379 research outputs found
Study of resolution of the PANDA GEM detector with Garfield
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Nebuliser therapy in the intensive care unit
- Author
- A Brah
- A Ka Tat Tsang
- A Konitzer-Smirnov
- A Rotkirch
- A Temkina
- BJ Baer
- C Farquhar
- C Ramazanoglu
- CM Hann
- D Altman
- D Cameron
- D Healey
- D Kulick
- DP Schluter
- E Lewin
- E Omel’chenko
- E Omel’chenko
- EK Sedgwick
- EW Said
- F Fukuyama
- F Stella
- F Stella
- I Brade
- IB Neumann
- IS Kon
- J Binnie
- J Butler
- J Butler
- J Weeks
- JD Brewer
- JK Puar
- K Plummer
- K Sarajeva
- K Weston
- L Duggan
- L Engelstein
- L Essig
- L Garber
- L McCall
- L Wolff
- M Besemeres
- M Foucault
- M Müller
- M Nemtsev
- M Vicinus
- MFI Manalansan
- N Duncan
- N Nartova
- N Nartova
- N Nartova
- NA Naples
- R Bleys
- S Ashwin
- S Seidman
- SI Golod
- T Boellstorff
- T Boellstorff
- V Kolossov
- W Leap
- Y Taylor
- Publication venue
- 'BMJ'
- Publication date
- 01/04/1997
- Field of study
The relationship between identity, lived experience, sexual practices and the language through which these are conveyed has been widely debated in sexuality literature. For example, ‘coming out’ has famously been conceptualised as a ‘speech act’ (Sedgwick 1990) and as a collective narrative (Plummer 1995), while a growing concern for individuals’ diverse identifications in relations to their sexual and gender practices has produced interesting research focusing on linguistic practices among LGBT-identified individuals (Leap 1995; Kulick 2000; Cameron and Kulick 2006; Farqhar 2000). While an explicit focus on language remains marginal to literature on sexualities (Kulick 2000), issue of language use and translation are seldom explicitly addressed in the growing literature on intersectionality. Yet intersectional perspectives ‘reject the separability of analytical and identity categories’ (McCall 2005:1771), and therefore have an implicit stake in the ‘vernacular’ language of the researched, in the ‘scientific’ language of the researcher and in the relationship of continuity between the two. Drawing on literature within gay and lesbian/queer studies and cross-cultural studies, this chapter revisits debates on sexuality, language and intersectionality. I argue for the importance of giving careful consideration to the language we choose to use as researchers to collectively define the people whose experiences we try to capture. I also propose that language itself can be investigated as a productive way to foreground how individual and collective identifications are discursively constructed, and to unpack the diversity of lived experience. I address intersectional complexity as a methodological issue, where methodology is understood not only as the methods and practicalities of doing research, but more broadly as ‘a coherent set of ideas about the philosophy, methods and data that underlie the research process and the production of knowledge’ (McCall 2005:1774). My points are illustrated with examples drawn from my ethnographic study on ‘lesbian’ identity in urban Russia, interspersed with insights from existing literature. In particular, I aim to show that an explicit focus on language can be a productive way to explore the intersections between the global, the national and the local in cross-cultural research on sexuality, while also addressing issues of positionality and accountability to the communities researched
Determinant representations of scalar products for the open XXZ chain with non-diagonal boundary terms
