| Sample search results for: a3 resonances |
| 1 | 2696 ieee transactions on ultrasonics, ferroelectrics, and frequency control, vol. 54, no. 12, december 2007 Correspondence | ||
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Summary: (x, t) t2 - bA 3 u(x, t) tx2 - Y A 2 u(x, t) x2 = f(x, t) x , (3) 08853010/$25.00 c 2007 IEEE #12... displacement) in the resonator, 60 GHz resonators are proposed with 50 motional impedance. I. Introduction... With quality factors (Q) often exceeding 10,000, vi- brating micromechanical ... |
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Source: Afshari, Ehsan - School of Electrical and Computer Engineering, Cornell University |
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Collection: Engineering |
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| 2 | Geometry of Resonance Tongues with Martin Golubitsky, Sijbo Holtman, Mark Levi, | ||
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Summary: ( ) exponentially narrow around families of parabolæ Fold between pictures 1 and 2 A3 Resonance p.27/36 #12... Geometry of Resonance Tongues Henk Broer with Martin Golubitsky, Sijbo Holtman, Mark Levi, Carles... Sim´o & Gert Vegter Instituut voor Wiskunde en Informatica Rijksuniversiteit Groningen ... |
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Source: Broer, H.W. - Department of Mathematics and Computing Science, Rijksuniversiteit Groningen |
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Collection: Mathematics ; Physics |
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| 3 | Appl Phys B (2010) 98: 353363 DOI 10.1007/s00340-009-3824-1 | ||
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Summary: (r) (a 3N × 1 ma- trix) in the cluster subspace has the form: E(r) = 3N n=1 An(s).Rn, (8) where Rn... Appl Phys B (2010) 98: 353363 DOI 10.1007/s00340-009-3824-1 Interplay of plasmon resonances... surface plasmon resonances is extended to binary nanostructures. Based on the near field coupling |
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Source: Floreano, Dario - Laboratory of Intelligent Systems, Ecole Polytechnique Fédérale de Lausanne |
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Collection: Computer Technologies and Information Sciences ; Engineering |
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| 4 | Icarus 193 (2008) 213223 www.elsevier.com/locate/icarus | ||
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Summary: are as follows: (A.2)hi = ei cosi, (A.3)ki = ei sini, (A.4)~ai = 2 i /mii, where we label the satellites... evolution through several resonances involving Mimas, Enceladus, and/or Dione is studied numerically... with an averaged resonance model. We find that, in the EnceladusDione 2:1 e-Enceladus type ... |
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Source: Wisdom, Jack - Computer Science and Artificial Intelligence Laboratory & Department of Earth, Atmospheric, and Planetary Sciences, Massachusetts Institute of Technology (MIT) |
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Collection: Physics |
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| 5 | VOLUME 82, NUMBER 12 P H Y S I C A L R E V I E W L E T T E R S 22 MARCH 1999 Strongly Enhanced Inelastic Collisions in a Bose-Einstein Condensate | ||
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Summary: the root-mean-square velocity n m2 y2 rms 4p ¯h2a . (3) The peak density n0 is given by n0 7 4 n... Inelastic Collisions in a Bose-Einstein Condensate near Feshbach Resonances J. Stenger, S. Inouye, M. R... near a Feshbach resonance. Feshbach resonances affect elastic collisions and ... |
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Source: Harvard University, Center for Ultracold Atoms, Alkali Quantum Gases Group |
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Collection: Physics |
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| 6 | J. Phys. III FYauce 5 (1995) 1245-1253 AUGUST 1995, PAGE 1245 Classification | ||
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Summary: ~t3 = a3 = ((~) lfr3j (3) where xm is the m~~ rooth of the Bessel function of the first kind and n... .85 77.80 06.70M Investigation on Displacement Sensitivity of Cylindrical Dielectric Resonators... 1995, accepted 3 May 1995) Abstract. In order to design displacement resonant transducers in UHF |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 7 | Robust and Efficient Interaction with Complex Systems * Glenn C. Foster | ||
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Summary: xn), with a period 4 dynamics (a=3.46). The resonant forcing function is computed with Eq. 5, however... maximum at b=a. (N=4, x0=0.37, a=3.6 , F=0.001). 4 Conclusions We show that resonant forcing functions... of a chaotic logistic map dynamics xn+1 = a xn (1 ... |
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Source: Hubler, Alfred - Department of Physics, University of Illinois at Urbana-Champaign |
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Collection: Physics |
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| 8 | SUPPORT LOSS IN MICROMECHANICALDISKRESONATORS Zhili Ha0 andFavrukh Ayazi | ||
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Summary: -supported disk resonators (a) 3pm-thick disk resonator (dula used in row 3 of Table I ) (b) beam dimensions (c... , Atlanta, GA 30332-0250, USA AFSTRACT In light of recent efforts to implement micromechanical resonators... with high+ and high frequency, an analytical model for support ... |
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Source: Ayazi, Farrokh - School of Electrical and Computer Engineering, Georgia Institute of Technology |
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Collection: Engineering |
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| 9 | COPYRIGHT NOTICE The material available on this page is presented to ensure timely dissemination | ||
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Summary: interaction near strong resonance leads to oscillatory instability. The 3-bus results first appeared in [8]. A... the first corollary in Arnold [2, chapter 6, section 30E]). APPENDIX B POWER SYSTEM MODELS A. 3-bus System... --I: FUNDAMENTAL THEORY AND APPLICATIONS, VOL. 48, NO. 3, MARCH 2001 Is Strong Modal ... |
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Source: Arizona State University, Power Systems Engineering Research Center |
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Collection: Power Transmission, Distribution and Plants |
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| 10 | 340 IEEE TRANSACTIONS ON CIRCUITS AND SYSTEMS--I: FUNDAMENTAL THEORY AND APPLICATIONS, VOL. 48, NO. 3, MARCH 2001 Is Strong Modal Resonance a Precursor to Power | ||
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Summary: interaction near strong resonance leads to oscillatory instability. The 3-bus results first appeared in [8]. A... the first corollary in Arnold [2, chapter 6, section 30E]). APPENDIX B POWER SYSTEM MODELS A. 3-bus System... . 3, MARCH 2001 Is Strong Modal Resonance a Precursor to Power ... |
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Source: Dobson, Ian - Department of Electrical and Computer Engineering, University of Wisconsin at Madison |
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Collection: Power Transmission, Distribution and Plants |
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| 11 | FIBER RING RESONATOR BASED OPTO-ELECTRONIC OSCILLATOR -PHASE NOISE OPTIMISATION AND THERMAL | ||
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Summary: (dBc/Hz) Frequency(Hz) Proc. of SPIE Vol. 7936 79360A-3 #12;3. OEO WHITE FREQUENCY NOISE OPTIMISATION The theoretical... FIBER RING RESONATOR BASED OPTO-ELECTRONIC OSCILLATOR - PHASE NOISE OPTIMISATION AND THERMAL... the quality Q factor in a system. Different types of optical resonators lead to Q factors ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 12 | nature materials | VOL 9 | SEPTEMBER 2010 | www.nature.com/naturematerials 707 alileo Galilei recognized the resonance effect in his study of | ||
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Summary: .0 1.0 0.5 Re(a1,2) 1 q 2 4 6 8q 5 4 a1 a1a2 a3 a3 a2 3 SurfacemodesVolumemodes 2 1 2 Figure 1... recognized the resonance effect in his study of musical strings as early as 1602. Subsequently it was found... that resonances -- such as mechanical, acoustic and elec- ... |
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Source: Zheludev, Nikolay - Optoelectronics Research Centre & School of Physics and Astronomy, University of Southampton |
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Collection: Materials Science ; Physics |
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| 13 | High-Order Micromechanical Electronic Filters Kun Wang and Clark T.-C. Nguyen | ||
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Summary: ) Equivalent LCR network. RQ11 RQ12 RQ31 Vf1 A2 A1 A3 Lx1Rx1 Cx1 Lx2Rx2 Cx2 Lx3Rx3 Cx3 C12 C23 -C23-C23-C12 -C... -to-single-ended converter A3. III. FILTER DESIGN Figure 4 presents an ideal bandpass filter spectrum and defines parameters... of three folded-beam resonators coupled by ... |
