780 research outputs found
Evaluation of the North West London Diabetes Foot Care Transformation Project: a mixed-methods evaluation
- Publication venue
- 'Ubiquity Press, Ltd.'
- Publication date
- 01/01/2022
- Field of study
Introduction: Diabetes foot ulceration (DFU) presents an enormous burden to those living with diabetes and to the local health systems and economies. There is an increasing interest in implementing integrated care models to enhance the quality of care for people living with diabetes and related complications and the value of co-production approaches to achieve sustainable change. This paper aims to describe the evaluation methodology for the North West London (NWL) Diabetes Foot Care Transformation project. Description: A mixed methods design including: i) a quasi-experimental quantitative analysis assessing the impact of the implementation of the local secondary care multi-disciplinary diabetes foot team clinics on service utilisation and clinical outcomes (amputations and number of healed patients); ii) a phenomenological, qualitative study to explore patient and staff experience; and iii) a within-trial cost-effectiveness analysis (pre and post 2017) to evaluate the programme cost-effectiveness. Discussion and Conclusion: Demonstrating the impact of multidisciplinary, integrated care models and the value of co-production approaches is important for health providers and commissioners trying to improve health outcome. Evaluation is also needed to identify strategies to overcome barriers which might have reduced the impact of the programme and key elements for improvement
Perivascular Expression and Potent Vasoconstrictor Effect of Dynorphin A in Cerebral Arteries
- Author
- A Ouyang
- A Thureson-Klein
- A Venteicher
- AI Faden
- AI Faden
- AI Faden
- AI Faden
- AI Faden
- AI Faden
- AI Faden
- AI Faden
- Attila Cselenyák
- B Brugos
- B Horváth
- BT Altura
- BT Altura
- C Severi
- CR Figley
- CS Roy
- D Massardier
- E Hamel
- EA Young
- H Tada
- J Hu
- J Lai
- JE Hardebo
- JF Tong
- JM Quillan
- JO Devine
- JP Headrick
- JP Headrick
- JR Grider
- JY Kong
- Ken Arai
- Krisztina Káldi
- L Zhang
- M Deli
- M Miura
- MA Moskowitz
- MA Moskowitz
- MC Thorogood
- P Sándor
- Péter Sándor
- R Uddman
- Rege Sugárka Papp
- RL Klein
- RM Arendt
- RM Caudle
- RM Caudle
- S Müller
- S Müller
- S Zhang
- SA Krumins
- SE Kapadia
- SJ Evans
- T Willis
- Tamás Németh
- TJ Schwedt
- TK Mcintosh
- V Shankar
- VM Pickel
- WM Armstead
- WM Armstead
- WM Armstead
- WM Armstead
- WM Armstead
- WM Armstead
- WM Armstead
- WM Armstead
- Z Benyó
- Z Benyó
- Z Lacza
- Zoltán Benyó
- Éva Ruisanchez
- Publication venue
- Public Library of Science
- Publication date
- 25/05/2012
- Field of study
BACKGROUND: Numerous literary data indicate that dynorphin A (DYN-A) has a significant impact on cerebral circulation, especially under pathophysiological conditions, but its potential direct influence on the tone of cerebral vessels is obscure. The aim of the present study was threefold: 1) to clarify if DYN-A is present in cerebral vessels, 2) to determine if it exerts any direct effect on cerebrovascular tone, and if so, 3) to analyze the role of κ-opiate receptors in mediating the effect. METHODOLOGY/PRINCIPAL FINDINGS: Immunohistochemical analysis revealed the expression of DYN-A in perivascular nerves of rat pial arteries as well as in both rat and human intraparenchymal vessels of the cerebral cortex. In isolated rat basilar and middle cerebral arteries (BAs and MCAs) DYN-A (1-13) and DYN-A (1-17) but not DYN-A (1-8) or