347 research outputs found
Polymer nanofilms with enhanced microporosity by interfacial polymerization
- Author
- AJ Brown
- Andrew G. Livingston
- AP Côté
- BD Freeman
- BS Ghanem
- CM Stafford
- D Fritsch
- DL Gin
- H Li
- H Qian
- H Sun
- HB Park
- HM El-Kaderi
- HW Kim
- I Ichinose
- J Weber
- JTA Jones
- JY Chung
- KE Hart
- Kim E. Jelfs
- L Abbott
- L Abbott
- L Dobrzańska
- LJ Abbott
- LJ Abbott
- LM Robeson
- M Carta
- M Carta
- M Pinheiro
- Maria F. Jimenez-Solomon
- Marta Munoz-Ibanez
- MD Guiver
- MF Jimenez Solomon
- MJ Frisch
- N Du
- N Du
- NB McKeown
- NB McKeown
- NB McKeown
- OM Yaghi
- P Gorgojo
- P Marchetti
- PM Budd
- PM Budd
- Q Song
- Q Song
- Q Song
- Q Song
- Qilei Song
- R Ameloot
- RR Nair
- S Karan
- S Karan
- S Karan
- S Kitagawa
- S Plimpton
- S Tsarkov
- T Rodenas
- T Tozawa
- TF Willems
- TM Murphy
- Y Peng
- YH See Toh
- YH See Toh
- YS Li
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 05/04/2016
- Field of study
Highly permeable and selective membranes are desirable for energy-efficient gas and liquid separations. Microporous organic polymers have attracted significant attention in this respect owing to their high porosity, permeability, and molecular selectivity. However, it remains challenging to fabricate selective polymer membranes with controlled microporosity which are stable in solvents. Here we report a new approach to designing crosslinked, rigid polymer nanofilms with enhanced microporosity by manipulating the molecular structure. Ultra-thin polyarylate nanofilms with thickness down to 20 nm were formed in-situ by interfacial polymerisation. Enhanced microporosity and higher interconnectivity of intermolecular network voids, as rationalised by molecular simulations, are achieved by utilising contorted monomers for the interfacial polymerisation. Composite membranes comprising polyarylate nanofilms with enhanced microporosity fabricated in-situ on crosslinked polyimide ultrafiltration membranes show outstanding separation performance in organic solvents, with up to two orders of magnitude higher solvent permeance than membranes fabricated with nanofilms made from noncontorted planar monomers
Ultrathin graphene-based membrane with precise molecular sieving and ultrafast solvent permeation
- Author
- A Akbari
- A. K. Geim
- A. N. Grigorenko
- A. Pratt
- B Radha
- C. Chi
- C. T. Cherian
- E Secchi
- F. C. Wang
- F. Guinea
- G Liu
- H Dai
- H Li
- H Wu
- J Abraham
- J Mulder
- J. C. Zhang
- K Celebi
- K Huang
- K. Huang
- KP Loh
- L Huang
- L Huang
- L Wang
- M Fathizadeh
- MF Jimenez-Solomon
- NFD Aba
- NR Wilson
- P Marchetti
- P Sun
- P Vandezande
- Q. Yang
- R. R. Nair
- RK Joshi
- RR Nair
- S Hong
- S Karan
- T Jain
- V. G. Kravets
- WJ Koros
- X Lin
- Y Han
- Y. Su
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
Graphene oxide (GO) membranes continue to attract intense interest due to their unique molecular sieving properties combined with fast permeation. However, their use is limited to aqueous solutions because GO membranes appear impermeable to organic solvents, a phenomenon not yet fully understood. Here, we report efficient and fast filtration of organic solutions through GO laminates containing smooth two-dimensional (2D) capillaries made from large (10-20 μm) flakes. Without modification of sieving characteristics, these membranes can be made exceptionally thin, down to â 1/410 nm, which translates into fast water and organic solvent permeation. We