- Author
- AG Izergin
- B Davies
- B Hou
- B-Y Hou
- B-Y Hou
- B-Y Hou
- Bo-Yu Hou
- CS Melo
- EK Sklyanin
- FA Smirnov
- G Felder
- HJ Vega de
- IB Frenkel
- J Cao
- J Gier de
- J Gier de
- JM Maillet
- Jun Feng
- Kang-Jie Shi
- Kun Hao
- N Kitanine
- O Tsuchiya
- R Murgan
- RI Nepomechie
- RI Nepomechie
- RI Nepomechie
- RJ Baxter
- S Ghoshal
- S-Y Zhao
- S-Y Zhao
- T-D Albert
- VE Korepin
- VE Korepin
- VG Drinfeld
- W Galleas
- W Galleas
- W-L Yang
- W-L Yang
- W-L Yang
- W-L Yang
- W-L Yang
- W-L Yang
- W-L Yang
- W-L Yang
- W-L Yang
- W-L Yang
- W-L Yang
- W-L Yang
- W-L Yang
- W-L Yang
- Wen-Li Yang
- WL Yang
- WL Yang
- Xi Chen
- Y Koyama
- Y-S Wang
- Yao-Zhong Zhang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 21/11/2010
- Field of study
With the help of the F-basis provided by the Drinfeld twist or factorizing
F-matrix for the open XXZ spin chain with non-diagonal boundary terms, we
obtain the determinant representations of the scalar products of Bethe states
of the model.Comment: Latex file, 28 pages, based on the talk given by W. -L. Yang at
Statphys 24, Cairns, Australia, 19-23 July, 201
Reduced sintering of mass-selected Au clusters on SiO2 by alloying with Ti: an aberration-corrected STEM and computational study
- Author
- Arkill
- Armistead
- Batson
- Batson
- Bela Sebok
- Blochl
- Bond
- Bone
- Bone
- Cao
- Christmann
- D'Souza
- Diercksen
- Duan
- Fujitani
- Gianfranco Pacchioni
- Gomez-Cortes
- Green
- Green
- Grimme
- Gruene
- Guan
- Hammer
- Han
- Han
- Haruta
- Haruta
- Haruta
- Henkelman
- Hernandez-Fernandez
- Holse
- Hu
- Hutchings
- Hvolbæk
- Ib Chorkendorff
- Kast
- Kresse
- Kresse
- Kresse
- Kresse
- Kresse
- Li
- Liu
- Liu
- Ma
- Ma
- Min
- Moler
- Molina
- Monkhorst
- Parker
- Perdew
- Perdew
- Philomena Schlexer
- Pratontep
- Remediakis
- Richard E. Palmer
- Saavedra
- Sandoval
- Sanville
- Schlexer
- Schlexer
- Schlexer
- Smirnov
- Taketoshi
- Tang
- Tosoni
- Veith
- Velazquez-Palenzuela
- von Issendorff
- Wang
- Wang
- Widmann
- Widmann
- Yang
- Young
- Yubiao Niu
- Zhang
- Publication venue
- 'Royal Society of Chemistry (RSC)'
- Publication date
- 01/01/2018
- Field of study
Au nanoparticles represent the most remarkable example of a size effect in heterogeneous catalysis. However, a major issue hindering the use of Au nanoparticles in technological applications is their rapid sintering. We explore the potential of stabilizing Au nanoclusters on SiO2 by alloying them with a reactive metal, Ti. Mass-selected Au/Ti clusters (400 000 amu) and Au2057 clusters (405 229 amu) were produced with a magnetron sputtering, gas condensation cluster beam source in conjunction with a lateral time-of-flight mass filter, deposited onto a silica support and characterised by XPS and LEIS. The sintering dynamics of mass-selected Au and Au/Ti alloy nanoclusters were investigated in real space and real time with atomic resolution aberration-corrected HAADF-STEM imaging, supported by model DFT calculations. A strong anchoring effect was revealed in the case of the Au/Ti clusters, because of a much increased local interaction with the support (by a factor 5 in the simulations), which strongly inhibits sintering, especially when the clusters are more than ∼0.60 nm apart. Heating the clusters at 100 °C for 1 h in a mixture of O2 and CO, to simulate CO oxidation conditions, led to some segregation in the Au/Ti clusters, but in line with the model computational investigation, Au atoms were still present on the surface. Thus size-selected, deposited nanoalloy Au/Ti clusters appear to be promising candidates for sustainable gold-based nanocatalysis
