This presentation from IEEE Wireless Communications & Networking Conference in 2011 started the 5G conversation and busted many of the myths about millimeter waves and their applicability to mobile wireless communications.
67. MMB Beamforming
The “most critical” technology for MMB
Beamforming Options
• Baseband Digital Beamforming
• Baseband Analog Beamforming (phase shifters)• Baseband Analog Beamforming (phase shifters)
• RF Beamforming (phase shifters)
Challenges
• Beam pattern/codebook design
• Beam training signal/procedure/algorithm design
• Beam tracking signal/procedure/algorithm design
67
Copyright by the authors, all rights reserved
68. Array of 2 Point Sources [1/3]
θ
r
cos
2
d
θ
cos
2
d
θ
1 2
2 2
cos cos
2 2
0 0
2 2
cos cos
2 2
02
2
d d
j j
d d
j j
E E E
E E e E e
e e
E E
π π
θ θ
λ λ
π π
θ θ
λ λ
−
−
= +
= +
+
=
Same amplitude, same phase
20
0
0
2
2
2 cos cos
2
Assuming 2 1 and / 2
cos cos
2
d
E E
E d
E
π
θ
λ
λ
π
θ
=
= =
=
Copyright by the authors, all rights reserved
69. Array of 2 Point Sources [2/3]
θ
r
cos
2
d
θ
cos
2
d
θ
1 2
2 2
cos cos
2 2
0 0
2 2
cos cos
2 2
02
2
d d
j j
d d
j j
E E E
E E e E e
e e
E E
π π
θ θ
λ λ
π π
θ θ
λ λ
−
−
= −
= −
−
=
Same amplitude, opposite phase
20
0
0
2
2
2 sin cos
2
Assuming 2 1 and / 2
sin cos
2
d
E jE
jE d
E
π
θ
λ
λ
π
θ
=
= =
=
Copyright by the authors, all rights reserved
70. Array of 2 Point Sources [2/3]
1 2
2 2
cos cos
2 2 2 2
0 0
2 2
cos cos
2 2 2 2
02
2
d d
j j
d d
j j
E E E
E E e E e
e e
E E
π δ π δ
θ θ
λ λ
π δ π δ
θ θ
λ λ
− + +
− + +
= +
= +
+
=
Same amplitude, arbitrary phase difference
θ
r
cos
2
d
θ
0
0
0
2
2
2
2 cos cos
2 2
Assuming 2 1 and / 2
cos cos
2 2
E E
d
E E
E d
E
π δ
θ
λ
λ
π δ
θ
=
= +
= =
= +
Copyright by the authors, all rights reserved
cos
2
d
θ
71. Dynamic Antenna Array [1/2]
)
)
+∆
)
3
cosθ+∆
)
4
cosθ+∆
θ
(
)
cos
d
θ+∆
d
2
2 cosj d
e
π
θ
λ
−2
cosj d
e
π
θ
λ
−
( )s t( )s t( )s t( )s t
2
2 cosj d
e
π
θ
λ
+
2
cosj d
e
π
θ
λ
+
( )s t
∆
(2
cos
d
θ+∆
(3
cos
d
θ
(4
cos
d
Copyright by the authors, all rights reserved
72. Dynamic Antenna Array [2/2]
A dynamic antenna array can point in any direction to maximize the received signal
Enhanced receiver/transmitter antenna gain (reduced PA power, LNA gain)
Improved diversity
Reduced multi-path fadingReduced multi-path fading
Null/ Suppress interfering signals
Spatial power combining:
•Less power per PA
•Simpler PA architecture
Copyright by the authors, all rights reserved
73. BB Digital Beamforming
( ) ( )1M
s t− ( ) ( )1N
r t−
( )1s t 1
t
w 1
r
w ( )2r t
( )0s t 0
t
w 0
r
w ( )1r t
M
Optimal capacity for all channel conditions: min(M,N) data streams
Can support a variety of MA schemes (TDMA / OFDMA / SC-FDMA / SDMA)
High hardware complexity: M(N) full transceivers
