{"id":388,"date":"2020-04-14T22:55:43","date_gmt":"2020-04-14T20:55:43","guid":{"rendered":"https:\/\/web.infn.it\/lhcb_milano\/?page_id=388"},"modified":"2023-12-18T11:23:06","modified_gmt":"2023-12-18T10:23:06","slug":"publications-2","status":"publish","type":"page","link":"https:\/\/web.infn.it\/lhcb_milano\/publications-2\/","title":{"rendered":"Publications"},"content":{"rendered":"\n<h1 class=\"wp-block-heading\"><strong><span class=\"color\" style=\"color:#0693e3\">2023<\/span><\/strong><\/h1>\n\n\n\n<ul class=\"wp-block-list\">\n<li>LHCb collaboration, <strong>Amplitude analysis of the \u039b+c \u2192 pK-\u03c0+ decay and \u039b+c baryon polarization measurement in semileptonic beauty hadron decays<\/strong>, Phys. Rev. D 108 (2023) 012023, DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.108.012023\">https:\/\/doi.org\/10.1103\/PhysRevD.108.012023<\/a>, arXiv: <a href=\"https:\/\/arxiv.org\/abs\/2208.03262v1\">2208.03262<\/a>.<\/li>\n<\/ul>\n\n\n\n<h1 class=\"wp-block-heading\"><strong><span class=\"color\" style=\"color:#0693e3\">2022<\/span><\/strong><\/h1>\n\n\n\n<ul class=\"wp-block-list\">\n<li>LHCb Collaboration, <strong>Observation of a $J\/\\psi \\Lambda$ resonance consistent with a strange pentaquark candidate in $\\B^{-}\\to J\/\\psi \\Lambda\\bar{p}$ decays<\/strong>,&nbsp;<a class=\"\" href=\"https:\/\/arxiv.org\/abs\/2210.10346\">arXiv:2210.10346<\/a>, submitted to <em>PRL<\/em>.&nbsp;<a class=\"\" href=\"https:\/\/arxiv.org\/abs\/2210.10346\">https:\/\/arxiv.org\/abs\/2210.10346<\/a><\/li>\n\n\n\n<li>LHCb collaboration,&nbsp;<strong>Amplitude analysis of the \u039b+c \u2192 pK-\u03c0+ decay and \u039b+c baryon polarization measurement in semileptonic beauty hadron decays<\/strong>, arXiv:&nbsp;<a href=\"https:\/\/arxiv.org\/abs\/2208.03262v1\">2208.03262<\/a>, accepted by&nbsp;<em>Phys. Rev. D<\/em><\/li>\n\n\n\n<li>LHCb collaboration,&nbsp;<strong>Long-lived particle reconstruction downstream of the LHCb magnet<\/strong>, arXiv:&nbsp;<a href=\"https:\/\/arxiv.org\/abs\/2211.10920\">2211.10920<\/a>, submitted to<em>&nbsp;Eur. Phys. C<\/em><\/li>\n\n\n\n<li>Biryukov, V.M., Ruiz-Vidal, J., <strong>Improved experimental layout for dipole moment measurements at the LHC<\/strong>,&nbsp;<em>Eur. Phys. J. C<\/em>&nbsp;82<strong>,&nbsp;<\/strong>149 (2022). DOI: <a href=\"https:\/\/doi.org\/10.1140\/epjc\/s10052-022-10114-5\">https:\/\/doi.org\/10.1140\/epjc\/s10052-022-10114-5<\/a>; <a href=\"arXiv:2110.00845\">arXiv:2110.00845<\/a><\/li>\n\n\n\n<li>Beteta, C. and others, <strong>The SALT, readout ASIC for silicon strip sensors of upstream tracker in the upgraded LHCb experiment Sensors<\/strong>&nbsp;(2022)&nbsp;22(1) 107&nbsp; DOI:&nbsp;<a href=\"https:\/\/www.mdpi.com\/1424-8220\/22\/1\/107\/htm\">10.3390\/s22010107<\/a><\/li>\n<\/ul>\n\n\n\n<h1 class=\"wp-block-heading\"><strong><span class=\"color\" style=\"color:#0693e3\">2021<\/span><\/strong><\/h1>\n\n\n\n<ul class=\"wp-block-list\">\n<li>R. Aaij et al. (LHCb collaboration), <strong>Evidence for a new structure in the $J\/\\psi p$ and $J\/\\psi \\bar{p}$ systems in $B_s^0 \\to J\/\\psi p \\bar{p}$ decays<\/strong>, <em>Phys.Rev.Lett.