text:
@online{anti_k,
	title = {[0802.1189] The anti-k\_t jet clustering algorithm},
	url = {https://arxiv.org/abs/0802.1189},
	urldate = {2020-05-25},
	file = {[0802.1189] The anti-k_t jet clustering algorithm:/home/akako/Zotero/storage/M6Q768NZ/0802.html:text/html}
}

@article{geant4,
	title = {Geant4—a simulation toolkit},
	volume = {506},
	issn = {0168-9002},
	url = {http://www.sciencedirect.com/science/article/pii/S0168900203013688},
	doi = {10.1016/S0168-9002(03)01368-8},
	abstract = {Geant4 is a toolkit for simulating the passage of particles through matter. It includes a complete range of functionality including tracking, geometry, physics models and hits. The physics processes offered cover a comprehensive range, including electromagnetic, hadronic and optical processes, a large set of long-lived particles, materials and elements, over a wide energy range starting, in some cases, from 250eV and extending in others to the {TeV} energy range. It has been designed and constructed to expose the physics models utilised, to handle complex geometries, and to enable its easy adaptation for optimal use in different sets of applications. The toolkit is the result of a worldwide collaboration of physicists and software engineers. It has been created exploiting software engineering and object-oriented technology and implemented in the C++ programming language. It has been used in applications in particle physics, nuclear physics, accelerator design, space engineering and medical physics.},
	pages = {250--303},
	number = {3},
	journaltitle = {Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment},
	shortjournal = {Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment},
	author = {{Geant4 Collaboration}},
	urldate = {2020-05-25},
	date = {2003-07-01},
	langid = {english},
	keywords = {Distributed software development, Geometrical modelling, Object-oriented technology, Particle interactions, Simulation, Software engineering},
	file = {ScienceDirect Snapshot:/home/akako/Zotero/storage/SMWK56RH/S0168900203013688.html:text/html;Full Text:/home/akako/Zotero/storage/5KXJ2K4U/Agostinelli et al. - 2003 - Geant4—a simulation toolkit.pdf:application/pdf}
}

@article{deepflavour,
	title = {Identification of heavy-flavour jets with the {CMS} detector in pp collisions at 13 {TeV}},
	volume = {13},
	issn = {1748-0221},
	url = {http://arxiv.org/abs/1712.07158},
	doi = {10.1088/1748-0221/13/05/P05011},
	abstract = {Many measurements and searches for physics beyond the standard model at the {LHC} rely on the efficient identification of heavy-flavour jets, i.e. jets originating from bottom or charm quarks. In this paper, the discriminating variables and the algorithms used for heavy-flavour jet identification during the first years of operation of the {CMS} experiment in proton-proton collisions at a centre-of-mass energy of 13 {TeV}, are presented. Heavy-flavour jet identification algorithms have been improved compared to those used previously at centre-of-mass energies of 7 and 8 {TeV}. For jets with transverse momenta in the range expected in simulated \${\textbackslash}mathrm\{t\}{\textbackslash}overline\{{\textbackslash}mathrm\{t\}\}\$ events, these new developments result in an efficiency of 68\% for the correct identification of a b jet for a probability of 1\% of misidentifying a light-flavour jet. The improvement in relative efficiency at this misidentification probability is about 15\%, compared to previous {CMS} algorithms. In addition, for the first time algorithms have been developed to identify jets containing two b hadrons in Lorentz-boosted event topologies, as well as to tag c jets. The large data sample recorded in 2016 at a centre-of-mass energy of 13 {TeV} has also allowed the development of new methods to measure the efficiency and misidentification probability of heavy-flavour jet identification algorithms. The heavy-flavour jet identification efficiency is measured with a precision of a few per cent at moderate jet transverse momenta (between 30 and 300 {GeV}) and about 5\% at the highest jet transverse momenta (between 500 and 1000 {GeV}).},
	pages = {P05011--P05011},
	number = {5},
	journaltitle = {Journal of Instrumentation},
	shortjournal = {J. Inst.},
	author = {{CMS Collaboration}},
	urldate = {2020-05-25},
	date = {2018-05-08},
	eprinttype = {arxiv},
	eprint = {1712.07158},
	keywords = {High Energy Physics - Experiment, Physics - Instrumentation and Detectors},
	file = {arXiv Fulltext PDF:/home/akako/Zotero/storage/XWDYFNGF/CMS Collaboration - 2018 - Identification of heavy-flavour jets with the CMS .pdf:application/pdf;arXiv.org Snapshot:/home/akako/Zotero/storage/BAVNLRN3/1712.html:text/html}
}

@article{run1_offshell,
	title = {Constraints on the Higgs boson width from off-shell production and decay to Z-boson pairs},
	volume = {736},
	issn = {03702693},
	url = {http://arxiv.org/abs/1405.3455},
	doi = {10.1016/j.physletb.2014.06.077},
	abstract = {Constraints are presented on the total width of the recently discovered Higgs boson, Gamma[H], using its relative on-shell and off-shell production and decay rates to a pair of Z bosons, where one Z boson decays to an electron or muon pair, and the other to an electron, muon, or neutrino pair. The analysis is based on the data collected by the {CMS} experiment at the {LHC} in 2011 and 2012, corresponding to integrated luminosities of 5.1 inverse femtobarns at a centre-of-mass energy sqrt(s) = 7 {TeV} and 19.7 inverse femtobarns at sqrt(s) = 8 {TeV}. A simultaneous maximum likelihood fit to the measured kinematic distributions near the resonance peak and above the Z-boson pair production threshold leads to an upper limit on the Higgs boson width of Gamma[H] {\textless} 22 {MeV} at a 95\% confidence level, which is 5.4 times the expected value in the standard model at the measured mass.},
	pages = {64--85},
	journaltitle = {Physics Letters B},
	shortjournal = {Physics Letters B},
	author = {{CMS Collaboration}},
	urldate = {2020-05-25},
	date = {2014-09},
	eprinttype = {arxiv},
	eprint = {1405.3455},
	keywords = {High Energy Physics - Experiment},
	file = {arXiv Fulltext PDF:/home/akako/Zotero/storage/7DRDN62S/CMS Collaboration - 2014 - Constraints on the Higgs boson width from off-shel.pdf:application/pdf;arXiv.org Snapshot:/home/akako/Zotero/storage/DXDC85XB/1405.html:text/html}
}

