Bluetooth Receiver
Bluetooth Receiver
Ryan Rogel, Kevin Owen
Abstract—A Bluetooth radio front end is developed and each
block is characterized. Bits are generated in MATLAB, GFSK
endcoded, and used as the input to this receiver model in
Cadence. The output is then analyzed for various bit sequences,
and input to a MATLAB demodulator. This circuit has 67 dB of
gain, a 1dB compression point of -21.9 dBm, and draws 7.86 mW
from 1.2 VDD. This circuit was designed in 0.13m IBM CMOS
Index Terms—Receiver, Bluetooth, GFSK
was developed in 1994 by Ericsson to provide
short-range, wireless data links with 1 Mb/s data rate.
Since then, Enhanced Data Rate (EDR) schemes have adopted
/4-DPSK and 8-DPSK modulation schemes to achieve data
rates of 2 and 3 Mb/s, respectively. Bluetooth has been
integrated into numerous devices including cell phones,
computers, speakers, printers, keyboards, and almost all
devices currently employing wireless technology. The
important figures of merit for any receiver include power
consumption, noise figure, input referred 1 dB compression
point, gain, and sensitivity. We will evaluate our receiver
against two published receivers over the last six years using
these as our comparison.
Fig. 1a. Frequency Shift Keying
Fig. 1b. Gaussian Frequency Shift Keying
Bluetooth uses Gaussian frequency shift keying, in which
bits are encoded as frequency deviation from the carrier using
a Gaussian filter. Figures 1a and 1b illustrate this concept.
Figure 1a illustrates FSK, in which the frequency deviation
occurs abruptly with each bit change, realized in time as a
tone multiplied by a square pulse. In frequency this is
equivalent to a sinc function convolved with an impulse,
which is infinitely wide, with non-negligible side-lobes.
Figure 1b illustrates the gradual frequency deviation from the
carrier accomplished by replacing the square pulse of the FSK
implementation with a Gaussian filter. Because a Gaussian
pulse in time is Gaussian in frequency, this modulation
scheme is realized in time as a Gaussian pulse multiplied with
a tone, which is a Gaussian pulse convolved with an impulse
in frequency. Due to the infinitely attenuating nature of a
Gaussian function, the bandwidth of the FSK signal is
lessened using GFSK.
in-phase and quadrature down-converted signals. Our system
uses direct down-conversion to avoid image rejection. This is
made feasible by not transmitting data at the carrier frequency,
which would be difficult to extract from the large DC output
characteristic of direct down-conversion.
The first stage of our system consists of an LNA and
preamplifier to provide high gain with low noise. This stage
also acts as an active balun, converting the single ended input
to a differential output. The next stage is the mixer, which
uses the differential output from the LNA and the differential
output of the VCO as its inputs. The VCO is an LC oscillator
for less phase noise than a ring oscillator, at the expense of
slightly higher power. The last block in our construction is an
active low pass filter, which also acts as a balun. The output
from this block is then demodulated in MATLAB. In the
sections that follow we analyze each block individually.
Figure 2 illustrates a system level block diagram of our
receiver. This receiver takes a single ended input, and outputs
The first stage of our system consists of an LNA and a
Fig. 2. System Block Diagram
preamplifier. The LNA is a cascoded common source
amplifier that is degenerated for input matching. This circuit is
illustrated in Figure 3, and the resonant frequency can be
calculated as in Equation 1.
0 
CGS  LG  LS 
Fig. 3. LNA
Eq. 1
The input impedance at 0 was calculated in class, and is
included as Equation 2.
 g 
Z IN  LS  m 
 CGS 
Eq. 2
From Equation 2, we can see that the real component of the
input impedance can be matched to the 50  source
impedance using gm, CGS, and LS. Furthermore, the output
load is tuned to 0, using CL and LD, which is used to
attenuate out-of-band frequencies, while allowing the desired
signal to pass to the preamplifier. The desired current density
through M1 in the LNA is achieved by mirroring IBIAS and
sizing M1 appropriately. M2 is used for cascoding in order to
achieve reverse isolation, limiting LO leakage to the antenna.
With this design we are able to achieve 14 dB of voltage gain
with 2 dB noise figure and 13.5 dB reverse isolation. The 1
dB compression point is -21 dBm, consuming 876 W from
1.2 VDD.
The preamplifier is illustrated in Figure 4, and serves as an
active balun in addition to providing additional gain. The
input from the LNA passes through the decoupling capacitor,
CBIG, and appears over CGS1 of the preamplifier. The gate of
M3 is biased with a DC voltage to keep it in saturation, which
serves as an AC ground. The output of this amplifier is
approximated in Equations 3a & 3b, illustrating how this
amplifier acts as an active balun.
