43 research outputs found
Diabetes and lipid screening among patients in primary care: A cohort study
- Author
- Publication venue
- BioMed Central
- Publication date
- 01/01/2008
- Field of study
<p>Abstract</p> <p>Background</p> <p>Obesity is associated with increased cardiovascular diseases and diabetes mellitus. Guidelines call for intensified glucose and lipid screening among overweight and obese patients. Data on compliance with these guidelines are scarce. The purpose of this study was to assess rates of diabetes and lipid screening in primary care according to demographic variables and weight status.</p> <p>Methods</p> <p>Over a 3-year follow-up period, we assessed screening rates for blood glucose, triglycerides, and HDL- and LDL-cholesterol among 5025 patients in primary care. From proportional hazards models we estimated screening rates among low, moderate, high, and very-high risk patients and compared them with recommendations of the American Diabetes Association (ADA), National Cholesterol Education Program (ATP III) and U.S. Preventive Services Task Force (USPSTF).</p> <p>Results</p> <p>Mean (SD) age was 47.4 (15.6); 69% were female, 21% were non-white, and 30% of males and 25% of females were obese (BMI ≥ 30 kg/m<sup>2</sup>). For both diabetes and lipid screening, the adjusted hazard was 260–330% higher among ≥65 than <35 year-olds, 50–90% higher in persons with BMI ≥ 35 than <25 kg/m<sup>2</sup>, 10–30% lower for females than males, and not lower among racial/ethnic minorities. Screening rates were at least 80% among very-high risk persons, which we defined as 55–64 years old, BMI ≥ 35 kg/m<sup>2</sup>, non-white, with baseline hypertension. In contrast, high-risk persons who were younger (35–44 years old) and less obese (BMI 30–<35 kg/m<sup>2</sup>) were screened less often (43% for LDL-cholesterol among females to 83% for diabetes among males) even though ADA, ATP III and USPSTF recommend diabetes and lipid screening among them.</p> <p>Conclusion</p> <p>Patients with higher BMI or age were more likely to be screened for cardiometabolic risk factors. Women were screened at lower rates than men. Even in a highly structured medical group practice, some obese patients were under-screened for diabetes and dyslipidemia.</p
Exploring the Conformational Transitions of Biomolecular Systems Using a Simple Two-State Anisotropic Network Model
- Author
- A Atilgan
- A Laio
- A Thomas
- A Yamashita
- AC Pan
- AD Schuyler
- AD Schuyler
- Avisek Das
- Benoît Roux
- Bert L. de Groot
- BW Zhang
- C Dellago
- C Müller
- C Toyoshima
- C Toyoshima
- C Toyoshima
- CW Müller
- D Bhatt
- D Bhatt
- D Chandler
- D Hamelberg
- D Seeliger
- D Yernool
- DE Shaw
- DL Winters
- DM Krger
- DM Zuckerman
- E Zomot
- F Tama
- F Zhu
- G Huber
- G Verdon
- H Abe
- H Grubmüller
- H Krishnamurthy
- H Vashisth
- H Vashisth
- I Bahar
- I Bahar
- I Bahar
- I Bahar
- IH Shrivastava
- Ivet Bahar
- J Franklin
- J Jiang
- JB Brokaw
- JJ Lacroix
- JL Adelman
- JR Perilla
- JW Chu
- K Arora
- KA Henzler-Wildman
- L Maragliano
- LM Espinoza-Fonseca
- M Gur
- M Gur
- M Lei
- M Tekpinar
- Mary Hongying Cheng
- MD Daily
- MD Daily
- Mert Gur
- MH Cheng
- MK Kim
- MK Kim
- MK Kim
- MM Tirion
- N Gō
- N Kantarci-Carsibasi
- N Reuter
- N Reyes
- O Beckstein
- O Miyashita
- P Maragakis
- P Sfriso
- PC Whitford
- PC Whitford
- PG Bolhuis
- R Elber
- R Elber
- RB Best
- S Jo
- S Kirmizialtin
- S Yang
- ST Stober
- Sunhwan Jo
- T Haliloglu
- TB Woolf
- TLM Sorensen
- TR Lezon
- V Ovchinnikov
- W E
