A study of the $B^+\to K^0_SK^+K^-\pi^+$ and $B^+\to K^0_SK^+K^+\pi^-$ decays is performed using proton-proton collisions at center-of-mass energies of 7, 8 and 13 TeV at the LHCb experiment. The $K^0_SK \pi$ invariant mass spectra from both decay modes reveal a rich content of charmonium resonances. New precise measurements of the $\eta_c$ and $\eta_c(2S)$ resonance parameters are performed and branching fraction measurements are obtained for $B^+$ decays to $\eta_c$, $J/\psi$, $\eta_c(2S)$ and $\chi_{c1}$ resonances. In particular, the first observation and branching fraction measurement of $B^+ \to \chi_{c0} K^0 \pi^+$ is reported as well as first measurements of the $B^+\to K^0K^+K^-\pi^+$ and $B^+\to K^0K^+K^+\pi^-$ branching fractions. Dalitz plot analyses of $\eta_c \to K^0_SK\pi$ and $\eta_c(2S) \to K^0_SK\pi$ decays are performed. A new measurement of the amplitude and phase of the $K \pi$ $S$-wave as functions of the $K \pi$ mass is performed, together with measurements of the $K^*_0(1430)$, $K^*_0(1950)$ and $a_0(1700)$ parameters. Finally, the branching fractions of $\chi_{c1}$ decays to $K^*$ resonances are also measured.
Invariant $\pi ^+ \pi ^- $ mass distribution for (a) $ K ^0_{\mathrm{SLL}}$ and (b) $ K ^0_{\mathrm{SDD}}$ candidates. The full (red) line indicates the fit results and the dashed (blue) line the background contribution. The vertical dashed lines indicate the region used to select the $ K ^0_{\mathrm{S}}$ signal. |
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Distributions of $ K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ invariant mass for (a) $ K ^0_{\mathrm{SLL}}$ and (b) $ K ^0_{\mathrm{SDD}}$ candidates and distributions of $ K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ invariant mass for (c) $ K ^0_{\mathrm{SLL}}$ and (d) $ K ^0_{\mathrm{SDD}}$ candidates. The full (red) lines indicate the signal component and the dashed (blue) lines the background. The vertical dashed lines indicate the regions used to select the $ B ^+ $ signals. |
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Invariant $ K ^0_{\mathrm{S}} K\pi$ mass distributions for (a) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and (b) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ candidates (two entries per event). |
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Invariant $ K ^0_{\mathrm{S}} K\pi$ invariant mass distributions, with the known $ { J \mskip -3mu/\mskip -2mu\psi }$ mass subtracted, in the $\eta _ c $ -- $ { J \mskip -3mu/\mskip -2mu\psi }$ mass region for (a) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and (b) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ candidates. The results of the fits are overlayed. |
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Invariant $ K ^0_{\mathrm{S}} K\pi$ mass distributions in the $\chi _{ c 1}$ -- $\eta_c(2S)$ mass region for (a) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and (b) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ candidates. The results of the fits are overlayed. |
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Invariant $ K ^+ K ^- $ mass distribution in the $\chi _{ c 0}$ - $\chi _{ c 2}$ mass region for $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ decays. The two $ K ^0_{\mathrm{S}}$ datasets are combined. The results of the fit are overlayed. The curves also include interference terms and therefore the $\chi _{ c 0}$ lineshape takes slightly negative values. |
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Definition of the angles (a) $\theta_{\pi}$, (b) $\theta_{K_1}$ and (c) $\phi_K$. |
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Efficiency projections (in arbitrary units) on $m_x( K ^0_{\mathrm{S}} K_1)$ for the (a) $ K ^0_{\mathrm{SLL}}$ and (b) $ K ^0_{\mathrm{SDD}}$ samples for the total $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ dataset. The curves are the results of fits made using seventh-order polynomials. |
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Efficiency projections (in arbitrary units) on $m( K ^0_{\mathrm{S}} K_1 \pi)$ for the (a) $ K ^0_{\mathrm{SLL}}$ and (b) $ K ^0_{\mathrm{SDD}}$ simulation samples separated for trigger conditions. |
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Two-dimensional efficiency fitted distributions in the $\eta _ c $ mass region for the (a) $ K ^0_{\mathrm{SLL}}$ and (d) $ K ^0_{\mathrm{SDD}}$ samples. Efficiency projections (in arbitrary units) for (b)-(c) $ K ^0_{\mathrm{SLL}}$ and (e)-(f) $ K ^0_{\mathrm{SDD}}$ simulation. The curves are the results from the fits according to Eq. 14. |
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Efficiency projections (in arbitrary units) in the $\chi _{ c 1}$ -- $\eta_c(2S)$ mass region for the (a)-(b) $ K ^0_{\mathrm{SLL}}$ and (c)-(d) $ K ^0_{\mathrm{SDD}}$ simulation. The curves are the results from fits performed using seventh-order polynomials. |
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Invariant $ K ^0_{\mathrm{S}} K\pi$ mass distributions in the $\eta _ c $ -- $ { J \mskip -3mu/\mskip -2mu\psi }$ signal region combining the $ K ^0_{\mathrm{SLL}}$ and $ K ^0_{\mathrm{SDD}}$ data for (a) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and (b) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ decays. The dark-gray area represents the $ K ^0_{\mathrm{S}} K\pi$ invariant-mass spectrum from the $ B ^+ $ sideband; the light-gray areas indicate the $\eta _ c $ signal and sideband regions. |
