914 resultados para Polarization gating


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We present a report of our analysis of wave vector dependence of the static dielectric function of a dipolar liquid obtained by a microscopic calculation. At low values of the wave vector (k), the longitudinal dielectric function ϵ(k) increases with k, in contradiction to some assumptions reported in the literature. As the value of k is increased, ϵ(k) diverges at a critical value kc which depends on the value of the long wavelength static dielectric constant (ϵ0) of the liquid. The dielectric function is negative for values of k greater than kc. At large values of k, the calculated ϵ(k) fails to attain the limiting value of unity. We attribute this result to the failure of the point dipole assumption made in the evaluation of the polarization correlation function required by the theory. The behavior of ϵ(k) for the dipolar liquid is compared with that of one component plasma for which reliable results can be obtained over the full range of wave vectors. For both systems, the stability conditions are fulfilled at all values of k. A plausible explanation of this rather exotic behavior of ϵ(k) is given.

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Li-doped ZnO thin films (Zn1-xLixO, x=0.05-0.15) were grown by pulsed-laser ablation technique. Highly c-axis-oriented films were obtained at a growth temperature of 500 degrees C. Ferroelectricity in Zn1-xLixO was found from the temperature-dependent dielectric constant and from the polarization hysteresis loop. The transition temperature (T-c) varied from 290 to 330 K as the Li concentration increased from 0.05 to 0.15. It was found that the maximum value of the dielectric constant at T-c is a function of Li concentration. A symmetric increase in memory window with the applied gate voltage is observed for the ferroelectric thin films on a p-type Si substrate. A ferroelectric P-E hysteresis loop was observed for all the compositions. The spontaneous polarization (P-s) and coercive field (E-c) of 0.6 mu C/cm(2) and 45 kV/cm were obtained for Zn0.85Li0.15O thin films. These observations reveal that partial replacement of host Zn by Li ions induces a ferroelectric phase in the wurtzite-ZnO semiconductor. The dc transport studies revealed an Ohmic behavior in the lower-voltage region and space-charge-limited conduction prevailed at higher voltages. The optical constants were evaluated from the transmission spectrum and it was found that Li substitution in ZnO enhances the dielectric constant.

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Monophasic Na0.5La0.5Bi4Ti4O15 powders were synthesized via the conventional solid-state reaction route. The X-ray powder diffraction (XRD), selected area electron diffraction (SAED) and high resolution transmission electron microscopy (HRTEM) studies carried out on the as synthesized powdered samples confirmed the phase to be a four-layer Aurivillius that crystallizes in an orthorhombic A2(1)am space group. The microstructure and the chemical composition of the sintered sample were examined by scanning electron microscope (SEM) equipped with an energy dispersive X-ray analyzer (EDX). The dielectric properties of the ceramics have been studied in the 27-700 degrees C temperature range at various frequencies (100 Hz to 1 MHz). A sharp dielectric anomaly was observed at 580 degrees C for all the frequencies corresponding to the ferroelectric to paraelectric phase transition. Saturated ferroelectric hysteresis loops were observed at 200 degrees C and the associated remnant polarization (P-r) and coercive field (E-c) were found to be 7.4 mu C/cm(2) and 34.8 kV/cm, respectively. AC conductivity analysis confirmed the existence of two different conduction mechanisms in the ferroelectric region. Activation energies calculated from the Arrhenius plots were similar to 0.24 eV and similar to 0.84 eV in the 300-450 degrees C and 450-580 degrees C temperature ranges, respectively. (C) 2010 Elsevier B.V. All rights reserved.

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Laboratory results of marked-ball wear tests are used to discuss the relative significance of corrosive and abrasive wear in wet grinding. The electrochemical mechanism was investigated by correlating the corrosive wear with the corrosion current obtained from polarization curves under abrasion. Slurry rheology governs the manner in which ground slurries coat grinding balls, thereby influencing not only the grinding efficiency but also abrasive wear. The effects of percent solids and a grinding aid are illustrated.

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A microscopic expression for the frequency and wave vector dependent dielectric constant of a dense dipolar liquid is derived starting from the linear response theory. The new expression properly takes into account the effects of the translational modes in the polarization relaxation. The longitudinal and the transverse components of the dielectric constant show vastly different behavior at the intermediate values of the wave vector k. We find that the microscopic structure of the dense liquid plays an important role at intermediate wave vectors. The continuum model description of the dielectric constant, although appropriate at very small values of wave vector, breaks down completely at the intermediate values of k. Numerical results for the longitudinal and the transverse dielectric constants are obtained by using the direct correlation function from the mean‐spherical approximation for dipolar hard spheres. We show that our results are consistent with all the limiting expressions known for the dielectric function of matter.

