First model-independent Dalitz analysis of B0→DK∗0B^0 \to DK^{*0}, D→KS0π+π−D\to K_S^0π^+π^- decay

preprint2016arXivOpen access
Belle CollaborationK. NegishiA. IshikawaH. YamamotoA. AbdesselamI. AdachiH. AiharaS. Al SaidD. M. AsnerV. AulchenkoT. AushevR. AyadV. BabuI. BadhreesS. BahinipatiA. M. BakichE. BarberioJ. BiswalG. BonviciniA. BozekM. BračkoT. E. BrowderV. ChekelianA. ChenB. G. CheonK. ChilikinR. ChistovK. ChoV. ChobanovaS. -K. ChoiY. ChoiD. CinabroJ. DalsenoM. DanilovZ. DoležalA. DrutskoyD. DuttaS. EidelmanH. FarhatJ. E. FastT. FerberB. G. FulsomV. GaurN. GabyshevA. GarmashD. GetzkowR. GillardR. GlattauerY. M. GohP. GoldenzweigB. GolobO. GrzymkowskaJ. HabaT. HaraK. HayasakaH. HayashiiX. H. HeT. HoriguchiW. -S. HouT. IijimaK. InamiR. ItohY. IwasakiI. JaegleD. JoffeK. K. JooT. JuliusK. H. KangT. KawasakiC. KieslingD. Y. KimJ. B. KimJ. H. KimK. T. KimM. J. KimS. H. KimY. J. KimK. KinoshitaB. R. KoP. KodyšS. KorparP. KrižanP. KrokovnyT. KumitaA. KuzminY. -J. KwonJ. S. LangeI. S. LeeP. LewisY. LiL. Li GioiJ. LibbyD. LiventsevP. LukinM. MasudaD. MatvienkoK. MiyabayashiH. MiyataR. MizukG. B. MohantyA. MollH. K. MoonR. MussaM. NakaoT. NanutZ. NatkaniecM. NayakN. K. NisarS. NishidaS. OgawaS. OkunoY. OnukiP. PakhlovG. PakhlovaB. PalC. W. ParkH. ParkT. K. PedlarL. PesántezR. PestotnikM. PetričL. E. PiilonenC. PulvermacherE. RibežlM. RitterA. RostomyanY. SakaiS. SandilyaL. SanteljT. SanukiY. SatoV. SavinovO. SchneiderG. SchnellC. SchwandaK. SenyoM. E. SeviorV. ShebalinC. P. ShenT. -A. ShibataJ. -G. ShiuF. SimonY. -S. SohnE. SolovievaS. StaničM. StaričM. StederM. SumihamaT. SumiyoshiU. TamponiY. TeramotoM. UchidaY. UnnoS. UnoP. UrquijoC. Van HulseP. VanhoeferG. VarnerA. VinokurovaA. VossenM. N. WagnerC. H. WangM. -Z. WangP. WangX. L. WangM. WatanabeY. WatanabeS. WehleK. M. WilliamsE. WonJ. YamaokaY. YamashitaS. YashchenkoJ. YeltonY. YookC. Z. YuanY. YusaZ. P. ZhangV. ZhilichV. ZhulanovA. Zupanc

Abstract

We report a measurement of the amplitude ratio rSr_S of B0→D0K∗0B^0 \to D^0K^{*0} and B0→D0ˉK∗0B^0 \to \bar{D^0}K^{*0} decays with a Dalitz analysis of D→KS0π+π−D\to K_S^0π^+π^- decays, for the first time using a model-independent method. We set an upper limit rS<0.87r_S < 0.87 at the 68\% confidence level, using the full data sample of 772×106772\times10^6 BBˉB\bar{B} pairs collected at the Υ(4S)Υ(4S) resonance with the Belle detector at the KEKB e+e−e^+e^- collider. This result is obtained from observables x−=+0.4−0.6−0.1+1.0+0.0±0.0x_- = +0.4 ^{+1.0 +0.0}_{-0.6 -0.1} \pm0.0, y−=−0.6−1.0−0.0+0.8+0.1±0.1y_- = -0.6 ^{+0.8 +0.1}_{-1.0 -0.0} \pm0.1, x+=+0.1−0.4−0.1+0.7+0.0±0.1x_+ = +0.1 ^{+0.7 +0.0}_{-0.4 -0.1} \pm0.1 and y+=+0.3−0.8−0.1+0.5+0.0±0.1y_+ = +0.3 ^{+0.5 +0.0}_{-0.8 -0.1} \pm0.1, where x±=rScos⁡(δS±ϕ3)x_\pm = r_S \cos(δ_S \pm ϕ_3), y±=rSsin⁡(δS±ϕ3)y_\pm = r_S \sin(δ_S \pm ϕ_3) and ϕ3 (δS)ϕ_3~(δ_S) is the weak (strong) phase difference between B0→D0K∗0B^0 \to D^0K^{*0} and B0→D0ˉK∗0B^0 \to \bar{D^0}K^{*0}.

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