9 research outputs found
PERFIL SANITÁRIO DE UNIDADES AGRÍCOLAS FAMILIARES PRODUTORAS DE LEITE CRU E ADEQUAÇÃO À LEGISLAÇÃO VIGENTE
- Author
- Almeida AC
- Amaral LA
- Arcuri EF
- Belchior APC
- Brito JRF
- Brito MAVP
- Brito MAVP
- Bueno VFF
- Busato A
- Coentrão CM
- Conboy MJ
- Ericsson UH
- Fagan EP
- Fassio LL
- Fernandes SAA
- Fröberg S
- Fröberg S
- Gonzalez HL
- Gonzalez HL
- Gonzalez SG
- González-Sedano M
- Guerreiro PK
- Martins MEP
- Matsubara MT
- Monteiro AM
- Nero LA
- Oliveira JLP
- Pinto CLO
- Polegato EPS
- Ramos LS
- Rezende ESJ
- Salfinger Y
- Sancanari JBD
- Santos CA
- Silva LCC
- Souza RP
- Topçu A
- Torres RA
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Appelt C
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin JF
- Argyropoulos S
- Arling JH
- Armbruster AJ
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avner G
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
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- Backman F
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- Bahilo JJL
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- Balasubramanian R
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- Bandyopadhyay A
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- Bergmann B
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- Bielski R
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Biondini A
- Birch-sykes CJ
- Bird GA
- Birman M
- Bisanz T
- Biswal JP
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- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blumenthal J
- Bobbink GJ
- Bobrovnikov VS
- Boehler M
- Boeriu OEV
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bolanos GR
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbely AG
- Borecka-Bielska HM
- Borgna LS
- Borissov G
- Bortoletto D
- Bosca SR
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bouquet R
- Bourdarios CA
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bracinik J
- Brahimi N
- Brandt G
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- Brau JE
- Brendlinger K
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- Brenner L
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- Brock I
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- Bruschi M
- Bruscino N
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
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- Bugge MK
- Bulekov O
- Bullard BA
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- Buttinger W
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- Calafiura P
- Calderini G
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- Callea G
- Caloba LP
- Calvet D
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- Calvetti M
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- Camarri P
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- Camerlingo MT
- Cameron D
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- Carducci G
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- Carlson BT
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- Carlson TI
- Carminati L
- Carnesale M
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- Casado MP
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- Castillo LRF
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- Catmore JR
- Cavaliere V
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- Celli F
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- Cerri A
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- Cerutti F
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- Chakraborty D
- Chala M
- Chan J
- Chan WS
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- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen B
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- Chen H
- Chen H
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen X
