Abstract:We compare the predictions of a range of existing models based on the Vector Meson Dominance hypothesis with data on e + e − → π + π − and e + e − → µ + µ − 1 Permanent address. 2 Present address.cross-sections and the phase and near-threshold behavior of the timelike pion form factor, with the aim of determining which (if any) of these models is capable of providing an accurate representation of the full range of experimental data. We find that, of the models considered, only that proposed by Bando et al. is … Show more
“…Using NSK data or any of both KLOE samples, instead of the PDG information, does not lead to predicted curves substantially different from their analogue already shown and commented upon in the previous subsection. Interesting parameter values have been extracted from global fits using only the (0.75-0.82) GeV region from the NSK and KLOE spectra for e + e − → π + π − and are reported in Table 1; they are in reasonable agreement with the reported branching ratio product F ω [29] and the Orsay phase [70,71] as well. Indeed, taking the RPP F ω value as reference, our estimates using the 70 MeV in- terval surrounding the interference region are at 0.1σ , 1.8σ and 3.0σ for respectively the NSK [27,29], KLOE08 [31] and KLOE10 [32] data samples.…”
Section: Predictions Using Thesupporting
confidence: 58%
“…The probabilities are those of the global fit; the last data column shows the contribution of each π + π − data set to the total χ 2 Using the RPP recommended value for Br(ω → π + π − ) and the Orsay phase information from [70] yields a value for F ω in good correspondence with expectations, as clear from the entry τ + PDG in Table 1. Using NSK data or any of both KLOE samples, instead of the PDG information, does not lead to predicted curves substantially different from their analogue already shown and commented upon in the previous subsection.…”
Section: Predictions Using Thementioning
confidence: 65%
“…For the missing phase information we adopt the result from the fit [70] for the Orsay phase of the ω → π + π − amplitude and the result from SND [72] for the phase of the φ → π + π − amplitude. 25 Following the discussion in the preceding sub- 24 By abusively, we mean, first that the "Orsay" phases for both the ω and φ mesons have no entry in the RPP and, second, that the benchmark represented by the processes listed in Sect.…”
Section: τ + Pdg Predictionsmentioning
confidence: 99%
“…(1.53 ± 0.13) % [24] and the Orsay phase from [70] as input values for the "τ + PDG" fit. The probabilities are those of the global fit; the last data column shows the contribution of each π + π − data set to the total χ 2 Using the RPP recommended value for Br(ω → π + π − ) and the Orsay phase information from [70] yields a value for F ω in good correspondence with expectations, as clear from the entry τ + PDG in Table 1.…”
A global fit of parameters allows us to pin down the Hidden Local Symmetry (HLS) effective Lagrangian, which we apply for the prediction of the leading hadronic vacuum polarization contribution to the muon g − 2. The latter is dominated by the annihilation channel e + e − → π + π − , for which data are available by scan (CMD-2 & SND) and ISR (KLOE-2008, KLOE-2010 experiments. It is well known that the different data sets are not in satisfactory agreement. In fact it is possible to fix the model parameters without using the π + π − data, by using instead the dipion spectra measured in the τ -decays together with experimental spectra for the π 0 γ , ηγ , π + π − π 0 , K + K − , K 0 K 0 final states, supplemented by specific meson decay properties. Among these, the accepted decay width for ρ 0 → e + e − and the partial widths and phase information for the ω/φ → π + π − transitions, are considered. It is then shown that, relying on this global data set, the HLS model, appropriately broken, allows to predict accurately the pion form factor below 1.05 GeV. It is shown that the data samples provided by CMD-2, SND and KLOE-2010 behave consistently with each other and with the other considered data. Consistency problems with the KLOE-2008 and BaBar data samples are substantiated. "All data" global fits are investigated by applying reweighting the conflicting data sets. Constraining to our best fit, the broken HLS model yields a th μ = (11 659 169.55 + +1.26 −0.59 φ + +0.00 −2.00 τ ± 5.21 th ) 10 −10 associated with a very good global fit probability. Correspondingly, we find that a μ = a exp μ − a th μ exhibits a significance ranging between 4.7 and 4.9σ .