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Dalitz plot of $\eta _ c \rightarrow K ^0_{\mathrm{S}} K\pi $ decays for (a) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and (b) $ K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ . The empty horizontal band in (b) is due to the removal of the $\overline{ D } {}^0 \rightarrow K ^+ \pi ^- $ channel. |
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Fit projections on the $ K ^- \pi ^+ $, $ K ^0_{\mathrm{S}} \pi ^+ $ and $ K ^0_{\mathrm{S}} K ^- $ invariant-mass distributions from the Dalitz-plot analysis of the $\eta _ c $ decay using the QMI model for $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ data. |
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Fit projections on the $ K ^+ \pi ^- $, $ K ^0_{\mathrm{S}} \pi ^- $ and $ K ^0_{\mathrm{S}} K ^+ $ invariant-mass distributions from the Dalitz-plot analysis of $\eta _ c $ decay using the QMI model for the $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ data. |
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Comparisons between the fitted $K \pi$ {\it S}-wave (a) amplitude and (b) phase obtained from the (black) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and (red) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ data. Note that the point at 1.425 $\text{ Ge V}$ is fixed at values 1.0 and 1.57 for amplitude and phase, respectively, and therefore there is no associated uncertainty. The plotted uncertainties are obtained averaging the uncertainties on the two adjacent mass measurements. |
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Argand diagram for the $K \pi$ {\it S}-wave averaged over the QMI results from $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ data. |
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Fit projections on the $ K ^- \pi ^+ $, $ K ^0_{\mathrm{S}} \pi ^+ $ and $ K ^0_{\mathrm{S}} K ^- $ invariant-mass distributions from the Dalitz-plot analysis of the $\eta _ c $ decay using the isobar model for the $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ data. Panels (a, c, e) show the most important resonant contributions. To simplify the plots, only resonant contributions relative to that mass projection are shown. Panels (b, d, f) show the interference terms for contributions greater than 3%. The legend in (a) also applies to (c) and the legend in (b) also applies to (d) and (f). |
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Fit to the (a) amplitude, (b) phase and (c) squared amplitude from the $\eta _ c $ QMI analysis using the results from the isobar-model analysis. The black points are obtained using the inverse-variance-weighted averages of the $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ data. The error bars are computed as the quadratic sum of the statistical and systematic uncertainties. The phase measurements in the $K \pi$ mass region below 0.90 $\text{ Ge V}$ are not included in the fit. |
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Invariant $ K ^0_{\mathrm{S}} K\pi$ mass distribution in the region of the $\eta_c(2S)$ resonance for $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ . The $\eta_c(2S)$ signal and sideband regions are indicated in light gray, while the incoherent background estimated from the $ B ^+ $ sidebands is shown in dark gray. |
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Dalitz plot of $\eta_c(2S) \rightarrow K ^0_{\mathrm{S}} K\pi $ decays for the $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ sample. |
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Dalitz-plot projections of the $\eta_c(2S) \rightarrow K ^0_{\mathrm{S}} K\pi $ decays from the $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ sample. The solid red line shows the fit result, the light gray shaded area is the contribution from the fitted sidebands and the dark shaded gray area is the contribution from the $ B ^+ $ sidebands. The empty region in the $ K ^0_{\mathrm{S}} K ^- $ invariant-mass projection is due to the removal of the contribution from $ D ^+_ s \rightarrow K ^0_{\mathrm{S}} K ^- $ decays. |
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Invariant $ K ^0_{\mathrm{S}} K\pi$ mass distribution in the region of the $\chi _{ c 1}$ / $\eta_c(2S)$ resonances for (a) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and (b) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ decays. In light gray are indicated the $\chi _{ c 1}$ signal region and sidebands. In dark gray is indicated the incoherent background estimated from the $ B ^+ $ sidebands. |
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Dalitz plot of $\chi _{ c 1} \rightarrow K ^0_{\mathrm{S}} K ^- \pi ^+ $ decays for the $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ sample. |
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Background-subtracted $K \pi$ and $ K ^0_{\mathrm{S}} \pi$ invariant-mass spectra from $\chi _{ c 1} \rightarrow K ^0_{\mathrm{S}} K\pi $ decays for the (a)-(b) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and (c)-(d) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ data. The results of the fits are overlaid. |