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Source: Nguyen, Clark T.-C. - Department of Electrical Engineering and Computer Sciences, University of California at Berkeley |
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Collection: Engineering |
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| 14 | Summary: Theory Working Group RICHARD BAARTMAN | ||
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Summary: Summary: Theory Working Group RICHARD BAARTMAN TRIUMF, 4004 Wesbrook Mall, Vancouver B.C., V6T 2A3... of resonance in synchrotron. (II) 2. Methods and accuracy of emittance growth and particle losses by resonance... RELATIONSHIP BETWEEN SINGLE PARTICLE AND COHERENT PICTURES OF RESONANCE ... |
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Source: Baartman, Richard Abram - TRIUMF |
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Collection: Plasma Physics and Fusion |
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| 15 | Summary: Theory Working Group RICHARD BAARTMAN | ||
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Summary: Summary: Theory Working Group RICHARD BAARTMAN TRIUMF, 4004 Wesbrook Mall, Vancouver B.C., V6T 2A3... of resonance in synchrotron. (II) 2. Methods and accuracy of emittance growth and particle losses by resonance... RELATIONSHIP BETWEEN SINGLE PARTICLE AND COHERENT PICTURES OF RESONANCE ... |
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Source: Baartman, Richard Abram - TRIUMF |
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Collection: Plasma Physics and Fusion |
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| 16 | 84 IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, VOL. 48, NO. 1, JANUARY 2000 An Efficient Full-Wave Method for Analysis of | ||
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Summary: by applying PMC basis functions (A3). The result of a convergence test for the com- plex frequency... ( and ) PMC modes (A3) modes where is the Bessel function of the first kind and is the th root of ; i... Full-Wave Method for Analysis of Dielectric Resonators Possessing Separable ... |
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Source: Hanson, George - Department of Electrical Engineering and Computer Science, University of Wisconsin-Milwaukee |
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Collection: Materials Science ; Engineering |
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| 17 | Multiple-state Feshbach resonances mediated by high-order couplings Christopher J. Hemming* and Roman V. Krems | ||
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Summary: bound states increases Fig. 2 . Model (ii). The couplings A2 A3 ¯ An-1 form the arithmetic series Ak=A2... of coupling when A is small. Model (iii). The couplings A2 A3 ¯ An-1 form the geometric series Ak=rk-2 A2... state energy k relative to energies of other bound states. Model (iv). The couplings ... |
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Source: Krems, Roman - Department of Chemistry, University of British Columbia |
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Collection: Physics ; Chemistry |
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| 18 | Measurement of lateral stress in argon implanted thin gold lms using quartz resonator techniques | ||
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Summary: and not for smoothness. The system of equations representing the three resonators is: fAT faAT ATDw ATD e À a3 f À a... Measurement of lateral stress in argon implanted thin gold ®lms using quartz resonator techniques A... three quartz resonators of dierent crystallographic cuts ... |
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Source: Webb, Roger P. - Department of Electronic Engineering, University of Surrey |
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Collection: Materials Science ; Physics ; Engineering |
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| 19 | J. Fluid Mech. (2010), vol. 643, pp. 437447. c Cambridge University Press 2010 doi:10.1017/S0022112009992850 | ||
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Summary: .8), it is seen that the amplitude of the resonant wave has a maximum of a3,max = a10 -3/1. If m < 1, then a1... d + a2 da2 d + a3 da3 d = 0. (3.1) Therefore we have, in general, da1 d = 1a2a3, da2 d = ... |
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Source: Alam, Mohammad-Reza - Department of Mechanical Engineering, Massachusetts Institute of Technology (MIT) |
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Collection: Engineering |
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| 20 | An electromechanical mixing technique has been demonstrated for accurately measuring the performance | ||
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Summary: -------= C x C x ------- Co d ------ 1 A1x A2x 2 A3x 3 ...+ + +( )= Fres CoV1 V2 V3+( ) 2d... -Q micromechani- cal resonators under conditions where parasitic effects could otherwise mask motional output... transducers, allowing an off-resonance input signal to mix down to a force at the ... |
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Source: Nguyen, Clark T.-C. - Department of Electrical Engineering and Computer Sciences, University of California at Berkeley |
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Collection: Engineering |
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| 21 | Baryon spectroscopy on the lattice Valentina Verduci | ||
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Summary: + a2e-E2t + a3e-E3t + ... + noise Valentina Verduci Baryon spectroscopy on the lattice #12;The Roper... Function Cij (t) = i (t) j (0) = a1e-E1t + a2e-E2t + a3e-E3t + ... exponential decay with the energy mass... Valentina Verduci Baryon spectroscopy on the lattice #12;The Roper ... |
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Source: Rossak, Wilhelm R. - Fakultät für Mathematik und Informatik, Friedrich-Schiller-Universität Jena |
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Collection: Computer Technologies and Information Sciences |
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| 22 | Icarus 188 (2007) 386399 www.elsevier.com/locate/icarus | ||
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Summary: :1, the satellites' semi-major axes must satisfy a3 P /a3 L 4; they then evolve following Eq. (1), and the two... #12;Icarus 188 (2007) 386399 www.elsevier.com/locate/icarus Orbital resonances in the inner... neptunian system I. The 2:1 ProteusLarissa mean-motion ... |
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Source: Hamilton, Douglas P. - Department of Astronomy, University of Maryland at College Park |
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Collection: Physics |
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| 23 | 860 IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, VOL. 15, NO. 2, JUNE 2005 Fabrication and Characterization of Superconducting | ||
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Summary: [18] exposing a bilayer resist (500 nm MMA- (8.5)MAA EL13 and 100 nm 950 K PMMA A3) by e... QED. The cavities are transmission line resonators made by photolithography. They are coupled to the input... bridge double-angle evaporation in superconducting resonators with high quality factor. An impor- tant |
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Source: Schoelkopf, Robert J.- Department of Applied Physics, Yale University; Wallraff, Andreas - Departement Physik, Eidgenössische Technische Hochschule Zürich (ETHZ) |
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Collection: Engineering ; Materials Science ; Physics |
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| 24 | Astronomy & Astrophysics manuscript no. aa3355-05 (DOI: will be inserted by hand later) | ||
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Summary: migrating via the Yarkovsky effect are first captured into three-body (5J-4S-1A, 3J+1S-1A, etc.), nonlinear... -type asteroids outside the Vesta family I. Interplay of nonlinear secular resonances and the Yarkovsky effect... the interplay of Yarkovsky effect and nonlinear secular resonances. The main ... |
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Source: Nesvorny, David - Department of Space Studies, Southwest Research Institute |
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Collection: Physics |
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| 25 | Mon. Not. R. Astron. Soc. (2011) doi:10.1111/j.1365-2966.2011.18442.x Dynamical resonant structures in meteoroid stream orbits | ||
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Summary: . Similarly, for first-order resonances we obtain amax a = ± 16 3 SRapprox n2a3 1 2 1 + SRapprox 27e4n2a2 1 2... of Physics and Astronomy, University of Western Ontario, London, Ontario N6A 3K7, Canada 4Department... coefficients describing the direct terms of the expansion of the ... |
