Abstract:The Y5V-1206 base-metal electrode (BME) multilayer ceramic capacitor (MLCC) chips have been characterised for crystalline phases using X-ray diffractometry (XRD), and microstructure using optical microscopy (OM), scanning electron microscopy (SEM) and transmission electron microscopy (TEM). The microstructure features found in the Ni electrode and the BaTiO 3 dielectric layer are discussed in terms of the tensile backstresses induced upon firing due to constrained sintering heterogeneously. The chemical compos… Show more
“…1) The tetragonal phase of perovskitestructured BaTiO 3 is widely used as a dielectric material in multi-layer ceramic capacitors (MLCCs) [2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18] on account of its exceptionally large permittivity at room temperature. The ferroelectric phase-transition mechanism can be explained in terms of the successive freezing of the triply degenerate polar soft-mode phonon at the À point in the high symmetry Pm " 3m structure.…”
The anisotropic nature of the permittivity of tetragonal BaTiO 3 has been investigated by means of first-principles calculations using densityfunctional perturbation theory and constrained-force approaches. Our calculations suggest that the origin of the anisotropy is the presence of a soft mode with very shallow double-well potential surface that results in non-frozen dipole moments parallel to the a-axes of the tetragonal crystal. Even at relatively low temperatures, the dipoles fluctuate back and forth, resulting in net zero dipole perpendicular to the c-axis in the absence of an electric field. The enormous permittivity observed experimentally parallel to the a-axis of tetragonal BaTiO 3 is a consequence of the relatively large polarization induced by these small lattice distortions, together with the low energy barrier that needs to be overcome to switch to the polarized structure. #
“…1) The tetragonal phase of perovskitestructured BaTiO 3 is widely used as a dielectric material in multi-layer ceramic capacitors (MLCCs) [2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18] on account of its exceptionally large permittivity at room temperature. The ferroelectric phase-transition mechanism can be explained in terms of the successive freezing of the triply degenerate polar soft-mode phonon at the À point in the high symmetry Pm " 3m structure.…”
The anisotropic nature of the permittivity of tetragonal BaTiO 3 has been investigated by means of first-principles calculations using densityfunctional perturbation theory and constrained-force approaches. Our calculations suggest that the origin of the anisotropy is the presence of a soft mode with very shallow double-well potential surface that results in non-frozen dipole moments parallel to the a-axes of the tetragonal crystal. Even at relatively low temperatures, the dipoles fluctuate back and forth, resulting in net zero dipole perpendicular to the c-axis in the absence of an electric field. The enormous permittivity observed experimentally parallel to the a-axis of tetragonal BaTiO 3 is a consequence of the relatively large polarization induced by these small lattice distortions, together with the low energy barrier that needs to be overcome to switch to the polarized structure. #
“…3(a and b), it can be seen that the continuity of the internal electrodes in the MLCC was about 88% with a lay down of approximately 0.6 mg/cm 2 . The dielectric film thickness after sintering was approximately 17 m and the electrode thickness was approximately 2.0 m. However, the continuity of internal 6 electrodes in commercial MLCCs is below 80% in general with particular reference to the Y5V-1206 MLCCs rated 1 F and manufactured by Yageo Co. [17]. Pure BaTiO 3 powders are often added to the metal electrode so as to decrease the coefficient mismatch of thermal expansion and increase the sintering match with the dielectric layers.…”
Section: Effect Of Cu Doped Ni Electrodes On the Microstructures Of Bmentioning
“…The EIA‐rated X7R and X5R BME‐MLCCs with ε r ≈ 1000–5000, Z5U and Y5V with ε r > 8000 are now categorized as class II capacitors. G av in X7R is usually less than 1.2 μm, some being much smaller at ~250–400 nm, whereas those of Y5V and Z5U ranging between ~3 and 10 μm (3–5 μm) are at least several times larger. The latter two have much higher relative permittivity, ε r ≈ 18 000 for Y5V and <14 000 for Z5U.…”
Section: Introductionmentioning
confidence: 96%
“…Both X7R and Y5V formulations include aliovalent ions as dopants, but X7R's ε r at ~1000–5000 is significantly lower . The Y5V microstructure is usually referred to as consisting of “solid‐solution” grains with solutes Ca and Zr distributed homogeneously in the grains. It appears that rather than the average grain size the doping system determines the high relative permittivity in BaTiO 3 ‐based mixed crystal.…”
Commercial EIA-Y5V base-metal-electrode multilayer ceramic capacitors (BME-MLCCs) made of (CaO+ZrO 2 )-doped BaTiO 3 are analyzed for the microstructure and investigated for its relation to dielectric properties. The characteristic diffuse scattering (DS) intensities observed in BaTiO 3 ceramics and the featureless "solid-solution" grains in Y5V capacitor chips are originated from multiple Ti sites in the dynamic BaTiO 3 structure. The pseudo-cubic (PC)-grains retaining the overall cubic (C-) symmetry metastably at room temperature are embedded with polar nanoregions (PNRs) in the ferroelectric (FE) tetragonal (T-), and rhombohedral (R-) phases, as revealed by high-resolution transmission electron microscopy (HRTEM). The presence of PNRs contributes effectively to large relative permittivity e r % 13 200 at 25°C. The FE T-domains grow from within PC-grains at the expense of embedded PNRs after prolonged annealing by extending "oxidizing firing" at 950°C in pO 2 = 10 -7 atm. These domains contain less Zr with otherwise homogeneously distributed solutes in PNR-dispersed PC-grains. Although preserving the relaxors characteristics, e r is reduced to~11 000 after 12 h, and then to~9000 after 24 h annealing. The reduction in e r is attributed to the annealing-induced FE T-domains grown at the expense of PNRs in PC-grains. The V€ ogel-Fulcher analysis indicates that Y5V ceramics are in the relaxor FE category, containing PNRs derived from polarization frustration.C. Alan Randall-contributing editor Manuscript No. 34036.
J ournaldispersion of e r were investigated for the crystalline phases using X-ray diffractometry (XRD). The microstructure and microanalysis were determined using scanning and transmission electron microscopy (SEM and TEM).
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