38 research outputs found
Expansão geográfica da leishmaniose visceral no Estado de Pernambuco
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Foco emergente de leishmaniose visceral em Mato Grosso do Sul
- Author
- Alencar JE
- Ana Lúcia Lyrio de Oliveira
- Anamaria Mello Miranda Paniago
- Araújo Sobrinho JR
- Arias JR
- Arruda W
- Bevilacqua PD
- Cascio A
- Cerbino Neto J
- Chagas E
- Costa CHN
- Croft SL
- Cupolilo E
- Cássia Rejane Leal
- Desjeux P
- Elisa Teruya Oshiro
- Galati EAB
- Grech V
- Guerin PJ
- Guerin PJ
- Guerra JAO
- Herwaldt B
- Magalhães PA
- Marcos Sanches
- Maria Elizabeth Cavalheiros Dorval
- Marzochi MCA
- Marzochi MCA
- Marzochi MCA
- Mendes WS
- Mendes WS
- Migone LE
- Márcio Neves Bóia
- Nunes VLB
- Oliveira AC
- Pastorino AC
- Pedrosa CMS
- Pessoa SB
- Ponde R
- Queiroz MJA
- Rego Jr FA
- Rivaldo Venâncio da Cunha
- Sherlock IA
- Silva AR
- Silva ES
- Tavares LMSA
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Two-particle azimuthal correlations in photonuclear ultraperipheral Pb plus Pb collisions at 5.02 TeV with ATLAS
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Abusleme Hoffman AC
- 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
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akesson TPA
- Akilli E
- Akimov A
- 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
- Alvarez Estevez M
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aparo MA
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arling J-H
- 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
- Austrup VA
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Backman F
- Bagnaia P
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Bakos E
- Balaji S
- Balasubramanian R
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barends KN
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
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- Barreiro F
- Barron U
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer P
- Bawa HS
- Bayirli A
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
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- Becker K
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- Beddall AJ
- Bednyakov VA
- Bee CP
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- Begalli M
- Begel M
- Behera A
- Behr JK
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
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- Berta P
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- Bethke S
- Betti A
- Bevan AJ
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bianchi RM
- Biebel O
- Bielski R
- Bierwagen K
- Biesuz N
- Biglietti M
- Billoud TR
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birch-sykes CJ
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Boeriu OEV
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bolanos GR
- Bold T
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borbely AG
- Borecka-Bielska HM
- Borgna LS
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bouaouda K
- Boudreau J
- Bouhova-Thacker E
- Boumediene D
- Bouquet R
- Bourdarios CA
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
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- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brener R
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- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Brueers B
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buescher V
- Bugge MK
- Bulekov O
- Bullard BA
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
- Camelia EA
- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capriles FGD
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli T
- Carlino G
- Carlson BT
- Carlson EM
- Carminati L
- Carnesale M
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carratta G
- Carter JWS
- Carter TM
- Casado MP
- Casha AF
- Castiglia EG
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavasinni V
- Celebi E
- Celli F
- Cerny K
- Cerqueira AS
- Cerri A
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- Cervelli A
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- Chakraborty D
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- Chargeishvili B
- Charlton DG
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- Chatterjee M
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- Chen B
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- Chen SJ
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- Chen Y
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- Cheng CL
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- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
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- Choi K
- Chomont AR
- Chou Y
- Chow YS
- Christopher LD
- Chu MC
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- Chudoba J
- Chwastowski JJ
- Cieri D
- Ciesla KM
- Cindro V
- Ciocio A
- Cirotto F
- Citron ZH
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- Ciubotaru DA
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- Clark A
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- Clawson SE
- Clement C
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- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
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- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Danninger M
- Dao V
- Darbo G
- Dattagupta A
- David C
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- Davis DR
- Dawson I
- de Andrade Filho LM
- De Araujo MV
- De Asmundis R
- De Beurs M
- De Castro S
- De Groot N
- de Jong P
- De la Torre H
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- de Renstrom PAB
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- Deviveiros PO
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- Di Ciaccio A
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- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/07/2021
- Field of study
