A Wideband Single-balanced Down-mixer for the 60 GHz Band in 65 nm CMOS

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A Wideband Single-balanced Down-mixer for the GHz Band in 5 nm CMOS Michael Kraemer, Mariano Ercoli, Daniela Dragomirescu, Robert Plana To cite this version: Michael Kraemer, Mariano Ercoli, Daniela Dragomirescu, Robert Plana. A Wideband Single-balanced Down-mixer for the GHz Band in 5 nm CMOS. Asia Pacific Microwave Conference (APMC 1), Dec 1, Yokohama, Japan. p.189-185, 1. <hal-5917> HAL Id: hal-5917 https://hal.archives-ouvertes.fr/hal-5917 Submitted on May 11 HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

A Wideband Single-balanced Down-mixer for the GHz Band in 5 nm CMOS Michael Kraemer # 1, Mariano Ercoli # Daniela Dragomirescu # 3, Robert Plana # # CNRS ; LAAS ; 7 avenue du colonel Roche, F-3177 Toulouse, France University of Toulouse ; UPS, INSA, INP, ISAE ; LAAS ; F-3177 Toulouse, France 1 mkraemer@laas.fr; mercoli@laas.fr; 3 daniela@laas.fr; plana@laas.fr Abstract This paper presents a single-balanced direct down conversion mixer for the unlicensed GHz band. It is based on a differential pair employing the current bleeding technique. An integrated GHz wideband passive balun allows the use of a single ended local oscillator (). The circuit is fabricated using the 5 nm bulk CMOS technology of ST Microelectronics. The mixer s baseband reaches from DC to GHz. The measured radio frequency () bandwidth exceeds 11 GHz, ranging from 5 GHz to at least 5 GHz. The measured, (intermediate frequency) and port return losses lie below - db, -15 db and -1 db, respectively, within this entire band. A maximum conversion gain of 9.1 db at 1 MHz from the carrier is achieved, while typical values measured at 1 GHz lie around db throughout the entire band. The mixer delivers these optimum results for powers as low as -5 dbm. The output referred 1 db compression point reaches -5 dbm for -1 dbm of power. The simulated single sideband (SSB) noise figure is of 9 db. Including the differential buffer that can drive two singleended 5 Ω loads, the circuit draws 1.8 ma from a 1 V supply. The pad-limited die size is only.5 x.9 mm. I. INTRODUCTION A major research topic in the domain of microwave engineering today is the design of low-power low-cost silicon transceiver front-ends for the unlicensed frequency band around GHz. While the first CMOS circuits for this purpose were designed in a 13 nm technology [1], the use of lower scale CMOS technologies (like 5 nm for the circuit in this paper) with higher unity gain frequencies (f T, f max )isone way to improve performance. However, the potential advantages are accompanied by drawbacks such as lower supply voltages (and thus decreased linearity), more stringent density rules and scaling of the metal back-end. This has to be taken into account during design. Furthermore, many early GHz radio frequency integrated circuits (ICs) employ transmission lines for matching purposes. This often results in large circuit sizes and thus increased cost. The better solution is the use of spiral inductors, as they do not only reduce circuit size, but also improve performance [], [3]. This paper presents the design and implementation of one of the basic building blocks of a GHz direct conversion receiver: the down-mixer. Different mixer circuits downconverting signals from the GHz band are described in literature, employing a multitude of topologies (cf. to [1], [], [5], [], [7], [8], [9], [1]). Compared to these circuits, the solution discussed in this paper presents a better compromise for integrated low-cost low-power receivers operating in the GHz band by achieving excellent performance while maintaining small size, low power requirements and a low power consumption (cf. section IV). The characterization of the circuit is facilitated by an integrated passive balun and a differential output buffer. II. MIXER DESIGN Fig. 1 illustrates