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  <title>Repository Collection:</title>
  <link rel="alternate" href="https://scholar.gist.ac.kr/handle/local/7935" />
  <subtitle />
  <id>https://scholar.gist.ac.kr/handle/local/7935</id>
  <updated>2026-09-12T14:57:59Z</updated>
  <dc:date>2026-09-12T14:57:59Z</dc:date>
  <entry>
    <title>Understanding Charge Density Wave Phase Transition in 1T-TaS2 via Machine Learning Force Field</title>
    <link rel="alternate" href="https://scholar.gist.ac.kr/handle/local/31976" />
    <author>
      <name>Koh, Kahyeon</name>
    </author>
    <id>https://scholar.gist.ac.kr/handle/local/31976</id>
    <updated>2025-09-08T02:51:18Z</updated>
    <published>2024-12-31T15:00:00Z</published>
    <summary type="text">Title: Understanding Charge Density Wave Phase Transition in 1T-TaS2 via Machine Learning Force Field
Author(s): Koh, Kahyeon
Abstract: Recently, the charge density wave (CDW) phases and their properties in various condensed matter systems have been widely studied. In condensed matter, the formation of CDWs and periodic lattice distortions leads to changes in the electronic transport properties. Among these materials, 1T-type tantalum disulfide (1T-TaS2) is a layered material, and its CDW phases indicate a two-step phase transition depending on thickness and temperature. Experimental studies have shown that its physical properties depend on the stacking order of its layers, which affects the CDW phase transitions. However, due to its strong correlation between electronic structure and complex atomic geometry, understanding the CDW phase transition in 1T-TaS2 is challenging from a theoretical perspective. In this study, we investigated the tendency for structural change from molecular dynamics (MD) with the machine learning force field (MLFF), to simulate multiscale dynamics. We extracted a MLFF for a 1T-TaS2 monolayer based on Ab Initio Molecular Dynamics (AIMD) simulation training data on an Angstrom scale. Using this MLFF in MD simulations, we performed large-scale (∼&lt; 100 nm^2) and long-time (∼&lt; ns) simulations of temperature-dependent dynamics. Through these simulations, we discovered CDW phase transitions and domain wall formations at various temperatures and times, and analyzed their atomic composition. Our results not only theoretically predicted the temperature-dependent bulk CDW phase transition of 1T-TaS2, but also observed microscopic dynamics. This suggests that it will provide explanations consistent with previous experimental results. In future studies, our MLFF approach methodology could be applied to investigate bulk 1T-TaS2. Moreover, our findings may contribute to future studies that analyze light-induced hidden phases in 1T-TaS2 in detail, and could be extended to understand CDW phase transitions in other materials.</summary>
    <dc:date>2024-12-31T15:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Traversable wormhole and quantum teleportation</title>
    <link rel="alternate" href="https://scholar.gist.ac.kr/handle/local/19859" />
    <author>
      <name>Yeong Han Park</name>
    </author>
    <id>https://scholar.gist.ac.kr/handle/local/19859</id>
    <updated>2025-06-30T12:12:20Z</updated>
    <published>2022-12-31T15:00:00Z</published>
    <summary type="text">Title: Traversable wormhole and quantum teleportation
Author(s): Yeong Han Park
Abstract: The quantum informative aspect of holographic principle incorporated with the ER$=$EPR conjecture suggests the dual geometry for an entangled thermofield double state is a non-traversable wormhole and recent studies have shown its traversability is governed by a non-local coupling of two boundaries. In the paper, we elaborate on the principle and the method on the wormhole opening and the signal teleportation for the supplementation of the duality including the formulation of double trace deformations and boundary conditions in the context of AdS/CFT correspondence. We also give proposals for further generalizing and resolving the dual configurations regarding several issues and subtleties.</summary>
    <dc:date>2022-12-31T15:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Time-of-flight measurements of deuterium ions and neutrons produced from laser-cluster fusion plasmas</title>
    <link rel="alternate" href="https://scholar.gist.ac.kr/handle/local/32669" />
    <author>
      <name>Jaehyun Song</name>
    </author>
    <id>https://scholar.gist.ac.kr/handle/local/32669</id>
    <updated>2025-12-30T12:01:00Z</updated>
    <published>2018-12-31T15:00:00Z</published>
    <summary type="text">Title: Time-of-flight measurements of deuterium ions and neutrons produced from laser-cluster fusion plasmas
Author(s): Jaehyun Song
