TY - BOOK ED - Mikelskis-Seifert, Silke ED - Rabe, Thorid T1 - Physik Methodik : Handbuch für die Sekundarstufe I und II Y1 - 2007 SN - 978-3-589-22377-0 PB - Cornelsen CY - Berlin ER - TY - JOUR A1 - Rabe, Thorid T1 - Schülerzentierte Unterrichtsansätze : Kooperatives Lernen in Gruppen Y1 - 2007 SN - 978-3-589-22377-0 ER - TY - JOUR A1 - Menzel, Ralf T1 - Photonics : linear and nonlinear interactions of laser light and matter Y1 - 2007 SN - 978-540-67074-2 PB - Springer CY - Berlin ER - TY - JOUR A1 - Palus, Milan A1 - Kurths, Jürgen A1 - Schwarz, Udo A1 - Seehafer, Norbert A1 - Novotna, Dagmar A1 - Charvatova, Ivanka T1 - The solar activity cycle is weakly synchronized with the solar inertial motion N2 - We study possible interrelations between the 300-year record of the yearly sunspot numbers and the solar inertial motion (SIM) using the recently developed technique of synchronization analysis. Phase synchronization of the sunspot cycle and the SIM is found and statistically confirmed in three epochs (1734-1790, 1855-1875 and 1907-1960) of the whole period 1700-2000. These results give quantitative support to the hypothesis that there is a weak interaction between the solar activity and the SIM. Y1 - 2007 UR - http://www.sciencedirect.com/ science?_ob=GatewayURL&_method=citationSearch&_urlVersion=4&_origin=SDVIALERTHTML&_version=1&_uoikey=B6TVM-4MYVG5S- 1&md5=92d1fc7094be5195504f17e1afb4f0d1 U6 - https://doi.org/10.1016/j.physleta.2007.01.039 ER - TY - JOUR A1 - Mikelskis, Helmut F. T1 - Unterrichtsprinzipien : exemplarisch - genetisch - sokratisch Y1 - 2007 SN - 978-3-589-22377-0 ER - TY - JOUR A1 - Mikelskis-Seifert, Silke A1 - Rabe, Thorid T1 - Der darbietende Unterricht : darbieten - was und wie? Y1 - 2007 SN - 978-3-589-22377-0 ER - TY - JOUR A1 - Kofod, Guggi A1 - Wirges, Werner A1 - Paajanen, Mika A1 - Bauer, Siegfried T1 - Energy minimization for self-organized structure formation and actuation N2 - An approach for creating complex structures with embedded actuation in planar manufacturing steps is presented. Self-organization and energy minimization are central to this approach, illustrated with a model based on minimization of the hyperelastic free energy strain function of a stretched elastomer and the bending elastic energy of a plastic frame. A tulip-shaped gripper structure illustrates the technological potential of the approach. Advantages are simplicity of manufacture, complexity of final structures, and the ease with which any electroactive material can be exploited as means of actuation. (c) 2007 American Institute of Physics. Y1 - 2007 UR - http://apl.aip.org/ U6 - https://doi.org/10.1063/1.2695785 SN - 0003-6951 ER - TY - BOOK A1 - Barceló, Pedro T1 - Alexander der Große Y1 - 2007 SN - 978-3-89678-610-4 PB - Primus-Verl. CY - Darmstadt ER - TY - JOUR A1 - Kowarik, Stefan A1 - Gerlach, Andreas A1 - Leitenberger, Wolfram A1 - Hu J, Witte A1 - Wöll, Christoph A1 - Schreiber, Frank T1 - Energy-dispersive X-ray reflectivity and GID for real-time growth studies of pentacene thin films N2 - We use energy-dispersive X-ray reflectivity and grazing incidence diffraction (GID) to follow the growth of the crystalline organic semiconductor pentacene on silicon oxide in-situ and in real-time. The technique allows for monitoring Bragg reflections and measuring X-ray growth oscillations with a time resolution of 1 min in a wide q-range in reciprocal space extending over 0.25-0.80 angstrom(-1), i.e. sampling a large number of Fourier components simultaneously. A quantitative analysis of growth oscillations at several q-points yields the evolution of the surface roughness, showing a marked transition from layer-by-layer growth to strong roughening after four monolayers of pentacene have been deposited. (c) 2006 Elsevier B.V. All rights reserved. Y1 - 2007 UR - http://www.sciencedirect.com/science/journal/00406090 U6 - https://doi.org/10.1016/j.tsf.2006.12.020 SN - 0040-6090 ER - TY - THES