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European Strategy meeting in Granada, May 2019 [Theory] Extended Higgs sectors and high-energy flavour dynamics Veronica Sanz 1

[Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

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Page 1: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

European Strategy meeting in Granada, May 2019

[Theory] Extended Higgs sectors and high-energy flavour dynamicsVeronica Sanz

1

Page 2: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Non-minimal EWSB: singlets/doublets

2

Page 3: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Singlets/doublets

3

A doublet Higgs has 4 dof

Higgs = (vev + higgs particle + W/Z dofs)

and that’s all we need in the SM

SUSY at least two doublets Composite Higgs no reason for global breaking to be minimal

Scalars will mix & modify Higgs

Why more? Occam’s razor

But in BSM models minimal EWSB is not generic

More structure/symmetries tend to need a more complex

scalar sector

Page 4: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Interplay Higgs/EWPO/direct

�S =1

6⇡c̄H(m�) log

✓m�

mZ

/ sin2 �EWPOmixing

massHiggsDirect

4

Page 5: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Phase transitions: a new opportunityAdditional contributions to the EW phase transition

from singlets and doubletsReach to 1st order? Baryogenesis and Gravitational waves

5

from ClineLISA’s proposal

Open new opportunities at the TeVColliders/LISA/EDMs

Page 6: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

500 1000 1500 2000 2500 3000 [GeV]φm

4−10

3−10

2−10

1−10

γ2

95

% C

.L.

lim

it o

n s

in

Higgs couplings:HL-LHCHE-LHCLHeCILC 500 GeVFCC-eeCEPCFCC-ee/eh/hhCLIC 3 TeV

EWPO:HL-LHCHE-LHCLHeCILC 500 GeVFCC-eeCEPCFCC-ee/eh/hhCLIC 3 TeV

Direct:HL-LHCHE-LHCCLIC 1.5 TeVCLIC 3 TeV 50 100 150 200 250 300

m2 [GeV]

0.0

0.5

1.0

1.5

2.0

2.5

3.0

a 2

�⇤T⇤

= 5

�⇤T⇤

= 2

�H

S2

FCC-all

CLIC3

Phase transitions: singlet example

MIXING NO MIXING, Z2

m�

thanks to Chala, LISA draft

6

Dots 1OPT from 1605.06123

Upper limit on singlet mass < TeVcorrelation with anomalous di-Higgs

Lessons common tosinglets/doublets

Page 7: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

On the UV origin of flavour

7

Page 8: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

The 3rd generation & flavour

8

The structure of EWSB (the origin of mass)

and the UV structure of flavourare linked

[from G Kane, Scientific American]

The third generation feels EWSB more strongly than the other two

may be a sensitive probe into flavour

Consistent with observations: we know of the flavour properties of the 1st and

2nd generation to be SM-like to a higher precision

Page 9: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Let’s make the third generation special

9

Example: Warped extra-dimensions

EWdynamics

UVdynamics

Our 4D-world measurements: distributions inside the extra-dimension*most fermions light because they do not feel EWSB that much

*third generation special because it happens to be (spatially) closer to the place where EWSB happens

What if Nature were higher-dimensional?

xdim

Page 10: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Let’s make the third generation special, again

10

Example: Partial compositeness

Mixing of third generation with fermions from the new strong sector happens to be larger than for the 1st and 2nd generations

Higgs as a Composite Higgs

What if there were a new strongly coupled sector?

Elementarysector

CompositeEW

sector3rd generation

1st-2nd generations

Page 11: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Top flavour and FCNCs

11

Page 12: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Top FCNC decays—typical predictions

Typical predictions (Snowmass 1311.2028 )

Best sensitivity to models 2HDM (FV) and RS

ph/9609279, ph/0606293

12

Page 13: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Top FCNC decays: in context

13

2HDM (FV) RS

Page 14: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

2HDM (FV)

14

Top FCNC decays—typical predictions

see recent analysis 1710.03752

Assuming flavour violation

/pmi mj

v

RSwarped extra-dimensions

precursor of modern partial compositeness models

Third generation is special, dynamically or by design

Page 15: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Leptoquarks and flavour anomalies

15

Page 16: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Flavour anomalies: is the SM breaking down?

16

current exp world averagefrom 1903.11517

SM prediction

Shaded region:U1 models

Page 17: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Flavour anomalies: current statusMoriond 2019, no paradigm shift

Data yet to be analysed and to be made public

One of the preferred explanations to this and other flavour anomaliesis the existence of new LQs, particularly U1

17

Page 18: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Leptoquarks? That’s so 80’s!

Objects with L and B numbersInitial motivation GUTs

possible in many models

SU(5), SO(10)Pati/Salam

squarks in RPV Ext TC/generic compositeness

PDG

18

Page 19: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

The U1 in a nutshell Review U1 in 1808.08179 recent 1903.11517,1704.05438v4

mass 1-2 TeV can explain the anomalies with LH couplingsdirect searches and indirect

high-pT searches

19

4 fermion operatorsflavour observableslow-energy indirect

Page 20: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

Model building a flavour anomalyEven if the anomalies went away

efforts to fit them in a theoretical context will remain

20

E.g. 1903.11517

The U1 in a UV-complete model is a difficult exercise

G4321 = SU(4)⇥ SU(3)0 ⇥ SU(2)⇥ U(1)0

PS3

Occam’s razorto principles

not to matter content

Gauge group

Flavour symmetry 3rd gen vs others

flavour is difficult

Page 21: [Theory] Extended Higgs sectors and high-energy flavour dynamics · 2019-06-04 · 0.0 0.5 1.0 1.5 2.0 2.5 3.0 a 2 ⇤ T⇤ =5 ⇤ T⇤ =2 HS 2-all CLIC3 Phase transitions: singlet

OutlookIs the Higgs sector minimal? Are there other scalar resonances participating in EWSB? We tackle this question with a combination of indirect EWPT, Higgs measurements (including di-Higgs) and direct searches

If not minimal, could the EW phase transition be strong 1st order? Scalars need to be light (< TeV) and typically modify the properties of the Higgs. Colliders have an excellent coverage to these scenarios. Exceptional opportunity to connect with GWs and theoretical approaches to fluid dynamics

If strong 1st order, could the EW phase transition explain baryogenesis? Connection to EDM measurements and other observables sensitive to CPV

Could we understand the UV origin of flavour with colliders? Possibly, if some preferential treatment of 3rd generation. Top FCNCs and B anomalies could provide the first clues. Theoretical efforts to fit all this in a full framework underway