258 research outputs found
Capturing Dynamicity and Uncertainty in Security and Trust via Situational Patterns
- Author
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2020
- Field of study
Co expression of SCF and KIT in gastrointestinal stromal tumours (GISTs) suggests an autocrine/paracrine mechanism
- Author
- A Catalano
- A Duensing
- A Erlandsson
- A Lemoine
- AL Drayer
- B Williams
- BP Rubin
- C Bredin
- CL Corless
- CR Antonescu
- CR Antonescu
- D Brouty-Boyé
- D Toksoz
- E Ricotti
- G Caruana
- G Caruana
- G Kondoh
- G Sommer
- GD Demetri
- GW Krystal
- H Lahm
- J Fujita
- J-F Emile
- JF Emile
- JF Emile
- JT Reilly
- K Hibi
- K Miyazawa
- L Ronnstrand
- LK Ashman
- M Inoue
- MC Heinrich
- MC Heinrich
- ML Lux
- N Théou
- N Théou-Anton
- O Voytyuk
- P Blume-Jensen
- PT Went
- R Saffroy
- R Zheng
- S Hirota
- S Tabone
- S Tabone
- SJ Hines
- T Nishida
- T Pietsch
- VC Broudy
- Publication venue
- Publication date
- 01/01/2006
- Field of study
KIT is a tyrosine kinase receptor expressed by several tumours, which has for specific ligand the stem cell factor (SCF). KIT is the main oncogene in gastrointestinal stromal tumours (GISTs), and gain-of-function KIT mutations are present in 70% of these tumours. The aim of the study was to measure and investigate the mechanisms of KIT activation in 80 KIT-positive GIST patients. KIT activation was quantified by detecting phosphotyrosine residues in Western blotting. SCF production was determined by reverse transcriptase–PCR, ELISA and/or immunohistochemistry. Primary cultures established from three GISTs were also analysed. The results show that KIT activation was detected in all cases, even in absence of KIT mutations. The fraction of activated KIT was not correlated with the mutational status of GISTs. Membrane and soluble isoforms of SCF mRNA were present in all GISTs analysed. Additionally, SCF was also detected in up to 93% of GISTs, and seen to be present within GIST cells. Likewise, the two SCF mRNA isoforms were found to be expressed in GIST-derived primary cultures. Thus, KIT activation in GISTs may in part result from the presence of SCF within the tumours
Sox6 Is Necessary for Efficient Erythropoiesis in Adult Mice under Physiological and Anemia-Induced Stress Conditions
- Author
- A Bauer
- A Montel-Hagen
- AB Cantor
- AC Heinrich
- AC Perkins
- AP Tsang
- B Dumitriu
- B Dumitriu
- B Nuez
- Bogdan Dumitriu
- C Geminard
- C Tian
- CC Stolt
- D Marinkovic
- D Noordermeer
- DM Wojchowski
- E Fibach
- F Canonne-Hergaux
- GD Longmore
- H Wu
- J Xu
- J Zhang
- Jan Jensen
- K Chen
- K de Jong
- K Srinoun
- KU Wagner
- L Gutiérrez
- LE Lenox
- M Socolovsky
- M Socolovsky
- M Socolovsky
- Michael J. Pazin
- MJ Koury
- MM Rhodes
- MP Menon
- N Hagiwara
- N Hagiwara
- N Motoyama
- N Quayum
- Nayeem Quayum
- O Cohen-Barak
- P Azmi
- P Bhattaram
- P Smits
- P Walfaren
- PA Gregoli
- Pallavi Bhattaram
- Peter Dy
- S Hayashi
- SI Kim
- SL Schrier
- T Hulsen
- TD Richmond
- V Lefebvre
- V Lefebvre
- VC Broudy
- Véronique Lefebvre
- WJ Bakker
- Y Fujiwara
- Y Han
- Yuanshuai Huang
- Z Yi
- Publication venue
- Public Library of Science
- Publication date
- 09/08/2010
- Field of study
BACKGROUND: Definitive erythropoiesis is a vital process throughout life. Both its basal activity under physiological conditions and its increased activity under anemia-induced stress conditions are highly stimulated by the hormone erythropoietin. The transcription factor Sox6 was previously shown to enhance fetal erythropoiesis together and beyond erythropoietin signaling, but its importance in adulthood and mechanisms of action remain unknown. We used here Sox6 conditional null mice and molecular assays to address these questions. METHODOLOGY/PRINCIPAL FINDINGS: Sox6fl/flErGFPCre adult mice, which lacked Sox6 in erythroid cells, exhibited compensated anemia, erythroid cell developmental