730 research outputs found
The europeanization of the interest intermediation of PASEGES between 1945 and 1967
- Publication venue
- 'National Documentation Centre (EKT)'
- Publication date
- 01/01/2016
- Field of study
The study strives to evaluate the impact of the EU on the political behavior of the Panhellenic Confederation of Unions of Agricultural Cooperatives during the largest part of the postwar period (1945-1967) with the help of a sophisticated analytical model, built around the Europeanization approach.The dissertation, more specifically, intends to contribute in an original and constructive manner to the production of knowledge in the field of European Studies by:-focusing on the considerably understudied european dimension of the interest intermediation of the hellenic agricultural movement (especially in a pre-accession context).-contributing to the academic discussion over the complex ontology of Europeanization through the development of a universally applicable definition of the phenomenon, expected to lay the foundation for the operationalization of said concept in its four basic dimensions (top-town – horizontal and bottom-up/ internal and external) within elaborate research projects.-further refining definitions of key concepts in the realm of group theory (e.g. EU lobbying).-enriching the bibliography on the Europeanization of the collective action of interest groups (especially agricultural), with new empirical evidence.The study’s research program, as well as other theoretical and methodological tools and approaches, are expected to further promote the analysis.Inter alia we decided to:-adopt a maximalist version of the concept of interest intermediation, in order to cover both internal as well as external aspects of PASEGES’s political presence (e.g. information and education policy, internal organizational structure and human resources management; relations to politicians, public servants, international organizations).-develop an eclectic model, employed to further enhance the analytical strength of Europeanization through the use of additional theoretical approaches (e.g. neofuntionalism, liberal intergovernmentalism), to some extent contradictory, but not overall incompatible.-make use of the methodological tool of the ‘theoretically informed comparative case study)’, in order to increase the validity and credibility of our empirical findings as far as the extent of the EU impact and the ‘relative importance’ of the EU are concerned.Among the main theoretical and empirical findings of the dissertation are the following:-It is possible to adopt an erga omnes definition of Europeanization and there exist analytical and methodological tools that, based on this definition, allow for the complete operationalization of the approach both in a pre- and a post-accession environment.-Between 1945 and 1967 the political bevahior of the Confederation becomes extensively europeanized. However, it is not always clear whether change is superficial or substantial as well as constrained to the multi-level (elected/ bureaucratic) leadership or equally affecting the rank-and-file.-The study of pre- and proto-EU Europeanization processes, where research is at an infant stage, has to be intensified. Respectively, the elaboration of complex research agendas, which examine such phenomena in their four fundamental dimensions, is deemed particularly useful.Η μελέτη επιχειρεί να αποτιμήσει τον κοινοτικό αντίκτυπο στην πολιτική συμπεριφορά της Πανελλήνιας Συνομοσπονδίας Ενώσεων Γεωργικών Συνεταιρισμών στο μεγαλύτερο διάστημα της μεταπολεμικής περιόδου (1945-1967) με τη βοήθεια ενός σύνθετου αναλυτικού μοντέλου, δομημένου γύρω από την προσέγγιση του Εξευρωπαϊσμού.Το διδακτορικό φιλοδοξεί, πιο συγκεκριμένα, να συνεισφέρει κατά τρόπο πρωτότυπο και γόνιμο στην παραγωγή γνώσης εντός του πεδίου των Ευρωπαϊκών Σπουδών:-εμβαθύνοντας στην ερευνητικά εν πολλοίς αγνοημένη ευρωπαϊκή διάσταση της διαμεσολάβησης συμφερόντων του εγχώριου αγροτικού κινήματος (πόσο μάλλον σε ένα προενταξιακό πλαίσιο).-συνεισφέροντας στην επιστημονική συζήτηση γύρω από τη σύνθετη οντολογία του Εξευρωπαϊσμού, μέσω της επεξεργασίας ενός ορισμού γενικής ισχύος του φαινομένου, ο οποίος να δημιουργεί τις προϋποθέσεις για την εργαλειοποίηση του σχετικού υποδείγματος και στις τέσσερις βασικές διαστάσεις του (κατωφερή – οριζόντια και ανωφερή/ εσωτερική και εξωτερική) στο πλαίσιο σύνθετων ερευνητικών προγραμμάτων.-συμβάλλοντας στην περαιτέρω επεξεργασία ορισμών για έννοιες - κλειδιά στον τομέα της θεωρίας των ομάδων (π.χ. EU lobbying).-εμπλουτίζοντας (εκ των πραγμάτων) τη βιβλιογραφία γύρω από τον Εξευρωπαϊσμό των ομάδων, και ιδιαίτερα των αγροτικών, με νέα εμπειρικά δεδομένα.Το ερευνητικό πρόγραμμα της μελέτης, καθώς και επιμέρους θεωρητικά και μεθοδολογικά εργαλεία και προσεγγίσεις, καλούνται να προωθήσουν περαιτέρω την ανάλυση. Στο σημείο αυτό μνημονεύουμε, ειδικότερα, την απόφασή μας:-να συλλάβουμε την έννοια της διαμεσολάβησης συμφερόντων κατά τρόπο μαξιμαλιστικό, προκειμένου η τελευταία να συμπεριλαμβάνει τόσο όψεις της εσωτερικής λειτουργίας της «Πανελληνίου» (π.χ. ενημερωτική και εκπαιδευτική πολιτική, εσωτερική οργανωτική δομή και διαχείριση προσωπικού) όσο και πτυχές των σχέσεων της Συνομοσπονδίας με τρίτους φορείς (λ.χ. πολιτικοί αξιωματούχοι, δημόσια διοίκηση, διεθνείς οργανισμοί).-να αναπτύξουμε ένα εκλεκτικό ερμηνευτικό μοντέλο, προσανατολισμένο στην περαιτέρω ενίσχυση των αναλυτικών δυνατοτήτων του Εξευρωπαϊσμού μέσω της αξιοποίησης πρόσθετων θεωρητικών υποδειγμάτων (π.χ. νεολειτουργισμός, φιλελεύθερος διακυβερνητισμός), σε ορισμένες πτυχές τους ανταγωνιστικών, όχι όμως ασύμβατων μεταξύ τους.-να αξιοποιήσουμε το μεθοδολογικό εργαλείο της «θεωρητικά ενημερωμένης συγκριτικής μελέτης περίπτωσης», με στόχο την αύξηση της εγκυρότητας και της αξιοπιστίας των εμπειρικών ευρημάτων μας ως προς το βαθμό της κοινοτικής επιρροής και της σχετικής σπουδαιότητας της Ε.Ε. («καθαρός» κοινοτικός αντίκτυπος).Στα κυριότερα θεωρητικά και εμπειρικά συμπεράσματα της διατριβής συγκαταλέγονται τα ακόλουθα:-Είναι δυνατή η υιοθέτηση ενός erga omnes ορισμού του Εξευρωπαϊσμού και προσφέρονται τα αναλυτικά και μεθοδολογικά εργαλεία, ώστε, βάσει του ορισμού αυτού, να επιτευχθεί η πλήρης εργαλειοποίηση της ανωτέρω προσέγγισης τόσο σε ένα προενταξιακό όσο και σε ένα μετενταξιακό περιβάλλον.-Μεταξύ 1945 και 1967 η πολιτική συμπεριφορά της «Πανελληνίου» εξευρωπαΐζεται εκτεταμένα, παρότι δεν καθίσταται πάντα σαφές κατά πόσο πρόκειται για επιφανειακές ή ουσιαστικές αλλαγές, όπως και αν αυτές αφορούν αποκλειστικά την πολυεπίπεδη (αιρετή/ υπηρεσιακή) αγροτοσυνεταιριστική ηγεσία ή και τη βάση.-Η μελέτη διαδικασιών προ- και πρωτο-κοινοτικού Εξευρωπαϊσμού, η οποία βρίσκεται σε αρχικό στάδιο, οφείλει να εντατικοποιηθεί. Αναλόγως, ως ιδιαίτερα χρήσιμη κρίνεται η ανάπτυξη σύνθετων ερευνητικών προγραμμάτων, τα οποία θα παρακολουθούν το φαινόμενο και στις τέσσερις θεμελιώδεις διαστάσεις του
