483 research outputs found
Min-max theory, Willmore conjecture and the energy of links
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/12/2013
- Field of study
A new multicompartmental reaction-diffusion modeling method links transient membrane attachment of E. coli MinE to E-ring formation
- Author
- A Minton
- A Szabo
- AD Dupuy
- AV Popov
- AV Popov
- B Huang
- B Treanor
- C Sanford
- CA Gomez-Uribe
- CH Hansen
- CL Woldringh
- CL Woldringh
- CV Rao
- D Fange
- D Greenfield
- D Hall
- D Ramos
- D Ridgway
- D Ridgway
- DA Drew
- DC Clarke
- DM Morris
- DM Raskin
- DM Raskin
- DT Gillespie
- DT Gillespie
- DW Adams
- EN Cytrynbaum
- F Tostevin
- FC Collins
- G Balgi
- G Meacci
- G Meacci
- GF King
- GF King
- GG Szpiro
- H Meinhardt
- H Zhou
- H Zhou
- H Zhou
- J Derr
- J Elf
- J Hattne
- J Lutkenhaus
- J Sung
- JA Dix
- JC Schaff
- JS Zon van
- JV Rodriguez
- K Kruse
- K Takahashi
- K Takahashi
- KC Huang
- L Boulianne
- L Ma
- M Ander
- M Fernandez-Suarez
- M Gibson
- M Howard
- M Howard
- M Loose
- M Smoluchowski von
- Masaru Tomita
- MT Klann
- N Ji
- N Pavin
- P Borowski
- P Rangamani
- RA Kerr
- RJ Ellis
- S Pichoff
- S Schaub
- S Wils
- S Zimmerman
- Satya Nanda Vel Arjunan
- SB Albada van
- SL Rowland
- SNV Arjunan
- SR Neves
- SS Andrews
- T Ideker
- TG Bernhardt
- U Resch-Genger
- Y Shih
- Y Shih
- Y Zhang
- Z Hu
- Z Hu
- Z Hu
- Z Hu
- Publication venue
- Publication date
- 01/01/2009
- Field of study
Many important cellular processes are regulated by reaction-diffusion (RD) of molecules that takes place both in the cytoplasm and on the membrane. To model and analyze such multicompartmental processes, we developed a lattice-based Monte Carlo method, Spatiocyte that supports RD in volume and surface compartments at single molecule resolution. Stochasticity in RD and the excluded volume effect brought by intracellular molecular crowding, both of which can significantly affect RD and thus, cellular processes, are also supported. We verified the method by comparing simulation results of diffusion, irreversible and reversible reactions with the predicted analytical and best available numerical solutions. Moreover, to directly compare the localization patterns of molecules in fluorescence microscopy images with simulation, we devised a visualization method that mimics the microphotography process by showing the trajectory of simulated molecules averaged according to the camera exposure time. In the rod-shaped bacterium _Escherichia coli_, the division site is suppressed at the cell poles by periodic pole-to-pole oscillations of the Min proteins (MinC, MinD and MinE) arising from carefully orchestrated RD in both cytoplasm and membrane compartments. Using Spatiocyte we could model and reproduce the _in vivo_ MinDE localization dynamics by accounting for the established properties of MinE. Our results suggest that the MinE ring, which is essential in preventing polar septation, is largely composed of MinE that is transiently attached to the membrane independently after recruited by MinD. Overall, Spatiocyte allows simulation and visualization of complex spatial and reaction-diffusion mediated cellular processes in volumes and surfaces. As we showed, it can potentially provide mechanistic insights otherwise difficult to obtain experimentally
Sm-Nd age of the fazenda brasileiro gabbro, Bahia, Brazil: example of robust behavior of the Sm-Nd isotopic system under extreme hydrothermal alteration
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aperio Bella L
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce AT
- Arfaoui S
- Arguin JF
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astbury A
- Atkinson M
- ATLAS Collaboration The
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Backus Mayes J
- Badescu E
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
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- Banerjee P
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- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barak L
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- Bardin DY
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- Barreiro Guimarães da Costa J
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- Battaglia A
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- Beemster LJ
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- Benchekroun D
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- Chalupkova I
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- Chekulaev SV
- Chelkov GA
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- Chernyatin V
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- 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 direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
- Author
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- Youssef S
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- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
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- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
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- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou N
- Zhu CG
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zinonos Z
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- 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