defects, and anisocytotic, short-lived red cells under physiological conditions, proving that Sox6 promotes basal erythropoiesis. Tamoxifen treatment of Sox6fl/flCaggCreER mice induced widespread inactivation of Sox6 in a timely controlled manner and resulted in erythroblast defects before reticulocytosis, demonstrating that impaired erythropoiesis is a primary cause rather than consequence of anemia in the absence of Sox6. Twenty five percent of Sox6fl/flErGFPCre mice died 4 or 5 days after induction of acute anemia with phenylhydrazine. The others recovered slowly. They promptly increased their erythropoietin level and amplified their erythroid progenitor pool, but then exhibited severe erythroblast and reticulocyte defects. Sox6 is thus essential in the maturation phase of stress erythropoiesis that follows the erythropoietin-dependent amplification phase. Sox6 inactivation resulted in upregulation of embryonic globin genes, but embryonic globin chains remained scarce and apparently inconsequential. Sox6 inactivation also resulted in downregulation of erythroid terminal markers, including the Bcl2l1 gene for the anti-apoptotic factor Bcl-xL, and in vitro assays indicated that Sox6 directly upregulates Bcl2l1 downstream of and beyond erythropoietin signaling. CONCLUSIONS/SIGNIFICANCE: This study demonstrates that Sox6 is necessary for efficient erythropoiesis in adult mice under both basal and stress conditions. It is primarily involved in enhancing the survival rate and maturation process of erythroid cells and acts at least in part by upregulating Bcl2l1
Population ecology of the sea lamprey (Petromyzon marinus) as an invasive species in the Laurentian Great Lakes and an imperiled species in Europe
- Author
- A Haro
- A Lelek
- A Lochet
- A Zerrenner
- AH Lawrie
- AJ Treble
- AL Derosier
- B Malmqvist
- B Malmqvist
- Bernardo R. Quintella
- BGH Johnson
- BJ Irwin
- BJ Wicks
- BR Quintella
- BR Quintella
- BR Quintella
- BR Quintella
- BR Quintella
- BR Smith
- BR Smith
- C Gardner
- C Taverny
- CB Renaud
- CE Goodwin
- CE Torgerson
- Charles P. Madenjian
- CJ Harvey
- CL Smith
- CP Hand
- CP Madenjian
- CP Madenjian
- CP Madenjian
- CP Madenjian
- CP Madenjian
- CS Mateus
- DD Dauble
- DD Potts
- DJ Bird
- DR Lowe
- DW McCauley
- E Ojutkangas
- EC Volk
- EK Moody
- EW Baxter
- FJ Rahel
- FWH Beamish
- FWH Beamish
- FWH Beamish
- FWH Beamish
- FWH Beamish
- FWH Beamish
- G Lassalle
- GA Bravener
- GC Becker
- GJ Farmer
- GJ Farmer
- GJA Hansen
- GL Christie
- GR Spangler
- GW Piavis
- H Bartels
- H Sugiyama
- HA Dawson
- HA Dawson
- HA Dawson
- HA Purvis
- HB Bigelow
- HH Moore
- HK Patrick
- IC Potter
- IC Potter
- IC Potter
- IJ Dolinsek
- J Freyhof
- J Holmes
- J Holmes
- J Mallatt
- J Waldman
- J Waldman
- Jeffrey W. Slade
- JF Kitchell
- JF Kitchell
- JG Weise
- JH Youson
- JH Youson
- JH Youson
- JH Youson
- JH Youson
- JJ Smith
- JM Oliveira
- JR Bence
- JR Kelso
- JRM Kelso
- JW Heinrich
- JW Hodges
- JW Slade
- K Kainua
- K Stier
- KM Mullett
- L Beaulaton
- LA Barker
- LA Barker
- LA Vrieze
- LA Vrieze
- LH Hanson
- LH Hanson
- LO Larsen
- M Gross
- MA Stapanian
- MB Bryan
- MB Trautman
- MF Fodale
- MG Mesa
- Michael J. Hansen
- MJ Genner
- MJ Hansen
- MJ Hansen
- MJ Lança
- MJ Siefkes
- ML Jones
- ML Jones
- ML Moser
- MP Henson
- MR Yap
- MS Sepúlveda
- MW Hardisty
- MW Hardisty
- MW Hardisty
- MW Hardisty
- MW Hardisty
- MW Hardisty
- MW Hardisty
- MW Hardisty
- MW Hardisty
- NA MacKay
- NO Andrade
- NS Johnson
- NS Johnson
- NS Johnson
- NS Johnson
- OT Gorman
- PA Cochran
- PA Cochran
- Pedro R. Almeida
- PJ Manion
- PJ Manion
- PJ Manion
- PJ Manion
- PR Almeida
- PR Almeida
- PR Almeida
- PR Almeida
- PW Smith
- PW Sorensen
- PW Webb
- R Bjerselius
- R Hogg
- R Rodriguez-Muñoz
- R Rodríguez-Muñoz
- R Rodríguez-Muñoz
- RA Bergstedt
- RA Bergstedt
- RA Bergstedt
- RE Thresher
- RE Thresher
- RG Halliday
