• No results found

Fermions, criticality and superconductivity She, J.H.

N/A
N/A
Protected

Academic year: 2021

Share "Fermions, criticality and superconductivity She, J.H."

Copied!
3
0
0

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

Hele tekst

(1)

Fermions, criticality and superconductivity

She, J.H.

Citation

She, J. H. (2011, May 3). Fermions, criticality and superconductivity. Casimir PhD Series.

Faculty of Science, Leiden University. Retrieved from https://hdl.handle.net/1887/17607

Version: Corrected Publisher’s Version

License: Licence agreement concerning inclusion of doctoral thesis in the Institutional Repository of the University of Leiden

Downloaded from: https://hdl.handle.net/1887/17607

Note: To cite this publication please use the final published version (if applicable).

(2)

Stellingen

accompanying the PhD thesis

Fermions, Criticality and Superconductivity

1. Below some finite critical temperature, infinitely long windings proliferate in both bosonic and fermionic systems. It is then the worldline supersymmetry that elim- inates the Meissner effect for a gas of charged fermions.

Chapter 2

2. The NP hardness of the fermion sign problem tells us that there is no mathemat- ically exact solution, but how many features of the physical world we understand well are actually based on exact mathematics?

Chapter 3

3. On approach to the quantum critical point, an interaction that was deemed irrel- evant initially, takes over and dominates.

Chapter 4

4. The scaling behavior of the free fermion case is special and the pair operator in a general conformal fermionic state can be characterized by a scaling dimension that is any real number smaller than one.

Chapter 5

5. The pairing mechanism in quantum critical metals is still under intense debate.

Since pairing happens in the Cooper channel, it is desirable to be able to measure the Cooper channel directly.

Chapter 6

6. Contrary to intuition, quantum mechanics actually renders a strongly interacting Bose or Fermi liquid to act like a system of free particles with renormalized mass.

R. P. Feynman, Phys. Rev. 91, 1291(1953)

7. The fermionic quantum critical states discovered in cuprates and heavy fermions are the desired high dimensional generalizations of the Luttinger liquid.

1

(3)

8. The original purpose of renormalization group (RG) was to explain universality of the critical exponents and yet retain the connection to microscopic physics; but the quantum critical point sect ignores the starting point of RG and deals only with its end result. Microscopic variables are seen as ‘irrelevant’ and ‘therefore’

unimportant.

P. W. Anderson, Physica B 318, 28(2002)

9. The existence of the string landscape suggests that our universe can be in a quan- tum glass state with large viscosity. The long distance dynamics slows down while the short distance dynamics stays the same. This explains the apparent smallness of the cosmological constant.

J. She, JCAP02(2007)021

10. A leader is best when people barely know that he exists, not so good when people obey and acclaim him, worst when they despise him.

Laozi, Tao Te Ching

Jian-Huang She Leiden, Feb. 22, 2011

2

Referenties

GERELATEERDE DOCUMENTEN

License: Licence agreement concerning inclusion of doctoral thesis in the Institutional Repository of the University of Leiden Downloaded.

License: Licence agreement concerning inclusion of doctoral thesis in the Institutional Repository of the University of Leiden Downloaded from: https://hdl.handle.net/1887/17607..

By applying pressure, magnetic field, or doping, a second- order phase transition can be tuned to zero temperature, producing a quantum critical point (QCP).. Such a singular

One can easily show [36] that below the Fermi temper- ature, worldlines with macroscopic winding number also proliferate in fermionic systems; this leads to a puzzle: the

Quite recently Mitas [79] proved a conjecture due to Ceperley [73], stating that the reach of the higher dimensional Fermi gas is ‘maximal’ in the sense that, for a given R 0 and τ

We find in our analysis that the QCP is indeed unstable towards a first order transition as a result of competition. Obviously details of the collapse of a QCP and the resulting

Instead of using the Fermi gas pair susceptibility (as in conventional BCS), we rely on the fact that conformal invariance fixes the analytical form of this response function in

Using a SIN tunneling junction, experimentalists can measure the imaginary part of the full dynamical pair susceptibility χ 00 p in the normal state of the quantum critical metals..