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
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- Abulaitia Y
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- Bagiacchi P
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- Bessidskaia O
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- Bloch I
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- Buckley AG
- Buda SI
- Budagov IA
- Buehrer F
- Buescher V
- Bugge L
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- Bulekov O
- Bundock AC
- Burckhart H
- Burdin S
- Burghgrave B
- Burke S
- Burmeister I
- Busato E
- Bussey P
- Bustos ACF
- Buszello CP
- Butler B
- Butler JM
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- Buttar CM
- Butterworth JM
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- Caforio D
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- Calderini G
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- Camillocci ES
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- Caminal Armadans R
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- Castelli A
- Castillo Gimenez V
- Castillo IS
- Castillo LRF
- Castillo LRF
- Castro NF
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- Catmore JR
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- Chalupkova I
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- Chekulaev SV
- Chelkov GA
- Chelstowska MA
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- Chen Y
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- Cheng Y
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- Chernyatin V
- Cheu E
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- Chiarella V
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- Chilingarov A
- Chiodini G
- Chisholm AS
- Chislett RT
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- Chow BKB
- Christidi IA
- Chromek-Burckhart D
- Chu ML
- Chudoba J
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- Coniavitis E
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- Consorti V
- Constantinescu S
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- Cortes-Gonzalez A
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- Costa G
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- Da Costa JGPF
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- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dafinca A
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- Dale O
- Dallaire F
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- De Castro S
- De Cecco S
- de Graat J
- De Groot N
- de Jong P
- De la Taille C
- De la Torre H
- de Lima DEF
- de Lima DEF
- De Lorenzi F
- De Mendizabal JB
- De Nooij L
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
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- Dechenaux B
- Dedovich DV
- Degenhardt J
- Deigaard I
- Del Peso J
- Del Prete T
- Delemontex T
- Deliot F
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- della Porta GZ
- della Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demilly A
- Demirkoz B
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
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- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
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- Di Valentino D
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- Dimitrievska A
- Dingfelder J
- Dionisi C
- Dita P
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- Dittus F
- Djama F
- Djobava T
- do Vale MAB
- Doan TKO
- Dobos D
- Dobson E
- Doglioni C
- Doherty T
- Dohmae T
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- Dolezal Z
- Dolgoshein BA
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- Dotti A
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- Dube S
- Dubreuil E
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- Ducu OA
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- Dudarev A
- Dudziak F
- Duehrssen M
- Dueren M
- Duflot L
- Duguid L
- Dunford M
- Dwuznik M
- Ebke J
- Edson W
- Edwards NC
- Ehrenfeld W
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Moursli A
- El Moursli RC
- Ellert M
- Elles S
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- Elmsheuser J
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- Elsing M
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- Emeliyanov D
- Emeliyanov D
- Enari Y
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- Endner OC
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- Endo M
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- Engelmann R
- Engelmann R
- Erdmann J
- Erdmann J
- Ereditato A
- Ereditato A
- Eriksson D
- Eriksson D
- Ernis G
- Ernis G
- Ernst J
- Ernst J
- Ernst M
- Ernst M
- Ernwein J
- Ernwein J
- Errede D
- Errede D
- Errede S
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- Ertel E
- Ertel E
- Escalier M
- Escalier M
- Esch H
- Esch H
- Escobar C
- Escobar C
- Espinal Curull X
- Espinal Curull X
- Esposito B
- Esposito B
- Etienne F
- Etienne F
- Etienvre AI
- Etienvre AI
- Etzion E
- Etzion E
- Evans H
- Evans H
- Fabbri L
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- Facini G
- Facini G
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- Fajardo LSG
- Fakhrutdinov RM
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- Falciano S
