Dissertations / Theses on the topic 'DDA simulation'
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Alves, Alves Estefania. "Émission de photons dans un microscope à effet tunnel : application à l'étude des propriétés optiques et électroniques de systèmes hybrides métal-semi-conducteur." Electronic Thesis or Diss., Toulouse 3, 2023. http://www.theses.fr/2023TOU30351.
Transition metal dichalcogenides (TMDs) are a family of semiconductors that exhibit a direct bandgap when their thickness is reduced to a monolayer, giving them remarkable optical and electronic properties, including high-efficiency luminescence. Photon emission from these monolayers is investigated using the STM-LE (Light Emission induced by Scanning Tunneling Microscopy) technique. This innovative method involves the localized injection of charge carriers into TMD monolayers through the tunneling current. This process results in the formation of excitons, electron-hole pairs bound by Coulomb forces, within the TMD monolayer. These excitons decay radiatively emitting photons whose energy corresponds to the direct bandgap of the semiconductor. This light emission process is experimentally studied using an STM microscope combined with a light detection system, enabling spectral and spatial analysis of the photon emission with nanometer-scale resolution. The electromagnetic interaction between TMD layers and their metallic substrates leads to the formation of hybrid metal-semiconductor structures, the optical and electronic properties of which are under investigation. The nature of the substrate (plasmonic or non-plasmonic) and its morphology (uniform or nanostructured) play a crucial role in both the intensity and spectral distribution of the emitted photons. Indeed, for plasmonic substrates, the photon emission process involves the electromagnetic coupling between plasmon modes excited by electron tunneling and excitons confined within the TMD monolayer. This interaction leads to an enhancement of the photon emission. Moreover, by tuning the morphology of the substrate, it becomes possible to modify this coupling and thus, the photon emission rate. Considering the significant role of the electromagnetic interaction between plasmon modes and excitons in the luminescence from TMD monolayers within a hybrid TMD/metal-plasmonic STM junction, electromagnetic numerical simulations are carried out using the DDA (Discrete Dipole Approximation) method. These simulations account for electron tunneling using the Quantum Corrected Model. By simulating the optical response of the junction to an incident excitation wave, the electromagnetic modes within the junction and their dependence on the tunneling parameters, such as tip-surface distance and bias voltage, are investigated. In particular, gap plasmon modes and the Fano-type plasmon-exciton coupling at the interface between the monolayer and the plasmon substrate are pointed out. Furthermore, the role of substrate morphology on the properties of these modes is also addressed. Based on theoretical models describing the light emission taking place in purely metallic STM junctions proposed in the literature, a model is developed to compute theoretical light emission spectra for a hybrid TMD/plasmonic-metal STM junction. This model takes into account the optical and electronic properties of the TMD monolayer, and the electron tunneling as the excitation source at the origin of the light emission phenomenon. In addition, using the results obtained from the numerical simulations, the electromagnetic coupling between the excitons confined in the TMD monolayer and the plasmons excited in the nanocavity formed by the tip-surface configuration of the STM is also considered. Finally, the effect of the substrate morphology on the light emission is studied theoretically. These results are compared with the experimental findings in order to validate the model presented
Frenzel, Erik. "Co-Simulation von LIGGGHTS® und SimulationX® zur Simulation des Zerkleinerungsprozesses in Brechern." Universitätsbibliothek Chemnitz, 2016. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-qucosa-206919.
Papapanagiotou, Nikolaos, Eugen Constantin, Sanjeev Singh, and Nikolaos Papapanagiotou. "Analysis of DDD and VDT simulation techniques to determine feasibility of using VDT simulation to validate DDD models." Monterey, California. Naval Postgraduate School, 2004. http://hdl.handle.net/10945/9925.
