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Coal Oil Point Reserve Annual Newsletter 2019
- Publication venue
- eScholarship, University of California
- Publication date
- 01/12/2019
- Field of study
The Coal Oil Point Reserve Annual Newsletter highlights the conservation, restoration, and research projects at the reserve in 2019
Remote Entanglement between a Single Atom and a Bose-Einstein Condensate
- Author
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Entanglement between stationary systems at remote locations is a key resource
for quantum networks. We report on the experimental generation of remote
entanglement between a single atom inside an optical cavity and a Bose-Einstein
condensate (BEC). To produce this, a single photon is created in the
atom-cavity system, thereby generating atom-photon entanglement. The photon is
transported to the BEC and converted into a collective excitation in the BEC,
thus establishing matter-matter entanglement. After a variable delay, this
entanglement is converted into photon-photon entanglement. The matter-matter
entanglement lifetime of 100 ÎŒs exceeds the photon duration by two orders
of magnitude. The total fidelity of all concatenated operations is 95%. This
hybrid system opens up promising perspectives in the field of quantum
information
An integrated approach for SNP calling based on population of genomes
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Cyclic AMP Control Measured in Two Compartments in HEK293 Cells: Phosphodiesterase KM Is More Important than Phosphodiesterase Localization
- Author
- A Hatzelmann
- A Terrin
- AS Bell
- C Russwurm
- CJ Schmidt
- DM Cooper
- E Degerman
- FG Boess
- GS Baillie
- GS McKnight
- JA Beavo
- JA Beavo
- Jacob Nielsen
- K Fujishige
- K Matthiesen
- Karina Matthiesen
- Karl-Wilhelm Koch
- KV Chin
- L Fawcett
- LC Tsai
- LI Jiang
- LM Dipilato
- LS Barak
- M Shelly
- M Zaccolo
- M Zaccolo
- M Zaccolo
- MJ Lynch
- P Wang
- PG Grant
- RF Oliveira
- SA Harrison
- SH Soderling
- SH Soderling
- T Sudo
- TA Goraya
- VO Nikolaev
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
The intracellular second messenger cyclic AMP (cAMP) is degraded by phosphodiesterases (PDE). The knowledge of individual families and subtypes of PDEs is considerable, but how the different PDEs collaborate in the cell to control a cAMP signal is still not fully understood. In order to investigate compartmentalized cAMP signaling, we have generated a membrane-targeted variant of the cAMP Bioluminiscence Resonance Energy Transfer (BRET) sensor CAMYEL and have compared intracellular cAMP measurements with it to measurements with the cytosolic BRET sensor CAMYEL in HEK293 cells. With these sensors we observed a slightly higher cAMP response to adenylyl cyclase activation at the plasma membrane compared to the cytosol, which is in accordance with earlier