QCD and strongly coupled gauge theories : challenges and perspectives
- Author
- A Accardi
- A Accardi
- A Accardi
- A Adams
- A Afanasev
- A Alexandru
- A Alexandru
- A Alexandru
- A Ali
- A Ali
- A Ali
- A Amato
- A Andronic
- A Andronic
- A Anisimov
- A Antognini
- A Antognini
- A Arvanitaki
- A Azatov
- A Banfi
- A Banfi
- A Barranco
- A Bazavov
- A Bazavov
- A Bazavov
- A Bazavov
- A Beraudo
- A Browman
- A Buzzatti
- A Bzdak
- A Bzdak
- A Calle-Cordon
- A Celis
- A Cheng
- A Chodos
- A Crivellin
- A Cucchieri
- A Czarnecki
- A Czarnecki
- A Denner
- A Deuzeman
- A Deuzeman
- A Deuzeman
- A Dobado
- A Donnachie
- A Donos
- A DotΘ
- A Drukier
- A Dumitru
- A Dumitru
- A Dumitru
- A Esposito
- A Forster
- A Francis
- A Freitas
- A Gal
- A Gouvea de
- A Gray
- A Grimbach
- A Gynther
- A Hameren van
- A Hameren van
- A Hasenfratz
- A Hoang
- A Hoang
- A H÷cker
- A Idilbi
- A Idilbi
- A Khodjamirian
- A Kisiel
- A Knecht
- A Knecht
- A Kovner
- A Kryjevski
- A Kulesza
- A Kurkela
- A Kurkela
- A Kurkela
- A Lenz
- A Li
- A Maas
- A Maas
- A Majumder
- A Majumder
- A Majumder
- A Menon
- A Mocsy
- A Mocsy
- A Morsch
- A Nyffeler
- A Orgogozo
- A Orgogozo
- A Ortiz
- A Patella
- A Paul
- A Pich
- A Pich
- A Pich
- A Pich
- A Pich
- A Pichlmaier
- A Pineda
- A Pineda
- A Pineda
- A Pineda
- A Pineda
- A Pineda
- A Pineda
- A Ramos
- A Ramos
- A Roeck De
- A Rothkopf
- A Salvio
- A Schmitt
- A Schmitt
- A Schmitt
- A Schmitt
- A Schmitt
- A Schmitt
- A Schwenk
- A Serebrov
- A Sibirtsev
- A Sternbeck
- A Thiel
- A Toia
- A Vairo
- A Vairo
- A Vuorinen
- A. Kalweit
- A. Mischke
- A. Pich
- A. S. Kronfeld
- A. Schmitt
- A. Vairo
- A. Vuorinen
- AA Andrianov
- AA Andrianov
- AA Khan
- AA Penin
- AA Penin
- AA Penin
- AA Petrov
- AB Balantekin
- AB Balantekin
- AB Larionov
- AB Zamolodchikov
- AC Aguilar
- AC Cordon
- AD Martin
- AD Martin
- AD Martin
- AE Bondar
- AE Nelson
- AE Snyder
- AH Mueller
- AH Mueller
- AJ Baltz
- AJ Buras
- AJ Buras
- AJ Buras
- AJ Buras
- AJ Buras
- AJ Buras
- AJ Buras
- AK Leibovich
- AL Fitzpatrick
- AL Fitzpatrick
- AM Bernstein
- AM Clogston
- AM Polyakov
- AM Polyakov
- AM Polyakov
- AM Poskanzer
- AP Bakulev
- AP Bakulev
- AP Bakulev
- AP Bakulev
- AP Serebrov
- AP Szczepaniak
- AR Zhitnitsky
- AS Arapoglu
- AS Gorsky
- AS Kronfeld
- AS Kronfeld
- AS Kronfeld
- AS Kronfeld
- AS Schwarz
- AT Davies
- AT Yue
- AV Anisovich
- AV Anisovich
- AV Anisovich
- AV Anisovich
- AV Anisovich
- AV Anisovich
- AV Belitsky
- AV Belitsky
- AV Belitsky
- AV Belitsky
- AV Efremov
- AV Kovalenko
- AV Kovalenko
- AV Manohar
- AV Manohar
- AV Manohar
- AV Manohar
- AV Radyushkin
- AV Radyushkin
- AV Radyushkin
- AV Radyushkin
- AV Smirnov
- AW Steiner
- AX El-Khadra
- AY Alekseev
- B Adeva
- B Adeva
- B Alver
- B Ananthanarayan
- B Batell
- B Bellazzini
- B Berdnikov
- B Bhattacharya
- B Bhattacharya
- B Blossier
- B Blossier
- B Dehnadi
- B Frois
- B Gong
- B Gong
- B Gong
- B Gong
- B Gong
- B Gong
- B Grzadkowski
- B Haskell
- B Haskell
- B Holdom
- B Holdom
- B Kubis
- B Lucini
- B Melić
- B Moussallam
- B Müller
- B Müller
- B MΣrkisch
- B Page
- B Pendleton
- B Pire
- B Plaster
- B Povh
- B Schenke
- B Schrempp
- B Sheikholeslami
- B Wu
- B. Ketzer
- BA Brown
- BA Burrington
- BA Dobrescu
- BA Kniehl
- BA Kniehl
- BA Thacker
- BB Back
- BB Brandt
- BC Regan
- BC Rislow
- BE Lautrup
- BG Zakharov
