1,225 research outputs found
Pulsed Lasers for Quantitative Ultrasonic NDE
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1992
- Field of study
There has been a lot of recent interest in the use of pulsed lasers for the generation of ultrasound in a range of media [1], due to advantages inherent in the generation process. These include the non-contact nature of the method, and the generation of a wide bandwidth over a small source area. The size and shape of the source can also be changed using suitable optics, as can the generation mechanism itself
Effect of rehabilitation exercise durations on the dynamic bone repair process by coupling polymer scaffold degradation and bone formation
- Author
- A Fritsch
- A Gopferich
- A Gopferich
- A Gopferich
- AR Horwithz
- C Ferrero
- C Hellmich
- C Hellmich
- CG Pitt
- D Courteix
- DE Thompson
- DP Fyhrie
- DR Carter
- DR Carter
- DR Carter
- F Burkersroda von
- FA Schulte
- H Cao
- H Li
- H Pistner
- H Tsuji
- H Tsuji
- HM Frost
- HM Frost
- HM Frost
- J Helder
- J Siepmann
- JC Hou
- JC Middleton
- KU Lewandrowski
- KW Luczynski
- L McIntosh
- LJ Gibson
- M Zhang
- MV Hillsley
- Nicola Pugno
- Q Chen
- Qiang Chen
- Quan Shi
- R Blanchard
- R Huiskes
- R Langer
- R Ruimerman
- RFM Oers van
- RG Sinclair
- RM Dillaman
- S Huang
- S Scheiner
- S Scheiner
- S Scheiner
- S Scheiner
- S Sturm
- SC Cowin
- SJ Hollister
- SJ Shefelbine
- T Adachi
- T Adachi
- TG Morgan
- TS Keller
- XS Wu
- Y Cao
- Y Chen
- Y Chen
- Y Wang
- YB Fan
- Zhi-Yong Li
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
Implantation of biodegradable scaffold is considered as a promising method to treat bone disorders, but knowledge of the dynamic bone repair process is extremely limited. In this study, based on the representative volume cell of a periodic scaffold, the influence of rehabilitation exercise duration per day on the bone repair was investigated by a computational framework. The framework coupled scaffold degradation and bone remodeling. The scaffold degradation was described by a function of stochastic hydrolysis independent of mechanical stimulation, and the bone formation was remodeled by a function of the mechanical stimulation, i.e., strain energy density. Then, numerical simulations were performed to study the dynamic bone repair process. The results showed that the scaffold degradation and the bone formation in the process were competitive. An optimal exercise duration per day emerged. All exercise durations promoted the bone maturation with a final Young's modulus of 1.9 ± 0.3 GPa. The present study connects clinical rehabilitation and fundamental research, and is helpful to understand the bone repair process and further design bone scaffold for bone tissue engineering
Low-frequency vibratory exercise reduces the risk of bone fracture more than walking: a randomized controlled trial
- Author
- Alejo Leal
- Armando Raimundo
- B Shea
- Bruyere O
- BS Roudsari
- Cardinale M
- Chubak J
- D Bonaiuti
- Delmas PD
- Eisman J
- FA Rodriguez
- Flieger J
- Frost HM
- Hass CT
- I Bautmans
- Kallinen M
- Kannus P
- Kelley GA
- King AC
- KM Palombaro
- L Wallace
- Lodder MC
- Mester J
- Mille ML
- Narcís Gusi
- Roelants M
- Rubin C
- Rubin C
- Rubin C
- Russo C
- Torvinen S
- Torvinen S
- Verschueren S
- Wolff I
- Yamazaki S
- Publication venue
- BioMed Central
- Publication date
- 01/01/2006
- Field of study
BACKGROUND: Whole-body vibration (WBV) is a new type of exercise that has been increasingly tested for the ability to prevent bone fractures and osteoporosis in frail people. There are two currently marketed vibrating plates: a) the whole plate oscillates up and down; b) reciprocating vertical displacements on the left and right side of a fulcrum, increasing the lateral accelerations. A few studies have shown recently the effectiveness of the up-and-down plate for increasing Bone Mineral Density (BMD) and balance; but the effectiveness of the reciprocating plate technique remains mainly unknown. The aim was to compare the effects of WBV using a reciprocating platform at frequencies lower than 20 Hz and a walking-based exercise programme on BMD and balance in post-menopausal women. METHODS: Twenty-eight physically untrained