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Source: Hamilton, Douglas P. - Department of Astronomy, University of Maryland at College Park |
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Collection: Physics |
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| 26 | JOURNAL OF MICROELECTROMECHANICAL SYSTEMS, VOL. 13, NO. 6, DECEMBER 2004 1043 VHF Single-Crystal Silicon Elliptic Bulk-Mode | ||
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Summary: ), respectively, the elastic equations for the P-wave and S-wave may be written as (3a) (3b) where in polar... -Crystal Silicon Elliptic Bulk-Mode Capacitive Disk Resonators--Part I: Design and Modeling Zhili Hao, Member, ASME... resonators operating in their elliptical bulk resonant mode. ... |
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Source: Ayazi, Farrokh - School of Electrical and Computer Engineering, Georgia Institute of Technology |
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Collection: Engineering |
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| 27 | Mon. Not. R. Astron. Soc. 000, 120 (2002) Printed 16 December 2010 (MN LATEX style file v2.2) Dynamical Resonant Structures in Meteoroid Stream | ||
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Summary: . Similarly, for first order resonances we obtain: amax a = ± 16 3 SRapprox n2a3 1 2 1 + SRapprox 27e4n2a2 1 2... coefficients describing the direct terms of the expansion of the disturbing function, = a/a , and G = n2 a3... = ± 16 3 SRapproxa3 GM 1 2 (5) Here the mean motion ... |
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Source: Hamilton, Douglas P. - Department of Astronomy, University of Maryland at College Park |
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Collection: Physics |
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| 28 | UHF High-Order Radial-Contour-Mode Disk Resonators John R. Clark, Mohamed A. Abdelmoneum, and Clark T.-C. Nguyen | ||
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Summary: ------------= Co1 r Co1 r ------------ Co1 d --------- 1 A1r A2r 2 A3r 3 ...+ + +( )= Fres CoVLOVRF 2d... 1 of 8 UHF High-Order Radial-Contour-Mode Disk Resonators John R. Clark, Mohamed A. Abdelmoneum... Abstract--A micromechanical, laterally vibrating disk resonator, fabricated via a technology combining |
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Source: Nguyen, Clark T.-C. - Department of Electrical Engineering and Computer Sciences, University of California at Berkeley |
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Collection: Engineering |
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| 29 | Transverse lightwave circuits in microstructured optical fibers: resonator | ||
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Summary: -1 r b)a) 3 2 1 3 2 1 2 0 2 1 2 1 10 1 1 2 1 = = =- = = - = - C C P P P wr wr... Transverse lightwave circuits in microstructured optical fibers: resonator arrays Maksim... is enabled by transverse resonator arrays built into a fiber crossection. Such a design allows unlimited |
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Source: Skorobogatiy, Maksim - Département de Génie Physique, École Polytechnique de Montréal |
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Collection: Engineering |
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| 30 | Europhys. Lett., 71 (1), pp. 6369 (2005) DOI: 10.1209/epl/i2005-10064-8 | ||
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Summary: Input and transmitted pulses through (a) 3D and (b) 2D double phononic crystals. The number of layers... Amplitude transmission coefficient through (a) 3D and (b) 2D double phononic crystals. The- oretical... crystals 67 Fig. 3 Frequency dependence of the measured group time through ... |
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Source: Page, John - Department of Physics and Astronomy, University of Manitoba |
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Collection: Physics |
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| 31 | This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research | ||
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Summary: axis a, 3:2 resonant argument, distance to Earth and to Mars. Step-like changes in a at 5300, 5700... , Athabasca University, 1 University Drive, Athabasca AB, T9S 3A3, Canada b Department of Physics, University... of Alberta, c/o 1 University Drive, Athabasca AB, T9S ... |
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Source: Wiegert, Paul - Department of Physics and Astronomy, University of Western Ontario |
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Collection: Physics |
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| 32 | Fermi National Accelerator Laboratory FERMILAB-Conf-99/276 | ||
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Summary: , b9. Similarlythe skew resonance 2Qx+Qy has primary contributionsfrom a3 and subsidiary contributions... was also derived from Scheme Zeroed random multipoles 2 (b3, b4, b5, b6) & (a3, a4, a5, a6) 4 (b3, b4, b5... , b6, b10) & (a3, a4, a5, ... |
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Source: Sen, Tanaji - Accelerator Physics Department, Fermi National Accelerator Laboratory |
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Collection: Physics |
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| 33 | Vol. 37 (2006) ACTA PHYSICA POLONICA B No 8 NEUTRINOPRODUCTION OF THE RESONANCES | ||
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Summary: be used for any resonance. The Q2 dependencies of gA 1 (Q2) and gA 3 (Q2) must be checked and determined... /2 = K R, + 1 2 Jem · (R) N, - 1 2 , (2.1) A3/2 = K R, + 3 2 Jem · (R) N, + 1 2 , (2.2) S1/2 = K qz Q2 R... |N = ¯u(p ) gV 1 µ2 (Q2 + q/q )5+ gV 2 µ i q5- gA 1 - ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 34 | T h e o p e n a c c e s s j o u r n a l f o r p h y s i c s New Journal of Physics | ||
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Summary: (dB) 20 25 3.4 3.6 (b)(a) 3.8 4.0 Frequency (GHz) 4.2 4.4 t = 0.2 mm t = 0.3 mm t = 0.4 mm t = 0.5 mm... .8 pF 1.8 2.0 Frequency (GHz) 2.2 2.4 2.6 2.8 3.0 (b)(a) 3.21.2 1.4 1.61.8 2.0 Frequency (GHz) 2.2 2... of magnetic resonances for different split-ring ... |
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Source: Foundation of Research and Technology, Hellas, Institute of Electronic Structure and Laser, Photonic, Phononic and Meta- Materials Group; Ozbay, Ekmel - Department of Electrical and Rlectronics Engineering & Physics, Bilkent University; Soukoulis, Costas - Ames Laboratory & Department of Physics and Astronomy, Iowa State University |
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Collection: Materials Science ; Physics |
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| 35 | JOURNAL OF MICROELECTROMECHANICAL SYSTEMS, VOL. 13, NO. 5, OCTOBER 2004 715 Nonlinear Limits for Single-Crystal | ||
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Summary: . MECHANICAL NONLINEARITY IN SILICON BAW RESONATORS As was shown in Section III-A3, the geometrical nonlinear... with the focus on mechanical nonlinearities. The bulk acoustic wave (BAW) resonators are shown to have orders... -of-magnitude higher energy storage capability than flex- ural beam ... |
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Source: Kaajakari, Ville - VTT Information Technology |
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Collection: Engineering |
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| 36 | Nanoscale optofluidic sensor arrays Sudeep Mandal1 | ||
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Summary: . Figure 1(b) shows the fundamental quasi-TE mode for this waveguide geometry. (a) (b) Fig. 1. (a) 3D... ). Figure 4(b) shows an SEM image of the NOSA. (a) (b) (c) Fig. 4. (a) 3D schematic showing a PDMS channel... is based on the use of arrays of 1D photonic crystal resonators which are ... |
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Source: Erickson, David - Sibley School of Mechanical and Aerospace Engineering, Cornell University |
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Collection: Chemistry ; Engineering |
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| 37 | ON THE EXISTENCE OF A SECOND J03C0 = 0+ RESONANCE AT HIGH EXCITATION ENERGY IN 24Mg | ||
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Summary: 12C(12C, a3 )2oNe, a strong conjecture existed that a J1t = 0+ resonance is present around... a particles leading to the Jn = 2- state at 4.97 MeV in 2°Ne(a3) since, in this case, even values... and a3 around 5.8 MeV for two mutually distant ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 38 | UNIVERSITY of CALIFORNIA Santa Barbara | ||
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Summary: resonator base wiring . . . . . . . . . . . . . . . 96 A.3 Expanded view of novel mechanical resonator base... . . . . . . . . . . . . . . . . . . . . . . . 130 A.2.3 Lithography and etches . . . . . . . . . . . . . . . . . . . . 133 A.3 Tips and tricks... . . . . . ... |