results from Fluorescence Resonance Energy Transfer (FRET) sensors. We have analyzed PDE activity in fractionated lysates from HEK293 cells using selective PDE inhibitors and have identified PDE3 and PDE10A as the major membrane-bound PDEs and PDE4 as the major cytosolic PDE. Inhibition of membrane-bound or cytosolic PDEs can potentiate the cAMP response to adenylyl cyclase activation, but we see no significant difference between the potentiation of the cAMP response at the plasma membrane and in cytosol when membrane-bound and cytosolic PDEs are inhibited. When different levels of stimulation were tested, we found that PDEs 3 and 10 are mainly responsible for cAMP degradation at low intracellular cAMP concentrations, whereas PDE4 is more important for control of cAMP at higher concentrations
Combination antiretroviral therapy and the risk of myocardial infarction
- Author
- Abbadesse V
- Abrams DI
- Abrescia N
- Akerlund B
- Alberici F
- Alessandrini A
- Anderson J
- Antinori A
- Antinori A
- Antunes F
- Arduino R
- Arici C
- Arici C
- Arlotti M
- Austin D
- Baker B
- Bal J
- Balestre E
- Ballardini G
- Banhegyi D
- Barton S
- Bartsch G
- Bartsch G
- Baxter J
- Bedini A
- Ben-Ishai Z
- Benfield T
- Beniowski M
- Bentwich Z
- Bentz L
- Bernard E
- Bernard N
- Bernasconi E
- Beylot C
- Beylot J
- Beylot J
- Bezian JH
- Bieckel M
- Blaizeau MJ
- Blaxhult A
- Blok W
- Bonarek M
- Bonasso M
- Bonnet F
- Borleffs J
- Boron-Kaczmarska A
- Bottari G
- Boulant B
- Brettle R
- Brevenboer B
- Brinkman K
- Bronsveld W
- Bruno R
- Bruun J
- Bucher H
- Burgisser P
- Cadafalch J
- Cadeo G
- Caggese L
- Caissotti C
- Calvo G
- Calvo G
- Calvo G
- Caramello P
- Cargnel A
- Carnevale G
- Carosi G
- Carr A
- Castelli F
- Castera L
- Cattacin S
- Chaillou S
- Chambon D
- Chene G
- Chiesi A
- Chiodo F
- Chiriann A
- Chirianni A
- Chossat I
- Chuah J
- Cioppi A
- Cipriano C
- Cipriano G
- Claessen F
- Clotet B
- Clumeck N
- Clumeck N
- Coadou B
- Codina C
- Cohn D
- Colangeli V
- Colebunders R
- Colomba A
- Conejero J
- Conri C
- Constans J
- Cooper D
- Coronado O
- Couzigou P
- Crane LR
- D'Alessandro M
- Dabis F
- Dabis F
- Danner S
- De La Taille C
- De Lalla F
- De Longis P
- De Luca A
- De Marco M
- de Marie S
- De Salvador-Guillouet F
- De Stefano C
- De Wit S
- De Wit S
- De Wit S
- de Wolf F
- Decoin M
- Del Cacho E
- Dellamonica P
- Delveaux S
- Diaz B
- Dietrich M
- Djossou F
- Domingo P
- Doutre MS
- Dupon M
- Dupon M
- Durant J
- Dutoit D
- Dutronc H
- Egger M
- El-Sadr WM
- El-Sadr WM
- El-Sadr WM
- Erb P
- Esposito R
- Esposito R
- Fankhauser W
- Faure I
- Ferrara S
- Ferraro T
- Fierz W
- Filandras A
- Filice G
- Finazzi R
- Fischer M
- Fisher E
- Fisher M
- Flamholc L
- Flepp M
- Fleury H
- Fontana A
- Fontas E
- Fontas E
- Formaggio AM
- Franci P
- Francioli P
- Francioli P
- Friedland G
- Friis-Moller N
- Friis-Moller N
- Frissen P
