Review of 3D Printed Millimeter-Wave and Terahertz Passive Devices

Zhang, Bing; Chen, Wei; Wu, Yanjie; Ding, Kang; Li, Rongqiang

doi:https://doi.org/10.1155/2017/1297931

International Journal of Antennas and Propagation

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Abstract Introduction Conclusions Conflicts of Interest Acknowledgments References Copyright Related Articles

Review Article | Open Access

Volume 2017 | Article ID 1297931 | https://doi.org/10.1155/2017/1297931

Review of 3D Printed Millimeter-Wave and Terahertz Passive Devices

Bing Zhang,¹Wei Chen,²Yanjie Wu,³Kang Ding,⁴and Rongqiang Li⁵

Academic Editor: Xiulong Bao

Received23 Mar 2017

Revised10 Jun 2017

Accepted19 Jun 2017

Published24 Jul 2017

Abstract

The 3D printing technology is catching attention nowadays. It has certain advantages over the traditional fabrication processes. We give a chronical review of the 3D printing technology from the time it was invented. This technology has also been used to fabricate millimeter-wave (mmWave) and terahertz (THz) passive devices. Though promising results have been demonstrated, the challenge lies in the fabrication tolerance improvement such as dimensional tolerance and surface roughness. We propose the design methodology of high order device to circumvent the dimensional tolerance and suggest specific modelling of the surface roughness of 3D printed devices. It is believed that, with the improvement of the 3D printing technology and related subjects in material science and mechanical engineering, the 3D printing technology will become mainstream for mmWave and THz passive device fabrication.

1. Introduction

Terahertz (THz) waves, or submillimeter/far-infrared waves, are defined as the electromagnetic (EM) radiation in the frequency from 0.1 to 10 THz. They cover a large portion of the EM spectrum between mid-infrared and microwave bands. This spectral domain has low frequency crystalline lattice vibrations and other intermolecular vibrations in many chemical and biological materials, including explosives, drugs, and other biomolecules. Many polar gases also have the distinctive finger print in the THz spectrum. The absorbed and reflected THz waves of these materials contain information that is not available in other frequency ranges. Hence, the THz is extensively explored for sensing and imaging applications. As a potential modality for sensing and imaging, the THz is considered safe because of its penetration capability through obstacles like paper, textile, ceramic, wood, and leather with negligible attenuation. THz technologies are also used for noninvasive and nondestructive sensing of targets under covers. Recently, THz spectroscopy and imaging of explosive related component have been investigated for defense usage.

Compared with relatively well-developed technologies and widespread applications in microwave, mid-infrared and optical bands, research, design, and technology developments in the THz band are still in infancy. A THz system is built up of various active and passive components. For the antenna and other passive devices, their dimensions are usually proportional to the wavelength. The wavelength of the THz EM waves lies in the range of 3 mm–30 μm, which endows the THz passive devices with very small profile. A small variation of the device dimension might give rise to large shift of the functional band. Consequently, the fabrication of THz antenna and passive devices requires sophisticated process of tight dimensional tolerance. Moreover, the surface roughness is the other equally important decisive factor for the THz antenna and passive devices. Large surface roughness leads to increased insertion loss. Thus, the fabrication process of THz passive device is required to have very smooth surface finishing.

Traditional fabrication methods of THz passive devices are computer numerical control (CNC) machining and electrical discharge machining (EDM) [1, 2]. The CNC process uses computer-controlled precision machine tools to cut the component out of a bulk material, in which the material utilization is low. In addition, the CNC process requires the operator to have sufficient experience and skills, which undoubtedly increases the manpower cost. The EDM etches the workpieces into the desired form by means of electrical discharge, which is usually used for machining super hard materials (such as titanium alloys, carbon steels, and cemented carbides). Its fabrication tolerance is much tighter than the CNC process, but the processing cycle is longer, and the processing cost is higher. From what is mentioned above, high labour cost, long processing cycle, and low material utilization of the traditional process are the main reasons for the high cost of THz passive device. The contradiction between the large demand and the unaffordable cost of THz devices is an urgent problem to be solved in both academia and industry.

