Oscillations, Waves, and Interactions - GWDG

Charge order in one-dimensional solids 331
[17] O. Klein, S. Donovan, M. Dressel, and G. Grüner, ‘Microwave cavity perturbation technique.
Part I: Principles’, Int. J. Infrared and Millimeter Waves 14, 2423 (1993); S.
Donovan, O. Klein, M. Dressel, K. Holczer, and G. Grüner, ‘Microwave cavity perturbation
technique. Part II: Experimental scheme’, Int. J. Infrared and Millimeter Waves
14, 2459 (1993); M. Dressel, S. Donovan, O. Klein, and G. Grüner, ‘Microwave cavity
perturbation technique. Part III: Applications’, Int. J. Infrared and Millimeter Waves
14, 2489 (1993); A. Schwartz, M. Dressel, A. Blank, T. Csiba, G. Grüner, A. A Volkov,
B. P. Gorshunov, and G. V. Kozlov, ‘Resonant techniques for studying the complex
electrodynamic response of conducting solids in the millimeter and submillimeter wave
spectral range’, Rev. Sci. Instrum. 66, 2943 (1995); M. Dressel, O. Klein, S. Donovan,
and G. Grüner, ‘High frequency resonant techniques for the study of the complex
electrodynamic response in solids’, Ferroelectrics 176, 285 (1996).
[18] H.-W. Helberg and B. Wartenberg, ‘Zur Messung der Stoffkonstanten ɛ und µ im GHz-
Bereich mit Resonatoren’, Z. Angew. Phys. 20, 505 (1966). The tradition goes back to
the Institut für Angewandte Elektrizität (Institute of Applied Electricity) founded in
the beginning of the 20th century and headed by Max Reich for a long time. Students
like Arthur von Hippel spread this knowledge all around the world and made highfrequency
investigations of solids to a powerful tool. The foundation of the Laboratory
of Insulation Research and the Radiation Laboratory at MIT during World War II
certainly had the largest impact.
[19] L. I. Buranov and I. F. Shchegolev, ‘Method of measuring conductivity of small crystals
at a frequency of 10 10 Hz’, Prib. Tekh. Eksp. (engl.) 14, 528 (1971); I. F. Shchegolev,
‘Electric and magnetic properties of linear conducting chains’, phys. stat. sol. (a) 12,
9 (1972); H.-W. Helberg and M. Dressel, ‘Investigations of organic conductors by the
Schegolev method’, J. Phys. I. (France) 6, 1683 (1996).
[20] B. P. Gorshunov, A. A Volkov, G. V. Kozlov, L. Degiorgi, A. Blank, T. Csiba, M.
Dressel, Y. Kim, A. Schwartz, and G. Grüner, ‘Charge density wave paraconductivity
in K0.3MoO3’, Phys. Rev. Lett. 73, 308 (1994); A. Schwartz, M. Dressel, B. Alavi, A.
Blank, S. Dubois, G. Grüner, B. P. Gorshunov, A. A. Volkov, G. V. Kozlov, S. Thieme,
L. Degiorgi, and F. Lévy, ‘Fluctuation effects on the electrodynamics of quasi onedimensional
conductors above the charge-density-wave transition’, Phys. Rev. B 52,
5643 (1995).
[21] A. V. Pronin, M. Dressel, A. Loidl, H. S. J. van der Zant, O. C. Mantel, and C. Dekker,
‘Optical investiations of the collective transport in CDW-films’, Physica B 244, 103
(1998).
[22] G. Kozlov and A. Volkov, ‘Coherent Source Submillimeter Wave Spectroscopy’, in Millimeter
and Submillimeter Wave Spectroscopy of Solids, edited by G. Grüner (Springer,
Berlin, 1998), p. 51; B. Gorshunov, A. Volkov, I. Spektor, A. Prokhorov, A. Mukhin,
M. Dressel, S. Uchida, and A. Loidl, ‘Terahertz BWO-spectrosopy’, Int. J. of Infrared
and Millimeter Waves, 26, 1217 (2005).
[23] K. Bender, K. Dietz, H. Endres, H.-W. Helberg, I. Hennig, H. J. Keller, H. W. Schäfer,
and D. Schweitzer, ‘(BEDT-TTF) 2+ J −
3 - A two-dimensional organic metal’, Mol. Cryst.
Liq. Cryst. 107, 45 (1984); M. Dressel, G. Grüner, J. P. Pouget, A. Breining, and D.
Schweitzer, ‘Field- and frequency dependent transport in the two-dimensional organic
conductor α-(BEDT-TTF)2I3’ J. de Phys. I (France) 4, 579 (1994).
[24] M. Dressel and N. Drichko, ‘Optical properties of two-dimensional organic conductors:
signatures of charge ordering and correlation effects’, Chem. Rev. 104, 5689 (2004); M.
Dressel, ‘Ordering phenomena in quasi one-dimensional organic conductors’, Naturwissenschaften
94, DOI 10.1007/s00114-007-0227-1 (2007).
[25] M. Dressel, S. Kirchner, P. Hesse, G. Untereiner, M. Dumm, J. Hemberger, A. Loidl,