E B Holzer’s research while affiliated with CERN and other places

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Publications (167)


First search for K+ → π0πμe decays
  • Article

November 2024

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15 Reads

Physics Letters B

M.U. Ashraf

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E. Minucci

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[...]

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A. Zinchenko

FIG. 3. Data distribution in the plane ðZ TAX ; CDA TAX Þ for e þ e − vertices without applying the LAV and ANTI0 veto conditions. CR and SR are masked.
FIG. 4. Observed and expected exclusion contours, at 90% CL, in the plane ðM A 0 ; εÞ for the A 0 → e þ e − analysis (left) and the combined A 0 → e þ e − and A 0 → μ þ μ − analyses (right) together with the expected AE1σ (green) and AE2σ (yellow) bands. Previous results, including the recent FASER result [25] are shown in gray. The NA62 A 0 → μ þ μ − result [10] is shown with a dot-dashed line in the right panel.
FIG. 5. Exclusion region in the plane of the ALP lifetime ðτ a Þ and the product of branching ratios BRðB → K ðÃÞ aÞ × BRða → e þ e − Þ in the search for an axionlike particle a produced in B meson decays (solid curve). Four values of the ALP mass are considered. The region of the parameter space above the black line is excluded at 90% CL. The excluded regions by CHARM [34] measurements are shown as gray-filled areas.
Search for Leptonic Decays of Dark Photons at NA62
  • Article
  • Full-text available

September 2024

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63 Reads

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2 Citations

Physical Review Letters

The NA62 experiment at CERN, configured in beam-dump mode, has searched for dark photon decays in flight to electron-positron pairs using a sample of 1.4 × 10 17 protons on dump collected in 2021. No evidence for a dark photon signal is observed. The combined result for dark photon searches in lepton–antilepton final states is presented and a region of the parameter space is excluded at 90% confidence level, improving on previous experimental limits for dark photon mass values between 50 and 600 MeV / c 2 and coupling values in the range 10 − 6 to 4 × 10 − 5 . An interpretation of the e + e − search result in terms of the emission and decay of an axionlike particle is also presented. Published by the American Physical Society 2024

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Development of a new CEDAR for kaon identification at the NA62 experiment at CERN

May 2024

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63 Reads

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1 Citation

Journal of Instrumentation

The NA62 experiment at CERN utilises a differential Cherenkov counter with achromatic ring focus (CEDAR) for tagging kaons within an unseparated monochromatic beam of charged hadrons. The CEDAR-H detector was developed to minimise the amount of material in the path of the beam by using hydrogen gas as the radiator medium. The detector was shown to satisfy the kaon tagging requirements in a test-beam before installation and commissioning at the experiment. The CEDAR-H performance was measured using NA62 data collected in 2023.





Improved calorimetric particle identification in NA62 using machine learning techniques

November 2023

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70 Reads

Journal of High Energy Physics

A bstract Measurement of the ultra-rare K+π+νν {K}^{+}\to {\pi}^{+}\nu \overline{\nu} K + → π + ν ν ¯ decay at the NA62 experiment at CERN requires high-performance particle identification to distinguish muons from pions. Calorimetric identification currently in use, based on a boosted decision tree algorithm, achieves a muon misidentification probability of 1 . 2 × 10 − 5 for a pion identification efficiency of 75% in the momentum range of 15–40 GeV/ c . In this work, calorimetric identification performance is improved by developing an algorithm based on a convolutional neural network classifier augmented by a filter. Muon misidentification probability is reduced by a factor of six with respect to the current value for a fixed pion-identification efficiency of 75%. Alternatively, pion identification efficiency is improved from 72% to 91% for a fixed muon misidentification probability of 10 − 5 .



Figure 2. Reconstructed m 2 miss (K e3 ) of signal candidates as a function of the time difference T γ − T LKr . The m 2 miss (K e3 ) condition is shown (red horizontal line), together with the signal selection time window (red vertical lines) and the side-bands (black dashed vertical lines).
A study of the K+ → π0e+νγ decay

September 2023

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70 Reads

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2 Citations

Journal of High Energy Physics

A bstract A sample of 1 . 3 × 10 ⁵ K ⁺ → π ⁰ e ⁺ νγ candidates with less than 1% background was collected by the NA62 experiment at the CERN SPS in 2017–2018. Branching fraction measurements are obtained at percent relative precision in three restricted kinematic regions, improving on existing results by a factor larger than two. An asymmetry, possibly related to T-violation, is investigated with no evidence observed within the achieved precision.


Figure 10. Distribution of CDA TAX vs Z TAX for µ + µ − events: expected combinatorial background (colour-scale plot) and data events (black dots). Validation and signal regions are masked for data. Additional regions, CR 3,2,1 , are not masked.
Figure 13. Expected number of events for the A decay to µ + µ − as a function of the A mass and coupling constant. Left (right) panel refers to bremsstrahlung (meson-decay) production. The black contours correspond to 2.3 events.
Figure 15. Distributions of CDA TAX vs Z TAX . Left: data (dots) and expected background (colourscale plot). Right: data (dots) and expected signal density (colour scale). Bins of 2 mm × 1 m size are used for the colour scale.
Search for dark photon decays to μ+μ− at NA62

September 2023

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83 Reads

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16 Citations

Journal of High Energy Physics

A bstract The NA62 experiment at CERN, designed to study the ultra-rare decay K ⁺ → π ⁺ νν \nu \overline{\nu} ν ν ¯ , has also collected data in beam-dump mode. In this configuration, dark photons may be produced by protons dumped on an absorber and reach a decay volume beginning 80 m downstream. A search for dark photons decaying in flight to μ ⁺ μ − pairs is reported, based on a sample of 1 . 4 × 10 ¹⁷ protons on dump collected in 2021. No evidence for a dark photon signal is observed. A region of the parameter space is excluded at 90% CL, improving on previous experimental limits for dark photon masses between 215 and 550 MeV /c ² .