MBA Professional Report
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The purpose of this MBA project was to determine whether and how VDT can emulate the results obtained from A2C2 Experiments. To do that, we have first focused on learning the basics of VDT and DDD simulation techniques and then on how the models used in DDD can be analyzed using VDT. To this end, we obtained experimental data from DDD Experiment 8 and created representative models in VDT to determine the similarities and differences. We also kept detailed records of our research to assist individuals in the future who may want to expand on our work. The project involved studying of DDD and VDT techniques, establishing building blocks in VDT, creating a best effort model for DDD Experiment 8 and studying the various outcomes. In this project we could not successfully replicate the complex DDD Experiment 8 scenarios within VDT. However, important conclusions were drawn that would go a long way towards helping future studies in this regard.
Deniz, Ertan. "Dds Based Mil-std-1553b Data Bus Interface Simulation." Master's thesis, METU, 2012. http://etd.lib.metu.edu.tr/upload/12614852/index.pdf.
Burkhard, Adam. "Komplexe Systeme mit dynamischem, nichtlinearem Verhalten durch Simulation verstehen und optimieren." Universitätsbibliothek Chemnitz, 2017. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-qucosa-225834.
Didoszak, Jarema M. "Parametric studies of DDG-81 ship shock trial simulations." Thesis, Monterey, Calif. : Springfield, Va. : Naval Postgraduate School ; Available from National Technical Information Service, 2004. http://library.nps.navy.mil/uhtbin/hyperion/04Mar%5FDidoszak.pdf.
Spruegel, Tobias C., and Sandro Wartzack. "Das FEA-Assistenzsystem – Analyseteil FEdelM." Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2016. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-215130.
Kleyer, Niklas Carl Simom. "TRAFFIC SIMULATIONS THROUGH ODE-, DDE SYSTEM MODELING AND NUMERICAL COMPUTATIONS." Thesis, KTH, Matematik (Inst.), 2014. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-148377.
The ODE- and DDE models are based on the same model with the only exception that the DDE model features reaction times. They are defined by consideration forces and sub-consideration forces. The values (h; k) determines the number of cars that each driver considers and therefore adds to the system as additional terms that are of the same form as the consideration forces, hence the sub prefix. The basic case where there are no sub-considerations involved is called the base case of the system and equals to (h; k) = (1; 1). The (h; k) of the system is determining the matrix B in equation (11) by the number of sub diagonals h and super diagonals k that are filled by weights of the forces. The time integrations can result in three base cases, unstable, stable oscillating and exponentially stable. These cases refer to the behavior of all system velocities. The unstable case can for limited time frames predict collisions between cars but otherwise diverge and cannot generally be used. Oscillating stable systems reach a constant velocity after a settling time and fits well into a realistic scenario. The exponential case reaches a constant velocity the fastest and is therefore the sought after solution. Both models are similar in this regard apart from the fact that the DDE model generally have a lot more system energy. Figures 1 and 4 are empirical proof that the models works as defined and can predict some traffic behavior. An interesting observation during testing was that the ODE exponential case would always remain exponential no matter the multiplication (; ; ) = C(; ; ), the only difference would be the system energy since larger acting forces are coupled with larger energies. The DDE model however is dependent on the system energy for stability since the delay sets a system energy limit for stability since too large forces coupled with delay will not achieve the optimum distance d. The system stability analysis can be reduced in both models to analyzing the homogeneous and particular parts separate. The expansions confirms in both cases what the time integrations shows and can give an idea of how the stability changes with one parameter changing. However, this is where the DDE model behaves completely different from the ODE model. For the ODE case it is possible to plot a complete eigenvalue chart whereas the DDE case has an infinite number of eigenvalues and is therefore impossible to completely chart. A conclusion that is in common between the models is that Fd(t) inherently is dominant and should as such be at lower priority compared to the other consideration forces in order to help system stability. Comparisons to the spring equation revealed that systems that prioritize Fd(t) too high converges to a system of particles in a chain connected by springs with no friction giving the observed behavior. Prioritizing F fr(t) help stability in both cases with the exception that DDE case will be stable for a sub interval (since the top limit comes from the system total energy) within the expansion whereas the ODE case remains stable through the whole intervall. The problems that come with larger systems are stability- and computation complexity related. All through the project has the models focused on the base case with no sub-considerations. The thesis is that adding sub-considerations will again stabilize an unstable system with the addition that each consecutive weight should deflate its value exponentially. The results proves that an unstable system can be stabilized by simply increasing the (h; k) of the system. This can have applications when the optimal weights are not enough to stabilize a large system. When computing the eigenvalues for large systems it puts strain on the algorithm ’eig’. According to [1] is the computation time complexity proportional to n3. What the resulting fit shows is that the relation is more quadratic than cubic and the reason is described to be the appearance of the system matrix for the base case. The matrix structure is similar to the one of the upper Hessenbergs which as a result saves time when transforming the input matrix which is the reason why the complexity is weakly cubic.
