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tuần 4 từ ngữ về ngày tháng năm ngày dạy  25 9 2014

PERFECTIONNEMENT DE COMMUNICATIONS SECURISEES AGT EN UTILISANT LA CRYPTOGRAPHIE QUANTIQUE

PERFECTIONNEMENT DE COMMUNICATIONS SECURISEES AGT EN UTILISANT LA CRYPTOGRAPHIE QUANTIQUE

Luận văn báo cáo - ngoại ngữ

... Physics, volume 74, pages 145 195 , Janvier 2002 [9] P M Gorman, P R Tapster, and J G Rarity "Secure FreeSpace Key Exchange To 1 .9 km In J Mod Opt of Physics, volume 48 , pages 1887 190 1, 2001 [10] ... 20 04 [ 19] C Kurtsiefer, P Zarda, M Halder, P Gorman, P Tapster, J Rarity, and H Weinfurter "Long Distance Free-Space Quantum Cryptography" Dans New Journal of Physics, volume 4, pages 43 . 143 . 14, ... 32833286, 199 8 [3] W T Buttler, R J Hughes, S K Lamoreaux, G L Morgan, J E Nordholt, and C G Peterson "Daylight Quantum Key Distribution Over 1.6 km" Dans Phys Rev Lett., volume 84, pages 56 5256 55,...
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Bài giảng Chapter 7 The Quantum-Mechanical Model of the Atom

Bài giảng Chapter 7 The Quantum-Mechanical Model of the Atom

Hóa học

... of 4. 62 x 10 14 s-1 Given: ν = 4. 62 x 10 14 s-1 Find: λ, (nm) Concept Plan: ν (s-1) λ (m) c λ= ν nm λ (nm) 10 9 m Relationships: λ∙ν = c, nm = 10 -9 m Solve: c 3.00 ×108 m • s -1 λ= = = 6 . 49 ×10 ... Relationships: λ∙ν = c, nm = 10 -9 m Solve: c 3.00 ×108 m • s -1 λ= = = 6 . 49 ×10 −7 m ν 4. 62 ×10 14 s -1 nm −7 6 . 49 ×10 m × 9 = 6 . 49 ×10 nm 10 m Check: the unit is correct, the wavelength is appropriate for ... 6.626 × 10 − 34  kg s h   1.675 × 10 − 24 g × λ= = 10 g mv  -27 1.675 ×10 kg 1.00 ×10  = 1.675 ×10 −27 kg ( ) m s   = 3 .96 × 10 9 m Tro, Chemistry: A Molecular Approach 49 Complimentary...
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Tài liệu THE QUANTUM IN CHEMISTRY: An Experimentalist’s View pptx

Tài liệu THE QUANTUM IN CHEMISTRY: An Experimentalist’s View pptx

Hóa học - Dầu khí

... 36(11), 17 69( 198 1); Env Sci Technol., 20 (4) , 3 19 ( 198 6); Chemtech., 21 (4) , 250 ( 199 1), Anal Chem., 66(12), 106R ( 19 94 ) 4A.M Thayer, Chem Eng News, 83, 49 (September 5, 2005) 29 1 .4 The Coexistence ... of Molecular Speeds 40 5 9. 5 The Pressure of a Dilute Gas 41 1 9. 6 Effusion and Wall Collisions 41 6 9. 7 The Model System with Potential Energy 41 8 9. 8 The Hard-Sphere Gas 42 2 9. 9 The Molecular Structure ... n (20.00 g) mol 20.1 79 g 0 .99 11 mol V (22 .40 0 L) m3 1000 L 0.02 240 0 m3 We now carry out the numerical calculation: P nRT V (0 .99 11 mol) 8.3 14 J K −1 mol−1 (273.15 K) 0.02 240 0 m3 1.005 × 105 J...
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Tài liệu Đề tài

Tài liệu Đề tài " Asymptotic faithfulness of the quantum SU(n) representations of the mapping class groups " pdf

