**5. RF applications**

The manufacturing of RF components by AM process is particularly challenging for different reasons. The internal channels of the parts have to be designed considering the typical AM post-processing operations, for example, powder removal in SLM or metal plating in SLA and FDM. Moreover, due to the typical accuracy of the AM processes, an electromagnetic robust design approach is mandatory in the case of high RF-performance components.

The simplest strategy consists of splitting the component into two or more parts. This way is usually employed in the case of SLA and FDM to ease electroless metal plating processes. Sometimes this is also used in SLM products, particularly for complex internal structures. The main drawback is misaligning the different parts with consequent leakage effect and, subsequently, higher losses. Moreover, the intrinsic features of AM processes are not employed, making their employment, therefore, less effective and convenient.

The designed part should be realized monolithically to take full advantage of the AM process. To achieve this goal, the electromagnetic design has to be adapted to the process in a so-called "*AM-oriented design*." The most important is aligning the propagation axis with the building direction, avoiding, at the same time, the presence of overhanging structure in the internal channel (for instance, stubs or corrugations). These criteria, then, force a complete reconsideration of well-known RF structures. One of the main advantages is better manufacturing accuracy and symmetry of the cross section (essential characteristic for dual-polarization components).

The following subsections summarize the most common 3D-printed RF components, namely—waveguides, filters, horn antennas, dual-polarization components (OMTs and septum polarizers). Finally, the last subsection describes some examples of the integration of different RF functionalities into a single component.

#### **5.1 Waveguides**

Waveguide lines are the simplest candidates for evaluating the best achievable accuracy of the AM technologies for microwave components. An important

parameter is the realized metal loss per wavelength/cm. Different factors influence these values:


Deep research has been done considering different AM technologies and a frequency range that spans from Ku- to E- band (10–170 GHz). A summary of these works with relevant results is reported in **Table 2**. As observed, SLM and SLA are the most commonly exploited technologies since they ensure good accuracy and low roughness compared to other AM processes.

Going more into detail, an interesting example of a waveguide manufactured by FDM is reported in ref. [10]. Firstly, a WR42 waveguide has been printed using ABS. Then, the same printer was customized to deposit a low-cost conductive silver ink. The manufactured waveguide exhibits a measured loss of 0.11 dB/cm for the entire K-band.

As far as the SLA is concerned, mainly the W- and D-band (75–170 GHz) have been considered. In Refs. [11–13], the copper plating has been applied, showing a Wband loss mean value of 0.06 dB/cm. An interesting comparison between commercial and SLA waveguides is reported in [12], showing that SLA components present a measured loss that is almost double of the commercial ones: 0.06 dB/cm versus 0.03 dB/cm and 0.26 dB/cm and 0.15 dB/cm in W- and D-band, respectively.

As far as the SLM is concerned, the main test refers to the frequency range from 18 to 110 GHz. Aluminum is the material most used. However, few examples have been carried out by using copper and nickel alloys [11]. An interesting comparison is presented in Ref. [11], where the authors compare the losses of a commercial WR42 waveguide with SLM (in aluminum) and a CNC machined realization. As it could be expected, the lowest attenuation occurs in the commercial waveguide (0.004 dB/cm), while the SLM and CNC parts exhibit a loss of about 0.02 dB/cm and 0.03 dB/cm, respectively. Still considering SLM, in Ref. [15], a study on the circular waveguide,


**Table 2.** *Losses of AM waveguides.*

operating in Ka-band, is carried out. The measured aluminum prototypes exhibit a loss of 0.01 dB/cm. The co-polar and cross-polar transmission coefficients have been measured to understand the SLM's feasibility for dual-polarization systems, thanks to the double symmetry shape. The measurements show a spurious cross-polarization term of 25 dB/40 dB.

A comparison, in W-band, between parts SLM realized with different alloys (aluminum, copper, and nickel alloys) is reported in Ref. [11], showing the better behavior of the aluminum prototype.

#### **5.2 Waveguide filters**

Filters are one of the most demanding elements from a manufacturing point of view. The high-standing waves developing inside the components lead to high sensitivity to mechanical tolerances and high susceptibility to multifactor discharge and passive intermodulation products (PIM). For this reason, they are an important benchmark for the AM manufacturing of passive waveguide components [3].

A detailed review of 3D-printed microwave filters has been recently reported [16]. The frequency range considered in literature is mainly 7–22 GHz, although a few examples at higher frequency bands (up to 110 GHz) have also been discussed. Metal, plastic, and ceramic materials have been employed in published works.

