Jin-Kwang Kim
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Jin-Kwang Kim has a total of 61 co-authors. Here are the top co-authors by number of shared publications:
- Jungho Kim
Argonne National Laboratory
6 shared publications B. J. Kim
Pohang University of Science and Technology
4 shared publications- Bumjoon Kim
Department of Physics, Pohang University of Science and Technology, Pohang, South Korea
4 shared publications - Jimin Kim
Center for Artificial Low Dimensional Electronic Systems, Institute for Basic Science (IBS), Pohang, South Korea
4 shared publications - Hoon Kim
Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Korea
3 shared publications Sunwook Park
Center for Artificial Low Dimensional Electronic Systems, Institute for Basic Science (IBS), 77 Cheongam-Ro, Pohang 37673, South Korea
3 shared publications
Latest Publications
- 2 November 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 114 (27) , 274401
Pressure-driven evolution of magnetic excitations in Sr 3 Ir 2 O 7
The easy $c$-axis collinear antiferromagnetic order of the bilayer square-lattice iridate ${\mathrm{Sr}}_{3}{\mathrm{Ir}}_{2}{\mathrm{O}}_{7}$ has motivated a diverse range of microscopic models. A previous high-pressure Raman study suggested a magnetic phase transition near 15 GPa at low temperatures, but the fundamental nature of this transition has remained unclear. Here, we utilize high-pressure resonant inelastic x-ray scattering, x-ray absorption spectroscopy (XAS), and x-ray magnetic circular dichroism (XMCD) to directly probe the evolution of magnetic excitations in ${\mathrm{Sr}}_{3}{\mathrm{Ir}}_{2}{\mathrm{O}}_{7}$ under compression. We identify three distinct pressure regimes. At low pressures, the system hosts a well-defined magnon characteristic of long-range antiferromagnetic order. Beyond a characteristic pressure, the magnon broadens substantially while its energy continues to harden, marking a crossover into a heavily damped paramagnon regime. Upon further compression, the paramagnon spectral weight is fully suppressed at a distinct second boundary. Both the crossover and the phase boundary exhibit a pronounced temperature dependence, shifting to higher pressures at lower temperatures. The crossover pressure lies near the previously identified Raman transition, whereas the second boundary extends beyond 22.5 GPa at 33 K. Throughout the explored pressure-temperature phase space, XAS and XMCD spectra reveal no discernible changes, ruling out any substantial departure from the ${J}_{\mathrm{eff}}=1/2$ state or a transition to an alternative magnetic configuration such as a spin-flip phase. We discuss these findings in the context of the competing microscopic models for magnetism in ${\mathrm{Sr}}_{3}{\mathrm{Ir}}_{2}{\mathrm{O}}_{7}$.- 2 November 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 114 (27) , 274401
Pressure-driven evolution of magnetic excitations in Sr 3 Ir 2 O 7
The easy $c$-axis collinear antiferromagnetic order of the bilayer square-lattice iridate ${\mathrm{Sr}}_{3}{\mathrm{Ir}}_{2}{\mathrm{O}}_{7}$ has motivated a diverse range of microscopic models. A previous high-pressure Raman study suggested a magnetic phase transition near 15 GPa at low temperatures, but the fundamental nature of this transition has remained unclear. Here, we utilize high-pressure resonant inelastic x-ray scattering, x-ray absorption spectroscopy (XAS), and x-ray magnetic circular dichroism (XMCD) to directly probe the evolution of magnetic excitations in ${\mathrm{Sr}}_{3}{\mathrm{Ir}}_{2}{\mathrm{O}}_{7}$ under compression. We identify three distinct pressure regimes. At low pressures, the system hosts a well-defined magnon characteristic of long-range antiferromagnetic order. Beyond a characteristic pressure, the magnon broadens substantially while its energy continues to harden, marking a crossover into a heavily damped paramagnon regime. Upon further compression, the paramagnon spectral weight is fully suppressed at a distinct second boundary. Both the crossover and the phase boundary exhibit a pronounced temperature dependence, shifting to higher pressures at lower temperatures. The crossover pressure lies near the previously identified Raman transition, whereas the second boundary extends beyond 22.5 GPa at 33 K. Throughout the explored pressure-temperature phase space, XAS and XMCD spectra reveal no discernible changes, ruling out any substantial departure from the ${J}_{\mathrm{eff}}=1/2$ state or a transition to an alternative magnetic configuration such as a spin-flip phase. We discuss these findings in the context of the competing microscopic models for magnetism in ${\mathrm{Sr}}_{3}{\mathrm{Ir}}_{2}{\mathrm{O}}_{7}$.- 13 December 2023
