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A millimeter-wave fundamental and subharmonic hybrid CMOS mixer for dual-band applications

Published online by Cambridge University Press:  09 September 2020

Fang Zhu
Affiliation:
Key Laboratory of RF Circuits and Systems of Ministry of Education, School of Electronics and Information, Hangzhou Dianzi University, Hangzhou, 310018, China
Guo Qing Luo*
Affiliation:
Key Laboratory of RF Circuits and Systems of Ministry of Education, School of Electronics and Information, Hangzhou Dianzi University, Hangzhou, 310018, China
*
Author for correspondence: Guo Qing Luo, E-mail: luoguoqing@hdu.edu.cn
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Abstract

This paper proposes and presents a millimeter-wave (MMW) fundamental and subharmonic hybrid mixer in a 65-nm CMOS technology. Based on a hybrid structure with two switching quads and a quasi-diplexer, the proposed circuit can function either as a fundamental mixer (FM) or a subharmonic mixer (SHM) for dual-band applications. An application of the MMW hybrid mixer in a concurrent dual-band receiver is also discussed, which indicates that the proposed mixer can operate at two different MMW frequency bands concurrently as long as the frequency conversion schemes are carefully designed. Measured results show that the 3-dB RF bandwidth of the MMW hybrid mixer ranges from 16 to 35 GHz for the FM mode and 30 to 53 GHz for the SHM mode, respectively.

Type
Frequency Mixers
Copyright
Copyright © The Author(s), 2020. Published by Cambridge University Press in association with the European Microwave Association

Introduction

With the development of wireless communication, sensing, and radar systems, demands for low-cost circuits and transceivers that can support multi-band and multi-mode operation are increasing rapidly [Reference Wolf, Joram, Schumann and Ellinger1Reference Jain, Tzeng, Zhou and Heydari8]. As a key component of dual-band transceivers, dual-band mixers deserve in-depth study.

Several dual-band fundamental mixers (FMs) with dual-band impedance matching networks have been developed under 6 GHz [Reference Abdelrheem, Elhak and Sharaf9Reference Hwang, Yoo and Yoo11]. However, it is difficult to implement local oscillators (LOs) with low phase noise and wide turning range at millimeter-wave (MMW) frequencies. By either mixing the input signal with the fundamental or higher-order harmonic component of the LO, dual-band performance can also be achieved [Reference Jackson and Saavedra12, Reference El-Nozahi, Amer, Sánchez-Sinencio and Entesari13]. The mixers, which can be reconfigured between fundamental and subharmonic modes by changing the LO waveforms [Reference Mazzanti, Vahidfar, Sosio and Svelto14] or the bias conditions [Reference Zhu, Wang and Wu15], have also been proposed for dual-band operation. In addition, an MMW dual-band switchable star mixer was also proposed by changing the effective length of the Marchand baluns [Reference Wang, Hou, Chen and Hong16]. However, these mixers can operate only in one band at a time, which are not suitable for concurrent dual-band applications [Reference Hashemi and Hajimiri17Reference Zhang, Hasan, Ghannouchi, Helaoui, Wu, Yu and Liu20].

In this paper, a fundamental and subharmonic hybrid CMOS mixer is proposed for MMW dual-band applications. Based on a hybrid structure with two switching quads and a quasi-diplexer, this circuit can function either as an FM or a subharmonic mixer (SHM). In addition, the hybrid mixer can operate at two MMW bands concurrently as long as the frequency conversion schemes are carefully designed.

