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1
Terabit DSLsNSF Workshop – July 12, 2018
NYU, Brooklyn
John CioffiProfessor Emeritus, Stanford EE
& CEO/COB ASSIA Inc.ASSIA: K. Kerpez, C. Hwang, I. Kanellakopoulos
2
xDSL Migration
26 km 4 km 2 km 1 km 500 m 300 m 100 m 30 m
10M
100M
1G
10G
100 G
1T
10T
Speed(bps)
=X - base-T(4 pairs)
4Tbase-T
40Tbase-T
4-bonded100 - 1000improvement
=x - DSW(1 pair)
T
100G
10G
10T
A A2A2+
VVec
FastFast2
MGFast
=X – DSL(1 pair)
10Gbase-T
3
▪ Fiber to the home average cost is $3000/home• No viable return on such investment for telcos
• Only deploy fiber in “cherry picked” regions• Still losing money on even that investment
▪ Fiber part way leaves cost ($100k - $1M/mile) shared over all subtended homes • Has better return on investment ($300/home)
▪ Could copper enable 5G wireless?• Outside “backhaul” needs high-speed to many many more small cell sites
Simplified Business Case
4
▪ Many and yet more smaller cells• 3.5, 28-30, 60-70 GHz
• 1 Gbps to 10 Gbps wireless access speeds
▪ Front/back-haul support of 5G Massive MIMO (vectoring for wireless)
5G small-cell infrastructure costs
4
Every “street lamp” (drop point)10 Gbps? Maybe more
Fiber ?
Or copper ?
• Deutsche Telekom CTO and CEO (MWC 2017)
– “5G fiber infrastructure cost is 300~500 BILLION € for Europe” (~ 100M cells –say 4000 €/ cell)
• Copper could be 10% of this cost (latency is few micro-second range)
5
Virtualization “CORD” & Data Center (DC)
Need for BandwidthVirtualization Server Consolidation
Virtualization fuels DC connection demand for Terabits
Match all 10G/100G baseFiber speeds on copper
10-40TBaseTPossible?
RemainsFiber on long haul
Main Copper Ethernet cost advantage = flexibility
$18BAnnual
Connectormarket
6
▪ Orders of magnitude speed increase for copper, helps:• wireless (5G)
• virtualization (data-center)
• Fiber = xTTH (residential) budgets
▪ Allows rethinking• Technical
• Financial (infrastructure capex)
Combine 2 known methods
6
Digital
Subscriber
Waveguide
Waveguides
Plasmon
Polariton
Vectoring
(massive
MIMO)
Sub mm WaveTransmission
(5G, 6G)
G.Fast/vecWi-Fi, LTE
7
The Waveguide Propagation Modes
8
r = 0.5 mm
rcopper = 0.25 mm
plastic insulator
copper wire
Air cores of waveguide
MIMOProcessor
Cross Section of a cable of twisted-pair wires
▪ Green areas (and blue) • Waves are guided• Current is not “in copper”• Copper guides the “wireless” waves• Wavelength < 0.5 mm
▪ Twisting causes• “Swiss Cheese” waveguides• Reflections• Many modes of possible propagation
▪ It’s a MIMO wireless challenge• Which is the same as a vectored DSL • Already proven in use
9
Surface Wave Transmission (1909 Sommerfeld wave)
• Surface Mode (or TM10)
– Waves use single wire in TM mode as guide
• E.g. Goubau antenna or “G-line”
• See also AT&T “AirGig”
– Effectively wireless transmission
• Works reasonably well (no atmosphere inside cable)
• Dielectric (plastic) can help (see [Wiltse]), p. 971) or hurt
– Energy still leaks off wire if bent
• Two twisted wires (or even split pairs)– Tends to hold energy to the pair (any pair) better
– TEM Plasmon Polariton mode (per wire to surrounding wires)Mathfaculty.com
SWEnergy
10
▪ Single wire TM01• Wiltse’s surface-wave measurements are 2mm wire core, not 0.5mm)• Measures attenuation/m
▪ Wiltse Extrapolation• .8 dB/m @ .1-.3 THz• Fatter wires
▪ Grischkowsky has .5 dB/m• For .52mm diameter Cu wire• 2nd wire would probably improve transfer• Like in twisted pair
▪ 100m should see 50-80 dB
▪ Bending is less of a problem• Each wire has a TM mode• Between wires is a TEM plasmon polariton mode• 2nd TEM “plasmonic” (weaker?) to other pairs – somewhat like