post-menopausal women were assigned at random to a WBV group or a Walking group. Both experimental programmes consisted of 3 sessions per week for 8 months. Each vibratory session included 6 bouts of 1 min (12.6 Hz in frequency and 3 cm in amplitude with 60° of knee flexion) with 1 min rest between bouts. Each walking session was 55 minutes of walking and 5 minutes of stretching. Hip and lumbar BMD (g·cm(-2)) were measured using dual-energy X-ray absorptiometry and balance was assessed by the blind flamingo test. ANOVA for repeated measurements was adjusted by baseline data, weight and age. RESULTS: After 8 months, BMD at the femoral neck in the WBV group was increased by 4.3% (P = 0.011) compared to the Walking group. In contrast, the BMD at the lumbar spine was unaltered in both groups. Balance was improved in the WBV group (29%) but not in the Walking group. CONCLUSION: The 8-month course of vibratory exercise using a reciprocating plate is feasible and is more effective than walking to improve two major determinants of bone fractures: hip BMD and balance
Impact of monopolar radiofrequency energy on subchondral bone viability
- Author
- A Ryan
- Anke Kuhn
- Arwed Weigel
- AS Turner
- BA Rahn
- DL Janzen
- DL Muscolo
- FA Barber
- FG Shellock
- HM Frost
- I Encalada
- J Kaplan
- K-H Frosch
- Karl-Heinz Frosch
- Keno G. Ferlemann
- Klaus M. Stürmer
- KM Stürmer
- KO Möller
- L Kaplan
- LD Kaplan
- LD Kaplan
- MJ Kääb
- ML Lotto
- O Cetik
- Peter Balcarek
- PM Bonutti
- RB Edwards 3rd
- RB Edwards 3rd
- RK Uthamanthil
- S Caffey
- S Li
- Tim A. Walde
- V Pruès-Latour
- Y Lu
- Y Lu
- Y Lu
- Y Lu
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2009
- Field of study
The purpose of this study was to analyze the impact of monopolar radiofrequency energy treatment on subchondral bone viability. The femoral grooves of six chinchilla bastard rabbits were exposed bilaterally to monopolar radiofrequency energy for 2, 4 and 8 s, creating a total of 36 defects. An intravital fluorescence bone-labeling technique characterized the process of subchondral bone mineralization within the 3 months following exposure to radiofrequency energy and was analyzed by widefield epifluorescence optical sectioning microscopy using an ApoTome. After 2 s of radiofrequency energy exposure, regular fluorescence staining of the subchondral bone was evident in all samples when compared to untreated areas. The depth of osteonecrosis after 4 and 8 s of radiofrequency energy treatment averaged 126 and 942 µm at 22 days (P < .05; P < .01). The 4 s treatment group showed no osteonecrosis after 44 days whereas the depth of osteonecrosis extended from 519 µm at 44 days (P < .01), to 281 µm at 66 days (P < .01) and to 133 µm at 88 days (P < .05) after 8 s of radiofrequency energy application. Though radiofrequency energy may induce transient osteonecrosis in the superficial zone of the subchondral bone, the results of this study suggest that post-arthroscopic osteonecrosis appears to be of only modest risk given the current clinical application in humans
Compressive deformation behavior modeling of AZ31 magnesium alloy at elevated temperature considering the strain effect
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Faecal pharmacokinetics of orally administered vancomycin in patients with suspected Clostridium difficile infection
- Author
- AM Bourgault
- C Wenisch
- DG Teasley
- DM Citron
- DR Baird
- E Bricker
- Eric H Frost
- F Tedesco
- FA Zar
- GR Matzke
- J Freeman
- J Freeman
- J Pepin
- J Pepin
- Jacques Pepin
- JG Bartlett
- JM Pogue
- Julie C Carrier
- K Saxton
- L Lemee
- LC Fortier
- Louis Valiquette
- Louis-Charles Fortier
- M Merrigan
- M Warny
- Milagros Gonzales
- MJ Robbins
- MN Dudley
- MP Bauer
- MR Keighley
- O Aspevall
- P Bidet
- PG Spitzer
- R Fekety
- R Fekety
- RA Lucas
- S Johnson
- SH Cohen
- SM Finegold
- SS Wong
- Stephanie Sirard
- VG Loo
- Publication venue
- BioMed Central
- Publication date
- 01/12/2010
- Field of study