<\/em>&nbsp;128&nbsp;(2022)&nbsp;062001,&nbsp; DOI:<a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.128.062001\" target=\"_blank\">10.1103\/PhysRevLett.128.062001<\/a><\/li>\n\n\n\n<li>S. Aiola, et al, \u200b<strong>Progress towards the first measurement of charm baryon dipole moments<\/strong>, Phys. Rev. D 103, 072003 (2021), DOI: <a href=\"https:\/\/arxiv.org\/ct?url=https%3A%2F%2Fdx.doi.org%2F10.1103%2FPhysRevD.103.072003&amp;v=107a8f63\">10.1103\/PhysRevD.103.072003<\/a>; \u200b<a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/2010.11902\" target=\"_blank\">arXiv: 2010.11902<\/a><\/li>\n<\/ul>\n\n\n\n<h1 class=\"wp-block-heading\"><strong><span class=\"color\" style=\"color:#0693e3\">2020<\/span><\/strong><\/h1>\n\n\n\n<ul class=\"wp-block-list\">\n<li>S. Aiola, et al, \u200b<strong>Hybrid seeding: A standalone track reconstruction algorithm for scintillating fibre tracker at LHCb<\/strong>,\u200b&nbsp;<em>Computer Physics Communications<\/em>, 2020, 107713, \u200b<a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1016\/j.cpc.2020.107713\" target=\"_blank\">DOI: 10.1016\/j.cpc.2020.107713<\/a>\u200b,&nbsp;<a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/2007.02591\" target=\"_blank\">a\u200brXiv: 2007.02591\u200b<\/a><\/li>\n\n\n\n<li>A. Dainese&nbsp;<em>et al.<\/em>, &nbsp;<strong>Physics Beyond Colliders QCD Working Group Report<\/strong>, J. Phys. G 47 (2020) 010501, <a rel=\"noreferrer noopener\" href=\"http:\/\/cds.cern.ch\/record\/2652442\" target=\"_blank\">CERN-PBC-REPORT-2018-008<\/a>, DOI: <a rel=\"noreferrer noopener\" href=\"http:\/\/dx.doi.org\/10.1088\/1361-6471\/ab4cd2\" target=\"_blank\">10.1088\/1361-6471\/ab4cd2<\/a>, arXiv:<a rel=\"noreferrer noopener\" href=\"http:\/\/arxiv.org\/abs\/arXiv:1901.04482\" target=\"_blank\"> 1901.04482<\/a><\/li>\n\n\n\n<li>J. Beacham&nbsp;<em>et al.<\/em>, <strong>Physics Beyond Colliders at CERN: Beyond the Standard Model Working Group Report<\/strong>,<strong> <\/strong>J. Phys. G 47 (2020) 010501, <a rel=\"noreferrer noopener\" href=\"https:\/\/cds.cern.ch\/record\/2652223\" target=\"_blank\">CERN-PBC-REPORT-2018-007<\/a>, DOI: <a rel=\"noreferrer noopener\" href=\"http:\/\/dx.doi.org\/10.1088\/1361-6471\/ab4cd2\" target=\"_blank\">10.1088\/1361-6471\/ab4cd2<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1901.09966\" target=\"_blank\">1901.09966<\/a>&nbsp;<\/li>\n\n\n\n<li>D. Marangotto, <strong>Extracting maximum information from polarised baryon decays via amplitude analysis: the <span class=\"katex-eq\" data-katex-display=\"false\">\\Lambda_{c}^{+}\\rightarrow pK^{-}\\pi^{+}<\/span> case<\/strong>, <em>Advances in High Energy Physics<\/em> (2020) 7463073, <a rel=\"noopener noreferrer\" href=\"https:\/\/doi.org\/10.1155\/2020\/7463073\" target=\"_blank\">DOI: 10.1155\/2020\/7463073<\/a>, <a rel=\"noopener noreferrer\" href=\"https:\/\/arxiv.org\/abs\/2004.12318\" target=\"_blank\">arXiv: 2004.12318<\/a><\/li>\n\n\n\n<li>D. Marangotto, <strong>Helicity Amplitudes for Generic Multibody particle decays featuring multiple decay chains, <\/strong>Advances in High Eneergy Physics (2020) 6674595, <a href=\"https:\/\/www.hindawi.com\/journals\/ahep\/2020\/6674595\/\">DOI: 10.1155\/2020\/6674595<\/a>, <a href=\"https:\/\/arxiv.org\/abs\/1911.10025\">arXiv:1911.10025<\/a>.