fish zebra. Page 3. Page 7. Page 6

Exploring Extended Scalar Sectors with Di Higgs Signals: A Higgs EFT Perspective

Studies of Higgs Potential (Higgs Boson Self Coupling Measurements)

Impact of a CP-violating Higgs Boson

Higgs Signals and Implications for MSSM

Heavy Vector Searches at the LHC

8.882 LHC Physics. Higgs Physics and Other Essentials. [Lecture 22, April 29, 2009] Experimental Methods and Measurements

Search for Invisible Decay of Higgs boson at LHC

Electroweak-scale Right-handed Neutrino Model And 126 GeV Higgs-like Particle

Statistics for the LHC Lecture 2: Discovery

Phenomenology of a light singlet-like scalar in NMSSM

Status of low energy SUSY models confronted with the 125 GeV Higgs data

Entropy, Baryon Asymmetry and Dark Matter from Heavy Neutrino Decays.

Light Higgs Discovery Potential with ATLAS, Measurements of Couplings and

5. Higgs Searches. The Higgs-mechanism in the SM Yukava-coupling, masses of fermions Higgs Production: Higgs decay channels. Higgs search at the LHC

Grover s algorithm. We want to find aa. Search in an unordered database. QC oracle (as usual) Usual trick

Higgs-charm Couplings

Vector boson scattering and triboson studies at ATLAS. Junjie Zhu University of Michigan May 25, 2017

Higgs Searches and Properties Measurement with ATLAS. Haijun Yang (on behalf of the ATLAS) Shanghai Jiao Tong University

12 Best Reasons to Like CP Violation

Observation of the Higgs boson production in association with top quarks

CMS Higgs Results Adi Bornheim Caltech

Natural SUSY and the LHC

Testing the low scale seesaw and leptogenesis

OIL & GAS EQUIPMENT RENTAL SOLUTIONS

CBSE , ˆj. cos CBSE_2015_SET-1. SECTION A 1. Given that a 2iˆ ˆj. We need to find. 3. Consider the vector equation of the plane.

Natural Electroweak Symmetry Breaking in NMSSM and Higgs at 100 GeV

Electroweak Baryogenesis

Higgs in the light of Hadron Collider limits: impact on a 4th generation

e e Collisions at ELIC

" = Y(#,$) % R(r) = 1 4& % " = Y(#,$) % R(r) = Recitation Problems: Week 4. a. 5 B, b. 6. , Ne Mg + 15 P 2+ c. 23 V,

Triplet Higgs Scenarios

Top properties and ttv LHC

at the Higgs factory

Evidence for tth production at ATLAS

WIMP dark matter and Baryogenesis

HiggsSignals. Testing BSM physics with LHC Higgs precision data. Tim Stefaniak. Deutsches Elektronen-Synchrotron DESY, Hamburg

The production of additional bosons and the impact on the Large Hadron Collider

Higgs Property Measurement with ATLAS

Evidence for Higgs Boson Decays to a Pair of τ-leptons

HKIAS Jan Higgcision. Higgs Boson Pair Production

Higgs Boson Physics at the Tevatron

Probing SUSY Contributions to Muon g-2 at LHC and ILC

Lepton non-universality at LEP and charged Higgs

The 2HDM in light of the recent LHC results. Rui Santos

1. The graph of a function f is given above. Answer the question: a. Find the value(s) of x where f is not differentiable. Ans: x = 4, x = 3, x = 2,

Higgs Physics. Yasuhiro Okada (KEK) November 26, 2004, at KEK

Search for SM Higgs Boson at CMS

Highlights of the MCTP Symposium on Higgs Boson Physics

Prospects and Blind Spots for Neutralino Dark Matter

Radiative penguins at hadron machines. Kevin Stenson! University of Colorado!

Unitarization procedures applied to a Strongly Interacting EWSBS

Higgs quantum numbers and couplings. E. Pianori University Of Warwick On behalf of the ATLAS and CMS collaborations

Composite Higgs and Flavor

Higgs Boson Physics, Part II

arxiv: v1 [hep-ph] 16 Mar 2017

Searching for neutral Higgs bosons in non-standard channels

Theory of the ElectroWeak Interactions

Light scalar at the high energy and intensity frontiers: example in the minimal left-right model

Electroweak unification

Have we seen a Higgs boson?

