boosting the discovery of โ†’ โ†’ ๐‰๐‰

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Boosting the discovery of โ†’ โ†’ at the LHC Kayoung Ban (๋ฐ˜๊ฐ€์˜) (Yonsei University) In collaboration with Wonsang Cho(Seoul National Univ.), Seongchan Park(Yonsei Univ.) 2018.10.30 2018 8 th KIAS Workshop 1 [email protected] [email protected] , [email protected]

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Boosting the discovery of

๐’‘ ๐’‘ โ†’ ๐’‰ ๐’‰ โ†’ ๐’ƒ ๐’ƒ ๐‰ ๐‰at the LHC

Kayoung Ban (๋ฐ˜๊ฐ€์˜)

(Yonsei University)

In collaboration with

Wonsang Cho(Seoul National Univ.), Seongchan Park(Yonsei Univ.)

2018.10.30

2018 8th KIAS Workshop 1

[email protected]

[email protected], [email protected]

โ€ข Higgs self-coupling

โœ“ Di-Higgs search has a meaning to measure the Higgs self

coupling and to understand the Higgs potential

โœ“ The topology is determine by each Higgs decay chain

Introduction

โ€ข Higgs pair production

Figure ref : arXiv:1512.08928

โ„’โ„Ž =1

2๐œ•๐œ‡โ„Ž๐œ•๐œ‡โ„Ž โˆ’

1

2๐‘šโ„Ž

2โ„Ž2 โˆ’ ๐œ…๐œ†๐œ†๐‘†๐‘€๐‘ฃโ„Ž3 โˆ’

๐‘š๐‘ก

๐‘ฃ๐‘ฃ + ๐œ…๐‘กโ„Ž าง๐‘ก๐ฟ๐‘ก๐‘… + โ„Ž. ๐‘ + โ‹ฏ

2

๐œ…๐‘ก๐œ…๐œ†

3

Signal vs Background

Channel Leptons X section Topology

HH2Tau 0 ~1.2 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐œโ„Ž +๐‘š๐‘’๐‘ก

TT2Tau 0 ~5097.2 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐œโ„Ž +๐‘š๐‘’๐‘ก

HH2Tau 1 ~1.3 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

HH2W*W 1 ~0.15 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

HH2WW* 1 ~0.15 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐œโ„Ž +๐‘š๐‘’๐‘ก

TT2Tau 1 ~5546.3 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

TT1Tau 1 ~29700.2 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

HH2Tau 2 ~0.36 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

HH2W*W1Tau 2 ~0.08 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

HH2WW*1Tau 2 ~0.08 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

HH2WW0Tau 2 ~0.47 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

TT2Tau 2 ~1508.7 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

TT1Tau 2 ~16158.3 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

TT0Tau 2 ~43263.9 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

@ 14TeV, 39.64 fb (HH), 953.6 fb (TT)

* ๐‘™ = ๐‘’ ๐‘œ๐‘Ÿ ๐œ‡

Channel Leptons X section Topology

HH2Tau 0 ~1.2 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐œโ„Ž +๐‘š๐‘’๐‘ก

TT2Tau 0 ~5097.2 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐œโ„Ž +๐‘š๐‘’๐‘ก

HH2Tau 1 ~1.3 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

HH2W*W 1 ~0.15 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

HH2WW* 1 ~0.15 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐œโ„Ž +๐‘š๐‘’๐‘ก

TT2Tau 1 ~5546.3 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

TT1Tau 1 ~29700.2 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

HH2Tau 2 ~0.36 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

HH2W*W1Tau 2 ~0.08 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

HH2WW*1Tau 2 ~0.08 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

HH2WW0Tau 2 ~0.47 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

TT2Tau 2 ~1508.7 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

TT1Tau 2 ~16158.3 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

TT0Tau 2 ~43263.9 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

4

Signal vs Background @ 14TeV, 39.64 fb (HH), 953.6 fb (TT)

* ๐‘™ = ๐‘’ ๐‘œ๐‘Ÿ ๐œ‡

Too Many ๐’• าง๐’• Background

5

How to reconstruct the missing information?

