737 research outputs found
Inflation osteoplasty: in vitro evaluation of a new technique for reducing depressed intra-articular fractures of the tibial plateau and distal radius
- Author
- Publication venue
- Springer Milan
- Publication date
- 01/01/2012
- Field of study
Ferromagnetic Semiconductors: Moving Beyond (Ga,Mn)As
- Author
- A Mauger
- A van Esch
- A. H. MacDonald
- AB Shick
- AM Nazmul
- B Beschoten
- C Ruster
- C Timm
- C Zener
- D Chiba
- DJ Priour Jr
- DP Norton
- E Johnston-Halperin
- E Johnston-Halperin
- E Kulatov
- EJ Singley
- F Matsukura
- G Alvarez
- G Bouzerar
- GA Fiete
- GT Thaler
- H Munekata
- H Ohno
- H Ohno
- H Ohno
- H Ohno
- H Saito
- H Shimizu
- HX Tang
- I Zutic
- I Žutić
- J Konig
- J Okabayashi
- J Schiemann
- J Schliemann
- J Schliemann
- JG Braden
- JMD Coey
- KC Ku
- KF Eid
- KM Yu
- KW Edmonds
- KW Edmonds
- L Bergqvist
- L Kronik
- LM Sandratskii
- M Berciu
- M Sawicki
- M Tanaka
- M van Schilfgaarde
- MB Stone
- ME Flatte
- ME Flatte
- MJ Calderon
- N Samarth
- N Theodoropoulou
- N. Samarth
- NA Theodoropoulo
- P Mahadevan
- P Mahadevan
- P Sharma
- P. Schiffer
- R Giraud
- R Mattana
- RC Myers
- RK Kawakami
- S Das Sarma
- S Dhar
- S Sanvito
- S-R Yang
- SA Chambers
- SA Chambers
- SA Wolf
- SB Ogale
- SC Erwin
- SE Park
- SH Chun
- SJ Pearton
- SJ Potashnik
- SJ Potashnik
- SR Shinde
- T Dietl
- T Dietl
- T Dietl
- T Hayashi
- T Jungwirth
- T Jungwirth
- T Sasaki
- T Story
- X Chen
- X Liu
- Y Matsumoto
- Y Nagai
- Y Ohno
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 08/03/2005
- Field of study
The recent development of MBE techniques for growth of III-V ferromagnetic
semiconductors has created materials with exceptional promise in spintronics,
i.e. electronics that exploit carrier spin polarization. Among the most
carefully studied of these materials is (Ga,Mn)As, in which meticulous
optimization of growth techniques has led to reproducible materials properties
and ferromagnetic transition temperatures well above 150 K. We review progress
in the understanding of this particular material and efforts to address
ferromagnetic semiconductors as a class. We then discuss proposals for how
these materials might find applications in spintronics. Finally, we propose
criteria that can be used to judge the potential utility of newly discovered
ferromagnetic semiconductors, and we suggest guidelines that may be helpful in
shaping the search for the ideal material.Comment: 37 pages, 4 figure
IFITM3 Inhibits Influenza A Virus Infection by Preventing Cytosolic Entry
- Author
- A Ablasser
- A Karlas
- A Pichlmair
- A Ropolo
- Abraham L. Brass
- AL Brass
- AR Lewin
- Bethany J. Ryan
- BK Saha
- CB Bridges
- CE Mire
- Christopher R. Chin
- CS Shi
- D Jiang
- DC Lawe
- DM Tscherne
- DM Weinstock
- DP Calfee
- DP Ritzwoller
- E Bernard
- Eric M. Feeley
- F Siegrist
- Gaurav D. Gaiha
- GB Melikyan
- HM van der Schaar
- I Le Blanc
- IC Huang
- J Dittmann
- J Lu
- J Mercer
- Jennifer S. Sims
- JF Cros
- JL Umbach
- JM Rojek
- JM Weidner
- JS Yount
- K Martin
- L Meertens
- LE Bradbury
- Li-Mei Chen
- M Bui
- M Lakadamyali
- M Tobiume
- MG Gutierrez
- Michael S. Diamond
- N Hanagata
- O Haller
- P Moffatt
- P Uchil
- P Zimmermann
- R Brem
- R Khor
- R Konig
- R Konig
- RA Lamb
- RA Smith
- RL Friedman
- Ruben O. Donis
- S Pankiv
- SB Sieczkarski
- SD Shapira
- SG Lazarowitz
- Sinu P. John
- SS Evans
- Stephen J. Elledge
- T Pertel
- T Ronni
- Thomas Pertel
- UC Lange
- UC Lange
- W Garten
- XF Wan
- Publication venue
- Public Library of Science
- Publication date
- 01/10/2011
- Field of study