dynorphin B (DYN-B) induced strong vasoconstriction in micromolar concentrations. The maximal effects, compared to a reference contraction induced by 124 mM K(+), were 115±6% and 104±10% in BAs and 113±3% and 125±9% in MCAs for 10 µM of DYN-A (1-13) and DYN-A (1-17), respectively. The vasoconstrictor effects of DYN-A (1-13) could be inhibited but not abolished by both the κ-opiate receptor antagonist nor-Binaltorphimine dihydrochloride (NORBI) and blockade of G(i/o)-protein mediated signaling by pertussis toxin. Finally, des-Tyr(1) DYN-A (2-13), which reportedly fails to activate κ-opiate receptors, induced vasoconstriction of 45±11% in BAs and 50±5% in MCAs at 10 µM, which effects were resistant to NORBI. CONCLUSION/SIGNIFICANCE: DYN-A is present in rat and human cerebral perivascular nerves and induces sustained contraction of rat cerebral arteries. This vasoconstrictor effect is only partly mediated by κ-opiate receptors and heterotrimeric G(i/o)-proteins. To our knowledge our present findings are the first to indicate that DYN-A has a direct cerebral vasoconstrictor effect and that a dynorphin-induced vascular action may be, at least in part, independent of κ-opiate receptors
The Impact of Global Warming and Anoxia on Marine Benthic Community Dynamics: an Example from the Toarcian (Early Jurassic)
- Author
- A Hallam
- A Nützel
- A Steckbauer
- A Tomašových
- ALA Johnson
- AM Bush
- AS Cohen
- AS Howard
- AS Howard
- B Riedel
- BA Caswell
- BA Caswell
- BL Nikitenko
- C Korte
- CE Savrda
- CL Belanger
- CR Pearce
- Crispin T. S. Little
- CTS Little
- CTS Little
- DB Kemp
- E Erba
- F Cecca
- F García Joral
- G Dera
- G Dera
- G Sælen
- G Sælen
- G Thorson
- GD Price
- H-J Röhl
- HC Jenkyns
- HC Jenkyns
- J Pálfy
- JB Kruskal
- JH Powell
- JHS Macquaker
- JJ Gómez
- JJ Gómez
- JM McArthur
- JM McArthur
- JP Bassoullet
- JT Greensmith
- JW Valentine
- JW Valentine
- K Pye
- K Roy
- KA Morris
- KG Miller
- KJ Willis
- KM Layou
- KR Clarke
- KR Clarke
- KR Clarke
- L Schwark
- LA Levin
- LA Levin
- M Aberhan
- M Aberhan
- M Stachowitsch
- Marie-Emilie Clémence
- ME Gahr
- ME Gahr
- ME Patzkowsky
- MK Howarth
- MK Howarth
- MK Howarth
- N Bonuso
- N Dubilier
- PB Wignall
- PB Wignall
- PB Wignall
- PG Oliver
- PG Oliver
- PJ Harries
- Q Li
- R Ludvigsen
- R Rosenberg
- R Vaquer-Sunyer
- RB Bucefalo Palliani
- RD Pancost
- Richard J. Butler
- Richard J. Twitchett
- RJ Diaz
- RJ Diaz
- RM Warwick
- RM Warwick
- RPS Jefferies
- RS Hori
- S Mailliot
- S Schouten
- SD Morten
- SG Ghadeer
- Silvia Danise
- SP Hesselbo
- TD Olszewski
- TR Bailey
- W Miller III
- W Oschmann
- WM Kemp
- Ø Hammer
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2013
- Field of study
The Pliensbachian-Toarcian (Early Jurassic) fossil record is an archive of natural data of benthic community response to global warming and marine long-term hypoxia and anoxia. In the early Toarcian mean temperatures increased by the same order of magnitude as that predicted for the near future; laminated, organic-rich, black shales were deposited in many shallow water epicontinental basins; and a biotic crisis occurred in the marine realm, with the extinction of approximately 5% of families and 26% of genera. High-resolution quantitative abundance data of benthic invertebrates were collected from the Cleveland Basin (North Yorkshire, UK), and analysed with multivariate statistical methods to detect how the fauna responded to environmental changes during the early Toarcian. Twelve biofacies were identified. Their changes through time closely resemble