- Chen Y
- Cheng CL
- Cheng HC
- Cheplakov A
- Cheremushkina E
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- Chevalier L
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- Chudoba J
- Chwastowski JJ
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- Codina EP
- Coelli S
- Cohen H
- Coimbra AEC
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- Collot J
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- Connell SH
- Connelly IA
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- Conventi F
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- Cooper-Sarkar AM
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- Cristoforetti M
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- Crosetti G
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- Cunningham WR
- Curcio F
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- Czurylo MM
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- D'Amico V
- D'Auria S
- D'Eramo L
- D'onofrio A
- D'Onofrio M
- D'uffizi M
- Da Costa AMMJ
- da Costa JBG
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dattagupta A
- David C
- Davidek T
- Davis DR
- Davis-Purcell B
- Dawson I
- de Andrade LM
- De Araujo MV
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- De Beurs M
- De Carvalho ALM
- De Castro S
- De Groot N
- de Jong P
- De K
- de la Hoz SG
- De la Torre H
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- De Maria A
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- de Renstrom PAB
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- De Salvo A
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- De Santis M
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- Degens J
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- Delitzsch CM
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- Della Pietra M
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- Delmastro M
- Delsart PA
- Demers S
- Demichev M
- Denisov SP
- Derendarz D
- Derue F
- Dervan P
- Desch K
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Quality of life correlates with muscle strength in patients with dermato- or polymyositis
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- A Bohan
- A Ponyi
- Christine Dalgård
- FH Souza
- FW Miller
- H Alexanderson
- Helene Alexanderson
- I Armadans-Tremolosa
- I Marie
- IM Bronner
- J Vlekkert van de
- JBD Bjørner
- JL Hundley
- Karina B. Poulsen
- LG Rider
- Louise P. Diederichsen
- Louise Weile
- LP Diederichsen
- LP Diederichsen
- M Regardt
- M Regardt
- R Goreshi
- R Goreshi
- SM Sultan
- Søren Jacobsen
- YL Chung
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Analysis of influencing factors on soil Zn content using generalized additive model
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- A Chandrasekaran
- A Guisan
- A Lehmann
- ACA Rudy
- C Li
- C Schulz-Zunkel
- C Tu
- CA Grant
- CJ Stone
- D Berg
- D Hou
- DD Brogniez
- E Masal
- ER Blankson
- F Edillo
- F Liu
- H Liu
- H Tang
- I Shtangeeva
- IK Kalavrouziotis
- J Elith
- JB Richardson
- JB Zhang
- JBD Souza
- K Glin´Skalewczuk
- K Ohki
- M Barberon
- MO Obiakor
- N Bouain
- Q Wenchuan
- R Amorós
- RA Koyak
- RE Mendoza
- RM Harrison
- S Ohshimo
- SN Wood
- SR Rathod
- TB Ouarda
- TFA Bishop
- TM Shatar
- TW Yee
- W Dong
- XL Wu
- Y Jia
- Z Nan
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for associated production of a Z boson with an invisibly decaying Higgs boson or dark matter candidates at s=13 TeV with the ATLAS detector
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- Yildiz HD
- Yin P
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- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner SV
- Zeitnitz C
- Zeng JC
- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
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- Zhang G