VOUT    g m1  g m 2 ro1ro 2  VGS 1
Eq. 3a
Fig. 4. Preamplifier
VOUT   g m 3  g m 4 ro 3 ro 4  VGS 1
Eq. 3b
These equations are in the ideal case, with a tail source of
infinite impedance. Finite tail source impedance causes slight
amplitude mismatch between VOUT- and VOUT+.
This amplifier uses cascode transistors M2 and M4 for
higher output impedance and gain, as well as improved
reverse isolation. The preamplifier has a noise figure of 6 dB,
15 dB voltage gain, 13 dB reverse isolation, and a 1 dB
compression point of -8 dBm, while consuming 990 W from
1.2 VDD.
The VCO is realized as an LC tank oscillator, which
provides better phase noise than a ring oscillator. The circuit
construction is illustrated in Figure 5. The tuning capacitors
were originally realized as source-drain connected NFETs, but
the back gate effect from LO leakage through the substrate
was amplified in the preamplifier, overwhelming the desired
signal. By using drain-source connected PFETs, we achieved
Fig. 7. Low Pass Filter
Fig. 5. VCO
accuracy of at least 2.5mV. However, the frequency response
to tuning voltage is nonlinear, having roughly square root
dependence. This implies that the step size would have to be
less than 2.5mV/channel (given a 1MHz channel) over certain
channels, requiring even stricter requirements on the DAC.
However, changing the ratio of C:Ctune can increase the tuning
step size.
This VCO has an output amplitude of 350 mV centered at
750 mV, consuming 562 W from 1.2 VDD.
Fig. 6. Double-Balanced Gilbert Cell Mixer
better isolation due to the isolated well. We later learned that
there are designated varactors in the kit, but did not employ
them in our design. The parallel capacitors, both labeled C,
are parallel MIM capacitor with equal capacitance, connected
oppositely. The purpose of doing this is to simulate similar
loading to both sides of the VCO for proper oscillation and
duty cycle. The inductor in the LC tank is a symmetrical
inductor, which is also to mimic equal loading to both sides of
the tank. This inductor has a center tap which can be used to
DC bias the output signal. We did not employ this feature
because this circuit is self-biasing and we wanted to avoid an
additional voltage reference. However, this feature can be
extremely useful because optimization of the mixer might
require a DC voltage at the LO input that cannot be achieved
using the self-biasing of the VCO.
Our VCO operates between 2.41GHz and 2.49 GHz with a
voltage tuning range of 400-600mV, requiring a DAC
Our mixer is a double-balanced Gilbert Cell mixer. Using
direct down-conversion we are able to avoid image rejection,
but the DC output of the mixer stage must be the DC input to
the next stage because we can no longer AC couple stages at
baseband. Figure 6 illustrates our mixer. The LO transistors
commutate the RF signal from one side to the other at 0. In
this configuration, the DC bias current through each side of
the output doesn’t vary in time (ideally), and only the RF
signal is commutated from side to side. Therefore, the LO is
not present at the output, and only the IF frequency is present
at the output. Because we are modulating to baseband, our IF
is zero and only the demodulated signal is present at the
output. Equation 4 illustrates the output of the mixer.
VBB  sgn VRF 
Eq. 4
This mixer has a 1 dB compression point of -4dBm, inputreferred 3.27 nV/Hz½ thermal noise floor with 200 kHz corner
frequency input referred, and 11dB noise figure at mod,
where mod is the maximum frequency deviation from the
carrier. The mixer consumes 1.98 mW from 1.2 VDD.
After down-conversion, the signal will need to be low-pass
filtered to remove the higher modulation terms. This can be
done with a passive filter, but in order to achieve additional
Fig. 9. Output for [010101010101] input at -80 dBm. In-phase (red),
quadrature (blue), and the sum of the two (black) are presented,
Fig. 8. The layout is 1.5x0.8mm2.
gain, we have chosen to use an active filter. Using an active
filter also acts as an active balun, recombining the differential
signal to a single ended output. Figure 7 illustrates our filter. It
is a differential amplifier with a current-mirror load, which
provides the balun functionality. By choosing an appropriate
value of CL, we can make the output node the dominant pole
and use this circuit as a low-pass filter with a 3 dB cutoff
frequency of 1/(RoutCL). This stage could also employ a
variable tail current source in order to achieve variable gain,
as the gain of this stage is gmRout, with gm being a function of
current density.
This stage provides 19.2 dB of gain, has a 1 dB
compression point of -2.1dBm, 750 kHz bandwidth (CL =
7pF), and consumes 136uW from 1.2VDD.
Figure 8 illustrates the layout of our chip. The inductors in
the VCO are symmetrical inductors, while the others are not.