- W Gan
- W Zheng
- WN Du
- Y Matsunaga
- Z Yang
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2014
- Field of study
Biomolecular conformational transitions are essential to biological functions. Most experimental methods report on the long-lived functional states of biomolecules, but information about the transition pathways between these stable states is generally scarce. Such transitions involve short-lived conformational states that are difficult to detect experimentally. For this reason, computational methods are needed to produce plausible hypothetical transition pathways that can then be probed experimentally. Here we propose a simple and computationally efficient method, called ANMPathway, for constructing a physically reasonable pathway between two endpoints of a conformational transition. We adopt a coarse-grained representation of the protein and construct a two-state potential by combining two elastic network models (ENMs) representative of the experimental structures resolved for the endpoints. The two-state potential has a cusp hypersurface in the configuration space where the energies from both the ENMs are equal. We first search for the minimum energy structure on the cusp hypersurface and then treat it as the transition state. The continuous pathway is subsequently constructed by following the steepest descent energy minimization trajectories starting from the transition state on each side of the cusp hypersurface. Application to several systems of broad biological interest such as adenylate kinase, ATP-driven calcium pump SERCA, leucine transporter and glutamate transporter shows that ANMPathway yields results in good agreement with those from other similar methods and with data obtained from all-atom molecular dynamics simulations, in support of the utility of this simple and efficient approach. Notably the method provides experimentally testable predictions, including the formation of non-native contacts during the transition which we were able to detect in two of the systems we studied. An open-access web server has been created to deliver ANMPathway results. © 2014 Das et al
Jets and energy flow in photon-proton collisions at HERA
- Author
- Aid S.
- Andreev V.
- Andrieu B.
- Appuhn R D.
- Arpagaus M.
- Babaev A.
- Ban Y.
- Baranov P.
- Barrelet E.
- Barschke R.
- Bartel W.
- Barth M.
- Bassler U.
- Beck H P.
- Behrend H J.
- Belousov A.
- Berger C.
- Bernardi G.
- Bernet R.
- Bertrand-Coremans G.
- Besanon M.
- Beyer R.
- Bhr J.
- Biddulph P.
- Bispham P.
- Bizot J C.
- Blobel V.
- Bn J.
- Bngener L.
- Borras K.
- Boudry V.
- Bourov S.
- Braemer A.
- Brasse F.
- Braunschweig W.
- Brger J.
- Brisson V.
- Bruncko D.
- Brune C.
- Bsser F W.
- Buchholz R.
- Buniatian A.
- Burke S.
- Burton M.
- Buschhorn G.
- Campbell A J.
- Carli T.
- Charles F.
- Charlet M.
- Clarke D.
- Clegg A B.
- Contreras J G.
- Cormack C.
- Coughlan J A.
- Courau A.
- Coutures C.
- Cozzika G.
- Criegee L.
- Cussans D G.
- Cvach J.
- Dagoret S.
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- Del Buono L.
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- Dllmann D.
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- Ebert J.
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- Egli S.
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- Eichler R.
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- Erdmann M.
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- Gorelov I.
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- Itterbeck H.