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Introduction Dicalcium strontium propionate (DCSP) undergoes a ferroelectric phase transition at about 28 1.5 K, with the spontaneous polarization occurring along the tetragonal C-axis.1 Takashige et al.2,3 have recently reported ferroelectricity in annealed samples of dicalcium lead propionate (DCLP) in the range 191 K to 331 K. The removal of the inner biasing field by annealing has been known in the case of DCLP3 and DCSP.4 Because of the possible dependence of the inner biasing field on the particle size, a study of the temperature dependence of the dielectric behaviour of the powdered samples of these compounds was undertaken.

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The interface between two polar semiconductors can support three types of phonon-plasmon-polariton modes propagating in three well-defined frequency windows ??1?[min(?1,?3),?R1], ??2?[max(?2,?4),?R2], and ??3?[min(?2,?4),?R3]. The limiting frequencies ?1,2,3,4 are defined by ?1(?)=0, ?2(?)=0, and ?R1,2,3 by ?1(?)+?2(?)=0, where ?i(?) are dielectric functions of the two media with i=1,2. The dispersion, decay distances, and polarization of the three modes are discussed. The variation of the limiting frequencies with the interface plasma parameter ???p22/?p12 reveals an interesting feature in the dispersion characteristics of these modes. For the interfaces for which the bulk coupled phonon-plasmon frequencies of medium 1 are greater than the LO frequency or are less than the TO frequency of medium 2, there exist two values of ?=?1 and ?2(

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Neuronaaliset nikotiinireseptorit liittyvät tupakkariippuvuuden lisäksi moniin neurologisiin sairauksiin, kuten Alzheimerin tautiin, skitsofreniaan, masennukseen ja tarkkaavaisuus- ja ylivilkkaushäiriöön. Nikotiinireseptorien stimulaation on tutkimuksissa havaittu parantavan kognitiota. Useat lääkeyritykset tutkivat nikotiinireseptoriagonisteja ja -antagonisteja eri neurologisten sairauksien hoidossa. Ongelmana nikotiinireseptori-agonisteja käytettäessä on reseptorissa tapahtuva desensitisaatio. Tällöin reseptori sulkeutuu, eikä aktivoidu vaikka agonistia olisi tarjolla tai sitoutuneena reseptoriin. Varsinkin alfa7-reseptori desensitoituu hyvin nopeasti agonistialtistuksen seurauksena. Reseptorien desensitoituminen voi kliinisessä käytössä aiheuttaa lääkeaineen tehon menetyksen. Perinteisen agonistin sitoutumiskohdan lisäksi nikotiinireseptorissa sijaitsee myös muita sitoutumiskohtia, joita kutsutaan allosteerisiksi sitoutumispaikoiksi. Tutkimuksissa on havaittu, että eräät allosteerisesti sitoutuvat aineet, kuten PNU-120596, voivat vahvistaa agonistin aikaansaamaa vastetta ja/tai estää reseptorin desensitoitumista. Näitä aineita kutsutaan positiivisiksi allosteerisiksi modulaattoreiksi ja niiden ajatellaan olevan vaihtoehto desensitoitumisen aiheuttamaan tehon menetyksen ongelmaan. Nikotiinireseptorien positiivisten allosteeristen modulaattorien tarkkaa vaikutusta ja sitoutumiskohtaa reseptoriin ei vielä tarkkaan tiedetä. Tutkimuksen aiheena oli karakterisoida positiivisten allosteeristen modulaattoreiden vaikutuksia alfa7-nikotiinireseptoriin. Tutkimuksessa tarkoituksena oli käyttää hyväksi laboratoriossa aiemmin tehtyä havaintoa, jonka mukaan alfa7-nikotiinireseptorin transmembraaniosan aminohappoon tehdyn mutaation L247T seurauksena positiiviset allosteeriset modulaattorit muuttuvat agonisteiksi. Haluttiin selvittää, kuinka agonistin sitoutumiskohtaan kohdennettua mutageneesiä käyttäen tehty mutaatio W149M tai W149F vaikuttavat PNU-120596:n kykyyn toimia agonistina alfa7L247T reseptoriin. Asetyylikoliini toimi konventionaalisen agonistin mallina tutkimuksessa. Tutkimuksen toinen tavoite oli tehdä mutaatio M253Lalfa7-reseptorin transmembraaniosaan. Mutaation on todettu estävän allosteeristen potentiaattoreiden kykyä voimistaa agonistin aikaansaamaa vastetta. Tarkoitus oli tutkia millaisia vaikutuksia M253L-mutaatiolla on allosteerisen potentiaattorin kykyyn toimia agonistina L247T-mutaation sisältävään reseptoriin. Mutatoidun reseptorin mRNA mikroinjektoitiin oosyyttiin ja elektrofysiologian avulla tutkittiin ilmennettyjen reseptorien toimintaa käyttäen kahden elektrodin jännitelukitus -menetelmää. Kaikki suunnitellut mutaatiot saatiin tehtyä onnistuneesti alfa7- ja alfa7L247T-reseptoreihin. Ortosteerisen sitoutumiskohdan mutaatio villin tyypin Į7-reseptorissa vaikutti hyvin voimakkaasti joko asetyylikoliinin sitoutumiseen reseptoriin tai reseptorin toimintaan, sillä asetyylikoliinilla ei reseptorista saatu mitattua vasteita. Myöskään PNU-120596 yksinään ei saanut aikaan vasteita alfa7W149M-reseptorissa. Kaksoismutatoidussa alfa7W149M/L247T-reseptorissa puolestaan havaittiin, että asetyylikoliinin annos-vaste -kuvaaja siirtyi huomattavasti enemmän oikealle kuin PNU-120596:n, kun verrattiin annos-vaste –kuvaajia alfa7L247T ja alfa7W149M/L247T–reseptoreiden välillä. Transmembraaniosan mutaatio M253L ei vaikuttanut PNU-120596:n kykyyn toimia agonistina alfa7L247T-reseptoriin, eikä sillä ollut vaikutusta asetyylikoliinin annosvaste-kuvaajiin. Tutkimus tukee aiempia havaintoja siitä, että positiivisten allosteeristen modulaattoreiden sitoutumiskohta nikotiinireseptorissa sijaitsisi transmembraaniosassa. M253L-mutaation osalta tulokset ovat hieman ristiriidassa aiempien tulosten kanssa. L247T-mutaatio vaikuttaa hyvin voimakkaasti nikotiinireseptorin toimintaan sekä sijaitsee aminohapon M253 läheisyydessä. On mahdollista, että se peittää M253L-mutaation vaikutuksen. Toisaalta voi olla, että M253 on aminohappo, joka vaikuttaa vain reseptorivasteiden voimistumiseen eikä allosteeristen potentiaattoreiden sitoutumiseen.

