IoT at Millimeter Wave Frequencies: Finding Hope...2020/01/01 · • Output power increases • PA...
Transcript of IoT at Millimeter Wave Frequencies: Finding Hope...2020/01/01 · • Output power increases • PA...
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© Eridan, 2019
IoT at Millimeter Wave Frequencies: Finding Hope
Earl McCune
CTO, Eridan Communications
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Outline
• What is the problem?
• Why is this the way it is?
• What can be done to improve the situation?
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Wireless Link Operating Objectives
• communication distance
• power efficiency and link efficacy
• bandwidth
• directivity
• penetration of foliage
• penetration of building structures
• environmental conditions
• human safety
• Costs: capital and operational
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Circuit Level
• Linear circuit (PA) efficiency
• Signal bandwidth vs. power draw
• Circuit linearity metric
• Circuit bandwidth (multi-band)
• Ohm’s Law
• Transistor speed (fT)
Key Physics
System Level
• Link Efficacy
• Antenna gain / directivity
• Modulation vs. TX power
• Bandwidth Efficiency (Efficacy)
• Human safety
• Occluded environments
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Inherent conflicts
• Modulation vs. Circuit Efficiency and Link Efficacy
• Communication distance vs. coverage
• Signal bandwidth vs. Power draw
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Circuit Efficiency
• Efficiency applies to any situation where a conservation principle applies- e.g.
• Efficiency improvement is a solved problem below 5 GHz- Though it is not yet widely implemented
• This technology does NOT scale to mmW frequencies
• For the near term, we appear to be doomed……
PDCPIN
POUT
PD
11% Efficiency
DC IN OUT DP P P P+ = +
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0 0.5 1 1.5 2 2.5 3 3.50
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VDS
(V)
Dra
in C
urr
ent
(A)
Incre
asin
g V
GS
Increasing PD
Vk(VGS)
Transmitter Physics• Linear transmitters
cannot be efficient– A direct consequence
of Ohm’s Law
• Efficient transmitters cannot have circuit linearity– Class-E approximates
this profile
• If the amplifier transistor is too slow to follow the paths of efficient operation– Then all of the
techniques developed for efficient operation disappear
– Linear operation still remains (see #1)
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I C(A
)
VCE (V)GaAs HBT
Envelope PDF
Signal envelope
Linear Transmitter Efficient Transmitter
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Why is Efficiency a Special Problem at millimeter wave frequencies?
• mmWave frequencies are much closer to
transistor speed boundaries
Transistor behavior changes at these frequencies
• Output power drops
• Circuit gain is lower
• Compression begins sooner
• Linear operating range shrinks
• 5G-New Radio uses identical modulation schemes
at all frequencies
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103
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fT / f
o
Achie
vable
Eff
icie
ncy (
%)
RL/RON=10
RL/RON=30
RL/RON=100
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0.001 0.01 0.1 1 10 100 1000
Ava
ilab
le G
ain
(d
B)
Frequency (GHz)mmWmW
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Millimeter Wave Power Drop
As frequency increases, the transition times eventually do not settle into ON
and OFF states: slew-rate limiting
• At low frequencies, the transition time is negligibly short and the transistor does switch
• Largest possible sinewave is 2(2/p) times the squarewave magnitude (=1.27x) [+2.1 dB]
• When slew-rate limiting is reached, the largest possible sinewave output is reduced
• Largest possible sinewave is 2(2/p)2
times the squarewave magnitude (=0.81x) [-1.8 dB]
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PA Thermal Management
• Available signal swing range is lower at mmW frequencies• Signal PAPR further reduces output power• More circuit stages are needed to make up total needed gain
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1%
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100%
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TX E
ffic
ien
cy
Signal PAPR (dB)
< 3 GHz
3-6 GHz
mm Wave
2G 2.5G 3G LTE 5G-NR
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Rat
io t
o O
utp
ut
Po
we
r
Circuit Energy Efficiency
Power Supply Size