FDM has been used in Ref. [17] to manufacture two X-band filters with PLA filament. Each component has been manufactured in two halves with an E-plane cut. The parts are coated with a copper spray to create a conductive surface for the galvanization process with further copper. Despite the accuracy of the printing and painting process, good results have been obtained for both filters. In Ref. [18], a twopole X-band filter in the WR90 waveguide insert has been manufactured using PC filament. The printed insert has been coated with a nickel spray and then electroplated with copper.

As far as the SLA process is concerned, in Ref. [19], a four-pole quasi-elliptic filter, working at 810 MHz 16 MHz, is presented. The filter is composed of two mushroom-shaped resonators. The filter has been realized in two blocks, metalized with silver painting and then electroplated with copper. The same manufacturing approach has been reported in Ref. [20] for a two-pole filter.

Considering SLM realizations, an example of a W-band filter is presented in Ref. [21]. The filter is based on five rectangular resonators coupled using inductive irises. Two stainless steel prototypes have been manufactured, one coated with 5 μm of copper showing different measured electrical conductivity: 1.25 107 S/m and 5.96 107 S/m, respectively. As far as, the scattering parameters are concerned, the stainless steel filter shows a center frequency shift down by 1.66 GHz and a minimum return loss of 24.41 dB in the passband, while the copper-plated presents a frequency shift of 0.9 GHz with a return loss is 26.56 dB.

Some examples of monolithic realization and comparison between materials and processes are reported in Refs. [9, 22]. In Ref. [9], a comparison for Ku/K filter prototypes realized both in SLM (in aluminum, titanium, and maraging steel alloys) and SLA (copper plated) is shown. The study proves that an AM-oriented architecture provides excellent results in both roughness and mechanical accuracy; at the same time, the metallization of the SLA component is extremely complicated in the inner surfaces of the filter. A similar comparison is reported in Ref. [22], where two prototypes, operating in X-band, have been manufactured—one by SLM with an aluminum-copper alloy, the other by SLA, and then copper electroplated. The most

interesting contribution of this paper was the excellent performance, even for the SLA filter.

Ceramic materials have also been used for the 3D printing of waveguide filters with two different approaches. The first method consists of manufacturing ceramic components, subsequently, metal plating. For example, in Ref. [23], a ceramic-filled resin has manufactured hemispherical resonator waveguide filters. Four Ka-band filters have been manufactured, metal plated, and measured with good RF results. The electroless plating process consists of a deposition of palladium, nickel, and copper, followed by a passivation layer of silver. In the second approach, the materials' dielectric properties are exploited to reduce the overall envelope.

For instance, Ref. [24] manufactured a dielectric perturber for a third-order filter with a bandpass shifting from 10 to 12 GHz. The filter was manufactured using copper with a standard manufacturing process, while the perturber was manufactured by SLA using zirconia (εr = 32, tan δ = 0.002). In Ref. [25], the authors used alumina (εr = 9.1, tan δ = 0.0001) to manufacture the dielectric resonators in a sixth-order quasi-elliptic bandpass filter. The housing has been 3D printing in two blocks using plastic material and then metal plated. An important aspect of this work is that no supports or glue are needed. The dielectric resonators are placed in the middle of their cavities to maximize their Q-factor.

#### **5.3 Horn antennas**

Waveguide horns are commonly used in high-performance antenna feed chains in SATCOM applications. This class of antennas, indeed, can provide excellent performances in terms of gain, bandwidth, return loss, and cross-polarization [26]. Therefore, much effort has been made to study the 3D printing of waveguide horns. Most of the works are from X-band to K-band (7–27 GHz), although some examples can be found up to 300 GHz [27].

As far as the SLA process is concerned, three works are particularly interesting. In the first one [28], a 2–12 GHz double-ridge horn antenna is presented. The internal surface has been coated with a layer of silver ink with a conductivity of 4 105 S/m.

In Ref. [29], a comparison between SLA and standard process (lathe in aluminum) has been considered to realize a spline horn operating in the Ku-band. Both prototypes exhibit good agreement between the simulated and measured value of the co-polar pattern, while worse performances in terms of losses and cross-polarization level can be noticed in the AM one. The latter is mainly related to the higher surface roughness, which has been estimated equal to 1.79 μm. In Ref. [30], a metal-plated 240 GHz choke horn antenna has been reported. The antenna has been designed to obtain 12 dBi gain from 200 to 280 GHz. The measured radiation pattern is in good agreement with the simulation.