@article{powhegv2,
	title = {{W+W-, WZ} and {ZZ} production in the {POWHEG}-{BOX}-V2},
	volume = {74},
	issn = {1434-6052},
	url = {https://doi.org/10.1140/epjc/s10052-013-2702-5},
	doi = {10.1140/epjc/s10052-013-2702-5},
	abstract = {We present an implementation of the vector boson pair production processes \$\${ZZ}\$\${ZZ}, \$\$W{\textasciicircum}+W{\textasciicircum}-\$\$W+W-and \$\${WZ}\$\${WZwithin} the {POWHEG}-{BOX}-V2. This implementation, derived from the {POWHEG} {BOX} version, has several improvements over the old one, among which the inclusion of all decay modes of the vector bosons, the possibility to generate different decay modes in the same run, speed optimization and phase space improvements in the handling of interference and singly resonant contributions.},
	pages = {2702},
	number = {1},
	journaltitle = {The European Physical Journal C},
	shortjournal = {Eur. Phys. J. C},
	author = {Nason, Paolo and Zanderighi, Giulia},
	urldate = {2020-05-25},
	date = {2014-01-23},
	langid = {english},
	file = {Springer Full Text PDF:/home/akako/Zotero/storage/C7DMJPHS/Nason and Zanderighi - 2014 - \$\$W^+W^-\$\$W+W-, \$\$WZ\$\$WZand \$\$ZZ\$\$ZZproduction in .pdf:application/pdf}
}

@article{cms_higgs,
	title = {Measurement of the properties of a Higgs boson in the four-lepton final state},
	volume = {89},
	issn = {1550-7998, 1550-2368},
	url = {http://arxiv.org/abs/1312.5353},
	doi = {10.1103/PhysRevD.89.092007},
	abstract = {The properties of a Higgs boson candidate are measured in the H to {ZZ} to 4l decay channel, with l = e, mu, using data from pp collisions corresponding to an integrated luminosity of 5.1 inverse femtobarns at the center-of-mass energy of sqrt(s) = 7 {TeV} and 19.7 inverse femtobarns at sqrt(s) = 8 {TeV}, recorded with the {CMS} detector at the {LHC}. The new boson is observed as a narrow resonance with a local significance of 6.8 standard deviations, a measured mass of 125.6 +- 0.4 (stat) +- 0.2 (syst) {GeV}, and a total width less than 3.4 {GeV} at the 95\% confidence level. The production cross section of the new boson times its branching fraction to four leptons is measured to be 0.93 +0.26 -0.23 (stat) +0.13 -0.09 (syst) times that predicted by the standard model. Its spin-parity properties are found to be consistent with the expectations for the standard model Higgs boson. The hypotheses of a pseudoscalar and all tested spin-one boson hypotheses are excluded at the 99\% confidence level or higher. All tested spin-two boson hypotheses are excluded at the 95\% confidence level or higher.},
	pages = {092007},
	number = {9},
	journaltitle = {Physical Review D},
	shortjournal = {Phys. Rev. D},
	author = {{CMS} Collaboration},
	urldate = {2020-05-25},
	date = {2014-05-14},
	eprinttype = {arxiv},
	eprint = {1312.5353},
	keywords = {High Energy Physics - Experiment},
	file = {arXiv Fulltext PDF:/home/akako/Zotero/storage/24NM2C36/CMS Collaboration - 2014 - Measurement of the properties of a Higgs boson in .pdf:application/pdf;arXiv.org Snapshot:/home/akako/Zotero/storage/DVLG7P3E/1312.html:text/html}
}

@article{jhugen,
	title = {New features in the {JHU} generator framework},
	url = {http://arxiv.org/abs/2002.09888},
	abstract = {We present an extension of the {JHUGen} and {MELA} framework, which includes an event generator and library for the matrix element analysis. It enables simulation, optimal discrimination, reweighting techniques, and analysis of a bosonic resonance and the triple and quartic gauge boson interactions with the most general anomalous couplings. The new features, which become especially relevant at the current stage of {LHC} data taking, are the simulation of gluon fusion and vector boson fusion in the off-shell region, associated \${ZH}\$ production at {NLO} {QCD} including the \$gg\$ initial state, and the simulation of a second spin-zero resonance. We also quote translations of the anomalous coupling measurements into constraints on dimension-six operators of an effective field theory. Some of the new features are illustrated with projections for experimental measurements with the full {LHC} and {HL}-{LHC} datasets.},
	journaltitle = {{arXiv}:2002.09888 [hep-ex, physics:hep-ph]},
	author = {Gritsan, Andrei V. and Roskes, Jeffrey and Sarica, Ulascan and Schulze, Markus and Xiao, Meng and Zhou, Yaofu},
	urldate = {2020-05-25},
	date = {2020-02-23},
	eprinttype = {arxiv},
	eprint = {2002.09888},
	keywords = {High Energy Physics - Experiment, High Energy Physics - Phenomenology},
	file = {arXiv Fulltext PDF:/home/akako/Zotero/storage/D9UDQRTG/Gritsan et al. - 2020 - New features in the JHU generator framework.pdf:application/pdf;arXiv.org Snapshot:/home/akako/Zotero/storage/K5DFQK7A/2002.html:text/html}
}