the pattern of faunal degradation and recovery observed in modern habitats affected by anoxia. All four successional stages of community structure recorded in modern studies are recognised in the fossil data (i.e. Stage III: climax; II: transitional; I: pioneer; 0: highly disturbed). Two main faunal turnover events occurred: (i) at the onset of anoxia, with the extinction of most benthic species and the survival of a few adapted to thrive in low-oxygen conditions (Stages I to 0) and (ii) in the recovery, when newly evolved species colonized the re-oxygenated soft sediments and the path of recovery did not retrace of pattern of ecological degradation (Stages I to II). The ordination of samples coupled with sedimentological and palaeotemperature proxy data indicate that the onset of anoxia and the extinction horizon coincide with both a rise in temperature and sea level. Our study of how faunal associations co-vary with long and short term sea level and temperature changes has implications for predicting the long-term effects of “dead zones” in modern oceans
X-Ray Spectroscopy of Stars
- Author
- A Antunes
- A Feldmeier
- A Feldmeier
- A Maggio
- A Maggio
- A Maggio
- A Meer van der
- A Telleschi
- A Telleschi
- A Telleschi
- A Telleschi
- A ud-Doula
- AC Brinkman
- AE Glassgold
- AG Emslie
- AH Gabriel
- AJ Willis
- AJJ Raassen
- AJJ Raassen
- AJJ Raassen
- AJJ Raassen
- AJJ Raassen
- AK Dupree
- AMT Pollock
- AMT Pollock
- AMT Pollock
- AW Fullerton
- B Ball
- B Ercolano
- B Fuhrmeister
- B Stelzer
- B Stelzer
- B Stelzer
- B Stelzer
- B Stelzer
- B Stelzer
- BE Wood
- BJ Wargelin
- BR Dennis
- BW Bopp
- C Argiroffi
- C Argiroffi
- C Argiroffi
- C Argiroffi
- C Liefke
- CA Tout
- CE Parnell
- CJ Schrijver
- CJ Schrijver
- CJ Schrijver
- CJ Schrijver
- CJ Schrijver
- CR Canizares
- CS Choi
- D Baade
- D García-Alvarez
- D García-Alvarez
- D García-Alvarez
- D Lorenzetti
- D Porquet
- DA Swartz
- DB Henley
- DB Henley
- DH Cohen
- DH Cohen
- DH Cohen
- DH Cohen
- DL McKenzie
- DP Huenemoerder
- DP Huenemoerder
- DP Huenemoerder
- DP Huenemoerder
- DR Ballantyne
- E Behar
- E Flaccomio
- E Franciosini
- E Gosset
- E Landi
- EI Vilkoviskii
- EJM Besselaar van den
- EN Parker
- EV Gotthelf
- F Damiani
- F Favata
- F Favata
- F Favata
- F Favata
- F Martins
- F Palla
- F Reale
- FD Seward
- FM Walter
- FM Walter
- FR Harnden Jr
- G Giardino
- G Giardino
- G Giardino
- G Peres
- G Rauw
- G Rauw
- G Rauw
- G Rauw
- GA Doschek
- GA Wade
- GAJ Hussain
- GAJ Hussain
- GAJ Hussain
- GH Herbig
- GH Herbig
- GH Herbig
- GHJ Oord van den
- GR Blumenthal
- H Sana
- H Sana
- H Sana
- H Schild
- H Zinnecker
- HM Antia
- HM Günther
- HM Günther
- HM Günther
- HRM Magee
- ID Howarth
- II Antokhin
- II Antokhin
- IJD Craig
- IR Stevens
- IR Stevens
- J Bally
- J Robrade
- J Robrade
- J Robrade
- J Robrade
- J Sanz-Forcada
- J Sanz-Forcada
- J Sanz-Forcada
- J Sanz-Forcada
- JC Bouret
- JC Bouret
- JC Brown
- JC Hénoux
- JF Albacete Colombo
- JF Donati
- JF Donati
- JF Donati
- JF Donati
- JF Vesecky
- JH Kastner
- JH Kastner
- JH Kastner
- JH Kastner
- JH Kastner
- JHMM Schmitt
- JHMM Schmitt
- JHMM Schmitt
- JHMM Schmitt
- JHMM Schmitt
- JHMM Schmitt
- JHMM Schmitt
- JJ Drake
- JJ Drake
- JJ Drake
- JJ Drake
- JJ Drake
- JJ Drake
- JJ Drake
- JJ Drake
- JJ Drake
- JJ Drake
- JJ Macfarlane
- JJ Macfarlane
- JM Laming
- JM Laming
- JM Laming
- JM Pittard
- JM Pittard
- JM Pittard
- JN Bahcall
- JP Cassinelli
- JP Cassinelli
- JP Cassinelli
- JP Cassinelli
- JT Schmelz
- JU Ness
- JU Ness
- JU Ness
- JU Ness
- JU Ness
- JU Ness
