115 research outputs found
Volatile and precious metal geochemistry of the Mount Isa ores and their host rocks
- Author
- Publication venue
- Publication date
- 01/01/1986
- Field of study
Geochemical and petrographic investigations of Pb-Zn-Ag
mineralization ( 12 orebody) and Cu-Co mineralization (1100 orebody)
from Mount Isa were undertaken. Over one hundred and twenty
carefully selected samples were analyzed for major and minor
elements and for some or all of the following volatile metals: Au,
Ag, Cd, As, Sb, Se, Bi, Co and Tl.
A strong Tl enrichment is observed in (pyritic) unmineralized
lateral equivalents of 12 orebody for several kilometers to the
north of the mine sequence. The Se and As contents, S/Se ratios and
S isotope relationships in the Pb-Zn ores and their host pyritic
shales preclude a magmatic or deep-seated hydrothermal S source.
The data suggest that sulfide S in the Urquhart Shales was derived
from reduction of a ''seawater"/evaporitic/pore water sulfate source.
Lateral variations in the thickness of mineralized intervals, the
nature of the sulfide-gangue textures in the ores, the pervasive K
and Tl enrichment in the host rocks and other chemical features of
the Pb-Zn ores indicate that much of the Mount Isa mineralization
formed epigenetically within the unconsolidated Urquhart Shales.
The Pb-Zn-Ag ores contain very little Au and it is argued that this
feature is best explained by the hydrothermal solutions that formed
the Pb-Zn ores being cool (<<200°C) and moderately oxidized.
The "silica dolomite" (the host to all the Mount Isa Cu
mineralization) formed from "normal" Urquhart Shale as a result of
intense fault-related hydrothermal activity (Perkins, 1984). The
alteration has silicified the shales adjacent to the fault, and
dolomite, phyllosilicates and "immobile" elements liberated during
the silicification have been re-deposited at higher levels up-dip in
the silica dolomite bodies. For the most part primary sulfide
textures have not been preserved.
It is argued that the distribution of several elements (notably Co,
Bi, As, Fe and S) in 1100 orebody and its location down-dip from a
strongly pyritic section of Urquhart Shale are good evidence that
stratiform Co (and Cu) mineralization was present in pyritic
Urquhart Shales prior to formation of the silica dolomite. Chemical
and {sotopic evidence suggests that the Cu mineralization had a similar s-~ource and formed from similar solutions to the Pb-Zn-Ag
ores.
A new co-genetic model for the Mount Isa Cu and Pb-Zn-Ag deposits in
which the mineralization formed from cool oxidized solutions in the
upper few meters of the unconsolidated Urquhart Shales is presented.
The metal-bearing solutions were expelled from their source rocks
(oxidized clastic sediments lower in the Mount Isa Group) during the
course of normal basin compaction and dewatering. Base metal
sulfides were fixed by sulfate reduction processes occuring in the
diagenetic environment of the Urquhart Shales. Weathered mafic
volcanic detritus may have been an important component of the source
Selection and Prioritization of Candidate Drug Targets for Amyotrophic Lateral Sclerosis Through a Meta-Analysis Approach
- Author
- A Gorio
- A Matilla
- A Neymotin
- Antonio Gianmaria Spampinato
- B Liu
- B Schutz
- C Carlesi
- C Casas
- C Janssen
- C Raoul
- C Sunyach
- CF Chan
- CG Saris
- CS Nicolas
- CW Lederer
- D Maglott
- D Offen
- D Singh
- DJ Graber
- DL Wheeler
- DR Marsh
- E Aronica
- E Nagata
- EW Stommel
- F Achilli
- F Albo
- FF Cox
- FL Conforti
- Francesca Luisa Conforti
- G Morello
- G Morello
- G Yu
- Giovanna Morello
- GP Oliveira de
- H Jarvelainen
- H Takuma
- HJ Habisch
- I Niebroj-Dobosz
- J Aebischer
- J Crespo-Barreto
- J Xin
- JD Mitchell
- JH Ward
- JK Ryu
- JM Scorisa
- JR Maximino
- K Tanaka
- K Xu
- L Ferraiuolo
- L Ferraiuolo
- LA Lampson
- LC Kudo
- LJ Martin
- M Brkic
- M De Paola
- M Kiaei
- M Mizuno
- M Paizs
- M Tateno
- M Tortarolo
- MC Dal Canto
- ME Woodbury
- MR Turner
- MR Vargas
- O Goureau
- OA Shemesh
- P Cassina
- P Heneberg
- P McGoldrick
- P Pasinelli
- P Van Damme
- PA McCombe
- PH Gordon
- PJ Shaw
- PL Vieira
- R Arnon
- R Costa
- RM Pascuzzi
- RS Ignarro
- S Cavallaro
- S Cavallaro
- S Cavallaro
- S Cavallaro
- S Kwak
- S Li
- S Millecamps
- S Paratore
- S Perrin
- S Petri
- S Petri
- Sebastiano Cavallaro
- SM Hearst
- T Bordet
- T Kabuta
- T Lenglet
- T Okuda
- Velia D’Agata
- VN Trieu
- VN Trieu
- W Boston-Howes
- W Dong
- W Huang
- Y Kajiwara
- Y Nikolsky
- Y Ohta
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb−1 of s√ = 13 TeV pp collision data with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aperio Bella L
- Arabidze G
- Aranda CP
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
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- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
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- Azuelos G
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- Baca MJ
- Bachacou H
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- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Baines JT
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- Bakker PJ
- Baldin EM
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- Bednyakov VA
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- Belotskiy K
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Benekos N
- Benhammou Y
- Benhar Noccioli E
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Bergsten LJ
- Beringer J
- Berlendis S
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- Bernard NR
- Bernardi G
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- Bernlochner FU
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- Bessidskaia Bylund O
