{"id":1566,"date":"2021-05-02T17:54:29","date_gmt":"2021-05-02T17:54:29","guid":{"rendered":"https:\/\/km3net.ific.uv.es\/?page_id=1566"},"modified":"2025-07-30T17:00:15","modified_gmt":"2025-07-30T15:00:15","slug":"particle-and-neutrino-physics","status":"publish","type":"page","link":"https:\/\/km3net.ific.uv.es\/km3net\/research\/particle-and-neutrino-physics\/","title":{"rendered":"Particle and Neutrino Physics"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-page\" data-elementor-id=\"1566\" class=\"elementor elementor-1566\">\n\t\t\t\t\t\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-39182562 elementor-hidden-tablet elementor-hidden-phone elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"39182562\" data-element_type=\"section\" data-settings=\"{&quot;jet_parallax_layout_list&quot;:[{&quot;jet_parallax_layout_image&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;_id&quot;:&quot;6b99772&quot;,&quot;jet_parallax_layout_image_tablet&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;jet_parallax_layout_image_mobile&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;jet_parallax_layout_speed&quot;:{&quot;unit&quot;:&quot;%&quot;,&quot;size&quot;:50,&quot;sizes&quot;:[]},&quot;jet_parallax_layout_type&quot;:&quot;scroll&quot;,&quot;jet_parallax_layout_direction&quot;:null,&quot;jet_parallax_layout_fx_direction&quot;:null,&quot;jet_parallax_layout_z_index&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_x&quot;:50,&quot;jet_parallax_layout_bg_x_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_x_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_y&quot;:50,&quot;jet_parallax_layout_bg_y_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_y_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_size&quot;:&quot;auto&quot;,&quot;jet_parallax_layout_bg_size_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_size_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_animation_prop&quot;:&quot;transform&quot;,&quot;jet_parallax_layout_on&quot;:[&quot;desktop&quot;,&quot;tablet&quot;]}]}\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-410d8ac3\" data-id=\"410d8ac3\" data-element_type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t\t\t<div class=\"elementor-element elementor-element-30b28d05 elementor-hidden-tablet elementor-hidden-phone elementor-widget elementor-widget-spacer\" data-id=\"30b28d05\" data-element_type=\"widget\" data-widget_type=\"spacer.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<div class=\"elementor-spacer\">\n\t\t\t<div class=\"elementor-spacer-inner\"><\/div>\n\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-63f56970 elementor-hidden-tablet elementor-hidden-phone elementor-widget elementor-widget-spacer\" data-id=\"63f56970\" data-element_type=\"widget\" data-widget_type=\"spacer.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<div class=\"elementor-spacer\">\n\t\t\t<div class=\"elementor-spacer-inner\"><\/div>\n\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-7d36ecd5 elementor-section-boxed elementor-section-height-default elementor-section-height-default elementor-invisible\" data-id=\"7d36ecd5\" data-element_type=\"section\" data-settings=\"{&quot;jet_parallax_layout_list&quot;:[{&quot;jet_parallax_layout_image&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;_id&quot;:&quot;3699b0b&quot;,&quot;jet_parallax_layout_image_tablet&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;jet_parallax_layout_image_mobile&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;jet_parallax_layout_speed&quot;:{&quot;unit&quot;:&quot;%&quot;,&quot;size&quot;:50,&quot;sizes&quot;:[]},&quot;jet_parallax_layout_type&quot;:&quot;scroll&quot;,&quot;jet_parallax_layout_direction&quot;:null,&quot;jet_parallax_layout_fx_direction&quot;:null,&quot;jet_parallax_layout_z_index&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_x&quot;:50,&quot;jet_parallax_layout_bg_x_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_x_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_y&quot;:50,&quot;jet_parallax_layout_bg_y_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_y_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_size&quot;:&quot;auto&quot;,&quot;jet_parallax_layout_bg_size_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_size_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_animation_prop&quot;:&quot;transform&quot;,&quot;jet_parallax_layout_on&quot;:[&quot;desktop&quot;,&quot;tablet&quot;]}],&quot;animation&quot;:&quot;fadeIn&quot;,&quot;background_background&quot;:&quot;classic&quot;}\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-41d08c5\" data-id=\"41d08c5\" data-element_type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t\t\t<div class=\"elementor-element elementor-element-1cfd041c elementor-widget elementor-widget-heading\" data-id=\"1cfd041c\" data-element_type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">Research<\/h2>\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-297e7ef4 