- Furrer H
- Furrer HJ
- Fuster M
- Gabbuti A
- Galloni D
- Galperine T
- Garcia-Benayas T
- Gargalianos P
- Gasiorowski J
- Gatell J
- Gatell JM
- Gelie P
- Gennero L
- Gerard M
- Gerstoft J
- Ghinelli F
- Godfried M
- Goebel FD
- Gonzalez-Lahoz J
- Gordin F
- Gorgievski M
- Gowers A
- Grima P
- Grisorio B
- Guttman R
- Gyssens I
- Hakangard C
- Hammer S
- Heidemann B
- Hemmer R
- Heripret L
- Hermans P
- Hildebrand M
- Hillbrand M
- Hirschel B
- Hirschel B
- Hoepelman I
- Horban A
- Houyez F
- Jacqmin-Gadda H
- Jaspers C
- Jaubert D
- Jeurissen F
- Johnson AM
- Johnson MA
- Jou A
- Juttmann J
- Kabeya K
- Kaiser L
- Karlsson A
- Karydis I
- Katlama C
- Katzenstein T
- Kauffmann R
- Keuter M
- Kind C
- Kirk O
- Kirk O
- Kirk O
- Kjaer J
- Klimkait T
- Knysz B
- Koger E
- Konopnicki D
- Koopmans P
- Koppel K
- Kosmidis J
- Kroon F
- Krum E
- Krum E
- La Gala A
- Labarerre S
- Lacoste D
- Lacut JY
- Lafarie S
- Lafarie S
- Lafon ME
- Lange J
- Lauper U
- Lavignolle V
- Lavignolle V
- Law G
- Law M
- Law MG
- Law MG
- Lawson-Ayayi S
- Lazzarin A
- Lazzarin A
- Le Bras M
- Le Bras M
- Ledergerber B
- Ledergerber B
- Leemhuis M
- Leng B
- Lichtner M
- Lo Caputo S
- Loeliger E
- Loiacono L
- Loveday C
- Lowe S
- Lundgren JD
- Lundgren JD
- Lundgren JD
- Lundgren JD
- Luskin-Hawk R
- Maayan S
- Machala L
- Maeland A
- Magnani G
- Mallal S
- Malvy D
- Manconi PE
- Mancuso S
- Manegold C
- Mannazzu M
- Mansinho K
- Markowitz N
- Martin-Carbonero L
- Martinelli C
- Masquelier B
- Mateau S
- Matute A
- Mazzotta F
- Mazzotta F
- McFarlane R
- Meenhorst P
- Meester R
- Meester R
- Menichetti F
- Mercey D
- Merchadou L
- Mercie P
- Merli S
- Mestre C
- Migliorino G
- Mijch A
- Miller V
- Minafra G
- Miro JM
- Mocroft A
- Moioli C
- Mondain-Miton V
- Monforte AD
- Monforte AD
- Monforte AD
- Monforte VO
- Monteforte AD
- Montesarchio E
- Montroni M
- Moreau F
- Moreau JF
- Morfeldt L
- Morfeldt L
- Morfeldt L
- Morlat P
- Moroni M
- Mulcahy F
- Mulder J
- Mura MS
- Mushatt D
- Mussini C
- Nappa S
- Narciso P
- Narciso P
- Nasti G
- Neaton J
- Neaton J
- Neau D
- Nellen F
- Nielsen J
- Noto P
- Nouts C
- Novati R
- Ochoa A
- Opravil M
- Ormaasen V
- Ortolani P
- Ortona L
- Paccaud F
- Pagano G
- Palmer G
- Panos G
- Pantaleo G
- Parkin J
- Pasquinucci S
- Pastecchia C
- Pastore G
- Payen MC
- Pedersen C
- Pehrson P
- Pellegrin I
- Pellegrin JL
- Pellegrin JL
- Perbost I
- Perdios J
- Pereira F
- Perenboom R
- Perez G
- Perrin L
- Petoumenos K
- Petoumenos K
- Petrelli E
- Petrosillo N
- Pezzotti P
- Pezzotti P
- Phillips AN
- Phillips AN
- Phillips AN
- Piano P
- Piazza M
- Piersantelli N
- Piffaretti JC
- Pinching A
- Piscopo R
- Pivetaud JP
- Pizzigallo E
- Pnyka M
- Pogany K
- Poggio A
- Poll B
- Poll B
- Pollack S
- Pradier C
- Pradier C
- Pradier C
- Pradier C
- Prestileo T
- Prins J
- Pristera R
- Proenca R
- Prokopowicz D
- Prouvost-Keller B