Mέτρηση της παραγωγής παραξενιάς σε συγκρούσεις πρωτονίου-πρωτονίου με το πείραμα ALICE στον LHC του CERN
- Publication venue
- Publication date
- 01/01/2020
- Field of study
Παρουσιάζεται η μελέτη που αφορά στην παραγωγή παράξενων και
πολυπαράξενων αδρονίων με το πείραμα ALICE στον LHC του CERN. Γίνεται μία
εισαγωγή σχετικά με το γενικό σκοπό του πειράματος και το κεντρικό ανιχνευτικό
σύστημα αυτού. Έπειτα, αναλύονται οι τεχνικές ταυτοποίησης αδρονίων με έμφαση στη
λειτουργία και απόδοση κάθε ανιχνευτή στη διαδικασία ταυτοποίησης. Ο κύριος άξονας
της μελέτης είναι η παρουσίαση των αποτελεσμάτων που αφορούν στην αυξημένη
παραγωγή παράξενων σωματιδίων σε περιβάλλον υψηλής πολλαπλότητας σε
συγκρούσεις pp σε ενέργεια κέντρου μάζας 7 TeV. To γεγονός που καθιστά αυτήν την
μελέτη πλέον ενδιαφέρουσα είναι ότι παρατηρείται για πρώτη φορά σε pp συγκρούσεις,
η εξαρτώμενη από την πολλαπλότητα αυξημένη παραγωγή παράξενων (Κ0s, Λ) και
πολυπαράξενων (Ξˉ, Ωˉ,) αδρονίων. Ακολουθεί παρουσίαση και σχολιασμός των
αποτελεσμάτων που αφορούν στην παραγωγή παράξενων και πολυπαράξενων
σωματιδίων σε συγκρούσεις p-Pb και Pb-Pb. Μελετάται, αρχικά, η εξάρτηση από την
πολλαπλότητα της παραγωγής πιονίων, καονίων, πρωτονίων και λάμδα σωματιδίων σε
συγκρούσεις p-Pb σε ενέργεια κέντρου μάζας 5.02 TeV . Παρουσιάζονται, επίσης, οι
μετρήσεις από την παραγωγή πολυπαράξενων βαρυονίων σε συγκρούσεις p-Pb στην ίδια
ενέργεια. Στη συνέχεια, διερευνώνται τα αποτελέσματα της παραγωγής σωματιδίων Κ0s
και Λ σε συγκρούσεις Pb-Pb σε ενέργεια κέντρου μάζας 2.76 ΤeV και της παραγωγής
πολυπαράξενων σωματιδίων σε μέση ωκύτητα, σε συγκρούσεις Pb-Pb, στην ίδια
ενέργεια. Tέλος, παρουσιάζονται τα συμπεράσματα για την παραγωγή παραξενιάς σε όλα
τα συστήματα σύγκρουσης.The production of strange and multistrange particles with the ALICE experiment at the CERN LHC is presented. An introduction about the general purpose of the experiment as well as the ALICE detector is taking place. The main purpose of this work is to present the results from the enhanced production of strange and multi-stange hadrons in high multiplicity pp collisions. This is a novel phenomenon, because the multiplicity dependent enhanced production of strange and multi-strange hadrons has never been observed before in pp collisions. A summary of the results concerning the strangeness production in p-Pb, Pb-Pb collisions follows. The centrality dependent production of pion, kaon, proton, Lamda and multi-strange baryons in p-Pb collisions at center of mass energy 7 TeV is studied. Moreover, the production of K0s, Lamda and multi-strange hadrons in Pb-Pb collisions at 2.76 TeV is presented. In conclusion, the most important results of the strangeness production with the ALICE experiment are summarized
Investigating the nature of the K∗0(700) state with π±K0S correlations at the LHC
- Author
- Abranches De Carvalho Leopoldo
- Acharya Shreyasi
- Adamová Dagmar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Al-Turany Mohammad
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Mas’ud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesús Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa Naji
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshäuser Harald
- Arata Carolina
- Arcelli Silvia
- Aresti Mauro
- Arnaldi Roberta
- Arneiro Jhoao Gabriel Martins Campos Almeida
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Baba Hitoshi
- Badalà Angela
- Badaro Saramela Thiago
- Bae Joonsuk
- Baek Yong Wook
- Bai Xiaozhi
- Bailhache Raphaëlle
- Bailung Yoshini
- Bala Renu
- Balbino Alessandro
- Baldisseri Alberto
- Balis Bartosz
- Banerjee Debjani
- Banoo Zarina
- Barile Francesco
- Barioglio Luca
- Barlou Maria
- Barman Banajit
- Barnaföldi Gergely Gábor
- Barnby Lee Stuart
- Barreau Emilie Martine
- Barreto De Oliveira Campos Leonardo
- Bartels Clara
- Barth Klaus
- Bartsch Esther
- Bastid Nicole
- Basu Sumit
- Batigne Guillaume
- Battistini Daniel
- Batyunya Boris
- Bauri Dibakar
- Bazo Alba José Luis
- Bearden Ian Gardner
- Beattie Caitlin
- Becht Pascal
- Behera Debadatta
- Belikov Iouri
- Bell Hechavarria Ailec de la Caridad
- Bellini Francesca
- Bellwied Rene
- Belokurova Svetlana
- Bencédi Gyula
- Bensaoula Adel
- Beolè Stefania
- Berdnikov Yaroslav
- Berdnikova Anastasia
- Bergmann Luisa
- Bertran Ferrer Marta
- Besoiu Mihaela Gabriela
- Betev Latchezar
- Bhaduri Partha Pratim
- Bhasin Anju
- Bhat Mohammad Asif
- Bhattacharjee Buddhadeb
- Bianchi Livio
- Bianchi Nicola
- Bielčík Jaroslav
- Bielčíková Jana
- Bigot Alexandre Patrick
- Bilandzic Ante
- Biro Gabor
- Biswas Saikat
- Bize Nicolas Luc
- Blair Justin Thomas
- Blau Dmitry S.
- Blidaru Mihail-Bogdan
- Bluhme Nora
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bodova Tea
- Boi Stefano
- Bok Jeongsu
- Boldizsar Laszlo
- Bombara Marek
- Bond Peter Matthew
- Bonomi Germano
- Borel Herve
- Borissov Alexander
- Borquez Carcamo Andres Gerardo
- Bossi Hannah
- Botta Elena
- Bratrud Lars
- Braun-Munzinger Peter
- Bregant Marco
- Broz Michal
- Bruno Giuseppe Eugenio
- Buckland Matthew Daniel
- Budnikov Dmitry
- Bufalino Stefania
- Burmasov Nazar
- Buthelezi Edith Zinhle
- Bylinkin Alexander
- Bysiak Sebastian Adam
- Bühler Paul
- Büsching Henner
- Cabanillas Noris Juan Carlos
- Cai Mengke
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Canedo Fabio de Moraes Canedo
- Carabas Mihai
- Carnesecchi Francesca
- Caron Robin Albert Andre
- Castillo Castellanos Javier Ernesto
- Catalano Fabio
- Cattaruzzi Samuele
- Ceballos Sanchez Cesar
- Cerri Rebecca
- Chakaberia Irakli
- Chakraborty Pritam
- Chandra Sinjini
- Chapeland Sylvain
- Chartier Marielle
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Cheng Tiantian
- Cheshkov Cvetan Valeriev
- Chibante Barroso Vasco Miguel
- Chinellato David Dobrigkeit
- Chizzali Emma Sophia
- Cho Jaeyoon
- Cho Soyeon
- Chochula Peter
- Choudhury Dhrubajyoti
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter L.
