A model independent study of sensitivity to CP violation in decays of charmed mesons to three-body final states

ilustraciones, diagramas

Autores:
Jaimes Elles, Sergio Javier
Tipo de recurso:
Fecha de publicación:
2021
Institución:
Universidad Nacional de Colombia
Repositorio:
Universidad Nacional de Colombia
Idioma:
eng
OAI Identifier:
oai:repositorio.unal.edu.co:unal/79828
Acceso en línea:
https://repositorio.unal.edu.co/handle/unal/79828
https://repositorio.unal.edu.co/
Palabra clave:
530 - Física
Mesones
VIOLACION DE LA PARIDAD DE CONJUGACION DE CARGA
Decay
CP violation
Dalitz Plot
Charm quark
Sensitivity
Standard Model
Miranda Procedure
Desintegración
Violacion CP
Figura de Dalitz
Quark encantado
Sensibilidad
Modelo Estándar
Procedimiento de Miranda
Rights
openAccess
License
Atribución-NoComercial-SinDerivadas 4.0 Internacional
id UNACIONAL2_19fab91dd306ef1cbb808814a05e557b
oai_identifier_str oai:repositorio.unal.edu.co:unal/79828
network_acronym_str UNACIONAL2
network_name_str Universidad Nacional de Colombia
repository_id_str
dc.title.eng.fl_str_mv A model independent study of sensitivity to CP violation in decays of charmed mesons to three-body final states
dc.title.translated.spa.fl_str_mv Un estudio independiente del modelo de sensibilidad a violación CP en desintegraciones de mesones encantados a tres estados finales
title A model independent study of sensitivity to CP violation in decays of charmed mesons to three-body final states
spellingShingle A model independent study of sensitivity to CP violation in decays of charmed mesons to three-body final states
530 - Física
Mesones
VIOLACION DE LA PARIDAD DE CONJUGACION DE CARGA
Decay
CP violation
Dalitz Plot
Charm quark
Sensitivity
Standard Model
Miranda Procedure
Desintegración
Violacion CP
Figura de Dalitz
Quark encantado
Sensibilidad
Modelo Estándar
Procedimiento de Miranda
title_short A model independent study of sensitivity to CP violation in decays of charmed mesons to three-body final states
title_full A model independent study of sensitivity to CP violation in decays of charmed mesons to three-body final states
title_fullStr A model independent study of sensitivity to CP violation in decays of charmed mesons to three-body final states
title_full_unstemmed A model independent study of sensitivity to CP violation in decays of charmed mesons to three-body final states
title_sort A model independent study of sensitivity to CP violation in decays of charmed mesons to three-body final states
dc.creator.fl_str_mv Jaimes Elles, Sergio Javier
dc.contributor.advisor.none.fl_str_mv Milanés Carreño, Diego Alejandro
dc.contributor.author.none.fl_str_mv Jaimes Elles, Sergio Javier
dc.contributor.researchgroup.spa.fl_str_mv Grupo de Partículas FENYX-UN
dc.subject.ddc.spa.fl_str_mv 530 - Física
topic 530 - Física
Mesones
VIOLACION DE LA PARIDAD DE CONJUGACION DE CARGA
Decay
CP violation
Dalitz Plot
Charm quark
Sensitivity
Standard Model
Miranda Procedure
Desintegración
Violacion CP
Figura de Dalitz
Quark encantado
Sensibilidad
Modelo Estándar
Procedimiento de Miranda
dc.subject.lemb.none.fl_str_mv Mesones
VIOLACION DE LA PARIDAD DE CONJUGACION DE CARGA
dc.subject.proposal.eng.fl_str_mv Decay
CP violation
Dalitz Plot
Charm quark
Sensitivity
Standard Model
Miranda Procedure
dc.subject.proposal.spa.fl_str_mv Desintegración
Violacion CP
Figura de Dalitz
Quark encantado
Sensibilidad
Modelo Estándar
Procedimiento de Miranda
description ilustraciones, diagramas
publishDate 2021
dc.date.accessioned.none.fl_str_mv 2021-07-21T21:12:08Z
dc.date.available.none.fl_str_mv 2021-07-21T21:12:08Z
dc.date.issued.none.fl_str_mv 2021
dc.type.spa.fl_str_mv Trabajo de grado - Maestría
dc.type.driver.spa.fl_str_mv info:eu-repo/semantics/masterThesis
dc.type.version.spa.fl_str_mv info:eu-repo/semantics/acceptedVersion
dc.type.content.spa.fl_str_mv Text
dc.type.redcol.spa.fl_str_mv http://purl.org/redcol/resource_type/TM
status_str acceptedVersion
dc.identifier.uri.none.fl_str_mv https://repositorio.unal.edu.co/handle/unal/79828
dc.identifier.instname.spa.fl_str_mv Universidad Nacional de Colombia
dc.identifier.reponame.spa.fl_str_mv Repositorio Institucional Universidad Nacional de Colombia
dc.identifier.repourl.spa.fl_str_mv https://repositorio.unal.edu.co/
url https://repositorio.unal.edu.co/handle/unal/79828
https://repositorio.unal.edu.co/
identifier_str_mv Universidad Nacional de Colombia
Repositorio Institucional Universidad Nacional de Colombia
dc.language.iso.spa.fl_str_mv eng
language eng
dc.relation.references.spa.fl_str_mv [1] HFLAV, Y. Amhis et al., Averages of b-hadron, c-hadron, and -lepton properties as of summer 2016, Eur. Phys. J. C 77 (2017) 895, arXiv:1612.07233.