Heatsink Size
5G-NR Sub-6
5G-NR mmWave
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I C(A
)
VCE (V)GaAs HBT
High Frequency
Low Frequency Cu & Fe
Al
( ) 20010dBPAPR
dBPAPR
− =
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Defining Amplifier Linear Range
P1dB is a poor definition of amplifier linearity range
Linearity = constant gain, independent of input value
Gain is constant only when S = dPOUT/dPIN = 1.00 dB/dB
Gain expansion when S > 1
Gain compression when S < 1
Nonlinear gain is distorting to the waveform
Linearity: gain must be independent of the input voltage
Proposal:
Amplifier linearity is defined when S = 1.00 within an error
band equal to the allowed distortion
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Gai
n (
linea
r)
Input Voltage (Vrms)
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0.0001 0.001 0.01 0.1
Gai
n (
linea
r)
Input Voltage (Vrms)
S=1.2
S=1.1
S=1.0S=0.9S=0.8
S=1.2S=1.1S=1.0S=0.9S=0.8
± x%S=1.0
( )1
,
0
0
S
out rms in
in
V Vgain S g
V V
−
= =
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Practical Linear PA: Range and Efficiency
5G-NR EVM spec is -30 dB
Corresponds to 3.3% distortion
Here, this distortion limit is well below P1dB
Sets the upper limit of signal output power (PEP)
Output backoff (OBO) = PSAT - PEP
Also sets the peak linear efficiency
Here 0 = 5% at the top of the linear range
Design goal: maximize the range of S = 1
only needs the POUT(PIN) curve
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Ou
tput
Pow
er (
dB
m);
Rati
omet
ric
Pow
er G
ain
(dB
); P
AE
(%)
Input Power (dBm)
Output Power (dBm)
Peak PAE
Ratiometric Power Gain
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Slo
pe
Po
wer
(d
B/d
B)
Input Power (dBm)
± 3%
P1dB
Linearrange
PSAT
PEP PSATOBO
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Add Modulation
0%
1%
2%
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6%
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PA E
ffic
ien
cy
Signal PAPR (dB)
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Ou
tput
Pow
er (
dB
m);
Rati
omet
ric
Pow
er G
ain
(dB
); P
AE
(%)
Input Power (dBm)
Output Power (dBm)
Peak PAE
Ratiometric Power Gain
PAPR
PTX
PEP
• The linearity upper limit applies to the modulated
signal upper limit: Peak Envelope Power (PEP)
• Signal average power is lower than PEP by the
modulation PAPR
• Efficiency drops further
• Signal envelope statistics have a major influence
on the final result
• The efficiency upper bound is known
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Why are we bothering with mmWaves?
Following the mantra
‘data rates must go higher’
Shannon showed that bandwidth efficiency is
constrained by link SNR
With a maximum link SNR
bps/Hz is upper bounded
More bps then requires more Hz bandwidth: mmW
2log 1 ; 0 1S
N
PR C UU
B B P
= +
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An
ten
na
Be
amw
idth
(de
gre
es)
Antenna Aperture (wavelengths)
Path Loss Issues
Actual LOS path loss is independent
of frequency
TX forms a EM field density (mW/m2)
What changes with frequency is the
RX antenna behavior
Scales with wavelength
mmW wavelength l is much shorter
Larger area antennas must be
directive:
( )21
, ,4 4
R T T T RpP d P P G G
d
ll
p p
=
RX Antenna
TX
Antenna
LOS
path-loss
rms signal power
into the channel
TX
RX
lPTGT PR
GR
d
p
T
PEPP
PAPR=
$$$
directivity
≥ 2
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Efficacy
• Has units (e.g. lumens/watt for lighting, bits per joule for digital
communication)
• Determines how effective a process is when using one resource
to provide another: result/resource
Power (watts) in
Energy (joules) in
Light (lumens) out
Data transfer
(bits) out
Digital CommunicationElectric lighting
bits/joulelumens/watt
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Link Efficacy
• Unit arithmetic relates the desired efficacy to its comprising link parameters
▪ These parameters are NOTindependent from each other
• Complete efficacy model includes all link parameters: signal, hardware, environment, and physics
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sec
EE
symbbb sym
JJ Watts
= = ( ),
220
02
10 10
10log
4( ) 10 10
dB
d dBdB
PAPR
p
EE sym T RSNRNFN M f G G d
kTB
l
p
−
−
=
( )2
1 cos360
RG p
=
−
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Link Efficacy
• Unit arithmetic relates the desired efficacy to its comprising link parameters
▪ These parameters are NOTindependent from each other