<p>Abstract</p> <p>Background</p> <p>Oral vancomycin (125 mg qid) is recommended as treatment of severe <it>Clostridium difficile </it>infection (CDI). Higher doses (250 or 500 mg qid) are sometimes recommended for patients with very severe CDI, without supporting clinical evidence. We wished to determine to what extent faecal levels of vancomycin vary according to diarrhoea severity and dosage, and whether it is rational to administer high-dose vancomycin to selected patients.</p> <p>Methods</p> <p>We recruited hospitalized adults suspected to have CDI for whom oral vancomycin (125, 250 or 500 mg qid) had been initiated. Faeces were collected up to 3 times/day and levels were measured with the AxSYM fluorescence polarization immunoassay.</p> <p>Results</p> <p>Fifteen patients (9 with confirmed CDI) were treated with oral vancomycin. Patients with ≥4 stools daily presented lower faecal vancomycin levels than those with a lower frequency. Higher doses of oral vancomycin (250 mg or 500 mg qid) led to consistently higher faecal levels (> 2000 mg/L), which were 3 orders of magnitude higher than the MIC<sub>90 </sub>of vancomycin against <it>C. difficile</it>. One patient receiving 125 mg qid had levels below 50 mg/L during the first day of treatment.</p> <p>Conclusions</p> <p>Faecal levels of vancomycin are proportional to the dosage administered and, even in patients with increased stool frequency, much higher than the MIC<sub>90</sub>. Patients given the standard 125 mg qid dosage might have low faecal levels during the first day of treatment. A loading dose of 250 mg or 500 mg qid during the first 24-48 hours followed by the standard dosage should be evaluated in larger studies, since it might be less disruptive to the colonic flora and save unnecessary costs.</p
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
- Bakker PJ
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barsov S
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertram IA
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bhattacharya DS
- Bhattarai P
- Bi R
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz N
- Biglietti M
- Billoud TR
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker E
- Boumediene D
- Bourdarios CA
- Boutle SK
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Broughton JH
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher V
- Bugge MK
- Bulekov O
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
- Camelia EA
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cantero J
- Cao T
- Cao Y
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carter JWS
- Casado MP
- Casha AF
- Casper DW
- Castelijn R
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavallaro E
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Cerda Alberich L
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chau CC
- Che S
- Chekanov S
- Chekulaev S
- Chelkov GA
- Chen B
- Chen C
- Chen CH
- Chen H
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov M
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Chytka L
- Cieri D
- Ciesla KM
- Cinca D
- Cindro V
- Cioara IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark MR
- Clark PJ
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Cohen H
- Coimbra AEC
- Cole B
- Colijn AP
- Collot J
- Conde Muino P
- Connell SH
- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar AM
- Corga KDV
- Cormier F
- Cormier KJR
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa MJ
- Costanza F
- Costanzo D
- Cowan G
- Cowley JW
- Crane J
- Cranmer K
- Crawley SJ
- Creager RA
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cukierman AR
- Cunningham WR
- Czekierda S
- Czodrowski P
- D'amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- da Costa JBG
- Da Fonseca Pinto J
- Da Via C
- Dabrowski W
- Dachs F
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Dann NS
- Danninger M
- Dao V
- Darbo G
- Dartsi O
- Dattagupta A
- Daubney T
- David C
- Davidek T
- Davis DR
- Dawson I
- De Asmundis R
- De Beurs M
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- de Lima DEF
- De Lima RT
- De Maria A
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Sousa MJDCS
- De K
- Debenedetti C
- Dedovich D
- Deiana AM
- Del Peso J
- Delgove D
- Deliot F
- Delitzsch CM
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Volpe D
- Delmastro M
- Delporte C
- Delsart PA
- DeMarco DA
- Demers S
- Demichev M
- Demontigny G
