540 research outputs found
Cardiovascular and hormonal responses to static handgrip in young and older healthy men
- Author
- A Housiiere
- A Jindra Jr
- A. Ziemba
- AJ Donato
- AM Weissler
- AM Weissler
- AR Lind
- AR Lind
- AU Ferrari
- AU Ferrari
- BL Sabates
- C Cardillo
- C Cardillo
- C Sachs
- CE Martin
- CE Martin
- CJ Charles
- CJ Charles
- CJ Charles
- DB Evans
- DH Spodick
- DHJ Thijssen
- DR Seals
- DR Seals
- E Mangieri
- E Mangieri
- E Thorin
- EG Lakatta
- G Cybulski
- G Cybulski
- G. Cybulski
- GF Levi
- GJ Palmer
- I Szokodi
- J Kato
- J Padilla
- JA Taylor
- JP Hinson
- JR Sowers
- JS Petrofsky
- JT Shepherd
- K Krzeminski
- K Krzeminski
- K Krzeminski
- K Meeran
- K Mishima
- K Nazar
- K Terata
- K Uchida
- K. Krzemiński
- K. Nazar
- M Kino
- MD Esler
- MH Huang
- N Fukai
- RM Bruno
- RM Martínez-Alvarez
- S Cottone
- S Khan
- S Yűksel
- SH Boutcher
- T Kita
- T Laitinen
- TA Markel
- TD Warner
- TL Whitsett
- U Scherrer
- VM Pigott
- WG Haynes
- WL Haskell
- WL Miller
- X Zhang
- Y Hattori
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2011
- Field of study
The purpose of this study was to investigate the effect of age on cardiovascular changes and plasma concentrations of adrenomedullin (ADM), catecholamines, endothelin-1 (ET-1) and plasma renin activity (PRA) in healthy men. A total of 15 young (21 ± 0.3 years) and 15 older (64 ± 0.7 years) healthy men performed two 3-min bouts of static handgrip at 30% of maximal voluntary contraction, alternately with each hand without any break between the bouts. During exercise heart rate (HR), blood pressure (BP), stroke volume (SV) and pre-ejection period (PEP) and left ventricle ejection time (LVET) were measured. Blood samples were taken before exercise, at the end of both exercise bouts and in the fifth minute of the recovery period. The handgrip-induced increases in HR and cardiac output were significantly smaller in older than in young men (p < 0.01). SV decreased only in older men (p < 0.001). There were no differences between groups in BP increases. The baseline plasma ADM and catecholamines were higher in older man compared to young subjects. Handgrip caused increases in plasma ADM, ET-1 and PRA only in older men (p < 0.05). The increases in plasma ADM correlated positively with those of noradrenaline (NA), PRA, ET-1 and LVET and negatively with changes in total peripheral resistance (TPR), SV, PEP and PEP/LVET ratio. The increases in plasma ET-1 correlated positively with those of NA, PRA, TPR, mean BP and SV. These results revealed that ADM, ET-1 and angiotensin II can contribute to maintain vascular tone during static exercise in older but not in younger men
Interactions of melatonin with mammalian mitochondria. Reducer of energy capacity and amplifier of permeability transition.
