It is clear that the light intensity is independent of the polarity. The threshold voltages V th of the bidirectional device are V th approximately 50 V at T = 300 K and V th approximately 4 V at T = 100 K. Figure 2 Integrated electroluminescence intensity of bidirectional field effect light-emitting and light-absorbing heterojunction device (for both voltage polarities). Temperatures of T = 100 and 300 K. Figure 3 shows the EL emission spectra as a function of

temperature. The peak wavelengths at T = 150 and 300 K are around λ = 1,236 and 1,288 nm, respectively. Theoretically, a red shift of the active material peak wavelength with selleck products temperature at a rate Blasticidin S price of 0.38 nm/K is predicted. We compare the experimental peak emission energy versus the temperature plot with the Varshni equation: where E 0 and E g (T) are the bandgaps at T = 0 K and at a finite temperature of T, respectively and α and β are around 4.8 × 10-4 eV · K-2 and 284 ± 167 K, respectively

[12, 13]. Figure 3 EL spectra of bidirectional THH-VCSOA-based GaInNAs/GaAs structures at different temperatures. The inset shows the temperature dependence of the peak energy (filled squares) compared with the Varshni equation (dotted lines). Tariquidar nmr The device was mounted on a temperature-controlled holder at varied temperatures. External voltage pulses up to 110 V were applied between the diffused contacts and the integrated EPL intensities of the THH-VCSOA are measured as a function of bias voltage with the photo-excitation power was kept constant at around 17 mW. In Figure 4, we show the peak intensities of EPL signals for both positive and negative polarities at T = 14°C and for positive polarity at temperatures of T = 30 and 44°C. Figure 4 Temperature-dependent amplified signal of bidirectional THH-VCSOA structure.

Amplified spectra are plotted as a function of applied voltages in Figure 5. It is clear from the figure that as the applied voltage increases, the integrated intensity increases with the emission peak at around 1,280 nm. Figure 5 Amplified intensity as a function of applied voltages between 30 and 200 V at T  = 300 K. The spectra of EL, PL, and the combined EPL of bidirectional THH-VCSOA device at 1,280 nm are shown in Figure 6. The spectra have a broad bandwidth due Methocarbamol to the fact that light was collected from the whole forward-biased area. The input signal of 488 nm is absorbed by the THH device, causing a modulation of the 1,280-nm light, thus acting as a wavelength converter. In EPL, the device is optically but also electrically pumped, with V app = 80 V in amplitude. The EL spectrum alone was also measured with V app = 80 V and the difference between EL + PL and EPL intensities is accountable for the gain from the device. Optical gains versus incident powers at various applied voltages are depicted in Figure 7. At T = 300 K, maximum gains of around 1.3, 3.