the block diagram of the designed mixer. The input port is single-ended, because the preceding circuit block is going to be the single-ended low noise amplifier presented in [11]. The differential intermediate frequency () output of the mixer is connected to a buffer amplifier based on a differential pair. The buffer is designed to drive a differential 1 Ω load (or alternatively two grounded 5 Ω terminations). The total circuit s power consumption is dominated by this buffer, which dissipates around 1 mw. In an integrated receiver circuit, this power-wasting buffer is not necessary because higher load impedances can be employed. The differential local oscillator () port of the mixer core is connected to a passive on-chip balun. The balun is composed of two symmetrical spiral transformers connected as indicated in Fig. 1. Its layout can be identified in Fig. 3, where the balun is connected to the pad by an inductor that resonates Fig. 1. Block diagram of the downconversion mixer with integrated balun and buffer

V DD V DD C 1 R 1 R 1 C 1 5μm C L 1 M M3 L 1 C R B V DD L L M1 L B C B 9μm L 3 L D + - Fig. 3. Die photo of the fabricated down-mixer Fig.. Simplyfied schematic of the mixer core without biasing details the pad capacitance. The employed balun topology allows a much better amplitude and phase balance compared to a single transformer with center tap. For further details on the balun design refer to [1]. Fig. illustrates the schematic of the mixer core. A current bleeding [1] approach is employed to permit ideal biasing of both transconductance (M1) and switching (M, M3) transistors. The current which by-passes the switching pair is determined by the resistor R B. It passes by the inductance L B, which at the same time resonates the parasitic capacitances present at the drain of M1 []. The transistor M1 is biased at the minimum noise current density of.15 ma/μm. Its width is 1x1 μm. M1 is degenerated by the inductor L D. This improves linearity and allows a simultaneous noise and power match. Inductors L,L 3 and L realize this match (taking into account also the pad capacitance) over a wide bandwidth. Transistors M and M3, which are 35x1 μm wide, are biased at very low current densities to allow fast switching. The resistive loads R 1 are short-circuited by C 1 for and frequencies to increase conversion gain G C and improve isolation. The inductor L 1 is used to match the gates of the switching pair to the balun s impedance. The capacitor C is inserted to cut the DC path and permit a bias voltage at the gates of M1 and M. A. Transistors The transistors used in the mixer circuit are general purpose (GP) devices. GP devices exhibit higher f max as low power (LP) devices at a given bias current, thus mandating their use for low power IC design. A consequence of the use of GP transistors is the lower breakdown voltage of 1 V, which limits the circuit s supply voltage. While the intrinsic performance of the transistors is well represented by the BSIM model, it does not take into account the custom layout. To obtain an extrinsic model that includes the optimized multi-finger layout used, a parasitic extraction is performed for all devices. B. Passive Devices As inductive matching elements, spiral inductors are used rather than transmission lines. Their performance with respect to size, realizable values and quality factor are superior even when using CMOS technologies with low resistivity substrates [3]. The design of the spiral inductors is lined out in []. The focus lies on minimizing the parasitics rather than maximizing the quality factor. Electromagnetic simulations using Sonnet are employed to do quantitative optimizations []. The S- parameters obtained by simulation of the final geometry are used to parametrize a -π model, which is employed in the circuit simulations to precisely predict the inductor s behavior. A similar approach is employed for the balun [1]. C. Fabricated Circuit The presented circuit was fabricated in the 5 nm CMOS technology of STMicroelectronics with two thick copper metal layers. Fig. 3 shows a photo of the fabricated circuit. A very small, pad limited die size of only.9mm x.5mm =.55mm is obtained, which is further reduced when integrating the mixer into the receiver. III. RESULTS The mixer circuit of Fig. 3 is measured on-wafer up to 5 GHz. The return loss is determined using an Anritsu ME788A vector network analyzer (VNA). The signal is generated by an Agilent E857D source that provides up to 1 dbm output power at GHz. Power conversion gain and power sweep measurements are done using the VNA as signal source and connecting

7-1 Return Loss in db - -3 - -5 Return Loss at port Return Loss at port G C in db 5 3 LSB, f = 1GHz USB, f = 1GHz LSB, f = GHz USB, f = GHz - 5 5 55 5 f in GHz 5 5 58 f in GHz Fig.. Measured return loss at and port Fig.. Conversion gain G C versus frequency for two different intermediate frequencies, both in upper (USB) and lower sideband (LSB). 7 G c in db 5 3 1 Conversion Gain (USB) for f = GHz, f =1GHz - -15-1 -5 5 1 P in dbm Fig. 5. Measured conversion gain versus power at f =GHzand f =1GHzfrom the upper sideband a Rohde & Schwarz FSU 7 GHz spectrum analyzer to one of the ports, while terminating the other one. All loss originating from cables and probes are subtracted from the obtained results, and 3 db are added to the output power to account for the differential signal. While measuring, the mixer is biased at the current densities determined during design. The bias of the switching pair depends on the power and is set to.7 V for the power sweep. For the other measurements, P equals -1 dbm and the switching pair is biased at.5 V. The circuit including buffers is drawing 1.8 ma from a 1 V supply, from which only.8 ma are attributed to the mixer core. Fig. illustrates the measured return loss (RL) at the and ports. An excellent broadband match is assured, contributing to a very flat, wideband response of the mixer. The measured RL stays below -15 db up to 5 GHz. The power is swept for f = GHz and f = 1 GHz to find the value that achieves maximum conversion gain G C. According to Fig. 5, this is the case at the low power value of -5 dbm. Fig. plots the conversion gain G C in the lower (LSB) and upper sideband (USB). A very flat, wideband response can be observed for frequencies of 1 GHz and GHz, while both sidebands are very symmetric. The conversion gain is around db at 1 GHz from the carrier over the whole band. The measurement frequency range was bounded to below 5 GHZ due to the used equipment. Fig. 7 shows the conversion gain for five fixed frequencies TABLE I COMPARISON OF PUBLISHED GHZ DOWN-CONVERSION MIXERS IN CMOS Reference Topology Technology G c NF (SSB) P OP 1dB P diss Die Size (nm) (GHz) (GHz) (db) (db) (dbm) (dbm) (mw) (mm ) Emami et al., 5 [1] single gate 13 55-1 - 11.5-5.5. 1.x1.7 Razavi, [] half Gilbert cell 13 N.A. 1 18* N.A. N.A..9 N.A. Tsai et al., 7 [5] Gilbert cell 9.1 5-75 3 ± N.A. - 93.55x.55 Zhang et al., 7 [] Gilbert cell 13 1 55-3 3 N.A. -1 N.A..9x.9 Kantanen et al, 8 [7] resistive 9. 9.8 N.A. 5-1 1.1x.7 Kim et al., 9 [8] half Gilbert cell 13 5.9 N.A. N.A. -15 8. N.A. Sakian et al., 9 [9] Gilbert cell 5-1.3 1 N.A. -1** N.A. Ercoli et al., 1 [13] passive 5 N.A. 5-7* -.9* 11.* -5* N.A. 15* N.A. this work half Gilbert cell 5-5 - 5 9.1 1* -5-5 1.8.9x.5 *simulated; **obtained from OIP3-1 db # voltage conversion gain;

