0

ferroelectrics relaxors and dipolar glasses

Ferroelectrics Characterization and Modeling Part 1 pdf

Ferroelectrics Characterization and Modeling Part 1 pdf

Kĩ thuật Viễn thông

... Ferroelectrics, Relaxors and Dipolar Glasses 181 Seweryn Miga, Jan Dec and Wolfgang Kleemann Chapter 11 135 Ferroelectrics Study at Microwaves 203 Yuriy Poplavko, Yuriy Prokopenko, Vitaliy Molchanov and ... and A M Umarji, Material Research Bulletin, 30, 427-434, (1995) [26] S P Singh, A K Singh, and D Pandey, J Phys.: Condense Matter 19, 036217, (2007) [27] S P Singh, A K Singh, and D Pandey, Ferroelectrics, ... Bichurin and Shashank Priya Chapter Impact of Defect Structure on ’Bulk’ and Nano-Scale Ferroelectrics Emre Erdem and Rüdiger-A Eichel Chapter Part Chapter 79 Microstructural Defects in Ferroelectrics...
  • 35
  • 403
  • 0
Ferroelectrics Characterization and Modeling Part 2 docx

Ferroelectrics Characterization and Modeling Part 2 docx

Kĩ thuật Viễn thông

... 140 K and 180 K show intensive bands at 635, 758, 810, 852, 928, 1027 cm-1 and 675, 795, 870, 912, 954, 1001, 1051, 1147 cm-1, respectively The broadening of the bands significantly 44 Ferroelectrics ... incoherent neutron scattering and 1H NMR 42 Ferroelectrics - Characterization and Modeling In the inelastic incoherent neutron scattering (IINS) spectra the intensity of selected bands depends on the ... state at 20 K(fig.2a) and 294 K (fig.2b) 46 Ferroelectrics - Characterization and Modeling Discussion Calculations of the vibrational spectra require the molecular structure and the force field...
  • 35
  • 420
  • 0
Ferroelectrics Characterization and Modeling Part 3 docx

Ferroelectrics Characterization and Modeling Part 3 docx

Kĩ thuật Viễn thông

... 001 Intensity (arb units) Ferroelectrics - Characterization and Modeling 60 2θ Fig (a) XRD patterns of calcined BTO and CFO powder and (b) XRD patterns of BT – 30 CF and BT – 35 CF magnetoelectric ... microstructure taken from (b) a BTOrich island, and (c) the CFO-rich matrix It can be seen that the grain sizes of both regions are 66 Ferroelectrics - Characterization and Modeling quite small: the average ... I: Composition and Unidirectional Solidification J.Mater.Sci pp 1705-1709 Dong S, Li J, and Viehland, D (2003) Ultrahigh Magnetic Field Sensitivity in Laminates of Terfenol-D and Pb(Mg1/3Nb2/3)O3-PbTiO3...
  • 35
  • 363
  • 0
Ferroelectrics Characterization and Modeling Part 4 ppt

Ferroelectrics Characterization and Modeling Part 4 ppt

Kĩ thuật Viễn thông

... (2001) Principles and Applications of Ferroelectrics and Related Materials, Oxford, Great Britain [21] Xu, Y (1991) Ferroelectric Materials and Their Applications, North Holland, Amsterdam [22] ... defects and their evolution [2] Defects will change optical, mechanical, electrical and electromechanical behaviors of ferroelectrics [3, 4] However current understanding is limited to bulk and thin ... considered for dynamic and nonvolatile random access memories, Pb(Zr,Ti)O3 is high piezoelectric constant material being used for actuators and transducers, and LaMnO3 and (La,Sr)CoO3 are being...
  • 35
  • 482
  • 0
Ferroelectrics Characterization and Modeling Part 5 docx

Ferroelectrics Characterization and Modeling Part 5 docx

Kĩ thuật Viễn thông

... capacitance and loss tangent of polycrystalline BFO films fabricated by PLD and CSD methods are shown in figure and figure 4, respectively 140 Ferroelectrics - Characterization and Modeling ... sublattice and competitive (ferroelectric and antiferroelectric) interactions occur between copper ions or (and) between copper ions and lattice Competitive interactions can also occur between copper and ... also fabricated by CSD method and is used as bottom electrode Both STO and LNO are perovskite structure and smaller crystal constant than BFO Therefore, the substrate and the LNO layer can induce...
  • 35
  • 429
  • 0
Ferroelectrics Characterization and Modeling Part 6 pptx