In order to meet the requirement of high-precision machining and reduce its manufacturing costs, the 3D printing technology began to be used in THz device fabrication. Most of its applications are seen as the fabrication of passive devices like waveguides, horn antennas, and cavity-based components. The 3D printing technology uses powder or liquid based materials to construct the component layer by layer. Different from traditional subtractive manufacturing (SM) processes, 3D printing is an additive manufacturing (AM) process that is environmentally friendly, of low cost, of low-power consuming, and highly flexible and has a short processing cycle. It has the following advantages: Efficient material utilization: raw materials that are not sintered or shaped can be used repeatedly; lower energy consumption; less demanding on the operator’s experience and thus lower labour costs; high flexibility: it is capable of realizing complex structure that is impossible to be fabricated by traditional processes, which gives designers more flexibility; short turn-around time: it eliminates the tool and the mold preparation time; hence the processing cycle is shorter.

In this paper, we will investigate using the 3D printing technology to fabricate THz antennas and passive devices. Firstly, we will review the history of the 3D printing technology. Then 3D printed mmWave and THz passive devices will be introduced. Thirdly, we will elaborate on the key factors for the performance of 3D printed mmWave and THz passive devices which are surface roughness and dimensional tolerance. Finally we will conclude the paper with prospects on the development trend of using the 3D printing technology for mmWave and THz passive device fabrication.

2. History of the 3D Printing Technology

Generally, the 3D printing technologies could be categorized as binding and depositing in terms of processes and metallic and dielectric in terms of materials. Figure 1 shows the history of 3D printing technology since it was invented in 1980, when Kodama applied a patent on rapid prototyping (RP). In 1986, a patent on stereolithography apparatus (SLA) was issued to Hull [3]. In 1992, Deckard et al. filed a patent on selective laser sintering [4]. Crump filed a patent on fused deposition modelling (FDM) in 1992 [5]. ARCAM was established in 1997 to develop the electron beam melting (EBM) technology [6]. MCP Technologies introduced the selective laser melting (SLM) in 2000 [7].

3. Review of 3D Printed Millimeter-Wave and Terahertz Passive Devices

3D printed mmWave and THz devices fall into categories of passive and active devices considering the functionalities. Because of the dimensional tolerance of existing 3D printing technologies, limited by the required gate length of mmWave transistors, it is very challenging to print a transistor of and falling in the mmWave spectrum. Most of the 3D printed mmWave and THz passive devices are seen as lenses, electromagnetic bandgap (EBG) structures, waveguide filters, and horns.

The first 3D printed mmWave passive device is a dual polarized horn reported in 2005 [8]. It was printed by SLA using Emerson and Coming HiK dielectric powder. It has an averaged gain of 12 dBi over the 34–40 GHz bandwidth. A Ka-band Luneburg lens with average 23 dBi gain was printed by ceramic stereolithography apparatus (CSLA) on photoreactive alumina in 2007 [9]. The CSLA was also used to print a Ka-band EBG bandpass filter (BPF) [10]. The filter has the center frequency of 32.94 GHz with 1.03% bandwidth. Frequency shift is caused by the dimensional tolerance in printing and shrinkage in postsintering. In 2008, a D-band (110–170 GHz) EBG resonator was printed by the micro SLA (μSLA) technology on alumina [11]. This work pushed the boundary of 3D printed devices from mmWave to THz spectrum. Lee et al. used the CSLA to print a W-band (75–110 GHz) EBG structure [12]. It has the 84–118 GHz bandgap. Then they transformed the EBG into an aperture antenna of 25 dBi gain [13]. Wu et al. conducted a series of experiments on the polymer jetting (PJ) technology. They firstly reported a 600 GHz woodpile structure (WPS) EBG and a 350 GHz Johnson EBG in 2008 [14], a G-band (140–220 GHz) hollow-core electromagnetic crystal (EXMT) waveguide in 2011 [15], and a D-band hollow-core EXMT antenna of 25 dBi gain in 2012 [16]. A Q-band (33–50 GHz) Luneburg lens was printed by Nguyen in 2010 [17], with 55–65 GHz bandwidth and 21 dBi gain. A W-band corrugated horn and waveguide were printed by SLA using UV-polymer in 2011 [18]. They were printed in split pieces and metal plated in postprocess. In 2013, a polymer jetted acrylic resin THz waveguide was reported [19]. A polymer jetted W-band dielectric reflectarray was introduced by Nayeri et al. in 2014 [20]. Later, in 2014, an H-band (220–325 GHz) waveguide and diagonal horn by SLA showed up [21]. Qu et al. reported an H-band SLA lens of 26.5 dBi gain [22]. In 2015, a Ka-band (26.5–40 GHz) offset stepped-reflector antenna was reported using SLS sintered nylon-polyamide [23]. A W-band waveguide and a W-band 6-order BPF were printed by D’Auria et al. in 2015 [24]. Besides, there are also works reported using 3D printing technologies for low frequency passive device fabrications [25–38].

