Dielectron production in proton-proton collisions at s = 7 $$ \sqrt{s}=7 $$ TeV
2018
- Shreyasi Acharya
- Fernando Torales Acosta
- Dagmar Adamová
- Jonatan Adolfsson
- M. M. Aggarwal
- G. Aglieri Rinella
- Michelangelo Agnello
- N. Agrawal
- Zubayer Ahammed
- Sang Un Ahn
- Salvatore Aiola
- Alexander Akindinov
- Mohammed Al-Turany
- Sk Noor Alam
- D. S. D. Albuquerque
- Dmitry Aleksandrov
- Bruno Alessandro
- R Alfaro-Molina
- Yasir Ali
- A. Alici
- Anton Alkin
- Johan Alme
- Torsten Alt
- Lucas Altenkamper
- Igor Altsybeev
- Mustafa Naji Anaam
- Cristian Andrei
- Dimitra Andreou
- Harry Arthur Andrews
- Anton Andronic
- Massimo Angeletti
- Venelin Anguelov
- Christopher Daniel Anson
- T. Antičić
- F. Antinori
- Pietro Antonioli
- Rafay Anwar
- Nicole Apadula
- Laurent Bernard Aphecetche
- H. Appelshäuser
- Silvia Arcelli
- R. Arnaldi
- Oliver Werner Arnold
- I. C. Arsene
- Mesut Arslandok
- Benjamin Audurier
- Andre Augustinus
- Ralf Peter Averbeck
- Mohd Danish Azmi
- A. Badalà
- Yong Wook Baek
- Stefano Bagnasco
- Raphaelle Marie Bailhache
- Renu Bala
- Alberto Baldisseri
- Markus Ball
- Rama Chandra Baral
- Anastasia Maria Barbano
- Roberto Barbera
- Francesco Barile
- Luca Barioglio
- G. G. Barnaföldi
- Lee Stuart Barnby
- Valerie Ramillien Barret
- Paolo Bartalini
- K. Barth
- Esther Bartsch
- N. Bastid
- Sumit Basu
- Guillaume Batigne
- Boris Batyunya
- Paul Christoph Batzing
- J.L. Bazo Alba
- I. G. Bearden
- Hans Beck
- Cristina Bedda
- N. K. Behera
- Iouri Belikov
- Francesca Bellini
- H. Bello Martinez
- Rene Bellwied
- Lucina Gabriela Espinoza Beltran
- Vladimir Belyaev
- Gyula Bencedi
- S. Beole
- Alexandru Bercuci
- Y. Berdnikov
- D. Berenyi
- Redmer Alexander Bertens
- Dario Berzano
- Latchezar Betev
- Partha Pratim Bhaduri
- Anju Bhasin
- Inayat Rasool Bhat
- Himani Bhatt
- Buddhadeb Bhattacharjee
- Jihyun Bhom
- Antonio Bianchi
- Livio Bianchi
- N. Bianchi
- Jaroslav Bielcik
- Jana Bielcikova
- Ante Bilandzic
- Gabor Biro
- Rathijit Biswas
- Saikat Biswas
- Justin Thomas Blair
- Dmitry Blau
- Christoph Blume
- Gianluigi Boca
- Friederike Bock
- A. G. Bogdanov
- Laszlo Boldizsar
- M. Bombara
- Germano Bonomi
- Matthias Bonora
- Herve Borel
- Alexander Borissov
- Marcello Borri
- Elena Botta
- Christian Bourjau
- Lars Bratrud
- P. Braun-Munzinger
- Marco Bregant
- Theo Alexander Broker
- Michal Broz
- Erik Jens Brucken
- Emilio M. Bruna
- Giuseppe Eugenio Bruno
- Dmitry Budnikov
- Henner Buesching
- Stefania Bufalino
- Paul Bühler
- Predrag Buncic
- Oliver Busch
- Z. Buthelezi
- Jamila Bashir Butt
- Jesse Thomas Buxton
- Jan Cabala
- Davide Caffarri
- Helen Louise Caines
- Alberto Caliva
- E. Calvo Villar
- Rabi Soto Camacho
- Paolo Camerini
- Aaron Allan Capon
- F. Carena
- Wisla Carena
- Francesca Carnesecchi
- J. Castillo Castellanos
- A. J. Castro
- Ester Anna Rita Casula
- C Ceballos Sánchez
- Sinjini Chandra
- Beomsu Chang
- Wan Chang
- Sylvain Chapeland
- Marielle Chartier
- Sukalyan Chattopadhyay
- Alex Chauvin
- Cvetan Valeriev Cheshkov
- Brigitte Cheynis
- V. Chibante Barroso
- D. D. Chinellato
- Soyeon Cho
- Peter Chochula
- Tasnuva Chowdhury
- Panagiotis Christakoglou
- C. H. Christensen
- Peter Christiansen
- Tatsuya Chujo
- Suh Urk Chung
- Corrado Cicalo
- Luisa Cifarelli
- Federico Cindolo
- Jean Willy Andre Cleymans
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- Alberto Collu
- Manuel Colocci
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- G. Conesa Balbastre
- Z. Conesa del Valle
- J. G. Contreras
- Thomas Michael Cormier
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- Mauro Rogerio Cosentino
- Filippo Costa
- Susanna Costanza
- Jana Crkovska
- Philippe Crochet
- E. Cuautle
- L. Cunqueiro
- Torsten Dahms
- A. Dainese
- S. Dani
- Meike Charlotte Danisch
- Andrea Danu
- Debabrata Das
- Indranil Das
- Supriya Das
- Ajay Kumar Dash
- S. Dash
- Sudipan De
- A. De Caro
- G. de Cataldo
- C. de Conti
- J. de Cuveland
- A. De Falco
- D. De Gruttola
- N. De Marco
- S. De Pasquale
- R. Derradi de Souza
- Hermann Franz Degenhardt