[2] LHCb, R. Aaij et al., Observation of CP Violation in Charm Decays, Phys. Rev. Lett. 122 (2019) 211803, arXiv:1903.08726.
[3] Particle Data Group, P. A. Zyla et al., Review of Particle Physics, PTEP 2020 (2020) 083C01.
[4] R. H. Dalitz, The puzzle, AIP Conf. Proc. 300 (1994) 141.
[5] S. U. Chung et al., Partial wave analysis in K matrix formalism, Annalen Phys. 4 (1995) 404.
[6] I. Bediaga et al., On a CP anisotropy measurement in the Dalitz plot, Phys. Rev. D 80 (2009) 096006, arXiv:0905.4233.
[7] I. Bediaga et al., Second Generation of Miranda Procedure for CP Violation in Dalitz Studies of B (n& D n& ntau) Decays, Phys. Rev. D 86 (2012) 036005, arXiv:1205.3036.
[8] M. S. Sozzi, Discrete symmetries and CP violation: From experiment to theory, 2008.
[9] Fayyazuddin and Riazuddin, Modern introduction to particle physics, World Scienti c, River Edge, N.J, 2012.
[10] T. D. Lee and C.-N. Yang, Question of Parity Conservation in Weak Interactions, Phys. Rev. 104 (1956) 254.
[11] C. S. Wu et al., Experimental Test of Parity Conservation in Decay, Phys. Rev. 105 (1957) 1413.
[12] R. L. Garwin, L. M. Lederman, and M. Weinrich, Observations of the Failure of Conservation of Parity and Charge Conjugation in Meson Decays: The Magnetic Moment Bibliography 65 of the Free Muon, Phys. Rev. 105 (1957) 1415.
[13] L. Hadjiivanov, Neutrino, parity violaton, V-A: a historical survey, arXiv:1812.11629.
[14] G. Costa and G. Fogli, Symmetries and group theory in particle physics. An introduction to space-time and internal symmetries, vol. 823, 2012.
[15] M. Gell-Mann, The Eightfold Way: A Theory of strong interaction symmetry, .
[16] C.-N. Yang and R. L. Mills, Isotopic spin conservation and a generalized gauge invariance, .
[17] E. Fermi, Tentativo di una teoria dellemissione dei raggi beta, Ric. Sci. 4 (1933) 491.
[18] F. L. Wilson, Fermis Theory of Beta Decay, Am. J. Phys. 36 (1968) 1150.
[19] Gargamelle Neutrino, F. J. Hasert et al., Observation of Neutrino Like Interactions Without Muon Or Electron in the Gargamelle Neutrino Experiment, Phys. Lett. B 46 (1973) 138.
[20] M. D. Schwartz, Quantum Field Theory and the Standard Model, Cambridge University Press, 2014.
[21] A. Pich, Electroweak Symmetry Breaking and the Higgs Boson, Acta Phys. Polon. B 47 (2016) 151, arXiv:1512.08749.
[22] Y. H. Ahn, H.-Y. Cheng, and S. Oh, Wolfenstein Parametrization at Higher Order: Seeming Discrepancies and Their Resolution, Phys. Lett. B 703 (2011) 571, arXiv:1106.0935.