- BG Zakharov
- BJ Menadue
- BJ Owen
- BM Roberts
- BO Lange
- BR Holstein
- BS Chandrasekhar
- BU Musch
- C Alexandrou
- C Alexandrou
- C Alexandrou
- C Alexandrou
- C Alexandrou
- C Alexandrou
- C Alexandrou
- C Amsler
- C Anastasiou
- C Anzai
- C Aubin
- C Aubin
- C Aubin
- C Aubin
- C Aubin
- C Bernard
- C Bourrely
- C Csaki
- C Csaki
- C DeTar
- C Ditsche
- C Donato Di
- C Fernández-Ramírez
- C Fernández-Ramírez
- C Fernández-Ramírez
- C Fuchs
- C Gale
- C Gattringer
- C Gattringer
- C Gattringer
- C Gerschel
- C Hartnack
- C Jayalath
- C Lourenτo
- C Manuel
- C McNeile
- C McNeile
- C McNeile
- C Meng
- C Michael
- C Michael
- C Morningstar
- C Nunez
- C Pelissier
- C Rappold
- C Ratti
- C Shen
- C Shen
- C-H Chang
- C-M Chang
- C-Y Chen
- C. A. Salgado
- CA Baker
- CA Baker
- CA Meyer
- CA Salgado
- CB Lang
- CB Lang
- CB Lang
- CB Paranavitane
- CE Carlson
- CE Carlson
- CE Carlson
- CE Wolfe
- CG Boyd
- CG Callan
- CG Parthey
- CJ Bomhof
- CJ Morningstar
- CL Korpa
- CL Schat
- CM Arnesen
- CM Maekawa
- CP Herzog
- CP Herzog
- CR Allton
- CS Fischer
- CS Fischer
- CT Hill
- CT Sachrajda
- CTH Davies
- CW Bauer
- CW Bauer
- CW Bauer
- CW Bauer
- CW Bauer
- CW Bauer
- CW Bernard
- D Arean
- D Babusci
- D Bailin
- D Bak
- D Bandurin
- D Banerjee
- D Becirevic
- D Becirevic
- D Becirevic
- D Bernecker
- D Besak
- D Binosi
- D Binosi
- D Blaschke
- D Blaschke
- D Blaschke
- D Bodeker
- D Bodeker
- D Bodeker
- D Boer
- D Boito
- D Diakonov
- D Diakonov
- D Diakonov
- D Dubbers
- D Dubbers
- D Dudal
- D Elander
- D Espriu
- D Florian de
- D Florian de
- D Florian de
- D Forde
- D Gaiotto
- D Gotta
- D Grumiller
- D Guadagnoli
- D Jido
- D Kang
- D Kharzeev
- D Kharzeev
- D Kharzeev
- D Mateos
- D Melconian
- D Mohler
- D Molnar
- D Müller
- D Ng
- D Page
- D Pirjol
- D Pirjol
- D Pirjol
- D Ruic
- D Sahoo
- D Steineder
- D Steineder
- D Teaney
- D Tong
- D Zwanziger
- D Zwanziger
- D-Y Chen
- D. Keane
- DA Demir
- DB Kaplan
- DB Kaplan
- DB Kaplan
- DB Kaplan
- DB Kaplan
- DB Leinweber
- DB Leinweber
- DC McGlinchey
- DE Kharzeev
- DE Kharzeev
- DE Kharzeev
- DE Morrissey
- DG Yakovlev
- DJ Dean
- DJ Salvat
- DJ Schwarz
- DM Alde
- DM Alde
- DM Asner
- DS Armstrong
- DT Son
- DT Son
- DT Son
- DT Son
- DT Son
- DT Son
- DV Amelin
- DV Shirkov
- DW Sivers
- E Applebaum
- E Botta
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Braaten
- E Conde
- E Dalgic
- E Eichten
- E Eichten
- E Epelbaum
- E Epelbaum
- E Ferreiro
- E Flowers
- E Franco
- E Frodermann
- E Golowich
- E Gregory
- E Gámiz
- E Iancu
- E Kiritsis
- E Kiritsis
- E Klempt
- E Kuflik
- E Laenen
- E Leader
- E Massot
- E Megias
- E Mereghetti
- E Perez
- E Poppitz
- E Rafael de
- E Schnedermann
- E Sezgin
- E Shintani
- E Shintani
- E Shintani
- E Shintani
- E Shuster
- E Witten
- E Witten
- E Witten
- E Witten
- E-M Ilgenfritz
- E. Kiritsis
- E. Pallante
- EB Gregory
- EC Poggio
- ED Skillman
- EE Jenkins
- EE Jenkins
- EE Kolomeitsev
- EG Ferreiro
- EJ Eichten
- EL Berger
- ER Berger
- ES Fraga
- F Antinori
- F Arleo
- F Arleo
- F Arleo
- F Arleo
- F Becattini
- F Berruto
- F Bezrukov
- F Bruckmann
- F Burger
- F Cachazo
- F Caravaglios
- F Cascioli
- F D'Eramo
- F D'Eramo
- F Diberder Le
- F Diberder Le
- F Dominguez
- F Englert
- F Feng
- F Gelis
- F Haas
- F Hautmann
- F Iocco
- F Jegerlehner
- F Jegerlehner
- F Jegerlehner
- F Karsch
- F Karsch
- F Karsch
- F Karsch
- F Lenz
- F Niecknig
- F Osterfeld
- F Preis
- F Preis
- F Steiner
- F Wilczek
- F-K Guo
- F-K Guo
- F-K Guo