- Author
- A Herxheimer
- A Slominski
- A Wölfler
- A. Toninello
- AB Lerner
- AC Santos
- AG Gornall
- AW Leung
- AW Leung
- BD Jensen
- C Pieri
- CI Gutiérrez
- E Agostinelli
- E. Agostinelli
- F Tietze
- G Loschen
- G Petrosillo
- GP McStay
- HM Zhang
- HR Lötscher
- I Bejarano
- J Arendt
- J Espino
- JJ Lemasters
- L. Zago
- M Büyükavcı
- M Martín
- M Salvi
- M. Bragadin
- M. Maritati
- MJ Hansson
- MT Grijalba
- N Buscemi
- N Kamo
- P. Martinis
- RA Osseni
- RJ Reiter
- RM Sainz
- S Cardillo
- S. Grancara
- SA Andrabi
- SR Pandi-Perumal
- T-Y Chan
- U Marchi De
- V Battaglia
- V Battaglia
- V Srinivasan
- V Yankovskaya
- V. Battaglia
- V. Rizzoli
- VM Cassone
- WC Schneider
- WH Bergstrom
- Z Matuszak
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Melatonin, a metabolic product of the amino acid tryptophan, induces a dose-dependent energy drop correlated with a decrease in the oxidative phosphorylation process in isolated rat liver mitochondria. This effect involves a gradual decrease in the respiratory control index and significant alterations in the state 4/state 3 transition of membrane potential (ΔΨ). Melatonin, alone, does not affect the insulating properties of the inner membrane but, in the presence of supraphysiological Ca2+, induces a ΔΨ drop and colloid-osmotic mitochondrial swelling. These events are sensitive to cyclosporin A and the inhibitors of Ca2+ transport, indicative of the induction or amplification of the mitochondrial permeability transition. This phenomenon is triggered by oxidative stress induced by melatonin and Ca2+, with the generation of hydrogen peroxide and the consequent oxidation of sulfydryl groups, glutathione and pyridine nucleotides. In addition, melatonin, again in the presence of Ca2+, can also induce substantial release of cytochrome C and AIF (apoptosis-inducing factor), thus revealing its potential as a pro-apoptotic agent
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- 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
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- 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
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- 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
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asawatavonvanich T
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Ayoub MK
- Azuelos G
- Bachacou H
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- Backes M
- Backman F
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- Bahmani M
- Bahrasemani H
- Bailey AJ
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- Bakker PJ
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- Tobon CAM
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- Trofymov A
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- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Turchikhin S
- Turgeman D
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- von Buddenbrock SE
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- Vukotic I
- Wagner P
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- Wahdan S
- Wahlberg H
- Walbrecht VM
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- Wallangen V
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- Warburton A
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- Warrack N
- Washbrook A
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- Webb AF
- Webb S
- Weber C
- Weber MS
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- Weber SM
- Weidberg AR
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
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- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
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- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
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- Wiik-Fuchs LAM
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- Wingerter-Seez I
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- Wong VWS
- Woods NL
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- Wozniak KW
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
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- Xiao X
- Xiotidis I
- Xu D
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- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
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- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
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- Yan Z
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- Yap YC
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- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
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- Zaripovas DR
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- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
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- Zhang DF
- Zhang G
- Zhang H
- Zhang J
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- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- 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
- 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
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Geographic range did not confer resilience to extinction in terrestrial vertebrates at the end-Triassic crisis
