Dissertations / Theses on the topic 'Impurity distribution'
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Sandven, Håkon. "Evaluation of Distribution Function Models for ICRH-induced Impurity Transport in Tokamaks." Thesis, KTH, Skolan för elektro- och systemteknik (EES), 2016. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-192460.
Full textFusionsenergi är utnyttjandet av energi som frigörs i kärnfusionsreaktioner, och har potential för att bli en energikälla som är mer hållbar, säkrare och renare än de primära energikällorna idag. Det grundläggande problemet för fusionskraft är energiinneslutning. Förorenande joner är en viktig källa för förlust av energiinneslutning i fusionsanläggningar med magnetisk inneslutning. Därför är föroreningstransport i fusionsplasma ett viktigt ämnesområde. Joncyklotronresonansupphettning (ICRH) har visats både experimentellt och teoretiskt att påverka föroreningstransport i tokamaker. En poloidal asymmetri i minoritetsjonerna ger en elektrisk potential, som orsakar förorening samlas på den inre sidan av fusionsanläggningen. Poloidal asymmetri i föroreningsdensiteten på ett fluxyta inducerar en netto radialflux över fluxytan. Detta projekt har jämfört ICRH-inducerad föroreningstransport för fyra approximativa distributionsfunktionsmodeller för minoritetsjon med numeriska resultat från SELFO koden. Detta har gjorts med beräkningar för JET-liknande, kon-centrisk tokamak-geometri med deuterium-plasma, väte som minoritetsjoner, och volfram som föroreningsjoner. Två modeller, s.k. bi-Maxwellian- och LFS bi-Maxwellianmodellen, används i existerande litteratur. Ytterligare två modeller introduceras, kallad tri-Maxwellian- och LFS tri-Maxwellianmodellen. Dessa modeller tar hänsyn till förekomsten av termiska och snabba joner i minoritetsbefolkningen. Resultaten visar att det finns tydliga skillnader mellan de olika modellerna, särskilt när resonansytan är på den inre sidan. Tri-Maxwellianmodellerna visar en klar förbättring över bi-Maxwellianmodellerna jämfört med SELFO. Det finns dock vissa särdrag i resultaten från SELFO som ingen av de approximative modellerna förutsäger, eftersom modellerna försummar breda banor. En möjlig barriär i den radiella transporten har också blivit identifierat på fluxytor där asymmetrin i föroreningsdensiteten liknar asymmetrin i den magnetiska fältstyrkan. LFS bi-Maxwellianmodellen förutsäger den radiella positionen av barriären mest noggrant och tillförlitligt jämfört med SELFO.
Haider, Asad Mahmood. "Measurement and control of impurity distribution in ultra pure gas delivery systems." Diss., The University of Arizona, 1993. http://hdl.handle.net/10150/186380.
Full textDal, Martello Elena. "Impurity distribution and reduction behaviour of quartz in the production of high purity silicon." Doctoral thesis, Norges teknisk-naturvitenskapelige universitet, Institutt for materialteknologi, 2012. http://urn.kb.se/resolve?urn=urn:nbn:no:ntnu:diva-17363.
Full textGarcia, Jonathan C. "Alternate configurations for blocked impurity band detectors." Thesis, Monterey, Calif. : Springfield, Va. : Naval Postgraduate School ; Available from National Technical Information Service, 2004. http://library.nps.navy.mil/uhtbin/hyperion/04Dec%5FGarcia.pdf.
Full textThesis Advisor(s): Nancy M. Haegel, Gamani Karunasiri. Includes bibliographical references (p. 43-45). Also available online.
Erwin. "Electron eigenvalues and eigenfunctions for a nanochannel with a finite rectangular barrier." Virtual Press, 1994. http://liblink.bsu.edu/uhtbin/catkey/917032.
Full textDepartment of Physics and Astronomy
Wei, Lun-Cun. "Etude de l'incorporation de b, c et o dans gaas prepare par la methode de czochralski (lec), en utilisant l'analyse par activation avec les particules chargees." Paris 6, 1987. http://www.theses.fr/1987PA066031.