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- Faltova J
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- Fang Y
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- Fanti M
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- Farilla A
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- Farooque T
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- Farrell S
- Farrell S
- Farrington SM
- Farrington SM
- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
- Fassnacht P
- Fassouliotis D
- Fassouliotis D
- Favareto A
- Favareto A
- Fayard L
- Fayard L
- Federic P
- Federic P
- Fedin OL
- Fedin OL
- Fedorko W
- Fedorko W
- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
- Feigl S
- Feligioni L
- Feligioni L
- Feng C
- Feng C
- Feng EJ
- Feng EJ
- Feng H
- Feng H
- Fenyuk AB
- Fenyuk AB
- Fernando W
- Fernando W
- Ferrag S
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- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
- Ferrara V
- Ferrari A
- Ferrari A
- Ferrari P
- Ferrari P
- Ferrari R
- Ferrari R
- Ferrer A
- Ferrer A
- Ferrere D
- Ferrere D
- Ferretti C
- Ferretti C
- Fiascaris M
- Fiascaris M
- Fiedler F
- Fiedler F
- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
- Filthaut F
- Fincke-Keeler M
- Fincke-Keeler M
- Finelli KD
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- Fiolhais MCN
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- Fiorini L
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- Firan A
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- Fischer J
- Fischer J
- Fisher MJ
- Fisher MJ
- Fitzgerald EA
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- Flechl M
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- Fleck I
- Fleck I
- Fleischmann P
- Fleischmann P
- Fleischmann S
- Fleischmann S
- Fletcher G
- Fletcher G
- Fletcher GT
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- Flick T
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- Floderus A
- Floderus A
- Florez Bustos AC
- Flowerdew MJ
- Flowerdew MJ
- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
- Fortin D
- Fournier D
- Fournier D
- Fox H
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- Francavilla P
- Francavilla P
- Franchini M
- Franchini M
- Franchino S
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- Francis D
- Francis D
- Franklin M
- Franklin M
- Franz S
- Franz S
- Fraternali M
- Fraternali M
- Fratin S
- Fratina S
- French ST
- French ST
- Friedrich C
- Friedrich C
- Friedrich F
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- Froidevaux D
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- Frost JA
- Frost JA
- Fukunaga C
- Fukunaga C
- Fulsom BG
- Fulsom BG
- Fuster J
- Fuster J
- Gabaldon C
- Gabaldon C
- Gabizon O
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gadatsch S
- Gadatsch S
- Gadomski S
- Gadomski S
- Gagliardi G
- Gagliardi G
- Gagnon P
- Gagnon P
- Galea C
- Galea C
- Galhardo B
- Galhardo B
- Gallas EJ
- Gallas EJ
- Gallo V
- Gallo V
- Gallop BJ
- Gallop BJ
- Gallus P
- Gallus P
- Galster G
- Galster G
- Gan KK
- Gan KK
- Gandrajula RP
- Gandrajula RP
- Gao J
- Gao YS
- Gao YS
- Gaob J
- Garberson F
- Garberson F
- Garcia Navarro JE
- Garcia Navarro JE
- Garcia BRM
- Garcia C
- Garcia C
- Garcia JAB
- Garcia-Sciveres M
- Garcia-Sciveres M
- Gardner RW
- Gardner RW
- Garelli N
- Garelli N
- Garonne V
- Garonne V
- Garrido MDMC
- Gatti C
- Gatti C
- Gaudio G
- Gaudio G
- Gaur B
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- Gauthier L
- Gauthier L
- Gauzzi P
- Gauzzi P
- Gavrilenko IL
- Gavrilenko IL
- Gay C
- Gay C
- Gaycken G
- Gaycken G
- Gazis EN
- Gazis EN
- Ge P
- Ge P
- Gecse Z
- Gecse Z
- Gee CNP
- Gee CNP
- Geerts DAA
- Geerts DAA
- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
- Gellerstedt K
- Gemme C
- Gemme C
- Gemmell A
- Gemmell A
- Genest MH
- Genest MH
- Gentile S
- Gentile S
- George M
- George M
- George S
- George S
- Gerbaudo D
- Gerbaudo D
- Gershon A
- Gershon A
- Ghazlane H
- Ghazlane H
- Ghodbane N
- Ghodbane N
- Giacobbe B
- Giacobbe B
- Giagu S
- Giagu S
- Giangiobbe V
- Giangiobbe V
- Giannetti P
- Giannetti P
- Gianotti F
- Gianotti F
- Gibbard B
- Gibbard B
- Gibson SM
- Gibson SM
- Gilchriese M
- Gilchriese M
- Gillam TPS
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- Gillberg D
- Gillberg D
- Gillman AR
- Gillman AR
- Gingrich DM
- Gingrich M
- Giokaris N
- Giokaris N
- Giordani MP
- Giordani MP
- Giordano R
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- Giorgi FM
- Giorgi FM
- Giraud PF
- Giraud PF
- Giugni D
- Giugni D
- Giuliani C
- Giuliani C
- Giunta M
- Giunta M
- Gjelsten BK
- Gjelsten BK
- Gkialas I
- Gkialas I
- Gladilin LK
- Gladilin LK
- Glasman C
- Glasman C
- Glatzer J
- Glatzer J
- Glazov A
- Glazov A
- Glonti GL
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- Goblirsch-Kolb M
- Goblirsch-Kolb M
- Goddard JR
- Goddard JR
- Godfrey J
- Godfrey J
- Godlewski J
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- Goeringer C
- Goeringer C
- Goessling C
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- Goldfarb S
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- Golubkov D
- Golubkov D
- Gomes A
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- Gonalo R
- Goncalo R
- Gonella L
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- Gonzalez de la Hoz S
