Dataset Open Access
{
"name": "Data publication: Path integral Monte Carlo results for electrons in 2D and 3D quantum dots",
"@type": "Dataset",
"distribution": [
{
"@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",
"fileFormat": "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>",
"url": "https://rodare.hzdr.de/record/1931",
"@id": "https://doi.org/10.14278/rodare.1931",
"keywords": [],
"license": "https://creativecommons.org/licenses/by/4.0/legalcode",
"datePublished": "2022-11-07",
"creator": [
{
"@type": "Person",
"name": "Dornheim, Tobias",
"affiliation": "CAUS / HZDR",
"@id": "https://orcid.org/0000-0001-7293-6615"
}
],
"@context": "https://schema.org/",
"identifier": "https://doi.org/10.14278/rodare.1931",
"sameAs": [
"https://www.hzdr.de/publications/Publ-35402"
]
}
| All versions | This version | |
|---|---|---|
| Views | 1,268 | 1,268 |
| Downloads | 8,115 | 8,177 |
| Data volume | 2.7 MB | 2.7 MB |
| Unique views | 873 | 873 |
| Unique downloads | 4,532 | 4,542 |