Full textKim, Kwang-Joo. "Impurity distributions in crystalline solid layer in melt crystallization /." Aachen : Shaker, 2002. http://bvbr.bib-bvb.de:8991/F?func=service&doc_library=BVB01&doc_number=009698552&line_number=0001&func_code=DB_RECORDS&service_type=MEDIA.
Full textFornara, Pascal. "Modélisation et simulation numérique de la croissance des siliciures pour la microélectronique." Université Joseph Fourier (Grenoble), 1996. http://www.theses.fr/1996GRE10082.
Full textBenkherourou, Ouahab. "Conception et mise au point d'un analyseur hemispherique en vue de spectroscopies d'electrons resolues angulairement : caracterisation d'interfaces si/sio::(2) et si/sio::(x)n::(y) obtenues par implantation ionique a faible energie." Université Louis Pasteur (Strasbourg) (1971-2008), 1987. http://www.theses.fr/1987STR13014.
Full textHussain, Tahir. "Novel impurity distributions in GaAs devices by focused ion beam implantation." Thesis, University of Cambridge, 1992. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.241086.
Full textMotahari, Sareh [Verfasser]. "Kondo physics and thermodynamics of the Anderson impurity model by distributional exact diagonalization / Sareh Motahari." Halle, 2017. http://d-nb.info/1147380651/34.
Full textBorsos, Akos. "Modelling and control of crystal purity, size and shape distributions in crystallization processes." Thesis, Loughborough University, 2017. https://dspace.lboro.ac.uk/2134/25478.
Full textKoumetz, Serge. "Modélisation de la diffusion du Be dans les structures épitaxiales en InGaAs pour les dispositifs microoptoélectroniques." Rouen, 1995. http://www.theses.fr/1995ROUE5037.
Full textWong-Leung, Jennifer. "The gettering of metals in silicon to defects induced by ion implantation." Phd thesis, 1997. http://hdl.handle.net/1885/145289.
Full textChang, Che Wei, and 張哲維. "Product yield, purity and effective impurity distribution coefficient for separation of the enantiomer mixture in stripping crystallization." Thesis, 2019. http://ndltd.ncl.edu.tw/cgi-bin/gs32/gsweb.cgi/login?o=dnclcdr&s=id=%22107CGU05063022%22.&searchmode=basic.
Full textRoro, Kittessa Tolessa. "Influence of V and Mn doping on the electrical transport properties of A Cr +1.2 at.% Ga alloy." Thesis, 2008. http://hdl.handle.net/10210/1360.
Full textImpurity resonance scattering effects are investigated in the Cr-Ga alloy system. This system has a triple point on its magnetic phase diagram where the paramagnetic (P), incommensurate (I) and commensurate (C) spin-density-wave (SDW) states co-exist. Alloying Cr with the nonmagnetic nontransitional element Ga affects the magnetic properties of Cr in a very unique way. In order to investigate the presence of resonant impurity scattering effects in binary Cr-Ga alloys, electrical resistivity measurements were carried out in the temperature range between 6 K and 85 K. The results of the investigation show: • A nonmonotonic increase in the residual resistivity of the Cr-Ga system with an increase in the Ga content, due to the presence of resonant impurity scattering of conduction electrons. • A low-temperature resistivity minimum observed in some of the Cr-Ga alloys, taken as further evidence for the presence of resonant impurity scattering effects on the conduction electrons. The impurity resonance scattering effects on the electrical resistivity of a Cr + 1.2 at.% Ga alloy, doped with V and Mn to tune the Fermi level through the impurity level, are also investigated. The investigation was complemented by thermal expansion and velocity of sound measurements in the temperature range 77 K to 450 K for the Cr + 1.2 at.% Ga alloy only. This specific Ga concentration was chosen to allow for studying resonant scattering effects in both the ISDW and CSDW phases of the system. This is possible because concentration of 1.2 at.