Andres Udal
Tallinn University of Technology
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Featured researches published by Andres Udal.
Journal of Applied Physics | 2007
Reeno Reeder; Z. Ikonić; P. Harrison; Andres Udal; Enn Velmre
In this work we consider lateral current pumped GaAs/AlGaAs quantum wells as sources of incoherent terahertz radiation. The lateral field heats the electrons in a two-dimensional quantum layer and increases the population of higher subbands, hence also increasing the radiation power generated in spontaneous intersubband emission processes. Digitally graded quasi-parabolic and simple square quantum wells are considered, and the advantages of both types are discussed. Calculations at lattice temperatures of 77 K and 300 K, for electric fields up to 10 kV/cm, show that the optical output power of ∼100−200 W/m2 may be achieved for the 7 THz source. The main peak of the spectrum, at 7 THz, of the quasi-parabolic quantum well exceeds the black body radiation at 300 K by approximately a factor of two and by two orders of magnitude at 77 K.
global engineering education conference | 2014
Kadri Umbleja; Vello Kukk; Martin Jaanus; Andres Udal
This paper introduces current work with automatic evaluation that has been done to enable algorithms generating proper feedback according to the mistakes students have made. Learning environment using novel competence based approach has been used to implement those concepts and over the years data from different development steps has been collected that can be used to verify the benefits to students results of offered algorithm that mimics step-by-step student answering process.
Materials Science Forum | 2004
Enn Velmre; Andres Udal; Vytautas Grivickas
Results confirming the high values of Seebeck coefficient phonon-drag component Sph in SiC are discussed and the relevant consequences to the thermoelectric figure-of-merit ZT=T S 2 / are studied. The fact that Sph increases at low temperatures as T 2.4 similarly for low-doped p-6H- SiC, Si and Ge is demonstrated. Materials comparison criterion Sph / meff, based on heat conductivity, lattice mobility and carrier effective mass is offered and Sph strength proportions 0.1 : 1 : 5 : 10 for Ge, Si, SiC and C (diamond) are proposed. Related to that high T500K phonon- drag domination limit is obtained for SiC. It is shown that the proportionality Sph , yielding ZT , could reverse some concepts accepted in thermoelectric material development. The best-case calculations predict good (>0.1) and excellent (>1) ZT values with steep temperature-dependence T 3…4 for low temperatures 50200K if sufficiently high electrical conductivity could be ensured. The last condition may be feasible for n-SiC with relatively shallow donor levels but difficult to achieve in the case of p-SiC with relatively deep acceptor levels.
Materials Science Forum | 2003
Enn Velmre; Andres Udal
The lattice heat conductivity in low-doped SiC is studied in the wide temperature range 50÷1200 K in order to estimate the strength coefficient a4P for 4-phonon scattering processes mechanism for later application in both heat conductivity and Seebeck coe fficient models. Heat conductivity calculations confirm the domination of the 4-phonon mechanism and t he secondary role of the 3-phonon Umklapp mechanism. The obtained a4P ≈1.5⋅10 −22 s/K gives very satisfactory result in Seebeck coefficient phonon drag component modeling. Introduction. To achieve accuracy in electrothermal device simulation the rel iabl models for the lattice heat conductivity κL and thermopower (Seebeck coefficient) S are needed. To model these material parameters the phonon transport and relevant scattering proc esses should be analyzed. The phonon flux is determining κL and the partial momentum transfer from phonons to electron and hole subsystems (phonon drag effect) increases remarkably the electron and hole Seebeck coefficient Sn,p values, especially at low temperatures. In SiC, according to the hi g heat conductivity and relatively low carrier mobilities, the phonon drag effect is approximately 5 ÷10 times stronger than in silicon [1]. Respectively in SiC the phonon drag component of the Seebeck coeffici ent typically (except low doped material of 10 15 cm range) dominates over classic diffusion component for all temperature range of practical application [1]. More detailed investigation predicts that parameters κL and S are strongly influenced by the 4phonon scattering processes (4-phonon mechanism). Below we will evaluate the s rength coefficient a4P for 4-phonon mechanism from experimental κL(T) in low-doped 6H-SiC in order to use this a4P later in improved theoretical model of Seebeck coefficient phonon drag component (see [1]) . Theoretical background and model description. The phonon drag effect was predicted theoretically for metals by Gurevich in 1946 [2,3] and then observed experi mentally in semiconductors by Frederikse, Geballe and Hull [4-7]. Frederikse [4] s howed also that the strength of this drag is proportional to the ratio of phonon and carrier mean free paths lph/lcarr which rises rapidly at lower temperatures [8]. Herring in his seminal papers [9,10] analyzed the role of lowenergy (i.e. long-wave, LW) phonons for κL and S and proposed a theory for lph calculation considering the 3-phonon LW mechanism. However, soon it was discovered [6,7] tha t Herring’s model provides obviously too long lph and, therefore, significantly overestimates the phonon drag contribution to the thermopower Sph. Our recent investigations reveal the same situation in the case of SiC [1,8,11], Si and Ge. Herring’s model predicts also too strong te mperature dependence Sph ∼T −3.5 [8,11] what disagrees with the observed experimental results Sph ∼T −1.8 ...−2.5 [1,7,8,12]. This indicates that some important phonon scattering processes reducing lph value have been omitted in Sph modeling. In order to overcome this problem, we decided to consider in the Sph model beside the Herring’s type 3-phonon processes also the 4-phonon processes introduced into the κL analysis by Pomeranchuk [13]. Detailed characterization of 3-phonon and 4-phonon processes is giv n, e.g. in Materials Science Forum Online: 2003-09-15 ISSN: 1662-9752, Vols. 433-436, pp 391-394 doi:10.4028/www.scientific.net/MSF.433-436.391
Materials Science Forum | 2007
Andres Udal; Enn Velmre
Recently published experimental results for 4H–SiC diodes up to 700 °C are used to deduce the hole lifetime temperature-dependence in n-base for high temperature range. The reverse recovery measurements are interpreted by the nonisothermal drift-diffusion simulator DYNAMIT. The uncertainties from lifetimes unknown behavior in emitter layers and consequences from possible nonuniform lifetime distribution in n-base are analyzed. Results show that up to temperature 400 °C nearly quadratic dependence of lifetime versus temperature τ ~ T 2 holds. At higher temperatures lifetime growth is accelerated approximately to quartic dependence τ ~ T 4.