Thạc sĩ - Cao học

... Phys 165 ( 19 94 ) , 281– a 296 [DN] J.-M Drezet and M S Narasimhan, Groupe de Picard des vari´t´s de modules ee de fibres semi-stables sur les courbes alg´briques, Invent Math 97 ( 198 9), 53– 94 e [Fal] ... on Mg , Comm Math Phys 128 ( 199 0), 42 1 42 6 [RSW] T R Ramadas, I M Singer, and J Weitsman, Some comments on Chern-Simons gauge theory, Comm Math Phys 126 ( 198 9), 40 9 42 0 [RT1] N Reshetikhin and ... the Kauffman bracket, Topology 31 ( 199 2), 685– 699 [BHMV2] ——— , Topological quantum field theories derived from the Kauffman bracket, Topology 34 ( 199 5), 883 92 7 [BMS] M Bordeman, E Meinrenken,...
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The Quantum-Mechanical Model of the Atom pdf

The Quantum-Mechanical Model of the Atom pdf

Kĩ thuật Viễn thông

... model (253 ) Section 7.2 electromagnetic radiation (2 54) amplitude (2 54) wavelength (l) (2 54) frequency (n) (255 ) electromagnetic spectrum (256 ) 5 090 X_07_ch7_p252-285.indd 280 gamma rays (256 ) X-rays ... barcode scanner that has a frequency of 4. 62 * 10 14 s-1 SOLUTION c l c 3.00 * 108 m> s l= = n 4. 62 * 10 14 1> s = 6 . 49 * 10-7 m nm = 6 . 49 * 10-7 m * = 6 49 nm 10 -9 m You are given the frequency of the ... electrons depends on the composition of the surface The presence of oxygen 5 090 X_07_ch7_p252-285.indd 283 44 45 46 47 48 49 atoms on the surface results in auger electrons with a kinetic energy of...
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Báo cáo

Báo cáo "Quantum kinetic equation in the quantum hadrondynamics (QHD-I) model " pptx

Báo cáo khoa học

... Scientific Singapore ( 19 94 ) [9] M.Le Bellac, Thermal Field Theory, Cambridge University Press ( 199 6) [10] S.Y Wang, Preprint hep-ph/0007 340 [11] H.A Weldon, Phys Rev D28 (2007) 198 3 ... relativistic nuclear many body problem, Adv Nucl Phys (Plenum Press), ( 19 74) 190 [2] J.P Blaizot, E Iancu, Parwani, Phys Rev D 52 ( 199 5) 2 543 [3] T Kunihiro, T Muto, T Takasuka, R Tamagaki, T Tatsumi, ... m2 ± (k2 + M ) − 4M m2 , ( 79) ± qW = 2M m2 W k 1− 2 2M mW ± (k2 + M ) − 4M m2 W , (80) 1 54 P.H Lien / VNU Journal of Science, Mathematics - Physics 24 (2008) 145 -1 54 + − with q ∈ (q − , q +),...
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Đề tài

Đề tài " On the distribution of matrix elements for the quantum cat map " pptx

Thạc sĩ - Cao học

... minimal periods, Comm Math Phys 29 (2003), 44 9 49 2 [7] M Feingold and A Peres, Distribution of matrix elements of chaotic systems, Phys Rev A 34 ( 198 6), 591 – 595 [8] J H Hannay and M V Berry, ... Sup (4) 37 (20 04) , 7 69 799 [13] F Mezzadri, On the multiplicativity of quantum cat maps, Nonlinearity 15 (2002), 90 5 92 2 [ 14] P Sarnak, Spectra of hyperbolic surfaces, Bull Amer Math Soc 40 (2003) ... Math Phys e 102 ( 198 5), 49 7–502 [3] M Degli Esposti, Quantization of the orientation preserving automorphisms of the torus, Ann Inst H Poincar´ Phys Th´or 58 ( 199 3), 323– 341 e e [4] M Degli Esposti,...
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the quantum physics of black holes and string theory

