Dataset Open Access

Data publication: Path integral Monte Carlo results for electrons in 2D and 3D quantum dots

Dornheim, Tobias

JSON-LD (schema.org) Export

{
  "url": "https://rodare.hzdr.de/record/1931", 
  "identifier": "https://doi.org/10.14278/rodare.1931", 
  "creator": [
    {
      "affiliation": "CAUS / HZDR", 
      "name": "Dornheim, Tobias", 
      "@id": "https://orcid.org/0000-0001-7293-6615", 
      "@type": "Person"
    }
  ], 
  "datePublished": "2022-11-07", 
  "keywords": [], 
  "name": "Data publication: Path integral Monte Carlo results for electrons in 2D and 3D quantum dots", 
  "@id": "https://doi.org/10.14278/rodare.1931", 
  "sameAs": [
    "https://www.hzdr.de/publications/Publ-35402"
  ], 
  "license": "https://creativecommons.org/licenses/by/4.0/legalcode", 
  "@type": "Dataset", 
  "@context": "https://schema.org/", 
  "distribution": [
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N4_lambda0.5_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N4_lambda0.5_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N4_lambda0_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N4_lambda0_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N4_lambda10_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N4_lambda10_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N4_lambda3_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N4_lambda3_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N6_lambda0.5_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N6_lambda0.5_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N6_lambda0_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N6_lambda0_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N6_lambda10_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N6_lambda10_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N6_lambda3_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig3_N6_lambda3_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N4_lambda0.5_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N4_lambda0.5_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N4_lambda0_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N4_lambda0_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N4_lambda10_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N4_lambda10_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N4_lambda3_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N4_lambda3_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N6_lambda0.5_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N6_lambda0.5_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N6_lambda0_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N6_lambda0_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N6_lambda10_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N6_lambda10_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N6_lambda3_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig4_N6_lambda3_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N4_2D_lambda0.5.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N4_2D_lambda0.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N4_2D_lambda10.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N4_2D_lambda3.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N4_3D_lambda0.5.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N4_3D_lambda0.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N4_3D_lambda10.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N4_3D_lambda3.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N6_2D_lambda0.5.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N6_2D_lambda0.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N6_2D_lambda10.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N6_2D_lambda3.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N6_3D_lambda0.5.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N6_3D_lambda0.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N6_3D_lambda10.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig5_N6_3D_lambda3.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig6_2D_N6_lambda3_Bose_kinetic_virial.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig6_2D_N6_lambda3_Fermi_kinetic_virial.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig6_3D_N6_lambda3_Bose_kinetic_virial.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig6_3D_N6_lambda3_Fermi_kinetic_virial.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig8_beta3_2D_lambda3_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig8_beta3_2D_lambda3_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig8_beta3_3D_lambda3_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig8_beta3_3D_lambda3_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig8_beta5_2D_lambda3_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig8_beta5_2D_lambda3_Fermi.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig8_beta5_3D_lambda3_Bose.res"
    }, 
    {
      "fileFormat": "res", 
      "@type": "DataDownload", 
      "contentUrl": "https://rodare.hzdr.de/api/files/25bcddd4-c903-4f8a-bbbd-b4c1e9003566/Fig8_beta5_3D_lambda3_Fermi.res"
    }
  ], 
  "description": "<p>This repository contains a collection of raw path integral Monte Carlo simulation results for various properties of electrons in 2D and 3D quantum dots published in Ref. [1].</p>\n\n\n\n<p>[1] http://iopscience.iop.org/article/10.1088/1367-2630/ac9f29</p>"
}
443
2,410
views
downloads
All versions This version
Views 443443
Downloads 2,4102,410
Data volume 799.7 kB799.7 kB
Unique views 186186
Unique downloads 402402
More info on how stats are collected.
Publication date:
November 7, 2022
DOI:
10.14278/rodare.1931

RODARE DOI Badge

DOI 

10.14278/rodare.1931

Markdown 

[![DOI](https://rodare.hzdr.de/badge/DOI/10.14278/rodare.1931.svg)](https://doi.org/10.14278/rodare.1931)

reStructedText 

.. image:: https://rodare.hzdr.de/badge/DOI/10.14278/rodare.1931.svg
   :target: https://doi.org/10.14278/rodare.1931

HTML 

<a href="https://doi.org/10.14278/rodare.1931"><img src="https://rodare.hzdr.de/badge/DOI/10.14278/rodare.1931.svg" alt="DOI"></a>

Image URL 

https://rodare.hzdr.de/badge/DOI/10.14278/rodare.1931.svg

Target URL 

https://doi.org/10.14278/rodare.1931

Related identifiers:
Identical to:
https://www.hzdr.de/publications/Publ-35402
Referenced by:
https://www.hzdr.de/publications/Publ-34421
Communities:
License (for files):
Creative Commons Attribution 4.0 International

Versions

Version 1 10.14278/rodare.1931 Nov 7, 2022
Cite all versions? You can cite all versions by using the DOI 10.14278/rodare.1930. This DOI represents all versions, and will always resolve to the latest one. Read more.

Share

Cite as

Export