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Annihilation dynamics plays a fundamental role in the baryon-antibaryon interaction (B-(B) over bar) at low-energy and its strength and range are crucial in the assessment of possible baryonic bound states. Experimental data on annihilation cross sections are available for the p-(p) over bar system but not in the low relative momentum region. Data regarding the B-(B) over bar interaction with strange degrees of freedom are extremely scarce, hence the modeling of the annihilation contributions is mainly based on nucleon-antinucleon (N-(N) over bar) results, when available. In this letter we present a measurement of the p-(p) over bar, p-(Lambda) over bar circle plus(p) over bar-Lambda and Lambda-(Lambda) over bar interaction using correlation functions in the relative momentum space in high-multiplicity triggered pp collisions at root s = 13 TeV recorded by ALICE at the LHC. In the p-(p) over bar system the couplings to the mesonic channels in different partial waves are extracted by adopting a coupled-channel approach with recent chi EFT potentials. The inclusion of these inelastic channels provides good agreement with the data, showing a significant presence of the annihilation term down to zero momentum. Predictions obtained using the Lednicky-Lyuboshits formula and scattering parameters obtained from heavy-ion collisions, hence mainly sensitive to elastic processes, are compared with the experimental p-(Lambda) over bar circle plus(p) over bar-Lambda and Lambda-(Lambda) over bar correlations. The model describes the Lambda-(Lambda) over bar data and underestimates the p-(Lambda) over bar circle plus(p) over bar-Lambda data in the region of momenta below 200 MeV/c. The observed deviation indicates a different contribution of annihilation channels to the two systems containing strange hadrons. (C) 2022 European Organization for Nuclear Research. Published by Elsevier B.V.
Investigating the role of strangeness in baryon-antibaryon annihilation at the LHC / Acharya, S., Adamov??, D., Adler, A., Adolfsson, J., Aglieri Rinella, G., Agnello, M., Agrawal, N., Ahammed, Z., Ahmad, S., Ahn, S.U., Ahuja, I., Akbar, Z., Akindinov, A., Al-Turany, M., Alam, S.N., Aleksandrov, D., Alessandro, B., Alfanda, H.M., Alfaro Molina, R., Ali, B., et al.. - In: PHYSICS LETTERS. SECTION B. - ISSN 0370-2693. - 829:(2022). [10.1016/j.physletb.2022.137060]
Investigating the role of strangeness in baryon-antibaryon annihilation at the LHC
S. Acharya;D. Adamov??;A. Adler;J. Adolfsson;G. Aglieri Rinella;M. Agnello;N. Agrawal;Z. Ahammed;S. Ahmad;S. U. Ahn;I. Ahuja;Z. Akbar;A. Akindinov;M. Al-Turany;S. N. Alam;D. Aleksandrov;B. Alessandro;H. M. Alfanda;R. Alfaro Molina;B. Ali;Y. Ali;A. Alici;N. Alizadehvandchali;A. Alkin;J. Alme;T. Alt;L. Altenkamper;I. Altsybeev;M. N. Anaam;C. Andrei;D. Andreou;A. Andronic;M. Angeletti;V. Anguelov;F. Antinori;P. Antonioli;C. Anuj;N. Apadula;L. Aphecetche;H. Appelsh??user;S. Arcelli;R. Arnaldi;I. C. Arsene;M. Arslandok;A. Augustinus;R. Averbeck;S. Aziz;M. D. Azmi;A. Badal??;Y. W. Baek;X. Bai;R. Bailhache;Y. Bailung;R. Bala;A. Balbino;A. Baldisseri;B. Balis;M. Ball;D. Banerjee;R. Barbera;L. Barioglio;M. Barlou;G. G. Barnaf??ldi;L. S. Barnby;V. Barret;C. Bartels;K. Barth;E. Bartsch;F. Baruffaldi;N. Bastid;S. Basu;G. Batigne;B. Batyunya;D. Bauri;J. L. Bazo