334 research outputs found
Fractional Systems and Fractional Bogoliubov Hierarchy Equations
- Author
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 30/05/2005
- Field of study
We consider the fractional generalizations of the phase volume, volume
element and Poisson brackets. These generalizations lead us to the fractional
analog of the phase space. We consider systems on this fractional phase space
and fractional analogs of the Hamilton equations. The fractional generalization
of the average value is suggested. The fractional analogs of the Bogoliubov
hierarchy equations are derived from the fractional Liouville equation. We
define the fractional reduced distribution functions. The fractional analog of
the Vlasov equation and the Debye radius are considered.Comment: 12 page
All-optical routing and switching for three-dimensional photonic circuitry
- Author
- A Szameit
- A Szameit
- A Szameit
- C Koos
- DN Christodoulides
- DN Christodoulides
- DN Christodoulides
- DN Christodoulides
- E Dulkeith
- ED Eugenieva
- F Dreisow
- F Lederer
- F Xia
- HS Eisenberg
- I Fushman
- I Mansour
- J Cardenas
- J Leuthold
- J Meier
- J Meier
- JW Fleischer
- K Asakawa
- K Itoh
- KG Makris
- M Heinrich
- M Heinrich
- M Heinrich
- O Bang
- RA Spanke
- S Nolte
- T Fukuda
- T Kampfrath
- T Pertsch
- TF Krauss
- VE Benes
- VR Almeida
- Y Vlasov
- Y Vlasov
- YA Vlasov
- YS Kivshar
- Publication venue
- Nature Publishing Group
- Publication date
- 01/01/2011
- Field of study
The ability to efficiently transmit and rapidly process huge amounts of data has become almost indispensable to our daily lives. It turned out that all-optical networks provide a very promising platform to deal with this task. Within such networks opto-optical switches, where light is directed by light, are a crucial building block for an effective operation. In this article, we present an experimental analysis of the routing and switching behaviour of light in two-dimensional evanescently coupled waveguide arrays of Y- and T-junction geometries directly inscribed into fused silica using ultrashort laser pulses. These systems have the fundamental advantage of supporting three-dimensional network topologies, thereby breaking the limitations on complexity associated with planar structures while maintaining a high dirigibility of the light. Our results show how such arrays can be used to control the flow of optical signals within integrated photonic circuits
Dynamic light diffusion, Anderson localization and lasing in disordered inverted opals: 3D ab-initio Maxwell-Bloch computation
- Author
- A Blanco
- A Fratalocchi
- A Lavrinenko
- A Lubatsch
- A Taflove
- A. Fratalocchi
- AA Chabanov
- AA Chabanov
- AF Koenderink
- C Conti
- C LΓ³pez
- C Vanneste
- C. Conti
- DS Wiersma
- DΒ S Wiersma
- E Yablonovitch
- F Reil
- F Scheffold
- FJP Schuurmans
- G Slavcheva
- GH Watson
- H Altug
- H Cao
- HΒ S SΓΆzΓΌer
- IΒ M Vellekoop
- J Huang
- JD Joannopoulos
- JF Galisteo-LΓ³pez
- K Busch
- K Sakoda
- KM Ho
- LK Teh
- M Allard
- M Scharrer
- M Storzer
- MM Sigalas
- O Painter
- P Lodahl
- R Frank
- S John
- S Noda
- SE Skipetrov
- V Yannopapas
- VA Mandelshtam
- X Jiang
- YA Vlasov
- YA Vlasov
- Z-Y Li
- ZL Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 26/02/2008
- Field of study
We report on 3D time-domain parallel simulations of Anderson localization of
light in inverted disordered opals displaying a complete photonic band-gap. We
investigate dynamic diffusion processes induced by femtosecond laser
excitations, calculate the diffusion constant and the decay-time distribution
versus the strength of the disorder. We report evidence of the transition from
