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Transcript
A 1.55 GHz to 2.45 GHz Center Frequency Continuous-Time
Bandpass Delta-Sigma Modulator for Frequency Agile Transmitters
Martin Schmidt, Markus Grözing,
Stefan Heck, Ingo Dettmann, Manfred Berroth
Dirk Wiegner, Wolfgang Templ, Andreas Pascht
Institute of Electrical and Optical
Communications Engineering
University of Stuttgart, Stuttgart, Germany
Alcatel-Lucent Bell Labs Stuttgart
Stuttgart, Germany
Abstract—This paper presents a 4th order continuous-time
bandpass delta-sigma modulator (CT-BPDSM) with a
programmable center frequency ranging from 1.55 GHz to
2.45 GHz. The modulator is suited to be applied in multistandard class-S power amplifiers. The circuit features a
multi-feedback architecture with return-to-zero (RZ) and
half-return-to-zero (HRZ) pulses. The loop filters consist of
LC-resonators
with
emitter
degenerated
input
transconductors and Q-enhancement circuits. A configuration
register allows to program the resonator input
transconductors, the Q-enhancement circuits and the
resonator capacitances with 5 bit resolution. Fine tuning of the
resonator center frequency is achieved with varactors. The
circuit is implemented in a 200 GHz-fT SiGe-bipolar
technology. The measured SNR at 2.2 GHz center frequency is
45.5 dB in a bandwidth of 20 MHz. At 1.55 GHz the SNR
decreases to 40.7 dB. The measured uplink UMTS-FDD
ACLR (adjacent channel leakage power ratio) of the
modulator output is 48.4 dB in the first adjacent channel.
Index Terms — Delta-sigma modulator, class-S power
amplifier, bipolar integrated circuit.
conventional linear PA is replaced by a power efficient
switching-mode amplifier. The pulse sequence for the
switching-mode amplifier input is generated from the analog
RF-signal by a continuous-time bandpass delta-sigma
modulator (CT-BPDSM). A bandpass filter reconstructs the
analog signal at the output of the PA (Fig. 1).
I.
INTRODUCTION
The strong growth of mobile communications has led to
many different standards. Users expect their mobile
terminals to work in any environment and at different
locations, whereas operators want to minimize their
hardware effort by reconfigurable or programmable base
station equipment. As a result, mobile terminals as well as
base stations should provide access to several coexisting
standards in different frequency bands.
The coding schemes in recent standards like UMTS
(Universal Mobile Telecommunications System) exhibit
higher peak to average power ratios (PAPR) than older ones
like GSM (Global System for Mobile communications).
This turns out to be a severe problem for the power
amplifier (PA) in the transmission chain: The higher the
PAPR the higher the back-off a conventional linear PA has
to provide and thus the lower the power efficiency will be.
The multitude of coexisting standards and the PA power
efficiency are two of the most important issues that
suppliers of RF transmitters have to face in the next years.
The class-S concept is seen as an attractive solution to both
– power efficiency and multi-standard, multi-band operation
[1, 2]. In a transmission chain with class-S concept the
In the long term digital delta-sigma signal processing in
CMOS [3, 4] with upsampling from base band to the
switching-mode amplifier input is considered as both costand energy-efficient. However, the required clock frequency
for signal frequencies above 2 GHz is not reached yet with
current CMOS technologies. With a continuous-time
BPDSM higher signal frequencies can be achieved due to
fast analog signal processing. As an analog RF input signal
is required, only the PA is replaced by the switching mode
amplifier and the reconstruction filter in the transmission
chain. This allows for upgrades of existing RF transmitters.
As well, CT-BPDSMs remain the only solution for
modulators in class-S amplifiers with signal frequencies
well beyond 2 GHz in the near future.
The experimental results of a CT-BPDSM with a fixed
center frequency at 2.2 GHz will be presented elsewhere [5].
This work describes a CT-BPDSM for multiband operation.
The paper is organized as follows: In Section II the
architecture of the modulator and the most important circuit
blocks are described. Measurement results are presented in
Section III and in Section IV a short conclusion is given.
Figure 1. Block diagram of a class-S power amplifier
II.