- Pugliese P
- Pusterla L
- Ragnaud JM
- Ragnaud JM
- Rahelinirina V
- Raise E
- Reiss P
- Reiss P
- Reiss P
- Reiss R
- Rhiebaut R
- Richter C
- Rickenbach M
- Rickenbach M
- Rispal P
- Rizzardini G
- Rockstroh J
- Roge B
- Roger PM
- Roth N
- Rudin C
- Ruggieri A
- Ruys T
- Sabin CA
- Sabin CA
- Saint-Marc T
- Salamon R
- Salcuni P
- Salzberger B
- Sambatakou H
- Sambeat MA
- Sampson J
- Santopadre P
- Santoro D
- Sawitz A
- Scasso A
- Scerbo A
- Schattenkerk JKE
- Schieveld S
- Schippers E
- Schneider M
- Schrey G
- Schupbach J
- Schurink C
- Sciandra M
- Scullard G
- Series C
- Sighinolfi L
- Sinicco A
- Sirera G
- Sjol A
- Sjol A
- Skett J
- Skinhoj P
- Soranzo ML
- Soravia-Dunand V
- Soriano V
- Soscia F
- Speck R
- Sprenger HG
- Staszewski S
- Staub T
- Sundstrom A
- Sunstrom A
- Suter F
- Tacconi L
- Taupin JL
- Taytard A
- Tchamgoue S
- Tedaldi E
- Telenti A
- Telenti A
- Telgt D
- Telzak E
- ten Kate RW
- ten Napel C
- ten Veen J
- Thiebaut R
- Thompson G
- Thulin G
- Tirelli U
- Torres F
- Torres F
- Tositti G
- Touchard D
- Tressler R
- Trimoulet P
- Trkola A
- Trocha H
- Tundo P
- Tural C
- Turner D
- Ursitti M
- Uwamaliya B
- van Dam P
- van der Ende M
- van der Geest S
- van der Heul C
- van der Meer J
- van der Poll T
- van der Valk M
- van der Ven A
- van der Ven E
- van Eeden A
- van Gorp E
- Van Laethem Y
- van Leusen R
- van Lunzen J
- Van Valkengoed L
- Vandenbos F
- Vangi D
- Vanhems P
- Vaque A
- Vella S
- Verbon A
- Vernazza P
- Vetter N
- Viallard JF
- Viard JP
- Vigevani GM
- Vimard E
- Vincenti A
- Vriesendorp R
- Vullo V
- Vullo V
- Watson K
- Weber J
- Weber R
- Weber R
- Weber R
- Weber R
- Weigel H
- Weller I
- Wentworth D
- Wit F
- Wood H
- Yerly S
- Yust I
- Zaccarelli M
- Zaheri S
- Zauli T
- Zoli A
- Publication venue
- 'Massachusetts Medical Society'
- Publication date
- 20/11/2003
- Field of study
First narrow-band search for continuous gravitational waves from known pulsars in advanced detector data
- Author
- D. E.
- J. F. J.
- Abbott B. P.
- Abbott R.
- Abbott T. D.
- Acernese F.
- Ackley K.
- Adams C.
- Adams T.
- Addesso P.
- Adhikari R. X.
- Adya V. B.
- Affeldt C.
- Afrough M.
- Agarwal B.
- Agathos M.
- Agatsuma K.
- Aggarwal N.
- Aguiar O. D.
- Aiello L.
- Ain A.
- Allen B.
- Allen G.
- Allocca A.
- Altin P. A.
- Alvarez M. Dovale
- Amato A.
- Ananyeva A.
- Angelova S. V.
- Antier S.
- Appert S.
- Arai K.
- Araya M. C.
- are R.
- Areeda J. S.
- ari B.
- Arnaud N.
- Arun K. G.
- Ascenzi S.
- Ashton G.
- Ast M.
- Aston S. M.
- Astone P.
- Atallah D. V.
- Aufmuth P.
- Aulbert C.
- AultONeal K.
- Austin C.
- Avila-Alvarez A.
- Babak S.
- Bacon P.
- Bader M. K. M.
- Bae S.
- Baker P. T.
- Baldaccini F.
- Ballardin G.
- Ballmer S. W.
- Banagiri S.
- Barayoga J. C.
- Barclay S. E.
- Barish B. C.
- Barker D.
- Barkett K.
- Barone F.
- Barr B.
- Barsotti L.
- Barsuglia M.
- Barta D.
