# A Circular Polarized Rectenna with Out-of-Band Suppression for Microwave Power Transmission

Authors: Weijun Hong; Yanjie Cao; Li Deng; Shufang Li; Mengmeng Li; Hongjie Liu
Journal: International Journal of Antennas and Propagation
 (2016)

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## Abstract

A novel circular polarized rectenna with out-of-band suppression is proposed in this paper. The circular polarization is realized by corner perturbation on a rectangular radiation patch and enhanced by a diagonal slim slot etched at the center of the patch. An open stub connecting to the quarter wavelength impedance transformer is used to suppress out-of-band wave through harmonics notching. The results of simulations and experiments agree very well, which show that the rectenna obtained −19 dB return loss at 2.4 GHz and −15.5 dB, −18.1 dB, and −11.4 dB suppression on second, third, and fourth harmonic frequency bands, respectively. The reflection coefficient in overall out-of-band, up to 10 GHz, is limited up to −3 dB. Integrated with a voltage doubling rectification circuit, the proposed rectenna can obtain 75.5% RF-to-DC conversion efficiency.


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## Body

## 1. Introduction

In recent years, wireless power transmission (WPT) has become an intriguing solution for contactless powering of low power consuming electronic devices, such as wireless sensors and body area network devices [1]. WPT can be achieved by different approaches such as near-field inductive coupling [2], magnetic resonant coupling [3, 4], and microwave power transmission (MPT) [5–19]. Comparing with the previous two power transferring approaches, MPT exhibits significant advantages on the ability of energy transfer direction controlling and much longer transmission range. In MPT systems, the terminals are supposed to be driven by direct current (DC) voltage; thus, to power the terminal, the RF front end of the MPT should be followed by a rectification circuit which transfers the alternative voltage at microwave frequency from receiving antenna to DC voltage output. Beside the large size, issues on mechanical connection and impedance mismatching between the antenna and the rectifier would inevitably cause reduction on energy conversion efficiency of the system.Rectenna is proposed as a solution for abovementioned problem, which acts as a microwave-to-dc power converter and is designed as a single device combing the functionality of receiving antenna and rectifier. Thus, the performance of rectenna has become one of the most important factors affecting the efficiency of MPT system. Traditional rectennas consist of a receiving antenna, a band-pass filter (BPF), a matching circuit, a rectifier, a low pass filter, and loads. The BPF is used for reflecting the harmonics generated by rectifier diodes due to their nonlinearity, therefore improving the efficiency of energy conversion. However, the general BPF has a large dimension and introduces nonnegligible insertion loss.Recent researches on rectenna proposed several methods to enhance power collection and conversion efficiency. The authors in [7–9] proposed multiband antennas to broaden the frequency band of power collection, which simultaneously raises difficulties on design of matching circuit. The authors in [10, 11] used antenna array to increase the gain of the receiver at particular receiving direction, which enlarged the overall size to times of single antenna and significantly increased the requirements on radiation pattern alignment between receiving antenna and the source. In [12–15], combinations of antenna and harmonic suppression filter were proposed to suppress the out-of-band signal; however, their structures are so complicated that they highly impact the power collection efficiency of the receiving antenna.A novel high efficiency rectenna with out-of-band suppression is proposed in this paper, which has two significant advantages: first, circular polarization is used to minimize the polarization mismatch to linear polarized transmitter; second, an open stub on transmission line and fan-shaped printed circuit instead of conventional BPF is designed to suppress harmonics at front-end and backend which finally alleviate out-of-band fluctuation. The performance of two types of filtering structure, single branch and double branch, is studied in this paper, and the previous one is finally adopted in the proposed rectenna. The rest of this paper is organized as follows. Section2 presents the design of rectenna including the design of circular polarized antenna and rectification circuit. Section 3 shows the results of simulations and experiments. Finally, conclusions are drawn in Section 4.