elementor-section-boxed elementor-section-height-default elementor-section-height-default elementor-invisible\" data-id=\"297e7ef4\" data-element_type=\"section\" data-settings=\"{&quot;jet_parallax_layout_list&quot;:[{&quot;jet_parallax_layout_image&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;_id&quot;:&quot;3699b0b&quot;,&quot;jet_parallax_layout_image_tablet&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;jet_parallax_layout_image_mobile&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;jet_parallax_layout_speed&quot;:{&quot;unit&quot;:&quot;%&quot;,&quot;size&quot;:50,&quot;sizes&quot;:[]},&quot;jet_parallax_layout_type&quot;:&quot;scroll&quot;,&quot;jet_parallax_layout_direction&quot;:null,&quot;jet_parallax_layout_fx_direction&quot;:null,&quot;jet_parallax_layout_z_index&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_x&quot;:50,&quot;jet_parallax_layout_bg_x_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_x_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_y&quot;:50,&quot;jet_parallax_layout_bg_y_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_y_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_size&quot;:&quot;auto&quot;,&quot;jet_parallax_layout_bg_size_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_size_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_animation_prop&quot;:&quot;transform&quot;,&quot;jet_parallax_layout_on&quot;:[&quot;desktop&quot;,&quot;tablet&quot;]}],&quot;animation&quot;:&quot;fadeIn&quot;}\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-79e47638\" data-id=\"79e47638\" data-element_type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t\t\t<div class=\"elementor-element elementor-element-6205a761 elementor-widget elementor-widget-image\" data-id=\"6205a761\" data-element_type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img width=\"182\" height=\"183\" src=\"https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/2021\/03\/Particle-2.jpg\" class=\"attachment-large size-large wp-image-1063\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/2021\/03\/Particle-2.jpg 182w, https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/2021\/03\/Particle-2-150x150.jpg 150w\" sizes=\"(max-width: 182px) 100vw, 182px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-73e7e918\" data-id=\"73e7e918\" data-element_type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t\t\t<div class=\"elementor-element elementor-element-2d720ccd elementor-widget elementor-widget-heading\" data-id=\"2d720ccd\" data-element_type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">Particle and Neutrino Physics<\/h2>\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-33a104f7 elementor-widget elementor-widget-text-editor\" data-id=\"33a104f7\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\tNeutrino telescopes such as KM3NeT not only use neutrinos as a tool to study astrophysical objects and other physics phenomena such as dark matter, but can also help to investigate neutrino properties and look for possible extensions of the Standard Model of Particle Physics (SM).\n<br><br>\nThe atmosphere is a copious source of neutrinos. These atmospheric neutrinos are in general a hindrance for astrophysical studies, but can provide very useful information about neutrinos themselves and the phenomenon of neutrino oscillations. In fact, atmospheric neutrinos played a key role in the discovery and understanding of this phenomenon.  \n<br><br>\nAtmospheric neutrinos cover a very wide range of energies and baselines (distances from source to detector) and therefore have a great potential to observe possible deviations from their expected behaviour in the SM.  Our research group is involved in the measurement  of the parameters that describe standard neutrino oscillations and the search for phenomena predicted in a variety of scenarios which go beyond the Standard Model. \n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-9f4d62f elementor-section-boxed elementor-section-height-default elementor-section-height-default elementor-invisible\" data-id=\"9f4d62f\" data-element_type=\"section\" data-settings=\"{&quot;jet_parallax_layout_list&quot;:[{&quot;jet_parallax_layout_image&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;_id&quot;:&quot;3699b0b&quot;,&quot;jet_parallax_layout_image_tablet&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;jet_parallax_layout_image_mobile&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;jet_parallax_layout_speed&quot;:{&quot;unit&quot;:&quot;%&quot;,&quot;size&quot;:50,&quot;sizes&quot;:[]},&quot;jet_parallax_layout_type&quot;:&quot;scroll&quot;,&quot;jet_parallax_layout_direction&quot;:null,&quot;jet_parallax_layout_fx_direction&quot;:null,&quot;jet_parallax_layout_z_index&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_x&quot;:50,&quot;jet_parallax_layout_bg_x_