Tami Pereg-Barnea

Theory of quasiparticle interference patterns in the pseudogap phase of the cuprate superconductors

A method is proposed to test for the nature of the pseudogap phase in cuprates using the recently developed technique of Fourier-transform scanning tunneling spectroscopy. We show that the observed quasiparticle interference patterns depend critically on the quasiparticle coherence factors, making it possible to distinguish between the pseudogap dominated by superconducting fluctuations from the pseudogap dominated by various particle-hole condensates.

Absolute values of the London penetration depth inYBa2Cu3O6+ymeasured by zero field ESR spectroscopy on Gd doped single crystals

Zero-field electron spin resonance (ESR) of dilute Gd ions substituted for Y in the cuprate superconductor

Gauge-invariant response functions in algebraic Fermi liquids

{\mathrm{YBa}}_{2}{\mathrm{Cu}}_{3}{\mathrm{O}}_{6+y}

Edge-state transport in Floquet topological insulators

is used as a novel technique for measuring the absolute value of the low-temperature magnetic penetration depth

Photon-Inhibited Topological Transport in Quantum Well Heterostructures.

\ensuremath{\lambda}(\stackrel{\ensuremath{\rightarrow}}{T}0).

QUASIPARTICLE INTERFERENCE PATTERNS AS A TEST FOR THE NATURE OF THE PSEUDOGAP PHASE IN THE CUPRATE SUPERCONDUCTORS

The Gd ESR spectrum of samples with

Anderson topological superconductor

\ensuremath{\approx}1%

Incommensurate spin density wave as a signature of spin-orbit coupling and precursor of topological superconductivity

substitution was obtained with a broadband microwave technique that measures power absorption bolometrically from 0.5 to 21 GHz. This ESR spectrum is determined by the crystal field that lifts the level degeneracy of the spin

Strong coupling expansion of the extended Hubbard model with spin-orbit coupling

7/2{\mathrm{Gd}}^{3+}

Dirac cones, Floquet side bands, and theory of time-resolved angle-resolved photoemission

ion and details of this spectrum provide information concerning oxygen ordering in the samples. The magnetic penetration depth is obtained by relating the number of Gd ions exposed to the microwave magnetic field to the frequency-integrated intensity of the observed ESR transitions. This technique has allowed us to determine precise values of