- F-K Guo
- F. J. Llanes-Estrada
- FA Berends
- FA Dolan
- FA Dolan
- FE Close
- FE Wietfeldt
- FE Wietfeldt
- FJ Tackmann
- FJM Farley
- FL Shapiro
- FV Gubarev
- G Aarts
- G Aarts
- G Aarts
- G Aarts
- G Agakishiev
- G Altarelli
- G Amoros
- G Bali
- G Bell
- G Bell
- G Bellini
- G Bevilacqua
- G Bevilacqua
- G Bhanot
- G Bozzi
- G Buchalla
- G Buchalla
- G Burdman
- G Burdman
- G Cacciapaglia
- G Cacciapaglia
- G Colangelo
- G Colangelo
- G Colangelo
- G Corcella
- G Cullen
- G Cullen
- G D'Ambrosio
- G D'Ambrosio
- G Degrassi
- G Ecker
- G Ecker
- G Eichmann
- G Eichmann
- G Eichmann
- G Eichmann
- G Eichmann
- G Endrődi
- G Hiller
- G Hiller
- G Isidori
- G Jungman
- G Ossola
- G Ossola
- G Ossola
- G Ossola
- G Ovanesyan
- G Prezeau
- G Ricciardi
- G Ricciardi
- G Ricciardi
- G Ricciardi
- G Watt
- G Watt
- G Wlazłowski
- G-Z Xu
- G. M. von Hippel
- G. Odyniec
- G. Ricciardi
- GA Miller
- GA Miller
- GA Miller
- GA Miller
- GC Donald
- GC Giecold
- GC Nayak
- GC Nayak
- GC Nayak
- GC Nayak
- GD Moore
- GF Giudice
- GF Teramond de
- GJ Gounaris
- GJ Gounaris
- GJ Mathews
- GM Divitiis de
- GM Divitiis de
- GM Divitiis de
- GM Divitiis de
- GM Divitiis de
- GP Engel
- GP Lepage
- GP Lepage
- GP Lepage
- GS Bali
- GS Bali
- GT Bodwin
- GT Bodwin
- GT Bodwin
- GT Bodwin
- GT Bodwin
- GT Bodwin
- GT Bodwin
- H Abuki
- H Chen
- H Chen
- H Flacher
- H Fujii
- H Fujii
- H Fujii
- H Fujii
- H Georgi
- H Georgi
- H Georgi
- H Hata
- H Jallouli
- H Johansson
- H Kowalski
- H Lenske
- H Leutwyler
- H Liu
- H Liu
- H Liu
- H Liu
- H Muther
- H Na
- H Na
- H Na
- H Neuberger
- H Neuberger
- H Ohki
- H Reinhardt
- H Sanchis-Alepuz
- H Satz
- H Satz
- H Song
- H Stoecker
- H-J Drescher
- H-K Guo
- H-N Li
- H-N Li
- H-N Li
- H-R Dong
- H-T Chen
- H-T Ding
- H-W Lin
- H-W Lin
- H-W Lin
- H-Y Cheng
- H-Y Cheng
- H. B. Meyer
- H. Sazdjian
- H. W. Lin
- H. Wittig
- HB Meyer
- HB Meyer
- HB Meyer
- HB Meyer
- HB Meyer
- HB Meyer
- HB Meyer
- HB Meyer
- HK Wohri
- HS Sharatchandra
- HT Ding
- I Balitsky
- I Balitsky
- I Balitsky
- I Bediaga
- I Bediaga
- I Bediaga
- I Bigi
- I Caprini
- I Caprini
- I Feige
- I Gahramanov
- I Giannakis
- I Giller
- I Helenius
- I Horvath
- I Kuznetsova
- I Sagert
- I Vitev
- IA Karpenko
- IB Khriplovich
- IB Khriplovich
- IB Khriplovich
- IC Cloet
- IC Cloet
- IG Aznauryan
- IG Aznauryan
- II Bigi
- IL Bogolubsky
- IO Cherednikov
- IO Cherednikov
- IO Cherednikov
- IO Cherednikov
- IR Klebanov
- IT Lorenz
- IV Danilkin
- IW Stewart
- IW Stewart
- IW Stewart
- IY Aref'eva
- J Alwall
- J Antoniadis
- J Arrington
- J Babington
- J Berges
- J Berges
- J Bernabeu
- J Bernabeu
- J Bijnens
- J Bijnens
- J Bijnens
- J Bijnens
- J Bijnens
- J Bijnens
- J Bijnens
- J Bijnens
- J Blümlein
- J Boer de
- J Braun
- J Braun
- J Brod
- J Brod
- J Brodzicka
- J Bsaisou
- J Bulava
- J Bulava
- J Bulava
- J Bulava
- J Casalderrey-Solana
- J Casalderrey-Solana
- J Casalderrey-Solana
- J Casalderrey-Solana
- J Chay
- J Cleymans
- J Collins
- J Dobaczewski
- J Dudek
- J Dudek
- J Ellis
- J Engel
- J Erdmenger
- J Erdmenger
- J Erler
- J Erler
- J Galloway
- J Gao
- J Gasser
- J Gasser
- J Gasser
- J Gasser
- J Gasser
- J Gasser
- J Gasser
- J Ghiglieri
- J Giedt
- J Gomez
- J Greensite
- J Greensite
- J Greensite
- J Harada
- J Harada
- J Heinonen
- J Hirn
- J Hisano
- J Jalilian-Marian
- J Jalilian-Marian
- J Jalilian-Marian
- J Kang
- J Kim
- J Laiho
- J Liao
- J Maldacena
- J Maldacena
- J Menendez
- J Menendez
- J Nagata
- J Polchinski
- J Pumplin
- J Rapaport
