# An UHF RFID Reader Antenna with Multitag Identification for Extremely Low-Temperature Medical Systems

Authors: Ji S. Jung; Jung N. Lee; Joung M. Kim; Jong K. Park
Journal: International Journal of Antennas and Propagation
 (2020)

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## Abstract

A radio frequency identification reader antenna having multitag identification for medical systems is presented, which consists of four PIFAs, two hybrid couplers, and four power dividers. The high isolation is achieved by the symmetric design of the antenna geometry and four power dividers, which are fed by two hybrid couplers. The experimental results show an isolation of more than 40 dB in the North American (902–928 MHz), Korean (917–923.5 MHz), and Japanese (916.7–923.5 MHz) RFID frequency bands.


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## Body

## 1. Introduction

The low-frequency (LF) and the high-frequency (HF) RFID systems make use of inductive coupling to carry power and data transmission between the tag and the reader antenna [1]. The UHF and microwave RFID systems use the propagation of electromagnetic (EM) waves to transfer information between the tag and reader antenna. LF and HF RFID systems are used for near-field RFID systems to use their security merits. However, the large size of the antenna limits its application in small items. Because the frequency band is low, the data transmission rate is slow and the transmission data volume is limitary. The UHF near-field RFID system is receiving much attention because of its promising item-level applications in pharmaceutical and medical systems. The physical antenna size can be suitably reduced to accomplish item-level tagging for small items, which requires the attachment of small antennas. The receiving reliability of the RFID reader antenna has been enhanced by the development of an HF band mutual coupling and UHF band backscattering method that combines a UHF band near-field RFID reader antenna such as a near field of microstrip antennas [2], the near field of a wire grid model [3], UHF near-field RFID reader antenna with capacitive couplers [4], an electrically large zero-phase-shift line grid array UHF near-field RFID reader antenna [5], a planar near-field RFID reader antenna for item-level tagging [6], and a novel broadband center-fed UHF near-field RFID reader antenna [7]. Typical UHF band near-field reader antenna forms a strong perpendicular magnetic field in the aperture and provides good identification of the tag for the near field. However, it has the defect of being unable to identify the tag in the far-field region. This increases the need for a single hybrid reader antenna that can identify near- and far-field tags at the same time. The tag antennas are powered by a continuous wave RF signal transmitted by a reader, and backscattering transmission from the reader sends back their data. The RF receiver of the reader inputs not only reflected signal from the tag but also leaked waves sent from the RF transmitter. This leakage wave makes a dent in the receiving sensitivity of the reader. The directly coupled continuous wave signal is much larger than the backscattered wave from tags, and the receiving part of the reader should detect the weak signal close to such a strong operating band interferer. The research on methods for improving the isolation to minimize this leakage signal is progressing [8–14].Circularly polarized (CP) reader antennas are widely used for UHF RFID systems [15–23]. In order to obtain well-read performance, the reader antennas need to be designed for CP, because CP antennas can increase orientation diversity and reduce the loss caused by the multipath effects between the reader and the tag antenna. The feeding structures of CP antennas can be categorized into single and multifeed. Single-feed CP antennas [15–20] have the advantages of simple structure, easy manufacture, and small size. However, the single-feed CP antenna, in its simplest form, has inherently narrow AR and narrow impedance bandwidths.The multifeed CP antennas have wider bandwidths than single-feed structures. The multifeed CP antennas use a hybrid feed network [21–23] and Wilkinson power dividers. This achieves wide impedance bandwidths and AR bandwidths. However, the multifeed CP antennas have low radiation efficiency and large size. Most of these antennas either have large antenna heights or narrow impedance bandwidths, which may not be suitable for practical applications.In this paper, we present a design for a UHF RFID reader antenna having multitag identification for medical systems. We improved the isolation between the antennas by using two hybrid couplers and four power dividers. The proposed reader antenna covers a range of North American (902–928 MHz), Korean (917–923.5 MHz), and Japanese (916.7–923.5 MHz) RFID frequency bands and its Tx/Rx isolation is 40 dB. The multitag identification rate is compared using a far-field reader antenna (Alien reader antenna) and a near-field reader antenna (MTG reader antenna). The simulation and fine-tuning of the reader antenna were carried out by using the commercial software Ansys HFSS. The proposed antenna has excellent isolation characteristics and a multitag identification rate.