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Source: Martinis, John M. - Department of Physics, University of California at Santa Barbara |
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Collection: Computer Technologies and Information Sciences ; Physics |
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| 39 | Stark and field-born resonances of an open square well in a static external electric field | ||
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Summary: =- and x= we find a1 z ,a2 z , and a3 z : 194101-2 A. Emmanouilidou and N. Moiseyev J. Chem. Phys. 122... - z Ai - V0 - z - Ai - z Ai - V0 - z , a3 = a1 Ai - - V0 - z + a2 Bi - - V0 - z / Ci+ - - z , as well... Stark and field-born resonances of an open square well in a static external ... |
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Source: Moiseyev, Nimrod - Department of Chemistry, Technion, Israel Institute of Technology |
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Collection: Chemistry ; Physics |
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| 40 | Maximum Number of Finite Transmission Zeros of Coupled Resonator Filters With Source/Load-Multiresonator Coupling and a Given Topology | ||
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Summary: determinants using Kramer's rule, i.e., cofactorill, [A-`h = Det(A) (3) This equation shows... Maximum Number of Finite Transmission Zeros of Coupled Resonator Filters With Source... be achieved by a network of n coupled resonators with a fixed topology matrix when the source or the load |
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Source: Bornemann, Jens - Department of Electrical and Computer Engineering. University of Victoria |
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Collection: Engineering |
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| 41 | coupled resonator optical waveguide 60 bending 60 Bending properties of single mode photonic crystal coupled resonator optical | ||
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Summary: mode splitting 1.(c) band diagram . 2. design CROW H-field . T1A-3/Photonics Conference 2007... input CROW output CROW hole 0.38a . 3.(b) coupling cavity CROW 30° dipole - design . CROW... 2 hole CROW 0.38a . Simulation 3.(c), bending transmission spectrum 3.(d) . ... |
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Source: Park, Namkyoo - School of Electrical Engineering and Computer Science, Seoul National University |
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Collection: Engineering |
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| 42 | ICARUS 127, 93111 (1997) ARTICLE NO. IS965669 | ||
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Summary: completely unknown. Specifying a point on the plot is equivalent to specifying the ratios a1 : a2 : a3... and a2/a3, it is compa- rable to the extent of evolution expected over Solar System occurs at a larger... ICARUS 127, 93111 (1997) ARTICLE NO. IS965669 Tidal Evolution into the Laplace ... |
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Source: Showman, Adam -Lunar and Planetary Laboratory, Department of Planetary Sciences, University of Arizona |
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Collection: Physics |
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| 43 | BRIDGED MICROMECHANICAL FILTERS Sheng-Shian Li, Mustafa U. Demirci, Yu-Wei Lin, Zeying Ren, and Clark T.-C. Nguyen | ||
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Summary: designs realized in this work. (a) 3CC filter with /4 bridging beam design (3CC /4). (b) 3CC filter with 3... --High-order micromechanical filters comprised of 3 to 4 mechanically coupled resonators, and employing for the first time... "bridging" between nonadjacent resonators to affect loss poles for better ... |
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Source: Nguyen, Clark T.-C. - Department of Electrical Engineering and Computer Sciences, University of California at Berkeley |
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Collection: Engineering |
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| 44 | Nonlinear Dyn (2007) 50:147160 DOI 10.1007/s11071-006-9148-3 | ||
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Summary: obtain A4 (3 cos() + 48) - 16A3 3 = - 2564 3( + 16)3 (39) The thickness of the 4:1 resonance band... - ate the constant of integration, we obtain the following equation A4 (3 cos() + 12) - 8A3 3 = - 164... A = - A2 2R (66) Integrating Equation (66), we obtain the first integral R2 2 + ... |
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Source: Rand, Richard H. - Department of Theoretical and Applied Mechanics, Cornell University |
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Collection: Engineering |
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| 45 | phys. stat. sol. (b) 244, No. 4, 11971201 (2007) / DOI 10.1002/pssb.200674506 2007 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim | ||
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Summary: at (a) 3.77 GHz and (b) 11.92 GHz. #12;1200 K. Aydin and E. Özbay: Experimental and numerical analyses... -VCH Verlag GmbH & Co. KGaA, Weinheim Original Paper Experimental and numerical analyses of the resonances... of split ring resonators Koray Aydin* and Ekmel Özbay Nanotechnology Research ... |
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Source: Ozbay, Ekmel - Department of Electrical and Rlectronics Engineering & Physics, Bilkent University |
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Collection: Physics ; Materials Science |
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| 46 | Session: FC2-A THIN FILM RESONATORS (FBAR) | ||
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Summary: for help with the network analyzer and RF probe station. FC2-A-3 511DE 2:00 p.m. ELECTRICALLY TUNABLE... Session: FC2-A THIN FILM RESONATORS (FBAR) Chair: A. Kong Northrop Grumman Corporation FC2-A-1 511... OF THIN FILM BULK ACOUSTIC WAVE RESONATORS Q. CHEN*, F. LI, and Q.-M. WANG, University of Pittsburgh |
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Source: MacDonald, Noel C. - Materials Department, University of California at Santa Barbara; Turner, Kimberly - Department of Mechanical and Environmental Engineering, University of California at Santa Barbara |
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Collection: Engineering ; Materials Science |
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| 47 | Icarus 159, 284299 (2002) doi:10.1006/icar.2002.6927 | ||
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Summary: of the 12/7 mean motion resonance with Jupiter (a 3.63 AU). Its orbit is very chaotic (Lyapunov time TL... for the outer belt. The p's are selected so that 1.9 a 3.9 AU. By adding the 3/2 resonance (a 3.96 AU), where... in the Asteroid Belt: A Comparative Study ... |
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Source: Varvoglis, Harry - Department of Physics, Aristotle University of Thessaloniki |
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Collection: Physics |
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| 48 | QUBIT-RESONATOR SYSTEM AS AN APPLICATION TO QUANTUM COMPUTATION | ||
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Summary: ^z + ¯h^a ^a - g(^a ^- + ^a^+ ), (3.15) which is the famous Jaynes-Cummings Hamiltonian. Here again... also be made by expanding the unitary transformation with the operator ^U = exp[(g/)(^a^+ - ^a ^- )]. 3... QUBIT-RESONATOR SYSTEM AS AN APPLICATION TO QUANTUM COMPUTATION Ren-Shou Huang ... |
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Source: Schoelkopf, Robert J.- Department of Applied Physics, Yale University |
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Collection: Engineering |
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| 49 | Nonlinear Waves Roger Grimshaw, Gennady El, Karima Khusnutdinova | ||
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Summary: (-i(1 + 2)) + (m 2 n 3 + m 3 n 2 )A 2A 3 exp(-i(2 + 3)) + (m 3 n 1 + m 1 n 3 )A 3A 1 exp(-i(3 + 1)) + c... . To avoid secular growth we require T1 + c1 X1 A1 = iµ1A 2A 3, T1 + c2 X1 A2 = iµ2A 3A 1, T1 + c3 X1 ... |
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Source: Khusnutdinova, Karima - Department of Mathematical Sciences, Loughborough University |
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Collection: Mathematics |
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| 50 | THE ASTRONOMICAL JOURNAL, 115:16531663, 1998 April 1998. The American Astronomical Society. All rights reserved. Printed in the U.S.A.( | ||
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Summary: t [ ) e [ g 1 [ h 1 )& [ h 1 ( (3) yields H1 res @ \ n 2 & ] n 1 J 2 AR E a 1 B2 L @ A3 4 sin2 v [ 1 2 B 1... eviction Hamiltonian is then H i \ n 2 & ] n 1 J 2 AR E a 1 B2 L @ A3 4 sin2 v [ 1 2 B 1 (1 [ e2)3@2 ] n 2... rights reserved. Printed in the U.S.A.( RESONANCES IN ... |
