Rolled-Up Nanotech: Illumination-Controlled Hydrofluoric Acid Etching of AlAs Sacrificial Layers
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- Costescu, R.M., Deneke, C., Thurmer, D.J. et al. Nanoscale Res Lett (2009) 4: 1463. doi:10.1007/s11671-009-9421-8
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The effect of illumination on the hydrofluoric acid etching of AlAs sacrificial layers with systematically varied thicknesses in order to release and roll up InGaAs/GaAs bilayers was studied. For thicknesses of AlAs below 10 nm, there were two etching regimes for the area under illumination: one at low illumination intensities, in which the etching and releasing proceeds as expected and one at higher intensities in which the etching and any releasing are completely suppressed. The “etch suppression” area is well defined by the illumination spot, a feature that can be used to create heterogeneously etched regions with a high degree of control, shown here on patterned samples. Together with the studied self-limitation effect, the technique offers a way to determine the position of rolled-up micro- and nanotubes independently from the predefined lithographic pattern.
KeywordsRolled-upNanotubesNanotechNanostructuresEtchingHydrofluoric acidIII–V layersIllumination-controlled
Introduction and Background
Rolled-up nanotech [1, 2] has become a powerful technology with applications in a broad range of research fields, including optofluidics , micromachinery [4–6], magnetofluidics [4, 7], biophysics [4, 8], nanomechanics , and waveguiding for different spectral ranges and applications [10–12]. Large arrays of periodically ordered microtubes can be fabricated by a combination of lithography and deliberate self-rolling of strained layers upon selective underetching [1, 13–15]. However, in some cases, it might be important to stimulate tube formation in certain areas and suppress tube formation outside those areas. Precise control over the lateral positioning and the number of windings is fundamental for the use of the tubes in optical resonators for sensors [16–20], hyperlenses [4, 21, 22], or electrical transport (curved electron gases) [23–27]. Numerous existing studies offer highly sophisticated methods for precise lateral positioning of rolled-up semiconductor nanostructures by controlling the starting edges [13–15, 28, 29], but difficulties arise for thin layers due to the extensive, successive lithography steps involved, and ways to control the stopping point of rolling remain largely lacking without modifying the structure.
Here, we demonstrate illumination-controlled hydrofluoric acid (HF) etching of a buried thin AlAs sacrificial layer. Sufficiently intense light exposure of a certain substrate area leads to a complete suppression of the underetching effect, and as a result, the formation of rolled-up InGaAs/GaAs tubes can be easily controlled spatially. This method allows for control over the roll-up stopping point and is suitable for very thin sacrificial layers.
The aim of this study was to quantify the observed “etch-suppression effect” (ESE) and precisely control the release of InGaAs/GaAs bilayers with an illumination technique.
Here, the experiments were performed using 20 nm In0.33Ga0.66As/20 nm GaAs structures on AlAs grown on (001) GaAs substrates by molecular beam epitaxy, where the thickness of the AlAs was varied from 4 to 20 nm. For experiments pertaining to the measurement of the onset of the etch suppression and rolling distance, the starting edges were defined by mechanical scratching, whereas photolithography and wet chemical etching (by H3PO4:H2O2:H2O solution) were used for controlling the etch suppression. Our specially designed setup involved an HF-resistant trough for etching with HF under light focused by a Zeiss optical microscope using different objective lenses of 5 × through 50 × magnification (for sample evolution during this process, see Fig. 1a and b). Other measurements were performed using illumination from a HeNe laser with maximum output power of 2 mW, as well as a laser with adjustable power (up to 20 mW) and wavelength (535–825 nm) with focusing optics or an optical fiber to illuminate the surface of the sample. For all measurements, the intensity of illumination was measured beforehand using a calibrated power meter. For samples that were etched, illuminated, and observed under the microscope, the settings on the illumination dial were used and the focused spot sizes for each magnification were assumed to be the same. For the quantitative measurements of tube rolling distance, optical images of the sample outside of solution once the etching was terminated were taken. From these images, the rolling distance could then be measured, which we define as distance from the starting edge to the center of the tube width, assumed to correspond to the stopping point of the underetching.
The resolution of the ES method was studied by precisely positioning the illumination spot on wet-chemically etched mesa structures of different shapes and sizes (on the order of 10–100 μm) during HF etching. The degree of etching suppression (given by the coverage area of unetched structures remaining on the sample) was measured versus distance from the center of illumination.
Characteristics of Etching Suppression Effect
Figure 1b shows an optical microscopy image of a structure composed of a 4 nm AlAs layer and a 40 nm symmetrical strained In0.33Ga0.66As/GaAs bilayer. The larger circular shape observed on the sample at the end of the HF experiment is formed by original mesa structures that were left unetched, while on the rest of the sample the bilayer mesas are underetched, leading to rolling up as expected.
