Low-Power Fully Integrated and Tunable
CMOS RF Wireless Receiver for ISM Band
Consumer Applications
Simon Cimin Li, Hong-Sing Kao, Chia-Pei Chen, and Chung-Chih Su
Abstract—A 0.25- m single-chip CMOS single-conversion tunable low intermediate frequency (IF) receiver operated in the 902–928-MHz industrial, scientific, and medical band is proposed. A new 10.7-MHz IF section that contains a limiting amplifier and a frequency modulated/frequency-shift-key demodulator is designed. The frequency to voltage conversion gain of the demodu-lator is 15 mV/kHz and the dynamic range of the limiting amplifier is around 80 dB. The sensitivity of the IF section including the demodulator and limiting amplifier is 72 dBm. With on-chip tunable components in the low-power low-noise amplifier (LNA) and LC-tank voltage-controlled oscillator circuit, the receiver measures an RF gain of 15 dB at 915 MHz, a sensitivity of 80 dBm at 0.1% bit-error rate, an input referred third-order inter-cept point of 9 dBm, and a noise figure of 5 dB with a current consumption of 33 mA and a 2450 m 2450 m chip area.
Index Terms—Demodulator, frequency synthesizer, low inter-mediate frequency (IF) receiver, noise amplifier (LNA), low-power receiver, mixer, RF CMOS, single-conversion receiver.
I. INTRODUCTION
T
HE DEMAND for low-cost wireless systems has soared in the recent past. There is a rapidly growing market for low-power short-range wireless systems for alarm systems, sen-sors, and controls. Because of their limited range and low data rates, these short-range systems often operate in the industrial, scientific, and medical (ISM) bands. There is a tradeoff among the antenna size, power consumption, and design feasibility that depends on the operation frequency. The ISM band of 915 MHz was selected for this paper as a compromise among these pa-rameters.The unrivaled growth of the wireless telecommunication systems has led to persistent demand for small, low-cost, low-power RF terminals. RF front-end design is pushed toward an ultimate goal of full integration in economical CMOS tech-nology, rendering significant space, cost, and power reductions.
Manuscript received January 16, 2004; revised May 29, 2004, August 20, 2004, and January 8, 2005. This work was supported in part by the National Science Council, Republic of China, under Contract NSC-86-88-2221-E-224-018. This paper was recommended by Associate Editor T. B. Tarim.
S. C. Li is with the Advanced Technology and Integrated System Laboratory (ATIS Laboratory), National Yunlin University of Science and Technology, Taiwan 640, R.O.C. and also with the Institute of Communication Engi-neering (ICE) National University of Tainan, Tainan, Taiwan, R.O.C. (e-mail: [email protected]; [email protected]).
H.-S. Kao and C.-P. Chen are with National Chiao-Tung University, Hsinchu, Taiwan, R.O.C.
C.-C. Su is with the AlfaPlus Semiconductor Inc., Hsinchu, Taiwan, R.O.C. Digital Object Identifier 10.1109/TCSI.2005.852926
Fig. 1. Proposed low-power low-IF 915 MHz ISM receiver.
To meet such demand, much work has been focused on real-izing fully integrated single-chip receiver (Rx) within CMOS technologies [1]–[6].
In this paper, a fully integrated single-chip wireless receiver integrated circuit (IC) is intended for use in the unlicensed 902–928 MHz ISM band as part of a system that communicates at rates between 2 and 390 kbps. The single-chip receiver IC contains a low-noise amplifier (LNA), a mixer, a frequency synthesizer, and a quadrature demodulator. It also features the capability of on-chip tuning in the analog front-end design. The architecture of the fully integrated and tunable CMOS heterodyne receiver is shown in Fig. 1.
The IC is housed in a 32-lead low-profile quad flat pack (LQFP) plastic package, and provides all the functions nec-essary to implement a binary frequency-shift key (BFSK) demodulation receiver system for many applications in the field of wireless communication. Based on the low-IF single conver-sion architecture, the receiver is implemented in the 0.25- m CMOS SP5M technology. Section II reviews receiver architec-tures including heterodyne and homodyne techniques, and it focuses on the proposed low-power low-IF single conversion receiver and their tradeoffs. The design of building blocks with on-chip tuning facility such as the low-noise amplifier (LNA), mixer, frequency synthesizer, voltage-controlled oscillator, and quadrature demodulator is presented in Section III, respec-tively. The experimental results of the single-chip receiver are summarized in Section IV, and a conclusion is provided.
