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Dive into the research topics where John Van Dyke is active.

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Featured researches published by John Van Dyke.


Proceedings of the National Academy of Sciences of the United States of America | 2014

Direct evidence for a magnetic f-electron–mediated pairing mechanism of heavy-fermion superconductivity in CeCoIn5

John Van Dyke; Freek Massee; Milan P. Allan; J. C. Séamus Davis; C. Petrovic; Dirk K. Morr

Significance In heavy-fermion materials, the magnetic moment of an f-electron atom, such as Ce, is screened via the Kondo effect resulting in the splitting of a conventional light band into two heavy bands within few millielectron volts of the Fermi energy. For decades it has been hypothesized that Cooper pairing and superconductivity of the resulting heavy electrons are mediated by the f-electron magnetism. By extracting the magnetic interactions of CeCoIn5 from heavy-fermion scattering interference, and by then predicting quantitatively a variety of characteristics expected for unconventional superconductivity driven by them, we provide direct evidence that the heavy-fermion Cooper pairing in this material is indeed mediated by f-electron magnetism. To identify the microscopic mechanism of heavy-fermion Cooper pairing is an unresolved challenge in quantum matter studies; it may also relate closely to finding the pairing mechanism of high-temperature superconductivity. Magnetically mediated Cooper pairing has long been the conjectured basis of heavy-fermion superconductivity but no direct verification of this hypothesis was achievable. Here, we use a novel approach based on precision measurements of the heavy-fermion band structure using quasiparticle interference imaging to reveal quantitatively the momentum space (k-space) structure of the f-electron magnetic interactions of CeCoIn5. Then, by solving the superconducting gap equations on the two heavy-fermion bands Ekα,β with these magnetic interactions as mediators of the Cooper pairing, we derive a series of quantitative predictions about the superconductive state. The agreement found between these diverse predictions and the measured characteristics of superconducting CeCoIn5 then provides direct evidence that the heavy-fermion Cooper pairing is indeed mediated by f-electron magnetism.


Nature Communications | 2016

Robust upward dispersion of the neutron spin resonance in the heavy fermion superconductor Ce1−xYbxCoIn5

Yu Song; John Van Dyke; I. K. Lum; Benjamin White; Sooyoung Jang; D. Yazici; Lei Shu; A. Schneidewind; Petr Cermak; Y. Qiu; M. B. Maple; Dirk K. Morr; Pengcheng Dai

The neutron spin resonance is a collective magnetic excitation that appears in the unconventional copper oxide, iron pnictide and heavy fermion superconductors. Although the resonance is commonly associated with a spin-exciton due to the d(s±)-wave symmetry of the superconducting order parameter, it has also been proposed to be a magnon-like excitation appearing in the superconducting state. Here we use inelastic neutron scattering to demonstrate that the resonance in the heavy fermion superconductor Ce1−xYbxCoIn5 with x=0, 0.05 and 0.3 has a ring-like upward dispersion that is robust against Yb-doping. By comparing our experimental data with a random phase approximation calculation using the electronic structure and the momentum dependence of the -wave superconducting gap determined from scanning tunnelling microscopy (STM) for CeCoIn5, we conclude that the robust upward-dispersing resonance mode in Ce1−xYbxCoIn5 is inconsistent with the downward dispersion predicted within the spin-exciton scenario.


Physical Review B | 2016

Controlling the flow of spin and charge in nanoscopic topological insulators

John Van Dyke; Dirk K. Morr

Controlling the flow of spin and charge currents in topological insulators (TIs) is a crucial requirement for applications in quantum computation and spin electronics. We demonstrate that such control can be established in nanoscopic two-dimensional TIs by breaking their time-reversal symmetry via magnetic defects. This allows for the creation of nearly fully spin-polarized charge currents, and the design of highly tunable spin diodes. Similar effects can also be realized in mesoscale hybrid structures in which TIs interface with ferro- or antiferromagnets.


Physical Review B | 2017

Orbital superconductivity, defects, and pinned nematic fluctuations in the doped iron chalcogenide FeSe0.45Te0.55

Saheli Sarkar; John Van Dyke; Peter O. Sprau; Freek Massee; U. Welp; Wai-Kwong Kwok; J. C. Séamus Davis; Dirk K. Morr

We demonstrate that the differential conductance, dI/dV , measured via spectroscopic imaging scanning tunneling microscopy in the doped iron chalcogenide FeSe0.45Te0.55, possesses a series of characteristic features that allow one to extract the orbital structure of the superconducting gaps. This yields nearly isotropic superconducting gaps on the two hole-like Fermi surfaces, and a strongly anisotropic gap on the electron-like Fermi surface. Moreover, we show that the pinning of nematic fluctuations by defects can give rise to a dumbbell-like spatial structure of the induced impurity bound states, and explains the related C 2-symmetry in the Fourier transformed differential conductance.


Physical Review B | 2016

Differential conductance and defect states in the heavy-fermion superconductor CeCoIn5.

John Van Dyke; J. C. Séamus Davis; Dirk K. Morr

This is a copy of an article published in Physical Review B.


Physical Review B | 2017

Effects of defects and dephasing on charge and spin currents in two-dimensional topological insulators

John Van Dyke; Dirk K. Morr

Using the non-equilibrium Keldysh Greens function formalism, we investigate the effect of defects on the electronic structure and transport properties of two-dimensional topological insulators (TI). We demonstrate how the spatial flow of charge changes between the topologically protected edge and bulk states and show that elastically and inelastically scattering defects that preserve the time reversal symmetry of the TI lead to qualitatively different effects on the TIs local electronic structure and its transport properties. Moreover, we show that the recently predicted ability to create highly spin-polarized currents by breaking the time-reversal symmetry of the TI via magnetic defects [Phys. Rev. B 93, 081401 (2016)] is robust against the inclusion of a Rashba spin-orbit interaction and the effects of dephasing, and remains unaffected by changes over a wide range of the TIs parameters. We discuss how the sign of the induced spin currents changes under symmetry operations, such as reversal of bias and gate voltages, or spatial reflections. Finally, we show that the insight into the interplay between topology and symmetry of the magnetic defects can be employed for the creation of novel quantum phenomena, such as highly localized magnetic fields inside the TI.


Bulletin of the American Physical Society | 2012

Superconductivity in Heavy Fermion Materials

John Van Dyke; Jeremy Figgins; Dirk K. Morr


Bulletin of the American Physical Society | 2018

Orbital superconductivity, defects and pinned nematic fluctuations in the doped iron chalcogenide FeSe 0.45 Te 0.55.

Saheli Sarkar; John Van Dyke; Peter O. Sprau; Freek Massee; U. Welp; Wai-Kwong Kwok; J. C. Davis; Dirk K. Morr


Bulletin of the American Physical Society | 2017

Robust Upward Dispersion of the Neutron Spin Resonance in the Heavy Fermion Superconductor Ce

Yu Song; John Van Dyke; I. K. Lum; B. D. White; Sooyoung Jang; D. Yazici; Lei Shu; Astrid Schneidewind; Petr Cermak; Y. Qiu; M. B. Maple; Dirk K. Morr; Pengcheng Dai


Bulletin of the American Physical Society | 2017

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John Van Dyke; Guanghua Zhang; Rebecca Flint

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Dirk K. Morr

University of Illinois at Chicago

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I. K. Lum

University of California

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M. B. Maple

University of California

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Y. Qiu

National Institute of Standards and Technology

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Petr Cermak

Forschungszentrum Jülich

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B. D. White

University of California

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