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- Publication venue
- Springer Verlag
- Publication date
- 01/01/1995
- Field of study
Multi-messenger observations of a binary neutron star merger
- Author
- Aab A
- Aartsen MG
- Abbott BP
- Abbott R
- Abbott TD
- Abbott TMC
- Abdalla H
- Abe F
- Abeysekara AU
- Abramo LR
- Abramowski A
- Abreu P
- Acernese F
- Acero F
- Ackermann M
- Ackley K
- Ackley K
- Adams C
- Adams J
- Adams SM
- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Afrough M
- Agarwal B
- Agathos M
- Agatsuma K
- Aggarwal N
- Aglietta M
- Agliozzo C
- Agudo I
- Aguiar OD
- Aguilar JA
- Aharonian F
- Ahlers M
- Ahrens M
- Aiello L
- Ain A
- Ajith P
- Akras S
- Al Samarai I
- Albert A
- Albert A
- Albuquerque IFM
- Albury JM
- Alcaniz JS
- Alexander KD
- Alfaro R
- Alighieri S Di Serego
- Allam S
- Allekotte I
- Allen B
- Allen G
- Allison J
- Allison JR
- Allocca A
- Almela A
- Altin PA
- Altmann D
- Alvarez C
- Alvarez JD
- Alvarez M Dovale
- Alvarez-Muiz J
- Amati L
- Amato A
- An T
- Ananyeva A
- Anastasi GA
- Anchordoqui L
- Andeen K
- Anderson JP
- Anderson SB
- Anderson T
- Anderson WG
- Andrada B
- Andre M
- Andreoni I
- Andreoni I
- Andringa S
- Angelova SV
- Anghinolfi M
- Angner EO
- Angus CR
- Annis J
- Ansseau I
- Antier S
- Anton G
- Antonelli LA
- Antonelli LA
- Anupama GC
- Aoki K
- Aoki W
- Appert S
- Aptekar RL
- Arai K
- Arakawa M
- Aramo C
- Araya MC
- Arcavi I
- Arceo R
- Ardid M
- Areeda JS
- Aresu G
- Argan A
- Argelles C
- Arnaud N
- Array LWA Long Wavelength
- Array MWA Murchison Widefield
- Arrieta M
- Arsene N
- Arteaga-Velzquez JC
- Artola R
- Arun KG
- Asakura Y
- Asaoka Y
- Ascenzi S
- Ashall C
- Ashley MCB
- Ashton G
- Asorey H
- Assis P
- Ast M
- Aston SM
- Astone P
- Atallah DV
- ATLAS
- Atwood WB
- Aubert J-J
- Aubert P
- Aublin J
- Auffenberg J
- Aufmuth P
- Aulbert C
- AultONeal K
- Austin C
- Avgitas T
- Avila G
- Avila-Alvarez A
- Awad A Kuotb
- Axani S
- Baar S
- Babak S
- Bachetti M
- Backes M
- Bacon P
- Bader MKM
- Badescu AM
- Bae S
- Bagherpour H
- Bai X
- Bailes M
- Baker PT
- Balaceanu A
- Balanutsa PV
- Balasubramanian A
- Balbinot E
- Baldaccini F
- Baldini L
- Ballardin G
- Ballmer SW
- Bally J
- Balzer A
- Banagiri S
- Banerji M
- Bannister KW
- Barayoga JC
- Barbarino C
- Barbato F
- Barber AS
- Barbiellini G
- Barbiellini G
- Barclay SE
- Baret B
- Barish BC
- Barker D
- Barkett K
- Barnard M
- Barnes J
- Barone F
- Barr B
- Barrios-Marti J
- Barron JP
- Barsotti L
- Barsuglia M
- Barta D
- Barthelmy SD
- Bartlett J
- Bartos I
- Barway S
- Barway S
- Barwick SW
- Basa S
- Bassiri R
- Basti A
- Bastieri D
- Batch JC
- Bauer FE
- Bauer FE
- Baum V
- Bawaj M
- Bay R
- Bayley JC
- Bazzan M
- Bazzano A
- Bchele M
- Beardmore AP
- Beardsley A
- Beatty JJ
- Becerril A
- Becherini Y
- Bechtol K
- Becker KH
- Becsy B
- Beer C
- Bejger M
- Belahcene I
- Belhorma B
- Bell AS
- Bellazzini R
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- Benoit-Levy A
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- Berisso M Gomez
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- Berry CPL
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- Bertaina ME
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- Bertin V
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- Blair CD
- Blair DG
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- Bloom ED
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- Bond IA
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- Bottacini E
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- Botticella MT
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- Brayeur L
- Breeveld AA
- Bregeon J
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- Brockill P
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- Brown DD
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- Bryan M
- Buchanan CC
- Buchholz P
- Buckley DAH
- Buckley-Geer E
- Budnev NM
- Buehler R
- Bueno A
- Bufano F
- Buffa F
- Buikema A
- Buitink S
- Bulgarelli A
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- Bulik T
- Bulik T
- Bulla M
- Bulten HJ
- Buonanno A
- Burgay M
- Burgess JM
- Burgman A
- Burhonov O
- Burke DL
- Burns E
- Burrows DN
- Buscemi M
- Buskulic D
- Buson S
- Bustillo J Caldern