A1 - Velagapudi, Rama Krishna T1 - Preparation and characterization of thermally stable guest-host Polymer thin films for non-lunear optical applications Y1 - 2008 CY - Potsdam ER - TY - THES A1 - Velagapudi, Rama Krishna T1 - Preparation and characterization of thermally stable guest-host polymer thin films for non-linear optical applications Y1 - 2008 CY - Potsdam ER - TY - JOUR A1 - Qiu, Xunlin A1 - Mellinger, Axel A1 - Wirges, Werner A1 - Gerhard, Reimund T1 - Spectroscopic study of dielectric barrier discharges in cellular polypropylene ferroelectrets N2 - The transient light emission from the dielectric barrier discharges (DBDs) in cellular polypropylene ferroelectrets subjected to high electric poling fields was spectroscopically measured. The spectrum shows strong emission from the second positive system of molecular nitrogen, N-2(C (3)Pi(u))-> N-2(B (3)Pi(g)), and the first negative system of N-2(+), N-2(+)(B (2)Sigma(+)(u))-> N-2(+)(X (2)Sigma(+)(g)), consistent with a DBD in air. When a dc voltage is applied stepwise to the ferroelectret film, light emission starts above a threshold, coinciding with the threshold voltage in obtaining piezoelectricity. From selected vibronic band strength ratios, the electric field in the discharge was determined and found to agree with Townsend breakdown. Y1 - 2007 UR - http://apl.aip.org/ U6 - https://doi.org/10.1063/1.2786597 ER - TY - THES A1 - Kasper, Lutz T1 - Diskursiv-narrative Elemente für den Physikunterricht. Entwicklung und Evaluation einer multimedialen Lernumgebung zum Erdmagnetismus Y1 - 2008 CY - Potsdam ER - TY - THES A1 - Blecua, Pedro T1 - Liquid morphologies on patterned surfaces Y1 - 2008 CY - Potsdam ER - TY - THES A1 - Rausche, Germar T1 - Ein Verfahren zur Bestimmung des Magnetfeldes in aktiven Strukturen der Sonnenkorona Y1 - 2008 CY - Potsdam ER - TY - JOUR A1 - Feudel, Fred A1 - Tuckerman, L. S. A1 - Gellert, Marcus A1 - Seehafer, Norbert T1 - Bifurcations of rotating waves in rotating spherical shell convection JF - Physical Review E N2 - The dynamics and bifurcations of convective waves in rotating and buoyancy-driven spherical Rayleigh-Benard convection are investigated numerically. The solution branches that arise as rotating waves (RWs) are traced by means of path-following methods, by varying the Rayleigh number as a control parameter for different rotation rates. The dependence of the azimuthal drift frequency of the RWs on the Ekman and Rayleigh numbers is determined and discussed. The influence of the rotation rate on the generation and stability of secondary branches is demonstrated. Multistability is typical in the parameter range considered. KW - nonsymmetric linear-systems KW - thermal-convection KW - fluid shells KW - hopf-bifurcation KW - onset KW - magnetoconvection KW - number KW - flow Y1 - 2015 U6 - https://doi.org/10.1103/PhysRevE.92.053015 SN - 1539-3755 SN - 1550-2376 VL - 92 IS - 5 PB - American Physical Society CY - Woodbury ER - TY - THES A1 - Habicht, Klaus T1 - Neutron-resonance spin-echo spectroscopy BT - a high resolution look at dispersive excitations Y1 - 2016 ER - TY - THES A1 - Krüsemann, Henning T1 - First passage phenomena and single-file motion in ageing continuous time random walks and quenched energy landscapes N2 - In der Physik gibt es viele Prozesse, die auf Grund ihrer Komplexität nicht durch physikalische Gleichungen beschrieben werden können, beispielsweise die Bewegung eines Staubkorns in der Luft. Durch die vielen Stöße mit Luftmolekülen führt es eine Zufallsbewegung aus, die so genannte Diffusion. Auch Moleküle in biologischen Zellen diffundieren, jedoch befinden sich in einer solchen Zelle im selben Volumen viel mehr oder viel größere Moleküle. Das beobachtete Teilchen stößt dementsprechend öfter mit anderen zusammen und die Diffusion wird langsamer, sie wird subdiffusiv. Mit der Zeit kann sich die Charakteristik der Subdiffusion ändern; dies wird als (mikroskopisches) Altern