25 research outputs found
The Edge Electric Field of a Pyroelectric and its Applications
Following a change of temperature of a pyroelectric (PE), a depolarizing
electric field appears both inside the PE, as well as outside its edges, the
edge depolarizing electric field (EDEF). The EDEF extends outwards up to a
distance of the order of magnitude of the PE width. The mapping and the
strength of the EDEF have been calculated and analyzed for the case of a
semi-infinite pyroelectric plate. This strong EDEF (104-105 V/cm), when
penetrating into the surrounding medium, creates a variety of physical effects:
inducing electrical current in a semiconductor and affecting its resistance,
accelerating charged and neutral particles in vacuum or in a gas, generating
electromagnetic waves, modifying optical characteristics by electrooptical and
photoelasic effects, generating piezoelectric deformation and more. We show
that these EDEF induced effects could serve as a basis for the development of
various applications and devices.Comment: 27 pages including 13 figure
Electric Field Effect Analysis of Thin PbTe films on high-epsilon SrTiO3 Substrate
Thin PbTe films (thickness 500 - 600 angstrom), deposited on SrTiO3, have
been investigated by electric field effect (EFE). The high resistivity of such
thin films warrants a high sensitivity of the EFE method. The SrTiO3 substrate
serves as the dielectric layer in the Gate-Dielectric-PbTe structure. Due to
the large dielectric constant of SrTiO3, particularly at low temperatures, the
electric displacement D in the film reaches the high value of about 10^8 V/cm,
and the EFE introduced charge into the PbTe film amounts to ~ 8 microC/cm2. The
high D permits to measure the EFE resistance and Hall constant over a wide
region of D, revealing the characteristic features of their D-dependence. An
appropriate theoretical model has been formulated, showing that, for such
films, one can measure the dependence of the Fermi level on D. In fact, we
demonstrate that shifting the Fermi level across the gap by varying D, the
density-of-states of the in-gape states can be mapped out. Our results show,
that the PbTe layers studied, possess a mobility gap exceeding the gap of bulk
PbTe.Comment: 27 pages, 12 figure
Thermal Wave Induced Edge Electrical Field of Pyroelectric: Spatial Pattern Mapping and Effect of Ambient Conditions
We have recently analyzed theoretically the main characteristics of the edge
depolarizing electric field (EDEF), in the vicinity of a non-polar face of a
pyroelectric. In this work we measured and characterized the EDEF, excited by a
harmonical thermal wave. We present here experimental results obtained on a
pyroelectric crystal LiTaO3, confirming our theoretical predictions. We present
the theoretical analysis and description of the thermal wave and the induced
harmonically varying EDEF. The calculations assume an equivalent circuit of a
pyroelectric capacitive current source. The measured magnitude of the EDEF and
its spatial variation agree well with the theoretical model. The effect of the
air pressure at the pyroelectric/air interface, on the EDEF, was determined in
the interval 10^3 - 10^-6 torr. We found that EDEF increases significantly with
decreasing air pressure, presumably due to diminishing of adsorption screening
at the polar faces. Teflon plates, covering the polar faces, prevent
accumulation of screening charged particles, resulting in a drastic increase of
EDEF
Characterization of high-temperature PbTe p-n junctions prepared by thermal diffusion and by ion-implantation
We describe here the characteristics of two types of high-quality PbTe
p-n-junctions, prepared in this work: (1) by thermal diffusion of In4Te3 gas
(TDJ), and (2) by ion implantation (implanted junction, IJ) of In (In-IJ) and
Zn (Zn-IJ). The results, as presented here, demonstrate the high quality of
these PbTe diodes. Capacitance-voltage and current-voltage characteristics have
been measured. The measurements were carried out over a temperature range from
~ 10 K to ~ 180 K. The latter was the highest temperature, where the diode
still demonstrated rectifying properties. This maximum operating temperature is
higher than any of the earlier reported results.