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- Gonzalez Parra G
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- Gonzalez BA
- Gonzalez-Sevilla S
- Gonzalez-Sevilla S
- Goossens L
- Goossens L
- Gorbounov PA
- Gorbounov PA
- Gordon HA
- Gordon HA
- Gorelov I
- Gorelov I
- Gorini B
- Gorini B
- Gorini E
- Gorini E
- Gorisek A
- Gorisek A
- Gornicki E
- Gornicki E
- Goshaw AT
- Goshaw AT
- Gostkin MI
- Gostkin MI
- Gouighri M
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- Goujdami D
- Goujdami D
- Goulette MP
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- Goussiou AG
- Goussiou AG
- Goy C
- Goy C
- Gozpinar S
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- Grabas HMX
- Grabas HMX
- Graber L
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- Grabowska-Bold I
- Grafstroem P
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- Gramling J
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- Grancagnolo F
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- Grancagnoloa F
- Grassi V
- Grassi V
- Gratchev V
- Gratchev V
- Gray HM
- Gray HM
- Graziani E
- Graziani E
- Grebenyuk OG
- Grebenyuk OG
- Greenwood ZD
- Greenwood ZD
- Gregersen K
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- Griffiths J
- Griffiths J
- Grillo AA
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- Grimm K
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- Grishkevich YV
- Griso SP
- Grivaz J-F
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- Grohs JP
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- Grohsjean A
- Gross AGE
- Gross E
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
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- Rosenthal O
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- Rossi LP
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- Royon CR
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- Rozen Y
- Ruan X
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- Rubinskiy I
- Rud VI
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- Rudolph MS
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- Rurikova Z
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- Ruschke A
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- Schorlemmer ALS
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- Schramm S
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- Schroeder TV
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- Schultz-Coulon H-C
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- Schune P
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- Schwartzman A
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- Sekula SJ
- Selbach KE
- Seliverstov DM
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- Serfon C
- Serin L
- Serkin L
- Serre T
- Seuster R
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shamim M
- Shan LY
- Shang R
- Shank JT
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- Shatalov PB
- Shaw K
- Shehu CY
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shiyakova M
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- Shochet MJ
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- Sinev NB
- Sipica V
- Siragusa G
- Sircar A
- Sisakyan AN
- Sivoklokov SY
- Sjoelin J
- Sjursen TB
- Skottowe HP
- Skovpen KY
- Skubic P
- Slater M
- Slavicek T
- Sliwa K
- Smakhtin V
- Smart BH
- Smestad L
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith KM
- Smizanska M
- Smolek K
- Snesarev AA
- Snidero G
- Snyder S
- Sobie R
- Socher F
- Soffer A
- Soh DA
- Solans CA
- Solar M
- Solc J
- Soldatov EY
- Soldevila U
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Song HY
- Soni N
- Sood A
- Sopczak A
- Sopko B
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- Sorin V
- Sosebee M
- Soualah R
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- Soukharev AM
- South D
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- Spreitzer T
- Spurlock B
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- Staerz S
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- Stamen R
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- Stanecka E
- Stanek RW
- Stanescu C
- Stanescu-Bellu M
- Stanitzki MM
- Stapnes S
- Starchenko EA
- Stark J
- Staroba P
- Starovoitov P
- Staszewski R
- Stavina P
- Steinberg P
- Stelzer B
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- Stelzer-Chilton O
- Stenzel H
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- Stonjek S
- Stradling AR
- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strandlie A
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- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Styles NA
- Su D
- Su J
- Subramaniam R
- Succurro A
- Sugaya Y
- Suhr C
- Suk M
- Sulin VV
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki Y
- Svatos M
- Swedish S
- Swiatlowski M
- Sykora I
- Sykora T
- Ta D
- Taccini C
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Taiblum N
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tam JYC
- Tan KG
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanasijczuk AJ
- Tannenwald BB
- Tannoury N
- Tapprogge S
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
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- Tashiro T
- Tassi E
- Tayalati Y
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- Teoh JJ