II. LOW-POWERLOW-IF SINGLECONVERSIONRx As IC technologies evolve, complexity, cost, power consump-tion, and the amount of components have been the primary cri-teria in receiver architectures design, so the relative importance of each of these criteria changes, allowing approaches that once seemed impractical to return as plausible solutions. There are 1057-7122/$20.00 © 2005 IEEE
two main types of receivers used in wireless telecommunication systems based on phase or frequency modulation: the hetero-dyne and homohetero-dyne receiver. The difference between them is in whether intermediate frequency (IF) is used or not. Hetero-dyne and homoHetero-dyne receivers are often called IF and zero-IF receivers, respectively. The low-power Rx architectures with a higher integrability such as zero-IF and low-IF Rxs are preferred topologies, while as CMOS fabrication technology can provide an economical solution over its bipolar counterpart. There are many unanswered questions in implementing the whole receiver in CMOS devices instead of bipolar junction transistors, which has hitherto been the usual way to implement low-power wire-less receivers.
A typical zero-IF Rx, direct conversion architecture, widely used in paging receivers is attractive when very low-power con-sumption is at premium [7]. If the IF is not at dc, an image re-ject filter or another arrangement may be needed to suppress the image channel [8], and inevitably this consumes substantial power. An active low-pass channel-select filter at zero IF always obtains a given dynamic range with lower power than a band-pass filter with the same band-passband centered at some nonzero IF [9]. The impasse of zero-IF Rxs is noise and mismatch or self-mixing related offsets that corrupt the required signal at low frequencies. The low-IF ( MHz) ISM Rx alleviates this problem by setting the IF frequency to typically one-half the channel bandwidth [1]. Fig. 1 shows the proposed low-power low-IF 915 MHz ISM heterodyne Rx. While selecting a 30-kHz channel at a center frequency of 900 MHz, that prohibitively needs large Q’s in bandpass, filtering is performed at progres-sively lower center frequencies. Channel-selection filtering is performed at low IF, which relaxes the requirements for the channel-selected filter. The tradeoff between image rejection and channel selection typically requires a relatively high IF, making it difficult to integrate the IF filter monolithically. For full integration of high-end RF systems, the low-IF Rx seems the best solution. Recent researches have demonstrated in sev-eral reported RF CMOS circuits in the global positioning sys-tems (GPS) [10] or Bluetooth [11]–[13]. Therefore, for intended use in the unlicensed 902–928 MHz ISM band, low-IF hetero-dyne Rx is the best choice for a conventional RF system product design.
III. BUILDINGBLOCKS OFLOW-IF ISM RECEIVER
A. Low-Power Tunable LNA
The design of LNA associates in a single transistor the foremost front-end design tradeoffs: impedance matching, power consumption, signal linearity, noise figure, and RF band-width. LNAs with a common-gate input, though convenient for providing a good 50- matching, provide an inherently higher noise figure. The noise, input matching, and stability requirements limit the acceptable LNA topologies to only a few. Widely used examples are inductively degenerated cas-code topologies as they provide both a high reverse isolation (thus ensuring stability) and an input resistance that can be set to 50 by design. To achieve a relatively low noise figure and a reasonable input match, an input-matched cascode LNA
Fig. 2. Tunable LNA circuit diagram.
topology with the inductive source degeneration (Fig. 2) is employed in the front-end design. To avoid uncertainties due to bond-wire inductance, both inductors connected with source and drain are integrated on the chip. Single-stage cascode LNAs have higher input referred third-order intercept point (IIP3) in comparison to multistage LNAs [14]. However, they tend to have a slightly lower power gain and reverse isolation . A low complicates simultaneous input and output matching of the LNA and its optimization. The cascode transistor as shown in Fig. 2 provides improved reverse iso-lation without adding excessive noise in the circuit. This can also reduce the Miller effect capacitance at the input. There is an on-chip impedance matching network at the output, which can match the output impedance to the external load of 50 , it corresponding to the input of the IR filter. Since the required is typically only dB, an extra degree of freedom can be introduced by realizing a nonperfect input match. The input power of the RF source is defined by
(1) where is the 50 impedance matched between the source and . The output power of the LNA is determined by the equivalent resistance of tunable resistive load 1–3 as indicated in Fig. 2 and by the current injected into the tuned load and one of the resistors after
(2) represents a combination of equivalent parallel resistance of the load inductor . The self-inductance is tuned out by the excess capacitance at that node. The output current is given by [15], [16]
(3) For a given frequency the highest level of power gain is obtained by making the input impedance (seen into the gate of ) as low as possible. This means that even though less
power is engaged at the LNA input, the power is exploited more efficiently to generate output current and, hence, output power. It is further seen [15] that the power gain of the LNA increases with increasing , i.e., with decreasing threshold voltage headroom [16] with deeper submicron CMOS technology.