“…Using NSK data or any of both KLOE samples, instead of the PDG information, does not lead to predicted curves substantially different from their analogue already shown and commented upon in the previous subsection. Interesting parameter values have been extracted from global fits using only the (0.75-0.82) GeV region from the NSK and KLOE spectra for e + e − → π + π − and are reported in Table 1; they are in reasonable agreement with the reported branching ratio product F ω [29] and the Orsay phase [70,71] as well. Indeed, taking the RPP F ω value as reference, our estimates using the 70 MeV in- terval surrounding the interference region are at 0.1σ , 1.8σ and 3.0σ for respectively the NSK [27,29], KLOE08 [31] and KLOE10 [32] data samples.…”
Section: Predictions Using Thesupporting
confidence: 58%
“…The probabilities are those of the global fit; the last data column shows the contribution of each π + π − data set to the total χ 2 Using the RPP recommended value for Br(ω → π + π − ) and the Orsay phase information from [70] yields a value for F ω in good correspondence with expectations, as clear from the entry τ + PDG in Table 1. Using NSK data or any of both KLOE samples, instead of the PDG information, does not lead to predicted curves substantially different from their analogue already shown and commented upon in the previous subsection.…”
Section: Predictions Using Thementioning
confidence: 65%
“…For the missing phase information we adopt the result from the fit [70] for the Orsay phase of the ω → π + π − amplitude and the result from SND [72] for the phase of the φ → π + π − amplitude. 25 Following the discussion in the preceding sub- 24 By abusively, we mean, first that the "Orsay" phases for both the ω and φ mesons have no entry in the RPP and, second, that the benchmark represented by the processes listed in Sect.…”
Section: τ + Pdg Predictionsmentioning
confidence: 99%
“…(1.53 ± 0.13) % [24] and the Orsay phase from [70] as input values for the "τ + PDG" fit. The probabilities are those of the global fit; the last data column shows the contribution of each π + π − data set to the total χ 2 Using the RPP recommended value for Br(ω → π + π − ) and the Orsay phase information from [70] yields a value for F ω in good correspondence with expectations, as clear from the entry τ + PDG in Table 1.…”
A global fit of parameters allows us to pin down the Hidden Local Symmetry (HLS) effective Lagrangian, which we apply for the prediction of the leading hadronic vacuum polarization contribution to the muon g − 2. The latter is dominated by the annihilation channel e + e − → π + π − , for which data are available by scan (CMD-2 & SND) and ISR (KLOE-2008, KLOE-2010 experiments. It is well known that the different data sets are not in satisfactory agreement. In fact it is possible to fix the model parameters without using the π + π − data, by using instead the dipion spectra measured in the τ -decays together with experimental spectra for the π 0 γ , ηγ , π + π − π 0 , K + K − , K 0 K 0 final states, supplemented by specific meson decay properties. Among these, the accepted decay width for ρ 0 → e + e − and the partial widths and phase information for the ω/φ → π + π − transitions, are considered. It is then shown that, relying on this global data set, the HLS model, appropriately broken, allows to predict accurately the pion form factor below 1.05 GeV. It is shown that the data samples provided by CMD-2, SND and KLOE-2010 behave consistently with each other and with the other considered data. Consistency problems with the KLOE-2008 and BaBar data samples are substantiated. "All data" global fits are investigated by applying reweighting the conflicting data sets. Constraining to our best fit, the broken HLS model yields a th μ = (11 659 169.55 + +1.26 −0.59 φ + +0.00 −2.00 τ ± 5.21 th ) 10 −10 associated with a very good global fit probability. Correspondingly, we find that a μ = a exp μ − a th μ exhibits a significance ranging between 4.7 and 4.9σ .