<\/li>\n\n\n\n<li>S. Aiola, et al, \u200b<strong>Hybrid seeding: A standalone track reconstruction algorithm for scintillating fibre tracker at LHCb<\/strong>,\u200b <em>Computer Physics Communications<\/em>, in press, 2020, \u200b<a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1016\/j.cpc.2020.107713\" target=\"_blank\">DOI: 10.1016\/j.cpc.2020.107713<\/a>\u200b, <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/2007.02591\" target=\"_blank\">a\u200brXiv: 2007.02591\u200b<\/a><\/li>\n\n\n\n<li>R. Aaij <em>et<\/em> al. (LHCb Collaboration), <strong>Search for CP violation and observation of P violation in <span class=\"katex-eq\" data-katex-display=\"false\">\\Lambda^0_b\\rightarrow p\\pi^\u2212\\pi^+\\pi^\u2212 <\/span> decays<\/strong>, Phys. Rev. D 102 (2020) 05110 (R), <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1103\/PhysRevD.102.051101\" target=\"_blank\">DOI: 10.1103\/PhysRevD.102.051101<\/a><\/li>\n\n\n\n<li>C. Barschel et al., <strong>LHC fixed target experiments: Report from the LHC Fixed Target Working Group of the CERN Physics Beyond Colliders Forum<\/strong>, <a href=\"https:\/\/cds.cern.ch\/record\/2653780?ln=en\">CERN-PBC-REPORT-2019-001<\/a> <\/li>\n\n\n\n<li>L. Henry et al., <strong>Search for New Physics via Baryon EDM at LHC<\/strong>, <em>Proceedings of the 28th International Symposium on Lepton Photon Interactions at High Energies (LP17), p. 384-393, 2020 World Scientific Publisher<\/em>, <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1142\/9789811207402_0028\" target=\"_blank\">DOI: 10.1142\/9789811207402_0028<\/a><\/li>\n<\/ul>\n\n\n\n<h1 class=\"wp-block-heading\"><strong><span style=\"color:#0693e3\" class=\"color\">2019<\/span><\/strong><\/h1>\n\n\n\n<ul class=\"wp-block-list\">\n<li>R. Aaij et al (LHCb Collaboration), <em>Observation of New Resonances in the <em><span class=\"katex-eq\" data-katex-display=\"false\"> \\Lambda_b^0\\pi^+\\pi^- <\/span><\/em> System<\/em>, <strong>Phys.Rev.Lett.&nbsp;123&nbsp;(2019)&nbsp;15,&nbsp;152001<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.123.152001\" target=\"_blank\">10.1103\/PhysRevLett.123.152001<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1907.13598\" target=\"_blank\">1907.13598<\/a><\/li>\n\n\n\n<li>R. Aaij et al (LHCb Collaboration), <em>Search for C\u200bP violation and observation of P violation in <span class=\"katex-eq\" data-katex-display=\"false\"> \\Lambda_b^0\\rightarrow p\\pi^-\\pi^+\\pi^- <\/span> decays<\/em>, <strong>submitted to Phys. Rev. Lett.<\/strong>, arXiv: <a href=\"https:\/\/arxiv.org\/abs\/1912.10741\">1912.10741<\/a><\/li>\n\n\n\n<li>R. Aaij et al (LHCb Collaboration), <em>Observation of <span class=\"katex-eq\" data-katex-display=\"false\"> B_{(s)}^0 \\rightarrow J\/\\Psi p\\bar{p} <\/span> decays and precision measurements of the <span class=\"katex-eq\" data-katex-display=\"false\"> B_{(s)}^0 <\/span> \u200bmasses<\/em>, <strong>Phys.Rev.Lett.&nbsp;122&nbsp;(2019)&nbsp;19,&nbsp;191804<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.122.191804\" target=\"_blank\">10.1103\/PhysRevLett.122.191804<\/a>; arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1902.05588\" target=\"_blank\">1902.05588<\/a><\/li>\n\n\n\n<li>R. Aaij et al (LHCb Collaboration), <em>Observation of Two Resonances in the <span class=\"katex-eq\" data-katex-display=\"false\"> \\Lambda_b^0 \\pi^{\\pm} <\/span> Systems and Precise Measurement of <span class=\"katex-eq\" data-katex-display=\"false\"> \\Sigma_b^{\\pm} <\/span> and <em><span class=\"katex-eq\" data-katex-display=\"false\"> \\Sigma_b^{*,\\pm} <\/span><\/em> properties<\/em>, <strong>Phys.Rev.Lett.