phantoms/split-pairs• TIR mode• Surface mode (maybe same as TM …)• 3 -- 4 modes per pair
Waveguide Measurements 2006
Wiltse
Grischkowsky
11
▪ Senses THz energy (as well as emits)
▪ Can be constructed (in arrays) in semiconductor• Uses also 3D circuit board (3D printer)
Single sensor/antenna basics
Courtesy, Prof A. Arbabian, Stanford
12
Vectoring = Massive MIMO
• Multiple modes for each wire– TM mode (“surface”) – TEM plasmon polariton mode– TIR modes (total internal reflection)
• “Swiss Cheese” Waveguide – ULTRA rich scattering (exactly what massive MIMO needs)
PhotoDetector
PhotoDetector
PhotoDetector
PhotoDetector
PhotoDetector
PhotoDetector
May not be ableto coordinate
on this side(as in DSL vectoring)
H
13
The Signal Processing
14
▪ 5G or Ethernet (singular value decomp)• xmit = M ; rcvr =F*
MIMO Channel – H
H = FLM*
H =RQ*
H =QR
Order of users will become important
• Downstream DSL (right QR decomp)
– xmit = Q ; small receiver (NLP =R*)
• Upstream DSL (left QR decomp)
– small xmit ; rcvr = Q* (DFE =R)
15
H (MIMO Channel) Model
▪ Channel (Grischkowsky)
▪ Xtalk (this paper)• Log normal
▪ 20 dBm total transmit power, flat transmit PSD
▪ 4096 subcarriers from 100 GHz to 300 GHz, 48.8 MHz subcarrier spacing• Bit loading from 1 to 12 bits/Hz• 10% phy-layer overhead removed before presenting results• 4.5 dB coding gain, 1.5 dB implementation loss• Carriers from 50 GHz to 150 GHz were used for the 10 Gbps results• Plasmonic TEM and TM1 modes are used for each wire• Extended to 8192 carriers below 100 meters (so up to 500 GHz)
▪ 50 pairs, vector precoded with either zero-forcing linear precoder or Non-Linear Precoder (NLP) using Generalized Decision Feedback Equalization (GDFE); ideal channel estimation assumed.
▪ -160 dBm/Hz background AWGN.
Mean k=0 dBVar = 6 dB
16
0
2
4
6
8
10
12
14
16
18
10
20
30
40
50
60
70
80
90
10
0
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0
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20
0
Dat
a R
ate
(Tb
ps)
per
Ho
me
Loop Length (m)
100-500 GHz TDSL, per Home data rates
NLP
Linear precoded
Results in Tbps [down+up]/pair
7/13/2018
1 Tbps at 100m
▪ Can any PON get 1 Tbps to each customer?
17
Waveguides: Longer Range, Lower Speed?
100 Gbps > 300m
10 Gbps > 500m(~0.5km)
0
0.5
1
1.5
2
2.5
3
10 30 50 70 90 110 130 150 170 190 210 230 250 270 290 310 330
Dat
a R
ate
(Tb
ps)
pe
r H
om
e
Loop Length (m)
60-120 GHz TDSL, per Home data rates
NLP
Linearprecoded
Repeated from last year
Note the Nonlinear Precoder(NLP) gains – this is important
18
Very-high speed TDSL
• Adding Plasmonic TM2 and TEM2 modes from 100-500 GHz on each wire
100 meters 300 meters 500 meters
2 Tbps 100 Gbps 10 Gbps
2 Tbps @100 m
0
2
4
6
8
10
12
14
16
18
20
10
20
30
40
50
60
70
80
90
10
0
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12
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0
17
0
18
0
19
0
20
0
Dat
a R
ate
(Tb
ps)
per
Ho
me
Loop Length (m)
100-500 GHz TDSL, per Home data rates
NLP
Linear precoded
19
Very long range Waveguide - squeezes low-end of band
19
0
0.5
1
1.5
2
2.5
3
3.5
4
4.5
5
600 610 620 630 640 650 660 670 680 690 700 710 720 730 740 750 760 770 780 790 800
Dat
a R
ate
(Gb
ps)
per
ho
me
Loop Length (m)
50-150 GHz TDSL, per Home data rates
1 Gbps at roughly 2100 feet (symmetric) or 640m
20
RF over Copper
To Network
Copper binder cable @ 300GHz
RF cable @ 28 GHz
Analog transceiver for copper DAS transceiver for 28GHz
StreetCabinet
DAS antenna
Analog modulator for Copper
Power over copper
• RF over copper is similar to RF over fiber– In addition, power can be sent over copper.