Alba;I. G. Bearden;C. Beattie;I. Belikov;A. D. C. Bell Hechavarria;F. Bellini;R. Bellwied;S. Belokurova;V. Belyaev;G. Bencedi;S. Beole;A. Bercuci;Y. Berdnikov;A. Berdnikova;D. Berenyi;L. Bergmann;M. G. Besoiu;L. Betev;P. P. Bhaduri;A. Bhasin;I. R. Bhat;M. A. Bhat;B. Bhattacharjee;P. Bhattacharya;L. Bianchi;N. Bianchi;J. Biel????k;J. Biel????kov??;J. Biernat;A. Bilandzic;G. Biro;S. Biswas;J. T. Blair;D. Blau;M. B. Blidaru;C. Blume;G. Boca;F. Bock;A. Bogdanov;S. Boi;J. Bok;L. Boldizs??r;A. Bolozdynya;M. Bombara;P. M. Bond;G. Bonomi;H. Borel;A. Borissov;H. Bossi;E. Botta;L. Bratrud;P. Braun-Munzinger;M. Bregant;M. Broz;G. E. Bruno;M. D. Buckland;D. Budnikov;H. Buesching;S. Bufalino;O. Bugnon;P. Buhler;Z. Buthelezi;J. B. Butt;S. A. Bysiak;D. Caffarri;M. Cai;H. Caines;A. Caliva;E. Calvo Villar;J. M. M. Camacho;R. S. Camacho;P. Camerini;F. D. M. Canedo;F. Carnesecchi;R. Caron;J. Castillo Castellanos;E. A. R. Casula;F. Catalano;C. Ceballos Sanchez;P. Chakraborty;S. Chandra;S. Chapeland;M. Chartier;S. Chattopadhyay;S. Chattopadhyay;A. Chauvin;T. G. Chavez;C. Cheshkov;B. Cheynis;V. Chibante Barroso;D. D. Chinellato;S. Cho;P. Chochula;P. Christakoglou;C. H. Christensen;P. Christiansen;T. Chujo;C. Cicalo;L. Cifarelli;F. Cindolo;M. R. Ciupek;G. Clai;J. Cleymans;F. Colamaria;J. S. Colburn;D. Colella;A. Collu;M. Colocci;M. Concas;G. Conesa Balbastre;Z. Conesa del Valle;G. Contin;J. G. Contreras;M. L. Coquet;T. M. Cormier;P. Cortese;M. R. Cosentino;F. Costa;S. Costanza;P. Crochet;E. Cuautle;P. Cui;L. Cunqueiro;A. Dainese;F. P. A. Damas;M. C. Danisch;A. Danu;I. Das;P. Das;P. Das;S. Das;S. Dash;S. De;A. De Caro;G. de Cataldo;L. De Cilladi;J. de Cuveland;A. De Falco;D. De Gruttola;N. De Marco;C. De Martin;S. De Pasquale;S. Deb;H. F. Degenhardt;K. R. Deja;L. Dello Stritto;S. Delsanto;W. Deng;P. Dhankher;D. Di Bari;A. Di Mauro;R. A. Diaz;T. Dietel;Y. Ding;R. Divi??;D. U. Dixit;??. Djuvsland;U. Dmitrieva;J. Do;A. Dobrin;B. D??nigus;O. Dordic;A. K. Dubey;A. Dubla;S. Dudi;M. Dukhishyam;P. Dupieux;N. Dzalaiova;T. M. Eder;R. J. Ehlers;V. N. Eikeland;D. Elia;B. Erazmus;F. Ercolessi;F. Erhardt;A. Erokhin;M. R. Ersdal;B. Espagnon;G. Eulisse;D. Evans;S. Evdokimov;L. Fabbietti;M. Faggin;J. Faivre;F. Fan;A. Fantoni;M. Fasel;P. Fecchio;A. Feliciello;G. Feofilov;A. Fern??ndez T??llez;A. Ferrero;A. Ferretti;V. J. G. Feuillard;J. Figiel;S. Filchagin;D. Finogeev;F. M. Fionda;G. Fiorenza;F. Flor;A. N. Flores;S. Foertsch;P. Foka;S. Fokin;E. Fragiacomo;E. Frajna;U. Fuchs;N. Funicello;C. Furget;A. Furs;J. J. Gaardh??je;M. Gagliardi;A. M. Gago;A. Gal;C. D. Galvan;P. Ganoti;C. Garabatos;J. R. A. Garcia;E. Garcia-Solis;K. Garg;C. Gargiulo;A. Garibli;K. Garner;P. Gasik;E. F. Gauger;A. Gautam;M. B. Gay Ducati;M. Germain;J. Ghosh;P. Ghosh;S. K. Ghosh;M. Giacalone;P. Gianotti;P. Giubellino;P. Giubilato;A. M. C. Glaenzer;P. Gl??ssel;D. J. Q. Goh;V. Gonzalez;L. H. Gonz??lez-Trueba;S. Gorbunov;M. Gorgon;L. G??rlich;S. Gotovac;V. Grabski;L. K. Graczykowski;L. Greiner;A. Grelli;C. Grigoras;V. Grigoriev;A. Grigoryan;S. Grigoryan;O. S. Groettvik;F. Grosa;J. F. Grosse-Oetringhaus;R. Grosso;G. G. Guardiano;R. Guernane;M. 