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Report from Working Group 3 : Beyond the Standard Model physics at the HL-LHC and HE-LHC / Cid Vidal, Xabier (Santiago de Compostela U., IGFAE) ; D'Onofrio, Monica (Liverpool U.) ; Fox, Patrick J (Fermilab) ; Torre, Riccardo (CERN ; INFN, Genoa) ; Ulmer, Keith A (Colorado U.) ; Aboubrahim, Amin (Northeastern U.) ; Albert, Andreas (RWTH Aachen U.) ; Alimena, Juliette (Ohio State U., Columbus (main)) ; Allanach, Benjamin C (Cambridge U., DAMTP) ; Alpigiani, Cristiano (Washington U., Seattle) et al.
This is the third out of five chapters of the final report [1] of the Workshop on Physics at HL-LHC, and perspectives on HE-LHC [2]. It is devoted to the study of the potential, in the search for Beyond the Standard Model (BSM) physics, of the High Luminosity (HL) phase of the LHC, defined as $3$ ab$^{-1}$ of data taken at a centre-of-mass energy of 14 TeV, and of a possible future upgrade, the High Energy (HE) LHC, defined as $15$ ab$^{-1}$ of data at a centre-of-mass energy of 27 TeV. [...]
arXiv:1812.07831; CERN-LPCC-2018-05.- Geneva : CERN, 2019-12-02 - 281 p. - Published in : CERN Yellow Rep. Monogr. 7 (2019) 585-865 Fulltext: PDF; arXiv: PDF; External link: Published Fulltext
In : HL/HE-LHC Workshop : Workshop on the Physics of HL-LHC, and Perspectives at HE-LHC, Geneva, Switzerland, 18 - 20 Jun 2018
Report on the Physics at the HL-LHC, and Perspectives for the HE-LHC, Geneva, Switzerland, 18 - 20 Jun 2018, pp.585-865

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Measurement of the Mass Difference Between Top and Anti-top Quarks at CDF / Aaltonen, T. (Helsinki Inst. of Phys.) ; Alvarez Gonzalez, B. (Cantabria Inst. of Phys. ; Oviedo U.) ; Amerio, S. (INFN, Padua) ; Amidei, D. (Michigan U.) ; Anastassov, A. (Fermilab ; Northwestern U.) ; Annovi, A. (Frascati) ; Antos, J. (Comenius U.) ; Apollinari, G. (Fermilab) ; Appel, J.A. (Fermilab) ; Arisawa, T. (Waseda U.) et al. /R. C. Group
We present a measurement of the mass difference between top ($t$) and anti-top ($\bar{t}$) quarks using $t\bar{t}$ candidate events reconstructed in the final state with one lepton and multiple jets. We use the full data set of Tevatron $\sqrt{s} = 1.96$ TeV proton-antiproton collisions recorded by the CDF II detector, corresponding to an integrated luminosity of 8.7 fb$^{-1}$. [...]
arXiv:1210.6131; FERMILAB-PUB-12-577-E.- 2013-03-18 - 7 p. - Published in : Phys. Rev. D 87 (2013) 052013 Fermilab Library: PDF; Fulltext: PDF; External link: Fermilab Library Server (fulltext available)

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Fundamental Physics at the Intensity Frontier Workshop on Fundamental Physics at the Intensity Frontier - Intensity Frontier Workshop 30 Nov - 2 Dec 2011 - Rockville, MD, USA / Hewett, J.L. (SLAC); Weerts, H. (Argonne); Brock, R. (Michigan State U.); Butler, J.N. (Fermilab); Casey, B.C.K. (Fermilab); Collar, J. (Chicago U., EFI); de Gouvea, A. (Northwestern U.); Essig, R. (SUNY, Stony Brook); Grossman, Y. (Cornell U., Phys. Dept.); Haxton, W. (UC, Berkeley) et al.
The Proceedings of the 2011 workshop on Fundamental Physics at the Intensity Frontier. Science opportunities at the intensity frontier are identified and described in the areas of heavy quarks, charged leptons, neutrinos, proton decay, new light weakly-coupled particles, and nucleons, nuclei, and atoms..
2012 - 229 p. arXiv:1205.2671 .- ANL-HEP-TR-12-25 .- SLAC-R-991 .- FERMILAB-CONF-12-879-PPD .- ANL-HEP-TR-12-25 .- SLAC-R-991 - Published in : 10.2172/1042577
10.2172/1042577

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Search for new phenomena in events with two $Z$ bosons and missing transverse momentum in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV / Aaltonen, T. (Helsinki Inst. of Phys.) ; Alvarez Gonzalez, B. (Cantabria Inst. of Phys. ; Oviedo U.) ; Amerio, S. (INFN, Padua) ; Amidei, D. (Michigan U.) ; Anastassov, A. (Fermilab ; Northwestern U.) ; Annovi, A. (Frascati) ; Antos, J. (Comenius U.) ; Apollinari, G. (Fermilab) ; Appel, J.A. (Fermilab) ; Arisawa, T. (Waseda U.) et al. /R. C. Group
We present a search for new phenomena in events with two reconstructed $Z$ bosons and large missing transverse momentum, sensitive to processes $p\bar{p}\rightarrow X_2X_2 \rightarrow Z Z X_1 X_1$, where $X_2$ is an unstable particle decaying as $X_2\rightarrow ZX_1$ and $X_1$ is undetected. The particles $X_1$ and $X_2$ may be, among other possibilities, fourth generation neutrinos or supersymmetric particles. [...]
arXiv:1112.1577; FERMILAB-PUB-11-645-E.- 2012 - 7 p. - Published in : Phys. Rev. D 85 (2012) 011104 Fulltext: PDF; External link: Fermilab Library Server (fulltext available)

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Measurement of the Top Pair Production Cross Section in the Lepton + Jets Channel Using a Jet Flavor Discriminant / for the CDF Collaboration
We present a new method to measure the top quark pair production cross section and the background rates with 2.7 fb$^{-1}$ of data from $p\bar{p}$ collisions at $\sqrt{s} =1.96$ TeV collected with the CDF II Detector. The size of the dataset was chosen to directly show the improvements of this new method. [...]
arXiv:1103.4821; FERMILAB-PUB-11-148-E.- 2011 - 7 p. - Published in : Phys. Rev. D 84 (2011) 031101 Fulltext: arXiv:1103.4821 - PDF; fermilab-pub-11-148-e - PDF; External links: Fermilab Library Server (fulltext available); Fermilab Today Result of the Week

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