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A. E. Asratyan

Publications and source records attributed to A. E. Asratyan.

11 recordsLinked to original sources

Search for formation of isospin-3/2 $Ξ$ states by neutrinos

A narrow peak near 1870 MeV is observed in the combined invariant-mass spectrum of the systems $ΛK^0_S π^-$, $ΛK^0_S π^+$, $ΛK^- π^-$, and $ΛK^- π^+$ formed in $ν_μ$- and $\bar{ν_μ}$-induced charged-current collisions with free protons, deuterons, and Neon nuclei. Observed width of the resonance is consistent with being entirely due to apparatus smearing. A possible interpretation of the peak is formation and three-body $ΛK π$ decay of an exotic baryon with $I = 3/2$ and $S = -2$.

hep-ex↗

Search for $Θ^+(1540)$ emission in hadron--nucleus collisions at 400--700 GeV

The data on hadron--nucleus collisions at 400--700 GeV, collected by the SELEX experiment at Fermilab, are analyzed for formation of the exotic pentaquark baryon $Θ^+(1540)$. A narrow enhancement near 1539 MeV is observed in the mass spectrum of the $pK^0_S$ system emitted at small $x_F$ from hadron collisions with copper nuclei. The statistical significance of the peak is near 9 standard deviations. Fitted width of the observed $pK^0_S$ resonance is consistent with being entirely due to experimental resolution, and its intrinsic width is restricted to $Γ< 3$ MeV at 90\% CL. The data favor positive rather than negative strangeness for the $pK^0_S$ resonance observed in $h$Cu collisions. At the same time, the $pK^0_S$ mass spectrum for collisions in carbon is featureless. The yield of $Θ^+$ baryons per $h$C collision is restricted to be $< 24$\% of the yield per $h$Cu collision.

hep-ex↗

Angular distribution in s-channel formation of the pentaquark $Θ^+$ baryon

Using the DIANA data on the charge-exchange reaction $K^+n \rightarrow pK^0$ on a bound neutron, in which the s-channel formation of the pentaquark baryon $Θ^+(1538)$ has been observed, we analyze the dependence of the background-subtracted $Θ^+ \rightarrow pK^0$ signal on the $K^0$ emission angle in the $pK^0$ rest frame. In order to describe the observed $\cosΘ_K^\mathrm{cms}$ distribution, invoking the interference between the nonresonant s-wave and the $Θ^+$-mediated higher-wave contributions to the amplitude of the charge-exchange reaction is required at a 2.8$σ$ level. The spin--parity assignment of 1/2$^-$ for the $Θ^+$ baryon is ruled out at a statistical level of 2.9 standard deviations. A physically-meaningful selection in $\cosΘ_K^\mathrm{cms}$ based on the observed angular dependence of the $Θ^+ \rightarrow pK^0$ signal allows to boost the statistical significance of the signal up to 7.1 standard deviations. This is far in excess of previously reported signals and renders the $Θ^+$ existence more credible.

hep-ex↗

Observation of a narrow baryon resonance with positive strangeness formed in $K^+$Xe collisions

The charge-exchange reaction K^+ Xe --> K^0 p Xe' is investigated using the data of the DIANA experiment. The distribution of the pK^0 effective mass shows a prominent enhancement near 1538 MeV formed by \sim 80 events above the background, whose width is consistent with being entirely due to the experimental resolution. Under the selections based on a simulation of K^+Xe collisions, the statistical significance of the signal reaches 5.5σ. We interpret this observation as strong evidence for formation of a pentaquark baryon with positive strangeness, Θ^+(uudd\bar{s}), in the charge-exchange reaction K^+ n --> K^0 p on a bound neutron. The mass of the Θ^+ baryon is measured as m(Θ^+) = 1538+-2 MeV. Using the ratio between the numbers of resonant and non-resonant charge-exchange events in the peak region, the intrinsic width of this baryon resonance is determined as Γ(Θ^+) = 0.34+-0.10 MeV.

nucl-ex↗

Experimental search for radiative decays of the pentaquark baryon Θ^+(1540)

The data on the reactions K^+Xe --> K^0 γX and K^+Xe --> K^+ γX, obtained with the bubble chamber DIANA, have been analyzed for possible radiative decays of the Θ^+(1540) baryon: Θ^+ --> K^0 p γand Θ^+ --> K^+ n γ. No signals have been observed, and we derive the upper limits Γ(Θ^+ --> K^0 p γ) / Γ(Θ^+ --> K^0 p) < 0.032 and Γ(Θ^+ --> K^+ n γ) / Γ(Θ^+ --> K^+ n) < 0.041 which, using our previous measurement of Γ(Θ^+ --> KN) = (0.39+-0.10) MeV, translate to Γ(Θ^+ --> K^0 p γ) < 8 keV and Γ(Θ^+ --> K^+ n γ) < 11 keV at 90% confidence level. We have also measured the cross sections of K^+ -induced reactions involving emission of a neutral pion: σ(K^+n --> K^0 p π^0) = (68+-18) \mub and σ(K^+N --> K^+ N π^0) = (30+-8) \mub for incident K^+ momentum of 640 MeV.