[23] CKM tter Group, J. Charles et al., CP violation and the CKM matrix: Assessing the impact of the asymmetric B factories, Eur. Phys. J. C 41 (2005) 1, arXiv:hep-ph/0406184.
[24] J. H. Christenson, J. W. Cronin, V. L. Fitch, and R. Turlay, Evidence for the 2 Decay of the K0 2 Meson, Phys. Rev. Lett. 13 (1964) 138.
[25] NA31, H. Burkhardt et al., First Evidence for Direct CP Violation, Phys. Lett. B 206 (1988) 169.
[26] BaBar, B. Aubert et al., Evidence for D0 D0 Mixing, Phys. Rev. Lett. 98 (2007) 211802, arXiv:hep-ex/0703020.
[27] BELLE, M. Staric et al., Evidence for D0 - D0 Mixing, Phys. Rev. Lett. 98 (2007) 211803, arXiv:hep-ex/0703036.
[28] CDF, T. Aaltonen et al., Evidence for D0 D0 mixing using the CDF II Detector, Phys. Rev. Lett. 100 (2008) 121802, arXiv:0712.1567.
[29] LHCb, R. Aaij et al., Observation of D0 D0 oscillations, Phys. Rev. Lett. 110 (2013) 101802, arXiv:1211.1230.
[30] BaBar, B. Aubert et al., Observation of CP violation in the B0 meson system, Phys. Rev. Lett. 87 (2001) 091801, arXiv:hep-ex/0107013.
[31] Belle, K. Abe et al., Observation of large CP violation in the neutral B meson system, Phys. Rev. Lett. 87 (2001) 091802, arXiv:hep-ex/0107061.
[32] BaBar, B. Aubert et al., Observation of direct CP violation in B0 ! K+ decays, Phys. Rev. Lett. 93 (2004) 131801, arXiv:hep-ex/0407057.
[33] Belle, Y. Chao et al., Evidence for direct CP violation in B0 |> K+ pi- decays, Phys. Rev. Lett. 93 (2004) 191802, arXiv:hep-ex/0408100.
[34] BaBar, P. del Amo Sanchez et al., Measurement of CP observables in B+> DCPK+ decays and constraints on the CKM angle , Phys. Rev. D 82 (2010) 072004, arXiv:1007.0504.
[35] Belle, A. Poluektov et al., Evidence for direct CP violation in the decay B->D(*)K, D->KsPi+Pi- and measurement of the CKM phase phi3, Phys. Rev. D 81 (2010) 112002, arXiv:1003.3360.
[36] LHCb, R. Aaij et al., Observation of CP violation in B ! DK decays, Phys. Lett. B 712 (2012) 203, arXiv:1203.3662, [Erratum: Phys.Lett.B 713, 351 (2012)].
[37] LHCb, R. Aaij et al., First observation of CP violation in the decays of B0 s mesons, Phys. Rev. Lett. 110 (2013) 221601, arXiv:1304.6173.
[38] LHCb, R. Aaij et al., Measurements of CP violation in the three-body phase space of charmless B decays, Phys. Rev. D 90 (2014) 112004, arXiv:1408.5373.
[39] LHCb, R. Aaij et al., Amplitude analysis of B ! K+K decays, Phys. Rev. Lett. 123 (2019) 231802, arXiv:1905.09244.
[40] C. Zemach, Use of angular momentum tensors, Phys. Rev. 140 (1965) B97.
[41] J. M. Blatt and V. F. Weisskopf, Theoretical nuclear physics, Springer, New York, 1952.
[42] F. Giacosa and G. Pagliara, On the spectral functions of scalar mesons, Phys. Rev. C 76 (2007) 065204, arXiv:0707.3594.
[43] J. R. Pelaez, Light scalars as tetraquarks or two-meson states from large N(c) and unitarized chiral perturbation theory, Mod. Phys. Lett. A 19 (2004) 2879, arXiv:hep-ph/0411107.
[44] LHCb, R. Aaij et al., Search for CP violation in D+ ! KK+ + decays, Phys. Rev. D 84 (2011) 112008, arXiv:1110.3970.
[45] LHCb, J. Alves, A.~Augusto et al., The LHCb Detector at the LHC, JINST 3 (2008) S08005.