PACI, EMANUELE. "Etude dea proteines a haute pression hydrostatique par simulation de dynamique moleculaire." Paris 6, 1996. http://www.theses.fr/1996PA066750.
Hering, Klaus. "Parallel Cycle Simulation." Universität Leipzig, 1996. https://ul.qucosa.de/id/qucosa%3A34504.
Hart, David T. "Ship shock trial simulation of USS Winston S. Churchill (DDG-81) : surrounding fluid effect /." Thesis, Monterey, Calif. : Springfield, Va. : Naval Postgraduate School ; Available from National Technical Information Service, 2003. http://library.nps.navy.mil/uhtbin/hyperion-image/03Mar%5FHart.pdf.
Köchel, Peter. "Simulation Optimisation: Approaches, Examples, and Experiences." Universitätsbibliothek Chemnitz, 2009. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-200900682.
Graupner, Achim, and Udo Sobe. "Offset-Simulation of Comparators." Universitätsbibliothek Chemnitz, 2007. http://nbn-resolving.de/urn:nbn:de:swb:ch1-200700897.
Heinrich, Stefan. "Modulbasierte Untersuchungen ebener Koppelgetriebe in SimulationX." Universitätsbibliothek Chemnitz, 2016. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-qucosa-206901.
Prud'homme, Simon. "Simulation dynamique transitoire non linéaire du flottement d'un modèle sectionnel non profilé à 3 DDL." Thèse, Université de Sherbrooke, 2015. http://hdl.handle.net/11143/6752.
Brueckner, Robert. "Modellierung und Simulation lokaler Rechnernetze." [S.l. : s.n.], 1996. http://www.bsz-bw.de/cgi-bin/xvms.cgi?SWB10324482.
Runge, Torsten, and Kondragunda Narendra. "Teamcenter Simulation Process Management." Technische Universität Chemnitz, 2018. https://monarch.qucosa.de/id/qucosa%3A21532.
Petrusa, Douglas C. "Evaluation and analysis of DDG-81 simulated athwartship shock response." Thesis, Monterey, Calif. : Springfield, Va. : Naval Postgraduate School ; Available from National Technical Information Service, 2004. http://library.nps.navy.mil/uhtbin/hyperion/04Jun%5FPetrusa.pdf.
Schenk, Tilman A. "Multiagentensysteme zur Simulation von Konsumentenentscheidungen." Doctoral thesis, Würzburg : Institut für Geographie der Universität Würzburg, 2008. http://opac.nebis.ch/cgi-bin/showAbstract.pl?sys=000253603.
Simmler, Urs. "Simulation-News in Creo 1.0." Universitätsbibliothek Chemnitz, 2011. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-qucosa-68394.
Paepcke, Anne. "NANDRAD 1.4 building simulation model." Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2017. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-230427.
Zimmer, Janek. "Simulation konvektiver Niederschlagsereignisse mit dem LMK." Wissenschaftliche Mitteilungen des Leipziger Instituts für Meteorologie ; 41 = Meteorologische Arbeiten aus Leipzig … und Jahresbericht … des Instituts für Meteorologie der Universität Leipzig ; 12 (2007), S. 139-152, 2007. https://ul.qucosa.de/id/qucosa%3A15579.
