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Search for the rare decay ! " →$ % &̅& at J-PARC KOTO experiment Satoshi Shinohara (Osaka Univ.), on behalf of the KOTO collaboration KAON2019 10-13 September 2019 University of Perugia (Italy) 2019/9/10 KAON2019 1
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Search for the rare decay!" → $%&&̅ at J-PARC KOTO experimentSatoshi Shinohara (Osaka Univ.),on behalf of the KOTO collaboration

KAON201910-13 September 2019 University of Perugia (Italy)

2019/9/10 KAON2019 1

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Contents• Introduction• Results of 2015 physics run• 2016~2018 data analysis-Single event sensitivity-BG estimation

2019/9/10 KAON2019 2

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!" → $%&&̅ decay• Direct CPV

• FCNC : highly suppressed decay-BR (SM) : 3�10-11

• Small theoretical uncertainty�~2%�→ Good probe for new physics search

2019/9/10

10-8

10-9

10-10

10-11

direct limit (KOTO 2015 result, Phys.Rev.Lett. 122 (2019) no.2, 021802)3.0�10-9 (90% C.L.)

SM prediction3.0�10-11

indirect limit (Grossman-Nir bound)1.5�10-9

&

Ws d

t

Z

KAON2019 3

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!" → $%&&̅ decay• Direct CPV

• FCNC : highly suppressed decay-BR (SM) : 3�10-11

• Small theoretical uncertainty�~2%�→ Good probe for new physics search

2019/9/10

10-8

10-9

10-10

10-11

indirect limit (Grossman-Nir bound)1.5�10-9

&

Ws d

t

Z

A.J.Buras, et al. JHEP11(2014)121 M.Tanimoto, K.Yamamoto PTEP 2016 (2016) no.12, 123B02

NP ?

direct limit (KOTO 2015 result, Phys.Rev.Lett. 122 (2019) no.2, 021802)3.0�10-9 (90% C.L.)

KAON2019 4

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KOTO experiment

2019/9/10

J-PARC @ Tokai village

KAON2019 5

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Signal

2019/9/10

KL

π0->2γ

!!̅ (undetectable)

#$ → &'!!̅ : &' → 2) + nothing

CsI calorimeter(reconstruct &' from 2))

Hermetic veto detectors

Au target

30 GeV/c

proton

pencil beam

(KL, n, γ)

KAON2019 6

collimator +

sweeping magnet

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Background

2019/9/10

KL

π0->2γ

!!̅ (undetectable)

ex.) #$ → 2'( → 4*

CsI calorimeter(reconstruct '( from 2*)

Hermetic veto detectors

30 GeV/cproton

pencil beam(KL, n, γ)

KAON2019 7

π0->2γAu target

collimator + sweeping magnet

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Reconstruction

2019/9/10

KL

π0->2γ

!!̅decay region(vacuum)

π0 decay Z position

π0 Pt(transverse

momentum)

pencil beam(KL, n, γ)

KAON2019 8

Missing transverse momentum → finite π0 pt

CsI

signal region on the Pt vs. Z plane(blinded analysis)

CsI calorimeter

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Dec2012

Dec2013

Dec2014

Jan2016

Dec2016

Dec2017

Dec2018

Acc

umul

ated

P.O

.T.

0102030405060708090

1001810×

Bea

m P

ower

(kW

)

0

20

40

60

80

100

History of data taking

2019/9/10

2013 data(PTEP 2017

021C01)

Operation

of Hadron

facility was

stopped.

2015 data

(Phys. Rev.

