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New Result on 𝐊+ → 𝛑+𝛎ത𝛎from the NA62 Experiment
Giuseppe Ruggiero (Lancaster University)
KAON 2019
Perugia, 10/09/2019
On behalf of the NA62 Collaboration
Outline
K+ → π+νതν @ NA62 (2017 Data)
• Physics case
• The NA62 experiment
• Data selection
• 𝜋0 rejection and the 𝜋0 → invisible decay
• Determination of the single event sensitivity
• Background studies
• Result
210/09/2019 Giuseppe Ruggiero - Kaon 2019
𝐊 → 𝛑𝛎ത𝛎 decays: a theoretically clean environment
• FCNC loop processes: sd coupling and highest CKM suppression
• Very clean theoretically: Short distance contribution. No hadronic uncertainties.
• SM predictions [Buras et al. JHEP 11 (2015) 33]
BR 𝐾+ → 𝜋+𝜈 ҧ𝜈 = 8.39 ± 0.30 ∙ 10−11𝑉𝑐𝑏
0.0407
2.8𝛾
73.2°
0.74
= 0.84 ± 0.10 ∙ 10−10
BR 𝐾𝐿 → 𝜋0𝜈 ҧ𝜈 = 3.36 ± 0.05 ∙ 10−11𝑉𝑢𝑏
0.00388
2𝑉𝑐𝑏
0.0407
2sin 𝛾
sin 73.2°
2
= 0.34 ± 0.06 ∙ 10−10
310/09/2019 Giuseppe Ruggiero - Kaon 2019
𝐊 → 𝛑𝛎ത𝛎 NP Sensitivity
• Simplified Z, Z’ models [Buras, Buttazzo,Knegjens, JHEP 1511 (2015) 166]
• Littlest Higgs with T-parity [Blanke, Buras, Recksiegel, EPJ C76 (2016) no.4 182]
• Custodial Randall-Sundrum [Blanke, Buras, Duling, Gemmler, Gori, JHEP 0903 (2009) 108]
• MSSM non-MFV [Tanimoto, Yamamoto, PTEP 2016 (2016) no.12, 123B02; Blazek, Matak, IntlJModPhys.A
29 (2014), 1450162; Isidori et al. JHEP 0608 (2006) 064]
• LFU violation models [Isidori et. al., Eur. Phys. J. C (2017) 77]
• Leptoquarks [S.Fajfer, et al. arXiv:1802.00786]
• Constraints from existing measurements (correlations model dependent)
Randall - SundrumZ’ (5 TeV) in constrained MFV LFU violation
410/09/2019 Giuseppe Ruggiero - Kaon 2019
𝐊+ → 𝛑+𝛎ത𝛎 Experimental State of the Art
𝐾+ decay in flight technique NA62𝐾+ decay at rest technique E787/E949
Data 2016
NA62
𝐵𝑅 𝐾+ → 𝜋+𝜈 ҧ𝜈 = 1.73−1.05+1.15 × 10−10
Phys. Rev. D 77, 052003 (2008)
Phys. Rev. D 79, 092004 (2009)
Phys. Lett. B 791, 156 (2019)
510/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 @ CERN - SPS
LHC
NA62
SPS
Primary goal:
Measurement of BR(K+ → π+νതν)
Technique:
K Decay – in – flight
Broader Physics program
~200 participants: Birmingham, Bratislava, Bristol, Bucharest, CERN, Dubna (JINR), Fairfax (GMU), Ferrara,Firenze, Frascati, Glasgow, Lancaster, Liverpool, Louvain-la-Neuve, Mainz, Moscow (INR), Naples, Perugia,Pisa, Prague, Protvino (IHEP) , Rome I, Rome II, San Luis Potosi, Torino, TRIUMF, Vancouver (UBC)
610/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Layout
Secondary positive beamDecay region and Detectors
Momentum 75 GeV/c, 1% rms
Divergence (RMS) 100 μrad
Transverse Size 60 × 30mm2
Composition ΤK+ 6% Τπ+ 70% p 24%
2017 typical Intensity 19 × 1011 ppp (450 MHz @ GTK3)
Fiducial region 60 m
K+ decay rate ~ 3 MHz
Vacuum 𝒪 10−6 mbar
Si pixel beam tracker + Straw tracker
LKr Calorimeter from NA48
Cerenkov counters for K id, RICH for p/m id
[NA62 Detector Paper, 2017 JINST 12 P05025]
MNP33400 GeV/c
SPS protons
710/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Runs
810/09/2019 Giuseppe Ruggiero - Kaon 2019* Including periods of beam off
𝐏𝐫𝐨𝐭𝐨𝐧𝐬𝐨𝐧𝐭𝐚𝐫𝐠𝐞𝐭
2014-15 (16) Pilot run, Commissioning runs