- Bartlett J.
- Bartos I.
- Bassiri R.
- Basti A.
- Batch J. C.
- Bawaj M.
- Bayley J. C.
- Bazzan M.
- Becsy B.
- Beer C.
- Bejger M.
- Belahcene I.
- Bell A. S.
- berg V.
- Berger B. K.
- Bergmann G.
- Bero J. J.
- Berry C. P. L.
- Bersanetti D.
- Bertolini A.
- Betzwieser J.
- Bh
- Bhagwat S.
- Bilenko I. A.
- Billingsley G.
- Billman C. R.
- Birch J.
- Birney R.
- Birnholtz O.
- Biscans S.
- Biscoveanu S.
- Bisht A.
- Bitossi M.
- Biwer C.
- Bizouard M. A.
- Blackburn J. K.
- Blackman J.
- Blair C. D.
- Blair D. G.
- Blair R. M.
- Bloemen S.
- Bock O.
- Bode N.
- Boer M.
- Bogaert G.
- Bohe A.
- Bondu F.
- Bonilla E.
- Bonn
- Boom B. A.
- Bork R.
- Boschi V.
- Bose S.
- Bossie K.
- Bouffanais Y.
- Bozzi A.
- BRADASCHIA CARLO
- Brady P. R.
- Branchesi M.
- Brau J. E.
- Briant T.
- Brillet A.
- Brinkmann M.
- Brisson V.
- Brockill P.
- Broida J. E.
- Brooks A. F.
- Brown D. A.
- Brown D. D.
- Brunett S.
- Buchanan C. C.
- Buikema A.
- Bulik T.
- Bulten H. J.
- Buonanno A.
- Buskulic D.
- Bustillo J. Calderon
- Buy C.
- Byer R. L.
- Cabero M.
- Cadonati L.
- Cagnoli G.
- Cahillane C.
- Callister T. A.
- Calloni E.
- Camp J. B.
- Canizares P.
- Cannon K. C.
- Cao H.
- Cao J.
- Capano C. D.
- CAPOCASA ELEONORA
- Carbognani F.
- Caride S.
- Carney M. F.
- Casentini C.
- Castro J. M. Gonzalez
- Caudill S.
- Cavaglia M.
- Cavalier F.
- Cavalieri R.
- Cella G.
- Cepeda C. B.
- Cerda-Duran P.
- Cerretani G.
- Cesarini E.
- Chamberlin S. J.
- Chan M.
- Chao S.
- Charlton P.
- Chase E.
- Chass
- Chatterjee D.
- Cheeseboro B. D.
- Chen H. Y.
- Chen X.
- Chen Y.
- Cheng H. -.P.
- Chia H.
- Chincarini A.
- Chiummo A.
- Chmiel T.
- Cho H. S.
- Cho M.
- Chow J. H.
- Christensen N.
- Chu Q.
- Chua A. J. K.
- Chua S.
- Chung A. K. W.
- Chung S.
- Ciani G.
- Ciolfi R.
- Cirelli C. E.
- Cirone A.
- Clara F.
- Clark J. A.
- Clearwater P.
- Cleva F.
- Cocchieri C.
- Coccia E.
- Cohadon P. -.F.
- Cohen D.
- Colla A.
- Collette C. G.
- Cominsky L. R.
- Constancio
- Conti L.
- Cooper S. J.
- Corban P.
- Corbitt T. R.
- Cordero-Carrion I.
- Corley K. R.
- Cornish N.
- Corsi A.
- Cortese S.
- Costa C. A.
- Costa C. F. Da Silva
- Coughlin M. W.
- Coughlin S. B.
- Coulon J. -.P.
- Countryman S. T.
- Couvares P.
- Covas P. B.
- Cowan E. E.
- Coward D. M.
- Cowart M. J.
- Coyne D. C.
- Coyne R.
- Creighton J. D. E.
- Creighton T. D.
- Cripe J.
- Crowder S. G.