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_x_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_y&quot;:50,&quot;jet_parallax_layout_bg_y_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_y_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_size&quot;:&quot;auto&quot;,&quot;jet_parallax_layout_bg_size_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_size_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_animation_prop&quot;:&quot;transform&quot;,&quot;jet_parallax_layout_on&quot;:[&quot;desktop&quot;,&quot;tablet&quot;]}],&quot;animation&quot;:&quot;fadeIn&quot;}\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-88c0b9a\" data-id=\"88c0b9a\" data-element_type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t\t\t<div class=\"elementor-element elementor-element-482cfda elementor-widget elementor-widget-text-editor\" data-id=\"482cfda\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\tKM3NeT has recently published the measurement of some key oscillation parameters with the ORCA6 detector, a configuration of KM3NeT\/ORCA that contains six detector units<sup>[1]<\/sup>. Despite the small size of ORCA6 compared to its final configuration (5% of the full ORCA) and limited recording time (540 days) the results are already close to those of other experiments, as can be seen in the following figure, where the 90% CL contours for the parameters sin<sup>2<\/sup>\u03b8<sub>23<\/sub> and \u0394m<sup>2<\/sup><sub>32<\/sub> from ORCA6 (in black) are shown together with those from other experiments:\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-9bc63d9 elementor-widget elementor-widget-image\" data-id=\"9bc63d9\" data-element_type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img src=\"https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/elementor\/thumbs\/Captura-de-pantalla-de-2025-04-01-17-16-37-r3q2is4afugryldhpnp1mojezfkk1shi8244nye6rk.png\" title=\"JHEP10(2024)206_ORCA6_limits\" alt=\"JHEP10(2024)206_ORCA6_limits\" loading=\"lazy\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-6de18a9 elementor-widget elementor-widget-text-editor\" data-id=\"6de18a9\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\tNew data with larger configurations of ORCA are readily available and we are presently studying them, so that our precision on these parameters will soon improve.\n\n<br><br>\n\nSome theories posit the existence of interactions not included in the SM. These \u201cnon-standard\u201d neutrino interactions that could come from new physics at a higher energy scale would change the shape of the spectrum of atmospheric neutrinos. We have studied the possibility of such non-standard interactions with the ORCA6 detectors. The absence of evidence has enabled us to limit the size of the parameters that describe these interactions (\u03b5<sub>e\u03bc<\/sub>, \u03b5<sub>e\u03c4<\/sub>, \u03b5<sub>\u03bc\u03bc<\/sub>, \u03b5<sub>\u03c4\u03c4<\/sub> and \u03b5<sub>\u03bc\u03c4<\/sub>). The limits that we obtain<sup>[2]<\/sup> are of the order of the best current limits, as can be seen in the following figure:\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-0172425 elementor-widget elementor-widget-image\" data-id=\"0172425\" data-element_type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img src=\"https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/elementor\/thumbs\/Captura-de-pantalla-de-2025-04-01-17-22-19-r3q2r8nzy61og934bbc62jorg9vhbq2jdxhg5lumzm.png\" title=\"ORCA6_NSI_limits\" alt=\"ORCA6_NSI_limits\" loading=\"lazy\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-3bee539 elementor-widget elementor-widget-text-editor\" data-id=\"3bee539\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\tQuantum decoherence is the process by which a physical system&#8217;s behaviour changes from that which can be explained by quantum mechanics to classical physics and can stem from various sources, including quantum gravity effects. Quantum decoherence in the neutrino system will give rise to deviations from the standard oscillations.\n\n<br><br>\n\nAgain using ORCA6 data we have been able to set limits on several possibilities of quantum decoherence<sup>[3]<\/sup>, as can be seen in the following figure:\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-5de2685 elementor-widget elementor-widget-image\" data-id=\"5de2685\" data-element_type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img width=\"768\" height=\"358\" src=\"https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/2025\/04\/Captura-de-pantalla-de-2025-04-01-17-25-39-768x358.png\" class=\"attachment-medium_large size-medium_large wp-image-2562\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/2025\/04\/Captura-de-pantalla-de-2025-04-01-17-25-39-768x358.png 768w, https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/2025\/04\/Captura-de-pantalla-de-2025-04-01-17-25-39-300x140.png 