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Topics Offered for Bachelor Theses

Our re­search group is constantly offering theses on the Bachelor level. On the Bachelor level, the topics are close to known results in scientific literature. Of course, she or he will be constantly supervised and supported in this endeavor by the head of the group and the other mem­bers of the re­search group!

For this reason, the possible topics are constantly evolving and no specific problems can be given here. Students interested in a Bachelor theses get a flavor of possible topics by the list given in list below. The presentation of the re­search group (in German) indicates useful capabilities for doing theoretical re­search which may offer some guidance.

Examples

Possible Topics

Besides analytical methods, numerical methods are essential in modern physics. In condensed matter theory, density matrix renormalization is a very powerful method, established by Steven R. White, and tailored to essentially one-dimensional systems.

If one wants to completely describe a quantum mechanical system, one way is to determine all the eigenvalues. But this is only possible for very small systems by means of the so-called Exact Diagonalization. If one wants to proceed to larger systems, one possible approach is to omit a large part of the Hilbert space in order to keep a simple, i.e., sufficiently small, system. But in doing so, only the smallest possible error in the wanted observables should be made. So which states are most likely to be omitted? This can be decided with the help of the eigenvalues of a density matrix.

The goal of the bachelor thesis is to reproduce the above sketched train of thought in detail. Diagonalization and density matrix renormalization will be illustrated by simple examples.

In the theoretical description, control pulses are terms in the Hamiltonian operator that are temporarily added. They are used to selectively influence the state of a quantum mechanical system. Here we consider a spin S=1/2 (NMR) or a so-called quantum bit or short qubit (quantum information).

In practice, it is never only the control pulse which influences the qubit, but also unwanted, but unavoidable interactions with the environment. By clever choices of the pulse shape, e.g., an amplitude as a function of time v(t), one can mitigate the effect of the environment. We have established equations that describe when a pulse is optimal in this sense.

The goal of the bacheolor work is to evaluate these equations explicitly for different pulses or pulse trains and to search for favorable pulse protocols. Technically, this requires one- and two-dimensional integrations, some of which can be solved efficiently with computer algebra programs and some with numerical programs.

By a clever choice of basis one can simplify quantum mechanical problems very much. A particularly elegant method for this is based on continuous unitary transformations (CUTs). A CUT corresponds to a rotation which is parametrized by a continuous variable. An important point is how one rotates, i.e. which axes of rotation one uses. For Hamiltonian operators the axis of rotation is called "generator".

Technically, one has to calculate a commutator and solve a differential equation system of O(10) variables. The latter can be done with any computer algebra program such as Maple or Mathematica. From quantum mechanics, one should know what a ground state is and a creation and annihilation operator of an energy quantum in a harmonic oscillator.

Then, the goal is to describe not only a harmonic potential but also a quartic potential which has a distinct double trough shape (like a W). In doing so, different generators can be tried out and compared which are also relevant for applications in research.

Coherent control of quantum systems is essential in many experiments, e.g., for high precision nuclear spin resonance or quantum information processing. There are many proposals for the optimization of coherent control, but they need to be verified on simple models before experimental realization. For this purpose, the time evolution of correlated systems is needed, e.g., of some O(5) spins.

The aim of the Bacheolor work is to calculate the time evolution of such systems from a few spins. For this purpose, a basis is chosen and one considers by which matrix the Hamiltonian operator is represented in the chosen basis. This matrix is numerically diagonalized using known implemented algorithms (in Matlab, Maple, Mathematica, Python or C). In this manner, the time-dependent Schrödinger equation is solved.

An alternative approach to temporal evolution is the so called Chebyshev expansion. The iterated application of the Hamilton operator to a single state vector allows one to determine expansion coefficients which in turn determine the time evolution up to a certain threshold time tmax.

Simulations consist in reproducing physical events directly in the computer. Monte Carlo simulations achieve this by statistical methods. A standard application is the description of continuous phase transitions. The simplest model to do so is the Ising model.

