179 research outputs found
Treatment of unstable sacral fractures with percutaneous reconstruction plate internal fixation
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Enhanced solar energy conversion in Au-doped, single-wall carbon nanotube-Si heterojunction cells
- Author
- AM Rao
- B Chandra
- B Shan
- BS Kong
- C Li
- Chen Xu
- D Kozawa
- Deren Yang
- DH Kim
- ES Snow
- HC Choi
- HH Atwater
- HH Kou
- Hong He
- HW Zhu
- HX Li
- I Khatri
- IH Lee
- Ishpal
- JG Park
- Jianjiang Zhao
- JQ Wei
- KK Kim
- KK Kim
- Leifeng Chen
- LF Chen
- LF Chen
- LH Zhang
- M Stadermann
- MH Ham
- MS Fuhrer
- P Pramod
- PL Ong
- PN Nirmalraj
- S Chiu
- SB Yang
- SB Yang
- SD Gobbo
- Shichao Zhao
- Shijun Zhang
- SM Kim
- V Saini
- VL Borgne
- VL Borgne
- W Zhou
- WZ Qian
- X Bai
- XM Hou
- Y He
- Y Jia
- YA Akimov
- YA Li
- Yuhong Mi
- ZF Bian
- ZR Li
- ZR Li
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
All-sky search for continuous gravitational waves from isolated neutron stars in the early O3 LIGO data
- Author
- Abbott R
- Abbott TD
- Abraham S
- Acernese F
- Ackley K
- Adams A
- Adams C
- Adhikari RX
- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Aleman KM
- Allen G
- Allocca A
- Altin PA
- Amato A
- Anand S
- Ananyeva A
- Anderson SB
- Anderson WG
- Ando M
- Angelova S
- Ansoldi S
- Antelis JM
- Antier S
- Appert S
- Arai Koji
- Arai Koya
- Arai Y
- Araki S
- Araya A
- Araya MC
- Areeda JS
- Arellano FE Pena
- Arene M
- Aritomi N
- Arnaud N
- Aronson SM
- Asada H
- Asali Y
- Ashton G
- Aso Y
- Aston SM
- Astone P
- Aubin F
- Aufmuth P
- AultoNeal K
- Austin C
- Babak S
- Badaracco F
- Bader MKM
- Bae S
- Bae Y
- Baer AM
- Bagnasco S
- Bai Y
- Baiotti L
- Baird J
- Bajpai R
- Ball M
- Ballardin G
- Ballmer SW
- Bals M
- Balsamo A
- Baltus G
- Banagiri S
- Bankar D
- Bankar RS
- Barayoga JC
- Barbieri C
- Barish BC
- Barker D
- Barneo P
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Barton MA
- Bartos I
- Bassiri R
- Basti A
- Bawaj M
- Bayley JC
- Baylor AC
- Bazzan M
- Becsy B
- Bedakihale VM
- Bejger M
- Belahcene I
- Benedetto V
- Beniwal D
- Benjamin MG
- Bennett TF
- Bentley JD
- BenYaala M
- Bergamin F
- Berger BK
- Bernuzzi S
- Bersanetti D
- Bertolini A
- Betzwieser J
- Bhandare R
- Bhandari A
- Bhattacharjee D
- Bhaumik S
- Bidler J
- Bilenko IA
- Billingsley G
- Birney R
- Birnholtz O
- Biscans S
- Bischi M
- Biscoveanu S
- Bisht A
- Biswas B
- Bitossi M
- Bizouard M-A
- Blackburn JK
- Blackman J
- Blair CD
- Blair DG
- Blair RM
- Bobba F
- Bode N
- Boer M
- Bogaert G
- Boldrini M
- Bondu F
- Bonilla E
- Bonnand R
- Booker P
- Boom BA
- Bork R
- Boschi V
- Bose N
- Bose S
- Bossilkov V
- Boudart V
- Bouffanais Y
- Bozzi A
- Bradaschia C
- Brady PR
- Bramley A
- Branch A
- Branchesi M
- Brau JE
- Breschi M
- Briant T
- Briggs JH
- Brillet A
- Brinkmann M
- Brockill P
- Brooks AF
- Brooks J
- Brown DD
- Brunett S
- Bruno G
- Bruntz R
- Bryant J
- Buikema A
- Bulik T
- Bulten HJ
- Buonanno A
- Buscicchio R
- Buskulic D
- Bustillo J Calderon
- Byer RL
- Cadonati L
- Caesar M
- Cagnoli G
- Cahillane C
- Cain HW
- Callaghan JD
- Callister TA
- Calloni E
- Camp JB
- Canepa M
- Cannavacciuolo M
- Cannon KC
- Cao H
- Cao J
- Cao Z
- Capocasa E
- Capote E
- Carapella G
- Carbognani F
- Carlin JB
- Carney MF
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- Casentini C
- Castaldi G
- Caudill S
- Cavaglia M
- Cavalier F
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- Cella G
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- Cesarini E
- Chaibi W
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- Champion B
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- Chandra K
- Chanial P
- Chao S
- Charlton P
- Chase EA
- Chassande-Mottin E
- Chatterjee D
- Chaturvedi M
- Chen A
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- Chen HY
- Chen J
- Chen K
- Chen X
- Chen Y-B
- Chen Y-R
- Chen Z
- Cheng H
- Cheong CK
- Cheung HY
- Chia HY
- Chiadini F
- Chiang C-Y
- Chierici R