delocalized Bloch oscillations to strongly localized resonances in
self-starting laser processes.Comment: 4 pages, 5 figure
Investigation of the formation of periodic domains structure by electron beam irradiation in lithium niobate single crystals with surface layer modified by proton exchange
- Author
- Publication venue
- Π£ΡΠ€Π£
- Publication date
- 01/01/2016
- Field of study
The equipment of the Ural Center for Shared Use βModern nanotechnologyβ UrFU was used. The research was made possible in part by RFBR (15-32-21102- mol_a_ved), by Government of the Russian Federation (Act 211, Agreement 02.A03.21.0006) and by President of Russian Federation grant for young scientists (MK-8441.2016.2
Beauty photoproduction measured using decays into muons in dijet events in ep collisions at sβ=318 GeV
- Author
- Abramowicz H (Abramowicz, H)
- Adamczyk L (Adamczyk, L)
- Adamus M (Adamus, M)
- Adler V (Adler, V)
- Aghuzumtsyan G (Aghuzumtsyan, G)
- Antonioli P (Antonioli, P)
- Antonov A (Antonov, A)
- Arneodo M (Arneodo, M)
- Bailey DS (Bailey, DS)
- Bamberger A (Bamberger, A)
- Barakbaev AN (Barakbaev, AN)
- Barbagli G (Barbagli, G)
- Barbi M (Barbi, M)
- Bari G (Bari, G)
- Barreiro F (Barreiro, F)
- Bartsch D (Bartsch, D)
- Basile M (Basile, M)
- Behrens U (Behrens, U)
- Bell M (Bell, M)
- Bellagamba L (Bellagamba, L)
- Benen A (Benen, A)
- Bertolin A (Bertolin, A)
- Bhadra S (Bhadra, S)
- Bloch I (Bloch, I)
- Bold T (Bold, T)
- Boos EG (Boos, EG)
- Borras K (Borras, K)
- Boscherini D (Boscherini, D)
- Brock I (Brock, I)
- Brook NH (Brook, NH)
- Brugnera R (Brugnera, R)
- Brummer N (Brummer, N)
- Bruni A (Bruni, A)
- Bruni G (Bruni, G)
- Bussey PJ (Bussey, PJ)
- Butterworth JM (Butterworth, JM)
- Bylsma B (Bylsma, B)
- Caldwell A (Caldwell, A)
- Capua M (Capua, M)
- Carli T (Carli, T)
- Carlin R (Carlin, R)
- Catterall CD (Catterall, CD)
- Chekanov S (Chekanov, S)
- Chiochia V (Chiochia, V)
- Chwastowski J (Chwastowski, J)
- Ciborowski J (Ciborowski, J)
- Ciesielski R (Ciesielski, R)
- Cifarelli L (Cifarelli, L)
- Cindolo F (Cindolo, F)
- Cloth P (Cloth, P)
- Cole JE (Cole, JE)
- Collins-Tooth C (Collins-Tooth, C)
- Contin A (Contin, A)
- Cooper-Sarkar AM (Cooper-Sarkar, AM)
- Coppola N (Coppola, N)
- Cormack C (Cormack, C)
- Corradi M (Corradi, M)
- Corriveau F (Corriveau, F)
- Cottrell A (Cottrell, A)
- D'Agostini G (D'Agostini, G)
- Dal Corso F (Dal Corso, F)
- Danilov P (Danilov, P)
- Dannheim D (Dannheim, D)
- De Pasquale S (De Pasquale, S)
- de Wolf E (de Wolf, E)
- del Peso J (del Peso, J)
- Dementiev RK (Dementiev, RK)
- Derrick M (Derrick, M)
- Deshpande A (Deshpande, A)
- Devenish RCE (Devenish, RCE)
- Dhawan S (Dhawan, S)
- Dobur D (Dobur, D)
- Dolgoshein BA (Dolgoshein, BA)
- Doyle AT (Doyle, AT)
- Drews G (Drews, G)
- Durkin LS (Durkin, LS)
- Dusini S (Dusini, S)
- Eisenberg Y (Eisenberg, Y)
- Ermolov PF (Ermolov, PF)
- Eskreys A (Eskreys, A)
- Ferrando J (Ferrando, J)
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- Geiser A (Geiser, A)
- Genta C (Genta, C)
- Gialas I (Gialas, I)
- Giusti P (Giusti, P)
- Gladilin LK (Gladilin, LK)
- Gladkov D (Gladkov, D)
- Glasman C (Glasman, C)
- Gliga S (Gliga, S)
- Goers S (Goers, S)
- Golubkov YA (Golubkov, YA)
- Goncalo R (Goncalo, R)
- Gonzalez O (Gonzalez, O)
- Gosau T (Gosau, T)
- Gottlicher P (Gottlicher, P)
- Grabowska-Bold I (Grabowska-Bold, I)
- Grijpink S (Grijpink, S)
- Grzelak G (Grzelak, G)
- Gutsche O (Gutsche, O)
- Gwenlan C (Gwenlan, C)
- Haas T (Haas, T)
- Hain W (Hain, W)
- Hall-Wilton R (Hall-Wilton, R)
- Hamatsu R (Hamatsu, R)
- Hamilton J (Hamilton, J)
- Hanlon S (Hanlon, S)
- Hart JC (Hart, JC)