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhou H
- Zhou N
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- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zivkovic L
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2022
- Field of study
A search for invisible decays of the Higgs boson as well as searches for dark matter candidates, produced together with a leptonically decaying Z boson, are presented. The analysis is performed using proton−proton collisions at a centre-of-mass energy of 13 TeV, delivered by the LHC, corresponding to an integrated luminosity of 139 fb−1 and recorded by the ATLAS experiment. Assuming Standard Model cross-sections for ZH production, the observed (expected) upper limit on the branching ratio of the Higgs boson to invisible particles is found to be 19% (19%) at the 95% confidence level. Exclusion limits are also set for simplified dark matter models and two-Higgs-doublet models with an additional pseudoscalar mediator
Search for long-lived charginos based on a disappearing-track signature using 136 fb(-1) of pp collisions at root s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin JF
- Argyropoulos S
- Arling JH
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Backman F
- Badea A
- Bagnaia P
- Bahilo JJL
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
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- Balasubramanian R
- Baldin EM
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- Balunas WK
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- Bandyopadhyay A
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barends KN
- Barillari T
- Barisits MS
- Barkeloo J
- Barklow T
- Barnett BM
- Barnett RM
- Baroncelli A
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- Barr AJ
- Barron U
- Barrue RFC
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bashta I
- Bassalat A
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- Latour BMD
- Lau TS
- Laudrain A
- Laurier A
- Lavorgna M
- Lawlor SD
- Lazzaroni M
- Le B
- Leban B
- Lebedev A
- LeBlanc M
- LeCompte T
- Ledroit-Guillon F
- Lee ACA
- Lee CA
- Lee GR
- Lee L
- Lee S
- Lee SC
- Leeuw LL
- Lefebvre B
- Lefebvre HP
- Lefebvre M
- Leggett C
- Lehmann K
- Lehmann N
- Leight WA
- Leisos A
- Leite MAL
- Leitgeb CE
- Leitner R
- Leney KJC
- Lenz T
- Leone S
- Leonidopoulos C
- Leopold A
- Leroy C
- Les R
- Lester CG
- Levchenko M
- Leveque J
- Levin D
- Levinson LJ
- Lewis DJ
- Li B
- Li B
- Li C
- Li CQ
- Li H
- Li H
- Li J
- Li K
- Li L
- Li M
- Li QY
- Li S
- Li X
- Li Y
- Li Z
- Li Z
- Li Z
- Li Z
- Liang Z
- Liberatore M
- Liberti B
- Lie K
- Lin K
- Linck RA
- Lindley RE
- Lindon JH
- Linss A
- Lionti AL
- Lipeles E
- Lipniacka A
- Liss TM
- Lister A
- Little JD
- Liu B
- Liu BX
- Liu JB
- Liu JKK
- Liu K
- Liu M
- Liu MY
- Liu P
- Liu X
- Liu Y
- Liu Y
- Liu YL
- Liu YW
- Livan M
- Llacer MM
- Lleres A
- Lloyd SL
- Lobodzinska EM
- Loch P
- Loffredo S
- Lohse T
- Lohwasser K
- Lokajicek M
- Long JD
- Long RE
- Longarini I
- Longo L
- Longo R
- Lopez MM
- Lopez RG
- Lopez SC
- Lorenz J
- Lory AM
- Losle A
- Lou X
- Lou X
- Lounis A
- Love J
- Love PA
- Lu G
- Lu M
- Lu S
- Lu YJ
- Lubatti HJ
- Luci C
- Lucotte A
- Luehring F
- Luise I
- Luminari L
- Lund-Jensen B
- Luongo NA
- Lutz MS
- Lynn D
- Lyons H
- Lysak R
- Lytken E
- Lyu F
- Lyubushkin V
- Lyubushkina T
- Ma H
- Ma LL
- Ma Y
- Mac Donell DM
- Maccarrone G
- Macdonald CM
- MacDonald JC
- Madar R
- Madden WDB
- Mader WF
- Madriz RGO
- Madysa N
- Maeda J
- Maeno T
- Maerker M
- Magerl V
- Magro J
- Mahon DJ
- Maidantchik C
- Maio A
- Maira NV
- Maj K
- Majersky O
- Majewski S
- Makovec N
- Malaescu B
- Malecki P
- Maleev VP
- Malito D
- Mallik U
- Malone C
- Maltezos S
- Malyukov S
- Mamuzic J
- Mancini G
- Mandalia JP
- Manghi FL
- Manh TN