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Trzcinski;B. A. Trzeciak;A. Tumkin;R. Turrisi;T. S. Tveter;K. Ullaland;A. Uras;M. Urioni;G. L. Usai;M. Vala;N. Valle;S. Vallero;N. van der Kolk;L. V. R. van Doremalen;M. van Leeuwen;P. Vande Vyvre;D. Varga;Z. Varga;M. Varga-Kofarago;A. Vargas;M. Vasileiou;A. Vasiliev;O. V??zquez Doce;V. Vechernin;E. Vercellin;S. Vergara Lim??n;L. Vermunt;R. V??rtesi;M. Verweij;L. Vickovic;Z. Vilakazi;O. Villalobos Baillie;G. Vino;A. Vinogradov;T. Virgili;V. Vislavicius;A. Vodopyanov;B. Volkel;M. A. V??lkl;K. Voloshin;S. A. Voloshin;G. Volpe;B. von Haller;I. Vorobyev;D. Voscek;J. Vrl??kov??;B. Wagner;C. Wang;D. Wang;M. Weber;R. J. G. V. Weelden;A. Wegrzynek;S. C. Wenzel;J. P. Wessels;J. Wiechula;J. Wikne;G. Wilk;J. Wilkinson;G. A. Willems;B. Windelband;M. Winn;W. E. Witt;J. R. Wright;W. Wu;Y. Wu;R. Xu;S. Yalcin;Y. Yamaguchi;K. Yamakawa;S. Yang;S. Yano;Z. Yin;H. Yokoyama;I. -K. Yoo;J. H. Yoon;S. Yuan;A. Yuncu;V. Zaccolo;A. Zaman;C. Zampolli;H. J. C. Zanoli;N. Zardoshti;A. Zarochentsev;P. Z??vada;N. Zaviyalov;H. Zbroszczyk;M. Zhalov;S. Zhang;X. Zhang;Y. Zhang;V. Zherebchevskii;Y. Zhi;D. Zhou;Y. Zhou;J. Zhu;Y. Zhu;A. Zichichi;G. Zinovjev;N. Zurlo
2022
Abstract
Annihilation dynamics plays a fundamental role in the baryon-antibaryon interaction (B-(B) over bar) at low-energy and its strength and range are crucial in the assessment of possible baryonic bound states. Experimental data on annihilation cross sections are available for the p-(p) over bar system but not in the low relative momentum region. Data regarding the B-(B) over bar interaction with strange degrees of freedom are extremely scarce, hence the modeling of the annihilation contributions is mainly based on nucleon-antinucleon (N-(N) over bar) results, when available. In this letter we present a measurement of the p-(p) over bar, p-(Lambda) over bar circle plus(p) over bar-Lambda and Lambda-(Lambda) over bar interaction using correlation functions in the relative momentum space in high-multiplicity triggered pp collisions at root s = 13 TeV recorded by ALICE at the LHC. In the p-(p) over bar system the couplings to the mesonic channels in different partial waves are extracted by adopting a coupled-channel approach with recent chi EFT potentials. The inclusion of these inelastic channels provides good agreement with the data, showing a significant presence of the annihilation term down to zero momentum. Predictions obtained using the Lednicky-Lyuboshits formula and scattering parameters obtained from heavy-ion collisions, hence mainly sensitive to elastic processes, are compared with the experimental p-(Lambda) over bar circle plus(p) over bar-Lambda and Lambda-(Lambda) over bar correlations. The model describes the Lambda-(Lambda) over bar data and underestimates the p-(Lambda) over bar circle plus(p) over bar-Lambda data in the region of momenta below 200 MeV/c. The observed deviation indicates a different contribution of annihilation channels to the two systems containing strange hadrons. (C) 2022 European Organization for Nuclear Research. Published by Elsevier B.V.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11583/2971887
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simulazione ASN
Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande.
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