attribute organic solvent permeation and sieving properties to randomly distributed pinholes interconnected by short graphene channels with a width of 1 nm. With increasing membrane thickness, organic solvent permeation rates decay exponentially but water continues to permeate quickly, in agreement with previous reports. The potential of ultrathin GO laminates for organic solvent nanofiltration is demonstrated by showing >99.9% rejection of small molecular weight organic dyes dissolved in methanol. Our work significantly expands possibilities for the use of GO membranes in purification and filtration technologies
Sequence-defined multifunctional polyethers via liquid-phase synthesis with molecular sieving
- Author
- A Khanal
- AC French
- Andrew G. Livingston
- B Lewandowski
- Christopher M. Williams
- D Oh
- E Bayer
- F Amir
- F Svec
- G Székely
- H Zhang
- J Dunleavy
- J Niu
- J Silva Burgal da
- JC Barnes
- JF Kim
- JF Lutz
- JF Lutz
- K Knop
- K Maranski
- K Nakatani
- K Takizawa
- K Takizawa
- M Porel
- M Porel
- M Zamfir
- Marc Schaepertoens
- MF Jimenez-Solomon
- NC Seeman
- NF König
- NG Engelis
- OJ Plante
- P Marchetti
- Patrizia Marchetti
- Piers R. J. Gaffney
- R McHale
- R Szweda
- RB Merrifield
- RK Roy
- Rongjun Chen
- Ruijiao Dong
- Ruiyi Liu
- S Karan
- S Okaya
- S Pfeifer
- S Pfeifer
- S Srichan
- SA Weissman
- SC Solleder
- SC Solleder
- SC Solleder
- T Bootwicha
- WJ Koros
- Y Hibi
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 10/10/2018
- Field of study
Synthetic chemists have devoted tremendous effort towards the production of precision synthetic polymers with defined sequences and specific functions. However, the creation of a general technology that enables precise control over monomer sequence, with efficient isolation of the target polymers, is highly challenging. Here, we report a robust strategy for the production of sequence-defined synthetic polymers through a combination of liquid-phase synthesis and selective molecular sieving. The polymer is assembled in solution with real-time monitoring to ensure couplings proceed to completion, on a three-armed star-shaped macromolecule to maximize efficiency during the molecular sieving process. This approach is applied to the construction of sequence-defined polyethers, with side-arms at precisely defined locations that can undergo site-selective modification after polymerization. Using this versatile strategy, we have introduced structural and functional diversity into sequence-defined polyethers, unlocking their potential for real-life applications in nanotechnology, healthcare and information storage
Development and evaluation of reverse transcription-loop-mediated isothermal amplification assay for rapid detection of enterovirus 71
- Author
- A Frydenberg
- AK Reddy
- E Ma
- EL Tan
- F Zhou
- GJ Van Doornum
- GS Fout
- H Komatsu
- I Schuffenecker
- J Langlet
- J Sun
- JL Davia
- K Mizuta
- KK Tee
- KP Chan
- Kun Li
- LX Mao
- LY Miao
- M Hagiwara
- M Imai
- MA Jimenez-Clavero
- Mei Shi
- MF Lee
- MM Parida
- N Hosaka
- NJ Schmidt
- Qingbo Jiang
- S Fukuda
- S Fukuta
- S Morishita
- SW Huang
- T Jiang
- T Kasahara
- T Notomi
- T Solomon
- TC Chen
- VA Shah
- WA Nix
- Weifeng Shi
- XL Xiao
- Y Wu
- Y Zhang
- Yun Ji
- Z Zhu
- Zuhuang Mi
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Canagliflozin and Renal Outcomes in Type 2 Diabetes and Nephropathy
- Author
- Abdallah J
- Abdul Ghani R
- Abdul Kadir K
- Abdullah R
- Abejuela Z