- Hartmann H (Hartmann, H)
- Hartner G (Hartner, G)
- Heaphy EA (Heaphy, EA)
- Heath GP (Heath, GP)
- Helbich M (Helbich, M)
- Heusch C (Heusch, C)
- Hilger E (Hilger, E)
- Hillert S (Hillert, S)
- Hirose T (Hirose, T)
- Hochman D (Hochman, D)
- Holm U (Holm, U)
- Iacobucci G (Iacobucci, G)
- Iga Y (Iga, Y)
- Inuzuka M (Inuzuka, M)
- Irrgang P (Irrgang, P)
- Jakob HP (Jakob, HP)
- Jones TW (Jones, TW)
- Kagawa S (Kagawa, S)
- Kahle B (Kahle, B)
- Kaji H (Kaji, H)
- Kananov S (Kananov, S)
- Karshon U (Karshon, U)
- Karstens F (Karstens, F)
- Kataoka M (Kataoka, M)
- Katkov II (Katkov, II)
- Kcira D (Kcira, D)
- Khein LA (Khein, LA)
- Kim JY (Kim, JY)
- Kim YK (Kim, YK)
- Kind O (Kind, O)
- Kisielewska D (Kisielewska, D)
- Kitamura S (Kitamura, S)
- Koffeman E (Koffeman, E)
- Kohno T (Kohno, T)
- Kooijman P (Kooijman, P)
- Koop T (Koop, T)
- Korzhavina IA (Korzhavina, IA)
- Kotanski A (Kotanski, A)
- Kotz U (Kotz, U)
- Kowal AM (Kowal, AM)
- Kowal M (Kowal, M)
- Kowalski H (Kowalski, H)
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- Krakauer D (Krakauer, D)
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- Kreisel A (Kreisel, A)
- Krumnack N (Krumnack, N)
- Kuze M (Kuze, M)
- Kuzmin VA (Kuzmin, VA)
- Labarga L (Labarga, L)
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- Lainesse J (Lainesse, J)
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- Lee JH (Lee, JH)
- Lelas D (Lelas, D)
- Levchenko BB (Levchenko, BB)
- Levy A (Levy, A)
- Li L (Li, L)
- Lightwood MS (Lightwood, MS)
- Lim H (Lim, H)
- Lim IT (Lim, IT)
- Limentani S (Limentani, S)
- Ling TY (Ling, TY)
- Liu X (Liu, X)
- Lohr B (Lohr, B)
- Lohrmann E (Lohrmann, E)
- Loizides JH (Loizides, JH)
- Long KR (Long, KR)
- Longhin A (Longhin, A)
- Lukina OY (Lukina, OY)
- Luzniak P (Luzniak, P)
- Maddox E (Maddox, E)
- Magill S (Magill, S)
- Mankel R (Mankel, R)
- Margotti A (Margotti, A)
- Marini G (Marini, G)
- Martin JF (Martin, JF)
- Mastroberardino A (Mastroberardino, A)
- Matsuzawa K (Matsuzawa, K)
- Mattingly MCK (Mattingly, MCK)
- McCubbin NA (McCubbin, NA)
- Mellado B (Mellado, B)
- Melzer-Pellmann IA (Melzer-Pellmann, IA)
- Menary S (Menary, S)
- Metlica F (Metlica, F)
- Meyer U (Meyer, U)
- Miglioranzi S (Miglioranzi, S)
- Milite M (Milite, M)
- Mirea A (Mirea, A)
- Monaco V (Monaco, V)
- Montanari A (Montanari, A)
- Musgrave B (Musgrave, B)
- Nagano K (Nagano, K)
- Namsoo T (Namsoo, T)
- Nania R (Nania, R)
- Nguyen CN (Nguyen, CN)
- Nigro A (Nigro, A)
- Ning Y (Ning, Y)
- Notz D (Notz, D)
- Nowak RJ (Nowak, RJ)
- Nuncio-Quiroz AE (Nuncio-Quiroz, AE)
- Oh BY (Oh, BY)
- Olkiewicz K (Olkiewicz, K)
- Pac MY (Pac, MY)
- Padhi S (Padhi, S)
- Paganis S (Paganis, S)
- Palmonari F (Palmonari, F)
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- Park IH (Park, IH)
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- Pawlak JM (Pawlak, JM)
- Pelfer PG (Pelfer, PG)
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- Pesci A (Pesci, A)
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- Plucinski P (Plucinski, P)
- Pokrovskiy NS (Pokrovskiy, NS)
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- Zeuner W (Zeuner, W)
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- Ziegler A (Ziegler, A)
- Ziegler A (Ziegler, A)
- Zotkin SA (Zotkin, SA)
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2003
- Field of study
The photoproduction of beauty quarks in events with two jets and a muon has
been measured with the ZEUS detector at HERA using an integrated luminosity of
110 pbβ1. The fraction of jets containing b quarks was extracted from the
transverse momentum distribution of the muon relative to the closest jet.
