MIMO Systems Theory and Applications Part 1 ppt

... = 13 K. Superconductor Year T C Reference NbO 19 33 1. 5 Sleight, 19 95 K x WO 3 19 67 6.0 Remeika et al., 19 67 LiTi 2 + x O 4 19 73 1. 2 Johnston et al., 19 73 BaPb 1 - x Bi x O 3 19 75 ... BiSrCaCu 2 O 6 + x 19 88 10 5 Maeda et al., 19 88 Tl 2 Ba 2 Ca 2 Cu 3 O 9 + x 19 88 11 0 Shimakawa et al., 19 88 HgBa 2 Ca 2 Cu 3 O 8 + x 19 93 13 0 Schilling &am...

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... correlations. 1 10 10 0 0 10 20 T c Bilayer hydrate Monolayer hydrate unhydrous Na 0.35 CoO 2 1 / T 1 T ( s -1 K -1 ) T ( K ) (b) 0 .1 1 10 10 0 0 .1 1 10 10 0 10 00 ~ T ~ T 3 1/ T 1 ( s -1 ) T ... Na x (H 3 O) z CoO 2 ·yH 2 O13 1 10 10 0 0 20 40 60 MLH M1 sample M2 sample IM sample SC sample 1 / T 1 T ( s -1 K -1 ) T ( K ) (b) Na x (H 3 O) z Co...

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... 640-643 , ISSN: 10 51- 8223. Narayana S. (2 011 ). Large scale integration issues in superconducting circuits, Proquest dissertations and theses, ISBN 97 811 2404 211 4. Nielsen M.A. and Chuang I.L. ... Theory and Applications Superconductivity – Theory and Applications 94 connecting J1 and J2. With proper circuit parameters, this induced current causes a voltage p...

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... 0 , , sin III III      , and  1 2 2 2 ,0 sin III n imp i           (28) From Eqs. (26) and (27) one obtains then the following expression for the critical temperature  0 11 1 111 1 1 ln 1 24 ... Rev. B, Vol. 22, No. 11 , (19 80) 514 2- 515 3. Andreev, A. F. (19 64). Thermal conductivity of the intermediate state of superconductors. Sov. Phys...

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... superconductor and permanent magnet. Journal Of Applied Physics 10 1, 11 3922 (2007). Superconductivity – Theory and Applications 16 4 Fig. 11 . X dependence of vertical force for Z =12 mm. 4.2 ... (19 91) 13 042 -13 048 Wacenovsky, M.; Weber, H.; Hyun, O.B. (19 89). Magnetization of grain-aligned hoba2cu3o7- delta. Physica C, 16 2 (19 89) 16 29 -16 30 Weber, H.W...

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... 0.4 H 1 10 -12 1 10 -11 1 10 -10 |F| 2 2.6 1. 7 0.86 0.02 µ= (b) 0 0 .1 H 0 1 10 -5 F 10 F 10 M 10 Fig. 8. Field dependence of FLL form factor F 1, 0 for µ = 0.02, 0.86, 1. 7, and 2.6 at T = 0.1T c in d-wave ... 0.4 H 1 10 -12 1 10 -11 1 10 -10 |F| 2 2.6 1. 7 0.86 0.02 µ= (b) 0 0 .1 H 0 1 10 -5 F 10 F 10 M 10 Fig. 8. Field dependence of FLL form fac...

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... integers i, j, k  12 12 12 12 12 , 12 , , 12 , 12 1 ,, 01 , , |||| || nnnn yy xx ij ij ij ij nn zij zij ij HHHH t EE xy               ( 21) , ,1, 1, 1 ,, 0 . || || || nn ... time-step n +1:  12 12 12 12 12 , 12 , , 12 , 12 1 ,, 01 , . |||| || nnnn yy xx ij ij ij ij nn zij zij ij HHHH t EE xy            ...

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... R fnm GR                        ( 61)    2 1 1 21. 21 2 21, 2 1 2 21. 21 , sin (2 1) 2 2 () 11 (2 1) (1) sin 4sin( 21) 2 L m nm nm La b nm am N L f JG R am NLamLGR     ... Physical Review B, Vol. 64, No. 12 , (September 20 01) , pp. 12 110 3 -1 - 12 110 3-4, ISSN 10 98- 012 1 Kee, C S.; Lim, H.; Ha, Y K.; Kim, J E. & Park, H...

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... Phys. Chem. Solids 28, pp .15 41- 1545 Bean C.P. (19 64), Magnetization of High-Field Superconductors, Rev.Mod.Phys. 36, 31- 39 Carr W.J. (19 83) AC Loss and Macroscopic Theory of Superconductors, ... Superconductivity – Theory and Applications 340 The degree of the foil anisotropy is seen from Figs .10 and 12 . It allows estimating of agreement between experimental data a...

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... expressed as Equation 17 . G dBd = 10 log 10 W rad W d rad = 10 log 10 ( W rad W i rad × W i rad W d rad ) = 10 (log 10 g − log 10 g d ) (17 ) 7 Operating Range Evaluation of RFID Systems Pref ac e Radio ... UHF RFID Tags 11 5 Benjamin D. Braaten and Masud A. Aziz Fully Printable Chipless RFID Tag 13 1 Stevan Preradovic and Nemai Karmakar The Interaction of Electrostatic D...

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