The cascode circuit of Fig. 2 incorporates inductive degener-ation to create a real part in the input impedance. Neglecting the gate–drain and source–bulk capacitance, we can write
(4) Thus, a proper choice of , and yields a real part of 50 . In practice, the last two terms may not resonate at the frequency of interest, necessitating the use of off-chip compo-nents at the input. At high frequencies, the required value of becomes comparable with the inductance of the ground bond wire, requiring multiple bonds or accurate modeling of the wire inductance. Also, the reduction of the equivalent transconduc-tance as a result of degeneration may magnify the noise con-tributed by . This is because the parasitic capacitance at the drain of provides some gain from the gate of to the output. Cascode LNAs have also been implemented in differen-tial form [2], [17]. While differendifferen-tial operation lowers the sen-sitivity to common-mode disturbance, it requires higher power dissipation to achieve the same noise figure as a single-ended counterpart. A single-ended LNA, in comparison with a dif-ferential LNA, dissipates approximately of the power [18] for the same noise and linearity of referred input. However, a single-ended LNA is more susceptible to pick up the substrate noise. Besides, the antenna signal is commonly single-ended; a means of conversion to differential form, e.g., a transformer is inevitable. A transformer either on-chip or off-chip, however, represents a bulky device.
The LNA should provide adequate gain and linearity in the RF input band of 902–928 MHz. As is small at low bias current, a large gain can only be achieved with high load impedance. In order to achieve the minimum external components for low cost and highly integrated consideration, the input of the LNA is single-ended input without external baluns. As we optimize the production yield against process variation as is concerned, the center frequency and gain of the LNA are tunable via selective switches ( and ) for combination the resistive 1–3 and/or capacitive 1–3 load. The proposed tunable LNA, operating at ISM band, draws 4.5 mA from a 3.3-V supply, yielding a total power consumption of merely 14.85 mW. The input reflection coefficient is dB. The power gain of the LNA is 12 dB, while the reverse isolation is more than 23 dB. The IIP3 of the LNA is dBm, which is more than sufficient for the ISM application.
B. Low-Power Downconversion Mixer
Downconversion mixers in the received path perform fre-quency translation by multiplying the signals at two distinct dif-ferential inputs, called the RF port and the local oscillator (LO) port. The incoming RF signal amplified by the LNA is usually single-ended and translated by the mixer to a lower IF. Since
Fig. 3. Downconversion mixer circuit diagram.
MOS transistors have a much higher IIP3 than bipolar transis-tors, the required linearization and LO drive in CMOS active mixers distinguish their design from their bipolar counterparts. Fig. 3 shows a single-balanced low-power downconversion CMOS mixer topology. The single-balanced configuration exhibits less input-referred noise than the double-balanced topology for a given power dissipation. A likely drawback of the single-balanced mixer is the LO-IF feedthrough. Note that and operate as a differential pair, and thus amplify the LO signal. If the IF is not much lower than the LO frequency then a first-order low-pass filter following the mixer may not adequately suppress the LO feedthrough without attenuating the IF signal. An IF bandpass filter (10.7 MHz with a bandwidth of 200 kHz) in this receiver architecture for a downmixing radio signal of 915 MHz is chosen for diminishing the effects of LO feedthrough. In Fig. 3, can be linearized with no need for explicit degeneration by simply increasing the gate-source overdrive voltage . This of course trades with the bias current or with the transistor aspect ratio, raising the power consumption or lowering the device transconductance. CMOS mixers typically demand large LO swings so that the switching pairs [e.g., and in Fig. 3] do not remain on simultaneously for a considerable period of time. Increasing the switching devices width can lower the required swing, but at the cost of increasing their noise contribution and higher capacitance in the RF signal path. Thus, the choice of device dimensions and bias currents play a critical role in performance. In particular, the downconversion mixer(s) must achieve high linearity and a reasonable noise figure under the constraint of required low-power consumption. The interface between the LNA and the mixer are capacitively coupled with a linearized transconductance. The value of establishes the mixer bias current, while is chosen large enough not to load down the gate circuit (and to also reduce its noise contribution). In practice, an IF bandpass filter acting as a channel-select filter (with bandwidth 200 kHz) would be used to remove the LO and other undesired spectral components from the output.