@article{nnpdf,
	title = {Parton distributions from high-precision collider data},
	url = {http://arxiv.org/abs/1706.00428},
	abstract = {We present a new set of parton distributions, {NNPDF}3.1, which updates {NNPDF}3.0, the first global set of {PDFs} determined using a methodology validated by a closure test. The update is motivated by recent progress in methodology and available data, and involves both. On the methodological side, we now parametrize and determine the charm {PDF} alongside the light quarks and gluon ones, thereby increasing from seven to eight the number of independent {PDFs}. On the data side, we now include the D0 electron and muon W asymmetries from the final Tevatron dataset, the complete {LHCb} measurements of W and Z production in the forward region at 7 and 8 {TeV}, and new {ATLAS} and {CMS} measurements of inclusive jet and electroweak boson production. We also include for the first time top-quark pair differential distributions and the transverse momentum of the Z bosons from {ATLAS} and {CMS}. We investigate the impact of parametrizing charm and provide evidence that the accuracy and stability of the {PDFs} are thereby improved. We study the impact of the new data by producing a variety of determinations based on reduced datasets. We find that both improvements have a significant impact on the {PDFs}, with some substantial reductions in uncertainties, but with the new {PDFs} generally in agreement with the previous set at the one sigma level. The most significant changes are seen in the light-quark flavor separation, and in increased precision in the determination of the gluon. We explore the implications of {NNPDF}3.1 for {LHC} phenomenology at Run {II}, compare with recent {LHC} measurements at 13 {TeV}, provide updated predictions for Higgs production cross-sections and discuss the strangeness and charm content of the proton in light of our improved dataset and methodology. The {NNPDF}3.1 {PDFs} are delivered for the first time both as Hessian sets, and as optimized Monte Carlo sets with a compressed number of replicas.},
	journaltitle = {{arXiv}:1706.00428 [hep-ex, physics:hep-ph]},
	author = {The {NNPDF} Collaboration and Ball, Richard D. and Bertone, Valerio and Carrazza, Stefano and Del Debbio, Luigi and Forte, Stefano and Groth-Merrild, Patrick and Guffanti, Alberto and Hartland, Nathan P. and Kassabov, Zahari and Latorre, José I. and Nocera, Emanuele R. and Rojo, Juan and Rottoli, Luca and Slade, Emma and Ubiali, Maria},
	urldate = {2020-06-08},
	date = {2017-09-22},
	eprinttype = {arxiv},
	eprint = {1706.00428},
	keywords = {High Energy Physics - Experiment, High Energy Physics - Phenomenology}
}

@article{solenoid_map,
	title = {Validation of the {CMS} Magnetic Field Map},
	volume = {28},
	issn = {1557-1939, 1557-1947},
	url = {http://arxiv.org/abs/1606.00382},
	doi = {10.1007/s10948-014-2809-4},
	abstract = {The Compact Muon Solenoid ({CMS}) is a general purpose detector, designed to run at the highest luminosity at the {CERN} Large Hadron Collider ({LHC}). Its distinctive features include a 4 T superconducting solenoid with 6-m-diameter by 12.5-m-length free bore, enclosed inside a 10,000-ton return yoke made of construction steel. The return yoke consists of five dodecagonal three-layered barrel wheels and four end-cap disks at each end comprised of steel blocks up to 620 mm thick, which serve as the absorber plates of the muon detection system. To measure the field in and around the steel, a system of 22 flux loops and 82 3-D Hall sensors is installed on the return yoke blocks. A {TOSCA} 3-D model of the {CMS} magnet is developed to describe the magnetic field everywhere outside the tracking volume measured with the field-mapping machine. The magnetic field description is compared with the measurements and discussed.},
	pages = {701--704},
	number = {2},
	journaltitle = {Journal of Superconductivity and Novel Magnetism},
	shortjournal = {J Supercond Nov Magn},
	author = {Klyukhin, V. I. and Amapane, N. and Ball, A. and Curé, B. and Gaddi, A. and Gerwig, H. and Mulders, M. and Calvelli, V. and Hervé, A. and Loveless, R.},
	urldate = {2020-06-01},
	date = {2015-02},
	eprinttype = {arxiv},
	eprint = {1606.00382},
	keywords = {Physics - Instrumentation and Detectors},
	file = {arXiv Fulltext PDF:/home/akako/Zotero/storage/WPCZDMJ6/Klyukhin et al. - 2015 - Validation of the CMS Magnetic Field Map.pdf:application/pdf;arXiv.org Snapshot:/home/akako/Zotero/storage/XL4DR6KR/1606.html:text/html}
}

@online{cms_slice,
	title = {{CMS} Detector Slice},
	url = {https://cds.cern.ch/record/2120661},
	abstract = {Slice showing {CMS} sub-detectors and how particles interact with them},
	titleaddon = {{CERN} Document Server},
	author = {Barney, David},
	urldate = {2020-06-01},
	date = {2016-01-12},
	langid = {english},
	note = {Library Catalog: cds.cern.ch
Number: {CMS}-{PHO}-{GEN}-2016-001},
	file = {Snapshot:/home/akako/Zotero/storage/BMBTW4YE/2120661.html:text/html}
}

@article{k_factor,
	title = {What is the Real K Factor?},
	abstract = {The theoretical K factor, describing the difference between the leading and higher order cross sections, has no precise deﬁnition. The deﬁnition is sensitive to the order of the ﬁt to the parton densities and the number of loops at which αs is evaluated. We describe alternate ways to deﬁne the K factor and show how the deﬁnition affects its magnitude and shape for examples of hadroproduction of W + bosons, Drell-Yan lepton pairs, and heavy quarks. We discuss which deﬁnition is appropriate under certain circumstances.},
	pages = {25},
	author = {Vogt, R},
	langid = {english},
	file = {Vogt - What is the Real K Factor.pdf:/home/akako/Zotero/storage/GS74B2PH/Vogt - What is the Real K Factor.pdf:application/pdf}
}

@online{luminosity,
	title = {{LumiPublicResults} {\textless} {CMSPublic} {\textless} {TWiki}},
	howpublished= {\url{https://twiki.cern.ch/twiki/bin/view/CMSPublic/LumiPublicResults}},
	urldate = {2020-06-05},
	file = {LumiPublicResults < CMSPublic < TWiki:/home/akako/Zotero/storage/GLKRNCAW/LumiPublicResults.html:text/html}
}