Circuit design and analysis

Figure 1 shows the schematic of the proposed MMW CMOS hybrid mixer. It consists of two switching quads (M 1M 8), equipped with 20-μm width transistors biased at VGS = 0.4 V. The selection of device size and bias voltage was made to obtain a maximum conversion gain (CG) following the procedure presented in [Reference Kodkani and Larson21]. Herein, the voltage VS (as shown in Fig. 1) is set to 0 V for simplicity, which can be set to other values to bias the baseband amplifiers in future work. Because there are no DC current paths for the transistors, the drain–source voltage (VDS) of the transistors is 0 V. Different from conventional SHMs [Reference Kodkani and Larson21, Reference Jen, Rose and Meyer22], an additional “quasi-diplexer” formed by CB 1, CB 2, CF 1, CF 2, LF 1, and LF 2 is inserted between the switching quads to establish a hybrid structure with two down-conversion paths (as shown in Fig. 1) for dual-band applications. The quasi-diplexer has a low-pass characteristic in path 1 and a high-pass characteristic in path 2. The values of CF 1, CF 2, LF 1, and LF 2 are chosen to make the cutoff frequency of the low-pass filter (LPF) higher than the IF frequency (fIF), whereas the values of CB 1 and CB 2 need to be small enough to block the IF signal in path 2. Three Marchand baluns are used to generate differential RF and LO signals [Reference Zhu, Wang and Wu15, Reference Zhu, Wang and Wu23]. A 90° coupler and an inductor (LC) are jointly used to provide an optimum LO phase distribution for the switching quads.

Fig. 1. Schematic of the proposed MMW CMOS hybrid mixer.

Assuming the two switching quads are driven by two phase-shifted square-wave LOs with a 50% duty cycle and the transistors are operating as ideal switches, the voltage across AA′ (as shown in Fig. 1) can be expressed as [Reference Zhao, Öjefors, Aufinger, Meister and Pfeiffer24]:

(1)$$\eqalign{v_{AA^{\prime}}( t) = & V_{RF}\cos ( 2\pi f_{RF}t) \displaystyle{4 \over \pi }\sum\limits_{n = 0}^\infty {\displaystyle{1 \over {2n + 1}}\sin [ 2\pi ( 2n + 1) f_{LO}t] } \cr {\kern 1pt} = & \displaystyle{ 2 \over \pi }V_{RF}\sum\limits_{n = 0}^\infty {\displaystyle{1 \over {2n + 1}}\sin [ 2\pi f_{RF}t-2\pi ( 2n + 1) f_{LO}t] } \cr {\kern 1pt} & + \displaystyle{ 2 \over \pi }V_{RF}\sum\limits_{n = 0}^\infty {\displaystyle{1 \over {2n + 1}}\sin [ 2\pi f_{RF}t + 2\pi ( 2n + 1) f_{LO}t]}}$$

where fLO is the LO frequency, VRF and fRF are the voltage amplitude and frequency of the RF signal, respectively.

Subharmonic mixing mode

For fRF = 2fLO ± fIF, where fIF is the IF frequency, the lowest frequency in (1) is fLO − fIF. Because fLO is much higher than fIF in MMW applications, all the frequency components in (1) will be blocked by the LPF in path 1, because the cutoff frequency of the LPF is much lower than fLO − fIF. Therefore, they can only be passed to BB′ (as shown in Fig. 1) for the second stage of mixing and the subharmonic mixing is obtained in path 2.

Theoretically, the best CG performance is achieved when the LO1 and LO2 are in quadrature [Reference Kodkani and Larson21, Reference Jen, Rose and Meyer22]. In practical, however, the optimum LO phase shift will drift away from 90° due to the parasitic effects of the transistors at MMW frequencies [Reference Zhao, Öjefors, Aufinger, Meister and Pfeiffer24] and the existence of the quasi-diplexer. Figure 2 illustrates the impact of the parasitic effects of the transistors and the existence of the quasi-diplexer on the simulated CG performance. For the SHM without the quasi-diplexer, the optimum LO phase shift drifts from 90 to 70° when the LO frequency moves from 0.24 to 24 GHz, due to the parasitic effects of the transistors [Reference Zhao, Öjefors, Aufinger, Meister and Pfeiffer24]. Meanwhile, the maximum CG is decreased significantly because the modulating currents in the mixer find a path to ground through the substrate resistance and the parasitic source–bulk and drain–bulk capacitances at higher frequencies [Reference Kodkani and Larson21]. By adding the quasi-diplexer, the optimum LO phase shift further drifts from 70 to 60° at 24-GHz LO frequency, because the quasi-diplexer introduces additional phase delays for the frequency components in (1). In addition, the maximum CG is further decreased by 1.9 dB due to the insertion loss of the quasi-diplexer. Figure 3 shows the simulated CGs of the proposed SHM with respect to LO phase shift for different LO frequencies. As can be observed, the optimum LO phase shift is 85, 70, 60, and 55° for the LO frequency of 16, 20, 24, and 28 GHz, respectively. In this study, the LO phase shift of 60° is chosen, so that the CG is close to the peak value for the LO frequency of 20, 24, and 28 GHz, respectively, whereas the CG is only 0.8 dB lower than its peak value for the LO frequency of 16 GHz.

