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5 Oct 2020: 5. Chern-Simons Theories. So far we’ve approached the quantum Hall states from a microscopic perspective, look-. ing at the wavefunctions which describe individual electrons. In this section, we take. a step back and describe the quantum Hall eect

8 Nov 2020: 8. Quantum Field Theory on the Plane. In this section, we step up a dimension. We will discuss quantum field theories in. d = 2 1 dimensions. Like their d = 1 1 dimensional counterparts, these theories. have application in various condensed matter

8 Nov 2020: In contrast,. – 200 –. acting with a Lorentz boost in SO(3, 1) will take you further and further away.

8 Nov 2020: 4. Lattice Gauge Theory 200. 4.1 Scalar Fields on the Lattice 202.

17 Jul 2020: Sutcliffe),Physics Letters 342B (1995) 196-200. 51. Geometry of Defect Scattering, in Formation and Interactions of TopologicalDefects, NATO ASI Series B: Physics Vol.

4 Nov 2020: For the simulations below, the physi-cally meaningful polariton lifetimes of 5, 20-200, and 200ps (or2ps/13ps/100ps for simulations in Figure 4) are used for barri-ers, gates, and

2 Feb 2020: Failure Prediction for Satellite Monitoring Systems Using Bayesian Networks. Steven Bottone, Daniel Lee, Clay Stanek DataPath, Inc., 13025 Danielson Street, Suite 200, Poway, CA 92064.

2 Feb 2020: 13. 0 50 100 150 200 250 300. x. 0.10. 0.05. ... 3 for Dirichlet and Neumann case. 0 50 100 150 200 250 300.

4 Feb 2020: 0 50 100 150 200 250 300 The random surface was fairly jagged, with a subfractalX autocorrelation function of the form. ... To begin this solution an 0 50 100 150 200 250 300initial value is required either for T'(0) or for h(O) (or yiji).

4 Feb 2020: This is bound- ed by. 0.25. 0.20 -. 0.15 -. 0.05 -. -0.10 -. -0.15. I. I. I. I. I. 0 100 200 ]00 400 500 600.