- Abouglila K
- Abraham O
- Abrahamsen I
- Abraira Munoz Ld
- Abramowitz M
- Abusnana S
- Accini Mendoza Jl
- Acosta I
- Agafyina A
- Agarwal R
- Agarwal Rajiv
- Aggarwal N
- Agra J
- Ahmed F
- Ahuad Guerrero Ra
- Aiello J
- Ainsworth P
- Aizenberg D
- Akiyama H
- Akright L
- Akyea-Djamson A
- Al-Karadsheh A
- Alamartine E
- Alappan R
- Albisu Jp
- Ali N
- Ali Z
- Alicic R
- Allison Dc
- Alvarez Garcia P
- Alvarisqueta A
- Alves da Costa Fa
- Amerena J
- Amigo A
- Amodeo C
- Andreeva V
- Andreotti Turatti La
- Angelescu Lm
- Angelova A
- Anghel V
- Antic S
- Aoki H
- Aquitania G
- Arauz-Pacheco C
- Arcos E
- Arfeen S
- Arif A
- Aronson R
- Arutchelvam V
- Arvind M
- Asano A
- Asmarats Mercadal L
- Atray N
- August P
- Avendano J
- Avram Ri
- Awad A
- Babikova J
- Badat A
- Bajaj H
- Baker J
- Bakris G
- Bakris George
- Barbarash O
- Barna O
- Barnard M
- Barnhill P
- Barranco E
- Barrera C
- Barrios C
- Bartaskova D
- Bartolacci I
- Barton P
- Barysheva O
- Beacom M
- Behara V
- Bellary S
- Belo D
- Belobradkova J
- Bentley-Lewis R
- Benusova O
- Berenguer R
- Berli Ma
- Bermudez L
- Bernardo M
- Bhushan Rs
- Bijata-Bronisz R
- Bilyk Sd
- Bin Shudim Ss
- Biscoveanu M
- Bompoint Severine
- Bonadonna R
- Bordonava A
- Borot S
- Botsyurko V
- Bowman-Stroud C
- Brandon D
- Breedt J
- Bregman R
- Brenner Barry M
- Brenner Bm
- Brusco O
- Buganova I
- Bull Scott
- Burst V
- Busch R
- Busegeanu Mm
- Calella P
- Camelo Sanches Fc
- Canaan Y
- Canani Lh
- Cannon Christopher P
- Cannon Cp
- Cantero Mc
- Capuano George
- Caringal C
- Cariou B
- Cartasegna Lr
- Castellino P
- Cercos E
- Cereto Castro F
- Ceriello A
- Chacra Ar
- Chae Dw
- Chang Ct
- Chang T
- Chapin L
- Charytan David M
- Charytan Dm
- Che Yusof Md
- Cheifetz A
- Chen E
- Chen N
- Chen Q
- Cherney D 3rd
- Chertow G
- Cheung Nw
- Chilito A
- Chiovato L
- Chizhov D
- Cho Ym
- Chouinard G
- Christensen T
- Christiano C
- Christofides E
- Chu Pei-Ling
- Chuang Lm
- Chuateco C
- Cif A
- Cigarran Guldris S
- Coffee L
- Cohen K
- Cohen R
- Cohen S
- Cohen-Stein D
- Coloma Gc
- Colombo H
- Comia Rs
- Commendatore V
- Conway J
- Cook C
- Correa Rotter Jr
- Cosma D
- Cournoyer S
- Coyne D
- Crisan C
- Cruz Jb
- Csecsei G
- Csiky B
- Cuadrado J
- Culak J
- Cuneo Ca
- Cunha Borges Jl
- Cunha V\ueancio Sa
- Cusumano Am
- D'Avila D
- da Silva Franco Rj
- Daboul N
- Danos P
- Daroza G
- Darwish R
- Daswani A
- David C
- Davies E
- Davies M
- Davies S
- Dawson A
- De Brouwer K
- de Carvalho Contieri Fl
- De Cosmo S
- De Nicola L
- De Serres S
- de Souza Portes E
- de Souza P
- de Zeeuw D
- de Zeeuw Dick
- Deak L
- Deboni Lm
- Deck K
- Deepak D
- Delos Santos L
- Demian Ld
- Derosa G
- Desouza C
- Destree M
- Dev D
- Dhillon M
- Di Carlo A
- Di Cianni G
- Diaz Escalante T
- Diaz Ruiz Jea
- Dimitrov S
- Distiller L
- Distiller L
- Djordjevic M
- Dobronravov V
- Dohnalova L
- Dominquez Lopez M
- Douthat Wg
- Dran Rd
- Drasnar T
- Dreval A
- Droste C
- Dua S
- Dub\ue9 F
- Dudar I
- Dudas M
- Dussol B
- Dzupina A
- Dzuponova J
- Eder F
- Edwards Robert
- Edwin Fm
- Egido de Los Rios J
- El Kossi M
- El-Shahawy M
- Elosegui Am
- English P
- Enriquez Sosa Fe
- Ervin J
- Esquenazi A
- Evans J
- Faghih M
- Farias E
- Faulmann G
- Fauvel Jp
- Ferariu Ie
- Ferkl R
- Fern\ue1ndez Montenegro Ma
- Fernandez Fresnedo G
- Fernandez Mf
- Feuerstein J
- Filho Ff
- Finkelstein H
- Fishbane S
- Flores Lozano F
- Flota Cervera Lf
- Fragale G
- Frasc\ue0 G
- Fraser D
- Fraser I
- Frenk Baron P
- Fretes Jo
