Search NASA⌕ Search

SEARCH · Search NASA

Results for “SCATTERPLOTS”

Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.

Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.

67 records · Page 4

The pp{yields}p{Lambda}K{sup +} and pp{yields}p{Sigma}{sup 0}K{sup +} reactions with chiral dynamics

We report on a theoretical study of the pp{yields}p{Lambda}K{sup +} and pp{yields}p{Sigma}{sup 0}K{sup +} reactions near threshold using a chiral dynamical approach. The production process is described by single-pion and single-kaon exchange. The final state interactions of nucleon-hyperon, K-hyperon, and K-nucleon systems are also taken into account. We show that our model leads to a fair description of the experimental data on the total cross section of the pp{yields}p{Lambda}K{sup +} and pp{yields}p{Sigma}{sup 0}K{sup +} reactions. We find that the experimental observed strong suppression of {Sigma}{sup 0} production compared to {Lambda} production at the same excess energy can be explained. However, ignorance of phases between some amplitudes does not allow one to properly account for the nucleon-hyperon final state interaction for the pp{yields}p{Sigma}{sup 0}K{sup +} reaction. We also demonstrate that the invariant mass distribution and the Dalitz plot provide direct information about the {Lambda} and {Sigma}{sup 0} production mechanisms and may be tested by experiments at COSY or HIRFL-CSR.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Charm mixing in a model-independent analysis of correlated D{sup 0}D{sup 0} decays

We investigate the impact of charm mixing on a model-independent {gamma} measurement using the Dalitz plot analysis of the three-body D decay from the B{sup +}{yields}DK{sup +} process, and show that ignoring the mixing at all stages of the analysis is safe up to a sub-degree level of precision. We also find that in the coherent production of the D{sup 0}D{sup *0} system in e{sup +}e{sup -} collisions, the effect of charm mixing is enhanced, and propose a model-independent method to measure charm mixing parameters in time-integrated Dalitz plot analysis at charm factories.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Measurement of CP violating asymmetries in B{sup 0{yields}}K{sup +}K{sup -}K{sub S}{sup 0} decays with a time-dependent Dalitz approach

We report a measurement of CP violating asymmetries in B{sup 0}(B{sup 0}){yields}K{sup +}K{sup -}K{sub S}{sup 0} decays with a time-dependent Dalitz approach. This analysis is based on a data sample of 657x10{sup 6} BB pairs accumulated at the {Upsilon}(4S) resonance with the Belle detector at the KEKB asymmetric-energy e{sup +}e{sup -} collider. As the result of an unbinned maximum likelihood fit to the selected candidates, the mixing-induced and direct CP violation parameters {phi}{sub 1}{sup eff} and A{sub CP} are obtained for B{sup 0{yields}{phi}}(1020)K{sub S}{sup 0}, B{sup 0{yields}}f{sub 0}(980)K{sub S}{sup 0}, and other B{sup 0{yields}}K{sup +}K{sup -}K{sub S}{sup 0} decays. We find four solutions that describe the data. There are {phi}{sub 1}{sup eff}(B{sup 0{yields}{phi}}(1020)K{sub S}{sup 0})=(32.2{+-}9.0{+-}2.6{+-}1.4) deg.; {phi}{sub 1}{sup eff}(B{sup 0{yields}{phi}}(1020)K{sub S}{sup 0})=(26.2{+-}8.8{+-}2.7{+-}1.2) deg.; {phi}{sub 1}{sup eff}(B{sup 0{yields}{phi}}(1020)K{sub S}{sup 0})=(27.3{+-}8.6{+-}2.8{+-}1.3) deg.; and {phi}{sub 1}{sup eff}(B{sup 0{yields}{phi}}(1020)K{sub S}{sup 0})=(24.3{+-}8.0{+-}2.9{+-}5.2) deg. The values for the CP violating phase in B{sup 0{yields}{phi}}(1020)K{sub S}{sup 0} are similar, but other properties of the Dalitz plot are quite different for the four solutions. These four solutions have consistent {phi}{sub 1}{sup eff} values for all three B-meson decay channels and none of them deviates significantly from the values measured in B{yields}(cc)K{sup 0} decays with the currently available statistics. In addition, we find no significant direct CP violation.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Relative phases in Dalitz plot amplitudes for D{sup 0{yields}}K{sub S{pi}}{sup +{pi}-} and D{sup 0{yields}{pi}0}K{sup +}K{sup -}