From what is mentioned above, it can be seen that for most of the dielectric 3D printed passive devices the fabrication process is to first print the device in split pieces and then to metal plate and finally to assemble. Compared with the traditional CNC and EDM metallic devices, they have advantages of light weight and low cost. However, the disadvantages are quite obvious: The process of metal plating and assembly increased the process complexity. The low mechanical strength of plastic and resin affects the life of the device. Pores in the dielectric body and different coefficient of thermal expansion make it impossible to be used in harsh environments such as space. The dielectric body ESD phenomenon will affect the other devices in the system. Metallic 3D printed devices effectively solve the problems due to the following: Good metal conductivity: metallic 3D printed THz devices can be printed in one run and do not require gold plating, which greatly reduces the process complexity and manufacturing costs. The physical strength of the metal makes the device life significantly extended. There is no thermal expansion related issue since the metal plating is not needed. The ESD problem is minor in metallic device.

Before 2012, the only reported metallic 3D printed mmWave device was an SLM 50 mm waveguide [39]. In 2015, Zhang from Chalmers University of Technology conducted a series of experiments on metallic 3D printed mmWave and THz devices [40]. Firstly, six V-band (50–75 GHz) horn antennas were printed to select the appropriate “material + process + postprocess” for our purpose. Processes used are SLM and binder jetting. Materials are Cu-15Sn and 316L stainless steel. Postprocesses adopted to improve the surface roughness are manual polishing, gold plating, and the micromachined process (MMP). Figure 2 shows the surface profile of the 3D printed V-band horns using ZeGage optical surface profilometer. Table 1 compares the measured surface roughness. The SLM Cu-15Sn with MMP rendered the most satisfactory surface roughness of Sa = 0.25 μm for mmWave and THz applications. However, the cost of MMP treatment equals the SLM printing cost. Balancing between the cost and performance, the SLM Cu-15Sn with manual polishing was chosen as the formula for following experiments [41].

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A series of mmWave and THz devices were printed after the formula of “material + process + postprocess” is chosen. E- (60–90 GHz), D- (110–170 GHz), and H-band (220–325 GHz) 3D printed horn antennas were reported to be of comparable performance with commercial counterparts, while featuring considerable cost reduction in Figure 3 [42]. Because most of the horn’s surface is touchable by the polishing kit, the 3D printed horn antennas feature very good surface finishing of Sa = 3 μm. Waveguides are also printed at the E-(WR-12), D-(WR-06), and H-band (WR-03) in Figure 4 [43]. ±5% dimensional tolerance is observed. Since the cross section of the waveguide is in the scale of millimeter, barely anything could be done to improve the inner surface roughness. As a result, the skin depth related insertion loss brought about by the surface roughness becomes apparent when the functional frequency increases. In general, the 3D printed waveguides show acceptable performance up to the E-band. For the D- and H-band 3D printed waveguide, space remains for the improvement of dimensional tolerance and surface roughness. Attempts have been made to print E-band BPF in Figure 5 [44]. Two Chebyshev waveguide iris BPFs of passbands 71–76 GHz and 81–86 GHz were printed. Subject to the undesirable dimensional tolerance and surface roughness, the BPFs demonstrate promising behavioral agreement between simulation and measurement. The 3D printed BPFs are assembled as a diplexer (Figure 6) and then formed together with the 3D printed E-band horn into a front end (Figure 7) [45]. Though behavioral agreement is observed between the simulation and measurement, the accumulated influence of the dimensional tolerance and surface roughness from different component of the front end becomes obvious from the shifted functional band and deteriorated insertion loss.

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4. Challenges and Solutions for 3D Printed MmWave and THz Devices

The two dominantly influential factors on the performance of 3D printed mmWave and THz devices are and dimensional tolerance and surface roughness. The former is decided by the material particle size, thermal shrinkage in sintering and postsintering, laser/electron beam size, and movement control of the laser/electron beam and the nozzle size. The latter is of more concern in 3D printing. It is related to material particle size, laser/electron beam size, density of the material powder, the Gaussianity of the laser beam, and the movement control of the laser/electron beam. Existing techniques to improve the surface quality of 3D printed devices include mechanical polishing, chemical polishing, MMP, and electroplating. However, limited by the existing process, effective improvement of the dimensional tolerance and surface roughness is difficult. Methodology to circumvent the dimensional tolerance would lead the 3D printed mmWave and THz device to a great leap forward to widespread applications. Accurate model to predict and evaluate the surface roughness related loss in 3D printed devices is valuable for quality control in industry.

