4 September 2020 to 2 October 2020
Europe/Athens timezone
After the physical conference, an internet only session took place 1 and 2 October 2020. This program appears in the timetable as well.

Trigger at CMS

2 Oct 2020, 12:00
30m
Room 1

Room 1

Talk Plenary

Speaker

Mia Tosi (Università degli Studi di Padova & INFN)

Description

The CMS experiment uses a two-level triggering system consisting of the Level-1, instrumented by custom-design hardware boards and delivering an output rate of 100 kHz, and the High Level Trigger, a streamlined version of the offline reconstruction software running on a computer farm, which sends a rate of about 1 kHz to permanent storage. This system has been evolving continuously since the startup of the LHC. While the current system will basically remain in use for the next LHC running period (Run-3 starting in 2022), new features and algorithms are already being developed to take care of higher data loads due to increasing LHC luminosity and pileup but also of new experimental signatures to be investigated (in particular, displaced decay vertices stemming from relatively long-lived particles created in proton-proton collisions). Machine-learning techniques such as Boosted Decision Trees have already started to be implemented in the trigger electronics and will occupy a more important place in the future. %The use of High-Level Synthesis (HLS) tools will allow physicists to formulate trigger requirements in a language closer to that of data analysis. To avoid missing completely unexpected signatures from New Physics, studies are underway to employ anomaly detection using autoencoders.

A major upgrade of the triggering system will then happen within the framework of the upgrade of the collider to the `High-Luminosity LHC', which will deliver a luminosity of $5-7.5 \times 10^{34} $cm$^{-2}$s$^{-1}$, corresponding to 140--200 pileup events. An important difference from the present system will be the fact that after the upgrade, information from the silicon strip tracker will be available already for the Level-1 Trigger. This will allow CMS to use so-called ``particle flow'' objects, i.e. signals seen not only in one subdetector but put together from all available subdetectors, resulting in much sharper efficiency turn-on curves for trigger objects. Also, trigger rates will rise by a factor of about 7.5 both at Level-1 (to 750 kHz) and at the High-Level Trigger (7.5~kHz) and the latency - the processing time available for arriving at the Level-1 trigger decision - will increase significantly, allowing for the use of more sophisticated algorithms at Level-1.

Details

Mia Tosi, Universita' degli Studi di Padova and INFN

Is this abstract from experiment? Yes
Name of experiment and experimental site CMS
Is the speaker for that presentation defined? Yes
Internet talk Yes

Author

Mia Tosi (Università degli Studi di Padova & INFN)

Presentation materials