G C in db 1 8 - f =5GHz f =58GHz f =GHz - 5 5 5 58 f in GHz f =GHz f = GHz Fig. 7. Conversion gain G C versus f for different frequencies. The is varying from 1 MHz to 5 GHz. -5 models and the fact that all parasitics are taken into account during simulation. IV. COMPARISON TO THE STATE OF THE ART Table I compares the presented work to GHz CMOS mixers found in literature. The proposed mixer has the smallest chip size, one of the highest gain values and a very wide and bandwidth that makes it one of the best candidates for an integrated receiver covering the worldwide available GHz band. The fact that its DC power consumption is relatively high originates from the buffers that drive two 5 Ω loads. Yet, the proposed mixer requires the lowest power. V. CONCLUSION The single balanced down-mixer presented in this paper is the perfect choice for low-cost low-power direct conversion receivers due to its conversion gain of up to 9. db, its low power requirement of -5 dbm, its moderate DSB noise figure of 1 db and its high OP 1dB of -5 dbm. Its ultra-wide bandwidth respects the channel requirement of all standards that exist for the unlicensed GHz band. The very small (pad-limited) size of only.9x.5 mm allows low cost integration. P in dbm -1-15 - P -1dB = -5dBm P Conversion Gain G C (f =GHz, P =-1dBm, f =GHz) - -15-1 -5 - P in dbm Fig. 8. P and G C versus P to illustrate nonlinearity and 1 db compression point while sweeping the over both sidebands. The peak in G C is achieved close to the carrier, while the 3 db bandwidth is around GHz (i.e. GHz of band around the frequency). Fig. 8 plots output power and conversion gain versus input power to illustrate the linearity of the circuit. An output referred 1 db compression point OP 1dB of -5 dbm is obtained for P = 1dBm. Isolation is less important for this mixer, due to the distance from baseband to / which allows inexpensive low pass filtering on-chip. to isolation is observed to be around 3 db, while to isolation is around 8 db. The former value is expected to increase if an integrated differential oscillator with even better phase balance provides the signal. The simulation of the Noise Figure (NF) using SPECTRE shows a double sideband (DSB) value of around 9 db, which gives a theoretical SSB value that lies at 1 db. Measurement results are expected to be very close due to the use of BSIM G C in db ACKNOWLEDGEMENT Thanks go to Prof. Sorin Voinigescu of University of Toronto and his students for valuable hints on mm-wave circuit design and STMicroelectronics for technology access. REFERENCES [1] S. Emami, C. H. Doan et al., A -GHz down-converting CMOS singlegate mixer, in IC 5, 5, pp. 13 1. [] M. Kraemer, D. Dragomirescu, and R. Plana, Accurate electromagnetic simulation and measurement of milimeter-wave inductors in bulk CMOS technology, Si 1, January 1. [3] T. Dickson, M.-A. LaCroix et al., 3-1-GHz inductors and transformers for millimeter-wave (Bi)CMOS integrated circuits, IEEE Trans. on MTT, vol. 53, no. 1, pp. 13 133, Jan. 5. [] B. Razavi, A -GHz CMOS receiver front-end, IEEE Journal of Solid-State Circuits, vol. 1, no. 1, pp. 17, Jan.. [5] J.-H. Tsai, P.-S. Wu, C.-S. Lin et al., A 5-75 GHz broadband gilbertcell mixer using 9-nm CMOS technology, Microwave and Wireless Components Letters, IEEE, vol. 17, no., pp. 7 9, April 7. [] F. Zhang, E. Skafidas, and W. Shieh, A -GHz double-balanced gilbert cell down-conversion mixer on 13-nm CMOS, IC 7, pp. 11 1, 3-5 7. [7] M. Kantanen, J. Holmberg et al., GHz frequency conversion 9 nm CMOS circuits, EuMIC 8, pp. 3, Oct. 8. [8] D.-H. Kim and J.-S. Rieh, A single-balanced -GHz down-conversion mixer in.13 um CMOS technology for WPAN applications, in IRMMW-THz 9, 1-5 9, pp. 1. [9] P. Sakian, R. Mahmoudi et al., A -GHz double-balanced homodyne down-converter in 5-nm CMOS process, pp. 58 1, 8-9 9. [1] M. Ercoli, M. Kraemer, D. D., and R. Plana, A high performance integrated balun for GHz application in 5nm CMOS technology, APMC 1, 1, under review. [11] M. Kraemer, D. Dragomirescu, and R. Plana, A low-power high-gain LNA for the GHz band in a 5 nm CMOS technology, in APMC 9, 9, pp. 115 1159. [1] S.-G. Lee and J.-K. Choi, Current-reuse bleeding mixer, Electronics Letters, vol. 3, no. 8, pp. 9 97, Apr. [13] M. Ercoli, M. Kraemer, D. Dragomirescu, and R. Plana, A passive mixer for GHz applications in CMOS 5nm technology, in GeMIC 1, 15-17 Mars 1.