- Chincarini A
- Chiofalo ML
- Chiummo A
- Cho G
- Cho HS
- Choate S
- Choudhary RK
- Choudhary S
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- Cohen DE
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- Collette CG
- Colpi M
- Compton CM
- Constancio M
- Conti L
- Cooper SJ
- Corban P
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- Cordero-Carrion I
- Corezzi S
- Corley KR
- Cornish N
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- Coulon J-P
- Countryman ST
- Cousins B
- Couvares P
- Covas PB
- Coward DM
- Cowart MJ
- Coyne DC
- Coyne R
- Creighton JDE
- Creighton TD
- Criswell AW
- Croquette M
- Crowder SG
- Cudell JR
- Cullen TJ
- Cumming A
- Cummings R
- Cuoco E
- D'Angelo B
- D'Antonio S
- D'Emilio V
- D'Onofrio L
- D'Urso D
- Dal Canton T
- Dalya G
- Dana A
- DaneshgaranBajastani LM
- Danilishin SL
- Danzmann K
- Darsow-Fromm C
- Dasgupta A
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- Dattilo V
- Dave I
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- Del Favero V
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- Deleglise S
- DeMarchi LM
- Demos N
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- Depasse A
- DeSalvo R
- Dhurandhar S
- Di Fiore L
- Di Fronzo C
- Di Giorgio C
- Di Giovanni F
- Di Girolamo T
- Di Lieto A
- Di Pace S
- Di Palma I
- Di Renzo F
- Diaz J Casanueva
- Diaz MC
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- Doravari S
- Dorrington I
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- Driggers JC
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- Dupej P
- Durante O
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- Eddolls G
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- Effler A
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- Eisenstein RA
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- Fidecaro F
- Figura P
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- Fishbach M
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- Fiumara V
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 15/10/2021
- Field of study
We report on an all-sky search for continuous gravitational waves in the frequency band 20-2000 Hz and with a frequency time derivative in the range of [-1.0,+0.1]×10-8 Hz/s. Such a signal could be produced by a nearby, spinning and slightly nonaxisymmetric isolated neutron star in our Galaxy. This search uses the LIGO data from the first six months of Advanced LIGO's and Advanced Virgo's third observational run, O3. No periodic gravitational wave signals are observed, and 95% confidence-level (C.L.) frequentist upper limits are placed on their strengths. The lowest upper limits on worst-case (linearly polarized) strain amplitude h0 are ∼1.7×10-25 near 200 Hz. For a circularly polarized source (most favorable orientation), the lowest upper limits are ∼6.3×10-26. These strict frequentist upper limits refer to all sky locations and the entire range of frequency derivative values. For a population-averaged ensemble of sky locations and stellar orientations, the lowest 95% C.L. upper limits on the strain amplitude are ∼1.4×10-25. These upper limits improve upon our previously published all-sky results, with the greatest improvement (factor of ∼2) seen at higher frequencies, in part because quantum squeezing has dramatically improved the detector noise level relative to the second observational run, O2. These limits are the most constraining to date over most of the parameter space searched
Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at root s=8 TeV
- Author
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
Peer reviewe
Effects of alirocumab on types of myocardial infarction: insights from the ODYSSEY OUTCOMES trial
- Author
- Abbas J
- Abbate A
- Abdullakutty J
- Abhyanakar AD
- Aboyans V
- Abrantes JAM
- Abu-Fadel M
- Acevedo M
- Adamkova V
- Adhyapak S
- Agarwal H
- Aggarwal R
- Aggarwal RK
- Aguirre A
- Ahmed H
- Ahremark U
- Ahuad Guerrero RA