With a noise figure of 6 dB and an IIP3 of dBm, a single-balanced mixer has a conversion gain of 3 dB with acceptable degradation in the overall noise and nonlinearity. It requires a low bias current of 0.5 mA to achieve downconversion in the receiver.
Fig. 4. (a) Tunable LC-tank VCO circuit diagram. (b) Charge pump schematic. (c) Architecture of frequency divider. (d) Logic block diagram of the prescaler. (e) Timing diagram of the prescaler.
C. Baseband Interface
After the RF signal is downconverted to the baseband, it must be channel-select filtered, IF amplified, demodulated, and data sliced. The channel-select filter is a low-cost discrete ceramic bandpass filter with a center frequency of 10.7 MHz and a band-width of 200 kHz. As the RF and IF sections of receivers incor-porate external components and hence perform a lesser portion of the signal processing stage task, the design of baseband inter-face between the downconversion mixer and the following stage becomes progressively more challenging. Moreover, noise-lin-earity-power tradeoffs limit the amount of gain provided by the RF and IF circuits. Since the signal at the mixer output is in the range of tens of microvolts and the interferers are quite
large (e.g., 60 dB above the signal level), both the noise and the nonlinearity of the IF amplifier are critical. Consequently, the baseband interface must process small signals in the pres-ence of large interferers. To avoid the reduction in the mixer voltage gain, the IF amplifier must exhibit a relatively high input impedance. Considering the interface between the mixer and the baseband section as shown in Fig. 1, the channel-select filter suppresses out the channel interferers, allowing the IF amplifier to be a nonlinear, high-gain amplifier.
D. Frequency Synthesizer With Tunable Voltage-Controlled Oscillator
The frequency synthesizer, as shown in Fig. 1, consists of an LC-tank voltage-controlled osicillator (VCO), a crystal
os-cillator, a programmable frequency divider, a phase-frequency detector (PFD), a charge pump (CP), and a loop filter. To fully integrate the phase-locked loop (PLL) frequency synthesizer, phase noise and spurious suppression must be traded off against integrated capacitance and settling time. Again, there is no sub-stitute for cubic inches since large external capacitors can im-plement the large time constant of the loop filter without large resistors (i.e., noise). The LC-tank VCO is the most key com-ponent in the frequency synthesizer. Fig. 4(a) shows the circuit diagram of a tunable LC-tank VCO. The architecture of VCO in this design is a complementary LC oscillator. nMOS and pMOS are connected as cross coupled to generate negative resistance. If this negative resistance could compensate for the loss of LC tank, the circuit will start oscillation. is the on-chip spiral inductor with a 3.7-nH inductance. The series resistance of the spiral inductor is around 4.6 , and its quality factor is 4.2 at 1 GHz. The varactor is implemented by a P+/N-well junction capacitor. The capacitance of the varactor is controlled by re-versed bias of the P+/N-well junction. To reduce sensitivity to power supply, the dc blocking capacitors are connected in se-ries to the varactor with a grounded resistor. The other advan-tage of this topology is that the controlled voladvan-tage can be a full swing between supply voltage and the ground. and ( and ) are cross connected for the positive feedback to form the negative resistor. acts like a tunable current source to control the output swing of the VCO. By means of selective switches , linear capacitors 5–7 are uti-lized to universal tune the VCO frequency band to improve the yield rate in mass production. An autotuning mechanism will be implemented in the future to reduce test costs.
Fig. 4(b) shows the schematic of the CP circuit. The sinking or/and sourcing current depends on the command of UPB to and the command of DN to , therefore and are switches. will discharge the parasitic capacitance on the drain of while is off. Otherwise, the charge will leak to the loop filter. Also, will discharge the parasitic capacitance on the drain of while is off. It can be observed that the sinking/sourcing current tends to zero when PLL is locked near the edge of the up/down command.
In a typical PLL type frequency synthesizer, a frequency divider is usually used to select the desired lock frequency. The architecture of the frequency divider incorporates a high speed dual-modulus prescaler (DMP), a low-speed programmable counter, and a low-speed swallow counter, as depicted in Fig. 4(c). Initially, DMP divides the input frequency by . The swallow counter counts the DMP output pulses until S pulses are reached. Then the DMP modulus control is changed, which forces the divide ratio of DMP to be changed to Np. The DMP output pulses are also counted in the program counter. Fig. 4(d) and (e) show a logic block and associated timing diagram of the prescaler. If the program counter has counted P pulses, it will reset itself and the swallow counter. The total divide ratio of the frequency divider can be represented as
(5) The use of a variable modulus prescaler at high frequency in-stead of using a fixed frequency prescaler has the advantage that
only the prescaler works at high frequency while the remaining divider circuitry works at much lower frequencies. This saves power, reduces the cost, and makes the layout of the divider rel-atively noncritical. The main contributors to the PLL synthesizer power consumption are the VCO (up to 70%, 23 mW) and the frequency divider (up to 30%, 9 mW). The phase noise contri-bution of the prescaler to the phase of frequency synthesizer is usually negligible. The overall noise from the prescaler is much lower than that of a crystal reference multiplied by the prescaler ratio [19].