300w, https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/2025\/04\/Captura-de-pantalla-de-2025-04-01-17-25-39-1024x478.png 1024w, https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/2025\/04\/Captura-de-pantalla-de-2025-04-01-17-25-39.png 1166w\" sizes=\"(max-width: 768px) 100vw, 768px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-a1fb3dd elementor-widget elementor-widget-text-editor\" data-id=\"a1fb3dd\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\tOur group has also searched for light sterile neutrinos. Some anomalous results from three experiments (BEST, LSND, and MiniBooNE) could be explained with an additional sterile neutrino state with a mass of the order of one MeV. The IceCube detector has been able to set limits to that possibility, as can be seen in the following plot of the parameters that describe the oscillation to this new state<sup>[4]<\/sup>:\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-266bd3c elementor-widget elementor-widget-image\" data-id=\"266bd3c\" data-element_type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img src=\"https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/elementor\/thumbs\/Captura-de-pantalla-de-2025-04-01-17-33-29-r3q38pi0ybyi7dppbd5kwn04v1s1d8eysdxa7py8zw.png\" title=\"IceCube_sterile_neutrinos\" alt=\"IceCube_sterile_neutrinos\" loading=\"lazy\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-adcaa86 elementor-widget elementor-widget-text-editor\" data-id=\"adcaa86\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\tAs this analysis indicated a mild preference (2.2\u03c3) for a light sterile neutrino in the muon-neutrino disappearance channel, a member of our research team, who participated in the IceCube\u2019s analysis, has continued it with the KM3NeT\/ARCA detector. The analysis revealed that ARCA can set competitive limits before the end of this decade.\n\n<br><br>\n\nThe ORCA detector of the KM3NeT experiment will be able to determine the neutrino mass ordering (NMO), that is, to disentangle between the two possible orderings of the neutrino mass states, i.e. normal (m<sub>1<\/sub> &lt; m<sub>2<\/sub> &lt; m<sub>3<\/sub>) or inverted (m<sub>3<\/sub> &lt; m<sub>1<\/sub> &lt; m<sub>2<\/sub>).\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-8e34c0a elementor-widget elementor-widget-image\" data-id=\"8e34c0a\" data-element_type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img width=\"482\" height=\"425\" src=\"https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/2025\/04\/llustrating-the-neutrino-mass-hierarchies-The-color-shading-indicates-the-fraction-U-ai.png\" class=\"attachment-medium_large size-medium_large wp-image-2564\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/2025\/04\/llustrating-the-neutrino-mass-hierarchies-The-color-shading-indicates-the-fraction-U-ai.png 482w, https:\/\/km3net.ific.uv.es\/wp-content\/uploads\/2025\/04\/llustrating-the-neutrino-mass-hierarchies-The-color-shading-indicates-the-fraction-U-ai-300x265.png 300w\" sizes=\"(max-width: 482px) 100vw, 482px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-ef7ec9c elementor-widget elementor-widget-text-editor\" data-id=\"ef7ec9c\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\tThe determination of the NMO with atmospheric neutrinos is based on the observation of a net difference in the event rates, resulting from a larger interaction cross section and the existing atmospheric flux difference for neutrinos with respect to antineutrinos. Due to this event rate difference, the strength of the matter effects is larger for normal ordering (NO) compared to inverted ordering (IO).\n\n<br><br>\n\nOur group is involved in the study of the determination of NMO with the KM3NeT\/ORCA detector.\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-619f390 elementor-widget elementor-widget-text-editor\" data-id=\"619f390\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t[1] \u201cMeasurement of neutrino oscillation parameters with the first six detection units of KM3NeT\/ORCA\u201d, KM3NeT coll., <i>Journal of High Energy Physics<\/i> <b>2024<\/b>, <i>206<\/i>(2024). DOI:<a href=\"https:\/\/doi.org\/10.1007\/JHEP10(2024)206\">10.1007\/JHEP10(2024)206<\/a> [<a href=\"https:\/\/arxiv.org\/abs\/2408.07015\">arXiv:2408.07015<\/a>]\n\n<br><br>\n\n[2] \u201cSearch for non-standard neutrino interactions with the first six detection units of KM3NeT\/ORCA\u201d, KM3NeT coll. [<a href=\"https:\/\/arxiv.org\/abs\/2411.19078\">arXiv:2411.19078<\/a>]\n\n<br><br>\n\n[3] \u201cSearch for quantum decoherence in neutrino oscillations with six detection units of KM3NeT\/ORCA\u201d, KM3NeT coll. [<a href=\"https:\/\/arxiv.org\/abs\/2410.01388\">arXiv:2410.01388<\/a>]\n\n<br><br>\n\n[4] \u201cSearch for an eV-Scale Sterile Neutrino Using Improved High-Energy \ud835\udf08<sub>\ud835\udf07<\/sub> Event Reconstruction in IceCube\u201d, IceCube coll., <i>Physical Review Letters<\/i> <b>2024<\/b>, <i>133<\/i>(201804). DOI:<a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.133.201804\">10.1103\/PhysRevLett.133.201804<\/a> [<a href=\"https:\/\/arxiv.org\/abs\/2405.08070\">arXiv:2405.08070<\/a>]\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-4560a30 elementor-widget elementor-widget-spacer\" data-id=\"4560a30\" data-element_type=\"widget\" data-widget_type=\"spacer.