- K Hamaguchi
- K Imanishi
- K Shibata
- K Shibata
- K Smith
- K Smith
- KA Hucht van der
- KG Stassun
- KH Nordsieck
- KJH Phillips
- KJH Phillips
- KV Getman
- L Hartmann
- L Prisinzano
- L Scelsi
- L Scelsi
- LB Lucy
- LM Oskinova
- LM Oskinova
- LM Oskinova
- LM Oskinova
- LM Oskinova
- M Audard
- M Audard
- M Audard
- M Audard
- M Audard
- M Audard
- M De Becker
- M De Becker
- M De Becker
- M Gagné
- M Gagné
- M Güdel
- M Güdel
- M Güdel
- M Güdel
- M Güdel
- M Güdel
- M Güdel
- M Güdel
- M Güdel
- M Güdel
- M Jardine
- M Jardine
- M Matranga
- M Rodonò
- M Siarkowski
- M Tsujimoto
- MA Guerrero
- MA Guerrero
- MA Leutenegger
- MA Leutenegger
- MA Smith
- Manuel Güdel
- MJ Aschwanden
- MS Giampapa
- N Calvet
- N Grevesse
- N Grosso
- N Linder
- N Markova
- N Pizzolato
- NA Miller
- NB Crosby
- NE White
- NE White
- NR Walborn
- NR Walborn
- NS Brickhouse
- NS Brickhouse
- NS Brickhouse
- NS Schulz
- P Gondoin
- P Gondoin
- P Testa
- P Testa
- P Testa
- P Testa
- P Testa
- P Testa
- PC Schneider
- PJ Cargill
- PR Young
- PS Wojdowski
- Q Li
- R Ignace
- R Ignace
- R Ignace
- R Mewe
- R Mewe
- R Mewe
- R Mewe
- R Nordon
- R Nordon
- R Nordon
- R Ottmann
- R Pallavicini
- R Pallavicini
- R Rosner
- R Ventura
- RA Osten
- RA Osten
- RA Osten
- RA Osten
- RA Osten
- RA Stern
- RH Kramer
- RJ Bray
- RK Prinja
- RK Ulrich
- RL Mutel
- RS Schnerr
- S Bowyer
- S Czesla
- S Hubrig
- S Hubrig
- S Hubrig
- S Krucker
- S Randich
- S Sciortino
- S Sciortino
- S Serio
- S Skinner
- S Watanabe
- SA Zhekov
- SA Zhekov
- SA Zhekov
- SG Gregory
- SH Pravdo
- SK Antiochos
- SK Antiochos
- SL Hawley
- SL Skinner
- SL Skinner
- SL Skinner
- SL Skinner
- SL Skinner
- SL Skinner
- SM Chung
- SM Kahn
- SP Owocki
- SP Owocki
- SP Owocki
- SP Owocki
- T Bai
- T Chlebowski
- T Eversberg
- T Preibisch
- TR Ayres
- TR Ayres
- TW Berghöfer
- TW Berghöfer
- U Feldman
- U Mitra-Kraev
- V Petit
- VL Kashyap
- W Chen
- WHM Ku
- WL Waldron
- WL Waldron
- WL Waldron
- WL Waldron
- WL Waldron
- WM Neupert
- Y Nazé
- Y Nazé
- Y Nazé
- Y Nazé
- Y Nazé
- Y Nazé
- Y Nazé
- Y Sugawara
- Y Tsuboi
- Yaël Nazé
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2009
- Field of study
(abridged) Non-degenerate stars of essentially all spectral classes are soft
X-ray sources. Low-mass stars on the cooler part of the main sequence and their
pre-main sequence predecessors define the dominant stellar population in the
galaxy by number. Their X-ray spectra are reminiscent, in the broadest sense,
of X-ray spectra from the solar corona. X-ray emission from cool stars is
indeed ascribed to magnetically trapped hot gas analogous to the solar coronal
plasma. Coronal structure, its thermal stratification and geometric extent can
be interpreted based on various spectral diagnostics. New features have been
identified in pre-main sequence stars; some of these may be related to
accretion shocks on the stellar surface, fluorescence on circumstellar disks
due to X-ray irradiation, or shock heating in stellar outflows. Massive, hot
stars clearly dominate the interaction with the galactic interstellar medium:
they are the main sources of ionizing radiation, mechanical energy and chemical
enrichment in galaxies. High-energy emission permits to probe some of the most
important processes at work in these stars, and put constraints on their most
peculiar feature: the stellar wind. Here, we review recent advances in our
understanding of cool and hot stars through the study of X-ray spectra, in
particular high-resolution spectra now available from XMM-Newton and Chandra.