The out-of-band phase noise of a PLL synthesizer is mainly determined by the VCO. The in-band phase noise, however, is determined by the remaining loop components and is mul-tiplied by the division factor of the prescaler. In order to achieve a fine frequency resolution, a high division factor is needed, severely deteriorating the in-band noise and, consequently, the root mean-square (rms) phase error , which may not ex-ceed 2 (i.e., dBc/Hz in a 200-kHz band). In order to in-crease the flexibility of the frequency synthesizer for settling time, the loop filter is implemented by off-chip discrete com-ponents. The crystal oscillator also requires a discrete crystal providing a reference signal with high quality. A CP current of 200 A is adopted in this design to achieve good stability, good transient behavior, low steady-state phase error, and low-power dissipation. A second-order loop filter is used to achieve loop bandwidth of 200 kHz.
E. IF Section
A low-voltage low-power 10.7-MHz IF section shown in Fig. 5(a) including a limiting amplifier and an frequency mod-ulated (FM) FSK demodulator is proposed. The FSK means that the information in the transmitted data is encoded by using two different frequencies. These two frequencies differ from each other by the selected deviation. In principle the IF signals processing circuit performs limitation of signal magnitude and signal demodulation in FM/FSK. A limiting amplifier in FM/FSK applications is usually employed in the limitation of the signal magnitude [20]. However, it may reduce the sensitivity and therefore degrade the recovered data bit-error rate (BER) due to a large dc offset [21]. Signal demodulation in FM/FSK requires an FM/FSK demodulator with high frequency discrimination as a result of the narrow signal bandwidth of the FSK. In fact, FSK can be regarded as a discrete FM signal whose frequencies are equally spaced and centered at a nominal carrier frequency.
The limiting IF amplifier represents essentially a chain of gain cells, which expand the different magnitudes of input signal into saturation. The limiting amplifier is implemented by a cascade of identical gain cells that come with an auxiliary output driver as shown in Fig. 5(b). The limiting amplifier is designed with a proper dc feedback loop. With the dc feedback loop, the dc offset can be suppressed and will not saturate the following stage. To extract dc offset voltage, a large discrete capacitor is necessary to save chip area. The core of the gain cells, as shown in Fig. 5(b), is a source-coupled differential input pair – with a diode-load – . and perform as a full-wave rectifier for converting the signal magnitude into
Fig. 5. (a) IF section. (b) Block diagram of the limiting amplifier with gain cell circuit. (c) Block diagram of the FM/FSK demodulator. (d) Proposed quadrature detector: multiplier circuit.
subsequent current. The outputs of each full-wave rectifier are connected in parallel to the external capacitor and resistor as shown in Fig. 5(b). Therefore, the resulting voltage in the ex-ternal capacitor and resistor will be proportional to IF signal amplitude. At the same time, it must yield a low-pass function to alleviate the dc offset due to mismatch. Fig. 5(c) shows a block diagram of the FM/FSK demodulator. The FM/FSK de-modulator employs a quadrature detector that is composed of an on-chip phase detector and an external tank phase shifter to achieve high discrimination function under low-voltage opera-tion. The proposed quadrature detector [22], [23], based on the multiplier output which in turn is proportional to the product of two input variables, for FM/FSK demodulation is shown in Fig. 5(d). In this structure, a phase shifter shifts the phase of the incoming FM signal by an amount that is proportional to its instantaneous frequency. A phase detector (PD) is then used to detect the phase difference between the limiting amplifier output signal and its phase-shifted signal. Finally, a low-pass post filter is used to remove high-frequency noise and extract the demodulated output. This method converts frequency deviation into shift of the phase. Therefore, appropriate value of the phase shift can improve the frequency discrimination in demodulation. The frequency to voltage conversion gain of the demodulator is 15 mV/kHz and the dynamic range of the limiting amplifier is around 80 dB. The sensitivity of the IF section including the de-modulator and limiting amplifier achieves dBm. The pro-posed IF section dissipates a power of 14 mW.