- RH Morman
- RH Morman
- RJ Young
- RJ Young
- RL Eshenroder
- RL Eshenroder
- RM Davis
- RW Griffiths
- S Eddy
- S Silva
- S Silva
- SB Morkert
- SD Gerking
- SL Haeseker
- SP Murdoch
- SP Sitar
- TD Meckley
- TJ Cline
- TJ Cline
- TJ Morse
- TM Neeson
- TM Sutton
- Todd B. Steeves
- TR Binder
- VC Applegate
- VC Applegate
- VJT Ginneken van
- W Li
- W Li
- WD Swink
- WD Swink
- WD Swink
- WJ Christie
- WP Sullivan
- Publication venue
- Springer Nature
- Publication date
- 01/01/2016
- Field of study
The sea lamprey Petromyzon marinus (Linnaeus) is both an invasive non-native species in the Laurentian Great Lakes of North America and an imperiled species in much of its native range in North America and Europe. To compare and contrast how understanding of population ecology is useful for control programs in the Great Lakes and restoration programs in Europe, we review current understanding of the population ecology of the sea lamprey in its native and introduced range. Some attributes of sea lamprey population ecology are particularly useful for both control programs in the Great Lakes and restoration programs in the native range. First, traps within fish ladders are beneficial for removing sea lampreys in Great Lakes streams and passing sea lampreys in the native range. Second, attractants and repellants are suitable for luring sea lampreys into traps for control in the Great Lakes and guiding sea lamprey passage for conservation in the native range. Third, assessment methods used for targeting sea lamprey control in the Great Lakes are useful for targeting habitat protection in the native range. Last, assessment methods used to quantify numbers of all life stages of sea lampreys would be appropriate for measuring success of control in the Great Lakes and success of conservation in the native range
Charged-particle distributions at low transverse momentum in √s=13 13 TeV pp interactions measured with the ATLAS detector at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- AbouZeid OS
- Abraham NL
- 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
- Alberich LC
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alstaty M
- Alviggi MG
- Amadio BT
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- 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
- Antel C
- Antonelli M
- Antonov A
- 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
- Armitage LJ
- 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
- 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
- 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
- Barisits M-S
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HP
- Becker K
- Becker M
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr JK
- Belanger-Champagne C
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Bendtz K
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Beringer J
- Berlendis S
- Berlingen JM
- Bernard NR
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertram IA
- Bertsche C
- Bertsche D
- Besjes GJ
- Bessner M
- Besson N
- Betancourt C
- Bethke S
- Bevan AJ
- Bhimji W
- Bianchi RM
- Bianchini L
- Bianco M
- Biebel O
- Biedermann D
- Bielski R
- 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
- Boerner D
- Bogaerts JA
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
- Boudreau J
- Bouffard J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bracinik J
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Bravo AG
- Brendlinger K
- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Bristow TM
- Britton D
- Britzger D
- Brochu FM
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
- Brosamer J
- Brost E
- Broughton JH
- Bruncko D
- Bruneliere R
- Bruni A
- Bruni G
- Bruni LS
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Bugge MK
- Bulekov O
- Bullock D
- Burckhart H
- Burdin S
- Burgard CD
- Burghgrave B
- Burka K
- Burke S
- Burmeister I
