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Oleksandra Deineka

Publications and source records attributed to Oleksandra Deineka.

9 recordsLinked to original sources

Coupled-channel Omnès matrix for the $D$-wave isoscalar $ππ/K\bar K$ system and its application to $J/ψ\toπ^{0}π^{0}γ,\,K_{S}K_{S}γ$

In this work, we construct the $D$-wave isoscalar $ππ/K\bar K$ coupled-channel Omnès matrix, formulated to satisfy unitarity, analyticity, and the appropriate asymptotic behavior. We employ a two-channel $K$-matrix model containing poles associated with the $f_{2}(1270)$ and $f_{2}'(1525)$ resonances. The resulting unitary scattering matrix, which reproduces the experimental $ππ\toππ$ and $ππ\to K\bar K$ data and PDG information, serves as input to the homogeneous two-channel Muskhelishvili-Omnès equation. We compare our Omnès matrix with previous constructions based on $ππ\to K\bar K$ phases extracted from sums of Breit-Wigner amplitudes. The Omnès matrix developed here provides a reliable dispersive input for form-factor calculations and resonance studies in the tensor-meson sector. As an application, we show that it enables a simultaneous and accurate description of the BESIII $J/ψ\toπ^{0}π^{0}γ$ and $J/ψ\to K_{S}K_{S}γ$ spectra in the $J=2$ electric-dipole (E1) partial wave.

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A dispersive estimate of the $a_0(980)$ contribution to $(g-2)_μ$

A dispersive implementation of the $a_0(980)$ resonance to $(g-2)_μ$ requires the knowledge of the double-virtual $S$-wave $γ^*γ^*\toπη/ K K(I=1)$ amplitudes. To obtain these amplitudes, we used a modified coupled-channel Muskhelishvili-Omnes formalism, with input from the left-hand cuts and the hadronic Omnes matrix. The latter was derived using a data-driven N/D method, where the hadronic left-hand cuts were approximated via a conformal expansion. Due to the absence of direct hadronic data in the $πη$ channel, the expansion coefficients were fitted to various experimental data sets on two-photon fusion processes with $πη$ and $K K$ final states. The resulting dispersive estimate for the $a_0(980)$ contribution to $(g-2)_μ$ is $a_μ^{HLbL}[a_0(980)]_{resc.}=-0.43(1)(2)\times 10^{-11}$, which presents an order of magnitude improvement in precision over the narrow resonance approximation.

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A dispersive estimate of the $a_0(980)$ contribution to hadronic light-by-light scattering in $(g-2)_μ$

A dispersive implementation of the $a_0(980)$ resonance to $(g-2)_μ$ requires the knowledge of the double-virtual $S$-wave $γ^*γ^*\toπη/ K\bar{K}_{I=1}$ amplitudes. To obtain these amplitudes we used a modified coupled-channel Muskhelischvili-Omnès formalism, with the input from the left-hand cuts and the hadronic Omnès function. The latter were obtained using a data-driven $N/D$ method in which the fits were performed to the different sets of experimental data on two-photon fusion processes with $πη$ and $K\bar{K}$ final states. This yields the preliminary dispersive estimate $a_μ^{HLbL}[a_0(980)]_{resc.}=-0.46(2)\times 10^{-11}$.

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Dispersive analysis of the $ππ$ and $πK$ scattering data

We present a data-driven analysis of the S-wave $ππ\to ππ\,(I=0,2)$ and $πK \to πK\,(I=1/2, 3/2)$ reactions using the partial-wave dispersion relation. The contributions from the left-hand cuts are parametrized using the expansion in a suitably constructed conformal variable, which accounts for its analytical structure. The partial-wave dispersion relation is solved numerically using the $N/D$ method. The fits to the experimental data supplemented with the constraints from chiral perturbation theory at threshold and Adler zero give the results consistent with Roy-like (Roy-Steiner) analyses. For the $ππ$ scattering we present the coupled-channel analysis by including additionally the $K\bar{K}$ channel. By the analytic continuation to the complex plane, we found poles associated with the lightest scalar resonances $σ/f_0(500)$, $f_0(980)$, and $κ/K_0^*(700)$. For all the channels we also performed the fits directly to the Roy-like (Roy-Steiner) solutions in the physical region, in order to minimize the $N/D$ uncertainties in the complex plane and to extract the most constrained Omnès functions.