โ„Ž

โ„Ž

๐‘

เดค๐‘๐’—๐‰

๐œโˆ’

๐œ+

๐œ‹0, ๐œ‹โˆ’โ€ฆ

๐’—๐‰

๐‘™+

๐’—๐’

โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œโˆ’๐œ+

๐œโˆ’ โ†’ ๐‘ฃ๐œ ๐œโ„Ž๐œ+ โ†’ เดฅ๐‘ฃ๐œ ๐‘™+ ๐œ๐‘™

Ex) HH2tau : 1 lepton + 1 tau_h Channel

# of Neutrinos >= 2

๐‡ โ†’ ๐‰๐‰/๐‘พ๐‘พ

6HH?

๐’• าง๐’•

A Needle(HH) in a stack of Needles(๐’• าง๐’•)

7

OptiMass introduction

โ€ข Augmented Lagrangian method

โ„’๐‘˜ ิฆ๐‘ฅ | ๐œ†, ๐œ‡ = ๐‘ด ๐’™ โˆ’

๐‘Ž=1

๐‘š

๐œ†๐‘Ž๐‘˜ ๐‘๐‘Ž ิฆ๐‘ฅ +1

2๐œ‡๐‘˜

๐‘Ž

๐‘๐‘Ž2 ิฆ๐‘ฅ .

๐œ†๐‘Ž๐‘˜+1 = ๐œ†๐‘Ž

๐‘˜ โˆ’๐‘๐‘Ž ิฆ๐‘ฅ๐‘˜๐œ‡๐‘˜

โœ“OM (OptiMass) ~ TARGET MASS

โœ“CD (Compatibility Distance) ~ 0 for TRUE SYSTEM

OPTIMASS: A Package for the Minimization of Kinematic Mass Functions with Constraints- Cho, Won Sang et al. JHEP 1601 (2016) 026 arXiv:1508.00589

๐‘€ = minimized mass variable function๐œ†๐‘Ž = ๐‘Ž๐‘ข๐‘”๐‘š๐‘’๐‘›๐‘ก๐‘’๐‘‘ ๐ฟ๐‘Ž๐‘”๐‘Ÿ๐‘Ž๐‘›๐‘”๐‘’ ๐‘๐‘Ž๐‘Ÿ๐‘Ž๐‘š๐‘’๐‘ก๐‘’๐‘Ÿ๐œ‡ = ๐‘๐‘’๐‘›๐‘Ž๐‘™๐‘ก๐‘ฆ ๐‘๐‘Ž๐‘Ÿ๐‘Ž๐‘š๐‘’๐‘ก๐‘’๐‘Ÿ

๐’™ = ๐’Ž๐’Š๐’”๐’”๐’Š๐’๐’ˆ๐’Ž๐’๐’Ž๐’†๐’๐’•๐’–๐’Ž๐’„๐’‚ = ๐’‘๐’‰๐’š๐’”๐’Š๐’„๐’‚๐’ ๐’„๐’๐’๐’”๐’•๐’“๐’‚๐’Š๐’๐’•๐’”

๐‘ค๐‘–๐‘กโ„Ž | ๐‘ ิฆ๐‘ฅ๐‘˜ | =

๐‘Ž

๐‘๐‘Ž ิฆ๐‘ฅ๐‘˜2๐‘ช๐‘ซ = | ๐‘ ิฆ๐‘ฅ๐‘˜ | < ๐œ‚โˆ—

โ„Ž

โ„Ž

๐‘

เดค๐‘ ๐’—๐‰

๐œโˆ’

๐œ+

๐œ‹0, ๐œ‹โˆ’โ€ฆ

๐’—๐‰

๐‘™+

๐’—๐’

๐‘ ๐‘ฆ๐‘ ๐‘ก๐‘’๐‘š

๐‘ ๐‘ข๐‘๐‘ ๐‘ฆ๐‘ ๐‘ก๐‘’๐‘š๐‘ ๐‘ข๐‘๐‘ ๐‘ฆ๐‘ ๐‘ก๐‘’๐‘š

8

โœ“ (0l) # ( Visible Features )

= 12 dim

โœ“ (0l) # ( OM Features )

= 6(hh)+14(ttbar) = 20 dim

โœ“ (1l) # ( Visible Features )

= 12 dim

โœ“ (1l) # ( OM Features )

= 30(hh)+22(ttbar) = 52 dim

โœ“ (2l) # ( Visible Features )

(2l) # ( OM Features )

= (Talk on Thu.

