1,354 research outputs found
Anopheles Imd Pathway Factors and Effectors in Infection Intensity-Dependent Anti-Plasmodium Action
- Author
- A Cohuet
- AC Bahia
- AM Mendes
- Ana C. Bahia
- C Frolet
- C Mitri
- CB Pumpuni
- CB Pumpuni
- CM Cirimotich
- David S. Schneider
- F Leulier
- George Dimopoulos
- GK Christophides
- J Rodrigues
- Jayme A. Souza-Neto
- Jessica Shiao
- JR Delaney
- L Gupta
- Lindsey S. Garver
- LS Garver
- M Fraiture
- M Kim
- M Povelones
- M Tsuda
- MA Osta
- MQ Benedict
- N Buchon
- N Lhocine
- N Silverman
- NT Nehme
- S Blandin
- S Kumar
- S Libert
- S Meister
- S Meister
- S Stöven
- S Stöven
- S Vidal
- SM Rottschaefer
- Suchismita Das
- Y Dong
- Y Dong
- Y Dong
- Yuemei Dong
- Publication venue
- Public Library of Science
- Publication date
- 07/06/2012
- Field of study
The Anopheles gambiae immune response against Plasmodium falciparum, an etiological agent of human malaria, has been identified as a source of potential anti-Plasmodium genes and mechanisms to be exploited in efforts to control the malaria transmission cycle. One such mechanism is the Imd pathway, a conserved immune signaling pathway that has potent anti-P. falciparum activity. Silencing the expression of caspar, a negative regulator of the Imd pathway, or over-expressing rel2, an Imd pathway-controlled NFkappaB transcription factor, confers a resistant phenotype on A. gambiae mosquitoes that involves an array of immune effector genes. However, unexplored features of this powerful mechanism that may be essential for the implementation of a malaria control strategy still remain. Using RNA interference to singly or dually silence caspar and other components of the Imd pathway, we have identified genes participating in the anti-Plasmodium signaling module regulated by Caspar, each of which represents a potential target to achieve over-activation of the pathway. We also determined that the Imd pathway is most potent against the parasite's ookinete stage, yet also has reasonable activity against early oocysts and lesser activity against late oocysts. We further demonstrated that caspar silencing alone is sufficient to induce a robust anti-P. falciparum response even in the relative absence of resident gut microbiota. Finally, we established the relevance of the Imd pathway components and regulated effectors TEP1, APL1, and LRIM1 in parasite infection intensity-dependent defense, thereby shedding light on the relevance of laboratory versus natural infection intensity models. Our results highlight the physiological considerations that are integral to a thoughtful implementation of Imd pathway manipulation in A. gambiae as part of an effort to limit the malaria transmission cycle, and they reveal a variety of previously unrecognized nuances in the Imd-directed immune response against P. falciparum
Transcriptomic and functional analysis of the Anopheles gambiae salivary gland in relation to blood feeding
- Author
- A Lanfrancotti
- AA James
- AA Lund
- AC Koutsos
- AK Ghosh
- Andrea Radtke
- Antonio M Mendes
- B Arca
- B Arca
- B Arca
- B Arca
- B Boisson
- BJ Mans
- CF Golenda
- D Vlachou
- DE Champagne
- E Calvo
- E Calvo
- E Calvo
- E Calvo
- E Calvo
- E Warr
- E Warr
- F Lombardo
- G Dimopoulos
- G Dimopoulos
- George Dimopoulos
- GJ Van Steijn
- GK Christophides
- H Isawa
- I Rosinski-Chupin
- IM Francischetti
- IM Francischetti
- JD Robertus
- Jesus G Valenzuela
- JG Valenzuela
- JG Valenzuela
- JM Ribeiro
- JM Ribeiro
- JM Ribeiro
- JM Ribeiro
- JM Ribeiro
- JM Ribeiro
- JM Ribeiro
- JP David
- KR Stark
- MA Okulate
- MA Osta
- ML Bolognesi
- MQ Benedict
- MW Pfaffl
- MZ Lin
- O Marinotti
- O Terenius
- OM Neira
- OM Neira
- P Baldacci
- P Siriyasatien
- PA Rossignol
- PE Hardin
- PX Xu
- R Aguilar
- RL Kerlin
- RM Waterhouse
- RQ Monteiro
- S Blandin
- S Das
- S Thangamani
- S Yoshida
- SF Altschul
- Suchismita Das
- U Frevert
- V Choumet
- W Nickel
- WV So
- XB Qiu
- Y Belkaid
- Y Dong
- Young-Jun Choi
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