- Maniatis IM
- Manisha M
- Mankinen KH
- Mann A
- Manousos A
- Mansoulie B
- Manthos I
- Manzano MR
- Manzoni S
- Marantis A
- Marchese L
- Marchiori G
- Marcisovsky M
- Marcoccia L
- Marcon C
- Marjanovic M
- Marshall Z
- Marti-Garcia S
- Martin MAP
- Martin TA
- Martin VJ
- Martin-Haugh S
- Martinelli L
- Martinez CM
- Martinez JLM
- Martinez M
- Martinez NL
- Martoiu VS
- Martyniuk AC
- Marzin A
- Maschek SR
- Masetti L
- Mashimo T
- Masik J
- Maslennikov AL
- Massa L
- Massarotti P
- Mastrandrea P
- Mastroberardino A
- Masubuchi T
- Matakias D
- Mathisen T
- Matic A
- Matsuzawa N
- Maurer J
- Maximov DA
- Mazini R
- Maznas I
- Mazza SM
- McCarthy TG
- McCormack WP
- McDonald EF
- McDougall AE
- Mcfayden JA
- McGinn C
- McGowan JP
- Mchedlidze G
- McKay MA
- McKee SP
- McLean KD
- McMahon SJ
- McNamara PC
- McPherson RA
- Mdhluli JE
- Meadows ZA
- Meehan S
- Megy T
- Mehlhase S
- Mehta A
- Meirose B
- Melini D
- Meloni F
- Melzer A
- Meng HY
- Meng L
- Menke S
- Mentink M
- Meoni E
- Merino JL
- Merkt SAM
- Merlassino C
- Mermod P
- Merola L
- Meroni C
- Merz G
- Meshkov O
- Meshreki JKR
- Metcalfe J
- Mete AS
- Meyer C
- Meyer JP
- Michetti M
- Middleton RP
- Mikenberg G
- Mikestikova M
- Mikuz M
- Mildner H
- Milic A
- Milke CD
- Miller DW
- Miller LS
- Milosavljevic MV
- Milov A
- Milstead DA
- Minaenko AA
- Minashvili IA
- Mince L
- Mincer AI
- Mindur B
- Mineev M
- Minegishi Y
- Mino Y
- Miotto GL
- Mir LM
- Mironova M
- Mitani T
- Mitsou VA
- Mittal M
- Miu O
- Miyagawa PS
- Miyazaki Y
- Mizukami A
- Mjornmark JU
- Mkrtchyan T
- Mlynarikova M
- Moa T
- Mobius S
- Mochizuki K
- Moder P
- Mogg P
- Mohamed ATA
- Mohammed AF
- Mohapatra S
- Mokgatitswane G
- Mondal B
- Mondal S
- Monig K
- Monnier E
- Montalbano A
- Montella M
- Monticelli F
- Morange N
- Morettini P
- Morgenstern M
- Morgenstern S
- Mori D
- Morii M
- Morinaga M
- Morisbak V
- Morley AK
- Morris AP
- Morvaj L
- Moschovakos P
- Moser B
- Mosidze M
- Moskalets T
- Moskvitina P
- Moss J
- Moyse EJW
- Muanza S
- Mueller J
- Muenstermann D
- Muino PC
- Mullier GA
- Mullin JJ
- Mungo DP
- Munoz DC
- Murin M
- Murin P
- Murray WJ
- Murrone A
- Muse JM
- Muskinja M
- Mwewa C
- Myagkov AG
- Myers AA
- Myers G
- Myska M
- Nachman BP
- Nackenhorst O
- Nagai K
- Nagano K
- Nagle JL
- NagNag A
- Nagy E
- Nairz AM
- Nakahama Y
- Nakamura K
- Nanjo H
- Napolitano F
- Narayan R
- Naryshkin I
- Naseri M
- Nass C
- Naumann T
- Navarro G
- Navarro JEG
- Navarro LB
- Navarro-Gonzalez J
- Nechaeva PY
- Nechansky F
- Neep TJ
- Negri A
- Negrini M
- Nellist C
- Nelson C
- Nelson K
- Nelson ME
- Nemecek S
- Nessi M
- Neubauer MS
- Neuhaus F
- Neundorf J
- Newhouse R
- Newman PR
- Ng CW
- Ng YS
- Ng YWY
- Ngair B
- Nguyen HDN
- Nickerson RB
- Nicolaidou R
- Nielsen DS
- Nielsen J
- Niemeyer M
- Nikiforou N
- Nikolaenko V
- Nikolic-Audit I
- Nikolopoulos K
- Nilsson P
- Nindhito HR
- Nisati A
- Nishu N
- Nisius R
- Nitta T
- Nobe T
- Noel DL
- Noguchi Y
- Nomidis I
- Nomura MA
- Norfolk MB
- Norisam RRB
- Novak J
- Novak T
- Novgorodova O
- Novotny L
- Novotny R
- Nozka L
- Ntekas K
- Nurse E
- O'Connor K
- O'Keefe MW
- O'Neil DC
- O'neill AP
- O'Shea V
- Oakham FG
- Ocariz J
- Ochi A
- Ochoa I
- Ochoa-Ricoux JP
- Oda S
- Odaka S
- Oerdek S
- Ogrodnik A
- Oh A
- Ohm CC
- Oide H
- Oishi R
- Ojeda ML
- Okazaki Y
- Okumura Y
- Olariu A
- Oliveira MVS
- Oliver JL
- Olsson MJR
- Olszewski A
- Olszowska J
- Onofre A
- Onyisi PUE
- OOncel O
- Oppen H
- Oreglia MJ
- Orellana GE
- Orestano D
- Orlando N
- Orr RS
- Ospanov R
- Otono H
- Ott PS
- Ottino GJ
- Ouchrif M
- Ouellette J
- Ould-Saada F
- Ouraou A
- Outschoorn VIM
- Ouyang Q
- Owen M
- Owen RE
- Ozcan VE
- Ozturk N
- Ozturk S
- Pacalt J
- Pacey HA
- Pachal K
- Pages AP
- Palacino G
- Palazzo S
- Palestini S
- Palka M
- Panchal DK
- Pandini CE
- Pani P