[46] LHCb, R. Aaij et al., LHCb Detector Performance, Int. J. Mod. Phys. A 30 (2015) 1530022, arXiv:1412.6352.
[47] R. Aaij et al., Performance of the LHCb Vertex Locator, JINST 9 (2014) P09007, arXiv:1405.7808.
[48] LHCb Outer Tracker Group, P. dArgent et al., Improved performance of the LHCb Outer Tracker in LHC Run 2, JINST 12 (2017) P11016, arXiv:1708.00819.
[49] LHCb RICH Group, M. Adinol et al., Performance of the LHCb RICH detector at the LHC, Eur. Phys. J. C 73 (2013) 2431, arXiv:1211.6759.
[50] J. Alves, A.~A. et al., Performance of the LHCb muon system, JINST 8 (2013) P02022, arXiv:1211.1346.
[51] R. Aaij et al., The LHCb Trigger and its Performance in 2011, JINST 8 (2013) P04022, arXiv:1211.3055.
[52] J. Back et al., LAURA++: A Dalitz plot fitter, Comput. Phys. Commun. 231 (2018) 198, arXiv:1711.09854.
[53] R. Brun and F. Rademakers, ROOT - An Object Oriented Data Analysis Framework, Nucl. Inst. Meth. in Phys. Res. A 389 (1997) 81, See also ROOT [software], Release v6.18/02, 23/08/2019.
[54] CLEO, P. Rubin et al., Search for CP Violation in the Dalitz-Plot Analysis of D+- |> K+ K- pi+-, Phys. Rev. D 78 (2008) 072003, arXiv:0807.4545.
[55] G. Choudalakis and D. Casadei, Plotting the Differences Between Data and Expectation, Eur. Phys. J. Plus 127 (2012) 25, arXiv:1111.2062.
dc.rights.spa.fl_str_mv Derechos reservados del autor
dc.rights.coar.fl_str_mv http://purl.org/coar/access_right/c_abf2
dc.rights.license.spa.fl_str_mv Atribución-NoComercial-SinDerivadas 4.0 Internacional
dc.rights.uri.spa.fl_str_mv http://creativecommons.org/licenses/by-nc-nd/4.0/
dc.rights.accessrights.spa.fl_str_mv info:eu-repo/semantics/openAccess
rights_invalid_str_mv Atribución-NoComercial-SinDerivadas 4.0 Internacional
Derechos reservados del autor
http://creativecommons.org/licenses/by-nc-nd/4.0/
http://purl.org/coar/access_right/c_abf2
eu_rights_str_mv openAccess
dc.format.extent.spa.fl_str_mv 80 páginas
dc.format.mimetype.spa.fl_str_mv application/pdf
dc.publisher.spa.fl_str_mv Universidad Nacional de Colombia
dc.publisher.program.spa.fl_str_mv Bogotá - Ciencias - Maestría en Ciencias - Física
dc.publisher.department.spa.fl_str_mv Departamento de Física
dc.publisher.faculty.spa.fl_str_mv Facultad de Ciencias
dc.publisher.place.spa.fl_str_mv Bogotá, Colombia
dc.publisher.branch.spa.fl_str_mv Universidad Nacional de Colombia - Sede Bogotá
institution Universidad Nacional de Colombia
bitstream.url.fl_str_mv https://repositorio.unal.edu.co/bitstream/unal/79828/1/license.txt
https://repositorio.unal.edu.co/bitstream/unal/79828/2/Tesis-Sergio-Jaimes.pdf
https://repositorio.unal.edu.co/bitstream/unal/79828/3/Tesis-Sergio-Jaimes.pdf.jpg
bitstream.checksum.fl_str_mv cccfe52f796b7c63423298c2d3365fc6
bcbc134923a812053f4c4ef01d54bf74
f42fa2eec74e39e183f881b995726271
bitstream.checksumAlgorithm.fl_str_mv MD5
MD5
MD5
repository.name.fl_str_mv Repositorio Institucional Universidad Nacional de Colombia
repository.mail.fl_str_mv repositorio_nal@unal.edu.co
_version_ 1814089873213095936