- Alexander Deisting
- Andrzej Deloff
- Silvia Delsanto
- Caterina Deplano
- Preeti Dhankher
- D. Di Bari
- A. Di Mauro
- B. Di Ruzza
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- Thomas Dietel
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- Yanchun Ding
- Roberto Divia
- Øystein Djuvsland
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- Benjamin Donigus
- Olja Dordic
- L. V. R. Doremalen
- Anand Kumar Dubey
- Andrea Dubla
- Laurent Ducroux
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- Pascal Dupieux
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- A. Feliciello
- Grigorii Feofilov
- A. Fernandez-Tellez
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- Andrea Festanti
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- Jan Figiel
- M. A. S. Figueredo
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- Sergey Fokin
- Enrico Fragiacomo
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- U. Frankenfeld
- Gabriele Gaetano Fronze
- Ulrich Fuchs
- Christophe Furget
- Artur Furs
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- J. J. Gaardhøje
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- S. K. Ghosh
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- H. Kim
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- T. Kim
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- A. Ohlson
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- Andile Mothegi Whitehead
- J. Wiechula
- Jon Wikne
- Grzegorz Andrzej Wilk
- Jeremy John Wilkinson
- Guido Alexander Willems
- M. C. S. Williams
- Emily Willsher
- Bernd Stefan Windelband
- William Edward Witt
- Rong Xu
- Serpil Yalcin
- Kosei Yamakawa
- Satoshi Yano
- Z. Yin
- Hiroki Yokoyama
- I. K. Yoo
- J. H. Yoon
- Volodymyr Yurchenko
- Valentina Zaccolo
- Ali Zaman
- Chiara Zampolli
- H. J. C. Zanoli
- Nima Zardoshti
- Andrey Zarochentsev
- Petr Závada
- N. Zaviyalov
- H. Zbroszczyk
- Mikhail Zhalov
- Xiaoming Zhang
- Yinhong Zhang
- Z. H. Zhang
- Chengxin Zhao
- Vladimir Zherebchevskii
- Natalia Zhigareva
- Dai-Mei Zhou
- You Zhou
- Zhuo Zhou
- Hongsheng Zhu
- J. Zhu
- Ya Zhu
- Antonino Zichichi
- Markus Bernhard Zimmermann
- Gennady Zinovjev
- J. Zmeskal
- Shuguang Zou
The first measurement of e+e− pair production at mid-rapidity (|ηe| < 0.8) in pp collisions at $$ \sqrt{s}=7 $$
TeV with ALICE at the LHC is presented. The dielectron production is studied as a function of the invariant mass (mee < 3.3 GeV/c2), the pair transverse momentum (pT,ee < 8 GeV/c), and the pair transverse impact parameter (DCAee), i.e., the average distance of closest approach of the reconstructed electron and positron tracks to the collision vertex, normalised to its resolution. The results are compared with the expectations from a cocktail of known hadronic sources and are well described when PYTHIA is used to generate the heavy-flavour contributions. In the low-mass region (0.14 < mee < 1.1 GeV/c2), prompt and non-prompt e+e− sources can be separated via the DCAee. In the intermediate-mass region (1.1 < mee < 2.7 GeV/c2), a double-differential fit to the data in mee and pT,ee and a fit of the DCAee distribution allow the total $$ \mathrm{c}\overline{\mathrm{c}} $$
and $$ \mathrm{b}\overline{\mathrm{b}} $$
cross sections to be extracted. Two different event generators, PYTHIA and POWHEG, can reproduce the shape of the two-dimensional mee and pT,ee spectra, as well as the shape of the DCAee distribution, reasonably well. However, differences in the $$ \mathrm{c}\overline{\mathrm{c}} $$
and $$ \mathrm{b}\overline{\mathrm{b}} $$
cross sections are observed when using the generators to extrapolate to full phase space. Finally, the ratio of inclusive to decay photons is studied via the measurement of virtual direct photons in the transverse-momentum range 1 < pT < 8 GeV/c. This is found to be unity within the statistical and systematic uncertainties and consistent with expectations from next-to-leading order perturbative quantum chromodynamic calculations.
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