- Busto J
- Butler NR
- Butler RE
- Buttu M
- Buy C
- Byer RL
- Caballero-Garcia MD
- Caballero-Mora KS
- Caballero-Mora KS
- Cabero M
- Cabral J
- Caccianiga L
- Cadonati L
- Cagnoli G
- Cahillane C
- Callister TA
- Calloni E
- CALTECH GROWTH JAGWAR
- Cameron RA
- Camilo F
- Camp JB
- Campana S
- Camuccio R
- Cancio A
- Canepa M
- Canfora F
- Canizares P
- Cannella C
- Cannizzaro G
- Cannon KC
- Cano Z
- Cao H
- Cao J
- Cao XL
- Capaccioli M
- Capano CD
- Capasso M
- Capistrn T
- Capocasa E
- Capone A
- Capozzi D
- Cappellaro E
- Caputo R
- Caramete L
- Caraveo P
- Caraveo PA
- Carbognani F
- Carboni G
- Cardenas B Vargas
- Cardillo M
- Caria T
- Caride S
- Carlin JL
- Carney MF
- Caroff S
- Carosi A
- Carr J
- Carramiana A
- Carretti E
- Cartier R
- Caruso R
- Carver T
- Casadio C
- Casado A Lopez
- Casanova S
- Casanova S
- Casasola V
- Casella P
- Casentini C
- Casey J
- Casier M
- Castander FJ
- Castangia P
- Castellina A
- Castellon A
- Castellon JL Nilo
- Castillo J Alvarez
- Castillo M
- Castro JM Gonzalez
- Castro ML Diaz
- Castro-Tirado AJ
- Casu S
- Catalani F
- Cataldi G
- Cattaneo PW
- Caudill S
- Cavagli M
- Cavalier F
- Cavalieri R
- Cavazzuti E
- Cazon L
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- Li XB
- Li XF
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- Parmiggiani N
- Parra A
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- Passuello D
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- Pearlstone BL
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- Pike S
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- Piro AL
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- Popolizio P
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- Prado RR
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- Principe G
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- Prodi GA
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- Prokoph H
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- Przybylski GT
- Pulone L
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- Ren Z
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- Reposeur T
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- Riviere C
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- Robie R
- Robinet F
- Rocchi A
- Rochester LS
- Rodi J
- Rodriguez H
- Rojas D Avila
- Rojas-Bravo C
- Rojo J Rodriguez
- Rol E
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- Rollins JG
- Roma VJ
- Romano R
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- Romer AK
- Romero M Dominguez
- Romie JH
- Romoli C
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- Rosell A Carnero
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- Ross MP
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- Rosswog S
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- Ruiz R Gracia
- Ruiz-Velasco E
- Rulten CB
- Rumyantsev VV
- Rusu F
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- Ryckbosch D
- Rykoff ES
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- Sadler EM
- Sadler EM
- Saffe C
- Saffi SJ
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- Sahakian V
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- Saito Y
- Sakamaki A
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- Sakellariadou M
- Sako M
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- Salafia OS
- Salamida F
- Salazar H
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- Saleem M
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- Salvadori I
- Salvaterra R
- Samajdar A
- Sammut L
- Sampedro L
- Sampson LM
- Samtleben DFE
- Sanchez B
- Sanchez DA
- Sanchez E
- Sanchez EJ
- Sanchez F
- Sanchez LE
- Sanchez-Losa A
- Sanchez-Lucas P
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- Sanchis-Gual N
- Sand DJ
- Sandberg V
- Sanders JR
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- Sandrock A
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- Santangelo A
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- Sarazin F
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- Sathyaprakash BS
- Sato R
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- Schmidt BP
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- Schneider A
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- Schoenell W