@article{particle_flow,
	title = {Particle-flow reconstruction and global event description with the {CMS} detector},
	volume = {12},
	issn = {1748-0221},
	url = {http://arxiv.org/abs/1706.04965},
	doi = {10.1088/1748-0221/12/10/P10003},
	abstract = {The {CMS} apparatus was identified, a few years before the start of the {LHC} operation at {CERN}, to feature properties well suited to particle-flow ({PF}) reconstruction: a highly-segmented tracker, a fine-grained electromagnetic calorimeter, a hermetic hadron calorimeter, a strong magnetic field, and an excellent muon spectrometer. A fully-fledged {PF} reconstruction algorithm tuned to the {CMS} detector was therefore developed and has been consistently used in physics analyses for the first time at a hadron collider. For each collision, the comprehensive list of final-state particles identified and reconstructed by the algorithm provides a global event description that leads to unprecedented {CMS} performance for jet and hadronic tau decay reconstruction, missing transverse momentum determination, and electron and muon identification. This approach also allows particles from pileup interactions to be identified and enables efficient pileup mitigation methods. The data collected by {CMS} at a centre-of-mass energy of 8 {TeV} show excellent agreement with the simulation and confirm the superior {PF} performance at least up to an average of 20 pileup interactions.},
	pages = {P10003--P10003},
	number = {10},
	journaltitle = {Journal of Instrumentation},
	shortjournal = {J. Inst.},
	author = {{CMS Collaboration}},
	urldate = {2020-06-05},
	date = {2017-10-06},
	eprinttype = {arxiv},
	eprint = {1706.04965},
	keywords = {High Energy Physics - Experiment, Physics - Instrumentation and Detectors}
}

@article{offshell_theory1,
	title = {Inadequacy of zero-width approximation for a light Higgs boson signal},
	volume = {2012},
	issn = {1029-8479},
	url = {https://doi.org/10.1007/JHEP08(2012)116},
	doi = {10.1007/JHEP08(2012)116},
	abstract = {In the Higgs search at the {LHC}, a light Higgs boson \$ {\textbackslash}left( \{\{115\}{\textbackslash},\{{\textbackslash}text\{{GeV}\}\} {\textbackslash}lesssim \{M\_\{{\textbackslash}text\{H\}\}\} {\textbackslash}lesssim \{13\}0{\textbackslash},\{{\textbackslash}text\{{GeV}\}\}\} {\textbackslash}right) \$is not excluded by experimental data. In this mass range, the width of the Standard Model Higgs boson is more than four orders of magnitude smaller than its mass. The zero-width approximation is hence expected to be an excellent approximation. We show that this is not always the case. The inclusion of off-shell contributions is essential to obtain an accurate Higgs signal normalisation at the 1\% precision level. For gg (→ H) → {VV}, V = W,Z, \$ {\textbackslash}mathcal\{O\} \$(10 \%) corrections occur due to an enhanced Higgs signal in the region {MV} V{\textgreater} 2 {MV}, where also sizable Higgs-continuum interference occurs. We discuss how experimental selection cuts can be used to exclude this region in search channels where the Higgs invariant mass cannot be reconstructed. We note that the H → V V decay modes in weak boson fusion are similarly affected.},
	pages = {116},
	number = {8},
	journaltitle = {Journal of High Energy Physics},
	shortjournal = {J. High Energ. Phys.},
	author = {Kauer, Nikolas and Passarino, Giampiero},
	urldate = {2020-06-05},
	date = {2012-08-23},
	langid = {english},
	file = {Submitted Version:/home/akako/Zotero/storage/FPM8VBZ3/Kauer and Passarino - 2012 - Inadequacy of zero-width approximation for a light.pdf:application/pdf}
}

@article{offshell_theory2,
	title = {Bounding the Higgs width at the {LHC} using full analytic results for gg → e−e+μ−μ+},
	volume = {2014},
	issn = {1029-8479},
	url = {https://doi.org/10.1007/JHEP04(2014)060},
	doi = {10.1007/JHEP04(2014)060},
	abstract = {We revisit the hadronic production of the four-lepton final state, e−e+μ−μ+, through the fusion of initial state gluons. This process is mediated by loops of quarks and we provide first full analytic results for helicity amplitudes that account for both the effects of the quark mass in the loop and off-shell vector bosons. The analytic results have been implemented in the Monte Carlo program {MCFM} and are both fast, and numerically stable in the region of low Z transverse momentum. We use our results to study the interference between Higgs-mediated and continuum production of four-lepton final states, which is necessary in order to obtain accurate theoretical predictions outside the Higgs resonance region. We have confirmed and extended a recent analysis of Caola and Melnikov that proposes to use a measurement of the off-shell region to constrain the total width of the Higgs boson. Using a simple cut-and-count method, existing {LHC} data should bound the width at the level of 25–45 times the Standard Model expectation. We investigate the power of using a matrix element method to construct a kinematic discriminant to sharpen the constraint. In our analysis the bound on the Higgs width is improved by a factor of about 1.6 using a simple cut on the {MEM} discriminant, compared to an invariant mass cut m4l{\textgreater} 300 {GeV}.},
	pages = {60},
	number = {4},
	journaltitle = {Journal of High Energy Physics},
	shortjournal = {J. High Energ. Phys.},
	author = {Campbell, John M. and Ellis, R. Keith and Williams, Ciaran},
	urldate = {2020-06-05},
	date = {2014-04-09},
	langid = {english},
	file = {Springer Full Text PDF:/home/akako/Zotero/storage/NBEGAR5Q/Campbell et al. - 2014 - Bounding the Higgs width at the LHC using full ana.pdf:application/pdf}
}

@book{offshell_poc,
	title = {Measurements of Higgs Boson Properties in Proton-Proton Collisions at $\sqrt{s} = 7$, 8 and 13 {TeV} at the {CERN} Large Hadron Collider},
	isbn = {978-3-030-25473-5},
	url = {https://www.springer.com/us/book/9783030254735},
	series = {Springer Theses},
	abstract = {This thesis documents the measurement of lifetime, width, mass, and couplings to two electroweak bosons of the recently-discovered Higgs boson using data from the {CMS} experiment at the Large Hadron Collider. Both on-shell (at the mass of around 125 {GeV}) and off-shell (above 200 {GeV}) Higgs boson production is studied and an excess of off-shell production with significance above two standard deviations is observed for the first time. The latter is a qualitative new way to study the Higgs field, responsible for generation of mass of all the known elementary particles. In addition, phenomenological tools have been developed with the Monte Carlo event generator and matrix element techniques for an optional analysis of {LHC} data. Optimization of the {CMS} data with careful alignment of the silicon tracker is also presented.},
	publisher = {Springer International Publishing},
	author = {Sarica, Ulascan},
	urldate = {2020-06-05},
	date = {2019},
	langid = {english},
	doi = {10.1007/978-3-030-25474-2},
	file = {Snapshot:/home/akako/Zotero/storage/UL2AITY7/9783030254735.html:text/html}
}