- Frias J
- Fuiano G
- Fulcher G
- Fulop P
- Fushtey I
- G\uf3rriz Jl
- Gaglia J
- Galan Serrano A
- Galindo-Ramos E
- Galphin C
- Gambaro G
- Gan Cl
- Gan S
- Garcia Ballesteros C
- Garcia Ortiz Lh
- Garcia I
- Garcia Nh
- Garibotto G
- Gastaldi A
- Gaupsiene E
- Gelersztein E
- Geloneze Neto B
- Genadieva V
- Genova-Hristova G
- George S
- Ghazi A
- Giorda C
- Glenny Ja
- Glinkina I
- Gnudi L
- Godlevska O
- Godoy Jorquera Jg
- Goldenberg R
- Golovchenko O
- Gomes M
- Gomez Rangel Jd
- Gomez O
- Gonzalez Colaso Pdc
- Gonzalez Martinez Fj
- Gonzalez Orellana Ra
- Gonzalez A
- Gonzalez E
- Gonzalez Jp
- Gopalakrishnan N
- Gorelick P
- Gorson D
- Gourdy P
- Govender R
- Govender V
- Gowda A
- Goycoa C
- Goykhman S
- Gracious N
- Greco B
- Greene T
- Greene Tom
- Greloni Gc
- Grineva E
- Grubb S
- Guinsburg A
- Gulati R
- Gunstone A
- Gupta A
- Gupta M
- Gyrina O
- Haase Fp
- Hadjadj S
- Halciakova K
- Hall T
- Haller H
- Halmagyi I
- Hammoud J
- Hancu N
- Handelsman S
- Hanif W
- Hansraj A
- Harcsa E
- Harris R
- Hartman I
- Hawley C
- Heerspink Hiddo J L
- Heerspink Hjl
- Henein S
- Hermida S
- Hernandez Triana E
- Herrera Jimenez Le
- Hershon K
- Hettiarachchi M
- Higuera Jd
- Hillis G
- Hiser D
- Holman R
- Home P
- Hon G
- Hotlos L
- Hristozov K
- Hsia Tl
- Hsieh Ch
- Hudson M
- Hufert K
- Hwang Sj
- Ignjatovic J
- Iitsuka T
- Ilavska A
- Irizar Santana Ss
- Ismail M
- Jackson A
- Jacob R
- Jaffer S
- Jaime M
- Jain D
- Jamal A
- Januszewicz A
- Januzzi J
- Jardine M
- Jardine Meg J
- Jardine Mj
- Jeong Ik
- Jerwan-Keim R
- Jha V
- Ji L
- Jimenez Florez F
- Jimeno C
- Jodar Gimeno Je
- Johnson A
- Johnson D
- Joseph F
- Joshi M
- Juncos Li
- Jurgens J
- Kaczmarek B
- Kajiyama S
- Kamenov Z
- Kaminska A
- Kashine S
- Kasner S
- Kaupke C
- Kawada T
- Kazmirchuk A
- Keightley G
- Keitel E
- Keltai K
- Kendereski A
- Keresztesi S
- Kern E
- Kerr Saraiva Jf
- Keshavamurthy Cb
- Khandwala H
- Khanna R
- Khirmanov V
- Khitan Z
- Khullar D
- Kim S
- Kim Sg
- Kim Yh
- Kiss K
- Kissela B
- Klein A
- Klokocnikova V
- Klyver Mi
- Kodera T
- Kohara Sk
- Koizumi M
- Kolansky D
- Kolesnyk I
- Kolesnyk M
- Kolmakova E
- Komisarenko I
- Kong Wy
- Kong Y
- Kono H
- Konyves L
- Koppolu D
- Kopyt N
- Koroleva T
- Korzh O
- Koundurdjiev A
- Kovar R
- Kovesdy C
- Koyama K
- Kozloviene D
- Kraft F
- Krane V
- Kravchun N
- Krishna G
- Krishnan S
- Kropp J
- Krynski F
- Kumar A
- Kumar J
- Kumar N
- Kumeda Y
- Kumwenda M
- Kurtz Lisboa Hr
- Kusnir J
- Kvitkova L
- Kwon Hs
- Kwon Mj
- Lalic K
- Lalic N
- Lam Sw
- Lanchiotti Pv
- Lane W
- Lastuvka J
- Latiff G
- Laviada Molina H
- Lawrence M
- Lazuka L
- Le Meur Y
- Lee Bw
- Lee J
- Lee Ly
- Lee Mk
- Legun O
- Lehrner L
- Leia C
- Leiter L
- Lentz J
- Leon de la Fuente Ra
- Levin A
- Levin Adeera
- Levinson D
- Lewis D
- Li D
- Li N
- Li W
- Li X
- Lim Sk
- Lim-Abrahan Ma
- Limos A
- Lin Cc
- Lin G
- Lin H
- Lin P
- Lindley R
- Liss K
- Liu J
- Loh Cl
- Lombard L
- Lozanov L
- Lu W
- Lu Yc
- Lukac M
- Luna Ceballos Ri
- Macdougall I
- Maddux A
- Madej A
- Madore F
- Mah Pm
- Mahaffey Kenneth W.
- Mahaffey Kw
- Maheshwari H
- Major L
- Malaver N
- Malberti F
- Malek Marin T
- Mandayam S
- Mandreoli M
- Manisha S
- Mankovskyy B
- Mannucci E
- Manocha Ab
- Mao H
- Marar I
- Marasaev V
- Marchetta N
- Margaritov V
- Martin Del Camp Blanco B
- Martinka E
- Martynyuk L
- Mascaro D
- Maxeiner S
- Mazur S
- Mcguire Dk
- Mcmahon A
- Medina Fari\uf1a M
- Mehta B
- Meininger G
- Meininger Gary
- Mele P
