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The upgrades for the ATLAS Pixel Detector will be staged in preparation for high luminosity LHC.
The electronics required for implementing both the L0 trigger for high luminosity p p physics and the L1 trigger for high pT Pb+Pb physics has been studied.
Electron storage rings are widely used for high luminosity colliders, damping rings in high-energy linear colliders, and synchrotron light sources.
To cope with the elevated occupancy, the ATLAS experiment plans to introduce an all silicon inner tracker for High Luminosity LHC (HL-LHC) operation.
Future detectors for high luminosity particle identification and ultra high energy neutrino observation would benefit from a digitizer capable of recording sensor signals with high analog bandwidth and large record depth, in a cost-effective, compact and low-power way.
While GaInAs quantum well (QW) emission wavelength is practically limited to approximately 1200 nm [6], by using dilute nitride GaInNAs QWs with a tiny fraction of nitrogen added to the highly strained GaInAs, the emission wavelength can be extended to 1220-1240 nm for high luminosity red light generation at 610 to 620 nm by frequency conversion [5].
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While a simple rebuild of the current detector could be done, the expectation is to design a new one, optimized for higher luminosity.
Further, for higher luminosity operation of the accelerator, simulation result on the shield design for reducing the background rate is also reported.
Upgrade of the ATLAS tracker detector for high-luminosity LHC conditions requires novel approaches to the pixel sensor design.
For high-luminosity upgrades of the LHC, up to 10 times higher background rates are expected which require replacement of the muon chambers in the critical detector regions.
For low-luminosity systems (L ⩽ 0.2LEdd), there exists only the solution of hard spectra; while for high-luminosity systems (L ⩾ 0.8LEdd), there exist both solutions of hard and soft spectra.
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