Lett. 122,

021802)

2016, 2017, 2018 data

KAON2019 9

2019 data

(covered in another talk)

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Detector and DAQ upgrade in 2016-2018• Barrel detector was upgraded in 2016.4-13.5X0 → 18.5X0

-!" → 2%& BG : ×1/3

• DAQ upgrade (covered in poster session)

-Online cluster counting (2017~)-Higher DAQ live time ratio

• ~80% (2015 @ 42kW beam) → ~99% (2018 @ 51kW beam)

2019/9/10

!" → 2%&

Inner barrel (IB)

online clustering map

Energy deposit map of CsI

KAON2019 10

cluster

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Result of 2015 physics run

2019/9/10 KAON2019 11

observed

expectation

contour : !" → $%&&̅ (MC)

Phys. Rev. Lett. 122, 021802

• Single event sensitivity :

1.30 ± 0.01-./. ± 0.14-1-. ×1034-No event in the signal region

• Upper limit (90% C.L.) :

Br(56 → 789:9) < 3.0�10-9

�10 improvement from

previous limit (KEK E391a)

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Toward 2016-2018 data analysis

• To suppress hadron cluster BG is important-Need more understanding-Need more reduction

2019/9/10 KAON2019 12

BG source No. events!" → $%$&$' 0.05 � 0.02!" → 2$' 0.02 � 0.02Other !" decays 0.03 � 0.01Hadron cluster 0.24 � 0.17Upstream $' 0.04 � 0.03CV ) 0.04 � 0.02Total 0.42 � 0.18

Neutron related BG

KL BG

2015 run background summary table

neutron

Hadron cluster BG

CSI

Phys. Rev. Lett. 122, 021802

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Toward 2016-2018 data analysis

• Higher beam power

→ larger signal loss due to the accidental hit

(76% loss in 2015 analysis)

• To achieve better sensitivity

→ Narrower veto window

-Need BG study due to the narrower veto window

2019/9/10 KAON2019 13

study from 2015 data

2018 June, 51kW

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2016~2018 data analysisSingle event sensitivityBG analysis

2019/9/10 KAON2019 14

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2016~2018 data analysisSingle event sensitivityBG analysis

2019/9/10 KAON2019 15

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Single event sensitivity (S.E.S)

• S.E.S = (KL yield)�(signal acceptance)

2019/9/10 KAON2019 16

reconstructed KL mass distributionfrom !" → 2%& analysis

KL yield (@ beam exit) : 7.1�1012

(increase by a factor of 1.5 from 2015 data)

Preliminary

(covered in poster session)

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Single event sensitivity (S.E.S)• S.E.S = (KL yield)�(signal acceptance)

• Signal box : determined by S/N• S.E.S : 6.9�10-10 (S.E.S2015 : 1.3�10-9)

2019/9/10 KAON2019 17

signal acceptance : 2.0�10-4

!" → $%&&̅ MC blind regionsignal region

2015 signal box

2016 ~ 2018 signal box

signal acceptance : + 6% (from 2015 signal box)

Preliminary

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2016~2018 data analysisSingle event sensitivityBG analysis

2019/9/10 KAON2019 18

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Hadron cluster BG

2019/9/10 KAON2019 19

n nn

Al target(10 mm thickness)

Physics run Special run

Physics data Control sample

n n

preliminary preliminary

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Hadron cluster BG update from 2015 (statistics)

2019/9/10 KAON2019 20

0

50

100

150

200

250

300

RUNAll

Pi0RecZ2000 3000 4000 5000 6000

Pi0Pt

050100150200250300350400450500

1163

3945 0

28375

821632010

82407(33753)

RUNAll

�~9

control sample (2015) control sample (2016~2018)

preliminary

The collection efficiency of control sample was improved by DAQ upgrade

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Hadron cluster BG update from 2015 (cut)

2019/9/10 KAON2019 21

1. Cluster shape cut with deep learning-S/N :�~2

from 2015

2. Pulse shape discrimination with Fourier transformation-S/N :�~1.8

from 2015

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Hadron cluster BG update from 2015 (estimation)

• Found contamination in the control sample-Developed more reliable estimation method-reduction : �~27 with the new method

2019/9/10 KAON2019 22

(10 mm thickness) (10 mm thickness)