- Burr JTP
- Busato E
- Buscher D
- Buscher V
- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Caforio D
- Cairo VM
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
- Calvet S
- Calvet TP
- Camarda S
- Camarri P
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canepa A
- Cantero J
- Cantrill R
- Cao T
- Caprini I
- Caprini M
- Capua M
- Caputo R
- Carbone RM
- Cardarelli R
- Cardillo F
- Carli I
- Carli T
- Carlino G
- Carminati L
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Casolino M
- Casper DW
- Castaneda-Miranda E
- Castelijn R
- Castelli A
- 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
- Ceradini F
- Cerio BC
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cerv M
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chatterjee A
- Chau CC
- Che S
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen K
- Chen S
- Chen S
- Chen X
- Chen Y
- Cheng HC
- Cheng HJ
- Cheng Y
- Cheplakov A
- Cheremushkina E
- Chernyatin V
- Cheu E
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chizhov MV
- Choi K
- Chomont AR
- Chouridou S
- Chow BKB
- Christodoulou V
- Chromek-Burckhart D
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
- Ciapetti G
- Ciftci AK
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- Cindro V
- Cioara IA
- Ciocca C
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubancan M
- Clark A
- Clark BL
- Clark MR
- Clark PJ
- Clarke RN
- Clement C
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- Coccaro A
- Cochran J
- Codina EP
- Coffey L
- Colasurdo L
- Cole B
- Colijn AP
- Collaboration ATLAS
- Collot J
- Colombo T
- Compostella G
- Coniavitis E
- Connell SH
- Connelly IA
- Consorti V
- Constantinescu S
- Conti G
- Conventi F
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- Cooper BD
- Cooper-Sarkar AM
- Cormier KJR
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cottin G
- Coutinho YA
- Cowan G
- Cox BE
- Cranmer K
- Crawley SJ
- Cree G
- Crepe-Renaudin S
- Crescioli F
- Cribbs WA
- Cristinziani M
- Croft V
- Crosetti G
- Cummings J
- Curatolo M
- Cuth J
- Cuthbert C
- Czirr H
- Czodrowski P
- D'amen G
- D'Auria S
- D'Onofrio M
- da Costa JBG
- Da Costa JGPF
- Da Via C
- Dabrowski W
- Dado T
- Dai T
- Dale O
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio DO
- Dandoy JR
- Dang NP
- Daniells AC
- Dann NS
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dassoulas J
- Dattagupta A
- Davey W
- David C
- Davidek T
- Davies M
- Davison P
- Dawe E
- Dawson I
- Daya-Ishmukhametova RK
- de Andrade Filho LM
- de Asmundis R
- De Benedetti A
- De Bruin PHS
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- de la Hoz SG
- De la Torre H
- de Lima DEF
- De Lorenzi F
- De Maria A
- De Mendizabal JB
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
- De Sousa MJDCS
- De K
- Dearnaley WJ
- Debbe R
- Debenedetti C
- Dedovich DV
- Dehghanian N
- Deigaard I
- Del Gaudio M
- Del Peso J
- Del Prete T
- Delgado AT
- Delgove D
- Deliot F
- Delitzsch CM
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Dell'Orso M
- Della Pietra M
- della Volpe D
- Delmastro M
- Delsart PA
- DeMarco DA
- Demers S
- Demichev M
- Demilly A
- Denis RDS
- Denisov SP
- Denysiuk D
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Dette K
- Devesa MR
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Ciaccio A
- Di Ciaccio L
- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipio R
- Di Valentino D
- Diaconu C
- Diamond M
- Dias FA
- Diaz MA
- Diehl EB
- Dietrich J
- Diglio S
- Dimitrievska A
- Dingfelder J
- Dita P
- Dita S
- Dittus F
- Djama F
- Djobava T
- Djuvsland JI
- do Vale MAB
- Dobos D
- Dobre M
- Doglioni C
- Dohmae T
- Dolejsi J
- Dolezal Z
- Dolgoshein BA
- Donadelli M
- Donati S
- Dondero P
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dos Santos SPA
- Dova MT
- Doyle AT
- Drechsler E
- Dris M
- Du Y
- Duarte-Campderros J