<p>Abstract</p> <p>Background</p> <p>The <it>Anopheles gambiae </it>salivary glands play a major role in malaria transmission and express a variety of bioactive components that facilitate blood-feeding by preventing platelet aggregation, blood clotting, vasodilatation, and inflammatory and other reactions at the probing site on the vertebrate host.</p> <p>Results</p> <p>We have performed a global transcriptome analysis of the <it>A. gambiae </it>salivary gland response to blood-feeding, to identify candidate genes that are involved in hematophagy. A total of 4,978 genes were found to be transcribed in this tissue. A comparison of salivary gland transcriptomes prior to and after blood-feeding identified 52 and 41 transcripts that were significantly up-regulated and down-regulated, respectively. Ten genes were further selected to assess their role in the blood-feeding process using RNAi-mediated gene silencing methodology. Depletion of the salivary gland genes encoding <it>D7L2</it>, <it>anophelin</it>, <it>peroxidase</it>, the <it>SG2 precursor</it>, and a <it>5'nucleotidase </it>gene significantly increased probing time of <it>A. gambiae </it>mosquitoes and thereby their capacity to blood-feed.</p> <p>Conclusions</p> <p>The salivary gland transcriptome comprises approximately 38% of the total mosquito transcriptome and a small proportion of it is dynamically changing already at two hours in response to blood feeding. A better understanding of the salivary gland transcriptome and its function can contribute to the development of pathogen transmission control strategies and the identification of medically relevant bioactive compounds.</p
The impact of surgical delay on resectability of colorectal cancer: An international prospective cohort study
- Author
- Abadia M
- Abassy J
- Abate E
- Abbott Tom EF
- Abdelaal Samir A
- Abdeldayem H
- Abdelkabir M
- Abdelsamed A
- Abdulwahed E
- Abiyere H
- Abou Chaar MK
- Abukhalaf SA
- Abukhalaf Sadi
- Adamina Michel
- Ademuyiwa Adesoji
- Ademuyiwa Adesoji O
- Adeyeye A
- Adisa Adewale
- Afzal MF
- Agarwal Arnav
- Aggarwal M
- Agnes A
- Agostini C
- Agrawal A
- Agrawal N
- Agresta F
- Aguiar Junior S
- Ahmed A
- Ahmed K
- Ahmed Nafees R
- Ahmed Z
- Ahn JH
- Aime A
- Akhtar N
- Akkulak Murat
- Akrivou D
- Al Abdallah M
- Al Riyami S
- Al Sayed M
- Al-Masri M
- Al-Najjar H
- Al-Slaibi I
- Alaa S
- Alakaloko Felix
- Alameer Ehab
- Alamri Alex
- Alawneh F
- Albertsmeier M
- Albertsmeier Markus
- Alderson Derek
- Aldokali N
- Alemanno G
- Alfieri S
- Algallai M
- Ali AA
- Alkadiki Ghadah Z
- Almaadany Faraj S
- Almeida AC
- Almeida-Reis R
- Almezghwi H
- Almond Max
- Alrahawy M
- Alser Osaid
- Alshaar Muhammad
- Alshareea E
- Alshareef K
- Alshryda Sattar
- Alsoufi A
- Altamirano Riquoir C
- Altomare DF
- Altomi I
- Alurralde C
- Alvarez MR
- Alvi A
- Alwarfly S
- AlZAEDE S
- Alzeerelhouseini IAH
- Amaral MJ
- Amira G
- Amorim E
- Amrani L
- Anania G
- Anastasi A
- Andrade Kam da Silva A
- Andrade R
- Annessi V
- Annicchiarico A
- Antonakis P
- Antonopoulou M
- Aprile A
- Aremu M
- Arias-Amezquita F
- Aribi N
- Aribi S
- Arkadopoulos N
- Armao T
- Armatura G
- Arminio A
- Arnaud Alexis P
- Arora A
- Arslan K
- Ashoush F
- Athanasakis E
- Attia D
- Augestad Knut Magne
- Aversano A
- Avlund T
- Awada Barakat J
- Ayasra F
- Ayasra Faris
- Ayasra Y
- Ayub B
- Ayubi A
- Ayyaz M
- Azevedo C
- Azevedo J
- Azevedo Jose
- Azevedo P
- Azman Mohd ZA
- Azzam AY
- Babalola O
- Badra R
- Bagraith K
- Baili E
- Balabel M
- Balconi A
- Baldari L
- Baldi C
- Baldini E
- Bali K
- Ballabio M
- Ballouhey Q
- Baloyiannis I
- Bandovas JP
- Bankhead-Kendall Brittany K
- Banky B
- Banuelos Romero E
- Baptista VH
- Barker D
- Barlow Emma
- Barod Ravi
- Barone R
- Baronio G
- Barrat B
- Barros Vieira A
- Bartalucci B
- Bartolini I
- Bashir Y
- Bass G
- Batistotti P
- Batstone Martin
- Baxevanidou K
- Beard David
- Becker R
- Bekele K
- Belia F
- Belkhadir ZH
- Bellacci A
- Belli A
- Bellolio F
- Bellora P
- Belluco C
- Belvedere A
- Bendjemar L
- Benkabbou A
- Benson Ruth A
- Bergamini C
- Bergeat D
- Bernante P
- Berselli M
- Bertelli G
- Bertolani E
- Besser N
- Beyer K
- Beyrne C
- Bezerra Santos T
- Bhangu Aneel A
- Bhat GA
- Bhat MA