- Chujo Tatsuya
- Ciacco Mario
- Cicalò Corrado
- Ciupek Michael Rudolf
- Clai Giulia
- Colamaria Fabio Filippo
- Colburn Jonathan Samuel
- Colella Domenico
- Colocci Manuel
- Concas Matteo
- Conesa Balbastre Gustavo
- Conesa Del Valle Zaida
- Contin Giacomo
- Contreras Nuno Jesus Guillermo
- Coquet Maurice Louis
- Cortese Pietro
- Cosentino Mauro Rogerio
- Costa Filippo
- Costanza Susanna
- Cot Corentin
- Crkovská Jana
- Crochet Philippe
- Cruz Torres Reynier
- Cui Pengyao
- Cuveland Jan de
- Czeslaw Miskowiec Dariusz
- Dainese Andrea
- Danisch Meike Charlotte
- Danu Andrea
- Das Prottay
- Das Prottoy
- Das Supriya
- Dash Archita Rani
- Dash Sadhana
- De Caro Annalisa
- De Cataldo Giacinto
- De Falco Alessandro
- De Gruttola Daniele
- De Marco Nora
- De Martin Chiara
- De Melo Paulino Maria Monalisa
- De Pasquale Salvatore
- Deb Rohaan
- Del Grande Raffaele
- Dello Stritto Luigi
- Deng Wenjing
- Dhankher Preeti
- Di Bari Domenico
- Di Mauro Antonio
- Diab Batoul
- Dietel Thomas
- Ding Yanchun
- Ditzel Janik
- Divià Roberto
- Dixit Dhruv Utpalkumar
- Djuvsland Øystein
- Dmitrieva Uliana
- Dobrin Alexandru Florin
- Dominguez Rosas Edgar
- Donigus Benjamin
- Doremalen Lennart Vincent Rogier van
- Duarte Galvan Carlos
- Dubinski Jan Michal
- Dubla Andrea
- Ducati Maria Beatriz de Leone Gay
- Dudi Sandeep
- Dupieux Pascal
- Durkac Martin
- Dzalaiova Natalia
- Eder Tabea Maria
- Ehlers Raymond James, III
- Eisenhut Florian
- Ejima Ren
- El Mard Bouziani Youssef
- Elia Domenico
- Erazmus Barbara Ewa
- Ercolessi Francesca
- Espagnon Bruno
- Espinoza Beltran Lucina Gabriela
- Eulisse Giulio
- Evans David
- Evdokimov Sergey
- Fabbietti Laura
- Faggin Mattia
- Faivre Julien
- Fan Feng
- Fan Wenqing
- Fantoni Alessandra
- Fasel Markus
- Feliciello Alessandro
- Feofilov Grigori A.
- Fernández Téllez Arturo
- Ferrandi De Oliveira Lucas
- Ferrero Andrea
- Ferrero Chiara
- Ferretti Alessandro
- Feuillard Victor Jose Gaston
- Fierro Rojas Pablo
- Filova Vendulka
- Finogeev Dmitry
- Fionda Fiorella Maria Celeste
- Flatland Erlend
- Flor Fernando Antonio
- Flores Amanda Nicole
- Foertsch Siegfried Valentin
- Fokin Ilya
- Fokin Sergey
- Fragiacomo Enrico
- Frajna Eszter
- Fuchs Ulrich
- Funicello Nicola
- Furget Christophe
- Furs Artur
- Fusayasu Takahiro
- Gaardhoeje Jens Joergen
- Gagliardi Martino
- Gago Medina Alberto Martín
- Gahlaut Tanu
- Gameiro Munhoz Marcelo
- Gangadharan Dhevan Raja
- Ganoti Paraskevi
- Garabatos Cuadrado Jose Maria
- Garcia Guardiano Gabriel
- Garcia-Solis Edmundo Javier
- García Chávez Tonatiuh
- García Martínez Ginés
- Gargiulo Corrado
- Gasik Piotr
- Gautam Amrit
- Germain Marie
- Ghimouz Abderrahmane
- Ghosh Chandrasekhar
- Giacalone Marco
- Gioachin Giulia
- Giubellino Paolo
- Giubilato Piero
- Glaenzer Aude Marie Camille
- Glimos Ewa
- Glässel Peter
- Goh Daniel Jia Qin
- Gonzalez Sebastian Victor Luis
- Gordeev Pavel
- Gorgon Marek Boguslaw
- Goswami Kangkan
- Gotovac Sven
- Grabski Varlen
- Graczykowski Łukasz Kamil
- Grecka Ekaterina
- Grelli Alessandro
- Grigoraș Costin
- Grigoryan Smbat
- Grigoryev Vladislav
- Grosa Fabrizio
- Grosso Raffaele
- Große-Oetringhaus Jan Fiete
- Grund David
- Grünwald Nadine Alice
- Guernane Rachid
- Guilbaud Maxime Rene Joseph
- Gulbrandsen Kristjan Herlache
- Gunji Taku
- Guo Wenda
- Gupta Anik
- Gupta Ramni
- Gupta Rashi
- Gwizdziel Katarzyna
- Gyulai Laszlo
- Gündem Tuba
- Hachiya Shimomura Maya
- Hadjidakis Cynthia Marie
- Haider Fakhar Ul
- Haidlova Sara
- Haldar Mintu
- Haller Barthélémy von
- Hamagaki Hideki
- Hamdi Abdennacer
- Han Younghoon
- Hanley Brian Gerald
- Hannigan Ryan
- Hansen Joachim
- Harris John William
- Harton Austin Vincent
- Hartung Michael Volker
- Hassan Hadi
- Hatzifotiadou Despina
- Hauer Philip
- Haugland Solheim Emilie
- Havener Laura Brittany
- Hellbär Ernst
- Helstrup Håvard
- Hemmer Marvin
- Herman Tomáš
- Hernandez Sabrina Gabrielle
- Herrera Corral Gerardo Antonio
- Herrmann Florian
- Herrmann Sarah Nina Edwige
- Hetland Kristin Fanebust
- Heybeck Benedict
- Hillemanns Hartmut
- Hippolyte Boris
- Hoffmann Felix Willi
- Hofman Bas
- Hong Geunhee
- Horst Maximilian
- Horzyk Adrian
- Hou Yongzhen
- Hristov Peter
- Huhn Patrick
- Huhta Laura Maria
- Humanic Thomas J.
- Hutson Alek
- Hutter Dirk
- Hwang Minyoung Chris
- Ilkaev Radiy
- Ilyas Hira
- Inaba Motoi
- Innocenti Gian Michele
- Ippolitov Mikhail
- Isakov Artem
- Isidori Tommaso
- Islam Md Samsul
- Ivanov Marian
- Ivanov Marian
- Ivanov Vladimir
- Iversen Kaare Endrup
- Jablonski Miroslaw
- Jacak Barbara
- Jacazio Nicolò
- Jacobs Peter Martin
- Jadlovska Slavka
- Jadlovsky Jan
- Jaelani Syaefudin
- Jahnke Cristiane
- Jakubcinova Zuzana
- Jakubowska Monika Joanna
- Janik Malgorzata Anna
- Janson Thomas
- Ji Su-jeong
- Jia Shihai
- Jonas Florian
- Jones Daniel Matthew
- Jowett John M.
- Jung Jerome
- Jung Michael
- Junique Antoine Jean-Simon
- Jusko Anton
- Kaewjai Jetnipit
- Kalinak Peter
- Kalteyer Annalena Sophie
- Kalweit Alexander Philipp
- Karatović David
- Karavichev Oleg V.
- Karavicheva Tatiana L.
- Karczmarczyk Przemyslaw
- Karpechev Evgeny
- Karwowska Maja Jadwiga
- Kebschull Udo
- Keidel Ralf
- Keijdener Darius
- Keil Markus
- Ketzer Bernhard
- Khade Swapnesh Santosh
- Khan Ahsan Mehmood
- Khan Mohammed Mohisin
- Khan Shaista
- Khanzadeev Alexei
- Kharlov Yury
- Khatun Anisa
- Khuntia Arvind
- Khuranova Zhanna
- Kileng Bjarte
- Kim Beomkyu
- Kim Chong
- Kim Dong Jo
- Kim Eun Joo
- Kim Jaehyun
- Kim Jiyoung
- Kim Junlee
- Kim Minjung
- Kim Se Yong
- Kim Taejun
- Kimura Kento
- Kirkova Aleksandrina
- Kirsch Stefan
- Kisel Ivan
- Kiselev Sergej N.