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Source: Wisdom, Jack - Computer Science and Artificial Intelligence Laboratory & Department of Earth, Atmospheric, and Planetary Sciences, Massachusetts Institute of Technology (MIT) |
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Collection: Physics |
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| 51 | Eigenstate assignments and the quantum-classical correspondence for highly-excited vibrational states of the Baggot H2O Hamiltonian | ||
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Summary: resonance channels in action space, as determined by Chirikov resonance analysis. More detailed analysis... determining the exact periodic orbits and their bifurcations and families of resonant 2-tori for the Baggot... resonance zones. These sequences provide insight into the nature of strongly mixed states ... |
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Source: Ezra, Gregory S.- Department of Chemistry and Chemical Biology, Cornell University |
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Collection: Chemistry |
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| 52 | Environmental Sciences Department Lucian Wielopolski, Ph.D. | ||
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Summary: Of The Transmissions At 5 MeV And 10 MeV In Uranium For: x=0.1 cm, R=1.012, CR=333c/s5mA, @ 3 IL= IL = 253 counts... Environmental Sciences Department Lucian Wielopolski, Ph.D.Lucian Wielopolski, Ph.D. GAMMA RESONANCE AND FISSION... TECHNOLOGY (GRFT) FOR DETECTION OF EXPLOSIVE AND NUCLEAR MATERIALS IN CARGO GAMMA ... |
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Source: Brookhaven National Laboratory, Environmental Chemistry Division, Department of Applied Science |
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Collection: Environmental Sciences and Ecology |
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| 53 | Electric-field-coupled resonators for negative permittivity metamaterials D. Schurig,a | ||
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Summary: mail: dschurig@duke.edu FIG. 1. Color online a The fabricated sample. b The geometric design: a=3... Electric-field-coupled resonators for negative permittivity metamaterials D. Schurig,a J. J. Mock... inductive-capacitive resonator is described that has a strong electric response. This ... |
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Source: Smith, David R. - Department of Electrical and Computer Engineering, Duke University |
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Collection: Materials Science |
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| 54 | Frequency-Selective MEMS for Miniaturized Communication Devices | ||
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Summary: -Transducers Folded-Beam µResonator Differential-to-Single Ended Amplifier, A2 A1 A3 Folding-Truss vi - vi ix32 ix31... by buffers A1 and A2, then directed to the differential- to-single-ended converter A3. Quarter... @eecs.umich.edu Abstract--With Q's in the tens to hundreds of ... |
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Source: Nguyen, Clark T.-C. - Department of Electrical Engineering and Computer Sciences, University of California at Berkeley |
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Collection: Engineering |
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| 55 | Microelectromechanical bandpass filters based on cyclic coupling architectures | ||
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Summary: : ARTICLE IN PRESS 350 n 300 c Q k |A2| |A1| |A3| |A4| |A5| |A6| 250 200200 150 :|plitude:|AnAm 100 50 0 0... .99 1 1.01 1.02 1.03 350 300 250 200 150 100 50 |A1| |A2 6| |A3 5| |A4| n kc Q Fig. 5. Amplitude... a c t Bandpass filters based on resonant microelectromechanical systems (MEMS) ... |
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Source: Rhoads, Jeffrey F. - School of Mechanical Engineering, Purdue University |
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Collection: Engineering |
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| 56 | Developments in Petroleum Science, 51 Editors: M. Nikravesh, F. Aminzadeh and L.A. Zadeh | ||
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Summary: . Alice 3 × × × × × × × × Chr. Alice 2 × × × × × × × × Beck Fred 4 × × × × × × Chr. Alice A3 × × × × × Chr... × × × × × × × Busby 2 × × × × × × × × Busby 3 × × × × × × × × × Busby A4 × × × × × × Busby A3... Elsevier Science B.V. All rights reserved 605 ... |
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Source: Mohaghegh, Shahab - Department of Petroleum and Natural Gas Engineering, West Virginia University |
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Collection: Fossil Fuels |
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| 57 | J. PHYS IV FRANCE 7 (1997) Colloque C1, Supplkmentau Journal de Physique I11de mars 1997 | ||
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Summary: domain walls in [loo]-oriented films (right). I .4 m 0 1 3 -a 3 . 2 - w $ 1 1 - hC 1.o 8m 0.9 2. Results... by mems of planar excitation-detection structllres at. lnicrowave frequencies. New rnultiple resonance... . The resonances are excited by rf magnetic fields which are parallel or perpendicular to the ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 58 | 870 PIERS Proceedings, Cambridge, USA, July 26, 2008 Dynamical Control of Terahertz Metamaterial Resonance Response | ||
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Summary: ) Cross-section view of one individual element. 3. FABRICATION Figure 3(a)3(h) detail the fabrication... Resonance Response Using Bimaterial Cantilevers H. Tao1 , A. Strikwerda2 , C. Bingham3 W. J. Padilla3 , X... for the dynamical control of the resonant electrical response of terahertz (THz) metamaterials. ... |
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Source: Boston University, Center for Nanoscience and Nanobiotechnology |
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Collection: Materials Science |
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| 59 | ICARUS 85, 394--443 (1990) Tidal Evolution of the Uranian Satellites | ||
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Summary: -89). The orbits of both satellites become chaotic during evolution through the eccentricity resonances associated... with a relatively large orbital eccentricity, which can damp to the current value in the time since resonance... approaching the resonance. Upon escaping from the resonance, the orbit of ... |
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Source: Wisdom, Jack - Computer Science and Artificial Intelligence Laboratory & Department of Earth, Atmospheric, and Planetary Sciences, Massachusetts Institute of Technology (MIT) |
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Collection: Physics |
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| 60 | Design and Evaluation of an Arbitration-Free Passive Optical Crossbar for On-chip Interconnection Networks | ||
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Summary: -shifted by 0.4 nm (~50 GHz). The resonance ER is maintained at 20 dB. Figures 3(a)-3(c) show the output port... -compatible microring resonators have emerged as viable on-chip optical interconnection networks to deliver high... and evaluation of an arbitration-free passive crossbar based on a microring ... |
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Source: Yoo, S. J. Ben - Department of Electrical and Computer Engineering, University of California, Davis |
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Collection: Engineering |
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| 61 | Nanomanipulation Using Silicon Photonic Crystal Resonators | ||
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Summary: resonator for enhanced optical trapping. (a) 3D schematic of the one-dimensional photonic crystal resonator... Nanomanipulation Using Silicon Photonic Crystal Resonators Sudeep Mandal, Xavier Serey, and David... optical trap exploiting optical resonance in ... |
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Source: Erickson, David - Sibley School of Mechanical and Aerospace Engineering, Cornell University |
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Collection: Chemistry ; Engineering |
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| 62 | PHYSICAL REVIEW A 81, 013833 (2010) Coherent-population-trapping resonances with linearly polarized light for | ||
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Summary: - e) + i/2] × i, m |, (A3) where d is the optical transition dipole moment operator, L is the laser... with minimal momentum Fe = I - Je = 1). In Eqs. (A2) and (A3) the Doppler shift kv [k = (k1 + k2)/2] and strong... PHYSICAL REVIEW A 81, 013833 (2010) Coherent-population-trapping ... |
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Source: Walsworth, Ronald L. - Department of Physics, Harvard University |
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Collection: Physics |