High system power consumption
( ) ( )1M − ( ) ( )1N
r t−
( )1
t
M
w −
( )1
r
N
w −
Copyright by the authors, all rights reserved
74. BB Analog Beamforming
1
t
w 1
r
w( )s t
0
t
w 0
r
w
( )r t
M
1 data stream, antenna weights applied at “analog” baseband
Achieves high antenna gain in an arbitrary direction
Intermediate hardware complexity: M(N) RF mixers
Intermediate power consumption
( )1
t
M
w −
( )1
r
N
w −
Copyright by the authors, all rights reserved
75. RF Beamforming
1
r
w
( )s t
0
r
w
( )r t
M
1
t
w
0
t
w
Σ
1 data stream, RF phase shifters only, digitally controlled
Achieves high antenna gain in an arbitrary direction
Low hardware complexity: N RF phase shifters
Low system power consumption
No (or limited) support simultaneous transmissions to multiple users (e.g. OFDMA / SC-FDMA / SDMA)
( )1
r
N
w −( )1
t
M
w −
Copyright by the authors, all rights reserved
82. RF Transceiver
Transceiver key RF components
• Antenna, Filters, Power Amplifier (PA), Low-Noise Amplifier
(LNA), Oscillator (VCO), Mixer and Data converters (DAC/ADC)
Copyright by the authors, all rights reserved
83. Nonlinear Device
In the most general sense, the output response of a nonlinear circuit
can be modeled as a Taylor series in terms of the input signal voltage
2 3
0 0 1 2 3
where the Taylor Coefficients are defined as
i i iv a a v a v a v= + + + +L
( )0 0
0
1
2
0
2 2
where the Taylor Coefficients are defined as
0
0
0
and higher order terms
ii
ii
a v
dv
a
vdv
d v
a
vdv
=
=
=
=
=
iv ov
Copyright by the authors, all rights reserved
84. Gain Compression
Consider the case where a single frequency sinusoid is applied to the input of a
nonlinear device such as a power amplifier
0 0
2 2 3 3
0 0 1 0 0 2 0 0 3 0 0
cos
cos cos cos
iv V t
v a aV t a V t a V t
ω
ω ω ω
ω
=
= + + + +
+
L
2 0
0 0 1 0 0 2 0
3 3 0 0
3 0 0 3 0
2 3
0 0 2 0 1 0 3 0 0
2
2 0 0 3
1 cos2
cos
2
cos cos21
cos
2 4
1 3
cos
2 4
1 1
cos2
2 4
t
v a aV t a V
t t
a V t a V
v a a V aV a V t
a V t a
ω
ω
ω ω
ω
ω
ω
+
= + + +
+
+ +
= + + + +
+
L
3
0 0cos3V tω +L
0
3
1 0 3 0
2
1 3 0
0
3
Voltage gain at frequency
3
34
4
is negative in most practical amplifiers
aV a V
G a a V
V
a
ω
+
= = +
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85. Intermodulation Distortion
Consider two-tone input voltage consisting of two closely spaced frequencies
2 1ω ω− 1 22ω ω− 2 12ω ω−
1ω 2ω
12ω 22ω
2 1ω ω+
13ω 23ω
2 12ω ω+1 22ω ω+
( )
( ) ( ) ( )
( ) ( )
0 1 2
2 32 3
0 1 0 1 2 2 0 1 2 3 0 1 2
2 2
0 1 0 1 1 0 2 2 0 1 2 0 2
2 2 3
2 0 1 2 2 0 1 2 3 0 1
cos cos
cos cos cos cos cos cos
1 1
cos cos 1 cos2 1 cos2
2 2
3 1
cos( ) cos( ) cos cos3
4 4
i
o
o
v V t t
v a aV t t a V t t a V t t
v a aV t aV t a V t a V t
a V t a V t a V t
ω ω