Relative phases of amplitudes for D meson decays to a light pseudoscalar meson P and a light vector meson V decaying to two pseudoscalar mesons will lead to characteristic interferences on the three-body Dalitz plot. These phases may be compared with predictions of a flavor-symmetric treatment which extracts contributing amplitudes and their relative phases from a fit to D{yields}PV decay rates. Good agreement was found previously for the cases of B{sup 0{yields}}K{sup +{pi}-{pi}0} and D{sup 0{yields}{pi}+{pi}-{pi}0}. The present work is devoted to the decays D{sup 0{yields}}K{sub S{pi}}{sup +{pi}-} and D{sup 0{yields}{pi}0}K{sup +}K{sup -}, for which agreement is not found. Several suggestions are offered for this discrepancy.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Role of P-wave inelasticity in J/{psi}{yields}{pi}{sup +}{pi}{sup -}{pi}{sup 0}

We discuss the importance of inelasticity in the P-wave {pi}{pi} amplitude on the Dalitz distribution of 3{pi} events in J/{psi} decay. The inelasticity, which becomes sizable for {pi}{pi} masses above 1.4 GeV, is attributed to KK{yields}{pi}{pi} rescattering. We construct an analytical model for the two-channel scattering amplitude and use it to solve the dispersion relation for the isobar amplitudes that parametrize the J/{psi} decay. We present comparisons between theoretical predictions for the Dalitz distribution of 3{pi} events with available experimental data.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Dalitz Analysis of Ds -> K K- pi-

We perform a Dalitz plot analysis of about 100,000 D{sub s}{sup +} decays to K{sup +}K{sup -}{pi}{sup +} and measure the complex amplitudes of the intermediate resonances which contribute to this decay mode. We also measure the relative branching fractions of D{sub s}{sup +} {yields} K{sup +}K{sup +}{pi}{sup -} and D{sub s}{sup +} {yields} K{sup +}K{sup +}K{sup -}. For this analysis we use a 384 fb{sup -1} data sample, recorded by the BABAR detector at the PEP-II asymmetric-energy e{sup +}e{sup -} collider running at center-of-mass energies near 10.58 GeV.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Radiative corrections to the Dalitz plot of K{sub l3}{sup {+-}} decays

We calculate the model-independent radiative corrections to the Dalitz plot of K{sub l3}{sup {+-}} decays to the order of ({alpha}/{pi})(q/M{sub 1}), where q is the momentum transfer and M{sub 1} is the mass of the kaon. The final results are presented, first, with the triple integration over the variables of the bremsstrahlung photon ready to be performed numerically and, second, in an analytical form. These two forms are useful to cross-check on one another and with other calculations. This paper is organized to make it accessible and reliable in the analysis of the Dalitz plot of precision experiments and is not compromised to fixing the form factors at predetermined values. It is assumed that the real photons are kinematically discriminated. Otherwise, our results have a general model-independent applicability.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Discrete contribution to {psi}{sup '}{yields}J/{psi}+{gamma}{gamma}

The decay mode {psi}(2S){yields}J/{psi}+{gamma}{gamma} is proposed in order to experimentally identify the effects of the coupling of charmonium states to the continuum D{bar D} states. To have a better understanding of such a two-photon decay process, in this work we restrict ourselves to investigate the contribution of the discrete part, in which the photons are mainly produced via the intermediate states {chi}{sub cJ}(nP). Besides calculating the resonance contributions of {chi}{sub cJ}(1P)(J=0,1,2), we also take into account the contributions of the higher excited states {chi}{sub cJ}(2P) and the interference effect among the 1P and 2P states. We find that the contribution of the 2P states and the interference terms to the total decay width is very tiny. However, for specific regions of the Dalitz plot, off the resonance peaks, we find that these contributions are sizable and should also be accounted for. We also provide the photon spectrum and study the polarization of J/{psi}.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Determining the photon polarization of the b{yields}s{gamma} using the B{yields}K{sub 1}(1270){gamma}{yields}(K{pi}{pi}){gamma} decay

Recently the radiative B decay to the strange axial-vector mesons, B{yields}K{sub 1}(1270){gamma}, has been observed with a rather large branching ratio. This process is particularly interesting as the subsequent K{sub 1} decay into its three-body final state allows us to determine the polarization of the photon, which is mostly left- (right-)handed for B(B) in the SM while various new physics models predict additional right- (left-)handed components. A new method is proposed to determine the polarization, exploiting the full Dalitz plot distribution, which seems to reduce significantly the statistical errors. This polarization measurement requires, however, detailed knowledge of the K{sub 1{yields}}K{pi}{pi} strong interaction decays, namely, the various partial wave amplitudes into the several possible quasi-two-body channels, as well as their relative phases. The pattern of partial waves is especially complex for the K{sub 1}(1270). We attempt to obtain the information through the combination of an experimental input and a theoretical one, provided by the {sup 3}P{sub 0} quark-pair-creation model.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Analysis of the decay D{sup 0}{yields}K{sub S}{sup 0}{pi}{sup 0}{pi}{sup 0}