• Copper waveguide mode will provide another rich scattering environment. – A cascade of two rich scattering matrices.
21
Signal Processing
• Conversion devices– Fortunately fiber designers have developed ADC’s and DACs
• 8-bit 65 GHz ADC today (fiber –used in 100-400 Gbps fiber) uses 750 mW (might need 4 for 250 GHz, and maybe 2 per wire), so 6-10 Watts
– 17 nm semiconductors (less in 7 nm?)
• Power-cost/bit is probably ok and much less than current ethernet
• Processing Capabilities– Vector Engine, even at per tone of 50 MHz
– 5 Giga-ops per tone roughly (on cancellation side in vectoring)
– 20 Tera-ops today (4000 tones) is about 10 Watts/line
• Watts/bit is probably ok and much less than current ethernet
– Start at 100 Gbps instead (1/10 the cost and power)?
• Recall early stage ADSL and VDSL started in similar ranges
22
Call for Early Lab Measurements
▪ Single excitation• Measure all output sensors• Photoconductive excitation and photo detectors
• Expensive but accurate
▪ Start with shorter cables• A 1m cable. (To test TM/TEM mode.)• Stepper positioning of transmitter and receiver• Collection of outputs at different frequencies and positions (H)• Use of periodic training sequences• Store on disk• MIMO signal processing can then occur
▪ Progress to longer cables• 100 m• Different configurations
▪ Investigate cost-effective mass-producible couplers
23
▪ Terabit/s per pair appears possible• Pre-competitive cooperation necessary for better
• Measures
• Consequent calculations and projections
▪ Early focus may be narrower band• 10 Gbps at 100’s of meters
• 5G wireless small cells “back/front” haul
• Data centers
▪ Needs early funding and personnel
Conclusions
7/13/2018
24
Essential to Reliably Fast Connectivity
www.assia-inc.com
Thank YouEnd of Presentation
25
Example Architecture
FFT (IFFT)&
AssociatedDSP
LINE
I/O
8Wires
Cat-”T”
100 GHz
200 GHz
300 GHz
400 GHz
500 GHz
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CFP4
4xCFP4
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4xCFP4
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CFP4
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CAUI-425G each
100GRouter/E switch
400GRouter/E switch
400GRouter/E switch
100GRouter/E switch
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Datacenter
Each band could be viewed as equivalent to “wavelength” in fiber architectures
26
Ethernet Results
• Uses Plasmonic TEM & TEM2, and TM1 and TM2 modes from 100-500 GHz on each of 8 wires
27
▪ Profs. Joe Kahn, L. Kazovsky, A. Arbabian, Stanford U.
▪ Dr. Ricky Ho, Apple
▪ Dr. S. Galli, Huawei
▪ Prof. D. Mittleman, Brown U.
▪ Dr. N. Swenson (Collinear)
▪ T. Cil (ASSIA)
▪ J.C. Wiltse, “Surface-Wave Propagation on a Single Metal Wire or Rod at Millimeter-Wave and Terahertz Frequencies,” Microwave Symposium Digest, 2006. IEEE MTT-S International, 11-16 June 2006.
▪ R.E. Collin, “Hertzian Dipole Radiating Over a Lossy Earth or Sea: Some Early and Late 20 th-Century Controversies” IEEE Ant and Prp. Magazine, Vol 46, No. 2, April 2004.
▪ T.I.Jeon, J. Zhang, and D. Grischkowsky, “THz Sommerfeld wave propagation on a single metal wire,” Appl. Phys. Letters, Vol 86, 2005.
Acknowledgements and Refs
28
Back Up - Electronics in the Terahertz Band