ω ω ω ω ω ω
ω ω ω ω
ω ω ω ω ω ω
= +
= + + + + + + +
= + + + + + +
+ − + + + +
L
3
1 3 0 2 2
3 3
3 0 2 1 2 1 2 3 0 1 2 1 2 1
1 2
3 1
cos cos3
4 4
3 3 3 3 3 3
cos cos(2 ) cos(2 ) cos cos(2 ) cos(2 )
2 4 4 2 4 4
Output spectrum consists of harmonics of the form
,
t a V t t
a V t t t a V t t t
m n m n
ω ω
ω ω ω ω ω ω ω ω ω ω
ω ω
+ +
+ + − + + + + − + + +
+ =
L
0, 1, 2 3,
These combinations of the two input frequencies are called intermodulation products
± ± ± L
2 1 1 22ω ω− 2 12ω ω− 2 1 2 12ω ω+1 22ω ω+
Copyright by the authors, all rights reserved
86. Third-Order Intercept Point (IP3)
1
1 2
2 2
1 0
2
2 2 6
2 3 0 3 0
1
2
1 3 9
2 4 32
These two powers are equal at the third-order IP
P a V
P a V a V
ω
ω ω−
=
= =
1 0
2 2 2 6
1 3
1
2
3
2 2 1
3 1
3
These two powers are equal at the third-order IP
Let input signal voltage at the IP be
1 9
2 32
4
3
21
2 3IP
IP
IP IP
IP
V V IP
V
a V a V
a
V
a
a
P P a V
a
ω =
=
=
= = =
Copyright by the authors, all rights reserved
87. Mixer
IFf
LOf
RF LO IFf f f= ± RFf
LOf
IF RF LOf f f= ±
IFf LOf
LO IFf f+LO IFf f−
0
RF LO IFf f f− =
RF LOf f+LOf0 RFf
( ) ( ) ( )
( ) ( ) ( )
cos2 cos2
cos2 cos2
2
RF LO IF LO IF
RF LO IF LO IF
v t K v t v t K f t f t
K
v t f f t f f t
π π
π π
= =
= − + +
( ) ( ) ( )
( ) ( ) ( )
cos2 cos2
cos2 cos2
2
IF LO RF LO RF
IF RF LO RF LO
v t K v t v t K f t f t
K
v t f f t f f t
π π
π π
= =
= − + +
Copyright by the authors, all rights reserved
88. Image Frequency
IFf LOf
RF LO IFf f f= +
0
IM LO IFf f f= −
IFf LOf
IM LO IFf f f= +
0
RF LO IFf f f= −
2 IFf 2 IFf
-fIF is mathematically identical to fIF because the frequency spectrum of any real signal is
symmetric about zero frequency , and thus contains negative as well as positive frequencies
A received RF signal at the image frequency fIM is indistinguishable at the IF stage from the
desired RF signal of frequency fRF
( )
( )
IF RF LO LO IF LO IF
IF IM LO LO IF LO IF
f f f f f f f
f f f f f f f
= − = + − =
= − = − − = −
( )
( )
IF RF LO LO IF LO IF
IF IM LO LO IF LO IF
f f f f f f f
f f f f f f f
= − = − − = −
= − = + − =
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89. Homodyne (Zero-IF) Receiver
( )
( )
( )
2
2
1 cos2
cos cos cos
2
After low pass filtering
1
2
1 cos2
sin sin sin
2
After low pass filtering
1
RF
RF RF RF
RF
RF RF RF
t
I t t t t
I t
t
Q t t t t
ω
ω ω ω
ω
ω ω ω
+
= = =
=
−
= = =
( )
1
2
Q t =
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Benefits Drawbacks
Less hardware LO Leakage
Low power consumption DC offset errors
No IF stage and hence no image filter I/Q mis-match
Flicker (or 1/f) noise
90. Super-heterodyne Receiver
LOf
IFf
Copyright by the authors, all rights reserved
Benefits Drawbacks
Good sensitivity High Q filter
