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Optimizing superconductor transport properties through large-scale simulation. Magnitude of the order parameter. For a 2D system at different magnetic fields. Magnitude of the order parameter. For a 2D system. Magnitude of the order parameter. For a 2D system — lager magnetic field. Iso-surface plot of the magnitude of the order parameter. For a 3D system. Iso-surface plot of the magnitude of the order parameter. For a 3D system — lager magnetic field. For a 3D system — even lager magnetic field.

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OSCon SciDAC | oscon-scidac.org Reviews

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Optimizing superconductor transport properties through large-scale simulation. Magnitude of the order parameter. For a 2D system at different magnetic fields. Magnitude of the order parameter. For a 2D system. Magnitude of the order parameter. For a 2D system — lager magnetic field. Iso-surface plot of the magnitude of the order parameter. For a 3D system. Iso-surface plot of the magnitude of the order parameter. For a 3D system — lager magnetic field. For a 3D system — even lager magnetic field.

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5 surface

6 superconductors

7 large-scale

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10 field

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OSCon SciDAC | oscon-scidac.org Reviews

https://oscon-scidac.org

Optimizing superconductor transport properties through large-scale simulation. Magnitude of the order parameter. For a 2D system at different magnetic fields. Magnitude of the order parameter. For a 2D system. Magnitude of the order parameter. For a 2D system — lager magnetic field. Iso-surface plot of the magnitude of the order parameter. For a 3D system. Iso-surface plot of the magnitude of the order parameter. For a 3D system — lager magnetic field. For a 3D system — even lager magnetic field.

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Optimizing superconductor transport properties through large-scale simulation. Defects in trapped superfluids.

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Optimizing superconductor transport properties through large-scale simulation. Schematics of a second-generation superconducting wire: YBa. Coated conductor, complex multilayer architecture of inexpensive materials. Inset shows the dynamics of vortices in the conductor in the presence of pinning centers. We will develop large-scale TDGL simulations that treat a fully macroscopic system of vortices and pinning defects. Answering these questions in the context of a versatile TDGL simulation represents a ma...

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Optimizing superconductor transport properties through large-scale simulation. A history of collaboration.

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Optimizing superconductor transport properties through large-scale simulation. Materials Science Division (MSD) team. Andreas Glatz glatz@anl.gov. Applied Mathematics and Computer Science Division (MCS) team.

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Optimizing superconductor transport properties through large-scale simulation. Ivan A. Sadovskyy, Ying Jia, Maxime Leroux, Jihwan Kwon, Hefei Hu, Lei Fang, Carlos Chaparro, Shaofei Zhu, Ulrich Welp, Jian-Min Zuo, Yifei Zhang, Ryusuke Nakasaki, Venkat Selvamanickam, George W. Crabtree, Alexei E. Koshelev, Andreas Glatz, and Wai-Kwong Kwok, Towards superconducting critical current by design. Advanced Materials (March 31, 2016). Jared Sagoff, Scientists optimize defects for better superconducting effects.

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Biological and Environmental Research. Advanced Scientific Computing Research (ASCR). Scientific Computation Application Partnerships in Basic Energy Sciences. Basic Energy Sciences (BES). Advanced Scientific Computing Research (ASCR). The following priority research directions form the basis for BES SciDAC Partnership projects:. Materials Under Extreme Environments. Advanced Modeling of Ions in Solutions, on Surfaces, and in Biological Environments. Lead Investigator: Roberto Car ( rcar@princeton.edu.

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Optimizing superconductor transport properties through large-scale simulation. Magnitude of the order parameter. For a 2D system at different magnetic fields. Magnitude of the order parameter. For a 2D system. Magnitude of the order parameter. For a 2D system — lager magnetic field. Iso-surface plot of the magnitude of the order parameter. For a 3D system. Iso-surface plot of the magnitude of the order parameter. For a 3D system — lager magnetic field. For a 3D system — even lager magnetic field.

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