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Projected $ K ^- \pi ^+ $ invariant mass spectra weighted by Legendre polynomial moments $P_L(\cos\theta_{ K ^0_{\mathrm{S}} })$ for $\eta _ c \rightarrow K ^0_{\mathrm{S}} K ^- \pi ^+ $ from $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ data. The drawn curves result from the Dalitz plot fit using the QMI method described in the text. |
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Projected $ K ^0_{\mathrm{S}} \pi ^+ $ invariant mass spectra weighted by Legendre polynomial moments $P_L(\cos\theta_{ K ^- })$ for $\eta _ c \rightarrow K ^0_{\mathrm{S}} K ^- \pi ^+ $ from $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ data. The drawn curves result from the Dalitz plot fit using the QMI method described in the text. |
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Projected $ K ^0_{\mathrm{S}} K ^- $ invariant mass spectra weighted by Legendre polynomial moments $P_L(\cos\theta_{\pi ^+ })$ for $\eta _ c \rightarrow K ^0_{\mathrm{S}} K ^- \pi ^+ $ from $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ data. The drawn curves result from the Dalitz plot fit using the QMI method described in the text. |
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Fit projections on the (a) $ K ^+ \pi ^- $, (b) $ K ^0_{\mathrm{S}} \pi ^- $ and (c) $ K ^0_{\mathrm{S}} K ^+ $ invariant mass distributions from the Dalitz-plot analysis of the $\eta _ c $ decay using the isobar model for $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ data. The curves show the most important resonant contributions. To simplify the plots only resonant contributions relative to that mass projection are shown. The legend in (a) applies also to (b). |
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Animated gif made out of all figures. |
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Fitted $ B ^+ $ signal yield and purity for $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ final states separated by $ K ^0_{\mathrm{S}}$ type. |
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Fitted $\eta _ c $ , $ { J \mskip -3mu/\mskip -2mu\psi }$ , $\eta_c(2S)$ and $\chi _{ c 1}$ parameters. For the $ { J \mskip -3mu/\mskip -2mu\psi }$ the $m'=m-m_{ { J \mskip -3mu/\mskip -2mu\psi } }$ value is reported. The first uncertainty is statistical, the second systematic. |
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Summary of systematic uncertainties on $ { J \mskip -3mu/\mskip -2mu\psi }$ and $\eta _ c $ resonance parameters. |
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List of the systematic uncertainties on the $\chi _{ c 1}$ and $\eta_c(2S)$ parameters. |
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Candidate events and purities in the $\eta _ c $ signal region and fractions of $ B ^+ $ sideband contributions in the $\eta _ c $ sideband regions for $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ decays. Low and high indicate the lower and higher sideband candidates. Because of the limited statistics, the values of $f_B$ are summed for the $ K ^0_{\mathrm{SLL}}$ and $ K ^0_{\mathrm{SDD}}$ data. |
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Results from the Dalitz-plot analysis of the $\eta _ c $ decay in (top) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ , (center) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ and (bottom) inverse-variance-weighted averages. The QMI model is used for the $K \pi$ {\it S}-wave. |
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Fractional interference contributions from the Dalitz-plot analysis of the $\eta _ c $ decay in $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ decays using the QMI model. Absolute values less than 3% are not listed. |
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Systematic uncertainties on (left) fractional contributions (%) and (right) phases (rad) in the $\eta _ c $ Dalitz-plot analysis in the $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ decay using the QMI model for the $K \pi$ {\it S}-wave. |
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Systematic uncertainties on (left) fractional contributions (%) and (right) phases (rad) in the $\eta _ c $ Dalitz-plot analysis in the $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ decay using the QMI model for the $K \pi$ {\it S}-wave. |
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Fitted parameters and significances of the resonances observed in the $\eta _ c $ Dalitz-plot analysis. Significances larger than 10$\sigma$ are evaluated as $\sqrt{\Delta(2 \log \cal L )}$. |
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Results from the Dalitz-plot analysis of the $\eta _ c $ using the isobar model for (top) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ decays, $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ decays (center) and their inverse-variance-weighted averages (bottom). |
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Fractional interference contributions from the Dalitz-plot analysis of the $\eta _ c $ decay in $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ decays using the isobar model. Absolute values less than 3% are not listed. |