To replicate, viruses must gain access to the host cell's resources. Interferon (IFN) regulates the actions of a large complement of interferon effector genes (IEGs) that prevent viral replication. The interferon inducible transmembrane protein family members, IFITM1, 2 and 3, are IEGs required for inhibition of influenza A virus, dengue virus, and West Nile virus replication in vitro. Here we report that IFN prevents emergence of viral genomes from the endosomal pathway, and that IFITM3 is both necessary and sufficient for this function. Notably, viral pseudoparticles were inhibited from transferring their contents into the host cell cytosol by IFN, and IFITM3 was required and sufficient for this action. We further demonstrate that IFN expands Rab7 and LAMP1-containing structures, and that IFITM3 overexpression is sufficient for this phenotype. Moreover, IFITM3 partially resides in late endosomal and lysosomal structures, placing it in the path of invading viruses. Collectively our data are consistent with the prediction that viruses that fuse in the late endosomes or lysosomes are vulnerable to IFITM3's actions, while viruses that enter at the cell surface or in the early endosomes may avoid inhibition. Multiple viruses enter host cells through the late endocytic pathway, and many of these invaders are attenuated by IFN. Therefore these findings are likely to have significance for the intrinsic immune system's neutralization of a diverse array of threats
Search for Charged Higgs Bosons in e+e- Collisions at \sqrt{s} = 189 GeV
- Author
- Acciarri M
- Achard P
- Adriani O
- Aguilar-Benitez M
- Alcaraz J
- Alemanni G
- Allaby J
- Aloisio A
- Alviggi MG
- Ambrosi G
- Anderhub H
- Andreev VP
- Angelescu T
- Anselmo F
- Arefiev A
- Azemoon T
- Aziz T
- Bagnaia P
- Baksay L
- Balandras A
- Ball RC
- Banerjee S
- Banerjee S
- Barczyk A
- Barillere R
- Barone L
- Bartalini P
- Basile M
- Battiston R
- Bay A
- Becattini F
- Becker U
- Behner F
- Bellucci L
- Berdugo J
- Berges P
- Bertucci B
- Betev BL
- Bhattacharya S
- Biasini M
- Biland A
- Blaising JJ
- Blyth SC
- Bobbink GJ
- Bohm A
- Boldizsar L
- Borgia B
- Bourilkov D
- Bourquin M
- Bourquin M
- Braccini S
- Braccini S
- Branson JG
- Branson JG
- Brigljevic V
- Brigljevic V
- Brochu F
- Brochu F
- Buffini A
- Buijs A
- Burger JD
- Burger WJ
- Busenitz J
- Button A
- Cai XD
- Campanelli M
- Capell M
- Carlino G
- Cartacci AM
- Casaus J
- Castellini G
- Cavallari F
- Cavallo N
- Cecchi C
- Cerrada M
- Cesaroni F
- Chamizo M
- Chang YH
- Chaturvedi UK
- Chemarin M
- Chen A
- Chen G
- Chen GM
- Chen HF
- Chen HS
- Chereau X
- Chiefari G
- Cifarelli L
- Cindolo F
- Civinini C
- Clare I
- Clare R
- Coignet G
- Colijn AP
- Colino N
- Costantini S
- Cotorobai F
- Cozzoni B
- Csilling A
- Cucciarelli S
- D'Alessandro R
- Dai TS
- de Asmundis R
- de Guevara PL
- de Jong P
- de la Cruz B
- De Notaristefani F
- De Salvo A
- Deglon P
- Degre A
- Deiters K
- della Volpe D
- Denes P
- Di Lodovico F
- Diemoz M
- Dionisi C
- Dittmar M
- Dominguez A
- Doria A
- Dova MT
- Duchesneau D
- Dufournaud D
- Duinker P
- Duran I
- El Mamouni H
- Engler A
- Eppling FJ
- Erne FC
- Extermann P
- Fabre M
- Faccini R
- Falagan MA
- Falciano S
- Favara A
- Fay J
- Fedin O
- Felcini M
- Ferguson T
- Ferroni F
- Fesefeldt H
- Fiandrini E
- Field JH
- Filthaut F
- Fisher PH
- Fisk I
- Forconi G
- Fredj L
- Freudenreich K
- Furetta C
- Galaktionov Y
- Ganguli SN
- Garcia-Abia P
- Gataullin M
- Gau SS
- Gentile S
- Gheordanescu N
- Giagu S
- Gong ZF
- Grenier G
- Grimm O
- Gruenewald MW
- Guida M
- Gupta VK
- Gurtu A
- Gutay LJ
- Haas D
- Hasan A
- Hatzifotiadou D
- Hebbeker T
- Herve A
- Hidas P
- Hirschfelder J
- Hofer H
- Holzner G
- Hoorani H
- Hou SR
- Iashvili I
- Jin BN
- Jones LW
- Josa-Mutuberria I
- Kamrad D
- Kaur M
- Khan RA
- Kienzle-Focacci MN
- Kim D
- Kim DH
- Kim JK
- Kim SC
- Kirkby J
- Kiss D
- Kittel W
- Klimentov A