- Published by Springer Nature in Nature
- Vol. 625 (7994) , 264-269
Quantum spin nematic phase in a square-lattice iridate
Spin nematic is a magnetic analogue of classical liquid crystals, a fourth state of matter exhibiting characteristics of both liquid and solid1,2. Particularly intriguing is a valence-bond spin nematic3,4,5, in which spins are quantum entangled to form a multipolar order without breaking time-reversal symmetry, but its unambiguous experimental realization remains elusive. Here we establish a spin nematic phase in the square-lattice iridate Sr2IrO4, which approximately realizes a pseudospin one-half Heisenberg antiferromagnet in the strong spin–orbit coupling limit6,7,8,9. Upon cooling, the transition into the spin nematic phase at TC ≈ 263 K is marked by a divergence in the static spin quadrupole susceptibility extracted from our Raman spectra and concomitant emergence of a collective mode associated with the spontaneous breaking of rotational symmetries. The quadrupolar order persists in the antiferromagnetic phase below TN ≈ 230 K and becomes directly observable through its interference with the antiferromagnetic order in resonant X-ray diffraction, which allows us to uniquely determine its spatial structure. Further, we find using resonant inelastic X-ray scattering a complete breakdown of coherent magnon excitations at short-wavelength scales, suggesting a many-body quantum entanglement in the antiferromagnetic state10,11. Taken together, our results reveal a quantum order underlying the Néel antiferromagnet that is widely believed to be intimately connected to the mechanism of high-temperature superconductivity12,13.
- 13 December 2023
- Published by Springer Nature in Nature
- Vol. 625 (7994) , 264-269
Quantum spin nematic phase in a square-lattice iridate
Spin nematic is a magnetic analogue of classical liquid crystals, a fourth state of matter exhibiting characteristics of both liquid and solid1,2. Particularly intriguing is a valence-bond spin nematic3,4,5, in which spins are quantum entangled to form a multipolar order without breaking time-reversal symmetry, but its unambiguous experimental realization remains elusive. Here we establish a spin nematic phase in the square-lattice iridate Sr2IrO4, which approximately realizes a pseudospin one-half Heisenberg antiferromagnet in the strong spin–orbit coupling limit6,7,8,9. Upon cooling, the transition into the spin nematic phase at TC ≈ 263 K is marked by a divergence in the static spin quadrupole susceptibility extracted from our Raman spectra and concomitant emergence of a collective mode associated with the spontaneous breaking of rotational symmetries. The quadrupolar order persists in the antiferromagnetic phase below TN ≈ 230 K and becomes directly observable through its interference with the antiferromagnetic order in resonant X-ray diffraction, which allows us to uniquely determine its spatial structure. Further, we find using resonant inelastic X-ray scattering a complete breakdown of coherent magnon excitations at short-wavelength scales, suggesting a many-body quantum entanglement in the antiferromagnetic state10,11. Taken together, our results reveal a quantum order underlying the Néel antiferromagnet that is widely believed to be intimately connected to the mechanism of high-temperature superconductivity12,13.
- Open Access
- 22 March 2023
- Published by International Union of Crystallography (IUCr) in Journal of Synchrotron Radiation
- Vol. 30 (3) , 643-649
Resonant inelastic X-ray scattering endstation at the 1C beamline of Pohang Light Source II
An endstation for resonant inelastic X-ray scattering (RIXS), dedicated to operations in the hard X-ray regime, has been constructed at the 1C beamline of Pohang Light Source II. At the Ir L 3-edge, a total energy resolution of 34.2 meV was achieved, close to the theoretical estimation of 34.0 meV, which considers factors such as the incident energy bandpass, intrinsic analyzer resolution, geometrical broadening of the spectrometer, finite beam-size effect and Johann aberration. The performance of the RIXS instrument is demonstrated by measuring the RIXS spectra of Sr2IrO4. The endstation can be easily reconfigured to measure energy-integrated intensities with very low background for diffuse scattering and diffraction experiments.
