9 research outputs found
Electron g-Factor Anisotropy in Symmetric (110)-oriented GaAs Quantum Wells
We demonstrate by spin quantum beat spectroscopy that in undoped symmetric
(110)-oriented GaAs/AlGaAs single quantum wells even a symmetric spatial
envelope wavefunction gives rise to an asymmetric in-plane electron
Land\'e-g-factor. The anisotropy is neither a direct consequence of the
asymmetric in-plane Dresselhaus splitting nor of the asymmetric Zeeman
splitting of the hole bands but is a pure higher order effect that exists as
well for diamond type lattices. The measurements for various well widths are
very well described within 14 x 14 band k.p theory and illustrate that the
electron spin is an excellent meter variable to map out the internal -otherwise
hidden- symmetries in two dimensional systems. Fourth order perturbation theory
yields an analytical expression for the strength of the g-factor anisotropy,
providing a qualitative understanding of the observed effects
Phonon-Assisted Tunneling of an Electron in a Strained Self-Assembled Quantum Dot Molecule
We calculate phonon-assisted relaxation rates in a self-assembled quantum dot molecule. The calculation is based on wave functions obtained within an envelope function approach, including strain effects. The single-phonon relaxation is shown to be efficient for separations between the dots around 10 nm when, in addition, the dots are brought close to resonance
Influence of velocity profile deformation on flow averaging tube flow coefficient
W pracy przedstawiono zasad臋 dzia艂ania rurek u艣redniaj膮cych oraz stanowisko do ich wzorcowania. Zaprezentowano wyniki bada艅 eksperymentalnych pomiaru strumienia powietrza przep艂ywomierzami spi臋trzaj膮cymi w strefie zaburzonego przep艂ywu za pojedynczym kolanem. Okre艣lono profile pr臋dko艣ci w wybranych miejscach instalacji. Wyznaczono charakterystyki wsp贸艂czynnika przep艂ywu K dla rurki o kszta艂cie op艂ywowym. Podano warto艣ci wsp贸艂czynnika korekcyjnego umo偶liwiaj膮cego zmniejszenie niepewno艣ci pomiaru przep艂ywu rurk膮 u艣redniaj膮c膮. Wykazano, 偶e lokalizacja przep艂ywomierza poni偶ej 5D za kolanem powoduje istotny wzrost niepewno艣ci pomiaru.This paper presents experimental results of the air flow across an obstacle formed by a 90 degree segmented elbow. The internal diameter of the pipeline was D=152 mm, while the range of the mean velocities w = 10 30 m/s. The velocity profiles were determined (using Prandtl tube) both in the vertical and horizontal plane [12] in the relative distances L/D of the pipeline from 3 D to 20 D (Figs. 5 and 6). In the places of the established velocity profiles a streamlined flow averaging tube [7] was placed to determine the characteristics of the flow coefficient K (Figs. 8 and 9) as a function of the mean velocity (and Re number). The scope of this paper is also to present an automated test stand (equipped with a dedicated computer program - data acquisition) for calibrating flowmeters. The results of the experiments are given in the form of charts and compared. Analysis of the effect of changing the position of the averaging probe (vertical, horizontal) was conducted together with examination of the influence of the distance behind the obstacle (elbow) on the K-factor value. The realized experiment allowed shortening the distance between the obstacle and flowmeter installation place and informing about the correction factor value which can be used to minimise the uncertainty of the air flow rate measurement (Fig. 10). It was assumed that the horizontal plane is better for probe installation because of almost axi-symmetrical velocity profile and better repeatability of measurement points (K-factor changes by about 1%)
Phonon-Assisted Tunneling of an Electron in a Strained Self-Assembled Quantum Dot Molecule
We calculate phonon-assisted relaxation rates in a self-assembled quantum dot molecule. The calculation is based on wave functions obtained within an envelope function approach, including strain effects. The single-phonon relaxation is shown to be efficient for separations between the dots around 10 nm when, in addition, the dots are brought close to resonance
Experimental determination of velocity profile in a rectangular channel
