Unconventional pairing in single FeSe layers
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July 2019 |
Superconducting Gap Anisotropy in Monolayer FeSe Thin Film
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September 2016 |
Interface-induced superconductivity and strain-dependent spin density waves in FeSe/SrTiO3 thin films
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May 2013 |
What makes the Tc of monolayer FeSe on SrTiO3 so high: a sign-problem-free quantum Monte Carlo study
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June 2016 |
Constrained sampling method for analytic continuation
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December 2016 |
Fragility of Charge Order Near an Antiferromagnetic Quantum Critical Point
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June 2018 |
Superconductivity above 100 K in single-layer FeSe films on doped SrTiO3
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November 2014 |
Coexistence of superconductivity and antiferromagnetism in (Li0.8Fe0.2)OHFeSe
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December 2014 |
Interface-Induced High-Temperature Superconductivity in Single Unit-Cell FeSe Films on SrTiO 3
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March 2012 |
Charge Order in the Holstein Model on a Honeycomb Lattice
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February 2019 |
Diagrammatic determinantal quantum Monte Carlo methods: Projective schemes and applications to the Hubbard-Holstein model
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July 2007 |
Charge-Density-Wave Transitions of Dirac Fermions Coupled to Phonons
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February 2019 |
Superconductivity dichotomy in K-coated single and double unit cell FeSe films on
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November 2015 |
Onset of the Meissner effect at 65 K in FeSe thin film grown on Nb-doped SrTiO 3 substrate
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July 2015 |
Competition Between Antiferromagnetic and Charge-Density-Wave Order in the Half-Filled Hubbard-Holstein Model
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December 2012 |
On the origin of the shallow and “replica” bands in FeSe monolayer superconductors
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March 2017 |
Routes to High-Temperature Superconductivity: A Lesson from FeSe/SrTiO 3
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March 2018 |
Phase diagram and electronic indication of high-temperature superconductivity at 65 K in single-layer FeSe films
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May 2013 |
Interfacial mode coupling as the origin of the enhancement of Tc in FeSe films on SrTiO3
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November 2014 |
Phonon Dispersion and the Competition between Pairing and Charge Order
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May 2018 |
Enhanced superconductivity due to forward scattering in FeSe thin films on SrTiO 3 substrates
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February 2016 |
Giant LO-TO splittings in perovskite ferroelectrics
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May 1994 |
Itinerant quantum critical point with frustration and a non-Fermi liquid
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July 2018 |
Evidence of cooperative effect on the enhanced superconducting transition temperature at the FeSe/SrTiO3 interface
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February 2019 |
Common electronic origin of superconductivity in (Li,Fe)OHFeSe bulk superconductor and single-layer FeSe/SrTiO3 films
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February 2016 |
Superconductivity and nematic fluctuations in a model of doped FeSe monolayers: Determinant quantum Monte Carlo study
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October 2016 |
Split Orthogonal Group: A Guiding Principle for Sign-Problem-Free Fermionic Simulations
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December 2015 |
Electron Phonon Coupling versus Photoelectron Energy Loss at the Origin of Replica Bands in Photoemission of FeSe on SrTiO 3
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June 2018 |
Ising Nematic Quantum Critical Point in a Metal: A Monte Carlo Study
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August 2016 |
Two-dimensional Holstein-Hubbard model: Critical temperature, Ising universality, and bipolaron liquid
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August 2018 |
Sign-Problem-Free Quantum Monte Carlo of the Onset of Antiferromagnetism in Metals
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December 2012 |
Solving the fermion sign problem in quantum Monte Carlo simulations by Majorana representation
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June 2015 |
Quasiparticle properties of the nonlinear Holstein model at finite doping and temperature
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August 2015 |
Sign-Problem-Free Fermionic Quantum Monte Carlo: Developments and Applications
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March 2019 |
Sufficient condition for absence of the sign problem in the fermionic quantum Monte Carlo algorithm
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April 2005 |
The electron–phonon interaction with forward scattering peak is dominant in high T c superconductors of FeSe films on ${{\rm{SrTiO}}}_{3}$ (TiO 2 )
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January 2017 |
Charge-density-wave and pairing susceptibilities in a two-dimensional electron-phonon model
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February 1991 |
Pseudogap crossover in the electron-phonon system
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May 2019 |
Symmetry-enforced self-learning Monte Carlo method applied to the Holstein model
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July 2018 |
Non-Fermi Liquid at ( ) Ferromagnetic Quantum Critical Point
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September 2017 |
Tuning the band structure and superconductivity in single-layer FeSe by interface engineering
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September 2014 |
What makes the T c of FeSe/SrTiO 3 so high?
