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Advances in Materials Science and Engineering
Volume 2014 (2014), Article ID 948708, 6 pages
Research Article

Improvement of Homogeneity and Aspect Ratio of Silicon Tips for Field Emission by Reactive-Ion Etching

Faculty of General Sciences and Microsystems Technology, OTH Regensburg, 93053 Regensburg, Bavaria, Germany

Received 16 February 2014; Accepted 9 March 2014; Published 6 April 2014

Academic Editor: Feng Zhao

Copyright © 2014 Robert Damian Lawrowski et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.


The homogeneity of emitters is very important for the performance of field emission (FE) devices. Reactive-ion etching (RIE) and oxidation have significant influences on the geometry of silicon tips. The RIE influences mainly the anisotropy of the emitters. Pressure has a strong impact on the anisotropic factor. Reducing the pressure results in a higher anisotropy, but the etch rate is also lower. A longer time of etching compensates this effect. Furthermore an improvement of homogeneity was observed. The impact of uprating is quite low for the anisotropic factor, but significant for the homogeneity. At low power the height and undercut of the emitters are more constant over the whole wafer. The oxidation itself is very homogeneous and has no observable effect on further variation of the homogeneity. This modified fabrication process allows solving the problem of inhomogeneity of previous field emission arrays.

1. Introduction

In vacuum microelectronic devices the field emission (FE) electron sources have advantages compared to classical thermionic cathodes. They offer no dissipation of energy in the medium (vacuum) and high radiation tolerance and work with high operation frequency [1]. The electron sources could be used in sensor systems, miniaturized microwave amplifier tubes, cathodes in electron optic systems (e.g., scanning electron microscope (SEM), scanning tunneling microscope (STM), transmission electron microscopy (TEM)), and high power THz sources as well as compact and fast-switching X-ray sources [2]. The cathode of the electron source is the most important and critical component of such devices. Small variation in emitter geometry leads to an inhomogeneity of emission. The field emission characteristics depend especially on the width of the potential barrier at the electrically conductive surface, which the electrons must tunnel through [3]. High electric fields reduce the width of this barrier (Figure 1). Nanostructures allow delivering these required fields microscopically, due to the locally enhanced field at the tip of the emitter. The field enhancement factor (1) which is defined by the ratio of microscopic to macroscopic field describes this relation [4]. Therefore, lower macroscopic field is necessary for tunneling:

Figure 1: Influence of an enhanced electric field on the surface barrier and the tunneling of electrons.

A possible approximation for is the ratio of height of the emitter to the radius of the tip. Consequently, fluctuations in height and tip radius vary strongly the -factor. Further enhanced fabrication techniques are required to replace typical cathodes in actual applications and allow novel vacuum devices.

By investigation of the influence of RIE parameters (pressure and power) on the geometry and aspect ratio of silicon emitter a chance of homogeneity can be observed.

2. Materials and Methods

2.1. Fabrication Process

Isotropic wet or dry and anisotropic dry etching are usual fabrication techniques for silicon (Si) microstructures. For reproducible emitters with high -factor and current carrying capacity, we use an anisotropic dry etching followed by a wet thermal oxidation [5] (Figure 2).

Figure 2: Schematic of the structured cathode fabrication process (simulated with IntelliSuite). (a) Thermal growth of SiO2 layer. (b) Photolithography with AZ5214. (c) Transferring of the structures into SiO2 by reactive-ion etching. (d) Reactive-ion etching of the bulk Si. (e) Sharpening of the tips by wet thermal oxidation. (f) Wet chemical removal of SiO2.

As bulk material 100 mm p-type silicon wafers with (100) orientation, boron doping, and a resistivity of 3.7–4.2 Ωcm are used. P-doped Si-FE-cathodes show FE-current saturation, which leads to very good current stabilization [6]. For masking a wet thermal oxide of 700 nm is grown on the substrate at 1000°C (Figure 2(a)). The position of the tips is defined by a photolithographic transfer of disks with a 3 μm diameter and triangular pitch of 20 μm into a photoresist (AZ5214) (Figure 2(b)). Anisotropic reactive-ion etching in an Oxford Plasmalab 80Plus transfers this adjustment to the SiO2 layer (Figure 2(c)). It uses CHF3 and O2 as process gases. To achieve the requested shape of the emitter another RIE process step is necessary. A mixture of SF6 and O2 etches bulk Si with the SiO2 discs as mask (Figure 2(d)). The anisotropy and so the geometry can be adjusted by the gas flows, chamber pressure, and RF power [7]. The remaining Si is oxidized thermally at 940°C for the final sharpening of the emitters (Figure 2(e)). The entire SiO2 is removed in the last step by wet chemical etching with a HF mixture (BOE 7 : 1) (Figure 2(f)).

To get significant investigation on the homogeneity each of the twelve chips on a wafer contains six arrays with a different number of tips (1, 7, 91, 271, 547, and 1141).

2.2. Measurement Techniques and Experimental Design

For the investigation of the influence of individual fabrication steps on the emitter, after each process step, some selected tips were observed by a SEM (JEOL 6510) (Figure 3). For a significant conclusion of the homogeneity eight tips on each array were scanned on every corner of the hexagonal layout and two in the middle of the array (Figure 4(a)). Two of three chips on each quarter of a wafer were investigated (Figure 4(b)).