- Panizzo G
- Paolozzi L
- Papadatos C
- Parajuli S
- Paramonov A
- Paraskevopoulos C
- Pardos CD
- Parida B
- Park TH
- Parker AJ
- Parker MA
- Parodi F
- Parrish EW
- Parsons JA
- Parzefall U
- Pascual JAG
- Pascuzzi VR
- Pasquali F
- Pasqualucci E
- Passaggio S
- Pastor ET
- Pastor OE
- Pastore F
- Pasuwan P
- Pater JR
- Pathak A
- Patton J
- Pauly T
- Paz IL
- Pearkes J
- Pedersen M
- Pedro R
- Peiffer T
- Peixoto APP
- Peleganchuk SV
- Pena JJ
- Penc O
- Peng C
- Peng H
- Penzin M
- Peralva BS
- Perego MM
- Perepelitsa DV
- Perez MV
- Perganti M
- Perini L
- Pernegger H
- Perrella S
- Perrevoort A
- Peters K
- Peters RFY
- Petersen BA
- Petersen TC
- Petit E
- Petousis V
- Petridou C
- Petroff P
- Petrucci F
- Pettee M
- Pettersson NE
- Petukhova K
- Peyaud A
- Pezoa R
- Pezzotti L
- Pezzullo G
- Pham T
- Phillips PW
- Phipps MW
- Piacquadio G
- Pianori E
- Piazza F
- Picazio A
- Piegaia R
- Pietreanu D
- Pilcher JE
- Pilkington AD
- Pinamonti M
- Pineda AS
- Pinfold JL
- Pino SAO
- Pinto JVD
- Pizzi DA
- Pizzimento L
- Pizzini A
- Pleier MA
- Plesanovs V
- Pleskot V
- Plotnikova E
- Podberezko P
- Poettgen R
- Poggi R
- Poggioli L
- Pogrebnyak I
- Pohl D
- Pokharel I
- Polesello G
- Poley A
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Pollock ZB
- Polychronakos V
- Ponce JMI
- Ponomarenko D
- Pontecorvo L
- Popa S
- Popeneciu GA
- Portales L
- Pospisil S
- Postolache P
- Potamianos K
- Potrap IN
- Potter CJ
- Potti H
- Poulsen T
- Poveda J
- Powell TD
- Pownall G
- Pozo JAA
- Pralavorio P
- Prapa MM
- Prell S
- Price D
- Primavera M
- Proffitt ML
- Proklova N
- Prokofiev K
- Prokoshin F
- Protopopescu S
- Proudfoot J
- Przybycien M
- Pudzha D
- Puzo P
- Pyatiizbyantseva D
- Qian J
- Qin Y
- Quadt A
- Queitsch-Maitland M
- Quintero DMP
- Ragusa F
- Rahal G
- Raine JA
- Rajagopalan S
- Ramos JM
- Ran K
- Rassloff DF
- Rauch DM
- Rave S
- Ravina B
- Ravinovich I
- Raymond M
- Read AL
- Readioff NP
- Rebuzzi DM
- Redlinger G
- Reeves K
- Reikher D
- Reiss A
- Rej A
- Rembser C
- Renardi A
- Renda M
- Rendel MB
- Rennie AG
- Renous DS
- Renteria CG
- Resconi S
- Resseguie ED
- Rettie S
- Reynolds B
- Reynolds E
- Rezanova OL
- Reznicek P
- Ricci E
- Richter R
- Richter S
- Richter-Was E
- Ridel M
- Rieck P
- Riedler P
- Rifki O
- Rijssenbeek M
- Rimoldi A
- Rimoldi M
- Rinaldi L
- Rinn TT
- Rinnagel MP
- Ripellino G
- Riu I
- Rivadeneira P
- Rizatdinova F
- Rizvi E
- Rizzi C
- Roberts BA
- Robertson SH
- Robin M
- Robinson D
- Robson A
- Rocchi A
- Roda C
- Rodriguez AR
- Rodriguez GRG
- Roe S
- Roggel J
- Rohne O
- Rojas JGRG
- Rojas RA
- Roland B
- Roland CPA
- Roloff J
- Romaniouk A
- Romano M
- Rompotis N
- Ronzani M
- Roos L
- Rosati S
- Rosin G
- Rosser BJ
- Rossi E
- Rossi E
- Rossi E
- Rossi LP
- Rossini L
- Rosten R
- Rotaru M
- Rottler B
- Rousseau D
- Rousso D
- Rovelli G
- Roy A
- Rozanov A
- Rozas AJ
- Rozen Y
- Ruan X
- Ruby AJ
- Ruggeri TA
- Ruhr F
- Ruiz-Martinez A
- Rummler A
- Rurikova Z
- Rusakovich NA
- Russell HL
- Rustige L
- Rutherfoord JP
- Ruttinger EM
- Rybar M
- Rye EB
- Ryzhov A
- Sabatini P
- Sabetta L
- Sadrozinski HFW
- Sadykov R
- Saenz SRP
- Safdari M
- Saha P
- Saha S
- Sahinsoy M
- Sahu A
- Saimpert M
- Saito M
- Saito T
- Salamani D
- Salamanna G
- Salas AS
- Salnikov A
- Salt J
- Salvatore D
- Salvatore F
- Salzburger A
- Samani BS
- Sammel D
- Sampsonidis D
- Sampsonidou D
- Sanchez CAS
- Sanchez FJM
- Sanchez J
- Sanchez LP
- Sandaker H
- Sander CO
- Sanderswood IG
- Sandesara JA
- Sandhoff M
- Sandoval C
- Sankey DPC
- Sannino M
- Sano Y
- Sansoni A
- Santoni C
- Santos H
- Santpur SN
- Santra A
- Santurio EV
- Saoucha KA
- Sapronov A
- Saraiva JG
- Sardain J
- Sasaki O
- Sato K
- Sauer C
- Sauerburger F
- Sauvan E
- Savard P
- Sawada R
- Sawyer C
- Sawyer L
- Sbarra C
- Sbrizzi A
- Scanlon T