IV. EXPERIMENTALRESULTS
A single-chip of low-IF 915 MHz receiver of single-conver-sion was fabricated by using a standard 1P5M CMOS tech-nology of 0.25 m. The fabricated receiver was measured under a nominal 3.3 V voltage supply, and it remained functional from 2.7 to 3.6 V and above. During measurement, the bare die was housed in a 32-lead LQFP plastic package. The dielectric of the PCB used in this work was standard FR4 with a relative dielec-tric constant of approximately 4.5 between 2–3 GHz. A socket with high frequency operation was used to contact the ICs in-stead of solder. Capacitors with different values were used as the bypass capacitors for and to filter out the noise with different frequencies. The self-resonance frequency of these ca-pacitors must be sufficiently high to pass the output signals with small loss.
Due to the input impedance of LNA being designed to around 50 over a large frequency bandwidth; the of the receiver input is smaller than dB. Fig. 6 shows versus frequency. The minimum value of was measured at 1 GHz. So, the receiver can achieve the maximum power transfer from the an-tenna. In order to obtain the maximum performance, no buffers were used after LNA for measurement.
The conversion gain of the RF front-end including the LNA and mixer is measured with a 10.7-MHz IF frequency. The LO signal is generated by an on-chip frequency synthesizer. The RF signal is fed by a RF signal generator. The frequency response of the RF front-end is shown in Fig. 7. The conversion gain is larger than 11 dB over the ISM band. Fig. 8 shows the noise figure of the RF front-end, which is less than 9 dB. The
min-Fig. 6. S of the LNA.
Fig. 7. Conversion gain of the ISM receiver’s front-end.
Fig. 8. Noise figure of the ISM receiver’s front-end.
imum noise figure of 5 dB is obtained at the RF front-end with a maximum conversion gain. The IIP3 of the RF front-end is measured by two applied tones with spacing of 1 MHz. The IIP3 of the RF front-end is dBm as shown in Fig. 9. This spec-ification is appropriate for many applications such as wireless mouse, wireless keyboard, etc.
With 0.1% BER, the sensitivity at IF input of the receiver is dBm. The maximum signal power of the demodulator can demodulate at IF input is 8 dBm. In an IF section, the limiting amplifier has a RSSI function. The RSSI output voltage versus
Fig. 9. IIP3 of the ISM receiver’s front-end.
Fig. 10. RSSI output voltage.
Fig. 11. VCO tuning range.
the IF input power is shown in Fig. 10. When the IF input power is larger than dBm, the curve is quite linear as shown in Fig. 10. In the limiter design, the current consumption is only 3 mA. The measured voltage gain is 78 dB over a 12-MHz band-width. In the proposed receiver, the quadrature demodulator is used to demodulate the FSK receiver signal. The current con-sumption is only 1 mA in the demodulator. The receiver data rate with 390 kbps can be achieved and the receiver sensitivity is dBm with 0.1% BER. In Fig. 11, the tuning character-istic measured from the on-chip LC VCO shows a tuning fre-quency range of 110 MHz varying from 860 to 970 MHz as the
Fig. 12. Current contribution of the ISM receiver.
Fig. 13. Chip photograph.
controlled voltage is changed between 0.2 and 2.3 V. As the os-cillation frequency of the quadrature VCO varies between min-imum and maxmin-imum in terms of the tuned range, the simulated peak-to-peak voltage swing of the quadrature VCO is around 1 – . Therefore, the oscillation of the quadrature VCO oc-curs in the regime of limited current. This large swing signal can make the switching MOS in Gilbert mixer function properly and reduces the noise from the switching MOS.
Fig. 12 shows the current contribution of the receiver chip with a typical power supply voltage of 3.3 V. The current con-sumption of the RF section including a LNA and a mixer is 12 mA. The IF section consumes 8 mA with the frequency syn-thesizer dissipates 13 mA. A photomicrograph of the fabricated 915 MHz receiver chip is shown in Fig. 13. The die size is 2450 m 2450 m. The input pin of the LNA is located in the middle of one side to minimize the length of the bonding wire. Thus, the influence of bonding wire variation can be minimized. Four on-chip spiral inductors are used in this design and they consume a large part of the chip area. Thus, reducing the number of the on-chip spiral inductors is an efficient way to reduce the
TABLE I
PERFORMANCESUMMARY OFTUNABLEISM RECEIVER
TABLE II
COMPARISONWITHPREVIOUSWORKS
chip area. The measured performances of the single-chip re-ceiver are summarized in Table I. Table II sums up a comparison with previous works.