We address issues related to coronal structure, flares, the composition of
coronal plasma, X-ray production in accretion streams and outflows, X-rays from
single OB-type stars, massive binaries, magnetic hot objects and evolved WR
stars.Comment: accepted for Astron. Astrophys. Rev., 98 journal pages, 30 figures
(partly multiple); some corrections made after proof stag
Search for Kaluza-Klein Graviton Emission in ppˉ Collisions at s=1.8 TeV using the Missing Energy Signature
- Author
- Acosta D
- Affolder T
- Akimoto H
- Albrow MG
- Ambrose D
- Amidei D
- Anikeev K
- Antos J
- Apollinari G
- Arisawa T
- Artikov A
- Asakawa T
- Ashmanskas W
- Azfar F
- Azzi-Bacchetta P
- Bacchetta N
- Bachacou H
- Badgett W
- Bailey S
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Baroiant S
- Barone M
- Bauer G
- Bedeschi F
- Behari S
- Belforte S
- Bell WH
- Bellettini G
- Bellinger J
- Benjamin D
- Bensinger J
- Beretvas A
- Berryhill J
- Bhatti A
- Binkley M
- Bisello D
- Bishai M
- Blair RE
- Blocker C
- Bloom K
- Blumenfeld B
- Blusk SR
- Bocci A
- Bodek A
- Bolla G
- Bolshov A
- Bonushkin Y
- Bortoletto D
- Boudreau J
- Brandl A
- Bromberg C
- Brozovic M
- Brubaker E
- Bruner N
- Budagov J
- Budd HS
- Burkett K
- Busetto G
- Byrum KL
- Cabrera S
- Calafiura P
- Campbell M
- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
- Castro A
- Cauz D
- Cecco SD
- Cerri A
- Cerrito L
- Chan AW
- Chang PS
- Chang PT
- Chapman J
- Chen C
- Chen YC
- Cheng MT
- Chertok M
- Chiarelli G
- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
- Christofek L
- Chu ML
- Chung JY
- Chung WH
- Chung YS
- Ciobanu CI
- Clark AG
- Coca M
- Connolly A
- Convery M
- Conway J
- Cordelli M
- Cranshaw J
- Culbertson R
- D'Auria S
- D'Onofrio M
- da Costa JG
- Dagenhart D
- de Barbaro P
- de Troconiz JF
- de Troconiz JF
- DeJongh F
- Dell'Agnello S
- Dell'Orso M
- Demers S
- Demortier L
- Deninno M
- Denis RS
- Derwent PF
- Devlin T
- Dionisi C
- Dittmann JR
- Dominguez A
- Donati S
- Dorigo T
- Eddy N
- Einsweiler K
- Engels E
- Erbacher R
- Errede D
- Errede S
- Eusebi R
- Fan Q
- Farrington S
- Feild RG
- Fernandez JP
- Ferretti C
- Field RD
- Fiori I
- Flaugher B
- Flores-Castillo LR
- Foster GW
- Franklin M
- Freeman J
- Friedman J
- Fukui Y
- Furic I
- Galeotti S
- Gallas A
- Gallinaro M
- Gao T
- Garcia-Sciveres M
- Garfinkel AF
- Gatti P
- Gay C
- Gerdes DW
- Gerstein E
- Giagu S
- Giannetti P
- Giolo K
- Giordani M
- Giromini P
- Glagolev V
- Glenzinski D
- Gold M
- Goldschmidt N
- Goldstein J
- Gomez G
- Goncharov M
- Gorelov I
- Goshaw AT
- Gotra Y
- Goulianos K
- Green C
- Greene MG
- Gresele A
- Grim G
- Grosso-Pilcher C
- Guenther M
- Guillian G
- Haas RM
- Haber C
- Hahn SR
- Halkiadakis E
- Hall C
- Handa T
- Handler R
- Happacher F
- Hara K
- Hardman AD
- Harris RM
- Hartmann F
- Hatakeyama K
- Hauser J
- Heinrich J
- Heiss A
- Hennecke M
- Herndon M
- Hill C
- Hocker A
- Hoffman KD
- Hollebeek R
- Holloway L
- Hou S
- Huffman BT
- Hughes R
- Huston J
- Huth J
- Ikeda H
- Incandela J
- Introzzi G
- Iori M
- Issever C
- Ivanov A
- Iwai J
- Iwata Y
- Iyutin B
- James E
- Jones M
- Joshi U
- Kambara H
- Kamon T
- Kaneko T
- Kang J
- Karr K
- Kartal S
- Kasha H
- Kato Y
- Keaffaber TA
- Kelley K
- Kelly M
- Kennedy RD
