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Charm Meson Spectra in e^+e^- Annihilation at 10.5 GeV c.m.e

M. Artuso

TL;DR

This work measures charm-hadron momentum spectra in non-resonant $e^+e^-$ annihilation at ${\sqrt{s}}\approx 10.5$ GeV with the CLEO II.V detector, focusing on $D^+$, $D^0$, $D^{*+}$, and $D^{*0}$ while excluding $B$-decay products. It uses multiple decay channels, mass-distribution fits, and two independent Monte Carlo samples to extract raw yields, correct for detection efficiency, and form $d\sigma/dx_p$ with robust systematic checks. The $D^0$ spectrum is used to tune JETSET fragmentation parameters, achieving reasonable reproduction of the $D^{*}$ spectra and offering constraints on nonperturbative charm fragmentation at this energy scale. The results provide high-precision, shape-focused fragmentation information that informs PQCD tests, evolution equations, and Monte Carlo modeling for heavy-flavor production in both $e^+e^-$ and hadron-hadron collisions.

Abstract

Using the CLEO detector at the Cornell Electron-positron Storage Ring, we have measured the scaled momentum spectra, dsigma/dx_p, and the inclusive production cross sections of the charm mesons D+, D0, D*+, and D*0 in e+e- annihilation at about 10.5 GeV center of mass energy, excluding the decay products of B mesons. The statistical accuracy and momentum resolution are superior to previous measurements at this energy.

Charm Meson Spectra in e^+e^- Annihilation at 10.5 GeV c.m.e

TL;DR

This work measures charm-hadron momentum spectra in non-resonant annihilation at GeV with the CLEO II.V detector, focusing on , , , and while excluding -decay products. It uses multiple decay channels, mass-distribution fits, and two independent Monte Carlo samples to extract raw yields, correct for detection efficiency, and form with robust systematic checks. The spectrum is used to tune JETSET fragmentation parameters, achieving reasonable reproduction of the spectra and offering constraints on nonperturbative charm fragmentation at this energy scale. The results provide high-precision, shape-focused fragmentation information that informs PQCD tests, evolution equations, and Monte Carlo modeling for heavy-flavor production in both and hadron-hadron collisions.

Abstract

Using the CLEO detector at the Cornell Electron-positron Storage Ring, we have measured the scaled momentum spectra, dsigma/dx_p, and the inclusive production cross sections of the charm mesons D+, D0, D*+, and D*0 in e+e- annihilation at about 10.5 GeV center of mass energy, excluding the decay products of B mesons. The statistical accuracy and momentum resolution are superior to previous measurements at this energy.

Paper Structure

This paper contains 40 sections, 4 equations, 25 figures, 12 tables.

Figures (25)

  • Figure 1: Resolution in $x_p$ for the $D^0$$\rightarrow$$K^-$$\pi^+$ channel. All momenta.
  • Figure 2: Examples of $M_{cand}$ distribution for two $D^{\star+}$ decay channels and one of the $D^{\star0}$ channels analyzed. (a) $D^{\star+}$$\rightarrow$($K^-$$\pi^+$)$\pi^+$. (b) $D^{\star+}$$\rightarrow$($K^-$$\pi^+$$\pi^+$$\pi^-$)$\pi^+$. (c) $D^{\star0}$$\rightarrow$($K^-$$\pi^+$$\pi^+$$\pi^-$)$\pi^0$. They show the $M_{cand}$ distribution for $Q$ in the $D^{\star+}$ signal region and for $Q$ in the $D^{\star+}$ side bands.
  • Figure 3: (a) Overlay of $D^0$ spectra (data) from double Gaussian and TAGMC shape signal fitting; (b) fractional difference of the two spectra.
  • Figure 4: Buildup of the background from its components to fit the $M(K^-{$K^-$}\pi^+{$π^+$})$ distribution. The solid histogram is data. Notice the offset on the yield axis.
  • Figure 5: Ratios of data spectrum after double Gaussian shape parameter smoothing to the one obtained without smoothing: (a) $D^+$$\rightarrow$$K^-$$\pi^+$$\pi^+$, (b) $D^0$$\rightarrow$$K^-$$\pi^+$, (c) $D^{\star+}$$\rightarrow$($K^-$$\pi^+$)$\pi^+$.
  • ...and 20 more figures