@article{pythia,
	title = {Tuning {PYTHIA} 8.1: the Monash 2013 tune},
	volume = {74},
	issn = {1434-6052},
	url = {https://doi.org/10.1140/epjc/s10052-014-3024-y},
	doi = {10.1140/epjc/s10052-014-3024-y},
	shorttitle = {Tuning {PYTHIA} 8.1},
	abstract = {We present an updated set of parameters for the {PYTHIA} 8 event generator. We reevaluate the constraints imposed by {LEP} and {SLD} on hadronization, in particular with regard to heavy-quark fragmentation and strangeness production. For hadron collisions, we combine the updated fragmentation parameters with the new {NNPDF}2.3 {LO} {PDF} set. We use minimum-bias, Drell–Yan, and underlying-event data from the {LHC} to constrain the initial-state-radiation and multi-parton-interaction parameters, combined with data from {SPS} and the Tevatron to constrain the energy scaling. Several distributions show significant improvements with respect to the current defaults, for both \$\$ee\$\$eeand \$\$pp\$\$ppcollisions, though we emphasize that interesting discrepancies remain in particular for strange particles and baryons. The updated parameters are available as an option starting from {PYTHIA} 8.185, by setting Tune:ee = 7 and Tune:pp = 14.},
	pages = {3024},
	number = {8},
	journaltitle = {The European Physical Journal C},
	shortjournal = {Eur. Phys. J. C},
	author = {Skands, P. and Carrazza, S. and Rojo, J.},
	urldate = {2020-06-05},
	date = {2014-08-15},
	langid = {english},
	file = {Springer Full Text PDF:/home/akako/Zotero/storage/HRGZNSFM/Skands et al. - 2014 - Tuning PYTHIA 8.1 the Monash 2013 tune.pdf:application/pdf}
}

@article{madgraph,
	title = {The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations},
	volume = {2014},
	issn = {1029-8479},
	url = {https://doi.org/10.1007/JHEP07(2014)079},
	doi = {10.1007/JHEP07(2014)079},
	abstract = {We discuss the theoretical bases that underpin the automation of the computations of tree-level and next-to-leading order cross sections, of their matching to parton shower simulations, and of the merging of matched samples that differ by light-parton multiplicities. We present a computer program, {MadGraph}5 {aMC}@{NLO}, capable of handling all these computations — parton-level fixed order, shower-matched, merged — in a unified framework whose defining features are flexibility, high level of parallelisation, and human intervention limited to input physics quantities. We demonstrate the potential of the program by presenting selected phenomenological applications relevant to the {LHC} and to a 1-{TeV} e+e− collider. While next-to-leading order results are restricted to {QCD} corrections to {SM} processes in the first public version, we show that from the user viewpoint no changes have to be expected in the case of corrections due to any given renormalisable Lagrangian, and that the implementation of these are well under way.},
	pages = {79},
	number = {7},
	journaltitle = {Journal of High Energy Physics},
	shortjournal = {J. High Energ. Phys.},
	author = {Alwall, J. and Frederix, R. and Frixione, S. and Hirschi, V. and Maltoni, F. and Mattelaer, O. and Shao, H.-S. and Stelzer, T. and Torrielli, P. and Zaro, M.},
	urldate = {2020-06-05},
	date = {2014-07-17},
	langid = {english},
	file = {Springer Full Text PDF:/home/akako/Zotero/storage/EGLQ44BB/Alwall et al. - 2014 - The automated computation of tree-level and next-t.pdf:application/pdf}
}

@article{djjvbf,
	title = {Search for a Higgs boson in the mass range from 145 to 1000 {GeV} decaying to a pair of W or Z bosons},
	volume = {2015},
	issn = {1029-8479},
	url = {http://arxiv.org/abs/1504.00936},
	doi = {10.1007/JHEP10(2015)144},
	abstract = {A search for a heavy Higgs boson in the H to {WW} and H to {ZZ} decay channels is reported. The search is based upon proton-proton collision data samples corresponding to an integrated luminosity of up to 5.1 inverse femtobarns at sqrt(s) = 7 {TeV} and up to 19.7 inverse femtobarns at sqrt(s) = 8 {TeV}, recorded by the {CMS} experiment at the {CERN} {LHC}. Several final states of the H to {WW} and H to {ZZ} decays are analyzed. The combined upper limit at the 95\% confidence level on the product of the cross section and branching fraction exclude a Higgs boson with standard model-like couplings and decays in the range 145 {\textless} m[H] {\textless} 1000 {GeV}. We also interpret the results in the context of an electroweak singlet extension of the standard model.},
	pages = {144},
	number = {10},
	journaltitle = {Journal of High Energy Physics},
	shortjournal = {J. High Energ. Phys.},
	author = {{CMS} Collaboration},
	urldate = {2020-06-08},
	date = {2015-10},
	eprinttype = {arxiv},
	eprint = {1504.00936},
	keywords = {High Energy Physics - Experiment},
	file = {arXiv Fulltext PDF:/home/akako/Zotero/storage/KCXEIEHY/CMS Collaboration - 2015 - Search for a Higgs boson in the mass range from 14.pdf:application/pdf;arXiv.org Snapshot:/home/akako/Zotero/storage/PFV225AL/1504.html:text/html}
}