- Konig AC
- Kopp A
- Korolko I
- Koutsenko V
- Kraber M
- Kraemer RW
- Krenz W
- Kunin A
- Laktineh I
- Landi G
- Lassila-Perini K
- Laurikainen P
- Lavorato A
- Le Coultre P
- Le Goff JM
- Lebeau M
- Lebedev A
- Lebrun P
- Lecomte P
- Lecoq P
- Lee HJ
- Leiste R
- Leonardi E
- Levtchenko P
- Li C
- Lin CH
- Lin WT
- Linde FL
- Lista L
- Liu ZA
- Lohmann W
- Longo E
- Lu YS
- Lubelsmeyer K
- Luci C
- Luckey D
- Lugnier L
- Luminari L
- Lustermann W
- Ma WG
- Maity M
- Malgeri L
- Malinin A
- Mana C
- Mangeol D
- Marchesini P
- Marian G
- Martin JP
- Marzano F
- Massaro GGG
- Mazumdar K
- McNeil RR
- Mele S
- Merola L
- Meschini M
- Metzger WJ
- Mihul A
- Milcent H
- Mirabelli G
- Mnich J
- Mohanty GB
- Molnar P
- Monteleoni B
- Moulik T
- Muanza GS
- Muheim F
- Muijs AJM
- Musy M
- Napolitano M
- Nessi-Tedaldi F
- Newman H
- Niessen T
- Nisati A
- Nowak H
- Oh YD
- Organtini G
- Ostonen R
- Palomares C
- Pandoulas D
- Paoletti S
- Paolucci P
- Paramatti R
- Park HK
- Park IH
- Pascale G
- Passaleva G
- Patricelli S
- Paul T
- Pauluzzi M
- Paus C
- Pauss F
- Peach D
- Pedace M
- Pensotti S
- Perret-Gallix D
- Petersen B
- Piccolo D
- Pierella F
- Pieri M
- Piroue PA
- Pistolesi E
- Plyaskin V
- Pohl M
- Pojidaev V
- Postema H
- Pothier J
- Produit N
- Prokofiev D
- Prokofiev DO
- Quartieri J
- Rahal-Callot G
- Rahaman MA
- Raics P
- Raja N
- Ramelli R
- Rancoita PG
- Raven G
- Razis P
- Ren D
- Rescigno M
- Reucroft S
- Riemann S
- Riles K
- Robohm A
- Rodin J
- Roe BP
- Romeo GC
- Romero L
- Rosca A
- Rosier-Lees S
- Rubio JA
- Ruschmeier D
- Rykaczewski H
- Salicio J
- Sanchez E
- Sanders MP
- Sarakinos ME
- Sarkar S
- Schafer C
- Schegelsky V
- Schmidt-Kaerst S
- Schmitz D
- Schopper H
- Schotanus DJ
- Schwering G
- Sciacca C
- Scianrino D
- Seganti A
- Servoli L
- Shevchenko S
- Shivarov N
- Shoutko V
- Shumilov E
- Shvorob A
- Siedenburg T
- Smith B
- Son D
- Spillantini P
- Steuer M
- Stickland DP
- Stone A
- Stone H
- Stoyanov B
- Straessner A
- Sudhakar K
- Sultanov G
- Sun LZ
- Suter H
- Swain JD
- Szillasi Z
- Sztaricskai T
- Tang XW
- Tauscher L
- Taylor L
- Timmermans C
- Ting SCC
- Ting SM
- Tonwar SC
- Toth J
- Tully C
- Tung KL
- Uchida Y
- Ulbricht J
- Valente E
- van Dalen JA
- van Dierendonck D
- van Gulik R
- van Rhee T
- Vesztergombi G
- Vetlitsky I
- Vicinanza D
- Viertel G
- Villa S
- Vivargent M
- Vlachos S
- Vodopianov I
- Vogel H
- Vogt H
- von der Mey M
- Vorobiev I
- Vorobyov AA
- Vorvolakos A
- Wadhwa M
- Wallraff W
- Wang M
- Wang XL
- Wang ZM
- Weber A
- Weber M
- Wienemann P
- Wilkens H
- Wu SX
- Wynhoff S
- Xia L
- Xu ZZ
- Yang BZ
- Yang CG
- Yang HJ
- Yang M
- Ye JB
- Yeh SC
- Zalite A
- Zalite Y
- Zhang ZP
- Zhu GY
- Zhu RY
- Zichichi A
- Ziegler F
- Zilizi G
- Zoller M
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/1999
- Field of study
A search for pair-produced charged Higgs bosons is performed with the L3
detector at LEP using data collected at a centre-of-mass energy of 188.6 GeV,
corresponding to an integrated luminosity of 176.4 pb^-1. Higgs decays into a
charm and a strange quark or into a tau lepton and its associated neutrino are
considered. The observed events are consistent with the expectations from
Standard Model background processes. A lower limit of 65.5 GeV on the charged
Higgs mass is derived at 95 % confidence level, independent of the decay
branching ratio Br(H^{+/-} -> tau nu)
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
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barsov S
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertram IA
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bhattacharya DS
- Bhattarai P
- Bi R
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz N
- Biglietti M
- Billoud TR