Transcription:

m H = 125.09 ± 0.24GeV

Y B n B s =(8.59 ± 0.11) 10 11 n B = n b n b( b) : n b s :

W = g 2 2/4 (s) B ( W T ) 4 =0.1 1.0 (b) B T 4 e E sph/t E sph :

v(t ) v v C T T C v C T C

V e (T ) T>T C T = T C T =0 T C v C v v C

v =0 v =0

v =0 v =0

v =0 v =0 n B = n L b n L b + n R b n R b =0 =0 =0

v =0 v =0 n B = n L b n L b + n R b n R b =0

n B =0 v =0 v w v =0 v w :

n B =0 v =0 v w v =0 v C T C > 1

m H > 73 GeV

m H > 73 GeV

d i, i = e, n, p

HV V Hff HHH H, HHH

HV V Hff HHH

V 0 = µ 2 HH H + H (H H) 2 +µ HS H HS + HS 2 H HS 2 +µ 3 SS + m2 S 2 S2 + µ S 3 S3 + S 4 S4 H(x) = G + (x) 1 (v + 2 h(x)+ig0 (x)), S(x) =v S + h S (x)

V 0 = µ 2 HH H + H (H H) 2 +µ HS H HS + HS 2 H HS 2 +µ 3 SS + m2 S 2 S2 + µ S 3 S3 + S 4 S4 (h, h S ) (H 1,H 2 )

(b) B <H H (b) B v C T C > g 2 4 E(T C ) [42.97 + (log correction)] sph(t C ) E :

V = g H 1 VV g SM hv V = cos F = g H 1 ff g SM hv V = cos V = F κ F 1.6 1.4 ATLAS and CMS LHC Run 1 1.2 ATLAS+CMS ATLAS 1 CMS 0.8 0.6 0.4 68% CL 95% CL Best fit SM expected 0.8 1 1.2 1.4 κ V

V = g H 1 VV g SM hv V = cos F = g H 1 ff g SM hv V V = F v C /T C =1 κ F 1.6 1.4 1.2 = cos ATLAS and CMS LHC Run 1 ATLAS+CMS ATLAS v C T C > sph (T C ) 1 0.8 CMS 0.6 0.4 68% CL 95% CL Best fit SM expected 0.8 1 1.2 1.4 κ V

V = g H 1 VV g SM hv V = cos F = g H 1 ff g SM hv V V = F v C /T C =1 κ F 1.6 1.4 1.2 ATLAS and CMS LHC Run 1 ATLAS+CMS ATLAS = cos v C T C > sph (T C ) 1 0.8 CMS 0.6 0.4 68% CL 95% CL Best fit SM expected 0.8 1 1.2 1.4 κ V

V = g H 1 VV g SM hv V = cos F = g H 1 ff g SM hv V V = F = cos v C /T C =1 v C T C > sph (T C ) v C = 206.75 T C 111.76 =1.85 sph(t C )=1.18 v C > 1 T C

rsm, tree H 1 H 1 H 1 H 1 =6[ H vc 3 + µ HS 2 s c2 + HS 2 s c (vs + v Sc )+ µ 3 + Sv S s 3 V = F ] v C /T C =1 v C T C > sph (T C ) = H 1 H 1 H 1 rsm H 1 H 1 H 1 SM H 1 H 1 H 1 SM H1 H 1 H 1

S BAU + j i

S BAU + j i 1, 2

n B = N g (s) B 2 v w v 2 w +2RD q 0 dz n L (z )e Rz /v w N g : n L : (s) B : v w : R : D q : n L n L

L = 1 2 i (c L v 2 P L + c R v 1 P R ) j +h.c. c L,R : Im[c L c R ] v 1,2 : i v 2 (y) v 1 (x) i

d WW f d H± W ± f γ ψ ± ψ ± ± ψ j ψ i H ± j i W ± f f f L = 1 2 i (c L v 2 P L + c R v 1 P R ) j +h.c. + p 1 + 2 c + L + 2 P L + c + R + 1 P R j c + L(R) c + L(R) = c L(R) c L(R)

c L = c R =0.42, m H ± = 400 GeV BAU L R = 225 d exp e < 8.7 10 29 e cm Y B /YB obs =1 Y B /YB obs =0.1 d e =1.0 10 29 e cm

BAU H S BAU H L3h S + (g S + i 5 g P ) + g S = cos H g P = sin H

d WW f d H± W ± f γ d H f,d HZ f ψ ± ψ ± ψ j ψ i H ± W ± f f f d sum f = d WW f + d H± W ± f + d H f + d HZ f d sum e =0

d WW f d H± W ± f γ d H f,d HZ f ψ ± ψ ± ψ j ψ i H ± W ± f f f d sum e =0 µ

0 d sum e d e =0 = d WW e + d H± W ± e + d H e + d HZ e m i = 300 GeV m j = 277 GeV H 90 0.0 0.2 0.4 0.6 0.8 1.0 1.2 µ H 1! 2

d sum e = d WW e + d H± W ± e + d H e + d HZ e 0 d e =1.0 10 29 e cm H µ =1.0 d e =1.0 10 29 e cm µ =0.9 0.0 0.2 0.4 0.6 0.8 1.0 1.2 90

0 d n =1.0 10 28 e cm d p =1.0 10 29 e cm H 45 µ =1.0 µ =1.0 µ =0.9 µ =0.9 90 0.0 0.2 0.4 0.6 0.8 1.0 1.2 0.0 0.2 0.4 0.6 0.8 1.0 1.2