- Kisiel Adam Ryszard
- Kitowski Jacek Pawel
- Klay Jennifer Lynn
- Klein Jochen
- Klein Spencer Robert
- Klein-Bösing Christian
- Kleiner Matthias
- Klemenz Thomas
- Kluge Alexander
- Kobdaj Chinorat
- Kollegger Thorsten
- Kondratyev Andrey
- Kondratyeva Natalia
- Konopka Piotr Jan
- Kornakov Van Georgui
- Korwieser Maximilian
- Koryciak Sebastian Dominik
- Kotliarov Artem
- Kovacic Nino
- Kovalenko Vladimir
- Kowalski Marek
- Kozhuharov Venelin Valeriev
- Kravčáková Adela
- Krcal Lubos
- Krivda Marian
- Krizek Filip
- Krizkova Gajdosova Katarina
- Kroesen Martin
- Krupova Diana Maria
- Kryshen Evgeny
- Králik Ivan
- Krüger Mario
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- Yang Shiming
- Yano Satoshi
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- Yin Zhongbao
- Yoo In-Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yüncü Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Závada Petr
- Önnerstad Anna
- Šafařík Karel
- Šerkšnytė Laura
- Šuljić Miljenko
- Publication venue
- Publication date
- 20/12/2023
- Field of study
The first measurements of femtoscopic correlations with the particle pair combinations π±K0S in pp collisions at s√=13 TeV at the Large Hadron Collider (LHC) are reported by the ALICE experiment. Using the femtoscopic approach, it is shown that it is possible to study the elusive K∗0(700) particle that has been considered a tetraquark candidate for over forty years. Boson source parameters and final-state interaction parameters are extracted by fitting a model assuming a Gaussian source to the experimentally measured two-particle correlation functions. The final-state interaction is modeled through a resonant scattering amplitude, defined in terms of a mass and a coupling parameter, decaying into a π±K0S pair. The extracted mass and Breit-Wigner width, derived from the coupling parameter, of the final-state interaction are found to be consistent with previous measurements of the K∗0(700). The small value and increasing behavior of the correlation strength with increasing source size support the hypothesis that the K∗0(700) is a four-quark state, i.e. a tetraquark state. This latter trend is also confirmed via a simple geometric model that assumes a tetraquark structure of the K∗0(700) resonance
Investigating the nature of the K0∗(700) state with π±KS0 correlations at the LHC
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Al-Turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Arata Carolina
- Arcelli Silvia
- Aresti Mauro
- Arnaldi Roberta
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Baba Hitoshi
- Badala Angela
- Badaro Saramela Thiago
- Bae Joonsuk
- Baek Yongwook
- Bai Xiaozhi
- Bailhache Raphaelle Marie
- Bailung Yoshini
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- Baldisseri Alberto
- Balis Bartosz
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- Barile Francesco
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- Bazo Alba Jose Luis
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- Wilhelmi Alexander
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- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 04/01/2024
- Field of study
International audienceThe first measurements of femtoscopic correlations with the particle pair combinations π±KS0 in pp collisions at s=13 TeV at the Large Hadron Collider (LHC) are reported by the ALICE experiment. Using the femtoscopic approach, it is shown that it is possible to study the elusive K0∗(700) particle that has been considered a tetraquark candidate for over forty years. Boson source parameters and final-state interaction parameters are extracted by fitting a model assuming a Gaussian source to the experimentally measured two-particle correlation functions. The final-state interaction is modeled through a resonant scattering amplitude, defined in terms of a mass and a coupling parameter, decaying into a π±KS0 pair. The extracted mass and Breit-Wigner width, derived from the coupling parameter, of the final-state interaction are found to be consistent with previous measurements of the K0∗(700). The small value and increasing behavior of the correlation strength with increasing source size support the hypothesis that the K0∗(700) is a four-quark state, i.e. a tetraquark state. This latter trend is also confirmed via a simple geometric model that assumes a tetraquark structure of the K0∗(700) resonance
Investigating the nature of the K0∗(700) state with π±KS0 correlations at the LHC
- Author
- Abranches De Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Al-turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Arata Carolina
- Arcelli Silvia
- Aresti Mauro
- Arnaldi Roberta
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Baba Hitoshi
- Badala Angela
- Badaro Saramela Thiago
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- Baek Yongwook
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- Barth Klaus
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- Basu Sumit
- Batigne Guillaume
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- Bazo Alba Jose Luis
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- Volpe Giacomo
- Von Haller Barthelemy
- Vorobyev Ivan
- Vozniuk Nikita
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- Wan Jie
- Wang Chunzheng
- Wang Dongfang
- Wang Yuanzhe
- Wang Yubiao
- Wegrzynek Adam Tadeusz
- Weiglhofer Felix Thomas
- Wenzel Sandro Christian
- Wessels Johannes Peter
- Weyhmiller Sierra Lisa
- Wiechula Jens
- Wikne Jon
- Wilhelmi Alexander
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- Publication date
- 10/12/2023
- Field of study
The first measurements of femtoscopic correlations with the particle pair combinations π±KS0 in pp collisions at s=13 TeV at the Large Hadron Collider (LHC) are reported by the ALICE experiment. Using the femtoscopic approach, it is shown that it is possible to study the elusive K0∗(700) particle that has been considered a tetraquark candidate for over forty years. Boson source parameters and final-state interaction parameters are extracted by fitting a model assuming a Gaussian source to the experimentally measured two-particle correlation functions. The final-state interaction is modeled through a resonant scattering amplitude, defined in terms of a mass and a coupling parameter, decaying into a π±KS0 pair. The extracted mass and Breit--Wigner width, derived from the coupling parameter, of the final-state interaction are found to be consistent with previous measurements of the K0∗(700). The small value and increasing behavior of the correlation strength with increasing source size support the hypothesis that the K0∗(700) is a four-quark state, i.e. a tetraquark state. This latter trend is also confirmed via a simple geometric model that assumes a tetraquark structure of the K0∗(700) resonance.The first measurements of femtoscopic correlations with the particle pair combinations π±KS0 in pp collisions at s=13 TeV at the Large Hadron Collider (LHC) are reported by the ALICE experiment. Using the femtoscopic approach, it is shown that it is possible to study the elusive K0∗(700) particle that has been considered a tetraquark candidate for over forty years. Boson source parameters and final-state interaction parameters are extracted by fitting a model assuming a Gaussian source to the experimentally measured two-particle correlation functions. The final-state interaction is modeled through a resonant scattering amplitude, defined in terms of a mass and a coupling parameter, decaying into a π±KS0 pair. The extracted mass and Breit-Wigner width, derived from the coupling parameter, of the final-state interaction are found to be consistent with previous measurements of the K0∗(700). The small value and increasing behavior of the correlation strength with increasing source size support the hypothesis that the K0∗(700) is a four-quark state, i.e. a tetraquark state. This latter trend is also confirmed via a simple geometric model that assumes a tetraquark structure of the K0∗(700) resonance