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Duffield EM
- Duflot L
- Duguid L
- Duhrssen M
- Dumancic M
- Dunford M
- Duren M
- Durglishvili A
- Duschinger D
- Dutta B
- Dyndal M
- Eckardt C
- Ecker KM
- Edgar RC
- Edwards NC
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Moursli RC
- Ellajosyula V
- Ellert M
- Elles S
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Enari Y
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- Zieminska D
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Measurements of distributions of charged particles produced in proton–proton collisions with a centre-of-mass energy of 13 TeV are presented. The data were recorded by the ATLAS detector at the LHC and correspond to an integrated luminosity of 151 μb −1 μb−1 . The particles are required to have a transverse momentum greater than 100 MeV and an absolute pseudorapidity less than 2.5. The charged-particle multiplicity, its dependence on transverse momentum and pseudorapidity and the dependence of the mean transverse momentum on multiplicity are measured in events containing at least two charged particles satisfying the above kinematic criteria. The results are corrected for detector effects and compared to the predictions from several Monte Carlo event generators
Measurement of W+W− production in association with one jet in proton–proton collisions at sqrt(s) = 8TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
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- Zemla A
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- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang R
- Zhang X
- Zhang Z
- Zhangb H
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- 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
- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2016
- Field of study
The production of W boson pairs in association with one jet in pp collisions at View the MathML sources=8 TeV is studied using data corresponding to an integrated luminosity of 20.3 fb−1 collected by the ATLAS detector during 2012 at the CERN Large Hadron Collider. The cross section is measured in a fiducial phase-space region defined by the presence of exactly one electron and one muon, missing transverse momentum and exactly one jet with a transverse momentum above 25 GeV and a pseudorapidity of |η|<4.5|η|<4.5. The leptons are required to have opposite electric charge and to pass transverse momentum and pseudorapidity requirements. The fiducial cross section is found to be View the MathML sourceσWWfid,1-jet=136±6(stat)±14(syst)±3(lumi) fb. In combination with a previous measurement restricted to leptonic final states with no associated jets, the fiducial cross section of WW production with zero or one jet is measured to be View the MathML sourceσWWfid,≤1-jet=511±9(stat)±26(syst)±10(lumi) fb. The ratio of fiducial cross sections in final states with one and zero jets is determined to be 0.36±0.050.36±0.05. Finally, a total cross section extrapolated from the fiducial measurement of WW production with zero or one associated jet is reported. The measurements are compared to theoretical predictions and found in good agreement
Search for pair production of Higgs bosons in the bb¯bb¯ final state using proton-proton collisions at √s=13 TeV with the ATLAS detector
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- Zhemchugov A
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- Zinser M
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- Zobernig G
- Zoccoli A
- Zu Theenhausen HM
- Zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2016
- Field of study