Figure 3: SEM images of the structured cathode fabrication process. (a) Developed photoresist. (b) Patterned SiO2 disks. (c) Etched bulk Si. (d) Final emitter.
Figure 4: Schematic position of the investigated (a) tips in an array (8 of 91) and (b) chips on each quarter (2 of 3)

The undercut of the SiO2-mask, due to the RIE step, was determined by SEM. The etch depth was measured with a KLA Tencor P16 profilometer. By this way, the anisotropic factor (2), which impacts the homogeneity and geometry of the emitters, was determined for diverse powers and pressures at the RIE step:

3. Results and Discussion

The power of plasma is varied from 90 to 150 W and the pressure from 50 to 90 mTorr, resulting in 9 several parameter sets (Table 1) with different anisotropy (Figure 5). The etching time amounts to 60 s. A full undercut of the SiO2 disks is caused by a pressure of 90 mTorr at high power (120 W or 150 W).

Table 1: Anisotropy factor depending on the etching parameters (pressure and power). Symbols in brackets belong to Figure 6.
Figure 5: SEM images of tips after the Si etching with three different anisotropy factors: (a) , (b) , and (c) .
3.1. Effect of RIE Parameters on the Geometry

The pressure has a strong effect on the factor of anisotropy. The reduction of pressure increases significantly the anisotropic factor (Figure 6(a)). Lower pressure causes fewer ions in the plasma, which are able to collide with each other at the same power in the chamber. Hence the ions are more directed perpendicular to the target. Therefore the anisotropic factor is high at low pressures and vice versa.

Figure 6: Dependence of the anisotropic factor on pressure (a) and power (b).

By increasing the power, the energy of the ions in the chamber is rising. At low pressure (blue line in Figure 6(b)) they are more able to impact the target without other hits. The anisotropic factor is rising, too. The higher the pressure is, the more reactive the molecules SF6 are in the plasma. That means that there are more possible collisions on the way, because of the higher number of ions in the chamber. Moreover the effect of the chemical reaction is stronger and the directions of the impacting ions are more distributed, so the etching result is less anisotropic. This results in a lower anisotropy factor, while energy is higher (green line in Figure 6(b)).

Due to a higher anisotropy of etching, the aspect ratio of the tip can be maximized. This causes a larger -factor.

3.2. Investigation on Homogeneity and Measurement Results

Changing power and pressure causes a variation of etch rates within the radius of the wafer, which is the homogeneity of the unit (Figure 7). SEM images are shown in Figure 8. Furthermore, low pressure (50 mTorr) results in quite homogeneous etching, regarding height of emitters and undercut of disks (Figures 7(c) and 7(d)). There are fewer ions in the plasma, due to low pressure in the chamber. The scattering of the ions on other particles and SiO2 disks on the wafer is lower, leading to a more controlled and homogeneous process. However the etch rate is lower. This effect can be compensated by a longer time (1.5x–2.0x) of etching.

Figure 7: Variation of the anisotropic factor from the averaged value of anisotropy on the quarter at different etch parameters: (a) and (b) 90 mTorr, 60 s, 90 W, (c) and (d) 50 mTorr, 90 s, 90 W. Values in brackets are the root mean square deviation and the arithmetic mean of the variation.
Figure 8: SEM images of the emitters after RIE of Si at different etching parameters: (a) and (b) 90 mTorr, 60 s, 90 W, (c) and (d) 50 mTorr, 90 s, 90 W.

The final oxidation thickness is dependent on the remaining diameter of the Si under the SiO2. The thermal wet oxidation is very homogeneous (a variation of less than 4% over the whole wafer). They have no observable effect on further differences of the homogeneity of the etched emitters.

Hence, with a lower pressure, it is possible to produce quite homogeneous cathodes with a high anisotropic factor across the wafer (Figures 8(c) and 8(d)).

FE measurements were performed on tip arrays, which were etched at low pressure (50 mTorr) and with an increased power of 120 W in order to get a high anisotropy factor (Figure 6). The height was around 1 μm with a radius of <40 nm and a tip-to-tip distance of 20 μm (Figure 9).

Figure 9: SEM images of emitters measured at the investigation: (a) with a height of 0 : 9 μm and (b) with a radius of 40 nm.

A comprehensive investigation of the field emission properties of these structures is given in [6]. The array with 547 emitters showed an integral FE-current up to 10−7 A at an electric field of 50 V/μm. An on-set-field of around 40 V/μm for a FE-current of 1 nA was measured. Furthermore the optimization in the RIE process results in a homogeneous emission over the entire array with almost 99% efficiency [6].

The investigation of the anisotropy over the wafer (part 3.2) proves that a low pressure of around 50 mTorr results in a good homogeneity of the emitters over the complete wafer area. The FE measurement showed a good homogeneity of all individual emitters within an array, too.

4. Conclusion and Outlook

The dependence of anisotropy on the etching parameters (pressure and power) of RIE was investigated. Higher pressure increases the lateral etching rate and results in lower anisotropy. The influence of power on the anisotropic factor depends on the pressure. Low pressure causes higher anisotropy with a less scattering of the anisotropic factor. The homogeneity over the entire wafer was improved and due to the higher anisotropy a high aspect ratio of the tips was realized. With adjusted power an optimized etching step was achieved. The field emission investigation shows homogeneous emission of the emitters, which were fabricated with this enhanced process. This opens the possibility to build homogeneous cathodes, which are able to carry stable current for advanced vacuum microelectronic devices.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.


The underlying project was founded by the German Federal Ministry of Education and Research with sponsorship-number 03FH004PX2. The authors of this paper assume resposibility for its content. The authors would like to thank the team for the support.


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