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- Airaksinen JK
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- Akatova E
- Akhter F
- Ako J
- Akright L
- Akyea-Djamson A
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- Al-Windy NYY
- Alan D
- Alcocer Gamba MA
- Alexander JH
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- Alexandru TM
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- Alonso Martin JJ
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- Zuniga JDH
- Zurakowski A
- Zuran I
- Zweiker R
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 01/01/2019
- Field of study
Aims The third Universal Definition of Myocardial Infarction (MI) Task Force classified MIs into five types: Type 1, spontaneous; Type 2, related to oxygen supply/demand imbalance; Type 3, fatal without ascertainment of cardiac biomarkers; Type 4, related to percutaneous coronary intervention; and Type 5, related to coronary artery bypass surgery. Low-density lipoprotein cholesterol (LDL-C) reduction with statins and proprotein convertase subtilisin–kexin Type 9 (PCSK9) inhibitors reduces risk of MI, but less is known about effects on types of MI. ODYSSEY OUTCOMES compared the PCSK9 inhibitor alirocumab with placebo in 18 924 patients with recent acute coronary syndrome (ACS) and elevated LDL-C (≥1.8 mmol/L) despite intensive statin therapy. In a pre-specified analysis, we assessed the effects of alirocumab on types of MI. Methods and results Median follow-up was 2.8 years. Myocardial infarction types were prospectively adjudicated and classified. Of 1860 total MIs, 1223 (65.8%) were adjudicated as Type 1, 386 (20.8%) as Type 2, and 244 (13.1%) as Type 4. Few events were Type 3 (n = 2) or Type 5 (n = 5). Alirocumab reduced first MIs [hazard ratio (HR) 0.85, 95% confidence interval (CI) 0.77–0.95; P = 0.003], with reductions in both Type 1 (HR 0.87, 95% CI 0.77–0.99; P = 0.032) and Type 2 (0.77, 0.61–0.97; P = 0.025), but not Type 4 MI. Conclusion After ACS, alirocumab added to intensive statin therapy favourably impacted on Type 1 and 2 MIs. The data indicate for the first time that a lipid-lowering therapy can attenuate the risk of Type 2 MI. Low-density lipoprotein cholesterol reduction below levels achievable with statins is an effective preventive strategy for both MI types.For complete list of authors see http://dx.doi.org/10.1093/eurheartj/ehz299</p
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search for the production of a pair of top squarks at the LHC is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar, because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with 35.9 fb(-1) of proton-proton collisions at a centre-of-mass energy of root s = 13 TeV, collected by the CMS detector in 2016, using events containing one electron-muon pair with opposite charge. The search is based on a precise estimate of the top quark pair background, and the use of the M-T2 variable, which combines the transverse mass of each lepton and the missing transverse momentum. No excess of events is found over the standard model predictions. Exclusion limits are placed at 95% confidence level on the production of top squarks up to masses of 208 GeV for models with a mass difference between the top squark and the lightest neutralino close to that of the top quark.Peer reviewe
Search for Higgs boson pair production in the gamma gamma b(b)over-bar final state in pp collisions at root s=13 TeV
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
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- Abu Zeid S