We present the results of a Dalitz plot analysis of D{sup 0}{yields}K{sub S}{sup 0}{pi}{sup 0}{pi}{sup 0} using the CLEO-c data set of 818 pb{sup -1} of e{sup +}e{sup -} collisions accumulated at {radical}(s)=3.77 GeV. This corresponds to 3x10{sup 6} D{sup 0}D{sup 0} pairs from which we select 1259 tagged candidates with a background of 7.5{+-}0.9 percent. Several models have been explored, all of which include the K{sup *}(892), K{sub 2}{sup *}(1430), K{sup *}(1680), the f{sub 0}(980), and the {sigma}(500). We find that the combined {pi}{sup 0{pi}0} S-wave contribution to our preferred fit is (28.9{+-}6.3{+-}3.1)% of the total decay rate while D{sup 0}{yields}K{sup *}(892){sup 0}{pi}{sup 0} contributes (65.6{+-}5.3{+-}2.5)%. Using three tag modes and correcting for quantum correlations we measure the D{sup 0}{yields}K{sub S}{sup 0}{pi}{sup 0}{pi}{sup 0} branching fraction to be (1.058{+-}0.038{+-}0.073)%.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Measurement of D{sup 0}-D{sup 0} Mixing Parameters Using D{sup 0}{yields}K{sub S}{sup 0}{pi}{sup +}{pi}{sup -} and D{sup 0}{yields}K{sub S}{sup 0}K{sup +}K{sup -} Decays

We report a direct measurement of D{sup 0}-D{sup 0} mixing parameters through a time-dependent amplitude analysis of the Dalitz plots of D{sup 0}{yields}K{sub S}{sup 0}{pi}{sup +}{pi}{sup -} and, for the first time, D{sup 0}{yields}K{sub S}{sup 0}K{sup +}K{sup -} decays. The low-momentum pion {pi}{sub s}{sup +} in the decay D{sup *+{yields}}D{sup 0{pi}}{sub s}{sup +} identifies the flavor of the neutral D meson at its production. Using 468.5 fb{sup -1} of e{sup +}e{sup -} colliding-beam data recorded near {radical}(s)=10.6 GeV by the BABAR detector at the PEP-II asymmetric-energy collider at SLAC, we measure the mixing parameters x=[1.6{+-}2.3(stat){+-}1.2(syst){+-}0.8(model)]x10{sup -3}, and y=[5.7{+-}2.0(stat){+-}1.3(syst){+-}0.7(model)]x10{sup -3}. These results provide the best measurement to date of x and y. The knowledge of the value of x, in particular, is crucial for understanding the origin of mixing.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Evidence for Direct CP Violation in the Measurement of the Cabbibo-Kobayashi-Maskawa Angle {gamma} with B{sup {+-}}{yields}D(*)K{sup (*){+-}} Decays

We report the measurement of the Cabibbo-Kobayashi-Maskawa CP-violating angle {gamma} through a Dalitz plot analysis of neutral D-meson decays to K{sub S}{sup 0}{pi}{sup +}{pi}{sup -} and K{sub S}{sup 0}K{sup +}K{sup -} produced in the processes B{sup {+-}}{yields}DK{sup {+-}}, B{sup {+-}}{yields}D*K{sup {+-}} with D*{yields}D{pi}{sup 0}, D{gamma}, and B{sup {+-}}{yields}DK*{sup {+-}} with K*{sup {+-}}{yields}K{sub S}{sup 0}{pi}{+-}, using 468 million BB pairs collected by the BABAR detector at the PEP-II asymmetric-energy e{sup +}e{sup -} collider at SLAC. We measure {gamma}=(68{+-}14{+-}4{+-}3) deg. (modulo 180 deg.), where the first error is statistical, the second is the experimental systematic uncertainty, and the third reflects the uncertainty in the description of the neutral D decay amplitudes. This result is inconsistent with {gamma}=0 (no direct CP violation) with a significance of 3.5 standard deviations.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Scalar mesons in the decays {eta}' {sup {yields}}3{pi}{sup 0} and {eta}' {sup {yields} {pi}0{pi}+{pi}-}

The decays {eta} {sup {yields}}3{pi}{sup 0} and {eta} {sup {yields} {pi}0{pi}+{pi}-} are considered within the isobar model. It is shown that, in order to explain the branching ratio and the shape of the Dalitz plot for the decay {eta}' {sup {yields}}3{pi}{sup 0}, it is sufficient to take into account the contributions of the {sigma} and a{sub 0} mesons. The inclusion of the {sigma} meson is necessary for reproducing the shape of the distribution over the Dalitz plot. The branching ratio for the decay {eta}' {sup {yields} {pi}0{pi}+{pi}-} is obtained. The predictions for the distributions over the Dalitz plot for this decay are presented. These predictions depend strongly on model parameters.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