hep-ex↗

Formation of a narrow baryon resonance with positive strangeness in K^+ collisions with Xe nuclei

The data on the charge-exchange reaction K^+Xe --> K^0 p Xe, obtained with the bubble chamber DIANA, are reanalyzed using increased statistics and updated selections. Our previous evidence for formation of a narrow pK^0 resonance with mass near 1538 MeV is confirmed and reinforced. The statistical significance of the signal reaches some 8σ(6σ) when estimated as S/\sqrt{B} (S/\sqrt{B+S}). The mass and intrinsic width of the Θ^+ baryon are measured as m = (1538+-2) MeV and Γ= (0.39+-0.10) MeV.

hep-ex↗

Further evidence for formation of a narrow baryon resonance with positive strangeness in K+ collisions with Xe nuclei

We have continued our investigation of the charge-exchange reaction K^+ Xe --> K^0 p Xe' in the bubble chamber DIANA. In agreement with our previous results based on part of the present statistics, formation of a narrow p K^0 resonance with mass of 1537+-2 MeV/c^2 is observed in the elementary transition K^+ n --> K^0 p on a neutron bound in the Xenon nucleus. Visible width of the peak is consistent with being entirely due to instrumental resolution and allows to place an upper limit on its intrinsic width: Γ< 9 MeV/c^2. A more precise estimate of the resonance intrinsic width, Γ= 0.36+-0.11 MeV/c^2, is obtained from the ratio between the numbers of resonant and non-resonant charge-exchange events. The signal is observed in a restricted interval of incident K^+ momentum, that is consistent with smearing of a narrow p K^0 resonance by Fermi motion of the target neutron. Statistical significance of the signal is some 7.3, 5.3, and 4.3 standard deviations for the estimators S/sqrt{B}, S/sqrt{S+B}, and S/sqrt{S+2B}, respectively. This observation confirms and reinforces our earlier results, and offers strong evidence for formation of a pentaquark baryon with positive strangeness in the charge-exchange reaction K^+ n --> K^0 p on a bound neutron.

hep-ex↗

Evidence for formation of a narrow pKshort resonance with mass near 1533 MeV in neutrino interactions

A narrow baryon resonance is observed in invariant mass of the pKshort system formed in neutrino and antineutrino collisions with nuclei. The mass of the resonance is estimated as (1533+-5)MeV. The observed width is less than 20 MeV, and is compatible with being entirely due to experimental resolution. The statistical significance of the signal is near 6.7 standard deviations. As the position of the observed resonance does not match the mass of any known Σ^{*+} state, we believe that it arises from neutrino production of the Θ^+ pentaquark baryon. The analysis is based on the data obtained in past neutrino experiments with big bubble chambers: WA21, WA25, WA59, E180 and E632.

hep-ex↗

A method for detecting $ν_τ$ appearance in the spectra of quasielastic CC events

A method for detecting the transition \omutau in long-baseline accelerator experiments, that consists in comparing the far-to-near ratios of the spectra of quasielastic CC events generated by high- and low-energy beams of muon neutrinos, is proposed. The test may be accessible to big water Cherenkov detectors and iron--scintillator calorimeters, and is limited by statistics rather than systematics.

hep-ex↗

Detecting tau-neutrino appearance in the spectra of quasielastic CC events

A method for detecting the transition numu->nutau in long-baseline accelerator experiments, that consists in comparing the far-to-near ratios of the spectra of quasielastic CC events generated by high- and low-energy beams of muon neutrinos, is proposed. The test may be accessible to big calorimeters with muon spectrometry like MINOS, and is limited by statistics rather than systematics.

hep-ex↗

Emulsion Chamber with Big Radiation Length for Detecting Neutrino Oscillations

A conceptual scheme of a hybrid-emulsion spectrometer for investigating various channels of neutrino oscillations is proposed. The design emphasizes detection of $τ$ leptons by detached vertices, reliable identification of electrons, and good spectrometry for all charged particles and photons. A distributed target is formed by layers of low-Z material, emulsion-plastic-emulsion sheets, and air gaps in which $τ$ decays are detected. The tracks of charged secondaries, including electrons, are momentum-analyzed by curvature in magnetic field using hits in successive thin layers of emulsion. The $τ$ leptons are efficiently detected in all major decay channels, including \xedec. Performance of a model spectrometer, that contains 3 tons of nuclear emulsion and 20 tons of passive material, is estimated for different experimental environments. When irradiated by the $ν_μ$ beam of a proton accelerator over a medium baseline of $ \sim 1$ km/GeV, the spectrometer will efficiently detect either the \omutau and \omue transitions in the mass-difference region of $Δm^2 \sim 1$ eV$^2$, as suggested by the results of LSND. When exposed to the neutrino beam of a muon storage ring over a long baseline of $ \sim$ 10-20 km/GeV, the model detector will efficiently probe the entire pattern of neutrino oscillations in the region $Δm^2 \sim 10^{-2}-10^{-3}$ eV$^2$, as suggested by the data on atmospheric neutrinos.

hep-ex↗