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| 63 | Icarus 188 (2007) 535539 www.elsevier.com/locate/icarus | ||
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Summary: in terms of the angular momentum and ec- centricity: E = ~E(L,e). Let n = GM/a3; we have (3) ~E L = n 1... in an equilibrium resonant configuration with other saturnian satellites can be estimated independently... that is observed to be coming from Enceladus. Equilibrium heating in possible past resonances ... |
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Source: Wisdom, Jack - Computer Science and Artificial Intelligence Laboratory & Department of Earth, Atmospheric, and Planetary Sciences, Massachusetts Institute of Technology (MIT) |
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Collection: Physics |
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| 64 | Vol. 5, No. 10/October 1988/J. Opt. Soc. Am. B 2015 Observation of resonances at subharmonics of the Rabi | ||
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Summary: the subharmonic behavior of the 100%AM interaction. In Figs. 3(a)-3(d), we show the phase plots formed by the in... Vol. 5, No. 10/October 1988/J. Opt. Soc. Am. B 2015 Observation of resonances at subharmonics... 14627 Received March 30,1988; accepted May 26, 1988 A series of resonances has been observed |
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Source: Stroud Jr., Carlos R. - Institute of Optics, University of Rochester; Stroud, Carlos R. - Institute of Optics & Department of Physics and Astronomy, University of Rochester |
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Collection: Engineering ; Physics |
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| 65 | CMOS-MEMS Resonator as a Signal Generator for Fully-Adiabatic Logic Circuits | ||
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Summary: Actuator comb Resonant beam (a) 3D model (b) Electrical isolation of silicon Figure 8: The 3D model... CMOS-MEMS Resonator as a Signal Generator for Fully-Adiabatic Logic Circuits Maojiao He (maojiaoh... -topped) voltage waveform. In this paper, we propose to use high-Q MEMS resonators to ... |
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Source: Frank, Michael P. - Department of Electrical and Computer Engineering, FAMU-FSU College of Engineering |
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Collection: Computer Technologies and Information Sciences |
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| 66 | Mon. Not. R. Astron. Soc. 322, 343355 (2001) Dynamical evolution of the PrometheusPandora system | ||
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Summary: of a resonance against tidal dissipation is obtained for eccentricities larger than epdstab 5 12jpj3 a3 pd Gmpro... apro apd 2 4 5 V bbbb` bbbbX W bbbba bbbbY 1a3 , 5 Â 1024 X 17 Pandora will encounter the resonance... if the eccentricity is lower than epdcrit , 4 ... |
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Source: Sicardy, Bruno - Observatoire de Paris |
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Collection: Physics |
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| 67 | Insights into Nuclear Clusters in 28 Si via Resonant Radiative | ||
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Summary: , Heslington, York YO10 5DD, UK 3 TRIUMF, 4004 Wesbrook Mall, Vancouver, B.C., V6T 2A3, Canada 4 Physics... Insights into Nuclear Clusters in 28 Si via Resonant Radiative Capture Measurements S. Courtin1... V) resonance at Triumf (Vancouver) using the stateoftheart Dragon 0° spectrometer and its very ... |
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|
Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 68 | Measures of Chaos in Hamiltonian Systems Ferdinand Verhulst | ||
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Summary: . In particular consider the Hamiltonian system H = H2 + (a1q2 1q2 + a2q2 1q3 + a3q1q2q3), (3) producing... the equations of motion ¨q1 + q1 = -(2a1q1q2 + 2a2q1q3 + a3q2q3), ¨q2 + 4q2 = -(a1q2 1 + a3q1q3), ¨q3 + 4q3... = -(a2q2 1 + ... |
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Source: Verhulst, Ferdinand - Department of Mathematics, Universiteit Utrecht |
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Collection: Mathematics |
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| 69 | Defect-mediated resonance shift of silicon-on-insulator racetrack resonators | ||
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Summary: temperatures is plotted. Fig. 2. Resonance shifting for device A/3E14-Boron. The trend of this result... . 2 where the transmitted power of device A/3E14-Boron after various post-implantation annealing... Defect-mediated resonance shift of silicon-on- insulator ... |
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Source: Bowers, John - Department of Electrical and Computer Engineering, University of California at Santa Barbara |
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Collection: Engineering |
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| 70 | Compact acoustic bandgap material based on a subwavelength collection of detuned Helmholtz resonators | ||
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Summary: to loading by a single Helmholtz resonator with dimensions of a2 ¼ 3.1 cm2 , d2 ¼ 4.5 cm, a3 ¼ 20.4 cm2 , FIG... area, a2, and the cavity area, a3. The neck and cavity lengths are given by d2 and d3, respectively... the length of the cavity. If the area of the cavity, ... |
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Source: Robertson, William - Department of Physics and Astronomy, Middle Tennessee State University |
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Collection: Physics |
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| 71 | The Magnetic-Resonance Force Microscope: A New Tool for High-Resolution, 3-D, Subsurface | ||
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Summary: . (a) 3-D rendering of the MRFM sensitive slice. (b) Synthetic truth image. (c) Slices through... The Magnetic-Resonance Force Microscope: A New Tool for High-Resolution, 3-D, Subsurface Scanned... , MELISSA M. MIDZOR, AND MICHAEL L. ROUKES Invited Paper The magnetic-resonance force microscope (MRFM |
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|
Source: Hammel, P. Chris - Department of Physics, Ohio State University; Roukes, Michael L. - Division of Engineering and Applied Science, California Institute of Technology |
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Collection: Materials Science ; Physics |
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| 72 | 1961 IRE TRANSACTIONS ON COMPONENT PARTS Realization of a Filter with Helical Components* | ||
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Summary: that this value is very close: to that value calculated in part "a." 3) Design of Resonator Dimensions. a... and Guillemins give a curve that shows the minimuni insertion loss at midband of Butterworth filters plott,ed a3... consequence of coaxial-resonator filters. ... |
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Source: Monroe, Christopher - Department of Physics, University of Maryland at College Park |
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Collection: Physics |
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| 73 | Proceedings of Asia-Pacific Microwave Conference 2006 Copyright 2006 IEICE | ||
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Summary: of 4.2 - 9.5GHz (a), 3.2 - 7.3GHz (b). Direct source-load coupling can be applied to the ultra... -wideband filters with source- load cross coupling and impedance stubs are presented. Stepped impedance resonators... connect individual resonators. Effective techniques such as open-stub lines and source-load ... |
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Source: Bornemann, Jens - Department of Electrical and Computer Engineering. University of Victoria |
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Collection: Engineering |
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| 74 | hal-00144114,version1-3May2007 Influence of the extent of the eigenstates of a system on the resonances | ||
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Summary: (, ), where Rl,p(r) = N-1 l,p 3/2 l,p a-3/2 jl(l,pr/a); if r > a, l,m,p(r) = 0. The energies of states (l, m... ,1 = 1 4 N-1 0 3/2 0,1 a-3/2 sin(0,1r/a) 0,1r/a , with 0,1 = and N0 = /2 1.25, 1,1 = 3 4 N-1 1 3/2 1... ,1 a-3/2 sin(1,1r/a) 1,1r/a - cos(1,1r/a) 1 ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 75 | Fig. 1 Circuit diagram of high-voltage generator with LCC resonant converter [3] Frequency / Duty Cycle Current-Mode Fuzzy Control | ||
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Summary: , the triangle centre value of e(t) is specified as -4A, -3A, -2A, -1A, 0A, +1A, +2A, +3A, +4A, respectively... 1 Fig. 1 Circuit diagram of high-voltage generator with LCC resonant converter [3] Frequency / Duty... Cycle Current-Mode Fuzzy Control for LCC Resonant ... |
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|