@online{rfrv_higgs_pas,
	title = {Measurements of properties of the Higgs boson in the four-lepton final state in proton-proton collisions at $\sqrt{s}=13 \mathrm{TeV}$},
	url = {https://cds.cern.ch/record/2668684},
	abstract = {Properties of the Higgs (H) boson are measured in the \${\textbackslash}mathrm\{H\}{\textbackslash}rightarrow\{{\textbackslash}rm Z\}\{{\textbackslash}rm Z\}{\textbackslash}rightarrow4{\textbackslash}ell\$ (\${\textbackslash}ell=\{{\textbackslash}rm e\},{\textbackslash}mu\$) decay channel. The full data sample of proton-proton collisions at a center-of-mass energy of \$13{\textasciitilde}{\textbackslash}mathrm\{{TeV}\}\$ is used, corresponding to an integrated luminosity of \$137.1{\textasciitilde}{\textbackslash}mathrm\{fb\}{\textasciicircum}\{-1\}\$ recorded in 2016, 2017, and 2018 by the {CMS} detector at the {LHC}. The signal-strength modifier \${\textbackslash}mu\$, defined as the ratio of the H boson rate in the \$4{\textbackslash}ell\$ channel to the Standard Model ({SM}) expectation, is measured to be \${\textbackslash}mu=0.94{\textasciicircum}\{+0.07\}\_\{-0.07\}(\{{\textbackslash}rm stat.\}) {\textasciicircum}\{+0.08\}\_\{-0.07\}(\{{\textbackslash}rm syst.\})\$ with the H boson mass profiled in the fit. The signal-strength modifiers for different H boson production modes are also constrained. Measurements of the simplified template cross sections, designed to quantify the different H boson production processes in specific regions of phase space, are reported. The cross section for the production of the \${\textbackslash}mathrm\{H\}{\textbackslash}rightarrow4{\textbackslash}ell\$ in a fiducial region closely matching the experimental selection of the leptons is measured to be \${\textbackslash}sigma\_\{\{{\textbackslash}rm fid.\}\}=2.73{\textasciicircum}\{+0.23\}\_\{-0.22\}(\{{\textbackslash}rm stat.\}){\textasciicircum}\{+0.24\}\_\{-0.19\}(\{{\textbackslash}rm syst.\}){\textasciitilde}\{{\textbackslash}rm fb\}\$ at \$m\_\{{\textbackslash}rm H\} = 125.09{\textasciitilde}{\textbackslash}mathrm\{{GeV}\}\$, compared to a {SM} prediction of \$2.76 {\textbackslash}pm 0.14{\textasciitilde}{\textbackslash}mathrm\{fb\}\$. Differential cross sections as a function of the \$p\_\{{\textbackslash}rm T\}\$ and rapidity of the H boson, the number of associated jets, and the \$p\_\{{\textbackslash}rm T\}\$ of the leading associated jet are determined. All results are found to be compatible with the {SM} predictions, within the measurements precision.},
	titleaddon = {{CERN} Document Server},
	urldate = {2020-06-05},
	date = {2019},
	langid = {english},
	note = {Library Catalog: cds.cern.ch
Number: {CMS}-{PAS}-{HIG}-19-001},
	file = {Full Text PDF:/home/akako/Zotero/storage/PAS26ULP/2019 - Measurements of properties of the Higgs boson in t.pdf:application/pdf}
}

@article{fastjet,
	title = {{FastJet} user manual},
	volume = {72},
	issn = {1434-6052},
	url = {https://doi.org/10.1140/epjc/s10052-012-1896-2},
	doi = {10.1140/epjc/s10052-012-1896-2},
	abstract = {{FastJet} is a C++ package that provides a broad range of jet finding and analysis tools. It includes efficient native implementations of all widely used 2→1 sequential recombination jet algorithms for pp and e+e− collisions, as well as access to 3rd party jet algorithms through a plugin mechanism, including all currently used cone algorithms. {FastJet} also provides means to facilitate the manipulation of jet substructure, including some common boosted heavy-object taggers, as well as tools for estimation of pileup and underlying-event noise levels, determination of jet areas and subtraction or suppression of noise in jets.},
	pages = {1896},
	number = {3},
	journaltitle = {The European Physical Journal C},
	shortjournal = {Eur. Phys. J. C},
	author = {Cacciari, Matteo and Salam, Gavin P. and Soyez, Gregory},
	urldate = {2020-06-08},
	date = {2012-03-16},
	langid = {english},
	file = {Springer Full Text PDF:/home/akako/Zotero/storage/3W9TIU8M/Cacciari et al. - 2012 - FastJet user manual.pdf:application/pdf}
}

@article{campbell_two_2016,
	title = {Two loop correction to interference in gg → {ZZ}},
	volume = {2016},
	issn = {1029-8479},
	url = {https://doi.org/10.1007/JHEP08(2016)011},
	doi = {10.1007/JHEP08(2016)011},
	abstract = {We present results for the production of a pair of on-shell Z bosons via gluon-gluon fusion. This process occurs both through the production and decay of the Higgs boson, and through continuum production where the Z boson couples to a loop of massless quarks or to a massive quark. We calculate the interference of the two processes and its contribution to the cross section up to and including order O(αs3). The two-loop contributions to the amplitude are all known analytically, except for the continuum production through loops of top quarks of mass m. The latter contribution is important for the invariant mass of the two Z bosons, (as measured by the mass of their leptonic decay products, m4l), in a regime where m4l≥ 2m because of the contributions of longitudinal bosons. We examine all the contributions to the virtual amplitude involving top quarks, as expansions about the heavy top quark limit combined with a conformal mapping and Padé approximants. Comparison with the analytic results, where known, allows us to assess the validity of the heavy quark expansion, and it extensions. We give results for the {NLO} corrections to this interference, including both real and virtual radiation.},
	pages = {11},
	number = {8},
	journaltitle = {Journal of High Energy Physics},
	shortjournal = {J. High Energ. Phys.},
	author = {Campbell, John M. and Ellis, R. Keith and Czakon, Michal and Kirchner, Sebastian},
	urldate = {2020-06-08},
	date = {2016-08-01},
	langid = {english},
	file = {Springer Full Text PDF:/home/akako/Zotero/storage/YVQV6U5F/Campbell et al. - 2016 - Two loop correction to interference in gg → ZZ.pdf:application/pdf}
}

