6533b7defe1ef96bd1276532

RESEARCH PRODUCT

Measurement of the neutralDmeson mixing parameters in a time-dependent amplitude analysis of theD0→π+π−π0decay

J. A. MckennaE. PaoloniJ. L. RitchieS. I. SerednyakovM. RotondoElisa ManoniG. De NardoR. Y. SoDebbie PayneM. RöhrkenB. N. RatcliffC. BüngerAlessandro PilloniGiulia CasarosaG. WormserD. E. HutchcroftM. T. GrahamJ. KimR. SaccoD. R. PeimerT. LeddigA. JawaheryAndrei GritsanG. CibinettoE. GabathulerT. SchroederW. R. InnesFlorian Urs BernlochnerR. F. SchwittersF. C. PorterF. PalomboT. LueckA. G. DenigA. J.s. SmithW. DunwoodieF. SimonettoW. S. LockmanA. M. EisnerYu. I. SkovpenG. R. BonneaudM. ChrzaszczE. Ben-haimC. VoßYu. G. KolomenskyA. OyangurenM. PiccoloG. BatignaniM. R. ConveryS. AkarX. C. LouC. TouramanisDouglas WrightS. EmeryO. GrünbergM. V. PurohitF. FortiG. MarchioriJ. AlbertT. S. MattisonB. T. MeadowsSw. BanerjeeG. RavenR. FacciniF. FerrarottoA. J. LankfordM. BombenM. D. SokoloffS. LuitzP. R. BurchatC. HastD. J. LangeR. CenciG. PireddaW. Panduro VazquezF. Le DiberderB. BhuyanRoger BarlowMartino MargoniR. C. FieldB. G. FulsomGabriele SimiR. GorodeiskyG. FinocchiaroV. LuthA. ZalloT. J. GershonC. L. DavisD. W. G. S. LeithD. A. RobertsM. S. AlamI. M. PeruzziF. F. WilsonA. CalcaterraB. G. PushpawelaA. HafnerF. BianchiB. OberhofE. M. T. PuccioS. PrellS. DittrichM. K. SullivanK. Yu. TodyshevM. FritschP. OngmongkolkulJames H CochranV. PoireauM. HeßD. B. MacfarlaneEleonora LuppiA. LusianiV. P. DruzhininZ. C. HuardJ. DorfanE. A. KravchenkoS. BettariniGeorge LaffertyN. ArnaudCrisostomo SciaccaD. AstonG. A. CowanE. GraugesD. BettoniF. AnulliMario GiorgiP. TarasAlessandro GazC. H. ChengC. HeartyS. H. RobertsonI. GarziaR. De SangroS. L. WuC. PatrignaniV. TisserandColin JessopD. J. SummersHerbert KochR. PrepostT. E. LathamL. M. CremaldiM. CarpinelliK. GriessingerL. VitaleF. Martinez-vidalDominik MüllerD. G. HitlinH. AhmedJ. ChauveauW. GradlL. LanceriJ. Va’vraV. B. GolubevG. VasseurK. T. FloodA. PalanoD. GambaPeter S. KimN. GuttmanP. PatteriA. M. LutzW. J. WisniewskiS. PassaggioN. TasneemJ. M. RoneyAidan Randle-condeV. E. BlinovJ. G. SmithB. EchenardD. BernardG. RizzoM. RamaC. CartaroJ. P. LeesM. VerderiF. Di LodovicoJ. OcarizR. GodangU. MallikN. NeriC. H. ChenS. M. SpanierV. SantoroJ. J. WalshD. N. BrownF. De MoriJames R. WilsonK. R. SchubertH. A. NealG. CalderiniG. EigenA. R. BuzykaevA. BeaulieuTim AdyeR. D. KassRoberto CalabreseMaurizio BiasiniJ. W. GaryOwen Rosser LongR. CheaibE. P. SolodovT. S. MiyashitaJ. A. ErnstA. P. OnuchinL. SunJ. M. LoseccoAdrian John BevanB. DeyR. KowalewskiM. EbertG. J. KingA. M. RossiM. BellisJoseph IzenJ. P. ColemanStephen SekulaC. BozziK. HonscheidR. StroiliM. PosoccoA. FilippiR. CowanA. RoodmanE. FioravantiRoland WaldiF. FerroniPaul Fraser HarrisonStephen Robert WagnerS. MartellottiI. M. NugentD. S. ChaoM. DavierAbner Soffer

subject

PhysicsParticle physicsMeson010308 nuclear & particles physicsElectron–positron annihilationResonanceCharge (physics)7. Clean energy01 natural sciencesNuclear physicsAmplitudePion0103 physical sciencesD mesonHigh Energy Physics::ExperimentProduction (computer science)010306 general physics

description

We measure the $D^0 - {\bar{D}}^0$ mixing parameters using a time-dependent amplitude analysis of the decay $D^0\to\pi^+\pi^-\pi^0$. The data were recorded with the BABAR detector at center-of-mass energies at and near the $\Upsilon(4S)$ resonance, and correspond to an integrated luminosity of approximately 468.1 ${\rm fb}^{-1}$. The neutral $D$ meson candidates are selected from $D^{*}(2010)^+\to D^0 \pi_s^+$ decays where the flavor at the production is identified by the charge of the low momentum pion, $\pi_s^+$. The measured mixing parameters are $x = (1.5\pm1.2\pm0.6) \%$ and $y = (0.2\pm0.9\pm0.5) \%$, where the quoted uncertainties are statistical and systematic, respectively.

https://doi.org/10.1103/physrevd.93.112014