By Dr. Wonsang Cho )

โ– Visible : CMS/ATLAS common features ~ ๐’‘๐‘ป, ๐šซ๐‘, ๐šซ๐“ โ€ฆ

Multi-Variable Classificationโ€ข All distinctive decay topology โ‡’ Characterized by each constraints, ๐‘๐‘Ž / systems

โ€ข Using OptiMass, we can reconstruct the mass of systems/subsystems

โ‡’ the classes for MVA classification

For 0 lepton Channel

OM h2ta S CD h2ta S

OM h2ta Mh1 CD h2ta Mh1

OM h2ta maxMta12 CD h2ta maxMta12

OM t2ta S CD t2ta S

OM t2ta maxMt12 CD t2ta maxMt12

OM t2ta maxMta12 CD t2ta maxMta12

OM t2ta maxMw12 CD t2ta maxMw12

OM t2ta maxMt12_c2_etas0

5

CD t2ta maxMt12_c2_etas0

5

OM t2ta maxMt12_c1_etas0

05

CD t2ta maxMt12_c1_etas0

05

OM t2ta maxMt12 c2_etas01

CD t2ta maxMt12 c2_etas01

For 1 lepton Channel

OM h2ta S CD h2ta S

OM h2ta Mh1 CD h2ta Mh1

OM h2ta maxMta12

CD h2ta maxMta12

OM h1tawos S CD h1tawos S

OM h1tawos Mh1 CD h1tawos Mh1

OM h1tawos maxMw12

CD h1tawos maxMw12

OM h1tawoff maxMw12

CD h1tawoff maxMw12

โ€ฆ โ€ฆ

OM t2ta S CD t2ta S

OM t2ta maxMt12 CD t2ta maxMt12

OM t2ta maxMta12 CD t2ta maxMta12

OM t2ta maxMw12 CD t2ta maxMw12

OM t1ta S CD t1ta S

OM t1ta maxMt12 CD t1ta maxMt12

โ€ฆ โ€ฆ

Event Selection

9

โ€ข Using โ€ฆ โ€ข MC : MG5_aMC v2.5.5 + MADSPIN (Decay)

โ€ข Showering : PYTHIA8

โ€ข Detector Simulation : Delphes

โ€ข CT10nlo for all Channel

โ€ข Cut โ€ฆโ€ข Delphes : Using delphes_card_ATLAS.dat

โ€ข Tau Tagging : ฮ”๐‘… < 0.4 , ฮ”๐‘…๐‘ก๐‘Ÿ๐‘Ž๐‘๐‘˜ < 0.2 , ๐‘ƒ๐‘‡๐‘‡๐‘Ÿ๐‘Ž๐‘๐‘˜ > 1.0 , ๐‘ƒ๐‘‡

๐œ > 2.0 , ๐œ‚๐œ < 2.5

1-prong Eff = 70% , N(>1)-prong eff = 60%

โ€ข Others are same with delphes_card_ATLAS.dat default

โ€ข Hadronic Tau decay using ALL N-prongs

0-lepton & 2-hadronic decay tau

10

Constraints of Mass

โ€ข Tau1 = 1.77

โ€ข Tau2 = 1.77

โ€ข Tau1 = Tau2

โ„Ž

โ„Ž

๐‘

เดค๐‘ ๐’—๐‰

๐œโˆ’

๐œ+

๐œ‹0, ๐œ‹โˆ’โ€ฆ

๐’—๐‰

๐‘™+

๐’—๐’

๐‘ ๐‘ข๐‘๐‘ ๐‘ฆ๐‘ ๐‘ก๐‘’๐‘š

11

OM/CD of (2l,1l,0l) Channels

12

DNN vs BDT

โ€ข Deep Neural Network

โœ“ Keras + Tensorflow module

โœ“ 7~8 hidden layers + 500 nodes per hidden layers

โœ“ 2 / 5 / 7 nodes output ( for each class )

โœ“ Using โ€˜RELUโ€™ Activation function + โ€˜SoftMaxโ€™ output layer

โœ“ Dropout = 0.2~3 + Batch Normalization

โ€ข Boost Decision Tree

โœ“ Using โ€˜AdaBoostClassificationโ€™ in sklearn module

โœ“ Max_depth = 2~3

โœ“ # of Estimators = 500~1000, learning rate = 0.01

โœ“ Algorithm = โ€˜SAMMEโ€™

13

ROC Result for 0 lep (2b+2tau_h)

DNN + Vis. + OM

Vis. + BDT

14

Significance Result for 0 lep (2b+2tau_h)

15

Result for 0 lep (2b+2tau_h)

Signal=1Background=0

DNN + Vis. + OM

DNN + Vis.