Fig. 2. Impact of the parasitic effects of the transistors and the existence of the quasi-diplexer on the simulated CG performance.

Fig. 3. Simulated CGs with respect to LO phase shift for different LO frequencies.

To achieve 60° of LO phase shift, a 350-pH inductor LC is inserted between the 90° coupler and the LO balun 2. Figure 4 compares the simulated CGs of the SHM with and without LC. By introducing the inductor LC, the CG of the SHM is improved significantly at high LO frequencies but a little degraded at low LO frequencies. In future work, the optimum LO phase distribution can be implemented by investigating a novel coupler with arbitrary phase shift.

Fig. 4. Simulated CGs of the SHM with and without the inductor LC.

Fundamental mixing mode

For fRF = fLO ± fIF, the lowest two frequencies in (1) are fIF and 2fLO − fIF. Because the IF signal is blocked by the capacitors CB 1 and CB 2 in path 2, it can only be passed to the IF1 port through path 1. Meanwhile, because the cutoff frequency of the LPF is much lower than 2fLO − fIF, all the frequency components in (1) except for the IF signal will be filtered by the LPF. Therefore, only the IF signal is passed through path 1 and the fundamental mixing is obtained in path 1.

Concurrent mixing mode

By carefully assigning the LO frequencies, the proposed hybrid mixer can also function as a concurrent dual-band mixer. For instance, Fig. 5 shows an application of the hybrid mixer in a concurrent dual-band receiver that is capable of simultaneous operation at two different frequencies (fRFA and fRFB) by imposing the following conditions: (1) fLOA = fRFA −  fIF, (2) fLOB = fRFB/2, (3) fIF > (BWA + BWB)/2, and (4) |fLOA − fLOB| > fIF + (BWA + BWB)/2. The frequency domain signal evolution in the concurrent dual-band receiver is also illustrated in Fig. 5. The proposed concurrent dual-band receiver can be viewed as a low-IF receiver for the signal of RFA and a subharmonic direct-conversion receiver for the signal of RFB. Therefore, both the receiver architectures have the advantage of low DC offsets [Reference Jen, Rose and Meyer22, Reference Crols and Steyaert25]. In addition, the flicker noise issues in low- and zero-IF CMOS receivers can also be mitigated by using passive mixers [Reference Redman-White and Leenaerts26Reference Wei, Meng, Wu and Tsung29].

Fig. 5. An architecture for concurrent dual-band receiver.

Experimental results

The proposed MMW hybrid mixer is fabricated using a standard TSMC 65-nm CMOS process. The photo of the chip is shown in Fig. 6 with a chip size of 0.69 × 0.73 mm2, including all pads and dummy metal. The mixer was measured via on on-wafer probing.

Fig. 6. Photo of chip of the proposed MMW hybrid CMOS mixer.