Due to the huge variety of possible cell distributions, the simulation of small-scale heavy convective precipitation events using mesoscale numerical weather prediction models is limited to a certain issue of investigation. Numerous authors addressed the examination of supercellular structures by idealized ow simulations to describe their behaviour under various atmospheric conditions (Atkins et al., 1999, Bluestein & Weisman, 2000, among others). The presented paper studies the sensitivity of simulated precipitation intensity in response to the available amount of instability, environmental wind speed and -shear as well as orographic in uences. For this purpose, the LMK model with 2:8km grid spacing has been applied without a parameterized treatment of convective processes. The model results of the simulations involving idealized initial conditions are reviewed related to a case study of a severe storm event in Saxony on June, 16th 2006.
Fischer, Mark. "Creo Simulation Live: A Design Revolution." Technische Universität Chemnitz, 2019. https://monarch.qucosa.de/id/qucosa%3A34309.
Krückeberg, Nico. "Von der Idee über die Entwicklung bis zum virtuellen Test : Mit ESI ́s SimulationX in die elektromobile Zukunft." Technische Universität Chemnitz, 2018. https://monarch.qucosa.de/id/qucosa%3A21508.
Steinbach, Gabi, Dennis Nissen, Manfred Albrecht, Ekaterina V. Novak, Pedro A. Sánchez, Sofia S. Kantorovich, Sibylle Gemming, and Artur Erbe. "Bistable self-assembly in homogeneous colloidal systems for flexible modular architectures." Universitätsbibliothek Chemnitz, 2016. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-qucosa-202517.
Dieser Beitrag ist aufgrund einer (DFG-geförderten) Allianz- bzw. Nationallizenz frei zugänglich
Evteev, Alexander V., Elena V. Levchenko, Irina V. Belova, and Graeme E. Murch. "Carbon diffusion in austenite: computer simulation and theoretical analysis: Carbon diffusion in austenite: computer simulation andtheoretical analysis." Diffusion fundamentals 6 (2007) 16, S. 1-2, 2007. https://ul.qucosa.de/id/qucosa%3A14190.
Stephan, Benjamin. "Simulation des Öffnungsverhaltens peelbarer Schalen." Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2018. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-236127.
Wähner, Ralf. "TCP-feste Handgelenke : Entwicklung und Simulation." Universitätsbibliothek Chemnitz, 2010. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-201000745.
Weiß, Jörg. "Modellbildung und Simulation radial gekoppelter Rotoren." Doctoral thesis, Bericht ; 1/2008, 2005. https://monarch.qucosa.de/id/qucosa%3A18883.
Paper- and printing machines contain radially coupled rolls. Vibrational phenomena has been experienced at higher rotational speeds. The mechanisms leading to these vibrations are to be found in a nonlinear contact behavior between the roller pairs. A systematic approach to modelling of rolls has been developed from a dynamics point of view. Selecting an appropriate contacting roll model, the roller pair model has been completed. The so obtained minimum model is best situated to work out the influence of selected parameters on the dynamical behavior. With the focus set on the coupling of the rolls a simplified contact model is developed. Experimental data are obtained from a testing rig in support of the theoretical analyses. Parameter values have been calculated from experimental results. As a conclusion, the simulation models show the vibrational phenomena observed at the test rig.
Hoffmann, Sebastian. "ANSYS Simulation und Additive Fertigung." Technische Universität Chemnitz, 2018. https://monarch.qucosa.de/id/qucosa%3A21503.
Zimmer, Janek. "Simulation konvektiver Niederschlagsereignisse mit dem LMK." Universitätsbibliothek Leipzig, 2017. http://nbn-resolving.de/urn:nbn:de:bsz:15-qucosa-223358.