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker E
- Boumediene D
- Bourdarios CA
- Boutle SK
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Broughton JH
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher V
- Bugge MK
- Bulekov O
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
- Camelia EA
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cantero J
- Cao T
- Cao Y
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carter JWS
- Casado MP
- Casha AF
- Casper DW
- Castelijn R
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavallaro E
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Cerda Alberich L
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chau CC
- Che S
- Chekanov S
- Chekulaev S
- Chelkov GA
- Chen B
- Chen C
- Chen CH
- Chen H
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov M
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Chytka L
- Cieri D
- Ciesla KM
- Cinca D
- Cindro V
- Cioara IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark MR
- Clark PJ
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
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- Zhemchugov A
- Zheng Z
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- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
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- 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
Search for the standard model Higgs boson at LEP
- Author
- Abbaneo D
- Abbaneo D
- Abbiendi G
- Abbiendi G
- Abdallah J
- Abreu P
- Achard P
- Adam W
- Adriani O
- Adzic P
- Affholderbach K
- Aguilar-Benitez M
- Ainsley C
- Akesson PF
- Albrecht T
- Alcaraz J
- Alderweireld T
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- Wermes N
- Werner S
- Wetterling D
- White R
- Wicke D
- Wickens J
- Wiedenmann W
- Wienemann P
- Wilkens H
- Wilkinson G
- Wilson GW
- Wilson JA
- Winter M
- Witek M
- Wolf G
- Wolf G
- Wu J
- Wu SL
- Wu SX
- Wu X
- Wunsch M
- Wyatt TR
- Wynhoff S
- Xia L
- Xie Y
- Xu R
- Xu ZZ
- Xue S
- Yamamoto J
- Yamashita S
- Yang BZ
- Yang CG
- Yang HJ
- Yang M
- Yeh SC
- Yuan C
- Yushchenko O
- Zachariadou K
- Zalewska A
- Zalewski P
- Zalite A
- Zalite Y
- Zavrtanik D
- Zeitnitz C
- Zer-Zion D
- Zhang J
- Zhang L
- Zhang ZP
- Zhao J
- Zhao W
- Zhu GY
- Zhu RY
- Zhuang HL
- Zhuravlov V
- Zichichi A
- Ziegler T
- Zilizi G
- Zimin NI
- Zimmermann B
- Zintchenko A
- Zito G
- Zivkovic L
- Zobernig G
- Zoller M
- Zupan M
- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 17/07/2003
- Field of study
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Khalek SA
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MS
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Gonzalez BA
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aoun S
- Bella LA
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Arfaoui S
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
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- Asman B
- Asquith L
- Assamagan K
- Astbury A
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- Aubert B
- Auge E
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- Avramidou R
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- Mayes JB
- Badescu E
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- Bailey DC
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- Caminal Armadans R
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- Castillo Gimenez V
- Castro NF
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- Caughron S
- Cavaliere V
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- Cavasinni V
- Ceradini F
- Cerqueira AS
- Cerri A
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- Cetin SA
- Chafaq A
- Chakraborty D
- Chalupkova I
- Chan K
- Chang P
