• No results found

Applications of the random-state approach to quantum many-body dynamics

N/A
N/A
Protected

Academic year: 2021

Share "Applications of the random-state approach to quantum many-body dynamics"

Copied!
2
0
0

Bezig met laden.... (Bekijk nu de volledige tekst)

Hele tekst

(1)

University of Groningen

Applications of the random-state approach to quantum many-body dynamics Zhao, Peiliang

IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you wish to cite from it. Please check the document version below.

Document Version

Publisher's PDF, also known as Version of record

Publication date: 2017

Link to publication in University of Groningen/UMCG research database

Citation for published version (APA):

Zhao, P. (2017). Applications of the random-state approach to quantum many-body dynamics. University of Groningen.

Copyright

Other than for strictly personal use, it is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license (like Creative Commons).

Take-down policy

If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim.

Downloaded from the University of Groningen/UMCG research database (Pure): http://www.rug.nl/research/portal. For technical reasons the number of authors shown on this cover page is limited to 10 maximum.

(2)

STELLINGEN

Behorende bij het proefschrift

Applications of the random-state approach to

quantum many-body dynamics

Peiliang Zhao

8 September 2017

1. The advantage of numerical methods for solving the time-dependent

Schrödinger equation is the ability to monitor the dynamics instantaneously, resulting in physical insight. (Chapter 2)

2. The random state approach allows for the calculation of the linear response properties of many-body quantum systems using only the time evolution of a single pure random state. (Chapter 3 and 4)

3. Different types of disorders can be recognized by their fingerprints appearing in the profiles of dc conductivity, carrier mobility, optical spectroscopy, and Landau level spectrum. (Chapter 5)

4. A Bloch-type quantum master equation describes well the dynamics of a spin-1/2 particle in contact with a thermal bath. (Chapter 6)

5. No friction is terrible.

6. It is wrong to think that the task of physics is to find out how Nature is. Physics concerns what we say about Nature. (Niels Bohr)

7. Probability is the main guide of life.

8. There are thousands of reasons to refuse to do something that you do not like. In contrast, one reason is enough to do something that you like. 9. Your life will not be better by chance but could be better by change.

10. 横看成岭侧成峰 ---- A mountain, when viewed in face, may look like a

Referenties

GERELATEERDE DOCUMENTEN

a general locally finite connected graph, the mixing measure is unique if there exists a mixing measure Q which is supported on transition probabilities of irreducible Markov

Consider the lattice zd, d;?: 1, together with a stochastic black-white coloring of its points and on it a random walk that is independent of the coloring.

This is a review of the staüstical properties of the scattermg matnx of a mesoscopic System Two geometnes are contrasted A quantum dot and a disordered wire The quantum dot is a

(The average refers to an ensemble of disordered media with different random positions of the scatterers. ) The degree of entanglement (as quantified either by the concurrence [6] or

The transition from pure-state to mixed-state entangle- ment will m general depend on the detailed form of the scat- tering matnx However, a universal legime is entered in the case

This universality was anticipated [3] from the random-matrix theory of energy levels, but could not previously be established because of the absence of translational invariance of

Equations (8) and (10) have two immediate implica- tions for the universality of the variance of a linear statis- tic on the transmission eigenvalues: (1) Equation (10) is a

In een recent rapport van het Engelse Institution of Engineering and Technology (IET, zie www.theiet.org) wordt een overzicht gegeven van de redenen waarom 16-