skip to main content
US FlagAn official website of the United States government
dot gov icon
Official websites use .gov
A .gov website belongs to an official government organization in the United States.
https lock icon
Secure .gov websites use HTTPS
A lock ( lock ) or https:// means you've safely connected to the .gov website. Share sensitive information only on official, secure websites.


Search for: All records

Creators/Authors contains: "Oskin, P"

Note: When clicking on a Digital Object Identifier (DOI) number, you will be taken to an external site maintained by the publisher. Some full text articles may not yet be available without a charge during the embargo (administrative interval).
What is a DOI Number?

Some links on this page may take you to non-federal websites. Their policies may differ from this site.

  1. We measure the complete set of angular coefficients J i for exclusive B ¯ D * ν ¯ decays ( = e , μ ). Our analysis uses the full 711 fb 1 Belle dataset with hadronic tag-side reconstruction. The results allow us to extract the form factors describing the B ¯ D * transition and the Cabibbo-Kobayashi-Maskawa matrix element | V cb | . Using recent lattice QCD calculations for the hadronic form factors, we find | V cb | = ( 40.7 ± 0.7 ) × 10 3 using the Boyd-Grinstein-Lebed parametrization, compatible with determinations from inclusive semileptonic decays. We search for lepton flavor universality violation as a function of the hadronic recoil parameter w and investigate the differences of the electron and muon angular distributions. We find no deviation from standard model expectations. Published by the American Physical Society2024 
    more » « less
  2. We report a search for a heavy neutral lepton (HNL) that mixes predominantly with ν τ . The search utilizes data collected with the Belle detector at the KEKB asymmetric energy e + e collider. The data sample was collected at and just below the center-of-mass energies of the ϒ ( 4 S ) and ϒ ( 5 S ) resonances and has an integrated luminosity of 915 fb 1 , corresponding to ( 836 ± 12 ) × 10 6 e + e τ + τ events. We search for production of the HNL (denoted N ) in the decay τ π N followed by its decay via N μ + μ ν τ . The search focuses on the parameter-space region in which the HNL is long-lived, so that the μ + μ originate from a common vertex that is significantly displaced from the collision point of the KEKB beams. Consistent with the expected background yield, one event is observed in the data sample after application of all the event-selection criteria. We report limits on the mixing parameter of the HNL with the τ neutrino as a function of the HNL mass. Published by the American Physical Society2024 
    more » « less
  3. We report measurements of time-dependent C P asymmetries in B 0 K S 0 π 0 γ decays based on a data sample of ( 388 ± 6 ) × 10 6 B B ¯ events collected at the ϒ ( 4 S ) resonance with the Belle II detector. The Belle II experiment operates at the SuperKEKB asymmetric-energy e + e collider. We measure decay-time distributions to determine C P -violating parameters S and C . We determine these parameters for two ranges of K S 0 π 0 invariant mass: m ( K S 0 π 0 ) ( 0.8 , 1.0 ) GeV / c 2 , which is dominated by B 0 K * 0 ( K S 0 π 0 ) γ decays, and a complementary region m ( K S 0 π 0 ) ( 0.6 , 0.8 ) ( 1.0 , 1.8 ) GeV / c 2 . Our results have improved precision as compared to previous measurements and are consistent with theory predictions. Published by the American Physical Society2025 
    more » « less
    Free, publicly-accessible full text available January 1, 2026
  4. We describe a measurement of charge-parity ( C P ) violation asymmetries in B 0 η K S 0 decays using Belle II data. We consider η η ( γ γ ) π + π and η ρ ( π + π ) γ decays. The data were collected at the SuperKEKB asymmetric-energy e + e collider between the years 2019 and 2022, and contain ( 387 ± 6 ) × 10 6 bottom-antibottom meson pairs. We reconstruct 829 ± 35 signal decays and extract the C P violating parameters from a fit to the distribution of the proper-decay-time difference between the two B mesons. The measured direct and mixing-induced C P asymmetries are C η K S 0 = 0.19 ± 0.08 ± 0.03 and S η K S 0 = + 0.67 ± 0.10 ± 0.03 , respectively, where the first uncertainties are statistical and the second are systematic. These results are in agreement with current world averages and standard model predictions. Published by the American Physical Society2024 
    more » « less
    Free, publicly-accessible full text available December 1, 2025
  5. A<sc>bstract</sc> We report a determination of the CKM angleϕ3, also known asγ, from a combination of measurements using samples of up to 711 fb−1from the Belle experiment and up to 362 fb−1from the Belle II experiment. We combine results from analyses ofB+→ DK+,B+→ Dπ+, andB+→ D*K+decays, whereDis an admixture ofD0and$$ {\overline{D}}^0 $$ D ¯ 0 mesons, in a likelihood fit to obtainϕ3= (75.2±7.6)°. We also briefly discuss the interpretation of this result. 
    more » « less
  6. The ratio of branching fractions R ( D * ) = B ( B ¯ D * τ ν ¯ τ ) / B ( B ¯ D * ν ¯ ) , where is an electron or muon, is measured using a Belle II data sample with an integrated luminosity of 189 fb 1 at the SuperKEKB asymmetric-energy e + e collider. Data is collected at the ϒ ( 4 S ) resonance, and one B meson in the ϒ ( 4 S ) B B ¯ decay is fully reconstructed in hadronic decay modes. The accompanying signal B meson is reconstructed as B ¯ D * τ ν ¯ τ using leptonic τ decays. The normalization decay, B ¯ D * ν ¯ , produces the same observable final-state particles. The ratio of branching fractions is extracted in a simultaneous fit to two signal-discriminating variables in both channels and yields R ( D * ) = 0.262 0.039 + 0.041 ( stat ) 0.032 + 0.035 ( syst ) . This result is consistent with the current world average and with Standard Model predictions. Published by the American Physical Society2024 
    more » « less