Badania zrealizowane na potrzeby niniejszego artyku艂u mia艂y na celu eksperymentaln膮 ocen臋 wp艂ywu typowego elementu armatury instalacyjnej oraz warto艣ci turbulencji przep艂ywu na wyznaczanie d艂ugo艣膰 odcinka prostego pozwalaj膮cego na stabilizacj臋 strugi przep艂ywaj膮cego p艂ynu.The research reported in this article was concerned with experimental evaluation of the effect of installation of a typical element of armature and the level of flow turbulence on the length of the straight tube section needed for the development of fluid flow. In order to carry out the tests, an experimental setup was built, which main element consists of a steel channel through which ambient air is delivered inside the installation. The channel has a square cross-section and length of 160 mm. Along this channel, a system of three 30o elbows was installed and combined to form a single 90掳 segmented bend. With the purpose of assessing the flow disturbance at specified distances from the flow obstruction, it was necessary to determine the velocity profile of the fluid flow in the channel. This goal applied a measuring system comprising a Pitot tube connected to a linear module. This setup provided the measurements of the velocity along the entire section of the channel with the measurement space traversed with a step equal to 2mm
Method of liquid flow measurement using a modified PIV method
W pracy przedstawiono wyniki bada艅 pomiaru pr臋dko艣ci ruchu cieczy. Pr臋dko艣膰 okre艣lono na podstawie zdj臋膰 fotograficznych z wizualizacji ruchu cieczy, w kt贸rej znajdowa艂y si臋 znaczniki optyczne. Przedstawiona metoda umo偶liwia wyznaczenie pr臋dko艣ci ruchu cieczy z dok艂adno艣ci膮 do kilku procent warto艣ci mierzonej.Phenomena related to the flow around different types of obstacles belong to one of the most difficult issues of fluid mechanics. Fluid flowing to the obstacle is disturbing what is associated with the formation of vortices. The frequency and intensity of vortices depend on flow and type of obstacle. The phenomenon is used in vortex flow meters. The paper present the test stand of flow visualization for vortex bluff bodies of vortex flowmeter. Very important parameter, which is necessary to designate in testing space is flow velocity. The paper proposes a method of measuring the velocity of liquid motion based on the image recorded during the visualization. The flow velocity was determined by the photographic images from the fluid flow visualization in which the tags were located. Pictures were taken with a camera with a long exposure time. The proposed method enables the determination of the fluid velocity to a certain percentage of the measured value. The uncertainty of this measurement significantly depends on the value of the measured velocity. In order to maintain the desired measurement accuracy, it is necessary to adjust the exposure time accordingly
Influence of typical flow disturbing elements on the flow rate in selected averaging Pitot tubes
Flowmeters with averaging Pitot tubes are becoming more and more common in the industrial practice. It is often the case in long straight sections of channels with large diameters that the conditions regarding the adequately long sections of pipelines before and behind a flowmeter cannot be fulfilled. This is associated with the occurrence of an additional measurement uncertainty with an unknown value. Most of the information regarding this issue can be found for the case of Venturi probes. The amount of data regarding the flow averaging Pitot tubes is also limited. Hence, the decision to undertake the proposed subject. The conducted research made it possible to state recommendations regarding the metrology of testing. The results indicate that it is not only the distance from the flow disturbing element that plays a role but it is also the plane in which the sensor is located that affects the uncertainty of measurements of the flow averaging Pitot tubes
Synthesis and catalytic behavior in olefin polymerization of bimetallic titanium(IV) silsesquioxane complex and its polymeric counterpart
Zsyntetyzowano, a nast臋pnie scharakteryzowano dwa tytanosilseskwioksany: nowy, nieznany dot膮d z literatury, tetrachloroditytanosilseskwioksan (2) i jego polimeryczny odpowiednik (3). Zbadano w艂a艣ciwo艣ci katalityczne otrzymanych zwi膮zk贸w w polimeryzacji etylenu i 1-oktenu. Obydwa prekatalizatory, po aktywacji za pomoc膮 Et2AlCl lub EtAlCl2, katalizuj膮 polimeryzacj臋 etylenu do polietylenu (PE) o ma艂ej masie molowej, kt贸ra zmniejsza si臋 zar贸wno ze wzrostem temperatury reakcji, jak i stosunku molowego Al:Ti. Kompleks (2) w po艂膮czeniu z metyloaluminoksanem lub zwi膮zkami boru jest tak偶e aktywny w polimeryzacji 1-oktenu.The new compound, tetrachlorodititanasilsesquioxane (2) and its polymeric analogue (3) have been synthesized, characterized and used for the first time in ethylene and 1-octene polymerization. These precatalysts, activated by Et2AlCl and EtAlCl2, were found to be catalytically active in polymerization of ethylene. The resulting polyethylenes have rather low molecular weight, decreasing with an increase in both reaction temperature and molar ratio of Al:Ti. In the presence of methylaluminoxane or boron compounds, the complex (2) also promotes polymerization of 1-octene