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Thursday,
13. Nov. 2025 |
Video-Recording for any system with MP4-support - Video.mp4 (ca. 388 Mb) |
15:15 – 16:15 |
"Simulating Hubbard model physics in moiré semiconductors"
Speaker: Prof. Kin Fai Mak
(Cornell University)
Abstract:
The strong Coulomb interactions between
many electrons in solids can induce
many fascinating phenomena, such as
magnetism, high-temperature superconductivity,
and electron fractionalization. In 1963,
physicists developed a model, known as
the Hubbard model, to describe such
interactions in a highly simplified manner.
The deceptively simple model is, however,
difficult to solve accurately even with
modern-day supercomputers. The physical
realizations and thus simulations of
the Hubbard model therefore have a vital
role to play in solving this important
problem. Moiré materials, metamaterials
built on artificial “moiré atoms”, have
emerged as a promising Hubbard model
simulator in recent years. In this talk,
I will discuss recent efforts on simulating
the Hubbard model in moiré semiconductors,
with a particular focus on the problem of
high-temperature superconductivity.
About the Speaker:
Kin Fai Mak obtained a PhD in physics from
Columbia University in 2010 after
completing a B.S. in Physics and
Mathematics from Hong Kong University of
Science and Technology in 2005. He is
currently the Josephson Family Professor
in Cornell University and also, since
2014, a scientific member and director of
Max Planck Institute for the Structure and
Dynamics of Matter in Germany.
He is the recipient of many awards and
honors including PRISM -Prize of the
Institute of Structure of Matter, ISM-CNR
- Senior category (2025), Gordon and
Betty Moore Foundation Experimental
Physics Investigators Award (2022),
Friedrich Wilhelm Bessel Research Award
(2021), and many more. His fields of
expertise include two-dimensional quantum
materials and heterostructures,
Spectroscopy, Exciton physics, Strong
correlation physics, Berry curvature effects
on optical and electrical phenomena,
Magnetism, and Unconventional superconductivity.