Higgs couplings in CMS in Run-2 Stephane Cooperstein (Princeton) on - - PowerPoint PPT Presentation

higgs couplings in cms in run 2
SMART_READER_LITE
LIVE PREVIEW

Higgs couplings in CMS in Run-2 Stephane Cooperstein (Princeton) on - - PowerPoint PPT Presentation

Higgs couplings in CMS in Run-2 Stephane Cooperstein (Princeton) on behalf of the CMS Collaboration 54th Rencontres de Moriond Electroweak unification and unified theories La Thuile, Italy, 16-23 March 2019 17/03/2019 S. Cooperstein


slide-1
SLIDE 1
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

54th Rencontres de Moriond Electroweak unification and unified theories La Thuile, Italy, 16-23 March 2019

Higgs couplings in CMS in Run-2

Stephane Cooperstein (Princeton)

  • n behalf of the CMS Collaboration

1

slide-2
SLIDE 2
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • H→bb

̅

  • Observation of H→bb

̅ last summer

  • H→μ+μ-
  • result with 7+8+13 TeV (2016) data
  • top-Higgs coupling
  • ttH observation last spring with 7+8+13 TeV (2016) data.
  • Updated results for 2/3 channels with 2017 data:
  • ttH multilepton (November)
  • ttH, H→γγ (November)
  • H→invisible
  • Combination of all search channels with 13 TeV (2016) data (September)
  • Combination with 7+8+13 TeV (2016) data (NEW)
  • most stringent limit on BF(H→inv)

Outline

Results shown today new since latest Higgs couplings combination, shown at Moriond last year

arXiv:1809.10733 Submitted to Eur. Phys. J. C

Spring/summer Fall NEW

2

slide-3
SLIDE 3
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • BF(H→bb

̅ ) ~ 58% for SM Higgs with mH = 125 GeV.

  • Inclusive H→bb

̅ search: challenging (factor 107-109 higher) multi-bjet background.

  • VH, H→bb

̅ most sensitive channel at LHC.

  • Leptonic V decay provides important handle
  • n background and simple trigger strategy.

H→bb ̅

  • thers

τ

ZZ

WW

γ

bb

γγ √

Observed:

?

√ √ √

3

slide-4
SLIDE 4
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • Require high-pT W or Z back-

to-back with respect to H→bb ̅ candidate.

  • Small fraction of inclusive H→bb

̅ events but S/B ~1-10%

  • Separate channels targeting Z→ℓℓ,

Z→νν, and W→ℓν

  • New for analysis of 2017 data:
  • Latest machine learning techniques

(DNN) to:

  • identify b-jets, estimate b-jet energy,

differentiate S vs. B

  • Kinematic fit in Z→ℓℓ channel
  • taking advantage of unique channel

topology (no inherent missing energy)

VH, H→bb ̅

Vector boson b-jet b-jet

4

slide-5
SLIDE 5
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • Including all H→bb

̅ published results from CMS (7+8+13 TeV).

  • Dedicated searches in ttH, VBF, and ggH

production modes as well as VH.

H→bb ̅ Combination

Significance 5.5σ exp 5.6σ obs

Observation of H→bb ̅ by the CMS Collaboration!

  • Phys. Rev. Lett. 121 (2018) 121801

= 1.04 ± 0.20

5

slide-6
SLIDE 6
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

H→µµ

  • Very rare decay: BF(H→µµ): ~0.022%
  • Clean experimental signature but large

Z/γ*→µµ background.

  • Boosted decision tree (BDT) trained to

discriminate S vs. B.

  • di-muon kinematics for ggH vs. B.
  • jet kinematics (when applicable) to

discriminate VBF H from B.

  • Μµµ and mass resolution not used as

inputs to avoid biasing background shape.

  • Categorize events by BDT score +

resolution and fit Μµµ.

6

slide-7
SLIDE 7
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

H→µµ: result with 2016 data

7+8+13 TeV

13 TeV (2016 data)

  • Phys. Rev. Lett. 122 (2019) 021801
  • Combination of 7+8+13 TeV (2016) data.
  • Measurement entirely statistics-dominated.
  • Approaching sensitivity to Higgs coupling to

second generation fermions!

  • Benefiting from excellent muon resolution in CMS.
  • 0.9σ (expected) with only 35.9 fb-1 13 TeV data.

Significance 1.0σ expected 0.9σ observed 95% CL UL: σ*BR 2.2 x SM expected 2.9 x SM observed

7

slide-8
SLIDE 8
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • Indirect sensitivity to yt via

measurement of gluon fusion production.