@article{caola_qcd_2016,
	title = {{QCD} corrections to vector boson pair production in gluon fusion including interference effects with off-shell Higgs at the {LHC}},
	volume = {2016},
	issn = {1029-8479},
	url = {https://doi.org/10.1007/JHEP07(2016)087},
	doi = {10.1007/JHEP07(2016)087},
	abstract = {We compute next-to-leading order ({NLO}) {QCD} corrections to the production of two massive electroweak bosons in gluon fusion. We consider both the prompt production process gg → V V and the production mediated by an exchange of an s-channel Higgs boson, gg → H∗ → V V . We include final states with both on- and off-shell vector bosons with leptonic decays. The gluonic production of vector bosons is a loop-induced process, including both massless and massive quarks in the loop. For gg → {ZZ} production, we obtain the {NLO} {QCD} corrections to the massive loops through an expansion around the heavy top limit. This approximation is valid below the top production threshold, giving a broad range of invariant masses between the Higgs production and the top production thresholds in which our results are valid. We explore the {NLO} {QCD} effects in gg → {ZZ} focusing, in particular, on the interference between prompt and Higgs-mediated processes. We find that the {QCD} corrections to the interference are large and similar in size to the corrections to both the signal and the background processes. At the same time, we observe that corrections to the interference change rapidly with the four-lepton invariant mass in the region around the {ZZ} production threshold. We also study the interference effects in gg → W +W − production where, due to technical limitations, we only consider contributions of massless loops. We find that the {QCD} corrections to the interference in this case are somewhat larger than those for either the signal or the background.},
	pages = {87},
	number = {7},
	journaltitle = {Journal of High Energy Physics},
	shortjournal = {J. High Energ. Phys.},
	author = {Caola, Fabrizio and Dowling, Matthew and Melnikov, Kirill and Röntsch, Raoul and Tancredi, Lorenzo},
	urldate = {2020-06-08},
	date = {2016-07-18},
	langid = {english},
	file = {Springer Full Text PDF:/home/akako/Zotero/storage/M4R63QBD/Caola et al. - 2016 - QCD corrections to vector boson pair production in.pdf:application/pdf}
}

@article{caola_qcd_2015,
	title = {{QCD} corrections to \${ZZ}\$ production in gluon fusion at the {LHC}},
	volume = {92},
	url = {https://link.aps.org/doi/10.1103/PhysRevD.92.094028},
	doi = {10.1103/PhysRevD.92.094028},
	abstract = {We compute the next-to-leading-order {QCD} corrections to the production of two Z-bosons in the annihilation of two gluons at the {LHC}. Being enhanced by a large gluon flux, these corrections provide a distinct and, potentially, the dominant part of the N3LO {QCD} contributions to Z-pair production in proton collisions. The gg→{ZZ} annihilation is a loop-induced process that receives the dominant contribution from loops of five light quarks, that are included in our computation in the massless approximation. We find that {QCD} corrections increase the gg→{ZZ} production cross section by O(50\%–100\%) depending on the values of the renormalization and factorization scales used in the leading-order computation and the collider energy. The large corrections to the gg→{ZZ} channel increase the pp→{ZZ} cross section by about 6\% to 8\%, exceeding the estimated theoretical uncertainty of the recent next-to-next-to-leading-order {QCD} calculation.},
	pages = {094028},
	number = {9},
	journaltitle = {Physical Review D},
	shortjournal = {Phys. Rev. D},
	author = {Caola, Fabrizio and Melnikov, Kirill and Röntsch, Raoul and Tancredi, Lorenzo},
	urldate = {2020-06-08},
	date = {2015-11-23},
	note = {Publisher: American Physical Society},
	file = {Full Text PDF:/home/akako/Zotero/storage/NHEPH6VF/Caola et al. - 2015 - QCD corrections to \$ZZ\$ production in gluon fusion.pdf:application/pdf}
}

@article{combine1,
	title = {Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined {ATLAS} and {CMS} analysis of the {LHC} \$pp\$ collision data at \${\textbackslash}sqrt\{s\}=\$ 7 and 8 {TeV}},
	volume = {2016},
	issn = {1029-8479},
	url = {http://arxiv.org/abs/1606.02266},
	doi = {10.1007/JHEP08(2016)045},
	abstract = {Combined {ATLAS} and {CMS} measurements of the Higgs boson production and decay rates, as well as constraints on its couplings to vector bosons and fermions, are presented. The combination is based on the analysis of five production processes, namely gluon fusion, vector boson fusion, and associated production with a \$W\$ or a \$Z\$ boson or a pair of top quarks, and of the six decay modes \$H {\textbackslash}to {ZZ}, {WW}\$, \${\textbackslash}gamma{\textbackslash}gamma, {\textbackslash}tau{\textbackslash}tau, bb\$, and \${\textbackslash}mu{\textbackslash}mu\$. All results are reported assuming a value of 125.09 {GeV} for the Higgs boson mass, the result of the combined measurement by the {ATLAS} and {CMS} experiments. The analysis uses the {CERN} {LHC} proton--proton collision data recorded by the {ATLAS} and {CMS} experiments in 2011 and 2012, corresponding to integrated luminosities per experiment of approximately 5 fb\${\textasciicircum}\{-1\}\$ at \${\textbackslash}sqrt\{s\}=7\$ {TeV} and 20 fb\${\textasciicircum}\{-1\}\$ at \${\textbackslash}sqrt\{s\} = 8\$ {TeV}. The Higgs boson production and decay rates measured by the two experiments are combined within the context of three generic parameterisations: two based on cross sections and branching fractions, and one on ratios of coupling modifiers. Several interpretations of the measurements with more model-dependent parameterisations are also given. The combined signal yield relative to the Standard Model prediction is measured to be 1.09 \${\textbackslash}pm\$ 0.11. The combined measurements lead to observed significances for the vector boson fusion production process and for the \$H {\textbackslash}to {\textbackslash}tau{\textbackslash}tau\$ decay of \$5.4\$ and \$5.5\$ standard deviations, respectively. The data are consistent with the Standard Model predictions for all parameterisations considered.},
	pages = {45},
	number = {8},
	journaltitle = {Journal of High Energy Physics},
	shortjournal = {J. High Energ. Phys.},
	author = {{ATLAS} and Collaborations, C. M. S.},
	urldate = {2020-06-08},
	date = {2016-08},
	eprinttype = {arxiv},
	eprint = {1606.02266},
	keywords = {High Energy Physics - Experiment},
	file = {arXiv Fulltext PDF:/home/akako/Zotero/storage/9YJMFJGR/ATLAS and Collaborations - 2016 - Measurements of the Higgs boson production and dec.pdf:application/pdf;arXiv.org Snapshot:/home/akako/Zotero/storage/YF9AU5K5/1606.html:text/html}
}

