Abstract

We analyze the energy spectra of $single$ b-jets and B-hadrons resulting from the production and decay of top quarks within the SM at the LHC at the NLO QCD. For both hadrons and jets, we calculate the correlation of the peak of the spectrum with the top quark mass, considering the "energy-peak" as an observable to determine the top quark mass. Such a method is motivated by our previous work where we argued that this approach can have reduced sensitivity to the details of the production mechanism of the top quark, whether it is higher-order QCD effects or new physics contributions. As part of the NLO improvement over the original proposal, we assess the residual sensitivity of the extracted top quark mass to perturbative effects both in top quark production and decay. For a 1% jet energy scale uncertainty (and assuming negligible statistical error), the top quark mass can then be extracted using the energy-peak of b-jets with an error +- (1.2 (exp) + 0.6(th)) GeV. We note that recently the CMS collaboration reported a top quark mass measurement based on the original proposal (with b-jets) so that our result contributes to a precise evaluation of the associated theory uncertainty. In view of the dominant jet energy scale uncertainty in the measurement using b-jets, we also investigate the extraction of the top quark mass from the energy-peak of the corresponding B-hadrons which, in principle, can be measured without this uncertainty. The calculation of the B-hadron energy spectrum is carried out using fragmentation functions at NLO. The dependence on the fragmentation scale turns out to be the largest theoretical uncertainty in this extraction of top quark mass. Future improvement of the treatment of bottom quark hadronization can reduce this uncertainty, rendering methods based on the B-hadron energy-peak competitive for the top quark mass measurement.

Highlights

  • A complete knowledge of the top-Higgs sector is a key step for a full exploration of standard model (SM) physics and for testing models of new physics

  • In light of the above discussion, in this paper we systematically develop a new method for the precision determination of the top quark mass with higher-order corrections taken into account, based on the energy distribution of b-jets and Bhadrons resulting from its decay, which promises to add significant information to the combination of methods presently available

  • The upshot of the above argument is that measuring this energy peak can afford us the opportunity for a determination of the top quark mass which can be rather insensitive to uncertainties in top quark production, whether arising from higher-order QCD effects within the SM or any possible new physics contribution beyond it

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Summary

Introduction

A complete knowledge of the top-Higgs sector is a key step for a full exploration of SM physics and for testing models of new physics. The upshot of the above argument is that measuring this energy peak can (in principle) afford us the opportunity for a determination of the top quark mass which can be rather insensitive to uncertainties in top quark production, whether arising from higher-order (as yet non-calculated) QCD effects within the SM or any possible new physics contribution beyond it. Extending the above discussion to possible new physics contribution to production of top quark, we see that the sensitivity of the energy peak to such effects is suppressed, because in this case it is weighted by the above small factors (or by the polarization fraction and velocity of the top quarks, in the case they have a preferred polarization state) This should be contrasted with the methods that assume the SM matrix element from the very beginning, which might (in principle) face the full impact of.

Energy spectra and the top quark mass
Eb-tag
B-hadrons results
Findings
Conclusions
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