- Kephart R
- Khazins D
- Kikuchi T
- Kilminster B
- Kim BJ
- Kim DH
- Kim HS
- Kim MJ
- Kim SB
- Kim SH
- Kim TH
- Kim YK
- Kirby M
- Kirk M
- Kirsch L
- Klimenko S
- Koehn P
- Kondo K
- Konigsberg J
- Korn A
- Korytov A
- Kostritskiy AV
- Kotcher J
- Kotelnikov K
- Kothari B
- Kotwal AV
- Kovacs E
- Kovacs E
- Kozelov AV
- Kozlovsky EA
- Krane J
- Krishnaswamy MR
- Krivkova P
- Kroll J
- Kroll J
- Kruse M
- Kruse M
- Krutelyov V
- Krutelyov V
- Krzywdzinski S
- Kubantsev M
- Kuhlmann SE
- Kuhlmann SE
- Kuleshov S
- Kulik Y
- Kunori S
- Kupco A
- Kurino K
- Kurino K
- Kuwabara T
- Kuwabara T
- Kuznetsov VE
- Kuznetsova N
- Kuznetsova N
- Laasanen AT
- Laasanen AT
- Lai N
- Lai N
- Lami S
- Lami S
- Lammel S
- Lammel S
- Lamoureux JI
- Lancaster J
- Lancaster J
- Lancaster M
- Lancaster M
- Lander R
- Lander R
- Landsberg G
- Lannon K
- Lannon K
- Lath A
- Lath A
- Latino G
- Latino G
- Le Y
- Le Y
- LeCompte T
- LeCompte T
- Lee AM
- Lee J
- Lee J
- Lee K
- Lee SW
- Lee SW
- Lee WM
- Leflat A
- Lehner F
- Leonardo N
- Leonardo N
- Leone S
- Leone S
- Leonidopoulos C
- Lewis JD
- Lewis JD
- Li J
- Li K
- Li K
- Li QZ
- Lima JGR
- Lin CS
- Lin CS
- Lincoln D
- Lindgren M
- Lindgren M
- Linn SL
- Linnemann J
- Lipton R
- Liss TM
- Liss TM
- Litvintsev DO
- Litvintsev DO
- Liu JB
- Liu JB
- Liu T
- Liu T
- Liu YC
- Liu YC
- Lobban O
- Lockyer NS
- Lockyer NS
- Loginov A
- Loginov A
- Loken J
- Loken J
- Loreti M
- Loreti M
- Lucchesi D
- Lucchesi D
- Lueking L
- Lukens P
- Lukens P
- Lundstedt C
- Luo C
- Lusin S
- Lusin S
- Lyons L
- Lyons L
- Lys J
- Lys J
- Maciel AKA
- Madaras RJ
- Madrak R
- Madrak R
- Maeshima K
- Maeshima K
- Maksimovic P
- Maksimovic P
- Malferrari L
- Malferrari L
- Malyshev VL
- Manankov V
- Manca G
- Manca G
- Mangano M
- Mangano M
- Mao HS
- Mariotti M
- Mariotti M
- Marshall T
- Martignon G
- Martignon G
- Martin A
- Martin A
- Martin M
- Martin M
- Martin MI
- Martin V
- Martin V
- Martinez M
- Martinez M
- Matthews JAJ
- Matthews JAJ
- Mattingly SEK
- Mayer J
- Mayorov AA
- Mazzanti P
- Mazzanti P
- McCarthy R
- McFarland KS
- McFarland KS
- McIntyre P
- McIntyre P
- McKigney E
- McMahon T
- Melanson HL
- Melnitchouk A
- Menguzzato M
- Menguzzato M
- Menzione A
- Menzione A
- Merkel P
- Merkel P
- Merkin M
- Merritt KW
- Mesropian C
- Mesropian C
- Meyer A
- Meyer A
- Miao C
- Miao T
- Miao T
- Miettinen H
- Mihalcea D
- Miller JS
- Miller JS
- Miller R
- Miller R
- Minato H
- Minato H
- Miscetti S
- Miscetti S
- Mishina M
- Mishina M
- Mitselmakher G
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- Miyazaki Y
- Moggi N
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- Mokhov N
- Mondal NK
- Montgomery HE
- Moore E
- Moore E
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- Moore R
- Moore RW
- Morita Y
- Morita Y
- Moulik T
- Moulik T
- Mukherjee A
- Mukherjee A
- Mulhearn M
- Mulhearn M
- Muller T
- Muller T
- Munar A
- Munar A
- Murat P
- Murat P
- Murgia S
- Murgia S
- Musy M
- Mutaf YD
- Nachtman J
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- Nagaslaev V
- Nagy E
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- Napora R
- Napora R
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- Narasimham VS
- Naumann NA
- Neal HA
- Neal HKorytov A