&nbsp;122&nbsp;(2019)&nbsp;1,&nbsp;012001<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.122.012001\" target=\"_blank\">10.1103\/PhysRevLett.122.012001<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1809.07752\" target=\"_blank\">1809.07752<\/a><\/li>\n<\/ul>\n\n\n\n<h1 class=\"wp-block-heading\"><strong><span style=\"color:#0693e3\" class=\"color\">2018<\/span><\/strong><\/h1>\n\n\n\n<ul class=\"wp-block-list\">\n<li>R. Aaij et al (LHCb Collaboration), <em>Search for beautiful tetraquarks in the <span class=\"katex-eq\" data-katex-display=\"false\"> \\Upsilon (1S) \\mu^+ \\mu^- <\/span> invariant-mass spectrum<\/em>, <strong>JHEP&nbsp;10&nbsp;(2018)&nbsp;086<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1007\/JHEP10(2018)086\" target=\"_blank\">10.1007\/JHEP10(2018)086<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1806.09707\" target=\"_blank\">1806.09707<\/a><\/li>\n\n\n\n<li>R. Aaij et al (LHCb Collaboration), <em>Central exclusive production of <span class=\"katex-eq\" data-katex-display=\"false\"> J\/\\Psi <\/span> and <span class=\"katex-eq\" data-katex-display=\"false\"> \\Psi(2S) <\/span> mesons in pp collisions at <span class=\"katex-eq\" data-katex-display=\"false\"> \\sqrt{s}=13 <\/span> TeV<\/em>, <strong>JHEP&nbsp;10&nbsp;(2018)&nbsp;167<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1007\/JHEP10(2018)167\" target=\"_blank\">10.1007\/JHEP10(2018)167<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1806.04079\" target=\"_blank\">1806.04079<\/a><\/li>\n\n\n\n<li>R. Aaij et al (LHCb Collaboration), <em>Search for CP violation using triple product asymmetries in <span class=\"katex-eq\" data-katex-display=\"false\"> \\Lambda^0_b \\rightarrow p K^- \\pi^+ \\pi^- <\/span>, <em><span class=\"katex-eq\" data-katex-display=\"false\"> \\Lambda^0_b \\rightarrow p K^- K^+ K^- <\/span><\/em> and <em><em><span class=\"katex-eq\" data-katex-display=\"false\"> \\Xi^0_b \\rightarrow p K^- K^- \\pi^+ <\/span><\/em><\/em> decays<\/em>, <strong>JHEP&nbsp;08&nbsp;(2018)&nbsp;039<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1007\/JHEP08(2018)039\" target=\"_blank\">10.1007\/JHEP08(2018)039<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1805.03941\" target=\"_blank\">1805.03941<\/a><span class=\"color\" style=\"color:#313131\"><\/span><\/li>\n\n\n\n<li><span class=\"color\" style=\"color:#313131\">R. Aaij et al (LHCb Collaboration), <em>Physics case for an LHCb Upgrade II \u2013 Opportunities in flavour physics, and beyond, in the HL-LHC era<\/em>, <a rel=\"noreferrer noopener\" href=\"https:\/\/cds.cern.ch\/record\/2636441\" target=\"_blank\">CERN-LHCC-2018-027<\/a><\/span>, <span class=\"color\" style=\"color:#313131\">arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1808.08865\" target=\"_blank\">1808.08865<\/a><\/span><\/li>\n<\/ul>\n\n\n\n<h1 class=\"wp-block-heading has-vivid-cyan-blue-color has-text-color\"><strong><span class=\"color\" style=\"color:#0693e3\">201<\/span>7<\/strong><\/h1>\n\n\n\n<ul class=\"wp-block-list\">\n<li>N. Neri, et al, <em>Testbeam results of the first real-time embedded tracking system with artificial