  • Assuming no BSM particles run in the

loop.

  • Direct sensitivity to yt via

measurement of ttH production (coupling at tree level).

  • σttH,13 TeV ~ 510 fb
  • Factor ~4 increase relative to σttH,8 TeV

Top-Higgs coupling

top associated production (ttH)

yt

gluon fusion production (ggH)

yt

8

slide-9
SLIDE 9
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

ttH measurements in CMS

  • ttH ~1% total Higgs production
  • Complex many-particle final

states

ttH search channel benefits/ challenges H→bb ̅ largest rate but combinatorics, challenging tt̅+bb ̅ bkg.

multilepton (H→WW*, ZZ* ,ττ)

lower rate but also less background H→γγ, ZZ(4l) very clean but small rate

9

slide-10
SLIDE 10
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

Observation of ttH

  • Phys. Rev. Lett. 120 (2018) 231801

Significance 4.2σ expected 5.2σ observed

Observation of ttH production by the CMS Collaboration!

  • Combination of all channels

(bb̅, multilepton, γγ) 7+8+13 TeV (2016 only)

  • Direct confirmation of Yukawa

coupling to top quarks

10

slide-11
SLIDE 11
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

CMS-PAS-HIG-18-019

Significance 2017 data only: 1.7σ (2.9σ)

  • 13 TeV (2016+2017):

3.2σ (4.0σ)

ttH multilepton with 2017 data

  • Events categorized by lepton

multiplicity as well as lepton flavor/ charge and b-tagging.

  • Improvements for 2017 analysis:
  • extended categorization
  • data-driven ttV modelling
  • Dedicated BDT’s trained per

category to discriminate signal from background.

  • Primary backgrounds: non-prompt

leptons, ttW, ttZ.

N e w ( + 2 1 7 d a t a ) s i n c e

  • b

s e r v a t i

  • n

11

slide-12
SLIDE 12
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

ttH, H→γγ with 2017 data

CMS-PAS-HIG-18-018

2016 + 2017

  • Events categorized by BDT score

and split by 0ℓ, ≧1ℓ.

  • Fit mγγ to extract signal.
  • Improvements for 2017 analysis:
  • additional categories
  • improved BDT with additional observables

12

slide-13
SLIDE 13
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • Measurement predominately

statistics-limited.

  • Smaller relative systematic

uncertainty than other ttH channels

ttH, H→γγ with 2017 data: results

Significance 2017 data only: 3.1σ (2.2σ)

  • 13 TeV (2016+2017):

4.1σ (2.7σ)

New (+2017 data) since observation

CMS-PAS-HIG-18-018

13

slide-14
SLIDE 14
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • Multiple potential contributions to

Γ(H→inv.)

  • Higgs coupled to BSM particles either:
  • not detectable (e.g. dark matter)
  • not yet accessed final states (long-lived,

background-dominated signatures,..)

  • VBF production most sensitive

H→inv. channel.

  • Characteristic signature allows for high

suppression of SM backgrounds.

VBF H→invisible

14

slide-15
SLIDE 15
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • Dominant backgrounds:

Z(νν)+jets and W(ℓv) +jets.

  • Extract Z(νν)+jets and

W(ℓv)+jets shapes from 1- and 2-lepton sidebands and fit mjj.

VBF H→invisible: fit strategy

Z(νν)+jets extrapolated from 2-lepton sideband W(lν)+jets extrapolated from 1- lepton sideband

15

slide-16
SLIDE 16
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • Combine independent H→inv. searches on 2016

data: VBF, Z(ll)H, W(q’q)H, ggH.

  • Set limits on Binv by assuming SM production rates.
  • VBF production channel most sensitive
  • 2016 VBF-only: Binv < 0.33 (0.25)
  • O(25%) improvement in sensitivity from adding VH and

ggH channels.

H→invisible combination

+ +

Binv < 0.26 (0.20) @95% CL

  • 16
slide-17
SLIDE 17
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

H→invisible combination: 7+8+13 TeV

Binv < 0.19 (0.15) Most stringent limit to date!

  • Reinterpretation in context of Higgs-

portal models of DM interactions.

  • Most stringent limits for MDM < 18 (7)

GeV assuming fermion (scalar DM) candidate.