@online{combine2,
	title = {Procedure for the {LHC} Higgs boson search combination in Summer 2011},
	url = {https://cds.cern.ch/record/1379837},
	abstract = {In this note, we report the results of the technical combination exercises conducted
by the group during Winter-Spring 2011 and summarize the decisions taken
in preparation for the statistical combination of the Standard Model Higgs boson searches
at the {LHC}. The procedure to be used for the combination in Summer 2011 is explicitly
detailed to avoid potential biases from decisions taken after the data have
been collected.},
	titleaddon = {{CERN} Document Server},
	urldate = {2020-06-08},
	date = {2011-08-16},
	langid = {english},
	note = {Institution: {CERN}-{CMS}-{NOTE}-2011-005
Library Catalog: cds.cern.ch
Number: {ATL}-{PHYS}-{PUB}-2011-011},
	file = {Full Text PDF:/home/akako/Zotero/storage/C42CLVH8/2011 - Procedure for the LHC Higgs boson search combinati.pdf:application/pdf;Snapshot:/home/akako/Zotero/storage/TRXTERPS/1379837.html:text/html}
}

@online{combine3,
	title = {[1103.0354] Incorporating Nuisance Parameters in Likelihoods for Multisource Spectra},
	url = {https://arxiv.org/abs/1103.0354},
	urldate = {2020-06-08},
	file = {[1103.0354] Incorporating Nuisance Parameters in Likelihoods for Multisource Spectra:/home/akako/Zotero/storage/CAS7N8XC/1103.html:text/html}
}


text:
@online{site:typescript,
	title   = {Linguaggio TypeScript},
	url     = {https://www.typescriptlang.org/}
}

@online{site:html,
	title   = {Linguaggio HTML},
	url     = {https://www.w3schools.com/html/}
}

@online{site:css,
	title   = {Linguaggio CSS},
	url     = {https://www.w3schools.com/css/}
}

@online{site:webstorm,
	title   = {WebStorm},
	url     = {https://www.jetbrains.com/webstorm/}
}

@online{site:angular,
	title   = {Angular2+},
	url     = {https://angular.io/}
}

@online{site:ionic,
	title   = {Ionic},
	url     = {https://ionicframework.com/}
}

@online{site:cordova,
	title   = {Cordova},
	url     = {https://cordova.apache.org/}
}

@online{site:protractor,
	title   = {Protractor},
	url     = {https://www.protractortest.org/#/}
}

@online{site:cucumber,
	title   = {Cucumber},
	url     = {https://cucumber.io/}
}

@online{site:selenium,
	title   = {Selenium},
	url     = {https://www.selenium.dev/documentation/en/}
}

@online{site:appium,
	title   = {Appium},
	url     = {http://appium.io/}
}

@online{site:handlebars,
	title   = {Handlebars},
	url     = {https://handlebarsjs.com/guide/}
}

@online{site:gitlab,
	title   = {Gitlab},
	url     = {https://about.gitlab.com/}
}

@online{site:jiras,
	title   = {Jira Software},
	url     = {https://www.atlassian.com/it/software/jira}
}

@online{site:confluence,
	title   = {Confluence},
	url     = {https://www.atlassian.com/it/software/confluence}
}

@online{site:agile-manifesto,
	title   = {Agile manifesto},
	url     = {https://agilemanifesto.org/iso/it/manifesto.html}
}

license: MIT

license_type: permissive

branch_name: refs/heads/master

extension: bib


text:
@article{Cacciotti-Saija2018,
 abstract = {Reduced cardiac autonomic function is associated with increased risk of cardiovascular disease (CVD), with heart rate variability (HRV) providing an accessible index of cardiac autonomic function. HRV may provide a candidate physiological mechanism linking reduced cardiac autonomic function to increased risk for CVD in schizophrenia illness. This study examines whether HRV is also reduced in a community sample of treatment-seeking participants experiencing early psychosis (n = 48) compared to healthy volunteers (n = 48) and social anxiety control groups (n = 48) matched by gender and age. HRV was assessed during a five-minute interbeat interval recording at rest. Participants also completed self-report psychiatric symptom measures. Early psychosis participants showed significant reductions in HRV compared to social anxiety and healthy control groups. Reductions in HRV were also observed in early psychosis participants taking anticholinergic medications compared to both control groups taking cardio-benign medications or who were non-medicated. Lastly, whether or not early psychosis participants were taking anticholinergic medications was not associated with reductions in HRV. Findings provide preliminary evidence that early psychosis is associated with reduced HRV. This study supports further research with larger sample sizes to precisely determine the influence of anticholinergic drugs on HRV in early psychosis populations.},
 author = {Cacciotti-Saija, Cristina and Quintana, Daniel S. and Alvares, Gail A. and Hickie, Ian B. and Guastella, Adam J.},
 copyright = {All rights reserved},
 doi = {10.1016/j.psychres.2018.08.068},
 issn = {0165-1781},
 journal = {Psychiatry Research},
 keywords = {Cardiovascular disease, First episode psychosis, Heart rate variability, Neuroleptics, Schizophrenia, Social anxiety disorder},
 language = {en},
 month = {November},
 pages = {293--300},
 title = {Reduced heart rate variability in a treatment-seeking early psychosis sample},
 url = {http://www.sciencedirect.com/science/article/pii/S0165178117316311},
 urldate = {2020-08-29},
 volume = {269},
 year = {2018}
}