the quantum physics of black holes and string theory

Vật lý

... Nucl Phys B486:77 ( 199 7) 41 Dijkgraaf R Nucl Phys B 543 : 545 ( 199 9) 42 Seiberg N, Witten E J High Energy Phys 99 04: 017 ( 199 9) 43 Larsen F, Martinec E J High Energy Phys 99 06:0 19 ( 199 9); Larsen ... J Phys Rev Lett 75 :47 24 ( 199 5) 19 Polchinski J hep-th /96 11050 ( 199 6) 20 Sen A hep-th /99 040 27 ( 199 9) 21 Witten E Nucl Phys B460:335 ( 199 6) 22 Tseytlin A hep-th /99 08105 ( 199 9) 23 Montonen C, Olive ... J High Energy Phys 99 11:002 ( 199 9); Dhar A, Mandal G, Wadia SR, Yogendran K hep-th /99 101 94 ( 199 9) 44 Cvetic M Nucl Phys Proc Suppl 56B:1 ( 199 7); Youm D Phys Rep 316:1 ( 199 9) 45 Maldacena J, Strominger...
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scientific american   -  1993 04  -  controlling the quantum jitters of atoms

scientific american - 1993 04 - controlling the quantum jitters of atoms

Toán học

... April 199 3 49 190 0 199 0 2050 AGE 85+ 80– 84 75– 79 70– 74 65– 69 60– 64 55– 59 50– 54 45 49 40 44 35– 39 30– 34 25 29 20– 24 15– 19 10– 14 5 9 0 4 400 300 200 100 MALE POPULATION (MILLIONS) 0 100 200 300 40 0 ... vanish 60 CURRENT PREDICTION 50 40 30 OBSERVED 20 PREDICTION AS OF 193 5 10 193 5 1 94 5 195 5 196 5 197 5 SOURCE: Social Security Administration 198 5 YEAR 199 5 2005 2015 2 025 STRAINS ON SOCIAL PROGRAMS, ... LOCALIZATION IN THE OWL M Konishi in The Harvey Lectures, Series 86, pages 47 Ð 64; 199 2 SCIENTIFIC AMERICAN April 199 3 Copyright 199 3 Scientific American, Inc 73 Catalysis on Surfaces Scientists can...
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squires, the mystery of the quantum world (second edition)

squires, the mystery of the quantum world (second edition)

Vật lý

... cast doubt on its validity In 191 2, Einstein wrote to a friend, ‘The more success the quantum theory has, the sillier it looks.’ [Letter to H Zangger, quoted on p 399 of the book Subtle i the Lord ... tests for reality given in 41 .2 In the next section we shall describe this other method of observation and see why it is so devastating to the idea of external reality 1 .4 The experimental challenge ... quantum theory 33 This is in accordance with the observations which we found so surprising in 41 .4 Detailed calculations yielding precise results are, of course, possible Similar calculations...
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Báo cáo hóa học:

Báo cáo hóa học: " Effects of Shape and Strain Distribution of Quantum Dots on Optical Transition in the Quantum Dot Infrared " doc

Hóa học - Dầu khí

... of C’s [ 19] and K’s (at 100 K) of zincblende InAs and GaAs bulk materials InAs GaAs C11(GPa) C12 (GPa) 83. 29 45 .26 C 44 (GPa) ˚ Kr (GPaA) 39. 59 60.0 170.13 215. 09 9. 59 15 .41 59. 315 74. 85 ˚ KX ... 1. 290 3 eV 1.2 1.0 0.8 0.8 0.6 CB HH LH 1.2 1.0 1.08 84 eV 0.6 0 .4 0. 097 8 eV 0.2 0.0 -0.2 -30 -20 -10 10 20 1.13 39 eV 0 .4 0.08 09 eV 0. 09 247 eV 0.2 0.0 lens QD 1 .4 1.3083 eV 0 .4 0.2 1.8 1.6 1 .4 1.2 ... -0.07500 (a) 12 8 4 0 εH -4 -8 -12 -12 -12 12 εB -4 -8 Z Axis (nm) -0.1300 (b) -8 -4 12 -12 12 (c) 8 12 12 (d) -4 -8 εH -4 εB -4 -8 -8 0.07000 -12 -12 -8 -4 12 0.1200 -12 -12 -8 -4 X Axis (nm) 123...
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The Quantum Mechanics Solver 28 docx