- Schaarschmidt J
- Schacht P
- Schaefer D
- Schaefer L
- Schafer U
- Schaffer AC
- Schaile D
- Schamberger RD
- Schanet E
- Scharf C
- Scharmberg N
- Schegelsky VA
- Scheirich D
- Schenck F
- Schernau M
- Schiavi C
- Schildgen LK
- Schillaci ZM
- Schioppa EJ
- Schioppa M
- Schlag B
- Schleicher KE
- Schlenker S
- Schmieden K
- Schmitt C
- Schmitt S
- Schoeffel L
- Schoening A
- Scholer PG
- Schopf E
- Schott M
- Schovancova J
- Schramm S
- Schroeder F
- Schroeder TV
- Schultz-Coulon HC
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schwemling P
- Schwienhorst R
- Sciandra A
- Sciolla G
- Scuri F
- Scutti F
- Seabra LFO
- Sebastian VS
- Sebastiani CD
- Sedlaczek K
- Seema P
- Seidel SC
- Seiden A
- Seidlitz BD
- Seiss T
- Seitz C
- Seixas JM
- Sekhniaidze G
- Sekula SJ
- Selem L
- Semprini-Cesari N
- Sen S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Severini H
- Sevova S
- Sforza F
- Sfyrla A
- Shabalina E
- Shaheen R
- Shahinian JD
- Shaikh NW
- Shan LY
- Shapiro M
- Sharma A
- Sharma AS
- Sharma S
- Shatalov PB
- Shaw K
- Shaw SM
- Sherwood P
- Shi L
- Shimmin CO
- Shimogama Y
- Shinner JD
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shochet MJ
- Shojaii J
- Shope DR
- Shrestha S
- Shrif EM
- Shroff MJ
- Shulga E
- Sicho P
- Sickles AM
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva CBDE
- Silverstein SB
- Simion S
- Simoniello R
- Simsek S
- Sinervo P
- Sinetckii V
- Singh S
- Sinha S
- Sinha S
- Sioli M
- Siral I
- Sivoklokov SY
- Sjolin J
- Skaf A
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith EA
- Smith HA
- Smith JL
- Smizanska M
- Smolek K
- Smykiewicz A
- Snesarev AA
- Snoek HL
- Snyder S
- Sobie R
- Soffer A
- Sohns F
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Solomon S
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Sonay A
- Song WY
- Sopczak A
- Sopio AL
- Sopkova F
- Sottocornola S
- Soualah R
- Soukharev AM
- Soumaimi Z
- South D
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spieker TM
- Spigo G
- Spina M
- Spiteri DP
- Spousta M
- Stabile A
- Stamen R
- Stamenkovic M
- Stampekis A
- Standke M
- Stanecka E
- Stanislaus B
- Stanitzki MM
- Stankaityte M
- Stapf B
- Starchenko EA
- Stark GH
- Stark J
- Starko DM
- Staroba P
- Starovoitov P
- Starz S
- Staszewski R
- Stavropoulos G
- Steinberg P
- Steinhebel AL
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stevenson TJ
- Stewart GA
- Stockton MC
- Stoicea G
- Stolarski M
- Stonjek S
- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strebler T
- Strizenec P
- Strohmer R
- Strom DM
- Strom LR
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Su D
- Su S
- Su X
- Suarez NB
- Suarez RG
- Sugizaki K
- Sulin VV
- Sullivan MJ
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun S
- Sun X
- Suster CJE
- Sutton MR
- Svatos M
- Swiatlowski M
- Swirski T
- Sykora I
- Sykora M
- Sykora T
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Tagiev E
- Taibah RHM
- Takashima R
- Takeda K
- Takeshita T
- Takeva EP
- Takubo Y
- Talby M
- Talyshev AA
- Tam KC
- Tame ZPA
- Tamir NM
- Tanaka A
- Tanaka J
- Tanaka R
- Tao Z
- Tapprogge S
- Tarem S
- Tariq K
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tassi E
- Tateno G
- Tayalati Y
- Taylor GN
- Taylor W
- Teagle H
- Tee AS
- Tehrani FS
- Teixeira-Dias P
- TenKate H
- Teoh JJ
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Themistokleous N
- Theveneaux-Pelzer T
- Thielmann O
- Thomas DW
- Thomas JP
- Thompson EA
- Thompson PD
- Thomson E
- Thorpe EJ
- Tian Y
- Tikhomirov V
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
- Tlou SH
- Tnourji A
- Todome K
- Todorova-Nova S
- Todt S
- Togawa M
- Tojo J
- Tokar S
- Tokushuku K
- Tolley E
- Tombs R
- Tomoto M
- Tompkins L
- Tornambe P
- Toro RC
- Torregrosa EF
- Torrence E
- Torres H
- Toscani M
- Tosciri C
- Toth J
