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Dive into the research topics where Jungseek Hwang is active.

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Featured researches published by Jungseek Hwang.


Physical Review Letters | 2010

SQUID-Based Microwave Cavity Search for Dark-Matter Axions

S.J. Asztalos; G. Carosi; C. Hagmann; D. Kinion; K. van Bibber; M. Hotz; L.J. Rosenberg; G. Rybka; J. Hoskins; Jungseek Hwang; P. Sikivie; D. B. Tanner; Richard Bradley; John Clarke

Axions in the microeV mass range are a plausible cold dark-matter candidate and may be detected by their conversion into microwave photons in a resonant cavity immersed in a static magnetic field. We report the first result from such an axion search using a superconducting first-stage amplifier (SQUID) replacing a conventional GaAs field-effect transistor amplifier. This experiment excludes KSVZ dark-matter axions with masses between 3.3 microeV and 3.53 microeV and sets the stage for a definitive axion search utilizing near quantum-limited SQUID amplifiers.


Journal of Applied Physics | 2014

Enhanced ferromagnetic properties in Ho and Ni co-doped BiFeO3 ceramics

J. S. Park; Young Joon Yoo; Jungseek Hwang; J.-H. Kang; B. W. Lee; Y. P. Lee

The magnetic properties of polycrystalline Bi1-xHoxFe1-yNiyO3 (x = 0, 0.1; y = 0, 0.03), which were prepared by the solid-state method, have been investigated. The powder X-ray diffraction reveals that all the samples are polycrystalline and show rhombohedral perovskite structure. The micro-Raman scattering studies confirm that Bi0.9Ho0.1Fe0.97Ni0.03O3 has a compressive lattice distortion induced by the simultaneous substitution of Ho and Ni ions at A and B-sites, respectively. From the magnetization dependences at room temperature, Bi0.9Ho0.1Fe0.97Ni0.03O3 has enhanced magnetization (0.2280 emu/g) and low coercive field (280 Oe). It was revealed that the Ni dopant plays an important role for the improved ferromagnetic properties and the Ho dopant favors the magnetic exchange interactions in the co-doped ceramic.


Physical Review D | 2011

Search for nonvirialized axionic dark matter

J. Hoskins; Jungseek Hwang; C. Martin; P. Sikivie; N. S. Sullivan; D. B. Tanner; M. Hotz; L.J. Rosenberg; G. Rybka; A. Wagner; S.J. Asztalos; G. Carosi; C. Hagmann; D. Kinion; K. van Bibber; Richard Bradley; John Clarke

Cold dark matter in the Milky Way halo may have structure defined by flows with low velocity dispersion. The Axion Dark Matter eXperiment high resolution channel is especially sensitive to axions in such low velocity dispersion flows. Results from a combined power spectra analysis of the high resolution channel axion search are presented along with a discussion of the assumptions underlying such an analysis. We exclude Kim-Shifman-Vainshtein-Zakharov axion dark matter densities of � * 0:2 GeV=cm 3 and Dine-Fischler-Srednicki-Zhitnitskii densities of � * 1:4 GeV=cm 3 over a mass range of ma ¼ 3:3 � eV to 3:69 � eV for models having velocity dispersions of � � & 3 � 10 � 6 .


ACS Nano | 2014

Fully transparent quantum dot light-emitting diode integrated with graphene anode and cathode.

Jung-Tak Seo; Junebeom Han; Taekyung Lim; Ki-Heon Lee; Jungseek Hwang; Heesun Yang; Sanghyun Ju

A fully transparent quantum dot light-emitting diode (QD-LED) was fabricated by incorporating two types (anode and cathode) of graphene-based electrodes, which were controlled in their work functions and sheet resistances. Either gold nanoparticles or silver nanowires were inserted between layers of graphene to control the work function, whereas the sheet resistance was determined by the number of graphene layers. The inserted gold nanoparticles or silver nanowires in graphene films caused a charge transfer and changed the work function to 4.9 and 4.3 eV, respectively, from the original work function (4.5 eV) of pristine graphene. Moreover the sheet resistance values for the anode and cathode electrodes were improved from ∼63,000 to ∼110 Ω/sq and from ∼100,000 to ∼741 Ω/sq as the number of graphene layers increased from 1 to 12 and from 1 to 8, respectively. The main peak wavelength, luminance, current efficiency, and optical transmittance of the fully transparent QD-LED integrated with graphene anode and cathode were 535 nm, ∼358 cd/m2, ∼0.45 cd/A, and 70-80%, respectively. The findings of the study are expected to lay a foundation for the production of high-efficiency, fully transparent, and flexible displays using graphene-based electrodes.


Journal of Applied Physics | 2013

High ferromagnetic transition temperature in multiferroic BiFe0.95Ni0.05O3 compound

Young Joon Yoo; Jungseek Hwang; Y. P. Lee; J. S. Park; J.-H. Kang; J. M. Kim; B. W. Lee; M. S. Seo

We have prepared BiFe0.95Ni0.05O3 by the standard solid-state reaction and rapid sintering. The structural analysis by x-ray diffraction for BiFe0.95Ni0.05O3 shows rhombohedral perovskite structure (R3c), and lattice constants a and c of BiFe0.95Ni0.05O3 are slightly increased as compared to those of BiFeO3. The Raman studies present the increase of oxygen vacancy by the Ni2+ substitution. The magnetic properties of BiFe0.95Ni0.05O3 are greatly improved, owing to the enhanced ferromagnetic interaction caused by the Fe/Ni coupling. BiFe0.95Ni0.05O3 sample is ferromagnetic with a cluster-glass state unlike the antiferromagnetic BiFeO3-based compounds.