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- Terzo S
- Testa M
- Teuscher RJ
- Therhaag J
- Theveneaux-Pelzer T
- Thomas JP
- Thomas-Wilsker J
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thompson RJ
- Thomsen LA
- Thomson E
- Thomson M
- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
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- Tisserant S
- Todorov T
- Todorova-Nova S
- Toggerson B
- Tojo J
- Tokar S
- Tokushuku K
- Tollefson K
- Tolley E
- Tomlinson L
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- Trigger IM
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- Tripiana MF
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- Trocme B
- Troncon C
- Trottier-McDonald M
- Trovatelli M
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- Trzebinski M
- Trzupek A
- Tsarouchas C
- Tseng JC-L
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman I
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tudorache A
- Tudorache V
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turecek D
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Uchida K
- Ueda I
- Ueno R
- Ughetto M
- Ugland M
- Uhlenbrock M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Unverdorben C
- Urbaniec D
- Urquijo P
- Usai G
- Usanova A
- Vacavant L
- Vacek V
- Vachon B
- Valencic N
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Vallecorsa S
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- Van Der Deijl PC
- van der Geer R
- van der Graaf H
- Van Der Leeuw R
- van der Ster D
- Van Eldik N
- Van Gemmeren P
- van Huysduynen LH
- Van Nieuwkoop J
- van Vulpen I
- Van Woerden MC
- Vanadia M
- Vandelli W
- Vanguri R
- Vaniachine A
- Vankov P
- Vannucci F
- Vaque FV
- Vardanyan G
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vazeille F
- Vazquez JGP
- Veatch J
- Veloso F
- Velz T
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Verzini MJA
- Vest A
- Vetterli MC
- Viazlo O
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigne R
- Villa M
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Virzi J
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vokac P
- Volpi G
- Volpi M
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuanh T
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahlberg H
- Wahrmund S
- Wakabayashi J
- Walder J
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- Walkowiak W
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- Walls FMG
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- Wanotayaroj C
- Warburton A
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- Washbrook A
- Wasicki C
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- Weber MS
- Weber SW
- Webster JS
- Weidberg AR
- Weigell P
- Weinert B
- Weingarten J
- Weiser C
- Weits H
- Wells PS
- Wemans ADV
- Wenaus T
- Wendland D
- Weng Z
- Wengler T
- Wenig S
- Wermes N
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- Werner P
- Wessels M
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- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilkens HG
- Will JZ
- Williams HH
- Williams S
- Willis C
- Willocq S
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- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winter BT
- Wittgen M
- Wittig T
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KHY
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wright M
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wyatt TR
- Wynne BM
- Xella S
- Xiao M
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yakabe R
- Yamada M
- Yamaguchi H
- Yamaguchi Y
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yanush S
- Yao L
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- 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
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
In Vitro Surfactant Structure-Toxicity Relationships: Implications for Surfactant Use in Sexually Transmitted Infection Prophylaxis and Contraception
- Author
- A Patrzykat
- A Perani
- A Stone
- B Liu
- B Simoncic
- BG Carpo
- BH Honig
- BJ Catalone
- BM Neves
- C Butor
- C Masurier
- C Tanford
- CH Spink
- D Perez Bercoff
- DB Vieira
- Dimas Tadeu Covas
- DM Phillips
- DM Zhu
- DP Wilson
- F Hladik
- F Hladik
- F Kopecky
- F Terris-Prestholt
- FC Krebs
- FC Krebs
- G Girolomoni
- G Velarde
- HS Ved
- J Kreiss
- J Nuttall
- J Piao
- J Ramalho-Santos
- J Stephenson
- JD Irvine
- JL Sampaio
- João Ramalho-Santos
- K Ekelund
- K Simons
- Katia A. Mesquita
- L Ackermann
- L Peterson
- LMBB Estronca
- M Aranzazu Partearroyo
- M Burns
- M Rescigno
- Marta Baptista
- MJ Moreno
- MK Dymond
- MSC Abreu
- N Ayotte
- Otília V. Vieira
- OV Vieira
- PJ Feldblum
- PJ Hitchcock
- PM Mesquita
- R Enomoto
- RA Cone
- RB Gennis
- RE Roddy
- RM Brito
- RN Fichorova
- RS Dias
- SS Seefeldt
- SZ Knezevic
- V Miller
- Winchil L. C. Vaz
- YC Lin
- Ângela S. Inácio
- Publication venue
- Public Library of Science
- Publication date
- 16/05/2011
- Field of study
Background
The need for woman-controlled, cheap, safe, effective, easy-to-use and easy-to-store topical applications for prophylaxis against sexually transmitted infections (STIs) makes surfactant-containing formulations an interesting option that requires a more fundamental knowledge concerning surfactant toxicology and structure-activity relationships.