V. CONCLUSION
This paper describes a tunable low-power fully integrated FSK receiver, which is a monolithic, single-chip receiver IC specially optimized for wireless consumer applications in the ISM band of 915 MHz. The IC offers a high level of integration such that minimal external components (e.g., the channel-select filter, the discriminator, and the loop filter) are required. With on-chip selective switches for resistive and capacitive load, the center frequency and gain of receiver front-end can be tunable against the process variation. The receiver’s sensitivity under bi-nary FSK demodulation is dBm with IF bandwidth of 200 kHz.
ACKNOWLEDGMENT
The authors wish to thank Prof. G. Turner-Walker for his proofread.
REFERENCES
[1] J. Crols and M. Steyaert, “A single-chip 900 MHz receiver front-end with a high performance low-IF topology,” IEEE J. Solid-State Circuits, vol. 30, no. 12, pp. 1483–1492, Dec. 1995.
[2] J. C. Rudell et al., “A 1.9-GHz wide-band IF double conversion CMOS receiver for cordless telephone applications,” IEEE J. Solid-State
Cir-cuits, vol. 32, no. 12, pp. 2071–2088, Dec. 1997.
[3] A. Rofougaran et al., “A single-chip 900-MHz spread-spectrum wireless transceiver in 1-m CMOS—Part II: Receiver design,” IEEE J.
[4] D. K. Shaeffer et al., “A 115-mW, 0.5m CMOS GPS receiver with wide dynamic-range active filters,” IEEE J. Solid-State Circuits, vol. 33, no. 12, pp. 2219–2231, Dec. 1998.
[5] P. Orsatti, F. Piazza, and Q. Huang, “A 20-mA-receiver, 55-mA-trans-mitter single-chip GSM transceiver in 0.25m CMOS,” IEEE J.
Solid-State Circuits, vol. 34, no. 12, pp. 1869–1880, Dec. 1999.
[6] S. Wu and B. Razavi, “A 900-MHz/1.8-GHz CMOS receiver for dual band applications,” IEEE J. Solid-State Circuits, vol. 33, no. 12, pp. 2178–2185, Dec. 1998.
[7] A. A. Abidi, “Direct-conversion radio transceiver for digital communi-cation,” IEEE J. Solid-State Circuits, vol. 30, no. 12, pp. 1399–1410, Dec. 1995.
[8] F. Behbahani, Y. Kishigami, J. Leete, and A. A. Abidi, “CMOS mixers and polyphase filters for large image rejection,” IEEE J. Solid-State
Cir-cuits, vol. 36, no. 6, pp. 873–887, Jun. 2001.
[9] A. A. Abidi, “Noise in active resonators and the available dynamic range,” IEEE Trans. Circuits Syst., vol. 39, pp. 296–299, Apr. 1992. [10] D. Shaeffer et al., “A 115 mW CMOS GPS receiver,” in Int. Solid-State
Circuits Conf. Tech. Dig., Feb. 2001, pp. 122–123.
[11] F. Op’tEynde et al., “A fully-integrated single-chip SOC for bluetooth,” in Int. Solid-State Circuits Conf. Tech. Dig., Feb. 2001, pp. 196–197. [12] A. Ajjikuttira et al., “A fully-integrated CMOS RFIC for bluetooth
ap-plications,” in Int. Solid-State Circuits Conf. Tech. Dig., Feb. 2001, pp. 198–199.
[13] N. Filiol et al., “A 22 mW bluetooth RF transceiver with direct RF mod-ulation and on-chip filtering,” in Solid-State Circuits Conf. Tech. Dig., Feb. 2001, pp. 202–203.
[14] N. Karanicolas, “A 2.7 V 900 MHz CMOS LNA and mixer,” IEEE J.
Solid-State Circuits, vol. 31, no. 12, pp. 1939–1944, Dec. 1996.
[15] T. H. Lee, The Design of CMOS Radio-Frequency Integrated
Cir-cuit. Cambridge, U.K.: Cambridge University Press, 1998, p. 282. [16] D. M. Pozar, Microwave Engineering, second ed. New York: Wiley,
1998.
[17] A. S. Shahani, D. K. Shaeffer, and T. H. Lee, “A 12 mW wide dynamic-range CMOS front-end for portable GPS receivers,” in Int. Solid-State
Circuits Conf. Tech. Dig., Feb. 1997, pp. 368–369.
