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1. Introduction Solid state physics Model-building Use of general principles crystallographers Drude and Sommerfeld model Improved model Fermi-liquid.

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Presentation on theme: "1. Introduction Solid state physics Model-building Use of general principles crystallographers Drude and Sommerfeld model Improved model Fermi-liquid."— Presentation transcript:

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2 1. Introduction Solid state physics Model-building Use of general principles crystallographers Drude and Sommerfeld model Improved model Fermi-liquid theory Explanation of superconductivity Kepler

3 1. Introduction Solid state physics Model-building Use of general principles Nyquist formula Onsager reciprocity relations Fluctuation-dissipation theorem Linear response theory Detailed balance Universality Fluctuation relation

4 1. Introduction Consider a time-reversal-invariant system Prob. Consider a process made of the following three steps: 1)The initial state of the system is measured; 2)The system undergoes unitary evolution; 3)The final state is determined through measurement. There is a simple relation between the two prob.

5 1. Introduction System N S Prob. Fluctuation relation?

6 1. Introduction Chirality -Excitation can propagate in one direction only. Ex) The edges of certain quantum Hall liquids, Chiral transport in the quantum Hall effect(QHE) Causality principle : the past do not affected by the future. In the chiral case, the right do not affected by the past on the left. RL

7 2. Fluctuation theorems The typical form of the fluctuation theorem The definitions of the forward and backward processes 1)Initially in both processes, the system obeys a Gibbs distribution 2)The dynamical equations in the backward process is obtained from the dynamical equations in the forward process by the time-reversal operation.

8 2. Fluctuation theorems 0 t with

9 2. Fluctuation theorems with Backward process Eigenstates

10 2. Fluctuation theorems Since

11 3. Saito-Utsumi relations 1) The electric current 2) The noise power 3) The third cumulant

12 3. Saito-Utsumi relations 3.1 Symmetric and antisymmetric variables definition The linear conductance is an even function The equilibrium noise power does not depend on the direction of B

13 3. Saito-Utsumi relations 3.2 Fluctuation relations for symmetric variables definition Nyquist formula

14 3. Saito-Utsumi relations 3.3 Fluctuation relations for antisymmetric variables

15 3. Saito-Utsumi relations 3.4 Microreversiblity

16 3. Saito-Utsumi relations 3.5 Experiment

17 4. Chiral systems

18 5. Fluctuation relations in chiral systems 5.1 Qualitative argument

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20 5. Fluctuation relations in chiral systems 5.2 Toy model

21 5. Fluctuation relations in chiral systems 5.3 General derivation

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23 5. Fluctuation relations in chiral systems 5.3 Generalizations

24 5. Fluctuation relations in chiral systems 5.4 Applications


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