Methodology/Principal Findings
We report in vitro effects of surfactant concentration, exposure time and structure on the viability of mammalian cell types typically encountered in the vagina, namely, fully polarized and confluent epithelial cells, confluent but non-polarized epithelial-like cells, dendritic cells, and human sperm. Representatives of the different families of commercially available surfactants – nonionic (Triton X-100 and monolaurin), zwitterionic (DDPS), anionic (SDS), and cationic (CnTAB (n = 10 to 16), C12PB, and C12BZK) – were examined. Triton X-100, monolaurin, DDPS and SDS were toxic to all cell types at concentrations around their critical micelle concentration (CMC) suggesting a non-selective mode of action involving cell membrane destabilization and/or destruction. All cationic surfactants were toxic at concentrations far below their CMC and showed significant differences in their toxicity toward polarized as compared with non-polarized cells. Their toxicity was also dependent on the chemical nature of the polar head group. Our results suggest an intracellular locus of action for cationic surfactants and show that their structure-activity relationships could be profitably exploited for STI prophylaxis in vaginal gel formulations. The therapeutic indices comparing polarized epithelial cell toxicity to sperm toxicity for all surfactants examined, except C12PB and C12BZK, does not justify their use as contraceptive agents. C12PB and C12BZK are shown to have a narrow therapeutic index recommending caution in their use in contraceptive formulations.
Conclusions/Significance
Our results contribute to understanding the mechanisms involved in surfactant toxicity, have a predictive value with regard to their safety, and may be used to design more effective and less harmful surfactants for use in topical applications for STI prophylaxis.Foundation for Science and
Technology of the Portuguese Ministry of Science and Higher Educatio
Photodynamic Antimicrobial Chemotherapy in Aquaculture: Photoinactivation Studies of Vibrio fischeri
- Author
- A Tavares
- Adelaide Almeida
- AE O'Connor
- AE Toranzo
- AJ Acher
- APJ Maestrin
- Augusto C. Tomé
- C Carvalho
- CMB Carvalho
- CML West
- D Halet
- DJW Moriarty
- DJW Moriarty
- E Alves
- Eliana Alves
- F Gábor
- FC Cabello
- G Bertoloni
- G Carvalho
- G Jori
- G Klein
- GD Lio-Po
- J Romalde
- JA Olafsen
- José A. S. Cavaleiro
- João P. C. Tomé
- JPC Tomé
- K Muroga
- L Costa
- M Jemli
- M Magaraggia
- M-A Ortner
- Maria A. F. Faustino
- Maria G. P. M. S. Neves
- Mark Alexander Webber
- MM Shivu
- Newton C. M. Gomes
- O Vadstein
- PA Reed
- R Bonnett
- R Prates
- R Rotomskis
- RJ Watts
- S Arijo
- T Defoirdt
- T Defoirdt
- T Defoirdt
- T Maisch
- T Smits
- Z Alouini
- ZJ Shao
- Ângela Cunha
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
BACKGROUND: Photodynamic antimicrobial chemotherapy (PACT) combines light, a light-absorbing molecule that initiates a photochemical or photophysical reaction, and oxygen. The combined action of these three components originates reactive oxygen species that lead to microorganisms' destruction. The aim was to evaluate the efficiency of PACT on Vibrio fischeri: 1) with buffer solution, varying temperature, pH, salinity and oxygen concentration values; 2) with aquaculture water, to reproduce photoinactivation (PI) conditions in situ. METHODOLOGY/PRINCIPAL FINDINGS: To monitor the PI kinetics, the bioluminescence of V. fischeri was measured during the experiments. A tricationic meso-substituted porphyrin (Tri-Py(+)-Me-PF) was used as photosensitizer (5 µM in the studies with buffer solution and 10-50 µM in the studies with aquaculture water); artificial white light (4 mW cm(-2)) and solar irradiation (40 mW cm(-2)) were used as light sources; and the bacterial concentration used for all experiments was ≈10(7) CFU mL(-1) (corresponding