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- Nelson C
- Nelson C
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- Neu C
- Neu C
- Neubauer MS
- Neubauer MS
- Neuberger D
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- Newman-Holmes C
- Newman-Holmes C
- Ngan CYP
- Ngan CYP
- Nicolaidi P
- Niell F
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- Nigmanov T
- Nigmanov T
- Niu H
- Niu H
- Nodulman L
- Nodulman L
- Nomerotski A
- Nomerotski A
- Nunnemann T
- O'Neil D
- Oguri V
- Oh SH
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- Oh YD
- Oh YD
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- Ohmoto T
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- Pagliarone C
- Palmonari F
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- Pan Y
- Paoletti R
- Paoletti R
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- Pappas SP
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- Yao W
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- Zsenei A
- Zucchelli Spatra AK
- Zucchelli Sychev D
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2004
- Field of study
We report on a search for direct Kaluza-Klein graviton production in a data
sample of 84 pb−1 of \ppb collisions at s = 1.8 TeV, recorded
by the Collider Detector at Fermilab. We investigate the final state of large
missing transverse energy and one or two high energy jets. We compare the data
with the predictions from a 3+1+n-dimensional Kaluza-Klein scenario in which
gravity becomes strong at the TeV scale. At 95% confidence level (C.L.) for
n=2, 4, and 6 we exclude an effective Planck scale below 1.0, 0.77, and 0.71
TeV, respectively.Comment: Submitted to PRL, 7 pages 4 figures/Revision includes 5 figure
Measurement of the average time-integrated mixing probability of b-flavored hadrons produced at the Tevatron
- Author
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- Affolder T
- Akimoto H
- Albrow MG
- Ambrose D
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- Bishai M
- Blair RE
- Blocker C
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- Blusk SR
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- Bodek A
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- Chirikov-Zorin I
- Chlachidze G
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- Christofek L
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- Landsberg G
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- Lockyer NS
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- Mayorov AA
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- McKigney E
- McMahon T
- Melanson HL
- Melnitchouk A
- Menguzzato M
- Menguzzato M
- Menzione A
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- Merkel P
- Merkel P
- Merkin M
- Merritt KW
- Mesropian C
- Mesropian C
- Meyer A
- Meyer A
- Miao C
- Miao T
- Miao T
- Miettinen H
- Mihalcea D
- Miller JS
- Miller JS
- Miller R
- Miller R
- Minato H
- Minato H
- Miscetti S
- Miscetti S
- Mishina M
- Mishina M
- Mitselmakher G
- Mitselmakher G
- Miyazaki Y
- Moggi N
- Moggi N
- Mokhov N
- Mondal NK
- Montgomery HE
- Moore E
- Moore E
- Moore R
- Moore R
- Moore RW
- Morita Y
- Morita Y
- Moulik T
- Moulik T
- Mukherjee A
- Mukherjee A
- Mulhearn M
- Mulhearn M
- Muller T
