Measurement of the Z boson cross-section in - Harvard University ...
Measurement of the Z boson cross-section in - Harvard University ...
Measurement of the Z boson cross-section in - Harvard University ...
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Chapter 2: The Accelerator and <strong>the</strong> Experiment 63<br />
from <strong>the</strong> calorimeters, <strong>the</strong> L1 trigger looks for signatures that may <strong>in</strong>dicate physics <strong>of</strong><br />
<strong>in</strong>terest, such as high-energy electrons, photons, jets, τ leptons, large miss<strong>in</strong>g energy<br />
and/or total energy, and high-pT muons. Ano<strong>the</strong>r function <strong>of</strong> <strong>the</strong> L1 trigger is to<br />
def<strong>in</strong>e Regions <strong>of</strong> Interest (RoI’s), i.e. , regions <strong>of</strong> <strong>the</strong> detector <strong>in</strong> which <strong>in</strong>terest<strong>in</strong>g<br />
activity has been found. RoI’s are used for seed<strong>in</strong>g <strong>the</strong> Level-2 trigger. The L1 trigger<br />
takes about 2.5 µs to make an accept/reject decision, which is equivalent to 100 bunch<br />
<strong>cross</strong><strong>in</strong>gs at <strong>the</strong> 25 ns <strong>cross</strong><strong>in</strong>g <strong>in</strong>terval. This duration is known as <strong>the</strong> trigger latency.<br />
The maximum L1 accept rate which <strong>the</strong> readout systems can accommodate is 75 kHz,<br />
upgradeable to 100 kHz.<br />
The front-end readout electronics <strong>of</strong> each subdetector conta<strong>in</strong>s data buffers known<br />
as pipel<strong>in</strong>es. Pipel<strong>in</strong>es <strong>in</strong> <strong>the</strong> muon system and <strong>the</strong> calorimetry have enough depth<br />
to hold data for <strong>the</strong> L1 latency <strong>of</strong> 2.5 µs. Upon an L1 accept decision, data from <strong>the</strong><br />
relevant cells is transferred to Readout drivers (RODs).<br />
The Level-2 (L2) trigger looks only at <strong>the</strong> RoI’s def<strong>in</strong>ed by L1. It has access to<br />
full-granularity <strong>in</strong>formation from all subdetectors with<strong>in</strong> <strong>the</strong> RoI’s. The <strong>in</strong>formation,<br />
extracted from <strong>the</strong> relevant RODs, amounts to ≈ 2% <strong>of</strong> <strong>the</strong> total event data for a<br />
typical event [98]. The L2 trigger has a latency <strong>of</strong> about 40 ms, and decreases <strong>the</strong><br />
event rate to 3.5 kHz.<br />
Events selected by <strong>the</strong> L2 trigger are transferred to <strong>the</strong> event builder, which is <strong>the</strong><br />
first stage <strong>of</strong> <strong>the</strong> Level-3 (L3) trigger. The event builder uses elaborate algorithms to<br />
fully reconstruct events us<strong>in</strong>g <strong>in</strong>formation from <strong>the</strong> entire detector. The reconstructed<br />
events are <strong>the</strong>n moved to <strong>the</strong> Event Filter (EF), which performs <strong>the</strong> f<strong>in</strong>al selection<br />
<strong>of</strong> events to be written to mass storage. The EF typically takes 4 seconds to process