We present infrared and Raman measurements of magnetite (Fe 3 O 4 ). This material is known to undergo a metal-insulator and a structural transition (Verwey transition) at T V = 120 K. At temperatures below T V , we observe a 1 strong gap-like suppression of the optical conductivity below 1000 cm −1 . The structural aspect of the Verwey transition demonstrates itself by the appearance of additional infrared-and Raman-active phonons. The frequencies of the infrared-active phonons show no significant singularities at the transition whereas their linewidths increase. The frequency and linewidth of the Ramanactive phonon at 670 cm −1 changes abruptly at the transition. For T < T V , we observe fine structures in the infrared and Raman spectra which may indicate strong anharmonicity of the system below the transition. Our estimate of the effective mass of the carriers above the transition to be m * ≈ 100m, where m is the electron mass. Our measurements favor a polaronic mechanism of conductivity and underline the importance of the electron-phonon interaction in the mechanism of the Verwey transition.
Under the influence of a 0.05 T magnetic field, 15-nm diameter cobalt nanoparticles covered with surfactants in a colloidal solution assemble into highly constrained linear chains along the direction of the magnetic field. The magnetic-field-induced (MFI) chains become floppy after removal of the field, folding into three-dimensional (3D) coiled structures upon gentle agitation. The 3D structures are broken into smaller units with vigorous agitation. The nanoparticles redisperse into the solvent upon ultrasonic agitation. Optical microscopy and transmission electron microscopy (TEM) are used to characterize the morphologies of the nanoparticle assemblies at various stages of this reversible process. The hysteresis loops and zero-field cooled/field cooled (ZFC/FC) curves reveal the interparticle coupling in the assemblies. MFI assembly provides a powerful tool to manipulate magnetic nanoparticles.
The properties of ferroelectric films are known to degrade when subjected to hydrogen in forming gas anneals. Earlier studies have attributed this degradation to the loss of oxygen from these films during these anneals. In this study, we show that though oxygen is lost during forming gas annealing, hydrogen incorporation is the primary mechanism for the degradation of ferroelectric properties. Raman spectra obtained from the forming gas-annealed films show evidence of polar hydroxil [OH−] bonds in the films. The most probable site for hydrogen ions is discussed based on ionic radii, crystal structure, electrical properties, and Raman spectra. We propose that the hydrogen ion is bonded with one of the apical oxygen ions and prevents the Ti ion from switching. Pyroelectric measurements on forming gas-annealed capacitors confirm that the capacitors no longer possess spontaneous polarization.
The low-frequency conductivity G\((O) of Bi2Sr2CaCu208 has a Drude-like component below Tc. Interpreting the width of this component as the quasiparticle relaxation rate (r ~'), we find that r "' decreases dramatically just below T^ in sharp contrast with the 7-linear r ~' above Tc and in Bi2Sr2Cu06. This decrease causes a peak in G\((O~-^ 0,T) for T just below T,, a peak which is due to the scattering rate and not to pair coherence effects, consistent with the lack of a coherence peak in the NMR relaxation rate. This result implies that the excitations which scatter the carriers are suppressed below T,.
We observed a dramatic improvement in the performance of polymer light-emitting diodes (LEDs) upon light doping of the organic layer. The LEDs betrayed symmetrical electrical and light-emission characteristics. Their turn-on voltage is lower and their external quantum and power conversion efficiencies are higher by nearly an order of magnitude when compared with devices that utilized a nominally undoped organic layer. We attributed these results to the modification of the tunneling barrier in metal–polymer–metal junctions due to the presence of an induced polarization electric field associated with the ionized dopant counterions and charged polymer chains.
An all‐organic device based on carbon nanotubes and semiconducting polymers is of great interest for opto‐electronic applications. A rectifying heterojunction formed by these novel materials is reported for the first time. The onset for nonlinear current injection is demonstrated to occur at an applied electric field more than on order of magnitude lower than for a semiconducting polymer/conducting oxide or metal heterojunction. The light sensitivity of the heterojunction was also investigated.
The Cu02-plane optical reflectance of superconducting La2 Sr"Cu04thin films (T, =31 K) has been measured over a wide frequency and temperature range. The optical conductivity in the normal state is well described by a temperature-dependent weak-coupling (X=0.25) free-carrier term plus an overdamped, weakly temperature-dependent, midinfrared component. The free-carrier plasma frequency is nearly constant, co~a =6300 cm, whereas the relaxation rate varies linearly with temperature above T, .In the superconducting state, according to our two-component approach, most of the Drude oscillator strength condenses to a 6(co) function. A two-fluid analysis gives a rapid drop in the quasiparticle damp-0 ing rate below T, . A reasonable estimate (-2750 A) for the ab-plane London penetration depth is obtained from the superfluid density. We observe that the midinfrared strength increases below T"suggesting that some (-15%%uo) of the free carriers do not condense into superconducting pairs and may have a strong interaction with pair-breaking excitations. Two absorption edges around 80 cm (3.7 k~T, ) and 400 cm (18 kz T, ) are seen but neither is assigned to the superconducting gap. Comparisons with a one-component picture described by a frequency-dependent scattering rate and effective mass are made and discussed. The far-infrared ab-plane phonons show systematic changes with temperature, which are associated with the structural transition near 250 K.
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