- 22 March 2023
- Published by International Union of Crystallography (IUCr) in Journal of Synchrotron Radiation
- Vol. 30 (3) , 643-649
Open AccessResonant inelastic X-ray scattering endstation at the 1C beamline of Pohang Light Source II
An endstation for resonant inelastic X-ray scattering (RIXS), dedicated to operations in the hard X-ray regime, has been constructed at the 1C beamline of Pohang Light Source II. At the Ir L 3-edge, a total energy resolution of 34.2 meV was achieved, close to the theoretical estimation of 34.0 meV, which considers factors such as the incident energy bandpass, intrinsic analyzer resolution, geometrical broadening of the spectrometer, finite beam-size effect and Johann aberration. The performance of the RIXS instrument is demonstrated by measuring the RIXS spectra of Sr2IrO4. The endstation can be easily reconfigured to measure energy-integrated intensities with very low background for diffuse scattering and diffraction experiments.
- 12 October 2022
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 6 (10) , 103401
Single crystal growth of iridates without platinum impurities
Iridates have attracted much interest in the last decade for their novel magnetism emerging in the limit of strong spin-orbit coupling and possible unconventional superconductivity. A standard for growing iridate single crystals has been the flux method using platinum crucibles. Here, we show that this widely used method compromises the sample quality by inclusion of platinum impurities. We find that single crystals grown in iridium crucibles show remarkable differences from those grown in platinum crucibles in their sample characterizations using Raman spectroscopy, resistivity, magnetization, optical third harmonic generation, resonant x-ray diffraction, and resonant inelastic x-ray scattering measurements. In particular, we show that several peaks of sizable intensities disappear in the Raman spectra of samples free of platinum impurities, and a significantly larger activation energy is extracted from the resistivity data compared to previously reported values. Furthermore, we find no evidence of the previously reported glide-symmetry-breaking structural distortions and confirm the space group of the lattice symmetry. Although the platinum impurities are not apparent in the magnetic properties and thus went unnoticed in the stoichiometric insulating phase for a long time, their effects can be much more detrimental to transport properties in chemically doped compounds. Therefore, our result suggests using growth methods that avoid platinum impurities for an investigation of the intrinsic physical properties of iridates, and possible superconducting phases.- 12 October 2022
- Published by American Physical Society (APS) in Physical Review Materials
- Vol. 6 (10) , 103401
Single crystal growth of iridates without platinum impurities
Iridates have attracted much interest in the last decade for their novel magnetism emerging in the limit of strong spin-orbit coupling and possible unconventional superconductivity. A standard for growing iridate single crystals has been the flux method using platinum crucibles. Here, we show that this widely used method compromises the sample quality by inclusion of platinum impurities. We find that single crystals grown in iridium crucibles show remarkable differences from those grown in platinum crucibles in their sample characterizations using Raman spectroscopy, resistivity, magnetization, optical third harmonic generation, resonant x-ray diffraction, and resonant inelastic x-ray scattering measurements. In particular, we show that several peaks of sizable intensities disappear in the Raman spectra of samples free of platinum impurities, and a significantly larger activation energy is extracted from the resistivity data compared to previously reported values. Furthermore, we find no evidence of the previously reported glide-symmetry-breaking structural distortions and confirm the space group of the lattice symmetry. Although the platinum impurities are not apparent in the magnetic properties and thus went unnoticed in the stoichiometric insulating phase for a long time, their effects can be much more detrimental to transport properties in chemically doped compounds. Therefore, our result suggests using growth methods that avoid platinum impurities for an investigation of the intrinsic physical properties of iridates, and possible superconducting phases.- Open Access
Single crystal growth of iridates without platinum impurities
Iridates have attracted much interest in the last decade for their novel magnetism emerging in the limit of strong spin-orbit coupling and possible unconventional superconductivity. A standard for growing iridate single crystals has been the flux method using platinum crucibles. Here, we show that this widely used method compromises the sample quality by inclusion of platinum impurities. We find that Sr2IrO4 single crystals grown in iridium crucibles show remarkable differences from those grown in platinum crucibles in their sample characterizations using Raman spectroscopy, resistivity, magnetization, optical third harmonic generation, resonant X-ray diffraction, and resonant inelastic X-ray scattering measurements. In particular, we show that several peaks of sizable intensities disappear in the Raman spectra of samples free of platinum impurities, and a significantly larger activation energy is extracted from the resistivity data compared to previously reported values. Furthermore, we find no evidence of the previously reported glide symmetry breaking structural distortions and confirm the I41/acd space group of the lattice symmetry. Although the platinum impurities are not apparent in the magnetic properties and thus went unnoticed in the stoichiometric insulating phase for a long time, their effects can be much more detrimental to transport properties in chemically doped compounds. Therefore, our result suggests using growth methods that avoid platinum impurities for an investigation of intrinsic physical properties of iridates, and possible superconducting phases.