Good selectivity High performance oscillator
LNA output impedance matched to 50 ohm is
difficult
Integration of HF image reject filter is a major
problem
91. Wideband-IF Receiver
( )sin IF tω
( )cos IF tω
LOω
( )I t
( )Q t
( )'I t
( )cos IF tω
( )Q t
( )'Q t
Copyright by the authors, all rights reserved
Benefits Drawbacks
Image cancellation by IR mixer IR Mixer
Image rejection from the RF front-end pre-
selection filter
Good phase noise performance
92. Wideband-IF Receiver (Image Rejection)
( ) ( ) ( )
( ) ( ){ } ( ) ( ){ }
( ) ( ) ( )
cos cos cos
1 1
cos cos cos cos
2 2
cos cos sin
RF RF IM IM LO
RF IF RF LO IM IF IM LO
RF RF IM IM LO
I t x t x t t
x t t x t t
Q t x t x t t
ω α ω β ω
ω α ω ω α ω β ω ω β
ω α ω β ω
= − + −
= − + + − + + + + −
= − + −
Low-side injection
Signal of interest
Image
RF LO LO IM IFω ω ω ω ω− = − =
( )cos cos cos sin sinRF RF RF RF RF RFx t x t x tω α α ω α ω− = +
( )cos cos cos sin sinIM IM IM IM IM IMx t x t x tω β β ω β ω− = +
( ) ( ) ( )
( ) ( ){ } ( )
cos cos sin
1 1
sin sin sin sin
2 2
RF RF IM IM LO
RF IF RF LO IM IF IM
Q t x t x t t
x t t x t
ω α ω β ω
ω α ω ω α ω β ω
= − + −
= − − + + − + + + ( ){ }
( ) ( ) ( ) ( ) ( ) ( )
( ) ( ) ( ) ( )
( ) ( ) ( )
After low-pass filtering
1 1
cos cos , sin sin
2 2
1 1
' cos sin cos cos 2
2 2
1 1
' sin cos sin sin 2
2 2
LO
RF IF IM IF RF IF IM IF
IF IF RF IM IF
IF IF RF IM
t
I t x t x t Q t x t x t
I t I t t Q t t x x t
Q t I t t Q t t x x
ω β
ω α ω β ω α ω β
ω ω α ω β
ω ω α ω
+ −
= − + + = − − + +
= − = + +
= + = + ( )
( ) ( )
After low-pass filtering
1 1
' cos , ' sin
2 2
IF
RF RF
t
I t x Q t x
β
α α
+
= =
Copyright by the authors, all rights reserved
93. Low-IF Receiver
( )2sin 2 LOf tπ
( )2cos 2 LOf tπ
( )2cos 2 LOf tπ
Copyright by the authors, all rights reserved
Benefits Drawbacks
Potential advantages of both heterodyne and
homodyne receivers.
ADC dynamic range
The IF frequency is just one or two channels
bandwith away from DC, which is just enough to
overcome DC offset problems.
Image reject mixer which is implemented in
digital baseband
94. Downlink RF Transceiver Requirement
Base station transmitter
•Transmit antennas / antenna arrays
• 20 – 30 dB antenna gain, horn antennas or phase antenna arrays (64 – 1024 elements)
•Power amplifier
• 20 – 50 dBm, >20% efficiency, EVM < 5% for OFDM waveform
•Packaging
• Integrated solution of antenna array / PA / MMIC / RFIC to minimize transmission loss• Integrated solution of antenna array / PA / MMIC / RFIC to minimize transmission loss
Mobile station receiver
• Receive antenna arrays
• 6 – 18 dB antenna gain, phase antenna arrays (4 – 64 elements)
• Receiver sensitivity < -80dBm
• Total Rx chain Noise Figure < 7dB
• Similar solutions exist today!