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
- Barajas CAC
- Cheatham S
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- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
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- Chen X
- Chen Y
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- Cheplakov A
- El Moursli RC
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
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- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chisholm AS
- Chislett RT
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- Choudalakis G
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- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
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- Ciocca C
- Ciocio A
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- Citron ZH
- Citterio M
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- Cummings J
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- Czodrowski P
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- D'Orazio A
- Da Cunha Sargedas De Sousa MJ
- Da Via C
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- Dafinca A
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- de Asmundis R
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- De Cecco S
- de Graat J
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- de Jong P
- De la Taille C
- De la Torre H
- De Lorenzi F
- de Mora L
- De Nooij L
- De Pedis D
- De Salvo A
- De Sanctis U
- De Santo A
- De Regie JBDV
- De Zorzi G
- Dearnaley WJ
- Debbe R
- Debenedetti C
- Dechenaux B
- Dedovich DV
- Degenhardt J
- Del Peso J
- Del Prete T
- Delemontex T
- Deliyergiyev M
- Dell'Acqua A
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- Della Pietra M
- della Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
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- Deviveiros PO
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- DeWilde B
- Dhaliwal S
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- Di Ciaccio A
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- della Porta GZ
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- Zhemchugov A
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- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fb−1 of s=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan β < 40
X-ray emission from the Sombrero galaxy: discrete sources
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Zotto P
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
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- Abi B
- Abolins M
- Abramowicz H
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- Acharya BS
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- Aguilar-Saavedra JA
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- Zieminska D
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- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
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- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Almond J
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Araque JP
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Aurousseau M
- Avolio G
- Azuelos G
- Azuma Y
- Baak MA
- Baas A
- Bacci C
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bain T
- Baines JT
- Baker OK
- Balek P
- Balli F
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- Banerjee S
- Bannoura AAE
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barberio EL
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- Barnett BM
- Barnett RM
- Barnovska Z
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- Barton AE
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
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