Open AccessSingle crystal growth of iridates without platinum impurities
Iridates have attracted much interest in the last decade for their novel magnetism emerging in the limit of strong spin-orbit coupling and possible unconventional superconductivity. A standard for growing iridate single crystals has been the flux method using platinum crucibles. Here, we show that this widely used method compromises the sample quality by inclusion of platinum impurities. We find that Sr2IrO4 single crystals grown in iridium crucibles show remarkable differences from those grown in platinum crucibles in their sample characterizations using Raman spectroscopy, resistivity, magnetization, optical third harmonic generation, resonant X-ray diffraction, and resonant inelastic X-ray scattering measurements. In particular, we show that several peaks of sizable intensities disappear in the Raman spectra of samples free of platinum impurities, and a significantly larger activation energy is extracted from the resistivity data compared to previously reported values. Furthermore, we find no evidence of the previously reported glide symmetry breaking structural distortions and confirm the I41/acd space group of the lattice symmetry. Although the platinum impurities are not apparent in the magnetic properties and thus went unnoticed in the stoichiometric insulating phase for a long time, their effects can be much more detrimental to transport properties in chemically doped compounds. Therefore, our result suggests using growth methods that avoid platinum impurities for an investigation of intrinsic physical properties of iridates, and possible superconducting phases.
- Open Access
- 20 January 2022
- Published by American Physical Society (APS) in Physical Review X
- Vol. 12 (1) , 011013
Ultrafast Renormalization of the On-Site Coulomb Repulsion in a Cuprate Superconductor
Ultrafast lasers are an increasingly important tool to control and stabilize emergent phases in quantum materials. Among a variety of possible excitation protocols, a particularly intriguing route is the direct light engineering of microscopic electronic parameters, such as the electron hopping and the local Coulomb repulsion (Hubbard ). In this work, we use time-resolved x-ray absorption spectroscopy to demonstrate the light-induced renormalization of the Hubbard in a cuprate superconductor, . We show that intense femtosecond laser pulses induce a substantial redshift of the upper Hubbard band while leaving the Zhang-Rice singlet energy unaffected. By comparing the experimental data to time-dependent spectra of single- and three-band Hubbard models, we assign this effect to an approximately 140-meV reduction of the on-site Coulomb repulsion on the copper sites. Our demonstration of a dynamical Hubbard renormalization in a copper oxide paves the way to a novel strategy for the manipulation of superconductivity and magnetism as well as to the realization of other long-range-ordered phases in light-driven quantum materials.- 20 January 2022
- Published by American Physical Society (APS) in Physical Review X
- Vol. 12 (1) , 011013
Open AccessUltrafast Renormalization of the On-Site Coulomb Repulsion in a Cuprate Superconductor
Ultrafast lasers are an increasingly important tool to control and stabilize emergent phases in quantum materials. Among a variety of possible excitation protocols, a particularly intriguing route is the direct light engineering of microscopic electronic parameters, such as the electron hopping and the local Coulomb repulsion (Hubbard ). In this work, we use time-resolved x-ray absorption spectroscopy to demonstrate the light-induced renormalization of the Hubbard in a cuprate superconductor, . We show that intense femtosecond laser pulses induce a substantial redshift of the upper Hubbard band while leaving the Zhang-Rice singlet energy unaffected. By comparing the experimental data to time-dependent spectra of single- and three-band Hubbard models, we assign this effect to an approximately 140-meV reduction of the on-site Coulomb repulsion on the copper sites. Our demonstration of a dynamical Hubbard renormalization in a copper oxide paves the way to a novel strategy for the manipulation of superconductivity and magnetism as well as to the realization of other long-range-ordered phases in light-driven quantum materials. - 27 May 2020
- Published by International Union of Crystallography (IUCr) in Journal of Synchrotron Radiation
- Vol. 27 (4) , 963-969
Montel mirror based collimating analyzer system for high-pressure resonant inelastic X-ray scattering experiments
Resonant inelastic X-ray scattering (RIXS) is increasingly playing a significant role in studying highly correlated systems, especially since it was proven capable of measuring low-energy magnetic excitations. However, despite high expectations for experimental evidence of novel magnetic phases at high pressure, unequivocal low-energy spectral signatures remain obscured by extrinsic scattering from material surrounding the sample in a diamond anvil cell (DAC): pressure media, Be gasket and the diamond anvils themselves. A scattered X-ray collimation based medium-energy resolution (∼100 meV) analyzer system for a RIXS spectrometer at the Ir L 3-absorption edge has been designed and built to remediate these difficulties. Due to the confocal nature of the analyzer system, the majority of extrinsic scattering is rejected, yielding a clean low-energy excitation spectrum of an iridate Sr2IrO4 sample in a DAC cell. Furthermore, the energy resolution of different configurations of the collimating and analyzing optics are discussed.