The in-phase and quadrature paths of the circuit have also
been laid out symmetrically to try and match these signal
paths. The LNAs have been placed as far as possible from
these parts of the circuit to try and minimize LO leakage from
the mixer and VCO to the earlier stages. This layout is
In demodulating the output signal, we found each received
bit results in an output pulse whose time constant is defined
Fig. 10. Output for [111111111111] input at -50 dBm. In-phase (red),
quadrature (blue), and the sum of the two (black) are presented,
by the bandwidth of the low-pass filter. Figure 9 illustrates the
output for an input of 010101010101. The output has the
expected bit rate of 1 MHz, with a rising edge for an incoming
zero bit, and a falling edge for an incoming one bit. This leads
to a concern that the output might saturate high or low for an
input with an imbalance of ones or zeros.
Figure 10 addresses this concern, and illustrates the output
for an input of 111111111111. We notice that the edge
initially falls with each bit as expected, but eventually begins
to rise. This can be explained by the phase shift that occurs
with each incoming bit. Because the bits are encoded as a
frequency deviation from the carrier, the phase offset between
the LO and signal that results from each incoming bit is the
integration of the frequency deviation over the bit interval.
This is visualized as the area under each Gaussian bit pulse in
Figure 1b. We can see in this figure that the area, and
therefore deviation, is constant for each bit, and varies only in
sign. This would be different for various modulation schemes,
but would still be known to the receiver, and therefore
deterministic from the received data.
Figure 11 illustrates the phase shift for Binary GFSK as a
rotation in the S-plane by a constant angle  for each
incoming bit. By ensuring that the pilot that precedes each
data packet contains an equal number of ones and zeros, we
can ensure that there is no phase offset resulting from this part
of the signal. Therefore, by representing bits 0 and 1 as
symbols -1 and 1, respectively, we can calculate the phase
offset for a given packet of length k using equation 5.
S n   1,1
Fig. 11. Binary GFSK constellation rotation due to phase offset.
n 1
offset   Sn * ,
2008 [3]
Gain [dB]
Tech. (CMOS)
2004 [2]
In this paper we have presented a Bluetooth radio front end
that has 67 dB of gain, a 1 dB compression point of -21.9
dBm, and draws 7.86 mW from 1.2 VDD. This chip was
designed in IBM 0.13m CMOS process. A comparison of
this chip and previous works is presented in Table 1.
Eq. 5
By maintaining the packet length short enough, we can ensure
that the phase deviation will not exceed tolerable bounds.
Lastly, in Figure 9 we note the rising edge triggered by the
incoming signal, which begins at 100ns. This energy can be
detected by the radio as an alert of incoming data, which can
be used to wake up the radio if a low power mode is desired.
We would like to thank Professor David Wentzloff,
Muhammad Faisal, Jonathan Brown, and Kuo Ken Huang for
their help in design and analysis of this circuit.
We were disappointed that we did not have enough time or
manpower to conduct a full noise analysis of this circuit. We
would have liked to determine the input referred noise
variance for this circuit to generate bit streams with varying
SNR values at the input. By demodulating the output and
calculating the BER for each SNR, we could create a waterfall
curve for this circuit and compare that with the ideal BPSK
waterfall curve. This data would also determine the sensitivity
for our receiver based on the required BER for a Bluetooth
receiver. However, this simulation would take days, as we
would have to run at least 1000 bits per SNR value to
determine a BER of just 10-3.
We would also have liked to write a more extensive
demodulation algorithm in MATLAB, testing it over various
conditions, and to have incorporated additional modulation
schemes using complex encoding to achieve higher data rates.
Cheung, V.S.L.; Luong, H.C.; , "A 1V 10-mW monolithic Bluetooth
receiver in a 0.35μm CMOS process," Solid-State Circuits Conference,
2003. ESSCIRC '03. Proceedings of the 29th European , vol., no., pp.
687- 690, 16-18 Sept. 2003.
Yeon-Jae Jung et aI, "A 2.4-GHz 0.25-um CMOS Dual-Mode Direct
Conversion Transceiver for Bluetooth and 802.l1b", IEEE J.Solid State
Circuits, Volume: 39 Issue: 7, JULY 2004.
Aboueldahab, W.F.; Sharaf, K.M.; , "A 1.2V low power CMOS receiver
for Bluetooth," Solid-State and Integrated-Circuit Technology, 2008.
ICSICT 2008. 9th International Conference on , vol., no., pp.1577-1580,
20-23 Oct. 2008.
Bluetooth Enhanced Data Rate (EDR): The Wireless Evolution. Tech.
Agilent Technologies. Print. Application Note.
Specification of the Bluetooth System Version 4.0. 30 June 2010. Master
Table of Contents & Compliance Requirements.
Was this manual useful for you? yes no
Thank you for your participation!

* Your assessment is very important for improving the work of artificial intelligence, which forms the content of this project

Download PDF