## 2. Rectenna Design

### 2.1. Antenna

Figure1 shows the antenna part of proposed rectenna. The configurations of corresponding parameters are listed in Table 1. The length of the patch is quarter wavelength which can be calculated by (1)L=14fε0μ01+εr/2,where f is the resonant frequency of antenna, ε0 and μ0 are the permittivity and permeability of air, respectively, and εr is the relative permittivity of substrate.Table 1
Dimensions of proposed antenna.
Parameter Value /mm L 1 28.9 L 2 8.4 L 3 4.0 L 4 16.8 L 5 10.0 D 5.0 W 1 28.9 W 2 0.4 W 3 3.0 W 4 0.6 W 5 2.9 W 6 2.0Figure 1
The layout of antenna part of proposed rectenna.The substrate of the proposed antenna is FR4, which has 1.5 mm thickness with dielectric constant of 4.4. The methods of slotting and corner perturbation are used to realize the circular polarization. A 4 mm∗ 3 mm stub connected to the quarter wave length impedance converter is used to suppress the harmonics at the higher order modes. The stub works as a half wavelength open circuit resonator whose length is about half wavelength of the second harmonics. The quarter wave length impedance transformer is used to match the input impedance of radiation patch to 50 Ω input port.


### 2.2. Rectification Circuit

We adopt the classical voltage doubling rectification circuit,Greinacher circuit, in the design. The circuit consisted of a 100 pF capacity cascaded with a ring composed of two Schottky diodes HSMS2862 and one 100 pF capacitor, as shown in Figures 2 and 3. As introduced in [16], HSMS2862 has a threshold voltage level of 650 mV, internal resistance of 6 Ω, and a breakdown voltage of 7 V and can work well up to 5.8 GHz. To reduce the high frequency fluctuation on output wave, a bypass capacitor would generally be used after the rectifier to conduct the alternating component to ground that would definitely cause power loss. Actually, the alternating signals in output wave are harmonic waves caused by the nonlinearity of diode. In this paper, we designed a printable fan-shape filtering structure to replace the low pass filter. The fan-shaped filtering structure can reflect the harmonics back to the rectification circuit, and these signals would partly be rectified to DC signal output; thus, the power transfer efficiency can be improved.Figure 2
The layout of single branch structure cascaded with rectification circuit and fan-shaped filtering structure.Figure 3
The layout of double branch structure cascaded with rectification circuit and fan-shaped filtering structure.As is known, the input impedance of Schottky diode varies with the input power that would cause issues of impedance mismatch between the antenna and the backend circuit with different receiving signal strength of antenna. In MPT systems, the terminal devices are probably in a state of motion during wireless charging process; thus, it is a great challenge on design of impedance match circuit. We proposed two impedance match structures here, single branch matching structure (SBS) as shown in Figure2 and double branch matching structure (DBS) as shown in Figure 3, and tested their performance in Section 3.


## 2.1. Antenna

Figure1 shows the antenna part of proposed rectenna. The configurations of corresponding parameters are listed in Table 1. The length of the patch is quarter wavelength which can be calculated by (1)L=14fε0μ01+εr/2,where f is the resonant frequency of antenna, ε0 and μ0 are the permittivity and permeability of air, respectively, and εr is the relative permittivity of substrate.Table 1
Dimensions of proposed antenna.
Parameter Value /mm L 1 28.9 L 2 8.4 L 3 4.0 L 4 16.8 L 5 10.0 D 5.0 W 1 28.9 W 2 0.4 W 3 3.0 W 4 0.6 W 5 2.9 W 6 2.0Figure 1
The layout of antenna part of proposed rectenna.The substrate of the proposed antenna is FR4, which has 1.5 mm thickness with dielectric constant of 4.4. The methods of slotting and corner perturbation are used to realize the circular polarization. A 4 mm∗ 3 mm stub connected to the quarter wave length impedance converter is used to suppress the harmonics at the higher order modes. The stub works as a half wavelength open circuit resonator whose length is about half wavelength of the second harmonics. The quarter wave length impedance transformer is used to match the input impedance of radiation patch to 50 Ω input port.


