Superconductivity Theory and Applications Part 1 pot

... = 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...

Ngày tải lên: 19/06/2014, 21:20

... weighted sum phases: 12 11 22 , ,cc          (14 ) for the free energy density (1) -(3) we obtain 2424 11 11 22 22 22 2 12 2 12 12 22 2 12 22 2 21 1 212 12 12 11 22 2cos 22 2cos 22 2cos. F d mm ...  Where 2 24 11 1 11 1 1 11 2 22 e FiA mc           (1) 2 24 222 22 2 2 11 2 22 e FiA mc           (2) an...

Ngày tải lên: 19/06/2014, 21:20

... measurements at T=4.5 K are summarised in Figs .12 (a), Fig .12 (b), Fig. 13 (a) and Fig .13 (b). The stack of left hand panels in Figs. 12 (a), 12 (b), 13 (a) and 13 (b) show the normalized V(t)/V 0 versus ... Creation and Annihilation of Metastable Vortex Phase as a Source of Excess Noise. Europhysics Letters Vol. 58, No. 1, pp 11 2 -11 8 Shi, A. C. & Berlinsky, A. J. (...

Ngày tải lên: 19/06/2014, 21:20

... Robust stability Let the linear system be given by the transfer function 1 110 1 110 11 11 () () (1) () (1) s L ss LL mm T mm nn nn mm TT m nn n bs b s bs b Gs e as a s as a s sn n b eV ... Topology and Different Kinds of Node Dynamics 423 Sabato Manfredi Chapter 8 Chapter 9 Part 4 Chapter 10 Chapter 11 Chapter 12 Chapter 13 Chapter 14 Chapter 15 Chapter 16 C...

Ngày tải lên: 20/06/2014, 04:20

... Bearings, Theory and Applications, Edited by Boštjan Polajžer p. cm. ISBN 978-953-307 -14 8-0 Magnetic Bearings, Theory and Applications4 3. System Identification 3 .1 System Identification and ... lead compensator Design and implementation of conventional and advanced controllers for magnetic bearing system stabilization 1 Design and implementation of conventiona...

Ngày tải lên: 20/06/2014, 06:20

... Diversity 415 Kadir M.F. A., Suaidi M.K. and Aziz M. Z. A. Chapter 8 Part 3 Chapter 9 Chapter 10 Chapter 11 Chapter 12 Chapter 13 Part 4 Chapter 14 Chapter 15 Chapter 16 Chapter 17 Part 5 Chapter 18 free ... modulated. 0 5 10 15 10 −6 10 −5 10 −4 10 −3 10 −2 10 1 10 0 SNR(dB) BER RayleighTx1Rx1 AlamoutiTx2Rx1 AlamoutiTx2Rx2 Fig. 5. BER curves for B...

Ngày tải lên: 21/06/2014, 03:20

... 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...

Ngày tải lên: 19/06/2014, 21:20

... high-pure (l el ∼ 10 0 μm) single-crystal normal metals Cu 10 0 Superconductivity – Theory and Applications Superconductivity – Theory and Applications 94 connecting J1 and J2. With proper ... 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. Ni...

Ngày tải lên: 19/06/2014, 21:20

... 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 ... effect for the major portion of electrons. 11 4 Superconductivity – Theory and Applications Superconductivity – Theory and Application...

Ngày tải lên: 19/06/2014, 21:20

... 14 2 010 17 :33:09 VECTOR STEP =1 SUB =1 TIME =1 FX ELEM =14 58 MIN= .15 7E-08 MAX= .14 1E-03 1 .353E -10 .10 3E-06 .206E-06 .308E-06 . 411 E-06 . 514 E-06 . 617 E-06 .720E-06 .822E-06 .925E-06 JUL 14 2 010 17 :39 :10 VECTOR STEP =1 SUB ... 2 010 17 :39 :10 VECTOR STEP =1 SUB =1 TIME =1 MX ELEM =14 59 MIN=.353E -10 MAX=.925E-06 1 3.865 669.99 13 36 2002 2668 3334 40 01...

Ngày tải lên: 19/06/2014, 21:20