“…Recently, it has been remarked [16] that the Hidden Local Symmetry (HLS) Model [17] provides another consistent framework for data analysis and a new expression for F π (s) at low energies. Indeed, besides the usual vector meson exchanges, this model predicts that some departure from standard VMD could show up as a residual direct coupling γπ + π − .…”
We analyze a pion form factor formulation which fulfills the Analyticity requirement within the Hidden Local Symmetry (HLS) Model. This implies an s-dependent dressing of the ρ − γ VMD coupling and an account of several coupled channels. The corresponding function F π (s) provides nice fits of the pion form factor data from s = −0.25 to s = 1 GeV 2 . It is shown that the coupling to KK has little effect, while ωπ 0 improves significantly the fit probability below the φ mass. No need for additional states like ρ(1450) shows up in this invariant-mass range. All parameters, except for the subtraction polynomial coefficients, are fixed from the rest of the HLS phenomenology. The fits show consistency with the expected behaviour of F π (s) at s = 0 up to O(s 2 ) and with the phase shift data on δ 1 1 (s) from threshold to somewhat above the φ mass. The ω sector is also examined in relation with recent data from CMD-2.
We examine the mechanisms producing departures from ideal mixing for vector mesons within the context of the Hidden Local Symmetry (HLS) model. We show that kaon loop transitions between the ideal combinations of the ω and φ mesons necessitate a field transformation in order to get the mass eigenstates. It is shown that this transformation is close to a rotation for processes involving, like meson decays, on-shell ω and φ mesons. The HLS model predicts a momentum dependent, slowly varying mixing angle between the ideal states. We examine numerically the consequences of this for radiative and leptonic decays of light mesons. The mean ω − φ mixing angle is found smaller than its ideal value; this is exhibited separately in radiative and in leptonic decays. Effects of nonet symmetry breaking in the vector sector are compared to those produced by the field rotation implied by the HLS model. * Supported by the US Department of Energy under contract DE-AC03-76SF00515The Hidden Local Symmetry (HLS) Model in both its non-anomalous [2] and anomalous (FKTUY) sectors [3] is a powerful tool for analyzing experimental data, by providing a clear framework with the fewest possible number of free parameters. For instance, it allows a 3-parameter description of the I = 1 pion form factor; this gives a statistically optimal description in an energy interval running from threshold to the φ mass. This has been shown by Ref. [4] in analyzing the world data set for e + e − → π + π − annihilation collected in Ref. [5]. The exercise has been repeated as successfully with the data set recently collected by the CMD-2 Collaboration on the VEPP-2M collider at Novosibirsk [6].However, in order to go beyond while staying within the framework defined by the HLS model and its anomalous sector, one needs to define a consistent scheme of symmetry breakings. Without SU(3) breaking, the HLS model cannot successfully describe the kaon form factors; without nonet symmetry breaking in the pseudoscalar (PS) sector, it cannot be used reliably to describe radiative decays of light mesons. The BKY mechanism [7,8] is a consistent way to introduce SU(3) breaking in both the vector (V) and PS sectors. It has been shown recently [9] that the BKY SU(3) breaking in the PS sector is in perfect agreement with all accessible predictions of Chiral Perturbation Theory [10-12] at first order in the breaking parameters. In order to reach this conclusion, the needed ingredients were only the BKY breaking in the PS sector (referred to hereafter as X A breaking), the kinetic energy term of the non-anomalous HLS Lagrangian and the P γγ Lagrangian of Wess, Zumino and Witten [13]. Thus, this part is on secure grounds.When dealing with PS mesons, the question of nonet symmetry breaking (NSB) cannot be avoided, as clear from Refs. [14,15] for instance. It was already introduced in the physics of single photon radiative decays (12 modes) by O'Donnell long ago [16], relying basically only on group theoretical considerations, but outside the context of effective Lagrangians. Th...
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