Notes
- 1.
As this work focuses on the proton collision data, the lead ion beams will not be discussed further.
- 2.
Apart from an initial, comparatively small 50 ns dataset.
- 3.
In addition there are smaller experiments, which will not be detailed here.
- 4.
The proton mass energy is negligible: \(\sim \)1 GeV, 10000 times smaller than the kinetic energy.
- 5.
“Coincide” is a simplification: in reality a small crossing angle gives the pp frame a non-zero transverse component in the lab frame.
- 6.
cross section, in units of barns, b, or cm\(^{-2}\): in some sense an area, a geometrical image of how likely it is to hit something. \(1 {\mathrm b} = 10^{-28} {\mathrm m}^2\).
- 7.
On average 20.7 in 2012 (50 ns bunch spacing), and 13.5 in 2015.
- 8.
Going from 40 MHz to 1 kHz means dismissing 99.9975% of the data.
- 9.
An elegant solution to this experimental trade-off is to read out a minimal amount of information from each event, which allows storing these at a higher rate. The challenge is ensuring that the reconstruction of these jets does not suffer from the loss of information from for instance the tracker. Far from being my idea, I still venture to say that with higher luminosities ahead of us, this type of “trigger-level” analysis and fast reconstruction of objects at trigger level is the way forward to retain sensitivity to phenomena in the sub-TeV scale, without requiring associated production of objects whose dedicated triggers have a lower prescale.
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Bryngemark, L.K. (2017). The Large Hadron Collider. In: Search for New Phenomena in Dijet Angular Distributions at √s = 8 and 13 TeV. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-67346-2_3
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