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The present paper deals with the study of the effects of electron (8 MeV) irradiation on the dielectric and ferroelectric properties of PbZrO3 thin films grown by sol-gel technique. The films were (0.62 mu m thick) subjected to electron irradiation using Microtron accelerator (delivered dose 80, 100, 120 kGy). The films were well crystallized prior to and after electron irradiation. However, local amorphization was observed after irradiation. There is an appreciable change in the dielectric constant after irradiation with different delivered doses. The dielectric loss showed significant frequency dispersion for both unirradiated and electron irradiated films. T (c) was found to shift towards higher temperature with increasing delivered dose. The effect of radiation induced increase of E >'(T) is related to an internal bias field, which is caused by radiation induced charges trapped at grain boundaries. The double butterfly loop is retained even after electron irradiation to the different delivered doses. The broader hysteresis loop seems to be related to radiation induced charges causing an enhanced space charge polarization. Radiation-induced oxygen vacancies do not change the general shape of the AFE hysteresis loop but they increase P (s) of the hysteresis at the electric field forced AFE to FE phase transition. We attribute the changes in the dielectric properties to the structural defects such as oxygen vacancies and radiation induced charges. The shift in T (C), increase in dielectric constant, broader hysteresis loop, and increase in P (r) can be related to radiation induced charges causing space charge polarization. Double butterfly and hysteresis loops were retained indicative of AFE nature of the films.

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The polarization properties of a twisted nematic liquid crystal display (TNLCD) are studied experimentally with the aim of using it as a wavelength selector. The output of a white LED is split into its constituent wavelengths with a resolution of 2-5 nm in proportion to a voltage applied to the TNLCD. The feasibility of employing the display as a wavelength selector in visible spectrometers is demonstrated. A simple inexpensive design of a spectrometer built around an LED and a TNLCD is suggested.