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Dispersive analysis of the $γγ\to D \bar{D}$ data and the confirmation of the $D \bar{D}$ bound state

In this paper, we present a data-driven analysis of the $γγ\to D^+D^-$ and $γγ\to D^0\bar{D}^0$ reactions from threshold up to 4.0 GeV in the $D\bar{D}$ invariant mass. For the $S$-wave contribution, we adopt a partial-wave dispersive representation, which is solved using the $N/D$ ansatz. The left-hand cuts are accounted for using the model-independent conformal expansion. The $D$-wave $χ_{c2}(3930)$ state is described as a Breit-Wigner resonance. The resulting fits are consistent with the data on the invariant mass distribution of the $e^+e^- \to J/ψD\bar{D}$ process. Performing an analytic continuation to the complex $s$-plane, we find no evidence of a pole corresponding to the broad resonance $X(3860)$ reported by the Belle Collaboration. Instead, we find a clear bound state below the $D\bar{D}$ threshold at $\sqrt{s_B} = 3695(4)$ MeV, confirming the previous phenomenological and lattice predictions.

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Data-driven dispersive analysis of the $ππ$ and $πK$ scattering

We present a data-driven analysis of the resonant S-wave $ππ\to ππ$ and $πK \to πK$ reactions using the partial-wave dispersion relation. The contributions from the left-hand cuts are accounted for using the Taylor expansion in a suitably constructed conformal variable. The fits are performed to experimental and lattice data as well as Roy analyses. For the $ππ$ scattering we present both a single- and coupled-channel analysis by including additionally the $K\bar{K}$ channel. For the latter the central result is the Omnès matrix, which is consistent with the most recent Roy and Roy-Steiner results on $ππ\to ππ$ and $ππ\to K\bar{K}$, respectively. By the analytic continuation to the complex plane, we found poles associated with the lightest scalar resonances $σ/f_0(500)$, $f_0(980)$, and $κ/K_0^*(700)$ for the physical pion mass value and in the case of $σ/f_0(500)$, $κ/K_0^*(700)$ also for unphysical pion mass values.

hep-ph↗

Dispersive analysis of the $γ^{*}γ^{*} \to ππ$ process

In this paper, we present a dispersive analysis of the double-virtual photon-photon scattering to two pions up to 1.5 GeV. Through unitarity, this process is very sensitive to hadronic final state interaction. For the $s$-wave, we use a coupled-channel $ππ,\, K\bar{K}$ analysis which allows a simultaneous description of both $f_0(500)$ and $f_{0}(980)$ resonances. For higher energies, $f_2(1270)$ shows up as a dominant structure which we approximate by a single channel $ππ$ rescattering in the $d$-wave. In the dispersive approach, the latter requires taking into account $t$- and $u$-channel vector-meson exchange left-hand cuts which exhibit an anomalous-like behavior for large space-like virtualities. In our paper, we show how to readily incorporate such behavior using a contour deformation. Besides, we devote special attention to kinematic constraints of helicity amplitudes and show their correlations explicitly.

hep-ph↗

Theoretical analysis of the $γγ^{(*)} \to π^0η$ process

The theoretical analysis of the $γγ\to π^0η$ process is presented within the energy range up to 1.4 GeV. The $S$-wave resonance $a_0(980)$ is described involving the coupled channel dispersive framework and the $D$-wave $a_2(1320)$ is approximated as a Breit-Wigner resonance. For the $a_0(980)$ the pole is found on the IV Riemann sheet resulting in a two-photon decay width of $Γ_{a_0\toγγ}=0.27(4)$ keV. The first dispersive prediction is provided for the single-virtual $γγ^*(Q^2)\toπ^0η$ process in the spacelike region up to $Q^2=1$ GeV$^2$.

hep-ph↗

Theoretical analysis of the $γγ\to π^0 η$ process

We present a theoretical study of the $γγ\to πη$ process from the threshold up to 1.4 GeV in the $πη$ invariant mass. For the s-wave $a_0(980)$ resonance state we adopt a dispersive formalism using a coupled-channel Omnès representation, while the d-wave $a_2(1320)$ state is described as a Breit-Wigner resonance. An analytic continuation to the $a_0(980)$ pole position allows us to extract its two-photon decay width as $Γ_{a_0\toγγ}=0.27(4)$ keV.

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