NEW RESULT

arXiv:1809.05937 submitted to Phys. Lett. B

C M S : s c a l a r D M C M S : f e r m i

  • n

D M

17

slide-18
SLIDE 18
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

(GeV)

µ 4

M

20 40 60 80 100 120 140

Events / 3 GeV

  • 1

10 1 10

2

10

(GeV)

µ 4

M

20 40 60 80 100 120 140

Events / 3 GeV

  • 1

10 1 10

2

10

(13 TeV)

  • 1

37.5 fb

CMS

Preliminary Data Background Model Boson Signals

(GeV)

µ 4

M

40 60 80 100 120 140

Events / 4 GeV

  • 1

10 1 10

2

10

(GeV)

µ 4

M

40 60 80 100 120 140

Events / 4 GeV

  • 1

10 1 10

2

10

(13 TeV)

  • 1

37.5 fb

CMS

Preliminary Data Background Model Boson Signals

  • SM BF’s inaccessible by many orders of

magnitude.

  • Four-muon final state.
  • Experimentally clean with very small SM

backgrounds

  • Excess at H or Z mass would be sign of

BSM physics.

H→J/ψJ/ψ, H→ΥΥ

H→J/ψJ/ψ H→ΥΥ

NEW RESULT

18

CMS-PAS-HIG-18-025

  • bserved

expected

B(H → J/ψJ/ψ) × 103

1.8 1.8+0.2

−0.1

B(H → ΥΥ) × 103

1.4 1.4 ± 0.1

B(Z → J/ψJ/ψ) × 106

2.2 2.8+1.2

−0.7

B(Z → ΥΥ) × 106

1.5 1.5 ± 0.1

slide-19
SLIDE 19
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • Third generation Yukawa couplings

firmly and directly established.

  • Observation of ttH and H→bb

̅ in 2018, previous observation of H→ττ.

  • Approaching sensitivity to second

generation via H→µµ.

  • Tightening constraints on H→inv.
  • most stringent limit:
  • Binv < 0.19 (0.15) @95% CL
  • Working towards improved legacy

measurements using full 13 TeV dataset.

Summary

19

slide-20
SLIDE 20
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

Thank you!

20

slide-21
SLIDE 21

Additional Material

slide-22
SLIDE 22
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • Pixel detector upgraded for 2017 data taking.
  • Additional layer with first tracking measurement closer to beam pipe.
  • Improvements in tracking efficiency, vertex resolution, and b-tagging

efficiency.

CMS Pixel Detector Phase 1 Upgrade

2017 2016 2017 2016

22

slide-23
SLIDE 23
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

B-tagging in CMS: DeepCSV

CMS-DP-2017-005

  • Deep neural network multi-classifier

(b, bb, c, cc, light).

  • Four hidden layers with a width of 100

nodes each.

  • Same track selection and input
  • bservables as previous boosted decision

tree (BDT)-based tagger.

23

slide-24
SLIDE 24
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

Higgs boson production modes at the LHC

24

slide-25
SLIDE 25
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

CMS delivered luminosity

25 1 Apr 1 May 1 Jun 1 Jul 1 Aug 1 Sep 1 Oct 1 Nov 1 Dec

Date (UTC)

20 40 60 80 100

Total Integrated Luminosity (fb¡1 )

£ 50

Data included from 2010-03-30 11:22 to 2018-10-26 08:23 UTC 2010, 7 TeV, 45.0 pb¡1 2011, 7 TeV, 6.1 fb¡1 2012, 8 TeV, 23.3 fb¡1 2015, 13 TeV, 4.2 fb¡1 2016, 13 TeV, 41.0 fb¡1 2017, 13 TeV, 49.8 fb¡1 2018, 13 TeV, 67.9 fb¡1 20 40 60 80 100

CMS Integrated Luminosity Delivered, pp

slide-26
SLIDE 26
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

Observation of ttH: details

CMS-HIG-17-0216, accepted for publication by JHEP JHEP 08 (2018) 066

  • Phys. Rev. Lett. 120 (2018) 231801

JHEP 06 (2018) 101

+ ttH, H→γγ ttH multilepton

  • ttH. H→bb

̅ fully hadronic ttH, H→bb ̅ 1+2l + Run-1 data

Significance 5.5σ expected 5.6σ observed

  • Combining all channels with

2016 data + Run-1

  • Observation of ttH production

by the CMS Collaboration!

26

slide-27
SLIDE 27
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

ttH combination: uncertainties

27

slide-28
SLIDE 28
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

ttH observation: per decay channel

28

slide-29
SLIDE 29
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • Challenging tt+bb background and combinatorics.
  • Systematically limited with 35.9 fb

2016 data.

ttH, H→bb ̅

29

Events / Bin

10

2

10

3

10

4

10

5

10

CMS

(13 TeV)

  • 1

35.9 fb

Data Background = 0.72) µ Signal ( = 1) µ SM (

(S/B)

10

Pre-fit expected log

2.5 − 2.0 − 1.5 − 1.0 − 0.5 −

Data / Bkg.

