Abstract
Jet production in relativistic heavy ion collisions is studied using Pb+Pb collisions at a center of mass energy of 2.76 TeV per nucleon.
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Notes
- 1.
The \(v_2\) was determined using cells at the electromagnetic scale. For jets using the GCW scheme, the \({E_\mathrm{T}^{\mathrm {raw}}}\) in Eq. 4.6 was first demodulated by the flow weight \(1+2v_{2\,i}\cos (2(\phi -\Psi _2))\), calibrated and then re-weighted by the same factor.
- 2.
It should be emphasized that this distribution is not trivially related to the efficiency shown in Fig. 4.7. One important difference is that the efficiency is shown as a function of \(p_\mathrm {T}\) of the truth jets. The survival fraction shown in Fig. 4.8 is evaluated as a function of reconstructed \(p_\mathrm {T}\), since the data is being used, which has the effects of upward feeding from finite resolution
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Angerami, A. (2014). Jet Reconstruction. In: Jet Quenching in Relativistic Heavy Ion Collisions at the LHC. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-01219-3_4
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DOI: https://doi.org/10.1007/978-3-319-01219-3_4
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