English

Status of Dual-readout R&D for a linear collider in T1015 Collaboration

Instrumentation and Detectors 2016-03-04 v1 High Energy Physics - Experiment

Abstract

The hadronic energy resolution required for an hadronic operating at lepton collider is at the limits or even exceeds that obtained with traditional techniques. Furthermore, it is a well established fact that the presence of an electromagnetic section in front of an hadron calorimeter, as occurs in the layouts of the majority of detectors operating at a collider, would deteriorate the hadronic energy resolution of the device. The novel ADRIANOADRIANO technology (\textit{A Dual-readout Integrally Active Non-segmented Option}), currently under development at Fermilab, overcomes the above limitations by complementing an integrally active calorimeter with the dual-readout technique. Detailed Monte Carlo studies indicate that the energy resolution is in the 25%/E25\%/\sqrt{E} - 38%/E38\%/\sqrt{E} interval with a linear response of the detector up to an energy of 200 GeV. A baseline configuration is chosen with an estimated energy resolution of σ(E)/E30%/E\sigma(E)/E\approx30\%/\sqrt{E}. Several prototypes have been built by \textit{T1015} Collaboration at Fermilab, to explore the effect of modifications of the layout from the baseline configuration. Preliminary results from several test beams at the \textit{Fermilab Test Beam Facility} (FTBF) of 1λI\sim1\lambda_{I} prototypes are presented. Future prospects with ultra-heavy glass are, also, summarized.

Keywords

Cite

@article{arxiv.1603.00909,
  title  = {Status of Dual-readout R&D for a linear collider in T1015 Collaboration},
  author = {Corrado Gatto and Vito Di Benedetto and Eileen Hahn and Anna Mazzacane},
  journal= {arXiv preprint arXiv:1603.00909},
  year   = {2016}
}

Comments

Talk presented at the International Workshop on Future Linear Colliders (LCWS15), Whistler, Canada, 2-6 November 2015. Calorimetry, Dual Readout, Total active calorimetry, ADRIANO project, T1015 Collaboration \PACS 29.40.Ka, 29.40.Mc, 29.40.Vj