## 2.2. Rectification Circuit

We adopt the classical voltage doubling rectification circuit,Greinacher circuit, in the design. The circuit consisted of a 100 pF capacity cascaded with a ring composed of two Schottky diodes HSMS2862 and one 100 pF capacitor, as shown in Figures 2 and 3. As introduced in [16], HSMS2862 has a threshold voltage level of 650 mV, internal resistance of 6 Ω, and a breakdown voltage of 7 V and can work well up to 5.8 GHz. To reduce the high frequency fluctuation on output wave, a bypass capacitor would generally be used after the rectifier to conduct the alternating component to ground that would definitely cause power loss. Actually, the alternating signals in output wave are harmonic waves caused by the nonlinearity of diode. In this paper, we designed a printable fan-shape filtering structure to replace the low pass filter. The fan-shaped filtering structure can reflect the harmonics back to the rectification circuit, and these signals would partly be rectified to DC signal output; thus, the power transfer efficiency can be improved.Figure 2
The layout of single branch structure cascaded with rectification circuit and fan-shaped filtering structure.Figure 3
The layout of double branch structure cascaded with rectification circuit and fan-shaped filtering structure.As is known, the input impedance of Schottky diode varies with the input power that would cause issues of impedance mismatch between the antenna and the backend circuit with different receiving signal strength of antenna. In MPT systems, the terminal devices are probably in a state of motion during wireless charging process; thus, it is a great challenge on design of impedance match circuit. We proposed two impedance match structures here, single branch matching structure (SBS) as shown in Figure2 and double branch matching structure (DBS) as shown in Figure 3, and tested their performance in Section 3.


## 3. Results and Discussion

### 3.1. Performance of Antenna

Figure4 shows the frequency behavior of the antenna reflection coefficient for antenna with and without slot. From the figure, we can see that slot in the center of radiation patch of the antenna can significantly improve the return loss at antenna resonant frequency 2.4 GHz, although it does not provide any improvements in out-of-band. That is because the slot makes the reactance of proposed antenna approach 0 Ω as shown in the circled part of Figure 5, but barely with effect on other frequencies as well as on resistance of the antenna. Figure 6 shows more important functionality of slot on cross polarization enhancement. From Figure 6, it appears that the main polarization pattern of proposed antenna is left-hand circular polarization (LHCP), and the slot improves the cross polarization with 18.27 dB, from 4.98 dB (without slot) to 23.25 dB (with slot).Figure 4
Simulated reflection coefficient characteristics for proposed antenna with and without slot.Figure 5
Simulated impedance for proposed antenna with and without slot.Figure 6
Radiation pattern of the antenna (a) without slot and (b) with slot.
(a) (b)Figure7 shows the simulated S11 of proposed antenna with and without stub. From the figure, we can see that the antenna without stub has four resonant frequencies at 2.2 GHz, 4.9 GHz, 6.1 GHz, and 9.2 GHz, with reflection coefficients −9.29 dB, −18.91 dB, −21.59 dB, and −13.98 dB, respectively. After adding the stub, the basic resonant frequency is tuned to 2.4 GHz with −18.28 dB reflection coefficient, and the reflection coefficient in all out-of-band is suppressed to greater than −3 dB. A prototype of the proposed antenna is fabricated as shown in Figure 8. The measured reflection coefficient is plotted in Figure 7. We can see that the results of simulation and experiment match very well.Figure 7
Simulated reflection coefficient for antenna with and without stub, and measured result of reflection coefficient of antenna.Figure 8
Prototype of the proposed antenna.