Considering the SLM process, six works are particularly significant [26, 27, 31–34]. The first four refer to the manufacturing of classical architecture to understand the applicability of the SLM technique. The last two show some interesting work in the exploration of AM features.

In Ref. [26], the manufacturing of three smooth-wall horns, working in Ku-, Ku/Kband, and Q/V-band, is presented. The smooth-wall design allows the alignment of the building direction with the propagation axis, ensuring a good cross-sectional symmetry and low cross-polarization level. The horns have been manufactured using aluminum alloy. All the antennas exhibit good agreements between measured and simulated values. In particular, return-loss higher than 33 dB, cross-polarization lower than 28 dB, and peak gain of 25 dBi have been obtained. Moreover, a 3D scan of the outer section of the horns reveals an accuracy between 0.06–0.08 mm.

In Ref. [27], the manufacturing of 300 GHz corrugated horn antennas. Four prototypes have been manufactured using a tin-bronze alloy with an electrical conductivity of 7 MS/m. The dimensions of the prototypes differ by 5% with respect to the theoretical model. Nevertheless, the measurement results have observed good symmetry between E-plane and H-plane. However, the antenna efficiency is relatively low due to the conductivity of the material used in manufacturing. To improve the RF performances, all the prototypes have been plated with 3 μm of gold (conductivity of 44 MS/m).

In Ref. [31], an X/Ku-band (8–18 GHz) chocked horn SLM manufactured in the aluminum alloy is presented. To investigate process manufacturing accuracy and repeatability, 15 prototypes have been manufactured, showing an overall accuracy of 0.1–0.3 mm and a roughness Ra of 3.5 μm. The feeding gap and the radiating aperture have been milled after the manufacturing process, with an accuracy of 0.02 mm.

In Ref. [32], a Ku-band spline horns SLM manufactured in aluminum and titanium alloys are presented. The manufactured components' roughness is about 16 μm for both the materials, but it reduces to 3.4 μm for the Al one after the post-processing. The radiation pattern of the two prototypes is in good correlation with the simulation, but the titanium horn exhibits a worse cross-polarization level due to a slight ellipticity of the aperture. In the same paper, the manufacturing of a cluster of four spline horns is presented, showing a mass reduction of 30% with respect to classical manufacturing.

In Ref. [33], a perforated X-band (8-12GHz) horn antenna has been presented to lighten the component. The holes' dimensions are lower than 1/15th of the wavelength at 12 GHz. Not considering the SMA connector, the antenna weight is just 8 g. The good agreement between simulated and measured RF results demonstrates an efficient method to reduce weight without affecting performance. A similar idea has been applied in Ref. [34] for a steel pyramidal horn antenna.

FDM process has been used to manufacture waveguide horns up to 15 GHz. In Ref. [35], the authors presented the first additively manufactured dielectric-loaded profiled conical horn antenna in the frequency range from 9 to 15 GHz. The component has been manufactured using polylactic acid (PLA) with relative permittivity *ϵ<sup>r</sup>* = 2.72. Two concentric dielectric cores with different infill factors have been printed to obtain the desired relative permittivity inside the horn. After the manufacturing process, the outer surfaces of the horn have been plated with 10 μm of copper. Surface roughness of 8.050 μm has been measured after the plating process. The measured radiation pattern is in good agreement with the simulation, with a cross-polarization level less than 21 dB up to 13 GHz. A measured S11 lower than 10 dB has been obtained from 10 to 14 GHz. The antenna exhibits a gain of 16.0–20.0 dBi and total efficiency of 60–91% over the frequency range from 9 to 15 GHz. In Ref. [36], three X-Ku pyramidal horn antennas have been 3D printed using ABS material and then metal plated using copper or chromium wand nickel, respectively. As expected, the copper prototype exhibits the best performance.

#### **5.4 Dual-polarization components**

Orthomode transducers (OMT) and septum polarizers are classical components used in dual-polarization antenna feed-chain systems. Separate the two linear polarization of

the incoming signal routing them to two different rectangular waveguides [37]. Septum polarizers are employed to route the two circular polarizations in the common waveguide (typically circular or square) to the TE10 modes in two different rectangular waveguides and vice versa. The most important parameters are insertion loss, isolation between the rectangular ports, and cross-polarization in transmission [38].