spelling Atribución-NoComercial-SinDerivadas 4.0 InternacionalDerechos reservados del autorhttp://creativecommons.org/licenses/by-nc-nd/4.0/info:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2Milanés Carreño, Diego Alejandro0cb1fc6bacb170f2b17b9f31777bf004Jaimes Elles, Sergio Javier6329671df887f00d878de35aadcce923Grupo de Partículas FENYX-UN2021-07-21T21:12:08Z2021-07-21T21:12:08Z2021https://repositorio.unal.edu.co/handle/unal/79828Universidad Nacional de ColombiaRepositorio Institucional Universidad Nacional de Colombiahttps://repositorio.unal.edu.co/ilustraciones, diagramasIn the study of decays of mesons to three body nal states the Dalitz plot analysis is a standard tool for the description of the phase space and CP violation searches in the quark sector. The technique applied for the study of these decays often depends on the model used for the description of the dynamics of the intermediate states. As an alternative, the Miranda procedure is used as a model independent method for detection of CP violation in decays of mesons. In this work we perform sensitivity studies using the Miranda procedure for the detection of CP violation on the decay D+ -> K-K+\pi+, using Monte Carlo generated samples. (Text taken from source)En el estudio de la desintegración de mesones en tres estados finales los diagramas Dalitz son una herramienta estandar para la descripción del espacio de fase y busquedas de violación CP en interacciones del sector de quarks. La tecnica usada para el estudio de estas desintegraciones a menudo depende del modelo usado para la descripción de la dinámica de los estados intermedios. Como una alternativa, el procedimiento de Miranda es usado como un método independiente del modelo para la detección de violación CP en desintegración de mesones. En este trabajo se realizó un estudio de sensibilidad a la detección de violación CP usando el procedimiento de Miranda en la desintegración D+ -> K-K+\pi+, usando muestras generadas por Monte Carlo. (Texto tomado de la fuente)MaestríaMagíster en Ciencias - FísicaFísica de partículas experimental80 páginasapplication/pdfengUniversidad Nacional de ColombiaBogotá - Ciencias - Maestría en Ciencias - FísicaDepartamento de FísicaFacultad de CienciasBogotá, ColombiaUniversidad Nacional de Colombia - Sede Bogotá530 - FísicaMesonesVIOLACION DE LA PARIDAD DE CONJUGACION DE CARGADecayCP violationDalitz PlotCharm quarkSensitivityStandard ModelMiranda ProcedureDesintegraciónViolacion CPFigura de DalitzQuark encantadoSensibilidadModelo EstándarProcedimiento de MirandaA model independent study of sensitivity to CP violation in decays of charmed mesons to three-body final statesUn estudio independiente del modelo de sensibilidad a violación CP en desintegraciones de mesones encantados a tres estados finalesTrabajo de grado - Maestríainfo:eu-repo/semantics/masterThesisinfo:eu-repo/semantics/acceptedVersionTexthttp://purl.org/redcol/resource_type/TM[1] HFLAV, Y. Amhis et al., Averages of b-hadron, c-hadron, and -lepton properties as of summer 2016, Eur. Phys. J. C 77 (2017) 895, arXiv:1612.07233.[2] LHCb, R. Aaij et al., Observation of CP Violation in Charm Decays, Phys. Rev. Lett. 122 (2019) 211803, arXiv:1903.08726.[3] Particle Data Group, P. A. Zyla et al., Review of Particle Physics, PTEP 2020 (2020) 083C01.[4] R. H. Dalitz, The puzzle, AIP Conf. Proc. 300 (1994) 141.[5] S. U. Chung et al., Partial wave analysis in K matrix formalism, Annalen Phys. 4 (1995) 404.[6] I. Bediaga et al., On a CP anisotropy measurement in the Dalitz plot, Phys. Rev. D 80 (2009) 096006, arXiv:0905.4233.[7] I. Bediaga et al., Second Generation of Miranda Procedure for CP Violation in Dalitz Studies of B (n& D n& ntau) Decays, Phys. Rev. D 86 (2012) 036005, arXiv:1205.3036.[8] M. S. Sozzi, Discrete symmetries and CP violation: From experiment to theory, 2008.