- Author
- AD Barnosky
- AF Budd
- AL Rode
- AL Rode
- AM Dunhill
- AM Dunhill
- BU Haq
- CE Myers
- CE Myers
- CM McCain
- D Jablonski
- D Jablonski
- D Jablonski
- D Jablonski
- D Jablonski
- D Jablonski
- DM Raup
- FM Gradstein
- GM Mace
- GT Lloyd
- J Alroy
- J Fröbisch
- J Whiteside
- JH Whiteside
- JJ Sepkoski
- JL Payne
- JW Valentine
- K Roy
- LH Tanner
- M Cardillo
- M Foote
- M Foote
- M Foote
- M Foote
- MC Langer
- MD Ezcurra
- MG Powell
- MJ Benton
- MJ Benton
- MJ Benton
- MJ Benton
- N Cooper
- P Raia
- P Upchurch
- PM Barrett
- RA Slatyer
- RBJ Benson
- RBJ Benson
- RBJ Benson
- RBJ Benson
- RJ Butler
- RJ Butler
- RK Bambach
- RL Don
- S Nürnberg
- SC Wang
- SL Brusatte
- SL Brusatte
- SL Pimm
- TJ Blackburn
- VM Savage
- W Kiessling
- YD Sun
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 11/08/2015
- Field of study
Rates of extinction vary greatly through geological time, with losses particularly concentrated in mass extinctions. Species duration at other times varies greatly, but the reasons for this are unclear. Geographical range correlates with lineage duration amongst marine invertebrates, but it is less clear how far this generality extends to other groups in other habitats. It is also unclear whether a wide geographical distribution makes groups more likely to survive mass extinctions. Here we test for extinction selectivity amongst terrestrial vertebrates across the end-Triassic event. We demonstrate that terrestrial vertebrate clades with larger geographical ranges were more resilient to extinction than those with smaller ranges throughout the Triassic and Jurassic. However, this relationship weakened with increasing proximity to the end-Triassic mass extinction, breaking down altogether across the event itself. We demonstrate that these findings are not a function of sampling biases; a perennial issue in studies of this kind
Study of matrix metalloproteinases and their inhibitors in prostate cancer
- Author
- A Ahmad
- A Boulay
- A Bratland
- A Remacle
- A Suárez
- AC Riddick
- AR Nelson
- B Brehmer
- B Fingleton
- C Hughes
- CC Lynch
- CE Brinckerhoff
- CJ Logothetis
- CM Overall
- D Millimaggi
- D Trudel
- F J Vizoso
- FJ Vizoso
- G Morgia
- H Yamashita
- I Flemming
- J Cao
- J Cao
- J M Fernández
- J M González
- J Mueller
- J Varani
- JM Freije
- K Gohji
- L O González
- L Zhang
- LA Cornelius
- LO Gonzalez
- M Demers
- M Egeblad
- M Semaan
- M Thewes
- MB Eisen
- MM Daja
- MP Chenard
- MR Cardillo
- MV Meng
- N Liu
- P Basset
- P Basset
- RD Bonfil
- RL Parker
- S Escaff
- S González-Reyes
- S Manes
- S Soni
- SM Nabha
- SM Pulukuri
- SO Wurtz
- ST Pang
- V Knauper
- V Noe
- V Turk
- VM Wasenius
- W Whitmore
- WA Sakr
- WD Zhong
- WG Stetler-Stevenson
- Y Jiang
- YA DeClerck
- Z Dong
- Publication venue
- Nature Publishing Group
- Publication date
- 01/01/2010
- Field of study
Reconstruction of hadronic decay products of tau leptons with the ATLAS experiment
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TP
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Alkire SP
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amadio BT
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Aranda CP
- Araque JP
- Araya ST
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkinson M
- Atlay NB
- Augsten K
- Aurousseau M
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baak MA
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bain T
- Baines JT
- Baker OK
- Baldin EM
- Balek P
- Balestri T
- Balli F
- Balunas WK
- Banas E
- Banerjee S
- Bannoura AAE
- Barajas CAC
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Basye A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Becker K
- Becker M
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr JK
- Belanger-Champagne C
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Bender M
- Bendtz K
- Benekos N
- Benhammou Y
- Benjamin DP
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Berghaus F
- Beringer J
- Berlingen JM
- Bernard C
- Bernard NR
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertsche C
- Bertsche D
- Besana MI
- Besjes GJ
- Bessner M
- Besson N
- Betancourt C
- Bethke S
- Bevan AJ
- Bhimji W
- Bianchi RM
- Bianchini L
- Bianco M
- Biebel O
- Biedermann D
- Biesuz NV
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biondi S
- Bjergaard DM
- Black CW
- Black JE
- Black KM
- Blackburn D
- Blair RE
- Blanchard J-B
- Blanco JE
- Blazek T
- Bloch I
- Blocker C
- Blum W
- Blumenschein U
- Blunier S
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boehler M
- Boeriu OEV
- Bogaerts JA
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Boldyrev AS
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Borroni S
- Bortfeldt J
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
- Boudreau J
- Bouffard J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Bousson N
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bozic I
- Bracinik J
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brendlinger K
- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Bristow TM
- Britton D
- Britzger D
- Brochu FM
- Brock I
- Brock R
- Bronner J
