# 3D Printed and Photonically Cured Graphene UHF RFID Tags on Textile, Wood, and Cardboard Substrates

Authors: M. Akbari; H. He; J. Juuti; M. M. Tentzeris; J. Virkki; L. Ukkonen
Journal: International Journal of Antennas and Propagation
 (2017)

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## Abstract

This paper introduces 3D direct writing and microdispensing of graphene ultrahigh frequency (UHF) radio-frequency-identification (RFID) antennas on textile, wood, and cardboard substrates, subsequently cured either by conventional oven or photonically by pulsed Xenon flashes. Photonic-cured passive UHF RFID graphene tags on cardboard, wood, and textile substrates achieve read ranges of 5.4, 4.6, and 4 meters, respectively. These results are superior to those achieved by the oven-cured tags that featured read ranges of 4.8, 4.5, and 3.6 meters, respectively. This work presents the first integration of 3D printing and photonic curing of graphene antennas on low-cost versatile substrates.


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## Body

## 1. Introduction

Recently, 3D direct writing and microdispensing have gained a great interest as they have the capability of printing versatile materials eliminating the need of masks and feature sizes as small as 20μm, as well as offering significant reductions in the amount of used material. 3D direct writing opens great possibilities in printing, for example, electrically functional radio-frequency (RF) devices, antennas, and wearable electronics [1–3].Integrating additive manufacturing processes with a photonic curing process enables the rapid and cost-effective manufacturing of electronics. The mechanism of photonic curing is based on rapid heating of films by intense photon flux and cooling via conduction, and it has been a transformative process in printed electronics manufacturing. The photonic curing allows for inexpensive, rapid, and completely maskless thermal processing along with excellent controllability. The use of pulsed light from a flash lamp is an excellent alternative to traditional thermal processing [4, 5].Metallic antenna additive manufacturing components have been extensively utilized in antenna manufacturing [5, 6]. However, these are relatively expensive, require high curing temperature, and involve many nonenvironmentally-friendly aspects, such as nonbiodegradable and toxic chemicals and solvents. Therefore, the utilization of alternative, nonmetallic components, such as carbonous nanomaterials, has gained a lot of attention. In particular, graphene shows extraordinary properties, including high charge mobility (200,000 cm2V−1s−1), zero band gap, and high mechanical properties (with Young modulus of ~1 TPa) [7, 8]. Additionally, utilizing graphene in antenna structures brings great possibilities, such as lightweight components, low curing temperatures, and especially low cost compared to metallic materials [7, 9].Recent works [9, 10] have demonstrated graphene-based antennas for passive radio-frequency-identification (RFID) applications. In antenna manufacturing, doctor blading and screen-printing have been utilized. The main limitation of these two methods is their inherent nonflexibility in design changes, due to the need of a stencil.In this work, we present ultrahigh frequency (UHF) RFID antennas fabricated by 3D printing environmental-friendly graphene inks on three different green substrates. The printed antennas were cured by heat in a conventional oven or by photonic curing with a flash lamp. Various tag antenna prototypes are presented on textile, wood, and cardboard substrates, and the effects of the two curing methods on the tag performance are studied.


## 2. Direct Write Microdispensing

We used nScrypt tabletop series 3D direct write microdispensing system to fabricate the graphene-based UHF RFID tags on different substrates. The system was equipped with a positive pressure pump with a high-precision computer actuated valve coupled with a nozzle. The air pressure was applied to the ink-filled syringe (See Figure1(a) for the 3D printing system), which was pushed into the main valve body, finally through the ceramic nozzle tip. By adjusting a constant material pressure and running a customizable computer-controlled valve “open and close” process, it can produce a controllable and consistent material flow rate, precise starts and stops, and the ability to utilize a wide range of material viscosities [11]. Furthermore, other critical parameters are the adjustment of the distance between the ceramic tip and the substrate, the speed of the tip, and the diameter of the nozzle tip. The latter was chosen according to the printed material and the final printing feature size.Figure 1
(a) 3D microdispensing system with an ink syringe and a ceramic nozzle tip and (b) schematic process of antenna fabrication.
(a)
(b)In this work, the used ink was functionalized Graphene Nanoplatelets (GNPs) ink (HDPlas® IGSC02002; Haydale Ltd., UK [12]), which was used to fabricate antennas on a 100% cotton fabric (thickness of 0.3 mm), normal rough packaging cardboard (thickness of 0.6 mm), and thin wood veneer (thickness of 0.65 mm). The printed antennas were then cured by a continuous pulsed light or in an oven, as shown in Figure 1.In this study, the tag antenna was selected to be a simple dipole as shown in Figure2(a). The used ceramic tip in the direct writing system had an inner diameter/outer diameter of 125 μm/175 μm, and the pressure for the material’s feed was adjusted to 16 psi. The printing spacing and angle were 250 microns and 0°, respectively, and the printing direction was parallel to the wood veneer as shown in Figure 2(a). Figure 2(b) shows that printing was carried out in two parts, as well as the starting and ending points.Figure 2
(a) 3D-printed RFID tag antenna (one layer) on wood and (b) image of printing direction.
(a)
(b)The printing resolution generally depends on the ceramic tip diameter, the substrate material, and the used ink. The wetting and absorption of the ink are affected by the substrate material properties. For instance, the width of a single printed graphene line (having a length of 10 mm) on cardboard, textile, and wood was approximately 450, 550, and 650μm, respectively. These printed lines are presented in Figure 3. As can be easily observed, the printed line on cardboard shows the best quality in terms of ink spreading and keeping fine boundaries compared to wood and fabric.Figure 3
Optical microscopic image of a single, one-layer graphene line deposited by 3D microdispenser on (a) wood, (b) cardboard, and (c) textile (magnification ×5).
(a)
(b)
(c)