% Ga is just above the triple point concentration. Doping with Mn to increase the electron concentration (eA) drives the alloy deeper into the CSDW phase region of the phase diagram, while doping with V, on the other hand, will drive the alloy towards the ISDW phase region. The results of the study are summarized as follows: • Two relatively sharp peaks, attributed to resonant impurity scattering effects, are observed in the curve of the residual resisitivity as a function of dopant concentration in the ISDW phase of the ternary (Cr0.988Ga0.012)1-xVx and (Cr0.988Ga0.012)1-yMny alloy systems. v • At 0 K the (Cr0.988Ga0.012)1-yMny alloy system transforms from the ISDW to the CSDW phase at y ≅ 0.0032, giving a CSDW phase for y > 0.0032. A peak is observed in the residual resistivity at about this Mn content. This peak can then either be ascribed to a jump occurring in the residual resistivity when the CSDW phase is entered from the ISDW phase or to resonant scattering effects. The conclusion is that the peak is rather related to the latter effect. • The resistivity as a function of temperature of the above two ternary alloy series show well-developed or weak minima at low temperatures for some of the samples. This is taken as further evidence of the influence of impurity resonant scattering effects on the resistivity of these alloys. • The resistivity and thermal expansion coefficient of the polycrystalline Cr0.988Ga0.012 alloy of the present study behaves anomalously close to the ISDW-CSDW phase transition temperature and warrant further investigation. The concentration-temperature magnetic phase diagram of the (Cr0.988Ga0.012)(Mn,V) alloy system was constructed from the magnetic transition temperatures obtained from electrical resistivity measurements. Theoretical analysis of the phase diagram was done using the two-band imperfect nesting model of Machida and Fujita. The results show: • A triple point at (0.21 at.% V, 225 K) where the ISDW, CSDW and P phases coexist on the magnetic phase diagram. • The curvature of all three theoretically calculated phase transition lines in the region of the triple point is of the same sign as that observed experimentally. • The theoretical fit is very good for the ISDW-P and ISDW-CSDW phase transition boundaries, while there is some discrepancy for the CSDW-P phase transition line. This may be attributed to the fact that the theory is one dimensional and that it does not include electron-hole pair breaking effects due to impurity scattering and also not effects of changes in the density of states due to alloying.
Dr. A.R.E Prinsloo Prof. H.L. Alberts
Kiger, Shanalyn. "Rutherford backscattering in ion-implanted and pulsed laser annealed Si and Ge." 1985. http://hdl.handle.net/2097/27521.
Full textSheppard, Leigh Russell Materials Science & Engineering Faculty of Science UNSW. "Defect chemistry and charge transport in niobium-doped titanium dioxide." 2007. http://handle.unsw.edu.au/1959.4/40542.
Full textDivekar, Prasad K. "Fourier deep level transient spectroscopy and its application to gold in silicon." Thesis, 2002. http://hdl.handle.net/1957/31712.
Full textGraduation date: 2003
Huang, Bo-siang, and 黃柏翔. "Investigation of thermal-fluid and impurity concentration distributions for growing multicrystalline Silicon." Thesis, 2012. http://ndltd.ncl.edu.tw/handle/73459087145632364626.
Full text國立中央大學
機械工程研究所
100
Directional solidification (DS) method is frequently used to produce the mc-Si ingots in the PV wafer industrial. The efficiency of an mc-Si solar cell depends strongly on the impurity content and level of the mc-Si wafers. In this study, numerical simulation of the transient temperature, velocity and concentration of oxygen and carbon and silicon carbide has been carried out in order to clarify the influence of gas shield on impurity transport of oxygen, carbon and silicon carbide in a directional solidification system furnace during the growth process. The installation of such a gas flow guidance device changes the gas and melt flow pattern in the furnace, which would affect the transport of carbon oxide and silicon oxide in the gas and oxygen and carbon in the melt. As the solidification fraction enlarges, the oxygen concentration in the melt decreases, because of the reduction in the amount of crucible surface immersed below the silicon melt. Results show that a decrease of the relative position of gas shield and gas-melt interface reduces the oxygen concentration in the melt but enlarges the carbon impurity. The distance between gas guidance device and free surface are presented using 2.7cm, 5.5cm, 8.3cm, 11cm, 13.8cm. The distance with 2.7cm can reduce oxygen concentration about 30% and show the minimum oxygen concentration in the ingot. Carbon concentration decreases with reducing height in the ingot, but carbon concentration increases when the height of gas shield changes from 5.5cm to 2.7cm. Thus, the optimum position to install the gas flow guidance device for obtaining the best carbon and oxygen levels in the ingot during the solidification process is 5.5cm.