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- Billoud TRV
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- Bjergaard DM
- Black JE
- Black KM
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blunier D
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
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- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
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- Boldyrev AS
- Bolz AE
- Bomben M
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- Bonilla JS
- Boonekamp M
- Borisov A
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- Bortfeldt J
- Bortoletto D
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- Boscherini D
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- Bossio Sola JD
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- Bouhova-Thacker EV
- Boumediene D
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- Boutle SK
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- Bullock D
- Burch TJ
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- Burgard CD
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- Burmeister I
- Burr JTP
- Buschmann E
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- Butterworth JM
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- Buttinger W
- Buzatu A
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- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
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- Calvente Lopez S
- Calvet D
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- Cameron D
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- Campana S
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- Canale V
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- Cao T
- Cao Y
- Capeans Garrido MDM
- Caprini I
- Caprini M
- Capua M
- Carbone RM
- Cardarelli R
- Cardillo FC
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casha AF
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
- Castillo IS
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan WS
- Chan YL
- Chapman JD
- Chargeishvili B
- Charlton DG
- Chau CC
- Che S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
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- Christodoulou V
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- Coimbra AEC
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- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar AM
- Corga KDV
- Cormier F
- Cormier KJR
- Corpe LD
- Corradi M
- Corrigan EE
- Corriveau F
- Cortes-Gonzalez A
- Costa MJ
- Costanzo D
- Cottin G
- Coutinho YA
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- Cox BE
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- Cranmer K
- Crawley SJ
- Creager RA
- Cree G
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- Crescioli F
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cukierman AR
- Cuth J
- Czekierda S
- Czodrowski P
- D'amen G
- D'Auria S
- D'Eramo L
- D'onofrio A
- D'Onofrio M
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
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- Dann ND
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- Dao V
- Darbo G
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- Daubney T
- Davey W
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- Davidek T
- Davis DR
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- Dawson I
- De Asmundis R
- De Benedetti A
- De Beurs M
- De Bruin PHS
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- de Lima DEF
- De Lorenzi F
- De Maria A
- De Pedis D
- De Regie JBDV
- De Salvo A
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- Debenedetti C
- Dedovich DV
- Dehghanian N
- Del Peso J
- Delgado AT
- Delgove D
- Deliot F
- Delitzsch CM
- Dell'Acqua A
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- Della Volpe D
- Delmastro M
- Delporte C
- Delsart PA
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- Demers S
- Demichev M
- Denisov SP
- Denysiuk D
- Derendarz D
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- Dette K
- Devesa MR
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Bello FA
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- Di Clemente WK
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- Dubinin F
- Dubovsky M
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- Ducourthial A
- Ducu OA
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- Zemaityte G
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- Zhemchugov A
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- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
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- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 17/02/2021
- Field of study
A search for the supersymmetric partners of quarks and gluons (squarks and gluinos) in final states containing jets and missing transverse momentum, but no electrons or muons, is presented. The data used in this search were recorded by the ATLAS experiment in proton-proton collisions at a centre-of-mass energy of s√ = 13 TeV during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. The results are interpreted in the context of various R-parity-conserving models where squarks and gluinos are produced in pairs or in association and a neutralino is the lightest supersymmetric particle. An exclusion limit at the 95% confidence level on the mass of the gluino is set at 2.30 TeV for a simplified model containing only a gluino and the lightest neutralino, assuming the latter is massless. For a simplified model involving the strong production of mass-degenerate first- and second-generation squarks, squark masses below 1.85 TeV are excluded if the lightest neutralino is massless. These limits extend substantially beyond the region of supersymmetric parameter space excluded previously by similar searches with the ATLAS detector
