Suppression of $\Lambda(1520)$ resonance production in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
2019
- Shreyasi Acharya
- Fernando Torales Acosta
- D. Adamová
- Jonatan Adolfsson
- M. M. Aggarwal
- Gianluca Aglieri Rinella
- Michelangelo Agnello
- Neelima Agrawal
- Z. Ahammed
- Sang Un Ahn
- S. Aiola
- A. Akindinov
- Mohammad Al-turany
- Sk Noor Alam
- Danilo Silva De Albuquerque
- Dmitry Aleksandrov
- Bruno Alessandro
- J. Molina
- Yasir Ali
- Andrea Alici
- Anton Alkin
- J. Alme
- T. Alt
- Lucas Altenkamper
- Igor Altsybeev
- Mustafa Naji Anaam
- Cristian Andrei
- Dimitra Andreou
- Harry Arthur Andrews
- A. Andronic
- Massimo Angeletti
- Venelin Anguelov
- Christopher Daniel Anson
- Tome Anticic
- F. Antinori
- Pietro Antonioli
- Rafay Anwar
- Nicole Apadula
- L. Aphecetche
- Harald Appelshaeuser
- S. Arcelli
- R. Arnaldi
- O. W. Arnold
- Ionut Cristian Arsene
- M. Arslandok
- B. Audurier
- Andre Augustinus
- Ralf Peter Averbeck
- M. D. Azmi
- Angela Badala
- Yong Wook Baek
- S. Bagnasco
- Raphaelle Marie Bailhache
- Renu Bala
- A. Baldisseri
- M. Ball
- Rama Chandra Baral
- A. M. Barbano
- R. Barbera
- Francesco Barile
- Luca Barioglio
- Gergely Gabor Barnafoldi
- Lee Stuart Barnby
- V. Barret
- P. Bartalini
- K. Barth
- E. Bartsch
- Nicole Bastid
- Sumit Basu
- G. Batigne
- B. Batyunya
- P. C. Batzing
- Jose Luis Bazo Alba
- Ian Gardner Bearden
- Hans Peter Beck
- C. Bedda
- N. K. Behera
- I. Belikov
- Francesca Bellini
- Hector Bello Martinez
- R. Bellwied
- Lucina Gabriela Espinoza Beltran
- V. Belyaev
- G. Bencedi
- S. Beole
- A. Bercuci
- Yaroslav Berdnikov
- Daniel Berenyi
- R. A. Bertens
- Dario Berzano
- L. Betev
- Partha Pratim Bhaduri
- Anju Bhasin
- I. R. Bhat
- H. Bhatt
- B. Bhattacharjee
- J. Bhom
- Antonio Bianchi
- Livio Bianchi
- Nicola Bianchi
- J. Bielcik
- J. Bielcikova
- Ante Bilandzic
- G. Biro
- R. Biswas
- S. Biswas
- J. T. Blair
- Dmitry Blau
- C. Blume
- G. Boca
- F. Bock
- Alexey Bogdanov
- Laszlo Boldizsar
- Marek Bombara
- G. Bonomi
- M. Bonora
- H. Borel
- A. Borissov
- M. Borri
- E. Botta
- C. Bourjau
- Lars Bratrud
- P. Braun-Munzinger
- Marco Bregant
- T. A. Broker
- Michal Broz
- E. Brucken
- Elena Bruna
- Giuseppe Eugenio Bruno
- Dmitry Budnikov
- H. Buesching
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- P. Buhler
- P. Buncic
- O. Busch
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- J. Butt
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- H. Caines
- A. Caliva
- Ernesto Calvo Villar
- Rabi Soto Camacho
- Paolo Camerini
- Aaron Allan Capon
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- W. Carena
- F. Carnesecchi
- Javier Ernesto Castillo Castellanos
- A. Castro
- Ester Anna Rita Casula
- Cesar Ceballos Sanchez
- Sinjini Chandra
- Beomsu Chang
- Wan Chang
- S. Chapeland
- Marielle Chartier
- Subhasis Chattopadhyay
- S. Chattopadhyay
- A. Chauvin
- C. Cheshkov
- B. Cheynis
- Vasco Miguel Chibante Barroso
- David Dobrigkeit Chinellato
- Soyeon Cho
- P. Chochula
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- P. Christiansen
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- Indranil Das
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- Sadhana Dash
- S. De
- Annalisa De Caro
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- D. De Gruttola
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- S. Yano
- Z. Yin
- H. Yokoyama
- In Kwon Yoo
- Jin Hee Yoon
- V. Yurchenko
- V. Zaccolo
- A. Zaman
- C. Zampolli
- Henrique Jose Correa Zanoli
- N. Zardoshti
- A. Zarochentsev
- P. Závada
- Nikolay Zavyalov
- H. Zbroszczyk
- Mikhail Zhalov
- Xiaoming Zhang
- Yonghong Zhang
- Z. Zhang
- C. Zhao
- Vladimir Zherebchevskii
- N. Zhigareva
- Daicui Zhou
- You Zhou
- Zhuo Zhou
- H. Zhu
- Jianhui Zhu
- Ya Zhu
- A. Zichichi
- M. B. Zimmermann
- G. Zinovjev
- Johann Zmeskal
- Shuguang Zou
The production yield of the Λ(1520) baryon resonance is measured at midrapidity in Pb-Pb collisions at sNN = 2.76 TeV with the ALICE detector at the Large Hadron Collider (LHC). The measurement is performed in the Λ(1520)→pK− (and charge conjugate) hadronic decay channel as a function of the transverse momentum (pT) and collision centrality. The ratio of the pT-integrated production of Λ(1520) baryons relative to Λ baryons in central collisions is suppressed by about a factor of 2 with respect to peripheral collisions. This is the first observation of the suppression of a baryonic resonance at the LHC and the first 3σ evidence of Λ(1520) suppression within a single collision system. The measured Λ(1520)/Λ ratio in central collisions is smaller than the value predicted by the statistical hadronization model calculations. The shape of the measured pT distribution and the centrality dependence of the suppression are reproduced by the EPOS3 Monte Carlo event generator. The measurement adds further support to the formation of a dense hadronic phase in the final stages of the evolution of the fireball created in heavy-ion collisions, lasting long enough to cause a significant reduction in the observable yield of short-lived resonances.
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