Ferroelectrics Characterization and Modeling Part 6 pptx

Kĩ thuật Viễn thông

... (3) Non-Linear Dielectric Response of Ferroelectrics, Relaxors and Dipolar Glasses 183 where G0 stands for the free energy at P = 0, A and T0 are constants B and C are usually smooth functions of ... Response of Ferroelectrics, Relaxors and Dipolar Glasses (c) (b) χ3 χ1 (a) 185 a3 0 Tc Tc Tf Tm Temperature Fig Schematic presentation of linear and nonlinear responses of classic ferroelectrics ... j7     (14) Non-Linear Dielectric Response of Ferroelectrics, Relaxors and Dipolar Glasses 187 where ω and E0 are the angular frequency and the amplitude of the applied electric field respectively...
  • 35
  • 339
  • 0
Ferroelectrics Characterization and Modeling Part 7 pdf

Ferroelectrics Characterization and Modeling Part 7 pdf

Kĩ thuật Viễn thông

... in SrTiO3, JETP-Lett., Vol 89, pp 457 - 467 Non-Linear Dielectric Response of Ferroelectrics, Relaxors and Dipolar Glasses 201 Leont’ev, I N., Leiderman, A., Topolov, V Yu & Fesenko, O E (2003) ... properties remain unknown Therefore, accurate and reliable measuring of dielectric constant and loss factor of bulk and thin film ferroelectrics and related materials remains an actual problem ... dependencies of domain structure and ferroelectric properties, and correlates physical properties, namely lattice 230 Ferroelectrics - Characterization and Modeling parameters and the volume fractions...
  • 35
  • 443
  • 0
Ferroelectrics Characterization and Modeling Part 8 doc

Ferroelectrics Characterization and Modeling Part 8 doc

Kĩ thuật Viễn thông

... 256 Ferroelectrics - Characterization and Modeling and 307 cm-1 bands in BaTi1-yCayO3 Fig.9 shows the bands 299, 520 and 723 cm -1 were independent of the formation of CaBa and CaTi in Bi-BCT and ... formation of the 520 and 723 cm-1 bands, and Ti-O bonds to the formation of the 262 and 299 cm-1 bands We also find the development of a weak new Raman band at 827cm-1 for Bi-BTC and Bi-BCT (see Fig ... Temperature dependence of the dielectric constant and the dielectric loss of Bi-BCT and Bi-BSCT for x=0.10 ((A) and (B)), x=0.20 ((C) and (D)) and y=0.05 at 0.1, 1, 10, 100 kHz (for dielectric...
  • 35
  • 250
  • 0
Ferroelectrics Characterization and Modeling Part 9 pot

Ferroelectrics Characterization and Modeling Part 9 pot

Kĩ thuật Viễn thông

... dielectric constants of ferrites, ferroelectrics and their composites vary randomly It is due to the mismatching of grains of ferrites and ferroelectrics in the composites and hence it is difficult to ... and PZT) are shown in figs (5 & 6) The dielectric constant increases with increase in temperature and becomes maximum at Curie temperature (Tc) and there after it decreases For BPZT and PZT ferroelectrics, ... relaxation time and the period of applied field 272 Ferroelectrics - Characterization and Modeling When loss is minimum, then relaxation time is greater than period of applied field and it is maximum...
  • 35
  • 290
  • 0
Ferroelectrics Characterization and Modeling Part 10 pot

Ferroelectrics Characterization and Modeling Part 10 pot

Kĩ thuật Viễn thông

... the values of VBO and CBO, it has been found that type-II band alignments form at the ZnO/SrTiO3 and ZnO/BaTiO3 interfaces, while type-I band alignments form at InN/SrTiO3 and InN/BaTiO3 interfaces ... on the values of VBO and CBO, it has been found that type-II band alignments form at the ZnO/STO and ZnO/BTO interfaces, while type-I band alignments form at the InN/STO and InN/BTO interfaces ... from the respective STO substrate and thick ZnO film Figure shows the XPS Ti 2p and Zn 2p CL narrow scans and the valence band spectra from the STO substrate and the thick ZnO/STO samples, respectively...
  • 35
  • 460
  • 0
Ferroelectrics Characterization and Modeling Part 11 potx