- Middleton J
- Milagres R
- Mileder M
- Miyauchi S
- Mizuyama K
- Mkrtumyan A
- Mlodawska-Choluj D
- Molina de Salazar Di
- Molnar M
- Montenegro Junior R
- Mookadam M
- Morales Franco G
- Morales Portillo C
- Mordujovich J
- Moreda R
- Moreira de Brito C
- Moreira Diaz Jp
- Moreno Loza Ot
- Morren F
- Morugova T
- Mostovoy Y
- Moustafa M
- Mu\uf1oz Lopez Mendoza M
- Mu\uf1oz Torres M
- Mucsi J
- Muirhead N
- Mujica Trenche S
- Munar Vila Ma
- Munteanu M
- Mustieles Rocha C
- Nagibovich G
- Nagibovich O
- Nam Ms
- Narayanan M
- Narvarte J
- Nassar T
- Navickas A
- Nazario Sabbag \uc2r
- Nazzer Hissa M
- Neal B
- Neal Bruce
- Nedogoda S
- Negru D
- Newman G
- Ng Ks
- Ngcakani N
- Nichol B
- Nicholls K
- Nicol P
- Nicolai S
- Nieto Iglesias J
- Niiya T
- Nik Ahmad Nnf
- Nisnisan J
- Nixon P
- Nonchev B
- Noonan P
- Noronha I
- Nortje H
- Nossuli Ak
- Novoa Pa
- Nowicki M
- Nowicki M
- O'Hare J
- O'Shaughnessy A
- Obialo C
- Obrador Vera G
- Obrador G
- Ochodnicka Z
- Oh Kh
- Oishi H
- Olelewe S
- Oliver M
- Onaca Ag
- Oosthuizen H
- Orio Si
- Orlowska-Kowalik G
- Oroszlan T
- Orozco Castellanos R
- Orsi E
- Ory I
- Osipova I
- Ota S
- Otreras F
- Ounadjela S
- Oviedo A
- Packham D
- Padron J
- Panarotto D
- Pankhaniya R
- Pantoja Perez J
- Paragh G
- Parfrey P
- Park Cy
- Park Sh
- Parker R
- Paschen B
- Pashkovska N
- Patel D
- Patel G
- Patel N
- Pavon H
- Pecoits Filho R
- Pecoits-Filho R
- Pella D
- Penfornis A
- Peralta Calcaneo J
- Pereira Ma
- Pererva L
- Perez Vera M
- Perez A
- Perez C
- Peringat J
- Perkovic V
- Perkovic Vlado
- Perlman A
- Pertseva T
- Pesickova S
- Peterfai E
- Peterka K
- Petrica L
- Petro G
- Pettis K
- Pharr W
- Philip S
- Phillips A
- Piatti P
- Pichette V
- Pillay-Ramaya L
- Plassmann G
- Plaza Mv
- Pollock C
- Pollock Carol
- Popa Ar
- Popenda G
- Popovic-Radinovic V
- Portoles Perez Jm
- Prasad N
- Proietto J
- Prozesky H
- Pumprla J
- Purighalla R
- Quesada Sim\uf3n Ma
- Quesada-Suarez L
- Rabasa-Lhoret R
- Raduan Ra
- Raffaele P
- Railey M
- Ramirez Roca La
- Ramos Jc
- Ramtoola S
- Ranetti Ae
- Rangelov R
- Ranjan R
- Raskina T
- Rastogi S
- Ratnasingam V
- Reddy J
- Reddy J
- Ren Y
- Rendell M
- Resk Jh
- Revesz K
- Rewerska B
- Reyes Rosano Ma
- Rheeder P
- Rich L
- Rista L
- Roberts A
- Robinson M
- Rodriguez Papini N
- Rodriguez Pattzi H
- Rodriguez H
- Roger S
- Rosas Guzman J
- Rosas S
- Rose L
- Rosero R
- Rosivall L
- Roussel R
- Rucker Joerg Ie
- Rychl\uedk I
- Rychlik I
- S\ue1nchez Arenales Ja
- Saaveddra Sanchez Sb
- Saavedra Gajardo V
- Saba F
- Sakakibara T
- Sala J
- Salazar Ma
- Samoylov O
- Samoylova Y
- Sanchez Mijangos Jh
- Sanchez Polo Jv
- Sankaram R
- Santoro D
- Santos F
- Santos Jc
- Saporito W
- Sarin R
- Sasso Fc
- Satyanarayana Rk
- Saudek F
- Saulnier Pj
- Saxena M
- Sazonova O
- Scharfstein D
- Schiavi Lb
- Schiller A
- Schmidt M
- Schreiman R
- Schuch T
- Scott D
- Scott R
- Scotton As
- Seeber M
- Sekkarie M
- Sennik D
- Sensenbrenner J
- Serafinceanu C
- Serrano Sanson P
- Serviddio G
- Sessa H
- Shahinfar S
- Shakeel M
- Shamkhalova M
- Shanik M
- Shaw S
- Sheth S
- Sheu Wh
- Shinkov A
- Shutemova E
- Shwartz Y
- Sim\uf5es de Almeida R
- Simo Canonge R
- Simon G
- Singh B
- Sinha Ad
- Slompo Ramos C
- Smatanova I
- Smirnov I
- Smith Casabella T
- Smith S
- Soares Fel\uedcio J
- Solomon R
- Song W
- Sood V
- Soto Gonzalez A
- Soto Mb
- Sowinski D
- Sprague A
- Spry L
- Sreedhar R
- Sreelatha M
- Starzec A
- Steele A
- Stella A
- Stephens J