Investigating the nature of the K0∗(700) state with π±KS0 correlations at the LHC
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Al-Turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Arata Carolina
- Arcelli Silvia
- Aresti Mauro
- Arnaldi Roberta
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Baba Hitoshi
- Badala Angela
- Badaro Saramela Thiago
- Bae Joonsuk
- Baek Yongwook
- Bai Xiaozhi
- Bailhache Raphaelle Marie
- Bailung Yoshini
- Bala Renu
- Balbino Alessandro
- Baldisseri Alberto
- Balis Bartosz
- Banerjee Debjani
- Banoo Zarina
- Barile Francesco
- Barioglio Luca
- Barlou Maria
- Barman Banajit
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Barreau Emilie Martine
- Barreto de Oliveira Campos Leonardo
- Bartels Clara
- Barth Klaus
- Bartsch Esther
- Bastid Nicole
- Basu Sumit
- Batigne Guillaume
- Battistini Daniel
- Batyunya Boris
- Bauri Dibakar
- Bazo Alba Jose Luis
- Bearden Ian Gardner
- Beattie Caitlin
- Becht Pascal
- Behera Debadatta
- Belikov Iouri
- Bell Hechavarria Ailec
- Bellini Francesca
- Bellwied Rene
- Belokurova Svetlana
- Bencedi Gyula
- Bensaoula Adel
- Beole Stefania Maria
- Berdnikov Yaroslav
- Berdnikova Anastasia
- Bergmann Luisa
- Bertran Ferrer Marta
- Besoiu Mihaela Gabriela
- Betev Latchezar
- Bhaduri Partha Pratim
- Bhasin Anju
- Bhat Mohammad Asif
- Bhattacharjee Buddhadeb
- Bianchi Livio
- Bianchi Nicola
- Bielcik Jaroslav
- Bielcikova Jana
- Bigot Alexandre Patrick
- Bilandzic Ante
- Biro Gabor
- Biswas Saikat
- Bize Nicolas Luc
- Blair Justin Thomas
- Blau Dmitry
- Blidaru Mihail Bogdan
- Bluhme Nora
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bodova Tea
- Boi Stefano
- Bok Jeongsu
- Boldizsar Laszlo
- Bombara Marek
- Bond Peter Matthew
- Bonomi Germano
- Borel Herve
- Borissov Alexander
- Borquez Carcamo Andres Gerardo
- Bossi Hannah
- Botta Elena
- Bratrud Lars
- Braun-Munzinger Peter
- Bregant Marco
- Broz Michal
- Bruno Giuseppe Eugenio
- Buckland Matthew Daniel
- Budnikov Dmitry
- Buesching Henner
- Bufalino Stefania
- Buhler Paul Alois
- Burmasov Nazar
- Buthelezi Edith Zinhle
- Bylinkin Aleksandr
- Bysiak Sebastian Adam
- Cabanillas Noris Juan Carlos
- Cai Mengke
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Carabas Mihai
- Carnesecchi Francesca
- Caron Robin Albert Andre
- Castillo Castellanos Javier Ernesto
- Catalano Fabio
- Cattaruzzi Samuele
- Ceballos Sanchez Cesar
- Cerri Rebecca
- Chakaberia Irakli
- Chakraborty Pritam
- Chandra Sinjini
- Chapeland Sylvain
- Chartier Marielle
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Cheng Tiantian
- Cheshkov Cvetan Valeriev
- Chibante Barroso Vasco Miguel
- Chizzali Emma Sophia
- Cho Jaeyoon
- Cho Soyeon
- Chochula Peter
- Choudhury Dhrubajyoti
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter
- Chujo Tatsuya
- Ciacco Mario
- Cicalo Corrado
- Ciupek Michael Rudolf
- Clai Giulia
- Colamaria Fabio Filippo
- Colburn Jonathan Samuel
- Colella Domenico
- Colocci Manuel
- Concas Matteo
- Conesa Balbastre Gustavo
- Conesa del Valle Zaida
- Contin Giacomo
- Contreras Nuno Jesus Guillermo
- Coquet Maurice Louis
- Cortese Pietro
- Cosentino Mauro Rogerio
- Costa Filippo
- Costanza Susanna
- Cot Corentin
- Crkovska Jana
- Crochet Philippe
- Cruz Torres Reynier
- Cui Pengyao
- Czeslaw Miskowiec Dariusz
- Dainese Andrea
- Danisch Meike Charlotte
- Danu Andrea
- Das Prottay
- Das Prottoy
- Das Supriya
- Dash Archita Rani
- Dash Sadhana
- de Caro Annalisa
- de Cataldo Giacinto
- de Cuveland Jan
- de Falco Alessandro
- de Gruttola Daniele
- de Leone Gay Maria Beatriz
- de Marco Nora
- de Martin Chiara
- de Melo Paulino Maria Monalisa
- de Moraes Canedo Fabio
- de Pasquale Salvatore
- Deb Rohaan
- del Grande Raffaele
- Dello Stritto Luigi
- Deng Wenjing
- Dhankher Preeti
- Di Bari Domenico
- Di Mauro Antonio
- Diab Batoul
- Dietel Thomas
- Ding Yanchun
- Ditzel Janik
- Divia Roberto
- Dixit Dhruv Utpalkumar
- Djuvsland Oeystein
- Dmitrieva Uliana
- Dobrigkeit Chinellato David
- Dobrin Alexandru Florin
- Dominguez Rosas Edgar
- Donigus Benjamin
- Duarte Galvan Carlos
- Dubinski Jan Michal
- Dubla Andrea
- Dudi Sandeep
- Dupieux Pascal
- Durkac Martin
- Dzalaiova Natalia
- Eder Tabea Maria
- Ehlers Raymond James
- Eisenhut Florian
- Ejima Ren
- El Mard Bouziani Youssef
- Elia Domenico
- Erazmus Barbara Ewa
- Ercolessi Francesca
- Espagnon Bruno
- Espinoza Beltran Lucina Gabriela
- Eulisse Giulio
- Evans David
- Evdokimov Sergey
- Fabbietti Laura
- Faggin Mattia
- Faivre Julien
- Fan Feng
- Fan Wenqing
- Fantoni Alessandra
- Fasel Markus
- Feliciello Alessandro
- Feofilov Grigorii
- Fernandez Tellez Arturo
- Ferrandi de Oliveira Lucas
- Ferrero Andrea
- Ferrero Chiara
- Ferretti Alessandro
- Feuillard Victor Jose Gaston
- Fierro Rojas Pablo
- Filova Vendulka
- Finogeev Dmitry
- Fionda Fiorella
- Fiorini da Silva Tiago
- Flatland Erlend
- Flor Fernando Antonio
- Flores Amanda Nicole
- Foertsch Siegfried Valentin
- Fokin Ilya
- Fokin Sergey
- Fragiacomo Enrico
- Frajna Eszter
- Fuchs Ulrich
- Funicello Nicola
- Furget Christophe
- Furs Artur
- Fusayasu Takahiro
- Gaardhoeje Jens Joergen
- Gagliardi Martino
- Gago Medina Alberto Martin
- Gahlaut Tanu
- Gameiro Munhoz Marcelo
- Gangadharan Dhevan Raja
- Ganoti Paraskevi
- Garabatos Cuadrado Jose Maria
- Garcia Chavez Tonatiuh
- Garcia Guardiano Gabriel
- Garcia-Solis Edmundo Javier
- Gargiulo Corrado
- Gasik Piotr Jan
- Gautam Amrit
- Germain Marie
- Ghimouz Abderrahmane
- Ghosh Chandrasekhar
- Giacalone Marco
- Gioachin Giulia
- Giubellino Paolo
- Giubilato Piero
- Glaenzer Aude Marie Camille
- Glassel Peter
- Glimos Ewa
- Goh Daniel Jia Qin
- Gonzalez Sebastian Victor Luis
- Gordeev Pavel
- Gorgon Marek Boguslaw
- Goswami Kangkan
- Gotovac Sven
- Grabski Varlen
- Graczykowski Lukasz Kamil
- Grecka Ekaterina
- Grelli Alessandro
- Grigoras Costin
- Grigoryan Smbat
- Grigoryev Vladislav
- Grosa Fabrizio
- Grosse-Oetringhaus Jan Fiete
- Grosso Raffaele
- Gruenwald Nadine Alice
- Grund David
- Guernane Rachid
- Guilbaud Maxime Rene Joseph
- Gulbrandsen Kristjan Herlache
- Gundem Tuba
- Gunji Taku
- Guo Wenda
- Gupta Anik
- Gupta Ramni
- Gupta Rashi
- Gwizdziel Katarzyna
- Gyulai Laszlo
- Hachiya Shimomura Maya
- Hadjidakis Cynthia Marie
- Haider Fakhar Ul
- Haidlova Sara
- Haldar Mintu
- Hamagaki Hideki
- Hamdi Abdennacer
- Han Younghoon
- Hanley Brian Gerald
- Hannigan Ryan Patrick
- Hansen Joachim
- Harris John William
- Harton Austin Vincent