- 27 May 2020
- Published by International Union of Crystallography (IUCr) in Journal of Synchrotron Radiation
- Vol. 27 (4) , 963-969
Montel mirror based collimating analyzer system for high-pressure resonant inelastic X-ray scattering experiments
Resonant inelastic X-ray scattering (RIXS) is increasingly playing a significant role in studying highly correlated systems, especially since it was proven capable of measuring low-energy magnetic excitations. However, despite high expectations for experimental evidence of novel magnetic phases at high pressure, unequivocal low-energy spectral signatures remain obscured by extrinsic scattering from material surrounding the sample in a diamond anvil cell (DAC): pressure media, Be gasket and the diamond anvils themselves. A scattered X-ray collimation based medium-energy resolution (∼100 meV) analyzer system for a RIXS spectrometer at the Ir L 3-absorption edge has been designed and built to remediate these difficulties. Due to the confocal nature of the analyzer system, the majority of extrinsic scattering is rejected, yielding a clean low-energy excitation spectrum of an iridate Sr2IrO4 sample in a DAC cell. Furthermore, the energy resolution of different configurations of the collimating and analyzing optics are discussed.
- Open Access
- 23 March 2020
- Published by American Physical Society (APS) in Physical Review B
- Vol. 101 (9) , 094428
Spin-wave gap collapse in Rh-dopedWe use resonant inelastic x-ray scattering (RIXS) at the Ir edge to study the effect of hole doping upon the Mott-insulating state in , via Rh replacement of the Ir site. The spin-wave gap, associated with XY-type spin-exchange anisotropy, collapses with increasing Rh content, prior to the suppression of the Mott-insulating state and in contrast to electron doping via La substitution of the Sr site. At the same time, despite heavy damping, the excitation spectra retain their overall amplitude and dispersion character. A careful study of the spin-wave spectrum reveals that deviations from the Heisenberg used to model the pristine system disappear at intermediate doping levels. These findings are interpreted in terms of a modulation of Ir-Ir correlations due to the influence of Rh impurities upon nearby Ir wave functions, even as the single-band model remains valid up to full carrier delocalization. They underline the importance of the transition metal site symmetry when doping pseudospin systems such as .- 23 March 2020
- Published by American Physical Society (APS) in Physical Review B
- Vol. 101 (9) , 094428
Open AccessSpin-wave gap collapse in Rh-dopedWe use resonant inelastic x-ray scattering (RIXS) at the Ir edge to study the effect of hole doping upon the Mott-insulating state in , via Rh replacement of the Ir site. The spin-wave gap, associated with XY-type spin-exchange anisotropy, collapses with increasing Rh content, prior to the suppression of the Mott-insulating state and in contrast to electron doping via La substitution of the Sr site. At the same time, despite heavy damping, the excitation spectra retain their overall amplitude and dispersion character. A careful study of the spin-wave spectrum reveals that deviations from the Heisenberg used to model the pristine system disappear at intermediate doping levels. These findings are interpreted in terms of a modulation of Ir-Ir correlations due to the influence of Rh impurities upon nearby Ir wave functions, even as the single-band model remains valid up to full carrier delocalization. They underline the importance of the transition metal site symmetry when doping pseudospin systems such as . - 1 August 2017
- Published by Elsevier in Journal of Magnetism and Magnetic Materials
- Vol. 435, 126-135
Magnetism on quasi-1-D lattices in novel non-centrosymmetric Ba 3 CrVS 4 O 3 and in centrosymmetric La 3 TM WS 3 O 6 ( TM = Cr, Fe, Co)
- 1 August 2017
- Published by Elsevier in Journal of Magnetism and Magnetic Materials
- Vol. 435, 126-135
Magnetism on quasi-1-D lattices in novel non-centrosymmetric Ba 3 CrVS 4 O 3 and in centrosymmetric La 3 TM WS 3 O 6 ( TM = Cr, Fe, Co)