[9] Fayyazuddin and Riazuddin, Modern introduction to particle physics, World Scienti c, River Edge, N.J, 2012.[10] T. D. Lee and C.-N. Yang, Question of Parity Conservation in Weak Interactions, Phys. Rev. 104 (1956) 254.[11] C. S. Wu et al., Experimental Test of Parity Conservation in Decay, Phys. Rev. 105 (1957) 1413.[12] R. L. Garwin, L. M. Lederman, and M. Weinrich, Observations of the Failure of Conservation of Parity and Charge Conjugation in Meson Decays: The Magnetic Moment Bibliography 65 of the Free Muon, Phys. Rev. 105 (1957) 1415.[13] L. Hadjiivanov, Neutrino, parity violaton, V-A: a historical survey, arXiv:1812.11629.[14] G. Costa and G. Fogli, Symmetries and group theory in particle physics. An introduction to space-time and internal symmetries, vol. 823, 2012.[15] M. Gell-Mann, The Eightfold Way: A Theory of strong interaction symmetry, .[16] C.-N. Yang and R. L. Mills, Isotopic spin conservation and a generalized gauge invariance, .[17] E. Fermi, Tentativo di una teoria dellemissione dei raggi beta, Ric. Sci. 4 (1933) 491.[18] F. L. Wilson, Fermis Theory of Beta Decay, Am. J. Phys. 36 (1968) 1150.[19] Gargamelle Neutrino, F. J. Hasert et al., Observation of Neutrino Like Interactions Without Muon Or Electron in the Gargamelle Neutrino Experiment, Phys. Lett. B 46 (1973) 138.[20] M. D. Schwartz, Quantum Field Theory and the Standard Model, Cambridge University Press, 2014.[21] A. Pich, Electroweak Symmetry Breaking and the Higgs Boson, Acta Phys. Polon. B 47 (2016) 151, arXiv:1512.08749.[22] Y. H. Ahn, H.-Y. Cheng, and S. Oh, Wolfenstein Parametrization at Higher Order: Seeming Discrepancies and Their Resolution, Phys. Lett. B 703 (2011) 571, arXiv:1106.0935.[23] CKM tter Group, J. Charles et al., CP violation and the CKM matrix: Assessing the impact of the asymmetric B factories, Eur. Phys. J. C 41 (2005) 1, arXiv:hep-ph/0406184.[24] J. H. Christenson, J. W. Cronin, V. L. Fitch, and R. Turlay, Evidence for the 2 Decay of the K0 2 Meson, Phys. Rev. Lett. 13 (1964) 138.[25] NA31, H. Burkhardt et al., First Evidence for Direct CP Violation, Phys. Lett. B 206 (1988) 169.[26] BaBar, B. Aubert et al., Evidence for D0 D0 Mixing, Phys. Rev. Lett. 98 (2007) 211802, arXiv:hep-ex/0703020.[27] BELLE, M. Staric et al., Evidence for D0 - D0 Mixing, Phys. Rev. Lett. 98 (2007) 211803, arXiv:hep-ex/0703036.[28] CDF, T. Aaltonen et al., Evidence for D0 D0 mixing using the CDF II Detector, Phys. Rev. Lett. 100 (2008) 121802, arXiv:0712.1567.[29] LHCb, R. Aaij et al., Observation of D0 D0 oscillations, Phys. Rev. Lett. 110 (2013) 101802, arXiv:1211.1230.[30] BaBar, B. Aubert et al., Observation of CP violation in the B0 meson system, Phys. Rev. Lett. 87 (2001) 091801, arXiv:hep-ex/0107013.[31] Belle, K. Abe et al., Observation of large CP violation in the neutral B meson system, Phys. Rev. Lett. 87 (2001) 091802, arXiv:hep-ex/0107061.[32] BaBar, B. Aubert et al., Observation of direct CP violation in B0 ! K+ decays, Phys. Rev. Lett. 93 (2004) 131801, arXiv:hep-ex/0407057.[33] Belle, Y. Chao et al., Evidence for direct CP violation in B0 |> K+ pi- decays, Phys. Rev. Lett. 93 (2004) 191802, arXiv:hep-ex/0408100.[34] BaBar, P. del Amo Sanchez et al., Measurement of CP observables in B+> DCPK+ decays and constraints on the CKM angle , Phys. Rev. D 82 (2010) 072004, arXiv:1007.0504.[35] Belle, A. Poluektov et al., Evidence for direct CP violation in the decay B->D(*)K, D->KsPi+Pi- and measurement of the CKM phase phi3, Phys. Rev. D 81 (2010) 112002, arXiv:1003.3360.