- Hartung Michael Volker
- Hassan Hadi
- Hatzifotiadou Despina
- Hauer Philip
- Haugland Solheim Emilie
- Havener Laura Brittany
- Hellbar Ernst
- Helstrup Haavard
- Hemmer Marvin
- Herman Tomas
- Hernandez Sabrina Gabrielle
- Herrera Corral Gerardo Antonio
- Herrmann Florian
- Herrmann Sarah Nina Edwige
- Hetland Kristin Fanebust
- Heybeck Benedict
- Hillemanns Hartmut
- Hippolyte Boris
- Hoffmann Felix Willi
- Hofman Bas
- Hong Geun Hee
- Horst Maximilian
- Horzyk Adrian
- Hou Yongzhen
- Hristov Peter Zahariev
- Huhn Patrick
- Huhta Laura Maria
- Humanic Thomas
- Hutson Alek
- Hutter Dirk
- Hwang Minyoung Chris
- Ilkaev Radiy
- Ilyas Hira
- Inaba Motoi
- Innocenti Gian Michele
- Ippolitov Mikhail
- Isakov Artem
- Isidori Tommaso
- Islam Md Samsul
- Ivanov Marian
- Ivanov Marian
- Ivanov Vladimir
- Iversen Kaare Endrup
- Jablonski Miroslaw
- Jacak Barbara
- Jacazio Nicolo
- Jacobs Peter Martin
- Jadlovska Slavka
- Jadlovsky Jan
- Jaelani Syaefudin
- Jahnke Cristiane
- Jakubcinova Zuzana
- Jakubowska Monika Joanna
- Janik Malgorzata Anna
- Janson Thomas
- Ji Su-Jeong
- Jia Shihai
- Jonas Florian
- Jones Daniel Matthew
- Jowett John
- Jung Jerome
- Jung Michael
- Junique Antoine Jean-Simon
- Jusko Anton
- Kaewjai Jetnipit
- Kalinak Peter
- Kalteyer Annalena Sophie
- Kalweit Alexander Philipp
- Karatovic David
- Karavichev Oleg
- Karavicheva Tatiana
- Karczmarczyk Przemyslaw
- Karpechev Evgeny
- Karwowska Maja Jadwiga
- Kebschull Udo Wolfgang
- Keidel Ralf
- Keijdener Darius
- Keil Markus
- Ketzer Bernhard Franz
- Khade Swapnesh Santosh
- Khan Ahsan Mehmood
- Khan Mohammed Mohisin
- Khan Shaista
- Khanzadeev Alexei
- Kharlov Yury
- Khatun Anisa
- Khuntia Arvind
- Khuranova Zhanna
- Kileng Bjarte
- Kim Beomkyu
- Kim Chong
- Kim Dong Jo
- Kim Eun Joo
- Kim Jaehyun
- Kim Jiyoung
- Kim Junlee
- Kim Minjung
- Kim Se Yong
- Kim Taejun
- Kimura Kento
- Kirkova Aleksandrina
- Kirsch Stefan
- Kisel Ivan
- Kiselev Sergey
- Kisiel Adam Ryszard
- Kitowski Jacek Pawel
- Klay Jennifer Lynn
- Klein Jochen
- Klein Spencer Robert
- Klein-Boesing Christian
- Kleiner Matthias
- Klemenz Thomas
- Kluge Alexander
- Kobdaj Chinorat
- Kollegger Thorsten Sven
- Kondratyev Andrey
- Kondratyeva Natalia
- Konig Joshua Leon
- Konigstorfer Stephan Alexander
- Konopka Piotr Jan
- Kornakov Van Georgui
- Korwieser Maximilian
- Koryciak Sebastian Dominik
- Kotliarov Artem
- Kovacic Nino
- Kovalenko Vladimir
- Kowalski Marek
- Kozhuharov Venelin Valeriev
- Kralik Ivan
- Kravcakova Adela
- Krcal Lubos
- Krivda Marian
- Krizek Filip
- Krizkova Gajdosova Katarina
- Kroesen Martin
- Kruger Mario
- Krupova Diana Maria
- Kryshen Evgeny
- Kucera Vit
- Kuhn Christian Claude
- Kuijer Paulus Gerardus
- Kumaoka Takuya
- Kumar Deekshit
- Kumar Lokesh
- Kumar Navneet
- Kumar Shyam
- Kundu Sourav
- Kurashvili Podist
- Kurepin Alexander
- Kurepin Alexey
- Kuryakin Alexey
- Kushpil Svetlana
- Kuskov Vladislav
- Kutyla Monika
- Kweon Min Jung
- Kwon Youngil
- La Pointe Sarah Louise
- La Rocca Paola
- Lafuente Mazuecos Antonio
- Lakrathok Anantachai
- Lamanna Massimo
- Landou Aimeric Robin
- Langoy Rune
- Larionov Pavel
- Laudi Elisa
- Lautner Lukas
- Lavicka Roman
- Lea Ramona
- Lee Hyungjun
- Legrand Iosif-Charles
- Legras Gauthier
- Lehrbach Johannes
- Lelek Tomasz Marcin
- Lemmon Roy Crawford
- Leon Monzon Ildefonso
- Lesch Marcel Markus
- Lesser Ezra Douglas
- Levai Peter
- Li Xiaomei
- Liang-Gilman Beatrice Eva
- Lien Jorgen Andre
- Lietava Roman
- Likmeta Iris
- Lim Bong-Hwi
- Lim Sanghoon
- Lindenstruth Volker
- Lindner Amelia
- Lippmann Christian
- Liu Donghai
- Liu Jian
- Loizides Constantinos
- Lokos Sandor
- Lomker Johanna
- Loncar Petra
- Lopez Torres Ernesto
- Lopez Xavier Bernard
- Lu Pengzhong
- Lugo Fabiola Viridiana
- Luhder Jens Robert
- Lunardon Marcello
- Luparello Grazia
- Ma Yugang
- Mager Magnus
- Maire Antonin
- Majerz Emilia Maria
- Makariev Martin Vasilev
- Malaev Mikhail
- Malfattore Giovanni
- Malik Nasir Mehdi
- Malik Qasim Waheed
- Malik Salman Khurshid
- Malinina Liudmila
- Mallick Dukhishyam
- Mallick Neelkamal
- Mandaglio Giuseppe
- Mandal Sushobhan Kumar
- Manko Vladislav
- Manso Franck
- Mantovani Sarti Valentina
- Manzari Vito
- Mao Yaxian
- Marcjan Robert Waclaw
- Margagliotti Giacomo Vito
- Margotti Anselmo
- Marin Ana Maria
- Markert Christina
- Martinengo Paolo
- Martinez Hernandez Mario Ivan
- Martinez-Garcia Gines
- Martins Campos Almeida Arneiro Jhoao Gabriel
- Martins Palhares Maria Paula
- Masciocchi Silvia
- Masera Massimo
- Masoni Alberto
- Massacrier Laure Marie
- Massen Olaf
- Mastroserio Annalisa
- Matonoha Oliver
- Mattiazzo Serena
- Matyja Adam Tomasz
- Mayer Christoph
- Mazzaschi Francesco
- Mazzilli Marianna
- Mckibben Lofnes Ingrid
- Mdhluli Joyful Elma
- Mejia Camacho Juan Manuel
- Melikyan Yury
- Menchaca-Rocha Arturo Alejandro
- Meninno Elisa
- Meres Michal
- Mesa Perez Guillermo
- Miake Yasuo
- Micheletti Luca
- Mihaylov Dimitar Lubomirov
- Mikhaylov Konstantin
- Modak Abhi
- Mohanty Bedangadas
- Molander Mikael Andreas
- Monira Shirajum
- Mordasini Cindy
- Moreira de Godoy Willems Denise Aparecida
- Morozov Igor
- Morsch Andreas
- Mrnjavac Teo
- Muccifora Valeria
- Muhuri Sanjib
- Mulligan James Declan
- Mulliri Alice
- Munoz Mendez Jesus Eduardo
- Munzer Robert Helmut
- Murakami Hikari
- Murray Sean
- Musa Luciano
- Musinsky Jan
- Myrcha Julian Wojciech
- Naik Bharati
- Nambrath Anjali Ila
- Nandi Basanta Kumar
- Nania Rosario
- Nappi Eugenio
- Nassirpour Adrian Fereydon
- Nath Abhishek
- Nattrass Christine
- Naydenov Momchil Nikolaev
- Neagu Alexandra
- Negru Adrian-Eduard
- Nekrasova Evgeniia
- Nellen Lukas
- Nepeivoda Roman
- Nese Sigurd
- Neskovic Gvozden
- Nicassio Nicola
- Nielsen Borge Svane
- Nielsen Emil Gorm
- Nikolaev Sergey
- Nikulin Sergey
- Nikulin Vladimir
- Noferini Francesco
- Noh Seoyoung
- Nomokonov Petr
- Norman Jaime
- Novitzky Norbert
- Nowakowski Piotr
- Nyanin Alexander
- Nystrand Joakim Ingemar
- Oh Saehanseul
- Ohlson Alice Elisabeth
- Okorokov Vitaly
- Oleniacz Janusz
- Onnerstad Anna
- Oppedisano Chiara
- Ortiz Velasquez Antonio
- Otwinowski Jacek Tomasz
- Oya Motomi
- Oyama Ken
- Pachmayer Yvonne Chiara
- Padhan Sonali
- Pagano Davide
- Paic Guy
- Paisano Guzman Sergio
- Palasciano Antonio
- Panebianco Stefano
- Panikkassery Salvan Malavika
- Park Hanseo
- Park Hyebin
- Park Jonghan
- Parkkila Jasper Elias
- Patley Yash
- Paul Biswarup
- Paz Jimenez Alom Antonio
- Pei Hua
- Peitzmann Thomas
- Peng Xinye
- Pennisi Michele
- Perciballi Stefania
- Peresunko Dmitry Yurevich
- Peretti Pezzi Rafael
- Pestov Yury
- Petrov Vitalii
- Petrovici Mihai
- Piano Stefano
- Pikna Miroslav
- Pillot Philippe
- Pinazza Ombretta
- Pinsky Lawrence
- Pinto Chiara
- Pisano Silvia
- Planinic Mirko
- Pliatskas Stylianidis Christos
- Pliquett Fabian
- Ploskon Mateusz Andrzej
- Poghosyan Martin
- Polishchuk Boris
- Politano Stefano
- Poljak Nikola
- Pop Amalia
- Porteboeuf Sarah Julie
- Pozdniakov Valerii
- Pradhan Kshitish Kumar
- Prasad Sidharth Kumar
- Prasad Suraj
- Preghenella Roberto
- Prino Francesco
- Pruneau Claude Andre
- Pshenichnov Igor
- Puccio Maximiliano
- Pucillo Sara
- Pugelova Zuzana
- Qiu Shi
- Quaglia Luca
- Ragoni Simone
- Rai Ananya
- Rakotozafindrabe Andry Malala
- Ramello Luciano
- Rami Fouad
