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弛豫铁电超晶格:高能量密度电容器。

Relaxor-ferroelectric superlattices: high energy density capacitors.

机构信息

Department of Physics and Institute for Functional Nanomaterials, University of Puerto Rico, San Juan, PR 00931-3343, USA.

出版信息

J Phys Condens Matter. 2012 Nov 7;24(44):445901. doi: 10.1088/0953-8984/24/44/445901. Epub 2012 Oct 10.

Abstract

We report the breakdown electric field and energy density of laser ablated BaTiO(3)/Ba((1-x))Sr(x)TiO(3) (x = 0.7) (BT/BST) relaxor-ferroelectric superlattices (SLs) grown on (100) MgO single crystal substrates. The dielectric constant shows a frequency dispersion below the dielectric maximum temperature (T(m)) with a merger above T(m) behaving similarly to relaxors. It also follows the basic criteria of relaxor ferroelectrics such as low dielectric loss over wide temperature and frequency, and 50 K shift in T(m) with change in probe frequency; the loss peaks follow a similar trend to the dielectric constant except that they increase with increase in frequency (40 kHz), and satisfy the nonlinear Vogel-Fulcher relation. Well-saturated ferroelectric hysteresis and 50-80% dielectric saturation are observed under high electric field (1.65 MV cm(-1)). The superlattices demonstrate an 'in-built' field in as grown samples at low probe frequency (<1 kHz), whereas it becomes more symmetric and centered with increase in the probe frequency system (>1 kHz) which rules out the effect of any space charge and interfacial polarization. The P-E loops show around 12.24 J cm(-3) energy density within the experimental limit, but extrapolation of this data suggests that the potential energy density could reach 46 J cm(-3). The current density versus applied electric field indicates an exceptionally high breakdown field (5.8-6.0 MV cm(-1)) and low current density (~10-25 mA cm(-2)) near the breakdown voltage. The current-voltage characteristics reveal that the space charge limited conduction mechanism prevails at very high voltage.

摘要

我们报告了激光烧蚀的 BaTiO(3)/Ba((1-x))Sr(x)TiO(3) (x = 0.7) (BT/BST) 弛豫铁电超晶格 (SL) 在 (100) MgO 单晶衬底上的击穿电场和能量密度。介电常数在介电最大值温度 (T(m)) 以下表现出频率色散,在 T(m) 以上合并表现出类似弛豫体的行为。它还遵循弛豫铁电体的基本准则,例如在宽温度和频率范围内介电损耗低,以及在探针频率变化时 T(m) 变化 50 K;损耗峰遵循与介电常数相似的趋势,除了它们随频率增加而增加(约 40 kHz),并且满足非线性 Vogel-Fulcher 关系。在高电场 (1.65 MV cm(-1)) 下观察到铁电滞后和 50-80%介电饱和。在低探针频率 (<1 kHz) 下,在生长样品中观察到超晶格的“内置”场,而随着探针频率系统的增加(>1 kHz),它变得更加对称和居中,排除了任何空间电荷和界面极化的影响。P-E 环在实验限制内显示约 12.24 J cm(-3) 的能量密度,但对该数据的外推表明潜在能量密度可能达到 46 J cm(-3)。电流密度与施加电场的关系表明击穿电场(5.8-6.0 MV cm(-1)) 异常高,击穿电压附近的电流密度 (10-25 mA cm(-2)) 低。电流-电压特性表明,在非常高的电压下,空间电荷限制传导机制占主导地位。

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