2016 Physics run (45 days*)
2017 Physics run (160 days*)
2018 Physics run (217 days*)
𝐃𝐚𝐭𝐞
NA62 Runs: Data Analyzed
910/09/2019 Giuseppe Ruggiero - Kaon 2019
~19 × 1011 protons per spill (3 s)
~2 × 1012 K+ decays
This talk
2014-15 (16) Pilot run, Commissioning runs
2016 Physics run (45 days*)
2017 Physics run (160 days*)
2018 Physics run (217 days*)
* Including periods of beam off
𝐏𝐫𝐨𝐭𝐨𝐧𝐬𝐨𝐧𝐭𝐚𝐫𝐠𝐞𝐭
𝐃𝐚𝐭𝐞
𝐊+ → 𝛑+𝛎ത𝛎 Decay-in-flight
mmiss2 = PK+ − Pπ+
2 Process Branching ratio
K+ → π+π0 γ 0.2067
K+ → μ+𝜈 γ 0.6356
K+ → π+π+π− 0.0558
K+ → π+π−e+ν 4.25 ∙ 10−5
1010/09/2019 Giuseppe Ruggiero - Kaon 2019
𝐊+ → 𝛑+𝛎ത𝛎 Decay-in-flight
mmiss2 = PK+ − Pπ+
2 Process Branching ratio
K+ → π+π0 γ 0.2067
K+ → μ+𝜈 γ 0.6356
K+ → π+π+π− 0.0558
K+ → π+π−e+ν 4.25 ∙ 10−5
Kinematic signal identificationR
eg
ion
1
Region 2
1110/09/2019 Giuseppe Ruggiero - Kaon 2019
𝐊+ → 𝛑+𝛎ത𝛎 Decay-in-flight
mmiss2 = PK+ − Pπ+
2
𝟏𝟓 < 𝐏𝛑+ < 𝟑𝟓 GeV/c
Particle ID (Cherenkov detectors)
Particle ID (Calorimeters, 𝜇 - veto)
Photon veto
Process Branching ratio
K+ → π+π0 γ 0.2067
K+ → μ+𝜈 γ 0.6356
K+ → π+π+π− 0.0558
K+ → π+π−e+ν 4.25 ∙ 10−5
Kinematic signal identificationR
eg
ion
1
Region 2
1210/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Cornerstones
𝒪 100 ps Timing between sub-detectors
𝒪 103 ÷ 104 Background suppression from kinematics
> 107 Muon suppression
> 107 π0 (from K+ → π+π0) suppression
1310/09/2019 Giuseppe Ruggiero - Kaon 2019
𝐊+ → 𝛑+𝛎ത𝛎 Analysis
• Trigger streams (hardware L0 + software L1): • «PNN»: kaon and charged particle identification, photon and muon veto
• «Control»: minimum bias
• Offline Analysis:
• Data samples: PNN; Control: K+ → π+π0, K+ → μ+ν, K+ → π+π+π−
• Blind analysis procedure: signal /control regions masked during the analysis
1) Selection
2) Determination of the single event sensitivity
3) Estimation and validation of the background
4) Opening of signal regions and results
1410/09/2019 Giuseppe Ruggiero - Kaon 2019
𝐊+ → 𝛑+𝛎ത𝛎 Selection
Selection
• K+- π+ matching
• K+ decays in the decay volume
• π+ identification (PID)
• photon rejection
• Multi-track rejection
1510/09/2019 Giuseppe Ruggiero - Kaon 2019
Measured performance
GTK-KTAG-RICH timing: 𝒪 100 ps
σ mmiss2 ~ 10−3 ΤGeV2 c4
π+ ID: εμ~10−8, επ+~64%
𝜋0 rej: 𝜀𝜋0~1.4 ∙ 10−8, 𝑝𝜋+𝜖 15,35 GeV/c
𝑚𝑚𝑖𝑠𝑠2 : π+/K+ 3-momentum from Straw/Gigatracker, 𝜋+ mass hypothesis
Control data
π+π+π− Region
π+π0 Region
μ+ν
Region
Signal Region 2
Signal
Region 1
𝐾+decays selected before PID
and 𝛾/multi-track rejection
𝝅+ 𝐦𝐨𝐦𝐞𝐧𝐭𝐮𝐦 [𝐆𝐞𝐕/𝐜]
𝒎𝒎𝒊𝒔𝒔
𝟐Τ
𝑮𝒆𝑽𝟐𝒄𝟒
𝛑𝟎 rejection and search for 𝛑𝟎 → invisibleA-priori evaluation of π0 rejection in 𝐾+ → 𝜋+𝜋0 (0.015 < 𝑚𝑚𝑖𝑠𝑠
2 < 0.021 ΤGeV2 c4)
• Same selection, and trigger stream as 𝐾+ → 𝜋+𝜈 ҧ𝜈, about Τ1 3 of the data used for 𝜋𝜈𝜈
• Single-𝛾 detection efficiency from data minimum-bias 𝐾+ → 𝜋+𝜋0 (Tag & Probe)
• π0 rejection evaluated from convolution with MC 𝐾+ → 𝜋+𝜋0 𝛾
• Validation: side-bands with expected rejection 𝒪 10−7 where 𝜋0 → invisible excluded
• π0 rejection expected: 2.8−2.1+5.0 × 10−9 (𝜋+ momentum 25-40 GeV/c)
1610/09/2019 Giuseppe Ruggiero - Kaon 2019
[E949, PRD72 (2005)]