- Ramillien Barret Valerie
- Rasa Marika
- Rasanen Sami Sakari
- Rath Rutuparna
- Rauch Max Philip
- Ravasenga Ivan
- Read Kenneth Francis
- Reckziegel Christian
- Redelbach Andreas Ralph
- Redlich Krzysztof
- Reetz Carolina Anna
- Regules Medel Hector David
- Rehman Attiq Ur
- Reidt Felix
- Reme-Ness Haakon Andre
- Reygers Klaus Johannes
- Riabov Andrei
- Riabov Viktor
- Ricci Riccardo
- Richter Matthias Rudolph
- Riedel Anton Albert
- Riegler Werner
- Riffero Andrea Giovanni
- Ristea Catalin-Lucian
- Rodriguez Cahuantzi Mario
- Rodriguez Ramirez Saul Anibal
- Roeed Ketil
- Roehrich Dieter
- Rogalev Roman
- Rogochaya Elena
- Rogoschinski Tim Sebastian
- Rohr David Michael
- Rojas Torres Solangel
- Rokita Przemyslaw Stefan
- Romanenko Gleb
- Ronchetti Federico
- Rosano Antonina
- Roslon Krystian
- Rossi Andrea
- Roy Ankhi
- Roy Subhadeep
- Rubini Nicola
- Ruggiano Daniela
- Rui Rinaldo
- Russek Pawel Grzegorz
- Russo Roberto
- Rustamov Anar
- Ryabinkin Evgeny
- Ryabov Yury
- Rybicki Andrzej Krzysztof
- Rytkonen Heidi Maria
- Ryu Jaehyeok
- Rzesa Wioleta
- Saarimaki Oskari Antti Matti
- Sadhu Samrangy
- Sadovskiy Sergey
- Saetre Jon-Are
- Safarik Karel
- Saha Sumit Kumar
- Saha Swati
- Sahoo Bhagyarathi
- Sahoo Raghunath
- Sahoo Sarita
- Sahu Dushmanta
- Sahu Pradip Kumar
- Saini Jogender
- Sakai Shingo
- Sambyal Sanjeev Singh
- Samitz Daniel
- Sanna Isabella
- Sarkar - Sinha Tinku
- Sarkar Debojit
- Sarma Pranjal
- Sarritzu Valerio
- Sas Mike
- Sasikumar Menon Anjaly
- Sawan Sawan
- Scapparone Eugenio
- Schambach Johann Joachim
- Scheid Horst Sebastian
- Schiaua Claudiu Cornel
- Schicker Rainer Martin
- Schlepper Felix
- Schmah Alexander
- Schmidt Christian Joachim
- Schmidt Hans Rudolf
- Schmidt Marten Ole
- Schmidt Martin
- Schmidt Nicolas
- Schmier Austin Robert
- Schotter Romain
- Schukraft Jurgen
- Schweda Kai Oliver
- Scioli Gilda
- Scomparin Enrico
- Seger Janet Elizabeth
- Sekiguchi Yuko
- Sekihata Daiki
- Selina Mariia
- Selyuzhenkov Ilya
- Senyukov Serhiy
- Seo Jin Joo
- Serebryakov Dmitry
- Serkin Leonid
- Serksnyte Laura
- Setoue Liveraro Gianni Shigeru
- Sevcenco Adrian
- Shaba Tebogo Joyce
- Shabetai Alexandre
- Shahoyan Ruben
- Shangaraev Artem
- Sharma Binti
- Sharma Deependra
- Sharma Himanshu
- Sharma Meenakshi
- Sharma Samarth
- Sharma Sheetal
- Sharma Upasana
- Shatat Afnan
- Sheibani Oveis
- Shigaki Kenta
- Shin Jaehyuck
- Shirinkin Sergey
- Shou Qiye
- Sibiryak Yury
- Siddhanta Sabyasachi
- Siemiarczuk Teodor
- Silvermyr David Olle Rickard
- Simantathammakul Tawanchat
- Simeonov Radoslav
- Singh Balwan
- Singh Bhawani
- Singh Kamaljeet
- Singh Ranbir
- Singh Randhir
- Singh Ravindra
- Singh Sweta
- Singh Vivek
- Singhal Vikas
- Sitar Branislav
- Sitta Mario
- Skaali Bernhard
- Skorodumovs Georgijs
- Slupecki Maciej
- Smirnov Nikolai
- Snellings Raimond
- Song Jihye
- Sonnabend Christian
- Sonneveld Jorine
- Soramel Francesca
- Soto-Hernandez Analyce Bella
- Spijkers Rik
- Sputowska Iwona Anna
- Staa Joey
- Stachel Johanna
- Stan Ionel
- Steffanic Patrick John
- Stiefelmaier Stephan Friedrich
- Stocco Diego
- Storehaug Ida
- Stratmann Peter
- Strazzi Sofia
- Sturniolo Alessandro
- Suire Christophe Pierre
- Sukhanov Mikhail
- Suljic Miljenko
- Sultanov Rishat
- Sumberia Vikash
- Sumowidagdo Suharyo
- Szarka Imrich
- Szymkowski Maciej
- Taghavi Seyed Farid
- Taillepied Guillaume
- Takahashi Jun
- Tambave Ganesh Jagannath
- Tang Siyu
- Tang Zebo
- Tapia Takaki Daniel Jesus
- Tapus Nicolae
- Tarasovicova Lucia Anna
- Tarzila Madalina-Gabriela
- Tassielli Giovanni Francesco
- Tauro Arturo
- Tavira Garcia Andrea
- Tejeda Munoz Guillermo
- Telesca Adriana
- Terlizzi Livia
- Terrevoli Cristina
- Thakur Sanchari
- Thomas Deepa
- Tikhonov Anatoly
- Tiltmann Nicolas
- Timmins Anthony Robert
- Tkacik Milan
- Tkacik Tomas
- Toia Alberica
- Tokumoto Ryoka
- Tomohiro Keisuke
- Topilskaya Nataliya
- Toppi Marco
- Tork Theraa M.A
- Torres Cabrera Maria Fernanda
- Torres Ramos Arianna Grisel
- Trifiro Antonio
- Triolo Andrea Sofia
- Tripathy Sushanta
- Tripathy Tulika
- Trogolo Stefano
- Tropp Klaudia
- Trubnikov Victor
- Trzaska Wladyslaw Henryk
- Trzcinski Tomasz Piotr
- Tumkin Alexandr
- Turrisi Rosario
- Tveter Trine Spedstad
- Ullaland Kjetil
- Ulukutlu Berkin
- Uras Antonio
- Urioni Marta
- Usai Gianluca
- Vala Martin
- Valencia Torres Victor
- Valle Nicolo
- van Doremalen Lennart
- van Leeuwen Marco
- van Veen Casper Arie
- van Weelden Roelof Jan Gijs
- Vande Vyvre Pierre
- Varga Dezso
- Varga Zoltan
- Vargas Torres Paola
- Vasileiou Maria
- Vasiliev Andrey
- Vasquez Beltran Yael Antonio
- Vazquez Doce Oton
- Vazquez Rueda Omar
- Vechernin Vladimir
- Vercellin Ermanno
- Vergara Limon Sergio
- Verma Rahul
- Vermunt Lucas Anne
- Vertesi Robert
- Verweij Marta
- Vickovic Linda
- Vilakazi Zabulon
- Villalobos Baillie Orlando
- Villani Anna
- Vinogradov Alexander
- Viqueira Rodriguez Manuel
- Virgili Tiziano
- Virta Maxim Mikael Olavi
- Vislavicius Vytautas
- Vodopyanov Alexander
- Voelkel Benedikt
- Volkl Martin Andreas
- Voloshin Sergey
- Volpe Giacomo
- von Haller Barthelemy
- Vorobyev Ivan
- Vozniuk Nikita
- Vrlakova Janka
- Wan Jie
- Wang Chunzheng
- Wang Dongfang
- Wang Yuanzhe
- Wang Yubiao
- Wegrzynek Adam Tadeusz
- Weiglhofer Felix Thomas
- Wenzel Sandro Christian
- Wessels Johannes Peter
- Weyhmiller Sierra Lisa
- Wiechula Jens
- Wikne Jon
- Wilhelmi Alexander
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 10/12/2023
- Field of study
International audienceThe first measurements of femtoscopic correlations with the particle pair combinations π±KS0 in pp collisions at s=13 TeV at the Large Hadron Collider (LHC) are reported by the ALICE experiment. Using the femtoscopic approach, it is shown that it is possible to study the elusive K0∗(700) particle that has been considered a tetraquark candidate for over forty years. Boson source parameters and final-state interaction parameters are extracted by fitting a model assuming a Gaussian source to the experimentally measured two-particle correlation functions. The final-state interaction is modeled through a resonant scattering amplitude, defined in terms of a mass and a coupling parameter, decaying into a π±KS0 pair. The extracted mass and Breit-Wigner width, derived from the coupling parameter, of the final-state interaction are found to be consistent with previous measurements of the K0∗(700). The small value and increasing behavior of the correlation strength with increasing source size support the hypothesis that the K0∗(700) is a four-quark state, i.e. a tetraquark state. This latter trend is also confirmed via a simple geometric model that assumes a tetraquark structure of the K0∗(700) resonance
Investigating the nature of the K0∗(700) state with π±KS0 correlations at the LHC
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Al-Turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
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- Wikne Jon
- Wilhelmi Alexander
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 04/01/2024
- Field of study