The aim of the bachelor thesis is to statistically simulate the Ising model in one and two dimensions. Some properties are to be determined as a function of temperature, for example the internal energy or the specific heat. It is interesting to characterize the phase transition by determining the transition temperature and critical exponents. The self-obtained results are to be compared with the exactly known results.

  • Werner Krauth
    Statistical Mechanics: Algorithms and Computations (zur Ausleihe/Ansicht vorhanden)
    Oxford Master Series in Statistical, Computational, and Theoretical Physics
    Oxford Uni­ver­sity Press, 2006

Topological effects have entered condensed matter physics at least since the 2016 Nobel Prize to David Thouless, Duncan Haldane and Michael Kosterlitz, and promise novel transport phenomena with reduced dissipation, i.e. less resistive losses, which can enable more sustainable in­for­mation processing in the longer term. Microscopically, spin-orbit coupling is the origin of topological twists in electronic quantum systems and thus in systems of localized electronic spins.

The aim of the bachelor thesis is to reproduce how a spin-orbit coupling leads to the asymmetric spin-spin couplings and to compute an ensuing effect such as the topological Zak phase and/or the formation of localized edge states.

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Location & approach

The campus of TU Dort­mund University is located close to interstate junction Dort­mund West, where the Sauerlandlinie A 45 (Frankfurt-Dort­mund) crosses the Ruhrschnellweg B 1 / A 40. The best interstate exit to take from A 45 is “Dort­mund-Eichlinghofen” (closer to South Campus), and from B 1 / A 40 “Dort­mund-Dorstfeld” (closer to North Campus). Signs for the uni­ver­si­ty are located at both exits. Also, there is a new exit before you pass over the B 1-bridge leading into Dort­mund.

To get from North Campus to South Campus by car, there is the connection via Vogelpothsweg/Baroper Straße. We recommend you leave your car on one of the parking lots at North Campus and use the H-Bahn (suspended monorail system), which conveniently connects the two campuses.

TU Dort­mund University has its own train station (“Dort­mund Uni­ver­si­tät”). From there, suburban trains (S-Bahn) leave for Dort­mund main station (“Dort­mund Hauptbahnhof”) and Düsseldorf main station via the “Düsseldorf Airport Train Station” (take S-Bahn number 1, which leaves every 20 or 30 minutes). The uni­ver­si­ty is easily reached from Bochum, Essen, Mülheim an der Ruhr and Duisburg.

You can also take the bus or subway train from Dort­mund city to the uni­ver­si­ty: From Dort­mund main station, you can take any train bound for the Station “Stadtgarten”, usually lines U41, U45, U 47 and U49. At “Stadtgarten” you switch trains and get on line U42 towards “Hombruch”. Look out for the Station “An der Palmweide”. From the bus stop just across the road, busses bound for TU Dort­mund University leave every ten minutes (445, 447 and 462). Another option is to take the subway routes U41, U45, U47 and U49 from Dort­mund main station to the stop “Dort­mund Kampstraße”. From there, take U43 or U44 to the stop “Dort­mund Wittener Straße”. Switch to bus line 447 and get off at “Dort­mund Uni­ver­si­tät S”.

The AirportExpress is a fast and convenient means of transport from Dortmund Airport (DTM) to Dortmund Central Station, taking you there in little more than 20 minutes. From Dortmund Central Station, you can continue to the university campus by interurban railway (S-Bahn). A larger range of international flight connections is offered at Düsseldorf Airport (DUS), which is about 60 kilometres away and can be directly reached by S-Bahn from the university station.

The H-Bahn is one of the hallmarks of TU Dort­mund University. There are two stations on North Campus. One (“Dort­mund Uni­ver­si­tät S”) is directly located at the suburban train stop, which connects the uni­ver­si­ty directly with the city of Dort­mund and the rest of the Ruhr Area. Also from this station, there are connections to the “Technologiepark” and (via South Campus) Eichlinghofen. The other station is located at the dining hall at North Campus and offers a direct connection to South Campus every five minutes.

The facilities of TU Dortmund University are spread over two campuses, the larger Campus North and the smaller Campus South. Additionally, some areas of the university are located in the adjacent “Technologiepark”.

Site Map of TU Dortmund University (Second Page in English).