bezeichnet. Ich untersuche in der vorliegenden Arbeit zwei mathematische Modelle für eindimensionale Subdiffusion, einmal den continuous time random walk (CTRW) und einmal die Zufallsbewegung in einer eingefrorenen Energielandschaft (QEL=quenched energy landscape). Beide sind Sprungprozesse, das heißt, sie sind Abfolgen von räumlichen Sprüngen, die durch zufallsverteilte Wartezeiten getrennt sind. Die Wartezeiten in der QEL sind räumlich korrelliert, während sie im CTRW unkorrelliert sind. Ich untersuche in der vorliegenden Arbeit verschiedene statistische Größen in beiden Modellen. Zunächst untersuche ich den Einfluss des Alters und den Einfluss der Korrellationen einer QEL auf die Verteilung der Zeiten, die das diffundierendes Teilchen benötigt, um eine (räumliche) Schwelle zu überqueren. Ausserdem bestimme ich den Effekt des Alters auf Ströme von (sub)diffundierenden Partikeln, die sich auf eine absorbierende Barriere zubewegen. Zuletzt beschäftige ich mich mit der Diffusion einer eindimensionalen Anordnung von Teilchen in einer QEL, in der diese als harte Kugeln miteinander wechselwirken. Dabei vergleiche ich die gemeinsame Bewegung in einer QEL und als individuelle CTRWs miteinander über die Standartabweichung von der Startposition, für die ich das Mittel über mehrere QELs untersuche. Meine Arbeit setzt sich zusammen aus theoretischen Überlegungen und Berechnungen sowie der Simulation der Zufallsprozesse. Die Ergebnisse der Simulation und, soweit vorhanden, experimentelle Daten werden mit der Theorie verglichen. N2 - In the first part of my work I have investigated the ageing properties of the first passage time distributions in a one-dimensional subdiffusive continuous time random walk with power law distributed waiting times of the form $\psi(\tau) \sim \tau^{-1-\alpha}$ with $0<\alpha<1$ and $1<\alpha<2$. The age or ageing time $t_a$ is the time span from the start of the stochastic process to the start of the observation of this process (at $t=0$). I have calculated the results for a single target and two targets, also including the biased case, where the walker is driven towards the boundary by a constant force. I have furthermore refined the previously derived results for the non-ageing case and investigated the changes that occur when the walk is performed in a discrete quenched energy landscape, where the waiting times are fixed for every site. The results include the exact Laplace space densities and infinite (converging) series as exact results in the time space. The main results are the dominating long time power law behavior regimes, which depend on the ageing time. For the case of unbiased subdiffusion ($\alpha < 1$) in the presence of one target, I find three different dominant terms for ranges of $t$ separated by $t_a$ and another crossover time $t^{\star}$, which depends on $t_a$ as well as on the anomalous exponent $\alpha$ and the anomalous diffusion coefficient $K_{\alpha}$. In all three regimes ($t \ll t_a$, $t_a \ll t \ll t^{\star}$, $t \gg t^{\star}$) one finds power law decay with exponents depending on $\alpha$. The middle regime only exists for $t_a \ll t^{\star}$. The dominant terms in the first two regimes (ageing regimes) come from the probability distribution of the forward waiting time, the time one has to wait for the stochastic process to make the first step during the observation. When the observation time is larger than the second crossover time $t^{\star}$, the first passage time density does not show ageing and the non-ageing first passage time dominates. The power law exponents in the respective regimes are $-\alpha$ for strong ageing, $-1-\alpha$ in the intermediate regime, and $-1-\alpha/2$ in the final non-ageing regime. A similar split into three regimes can be found for $1<\alpha<2$, only with a different second crossover time $t^*$. In this regime the diffusion is normal but also age-dependent. For the diffusion in quenched energy landscapes one