The saturation current density, J0, in both diode types, was ~ 10^-5 A/cm2 at
80 K, while at 180 K J0 ~ 10^-1 A/cm2 in TDJ and ~ 1 A/cm2 in both
ion-implanted junctions. At 80 K the reverse current started to increase
markedly at a bias of ~ 400 mV for TDJ, and at ~550 mV for IJ. The ideality
factor n was about 1.5-2 for both diode types at 80 K. The analysis of the C-V
plots shows that the junctions in both diode types are linearly graded. The
analysis of the C-V plots allows also determining the height of the junction
barrier, the concentrations and the concentration gradient of the impurities,
and the temperature dependence of the static dielectric constant. The
zero-bias-resistance x area products (R0Ae) at 80 K are: 850 OHMcm2 for TDJ,
250 OHMcm2 for In-IJ, and ~ 80 OHMcm2 for Zn-IJ, while at 180 K R0Ae ~ 0.38
OHMcm2 for TDJ, and ~ 0.1 OHMcm2 for IJ. The estimated detectivity is: D* ~
10^10 cmHz^(1/2)/W up to T=140 K, determined mainly by background radiation,
while at T=180 K, D* decreases to 108-107 cmHz^(1/2)/W, and is determined by
the Johnson noise
ΠΠΠΠΠ’ΠΠΠΠΠΠ ΠΠΠΠΠΠ«Π Π‘ΠΠ‘Π£ΠΠΠ‘Π’Π«Π ΠΠ ΠΠ’ΠΠΠ«: ΠΠ‘Π‘ΠΠΠΠΠΠΠΠΠ IN VIVO
Porcine intrathoracic arteries were devitalized by application of low temperatures and electron beam irradiati- on. The resulted connective tissues vascular scaffolds could be used as the prosthesis of small diameter arteries (β€6 mm). Biocompatibility, immunogenicity degree and thrombogenicity were estimated in the study. Results of electron microscopy are presented. Described treatment reduces an immunogenicity of xenoarteries, their ade- quate functioning during 6 months was shown by means of experimental surgeries.Β ΠΠ»Ρ Π΄Π΅Π²ΠΈΡΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΡ
Π³ΡΡΠ΄Π½ΡΡ
Π°ΡΡΠ΅ΡΠΈΠΉ ΡΠ²ΠΈΠ½Π΅ΠΉ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»ΠΈ Π½ΠΈΠ·ΠΊΠΈΠ΅ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΈ ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΠ΅ ΠΏΠΎΡΠΎΠΊΠΎΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ². ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠΎΠ΅Π΄ΠΈΠ½ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΠΊΠ°Π½Π½ΡΠ΅ ΡΠΎΡΡΠ΄ΠΈΡΡΡΠ΅ ΡΠΊΠ°ΡΡΠΎΠ»Π΄Ρ Π² Π΄Π°Π½Π½ΠΎΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ Π±ΡΠ»ΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Ρ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΏΡΠΎΡΠ΅Π·ΠΎΠ² Π°ΡΡΠ΅ΡΠΈΠΉ ΠΌΠ°Π»ΠΎΠ³ΠΎ Π΄ΠΈΠ°ΠΌΠ΅ΡΡΠ° (β€6 ΠΌΠΌ). Π ΡΠ°Π±ΠΎΡΠ΅ ΠΈΠ·ΡΡΠ°Π»ΠΈ Π±ΠΈΠΎΡΠΎΠ²ΠΌΠ΅- ΡΡΠΈΠΌΠΎΡΡΡ, ΡΡΠ΅ΠΏΠ΅Π½Ρ ΠΈΠΌΠΌΡΠ½ΠΎΠ³Π΅Π½Π½ΠΎΡΡΠΈ, ΡΡΠΎΠΌΠ±ΠΎΠ³Π΅Π½Π½ΠΎΡΡΡ Π΄Π΅Π²ΠΈΡΠ°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
Π°ΡΡΠ΅ΡΠΈΠΉ. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°- ΡΡ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΠΈΠΌΠΌΡΠ½ΠΎΠ³Π΅Π½Π½ΠΎΡΡΠΈ Π΄Π΅Π²ΠΈΡΠ°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΊΡΠ΅Π½ΠΎΠ°ΡΡΠ΅ΡΠΈΠΉ. ΠΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΠ΅ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΈ ΠΏΡΠΎΠ΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΠΎΠ²Π°Π»ΠΈ ΠΈΡ
Π°Π΄Π΅ΠΊΠ²Π°ΡΠ½ΠΎΠ΅ ΡΡΠ½ΠΊΡΠΈΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ 6 ΠΌΠ΅Ρ.
INFLUENCE OF THE METAL MATRIX STRUCTURE OF HIGH-DUTY CAST IRON ON COERCIVELY SENSITIVE MAGNETIC PARAMETER AND SPEED OF SOUND
The analysis of influence of changes in the structure of the metal base of high-duty cast ironcompact castings with a constant form of graphite inclusions on the coercive sensitive magnetic parameters and the speed of sound is held. The efficiency of joint use of the results of magnetic and ultrasonic measurements to control the shape of inclusions in the iron and pearlite content in its metallic matrix is shown