Due to the huge variety of possible cell distributions, the simulation of small-scale heavy convective precipitation events using mesoscale numerical weather prediction models is limited to a certain issue of investigation. Numerous authors addressed the examination of supercellular structures by idealized ow simulations to describe their behaviour under various atmospheric conditions (Atkins et al., 1999, Bluestein & Weisman, 2000, among others). The presented paper studies the sensitivity of simulated precipitation intensity in response to the available amount of instability, environmental wind speed and -shear as well as orographic in uences. For this purpose, the LMK model with 2:8km grid spacing has been applied without a parameterized treatment of convective processes. The model results of the simulations involving idealized initial conditions are reviewed related to a case study of a severe storm event in Saxony on June, 16th 2006
Ziegenhein, Thomas, Dirk Lucas, Roland Rzehak, and Eckhard Krepper. "Closure relations for CFD simulation of bubble columns." Helmholtz-Zentrum Dresden-Rossendorf, 2014. http://nbn-resolving.de/urn:nbn:de:bsz:d120-qucosa-144231.
Heinrich, Stefan. "Parameterstudien und Co-Simulation ebener Koppelgetriebe." Universitätsbibliothek Chemnitz, 2017. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-qucosa-225974.
Schüler, Heiko. "Simulation von Lötprozessen beim Metall-Keramik-Löten." Doctoral thesis, Universitätsbibliothek Chemnitz, 2001. http://nbn-resolving.de/urn:nbn:de:swb:ch1-200100991.
Jahangiri, P., S. Ferguson, R. Doering, K. Buckley, F. Benard, P. Schaffer, M. Martinez, and C. Hoehr. "Numerical simulation of a liquid cyclotron target." Helmholtz-Zentrum Dresden - Rossendorf, 2015. http://nbn-resolving.de/urn:nbn:de:bsz:d120-qucosa-166019.
Guenther, Marco. "Werkzeuge für die Modellierung und Simulation in drahtlosen Netzwerken." Universitätsbibliothek Chemnitz, 2003. http://nbn-resolving.de/urn:nbn:de:swb:ch1-200300765.
DiDomizio, Richard, Afina Lupulescu, and Martin E. Glicksman. "Simulation of Fick’s verification of the 2nd law." Diffusion fundamentals 4 (2006) 2, S. 1-14, 2006. https://ul.qucosa.de/id/qucosa%3A14275.
Valikova, Irina V., and Andrei V. Nazarov. "Simulation of diffusion under pressure in bcc metals." Diffusion fundamentals 3 (2005) 11, S. 1-15, 2005. https://ul.qucosa.de/id/qucosa%3A14298.
Belova, Irina V., and Graeme E. Murch. "Computer simulation of the formation of hollow nanocrystals." Diffusion fundamentals 2 (2005) 9, S. 1-2, 2005. https://ul.qucosa.de/id/qucosa%3A14339.
Cai, Qiong, Alex Buts, Nigel Seaton, and Mark Biggs. "Molecular simulation of gas transport in nanoporous carbons." Diffusion fundamentals 2 (2005) 11, S. 1-2, 2005. https://ul.qucosa.de/id/qucosa%3A14341.
Valikova, Irina, and Andrei Nazarov. "Simulation of diffusion under pressure in BCC metals." Diffusion fundamentals 2 (2005) 39, S. 1-2, 2005. https://ul.qucosa.de/id/qucosa%3A14369.
Metz, Werner. "Linear barotropic simulation of atmospheric low-frequency variability." Universität Leipzig, 1995. https://ul.qucosa.de/id/qucosa%3A15014.
Ein stationäres barotropes Modell, das bezüglich eines (aus einem GCM Experiment abgeleiteten) 500 hPa Grundzustandes linearisiert ist, wird für einen Satz von 'beobachteten' Antriebsfeldern gelöst. Dabei zeigt sich, daß die führende Mode der langperiodischen atmosphärischen Variabilität (EOF) im GCM Experiment durch das lineare Modell sehr gut simuliert wird. Weiterhin stellt sich heraus, daß hierfür die Antriebsfelder und die singulären Moden des linearen Modelloperators die gleiche Bedeutung besitzen. Auf die Wichtigkeit der Anwendung des Modells bezüglich des äquivalentbarotropen Niveaus wird hingewiesen.
Tran, Ngoc Tu. "Creating material properties for thermoset injection molding simulation process." Universitätsverlag Chemnitz, 2019. https://monarch.qucosa.de/id/qucosa%3A38380.