- Muller T
- Munar A
- Munar A
- Murat P
- Murat P
- Murgia S
- Murgia S
- Musy M
- Mutaf YD
- Nachtman J
- Nachtman J
- Nagaslaev V
- Nagy E
- Nahn S
- Nahn S
- Nakada H
- Nakada H
- Nakano I
- Nakano I
- Nakaya T
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- Narain M
- Narasimham VS
- Naumann NA
- Neal HA
- Neal HKorytov A
- Negret JP
- Nelson C
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- Nelson S
- Nelson T
- Nelson T
- Neu C
- Neu C
- Neubauer MS
- Neubauer MS
- Neuberger D
- Neuberger D
- Newman-Holmes C
- Newman-Holmes C
- Ngan CYP
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- Nicolaidi P
- Niell F
- Niell F
- Nigmanov T
- Nigmanov T
- Niu H
- Niu H
- Nodulman L
- Nodulman L
- Nomerotski A
- Nomerotski A
- Nunnemann T
- O'Neil D
- Oguri V
- Oh SH
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- Ohmoto T
- Ohmoto T
- Ohsugi T
- Ohsugi T
- Oishi R
- Oishi R
- Okusawa T
- Okusawa T
- Olsen J
- Olsen J
- Orejudos W
- Orejudos W
- Oshima N
- Padley P
- Pagliarone C
- Pagliarone C
- Palmonari F
- Palmonari F
- Pan Y
- Paoletti R
- Paoletti R
- Papadimitriou V
- Papadimitriou V
- Pappas SP
- Parashar N
- Partos D
- Partos D
- Partridge R
- Parua N
- Patrick J
- Patrick J
- Patwa A
- Pauletta G
- Pauletta G
- Paulini M
- Paulini M
- Pauly T
- Pauly T
- Paus C
- Paus C
- Pellett D
- Pellett D
- Penzo A
- Penzo A
- Pescara L
- Pescara L
- Peters O
- Petroff P
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 08/09/2003
- Field of study
We have measured the number of like-sign (LS) and opposite-sign (OS) lepton
pairs arising from double semileptonic decays of b and bˉ-hadrons,
pair-produced at the Fermilab Tevatron collider. The data samples were
collected with the Collider Detector at Fermilab (CDF) during the 1992-1995
collider run by triggering on the existence of μμ and eμ candidates
in an event. The observed ratio of LS to OS dileptons leads to a measurement of
the average time-integrated mixing probability of all produced b-flavored
hadrons which decay weakly, χˉ=0.152±0.007 (stat.) ±0.011
(syst.), that is significantly larger than the world average χˉ=0.118±0.005.Comment: 47 pages, 10 figures, 15 tables Submitted to Phys. Rev.
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
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- Yamazaki T
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- Yang H
- Yang UK
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- Yanush S
- Yao L
- Yasu Y
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- Ye S
- Yen AL
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- Zeniš T
- Zerwas D
- Zevi Della Porta G
- Zhang D
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivković L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
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
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- 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 neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
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
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- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- 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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