Materials Science Forum | 2003
Bikbajevas; Grivickas; M. Stölzer; Enn Velmre; Andres Udal; Paulius Grivickas; Mikael Syväjärvi; Rositsa Yakimova
The temperature dependence of Seebeck coefficient (S) for p-6H-SiC has been obtained. It increases from 2 up to 5.2 mV/K when temperature decreases from 400 down to 240 K. It is shown that phonon d ...
international conference on signals and electronic systems | 2014
Martin Jaanus; Andres Udal; Vello Kukk; Kadri Umbleja
While the robotics is becoming the more important branch of technology and industry, the teaching of industrial robotics has remained rather limited and expensive due to high cost of the industrial equipment and workrooms. Those drawbacks may be overcome by using the reduced size educational robot arm and the remote control of it via the interactive e-learning environment. The present paper describes the technical solutions that were designed and realized in order to give the possibility to students to learn the basics of industrial robot programming via the interactive environment.
Archive | 2017
Andres Udal; Martin Jaanus; Gintaras Valušis; Irmantas Kašalynas; Z. Ikonić; D. Indjin
In recent years remarkable progress has been made in filling the “terahertz gap” of compact sources from the “optical” side using quantum cascade lasers and difference frequency generation systems. On the “electronic” side the range up to 0.5 THz is covered by several devices like Gunn diodes, IMPATT diodes and HEMT transistors. However for the most difficult central range 0.5–2 THz, which includes frequencies for detection of explosives and several airborne threats, along with the popular semi-compact Schottky diodes based frequency multiplier systems, the resonant tunneling diodes (RTD) as micrometer-size range ultrafast electronic devices able to operate at room temperature may offer a real solution for the design of compact portable equipment. It has been predicted that frequency limit for operation of the RTDs may extend up to 3 THz if the problem of the low, microwatt-range output power could be solved. Over the last 10 years remarkable progress has been achieved in increasing the output power of RTDs by almost 2 orders of magnitude, and in extending the operation frequencies from earlier 0.7 THz range to the values near 2 THz, thus making RTDs competitive with the Schottky diode based multipliers. The chapter compares the RTDs with other compact THz sources and discusses the design approaches that have yielded remarkable increase of power and frequency of RTDs.
global engineering education conference | 2014
Martin Jaanus; Kadri Umbleja; Vello Kukk; Andres Udal
This paper describes the implementation and the application experience of learning with the Home Laboratory Kits. HomeLabKit is a small suitcase containing everything needed to perform laboratory exercises in the courses of the electrical engineering. The HomeLabKit has been tested in the real learning process for several years.
2014 14th Biennial Baltic Electronic Conference (BEC) | 2014
Reeno Reeder; Andres Udal; Enn Velmre; A. Valavanis; Jonny Cooper; Andrew Grier; P. Harrison
One of the most efficient device producing coherent high power radiation in terahertz range in electromagnetic spectrum is Quantum Cascade Laser (QCL). During over a decade of history, together with intensive development of terahertz quantum cascade lasers, respecting simulation software tools has been developed too. The process of development of simulation software is a sophisticated task, because many fields of science meet there - quantum electronics, computing technologies, software development etc. The progress in computing power have made simulation tools much more handy, as calculations of non-complex quantum well heterostructures can be run on a personal computer during a considerable time. Simulation of Quantum Cascade Lasers with complex structures can still be very time-consuming. In this paper few strategies on how to improve and optimize QWWAD software tools are analysed, implemented and corresponding results presented. Improvement of eigenvalue problem solution gave 20 times faster algorithm in solving Schrödinger equation. Other ideas did not give remarkable success.