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Candidate events in the signal region, purities, and $ B ^+ $ background contributions to the $\eta_c(2S) \rightarrow K ^0_{\mathrm{S}} K\pi $ Dalitz-plot analysis separated for $ K ^0_{\mathrm{S}}$ types. The incoherent background fractions $f_B$ in the low and high sidebands refer to the sum of the $ K ^0_{\mathrm{SLL}}$ and $ K ^0_{\mathrm{SDD}}$ data. |
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Systematic uncertainties on (left) fractional contributions (%) and (right) phases in the $\eta_c(2S)$ Dalitz-plot analysis in $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ decay using the isobar model. |
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Results from the Dalitz-plot analysis of $\eta_c(2S) \rightarrow K ^0_{\mathrm{S}} K\pi $ in the $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ final state using the isobar model. |
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Fractional interference contributions from the Dalitz plot analysis of the $\eta_c(2S)$ decay in $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ decays using the isobar model. Absolute values less than 5% are not listed. |
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Candidate events and purities of $\chi _{ c 1}$ for the $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ final states separated for the $ K ^0_{\mathrm{SLL}}$ and $ K ^0_{\mathrm{SDD}}$ data. The incoherent background fractions $f_B$ values for the lower and higher sideband regions are computed for the sum of the $ K ^0_{\mathrm{SLL}}$ and $ K ^0_{\mathrm{SDD}}$ data. |
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Results from the fits to the $K \pi$ and $ K ^0_{\mathrm{S}} \pi$ background-subtracted invariant-mass distributions in the $\chi _{ c 1}$ decay for the (top) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and (bottom) $ K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ data. |
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Inverse-variance-weighted averages of the fractional contributions for $\chi _{ c 1}$ decays to $K^*\overline{ K } $ resonances from the $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ final states. The branching fractions of the $\chi _{ c 1} \rightarrow K ^0_{\mathrm{S}} K\pi $ decays to $K^{*}(892)$ and the $K^{*}_2(1430)$ resonances are also included. The reported uncertainties are statistical, systematic and from the uncertainty on the $\chi _{ c 1}$ branching fraction (see text) [3]. |
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Resulting yields and total charm fraction from the fits to the four-body, three-body and two-body invariant-mass spectra uncorrected for efficiency for the (top) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^- \pi ^+ $ and (bottom) $ B^+\rightarrow K ^0_{\mathrm{S}} K ^+ K ^+ \pi ^- $ data, separated by $ K ^0_{\mathrm{S}}$ category. The quoted uncertainties are statistical only. |
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Ratios of efficiency-corrected intermediate-resonance yields relative to the yield of the (top) $\eta _ c $ and (bottom) $ { J \mskip -3mu/\mskip -2mu\psi }$ resonances. The first uncertainty is statistical, the second systematic. |
Table_21.pdf [62 KiB] HiDef png [142 KiB] Thumbnail [73 KiB] tex code |
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Measured branching fractions with the $\eta _ c $ resonance as a reference using the (top) $ B^+\rightarrow K ^0 K ^+ K ^- \pi ^+ $ and (bottom) $ B^+\rightarrow K ^0 K ^+ K ^+ \pi ^- $ data. The first uncertainty is statistical, the second systematic and the third due to the PDG uncertainty on the $ B ^+ \rightarrow \eta _ c K ^+ $ branching fraction. |
Table_22.pdf [70 KiB] HiDef png [90 KiB] Thumbnail [45 KiB] tex code |
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Measured branching fractions with the $ { J \mskip -3mu/\mskip -2mu\psi }$ resonance as a reference using the (top) $ B^+\rightarrow K ^0 K ^+ K ^- \pi ^+ $ and (bottom) $ B^+\rightarrow K ^0 K ^+ K ^+ \pi ^- $ data. The first uncertainty is statistical, the second systematic, the third due to the PDG uncertainty on the $ B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi } K ^+ $ branching fraction. |
Table_23.pdf [69 KiB] HiDef png [84 KiB] Thumbnail [43 KiB] tex code |
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Measured branching fractions using (top) the $\eta _ c $ and (bottom) the $ { J \mskip -3mu/\mskip -2mu\psi }$ resonance as reference for $ B^+\rightarrow K ^0 K ^+ K ^- \pi ^+ $ data. The first uncertainty is statistical, the second systematic, the third due to the PDG uncertainty on the $ B ^+ \rightarrow \eta _ c K ^+ $ or $ B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi } K ^+ $ branching fraction. The PDG reports an upper limit $ B ^+ \rightarrow \chi _{ c 0} K^{*+}<0.21 \times 10^{-3}$. |
Table_24.pdf [68 KiB] HiDef png [57 KiB] Thumbnail [29 KiB] tex code |
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Inverse-variance averaged numerical values of the measured $K \pi$ {\it S}-wave as a function of the $K \pi$ mass. The first uncertainty is statistical, the second systematic. The values at $K \pi$ mass of 1.425 $\text{ Ge V}$ (in italics) are fixed. |
Table_25.pdf [54 KiB] HiDef png [420 KiB] Thumbnail [206 KiB] tex code |
Created on 27 April 2024.