2:00 pm - 4:00 pm Nanopore technology: from DNA sequencing to drug discovery October 28 @ 2:00 pm - 4:00 pm Nanopore technology: from DNA sequencing to drug discovery
3:00 pm - 4:00 pm Radiative cooling to harvest water from air October 28 @ 3:00 pm - 4:00 pm Radiative cooling to harvest water from air
9:00 am - 10:00 am Symmetry enforced entanglement in maximally mixed states October 29 @ 9:00 am - 10:00 am Symmetry enforced entanglement in maximally mixed states
9:00 am - 10:00 am Coadjoint-orbit Bosonization of a Fermi surface in a magnetic field November 5 @ 9:00 am - 10:00 am Coadjoint-orbit Bosonization of a Fermi surface in a magnetic field
10:00 am - 11:00 am Nanopores for fingerprinting and sequencing individual proteins November 6 @ 10:00 am - 11:00 am Nanopores for fingerprinting and sequencing individual proteins
3:00 pm - 4:00 pm Nanotechnology for single-molecule biology: from nanopore protein sequencing to chromosome organization November 6 @ 3:00 pm - 4:00 pm Nanotechnology for single-molecule biology: from nanopore protein sequencing to chromosome organization
10:00 am - 11:00 am DNA loop extrusion by the SMC molecular motors that organize our chromosomes November 7 @ 10:00 am - 11:00 am DNA loop extrusion by the SMC molecular motors that organize our chromosomes
10:00 am - 11:00 am Building a synthetic cell from the bottom up November 8 @ 10:00 am - 11:00 am Building a synthetic cell from the bottom up
9:00 am - 12:00 pm Quantized axial charge and the chiral anomaly in a Hamiltonian lattice model November 12 @ 9:00 am - 12:00 pm Quantized axial charge and the chiral anomaly in a Hamiltonian lattice model
10:00 am - 11:00 am Cosmology: A Golden Era November 19 @ 10:00 am - 11:00 am Cosmology: A Golden Era
November 6 @ 3:00 pm - 4:00 pm Nanotechnology for single-molecule biology: from nanopore protein sequencing to chromosome organization
November 7 @ 10:00 am - 11:00 am DNA loop extrusion by the SMC molecular motors that organize our chromosomes
November 12 @ 9:00 am - 12:00 pm Quantized axial charge and the chiral anomaly in a Hamiltonian lattice model