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We report on the fabrication and characterization of a device which allows the formation of an antidot lattice (ADL) using only electrostatic gating. The antidot potential and Fermi energy of the system can be tuned independently. Well defined commensurability features in magnetoresistance as well as magnetothermopower are observed. We show that the thermopower can be used to efficiently map out the potential landscape of the ADL. (C) 2010 American Institute of Physics. doi: 10.1063/1.3493268]

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The complex permittivity characteristics of epoxy nanocomposite systems were examined and an attempt has been made to understand the underlying physics governing some of the unique macroscopic dielectric behaviors. The experimental investigations were performed using two different nanocomposite systems with low filler concentrations over the frequency range of 10(-2)-400 Hz, but for some cases, the data has been reported upto 10(6) Hz for a better understanding of the behaviors. Results demonstrate that nanocomposites do possess unique permittivity behaviors as compared to those already known for unfilled polymer and microcomposite systems. The nanocomposite real permittivity and tan delta values are found to be lower than that of unfilled epoxy. In addition, results show that interfacial polarization and charge carrier mobilities are suppressed in epoxy nanocomposite systems. The complex permittivity spectra coupled with the ac conductivity characteristics with respect to frequency was found to be sufficient to identify several of the nanocomposite characteristics like the reduction in permittivity values, reduction in the interfacial polarization mechanisms and the electrical conduction behaviors. Analysis of the results are also performed using electric modulus formalisms and it has been seen that the nanocomposite dielectric behaviors at low frequencies can also be explained clearly using this formalism.

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Polarization switching processes in TAAP and DTAAP have been studied by the Merz method. The switching process in DTAAP is slower than in TAAP. The temperature dependence of switching time indicates that the crystal might contain groups of domain nuclei with different activation energies. X-ray irradiation causes an increase in the threshold field below which switching could not occur and decrease in the mobility of domain walls. Irradiation decreases the peak value of dielectric constant, Tc and increases the value of coercive field. Domain structure studies on TAAP crystals have shown that the crystals grow as both predominantly single domain and multi domains, depending on which the internal bias increases or remains unaffected upon irradiation.

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Excitation spectra and transient and steady-state photoconductivity have been studied in undoped and 0.8-mole% Cu-doped single-crystal β-AgI between 150 and 260°K. A single peak in the spectral response was found to occur in each case, at 2.88 eV for undoped and at 2.81 eV for copper-doped specimens at 260 K, the difference being due to a decrease in band gap. The anisotropy due to polarization of incident radiation parallel or perpendicular to the c direction, which is a measure of the energy difference between the Γ9 and Γ7 levels in the valence band, was found to be 0.010 eV. Transient-photoconductivity experiments showed that the hole lifetime was 6 μ sec at 300°K, an order of magnitude larger than the electron lifetime. The hole drift mobility was found to be 12±2 cm2/ V sec at 300°K and limited by traps at a depth of 0.51±0.01 eV with concentration (3-5)×109/cm3 and capture cross section 10-11 cm2. The study of photoconductivity decay versus temperature revealed the presence of shallow hole traps at 0.14±0.02 eV with concentration greater than 1016/cm3 and capture cross section 10-19 cm2. The steady-state photoconductivity was determined by the deep hole traps at 0.51 eV, and showed the presence of shallow electron traps at a depth of 0.28 eV. The trap distribution was found to be substantially the same in pure and copper-doped specimens, indicating the monovalent substitutional role of copper. The effects of iodine annealing, cadmium doping, and heating above the transition temperature were also studied. The possible nature of the traps is discussed.

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Sr2TiMnO6, a double perovskite associated with high degree of B-site cation disorder was investigated in detail for its structural, magnetic, and dielectric properties. Though x-ray powder diffraction analysis confirms its cubic structure, first order Raman scattering and infrared reflectivity spectra indicate a breaking of the local cubic symmetry. The magnetization study reveals an anomaly at 14 K owing to a ferrimagnetic/canted antiferromagneticlike ordering arising from local Mn-O-Mn clusters. Saturated M-H hysteresis loops obtained at 5 K also reflect the weak ferromagnetic exchange interactions present in the system and an approximate estimation of Mn3+/Mn4+ was done using the magnetization data for the samples sintered at different temperatures. The conductivity and dielectric behavior of this system has been investigated in a broad temperature range of 10 to 300 K. Intrinsic permittivity was obtained only below 100 K whereas giant permittivity due to conductivity and Maxwell-Wagner polarization was observed at higher temperatures. X-ray photoemission studies further confirmed the presence of mixed oxidation states of Mn and the valence band spectra analysis was carried out in detail. (C) 2010 American Institute of Physics. doi: 10.1063/1.3500369]