Starting with SLM realizations, a C-band septum polarizer operating in the frequency band 3.6–4.4 GHz is shown in Ref. [39]. The component has been manufactured of Scalmalloy® with a measured dimensional error of 0.6 mm. The return loss is better than 25 dB and the isolation greater than 23 dB, while the deviation between measured and simulated axial ratio is about 1 dB mainly caused by a not perfectly circular common section. Moving up in frequency, in Ref. [40], two single sidearm OMTs are presented. The components are designed in the frequency band 10–15 GHz. The two OMTs have been compared with a realization by conventional manufacturing techniques. In this work, the OMT geometry realized was not figured out for AM process.

Nevertheless, both components exhibit RF performances in good accordance with the traditionally machined components. An example of an OMT realization of an AMoriented geometry is reported in Ref. [41], where the RF measured performances well match the simulated one. Isolation over 50 dB and return loss better than 20 dB have been achieved in the operative frequency range. Considering the Ka-band, an asymmetric side-coupling OMT has been presented in Ref. [37]. The OMT geometry has been conceived to be AM-oriented by using a multi-slope junction. The manufactured prototype exhibits good accordance with measured and simulated RF results. In particular, the insertion loss is lower than 0.25 dB, and the return loss is better than 27 dB. Then, in Ref. [42], the OMT design has been integrated with a twist in the coupled arm. The measured results are in good agreement with the simulation. In particular, the return loss for both polarizations is better than 27 dB, and the insertion loss is lower than 0.15 dB and 0.2 dB for the inline and coupled channels, respectively, which corresponds to an equivalent resistivity of 16 μΩcm. The prototype has been controlled by a computer tomography scanner showing a mechanical accuracy in the range 0.02–0.04 mm.

By considering the SLA process, in Ref. [43], a V-Band (50–75 GHz) OMT manufactured is presented. The OMT has been metal plated with a process developed by SWISSto12. This consists of copper plating and passivation using a thin layer of gold or silver. The novelty of this OMT is the multi-step conical post on the turnstile junction. This permits easy printing by SLA.

Septum polarizers have also been realized. In Ref. [38], a Ka-band prototype realized in SLM is presented. Two 45° bends have been integrated to accommodate standard WR28 flanges. The device has been designed to align the propagation axis with the building direction to guarantee the best cross-sectional symmetry. Thanks to this choice, the measured cross-polarization level is better than 30 dB and the isolation better than 28 dB.

In Ref. [44], a broadband septum polarizer has been manufactured in SLA and copper plated. The paper shows a novel design with a triangular common port design that allows a higher bandwidth than circular or square waveguide polarizers. The polarizer has been firstly designed in W-band and manufactured with a standard machining process. Then, the design was scaled in K-band and manufactured with an SLA printer. The prototype has been coated with conductive ink and then subjected to galvanic copper plating. Both the components exhibit isolation greater than 17 dB and a return loss better than 14 dB over 37.8% of bandwidth. Moreover, the insertion loss is lower than 0.4 dB for the 3D-printed prototype.

### **5.5 Integrated components**

As reported in Ref. [40], one of the main advantages of the AM technologies is the free shape feature that can lead to an additional degree of freedom in the design of RF components, for instance, the integration of different functionalities (electromagnetic, mechanical, and thermal) in a monolithic component [45].

The previous survey has shown the evolution of the employment of AM process in the realization of guided microwave components, improving the quality of the realized parts, but this potentiality of AM is still not fully explored. A survey of some interesting and successful examples of this initial work is reported.

In Ref. [46], a mono-block Ku-band front-end, a combination of two integrated sub-assembly, a diplexer, and a 2 2 horn antenna array, has been presented. The components have been manufactured using the SLA technology and metalized with copper and tin with an electrolytic process. Measurement results agree with the simulated performances with a frequency shift of 150 MHz that can be related to the thickness of the metal deposition, not considered during the design.

In Ref. [38], a Ka-band feed horn integrated with a septum polarizer, manufactured with the SLM process using aluminum alloy. The septum polarizer, presented in the previous section, has been integrated with a smooth-wall horn. The measured values of return loss, cross-polarization, and isolation are comparable with the results of the septum polarizer alone, namely a return loss better than 25 dB, an isolation between the rectangular waveguide higher than 27 dB, and a crosspolarization better than 28 dB. The measurement results are comparable with those obtained with a standard manufacturing process in a split block layout.

