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We develop an efficient computational framework to quantify\n 0~K surface-state transmission in TSM nanowires derived from Wannier\n tight-binding models that faithfully reproduce relativistic density\n functional theory results. Utilizing the non-equilibrium Green's\n function formalism, we systematically screen materials across chemical\n potentials and transport directions, producing a dataset of 3000 surface\n transmission values. This dataset supports machine learning models for\n rapid interconnect compound identification.","descriptionType":"Abstract"},{"description":"# Accelerated discovery of topological metals for nanoscale interconnects\n Dataset DOI: [10.5061/dryad.12jm63zb7](10.5061/dryad.12jm63zb7) ##\n Description of the data and file structure ### Files and variables ####\n File: NanowireData.xlsx **Description:** Data table containing extract\n surface transmission as a function of geometry and doping. Computed\n surface energies are also included. Used to train regression model.  #####\n Variables * Compound + Transmission Direction/Surface: Chemical formula\n and geometry of nanowire for computations * Surface energy: Computed\n surface energy in eV/Å^2^ * Ef: Doping of Fermi energy in eV * Normalized\n Surface Transmission: Extracted value of surface transmission in units of\n (e^2^/h)/H where H is the height of the nanowire as detailed in Fig. 1. of\n the accompanying manuscript.  #### File: Interconnect_Results_Summary.html\n **Description:** Interactive scatter plot of data in NanowireData.csv\n points are colored by the metric detailed in Fig. 5 of the accompanying\n manuscript. #### File: NanowireData.pdf **Description:** PDF version of\n data in NanowireData.csv #### File: SM_Results.pdf **Description:**  PDF\n containing crystal structure image, lattice constants and nanowire\n transmission scaling as a function of thickness for extraction of surface\n transmission for each material screened.","descriptionType":"TechnicalInfo"}],"geoLocations":[],"fundingReferences":[{"schemeUri":"https://ror.org","funderName":"National Science and Technology Council","awardNumber":"MOST 114-2112-M-001-055-MY3","funderIdentifier":"https://ror.org/02kv4zf79","funderIdentifierType":"ROR"},{"schemeUri":"https://ror.org","funderName":"National Science and Technology Council","awardNumber":"NSTC 112-2112-M-A49-047-MY3","funderIdentifier":"https://ror.org/02kv4zf79","funderIdentifierType":"ROR"},{"schemeUri":"https://ror.org","funderName":"Semiconductor Research Corporation","funderIdentifier":"https://ror.org/047z4n946","funderIdentifierType":"ROR"},{"schemeUri":"https://ror.org","funderName":"Defense Advanced Research Projects Agency","funderIdentifier":"https://ror.org/02caytj08","funderIdentifierType":"ROR"}],"xml":"<?xml version="1.0" encoding="UTF-8"?>
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      The sharp increase in resistivity of copper interconnects at ultra-scaled
      dimensions threatens the continued miniaturization of integrated circuits.
      Topological metals with gapless surface states (Fermi arcs) protected by
      bulk topological invariants offer robust, backscattering-immune
      conduction. We develop an efficient computational framework to quantify
      0~K surface-state transmission in TSM nanowires derived from Wannier
      tight-binding models that faithfully reproduce relativistic density
      functional theory results. Utilizing the non-equilibrium Green's
      function formalism, we systematically screen materials across chemical
      potentials and transport directions, producing a dataset of 3000 surface
      transmission values. This dataset supports machine learning models for
      rapid interconnect compound identification.
    </description>
    <description descriptionType="TechnicalInfo">
      # Accelerated discovery of topological metals for nanoscale interconnects
      Dataset DOI: [10.5061/dryad.12jm63zb7](10.5061/dryad.12jm63zb7) ##
      Description of the data and file structure ### Files and variables ####
      File: NanowireData.xlsx **Description:** Data table containing extract
      surface transmission as a function of geometry and doping. Computed
      surface energies are also included. Used to train regression model.  #####
      Variables * Compound + Transmission Direction/Surface: Chemical formula
      and geometry of nanowire for computations * Surface energy: Computed
      surface energy in eV/Å^2^ * Ef: Doping of Fermi energy in eV * Normalized
      Surface Transmission: Extracted value of surface transmission in units of
      (e^2^/h)/H where H is the height of the nanowire as detailed in Fig. 1. of
      the accompanying manuscript.  #### File: Interconnect_Results_Summary.html
      **Description:** Interactive scatter plot of data in NanowireData.csv
      points are colored by the metric detailed in Fig. 5 of the accompanying
      manuscript. #### File: NanowireData.pdf **Description:** PDF version of
      data in NanowireData.csv #### File: SM_Results.pdf **Description:**  PDF
      containing crystal structure image, lattice constants and nanowire
      transmission scaling as a function of thickness for extraction of surface
      transmission for each material screened.
    </description>
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