Application of zero-temperature-gradient zero-bias thermally stimulated current spectroscopy to ultrathin high-dielectric-constant insulator film characterization
Abstract:Previously, we have reported our application of the zero-bias thermally stimulated current (ZBTSC) spectroscopy technique to study defect states in high-dielectric-constant insulator films such as tantalum oxide with much less parasitic current which can be a serious limitation for the conventional thermally stimulated current method. However, a parasitic current can still be observed for ZBTSC because of a small parasitic temperature gradient across the sample. The thermal design of the ZBTSC system can be im… Show more
“…In addition to thermopolarization current, the current may originate from the small voltage burden on the picoammeter (about 300 µV in case of device used in our experiments) or from a temperature gradient across the sample (potential difference of Seebeck effect). 66 Let us assume that the current originates from one of these three sources. For a sample with a perfect centric symmetry, the two orientations of a sample, "up" and "down", should be equivalent and the response to either the voltage or the temperature gradient should be the same, regardless of the orientation of the sample.…”
BaTiO3 appears in cubic and hexagonal variants, both of which are
centrosymmetric. Samples of cubic BaTiO3 are known to exhibit breaking of the
centric symmetry locally and globally. It has been proposed that the local
symmetry breaking originates in polar regions, the precursors of the
ferroelectric phase. Origins of the macroscopic symmetry breaking, which are
not well understood, have been previously tentatively correlated with
inhomogeneities in the samples, such as strain gradients that may align or
redistribute objects such as charged point defects or polar regions making
material macroscopically polar. No such data are available for BaTiO3 with
hexagonal symmetry. We compare dielectric, elastic, and pyroelectric properties
of the two materials in polycrystalline form. In contrast to cubic BaTiO3,
hexagonal BaTiO3 does not exhibit macroscopic pyroelectric response at room
temperature. This is consistent with apparent absence of polar regions in the
hexagonal material and the fact that in hexagonal BaTiO3 strain rather then
polarization is the order parameter for the phase transition into
ferroelectric-ferroelastic phase. The thermally stimulated currents measured in
hexagonal and cubic BaTiO3, however, show that both materials exhibit
noncentric macroscopic symmetry. This result supports the idea that extrinsic
factors such as strain gradients, which are apparently common for both
materials, may break the macroscopic symmetry, which may then lead to alignment
and redistribution of polar regions or charged defects.Comment: accepted in Journal of Applied Physic
“…In addition to thermopolarization current, the current may originate from the small voltage burden on the picoammeter (about 300 µV in case of device used in our experiments) or from a temperature gradient across the sample (potential difference of Seebeck effect). 66 Let us assume that the current originates from one of these three sources. For a sample with a perfect centric symmetry, the two orientations of a sample, "up" and "down", should be equivalent and the response to either the voltage or the temperature gradient should be the same, regardless of the orientation of the sample.…”
BaTiO3 appears in cubic and hexagonal variants, both of which are
centrosymmetric. Samples of cubic BaTiO3 are known to exhibit breaking of the
centric symmetry locally and globally. It has been proposed that the local
symmetry breaking originates in polar regions, the precursors of the
ferroelectric phase. Origins of the macroscopic symmetry breaking, which are
not well understood, have been previously tentatively correlated with
inhomogeneities in the samples, such as strain gradients that may align or
redistribute objects such as charged point defects or polar regions making
material macroscopically polar. No such data are available for BaTiO3 with
hexagonal symmetry. We compare dielectric, elastic, and pyroelectric properties
of the two materials in polycrystalline form. In contrast to cubic BaTiO3,
hexagonal BaTiO3 does not exhibit macroscopic pyroelectric response at room
temperature. This is consistent with apparent absence of polar regions in the
hexagonal material and the fact that in hexagonal BaTiO3 strain rather then
polarization is the order parameter for the phase transition into
ferroelectric-ferroelastic phase. The thermally stimulated currents measured in
hexagonal and cubic BaTiO3, however, show that both materials exhibit
noncentric macroscopic symmetry. This result supports the idea that extrinsic
factors such as strain gradients, which are apparently common for both
materials, may break the macroscopic symmetry, which may then lead to alignment
and redistribution of polar regions or charged defects.Comment: accepted in Journal of Applied Physic
“…[17][18][19][20][21][22] The precursor used was tantalum ethoxide with the chemical formula of Ta(OC 2 H 5 ) 5 . As deposited Ta 2 O 5 film is amorphous and very leaky.…”
Section: Methodsmentioning
confidence: 99%
“…[17][18][19][20][21][22] Conventional TSC technique suffers from a serious parasitic current problem because of the need to apply a bias voltage to the sample. The purpose of "zero bias" is to solve this parasitic current problem.…”
Historically, it has been difficult to correlate the leakage current of capacitor structures involving high-k dielectric materials and defect states detected spectroscopically by the thermally stimulated current (TSC) technique. Four mechanisms are proposed and solutions are explained with tantalum oxide as an example. One of the mechanisms is the limitation of the TSC technique itself because of the presence of a parasitic current due to the bias voltage used. This can be solved by migrating to more advanced versions of TSC like zero-bias TSC or zero-temperature-gradient zero-bias TSC. In addition, another possible mechanism is that some defect states may have an electron repulsive energy barrier. Furthermore, another possible mechanism is that the leakage current may be insensitive to the presence of defect states under some situations; a unified Schottky-Poole-Frenkel model is proposed by the author to explain such a situation. Finally, another mechanism is due to the non-uniform distribution of defect states. Sometimes, this can be solved by using a 2-zone model proposed by the author.
“…Charge relaxation during the heating scan of the ZB-TSC can be discussed [9] in terms of motion of the zero electric-field planes (ZFP) along the sample depth. Details on the ZB-TSC technique applied on different semiconductor materials are reported in [10,11].…”
We report on the investigation of the radiation damage induced by neutron irradiation on both nand p-type Magnetic Czochralski silicon pad detectors by the Thermally Stimulated Currents (TSC) technique. Detectors have been irradiated with fast neutrons in the range 10 14-10 16 n/cm 2. Priming conditions have been studied in detail in order to investigate the residual electric field due to frozen charged traps after the priming step and its influence on the TSC emission. Zero bias TSC measurements have also been performed as an additional tool to study the defects distribution and the residual electric field. The electric field distribution inside the sample and its effect on the TSC emission are qualitatively explained by a band diagrams description.
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