## 2. Design of the Planar Inverted F Antenna

The geometry and dimensions of the configuration are depicted in Figure1. It has the dimensions of 150 mm × 150 mm, and the dielectric substrate of FR-4 (thickness: 1.0 mm, εr = 4.4, loss δ = 0.025) is used.Figure 1
Geometry of the proposed PIFA.The prototype consists of three 0.035 mm thickness copper layers with the one antenna and upper ground plane placed at the top and a bottom ground plane placed at the bottom. The antenna is probe fed and a shorting line connects the upper ground plane.Figure2 shows the measured and simulated reflection coefficient of the Planar Inverted F Antenna (PIFA). The simulation results are obtained using the simulation tool Ansys HFSS [24], and the reliability of the obtained results is confirmed. The measured frequency ranges from 860 to 960 MHz in the UHF band and has a 100 MHz bandwidth, which agrees well with the HFSS simulated results. We investigated the effects of the geometrical parameters on the reflection coefficient by measuring the reflection coefficients for the different parameters.Figure 2
Measured and simulated results of the PIFA.Figure3 shows the measured reflection coefficient for different radiator lengths and separation distances between the shorting and feed lines. Figure 3(a) shows that as the radiator length (L) is increased, the UHF RFID frequency band is moved to the lower frequency. The optimized value in this design is 70 mm. The whole antenna structure cannot be changed, and the frequency can be controlled rather simply. As shown in Figure 3(b), as the distances (D) between the shorting and feed lines increases, the antenna impedance becomes poor. The optimized value in this design is 14 mm.Figure 3
Effects of antenna geometry on reflection coefficient: (a) radiator length and (b) separation distances between a shorting line and a feed line.
(a)(b)The measured and simulated radiation patterns at 860, 920, and 960 MHz for the proposed antenna are plotted in Figure4. The radiation patterns in the xz-plane are nearly omnidirectional for all frequencies, and those in the yz-plane are very monopole-like. These radiation patterns are also stable across the respective operating frequency bands. The measured antenna gains are 2.7 dBi at 860 MHz, 2.9 dBi at 920 MHz, and 3.2 dBi at 960 MHz.Figure 4
Measured and simulated radiation patterns: (a)yz-plane and (b) xz-plane.
(a)(b)


## 3. Design of the RFID Reader Antenna

The RFID reader antenna can be configured with two or more separated radiating elements for transmitting and receiving, and their separation distance is set to be large enough to give the required Tx and Rx isolation. However, the overall antenna size depends upon the separation distance between radiating elements, and very much larger antenna size is needed to achieve higher Tx and Rx isolation. In addition, a circulator is used for a reader antenna between the transmitter and receiver for the cancellation of the transmit leakage wave. However, when the reader antenna is not matched to the circulator, the isolation between the transmitter and receiver is affected by the reflection coefficient of the reader antenna.Figure5 shows the equivalent circuits with a Wilkinson power divider, which has two hybrid couplers. The scattering matrix for the ideal 3-dB hybrid coupler is as follows:(1)b1ap1′ap4′b4=−120j10j001100j01j0a1bp1′bp4′a4,(2)b2bp2bp3b3=−120j10j001100j01j0a2ap2ap3a3.Figure 5
The equivalent circuits with a Wilkinson power divider.The scattering matrix of the ideal 90° Wilkinson power divider is expressed as follows:(3)bp1b5ap2=−j2011100100ap1a5bp2,(4)bp4b6ap3=−j2011100100ap4a6bp3.From equations (1)–(4), input and output equations are given as follows:(5)b1b4=−12j11jbp1′bp4′,ap1′bp4′=−12j11ja1a4,b2b3=−12j11jap2ap3,bp2bp3=−12j11ja2a3.It can be substituted by the following equation:(6)bp1bp4=bp2bp3,ap2ap3=a5a6=Γa00Γbb5b6,b5b6=ap2ap3.Two transfer functions for input and output:(7)b1b4=−12j11jbp1′bp4′,bp1′bp4′=βa00βbbp1bp4,b1b4=−12j11jβa00βbbp1bp4=−12j11jβa00βb−12j11ja2a3=12−βa−βbjβa+βbjβa+βbβa−βba2a3,b2b3=−12j11jΓa00Γbap1ap4,ap1ap4=βa00βbap1′ap4′,b2b3=−12j11jΓa00Γbβa00βb−12j11ja1a4=12−βaΓa−βbΓbjβaΓa+βbΓbjβaΓa+βbΓbβaΓa−βbΓba1a4,where βa and βb are the amplitude and phase errors of the compensated circuits in paths. The four-port equations for a hybrid coupler with Wilkinson power divider have the following scattering matrix:(8)b1b2b3b4=120−βa−βbjβa+βb0−βaΓa−βbΓb00jβaΓa+βbΓbjβaΓa+βbΓb00βaΓa−βbΓb0jβa+βbβa−βb0a1a2a3a4.When the ideal case (βa=βb=1),(9)b2a1=−12Γa−Γb=0.The scattering matrix seen by the Tx and Rx ports can be expressed as follows:(10)a5a6=ΓaCCΓbb5b6,where a5 and a6 represent the incident wave and reflected wave, Γa and Γb are reflection coefficients, and C is the coupling coefficient.We can derive the reflection coefficient at the antenna port as follows:(11)RL=−20logb1a1=−20log12Γb−Γa+jC.As the proposed reader antenna has a rotationally symmetrical geometry,Γa and Γb are equal, and from (10),(12)RL=−20logC.The reflection coefficient (RL) at the reader antenna port is the same as the isolation between ports Tx and Rx, if the 90° Wilkinson power divider is ideal.This article presents a four-feed PIFA, two hybrid couplers, and four Wilkinson power dividers with wide beamwidths and bandwidths. The proposed antenna artificially reduced the gain of the antenna by using two hybrid couplers and four Wilkinson power dividers. We need low read distances for medical application as this will prevent the reading of unnecessary tags in the vicinity. The radiating patch is fed by the feed network with equal amplitude and the antenna consists of four PIFAs sequentially rotated and fed with phase angles of 0°, 90°, 180°, and 270°.The geometry of the proposed reader antenna is shown in Figure6. The antenna is composed of four printed PIFAs, two hybrid couplers, and four Wilkinson power dividers. The four printed PIFAs are sequentially rotated and fed with equal amplitudes, but with different phase angles 0°, 90°, 180°, and 270°. The proposed reader antenna has dimensions of 150 mm × 150 mm, and the dielectric substrate of FR-4 (thickness: 1 mm, εr: 4.4, δ = 0.025) is used. Four print PIFA feed points are directly connected to the bottom microstrip feed line network (A, B, C, and D). The optimal parameters can be chosen as AL = 70 mm, AW = 5 mm, AL2 = 50 mm, and AH = 17 mm based on the extensive simulation using Ansys HFSS. Figure 7 shows the simulated results for the feed point arrangements.Figure 6
Geometry of the proposed reader antenna: (a) Top plane and (b) bottom plane.
(a)(b)Figure 7
Simulated mutual coupling against frequency between feed point, and radiator point.The printed PIFA was then removed and the antenna part was replaced by a metal ground. The simulations were performed using Ansys HFSS. Figure7 shows that the value of min Sba,Sca is the smallest. Therefore, because Sca > Sba, port b should be used as the Rx port corresponding to the Tx port a. Port c and d were terminated with 50 Ω. The simulation was performed in order to investigate the characteristics of the mutual coupling between the radiator point (A, B, C, and D). In all cases, the obtained characteristic of 20 dB isolation is shown in Figure 7.