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November 2015 |
A Novel Technique for the Simulation of Interacting Fermion Systems
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April 1989 |
Majorana Positivity and the Fermion Sign Problem of Quantum Monte Carlo Simulations
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June 2016 |
Majorana-Time-Reversal Symmetries: A Fundamental Principle for Sign-Problem-Free Quantum Monte Carlo Simulations
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December 2016 |
Competing Orders in a Nearly Antiferromagnetic Metal
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August 2016 |
Phonon linewidth due to electron-phonon interactions with strong forward scattering in FeSe thin films on oxide substrates
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August 2017 |
Electronic origin of high-temperature superconductivity in single-layer FeSe superconductor
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January 2012 |
Dipolar phonons and electronic screening in monolayer FeSe on
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August 2017 |
Charge transfer and electron-phonon coupling in monolayer FeSe on Nb-doped
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June 2016 |
Renormalization of spectra by phase competition in the half-filled Hubbard-Holstein model
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April 2015 |
Role of phonon penetrating into thin FeSe films in the enhancement of superconductivity
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August 2016 |
Monolayer FeSe on SrTiO 3
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journal
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March 2017 |
Stochastic method for analytic continuation of quantum Monte Carlo data
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May 1998 |
Nature of the effective interaction in electron-doped cuprate superconductors: A sign-problem-free quantum Monte Carlo study
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June 2017 |
Interface induced high temperature superconductivity in single unit-cell FeSe films on SrTiO3
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text
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January 2012 |
Electronic Origin of High Temperature Superconductivity in Single-Layer FeSe Superconductor
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text
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January 2012 |
Sign-problem-free quantum Monte Carlo of the onset of antiferromagnetism in metals
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text
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January 2012 |
Interfacial mode coupling as the origin of the enhancement of Tc in FeSe films on SrTiO3
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text
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January 2013 |
Renormalization of spectra by phase competition in the half-filled Hubbard-Holstein model
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text
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January 2015 |
Constrained sampling method for analytic continuation
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text
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January 2015 |
Common Electronic Origin of Superconductivity in (Li,Fe)OHFeSe Bulk Superconductor and Single-Layer FeSe/SrTiO3 Films
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text
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January 2015 |
Onset of the Meissner effect at 65 K in FeSe thin film grown on Nb doped SrTiO3 substrate
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text
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January 2015 |
What makes the Tc of monolayer FeSe on SrTiO3 so high: a sign-problem-free quantum Monte Carlo study
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text
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January 2015 |
Superconducting gap anisotropy in monolayer FeSe thin film
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text
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January 2015 |
Majorana Positivity and the Fermion sign problem of Quantum Monte Carlo Simulations
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text
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January 2016 |
Majorana-time-reversal symmetries: a fundamental principle for sign-problem-free quantum Monte Carlo simulations
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text
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January 2016 |
Phonon linewidth due to electron-phonon interactions with strong forward scattering in FeSe thin films on oxide substrates
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text
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January 2017 |
Monolayer FeSe on SrTiO$_3$
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text
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January 2017 |
Itinerant quantum critical point with frustration and non-Fermi-liquid
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text
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January 2017 |
Charge Order in the Holstein Model on a Honeycomb Lattice
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text
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January 2018 |
A sufficient condition for the absence of the sign problem in the fermionic quantum Monte-Carlo algorithm
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text
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January 2004 |