### 3.2. Performance of Rectification Circuit

Performance of proposed rectification circuit is simulated with software Agilent ADS. Figures9 and 10 show that the input impedance of SBS and DBS varies with the input power, respectively. The resistance of DBS decreases dramatically when input power is greater than 20 dBm, while its reactance keeps steady at about 6 Ω, as shown in Figure 9. In contrast, the resistance of SBS increases obviously to about 100 Ω at 28 dBm input power and then decreases dramatically, and its reactance keeps increasing fast to about 155 Ω with 40 dBm input power. However, while under lower input power, 19 dBm of SBS and 21 dBm of DBS, the impedance curves of both structures are quite flat, which means that both structures can work well in ambient power collection which would probably be less than 20 dBm. From Figure 11, we can see that the proposed system can provide 5.45 V DC voltage with a 19 dBm sinusoid wave input at 2.4 GHz, which is adequate for most portable devices, such as wireless sensors and body area network devices, even mobile phones.Figure 9
Input impedance of SBS.Figure 10
Input impedance of DBS.Figure 11
Output voltage of rectification circuit with 18 dBm input sinusoidal wave.Figures12 and 13 show the efficiency of SBS and DBS rectification circuits as function of input power. Figure 12 shows that the efficiency of SBS increases from 63% to 75.5% within the input power range from 10 dBm to 19 dBm and turns to decrease after input power beyond 19 dBm. The efficiency curve of DRC has similar trend as shown in Figure 13, but with different turning point at 20 dBm with the highest efficiency of 50.4%.Figure 12
Efficiency of SBS.Figure 13
Efficiency of DBS.By contrasting Figures12 and 13, it appears that SBS outperforms DBS on efficiency; thus, we adopted SBS to be the rectification structure in our MPT system. The manufactured prototype of SBS is shown in Figure 14. We use a Universal Software Radio Peripheral (USRP) to generate the input signal for performance validation of the rectification circuit. The frequency and power of the signal generated by USRP can be feasibly adjusted by programming on development platform Labview. The output power of signal is calibrated by spectrum analyzer, as shown in Figure 15. The measurement process is shown in Figure 16; we connect the output port of USRP to SBS input port and use a AVO meter to measure the DC voltage at the output port. The measurement result agrees with the simulation result in Figure 11, and the deviation is only 0.2 V.Figure 14
Prototype of the SBS rectification circuit.Figure 15
Experimental setups: an USRP is used to generate signal for the MPT system, the frequency and power of signal are controlled by programming on development platform Labview, and the power of signal is calibrated with spectrum analyzer.Figure 16
Experiment to validate the performance of proposed system.In Table2, the efficiency performance of the proposed rectenna is compared with those of some published rectenna designs. Obviously, the proposed rectenna is able to achieve good impedance matching and higher conversion efficiency than most of current designs.Table 2
Comparison of conversion efficiency of different rectennas.
Rectenna structure Max conversion efficiency [8] 65.2% [17] with dual patch 70% [17] with 6-patch array or 16-patch array 74% [18] 37.1% [19] 70% This work 75.5%


## 3.1. Performance of Antenna

Figure4 shows the frequency behavior of the antenna reflection coefficient for antenna with and without slot. From the figure, we can see that slot in the center of radiation patch of the antenna can significantly improve the return loss at antenna resonant frequency 2.4 GHz, although it does not provide any improvements in out-of-band. That is because the slot makes the reactance of proposed antenna approach 0 Ω as shown in the circled part of Figure 5, but barely with effect on other frequencies as well as on resistance of the antenna. Figure 6 shows more important functionality of slot on cross polarization enhancement. From Figure 6, it appears that the main polarization pattern of proposed antenna is left-hand circular polarization (LHCP), and the slot improves the cross polarization with 18.27 dB, from 4.98 dB (without slot) to 23.25 dB (with slot).Figure 4
Simulated reflection coefficient characteristics for proposed antenna with and without slot.Figure 5
Simulated impedance for proposed antenna with and without slot.Figure 6
Radiation pattern of the antenna (a) without slot and (b) with slot.
(a) (b)Figure7 shows the simulated S11 of proposed antenna with and without stub. From the figure, we can see that the antenna without stub has four resonant frequencies at 2.2 GHz, 4.9 GHz, 6.1 GHz, and 9.2 GHz, with reflection coefficients −9.29 dB, −18.91 dB, −21.59 dB, and −13.98 dB, respectively. After adding the stub, the basic resonant frequency is tuned to 2.4 GHz with −18.28 dB reflection coefficient, and the reflection coefficient in all out-of-band is suppressed to greater than −3 dB. A prototype of the proposed antenna is fabricated as shown in Figure 8. The measured reflection coefficient is plotted in Figure 7. We can see that the results of simulation and experiment match very well.Figure 7
Simulated reflection coefficient for antenna with and without stub, and measured result of reflection coefficient of antenna.Figure 8
Prototype of the proposed antenna.