CIRCUIT DESIGN
A. System architecture
Fig. 2 shows the block diagram of the circuit. A multifeedback architecture with RZ and HRZ pulses is used for
the modulator [6]. HRZ pulses are generated by a latch with
a subsequent RZ latch. The feedback currents k1r, k1h, k2r
and k2h can be controlled by externally applied currents via
current mirrors.
Each transconductor is set up of 5 binary weighted
stages that can be switched on and off separately. Currents
Ictrl from the configuration register control the bias voltage
Vb of the current source of the individual transconductors
via the circuit in Fig. 3 (c) and thus allow the individual
stages to be switched on and off.
Figure 2. Modulator block diagram with configuration register
and programmable transconductors Gq and Gm and LC-resonator
capacitors.
The Gq transconductors compensate for resistive losses
in the resonator. The transconductors Gm allow to control
the resonator voltage swing. The transconductors are
decoupled at the input by emitter followers. All
transconductances and the capacitances in the resonators can
be controlled separately via a configuration register with a
resolution of 5 bit.
In order to prevent metastability of the clocked
comparator a preamplifier is used. The preamplifier
introduces additional excess loop delay. The loop delay is
compensated by driving the comparator with a clock signal
that is delayed versus the clock signal of the digital to
analog converters (DAC). Layout caused parasitic effects
that influence the excess loop delay are minimized by a
signal flow oriented layout of the clock and the signal path.
B. Programmable transconductance
The lower end of the modulator dynamic range is
governed by the noise currents that are injected into the
resonators by the loss of the inductors, by the switchable
capacitors and by the transconductors. The upper end of the
dynamic range is limited by the transconductors’
nonlinearity. For a large dynamic range, low-noise
transconductors with high linearity are needed. This can be
achieved with emitter-degenerated differential pairs.
Fig. 3 shows two different topologies for the emitter
degeneration. The transconductor in Fig. 3 (a) requires a
higher supply voltage due to the series resistor. For this
circuit only the differential pair transistors and degeneration
resistors have a significant noise contribution. The noise of
the common current source transistor and degeneration
resistor appears as a common mode voltage at the
differential output. The circuit in Fig. 3 (b) exhibits more
circuit noise. The noise currents that are generated by the
two current source transistors and current source
degeneration resistors couple into the two complementary
outputs separately. The current source noise is not converted
to a common mode signal at the differential output. The
difference in noise power at the differential outputs was
simulated to be 4.6 dB, therefore the transconductor in
Fig. 3 (a) is chosen for this design.
C. Programmable resonator capacitance
The capacitance of the differential LC resonator consists
of two fixed capacitors Cfix connected to ground, five binary
weighted capacitors Ci with switches si for coarse tuning
and a varactor Cvar for fine tuning. Fig. 4 shows the circuit
that implements a switchable differential capacitor Ci. It
consists of two capacitors Ci that are connected to the
differential signal lines with one plate and to the emitters of
switchable emitter followers with the other plate. If the
emitter followers are switched on by Ictrl, both capacitors are
connected between one of the differential signals and a
complementary signal replica that is generated by the
emitter follower. For Ictrl = 0 the capacitors are floating and
the effective capacitance between the differential signal
lines is minimized. The total effective capacitance Ceff
between the differential signal lines can be calculated as
Ceff =
Cfix
+ ∑ si Ci + C var
2 i =1K5
with si ∈ {0,1} .
Ictrl
I0/2
I0/2
Vb
c)
Figure 3. Two types of emitter degenerated transconductors.
(a) series degeneration, (b) shunt degeneration. (c) bias control.
Ci
Ci
Figure 4. Switchable capacitor Ci with emitter followers that
generate differential replica signals.
The chip is implemented in a 200 GHz ft SiGe bipolar
technology (B7HF200) from Infineon and occupies a chip
area of 2.2 mm2. A chip photograph is shown in Fig. 5. The
measurement setup consists of a Rohde&Schwarz SMF100A for the generation of the clock signal, a SMU-200 for
sinusoidal and modulated RF input signals and the spectrum
analyzer FSQ-8. Measurements are automated with GPIB
and read out with Matlab. 180°-hybrid directional couplers
are used for single-ended-to-differential conversion for the
clock and the input signal and for the differential-to-singleended conversion of the output signal. The clock frequency
is 7.5 GHz for all measurements.