- Schoenen S
- Schofield RMS
- Scholten O
- Schonbeck A
- Schoneberg S
- Schoorlemmer H
- Schovnek P
- Schreiber E
- Schroder FG
- Schroder S
- Schroder SL
- Schssler F
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- Schulz A
- Schulz A
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- Schwalbe SG
- Schwanke U
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- Sciutto SJ
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- Segreto A
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- Seitenzahl IR
- Sekiguchi Y
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- Sevilla-Noarbe I
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- Shahriar MS
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- Shannon RM
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- Shimizu Y
- Shimomukai R
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- Shoemaker DH
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- Siemens X
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- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ~1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40+8-8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 Mo. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ~40 Mpc) less than 11 hours after the merger by the One- Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transient’s position ~9 and ~16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta
Measurement of the inclusive cross-section for the production of jets in association with a Z boson in proton-proton collisions at 8 TeV using the ATLAS detector
- Author
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- Abbott B
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- Abhayasinghe DK
- Abidi SH
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- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/10/2019
- Field of study
The inclusive cross-section for jet production in association with a Z boson decaying into an electron–positron pair is measured as a function of the transverse momentum and the absolute rapidity of jets using 19.9 fb −1 of s√=8 TeV proton–proton collision data collected with the ATLAS detector at the Large Hadron Collider. The measured Z + jets cross-section is unfolded to the particle level. The cross-section is compared with state-of-the-art Standard Model calculations, including the next-to-leading-order and next-to-next-to-leading-order perturbative QCD calculations, corrected for non-perturbative and QED radiation effects. The results of the measurements cover final-state jets with transverse momenta up to 1 TeV, and show good agreement with fixed-order calculations
Identification and rejection of pile-up jets at high pseudorapidity with the ATLAS detector
- Author
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- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
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- Yildiza H Duran
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- Zieminska
- Zimine NI
- Zimmermann C
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- Zobernig G
- Zoccoli A
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- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
The rejection of forward jets originating from
additional proton–proton interactions (pile-up) is crucial for
a variety of physics analyses at the LHC, including Standard
Model measurements and searches for physics beyond
the Standard Model. The identification of such jets is challenging
due to the lack of track and vertex information in
the pseudorapidity range |η| > 2.5. This paper presents a
novel strategy for forward pile-up jet tagging that exploits
jet shapes and topological jet correlations in pile-up interactions.
Measurements of the per-jet tagging efficiency are
presented using a data set of 3.2 fb−1 of proton–proton collisions
at a centre-of-mass energy of 13 TeV collected with the
ATLAS detector. The fraction of pile-up jets rejected in the
range 2.5 < |η| < 4.5 is estimated in simulated events with
an average of 22 interactions per bunch-crossing. It increases
with jet transverse momentum and, for jets with transverse
momentum between 20 and 50 GeV, it ranges between 49%