## 4. Experiment Results of the Proposed Reader Antenna

The proposed reader antenna design approach is verified by implementing a prototype antenna and measuring its performance. The simulation results have been obtained from commercial Ansys HFSS software to ensure that the obtained results are trustworthy. The reflection coefficient and isolation of the reader antenna were measured with an Agilent Vector Network Analyzer (85107B) in an anechoic chamber.Figure8(a) shows the measured input impedance on a Smith chart for the two feed port (Tx and Rx ports) of the reader antenna; they clearly have the same behavior over the frequency range. Figure 8(b) shows the measured reflection coefficient and interport coupling between the Tx ports. The antenna is operated from 780 to 1000 MHz with a bandwidth of 25%. The impedance bandwidth obtained is wide enough to cover North American (902–928 MHz), Korean (917–923.5 MHz), and Japanese (916.7–923.5 MHz) applications. The measured interport coupling between the Tx and Rx ports of the proposed antenna is better than 40 dB over the frequency band.Figure 8
Measured input impedance, reflection coefficient, and interport coupling of the proposed reader antenna: (a) input impedance on a Smith chart and (b) reflection coefficient and isolation.
(a)(b)Figure9 shows the measured radiation patterns of the proposed reader antenna at resonant frequencies 902, 920, and 928 MHz for the Tx port. Experimental results of the radiation patterns were obtained in an anechoic chamber at the Korea RFID/USN Center, Inchon, and the Republic of Korea. The antenna gains and radiation patterns were measured in the middle range using an Agilent E5071C antenna measurement system. The antenna has stable radiation patterns and low back lobes across the entire bandwidth. The antenna has a symmetrical design, so the radiation patterns are almost symmetrical. The measured radiation performance is given in Table 1.Figure 9
Measured radiation patterns: (a)yz-plane at 902 MHz, (b) yz-plane at 920 MHz, (c) yz-plane at 928 MHz, (d) R/LHCP at 902 MHz, (e) R/LHCP at 920 MHz, and (f) R/LHCP at 928 MHz.
(a)(b)(c)(d)(e)(f)Table 1
Measured radiation performance of the reader antenna.
Frequency (MHz)Gain (dBic)AR (dB)HPBW (deg)F/B ratio (dB)Efficiency (%)Bore sightBore sightyz-planxz-planyz-planxz-plan902Sim.0.60.8290°68°11.81238Mea.0.530.894°70.81°1212.6730.3920Sim.1.921.0272°65°10.0811.2352Mea.1.03180°70.51°1111.9746.9928Sim.1.20.8870°66.5°910.7241Mea.0.980.875°70.09°9.610.9839.43