Measurement of Azimuthal Anisotropy of Muons from Charm and Bottom Hadrons in pp Collisions at √s = 13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
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- Cardillo FC
- Carli I
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- Carminati L
- Carney RMD
- Caron S
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- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 28/02/2020
- Field of study
The elliptic flow of muons from the decay of charm and bottom hadrons is measured in
p
p
collisions at
√
s
=
13
 
 
TeV
using a data sample with an integrated luminosity of
150
 
 
pb
−
1
recorded by the ATLAS detector at the LHC. The muons from heavy-flavor decay are separated from light-hadron decay muons using momentum imbalance between the tracking and muon spectrometers. The heavy-flavor decay muons are further separated into those from charm decay and those from bottom decay using the distance-of-closest-approach to the collision vertex. The measurement is performed for muons in the transverse momentum range 4–7 GeV and pseudorapidity range
|
η
|
<
2.4
. A significant nonzero elliptic anisotropy coefficient
v
2
is observed for muons from charm decays, while the
v
2
value for muons from bottom decays is consistent with zero within uncertainties
Properties of jet fragmentation using charged particles measured with the ATLAS detector in pp collisions at root s=13 TeV
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
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- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/09/2019
- Field of study
This paper presents a measurement of quantities related to the formation of jets from high-energy quarks and gluons (fragmentation). Jets with transverse momentum 100 GeV 500 MeV and |η| < 2.5 are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the two leading jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons with parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark and gluon extractions using input from simulation. The simulations provide a reasonable description of the quark-like data across the jet
Pt range presented in -this measurement, but the gluon-like data have systematically fewer charged particles than the simulation
Reconstruction and identification of boosted di-Ï„ systems in a search for Higgs boson pairs using 13 TeV proton-proton collision data in ATLAS
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
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- Adiguzel A
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- Aguilar-Saavedra JA
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- Akatsuka S
- Akesson TPA
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- Akimov AV
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- Aleksandrov IN
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- Zhao Z
- Zhemchugov A
- Zhou B
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- Zhou L
- Zhou M
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- Zhu CG
- Zhu H
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- Zhu J
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- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
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- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 30/11/2020
- Field of study
In this paper, a new technique for reconstructing and identifying hadronically decaying τ+τ− pairs with a large Lorentz boost, referred to as the di-τ tagger, is developed and used for the first time in the ATLAS experiment at the Large Hadron Collider. A benchmark di-τ tagging selection is employed in the search for resonant Higgs boson pair production, where one Higgs boson decays into a boosted bb¯¯ pair and the other into a boosted τ+τ− pair, with two hadronically decaying τ-leptons in the final state. Using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of 13 TeV, the efficiency of the di-τ tagger is determined and the background with quark- or gluon-initiated jets misidentified as di-τ objects is estimated. The search for a heavy, narrow, scalar resonance produced via gluon-gluon fusion and decaying into two Higgs bosons is carried out in the mass range 1–3 TeV using the same dataset. No deviations from the Standard Model predictions are observed, and 95% confidence-level exclusion limits are set on this model
A search for the dimuon decay of the Standard Model Higgs boson with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aperio Bella L
- Arabidze G
- Aranda CP
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Armstrong A
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- Publication venue
- 'Elsevier BV'
- Publication date
- 10/01/2021
- Field of study
A search for the dimuon decay of the Standard Model (SM) Higgs boson is performed using data corresponding to an integrated luminosity of collected with the ATLAS detector in Run 2 pp collisions at TeV at the Large Hadron Collider. The observed (expected) significance over the background-only hypothesis for a Higgs boson with a mass of 125.09 GeV is 2.0σ (1.7σ). The observed upper limit on the cross section times branching ratio for is 2.2 times the SM prediction at 95% confidence level, while the expected limit on a signal assuming the absence (presence) of a SM signal is 1.1 (2.0). The best-fit value of the signal strength parameter, defined as the ratio of the observed signal yield to the one expected in the SM, is
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