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| 001 | 1039743 | ||
| 005 | 20250220092010.0 | ||
| 024 | 7 | _ | |a arXiv:2412.15817 |2 arXiv |
| 037 | _ | _ | |a FZJ-2025-01782 |
| 088 | _ | _ | |a arXiv:2412.15817 |2 arXiv |
| 100 | 1 | _ | |a Kämpfer, David |0 P:(DE-HGF)0 |b 0 |e First author |
| 245 | _ | _ | |a Imaging the transition from diffusive to Landauer resistivity dipoles |
| 260 | _ | _ | |c 2024 |
| 336 | 7 | _ | |a Preprint |b preprint |m preprint |0 PUB:(DE-HGF)25 |s 1739863370_1838 |2 PUB:(DE-HGF) |
| 336 | 7 | _ | |a WORKING_PAPER |2 ORCID |
| 336 | 7 | _ | |a Electronic Article |0 28 |2 EndNote |
| 336 | 7 | _ | |a preprint |2 DRIVER |
| 336 | 7 | _ | |a ARTICLE |2 BibTeX |
| 336 | 7 | _ | |a Output Types/Working Paper |2 DataCite |
| 520 | _ | _ | |a A point-like defect in a uniform current-carrying conductor induces a dipole in the electrochemical potential, which counteracts the original transport field. If the mean free path of the carriers is much smaller than the size of the defect, the dipole results from the purely diffusive motion of the carriers around the defect. In the opposite limit, ballistic carriers scatter from the defect $-$ for this situation Rolf Landauer postulated the emergence of a residual resistivity dipole (RRD) that is independent of the defect size and thus imposes a fundamental limit on the resistance of the parent conductor in the presence of defects. Here, we study resistivity dipoles around holes of different sizes in two-dimensional Bi films on Si(111). Using scanning tunneling potentiometry to image the dipoles in real space, we find a transition from linear to constant scaling behavior for small hole sizes, manifesting the transition from diffusive to Landauer dipoles. The extracted parameters of the transition allow us to estimate the Fermi wave vector and the carrier mean free path in our Bi films. |
| 536 | _ | _ | |a 5213 - Quantum Nanoscience (POF4-521) |0 G:(DE-HGF)POF4-5213 |c POF4-521 |f POF IV |x 0 |
| 588 | _ | _ | |a Dataset connected to DataCite |
| 700 | 1 | _ | |a Kovalchuk, Serhii |0 P:(DE-Juel1)195702 |b 1 |u fzj |
| 700 | 1 | _ | |a Hofmann, Jonathan K. |0 P:(DE-Juel1)192445 |b 2 |u fzj |
| 700 | 1 | _ | |a Balashov, Timofey |0 P:(DE-Juel1)179477 |b 3 |u fzj |
| 700 | 1 | _ | |a Cherepanov, Vasily |0 P:(DE-Juel1)128762 |b 4 |u fzj |
| 700 | 1 | _ | |a Voigtländer, Bert |0 P:(DE-Juel1)128794 |b 5 |u fzj |
| 700 | 1 | _ | |a Morawski, Ireneusz |0 P:(DE-HGF)0 |b 6 |
| 700 | 1 | _ | |a Tautz, F. Stefan |0 P:(DE-Juel1)128791 |b 7 |u fzj |
| 700 | 1 | _ | |a Lüpke, Felix |0 P:(DE-Juel1)162163 |b 8 |e Corresponding author |u fzj |
| 856 | 4 | _ | |u https://arxiv.org/pdf/2412.15817 |
| 909 | C | O | |o oai:juser.fz-juelich.de:1039743 |p VDB |
| 910 | 1 | _ | |a Forschungszentrum Jülich |0 I:(DE-588b)5008462-8 |k FZJ |b 0 |6 P:(DE-HGF)0 |
| 910 | 1 | _ | |a Forschungszentrum Jülich |0 I:(DE-588b)5008462-8 |k FZJ |b 1 |6 P:(DE-Juel1)195702 |
| 910 | 1 | _ | |a Forschungszentrum Jülich |0 I:(DE-588b)5008462-8 |k FZJ |b 2 |6 P:(DE-Juel1)192445 |
| 910 | 1 | _ | |a Forschungszentrum Jülich |0 I:(DE-588b)5008462-8 |k FZJ |b 3 |6 P:(DE-Juel1)179477 |
| 910 | 1 | _ | |a Forschungszentrum Jülich |0 I:(DE-588b)5008462-8 |k FZJ |b 4 |6 P:(DE-Juel1)128762 |
| 910 | 1 | _ | |a Forschungszentrum Jülich |0 I:(DE-588b)5008462-8 |k FZJ |b 5 |6 P:(DE-Juel1)128794 |
| 910 | 1 | _ | |a Forschungszentrum Jülich |0 I:(DE-588b)5008462-8 |k FZJ |b 7 |6 P:(DE-Juel1)128791 |
| 910 | 1 | _ | |a Forschungszentrum Jülich |0 I:(DE-588b)5008462-8 |k FZJ |b 8 |6 P:(DE-Juel1)162163 |
| 913 | 1 | _ | |a DE-HGF |b Key Technologies |l Natural, Artificial and Cognitive Information Processing |1 G:(DE-HGF)POF4-520 |0 G:(DE-HGF)POF4-521 |3 G:(DE-HGF)POF4 |2 G:(DE-HGF)POF4-500 |4 G:(DE-HGF)POF |v Quantum Materials |9 G:(DE-HGF)POF4-5213 |x 0 |
| 914 | 1 | _ | |y 2024 |
| 920 | 1 | _ | |0 I:(DE-Juel1)PGI-3-20110106 |k PGI-3 |l Quantum Nanoscience |x 0 |
| 980 | _ | _ | |a preprint |
| 980 | _ | _ | |a VDB |
| 980 | _ | _ | |a I:(DE-Juel1)PGI-3-20110106 |
| 980 | _ | _ | |a UNRESTRICTED |
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