## 5. Experiment Results of Multitag Identification Rate for Medical Sample Tube

We published a paper on an ultracompact UHF passive RFID tag antenna for medical sample tubes [25]. The multitag identification rate was compared using two types of reader antenna (far and near-field). We measured the reading range and multitag identification rate using the proposed reader antenna.The tag antenna was described in [25] and the number of sample tubes is one hundred medical sample tubes. Figure 10 shows the setup environment of multitag identification rate. The medical sample tubes are measured using three types of reader antenna: near-field (MT-269508), far-field (ALA-97C), and the proposed reader antenna. The reader antennas are positioned under the sample tube box at the separation distance, and tag identifications is performed. The multitag identification rate measurement is carried out in an anechoic chamber at the Korea RFID/USN Center, Inchon, the Republic of Korea. The input power of the reader is 1 W (30 dBm). The medical sample tubes are measured at an interval of four seconds, and the reader antenna automatically moves from 10 mm to 100 mm.Figure 10
Setup environment of multitag identification rate: (a) alien far-field reader antenna, (b) MTG near-field reader antenna, and (c) proposed reader antenna.
(a)(b)(c)Figure11 shows the measured reading range and multitag identification rate for three cases. From the figure, the near-field reader antenna is identified to have a maximum of 95 sample tubes at 10 mm, the far-field reader antenna is identified to have a maximum of 88 sample tubes at 20 mm, and the proposed reader antenna is identified to have a maximum of 100 sample tubes at 10 mm. The proposed reader antenna is perfectly identified at 10 mm. We need low read distances for medical application as it will prevent reading unnecessary tags in the vicinity, and, hence, the proposed reader antenna performs better than a regular high-gain antenna. Table 2 is a comparison with references [6, 7]. Both antennas are near-field reader antennas. As shown in the table, it can be confirmed that the multitag identification rate and the number of the proposed reader antenna is excellent.Figure 11
The number of tag identification.Table 2
Tag identification rate comparison.
ProposedRef [6]Ref [7]Frequency (MHz)780–1000910–940814–1050Gain (fc = 920 MHz)1.03 dBic6.8 dBi—Size (mm)150 × 150 × 1300 × 300 × 100170 × 170 × 1Reader typeFar-fieldNaer-fieldNaer-fieldNumber of tags (EA)10010025Tag identification (%)10080100Freeze preservation is required to prevent the degradation of blood and human tissue samples. The RFID system used presently in the smart cold chain operates at −40°C, but no system currently available can operate at −80°C. The real-time use of an RFID system at extremely low temperatures is very difficult because of the serious electric wave distortion due to humidity and frost. We performed measurements on medical sample tubes filled with a normal saline solution at an extremely low temperature (−80°C). These extremely low temperature experiments were performed at the Chungnam National University Hospital, Daejeon, the Republic of Korea. We measured the identification rate at 3-week intervals for 10 sample tube boxes placed in a freezer. Figure12 shows the setup of an extremely low temperature experiment.Figure 12
Setup environment of an extremely low temperature experiment: (a) sample tube boxes placed in a freezer, (b) setup temperature, (c) measurement setup, and (d) measured results.
(a)(b)(c)(d)The measurements obtained at an extremely low temperature are given in Table3. As shown in Table 3, the proposed reader antenna completely identified all samples in extremely low temperature condition for all periods.Table 3
Measurement performance at an extremely low temperature.
Week (W)Tube box samples123456789101100100100100100100100100100100310010010010010010010010010010061001001001001001001001001001009100100100100100100100100100100


## 6. Conclusion

In this paper, we present the design of a UHF RFID reader antenna that uses the far-field region. We improved the isolation between antennas by using two hybrid couplers and four power dividers. The proposed reader antenna was designed, fabricated, and tested for UHF RFID applications. The proposed reader antenna covers a range of 860 MHz to 960 MHz and its Tx/Rx isolation is 40 dB. A comparison of the multitag identification rate of the far-field reader antenna and a near-filed reader antenna shows that the proposed reader antenna has an excellent isolation feature and multitag identification rate. Measurement results also showed that the proposed reader antenna could completely identify all samples even at extremely low temperature conditions.



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*Source: 2482961-2020-07-10.xml*