The output spectrum for an input signal frequency of
2.2 GHz can be seen in Fig. 6. The measured single-ended
output signal swing is 250 mV. The circuit draws 1.06 W
from a 3.1 V supply including the bipolar configuration and
control circuitry. Output signal and noise power in a
bandwidth of 20 MHz are plotted in Fig. 7 versus the input
power. The change from linear operation to compression is
very abrupt. The modulator starts to get saturated for an
input power about one dB below the 1-dB compression
point. This is also exactly the point where the output power
begins to deviate from its linear increase with the input
power. Therefore a reasonable estimate for the peak SNR
within the linear operation range is measured one dB below
the 1-dB compression point. The noise power density is
measured at 10 MHz offset from the carrier. The noise
power is flat in a bandwidth of at least 25 MHz around the
carrier (see also Fig. 9). The measured peak SNR is 45.5 dB
in a bandwidth of 20 MHz.
The output signal and noise power is plotted versus the
center frequency tuning range in Fig. 8. Output and noise
power are measured at the point of the peak SNR described
above. While the output power saturates at about the same
power level for all frequencies, the noise power increases
for lower signal frequencies. This is caused by the
decreasing Q factor of the resonator for lower frequencies.
However, the measured peak SNR at 1.55 GHz is still
40.7 dB. The dissipated power increases moderately from
992 mW at 2.45 GHz to 1.27 W at 1.55 GHz. This is due to
the current that is consumed by the emitter followers in the
switchable capacitors Ci.
The peak SNR of the modulator could be made even
larger with a better Q factor of the resonators. Unfortunately
the programmable Q-enhancement circuits are too weak to
cancel all the resonator losses. This is due to an
underestimation of the resonator losses in the design process
and will be corrected in future designs.
One of the most important criteria for RF transmitters is
the adjacent channel leakage power ratio (ACLR). The
power ratio of modulated UMTS-FDD (frequency division
duplex) uplink and downlink signals is measured (Fig. 9).
For uplink transmission, the modulator reaches an ACLR of
48.4 dB and 49 dB for channels that are 5 MHz and 10 MHz
offset from the carrier, respectively, at an input power level
of -11dBm. For a UMTS-FDD downlink signal the
measured ACLR is 42.8 dB at 5 MHz offset and 43.5 dB at
10 MHz offset at an input power level of -17 dBm.
Figure 5. Chip photograph
-20
-30
Output power [dBm]
EXPERIMENTAL RESULTS
-40
-50
-60
-70
-80
0
1
2
3
4
5
Frequency [GHz]
6
7
Figure 6. Measured modulator output spectrum at 2.2 GHz input
signal frequency. The spectrum analyzer resolution and video
bandwidths are 1 MHz, the sweep time is 10 s.
0
1 dB compression point
-10
Output power [dBm]
III.
-20
-30
Pout
peak
SNR
-40
-50
Pnoise
-60
-40
-35
-30
-25
-20
-15
-10
-5
0
Input power [dBm]
Figure 7. Output power and noise power in a bandwith of 20 MHz
at 2.2 GHz input signal frequency. 1-dB compression point and
peak SNR (within linear operation range) indicated.
0
-5
A comparison of delta-sigma modulators in the GHz
frequency range is given in Table I. This is the first tunable
modulator that reaches signal frequencies beyond 2 GHz
while using a moderate clock frequency of 7.5 GHz that is
suited for switching mode RF power amplifiers.
Pout
-10
Power [dBm]
-15
-20
CONCLUSION
-25
-30
-35
-40
Pnoise
-45
-50
-55
1.55
1.65
1.75
1.85
1.95
2.05
2.15
2.25
2.35
2.45
Frequency [GHz]
Figure 8. Output power and corresponding noise power in a
bandwidth of 20 MHz versus modulator center frequency
measured at the point of the peak SNR as indicated in Fig. 7.
A CT-BPDSM with a continuous center frequency
tuning range of 900 MHz is presented for the first time. The
large tuning range is based on configurable resonator
capacitors that are implemented with switchable emitter
followers.