The Quantum Mechanics Solver 28 docx

Khoa học xã hội

... oscillator, 7, 1 09, 197 harmonic potential, 193 He+ , 69 heavy ion therapy, 94 Heisenberg inequalities, 60 hidden variables, 99 , 101 Hilbert space, holes, 211 hydrocarbon ions, 231 hydrogen, 2 49 , 255 magnetic ... entangled states, 3, 99 entanglement, eraser, 155 excitons, 206 identical particles, 10 interaction time, 88, 91 interference, 155, 1 59 ion beams, 94 ion therapy, 94 ionization energy, 69 ions in matter, ... J.-M., 1 19, 145 Raizen, M., 285 Ramsey, N.F., 47 , 53, 156 Reichel, J., 285 Rich, J., VII Richard, J.-M., 192 Roger, G., 108 Rosen, N., 99 , 108 Roug´, A., VII e Maali, A., 1 19, 145 Maitre, X., 1 19 Maleki,...
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The Quantum Mechanics Solver 1 ppsx

The Quantum Mechanics Solver 1 ppsx

Khoa học xã hội

... Particles 1 94 19. 3 Energy of a Bose–Einstein Condensate 195 19 .4 Condensates with Repulsive Interactions 195 19. 5 Condensates with Attractive ... and Liquid He 258 25 .4 The Sticking Probability 258 25. 5 Solutions 2 59 25. 6 Comments ... 246 24. 2 Muonium in Silicon 247 24. 3 Solutions 2 49 25 Quantum Reflection of Atoms...
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The Quantum Mechanics Solver 2 docx

The Quantum Mechanics Solver 2 docx

Khoa học xã hội

... functions on the sphere of radius one The first are: , Y0,0 (θ, ϕ) = √ 4 Y1,1 (θ, ϕ) = − sin θ eiϕ , 8π Y1,0 (θ, ϕ) = cos θ , 4 Y1,−1 (θ, ϕ) = sin θ e−iϕ 8π Exactly Soluble Problems Spin In addition ... functions are the Hermite functions The ground state |n = is given by: ψ0 (x) = √ exp(−x2 / 2x2 ) π 1 /4 x0 Higher dimension harmonic oscillator problems are deduced directly from these results The Coulomb ... electrostatic field of the proton me ) and we set We note µ the reduced mass (µ = me mp /(me + mp ) e2 = q / (4 ) Since the Coulomb potential is rotation invariant, we can find ˆ ˆ ˆ a basis of states common...
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The Quantum Mechanics Solver 3 docx

The Quantum Mechanics Solver 3 docx

Vật lý

... reaction (1.1) We recall that mp c2 = 93 8.27 MeV and mn c2 = 93 9.57 MeV 1.1.6 The detectors measure neutrino fluxes with an accuracy of ∼ 10% (a) Assuming ∆m2 c4 = 10 4 eV2 , determine the minimal distance ... oscillation length L 4 ¯ p h , |∆m2 | c2 ∆m2 = m2 − m2 (1.6) 1.1.3 Calculate the oscillation length L for an energy E a mass difference ∆m2 c4 = 10 4 eV2 pc = MeV and L= 1.1 .4 One measures the ... hk: ¯ dσ = dΩ 2mgca2 h ¯ 1+ 4a2 k sin2 (θ/2) (Born) , where θ is the scattering angle between p and p The total cross-section is then: 4 a2 mgca (Born) σ(k) = h ¯ + 4k a2 Collision Processes...
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