A search for Higgs-boson pair production in the bb ¯ bb ¯ final state is carried out with 3.2 fb −1 of proton-proton collision data collected at s √ =13 TeV with the ATLAS detector. The data are consistent with the estimated background and are used to set upper limits on the production cross section of Higgs-boson pairs times branching ratio to bb ¯ bb ¯ for both nonresonant and resonant production. In the case of resonant production of Kaluza-Klein gravitons within the Randall-Sundrum model, upper limits in the 24 to 91 fb range are obtained for masses between 600 and 3000 GeV, at the 95% confidence level. The production cross section times branching ratio for nonresonant Higgs-boson pairs is also constrained to be less than 1.22 pb, at the 95% confidence level
Measurement of Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
- Author
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- Catastini P
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- Chafaq A
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- Chalupkova I
- Chang P
- Chapleau B
- Chapman JD
- Charfeddine D
- Charlton DG
- Chau CC
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
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- Daniells AC
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- Dawson I
- Daya-Ishmukhametova RK
- de Andrade Filho LM
- de Asmundis R
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- Zhemchugov A
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- Zibell A
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- Zimmermann C
- Zimmermann R
- Zimmermann S
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- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 4.5 fb[superscript −1] of proton-proton collisions data at √s=7 TeV and 20.3 fb[superscript −1] at √s=8 TeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be μ=1.17±0.27 at the value of the Higgs boson mass measured by ATLAS, m[subscript H]=125.4 GeV. The analysis is optimized to measure the signal strengths for individual Higgs boson production processes at this value of m[subscript H]. They are found to be μ[subscript ggF]=1.32±0.38, μ[subscript VBF]=0.8±0.7, μ[subscript WH]=1.0±1.6, μ[subscript ZH]=0.1[superscript +3.7 subscript −0.1], and μ[subscript t [bar over t] H] =1.6[superscript +2.7 subscript −1.8], for Higgs boson production through gluon fusion, vector-boson fusion, and in association with a W or Z boson or a top-quark pair, respectively. Compared with the previously published ATLAS analysis, the results reported here also benefit from a new energy calibration procedure for photons and the subsequent reduction of the systematic uncertainty on the diphoton mass resolution. No significant deviations from the predictions of the Standard Model are found.European Organization for Nuclear ResearchUnited States. Dept. of EnergyNational Science Foundation (U.S.)Brookhaven National Laborator
Search for dark matter at √s=13 TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam ER
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty M
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders JK
- Andersb CF
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
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- Kobayashi A
- Kobayashi D
- Kobayashi T
- Kobel M
- Kocian M
- Kodys P
- Koehler NM
- Koeneke K
- Koffas T
- Koffeman E
- Kohler MK
- Koi T
- Kolb M
- Koletsou I
- Komar AA
- Komori Y
- Kondo T
- Kondrashova N
- Konig AC
- Kono T
- Konoplich R
- Konstantinidis N
- Kopeliansky R
- Koperny S
- Kopp AK
- Korcyl K
- Kordas K
- Korn A
- Korol AA
- Korolkov I
- Korolkova EV
- Kortner O
- Kortner S
- Kosek T
- Kostyukhin VV
- Kotwal A
- Koulouris A
- Kourkoumeli-Charalampidi A
- Kourkoumelis C
- Kourlitis E
- Kouskoura V
- Kowalewska AB
- Kowalewski R
- Kowalski TZ
- Kozakai C
- Kozanecki W
- Kozhin AS
- Kramarenko VA
- Kramberger G
- Krasnopevtsev D
- Krasny MW
- Krasznahorkay A
- Krauss D
- Kremer JA
- Kretzschmar J
- Kreutzfeldt K
- Krieger P
- Krizka K
- Kroeninger K
- Kroha H
- Kroll J
- Kroll J
- Kroseberg J
- Krstic J
- Kruchonak U
- Krueger H
- Krumnack N
- Kruse MC
- Kubota T
- Kucuk H
- Kuday S