Ferroelectrics Characterization and Modeling Part 11 potx

Kĩ thuật Viễn thông

... eCF and pr (a) (b) Fig 13 Hysteresis loops for various values of δ : (a) δ =3.0, 10.0 and 50.0; (b) δ = —3.0, —10.0 and —50.0; for t = 0.0, e0 = 3.0, and ω = 0.1 (Ong and Ahmad, 2009) Summary and ... phase transition temperature and T1 = T0 + 3B3 /(4γ A) , where B, γ and A are the Landau parameters This formula indicates 358 Ferroelectrics - Characterization and Modeling that there is a definite ... two examples given in Figs and and Tables and 2, we have also fitted other calculated data for various thicknesses and values of δ by the formulations mentioned above; and we have found that the...
  • 35
  • 299
  • 0
Ferroelectrics Characterization and Modeling Part 12 pdf

Ferroelectrics Characterization and Modeling Part 12 pdf

Kĩ thuật Viễn thông

... 3s and 3p states and O 2s and 2p states in BaTiO3 : (a) anisotropic Coulomb repulsions between Ti 3s and 3px ( y) states and O x ( y) 2s and 2px ( y) states, and between Ti 3s and 3pz states and ... between Ti 3s and 3pz 396 Ferroelectrics - Characterization and Modeling Ferroelectrics states and O 2pz states not favourably cause Ti ion displacement Experimentally, on the other hand, Kuroiwa ... between Ti 3s and 3px ( y) states and O x ( y) 2s and 2px ( y) states, in addition to the dipole-dipole interaction, overcome the Coulomb repulsions between Ti 3s and 3pz states and Oz 2s and 2pz states...
  • 35
  • 300
  • 0
Ferroelectrics Characterization and Modeling Part 13 ppt

Ferroelectrics Characterization and Modeling Part 13 ppt

Kĩ thuật Viễn thông

... (North-Holland, Amsterdam, 1974) [10] R J Nelmes, Ferroelectrics 71, 87 (1987) [11] Y Takagi, Ferroelectrics 72, 67 (1987) [12] F Gervais and P Simon, Ferroelectrics 72, 77 (1987) [13] G Samara, Ferroelectrics ... 2006) [87] D S Bystrov and E A Popova, Ferroelectrics 72, 147 (1987) 436 26 Ferroelectrics - Characterization and Modeling Will-be-set-by-IN-TECH ˇ s [88] R Blinc and B Zekˇ, Ferroelectrics 72, ... Will-be-set-by-IN-TECH [7] G Busch and P Scherrer, Naturwiss 23, 737 (1935) [8] G Busch, Helv Phys Acta 11, 269 (1938) ˇ s [9] R Blinc and B Zekˇ, in Soft Modes in Ferroelectrics and Antiferroelectrics, edited...
  • 35
  • 274
  • 0
Ferroelectrics Characterization and Modeling Part 15 pptx

Ferroelectrics Characterization and Modeling Part 15 pptx

Kĩ thuật Viễn thông

... negative and positive(step 2) and stress (compressive and tensile stress) (step 1) In conclusion, we could determine P(T) and P(θ) from P(E) (steps and 3),P(E) and P(θ) from P(T) (steps and 2), and ... (steps and 3), P(E) and P(θ) from P(T) (steps and 2), and at the end we can determine P(E) and P(T) from P(θ) (steps and 3), Fig Schematic illustration of the scaling laws Nonlinearity and Scaling ... and dD = ε 33 dE + pdθ D = ε 0E + P (12) (13) D, P, E, θ and Γ and G represent the electric displacement, the polarization, the electric field, the temperature and the entropy, respectively, and...
  • 35
  • 307
  • 0
Ferroelectrics Characterization and Modeling Part 16 potx

