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Advantages of axially aligned crystals used in positron production at future linear colliders

X. Artru, R. Chehab, M. Chevallier, and V. Strakhovenko
Phys. Rev. ST Accel. Beams 6, 091003 – Published 22 September 2003

Abstract

The characteristics of the electron-photon showers initiated by 2 to 10 GeV electrons aligned along the 111 axis of tungsten crystals are compared with those for the amorphous tungsten. In this energy range, as known, the positron yield at the optimal target thicknesses is larger in a crystal case only by several percent. However, the amount of the energy deposition in a crystal turns out to be considerably (by 20%–50%) lower than in an amorphous target providing the same positron yield, while the peak energy-deposition density is approximately of the same magnitude in both cases.

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  • Received 1 July 2003

DOI:https://doi.org/10.1103/PhysRevSTAB.6.091003

This article is available under the terms of the Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.

Authors & Affiliations

X. Artru1, R. Chehab2, M. Chevallier1, and V. Strakhovenko3,*

  • 1IPN-Lyon, IN2P3/CNRS et University Claude Bernard, 69622 Villeurbanne, France
  • 2LAL, IN2P3/CNRS et University de Paris-Sud, BP 34-91898, Orsay cedex, France
  • 3Budker-INP, 11 Ac. Lavrentyeva, 630090, Novosibirsk, Russia

  • *Corresponding author. Email address: v.m.strakhovenko@inp.nsk.su

Article Text

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Vol. 6, Iss. 9 — September 2003

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Images

  • Figure 1
    Figure 1
    Mean energy of the initial electron in units of the incident beam energy, E0=10   GeV (a), and fractions of the total energy carried correspondingly by all charged particles and photons (b). Solid lines are for amorphous and dashed lines for crystal tungsten target. The incident beam is directed along the 111 axis of the crystal.Reuse & Permissions
  • Figure 2
    Figure 2
    Energy deposition rate per charged particle (a) and the logarithmic increment (b) in tungsten targets at E0=10GeV. Solid lines are for amorphous and dashed lines for crystal targets.Reuse & Permissions
  • Figure 3
    Figure 3
    Fraction of energy ΔEdep(z)/E0 deposited in z slices (a) and number of accepted positrons as a function of the deposited energy Edep/E0 (b) at E0=2GeV (curves 1), 6.2 GeV (curves 2), and 10 GeV (curves 3). Solid lines are for amorphous and dashed lines for crystal targets.Reuse & Permissions
  • Figure 4
    Figure 4
    (a) Mean positron energy (in MeV, upper curves) and transverse momentum (in MeV/c, lower curves); (b) beam spot area development. Incoming energies are E0=2GeV (curves 1), 6.2 GeV (curves 2), and 10 GeV (curves 3). S0 corresponds to the incident beam. The straight line y=1 on (b) is drawn to guide the eye. Solid lines are for amorphous and dashed lines for crystal targets.Reuse & Permissions
  • Figure 5
    Figure 5
    (a) Energy-deposition density in the internal cylinder, versus the depth, at indicated initial energies; (b) transverse distribution of the energy-deposition density at z=4.0X0. Solid lines are for amorphous and dashed lines for crystal targets.Reuse & Permissions
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