Result• BR(π0 → invisible) normalized to 𝜋0 → 𝛾𝛾
• Background expected: 10−8+22 (𝐾+ → 𝜋+𝜋0)
• Events observed: 12
BR π0 → invisible < 4.4 × 10−9 @ 90% CLUL 60 times stronger than past measurement
𝝅𝝂𝝂: Data After Selection
Region 2
Region 1
π+π0
Control Regions
Upstream background control region
μ+νControl Region
High - P
control region
Control and signal regions MASKED
1710/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Preliminary
π+π+π−
Control Region
𝝅𝝂𝝂 Single Event Sensitivity (S.E.S.)
S. E. S. =Br πνν
Nπνν𝑒𝑥𝑝
• Ratio of πνν and π+π0 acceptances allows cancellation of systematic effects
• Computation in bins of π+ momentum and instantaneous beam intensity
Nπνν𝑒𝑥𝑝
≈ Nππ εRV εtriggerAπννAππ
Br πνν
Br ππ
Nπνν𝑒𝑥𝑝
Expected number of πνν events
Br πνν SM πνν branching ratio
Nππ K+ → π+π0 from control πνν-like selected without γ/multiplicity rejection
εRV πνν loss due to γ/multi-track rejection because of random activity
εtrigger PNN trigger efficiency
Aπνν,ππ Monte Carlo acceptances for πνν (~3.0%*) and π+π0 (~8.5%)
Br ππ PDG K+ → π+π0 branching ratio
1810/09/2019 Giuseppe Ruggiero - Kaon 2019* Vector form factors
𝝅𝝂𝝂 Single Event Sensitivity
𝛆𝐑𝐕 measured on K+ → μ+ν data 𝛆𝒕𝒓𝒊𝒈𝒈𝒆𝒓 measured on data
1910/09/2019 Giuseppe Ruggiero - Kaon 2019
• Intensity measured event-by-event using Gigatracker time sidebands
NA62 Preliminary𝜀𝑅𝑉 2017 = 0.638 ± 0.014
𝝅𝝂𝝂 S.E.S: Results
• Integrated over beam intensity and 𝜋+ momentum
• Error budget (S.E.S.)
• External error on 𝑁𝜋𝜈𝜈𝑒𝑥𝑝
from 𝐵𝑟(𝜋𝜈𝜈) = 0.84 ± 0.10 × 10−10
2010/09/2019 Giuseppe Ruggiero - Kaon 2019
𝑆. 𝐸. 𝑆. = 0.389 ± 0.021 × 10−10 𝑁𝜋𝜈𝜈𝑒𝑥𝑝
= 2.16 ± 0.12 ± 0.26𝑒𝑥𝑡
𝝅𝝂𝝂: Data After Selection
π+π0
Control Regions
Upstream background control region
μ+νControl Region
High - P
control region
Control and signal regions MASKED
2110/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Preliminary
π+π+π−
Control Region
Region 2
Region 1
𝐊+ → 𝛑+𝛑𝟎 Backgrounds
Fraction of π+π0
in signal region measured on control data
Data in π+π0 regionafter πνν selection:γ −rejection applied
Minimum bias K+ → π+π0 data used
to study the tails of the mmiss2
Expected K+ → π+π0
in signal regions afterπνν selection
2210/09/2019 Giuseppe Ruggiero - Kaon 2019
Background Validation
K+ → π+π0 background expectedand observed in control regions(CR1+CR2) after πνν selection
K+ → μ+ν background expected andobserved in control region (CR) afterπνν selection
2310/09/2019 Giuseppe Ruggiero - Kaon 2019
Expected Background from 𝑲+
decays
2410/09/2019 Giuseppe Ruggiero - Kaon 2019
Normal 𝐊+Decay
Achromat
𝐊+(𝟕𝟓 𝐆𝐞𝐕)
Collimator
1st Straw Chamber
Decay region
𝐊+(𝟕𝟓 𝐆𝐞𝐕)
𝜸, 𝝂
𝜸, 𝝂
Decay vertex
Gigatracker
z
y
2510/09/2019 Giuseppe Ruggiero - Kaon 2019
Normal 𝐊+Decay
Achromat
𝐊+(𝟕𝟓 𝐆𝐞𝐕)
Collimator
1st Straw Chamber
Decay region
𝐊+(𝟕𝟓 𝐆𝐞𝐕)
𝜸, 𝝂
𝜸, 𝝂
Decay vertex
z
y
𝐾+ → 𝜋+𝜈 ҧ𝜈 projected at collimator (MC)
2610/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Preliminary
Upstream Decay / Interaction
Achromat
𝐊+(𝟕𝟓 𝐆𝐞𝐕)
Collimator
1st Straw Chamber
Decay region
𝜸𝜸
• K+ decays/interacts in the achromat
• Secondary 𝜋+ downstream
• Beam elements block additional particles