16

Classification Result for (1l) Channels

17

Rank Feature Variables Importance

1 OM h2ta maxMta12 11%

2 dR_bb 10%

3 mt2_bbtata 9%

4 CD t2ta maxMta12 9%

5 CD h2ta maxMta12 9%

6 CD h2ta S 8%

7 pT_tata 8%

8 CD h2ta Mh1 7%

9 CD t2ta maxMt12 c2_etas01 7%

10 dR_tata 5%

11 pT_bb 3%

12 OM t2ta maxMt12 c1_etas1 3%

13 OM t2ta maxMt12 c2_etas01 2%

14 dphi_bbmet 2%

15 OM h2ta Mh1 2%

16 OM t2ta maxMt12 2%

Variable Importance Score Result for (0/1) lepton

Rank Feature Variables Importance

1 OM h2ta maxMta12 21%

2 OM h1tawos Mw1 15%

3 dr_lta 10%

4 pt_lta 10%

5 OM h2ta Mh1 9%

6 dr_bb 5%

7 CD h2ta S 5%

8 CD h2ta Mh1 5%

9 mt_ta1 3%

10 OM h1tawoff Mw2 2%

11 OM h1tawos maxMw12 2%

12 OM h1tawos Mh1 2%

13 OM h1tawoff Mh1 c2_etas100 1%

14 OM h1tawoff maxMw12 1%

15 CD h1tawos Mh1 1%

16 CD t1ta S 1%

17 CD h1tawos Mh1 c2_etas10 1%

Result of 0/1-lepton

18

@ 14TeV, 39.64 fb (HH), 953.6 fb (TT)

1000 fb luminosity (1 abโˆ’1)

HH2Tau TT2Tau HH2Tau TT2Tau

Cross Section ~1.2 ~5097.2 ~1.6 ~35246.5

Number of Detected ~1,200 ~5,097,200 ~1,600 ~35,246,500

โ†“ # of remained โ†“

BDT + Visible ~240 ~65,659 ~328 ~19,803

BDT + Visible + OM ~240 ~17,630 ~328 ~18,615

DNN + OM ~240 ~3,205 ~328 ~3,329

DNN + Visible + OM ~240 ~1,995 ~328 ~2,831

Assume the same amount of signal

19

โœ“ Discovering HH is important

โœ“ But we have to distinguish the signal from the HUGE

background (ttbar)

โœ“ We introduce

- New Handles : โ€œOPTIMASS Variablesโ€ (~40)

- Improved Classification Method : โ€œDNNโ€

Conclusion

!!! Use DNN + OPTIMASS Variables !!!

AUC(CMS, BDT) = 0.91 -> AUC(Ours) = 0.97

Q&A

20

BACK

UP

21

โ€ข CMS-HIG 17-002

โ€ข 'dr_tata', 'dr_bbโ€™

โ€ข 'dphi_bbtataโ€™, 'dphi_tatamet'', 'dphi_bbmet', 'dphi_ta1met', 'dphi_ta2met'

โ€ข 'pt_tata', 'pt_bbโ€™

โ€ข 'mt2_bbtata,'mt_ta1', 'mt_ta2'

22

โ–Visible : CMS/ATLAS common features

23

How to reconstruct the missing information?