- J Schaffner
- J Schaffner-Bielich
- J Schukraft
- J Schweizer
- J Shu
- J Siebenson
- J Stahov
- J Steinheimer
- J Thaler
- J Vries de
- J Vries de
- J Vries de
- J Xu
- J Xu
- J-H Kim
- J-J Wu
- J-P Blaizot
- J-W Qiu
- J-Y Chiu
- J-Y Chiu
- J-Z Li
- J. Erdmenger
- J. L. Goity
- J.-W. Qiu
- JA Formaggio
- JA Oller
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- Z. Fodor
- Publication venue
- Publication date
- 01/01/2014
- Field of study
We highlight the progress, current status, and open challenges of QCD-driven physics, in theory and in experiment. We discuss how the strong interaction is intimately connected to a broad sweep of physical problems, in settings ranging from astrophysics and cosmology to strongly coupled, complex systems in particle and condensed-matter physics, as well as to searches for physics beyond the Standard Model. We also discuss how success in describing the strong interaction impacts other fields, and, in turn, how such subjects can impact studies of the strong interaction. In the course of the work we offer a perspective on the many research streams which flow into and out of QCD, as well as a vision for future developments.Peer reviewe
Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at root s=8 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adair A
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adzic P
- Agapitos A
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Al-bataineh A
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Alderweireldt S
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alimena J
- Almond J
- Alunni Solestizi L
- Alverson G
- Alves FL
- Alves GA
- Alyari M
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- Zevi Della Porta G
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
Peer reviewe
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta G
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-Bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexakhin V
- Alexander J
- Alhusseini M
- Ali MAB Md
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez JD Ruiz
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa K Hurtado
- Anderson D
- Andrea J
- Andreev V
- Andreev Yu
- Andrews MB
- Androsov K
- Angioni GL Pinna
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arndt T
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asghar MI
- Asilar E
- Askew A
- Assran Y
- Atakisi IO
- Atay S
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avila C
- Ayala E
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Bagliesi G
- Bahinipati S
- Baidali S
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Ball AH
- Ball F
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- Banerjee S
- Banerjee S
- Bani L
- Bansal S
- Barbagli G
- Barberis E
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- Baringer P
- Barker A
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- Barney D
- Baron O
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- Barrera C Oropeza
- Barria P
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- Bartek R
- Barth C
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- Bartosik N
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- Beretvas A
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- Berger P
- Beri SB
- Bernardes CA
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- Berry D
- Berryhill J
- Bertsche D
- Besancon M
- Beschi A
- Betts RR
- Bhandari R