2710/09/2019 Giuseppe Ruggiero - Kaon 2019
z
y
Upstream Background
Achromat
𝐊+(𝟕𝟓 𝐆𝐞𝐕)
Collimator
1st Straw Chamber
Decay regionIn-time pileupbeam particle
𝜸𝜸
• K+ decays/interacts in the achromat
• Secondary 𝜋+ downstream
• Beam elements block additional particles
• Pileup beam particle tagged as K+
Fake decay vertex
2810/09/2019 Giuseppe Ruggiero - Kaon 2019
z
y
Upstream Background
Achromat
𝐊+(𝟕𝟓 𝐆𝐞𝐕)
Collimator
1st Straw Chamber
Decay regionIn-time pileupbeam particle
𝜸𝜸
Fake decay vertex
• K+ decays/interacts in the achromat
• Secondary 𝜋+ downstream
• Beam elements block additional particles
• 𝜋+ scattering in straw chamber 1
• Pileup beam particle tagged as K+
2910/09/2019 Giuseppe Ruggiero - Kaon 2019
z
y
NA62 Preliminary
Upstream Background
Achromat
𝐊+(𝟕𝟓 𝐆𝐞𝐕)
Collimator
1st Straw Chamber
Decay regionIn-time pileupbeam particle
𝜸𝜸
Fake decay vertex
• K+ decays/interacts in the achromat
• Secondary 𝜋+ downstream
• Beam elements block additional particles
• 𝜋+ scattering in straw chamber 1
• Pileup beam particle tagged as K+
3010/09/2019 Giuseppe Ruggiero - Kaon 2019
z
y
NA62 PreliminaryRegion removed offline
Upstream Background
Achromat
𝐊+(𝟕𝟓 𝐆𝐞𝐕)
Collimator
1st Straw Chamber
Decay regionIn-time pileupbeam particle
𝜸𝜸
• K+ decays/interacts in the achromat
• Secondary 𝜋+ downstream
• Beam elements block additional particles
• 𝜋+ scattering in straw chamber 1
• Pileup beam particle tagged as K+
Count events on data withinverted 𝐾 − 𝜋 matching
Estimate the probability tooccur from data/simulation
3110/09/2019 Giuseppe Ruggiero - Kaon 2019
z
y
Fake decay vertex
Total Expected Background
3210/09/2019 Giuseppe Ruggiero - Kaon 2019
Final Background ValidationSignal and background evaluated in the 35-40 GeV/c signal-like regions
𝐛𝐚𝐜𝐤𝐠𝐫𝐨𝐮𝐧𝐝 = 𝟎. 𝟔𝟐 ± 𝟎. 𝟏𝟑
𝐬𝐢𝐠𝐧𝐚𝐥 = 𝟎. 𝟏𝟑 ± 𝟎. 𝟎𝟏
3310/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Preliminary
Final Background Validation1 event observed in 35-40 GeV/c region
3410/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Preliminary
Opening the Box
3510/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Preliminary
3610/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Preliminary
Box Opened
3710/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Preliminary
Box Opened2 events observed in signal region
2017 Result• Counting experiment
𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 = 0.20−0.20+0.69 × 10−10• Two-sided 68% band:
• Upper limits (CLs method)
3810/09/2019 Giuseppe Ruggiero - Kaon 2019
Observed Expected (background only) CL
𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 < 1.76 × 10−10 𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 < 1.41 × 10−10 90%
𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 < 2.11 × 10−10 𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 < 1.76 × 10−10 95%
Events observed 2
Single event sensitivity 0.389 ± 0.021 × 10−10
Expected background 1.50 ± 0.30
𝒎𝒎𝒊𝒔𝒔𝟐 Signal and Background 2017
3910/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Preliminary
2016+2017 Result
𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 = 0.47−0.47+0.72 × 10−10• Two-sided 68% band:
