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| 001 | 856610 | ||
| 005 | 20210129235331.0 | ||
| 037 | _ | _ | |a FZJ-2018-05978 |
| 041 | _ | _ | |a English |
| 100 | 1 | _ | |a Jin, Fengping |0 P:(DE-Juel1)144355 |b 0 |e Corresponding author |u fzj |
| 111 | 2 | _ | |a Quantum Many-Body Methods In Condensed Matter Systems |c Julich |d 2018-09-24 - 2018-09-27 |w Germany |
| 245 | _ | _ | |a Quantum typicality approach: Application to transport in the one-dimensional Hubbard model |
| 260 | _ | _ | |c 2018 |
| 336 | 7 | _ | |a Conference Paper |0 33 |2 EndNote |
| 336 | 7 | _ | |a Other |2 DataCite |
| 336 | 7 | _ | |a INPROCEEDINGS |2 BibTeX |
| 336 | 7 | _ | |a conferenceObject |2 DRIVER |
| 336 | 7 | _ | |a LECTURE_SPEECH |2 ORCID |
| 336 | 7 | _ | |a Conference Presentation |b conf |m conf |0 PUB:(DE-HGF)6 |s 1540358109_17681 |2 PUB:(DE-HGF) |x Invited |
| 520 | _ | _ | |a In quantum theory, a typical state is a pure random state representing the majority of all possible states, drawn at random from a high-dimensional Hilbert space. The concept of typicality says that such a random state has the same properties as the full statistical ensemble. This concept, together with numerically solving the time-dependent Schrödinger equation (TDSE), is the basis of the so-called quantum typicality approach. It can be used to calculate various properties of quantum systems, such as the density of states (DOS) or certain static and dynamic functions.In this talk, I will start by reviewing the leading methods to solve the TDSE. Following this, I will present the basic concepts contained in the quantum typicality approach. Finally, I will present results of applying the method to transport in the 1D Hubbard model. |
| 536 | _ | _ | |a 511 - Computational Science and Mathematical Methods (POF3-511) |0 G:(DE-HGF)POF3-511 |c POF3-511 |f POF III |x 0 |
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| 914 | 1 | _ | |y 2018 |
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