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- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 classification A1.
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 date "1973".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 language "eng".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 type journalArticle.
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 hasPart 01JAYSRW638WYF8FCDYQ67BRE0.pdf.
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 subject "Chemistry".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 subject "Physics and Astronomy".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 doi "10.1002/pssa.2210200140".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 issn "0031-8965".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 issn "1521-396X".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 issue "1".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 volume "20".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 abstract "The conductivity of pure and doped (Mo, Ti) V2O5 single crystals is measured along the three crystallographic directions in the temperature range 90 to 350° K. For T < 140° K, it is shown that conduction can be considered as a variable range hopping between defect levels, situated in the neighbourhood of the Fermi-level. From combined de and ac measurements, the concentration of localized states is found to be about 1019 cm−3. In the intermediate temperature range 140° K < T < 350° K, the observed anisotropy is explained assuming that conduction is due to hopping along vanadium chains. Attention is drawn to the influence of random potential fluctuations.".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 author 78964EC2-B25E-11E6-B104-2D2FD0AF0289.
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 author F3313E58-F0ED-11E1-A9DE-61C894A0A6B4.
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 author urn:uuid:f7e26ca0-cc88-4e5a-8740-9354bbb972df.
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 dateCreated "2024-10-24T08:15:30Z".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 dateModified "2024-11-28T00:19:46Z".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 name "On the electrical conductivity of V2O5 single crystals".
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 pagination urn:uuid:e9c65d19-2224-4e7a-9231-20c984ecb666.
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 sameAs LU-01JAYSGNDE7Y3DR9ZQDFRPFWM5.
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 sourceOrganization urn:uuid:76583d35-8ea2-4eac-9cdb-ecba64e95d3e.
- 01JAYSGNDE7Y3DR9ZQDFRPFWM5 type A1.