โ„Ž

โ„Ž

๐‘

เดค๐‘๐’—๐‰

๐œโˆ’

๐œ+

๐œ‹0, ๐œ‹โˆ’โ€ฆ

๐’—๐‰

๐‘™+

๐’—๐’

โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œโˆ’๐œ+

๐œโˆ’ โ†’ ๐‘ฃ๐œ ๐œโ„Ž๐œ+ โ†’ เดฅ๐‘ฃ๐œ ๐‘™+ ๐œ๐‘™

Ex) HH2tau : 1 lepton + 1 tau_h Channel

# of Neutrinos >= 2

Too Many invisible particles

from each distinctive/complicated

decay topologies

โ€ข 0-leptons + 2-hadronic decay tau (2 class)

โ€ข ๐‘†๐บ โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐œโ„Ž +๐‘š๐‘’๐‘ก

โ€ข ๐ต๐บ าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐œโ„Ž +๐‘š๐‘’๐‘ก

โ€ข 1-leptons + 1-hadronic decay tau (5 class)

โ€ข ๐‘†๐บ โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

โ€ข ๐‘†๐บ โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

โ€ข ๐‘†๐บ โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐œโ„Ž +๐‘š๐‘’๐‘ก

โ€ข ๐ต๐บ าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

โ€ข ๐ต๐บ าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

โ€ข 2-leptons + 0-hadronic decay tau (7 class)

โ€ข ๐‘†๐บ โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

โ€ข ๐‘†๐บ โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

โ€ข ๐‘†๐บ โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

โ€ข ๐‘†๐บ โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

โ€ข ๐ต๐บ าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

โ€ข ๐ต๐บ าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

โ€ข ๐ต๐บ าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

Event Selection

24

* ๐‘™ = ๐‘’ ๐‘œ๐‘Ÿ ๐œ‡

0-lepton & 2-hadronic decay tau

25

Event Selection

26

โ€ข Using โ€ฆ โ€ข MG5_aMC v2.5.5 + MADSPIN / Delphes / PYTHIA8

โ€ข CT10nlo

โ€ข Cut โ€ฆโ€ข Delphes : Using delphes_card_ATLAS.dat

โ€ข Tau Tagging : ฮ”๐‘… < 0.4 , ฮ”๐‘…๐‘ก๐‘Ÿ๐‘Ž๐‘๐‘˜ < 0.2 , ๐‘ƒ๐‘‡๐‘‡๐‘Ÿ๐‘Ž๐‘๐‘˜ > 1.0 , ๐‘ƒ๐‘‡

๐œ > 2.0 , ๐œ‚๐œ < 2.5

1-prong Eff = 70% , N(>1)-prong eff = 60%

โ€ข Hadronical Tau decay using ALL N-prongs

1-lepton & 1-hadronic decay tau

27

2-lepton & 0-hadronic decay tau

28

Constraints of Mass

โ€ข H1 (tata) = 125.

โ€ข H2 (bb) = 125.

โ€ข Tau1 = Tau2

0-lepton & 2-hadronic decay tau

29

Constraints of Mass

โ€ข H1(tautau)= 125

โ€ข H2(bb)= 125

โ€ข Tau1 = Tau2

1-lepton & 1-hadronic decay tau

30

Constraints of Mass

โ€ข t1 = t2

โ€ข W1 = 80.4

โ€ข W2 = 80.4

โ€ข tau1 = 1.77

โ€ข tau2 = 1.77

2-lepton & 0-hadronic decay tau

31

Constraints of Mass

โ€ข H1 (tautau) = 125.

โ€ข H2 (bb) = 125.

โ€ข Tau1 = Tau2

Back up slides - OptiMass introduction

32

โ€ข Lagrange multipliers

๐‘€ เดฑ๐‘ฅโˆ— โ‰ก min๐‘ฅโˆˆโ„๐‘›

๐‘€ เดฑ๐‘ฅ ๐‘ . ๐‘ก. ๐‘๐‘Ž=1,โ€ฆ,๐‘š เดฑ๐‘ฅโˆ— = 0.

โ„’ ิฆ๐‘ฅ, ๐œ† = ๐‘€ ิฆ๐‘ฅ โˆ’

๐‘Ž=1

๐‘š

๐œ†๐‘Ž ๐‘๐‘Ž ิฆ๐‘ฅ .

constraintsMinimum value of the function

OPTIMASS: A Package for the Minimization of Kinematic Mass Functions with Constraints- Cho, Won Sang et al. JHEP 1601 (2016) 026 arXiv:1508.00589

โ€ข Penalty methods

๐‘ƒ ิฆ๐‘ฅ, ๐œ‡ โ‰ก ๐‘€ ิฆ๐‘ฅ +1

2๐œ‡

๐‘Ž=1

๐‘๐‘Ž2 ิฆ๐‘ฅ .