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Hadron cluster BG

2019/9/10 KAON2019 23

0.02 ±0.00

0.00 ±0.00

0.00 ±0.00

0.01 ±0.00

0.00 ±0.00

0.01 ±0.00

Preliminary

Extended signal region to downstream from this result

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Upstream-π0 BG

• Halo-neutron hits upstream detector- γ + γ

• small visible energy shifted reconstructed Z position

-n + γ• various reconstructed Z position

-Shrink signal box of upstream Z• #BGupstream-π0 : 0.00 ± 0.00

2019/9/10 KAON2019 24

n

π0->2γ

CsI

Preliminary

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CV-η BG

• Neutron hits Charged Veto (CV) and generates η- reconstruction :

assumed π0 mass-mη ~ 4mπ

0

→ reconstructed Z position : shifted in the signal region

#BGη = 0.03 ± 0.01

2019/9/10 KAON2019 25

η->2γn

CV (front)Z = 5862 [mm]

CSI Z = 6168 [mm]

CsI

Preliminary

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Overlapped pulse BG • Overlapped pulse shifts measured time-Narrower veto window

• recover signal acceptance• increase BG from overlapped pulse

2019/9/10 KAON2019 26

clock [8ns]

example of overlapped waveform

puls

e he

ight

[a.u

.]

veto window

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Overlapped pulse BG

2019/9/10 KAON2019 27

• Overlapped pulse discriminator-Pulse shape information : Fourier transformation- χ2 : compared with single hit template

Preliminary

w/o new methodw/ new method

χ2 distribution of upstream detector

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Overlapped pulse BG• Narrower veto window + overlapped pulse discriminator

2019/9/10 KAON2019 28

Overlapped pulse BG from !" → 3%& MC analysis

Overlapped pulse BG from !" → %'( MC analysis

Narrower veto window : Recovered 10% signal acceptanceNo remaining event due to overlapped pulse

PreliminaryPreliminary

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!" → $%$&$' BG• Neural net with deep leaning for !" → $%$&$' BG-Similar behavior as $' Pt and Z cut-S/N : improved even after applying Pt and Z cut which is

optimized !" → $%$&$' BG

2019/9/10 KAON2019 29

!" → $'((̅ efficiency !" → $%$&$' reductionPreliminary

Preliminary

Rec. π0 Z [mm] Rec. π0 Z [mm]

Rec

. π0

Pt [M

eV]

Rec

. π0

Pt [M

eV]

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!" → $%$&$' BG• Applying neural net with deep leaning cut-#BG!" → $%$&$' : 0.02 → <0.02 (90% C.L.)- signal acceptance : 90%

2019/9/10 KAON2019 30

2.05 ±0.14

0.02 ±0.01

0.65 ±0.08(including blind region)

0.05 ±0.02

0.01 ±0.01

<0.02

before Neural net cut after Neural net cut

observedexpectation of !" → $%$&$' BG

PreliminaryPreliminary

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!" → 2%&, !" → 2' BG

2019/9/10 KAON2019 31

Result from !" → 2%& MC study Result from !" → 2' MC study

PreliminaryPreliminary

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BG summary

2019/9/10 KAON2019 32

0

1

2

3

4

5

6

7

&&MinCSDDLVal>0.985&&MaxThetaChisq<4.5&&MinWFourierLH>0.5&&EtaCSD>0.91&&KLpipipi0DLVal>0.922

Pi0RecZ2000 3000 4000 5000 6000

Pi0Pt

050100150200250300350400450500&&MinCSDDLVal>0.985&&MaxThetaChisq<4.5&&MinWFourierLH>0.5&&EtaCSD>0.91&&KLpipipi0DLVal>0.922

462 0 0

0

00473.1 ±4.2 0.08 ± 0.06 0.00 ± 0.00

0.18± 0.09

0.00± 0.00

0.07± 0.05

0.05 ± 0.02

#BGKLpi0pi0 <0.18

KLpi+pi-pi0 <0.02

KL3pi0 (overlapped pulse)

