Tuesday, 3 July 2012

Recent PRL using TeraView's spectrometer

Phonon Energy Gaps in the Charged Incommensurate Planes of the Spin-Ladder Sr14Cu24O41 Compound by Raman and Infrared Spectroscopy


PRL 108, 217401 (2012)


V. K. Thorsmølle1,2,4,*C. C. Homes3,†A. Gozar3,‡G. Blumberg4J. L. M. van Mechelen2A. B. Kuzmenko2S. Vanishri5C. Marin5, and H. M. Rønnow6 

1Laboratory for Photonics and Interfaces, École Polytechnique Fédérale de Lausanne (EPFL), CH-1015, Switzerland
2Département de Physique de la Matière Condensée, Université de Genève, CH-1211 Genève 4, Switzerland
3Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA
4Department of Physics and Astronomy, Rutgers, The State University of New Jersey, Piscataway, New Jersey 08854, USA
5CEA Grenoble, INAC, SPSMS, IMAPEC, 17 rue des Martyrs, 38054 Grenoble, France
6Laboratory for Quantum Magnetism, École Polytechnique Fédérale de Lausanne (EPFL), CH-1015, Switzerland



Abstract

The terahertz (THz) excitations in the quantum spin-ladder system Sr14Cu24O41 have been determined along the c axis using THz time-domain, Raman, and infrared spectroscopy. Low-frequency infrared and Raman active modes are observed above and below the charge-ordering temperature Tco≃200  K over a narrow interval ≃1–2  meV (≃8–16  cm-1). A new infrared mode at ≃1  meV develops below ≃100  K. The temperature dependence of these modes shows that they are coupled to the charge- and spin-density-wave correlations in this system. These low-energy features are conjectured to originate in the gapped sliding motion of the chain and ladder subsystems, which are both incommensurate and charged.


For full paper see http://prl.aps.org/abstract/PRL/v108/i21/e217401



TPS Spectra 300

............The THz-TDS experiments (TPI spectra 1000, TeraView Ltd.) were performed in transmission geometry with the sample mounted inside an optical cryostat capable of reaching 5 K. To obtain the complex conductivity and the transmittance window of the time-domain signals lasting beyond 60 ps (containing several Fabry-Perot internal sample reflections),............................










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