Two-particle long-range azimuthal correlations are measured in photonuclear collisions using
1.7
nb
−
1
of 5.02 TeV
Pb
+
Pb
collision data collected by the ATLAS experiment at the CERN Large Hadron Collider. Candidate events are selected using a dedicated high-multiplicity photonuclear event trigger, a combination of information from the zero-degree calorimeters and forward calorimeters, and from pseudorapidity gaps constructed using calorimeter energy clusters and charged-particle tracks. Distributions of event properties are compared between data and Monte Carlo simulations of photonuclear processes. Two-particle correlation functions are formed using charged-particle tracks in the selected events, and a template-fitting method is employed to subtract the nonflow contribution to the correlation. Significant nonzero values of the second- and third-order flow coefficients are observed and presented as a function of charged-particle multiplicity and transverse momentum. The results are compared with flow coefficients obtained in proton-proton and proton-lead collisions in similar multiplicity ranges, and with theoretical expectations. The unique initial conditions present in this measurement provide a new way to probe the origin of the collective signatures previously observed only in hadronic collision
Dijet Resonance Search with Weak Supervision Using root S=13 TeV pp Collisions in the ATLAS Detector
- Author
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zinonos Z
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- Zivkovic L
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 25/09/2020
- Field of study
This Letter describes a search for narrowly resonant new physics using a machine-learning anomaly
detection procedure that does not rely on signal simulations for developing the analysis selection. Weakly
supervised learning is used to train classifiers directly on data to enhance potential signals. The targeted
topology is dijet events and the features used for machine learning are the masses of the two jets. The
resulting analysis is essentially a three-dimensional search A → BC, for mA ∼ OðTeVÞ, mB; mC ∼
Oð100 GeVÞ and B, C are reconstructed as large-radius jets, without paying a penalty associated with
a large trials factor in the scan of the masses of the two jets. The full run 2 ffiffi
s p ¼ 13 TeV pp collision
dataset of 139 fb−1 recorded by the ATLAS detector at the Large Hadron Collider is used for the search.
There is no significant evidence of a localized excess in the dijet invariant mass spectrum between 1.8 and
8.2 TeV. Cross-section limits for narrow-width A, B, and C particles vary with mA, mB, and mC. For
example, when mA ¼ 3 TeV and mB ≳ 200 GeV, a production cross section between 1 and 5 fb is
excluded at 95% confidence level, depending on mC. For certain masses, these limits are up to 10 times
more sensitive than those obtained by the inclusive dijet search. These results are complementary to the
dedicated searches for the case that B and C are standard model boson
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Acharya BS
- Achkar B
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- Agapopoulou C
- Agaras MN
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- Aguilar-Saavedra JA
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- Alberghi GL
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- Zakharchuk N
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- Zemaityte G
- Zeng JC
- Zenin O
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
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- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 02/07/2021
- Field of study
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fb−1 of s√ = 13 TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015–2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single Z boson production, Higgs boson production and on-shell ZZ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The Z → 4ℓ branching fraction is extracted, giving a value of (4.41 ± 0.30) × 10−6. Constraints on effective field theory parameters and a model based on a spontaneously broken B − L gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information
Search for dark matter in events with missing transverse momentum and a Higgs boson decaying into two photons in pp collisions at root s=13 TeV with the ATLAS detector
- Author
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- Abhayasinghe DK
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- Zhemchugov A
- Zheng Z
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- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/10/2021
- Field of study
A search for dark-matter particles in events with large missing transverse momentum and a Higgs boson candidate decaying into two photons is reported. The search uses 139 fb−1 of proton-proton collision data collected at s√ = 13 TeV with the ATLAS detector at the CERN LHC between 2015 and 2018. No significant excess of events over the Standard Model predictions is observed. The results are interpreted by extracting limits on three simplified models that include either vector or pseudoscalar mediators and predict a final state with a pair of dark-matter candidates and a Higgs boson decaying into two photons
Medium-Induced Modification of Z-Tagged Charged Particle Yields in Pb+Pb Collisions at 5.02 TeV with the ATLAS Detector
- Author
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- Abbott B
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- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Agapopoulou C
- Agaras MN
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- Aguilar-Saavedra JA
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- Aielli G
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- Alberghi GL
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- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 19/02/2021