Differential cross sections for beauty production as a function of the
transverse momentum and pseudorapidity of the muon, of the associated jet and
of xΞ³jetsβ, the fraction of the photon's momentum participating in
the hard process, are compared with MC models and QCD predictions made at
next-to-leading order. The latter give a good description of the data.Comment: 32 pages, 6 tables, 7 figures Table 6 and Figure 7 revised September
200
Evidence for the h_b(1P) meson in the decay Upsilon(3S) --> pi0 h_b(1P)
- Author
- Adametz A.
- Adye T.
- Ahmed H.
- Alam M. S.
- Albert J.
- Allen M. T.
- Alwyn K. E.
- Andreassen R.
- Angelini C.
- Anh TV
- Anulli F.
- Arnaud N.
- Asgeirsson D. J.
- Aston D.
- Atmacan H.
- Ayad R.
- Bailey D.
- Baldini-Ferroli R.
- Band H. R.
- Banerjee Sw.
- Bard D. J.
- Barlow R. J.
- Bartoldus R.
- Batignani G.
- Behera P. K.
- Bellis M.
- Ben-Haim E.
- Benitez J. F.
- Bernard D.
- Bernlochner F. U.
- Bettarini S.
- Bettoni D.
- Bevan A. J.
- Bhuyan B.
- Bianchi F.
- Biasini M.
- Biassoni P.
- Bingham I.
- Blinov V. E.
- Bloom P. C.
- Blount N. L.
- Bomben M.
- Bondioli M.
- Bonneaud G. R.
- Bozzi C.
- Brau J.
- Briand H.
- Brown D. N.
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- Buenger C.
- Burchat P. R.
- Buzykaev A. R.
- Cakir IT
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- Eigen G.
- Eisner A. M.
- Emery S.
- Ernst J. A.
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- Ferrarotto F.
- Ferrer JAV
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- Gioi L. Li
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- Golubev V. B.
- Gradl W.
- Graham M. T.
- Grauges E.
- Grenier P.
- Gritsan A. V.
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- Jasper H.
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- Kass R.
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- Khan A.
- Kim H.
- Kim P.
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- Kravchenko E. A.
- Kroeger R.
- Kroseberg J.
- Lacker H. M.
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- Lindsay C.
- Liu F.
- Lo Vetere M.
- Lockman W. S.
- Lombardo V.
- Long O.
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- LoSecco J. M.
- Lou X. C.
- Lu C.
- Lueck T.
- Luitz S.
- Lund P.
- Luppi E.
- Lusiani A.
- Luth V.
- Lutz A. M.
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- Manoni E.
- Marchiori G.
- Margoni M.
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- Martinez-Vidal F.
- Mattison T. S.
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- Nagel M.
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- Neal H.
