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π€ Talks
π Posters
Physical Review X, Physical Review Letters, Physical Review B
Short description of portfolio item number 1
Short description of portfolio item number 2 
Christopher Fechisin, Kunal Sharma, Przemyslaw Bienias, Steven L. Rolston, J. V. Porto, Michael J. Gullans, Alexey V. Gorshkov
Rydberg arrays exhibit remarkable many-body physics due to strong Rydberg-Rydberg interactions which are possible between their constituent atoms. We present a protocol which leverages this physics to non-destructively count photons by temporarily storing them in the array.

Maissam Barkeshli, Christopher Fechisin, Zohar Komargodski, Siwei Zhong
We study the effects of lattice rotational and translational symmetries on Dirac cones in lattice models and the Dirac fermion field theories to which they flow in the continuum. In particular, we find that models defined on lattices with defects flow to field theories with additional magnetic flux, the amount of which is determined by universal topological data. We use defect conformal field theory to identify observables sensitive to this additional flux and then measure it in critical lattice models.

Christopher Fechisin, Nathanan Tantivasadakarn, Victor V. Albert
The cluster state is the simplest example of SPT order, protected by a $\mathbb{Z}_2\times\mathbb{Z}_2$ symmetry. In this work, we show that a generalized cluster state with fusion category symmetry $G\times\text{Rep}(G)$ shares many qualitative features with the ordinary cluster state and should be thought of as an SPT protected by a non-invertible symmetry.

Jeet Shah, Christopher Fechisin, Yu-Xin Wang, Joseph T. Iosue, James D. Watson, Yan-Qi Wang, Brayden Ware, Alexey V. Gorshkov, Cheng-Ju Lin
In this work, we interrogate the analogy between (i) pure state SPTs as ground states of local Hamiltonians and (ii) mixed state SPTs as steady states of local Lindbladians. We construct a Lindbladian which hosts a simple mixed-state SPT within its steady-state subspace, then add symmetric local perturbations to see if the new steady states lie in the same mixed-state phase as the original. We find that for generic symmetric perturbations, the answer is no, due to the onset of strong-to-weak spontaneous symmetry breaking.

Undergraduate course, University 1, Department, 2014
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Workshop, University 1, Department, 2015
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