Abstract: Previous studies have shown that, by irradiating deuterium containing clusters with intense laser pulses, one can generate deuterium ions energetic enough to create nuclear fusion reactions. The rate of DD fusion reactions increases with the relative velocity of the colliding ions. Therefore, measuring the ion temperature of fusion plasmas is essential for fusion research. We produced deuterium clusters with a high pressure (~50 bar), cryo-cooled (~87 K) deuterium gas using a supersonic nozzle with an orifice diameter of 0.79 mm and an expansion half angle of 5˚. We irradiated the cluster targets with intense laser pulses (10^16-10^18  Wcm^(-2)) and produced deuterium fusion plasmas. The average radius of deuterium clusters was about 10 nm based on our Rayleigh scattering measurements. We have designed and built our own neutron detectors to measure the fusion yields. We confirmed the production of 2.45 MeV fusion neutrons from the plasma using neutron time-of-flight technique. We have also built ion detectors using micro-channel plates, and have measured the time-of-flight of deuterium ions originating from the plasma. Our ion time-of-flight signals indicate that we produced deuterium plasmas with temperatures as high as 14 keV from the experiment. The yields of energetic deuterium ions and 2.45 MeV fusion neutrons are estimated to be 10^14 ions per shot and 10^5 neutrons per shot, respectively.</summary>
    <dc:date>2018-12-31T15:00:00Z</dc:date>
  </entry>
  <entry>
    <title>The quantum paraelectricity of perovskite oxides from first-principle calculation</title>
    <link rel="alternate" href="https://scholar.gist.ac.kr/handle/local/19817" />
    <author>
      <name>Lym, Yongsik</name>
    </author>
    <id>https://scholar.gist.ac.kr/handle/local/19817</id>
    <updated>2025-06-30T12:11:22Z</updated>
    <published>2023-12-31T15:00:00Z</published>
    <summary type="text">Title: The quantum paraelectricity of perovskite oxides from first-principle calculation
Author(s): Lym, Yongsik
Abstract: Perovskites have been widely utilized in various applications due to their ability to transition into
different phases such as ferroelectricity, ferromagnetism, and superconductivity, depending on external
conditions. A new class of phase known as quantum paraelectricity (QPE) has been discovered,
which do not undergo phase transitions even at low temperatures away from conventional ferroelectric
materials. The underlying cause of this behavior is attributed to quantum fluctuations occurring at
low temperature, and extensive research is being conducted to microscopically elucidate the properties
of QPE in terms of quantum fluctuation. A representative study is proceeded in the SrTiO3 by
highlighting the interaction between lattice elongation and ferroelectric soft modes based on the first
principle calculations.
  In our research, we investigated QPE behavior in the specific perovskite oxides, such as KTaO3
and EuTiO3, and aimed to unravel the nature of QPE behavior. For this, we first studied the methodology
of the aforementioned study on SrTiO3 to verify our numerical configurations, and then applied
the methodology to our chosen QPE candidates (KTaO3 and EuTiO3). The specific methodology
involved the following steps: We used four functionals (LDA, PBE, PBEsol, HSE06) to find the one
that best describes the ferroelectric soft mode. For this, we performed DFPT (Density Functional
Perturbation Theory) and then confirmed whether these methods achieved an unstable equilibrium
at the equilibrium point. Subsequently, to incorporate quantum fluctuations of the material, we introduced
the lattice–Schr¨odinger equation, calculated the mode frequencies from this, and used these
frequencies as a measure of QPE characteristics.
  We can confirm QPE for the above two materials from PBE functionals. In the case of KTaO3,
unlike SrTiO3, the influence of lattice elongation was negligible, and due to the cubic symmetry of the
structure, there were no modes preferred in specific axial directions. Therefore, the mode could be
described as a linear combination of modes in each axial direction as 3D quantum harmonic oscillator
model. In the case of EuTiO3, the interaction between the spins on Eu and the lattice affects the QPE
iproperties. Furthermore, by analyzing the cause of the variation in mode frequencies depending on
the degree of spin interaction, we identified that this variation was related to the electron occupancy
of the 3d-orbitals of the transition metal. In conclusion, we verified that both materials show QPE
based on the first-principle calculation.</summary>
    <dc:date>2023-12-31T15:00:00Z</dc:date>
  </entry>
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