- Tovey DR
- Traeet A
- Treado CJ
- Trefzger T
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Trischuk DA
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trovato F
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tsiamis A
- Tsiareshka PV
- Tsirigotis A
- Tsiskaridze V
- Tskhadadze EG
- Tsopoulou M
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsur O
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tuna AN
- Turchikhin S
- Turgeman D
- Turner RJ
- Turra R
- Tuts PM
- Tzamarias S
- Tzanis P
- Tzovara E
- Uchida K
- Ukegawa F
- Unal G
- Unal M
- Undrus A
- Unel G
- Ungaro FC
- Uno K
- Urban J
- Urban SC
- Urquijo P
- Usai G
- Ushioda R
- Usman M
- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
- Vafeiadis T
- Valderanis C
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- VallsFerrer JA
- Van Daalen TR
- Van Gemmeren P
- Van Stroud S
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vannicola D
- Vannoli L
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasile ME
- Vaslin L
- Vasquez GA
- Vazeille F
- Vazquez CJB
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veliscek I
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Vera AMR
- Verbytskyi A
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vernieri C
- Verschuuren PJ
- Verzini MJA
- Vesterbacka ML
- Vetterli MC
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Villhauer EM
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
A search for long-lived charginos produced either directly or in the cascade decay of heavy prompt gluino states is presented. The search is based on proton- proton collision data collected at a centre-of-mass energy of root s = 13 TeV between 2015 and 2018 with the ATLAS detector at the LHC, corresponding to an integrated luminosity of 136 fb(-1). Long-lived charginos are characterised by a distinct signature of a short and then disappearing track, and are reconstructed using at least four measurements in the ATLAS pixel detector, with no subsequent measurements in the silicon-microstrip tracking volume nor any associated energy deposits in the calorimeter. The final state is complemented by a large missing transverse-momentum requirement for triggering purposes and at least one high-transversemomentum jet. No excess above the expected backgrounds is observed. Exclusion limits are set at 95% confidence level on the masses of the chargino and gluino for different chargino lifetimes. Chargino masses up to 660 (210) GeV are excluded in scenarios where the chargino is a pure wino (higgsino). For charginos produced during the cascade decay of a heavy gluino, gluinos with masses below 2.1 TeV are excluded for a chargino mass of 300 GeV and a lifetime of 0.2 ns
Search for resonant pair production of Higgs bosons in the b(b)over-barb(b)over-bar final state using pp collisions at root s=13 TeV with the ATLAS detector
- Author
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- Abbott B
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
A search for resonant Higgs boson pair production in the b (b) over barb (b) over bar final state is presented. The analysis uses 126 fb(-1)- 139 fb(-1) of pp collision data at root s = 13 TeV collected with the ATLAS detector at the Large Hadron Collider. The analysis is divided into two channels, targeting Higgs boson decays which are reconstructed as pairs of small-radius jets or as individual large-radius jets. Spin-0 and spin2 benchmark signal models are considered, both of which correspond to resonant HH production via gluon-gluon fusion. The data are consistent with Standard Model predictions. Upper limits are set on the production cross section times branching ratio to Higgs boson pairs of a new resonance in the mass range from 251 GeV to 5 TeV