Source: Paderborn, Universität - Fakultät für Elektrotechnik, Informatik und Mathematik, Fachgebiet Leistungselektronik und Elektrische Antriebstechnik |
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Collection: Engineering |
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| 76 | Effect of thin silicon dioxide layers on resonant frequency in infrared metamaterials | ||
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Summary: 32816-2700, U.S.A. 2 Sandia National Laboratories, P.O. 5800, Albuquerque NM 87185-1082, U.S.A. 3 AMPAC... Effect of thin silicon dioxide layers on resonant frequency in infrared metamaterials D. J. Shelton... and the underlying substrate. We have measured the resonant frequencies of split ring ... |
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|
Source: Boreman, Glenn D. - School of Optics (CREOLE), University of Central Florida |
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Collection: Physics |
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| 77 | Mon. Not. R. Astron. Soc. 000, 000000 (0000) Printed 14 January 2009 (MN LATEX style file v2.2) On the 2/1 resonant planetary dynamics -Periodic orbits | ||
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Summary: as a critical point in the general problem and the asym- metric family A3 bifurcates from it (Fig. 5b). Actually... , A3 can be considered as the continuation of the family EA 1p. No singularities are obtained... and A3 at = ¯2 and the formation of the new families ... |
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Source: Hadjidemetriou, John D. - Department of Physics, Aristotle University of Thessaloniki |
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Collection: Physics |
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| 78 | T h e o p e n a c c e s s j o u r n a l f o r p h y s i c s New Journal of Physics | ||
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Summary: ) = a(t)ei0t + a (t)e-i0t + 0 48 a3 ei30t + a3 e-i30t + · · · , (13) where = - 0 4 , = a00 4 1 + 0 2... frequency = 1/ LC + ( 1). Then we can introduce the ansatz I = aeit/ LC + a eit/ LC - i LC 8 a3 ei3t... / LC + i LC 8 ... |
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Source: Gavilan, Marcel G. Clerc - Departamento de Física, Universidad de Chile |
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Collection: Physics |
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| 79 | All-optical diode in an asymmetrically apodized Kerr nonlinear microresonator system | ||
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Summary: -photon absorption and three-photon absorption, are charac- terized by the coefficients a1, a2 and a3, respectively... ; tÞ À 1 2 ða1 þ a2I þ a3I2 ÞAðz À dz; tÞ; (1) where dz and dt ¼ dz=ðc=neffÞ are the discretization... rm cm2 /GW, and nonlinear loss parameters a2 ¼ 0:05 cm/GW and ... |
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Source: Busch, Kurt - Department of Physics, Univ. Karlsruhe |
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Collection: Physics ; Materials Science |
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| 80 | Icarus 155, 454474 (2002) doi:10.1006/icar.2001.6737, available online at http://www.idealibrary.com on | ||
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Summary: ://www.idealibrary.com on Stable Chaos in High-Order Jovian Resonances Kleomenis Tsiganis, Harry Varvoglis, and John D... that the occurrence of stable chaos in the 12/7 mean motion resonance with Jupiter is related to the fact... of resonant periodic orbits, both for the planar and for the 3-D problem, also oc- curs in other ... |
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|
Source: Hadjidemetriou, John D. - Department of Physics, Aristotle University of Thessaloniki; Varvoglis, Harry - Department of Physics, Aristotle University of Thessaloniki |
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Collection: Physics |
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| 81 | Appl Phys A (2009) 95: 11111118 DOI 10.1007/s00339-009-5121-6 | ||
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Summary: is related as c2 d2 = A1/4e-iL/4 0 0 A-3/4ei3L/4 b2 a2 , (2) where A is the fraction of the electric... nanophotonics, optical crossbars based on CMOS-compatible microring resonators have emerged as viable on... a microring resonator matrix-based optical crossbar that can be used in an on- chip optical ... |
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Source: Yoo, S. J. Ben - Department of Electrical and Computer Engineering, University of California, Davis |
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Collection: Engineering |
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| 82 | 534 JOURNAL OF MICROELECTROMECHANICAL SYSTEMS, VOL. 8, NO. 4, DECEMBER 1999 High-Order Medium Frequency | ||
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Summary: folded-beam resonators cou- pled by flexural mode springs are demonstrated using an inte- grated circuit... -wavelength coupling beams attached to resonators at velocity-controllable locations is shown to suppress passband... resolution required to achieve a given percent bandwidth. Ratioed folded- beam micromechanical resonators |
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|
Source: Nguyen, Clark T.-C. - Department of Electrical Engineering and Computer Sciences, University of California at Berkeley |
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Collection: Engineering |
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| 83 | THERMOELASTIC DAMPING IN TRENCH-REFILLED POLYSILICON Reza Abdolvand 1 | ||
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Summary: the existence of such a void in the width sense drive polysilicon SCS 2A3.1 TRANSDUCERS `03 The 12th... ) Void Thickness SCS 2A3.1 TRANSDUCERS `03 The 12th International Conference on Solid State Sensors... polysilicon beams. 2 1 h 2 2 2 w 2A3.1 TRANSDUCERS `03 The ... |
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Source: Ayazi, Farrokh - School of Electrical and Computer Engineering, Georgia Institute of Technology |
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Collection: Engineering |
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| 84 | Dynamical instability in kicked Bose-Einstein condensates J. Reslen,1 | ||
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Summary: in the weakly interacting limit #12;1 a3 s where is the density. A limit is identified where this condition... we conclude instead that instability is due to resonant driving of Bogoliubov modes. We investigate... properties of the resonances and yields good agreement with mean-field numerics. PACS numbers: ... |
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Source: Monteiro, Tania - Department of Physics and Astronomy, University College London |
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Collection: Physics |
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| 85 | PURDUE UNIVERSITY GRADUATE SCHOOL | ||
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Summary: . . . . . . . . . . . . . . . . . . . . . . . . . . . 126 A.2 Fabrication Steps on SOI Chip . . . . . . . . . . . . . . . . . 126 A.3 Fabrication Steps... . . . . . . . . . . . . . . . . . . . . . . . . . 20 3.1.1 n Coupled Resonators in an Open-Chain . . . . . . . . . . . 21 3.2 n Coupled Resonators... . . ... |
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Source: Rhoads, Jeffrey F. - School of Mechanical Engineering, Purdue University |
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Collection: Engineering |
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| 86 | SPECTRUM OF A FLUID-LOADED VIBRATING PLATE: THE MULTIPLE RESONANCE PHENOMENON | ||
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Summary: for k ± by the stationary phase method [1]: I1(k) k± h1 3mn(0) 2ka eika+i 4 = (-1)m m2 2 2a3 2ka eika... equation has the following approximation for k ± mn (k) 1 (ik)4 (-1)m m2 2 2a3 2ka eika+i 4 + (-1)n n2 2... of mn (k). For given m and n and for |k| , one has lim |k| j1m(k) = -(-1)m m2 2 eiak ... |
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|
Source: Ecole Polytechnique, Centre de mathématiques |
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|
Collection: Mathematics |
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| 87 | Nature Macmillan Publishers Ltd 1998 NATURE |VOL 392 |12 MARCH 1998 151 | ||
|
Summary: , the density scales instead like N(Na)-2/3 resulting in at most a 50% change for a/a~. (3) We assumed... of Feshbach resonances in a BoseEinstein condensate S. Inouye*, M. R. Andrews*, J. Stenger*, H.-J. Miesner... a so-called `Feshbach resonance'. Two such resonances have now been ... |
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Source: Harvard University, Center for Ultracold Atoms, Alkali Quantum Gases Group |
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Collection: Physics |