We also found that the ESE is time dependent, i.e., the etching time under illumination determines whether further etching will continue once the illumination is removed. In our experiments, we found that for samples where the high intensity light exposure was kept short, the layers were able to start rolling after being removed from the light source. This effect was found to not only depend on the light intensity but also on the thickness of the AlAs layer, which suggests that the etch suppression is a dynamic process that depends on the access of HF to the AlAs layer and the exchange of products and reactants in this region. This conclusion is further corroborated by the fact that with increasing AlAs thickness the rolling distance of the strained bilayer becomes independent of the AlAs gap size (Fig. 3).
Using Etch Suppression for Nanotube Positioning
The ESE was used to position and control the roll up of tubes from strained InGaAs/GaAs bilayers. The patterning allowed us to create well-defined starting edges suitable for the illumination experiment (as in Fig. 1). By cleverly integrating this process, one can obtain both etched regions with rolled-up layers and unetched regions within a small area on the sample. Furthermore, this technique is useful for applications since, during the ES, the structures remain unchanged other than the “blocking” at the starting edge.
Discussion, Uncertainties, and Limitations
We investigated the rolling distance as a function of illumination intensity used during the HF etching of AlAs/InGaAs/GaAs structures on GaAs for different sacrificial layer thicknesses. For AlAs layers thinner than 10 nm, total suppression of the etching process occurs beyond a threshold intensity that increases with increasing AlAs thickness.
The ESE is clearly influenced by the AlAs-HF reaction rate as well as the physical characteristics of the structure: the larger the sacrificial layer gap and faster the reaction rate, the higher the intensity of illumination needed to suppress the etching. This trend continues up to a point where the reaction is no longer illumination dependent and suppression is no longer possible. A further series of experiments involving etching with filtered light and a focused laser beam of varying wavelengths (not presented here) suggests that the ESE is preserved for lower energies than the AlAs band gap and therefore any photochemical effect in HF cannot depend on light excitation of the AlAs material. We have also eliminated the possibility that heating plays a significant role in the ESE, since experiments that involve heating samples in HF solution past the boiling point show an enhancement rather than suppression of the etching and hence would counteract this effect.
We believe that for the ESE found in samples etched with HF for shorter times under illumination levels close to the threshold value from Fig. 2, the strained bilayer remains intact because the sacrificial layer was not underetched at the starting edge, which may happen through the accumulation of solid As and As oxide following from a photochemical interaction at the GaAs surface in the presence of HF.
The process through which AlAs sacrificial layers are wet-etched with hydrofluoric acid (HF) [34–43] as well as the laser-induced etching of semiconductors by a dilute acid solution [44–46] have been investigated previously in some depth. In HF-AlAs reactions, any passivating As formed at the surface is usually oxidized and then dissolved, thus allowing new access to the etch front and sustaining etching . But if the rate of As production exceeds that of oxide formation, or if the type of oxide is stable in the HF, then the etching will be inhibited. From laser-induced etching studies, it is clear that porous stable oxide films formed at the semiconductor surface give a time dependence for the process . During the redox reaction, As(III) must be complexed by water and dissolved as HAsO2 and As2O3, but when the concentration of As(III) surpasses the solubility limit, there is precipitation of As at the surface, slowing down the reaction. Our results match well with this type of process, and we propose that the ESE occurs in a similar fashion: the formation of very small amounts of As or As2O3 at the AlAs gap, which would nonetheless be enough to block access of HF to films under 10 nm, can effectively suppress the underetching of the AlAs layer. In accordance with our findings, the thicker the sacrificial layer gap and the faster the HF etching rate, the less likely the ESE takes place. In the suppression regime for thinner AlAs layers, for higher intensities of illumination the photogeneration of holes is more pronounced leading to a faster subsequent passivation (and reaching of the ESE limit with time). For thicker AlAs layers, higher illumination can still lead to changes at the GaAs substrate interface  but does not hinder the etching of the AlAs.
While the self-limitation of the maximum rolling distance of RUNTs allows for the precise tuning of the number of rotations as a function of the sacrificial layer, the illumination permits the exact positioning of the tube in combination with common lithographic technology. Fine-tuning the etch suppression with patterned samples can yield a useful way of precisely controlling the roll up of strained InGaAs/GaAs bilayers and the entire tube fabrication process, as well as other more general laser-assisted microfabrication applications, with a convenient, customizable method. In this way, it is complementary to pre-pattering of the sample by lithographic means and allows for a full control over the position of the produced RUNTs.
The authors would like to thank Emica Coric, Dr. Stefan Baunack, Dr. Jurgen Thomas, and Dr. Ingolf Monch for processing and characterization help, and Dr. Armando Rastelli and Dr. Francesca Cavallo for fruitful discussions.