To simulate the injection molding process, it is necessary to set material data. The material data for an injection molding process must include a viscosity model and its fitted coefficients, heat capacity coefficients, thermal conductivity coefficients, a PVT model and its coefficients, a curing model and its coefficients (only for reactive injection molding). With thermoplastics injection molding simulation, the material data is generally available from simulation tools. Users could easily choose thermoplastics material data that was already embedded in the material data bank of simulation tools to simulate the entire phases of thermoplastics injection molding process. However, with thermosets injection molding simulation, the material data is found in limited sources and seldom available from data bank of simulation tools because of complication not only in rheological and thermal properties measurement but also in modeling rheological and cure kinetics mathematical models. Therefore, with thermoset injection molding compounds that its material data bank has not been found in data bank of simulation tools, before setting material data, it is necessary to create its own material data that simulation packages do not supply a tool. Therefore, to solve this problem, it requires an extensive knowledge base in measurements of material properties as well as optimization algorithm. In addition, to simulate exactly the thermosets injection molding compound process, it requires a profound knowledge in the mold filling characteristics of thermoset injection molding compounds. However, investigation of flow behavior of thermosets injection molding compounds inside the mold has not been adequately described. Up to now, there has not been any article that shows a complete way to create thermoset material data from measured experimental data (thermal data and rheological data) for the reactive injection molding simulation process. These problems are leading to the users ‘dependency on the material data bank of simulation tools, leading to restriction in application of computer simulation in the thermoset injection molding simulation and comparison between experimental and simulation results. Furthermore, there is still a big question related to whether there is or no slip phenomenon between thermosets melt and the wall surface during filling the cavity, for which has not yet been found an exact answer. Because of this the effect of wall slip on the cavity surface is still ignored during thermoset injection molding simulation process. This thesis focused on three key scientific goals. The first one is innovation of a new technical method to explain the mold filling behavior of thermoset injection molding compounds physically. The second key goal is developing numerical method to create thermoset material data sheet for simulation of mold filling characterizations of thermoset injection molding compounds. Finally, creating a simulation tool base on the physical technique and generated material data sheet.
Anders, Denis. "Numerische Simulation und experimentelle Validierung statischer Mischelemente." Technische Universität Chemnitz, 2019. https://monarch.qucosa.de/id/qucosa%3A34245.
Messig, Danny. "Numerical simulation of pulverized coal combustion." Doctoral thesis, Technische Universitaet Bergakademie Freiberg Universitaetsbibliothek "Georgius Agricola", 2017. http://nbn-resolving.de/urn:nbn:de:bsz:105-qucosa-228707.
Joppa, M., H. Köhler, S. Kricke, J. P. Majschak, J. Fröhlich, and F. Rüdiger. "Simulation der Strahlreinigung: Diffusionsmodell für quellbare Verschmutzungen." Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2018. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-236389.
Neugebauer, R., P. Klimant, and M. Witt. "Realistic Machine Simulation with Virtual Reality." Universitätsbibliothek Chemnitz, 2014. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-qucosa-151993.
Landgraf, Ralf. "Modellierung und Simulation der Aushärtung polymerer Werkstoffe." Doctoral thesis, Universitätsbibliothek Chemnitz, 2015. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-qucosa-187720.
This work deals with the continuum mechanical formulation of curing phenomena in polymers as well as the implementation and simulation of curing models within the finite element method. Based on a general modelling framework, a specified material model for the simulation of curing processes in an acrylic bone cement is developed. Moreover, different finite element simulations regarding the clinical procedure of vertebroplasty are presented
Polanowski, Piotr, and Andrzej Sikorski. "Simulation of diffusion in a crowded environment." Universitätsbibliothek Leipzig, 2015. http://nbn-resolving.de/urn:nbn:de:bsz:15-qucosa-183392.
Heine, Andreas. "Berechnung und Simulation von Kurvenschrittgetrieben." Universitätsbibliothek Chemnitz, 2017. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-qucosa-225959.