and 67% with an efficiency of 85% for selecting hard-scatter
jets. A case study is performed in Higgs boson production
via the vector-boson fusion process, showing that these techniques
mitigate the background growth due to additional
proton–proton interactions, thus enhancing the reach for such
signatures
Measurement of jet fragmentation in Pb+Pb and pp collisions at √SNN = 2.76 TeV with the ATLAS detector at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
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- Abidi SH
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- Ozcan VE
- Ozturk N
- Pachal K
- Pacheco Pages A
- Paganini M
- Paige F
- Pais P
- Palacino G
- Palazzo S
- Palestini S
- Palka M
- Pallin D
- Panagiotopoulou ES
- Panagoulias I
- Pandini CE
- Pani P
- Panitkin S
- Pantea D
- Paolozzi L
- Papadopoulou TD
- Papageorgiou K
- Paramonov A
- Parker AJ
- Parker KA
- Parker MA
- Parodi F
- Parsons JA
- Parzefall U
- Pascuzzi VR
- Pasner JM
- Pasqualucci E
- Passaggio S
- Pastore F
- Pataraia S
- Pater JR
- Pauly T
- Paz IL
- Pearce J
- Pearson B
- Pedraza Lopez S
- Pedro R
- Peleganchuk SV
- Penc O
- Peng C
- Peng H
- Penwell J
- Peralva BS
- Perego MM
- Perepelitsa DV
- Perini L
- Pernegger H
- Perrella S
- Peschke R
- Peshekhonov VD
- Peters K
- Peters RFY
- Petersen BA
- Petersen TC
- Petit E
- Petridis A
- Petridou C
- Petroff P
- Petrolo E
- Petrov M
- Petrucci F
- Pettersson NE
- Peyaud A
- Pezoa R
- Phillips PW
- Piacquadio G
- Pianori E
- Picazio A
- Piccaro E
- Pickering MA
- Piegaia R
- Pilcher JE
- Pilkington AD
- Pin AWJ
- Pinamonti M
- Pinfold JL
- Pino SAO
- Pirumov H
- Pitt M
- Plazak L
- Pleier M-A
- Pleskot V
- Plotnikova E
- Pluth D
- Podberezko P
- Poettgen R
- Poggi R
- Poggioli L
- Pohl D
- Polesello G
- Poley A
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Polychronakos V
- Pommes K
- Ponce JMI
- Ponomarenko D
- Pontecorvo L
- Pope BG
- Popeneciu GA
- Poppleton A
- Pospisil S
- Potamianos K
- Potrap IN
- Potter CJ
- Potter CT
- Poulard G
- Poveda J
- Pralavorio P
- Pranko A
- Prell S
- Price D
- Price LE
- Primavera M
- Prince S
- Proklova N
- Prokofiev K
- Prokoshin F
- Protopopescu S
- Proudfoot J
- Przybycien M
- Puddu D
- Puri A
- Puzo P
- Qian J
- Qin G
- Qin Y
- Quadt A
- Quayle WB
- Queitsch-Maitland M
- Quilty D
- Raddum S
- Radeka V
- Radescu V
- Radhakrishnan SK
- Radloff P
- Rados P
- Ragusa F
- Rahal G
- Raine JA
- Ramos JM
- Rodriguez LP
- Rozas AJ
- Sanchez FJM
- Solis AL
- Theenhausen HMZ
- Toro RC
- Vazquez JGP
- Villar DIN
- Walls FMG
- Yildiz HD
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/06/2017
- Field of study
The distributions of transverse momentum and longitudinal momentum fraction of charged particles in jets are measured in Pb+Pb and pp collisions with the ATLAS detector at the LHC. The distributions are measured as a function of jet transverse momentum and rapidity. The analysis utilises an integrated luminosity of 0.14 nb−1−1 of Pb+Pb data and 4.0 pb−1−1 of pp data collected in 2011 and 2013, respectively, at the same centre-of-mass energy of 2.76 TeV per colliding nucleon pair. The distributions measured in pp collisions are used as a reference for those measured in Pb+Pb collisions in order to evaluate the impact on the internal structure of jets from the jet energy loss of fast partons propagating through the hot, dense medium created in heavy-ion collisions. Modest but significant centrality-dependent modifications of fragmentation functions in Pb+Pb collisions with respect to those in pp collisions are seen. No significant dependence of modifications on jet pTpT and rapidity selections is observed except for the fragments with the highest transverse momenta for which some reduction of yields is observed for more forward jets
Aerobic and anaerobic respiratory systems in Campylobacter fetus subsp. jejuni grown in atmospheres containing hydrogen
- Author
- Publication venue
- 'American Society for Microbiology'
- Publication date
- Field of study
Elastic and Creep Properties of Alumina-Based Single Fibers
- Author
- Publication venue
- 'Wiley'
- Publication date
- Field of study
Discussion on Spinal Caries with Paraplegia
- Author
- Publication venue
- 'SAGE Publications'
- Publication date
- Field of study