• Complete efficacy model includes all link parameters: signal, hardware, environment, and physics
secsec
sec
EE
symbbb sym
JJ Watts
= =
2log ;b N M
sym=
2
bsymM =
OUTDC
PP
=
fsym
( ),
220
02
10 10
10log
4( ) 10 10
dB
d dBdB
PAPR
p
EE sym T RSNRNFN M f G G d
kTB
l
p
−
−
=
1E-16
1E-14
1E-12
1E-10
1E-08
1E-06
0.0001
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QA
M B
it-e
rro
r R
ate
(B
ER
)SNR (dB)
4 QAM 16 QAM 64 QAM 256 QAM
10b/sym 12b/sym 14b/sym 16b/sym
18b/sym 20b/sym 22b/sym 24b/sym
0 0
S b b bd BW
N
P E f Esnr
P N B N= = =
0.01
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1000000
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Ene
rgy
Effi
cacy
(b/J
) ; T
X P
ow
er
(W)
Propagation Constant
b/J, 750 MHz
b/J, 1900 MHz
b/J, 3600 MHz
TX Power, 3600 MHz
TX Power, 1900 MHz
TX Power, 750 MHz
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1000000
10000000
100000000
1E+09
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Ene
rgy
Effi
cacy
(b/J
) ; T
X P
ow
er
(W)
Distance (m)
b/J, 750 MHz
b/J, 1900 MHz
b/J, 3600 MHz
TX Power, 3600 MHz
TX Power, 1900 MHz
TX Power, 750 MHz
p = 3.1
d = 1000m
LOS reflection
penetration
occlusion
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Antenna Gain and Directivity
Signal power density: mW/cm2
More mW into the RX requires more antenna area (cm2)Independent of frequency!
Directivity (beamwidth) narrows as antenna size increasesMeasured in wavelengthsCorresponds to antenna “gain”Antenna must be aimed
Related by the Fourier Transform“Time domain” – Antenna aperture in wavelengths“Frequency domain” – Antenna directivity in radians
Directivity (gain) and coverage are in opposition
( ) ( )2
,
1 cos360
T RG G p
=
−
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An
ten
na
Gai
n G
A(d
B)
Antenna Beamwidth (degrees)
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Align Modulation to mmW Circuit Capabilities
• OFDM (3GPP 5G-NR)- requires circuit linearity
(output backoff)
- and has a large PAPR (~7-10 dB)
• pPSK- PAPR = 0dB
- No linearity required
• Output power increases
• PA efficiency increases 10-fold (or more)
• OpEx decreases by 10x
• Large decrease in power supply and heatsink sizes
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Ou
tput
Pow
er (
dB
m);
Rati
omet
ric
Pow
er G
ain
(dB
); P
AE
(%)
Input Power (dBm)
Output Power (dBm)
Peak PAE
Ratiometric Power Gain
PAPR
PTX PEP PSAT
rms 1.000 [+2.5 dB]spacing 0.390 [-1.6 dB]
16-PSK
Output backoff
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Rat
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utp
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Circuit Energy Efficiency
Power Supply Size
Heatsink Size
pPSK
OFDM
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mmW Safety – Human RF Exposure
IEEE-C95.1 calls for power density of 1 mW/cm2 as an upper limit when there is unrestricted
antenna access (e.g. a mobile device)
Published unit is often EIRP
Beamwidth contributions, more involved calculation
… are any present mmW handset products safe??
# o
f el
emen
ts p
er a
rray
sid
e
# o
f el
emen
ts p
er a
rray
sid
e
Total TX EIRP (far field)Total TX Power
4 antennas (2x2), 4 dBm each
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Conclusions
• Dominant contributors to extremely low mmW efficiency
• Requirement for circuit linearity
• Signal PAPR greatly exceeding 3 dB
• mmW transistor operation is never as good as at sub-6 frequencies
• Transistor improvements will likely take a decade
• High efficiency modes familiar at sub-6 are not available (yet)
• Fast improvements require changing the mmW signal modulation
• One option is to adopt circular constellations
• Increases the useful output power from any existing PA
• Circuit linearity is not needed (recover the backoff)
• PAPR is 0 dB (recover PAPR power loss)
• Efficiency improves by at least 15x
• Network coverage improves dramatically
• No compromise on baseline bandwidth efficiency
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Summary
There is hope!
But…
• Transistors today are not fast enough to access traditional
high-efficiency behaviors at mmWave frequencies
• Adopting a constant envelope signal with good bandwidth
efficiency (e.g. 16-pPSK) is doable now
• Will recover most of the efficiency loss
• Will greatly expand network coverage
• Requires action from 3GPP
• Operators can demand the performance they really need from
their suppliers – and from 3GPP