• Upper limits (CLs method)
4010/09/2019 Giuseppe Ruggiero - Kaon 2019
Observed Expected (background only) CL
𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 < 1.85 × 10−10 𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 < 1.32 × 10−10 90%
𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 < 2.44 × 10−10 𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 < 1.62 × 10−10 95%
Events observed 3
Single event sensitivity 0.346 ± 0.017 × 10−10
Expected background 1.65 ± 0.31
• 2016 and 2017 data uncorrelated
𝐊+ → 𝛑+𝛎ത𝛎 Experimental Status
4110/09/2019 Giuseppe Ruggiero - Kaon 2019
PRD 10 (1974) 897
NPB 304 (1988) 205
PRD 54 (1996) 6782
PRD 76 (2007) 034017
PRD 83 (2011) 034030
JHEP 11 (2015) 33
NA62 Preliminary
𝐊+ → 𝛑+𝛎ത𝛎 Experimental Status
4210/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Preliminary
𝑲+ → 𝝅+𝝂ത𝝂 and 𝑲𝑳 → 𝝅𝟎𝝂ത𝝂
4310/09/2019 Giuseppe Ruggiero - Kaon 2019
• New Grossman – Nir limit: 𝐵𝑟 𝐾𝐿 → 𝜋0𝜈𝜈 < 8.14 × 10−10 @ 90% 𝐶𝐿
Conclusions
• Two events in signal region observed in 2017 data• S. E. S. = 0.389 ± 0.021 × 10−10
• Expected background: 1.50 ± 0.30 events
4410/09/2019 Giuseppe Ruggiero - Kaon 2019
• Constraints on the largest enhancements allowed by NP models
• 𝐾+ → 𝜋+𝑋, 𝑋 →invisible at the 𝜋0 mass:
• 2016+2017 NA62 result:
𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 < 1.85 × 10−10 @ 90% 𝐶𝐿
𝐵𝑟 𝐾+ → 𝜋+𝜈 ҧ𝜈 = 0.47−0.47+0.72 × 10−10
𝐵𝑟 π0 → invisible < 4.4 × 10−9 @ 90% 𝐶𝐿
Plans
• 2018 data analysis in progress• 2 × 2017 data sample
• On-going studies to increase signal efficiency
• On-going studies to reduce the random veto
• Shape analysis
4510/09/2019 Giuseppe Ruggiero - Kaon 2019
• >2021 data taking: • Plans to strongly suppress the upstream background
• Run at higher beam intensity foreseen
10/09/2019 Giuseppe Ruggiero - Kaon 2019 46
SPARES
Particle Identification
Calorimeters RICH
4710/09/2019 Giuseppe Ruggiero - Kaon 2019
NA62 Preliminary
Upstream Background Estimate
• Probability to tag a pileup beam particle as a K+ depends on• Closest distance of approach (CDA) between kaon and pion track
• Timing between KTAG – Gigatracker – RICH
4810/09/2019 Giuseppe Ruggiero - Kaon 2019
• Probability estimation («mis-tag probability»)• CDA shape of upstream events from simulation validated with data
• Computed as a function of KTAG – Gigatracker and KTAG – RICH time difference
• Background estimation• Number of upstream events from data selected with inverted K+/π+ matching
• Upstream events weigthed with the mis-tag probability as a function of the KTAG – Gigatracker and KTAG – RICH time difference
• Estimation validated on data inverting cuts against upstream events
Upstream Background Validation
4910/09/2019 Giuseppe Ruggiero - Kaon 2019
• Sample: upstream-enriched data sets selected
in mmiss2 signal regions
• Expectation: result of the upstream estimation applied to a given sample
NA62 Preliminary
𝐊+ → 𝛑+𝛑−𝐞+𝛎 (𝑲𝒆𝟒) Background:
Validation
5010/09/2019 Giuseppe Ruggiero - Kaon 2019
• Sample: Ke4-enriched data
sets selected in mmiss2 signal
regions
• Expectation: MC normalized to 𝐾+ → 𝜋+𝜋0 like 𝜋𝜈𝜈
NA62 Preliminary