- Strzelecka A
- Suchinda P
- Sudhakar B
- Sultan S
- Sun J
- Sun L
- Surampudi P
- Sussman S
- Svyshchenko Y
- Symonds R
- Takacs R
- Takai M
- Tamayo Y Orozco JA
- Tan A
- Tan G
- Tangri N
- Tellez Chavez E
- Temelkova M
- Terns Riera M
- Terrelonge A
- Terront Lozano Ma
- Tesar V
- Thervet E
- Thimmaiah R
- Thom\ue9 F
- Thompson M
- Tibes Hachmann Jc
- Tinahones Madueno Fj
- Toarba C
- Tolentino M
- Tomashkevych H
- Tomonaga O
- Topchii I
- Torshizi A
- Travis K
- Trespalacios F
- Trevisan R
- Trippe B
- Trueba P
- Tryshchuk N
- Tsang V
- Tseluyko V
- Tsujimoto M
- Tu P
- Turchin A
- Turcios Juarez E
- Turner W
- Twahirwa M
- Ulla Mr
- Updegrove J
- Urbanaviciene E
- Uriasyev O
- Valderrama Cometa L
- Valdes Depeda A
- Valdez M
- Valenzuela A
- Valis M
- Vallejos A
- Van Buren P
- Vangel S
- Vannorsdall M
- Vargas Alonso Rd
- Varghese F
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- Vyasam Rc
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- Yao C
- Yap Ye
- Yavin Yshai
- Ygpuara Mdl
- Yin A
- Yoiti Hayashida C
- Yoon Kh
- Yost L
- Young S
- Yu X
- Yumita W
- Yupanqui H
- Zaidman Cj
- Zalunardo N
- Zamarripa Escobedo R
- Zanata Petry Tb
- Zanella Mt
- Zaniewski-Singh M.
- Zanoli L
- Zaoui P
- Zateyshchikova A
- Zateyshshikov D
- Zaviriukha V
- Zemek S
- Zhang H
- Zhang Hong
- Zhao M
- Zheng H
- Zinman B
- Zinman Bernard
- Zlova T
- Zsom M
- Zub L
- Zykova T
- Publication venue
- 'Massachusetts Medical Society'
- Publication date
- 01/01/2019
- Field of study
BACKGROUND Type 2 diabetes mellitus is the leading cause of kidney failure worldwide, but few effective long-term treatments are available. In cardiovascular trials of inhibitors of sodium–glucose cotransporter 2 (SGLT2), exploratory results have suggested that such drugs may improve renal outcomes in patients with type 2 diabetes. METHODS In this double-blind, randomized trial, we assigned patients with type 2 diabetes and albuminuric chronic kidney disease to receive canagliflozin, an oral SGLT2 inhibitor, at a dose of 100 mg daily or placebo. All the patients had an estimated glomerular filtration rate (GFR) of 30 to 300 to 5000) and were treated with renin–angiotensin system blockade. The primary outcome was a composite of end-stage kidney disease (dialysis, transplantation, or a sustained estimated GFR of <15 ml per minute per 1.73 m 2), a doubling of the serum creatinine level, or death from renal or cardiovascular causes. Prespecified secondary outcomes were tested hierarchically. RESULTS The trial was stopped early after a planned interim analysis on the recommendation of the data and safety monitoring committee. At that time, 4401 patients had undergone randomization, with a median follow-up of 2.62 years. The relative risk of the primary outcome was 30% lower in the canagliflozin group than in the placebo group, with event rates of 43.2 and 61.2 per 1000 patient-years, respectively (hazard ratio, 0.70; 95% confidence interval [CI], 0.59 to 0.82; P=0.00001). The relative risk of the renal-specific composite of end-stage kidney disease, a doubling of the creatinine level, or death from renal causes was lower by 34% (hazard ratio, 0.66; 95% CI, 0.53 to 0.81; P<0.001), and the relative risk of end-stage kidney disease was lower by 32% (hazard ratio, 0.68; 95% CI, 0.54 to 0.86; P=0.002). The canagliflozin group also had a lower risk of cardiovascular death, myocardial infarction, or stroke (hazard ratio, 0.80; 95% CI, 0.67 to 0.95; P=0.01) and hospitalization for heart failure (hazard ratio, 0.61; 95% CI, 0.47 to 0.80; P<0.001). There were no significant differences in rates of amputation or fracture. CONCLUSIONS In patients with type 2 diabetes and kidney disease, the risk of kidney failure and cardiovascular events was lower in the canagliflozin group than in the placebo group at a median follow-up of 2.62 years