<0.04

Ke3 (overlapped pulse) <0.09

KL2gamma 0.00 � 0.00

Upstream π0 0.00�0.00

Hadron cluster 0.02 �0.00

CV-pi0 <0.10

CV-eta 0.03�0.01

Total 0.05±0.02

S.E.S : 6.9�10-10

observedexpectation

Preliminary

Preliminary

0.33 ± 0.11 (including signal region)

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0

1

2

3

4

5

6

7

&&MinCSDDLVal>0.985&&MaxThetaChisq<4.5&&MinWFourierLH>0.5&&EtaCSD>0.91&&KLpipipi0DLVal>0.922

Pi0RecZ2000 3000 4000 5000 6000

Pi0Pt

050100150200250300350400450500&&MinCSDDLVal>0.985&&MaxThetaChisq<4.5&&MinWFourierLH>0.5&&EtaCSD>0.91&&KLpipipi0DLVal>0.922

2019/9/10 KAON2019 33

Preliminary

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0

1

2

3

4

5

6

7

&&MinCSDDLVal>0.985&&MaxThetaChisq<4.5&&MinWFourierLH>0.5&&EtaCSD>0.91&&KLpipipi0DLVal>0.922

Pi0RecZ2000 3000 4000 5000 6000

Pi0Pt

050100150200250300350400450500&&MinCSDDLVal>0.985&&MaxThetaChisq<4.5&&MinWFourierLH>0.5&&EtaCSD>0.91&&KLpipipi0DLVal>0.922

2019/9/10 KAON2019 34

Preliminary

unblinded in the end of Aug. 2019

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2019/9/10 KAON2019 35

0

1

2

3

4

5

6

7

&&MinCSDDLVal>0.985&&MaxThetaChisq<4.5&&MinWFourierLH>0.5&&EtaCSD>0.91&&KLpipipi0DLVal>0.749

Pi0RecZ2000 3000 4000 5000 6000

Pi0Pt

050100150200250300350400450500&&MinCSDDLVal>0.985&&MaxThetaChisq<4.5&&MinWFourierLH>0.5&&EtaCSD>0.91&&KLpipipi0DLVal>0.749

upstream detector

On-timing peak is shifted by large pulse

on-time

waveform of the event

measured time

0.08 ± 0.06

0.18± 0.09

473.1 ±4.2

0.00± 0.00

0.07± 0.05

0.05�0.02

expectation

Prelimin

ary

Preliminary

clock [8ns]AD

C [c

ount

s]

0.33�0.11

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2019/9/10 KAON2019 36

0

1

2

3

4

5

6

7

&&MinCSDDLVal>0.985&&MaxThetaChisq<4.5&&MinWFourierLH>0.5&&EtaCSD>0.91&&KLpipipi0DLVal>0.749

Pi0RecZ2000 3000 4000 5000 6000

Pi0Pt

050100150200250300350400450500&&MinCSDDLVal>0.985&&MaxThetaChisq<4.5&&MinWFourierLH>0.5&&EtaCSD>0.91&&KLpipipi0DLVal>0.749

#BGKL3pi0 (overlapped pulse) <0.04

Ke3 (overlapped pulse) <0.09

BG estimation related overlapped pulse

• Underestimated the BG from overlapped pulse?

• Checking the properties of the other candidates

• Did we miss other background sources?• planning to reevaluate

other BG sources

0.08 ± 0.06

0.18± 0.09

0.00± 0.00

0.07± 0.05

expectation

Preliminary

Prelimin

ary

0.05�0.02

0.33�0.11

473.1 ±4.2

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Summary• !" → $%&&̅ at J-PARC KOTO experiment

• S.E.S : 6.9�10-10

• BG estimation : 0.05 ± 0.02

• Opened the box

→ 4 candidates in the signal region

Event properties:

One event : overlapped waveform

Checking other candidates carefully

2019/9/10 KAON2019 37

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END

2019/9/10 KAON2019 38


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