- Biala M
- Bianchini M
- Bianco F
- Biel Juan Rey
- Bigam D
- Biondi A
- Birolo SL
- Bisagni P
- Blanco-Colino Ruth
- Bodanese B
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- Bondurri A
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- Borges Castro F
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- Borroni G
- Bouchagier K
- Bouche PA
- Bouliaris K
- Boutros M
- Bowman S
- Boyce R
- Brachini G
- Bradulskis S
- Braham H
- Brar Amanpreet
- Bravo Ana Minaya
- Breen Kerry A
- Bretherton Chris
- Bristow Rob
- Bromage Steve
- Brown C
- Brunelli Alessandro
- Bruscino A
- Buarque Igor Lima
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- Bucci Fares A
- Buerba GA
- Burgan D
- Burke Joshua
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- Bywater Edward
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- Capunge I
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- Cetares C
- Chaar Mohammad
- Chakrabortee Sohini
- Chan E
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- Chatzikomnitsa P
- Chaudhry Daoud
- Chebaro A
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- Christensen P
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- Publication venue
- 'Royal College of Obstetricians & Gynaecologists (RCOG)'
- Publication date
- 01/06/2022
- Field of study
AIM: The SARS-CoV-2 pandemic has provided a unique opportunity to explore the impact of surgical delays on cancer resectability. This study aimed to compare resectability for colorectal cancer patients undergoing delayed versus non-delayed surgery. METHODS: This was an international prospective cohort study of consecutive colorectal cancer patients with a decision for curative surgery (January-April 2020). Surgical delay was defined as an operation taking place more than 4 weeks after treatment decision, in a patient who did not receive neoadjuvant therapy. A subgroup analysis explored the effects of delay in elective patients only. The impact of longer delays was explored in a sensitivity analysis. The primary outcome was complete resection, defined as curative resection with an R0 margin. RESULTS: Overall, 5453 patients from 304 hospitals in 47 countries were included, of whom 6.6% (358/5453) did not receive their planned operation. Of the 4304 operated patients without neoadjuvant therapy, 40.5% (1744/4304) were delayed beyond 4 weeks. Delayed patients were more likely to be older, men, more comorbid, have higher body mass index and have rectal cancer and early stage disease. Delayed patients had higher unadjusted rates of complete resection (93.7% vs. 91.9%, P = 0.032) and lower rates of emergency surgery (4.5% vs. 22.5%, P < 0.001). After adjustment, delay was not associated with a lower rate of complete resection (OR 1.18, 95% CI 0.90-1.55, P = 0.224), which was consistent in elective patients only (OR 0.94, 95% CI 0.69-1.27, P = 0.672). Longer delays were not associated with poorer outcomes. CONCLUSION: One in 15 colorectal cancer patients did not receive their planned operation during the first wave of COVID-19. Surgical delay did not appear to compromise resectability, raising the hypothesis that any reduction in long-term survival attributable to delays is likely to be due to micro-metastatic disease
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
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- Aad G
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- Zeißner SV
- Zemaityte G
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- Zeng Q
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- Zhao X
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- Zhemchugov A
- Zhou B
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- Zhou L
- Zhou M
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- Zhou N
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- 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
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Performance of missing transverse momentum reconstruction with the ATLAS detector using proton–proton collisions at √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