cannot detect ageing. The first passage time density shows a quenched power law $^\sim t^{-(1+2\alpha)/(1+\alpha)}$. For diffusion between two target sites and the biased diffusion towards a target only two scaling regimes emerge, separated by the ageing time. In the ageing case $t \ll t_a$ the forward waiting time is again dominant with power law exponent $-\alpha$, while the non-ageing power law $-1-\alpha$ is found for all times $t \gg t_a$. An intermediate regime does not exist. The bias and the confinement have similar effects on the first passage time density. For quenched diffusion, the biased case is interesting, as the bias reduces correlations due to revisiting of the same waiting time. As a result, CTRW like behavior is observed, including ageing. Extensive computer simulations support my findings. The second part of my research was done on the subject of ageing Scher-Montroll transport, which is in parts closely related to the first passage densities. It explains the electrical current in an amorphous material. I have investigated the effect of the width of a given initial distribution of charge carriers on the transport coefficients as well as the ageing effect on the emerging power law regimes and a constant initial regime. While a spread out initial distribution has only little impact on the Scher-Montroll current, ageing alters the behavior drastically. Instead of the two classical power laws one finds four current regimes, up to three of which can appear in a single experiment. The dominant power laws differ for $t \ll t_a, t_c$, $t_a \ll t \ll t_c$, $t_c \ll t \ll t_a$, and $t \gg t_a,t_c$. Here, $t_c$ is the crossover time of the non-aged Scher-Montroll current. For strongly aged systems one can observe a constant current in the first regime while the others are dominated by decaying power laws with exponents $\alpha -1$, $-\alpha$, and $-1-\alpha$. The ageing regimes are the 1st and 3rd one, while the classical regimes are the 2nd and the 4th. I have verified the theory using numerical integration of the exact integrals and applied the new results to experimental data. In the third part I considered a single file of subdiffusing particles in an energy landscape. Every occupied site of the landscape acts as a boundary, from which a particle is immediately reflected to its previous site, if it tries to jump there. I have analysed the effects single-file diffusion a quenched landscape compared to an annealed landscape and I have related these results to the number of steps and related quantities. The diffusion changes from ultraslow logarithmic diffusion in the annealed or CTRW case to subdiffusion with an anomalous exponent $\alpha/(1+\alpha)$ in the quenched landscape. The behavior is caused by the forward waiting time, which changes drastically from the quenched to the annealed case. Single-file effects in the quenched landscape are even more complicated to consider in the ensemble average, since the diffusion in individual landscapes shows extremely diverse behavior. Extensive simulations support my theoretical arguments, which consider mainly the long time evolution of the mean square displacement of a bulk particle. KW - continuous time random walk KW - quenched energy landscape KW - first passage time KW - Scher-Montroll transport KW - single-file motion KW - Zufallsbewegung KW - Diffusion KW - eingefrorene Energielandschaft KW - Scher-Montroll Transport KW - Wartezeitverteilung Y1 - 2016 ER - TY - THES A1 - Anielski, Alexander T1 - Entwicklung einer mikrofluidischen, adaptiv geregelten Messapparatur zur quantitativen Untersuchung von Chemotaxis mit Hilfe der Flussfotolyse KW - Flussfotolyse KW - Konzentration KW - Chemotaxis KW - Mikrokanal KW - Dictyostelium KW - flow photolysis KW - concentration KW - chemotaxis KW - microchannel KW - Dictyostelium Y1 - 2015 ER - TY - THES A1 - Wenz, Leonie T1 - Climate change impacts in an increasingly connected world Y1 - 2016 ER -