Ferroelectrics Characterization and Modeling Part 16 potx

Kĩ thuật Viễn thông

... Crawley and Anderson 1990, Zhou and Kamlah 2006) The electrical and mechanical responses of PZT are also shown to be time-dependent, especially under high electric field (Fett and Thun 1998; Cao and ... (Findley and Lai, 1967), multiple integral model (Green and Rivlin 1957), finite strain integral models (Pipkins and Rogers 1968; Rajagopal and Wineman 2010), single integral models (Pipkins and Rogers ... this complication The Landau Khalatnikov equations in Equation (33) are appropriate 522 10 Ferroelectrics - Characterization and Modeling Will-be-set-by-IN-TECH for displacive ferroelectrics that...
  • 35
  • 315
  • 0
Ferroelectrics Characterization and Modeling Part 17 docx

Ferroelectrics Characterization and Modeling Part 17 docx

Kĩ thuật Viễn thông

... Ferroelectric Ceramics,” J Intel Material Systems and Structures, 12, pp 79-91 [22] Lines, M.E and Glass, A E (2009) Principles and Applications of Ferroelectrics and Related Materials, Oxford University ... Engineering and Sciences, 24, pp 215-238 560 Ferroelectrics - Characterization and Modeling [34] Zhou, D and Kamlah, M (2006), “Room-temperature Creep of Soft PZT under Static Electrical and Compressive ... Since we need expressions for σ and D in order to solve Equation (31), we rewrite Equation (36) and (37) and obtain Modeling and Numerical Simulation of Modeling and Numerical Simulation Ferroelectric...
  • 35
  • 302
  • 0
Ferroelectrics Characterization and Modeling Part 18 pdf

Ferroelectrics Characterization and Modeling Part 18 pdf

Kĩ thuật Viễn thông

... Determination of Real and Complex Elastic, Dielectric and Piezoelectric Moduli in Piezoceramic Materials, IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control 55(2): 465–475 Landis, C M ... constitutive modeling of ferroelectrics, Current Opinion in Solid State and Materials Science 8: 59–69 Linnemann, K., Klinkel, S & Wagner, W (2009) A constitutive model for magnetostrictive and piezoelectric ... procedure and computation of overall moduli, Proceedings of the IUTAM conference on multiscale modeling of fatigue, damage and fracture in smart materials, Springer, Heidelberg 586 26 Ferroelectrics...
  • 3
  • 225
  • 0
FERROELECTRICS CHARACTERIZATION AND MODELING docx

FERROELECTRICS CHARACTERIZATION AND MODELING docx

Kĩ thuật Viễn thông

... Ferroelectrics, Relaxors and Dipolar Glasses 181 Seweryn Miga, Jan Dec and Wolfgang Kleemann Chapter 11 135 Ferroelectrics Study at Microwaves 203 Yuriy Poplavko, Yuriy Prokopenko, Vitaliy Molchanov and ... and A M Umarji, Material Research Bulletin, 30, 427-434, (1995) [26] S P Singh, A K Singh, and D Pandey, J Phys.: Condense Matter 19, 036217, (2007) [27] S P Singh, A K Singh, and D Pandey, Ferroelectrics, ... Bichurin and Shashank Priya Chapter Impact of Defect Structure on ’Bulk’ and Nano-Scale Ferroelectrics Emre Erdem and Rüdiger-A Eichel Chapter Part Chapter 79 Microstructural Defects in Ferroelectrics...
  • 598
  • 1,301
  • 0
statistical physics of spin glasses and information processing an introduction - nishimori h.

statistical physics of spin glasses and information processing an introduction - nishimori h.

Vật lý

... Edwards–Anderson model (Edwards and Anderson 1975) The randomness in site positions (site randomness) is considered less relevant to the macroscopic properties of spin glasses compared to the randomness ... Tree-like and nested structures in an ultrametric space The distance between C and D is equal to that between C and E and to that between D and E, which is smaller than that between A and C and that ... 1.3.3 Free energy and the Landau theory 1.4 Infinite-range model 1.5 Variational approach Mean-field theory of spin glasses 2.1 Spin glass and the Edwards–Anderson model 2.1.1 Edwards–Anderson model...
  • 252
  • 502
  • 0

Xem thêm