## 3. Curing: Conventional Oven versus Photonic Curing

The printed sample lines were subjected to a series of flashes from a Xenon sintering system (Sinteron 2010-L, Xenon Corp.), where the distance from the test sample to the window of the lamp housing was 25 mm. The used operating mode was continuous mode, as a single pulse was not sufficient to cure the graphene layer, and eventually left it wet. In the continuous mode, three parameters are adjustable: high voltage (HV) value, pulse width, and period. The principle of the continuous flash mode is presented in Figure4. A static pulse width and period were used, and the HV value and the number of pulses were adjusted to find out the optimized parameters for the printed graphene layers. Initially, the optimized parameters for the printed 10 mm long lines were studied on the cardboard substrate. For comparison, samples were also cured in an oven at 60°C for 30 minutes, as presented in the ink datasheet [12], and in normal office conditions for 24 hours.Figure 4
Continuous flash mode.The printed lines on cardboard were subjected to a flash created with HV in the range of 1900 V to 2300 V, and a different number of pulses were used with the pulse width of 2100μs and a period of 1100 ms. The resistances of the cured samples were measured by a multimeter and they are presented in Table 1. It was noticed that the cardboard starts burning when subjected to pulses with a HV more than 2300 V. As can be seen from Table 1, there is a threshold, that is, 1900 V and 2100 V with 8 pulses, both producing a resistance of 40 Ω. The resistance started to decrease when the voltage was increased to 2200 V and more pulses were used. However, there is a risk of bumps creation and delamination by further increasing the number of pulses. In general, using a high HV and a large number (above 8) of pulses decreases the resistance value, unless it ends up to substrate burning or to the creation of undesired bumps.Table 1
Resistance of a printed graphene line on cardboard with different curing parameters.
Curing method
Office conditions
Oven
Photonic (HV, number of pulses, and duration of whole curing process)
Parameters
24 h
60°C30 min
1900 V8 15 s
1900 V16 30 s
2100 V8 15 s
2100 V24 45 s
2200 V8 15 s
2200 V16 30 s
2300 V8 15 s
2300 V16 30 s
R (Ω)
60
29
40
32
40
27
35
32
35
45By using continuous pulses (with a HV of 2200 V and overall eight pulses), the resistance of the sample line is about 35 Ω, which is close to the resistance of a sample cured in an oven. The highest resistance was achieved when the samples were left to cool off in office conditions.In the case of the fabric and wood substrates, a lower HV, of about 1900 V, is needed, due to the flammability of those substrates. The optimized pulsed Xenon flash parameters for curing graphene ink on different substrate materials are presented in Table2.Table 2
Optimized photonic curing parameters for different substrate materials.
Substrate
High voltage (V)
Pulse width(µs)
Number of pulses
Period(ms)
Duration of whole curing process (s)
Cardboard
2200
2100
8
1100
15
Wood
1900
2100
6
1100
11
Fabric
1900
2100
6
1100
11