Measurements of sensor radiation damage in the ATLAS inner detector using leakage currents
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Zwalinski L
- Publication venue
- IOP
- Publication date
- 01/01/2021
- Field of study
Non-ionizing energy loss causes bulk damage to the silicon sensors of the ATLAS pixel and strip detectors. This damage has important implications for data-taking operations, charged-particle track reconstruction, detector simulations, and physics analysis. This paper presents simulations and measurements of the leakage current in the ATLAS pixel detector and semiconductor tracker as a function of location in the detector and time, using data collected in Run 1 (2010–2012) and Run 2 (2015–2018) of the Large Hadron Collider. The extracted fluence shows a much stronger |z|-dependence in the innermost layers than is seen in simulation. Furthermore, the overall fluence on the second innermost layer is significantly higher than in simulation, with better agreement in layers at higher radii. These measurements are important for validating the simulation models and can be used in part to justify safety factors for future detector designs and interventions.publishedVersio
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
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- Sjölin J
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- Soldatov EY
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- Solodkov AA
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- Solovyanov OV
- Solovyev V
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- Sopczak A
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- Taffard A
- Tafirout R
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- Talyshev AA
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- Tanaka A
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- Trischuk DA
- Trocmé B
- Troncon C
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- Veatch J
- Vecchio V
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- Vermeulen JC
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- Vgenopoulos A
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- Vickey Boeriu OE
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
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- Villhauer EM
- Vilucchi E
- Vincter MG
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- Visibile A
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- Vladimirov V
- Voevodina E
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- Wiedenmann W
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- Wilkens HG
- Williams DM
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- Willocq S
- Wilson BJ
- Windischhofer PJ
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- Winter BT
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- Wobisch M
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- Yabsley B
- Yacoob S
- Yamaguchi Y
- Yamashita E
- Yamauchi H
- Yamazaki T
- Yamazaki Y
- Yan J
- Yan S
- Yan Z
- Yang HJ
- Yang HT
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- Yang Y
