Magnetic phase transition for defect induced electron spins from fully metal-semiconductor separated SWCNTs

ESR experiments from PtRhRe grown and highly semiconductor—metal separated single‐walled carbon nanotubes (SWCNTs) were performed at 9.45 GHz and temperatures T between 0.39 and 200 K. No explicit evidence was found for a response from itinerant electrons in the metallic tubes. Rather, in both the m...

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Bibliographic Details
Published in:physica status solidi (b) Vol. 249; no. 12; pp. 2562 - 2567
Main Authors: Havlicek, M., Chernov, A., Jantsch, W., Wilamowski, Z., Yanagi, K., Kataura, H., Rümmeli, M. H., Malissa, H., Kuzmany, H.
Format: Journal Article
Language:English
Published: Berlin WILEY-VCH Verlag 01-12-2012
WILEY‐VCH Verlag
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Summary:ESR experiments from PtRhRe grown and highly semiconductor—metal separated single‐walled carbon nanotubes (SWCNTs) were performed at 9.45 GHz and temperatures T between 0.39 and 200 K. No explicit evidence was found for a response from itinerant electrons in the metallic tubes. Rather, in both the metallic (M) and the semiconducting (SC) tubes, the ESR signal originates from quasi‐localized defect spins but interactions with free electrons render the two systems characteristically different. The spin susceptibility was of Curie–Weiss type for T ≥ 10 K. For annealed samples it drops for lower T indicating a transition to a ferromagnetic state. Linewidths decrease and increase with increasing T for M and SC tubes, respectively. As a consequence they cross for the two systems. Interaction of spins with free carriers in M tubes via an RKKY type mechanism and increase of linewidth with temperature for SC tubes due to spin–lattice interaction is suggested to be responsible for this.
Bibliography:istex:16B0E19AE1D51F6CB0FD0E6C03AF2878EF2C449B
ark:/67375/WNG-DP9V1DWB-P
ArticleID:PSSB201200426
Deceased
ISSN:0370-1972
1521-3951
DOI:10.1002/pssb.201200426