Scientific Reports | 2016

Phase transitions via selective elemental vacancy engineering in complex oxide thin films

Sang A Lee; Hoidong Jeong; Sungmin Woo; Jae-Yeol Hwang; Si-Young Choi; Sung-Dae Kim; Minseok Choi; Seulki Roh; Hosung Yu; Jungseek Hwang; Sung Wng Kim; Woo Seok Choi

Defect engineering has brought about a unique level of control for Si-based semiconductors, leading to the optimization of various opto-electronic properties and devices. With regard to perovskite transition metal oxides, O vacancies have been a key ingredient in defect engineering, as they play a central role in determining the crystal field and consequent electronic structure, leading to important electronic and magnetic phase transitions. Therefore, experimental approaches toward understanding the role of defects in complex oxides have been largely limited to controlling O vacancies. In this study, we report on the selective formation of different types of elemental vacancies and their individual roles in determining the atomic and electronic structures of perovskite SrTiO3 (STO) homoepitaxial thin films fabricated by pulsed laser epitaxy. Structural and electronic transitions have been achieved via selective control of the Sr and O vacancy concentrations, respectively, indicating a decoupling between the two phase transitions. In particular, O vacancies were responsible for metal-insulator transitions, but did not influence the Sr vacancy induced cubic-to-tetragonal structural transition in epitaxial STO thin film. The independent control of multiple phase transitions in complex oxides by exploiting selective vacancy engineering opens up an unprecedented opportunity toward understanding and customizing complex oxide thin films.


Physical Review B | 2011

Ultrapure multilayer graphene in bromine-intercalated graphite

Jungseek Hwang; J. P. Carbotte; Sefaattin Tongay; A. F. Hebard; D. B. Tanner

We investigate the optical properties of bromine-intercalated highly orientated pyrolytic graphite (Br-HOPG) and provide an interpretation of the data. We observe absorption features below 620 meV which are absent in the absorption spectrum of graphite. Comparing our results with those of theoretical studies on graphite, single- and bilayer graphene, as well as recent optical studies of multilayer graphene, we conclude that Br-HOPG contains the signatures of ultrapure bilayer graphene, ultrapure single-layer graphene, and graphite. The observed supermetallic conductivity of Br-HOPG is identified with the presence of very high mobility (� 121000 cm 2 V −1 s −1 at room temperature and at very high carrier density), multilayer graphene components in our sample. This could provide an avenue for single- and multilayer graphene research.


Physical Review B | 2011

In situ measurements of the optical absorption of dioxythiophene-based conjugated polymers

Jungseek Hwang; Irina Schwendeman; B. C. Ihas; R. J. Clark; M. Cornick; Maria Nikolou; A. Argun; John R. Reynolds; D. B. Tanner

Conjugated polymers can be reversibly doped by electrochemical means. This doping introduces new sub-bandgap optical absorption bands in the polymer while decreasing the bandgap absorption. To study this behavior, we have prepared an electrochemical cell allowing measurements of the optical properties of the polymer. The cell consists of a thin polymer film deposited on gold-coated Mylar behind which is another polymer that serves as a counterelectrode. An infrared transparent window protects the upper polymer from ambient air. By adding a gel electrolyte and making electrical connections to the polymer-on-gold films, one may study electrochromism in a wide spectral range. As the cell voltage (the potential difference between the two electrodes) changes, the doping level of the conjugated polymer films is changed reversibly. Our experiments address electrochromism in poly(3,4-ethylene-dioxy-thiophene) (PEDOT) and poly(3,4-dimethyl-propylene-dioxy-thiophene) (PProDOT-Me


Synthetic Metals | 2001

Dioxypyrrole and dioxythiophene based conducting polymers : properties and applications

I. Giurgiu; K. Zong; John R. Reynolds; Wei-Po Lee; Keith Richard Brenneman; Alexey Vyacheslavovich Saprigin; Arthur J. Epstein; Jungseek Hwang; D. B. Tanner

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Applied Spectroscopy | 2013

Near-Infrared Studies of Glucose and Sucrose in Aqueous Solutions: Water Displacement Effect and Red Shift in Water Absorption from Water-Solute Interaction

Youngeui Jung; Jungseek Hwang

). This closed electrochemical cell allows the study of the doping induced sub-bandgap features (polaronic and bipolaronic modes) in these easily oxidized and highly redox switchable polymers. We also study the changes in cell spectra as a function of polymer thickness and investigate strategies to obtain cleaner spectra, minimizing the contributions of water and gel electrolyte features.

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D. Kinion

Lawrence Livermore National Laboratory

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G. Carosi

Lawrence Livermore National Laboratory

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G. Rybka

University of Washington

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K. van Bibber

University of California

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L.J. Rosenberg

Lawrence Livermore National Laboratory

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M. Hotz

University of Washington

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Richard Bradley

National Radio Astronomy Observatory

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S.J. Asztalos

Massachusetts Institute of Technology

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