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Ye H
- Ye H
- Ye J
- Ye S
- Ye X
- Yeh Y
- Yeletskikh I
- Yeo BK
- Yexley MR
- Yin P
- Yorita K
- Younas S
- Young C
- Young CJS
- Yu C
- Yu Y
- Yuan M
- Yuan R
- Yue L
- Zaazoua M
- Zabinski B
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zamora Saa JA
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
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- Zhang R
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
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- Zhou Y
- Zhu CG
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- Zhu Y
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- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Measurements of W+W−+ ≥ 1 jet production cross-sections in pp collisions at s = 13 TeV with the ATLAS detector
- Author
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Fiducial and differential cross-section measurements of W+W− production in
association with at least one hadronic jet are presented. These measurements are sensitive
to the properties of electroweak-boson self-interactions and provide a test of perturbative
quantum chromodynamics and the electroweak theory. The analysis is performed using
proton-proton collision data collected at p
s = 13TeV with the ATLAS experiment, corresponding
to an integrated luminosity of 139 fb−1. Events are selected with exactly one oppositely
charged electron-muon pair and at least one hadronic jet with a transverse momentum
of pT > 30 GeV and a pseudorapidity of |�| < 4.5. After subtracting the background
contributions and correcting for detector effects, the jet-inclusive W+W−+ � 1 jet fiducial
cross-section and W+W−+ jets differential cross-sections with respect to several kinematic
variables are measured. These measurements include leptonic quantities, such as the lepton
transverse momenta and the transverse mass of the W+W− system, as well as jet-related
observables such as the leading jet transverse momentum and the jet multiplicity. Limits on
anomalous triple-gauge-boson couplings are obtained in a phase space where interference
between the Standard Model amplitude and the anomalous amplitude is enhanced
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
- Author
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- Zanzi D
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- Zeißner SV
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerradi S
- Zerwas D
- Zgubič M
- Zhang B
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- Zhang G
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- Zhang X
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- 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 NI
- Zimmermann S
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- Field of study
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fb−1 is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain b-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26+17−15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24+7−6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 ± 2.4 fb
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Appelt C
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin JF
- Argyropoulos S
- Arling JH
- Armbruster AJ
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avner G
- Avolio G
- Ayoub MK
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
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