[18] F. Stubbe, S. V. Kishore, C. Hull, and V. Torrel, “A CMOS RF-receiver front-end for 1 GHz,” in Proc. Symp. VLSI Circuits Tech. Dig., 1998, pp. 80–83.
[19] M. Driscoll and T. Merrell, “Spectral performances of frequency mul-tiplier and dividers,” in Proc. 46th IEEE Ann. Freq. Contr. Symp., May 1992, pp. 193–200.
[20] S. Khorram, A. Rofougaran, and A. A. Abidi, “A CMOS limiting am-plifier and signal-strength indicator,” in Proc. Symp. VLSI Circuits Dig.
Tech. Papers, Jun. 1995, pp. 95–96.
[21] M. Nakamura et al., “An instantaneous response CMOS optical receiver IC with wide dynamic range and extremely high sensitivity using feed-forward autobias adjustment,” IEEE J. Solid-State Circuits, vol. 30, pp. 991–997, Sep. 1995.
[22] V. Thomas, J. Fenk, and S. Beyer, “A one-chip 2 GHz single superheat receiver for 2-Mb/s FSK radio communication,” in Proc. IEEE Int.
Solid-State Circuits Conf., Feb. 1994, pp. 42–43.
[23] S.-Y. Hsiao and C.-Y. Wu, “A parallel structure for CMOS four-quad-rant analog multipliers and its application to 2-GHz RF downconversion mixer,” IEEE J. Solid-State Circuits, vol. 33, no. 6, pp. 859–869, Jun. 1998.
[24] S. Tadjpour, E. Cijvat, E. Hegazi, and A. A. Abidi, “A 900-MHz dual conversion low-IF GSM receiver in 0.35-m CMOS,” IEEE J.
Solid-State Circuits, vol. 36, no. 12, pp. 1992–2002, Dec. 2001.
Simon Cimin Li received the B.S. degree in
elec-trophysics from National Chiao-Tung University, Hsinchu, Taiwan, R.O.C., in 1982 and the M.S. de-gree in electrical engineering from National Taiwan University, Taipei, R.O.C., in 1984. He received the Ph.D. degree in electrical engineering from Rensselaer Polytechnic Institute, Troy, NY, in 1991.
He was the Codirector of Chip Implementation Center (CIC), National Science Council (NSC), R.O.C., 1992. Since then, he has been the Director of Advanced Technology and Integrated System Lab-oratory (ATIS Lab.), National Yunlin University of Science and Technology, Taiwan, R.O.C. In 2003, he joined Taiwan SPIN Research Center, Taiwan, R.O.C. He is an Invitee at the Institute of Communication Engineering (ICE) National University of Tainan, Tainan, Taiwan, R.O.C. His research interests include low-voltage analog integrated circuit design, RF communication circuits design, magnetic random access memory (MRAM), and wireless transceivers in RFID applications.
Dr. Li received an IBM Graduate Scholarship in 1987 and an SRC Graduate Research Assistantship from 1988 to 1991.
Hong-Sing Kao was born in Taipei, Taiwan, R.O.C.,
in 1972. He received the B.S. degree from the Department of Electronics Engineering, National Yunlin University of Science and Technology, Yunlin, Taiwan, R.O.C., and the Ph.D. degree from the Institute of Electronics, National Chiao-Tung University, Hsinchu, Taiwan, R.O.C., in 1995 and 2003, respectively.
In 2003, he joined the Department of Communica-tion Engineering, NaCommunica-tional Chiao-Tung University, as a Postdoctoral Researcher. His research interests in-clude analog integrated circuits design and RF integrated circuits design.
Chia-Pei Chen was born in Chia-I, Taiwan, R.O.C.,
in 1972. He received the M.S. degree from the Institute of Electro-Optical Engineering, National Chiao-Tung University, Hsinchu, Taiwan, R.O.C., in 1997. He is currently working toward the Ph.D. degree at the Institute of Electronics, National Chiao-Tung University.
His research interests include analog integrated circuits design and RF integrated circuits design.
Chung-Chih Su was born in Hawlian, Taiwan,
R.O.C., in 1968. He received the B.S. degree from the Department of Electronics Engineering, National Yunlin University of Science and Technology, Yunlin, Taiwan, R.O.C., and the M.S. degree from the Institute of Electronics, National Chiao-Tung University, Hsinchu, Taiwan, R.O.C., in 1994 and 2002, respectively.
He is currently with AlfaPlus Semiconductor Inc., Taiwan, R.O.C., working on RF CMOS circuit and transceivers for wireless communications.