๐‘€ = minimized mass variable function๐œ†๐‘Ž = ๐‘Ž๐‘ข๐‘”๐‘š๐‘’๐‘›๐‘ก๐‘’๐‘‘ ๐ฟ๐‘Ž๐‘”๐‘Ÿ๐‘Ž๐‘›๐‘”๐‘’ ๐‘๐‘Ž๐‘Ÿ๐‘Ž๐‘š๐‘’๐‘ก๐‘’๐‘Ÿ๐œ‡ = ๐‘๐‘’๐‘›๐‘Ž๐‘™๐‘ก๐‘ฆ ๐‘๐‘Ž๐‘Ÿ๐‘Ž๐‘š๐‘’๐‘ก๐‘’๐‘Ÿ

-> It does NOT tell us which is the correct minimizer among

the N-stationary points!

33

Back up slides - OptiMass introduction

โœ“ The evolution of the intermediate feasibility tolerance ๐œ‚๐‘˜

โœ“ The real feasibility ๐‘๐‘– ๐‘ฅ๐‘˜

โœ“ The scale set by the ultimate feasibility tolerance ๐œ‚โˆ—

34

Back up slides โ€“ OPTIMASS Algorithm ExampleOPTIMASS: A Package for the Minimization of Kinematic Mass

Functions with Constraints - Cho, Won Sang et al. JHEP 1601 (2016) 026 arXiv:1508.00589 (pg 17-18)

35

36

โ€ข Di-Higgs search in โ€ฆโ€ข 2b + 2-lep

โ€ข 2b + 1-lep + 1-tau_h

โ€ข 2b + 2-tau_h

โ€ข High Level Feature variables for each decay channelโ€ข Existing (low level) variables (P_T/deltaR/MT2 โ€ฆ)

โ€ข OPTIMASS variables (om/cd)

โ€ข Around 40~70 variables

โ€ข Using Deep Neural Networkโ€ข Multi-class Classification

โ€ข Better performance than only using low level features

Summary(Backup)

Use DNN + OPTIMASS Variables!!!

37

Multi-Class ClassificationBinary classification Multi-Class classification

Green or Else

Blue or Else

Orange or ElseBlue or Orange

โ– Visible : CMS/ATLAS common featuresโ– Visible : CMS/ATLAS common features

38

Channel Leptons X section Topology

HH2Tau 0 ~1.2 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐œโ„Ž +๐‘š๐‘’๐‘ก

TT2Tau 0 ~5097.2 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐œโ„Ž +๐‘š๐‘’๐‘ก

HH2Tau 1 ~1.3 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

HH2W*W 1 ~0.15 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

HH2WW* 1 ~0.15 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐œโ„Ž +๐‘š๐‘’๐‘ก

TT2Tau 1 ~5546.3 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

TT1Tau 1 ~29700.2 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐œโ„Ž ๐‘™ + ๐‘š๐‘’๐‘ก

HH2Tau 2 ~0.36 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐œ ๐œ โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

HH2W*W1Tau 2 ~0.08 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

HH2WW*1Tau 2 ~0.08 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

HH2WW0Tau 2 ~0.47 โ„Žโ„Ž โ†’ ๐‘ ๐‘ ๐‘ค ๐‘คโˆ— โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

TT2Tau 2 ~1508.7 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐œ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

TT1Tau 2 ~16158.3 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐œ ๐‘™ + ๐‘š๐‘’๐‘ก โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

TT0Tau 2 ~43263.9 าง๐‘ก๐‘ก โ†’ ๐‘ ๐‘ค ๐‘ ๐‘ค โ†’ ๐‘ ๐‘ ๐‘™ ๐‘™ + ๐‘š๐‘’๐‘ก

39

Signal vs Background @ 14TeV, 39.64 fb (HH), 953.6 fb (TT)

* ๐‘™ = ๐‘’ ๐‘œ๐‘Ÿ ๐œ‡

Too Many invisible particles

from each distinctive/complicated

decay topologies