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| 88 | Two-photon selective reflection M. Gorris-Neveux, P. Monnot, S. Saltiel,* R. Barbe, J.-C. Keller, | ||
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Summary: of the denominator of A1 : b 1 2 ~ s i 2 ~ ia2 s 1 2 ~ s i 2 ~ ia2 s 2 ~ p 2 s A3 and c 1 2 ~ s i 2 ~ ia2 s 1 2 ~ s i... 2 ~ ia2 s 2 ~ p 2 s . A4 The expressions A3 and A4 include the square root of complex quantity... associated with atoms moving quasiparallel to the dielectric interface, and therefore ... |
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|
Source: Saltiel, Solomon - Faculty of Physics, University of Sofia |
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|
Collection: Physics |
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| 89 | Vol. 42 (2011) ACTA PHYSICA POLONICA B No 34 RADIATIVE CAPTURE IN THE 12 | ||
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Summary: Colombia, V6T 2A3, Canada (Received February 7, 2011) This paper discusses how the radiative capture... process can shed light on the origin of the resonances observed in light heavy-ion collisions. The impact... of resonant features on the fusion cross-sections is described from energies around the Coulomb ... |
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|
Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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|
Collection: Physics |
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| 90 | Chemical Physics 57 (1981) 2.53-259 North-Holland Publishing Company | ||
|
Summary: Antiresonance energy Excitation energy srructure (I&!) (`A3 k3 (En) 33, cZAs chartree) (hartreef (kczl) @sat) (k... RESONANCE BETWXEN GENERALIZED VALENCE BOND WAVEFUNCX'IONS Arthur F. VOTER and Wiiliam A. GODDARD III Arthur... only describe one of the bonding structures, dlotiiing no explicit mixing or ... |
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|
Source: Goddard III, William A. - Materials and Process Simulation Center & Department of Chemistry, California Institute of Technology |
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|
Collection: Materials Science |
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| 91 | May 15, 1993 / Vol. 18, No. 10 / OPTICS LETTERS 781 Extra resonances in time-domain four-wave mixing | ||
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Summary: /Fv)kl + (k2/k3)[exp(- r d) - cos(Ad)exp(-Fed)] - (k4 /k3)sin(Ad)exp(-Fed), (3a) (3b) C = - (A/rF,)kl+ (k2/k3... May 15, 1993 / Vol. 18, No. 10 / OPTICS LETTERS 781 Extra resonances in time-domain four... Received December 9, 1992 We show that extra resonances, such as those caused in frequency-domain ... |
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Source: Fayer, Michael D. - Department of Chemistry, Stanford University |
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Collection: Chemistry |
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| 92 | Nonlinear Resonant Oscillations in Closed Tubes of Variable Cross Section | ||
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Summary: , ) is of the form x ( 1 s f3 x ) 1 2 s 2 f3 2 = C1(x) sin + A3 C3(x) sin 3 , (25) with f3(0, ) = 0, f3(1, ) = 0, (26... ) and where C1(x) = [A3 E1(x) + A 0 1s ]0 + 1[A3 C4(x) 1 A s ]. (27) In (27) C4(x) = 1 2s [ ( B s )0 + B( s )0... and forcing terms, all terms on ... |
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Source: Cork, University College - Department of Applied Mathematics |
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Collection: Mathematics |
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| 93 | Giant enhancement of electric field between two close metallic grains due to plasmonic resonance | ||
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Summary: ). Therefore the resonance condi- tion survives if / a , which leads to the condi- tion 2 a3/2 1/2 , justifying... of the grains is determined by the dis- tances a and can be estimated as d E a a3 Ec a2 . The geometrical factor... the ex- pressions one finds G a/ ... |
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Source: Lebedev, Vladimir - Landau Institute for Theoretical Physics |
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Collection: Physics |
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| 94 | All-optical switching, bistability, and slow-light transmission in photonic crystal waveguide-resonator structures | ||
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Summary: All-optical switching, bistability, and slow-light transmission in photonic crystal waveguide-resonator... Received 17 May 2006; published 5 October 2006 We analyze the resonant linear and nonlinear transmission... through a photonic crystal waveguide side- coupled to a Kerr-nonlinear photonic crystal resonator. First |
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Source: Australian National University, Research School of Physical Sciences and Engineering, Nonlinear Physics Centre; Busch, Kurt - Department of Physics, Univ. Karlsruhe |
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Collection: Materials Science ; Physics |
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| 95 | Copyright 2002 IEEE. Reprinted from IEEE Photonics Technology Letters, vol. 14, pp. | ||
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Summary: of equations (3a) (3b) where is the coupling coefficient and . A similar relationship exists for the probe... , VOL. 14, NO. 1, JANUARY 2002 All-Optical Nonlinear Switching in GaAsAlGaAs Microring Resonators V... in compact GaAsAlGaAs microring resonators at the 1.55- m wavelength. Switching is ... |
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Source: Ho, Ping-Tong - Department of Electrical and Computer Engineering, University of Maryland at College Park |
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Collection: Engineering |
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| 96 | Nonlinear Dynamics (2006) 45: 237247 DOI: 10.1007/s11071-006-2424-4 c Springer 2006 | ||
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Summary: 2 0 4 - 3A3 0 4 + B0 sin ( ) 2 - A0 cos ( ) 2 - B0c 2 (16) A0 and B0 in Equations (13) and (14... Nonlinear Quasiperiodic Mathieu Equation Near 2:2:1 Resonance NAZHA ABOUHAZIM1 , RICHARD H. RAND2... :2:1 resonance. By using a double perturbation method which assumes that both and are small, we approximate |
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Source: Rand, Richard H. - Department of Theoretical and Applied Mechanics, Cornell University |
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Collection: Engineering |
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| 97 | DESIGN NOTE TRIUMF 4004 WESBROOK MALL, VANCOUVER, B.C. CANADA V6T 2A3 | ||
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Summary: TRIUMF DESIGN NOTE TRIUMF 4004 WESBROOK MALL, VANCOUVER, B.C. CANADA V6T 2A3 TRI-DN-02-14 July 2002... Response of cavity voltage amplitude and phase to sinusoidal modulations of the resonance frequency based... on the LCR equivalent circuit Shane Koscielniak Abstract Based on the LCR parallel resonator, ... |
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Source: Koscielniak, Shane - TRIUMF Canada's National Laboratory for Particle and Nuclear Physics |
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Collection: Plasma Physics and Fusion |
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| 98 | N AND RESONANCES I. Introduction | ||
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Summary: /2 and A3/2, have been obtained in partial-wave analyses of single-pion photo- production, photoproduction... of the helicity amplitudes A1/2 and A3/2 by = k2 2MN (2J + 1)MR |A1/2|2 + |A3/2|2 . Here MN and MR... 1 N AND RESONANCES I. ... |
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Source: Lawrence Berkeley National Laboratory, Computational Research Division, Distributed Systems Department, Data Intensive Distributed Computing Group |
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Collection: Computer Technologies and Information Sciences |
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| 99 | LPC Report PCCF RI 0003 4 February, 2000 | ||
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Summary: 11 1 1/2 A1- P31 1 1/2 A1- P33 1 3/2 A1+ B1+ D13 2 3/2 A2- B2- D15 2 5/2 A2+ B2+ F15 3 5/2 A3- B3- F... 35 3 5/2 A3- B3- F37 3 7/2 A3+ B3+ 3.1 Isospin structure of matrix elements The matrix element... state defined by the isospin I of the N system A(I) , ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 100 | ccsd-00003019,version1-7Oct2004 Expansion of a lithium gas in the BEC-BCS | ||
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Summary: atom density n. When n|a|3 1 the system enters a strongly interacting regime that represents... . The solid curve corresponds to a finite temperature mean field model with T = 0.5 T0 C. Arrow: kF|a| = 3... Li Fermi gases near Feshbach reso- nances. A broad s-wave resonance is used to form ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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