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search for the production of a pair of top squarks at the LHC is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar, because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with 35.9 fb(-1) of proton-proton collisions at a centre-of-mass energy of root s = 13 TeV, collected by the CMS detector in 2016, using events containing one electron-muon pair with opposite charge. The search is based on a precise estimate of the top quark pair background, and the use of the M-T2 variable, which combines the transverse mass of each lepton and the missing transverse momentum. No excess of events is found over the standard model predictions. Exclusion limits are placed at 95% confidence level on the production of top squarks up to masses of 208 GeV for models with a mass difference between the top squark and the lightest neutralino close to that of the top quark.Peer reviewe
Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-Bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexander J
- Alhusseini M
- Ali MAB Md
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- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez JD Ruiz
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- Andreev Yu
- Andrews MB
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search for dark matter produced in association with top quarks in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. The data set used corresponds to an integrated luminosity of 35.9 fb(-1) recorded with the CMS detector at the LHC. Whereas previous searches for neutral scalar or pseudoscalar mediators considered dark matter production in association with a top quark pair only, this analysis also includes production modes with a single top quark. The results are derived from the combination of multiple selection categories that are defined to target either the single top quark or the top quark pair signature. No significant deviations with respect to the standard model predictions are observed. The results are interpreted in the context of a simplified model in which a scalar or pseudoscalar mediator particle couples to a top quark and subsequently decays into dark matter particles. Scalar and pseudoscalar mediator particles with masses below 290 and 300 GeV, respectively, are excluded at 95% confidence level, assuming a dark matter particle mass of 1 GeV and mediator couplings to fermions and dark matter particles equal to unity.Peer reviewe
FCC Physics Opportunities: Future Circular Collider Conceptual Design Report Volume 1
- Author
- Abada A
- Abbrescia M
- AbdusSalam SS
- Abdyukhanov I
- Abramov A
- Aburaia M
- Acar AO
- Adzic PR
- Agrawal P
- Aguilar-Saavedra JA
- Aguilera-Verdugo JJ
- Ahnen JV
- Aiba M
- Aichinger I
- Aielli G
- Akay A
- Akhundov A
- Aksakal H
- Alaniz EC
- Albacete JL
- Albergo S
- Alekou A
- Aleksa M
- Aleksan R
- Alexahin Y
- Alia RG
- Alioli S
- Allanach BC
- Allport PP
- Altinli M
- Altmannshofer W
- Amann RW
- Ambrosio G
- Amorim D
- Amstutz O
- Anderlini L
- Andreazza A
- Andreini M
- Andriatis A
- Andris C
- Andronic A
- Angelucci M
- Antinori F
- Antipov SA
- Antonelli M
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- Antusch S
- Anulli F
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- Appleby RB
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- Arias S
- Armesto N
- Arnaldi R
- Arsenyev SA
- Arzeo M
- Asai S
- Aslanides E
- Astapovych D
- Atanasov M
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- Attie D
- Auchmann B
- Audurier A