4.1. Dimensional Tolerance

The influence of dimensional tolerance is reflected by deteriorated reflection coefficient, increased insertion loss, and severe passive intermodulation. It is more meaningful to avoid the dimensional tolerance under the premise that the improvement of dimensional tolerance of 3D printing technologies has come to a limit. The high order mode structure expands the volume of fundamental mode structure, thereby weakening the influence of the processing volume tolerance on the device performance. However, by doing this high order modes are excited. For example, as shown in Figure 8, after transforming a fundamental mode V-band (60–90 GHz) waveguide twist into a high order mode waveguide twist, its immunity to the dimensional tolerance is significantly improved at the cost of high order mode excitation. The flatness of the insertion loss of high order mode waveguides appears to deteriorate. The performance of the high order mode waveguides is still comparable to that of the standard fundamental mode waveguides in a narrow band (e.g., 66–74 GHz). In practice, most RF passive components are not required to function in a full bandwidth. The high order design methodology can effectively avoid the effect of dimensional tolerance on the device performance while guaranteeing the required functionality in a specific bandwidth.

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4.2. Surface Roughness

Not-well-controlled surface roughness may give rise to increased insertion loss and deteriorated passive intermodulation (PIM). Hammerstad and Jensen model, Huray model, and Hall models are representative classic roughness empirical models. They model the rough surface as a two-dimensional structure with periodic properties. These models have reference value in the analysis of conductor loss in planar transmission line structure. Depending on the material and process, different correction factors are introduced for specific applications, such as the correction factor introduced in the Hammerstad and Jensen model:However, the above models are only applicable to the analysis of roughness related losses in planar microstrip structures; there is no effective model for the roughness analysis of 3D printed THz devices. The 3D printed device is different from the traditional device in the roughness characterization due to the specific process and material. For example, the 3D printed surface roughness is limited by the material particle diameter; the same printer using different materials may result in obviously different surface finishing. Due to the nonuniform particle diameter of the material, the root mean square of surface roughness is usually larger than that of the conventional device in roughness. Since the device is printed layerwise and the laser used usually features a Gaussian beam, the roughness of the metal 3D printing device may be subject to periodic distribution in large scale and Gaussian distribution in small scale. Based on the classic model, a correction factor of the 3D printed THz device should be introduced, and the empirical formula of the device loss and roughness should be established. The establishment of the statistic model of the 3D printed surface roughness will benefit the academia in device performance prediction and the industry in quality control.

5. Conclusions

This paper reviews the state-of-the-art 3D printed mmWave and THz devices. They largely fall into the dielectric and the metallic categories. The dielectric 3D printed devices stand out with low body mass, while the thermal stability, physical stability, and process complexity are of concern. The metallic 3D printed devices outperform in the thermal stability and physical stability at the cost of increased body loading. The widespread applications of using 3D printing technology for mmWave and THz device fabrication had come to a bottleneck because of the limited dimensional tolerance and surface roughness. By adopting the methodology of high order device, the dimensional tolerance could be circumvented. A precise model of 3D printed surface roughness could be helpful to predict and evaluate the roughness related loss. Besides, a hybrid printing technology that merges with the traditional CNC process is recently available. The printing and machining processes are carried out within a single machine at intervals. This effectively improves the dimensional tolerance and surface roughness by the machining process, while remaining eco-friendly and cost-effective by the 3D printing technology. A quasi 3D printing process, or 2.5D printing process, is under development. It merges with mask printing for dimensional tolerance control. It is very promising that, with the development of 3D printing technology and disciplines in material science and mechanical engineering, 3D printed mmWave and THz device will become the mainstream solution in both academia and industry.

Conflicts of Interest

The authors declare there are no conflicts of interest regarding the publication of this paper.

Acknowledgments

This work was supported by the Startup Foundation for Young Talent from Sichuan University, Research Project of Guangdong Province (2013B090500035), Youth Foundation of Guangdong University of Technology (15ZK0038), and Science and Technology Program of Guangzhou (2014J4100202). This work was also supported by the Sichuan Provincial Science and Technology Project of China (2015FZ0112), the Foundation of Chengdu University of Information Technology (J201602), and the Scholarship from China Scholarship Council (201508515023).

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Copyright

Copyright © 2017 Bing Zhang 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.

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