## 3.2. Performance of Rectification Circuit

Performance of proposed rectification circuit is simulated with software Agilent ADS. Figures9 and 10 show that the input impedance of SBS and DBS varies with the input power, respectively. The resistance of DBS decreases dramatically when input power is greater than 20 dBm, while its reactance keeps steady at about 6 Ω, as shown in Figure 9. In contrast, the resistance of SBS increases obviously to about 100 Ω at 28 dBm input power and then decreases dramatically, and its reactance keeps increasing fast to about 155 Ω with 40 dBm input power. However, while under lower input power, 19 dBm of SBS and 21 dBm of DBS, the impedance curves of both structures are quite flat, which means that both structures can work well in ambient power collection which would probably be less than 20 dBm. From Figure 11, we can see that the proposed system can provide 5.45 V DC voltage with a 19 dBm sinusoid wave input at 2.4 GHz, which is adequate for most portable devices, such as wireless sensors and body area network devices, even mobile phones.Figure 9
Input impedance of SBS.Figure 10
Input impedance of DBS.Figure 11
Output voltage of rectification circuit with 18 dBm input sinusoidal wave.Figures12 and 13 show the efficiency of SBS and DBS rectification circuits as function of input power. Figure 12 shows that the efficiency of SBS increases from 63% to 75.5% within the input power range from 10 dBm to 19 dBm and turns to decrease after input power beyond 19 dBm. The efficiency curve of DRC has similar trend as shown in Figure 13, but with different turning point at 20 dBm with the highest efficiency of 50.4%.Figure 12
Efficiency of SBS.Figure 13
Efficiency of DBS.By contrasting Figures12 and 13, it appears that SBS outperforms DBS on efficiency; thus, we adopted SBS to be the rectification structure in our MPT system. The manufactured prototype of SBS is shown in Figure 14. We use a Universal Software Radio Peripheral (USRP) to generate the input signal for performance validation of the rectification circuit. The frequency and power of the signal generated by USRP can be feasibly adjusted by programming on development platform Labview. The output power of signal is calibrated by spectrum analyzer, as shown in Figure 15. The measurement process is shown in Figure 16; we connect the output port of USRP to SBS input port and use a AVO meter to measure the DC voltage at the output port. The measurement result agrees with the simulation result in Figure 11, and the deviation is only 0.2 V.Figure 14
Prototype of the SBS rectification circuit.Figure 15
Experimental setups: an USRP is used to generate signal for the MPT system, the frequency and power of signal are controlled by programming on development platform Labview, and the power of signal is calibrated with spectrum analyzer.Figure 16
Experiment to validate the performance of proposed system.In Table2, the efficiency performance of the proposed rectenna is compared with those of some published rectenna designs. Obviously, the proposed rectenna is able to achieve good impedance matching and higher conversion efficiency than most of current designs.Table 2
Comparison of conversion efficiency of different rectennas.
Rectenna structure Max conversion efficiency [8] 65.2% [17] with dual patch 70% [17] with 6-patch array or 16-patch array 74% [18] 37.1% [19] 70% This work 75.5%


## 4. Conclusions

A high efficiency circular polarization rectenna with features of out-of-band suppression has been proposed for microwave power transfer system. The rectenna is in 150 mm × 55 mm overall size printed on 1.5 mm FR4 substrate. −15.5 dB, −18.1 dB, and −11.4 dB depressions on 2nd to 4th harmonic frequency band, respectively, are achieved. After harmonic suppression, the antenna shows a flatS11 curve up to −3 dB in overall out-of-band. By integrating with SBS, the proposed rectenna can achieve 75.5% RF-to-DC conversion efficiency with 19 dBm input signal power. The conversion efficiency keeps higher than 63% during input power ranging from 10 dBm to 19 dBm.The proposed rectenna can widely be applied in small size electronic devices, which can significantly enhance the capability for ambient power collection of MPT by avoiding polarization mismatch with linear polarized transmission antenna, and greatly help saving time for charging of battery or bulk capacitor in relative low RF power ambient environments with high RF-to-DC conversion efficiency.



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*Source: 8628496-2016-11-13.xml*