Teng, Ying-yang, and 鄧應揚. "Investigation of thermal-fluid and impurity concentration distributions for growing the solar multicrystalline Siingots." Thesis, 2011. http://ndltd.ncl.edu.tw/handle/68989205196334204111.
Full text國立中央大學
機械工程研究所
99
The silicon (Si) solar cell is still the highest market share nowadays. To accomplish the goal of grid parity, for the solar cell, the wafer quality has to improve, and the production cost has to reduce. The high concentration of carbon and oxygen impurity cause the dislocation and thermal donor in the mc-Si wafer, respectively. The carbon and oxygen are the main impurity for affecting the efficiency of solar cell. The simulations of thermal flow field, carbon concentration, oxygen concentration and silicon oxide concentration in directional solidification system (DSS) are carried out by the finite volume method (FVM) in this study. The distributions of carbon and oxygen concentration in the grown ingot were measured by the SAS Company and the measurement results are compared with that of the simulation predictions. The simulation results are in good agreement with the experimental ones. The simulation shows that the melt convection is induced by buoyancy force. The flow pattern in the melt changes during the growth process. In order to improve the uniformity of carbon distribution in the melt, a heat insulation of crucible is used to increase the temperature gradient and vortex intensity of melt. Using wafers of the whole ingot obtained from the modified case, the average conversion efficiency of solar cells can be improved up to 1.8% of the one of standard case. As the solidification fraction enlarges, the oxygen concentration in the melt diminishes, because of the reduction in the amount of crucible surface immersed below the silicon melt. When the solidification fraction is small, the oxygen concentration is higher with a higher furnace pressure than with a lower one due to there being less SiO evaporation at the free surface. When the solidification fraction increases, because of the cooling effect of the argon gas, the oxygen concentration is smaller when the furnace pressure is higher rather than lower. Hence, to adjust variably the furnace pressure during the mc-Si ingot growth is good method for reducing the oxygen concentration. To increase the argon flow rate can bring more evaporated SiO gas above the free surface outwards the furnace; hence the oxygen concentration in the melt is decrease. In the present study, the gas guiding plate is used to increase the argon velocity above the free surface. The effect of reducing oxygen concentration for the gas guiding plat is similar to the one of increasing the 25% amount of original argon flow rate. The gas guiding plate can decrease the oxygen concentration without increase the argon flow rate, the furnace enhancement can be used on advancing the wafer’s quality.
Witting, Ian Thomas. "Defect and impurity distributions in traditionally cast multicrystalline and cast monocrystalline silicon for solar substrates." 2008. http://www.lib.ncsu.edu/theses/available/etd-08192008-122257/unrestricted/etd.pdf.
Full textPan, Chun-Kuei, and 潘俊桂. "Evaluation of 2-Dimension Impurity Function Band Prioritization Using Mutual Information for Hyperspectral Images under Different Distributions." Thesis, 2018. http://ndltd.ncl.edu.tw/handle/4t3dg6.
Full text國立臺北科技大學
電機工程系
106
In recent years, the technology of remote sensing has improved significantly. To solve the problem of over-sized data and bands, band selection method has been widely utilized to reduce the dimensions of images. In this way, Hughes phenomenon can be avoided and the computation time can also be reduced. Two-dimension Impurity Function Band Prioritization (2D-IFBP) method has been proposed by other researcher. It utilizes Mutual Information (MI) and bivariate normal distribution to calculate the overlapping rate between two classes from the two-dimensional domain. In addition, 2D-IFBP is used to modify the band order of IFBP to obtain the better result. In this thesis, some other bivariate distributions will also be applied such as uniform distribution, exponential distribution, and T distribution to evaluate its characteristic of Mutual Information. In this experiment, the data sets of Salinas, Washington DC mall and Pavia University are used to verify the influence of different distributions on 2D-IFBP. The experimental results show that the first and the second data sets are more like normal distribution but the data set of Pavia University is more like T distribution. Moreover, T distribution has the same dimension reduction rate as normal distribution but it possesses the better accuracy rate than the other one. Hence, trying to utilize different distributions for the specific data sets is more appropriate than conventional method.