- Cullen T. J.
- Cumming A.
- Cunningham L.
- Cuoco E.
- D'Antonio S.
- Dal Canton T.
- Dalya G.
- Danilishin S. L.
- Danzmann K.
- Dasgupta A.
- Dattilo V.
- Dave I.
- Davier M.
- Davis D.
- Daw E. J.
- Day B.
- De Laurentis M.
- De Pietri R.
- De Rosa R.
- De Rossi C.
- de Varona O.
- De S.
- DeBra D.
- Degallaix J.
- Del Pozzo W.
- Deleglise S.
- Demos N.
- Denker T.
- Dent T.
- Dergachev V.
- DeRosa R. T.
- DeSalvo R.
- Devenson J.
- Dhur
- Di Fiore L.
- Di Giovanni M.
- Di Girolamo T.
- Di Lieto A.
- Di Pace S.
- Di Palma I.
- Di Renzo F.
- Diaz J. Casanueva
- Diaz M. C.
- Doctor Z.
- Dolique V.
- Donovan F.
- Dooley K. L.
- Doravari S.
- Dorrington I.
- Douglas R.
- Downes T. P.
- Drago M.
- Dreissigacker C.
- Driggers J. C.
- Du Z.
- Ducrot M.
- Dupej P.
- Dwyer S. E.
- e-Mottin E.
- Edo T. B.
- Edwards M. C.
- Effler A.
- Eggenstein H. -.B.
- Ehrens P.
- Eichholz J.
- Eikenberry S. S.
- Eisenstein R. A.
- er-Hyde D. C.
- ers J. R.
- erson S. B.
- erson W. G.
- Essick R. C.
- Estevez D.
- Etienne Z. B.
- Etzel T.
- Evans M.
- Evans T. M.
- ez I. Magana
- ez-Galiana A.
- Factourovich M.
- Fafone V.
- Fair H.
- Fairhurst S.
- Fan X.
- Farinon S.
- Farr B.
- Farr W. M.
- Fauchon-Jones E. J.
- Favata M.
- Fays M.
- Fee C.
- Fehrmann H.
- Feicht J.
- Fejer M. M.
- Fern
- Ferrante I.
- Ferreira E. C.
- Ferrini F.
- Fidecaro F.
- Finstad D.
- Fiori I.
- Fiorucci D.
- Fishbach M.
- Fisher R. P.
- Fitz-Axen M.
- Flaminio R.
- Fletcher M.
- Fong H.
- Font J. A.
- Forsyth P. W. F.
- Forsyth S. S.
- Fournier J. -.D.
- Frasca S.
- Frasconi F.
- Frei Z.
- Freise A.
- Frey R.
- Frey V.
- Fries E. M.
- Fritschel P.
- Frolov V. V.
- Fulda P.
- Fyffe M.
- Gabbard H.
- Gadre B. U.
- Gaebel S. M.
- Gair J. R.
- Gammaitoni L.
- Ganija M. R.
- Gaonkar S. G.
- Garcia-Quiros C.
- Garufi F.
- Gateley B.
- Gaudio S.
- Gaur G.
- Gayathri V.
- Gehrels N.
- Gemme G.
- Genin E.
- GENNAI ALBERTO
- George D.
- George J.
- Gergely L.
- Germain V.
- Ghonge S.
- Ghosh Abhirup
- Ghosh Archisman
- Ghosh S.
- Giaime J. A.
- Giardina K. D.
- Giazotto A.
- Gill K.
- Glover L.
- Goetz E.
- Goetz R.
- Gomes S.
- Goncharov B.
- Gonzalez G.
- Gopakumar A.
- Gorodetsky M. L.
- Gossan S. E.
- Gosselin M.
- Gouaty R.
- Grado A.
- Graef C.
- Granata M.
- Grant A.
- Gras S.
- Gray C.
- Greco G.
- Green A. C.
- Gretarsson E. M.
- Groot P.
- Grote H.