0.6 0.8 1.0 1.2 1.4

= 125 GeV

H

at m

SM

σ / σ = µ Best fit

2 − 2 4 6

Combined Dilepton Single-lepton

CMS

(13 TeV)

  • 1

35.9 fb syst stat tot µ

  • 0.43

+0.44

  • 0.26

+0.27

  • 0.50

+0.52

0.84

  • 0.95

+1.04

  • 0.60

+0.63

  • 1.12

+1.21

  • 0.24
  • 0.38

+0.38

  • 0.24

+0.24

  • 0.45

+0.45

0.72

Significance 2.2σ exp 1.6σ obs

  • 1
slide-30
SLIDE 30
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

30

Uncertainty source

±∆µ (observed) ±∆µ (expected)

Total experimental

+0.15/−0.16 +0.19/−0.17

b tagging

+0.11/−0.14 +0.12/−0.11

jet energy scale and resolution

+0.06/−0.07 +0.13/−0.11

Total theory

+0.28/−0.29 +0.32/−0.29

tt+hf cross section and parton shower

+0.24/−0.28 +0.28/−0.28

Size of the simulated samples

+0.14/−0.15 +0.16/−0.16

Total systematic

+0.38/−0.38 +0.45/−0.42

Statistical

+0.24/−0.24 +0.27/−0.27

Total

+0.45/−0.45 +0.53/−0.49

ttH, H→bb ̅ uncertainties

slide-31
SLIDE 31
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

  • Simultaneous fit of BDT distribution in

Z→ℓℓ, Z→νν, and W→ℓν channels.

  • Phys. Lett. B 780 (2018) 501
  • Evidence for H→bb

̅ !

  • 30% precision on signal strength (3.8σ)

when combined with Run-1 result.

2016 VH, H→bb ̅ Result

Significance 2.8σ expected 3.3σ observed

31

slide-32
SLIDE 32
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019 2-lepton 1-lepton 0-lepton

per-channel DNN’s to discriminate S from B

DNN multiclassifiers to differentiate background components (V+bb, V+b, V+udcsg, tt)

  • Constrain V+bb, V+b,

V+udcsg, tt normalizations from data.

  • Simultaneous fit of all

regions to extract single signal strength.

VH, H→bb ̅ : signal extraction

32

slide-33
SLIDE 33
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

VZ, Z→bb ̅ cross-check

  • Validate analysis strategy by extracting VZ, Z→bb

̅ signal with same techniques.

  • Same final state and similar kinematics as VH, H→bb

̅ signal.

  • Minimal changes to analysis strategy:
  • shift M(bb

̅ ) selection to include Z(bb ̅ ).

  • re-train DNN to discriminate VZ, Z→bb

̅ “signal”

  • Otherwise everything is the same as the VH, H→bb

̅ analysis:

  • same DNN inputs, same fit strategy

Channel compatibility: 64%

Well consistent with SM expectation

Significance 5.0σ expected 5.2σ observed

  • Signal strength

µ = 1.05 ± 0.22

33

slide-34
SLIDE 34
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

Channel compatibility: 64%

  • Standalone evidence for VH,

H→bb ̅ with 2017 dataset.

2017 VH, H→bb ̅ Result

Channel compatibility: 97%

Significance 3.1σ expected 3.3σ observed

  • Signal strength

µ = 1.08 ± 0.34

34

slide-35
SLIDE 35
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

VH, H→bb ̅ uncertainties

  • Important statistical as well as

systematic uncertainty component.

  • For 2017 analysis alone statistical

uncertainty is still the largest contribution.

  • Primary systematic uncertainties:
  • Background normalization and

modelling

  • Impact reduced through use of

background DNN multi-classifier.

  • B-tagging efficiency and

misidentification rate

  • Limited statistical precision of simulated

background events.

  • Primary theoretical uncertainties due to

renormalization and factorization scales.