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- Zucchelli S. Stradling AR
- Zucchelli SVazquez F.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Using a sample of 122 million Upsilon(3S) events recorded with the BaBar
detector at the PEP-II asymmetric-energy e+e- collider at SLAC, we search for
the hbβ(1P) spin-singlet partner of the P-wave chi_{bJ}(1P) states in the
sequential decay Upsilon(3S) --> pi0 h_b(1P), h_b(1P) --> gamma eta_b(1S). We
observe an excess of events above background in the distribution of the recoil
mass against the pi0 at mass 9902 +/- 4(stat.) +/- 2(syst.) MeV/c^2. The width
of the observed signal is consistent with experimental resolution, and its
significance is 3.1sigma, including systematic uncertainties. We obtain the
value (4.3 +/- 1.1(stat.) +/- 0.9(syst.)) x 10^{-4} for the product branching
fraction BF(Upsilon(3S)-->pi0 h_b) x BF(h_b-->gamma eta_b).Comment: 8 pages, 4 postscript figures, submitted to Phys. Rev. D (Rapid
Communications
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
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- Yoosoofmiya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zdrazil M
- Zeitnitz C
- Zeller M
- Zema PF
- Zemla A
- Zendler C
- Zenin AV
- Zenin O
- Zenis T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zilka B
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- 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
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
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- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
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- Antonaki A
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- Antonov A
- Antos J
- Anulli F
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- Apolle R
- Arabidze G
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- Yamazaki Y
- Yan Z
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- Yildizb HD
- Yilmaz M
- Yoosootiniya R
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- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
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- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
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- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- 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 βs = 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 pTβ₯20 GeV and pseudorapidities {pipe}Ξ·{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}Ξ·{pipe}<0. 8) for jets with 60β€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2β€{pipe}Ξ·{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. Β© 2013 CERN for the benefit of the ATLAS collaboration
The Study of Quantum Interference in Metallic Photonic Crystals Doped with Four-Level Quantum Dots
- Author
- Ali Hatef
- BD Gerardot
- CM Soukoulis
- E Paspalakis
- E Yablonovitch
- ER Brown
- F Cuesta-Soto
- G Raschke
- H Nakamura
- I El-Kady
- I Haque
- I Puscasu
- JG Fleming
- JM Lourtioz
- K Asakawa
- K Hennessy
- K Liu
- K Yasumoto
- M Scalora
- Mahi Singh
- MJ Bloemer
- MR Singh
- MR Singh
- MR Singh
- MSZ Marlan Orvil Scully
- N Eradat
- P Lodahl
- P Zhou
- S John
- S John
- S John
- S John
- S John
- SGJ John
- SY Lin
- SY Zhu
- T Yoshle
- U Akram
- VI Rupasov
- VI Rupasov
- VI Rupasov
- YA Vlasov
- Z Wang
- Publication venue
- Springer
- Publication date
- 01/01/2010
- Field of study
In this work, the absorption coefficient of a metallic photonic crystal doped with nanoparticles has been obtained using numerical simulation techniques. The effects of quantum interference and the concentration of doped particles on the absorption coefficient of the system have been investigated. The nanoparticles have been considered as semiconductor quantum dots which behave as a four-level quantum system and are driven by a single coherent laser field. The results show that changing the position of the photonic band gap about the resonant energy of the two lower levels directly affects the decay rate, and the system can be switched between transparent and opaque states if the probe laser field is tuned to the resonance frequency. These results provide an application for metallic nanostructures in the fabrication of new optical switches and photonic devices
Study of the K- -> pi0 e- nu decay
- Author
- A. A. Sokolov
- A. P. Filin
- A. S. Konstantinov
- A. V. Inyakin
- A. Yu. Polyarush
- B. Zh. Zalikhanov
- E. S. Ginsberg
- E. V. Vlasov
- G. A. Akopdzhanov
- G. I. Britvich
- H. Steiner
- I. G. Britvich
- I. V. Ajinenko
- I. Ya. Korolkov
- J. Gasser
- K. S. Belous
- M. M. Shapkin
- N. A. Shalanda
- N. E. Smirnov
- O. G. Tchikilev
- O. P. Yushchenko
- S. A. Akimenko
- S. A. Akimenko
- S. Shimizu
- S. V. Laptev
- S. V. Yashchenko
- V. A. Khmelnikov
- V. A. Polyakov
- V. A. Senko
- V. E. Postoev
- V. F. Konstantinov
- V. F. Obraztsov
- V. I. Romanovsky
- V. I. Shelikhov
- V. M. Leontiev
- V. M. Ronjin
- V. N. Bolotov
- V. N. Bolotov
- V. N. Govorun
- V. P. Novikov
- V. Z. Serdyuk
- Publication venue
- 'Pleiades Publishing Ltd'
- Publication date
- 17/12/2001
- Field of study
The decay K- -> pi0 e- nu has been studied using in-flight decays detected
with "ISTRA+" setup operating at the 25 GeV negative secondary beam of the U-70
PS. About 130K events were used for the analysis. The lambda_+ parameter of the
vector formfactor has been measured: lambda_+ = 0.0293 +- 0.0015(stat) +-
0.002(syst).
The limits on the possible tensor and scalar couplings have been derived:
f_T/f_+(0)=-0.044 +0.059 -0.057 (stat) f_S/f_+(0)=-0.020 +0.025 -0.016 (stat)Comment: 11 pages, Latex, 9 picture
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