retina<\/em>, <strong>Nucl.Instrum.Meth.A&nbsp;845&nbsp;(2017)&nbsp;607<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1016\/j.nima.2016.05.129\" target=\"_blank\">10.1016\/j.nima.2016.05.129<\/a><\/li>\n\n\n\n<li>R. Aaij et al (LHCb Collaboration), <span class=\"katex-eq\" data-katex-display=\"false\"> \\chi_{c1} <\/span> and <em><span class=\"katex-eq\" data-katex-display=\"false\"> \\chi_{c2} <\/span> Resonance Parameters with the Decays&nbsp;<span class=\"katex-eq\" data-katex-display=\"false\"> \\chi_{c1,c2} \\rightarrow J\/\\Psi \\mu^+ \\mu^- <\/span><\/em>, <strong>Phys.Rev.Lett.&nbsp;119&nbsp;(2017)&nbsp;22,&nbsp;221801<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.119.221801\" target=\"_blank\">10.1103\/PhysRevLett.119.221801<\/a>; arXiv: <a href=\"https:\/\/arxiv.org\/pdf\/1709.04247.pdf\">1709.04<\/a><a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1709.04247\" target=\"_blank\">2<\/a><a href=\"https:\/\/arxiv.org\/pdf\/1709.04247.pdf\">47<\/a><\/li>\n\n\n\n<li>R. Aaij et al (LHCb Collaboration), <em>Measurement of CP observables in <span class=\"katex-eq\" data-katex-display=\"false\"> B^{\\pm} \\rightarrow D^{(\u2217)} K^{\\pm} <\/span> and <em><span class=\"katex-eq\" data-katex-display=\"false\"> B^{\\pm} \\rightarrow D^{(\u2217)} \\pi^{\\pm} <\/span><\/em><\/em> <em>decays<\/em>, <strong>Phys.Lett.B&nbsp;777&nbsp;(2018)&nbsp;16-30<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1016\/j.physletb.2017.11.070\" target=\"_blank\">10.1016\/j.physletb.2017.11.070<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1708.06370\" target=\"_blank\">1708.06370<\/a><\/li>\n\n\n\n<li>R. Aaij et al (LHCb Collaboration), <em>Observation of the decay <span class=\"katex-eq\" data-katex-display=\"false\"> \\Lambda_b^0 \\rightarrow pK^\u2212\\mu^+\\mu^- <\/span> and a search for C\u200bP violation<\/em>, <strong>JHEP&nbsp;06&nbsp;(2017)&nbsp;108<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1007\/JHEP06(2017)108\" target=\"_blank\">10.1007\/JHEP06(2017)108<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1703.00256\" target=\"_blank\">1703.00256<\/a><\/li>\n\n\n\n<li>E. Bagli at al, <em>Electromagnetic dipole moments of charged baryons with bent crystals at the LHC<\/em>, <strong>Eur. Phys. J. C (2017) 77:828<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1140\/epjc\/s10052-017-5400-x\" target=\"_blank\">10.1140\/epjc\/s10052-017-5400-x<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/1708.08483\" target=\"_blank\">1708.08483<\/a><\/li>\n\n\n\n<li>F. J. Botella et al, <em>On the search for the electric dipole moment of strange and charm baryons at LHC<\/em>, <strong>Eur. Phys. J. C (2017) 77:181<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1140\/epjc\/s10052-017-4679-y\" target=\"_blank\">10.1140\/epjc\/s10052-017-4679-y<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1612.06769\" target=\"_blank\">1612.06769<\/a><\/li>\n\n\n\n<li>R. Aaij et al (LHCb Collaboration), <em>Measurement of matter-antimatter differences in beauty baryon decays<\/em>, <strong>Nature Phys.