- Grunewald S.
- Gruning P.
- Guidi G. M.
- Guo X.
- Gupta A.
- Gupta M. K.
- Gushwa K. E.
- Gustafson E. K.
- Gustafson R.
- Halim O.
- Hall B. R.
- Hall E. D.
- Hamilton E. Z.
- Hammond G.
- Haney M.
- Hanke M. M.
- Hanks J.
- Hanna C.
- Hannam M. D.
- Hannuksela O. A.
- Hanson J.
- har S.
- Hardwick T.
- Harms J.
- Harry G. M.
- Harry I. W.
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- Publication venue
- American Physical Society
- Publication date
- 01/01/2017
- Field of study
Spinning neutron stars asymmetric with respect to their rotation axis are potential sources of
continuous gravitational waves for ground-based interferometric detectors. In the case of known pulsars a
fully coherent search, based on matched filtering, which uses the position and rotational parameters
obtained from electromagnetic observations, can be carried out. Matched filtering maximizes the signalto-
noise (SNR) ratio, but a large sensitivity loss is expected in case of even a very small mismatch
between the assumed and the true signal parameters. For this reason, narrow-band analysis methods have
been developed, allowing a fully coherent search for gravitational waves from known pulsars over a
fraction of a hertz and several spin-down values. In this paper we describe a narrow-band search of
11 pulsars using data from Advanced LIGOâs first observing run. Although we have found several initial
outliers, further studies show no significant evidence for the presence of a gravitational wave signal.
Finally, we have placed upper limits on the signal strain amplitude lower than the spin-down limit for 5 of
the 11 targets over the bands searched; in the case of J1813-1749 the spin-down limit has been beaten for
the first time. For an additional 3 targets, the median upper limit across the search bands is below the
spin-down limit. This is the most sensitive narrow-band search for continuous gravitational waves carried
out so far
Recommended from our members
Modelling the Volatility of TOCOM Energy Futures: A Regime Switching Realised Volatility Approach
- Author
- Admati
- Agnolucci
- Alizadeh
- Alquist
- Amir H. Alizadeh
- Andersen
- Andersen
- Andersen
- Andersen
- Andersen
- Andersen
- Andersen
- Andersen
- Barndorff-Nielsen
- Barndorff-Nielsen
- Barndorff-Nielsen
- Cabedo
- Chen
- Chen
- Chih-Yueh Huang
- Christoffersen
- Corsi
- Diebold
- Fan
- Figlewski
- Hamilton
- Hansen
- Haugom
- Herrera
- Huang
- Huang
- Ian W. Marsh
- Klein
- Kupiec
- Kyle
- Lamoureux
- Lee
- Liu
- Liu
- Ljung
- Lux
- LyĂłcsa
- Ma
- Martens
- McAleer
- Nomikos
- Patton
- Patton
- Poon
- Sadeghi
- Sadorsky
- SĂ©vi
- Taylor
- Tseng
- Vo
- Wang
- Wei
- Wei
- Publication venue
- 'Elsevier BV'
- Publication date
- 27/06/2019
- Field of study
This paper combines the Heterogeneous Autoregressive Realised Volatility (HAR-RV) model and the Markov Regime Switching (MRS) approach to estimate and forecast volatility of energy futures contracts traded at the Tokyo Commodity Exchange (TOCOM). The proposed MRS-HAR-RV model allows the dynamics of the realised volatility to change as market conditions change. The dataset consists of intraday prices for gasoline, kerosene and crude oil futures. Estimation results suggest MRS-HAR-RV model can capture dynamics of price volatility of energy futures better than alternative models. However, out-of-sample forecast evaluation results show that MRS-HAR-RV can only produce better forecasts for more liquid contracts. Moreover, MRS-HAR-RV model seems to less over-predict and more under-predict the volatility compared to HAR-RV, HAR-RV-CJ, GARCH, and MRS-GARCH models
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
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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 fbâ1 of â 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 inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
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