IoT at Millimeter Wave Frequencies: Finding Hope...2020/01/01  · • Output power increases • PA...

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1 © Eridan, 2019 IoT at Millimeter Wave Frequencies: Finding Hope Earl McCune CTO, Eridan Communications

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

    0.2

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    1

    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

    -10

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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]

    -1.5

    -1

    -0.5

    0

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    1

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    -1

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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

    0%

    1%

    10%

    100%

    0 2 4 6 8 10 12 14 16 18

    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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    0% 10% 20% 30% 40%

    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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    0.01

    0.015

    0.02

    0.025

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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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    0 0.01 0.02 0.03 0.04

    Gai

    n (

    linea

    r)

    Input Voltage (Vrms)

    1

    10

    100

    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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    4%

    5%

    6%

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    PA E

    ffic

    ien

    cy

    Signal PAPR (dB)

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    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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    0.1

    1

    10

    100

    1000

    0.1 1 10 100

    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

    secsec

    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

    0.01

    1

    0 10 20 30 40 50 60 70 80 90

    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

    0.1

    1

    10

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    1000000

    2 2.5 3 3.5 4

    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

    0.001

    0.01

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    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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    0.1 1 10 100

    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

    0

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    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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    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