&nbsp;13&nbsp;(2017)&nbsp;391-396<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1038\/nphys4021\" target=\"_blank\">10.1038\/nphys4021<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1609.05216\" target=\"_blank\">1609.05216<\/a> <\/li>\n\n\n\n<li>A. Abba et al, <em>Silicon telescope for prototype sensor characterization using particle beams and cosmic rays<\/em>,<em> <\/em><strong>JINST 12 (2017) C03060<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1088\/1748-0221\/12\/03\/C03060\" target=\"_blank\">10.1088\/1748-0221\/12\/03\/C03060<\/a><\/li>\n<\/ul>\n\n\n\n<h1 class=\"wp-block-heading has-vivid-cyan-blue-color has-text-color\"><strong><span class=\"color\" style=\"color:#0693e3\">201<\/span>6<\/strong><\/h1>\n\n\n\n<ul class=\"wp-block-list\">\n<li>K. Carvalho Akiba, et al, <em>The HeRSCheL detector: high-rapidity shower counters for LHCb<\/em>, <strong>JINST&nbsp;13&nbsp;(2018)&nbsp;04,&nbsp;P04017<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1088\/1748-0221\/13\/04\/P04017\" target=\"_blank\">10.1088\/1748-0221\/13\/04\/P04017<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1801.04281\" target=\"_blank\">1801.04281<\/a><\/li>\n\n\n\n<li>A. Merli, <em>Search for CP violation using triple-product asymmetries in <em><span class=\"katex-eq\" data-katex-display=\"false\"> \\Lambda^0_b \\rightarrow p h^- h^+ h^- <\/span> and <em><span class=\"katex-eq\" data-katex-display=\"false\"> \\Xi^0_b \\rightarrow p h^- h^- h^+ <\/span><\/em><\/em> decays, <\/em><strong>Nuovo Cim.C&nbsp;39&nbsp;(2016)&nbsp;2,&nbsp;273<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1393\/ncc\/i2016-16273-2\" target=\"_blank\">10.1393\/ncc\/i2016-16273-2<\/a><\/li>\n<\/ul>\n\n\n\n<h1 class=\"wp-block-heading has-vivid-cyan-blue-color has-text-color\"><strong><span class=\"color\" style=\"color:#0693e3\">201<\/span>4<\/strong><\/h1>\n\n\n\n<ul class=\"wp-block-list\">\n<li>R. Aaij et al (LHCb Collaboration), <em>Search for&nbsp;CP&nbsp;violation using&nbsp;T-odd correlations in <span class=\"katex-eq\" data-katex-display=\"false\"> D^0 \\rightarrow K^+K^-\\pi^+\\pi^- <\/span> decays<\/em>, <strong>JHEP 10 (2014) 005<\/strong>, DOI: <a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1007\/JHEP10(2014)005\" target=\"_blank\">10.1007\/JHEP10(2014)005<\/a>, arXiv: <a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/1408.1299\" target=\"_blank\">1408.1299<\/a><\/li>\n<\/ul>\n\n\n\nngg_shortcode_0_placeholder\n","protected":false},"excerpt":{"rendered":"<p>2023 2022 2021 2020 2019 2018 2017 2016 2014<\/p>\n","protected":false},"author":3,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"ngg_post_thumbnail":0,"footnotes":""},"class_list":["post-388","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/web.infn.it\/lhcb_milano\/wp-json\/wp\/v2\/pages\/388","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/web.infn.it\/lhcb_milano\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/web.infn.it\/lhcb_milano\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/web.infn.it\/lhcb_milano\/wp-json\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/web.infn.it\/lhcb_milano\/wp-json\/wp\/v2\/comments?post=388"}],"version-history":[{"count":79,"href":"https:\/\/web.infn.it\/lhcb_milano\/wp-json\/wp\/v2\/pages\/388\/revisions"}],"predecessor-version":[{"id":911,"href":"https:\/\/web.infn.it\/lhcb_milano\/wp-json\/wp\/v2\/pages\/388\/revisions\/911"}],"wp:attachment":[{"href":"https:\/\/web.infn.it\/lhcb_milano\/wp-json\/wp\/v2\/media?parent=388"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}