- Brooijmans G
- Brooks T
- Brooks WK
- Brosamer J
- Brost E
- Bruncko D
- Bruneliere R
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher D
- Buescher V
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- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
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- Yao W-M
- Yap YC
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- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
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- Yuen SPY
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zalieckas J
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- Zambito S
- Zanello L
- Zanzi D
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- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou L
- Zhou L
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2016
- Field of study
This paper presents a new method of reconstructing the individual charged and neutral hadrons in tau decays with the ATLAS detector. The reconstructed hadrons are used to classify the decay mode and to calculate the visible four-momentum of reconstructed tau candidates, significantly improving the resolution with respect to the calibration in the existing tau reconstruction. The performance of the reconstruction algorithm is optimised and evaluated using simulation and validated using samples of Z→ττ and Z(→μμ)+jets events selected from proton–proton collisions at a centre-of-mass energy √s=8TeV, corresponding to an integrated luminosity of 5 fb−1.- We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently. We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF and DNSRC, Denmark; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, HGF, and MPG, Germany; GSRT, Greece; RGC, Hong Kong SAR, China; ISF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; RCN, Norway; MNiSW and NCN, Poland; FCT, Portugal; MNE/IFA, Romania; MES of Russia and NRC KI, Russian Federation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZS, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons of Bern and Geneva, Switzerland; MOST, Taiwan; TAEK, Turkey; STFC, United Kingdom; DOE and NSF, United States of America. In addition, individual groups and members have received support from BCKDF, the Canada Council, CANARIE, CRC, Compute Canada, FQRNT, and the Ontario Innovation Trust, Canada; EPLANET, ERC, FP7, Horizon 2020 and Marie Sklodowska-Curie Actions, European Union; Investissements d'Avenir Labex and Idex, ANR, Region Auvergne and Fondation Partager le Savoir, France; DFG and AvH Foundation, Germany; Herakleitos, Thales and Aristeia programmes co-financed by EU-ESF and the Greek NSRF; BSF, GIF and Minerva, Israel; BRF, Norway; the Royal Society and Leverhulme Trust, United Kingdom. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN and the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA) and in th
Search for anomalous couplings in the W tb vertex from the measurement of double differential angular decay rates of single top quarks produced in the t-channel with the ATLAS detector
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- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 13/10/2015
- Field of study
The electroweak production and subsequent decay of single top quarks is determined by the properties of the Wtb vertex. This vertex can be described by the complex parameters of an effective Lagrangian. An analysis of angular distributions of the decay products of single top quarks produced in the t -channel constrains these parameters simultaneously. The analysis described in this paper uses 4.6 fb−1 of proton-proton collision data at √s =7 TeV collected with the ATLAS detector at the LHC. Two parameters are measured simultaneously in this analysis. The fraction f 1 of decays containing transversely polarised W bosons is measured to be 0.37 ± 0.07 (stat.⊕syst.). The phase δ − between amplitudes for transversely and longitudinally polarised W bosons recoiling against left-handed b-quarks is measured to be −0.014π ± 0.036π (stat.⊕syst.). The correlation in the measurement of these parameters is 0.15. These values result in two-dimensional limits at the 95% confidence level on the ratio of the complex coupling parameters g R and V L, yielding Re[g R /V L] ∈ [−0.36, 0.10] and Im[g R /V L] ∈ [−0.17, 0.23] with a correlation of 0.11. The results are in good agreement with the predictions of the Standard Model
Anatomy of the sign-problem in heavy-dense QCD
- Author
- Adam E Romero
- Aranda C Padilla
- Arjanovic MM
- Armadans R Caminal
- Astigarraga ME Pozo
- Barajas CA Chavez
- Bechtle P
- Beck HP
- Becker K
- Becker M
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- Bednyakov VA
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- Beemster LJ
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- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
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- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
QCD at finite densities of heavy quarks is investigated
using the density-of-states method. The phase factor
expectation value of the quark determinant is calculated to
unprecedented precision as a function of the chemical potential.