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- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search is presented for the production of a pair of Higgs bosons, where one decays into two photons and the other one into a bottom quark-antiquark pair. The analysis is performed using proton-proton collision data at root s = 13 TeV recorded in 2016 by the CMS detector at the LHC, corresponding to an integrated luminosity of 35.9 fb(-1) . The results are in agreement with standard model (SM) predictions. In a search for resonant production, upper limits are set on the cross section for new spin-0 or spin-2 particles. For the SM-like nonresonant production hypothesis, the data exclude a product of cross section and branching fraction larger than 2.0 fb at 95% confidence level (CL), corresponding to about 24 times the SM prediction. Values of the effective Higgs boson self-coupling K X are constrained to be within the range -11 < K-lambda < 17 at 95% CL, assuming all other Higgs boson couplings are at their SM value. The constraints on K-lambda, are the most restrictive to date. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state with two bquarks and two tau leptons in proton-proton collisions at root s=13 TeV The CMS Collaboration
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- Abdullah Wan WAT
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- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for an exotic decay of the Higgs boson to a pair of light pseudoscalar bosons is performed for the first time in the final state with two b quarks and two tau leptons. The search is motivated in the context of models of physics beyond the standard model (SM), such as two Higgs doublet models extended with a complex scalar singlet (2HDM + S), which include the next-to-minimal supersymmetric SM (NMSSM). The results are based on a data set of proton-proton collisions corresponding to an integrated luminosity of 35.9 fb(-1), accumulated by the CMS experiment at the LHC in 2016 at a center-of-mass energy of 13 TeV. Masses of the pseudoscalar boson between 15 and 60 GeVare probed, and no excess of events above the SM expectation is observed. Upper limits between 3 and 12% are set on the branching fraction B(h -> aa -> 2 tau 2b) assuming the SM production of the Higgs boson. Upper limits are also set on the branching fraction of the Higgs boson to two light pseudoscalar bosons in different 2HDM + S scenarios. Assuming the SM production cross section for the Higgs boson, the upper limit on this quantity is as low as 20% for a mass of the pseudoscalar of 40 GeV in the NMSSM. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at \sqrt{s} = 13 TeV
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- Wissing C
- Wittich P
- Wittmann J
- Wittmer B
- Woehrmann C
- Wolf M
- Wolf R
- Wolfe E
- Womersley WJ
- Wong K
- Wood D
- Wood J
- Woodard A
- Woods N
- Wright D
- Wright J
- Wu Z
- Wulsin HW
- Wulz C-E
- Wurthwein F
- Wyslouch B
- Xia F
- Xiao M
- Xiao R
- Xie S
- Xie W
- Xu Q
- Yagil A
- Yalvac M
- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
- You C
- Yu D
- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
- Zhang J
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zito G
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuolo D
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2019
- Field of study
A search for nonresonant excesses in the invariant mass spectra of electron and muon pairs is presented. The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the CMS experiment in 2016, corresponding to a total integrated luminosity of 36 fb^{-1}. No significant deviation from the standard model is observed. Limits are set at 95% confidence level on energy scales for two general classes of nonresonant models. For a class of fermion contact interaction models, lower limits ranging from 20 to 32 TeV are set on the characteristic compositeness scale Λ. For the Arkani-Hamed, Dimopoulos, and Dvali model of large extra dimensions, the first results in the dilepton final state at 13 TeV are reported, and values of the ultraviolet cutoff parameter Λ_{T} below 6.9 TeV are excluded. A combination with recent CMS diphoton results improves this exclusion to Λ_{T} below 7.7 TeV, providing the most sensitive limits to date in nonhadronic final states
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