The angular-dependent magnetoresistance in α(BEDT- TTF)2KHg(SCN)4

Dóra, B.; Maki, K.; Korin-Hamzic, B.; Basletic, M.; Virosztek, A.; Kartsovnik, M. V.; Müller, H.

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The angular-dependent magnetoresistance in α(BEDT- TTF)₂KHg(SCN)₄

Dóra, B., Maki, K., Korin-Hamzic, B., Basletic, M., Virosztek, A., Kartsovnik, M. V., et al. (2002). The angular-dependent magnetoresistance in α(BEDT- TTF)₂KHg(SCN)₄. Europhysics Letters, 60(5), 737-742. Retrieved from http://www.edpsciences.org/articles/epl/abs/2002/23/7384/7384.html.

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Datensatz-Permalink: https://hdl.handle.net/11858/00-001M-0000-002B-368C-A Versions-Permalink: https://hdl.handle.net/11858/00-001M-0000-002B-368D-8

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Dóra, B.¹, Autor
Maki, K.¹, Autor
Korin-Hamzic, B., Autor
Basletic, M., Autor
Virosztek, A., Autor
Kartsovnik, M. V., Autor
Müller, H., Autor

Affiliations:
1Max Planck Institute for the Physics of Complex Systems, Max Planck Society, ou_2117288

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MPIPKS: Electronic structure

Zusammenfassung: In spite of extensive experimental studies of the angular- dependent magnetoresistance (ADMR) of the low-temperature phase (LTP) of alpha-(BEDT-TTF)(2)KHg(SCN)(4) about a decade ago, the nature of LTP remains elusive. Here we present a new study of ADMR of LTP in alpha-(ET)(2) salts assuming that LTP is unconventional charge density wave (UCDW). In the presence of magnetic field the quasi-particle spectrum in UCDW is quantized, which gives rise to striking ADMR in UCDW. The present model appears to account for many existing ADMR data of alpha-(BEDT-TTF)(2)KHg(SCN)(4) remarkably well.