- Alconada Verzini MJ
- 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 Gonzalez B
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- 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
- Arabidze G
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armadans R Caminal
- Armbruster AJ
- Armitage LJ
- Armstrong A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in proton–proton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying τ -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fb−1
Measurement of VH, H → b b ¯ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
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- Alison J
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- Alviggi MG
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- An F
- Anastopoulos C
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- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
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- Angelozzi I
- Angerami A
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- Zhemchugov A
- Zheng Z
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- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex
Search for pairs of highly collimated photon-jets 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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- Zhao X
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- Zhao Z
- Zhemchugov A
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- Zhou L
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- Zhu CG
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- 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
- Zu Theenhausen H Meyer
- Zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/08/2018
- Field of study
Results of a search for the pair production of photon-jets—collimated groupings of photons—in the ATLAS detector at the Large Hadron Collider are reported. Highly collimated photon-jets can arise from the decay of new, highly boosted particles that can decay to multiple photons collimated enough to be identified in the electromagnetic calorimeter as a single, photonlike energy cluster. Data from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 36.7 fb−1, were collected in 2015 and 2016. Candidate photon-jet pair production events are selected from those containing two reconstructed photons using a set of identification criteria much less stringent than that typically used for the selection of photons, with additional criteria applied to provide improved sensitivity to photon-jets. Narrow excesses in the reconstructed diphoton mass spectra are searched for. The observed mass spectra are consistent with the Standard Model background expectation. The results are interpreted in the context of a model containing a new, high-mass scalar particle with narrow width, X, that decays into pairs of photon-jets via new, light particles, a. Upper limits are placed on the cross section times the product of branching ratios σ×B(X→aa)×B(a→γγ)2 for 200 GeV<mX<2 TeV and for ranges of ma from a lower mass of 100 MeV up to between 2 and 10 GeV, depending upon mX. Upper limits are also placed on σ×B(X→aa)×B(a→3π0)2 for the same range of mX and for ranges of ma from a lower mass of 500 MeV up to between 2 and 10 GeV
Multi-messenger observations of a binary neutron star merger
- Author
- Aab A
- Aartsen MG
- Abbott BP
- Abbott R
- Abbott TD
- Abbott TMC
- Abdalla H
- Abe F
- Abeysekara AU
- Abramo LR
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- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ~1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40+8-8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 Mo. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ~40 Mpc) less than 11 hours after the merger by the One- Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transient’s position ~9 and ~16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
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- Zhemchugov A
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
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