Results are validated using those from a reweighting
approach where the latter can produce a significant signalto-noise
ratio. We confirm the particle–hole symmetry at low
temperatures, find a strong sign problem at intermediate values
of the chemical potential, and an inverse Silver Blaze
feature for chemical potentials close to the onset value: here,
the phase-quenched theory underestimates the density of the
full theory
Modelling Z → ττ processes in ATLAS with τ-embedded Z → μμ data
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Alkire SP
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi G
- Amadio BT
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
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- Amoroso S
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- Amundsen G
- Anastopoulos C
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- Aoki M
- Arabidze G
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- Araque JP
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- Arika M
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- Artamonov A
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- Zhemchugov A
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- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2015
- Field of study
This paper describes the concept, technical realisation and validation of a largely data-driven method to model events with Z→ττ decays. In Z→μμ events selected from proton-proton collision data recorded at √s=8 TeV with the ATLAS experiment at the LHC in 2012, the Z decay muons are replaced by τ leptons from simulated Z→ττ decays at the level of reconstructed tracks and calorimeter cells. The τ lepton kinematics are derived from the kinematics of the original muons. Thus, only the well-understood decays of the Z boson and τ leptons as well as the detector response to the τ decay products are obtained from simulation. All other aspects of the event, such as the Z boson and jet kinematics as well as effects from multiple interactions, are given by the actual data. This so-called τ-embedding method is particularly relevant for Higgs boson searches and analyses in ττ final states, where Zarrowττ decays constitute a large irreducible background that cannot be obtained directly from data control samples. In this paper, the relevant concepts are discussed based on the implementation used in the ATLAS Standard Model H→ττ analysis of the full datataset recorded during 2011 and 2012
Measurements of the top quark branching ratios into channels with leptons and quarks with the ATLAS detector
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- Shochet MJ
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- Shrestha S
- Shulga E
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- Sisakyan AN
- Sivoklokov SY
- Sjoelin J
- Sjursen TB
- Skinner MB
- Skottowe HP
- Skubic P
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- Slavicek T
- Slawinska M
- Sliwa K
- Smakhtin V
- Smart BH
- Smestad L
- Smirnov SY
- Smirnov Y
- Smirnova LN
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- Snesarev AA
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- Straessner A
- Stramaglia ME
- Strandberg J
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- Strauss M
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- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
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- Sundermann JE
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- Susinno G
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- Swedish S
- Swiatlowski M
- Sykora I
- Sykora T
- Ta D
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- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Takubo Y
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- Talyshev AA
- Tam JYC
- Tan KG
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- Tanaka R
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- Tannenwald BB
- Tannoury N
- Tapprogge S
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- Tarrade F
- Tartarelli GF
- Tas P
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- Tashiro T
- Tassi E
- Tayalati Y
- Taylor FE
- Taylor GN
- Taylor W
- Tehrani FS
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- Thomas JP
- Thomas-Wilsker J
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- Thompson EN
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- Thompson RJ
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- Thomson M
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- Tskhadadze EG
- Tsukerman II
- Tsulaia V
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- Wingerter-Seez I
- Winklmeier F
- Winter BT
- Wittgen M
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KHY
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wu M
- Wu M
- Wu SL
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- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yakabe R
- Yamada M
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
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- Young C
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- Youssef S
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- Yu JM
- Yuan L
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently. We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF Helmholtz Association, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; RGC, Hong Kong SAR, China; ISF, MINERVA, GIF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW and NCN, Poland; GRICES and FCT, Portugal; MNE/IFA, Romania; MES of Russia and NRC KI, Russian Federation; JINR; MSTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SER, SNSF and Cantons of Bern and Geneva, Switzerland; NSC, Taiwan; TAEK, Turkey; STFC, the Royal Society and Leverhulme Trust, United Kingdom; DOE and NSF, United States of America. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN and the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA) and in the Tier-2 facilities worldwide
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