[36] LHCb, R. Aaij et al., Observation of CP violation in B ! DK decays, Phys. Lett. B 712 (2012) 203, arXiv:1203.3662, [Erratum: Phys.Lett.B 713, 351 (2012)].[37] LHCb, R. Aaij et al., First observation of CP violation in the decays of B0 s mesons, Phys. Rev. Lett. 110 (2013) 221601, arXiv:1304.6173.[38] LHCb, R. Aaij et al., Measurements of CP violation in the three-body phase space of charmless B decays, Phys. Rev. D 90 (2014) 112004, arXiv:1408.5373.[39] LHCb, R. Aaij et al., Amplitude analysis of B ! K+K decays, Phys. Rev. Lett. 123 (2019) 231802, arXiv:1905.09244.[40] C. Zemach, Use of angular momentum tensors, Phys. Rev. 140 (1965) B97.[41] J. M. Blatt and V. F. Weisskopf, Theoretical nuclear physics, Springer, New York, 1952.[42] F. Giacosa and G. Pagliara, On the spectral functions of scalar mesons, Phys. Rev. C 76 (2007) 065204, arXiv:0707.3594.[43] J. R. Pelaez, Light scalars as tetraquarks or two-meson states from large N(c) and unitarized chiral perturbation theory, Mod. Phys. Lett. A 19 (2004) 2879, arXiv:hep-ph/0411107.[44] LHCb, R. Aaij et al., Search for CP violation in D+ ! KK+ + decays, Phys. Rev. D 84 (2011) 112008, arXiv:1110.3970.[45] LHCb, J. Alves, A.~Augusto et al., The LHCb Detector at the LHC, JINST 3 (2008) S08005.[46] LHCb, R. Aaij et al., LHCb Detector Performance, Int. J. Mod. Phys. A 30 (2015) 1530022, arXiv:1412.6352.[47] R. Aaij et al., Performance of the LHCb Vertex Locator, JINST 9 (2014) P09007, arXiv:1405.7808.[48] LHCb Outer Tracker Group, P. dArgent et al., Improved performance of the LHCb Outer Tracker in LHC Run 2, JINST 12 (2017) P11016, arXiv:1708.00819.[49] LHCb RICH Group, M. Adinol et al., Performance of the LHCb RICH detector at the LHC, Eur. Phys. J. C 73 (2013) 2431, arXiv:1211.6759.[50] J. Alves, A.~A. et al., Performance of the LHCb muon system, JINST 8 (2013) P02022, arXiv:1211.1346.[51] R. Aaij et al., The LHCb Trigger and its Performance in 2011, JINST 8 (2013) P04022, arXiv:1211.3055.[52] J. Back et al., LAURA++: A Dalitz plot fitter, Comput. Phys. Commun. 231 (2018) 198, arXiv:1711.09854.[53] R. Brun and F. Rademakers, ROOT - An Object Oriented Data Analysis Framework, Nucl. Inst. Meth. in Phys. Res. A 389 (1997) 81, See also ROOT [software], Release v6.18/02, 23/08/2019.[54] CLEO, P. Rubin et al., Search for CP Violation in the Dalitz-Plot Analysis of D+- |> K+ K- pi+-, Phys. Rev. D 78 (2008) 072003, arXiv:0807.4545.[55] G. Choudalakis and D. Casadei, Plotting the Differences Between Data and Expectation, Eur. Phys. J. Plus 127 (2012) 25, arXiv:1111.2062.EspecializadaLICENSElicense.txtlicense.txttext/plain; charset=utf-83964https://repositorio.unal.edu.co/bitstream/unal/79828/1/license.txtcccfe52f796b7c63423298c2d3365fc6MD51ORIGINALTesis-Sergio-Jaimes.pdfTesis-Sergio-Jaimes.pdfTesis de Maestría en Ciencias, Físicaapplication/pdf4221887https://repositorio.unal.edu.co/bitstream/unal/79828/2/Tesis-Sergio-Jaimes.pdfbcbc134923a812053f4c4ef01d54bf74MD52THUMBNAILTesis-Sergio-Jaimes.pdf.jpgTesis-Sergio-Jaimes.pdf.jpgGenerated Thumbnailimage/jpeg4567https://repositorio.unal.edu.co/bitstream/unal/79828/3/Tesis-Sergio-Jaimes.pdf.jpgf42fa2eec74e39e183f881b995726271MD53unal/79828oai:repositorio.unal.edu.co:unal/798282023-07-24 23:03:56.861Repositorio Institucional Universidad Nacional de Colombiarepositorio_nal@unal.edu.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