The measured and simulated CGs versus LO power level (fLO = 24 GHz, fIF = 100 MHz) for both SHM and FM modes of the mixer are shown in Fig. 7. It is observed that an LO power of 10 dBm is required for the SHM. Figure 8 shows the measured and simulated CGs versus RF frequency for both modes of the mixer. The maximum CG of the mixer is −13.7 and −7.6 dB for the SHM and FM modes, respectively, the 3-dB RF bandwidth is from 30 to 53 GHz and 16 to 35 GHz for the SHM and FM modes, respectively. The measured CGs of this mixer are considerably lower than that in [Reference Zhu, Wang and Wu15], due to the following reasons: (1) the lack of IF buffers, which provide about 7-dB power gain in [Reference Zhu, Wang and Wu15]; (2) the transconductance (gm) of the transistors is lower than that in [Reference Zhu, Wang and Wu15] due to VDS = 0 V; (3) the quasi-diplexer also introduces 1.9-dB additional insertion loss, as shown in Fig. 2. The measured 3-dB IF bandwidth is 1.2 and 1.5 GHz for the SHM and FM modes, respectively. The measured LO-to-RF and 2LO-to-RF isolations are better than 40 and 58 dB, respectively, as shown in Fig. 9. The measured input 1 dB power compression point (IP 1dB) of the mixer is 4 and 6 dBm for the SHM and FM modes, respectively. A performance summary and comparison to other dual-band MMW mixers are shown in Table 1.

Fig. 7. Measured and simulated CGs versus LO power for both subharmonic and fundamental modes.

Fig. 8. Measured and simulated CGs versus RF frequency for both subharmonic and fundamental modes.

Fig. 9. Measured LO-to-RF and 2LO-to-RF isolations.

Table 1. Comparison of MMW dual-band mixers

Conclusion

In this paper, a millimeter-wave (MMW) fundamental and subharmonic hybrid dual-band CMOS mixer is proposed and presented. Based on a hybrid structure with two switching quads and a quasi-diplexer, the proposed mixer can function as an FM or a SHM. In addition, the hybrid mixer can also operate at two MMW bands concurrently as long as the frequency conversion schemes are carefully designed. This is very appealing for MMW systems to reduce the system size, increase the versatility, and/or extend the available bandwidth.

Acknowledgement

This work was supported by in part by the Natural Science Foundation of China under Grant 61901147 and in part by the Qianjiang Talent Project Type-D of Zhejiang under Grant QJD1902012.

Fang Zhu received his B.S. degree in electronics and information engineering from Hangzhou Dianzi University, Hangzhou, China, in 2009, and his M.S. and Ph.D. degrees in electromagnetic field and microwave technique from Southeast University, Nanjing, China, in 2011 and 2014, respectively. From 2014 to 2016, he was a MMIC Designer with Nanjing Milliway Microelectronics Technology Co., Ltd., Nanjing, China. From 2016 to 2019, he was a Postdoctoral Research Fellow with the Poly-Grames Research Center, Polytechnique Montréal, Montréal, QC, Canada. He is currently a Professor with the School of Electronics and Information, Hangzhou Dianzi University, Hangzhou, China. His current research interests include microwave and millimeter-wave integrated circuits, components and transceivers for wireless communication and sensing systems.

Guo Qing Luo received his B.S. degree from the China University of Geosciences, Wuhan, China, in 2000, his M.S. degree from Northwest Polytechnical University, Xi'an, China, in 2003, and his Ph.D. degree from Southeast University, Nanjing, China, in 2007. Since 2007, he has been a Lecturer with the faculty of School of Electronics and Information, Hangzhou Dianzi University, Hangzhou, China, and was promoted to Professor in 2011. From October 2013 to October 2014, he joined the Department of Electrical, Electronic and Computer Engineering, Heriot-Watt University, Edinburgh, UK, as a Research Associate, where he was involved in developing low profile antennas for UAV applications. He has authored or co-authored over 110 technical papers in refereed journals and conferences and holds 19 patents. His current research interests include RF, microwave and mm-wave passive devices, antennas, and frequency selective surfaces.

