vides a quadrature phase for 2.4 GHz and an octal phase for 5.2
GHz to generate an IQ signal for the sub-harmonic mixer. Figure
3 shows the sub-harmonic mixer schematic [3]. This mixer can
also be used as a traditional Gilbert mixer if LO_0 port is con-
nected to LO_180 port; and the LO_90 port is connected to
LO_270 port simultaneously. Therefore, the circuit design can be
simplified. There is an additional function of this mixer, which is
a band selector. Depending on the receiving RF signal strength, a
band-selecting control signal coming from the baseband can be
used to control the on/off of this mixer. Because of this mecha-
nism, we can easily select which band we chose before the band-
pass filter. A 10 MHz center frequency and 20 MHz bandwidth
polyphase band-pass filter is designed to provide the image rejec-
tion and filtering out the unwanted high frequency signal. To save
power consumption and chip area, gm-C cell is implemented for
this polyphase band-pass filter.
3. MEASUREMENT RESULT
This concurrent compact dual-band receiver is implemented using
HHNEC 0.18-m CMOS 1P6M technology. For a 1.8 V power
supply, the overall power consumptions is simulated to be 66.1
mW. Table 1 summarizes all the measurement results. The pro-
posed dual-band receiver has a fairly good performance as com-
pared with the conventional receivers of individual receiving paths
(as shown in Table 2). For noise issue, differential design concept
is introduced. In addition, we not only use double guard ring layout
style (N-well and P-substrate) to surround each individual block,
but also individual power supply is used for each block. Another
layout consideration is the RF signal penetrating through substrate
issue; therefore, a metal1-shielding layer is added to form an ideal
ground plate. Figure 4 shows the die photo of the proposed RF
front-end chip with a die size of 2450 1700 m
2
. Figure 5 shows
the dual-band receiver and Figure 6 shows the measured results.
4. CONCLUSION
A low-cost and low-power IEEE 802.11a/b/g compact dual-band
radio receiver for wireless LAN applications has been designed in
a standard 0.18-m CMOS 1P6M technology. To save chip area,
sub-harmonic mixer is used so that only one multi-modulus syn-
thesizer is needed for this compact dual-band receiver design. The
receiver has a simulated 2.8 dB and 4.3 dB receiver chain noise
figure at 2.45 GHz and 5.25 GHz, respectively. For a 1.8 V power
supply, the overall power consumption was only 66.1 mW.
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© 2009 Wiley Periodicals, Inc.
EFFICIENT TENSOR BASED FDTD
SCHEME FOR MODELING SLOPED
INTERFACES IN LOSSY MEDIA
Gurpreet Singh,
1
Eng Leong Tan,
1
and Zhi Ning Chen
2
1
School of Electrical and Electronic Engineering, Nanyang
Technological University, Singapore 639798; Corresponding author:
gurp0002@ntu.edu.sg
2
Institute for Infocomm Research, Singapore
Received 5 October 2008
ABSTRACT: This article presents an efficient tensor based finite-differ-
ence time-domain (FDTD) scheme for modeling sloped interfaces in
lossy media. The formulated scheme achieves its improved efficiency by
implicitly solving the internal fields affected by an interface. This per-
mits the reduction of updating coefficients in the scheme. FDTD simula-
tions that are generally used to compute scattering parameters or radar
cross sections gain from this implicit computation. The scheme is formu-
lated without assuming any single frequency approximation, previously
assumed in the literature. This permits FDTD simulation results over a
wide frequency bandwidth in a single FDTD simulation run. To allow a
more accurate and conformal approximation, the scheme extends the
use of cell filling ratio to lossy media. © 2009 Wiley Periodicals, Inc.
Microwave Opt Technol Lett 51: 1530 –1537, 2009; Published online in
Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mop.
24398
Key words: finite-difference time-domain (FDTD) method; 2-dimension
tensor; sloped interfaces; lossy media
1. INTRODUCTION
The finite-difference time-domain (FDTD) method has been
widely used to obtain solutions of Maxwell’s equations in complex
geometries with complex materials. However, a significant flaw is
its staircase approximation of planar, sloped or curved interfaces
between different media on a Cartesian FDTD grid. Various meth-
ods [1, 2] have been proposed to minimize the errors caused by the
staircase approximation. One such class of methods is based on
properly constructing an average of the material’s properties in the
vicinity of the interface and using it to accurately solve the affected
field components. For dielectrics, various effective permittivities
have been determined in previous literature [2–5]. However, these
permittivites do not completely account for the effective anisot-
ropy induced by sloped or curved interface.
1530 MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 51, No. 6, June 2009 DOI 10.1002/mop