to a bioluminescence level of 10(5) relative light units--RLU). The variations in pH (6.5-8.5), temperature (10-25°C), salinity (20-40 g L(-1)) and oxygen concentration did not significantly affect the PI of V. fischeri, once in all tested conditions the bioluminescent signal decreased to the detection limit of the method (≈7 log reduction). The assays using aquaculture water showed that the efficiency of the process is affected by the suspended matter. Total PI of V. fischeri in aquaculture water was achieved under solar light in the presence of 20 µM of Tri-Py(+)-Me-PF. CONCLUSIONS/SIGNIFICANCE: If PACT is to be used in environmental applications, the matrix containing target microbial communities should be previously characterized in order to establish an efficient protocol having into account the photosensitizer concentration, the light source and the total light dose delivered. The possibility of using solar light in PACT to treat aquaculture water makes this technology cost-effective and attractive
Progression to microalbuminuria in patients with type 1 diabetes: a seven-year prospective study
- Author
- American Diabetes Association
- AS Krolewski
- B Barone
- BA Coonrod
- BA Perkins
- BA Perkins
- Bráulio Santos
- CE Mogensen
- CG Schalkwijk
- Diabetes Epidemiology Research International Mortality Study Group
- ER Mathiesen
- ES Kilpatrick
- FC Parra
- G Penno
- G Roglic
- IH de Boer
- J Tuomilehto
- J Tuomilehto
- JL Gross
- JQ Purnell
- L Perségol
- LM Thorn
- MAL Gabbay
- Marilia B Gomes
- MB Gomes
- MB Gomes
- MC Thomas
- ME Cooper
- ME Molitch
- ML Stone
- N Chaturvedi
- N Chatuverdi
- N Tolonen
- P Hovind
- P Rossing
- Pedro CB da Silva
- Ricardo Neves
- Roberta A Cobas
- S Giunti
- SD Sibley
- SH Castro
- The Diabetes Control and Complications Trial Research Study Group (DCCT)
- TJ Orchard
- Writing team for the Diabetes control and complications trial/Epidemiology of diabetes interventions and complications research group
- WT Friedewald
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>The presence of microalbuminuria can be associated with overt nephropathy and cardiovascular disease in patients with type 1 diabetes (T1D). We aimed to determine the incidence and evaluate the baseline predictors for the development of microalbuminuria in patients with T1D.</p> <p>Methods</p> <p>This study is a longitudinal cohort study of 122 normoalbuminuric patients with T1D who were receiving routine clinical care at baseline. A detailed medical history was taken, and a physical examination was performed at baseline. All of the patients were regularly examined for diabetes-associated complications. An analysis of predictors was performed using the Cox regression.</p> <p>Results</p> <p>Over 6.81 (3.59-9.75) years of follow-up, 50 (41%) of the patients developed microalbuminuria. The incidence density was 6.79/100 people per year (95% CI 5.04-8.95), and the microalbuminuria developed after 5.9 (2.44-7.76) and 11 (5-15) years of follow-up and diabetes duration, respectively. After an individual Cox regression, the baseline variables associated with the development of microalbuminuria were age, age at diagnosis, duration of diabetes, systolic and diastolic blood pressure, fasting glycemia, body mass index (BMI), total cholesterol and triglycerides levels, cholesterol/HDL ratio and a family history of type 2 diabetes.After a multivariate Cox regression, the only independent factors associated with the development of microalbuminuria were BMI [HR 1.12 (1.03-1.21)] and cholesterol/HDL ratio [HR 1.32 (1.05-1.67)].</p> <p>Conclusions</p> <p>A higher BMI and cholesterol/HDL ratio increased the risk of developing microalbuminuria in young patients with T1D after a short follow-up. Both risk factors are modifiable and should be identified early and followed closely.</p
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