Intersubband Emitters: GaAs-based Quantum-Cascade Lasers

Correlation between emission frequency and location on the wafer for terahertz quantum-cascade lasers

The correlation between the emission frequency and the location on the wafer due to an inhomogeneous growth rate across the wafer was investigated for GaAs/AlAs terahertz (THz) quantum-cascade lasers (QCLs) using experiments and simulations. For several wafers, we observe a blue shift of the emission frequency from the center to the edge of the wafer. This blue shift is attributed to a decrease of the thickness of the QCL, which can be determined with spectroscopic techniques. The correlation of the calculated frequencies with the actual emission frequencies of QCLs fabricated from different locations on the wafer allows to establish an effective method for the fabrication of THz QCLs emitting at a particular target frequency.

Fig. 1(a) Deviation of the growth rate measured by ex-situ spectral reflectivity scans as a function of the distance from the center for wafer A. The corresponding relative thickness of the QCL is given on the right-hand side. The location of the QCLs on (b) wafer A and (c) wafers B and C as a function of emission frequency measured at 30 K for continuous-wave (cw) operation (filled rectangles) and 50 K for pulsed operation (hatched rectangles). The horizontal dotted lines connect the dominant peaks for lasers under cw operation. The simulated results are indicated by asterisks, and the results of the fits are marked by the dashed lines.

 

Due to the high emission powers and narrow line widths in continuous-wave (cw) operation, THz QCLs are promising sources for high-resolution spectroscopy. As examples, the transition between rotational states of the hydroxyl radical (OH) at 3.55 THz and the fine-structure transition of neutral atomic oxygen (OI) at 4.75 THz are of current interest in astronomy and planetary science. These spectral lines can be measured by a heterodyne spectrometer using a THz QCL in a local oscillator. Furthermore, THz QCLs are developed as suitable radiation sources for the detection of Si, Al, N+, and O atoms/ions in plasma processes by high-resolution absorption spectroscopy of the respective fine-structure transitions in the THz spectral region.

 

The relative change in the growth rate and thickness of the QCL across the wafer were evaluated by ex-situ spectral reflectivity scans for three wafers A, B, and C. Figure 1(a) depicts the relative change in the growth rate (QCL thickness) with respect to the growth rate (QCL thickness) at the center of the wafer A. The emission frequencies of a number of QCLs fabricated from wafer A (B and C) based on a design for 3.36 THz (3.92 THz), which are located in different regions of the wafer, exhibit a blue shift with a decreasing growth rate from the center to the edge of the wafer. Using Fourier transform-based simulations, we calculated the frequency as a function of the relative thickness of the QCL. By utilizing the dependence shown in Fig. 1(a), the frequency is calculated as a function of the location, which is well reproduced by a power law. This power law describes the correlation between the emission frequency of the QCLs and the location on the wafer as indicated by the dashed lines in Figs. 1(b) and 1(c). The simulated frequencies agree well with the experimental results. Using this universal power law, the covered frequency range for a new wafer can now be predicted, and the suitable position on the wafer from which a THz QCL with an application-defined emission frequency is fabricated can be efficiently determined. Rather than growing several homogeneous wafers with a wafer-to-wafer variation of the nominal active-region thickness, THz QCLs with customized emission frequencies can be efficiently fabricated by making use of this well-defined frequency dependence across the wafer.

 

 

1 Author X. Lü , B. Röben , L. Schrottke , K. Biermann , H. T. Grahn
Title

Correlation between frequency and location on the wafer for terahertz quantum-cascade lasers

Source Semicond. Sci. Technol. , 36 , 035012 ( 2021 )
DOI : 10.1088/1361-6641/abdd4b | 3231 Cite : Bibtex RIS
X. Lü, B. Röben, L. Schrottke, K. Biermann, and H. T. Grahn

Contact

Prof. Dr. Holger T. Grahn

Head of Department 

+49 30 20377-318

htgrahn@pdi-berlin.de

Dr. Lutz Schrottke

Senior Scientist

+49 30 20377-339

lutz@pdi-berlin.de