Citations (80)


... An interpretation of the results in a dark photon model are given in Fig. 19. This includes the initial sensitivity of FASER with a track-based analysis [9] as discussed in Appendix A. Additionally, search results from NA62 [115], NA64 [116], NuCal [93,117] and E141 [118,119] are shown. ...

Reference:

Shining Light on the Dark Sector: Search for Axion-like Particles and Other New Physics in Photonic Final States with FASER
Search for Leptonic Decays of Dark Photons at NA62

Physical Review Letters

... This additional magnet spectrometer also reduces the background from in-flight kaons decays given a shorter distance to the target by a factor ∼ 10 −1 . It is worth noting that this background could be further reduced and controlled by proper identification of kaons along the beam-line through the use of Cherenkov counter with achromatic ring focus (CEDAR) [111]. Finally, the computations of the projected limits assume a reduction of the background related to non-hermeticity of the detectors'. ...

Development of a new CEDAR for kaon identification at the NA62 experiment at CERN

Journal of Instrumentation

... The ALP-gluon limits in comparison with results from NA62 [90][91][92], BaBar [74], flavour constraints [20], NuCal [20,93], CHARM [94], NA48 [95,96], E949 [97][98][99] and from the total decay width of the kaon [96] are shown in Fig. 17(c). Fig. 18(a) displays the existing constraints for the U(1) B model in comparison to the FASER limit presented. ...

Measurement of the K+ → π+γγ decay
  • Citing Article
  • March 2024

Physics Letters B

... There are specific observables in the kaon sector that have been under intense experimental scrutiny to further augment our understanding of the Standard Model (SM). They include the golden channels: BR(K + → π + νν) at NA62 [1] and BR(K L → π 0 νν) at KOTO [2,3], the rare decay modes BR(K + → π + µμ) at NA62 [4] and K S → µµ at LHCb [5]. These analyses were preceded by several past endeavours that is inclusive of those at E865 [6] and NA48/2 [7] for BR(K + → π + eē) and at NA48/2 [8] for BR(K + → π + µμ). ...

Addendum to: A measurement of the K+ → π+μ+μ− decay

Journal of High Energy Physics

... In the same regime however, the two electrons produced by the new particle decay will carry each E ∼ m X /2, allowing a larger fraction to pass the momentum cut. B v 2 H a K q j o g Q u H c + 7 l 3 n u C i D N t f P / N S / X 1 D w w O D Y + k R 8 f G J y Y z U 9 M l H V p F a J G E P F T l A G v K m a R F w w y n 5 U h R L A J O j 4 P z v Y 5 / f E G V Z q E 8 M u 2 I 1 g R u S d Z k B B s n 1 T N z V 8 V 6 f F A V N r k 6 W Y e 7 s C q t i O k a Q k k 9 s + x n / S 6 g n 8 3 l N t D G l i O b O z m E t i H 6 t J b z i w u n q d v Z x 0 I 9 8 1 5 t h M Q K K g 3 h W O s K 8 i N T i 7 E y j H C a p K t W 0 w i T c 9 y i F U c l F l T X 4 u 4 L C V x x S g M 2 Q + V K G t h V v 0 / E W G j d F o H r F N i c 6 d 9 e R / z L q 1 j T 3 K 7 F T E b W U E l 6 i 5 q W Q x P C T h 6 w w R Q l h r c d w U Q x d y s k Z 1 h h Y l x q P 7 Z o Z i U z l 0 n a J f P 1 P v y f l N a z a We consider the secondary muon flux produced at NA62 in dump mode [62], which has been simulated in Ref. [42]. The idea is that the muons could decay in flight to an ALP plus electron, for which we saturate the branching limit BR (µ → e + inv.) ≤ 2.6 × 10 −6 from Jodidio et.al. ...

Search for dark photon decays to μ+μ− at NA62

Journal of High Energy Physics

... Although no signs of LN or LF violation are observed, these results set the current world's most stringent upper limits (UL) on the branching ratios, improving considerably over the previous best results. Of particular Decay channel Previous BR UL [8] NA62 BR UL Improvement + → − + + 8.6 × 10 −11 4.2 × 10 −11 [9] ∼ factor 2 + → − + + 6.4 × 10 −10 5.3 × 10 −11 [10] ∼ factor 12 [10] first search + → − + + 5.0 × 10 −10 4.2 × 10 −11 [11] ∼ factor 12 + → + − + 5.2 × 10 −10 6.6 × 10 −11 [11] ∼ factor 8 [12] ∼ factor 250 interest is the channel + → − + + ( ), which can violate LN or LF depending on the flavor of the neutrino in the final state. The only previous search for this process dates back to the Geneva-Saclay experiment in 1976 [7]. ...

A search for the → decay
  • Citing Article
  • January 2023

Physics Letters B

... The model can be tested by the current and future measurements of various flavor experiments like Kaon rare decays, in addition to high energy collider experiments as well as gravitational wave observations. For example, top-charm mixing and its CP violating phase are important parameters to test the model via the signals at direct search experiments [49][50][51][52][53][54][55] and various transition processes of K mesons and B mesons [56][57][58][59][60][61][62][63][64]. In particular, they would be testable via the golden modes K → πνν [65,66] at KOTO experiment at J-PARK [62,67] and NA62 experiment at the CERN SPS [63,64]. ...

Measurement of the very rare K+π+ννˉK^+ \to \pi^+ \nu \bar\nu decay