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Dette K
- Deutsch C
- Devesa MR
- Deviveiros PO
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Micco B
- Di Nardo R
- Di Petrillo KF
- Di Sipio R
- Diaconu C
- Dias FA
- Diaz LP
- Diaz MA
- Diaz YD
- Dickinson J
- Diehl EB
- Dietrich J
- Dimitrievska A
- Ding W
- Dingfelder J
- Dittus F
- Djama F
- Djobava T
- Djuvsland J
- Do Vale TD
- Dobre M
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Dominguez LP
- Don MMR
- Donadelli M
- Dong B
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Dreyer T
- Drobac AS
- Du D
- Duan Y
- Dubinin F
- Dubovsky M
- Dubreuil A
- Duchovni E
- Duckeck G
- Ducourthial A
- Ducu OA
- Duda D
- Dudarev A
- Dudder AC
- Duelsen C
- Dueren M
- Duffeld EM
- DuflOt L
- Duhrssen M
- Dumancic M
- Dumitriu AE
- Duncan AK
- Dunford M
- Duperrin A
- Durglishvili A
- Duschinger D
- Dutta B
- Duvnjak D
- Dyckes G
- Dyndal M
- Dysch S
- Dziedzic BS
- Ecker KM
- Eggleston MG
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Jarrari H
- El Kossei R
- El Moursli RC
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Emerman A
- Enari Y
- Epland MB
- Erdmann J
- Ereditato A
- Erland PA
- Errenst M
- Escalier M
- Escobar C
- Estrada Pastor O
- Etzion E
- Evans H
- Ezhilov A
- Fabbri F
- Fabbri L
- Fabiani V
- Facini G
- Fakhrutdinov RM
- Falciano S
- Falke PJ
- Falke S
- Faltova J
- Fang Y
- Fanourakis G
- Fanti M
- Faraj M
- Farbin A
- Farilla A
- Farina EM
- Farooque T
- Farrington SM
- Farthouat P
- Fassi F
- Fassnacht P
- Fassouliotis D
- Fawcett WJ
- Fayard L
- Fedin OL
- Fedorko W
- Fehr A
- Feickert M
- Feligioni L
- Fell A
- Feng C
- Feng M
- Fenton MJ
- Fenyuk AB
- Ferguson SW
- Ferrando J
- Ferrante A
- Ferrari A
- Ferrari P
- Ferrari R
- Ferrer A
- Ferrer JAV
- Ferrere D
- Ferretti C
- Fiedler F
- Filipcic A
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- Zu Theenhausen HM
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- 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
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
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- Abreu H
- Abulaitia Y
- Acharya BS
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- Ahlen SP
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- Akimov AV
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- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
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- Allbrooke BMM
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- Zurzolo G
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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 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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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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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
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TP
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
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- Alimonti G
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- Allbrooke BMM
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- 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
- Walsh B
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- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Warsinsky M
- Washbrook A
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- Watson AT
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- Waugh BM
- Webb S
- Weber MS
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- 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
- Werner M
- Werner P
- Wessels M
- Wetter J
- Whalen K
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- Whiteson D
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilkens HG
- Will JZ
- Williams HH
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- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winter BT
- Wittgen M
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- 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
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- 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
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