35

slide-36
SLIDE 36
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

VH, H→bb ̅ combination details

36

slide-37
SLIDE 37
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

H→µµ: BDT distribution

37

slide-38
SLIDE 38
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

H→µµ: BDT categories

38 BDT response Maximum ggH VBF WH ZH ttH Signal Bkg/GeV FWHM Bkg fit S/

B quantile [%] muon |η| [%] [%] [%] [%] [%] @125 GeV

[GeV]

function @ FWHM 0 – 8

|η|< 2.4

4.9 1.3 3.3 6.3 32 21.2 3.13 × 103 4.2 mBW Bdeg 4 0.12 8 – 39 1.9 <|η|< 2.4 5.6 1.7 3.9 3.5 1.3 22.3 1.34 × 103 7.2 mBW Bdeg 4 0.16 8 – 39 0.9 <|η|< 1.9 10 2.8 6.5 6.4 5.2 41.1 2.24 × 103 4.1 mBW Bdeg 4 0.29 8 – 39

|η|< 0.9

3.2 0.8 1.9 2.1 3.5 12.7 7.83 × 102 2.9 mBW Bdeg 4 0.18 39 – 61 1.9 <|η|< 2.4 2.9 1.7 2.7 2.7 0.3 11.8 4.37 × 102 7.0 mBW Bdeg 4 0.14 39 – 61 0.9 <|η|< 1.9 7.2 3.3 6.1 5.2 1.3 29.2 9.70 × 102 4.0 mBW Bdeg 4 0.31 39 – 61

|η|< 0.9

3.6 1.1 2.6 2.2 0.9 14.5 4.81 × 102 2.8 mBW 0.26 61 – 76 1.9 <|η|< 2.4 1.2 1.5 1.8 1.7 0.2 5.2 1.48 × 102 7.6 mBW Bdeg 4 0.11 61 – 76 0.9 <|η|< 1.9 4.8 3.6 4.5 4.4 0.7 20.3 5.12 × 102 4.2 mBW Bdeg 4 0.29 61 – 76

|η|< 0.9

3.2 1.6 2.3 2.1 0.6 13.1 3.22 × 102 3.0 mBW 0.28 76 – 91 1.9 <|η|< 2.4 1.2 3.1 2.2 2.1 0.2 5.8 1.04 × 102 7.1 mBW Bdeg 4 0.14 76 – 91 0.9 <|η|< 1.9 4.4 8.7 6.2 6.0 1.1 20.3 3.60 × 102 4.2 mBW Bdeg 4 0.35 76 – 91

|η|< 0.9

3.1 4.0 3.8 3.6 0.9 13.7 2.36 × 102 3.2 mBW 0.34 91 – 95

|η|< 2.4

1.7 6.4 2.5 2.6 0.5 8.6 96.0 4.0 mBW 0.28 95 – 100

|η|< 2.4

2.0 19 1.5 1.4 0.7 13.7 83.4 4.1 mBW 0.48 0 – 100

|η|< 2.4

59 61 51 52 49 253 1.30 × 104 3.9

slide-39
SLIDE 39
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

Highly boosted inclusive H→bb ̅ search

  • b-jets increasingly likely to “merge” with

increasing pT(H).

  • Uses jet substructure techniques to “tag”

large jets which contain both b-quarks.

  • First observation (5.1σ) of Z→bb

̅ in single merged jet topology!

  • New contribution to Higgs differential

measurement at high pT(H).

b-jet b-jet

  • Previously thought to be infeasible at LHC

due to overwhelming multi-jet background.

pT(H) > 450 GeV

  • Phys. Rev. Lett. 120 (2018) 071802

39

slide-40
SLIDE 40
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

H→ττ observation

  • Higgs fermionic decay channel with

best combination of selection efficiency and background rejection.

  • Primary challenges: mass

resolution, trigger.

  • First direct experimental
  • bservation of a Yukawa

coupling:

  • With 7+8 TeV data by

combining ATLAS + CMS measurements.

  • Single experiment
  • bservations with 13 TeV data.
  • Phys. Lett. B 779 (2018) 283

40

slide-41
SLIDE 41
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

H→ττ observation: per channel and production mode

41

slide-42
SLIDE 42
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

tHq

  • Interference term between two LO diagrams

exposes relative sign of κV vs. κt.

  • Destructive interference in SM: σSM(κV =κt=1)

= 70.96 fb.

  • For inverted top coupling cross section

increased by order of magnitude.

  • Two dedicated CMS analyses:
  • multi-lepton: CMS-PAS-HIG-17-005
  • bb

̅ : CMS-PAS-HIG-16-019

κV κt

42

slide-43
SLIDE 43
  • S. Cooperstein (Princeton)

17/03/2019 Moriond EW 2019

H→J/ψJ/ψ, H→ΥΥ diagrams

43