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PMT calibration of a scintillation detector using primary scintillation

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PMT calibration of a scintillation detector using primary scintillation

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dc.contributor.author Freitas, E. D. C. es_ES
dc.contributor.author Fernandes, L. M. P. es_ES
dc.contributor.author Yahlali, N. es_ES
dc.contributor.author Perez, J. es_ES
dc.contributor.author Alvarez, V. es_ES
dc.contributor.author Borges, F. I. G. es_ES
dc.contributor.author Camargo, M. es_ES
dc.contributor.author Carcel, S. es_ES
dc.contributor.author Cebrian, S. es_ES
dc.contributor.author Esteve Bosch, Raul es_ES
dc.contributor.author Marí Romero, Antonio Francisco es_ES
dc.contributor.author Mora Mas, Francisco José es_ES
dc.contributor.author Pérez Aparicio, José Luis es_ES
dc.contributor.author Rodríguez Samaniego, Javier es_ES
dc.contributor.author Toledo Alarcón, José Francisco es_ES
dc.date.accessioned 2016-10-17T09:21:07Z
dc.date.available 2016-10-17T09:21:07Z
dc.date.issued 2015-02
dc.identifier.issn 1748-0221
dc.identifier.uri http://hdl.handle.net/10251/71899
dc.description.abstract We have studied the calibration of PMTs in scintillation detectors, inducing single electron response on the PMT from primary scintillation produced by x-ray interaction. The results agree with those obtained by the commonly used single electron response (SER) method, which uses LED light pulses to induce the PMT SER. The use of the primary scintillation for PMT calibration will be convenient in situations where the PMT is already in situ, when it becomes difficult or even impossible to apply the SER method, e.g. in commercial sealed scintillator/PMT devices. Furthermore, we have experimentally investigated the possibility of fitting the high-charge tail of the PMT SER pulse-height distribution to an exponential function, inferring the PMT gain from the inverse of the exponent. The results of the exponential fit method agree with those obtained by the SER method for pulse-height distributions resulting from an average number of around 1.0 photoelectrons reaching the first dynode per light/scintillation pulse. The SER method has higher precision and, therefore, is used in a larger number of applications. Nevertheless, the exponential fit method will be useful in situations where the single photoelectron peak is under the background or noise peak and it may present an alternative, simple way, for relative gain calibration of PMT arrays as well as for monitoring the PMT gain variations. es_ES
dc.description.sponsorship The NEXT experiment is supported by the following agencies and institutions: the European Research Funding through an ERC Advanced Grant (NEXT 2013); Ministerio de Economia y Competitividad of Spain under grants CONSOLIDER-Ingenio 2010 CSD2008- 0037 (CUP), FPA2009-13697-C04-04 and FIS2012-37947-C04; the Portuguese FCT and FEDER through program COMPETE, project PTDC/FIS/103860/2008. C.M.B. Monteiro acknowledges grant SFRH/BPD/76842/2011 from FCT. en_EN
dc.language Inglés es_ES
dc.publisher IOP Publishing es_ES
dc.relation.ispartof Journal of Instrumentation es_ES
dc.rights Reserva de todos los derechos es_ES
dc.subject Photon detectors for UV es_ES
dc.subject Visible and IR photons es_ES
dc.subject Scintillators es_ES
dc.subject Scintillation and light emission processes es_ES
dc.subject.classification MECANICA DE LOS MEDIOS CONTINUOS Y TEORIA DE ESTRUCTURAS es_ES
dc.subject.classification TECNOLOGIA ELECTRONICA es_ES
dc.title PMT calibration of a scintillation detector using primary scintillation es_ES
dc.type Artículo es_ES
dc.identifier.doi 10.1088/1748-0221/10/02/C02039
dc.relation.projectID info:eu-repo/grantAgreement/MICINN//CSD2008-00037/ES/Canfranc Underground Physics/ es_ES
dc.relation.projectID info:eu-repo/grantAgreement/J4FCT/5876-PPCDTI/103860/PT/
dc.relation.projectID info:eu-repo/grantAgreement/MICINN//FPA2009-13697-C04-04/ES/Fisica Experimental De Neutrinos En El Ific/
dc.relation.projectID info:eu-repo/grantAgreement/J4FCT/SFRH/SFRH/BPD/76842/2011/PT/
dc.relation.projectID info:eu-repo/grantAgreement/MINECO//FIS2012-37947-C04-04/ES/ADQUISICION DE DATOS Y DISEÑO MECANICO PARA EL EXPERIMENTO NEXT/
dc.relation.projectID info:eu-repo/grantAgreement/MINECO//FIS2012-37947-C04-03/ES/PROYECTO NEXT- MEDIDA DE ENERGIA Y TRAYECTORIAS/ es_ES
dc.relation.projectID info:eu-repo/grantAgreement/MINECO//FIS2012-37947-C04-01/ES/CONSTRUCCION DEL EXPERIMENTO NEXT EN EL LSC DE CANFRANC/ es_ES
dc.rights.accessRights Cerrado es_ES
dc.contributor.affiliation Universitat Politècnica de València. Departamento de Ingeniería Electrónica - Departament d'Enginyeria Electrònica es_ES
dc.contributor.affiliation Universitat Politècnica de València. Instituto de Instrumentación para Imagen Molecular - Institut d'Instrumentació per a Imatge Molecular es_ES
dc.contributor.affiliation Universitat Politècnica de València. Departamento de Mecánica de los Medios Continuos y Teoría de Estructuras - Departament de Mecànica dels Medis Continus i Teoria d'Estructures es_ES
dc.description.bibliographicCitation Freitas, EDC.; Fernandes, LMP.; Yahlali, N.; Perez, J.; Alvarez, V.; Borges, FIG.; Camargo, M.... (2015). PMT calibration of a scintillation detector using primary scintillation. Journal of Instrumentation. 10:1-9. https://doi.org/10.1088/1748-0221/10/02/C02039 es_ES
dc.description.accrualMethod S es_ES
dc.relation.publisherversion http://dx.doi.org/10.1088/1748-0221/10/02/C02039 es_ES
dc.description.upvformatpinicio 1 es_ES
dc.description.upvformatpfin 9 es_ES
dc.type.version info:eu-repo/semantics/publishedVersion es_ES
dc.description.volume 10 es_ES
dc.relation.senia 282111 es_ES
dc.contributor.funder Ministerio de Ciencia e Innovación es_ES
dc.contributor.funder Fundação para a Ciência e a Tecnologia, Portugal es_ES
dc.contributor.funder European Research Council es_ES


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