References

Wolf, R, Joram, N, Schumann, S and Ellinger, F (2016) Dual-band impedance transformation networks for integrated power amplifiers. International Journal of Microwave and Wireless Technologies 8, 17.CrossRefGoogle Scholar
Malakooti, SA, Hayati, M, Fahimi, V and Afzali, B (2016) Generalized dual-band branch-line coupler with arbitrary power division ratios. International Journal of Microwave and Wireless Technologies 8, 10511059.CrossRefGoogle Scholar
Alqaisy, M, Chakrabraty, C, Ali, J and Alhawari, ARH (2015) A miniature fractal-based dual-mode dual-band microstrip bandpass filter design. International Journal of Microwave and Wireless Technologies 7, 127133.CrossRefGoogle Scholar
Mondal, S and Paramesh, J (2019) A reconfigurable 28-/37-GHz MMSE-adaptive hybrid-beamforming receiver for carrier aggregation and multi-standard MIMO communication. IEEE Journal of Solid-State Circuits 54, 13911406.CrossRefGoogle Scholar
Kijsanayotin, T and Buckwalter, JF (2014) Millimeter-wave dual-band, bidirectional amplifier and active circulator in a CMOS SOI process. IEEE Transactions on Microwave Theory and Techniques 62, 30283040.CrossRefGoogle Scholar
Jain, V, Javid, B and Heydari, P (2009) A BiCMOS dual-band millimeter-wave frequency synthesizer for automotive radars. IEEE Journal of Solid-State Circuits 44, 21002113.CrossRefGoogle Scholar
Lv, G, Chen, W, Chen, X and Feng, Z (2018) An energy-efficient Ka/Q dual-band power amplifier MMIC in 0.1-μm GaAs process. IEEE Microwave and Wireless Components Letters 28, 530532.CrossRefGoogle Scholar
Jain, V, Tzeng, F, Zhou, L and Heydari, P (2009) A single-chip dual-band 22-29-GHz/77-81-GHz BiCMOS transceiver for automotive radars. IEEE Journal of Solid-State Circuits 44, 34693485.CrossRefGoogle Scholar
Abdelrheem, TA, Elhak, HY and Sharaf, KM (2003) A concurrent dual-band mixer for 900-MHz/1.8 GHz RF front-ends. IEEE International Midwest Circuits and Systems Symposium 3, 12911294.CrossRefGoogle Scholar
Liang, C-P, Rao, P-Z, Huang, T-J and Chung, S-J (2009) A 2.45/5.2 GHz image rejection mixer with new dual-band active notch filter. IEEE Microwave and Wireless Components Letters 19, 716718.CrossRefGoogle Scholar
Hwang, YS, Yoo, SS and Yoo, HJ (2005) A 2 GHz and 5 GHz dual-band direct conversion RF frontend for multi-standard applications. IEEE International SOC Conference 189192.Google Scholar
Jackson, BR and Saavedra, CE (2010) A dual-band self-oscillating mixer for C-band and X-band applications. IEEE Transactions on Microwave Theory and Techniques 58, 318323.CrossRefGoogle Scholar
El-Nozahi, M, Amer, A, Sánchez-Sinencio, E and Entesari, K (2010) A millimeter-wave (24/31-GHz) dual-band switchable harmonic receiver in 0.18-μm SiGe process. IEEE Transactions on Microwave Theory and Techniques 58, 27172730.CrossRefGoogle Scholar
Mazzanti, A, Vahidfar, MB, Sosio, M and Svelto, F (2010) A low phase-noise multi-phase LO generator for wideband demodulators based on reconfigurable sub-harmonic mixers. IEEE Journal of Solid-State Circuits 45, 21042115.CrossRefGoogle Scholar
Zhu, F, Wang, K and Wu, K (2019) A reconfigurable low-voltage and low-power millimeter-wave dual-band mixer in 65-nm CMOS. IEEE Access 7, 3335933368.CrossRefGoogle Scholar
Wang, C, Hou, D, Chen, J and Hong, W (2019) A dual-band switchable MMIC star mixer. IEEE Microwave and Wireless Components Letters 29, 737740.CrossRefGoogle Scholar
Hashemi, H and Hajimiri, A (2002) Concurrent multiband low-noise amplifiers – theory, design, and applications. IEEE Transactions on Microwave Theory and Techniques 50, 288301.CrossRefGoogle Scholar