Measurement of the nuclear modification factor for muons from charm and bottom hadrons in Pb+Pb collisions at 5.02 TeV with the ATLAS detector
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- Abhayasinghe DK
- Abidi SH
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- Yexley MR
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
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- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zenz S
- Zerradi S
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
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- Zhang R
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- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhou H
- Zhou N
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- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
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- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Ziolkowski M
- Zivkovic L
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2022
- Field of study
Heavy-flavour hadron production provides information about the transport properties and microscopic structure of the quark–gluon plasma created in ultra-relativistic heavy-ion collisions. A measurement of the muons from semileptonic decays of charm and bottom hadrons produced in Pb+Pb and pp collisions at a nucleon–nucleon centre-of-mass energy of 5.02 TeV with the ATLAS detector at the Large Hadron Collider is presented. The Pb+Pb data were collected in 2015 and 2018 with sampled integrated luminosities of 208μb−1 and 38μb−1, respectively, and pp data with a sampled integrated luminosity of 1.17pb−1 were collected in 2017. Muons from heavy-flavour semileptonic decays are separated from the light-flavour hadronic background using the momentum imbalance between the inner detector and muon spectrometer measurements, and muons originating from charm and bottom decays are further separated via the muon track's transverse impact parameter. Differential yields in Pb+Pb collisions and differential cross sections in pp collisions for such muons are measured as a function of muon transverse momentum from 4 GeV to 30 GeV in the absolute pseudorapidity interval |η|<2. Nuclear modification factors for charm and bottom muons are presented as a function of muon transverse momentum in intervals of Pb+Pb collision centrality. The bottom muon results are the most precise measurement of b quark nuclear modification at low transverse momentum where reconstruction of B hadrons is challenging. The measured nuclear modification factors quantify a significant suppression of the yields of muons from decays of charm and bottom hadrons, with stronger effects for muons from charm hadron decays
Determination of the parton distribution functions of the proton using diverse ATLAS data from pp collisions at root s=7, 8 and 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
This paper presents an analysis at next-to-next-to-leading order in the theory of quantum chromodynamics for the determination of a new set of proton parton distribution functions using diverse measurements in pp collisions at root s = 7, 8 and 13 TeV, performed by the ATLAS experiment at the Large Hadron Collider, together with deep inelastic scattering data from ep collisions at the HERA collider. The ATLAS data sets considered are differential cross-section measurements of inclusive W-+/- and Z/gamma* boson production, W-+/- and Z boson production in association with jets, t (t) over bar production, inclusive jet production and direct photon production. In the analysis, particular attention is paid to the correlation of systematic uncertainties within and between the various ATLAS data sets and to the impact of model, theoretical and parameterisation uncertainties. The resulting set of parton distribution functions is called ATLASpdf21