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- Aune S
- Avino F
- Avrillaud G
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- Azatov A
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- Bachacou H
- Baek YW
- Baglin V
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- Yanehsari MK
- Yang G
- Yang HJ
- Yao W-M
- Yazgan E
- Yermolchik V
- Yildiz HD
- Yilmaz A
- Yilmaz A
- Yoo H-D
- Yost SA
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- Yu T-T
- Zaborowska A
- Zadeh SG
- Zadeh SG
- Zahnd M
- Zanetti M
- Zanotto L
- Zawiejski L
- Zeiler P
- Zerlauth M
- Zernov SM
- Zevi Dell Porta G
- Zhang C
- Zhang H
- Zhang Y
- Zhang Z
- Zhao Z
- Zhong Y-M
- Zhou D
- Zhou J
- Zhuang P
- Zick G
- Zimmermann F
- Zinn-Justin J
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- Zlobin AV
- Zobov M
- Zupan J
- Zurita J
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/06/2019
- Field of study
We review the physics opportunities of the Future Circular Collider, covering its e+e-, pp, ep and heavy ion programmes. We describe the measurement capabilities of each FCC component, addressing the study of electroweak, Higgs and strong interactions, the top quark and flavour, as well as phenomena beyond the Standard Model. We highlight the synergy and complementarity of the different colliders, which will contribute to a uniquely coherent and ambitious research programme, providing an unmatchable combination of precision and sensitivity to new physics
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmed A
- Ahuja S
- Aime C
- Akchurin N
- Akgun B
- Akpinar A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allen B
- Almond J
- Alvarez Gonzalez B
- Alverson G
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Amendola C
- Amin N
- Amram O
- Amsler C
- Anagnostou G
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Antchev G
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Apyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Aruta C
- Asavapibhop B
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Asmuss P
- Aspell P
- Atakisi IO
- Atanassov I
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awais A
- Awan MIM
- Ayala E
- Ayala G
- Aydogmus Sen F
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Baginyan A
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Bakirci MN
- Baldenegro Barrera C
- Ball AH
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barnes VE
- Barney D
- Baron O
- Barrio Luna M
- Bartek R
- Bartosik N
- Bartók M
- Bastos D
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
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- Özçelik Ö
- Široký J
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
A search for dark matter in the form of strongly interacting massive particles (SIMPs) using the CMS detector at the LHC is presented. The SIMPs would be produced in pairs that manifest themselves as pairs of jets without tracks. The energy fraction of jets carried by charged particles is used as a key discriminator to suppress efficiently the large multijet background, and the remaining background is estimated directly from data. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 16.1 fb - 1 , collected with the CMS detector in 2016. No significant excess of events is observed above the expected background. For the simplified dark matter model under consideration, SIMPs with masses up to 100 GeV are excluded and further sensitivity is explored towards higher masses
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