## 4. Materials Characterization

The graphene UHF RFID tags printed on wood, cardboard, and fabric, and then cured in an oven, are referred to as samples W1, C1, and F1, respectively. The tags on wood, cardboard, and fabric, which were subjected to Xenon flash pulses, are referred to as samples W2, C2, and F2.A 3D laser microscope (VK-X100/X200) was used to analyze the morphology and microstructure of the fabricated samples. According to the results presented in Figures5–7 and Table 3, the difference between the microstructures and the 3D topography of the oven-cured and photonic-cured samples is obvious. C1, W1, and F1 have a uniform microstructure and only a small difference between the highest and lowest thickness values. However, C2, W2, and F2 show a larger thickness gradient and a less uniform microstructure.Table 3
The peak read range of each tag antenna together with the corresponding thickness, average thickness gradient, and sheet resistance.
Substrate
Curing method
Read range (m)
Average thickness (µm)
Thickness gradient (µm)
4-point sheet resistance (Ω/sq)
C1
Cardboard
Oven
4.8
17.6
35
31.84
C2
Photonic
5.4
74
140
31.25
F1
Fabric
Oven
3.6
91.2
90
27.40
F2
Photonic
4
67
100
26.08
W1
Wood
Oven
4.5
29.6
30
68.49
W2
Photonic
4.6
51.3
80
48.50Figure 5
(a, b) Laser microscope and 3D topography images of oven-cured C1 and (c, d) photonic-cured C2.
(a)
(b)
(c)
(d)Figure 6
(a, b) Laser microscope and 3D topography images of oven-cured W1 and (c, d) photonic-cured W2.
(a)
(b)
(c)
(d)Figure 7
(a, b) Laser microscope and 3D topography images of oven-cured F1 and (c, d) photonic-cured F2.
(a)
(b)
(c)
(d)Furthermore, the 4-point sheet resistances of the tags were measured by a manual probe station (Wentworth Labs) and a Keithley multimeter. Despite the fact that oven-cured samples are more uniform, the sheet resistances of the oven-cured samples are higher than those of the photonic-cured samples. The reason is probably related to the fact that the printed layer is quite thick, so the nonuniformity of surface did not have dramatic effect on the sheet resistance. See Table3 for these results.Figure8 shows the scanning electron microscope images of a cross-section of sample C2 (photonically cured antenna on cardboard), demonstrating that a 20 μm thick layer of ink has penetrated. This shows excellent adhesion between the dispensed ink and substrate and leads to remarkable durability.Figure 8
SEM image of a cross-section area of C2, which shows the graphene layer and cardboard interface.After the antenna manufacturing, the tag integrated circuits (IC) were attached. The utilized IC was NXP UCODE G2iL series RFID IC with a wake-up power of −18 dBm (15.8μW) that was provided by the manufacturer in a strap structure with 3 × 3 mm2 pads. The pads were attached to the antenna with conductive silver epoxy (Circuit Works CW2400).


## 5. Wireless Measurements

The tags’ performances were wirelessly measured with a Voyantic Tagformance system [13]. It contains an RFID reader with an adjustable transmission frequency (0.8⋯1 GHz) and output power (up to 30 dBm) and providing the recording of the backscattered signal strength (down to −80 dBm) from the tag under test.The tag’s lowest continuous-wave transmission power (threshold power:Pth) was recorded. Here Pth is defined as the lowest power at which a valid 16-bit random number from the tag is received as a response to the query command in ISO 18000-6C communication standard. In addition, the wireless channel from the reader antenna to the location of the tag under test was first characterized using a system reference tag with known properties. As has been detailed in [14], this enabled us to estimate the attainable read range of the tag (dtag) versus frequency from(1)dtag=λ4πEIRPΛPth∗Pth,where λ is the wavelength transmitted from the reader antenna, Pth is the measured threshold power of the tag, Λ is a known constant describing the sensitivity of the system reference tag, Pth∗ is the measured threshold power of the RFID system reference tag, and EIRP is the emission limit of an RFID reader, given as equivalent isotropic radiated power. Here EIRP = 3.28 W, which is the emission limit in European countries.Figure9 shows the read range values of the 3D printed graphene RFID tags (from 800 MHz to 1000 MHz) on cardboard, wood, and textile, fabricated by using the two different curing methods. According to the results shown in Figure 9 and Table 3, all photonic-cured tags feature longer read ranges compared to similar oven-cured samples. For instance, the read range peak for a photonic-cured tag on cardboard (C2) is about 5.4 meters, while it is about 4.8 meters for the oven-cured tag (C1). The tags on cardboard show longest read ranges, compared to tags on fabric and wood substrates. The reason lies on the properties of the substrate materials and depends on, for example, spreading of the ink on the substrate and absorption of the ink into the substrate, along with the photonic curing limitations of the antennas on fabric and wood, where a lower HV value and pulse numbers had to be used, compared to the cardboard samples (see Table 2 for the used curing/drying parameters).Figure 9
Read range values of oven- and photonic-cured graphene tags on cardboard (C1, C2), wood (W1, W2), and fabric (F1, F2).The same tag antenna design has been previously fabricated from copper tape. This tag is a good reference for the fabricated graphene tags, and it showed peak read ranges of approximately 12 meters [15]. The same tag design has also been reported to be 3D-printed using silver and copper inks [16]. The achieved peak read ranges for the copper- and silver-based tags were around 6 and 11 meters, respectively. Thus, the graphene tags cannot yet offer comparable read ranges, due to the higher sheet resistance of the dispensed graphene layer.The results achieved in this study show the effectiveness of photonic curing, which, based on these achieved outcomes, could replace the heating in case of printed graphene structures. This would significantly cut down the manufacturing time.


## 6. Conclusion

Using 3D printing and subsequent photonic curing introduces a fast and cost-effective way for graphene-based antenna manufacturing on versatile substrates. In this study, photonic-cured tags showed longer read ranges, from 4 to 5.4 meters, compared to similar oven-cured samples on all three studied substrates, textile, cardboard, and wood. To the best of our knowledge, these results are the first ones presenting 3D printed and photonically cured graphene antennas.



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*Source: 7327398-2017-06-20.xml*