- Kuechler JT
- Kuehn S
- Kugel A
- Kuger F
- Kuhl T
- Kukhtin V
- Kukla R
- Kulchitsky Y
- Kuleshov S
- Kulinich YP
- Kuna M
- Kunigo T
- Kupco A
- Kupfer T
- Kuprash O
- Kurashige H
- Kurchaninov LL
- Kurochkin YA
- Kurth MG
- Kus V
- Kuutmann EB
- Kuwertz ES
- Kuze M
- Kvita J
- Kwan T
- Kyriazopoulos D
- La Rosa Navarro JL
- La Rosa A
- La Rotonda L
- Lacasta C
- Lacava F
- Lacey J
- Lacker H
- Lacour D
- Ladygin E
- Lafaye R
- Laforge B
- Lagouri T
- Lai S
- Lammers S
- Lampl W
- Lancon E
- Landgraf U
- Landon MPJ
- Lanfermann MC
- Lang VS
- Lange JC
- Langenberg RJ
- Lankford AJ
- Lanni F
- Lantzsch K
- Lanza A
- Lapertosa A
- Laplace S
- Laporte JF
- Lari T
- Lassnig M
- Latour BMD
- Laurelli P
- Lavrijsen W
- Law AT
- Laycock P
- Lazovich T
- Lazzaroni M
- Le Dortz O
- Le Guirriec E
- Le Quilleuc EP
- Le B
- LeBlanc M
- LeCompte T
- Ledroit-Guillon F
- Lee CA
- Lee GR
- Lee L
- Lee SC
- Lefebvre B
- Lefebvre G
- Lefebvre M
- Legger F
- Leggett C
- Lehan A
- Lei X
- Leight WA
- Leite MAL
- Leitner R
- Lellouch D
- Lemmer B
- Leney KJC
- Lenz T
- Lenzi B
- Leone R
- Leone S
- Leonidopoulos C
- Lerner G
- Leroy C
- Lesage AAJ
- Lester CG
- Levchenko M
- Leveque J
- Levin D
- Levinson LJ
- Levy M
- Lewis D
- Li B
- Li C
- Li H
- Li L
- Li Q
- Li S
- Li X
- Li Y
- Liang Z
- Liberti B
- Liblong A
- Lie K
- Liebal J
- Liebig W
- Limosani A
- Lin SC
- Lin TH
- Lindquist BE
- Lionti AE
- Lipeles E
- Lipniacka A
- Lisovyi M
- Liss TM
- Lister A
- Litke AM
- Liu B
- Liu H
- Liu H
- Liu J
- Liu JB
- Liu JKK
- Liu K
- Liu L
- Liu M
- Liu Y
- Liu YL
- Livan M
- Llacer MM
- Lleres A
- Lloyd SL
- Lo Sterzo F
- Lo CY
- Lobodzinska EM
- Loch P
- Loebinger FK
- Loesel PJ
- Loesle A
- Loew KM
- Loginov A
- Lohse T
- Lohwasser K
- Lokajicek M
- Long BA
- Long JD
- Long RE
- Longo L
- Looper KA
- Lopez JA
- Lopez SP
- Lorenz J
- Losada M
- Lou X
- Lounis A
- Love J
- Love PA
- Lu H
- Lu N
- Lu YJ
- Lubatti HJ
- Luci C
- Lucotte A
- Luedtke C
- Luehring F
- Lukas W
- Luminari L
- Lund-Jensen B
- Lundberg O
- Luzi PM
- Lynn D
- Lysak R
- Lytken E
- Lyubushkin V
- Ma H
- Ma LL
- Ma Y
- Maccarrone G
- Macchiolo A
- Macdonald CM
- Macek B
- Machado Miguens J
- Madaffari D
- Madar R
- Madden WDB
- Mader WF
- Madsen A
- Maeda J
- Maeland S
- Maeno T
- Maettig P
- Maevskiy AS
- Magradze E
- Mahlstedt J
- Maiani C
- Maidantchik C
- Maier AA
- Maier T
- Maio A
- Majersky O
- Majewski S
- Makida Y
- Makovec N
- Malaescu B
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- Maleev VP
- Malek F
- Mallik U
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- Malyukov S
- Mamuzic J
- Mancini G
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- Mandic I
- Maneira J
- Manghi FL
- Manh TN
- Manhaes de Andrade Filho L
- Mann A
- Manousos A
- Mansoulie B
- Mansour JD
- Mantifel R
- Mantoani M
- Manzoni S
- Mapelli L
- Marceca G
- March L
- Marchese L
- Marchiori G
- Marcisovsky M
- Marjanovic M
- Marley DE
- Marroquim F
- Marsden SP
- Marshall Z
- Martensson MUF
- Marti-Garcia S
- Martin CB
- Martin TA
- Martin VJ
- Martin-Haugh S
- Martinez M
- Martinez NL
- Martoiu VS
- Martyniuk AC
- Marzin A
- Masetti L
- Mashimo T
- Mashinistov R
- Masik J
- Maslennikov AL
- Massa L
- Mastrandrea P
- Mastroberardino A
- Masubuchi T
- Mateos DL
- Maurer J
- Maxfield SJ
- Maximov DA
- Mazini R
- Maznas I
- Mazza SM
- Mc Fadden NC
- Mc Goldrick G
- Mc Kee SP
- McCarn A
- McCarthy RL
- McCarthy TG
- McClymont LI
- McDonald EF
- Mcfayden JA
- Mchedlidze G
- McMahon SJ
- McNamara PC
- McPherson RA
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- Megy TJ
- Mehlhase S
- Mehta A
- Meideck T
- Meier K
- Meirose B
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- Melo M
- Meloni F
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- Meng XT
- Mengarelli A
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- Mills C
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- Milov A