• 60GHz CMOS RFIC with phase antenna array (BWRC)
• 60GHz Single-chip integrated antenna and RFIC (GEDC)
• Packaging
• Integrated solution of antenna array / LNA / MMIC / RFIC to minimize transmission loss
94
Copyright by the authors, all rights reserved
95. Uplink RF Transceiver Requirement
Mobile station transmitter
• Transmit antenna arrays
• 6 – 18 dB antenna gain, phase antenna arrays (4 – 64 elements)
• Power amplifier
• 20 – 23 dBm, >20% efficiency, EVM < 5% for 16QAM single-carrier waveform
• Packaging• Packaging
• Integrated solution of antenna array / PA / MMIC / RFIC to minimize transmission loss
• Power consumption on the order of 100mW ~ 1W
Base station receiver
• Receiving antennas / antenna arrays
• 20 – 30 dB antenna gain, horn antennas or phase antenna arrays (64 – 1024 elements)
• Receiver sensitivity < -95 dBm
• Total Rx Noise Figure < 5dB
• Packaging
• Integrated solution of antenna array / PA / MMIC / RFIC to minimize transmission loss
95
Copyright by the authors, all rights reserved
96. Travelling Wave Tube (TWT) Power Amplifier
TWT amplifiers have been extensively used for high power applications at millimeter wave
frequencies
• Provides KWs to MWs power for satellite and radar
• Cost in 10K’s of US$ (too expensive for cellular)
Need to consider solid-state amplifier design for MMB
Copyright by the authors, all rights reserved
97. Solid-state Power Amplifier
Gallium-Nitride based power amplifier
•Wide bandgap materials such as gallium nitride (GaN) or silicon carbide (SiC) have much larger bandgaps
than conventional semiconductors
•Gallium-nitride High Electron Mobility Transistor (GaN HEMT) devices have breakdown voltages 10 times
higher than GaAs HEMT devices, allowing GaN HEMT devices to operate with much higher voltages
97
Source: “Gallium Nitride
(GaN) Microwave
Transistor Technology
For Radar Applications”,
Microwave Journal,
January 2008
98. Solid-state Power Amplifier
State-of-the-art for solid-state mmWave PAs
•11 Watts at 34 GHz (D. C. Streit, et. al., “The future of compound semiconductors for aerospace and
defense applications”, CSIC 2005)
•842 mW at 88 GHz (M. Micovic, et. al., “W-Band GaN MMIC with 842mW output power at 88 GHz”, IMS
2010)
•5.2 Watts at 95 GHz with a 12-way radial-line combiner (James Schellenberg, et. al., “W-Band, 5W solid-
state power amplifier/combiner”, IMS 2010)
98
Source: “Gallium Nitride
(GaN) Microwave
Transistor Technology
For Radar Applications”,
Microwave Journal,
January 2008
99. Cascaded Constructive Wave Amplifier
• Forward wave is amplified as it propagates along the transmission line
• Backward wave is attenuated as it propagates
• Distribution of N cascaded traveling wave stages
• Active devices along the transmission line provide feedback
• Relative phase of transmission line and active device determines amplification/
attenuation.
Source: J. Buckwalter and J. Kim, ISSCC 2009
100. Low-Noise Amplifier [1/2]
Single Stage 60 GHz LNA
Source: Javier Alvarado, PhD thesis, May 2008
Gain 12 dB
Noise Figure 5 dB over 57 – 64 GHz
Power Consumption 4.5mA from a 1.8 V source
1-dB compression point +1.5dBm
Efficiency 17.4%
Process IBM0.12 μm, 200 GHz fT, SiGe technology.
101. Low-Noise Amplifier [2/2]
Two Stage 23–32GHz LNA
Source: El-Nozahi et al,
IEEE JOURNAL OF SOLID-STATE CIRCUITS, FEB 2010
Gain 12 dB
Noise Figure 4.5–6.3dB over 23–32 GHz
Power Consumption 13mW from a 1.5 V source
IP3 -4.5dBm to -6.3dBm [stage1=-2dBm, stage2=7dBm]
Efficiency NA
Process Jazz Semiconductor 0.18 m BiCMOS
1
3, 3,1 3,2
1 1
tot
G
IP IP IP
= +