Topological Materials as Platforms for New Particles and Electromagnetic Responses
Topological Materials as Platforms for New Particles and Electromagnetic Responses
-
1. Topological materials as platf…
0
00:00/00:00
-
2. Outline
142.40907574240907
00:00/00:00
-
3. Types of order
236.87020353687021
00:00/00:00
-
4. Berry phase in solids
333.83383383383386
00:00/00:00
-
5. Berry phase
418.78545211878549
00:00/00:00
-
6. Berry phase
480.54721388054725
00:00/00:00
-
7. Berry phase in solids
561.327994661328
00:00/00:00
-
8. A non-Abelian example
656.22288955622287
00:00/00:00
-
9. What about metals?
752.71938605271941
00:00/00:00
-
10. Anomalous Hall effect (100+ ye…
857.15715715715714
00:00/00:00
-
11. Two"mystery" effects in optics
911.31131131131133
00:00/00:00
-
12. More on standard (non-quantize…
989.38938938938941
00:00/00:00
-
13. Another mystery effect:
1023.1898565231899
00:00/00:00
-
14. 3D Dirac andWeyl metals
1060.3603603603604
00:00/00:00
-
15. Weyl semimetals
1135.6022689356023
00:00/00:00
-
16. How does this translate to sol…
1175.9092425759093
00:00/00:00
-
17. Linear optics: summary of CME/…
1248.848848848849
00:00/00:00
-
18. Nonlinear effects in metals
1293.0263596930265
00:00/00:00
-
19. Optical quantization in semime…
1317.8511845178512
00:00/00:00
-
20. Experimental evidence that non…
1361.1611611611613
00:00/00:00
-
21. Theoretical understanding of n…
1410.4771438104772
00:00/00:00
-
22. Quantized CPGE
1440.7741074407741
00:00/00:00
-
23. What is the "quantum"?
1494.0273606940275
00:00/00:00
-
24. Simplified picture of origin o…
1547.2138805472139
00:00/00:00
-
25. Experimental detection
1584.7180513847181
00:00/00:00
-
26. Experimental detection
1618.1181181181182
00:00/00:00
-
27. Conclusions Nonlinear optics h…
1649.2826159492827
00:00/00:00
-
28. Acknowledgements
1688.0880880880882
00:00/00:00