- Milstead DA
- Minaenko AA
- Minami Y
- Minashvili IA
- Mincer AI
- Mindura B
- Mineev M
- Minegishi Y
- Ming Y
- Miotto GL
- Mir LM
- Mistry KP
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- Mitrevski J
- Mitsou VA
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- Miyagawa PS
- Mizukami A
- Mjornmark JU
- Mkrtchyan T
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- Moa T
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- Moenig K
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- Morettinia P
- Morgenstern S
- Mori D
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- Morinaga M
- Morisbak V
- Morley AK
- Mornacchi G
- Morris JD
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- Mosidze M
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- Murray WJ
- Musheghyan H
- Muskinja M
- Myagkov AG
- Myska M
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- Nagata K
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- Nakano I
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- Naryshkin I
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- Nechaeva PY
- Neep TJ
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- Noguchi Y
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- Nomura MA
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- Novgorodova O
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- Nurse E
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- Okawa H
- Okumura Y
- Okuyama T
- Olariu A
- Oleiro Seabra LF
- Olszewski A
- Olszowska J
- Onofre A
- Onogi K
- Onyisi PUE
- Oreglia MJ
- Oren Y
- Orestano D
- Orlando N
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- Ortiz NGG
- Osculati B
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- Otono H
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- Papadopoulou TD
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- Pasqualucci E
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- Pastor ET
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- Perepelitsa DV
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- Pino SAO
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- Poley A
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- Polychronakos V
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- Ponomarenko D
- Pontecorvo L
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- Zu Theenhausena HM
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
Results of a search for physics beyond the Standard Model in events containing an energetic photon and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider are reported. As the number of events observed in data, corresponding to an integrated luminosity of 36.1 fb−1 of proton–proton collisions at a centre-of-mass energy of 13 TeV, is in agreement with the Standard Model expectations, model-independent limits are set on the fiducial cross section for the production of events in this final state. Exclusion limits are also placed in models where dark-matter candidates are pair-produced. For dark-matter production via an axial-vector or a vector mediator in the s-channel, this search excludes mediator masses below 750–1200 GeV for dark-matter candidate masses below 230–480 GeV at 95% confidence level, depending on the couplings. In an effective theory of dark-matter production, the limits restrict the value of the suppression scale M∗ to be above 790 GeV at 95% confidence level. A limit is also reported on the production of a high-mass scalar resonance by processes beyond the Standard Model, in which the resonance decays to Zγ and the Z boson subsequently decays into neutrinos
Search for the b(b)over-bar decay of the Standard Model Higgs boson in associated (W/Z)H production with the ATLAS detector
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
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