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<div class=\"elementor-spacer\">\n\t\t\t<div class=\"elementor-spacer-inner\"><\/div>\n\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-74e7b0b elementor-section-boxed elementor-section-height-default elementor-section-height-default elementor-invisible\" data-id=\"74e7b0b\" data-element_type=\"section\" data-settings=\"{&quot;jet_parallax_layout_list&quot;:[{&quot;jet_parallax_layout_image&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;_id&quot;:&quot;3699b0b&quot;,&quot;jet_parallax_layout_image_tablet&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;jet_parallax_layout_image_mobile&quot;:{&quot;url&quot;:&quot;&quot;,&quot;id&quot;:&quot;&quot;,&quot;size&quot;:&quot;&quot;},&quot;jet_parallax_layout_speed&quot;:{&quot;unit&quot;:&quot;%&quot;,&quot;size&quot;:50,&quot;sizes&quot;:[]},&quot;jet_parallax_layout_type&quot;:&quot;scroll&quot;,&quot;jet_parallax_layout_direction&quot;:null,&quot;jet_parallax_layout_fx_direction&quot;:null,&quot;jet_parallax_layout_z_index&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_x&quot;:50,&quot;jet_parallax_layout_bg_x_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_x_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_y&quot;:50,&quot;jet_parallax_layout_bg_y_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_y_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_size&quot;:&quot;auto&quot;,&quot;jet_parallax_layout_bg_size_tablet&quot;:&quot;&quot;,&quot;jet_parallax_layout_bg_size_mobile&quot;:&quot;&quot;,&quot;jet_parallax_layout_animation_prop&quot;:&quot;transform&quot;,&quot;jet_parallax_layout_on&quot;:[&quot;desktop&quot;,&quot;tablet&quot;]}],&quot;animation&quot;:&quot;fadeIn&quot;}\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-dc79736\" data-id=\"dc79736\" data-element_type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t\t\t<div class=\"elementor-element elementor-element-9fdf70e elementor-widget elementor-widget-jet-button\" data-id=\"9fdf70e\" data-element_type=\"widget\" data-widget_type=\"jet-button.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t<div class=\"elementor-jet-button jet-elements\"><div class=\"jet-button__container\">\n\t<a class=\"jet-button__instance jet-button__instance--icon-left hover-effect-1\" href=\"https:\/\/km3net.ific.uv.es\/research\/\">\n\t\t<div class=\"jet-button__plane jet-button__plane-normal\"><\/div>\n\t\t<div class=\"jet-button__plane jet-button__plane-hover\"><\/div>\n\t\t<div class=\"jet-button__state jet-button__state-normal\">\n\t\t\t<span class=\"jet-button__label\">Research<\/span>\t\t<\/div>\n\t\t<div class=\"jet-button__state jet-button__state-hover\">\n\t\t\t<span class=\"jet-button__label\">Back<\/span>\t\t<\/div>\n\t<\/a>\n<\/div>\n<\/div>\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-4e9eca2 elementor-widget elementor-widget-spacer\" data-id=\"4e9eca2\" data-element_type=\"widget\" data-widget_type=\"spacer.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<div class=\"elementor-spacer\">\n\t\t\t<div class=\"elementor-spacer-inner\"><\/div>\n\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>Research Particle and Neutrino Physics Neutrino telescopes such as KM3NeT not only use neutrinos as a tool to study astrophysical objects and other physics phenomena such as dark matter, but can also help to investigate neutrino properties and look for possible extensions of the Standard Model of Particle Physics (SM). The atmosphere is a copious [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":18,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"full-width.php","meta":[],"acf":[],"_links":{"self":[{"href":"https:\/\/km3net.ific.uv.es\/km3net\/wp-json\/wp\/v2\/pages\/1566"}],"collection":[{"href":"https:\/\/km3net.ific.uv.es\/km3net\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/km3net.ific.uv.es\/km3net\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/km3net.ific.uv.es\/km3net\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/km3net.ific.uv.es\/km3net\/wp-json\/wp\/v2\/comments?post=1566"}],"version-history":[{"count":30,"href":"https:\/\/km3net.ific.uv.es\/km3net\/wp-json\/wp\/v2\/pages\/1566\/revisions"}],"predecessor-version":[{"id":2612,"href":"https:\/\/km3net.ific.uv.es\/km3net\/wp-json\/wp\/v2\/pages\/1566\/revisions\/2612"}],"up":[{"embeddable":true,"href":"https:\/\/km3net.ific.uv.es\/km3net\/wp-json\/wp\/v2\/pages\/18"}],"wp:attachment":[{"href":"https:\/\/km3net.ific.uv.es\/km3net\/wp-json\/wp\/v2\/media?parent=1566"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}