In Ref. [47], an interesting study of an integrated feed system working in the frequency band in X-band (from 7.2 to 8.2 GHz) is presented. The device is composed of a circular horn antenna and an OMT. The authors compare the 3D printing of the feed system as a mono-block with the manufacturing in two symmetric pieces. Both the components have been printed using SLA and copper plated with a three-step metallization process. Although the two-pieces prototype has the advantages of an easier manufacturing process and the thickest metal coating, the monolithic component exhibits better RF performances.

A similar component has been developed and presented in Ref. [48]. The integrated Ku-band feed chain consists of a spline horn and an OMT and has been manufactured using the SLM process. The RF performances are compared with those obtained with standard machining processes. An X-band feed chain has been presented in the same paper. The developed component consists of a spline horn and a compact E-plane waveguide coupler. The feed chain is three times lighter than a comparable, conventional manufactured component. Perfect agreement with the simulated performance has also been obtained with these components.

In Ref. [49], an entire Ku-band feed cluster manufactured by SLM technology, suitable for SFB scenarios, is presented. The feed cluster operates in Tx- and Rxfrequency bands. The component consists of 18 feed chains composed of a horn, a transition, a single sidearm OMT and waveguide routing to provide interfaces for the measurement. The scattering parameters have been measured for both the frequency bands showing a return loss better than 19.5 dB and the isolation below 50 dB. The feed cluster exhibits excellent agreement between simulated and measured values of the pattern at 11.30 and 14–25 GHz.

#### *Additive Manufacturing of RF Waveguide Components DOI: http://dx.doi.org/10.5772/intechopen.104106*

In Ref. [50], a high gain K-band feed chain has been manufactured by SLM using aluminum alloy. The measurement results show return loss and port-to-port isolation better than 23 dB. The axial ratio is between 0.1 and 0.5 dB, while the cross-polar discrimination (XPD) is better than 30 dB. The measurements show good manufacturing accuracy with good rotational symmetry.

In Ref. [51], a passive front end for satellite communication, manufactured by SLM technology using aluminum alloy, is discussed. The component comprises four conical horns, four rectangular-to-circular waveguide tapers, two-stage 1 4 power dividers, and a WR-42 waveguide interface. The scattering parameters have been measured in the frequency band 19–21 GHz. Discrepancies between simulated and measured RF performances have been observed. They are mainly due to the dimensional tolerance and surface roughness of the fabrication process.

In Ref. [52], a leaky-wave antenna integrated with an OMT operating in K-band is presented. The antenna consists of a triple-ridge square waveguide perforated on its top wall with crossed slots. The component has been printed by SLA with the propagation axis aligned with the building direction to enhance the good symmetry of the antenna. Then, copper plating was applied. The measurements prove the high precision of the process. In particular, the 3D-printed prototype exhibits a return loss better than 16 dB, port isolation better than 40 dB, and a cross-polarization level below 35 dB.

A K/Ka-band dual-circular polarization antenna feed chain has been reported in Ref. [53]. The device has been designed with an AM-oriented approach. A prototype has been manufactured by SLM with aluminum alloy. The chain is composed of a dual-band orthomode junction (OMJ) which symmetrically extracts the K-band signal while the Ka-band one propagates inline to a series of circular steps connected to a Kaband septum polarizer. Each of the four arms, where the K-band signal propagates, is integrated with a low-pass filter to isolate the channels from the Ka-band signals. Subsequently, these four arms are recombined in a turnstile junction connected to a Kband septum polarizer. The measured performances of the prototype show very satisfactory performance with values typically required for SATCOM application (i.e., isolation between the bands better than 50 dB, return loss, and isolation between the two polarizations of the same bands than 20 dB).

Finally, a complex RF component is presented in Ref. [54], where a Ku/K-band filter is integrated with an H-plane bend and 90<sup>o</sup> twist. The conceived geometry makes AM process the only feasible manufacturing technique. The design shows a 70% weight/volume reduction compared to a solution obtained assembling three different parts realized by standard machining. The idea has been stressed by considering the realization of three prototypes with different bend radii to make the device as smaller as possible. Good agreement between measured and simulated RF performance has been achieved even for the prototypes with a bend radius of 30 mm. The three components exhibit a rejection better than 60 dB and an insertion loss better than 0.2 dB. The return loss is better than 25 dB for the prototype with a bend radius of 40 mm, while it is better than 20 dB for the other prototypes.