- Field of study
The yield of charged particles opposite to a
Z
boson with large transverse momentum (
p
T
) is measured in
260
 
 
pb
−
1
of
p
p
and
1.7
 
 
nb
−
1
of
Pb
+
Pb
collision data at 5.02 TeV per nucleon pair recorded with the ATLAS detector at the Large Hadron Collider. The
Z
boson tag is used to select hard-scattered partons with specific kinematics, and to observe how their showers are modified as they propagate through the quark-gluon plasma created in
Pb
+
Pb
collisions. Compared with
p
p
collisions, charged-particle yields in
Pb
+
Pb
collisions show significant modifications as a function of charged-particle
p
T
in a way that depends on event centrality and
Z
boson
p
T
. The data are compared with a variety of theoretical calculations and provide new information about the medium-induced energy loss of partons in a
p
T
regime difficult to measure through other channels
Search for pair production of third-generation scalar leptoquarks decaying into a top quark and a τ-lepton in pp collisions at s√ = 13 TeV with the ATLAS detector
- Author
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- Abhayasinghe DK
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- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhou H
- Zhou M
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
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- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 30/06/2021
- Field of study
A search for pair production of third-generation scalar leptoquarks decaying into a top quark and a τ-lepton is presented. The search is based on a dataset of pp collisions at s√ = 13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. Events are selected if they have one light lepton (electron or muon) and at least one hadronically decaying τ -lepton, or at least two light leptons. In addition, two or more jets, at least one of which must be identified as containing b-hadrons, are required. Six final states, defined by the multiplicity and flavour of lepton candidates, are considered in the analysis. Each of them is split into multiple event categories to simultaneously search for the signal and constrain several leading backgrounds. The signal-rich event categories require at least one hadronically decaying τ-lepton candidate and exploit the presence of energetic final-state objects, which is characteristic of signal events. No significant excess above the Standard Model expectation is observed in any of the considered event categories, and 95% CL upper limits are set on the production cross section as a function of the leptoquark mass, for different assumptions about the branching fractions into tτ and bν. Scalar leptoquarks decaying exclusively into tτ are excluded up to masses of 1.43 TeV while, for a branching fraction of 50% into tτ, the lower mass limit is 1.22 TeV
Measurement of jet-substructure observables in top quark, W boson and light jet production in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
- Acharya BS
- Adachi S
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- Adelman J
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- Aguilar-Saavedra JA
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- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
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- Alimonti G
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- Calandri A
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- Calfayan P
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- Calvet D
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- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
- Cameron D
- Camincher C
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- Camplani A
- Campoverde A
- Canale V
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- Casado MP
- Casha AF
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- Catmore JR
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- de Renstrom PAB
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 06/08/2019
- Field of study
A measurement of jet substructure observables is presented using data collected in 2016 by the ATLAS experiment at the LHC with proton-proton collisions at s√ = 13 TeV. Large-radius jets groomed with the trimming and soft-drop algorithms are studied. Dedicated event selections are used to study jets produced by light quarks or gluons, and hadronically decaying top quarks and W bosons. The observables measured are sensitive to substructure, and therefore are typically used for tagging large-radius jets from boosted massive particles. These include the energy correlation functions and the N-subjettiness variables. The number of subjets and the Les Houches angularity are also considered. The distributions of the substructure variables, corrected for detector effects, are compared to the predictions of various Monte Carlo event generators. They are also compared between the large-radius jets originating from light quarks or gluons, and hadronically decaying top quarks and W bosons
OXYGEN-CONSUMPTION RELATED TO SIZE AND SEX IN THE TROPICAL MILLIPEDE PSEUDONANNOLENE-TRICOLOR (DIPLOPODA, SPIROSTREPTIDA)
- Publication venue
- Elsevier B.V.
- Publication date
- Field of study
1. The oxygen consumption of the tropical millipede, Pseudonannolene tricolor (Spirostreptida, Pseudonannolenidae) was studied in both male and female animals (body mass varying from 0.242 to 2.802 g) using a Warburg microrespirometer at 25-degrees-C.2. The allometric equation M = a W(b) was used in order to check the metabolic increases with increasing body mass. The b exponents were, respectively, 0.68 for males and 0.60 for females.3. Results are discussed in terms of the meaning of the b values in Diplopoda and animals in general.4. A relationship between volume and body mass in P. tricolor is also reported