Moreover,
input
and
Q-enhancement
transconductors are configurable. The measured SNR in
20 MHz bandwidth is 45.5 dB at a signal frequency of
2.2 GHz while the modulator consumes 1.06 W from a
3.1 V power supply. The UMTS-FDD ACLR for uplink
transmission is 48.4 dB and thus well beyond the
requirements. The SNR and the ACLR can be further
improved by extended Q-enhancement circuits.
ACKNOWLEDGMENT
-30
The authors thank Infineon technologies for layout and
tape-out support.
-35
Output power [dBm]
-40
-45
REFERENCES
-50
[1]
-55
-60
-65
-70
-75
-80
-85
2.19
2.195
2.2
2.205
2.21
Frequency [GHz]
Figure 9. ACLR measurement for UMTS FDD downlink
transmission. The signal is centered at 2.2 GHz, the adjacent
channels at ±5 MHz and ±10 MHz are marked with a hatching
pattern.
TABLE I.
COMPARISON OF DELTA-SIGMA MODULATORS IN
THE GHZ FREQUENCY RANGE
Ref.
Process
fsignal
[GHz]
fclock
[GHz]
SNR
[dB]
[7]
SiGe
1
4
53
4
59
350
[8]
InP
1.4
4
76
1
76
7700
[9]
BiCMOS
2
40
52
120
72.8
1600
[10] BiCMOS
0.95
3.8
59
1
59
75
[5]
SiGe
2.17
7.5
45
20
58
450
this
work
SiGe
2.2
7.5
45.5
20
58.5
1060
1.55
7.5
40.7
20
53.7
1270
*normalized to a bandwidth of 1 MHz
BW
[MHz]
SNR*
[dB]
Power
[mW]
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utilising bandpass delta-sigma modulator and switching mode power
amplifier," ISCAS 2004, pp. 633-636, May 2004.
[2] M. Iwamoto, A. Jayaraman, G. Hanington, P. F. Chen, A. Bellora,
W. Thornton, L. E. Larson and P. M. Asbeck, "Bandpass delta-sigma
class-S amplifier," IEEE Electronics Letters, vol 36, no. 12, pp 10101012, June 2000.
[3] T. Alpert, M. Schmidt, I. Dettmann, T. Veigel, M. Grözing, M.
Berroth, “Concept for a 12-bit Digital Bandpass Delta-Sigma
Modulator for Power Amplifier Applications,” ESSCIRC 2008,
Fringe P1, Sept. 2008.
[4] A. Frappé, B. Stefanelli, A. Flament, A. Kaiser, A. Cathelin, “An alldigital delta-sigma RF signal generator for mobile communication
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[5] M. Schmidt, S. Heck, I. Dettmann, M. Grözing, M. Berroth, D.
Wiegner, W. Templ, “Continuous-time delta-sigma modulator for a
signal frequency of 2.2 GHz,” to be published at the German
Microwave Conference (GeMiC) 2009, Munich, Germany.
[6] O. Shoaei and W. M. Snelgrove, "A multi-feedback design for LC
bandpass delta-sigma modulators," ISCAS 1995, vol. 1, pp. 171-174,
May 1995.
[7] Weinan Gao; Cherry, J.A.; Snelgrove, W.M., "A 4 GHz fourth-order
SiGe HBT band pass ΔΣ modulator ," VLSI Circuits 1998, pp.174175, June 1998.
[8] L. Luh; J. Jensen; C.-M. Lin; C.-T. Tsen; D. Le; A. Cosand; S.
Thomas; C. Fields, "A 4 GHz 4th-Order Passive LC Bandpass DeltaSigma Modulator with IF at 1.4 GHz," VLSI Circuits 2006, pp.168169, 2006.
[9] Chalvatzis, T.; Voinigescu, S.P., "A low-noise 40-GS/s continuoustime bandpass Delta-Sigma ADC centered at 2 GHz," RFIC 2006,
June 2006.
[10] B.K. Thandri and J. Silva-Martinez, “A 63 dB 75 mW bandpass
delta-sigma RF ADC at 950 MHz using 3.8 GHz clock in 0.25 μm
SiGe BiCMOS technology”, IEEE Journal of Solid-State Circuits,
vol. 42, no 2, pp.269-279, Feb 2007.