International audienceThe first measurements of femtoscopic correlations with the particle pair combinations π±KS0 in pp collisions at s=13 TeV at the Large Hadron Collider (LHC) are reported by the ALICE experiment. Using the femtoscopic approach, it is shown that it is possible to study the elusive K0∗(700) particle that has been considered a tetraquark candidate for over forty years. Boson source parameters and final-state interaction parameters are extracted by fitting a model assuming a Gaussian source to the experimentally measured two-particle correlation functions. The final-state interaction is modeled through a resonant scattering amplitude, defined in terms of a mass and a coupling parameter, decaying into a π±KS0 pair. The extracted mass and Breit-Wigner width, derived from the coupling parameter, of the final-state interaction are found to be consistent with previous measurements of the K0∗(700). The small value and increasing behavior of the correlation strength with increasing source size support the hypothesis that the K0∗(700) is a four-quark state, i.e. a tetraquark state. This latter trend is also confirmed via a simple geometric model that assumes a tetraquark structure of the K0∗(700) resonance
Investigating the nature of the K0∗(700) state with π±KS0 correlations at the LHC
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Al-Turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa
- Andrei Cristian
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- Andronov Evgeny
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- Wilhelmi Alexander
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- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 04/01/2024
- Field of study
International audienceThe first measurements of femtoscopic correlations with the particle pair combinations π±KS0 in pp collisions at s=13 TeV at the Large Hadron Collider (LHC) are reported by the ALICE experiment. Using the femtoscopic approach, it is shown that it is possible to study the elusive K0∗(700) particle that has been considered a tetraquark candidate for over forty years. Boson source parameters and final-state interaction parameters are extracted by fitting a model assuming a Gaussian source to the experimentally measured two-particle correlation functions. The final-state interaction is modeled through a resonant scattering amplitude, defined in terms of a mass and a coupling parameter, decaying into a π±KS0 pair. The extracted mass and Breit-Wigner width, derived from the coupling parameter, of the final-state interaction are found to be consistent with previous measurements of the K0∗(700). The small value and increasing behavior of the correlation strength with increasing source size support the hypothesis that the K0∗(700) is a four-quark state, i.e. a tetraquark state. This latter trend is also confirmed via a simple geometric model that assumes a tetraquark structure of the K0∗(700) resonance
Investigating the nature of the K0∗(700) state with π±KS0 correlations at the LHC
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Al-Turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
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- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
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- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
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- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
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- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 04/01/2024
- Field of study
International audienceThe first measurements of femtoscopic correlations with the particle pair combinations π±KS0 in pp collisions at s=13 TeV at the Large Hadron Collider (LHC) are reported by the ALICE experiment. Using the femtoscopic approach, it is shown that it is possible to study the elusive K0∗(700) particle that has been considered a tetraquark candidate for over forty years. Boson source parameters and final-state interaction parameters are extracted by fitting a model assuming a Gaussian source to the experimentally measured two-particle correlation functions. The final-state interaction is modeled through a resonant scattering amplitude, defined in terms of a mass and a coupling parameter, decaying into a π±KS0 pair. The extracted mass and Breit-Wigner width, derived from the coupling parameter, of the final-state interaction are found to be consistent with previous measurements of the K0∗(700). The small value and increasing behavior of the correlation strength with increasing source size support the hypothesis that the K0∗(700) is a four-quark state, i.e. a tetraquark state. This latter trend is also confirmed via a simple geometric model that assumes a tetraquark structure of the K0∗(700) resonance
Common femtoscopic hadron-emission source in pp collisions at the LHC
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Al-Turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
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- Augustinus Andre
- Averbeck Ralf Peter
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- Voloshin Sergey
- Volpe Giacomo
- von Haller Barthelemy
- Vorobyev Ivan
- Vozniuk Nikita
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- Wan Jie
- Wang Chunzheng
- Wang Dongfang
- Wang Yuanzhe
- Wang Yubiao
- Wegrzynek Adam Tadeusz
- Weiglhofer Felix Thomas
- Wenzel Sandro Christian
- Wessels Johannes Peter
- Weyhmiller Sierra Lisa
- Wiechula Jens
- Wikne Jon
- Wilhelmi Alexander
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 05/12/2023
- Field of study
International audienceThe femtoscopic study of pairs of identical pions is particularly suited to investigate the effective source function of particle emission, due to the resulting Bose-Einstein correlation signal. In small collision systems at the LHC, pp in particular, the majority of the pions are produced in resonance decays, which significantly affect the profile and size of the source. In this work, we explicitly model this effect in order to extract the primordial source in pp collisions at s=13 TeV from charged π-π correlations measured by ALICE. We demonstrate that the assumption of a Gaussian primordial source is compatible with the data and that the effective source, resulting from modifications due to resonances, is approximately exponential, as found in previous measurements at the LHC. The universality of hadron emission in pp collisions is further investigated by applying the same methodology to characterize the primordial source of K-p pairs. The size of the primordial source is evaluated as a function of the transverse mass (mT) of the pairs, leading to the observation of a common scaling for both π-π and K-p, suggesting a collective effect. Further, the present results are compatible with the mT scaling of the p-p and p−Λ primordial source measured by ALICE in high multiplicity pp collisions, providing compelling evidence for the presence of a common emission source for all hadrons in small collision systems at the LHC. This will allow the determination of the source function for any hadron--hadron pairs with high precision, granting access to the properties of the possible final-state interaction among pairs of less abundantly produced hadrons, such as strange or charmed particles
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