Liu, Y (2017) Adaptive blind postdistortion and equalization of system impairments for a single-channel concurrent dual-band receiver. IEEE Transactions on Microwave Theory and Techniques 65, 302314.CrossRefGoogle Scholar
Olopade, AO, Hasan, A and Helaoui, M (2013) Concurrent dual-band six-port receiver for multi-standard and software defined radio applications. IEEE Transactions on Microwave Theory and Techniques 61, 42524261.CrossRefGoogle Scholar
Zhang, W, Hasan, A, Ghannouchi, FM, Helaoui, M, Wu, Y, Yu, C and Liu, Y (2018) Concurrent dual-band low intermediate frequency receiver based on the multiport correlator and single local oscillator. IEEE Microwave and Wireless Components Letters 28, 353355.CrossRefGoogle Scholar
Kodkani, RM and Larson, LE (2008) A 24-GHz CMOS passive subharmonic mixer/downconverter for zero-IF applications. IEEE Transactions on Microwave Theory and Techniques 56, 12471256.CrossRefGoogle Scholar
Jen, H, Rose, S and Meyer, R (2006) A 2.2 GHz sub-harmonic mixer for direct conversion receivers in 0.13 μm CMOS. IEEE International Solid-State Circuits Conference Technical Digest 18401849.Google Scholar
Zhu, F, Wang, K and Wu, K (2019) Design considerations for image-rejection enhancement of quadrature mixers. IEEE Microwave and Wireless Components Letters 29, 216218.CrossRefGoogle Scholar
Zhao, Y, Öjefors, E, Aufinger, K, Meister, TF and Pfeiffer, UR (2012) A 160-GHz subharmonic transmitter and receiver chipset in an SiGe HBT technology. IEEE Transactions on Microwave Theory and Techniques 60, 32863299.CrossRefGoogle Scholar
Crols, J and Steyaert, MSJ (1998) Low-IF topologies for high-performance analog front ends of fully integrated receivers. IEEE Transactions on Circuits and Systems II Analog and Digital Signal Processing 45, 269282.CrossRefGoogle Scholar
Redman-White, W and Leenaerts, DMW (2001) 1/f Noise in passive CMOS mixers for low and zero IF integrated receivers. IEEE European Solid-State Circuits Conference (ESSCIRC) 4144.Google Scholar
Sacchi, E, Bietti, I, Erba, S, Tee, L, Vilmercati, P and Castello, R (2003) A 15 mW, 70 kHz 1/f corner direct conversion CMOS receiver. IEEE Custom Integrated Circuits Conference, 459462.Google Scholar
Zhou, S and Chang, MCF (2005) A CMOS passive mixer with low flicker noise for low-power direct-conversion receiver. IEEE Journal of Solid-State Circuits 40, 10841093.CrossRefGoogle Scholar
Wei, HJ, Meng, C, Wu, PY and Tsung, KC (2008) K-band CMOS sub-harmonic resistive mixer with a miniature Marchand balun on lossy silicon substrate. IEEE Microwave and Wireless Components Letters 18, 4042.CrossRefGoogle Scholar
Bao, M, Jacobsson, H, Aspemyr, L, Carchon, G and Sun, X (2006) A 9–31-GHz subharmonic passive mixer in 90-nm CMOS technology. IEEE Journal of Solid-State Circuits 41, 22572264.CrossRefGoogle Scholar
Figure 0

Fig. 1. Schematic of the proposed MMW CMOS hybrid mixer.

Figure 1

Fig. 2. Impact of the parasitic effects of the transistors and the existence of the quasi-diplexer on the simulated CG performance.

Figure 2

Fig. 3. Simulated CGs with respect to LO phase shift for different LO frequencies.

Figure 3

Fig. 4. Simulated CGs of the SHM with and without the inductor LC.

Figure 4

Fig. 5. An architecture for concurrent dual-band receiver.

Figure 5

Fig. 6. Photo of chip of the proposed MMW hybrid CMOS mixer.

Figure 6

Fig. 7. Measured and simulated CGs versus LO power for both subharmonic and fundamental modes.

Figure 7

Fig. 8. Measured and simulated CGs versus RF frequency for both subharmonic and fundamental modes.

Figure 8

Fig. 9. Measured LO-to-RF and 2LO-to-RF isolations.

Figure 9

Table 1. Comparison of MMW dual-band mixers