john l. schadler continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“...

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Page 1: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21
Page 2: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

โ€œAntenna Technology For ATSC 3.0 โ€“ Boosting the Signal Strengthโ€

Continuation

John L. Schadler

Page 3: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

4KUHDTV

โ€ข

โ€ข

โ€ข

โ€ข

Page 4: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

Outdoor reception of the Bootstrap signal

.25 Mbit Deep indoor mobile to small handheld receiver

48 dBu

95 dBu

Page 5: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

Effect of heavy beam tilt Effect of heavy null fill

Addition of SFNs

Page 6: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

Most effective way to design for service and provide even distribution of high signal strength โ€“ High null fill + SFNs

โ€ข Saturate in the vicinity of the main antenna by increasing the null fill

โ€ข Add SFN sites around coverage perimeter to boost the signal strength outside of the high null fill area

+ SFN

Page 7: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

โ€ข ATSC 3.0 MISO scheme โ€“ TDCFSโ€ข Transmitting two uncorrelated signals to a single receiverโ€ข Cost effective

โ€ข Increase the complexity of the transmitter โ€“ not the receiverโ€ข ATSC 3.0 SFN sites will serve many receivers

โ€ข Economical to add equipment cost at the transmit site rather than the receiver

โ€ข Receiver remains small and affordable

Page 8: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

โ€ข TDCFS can be deployed in either a co-located or distributed configuration

โ€ข Does not require any new RF equipment within the existing SFN

Co-located Distributed

โ€ข Diversity gain throughout the coverage area

Page 9: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

Diversity gain Boosting the RSSโ‰ก

Max diversity gain is based on the total number of independent signal paths

M transmit antennas N receive antennas

1 โ‰ค ๐บ๐‘‘ โ‰ค ๐บ๐‘š๐‘Ž๐‘ฅ = ๐‘€ โˆ— ๐‘

3 dB improvement in RSS can be achieved when 2 x 1 MISO diversity is applied

Page 10: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

โ€ข Traditionallyโ€ข Spatial diversity

โ€ข Separate antennasโ€ข Difficult to implement

โ€ข Space limitationsโ€ข Polarization diversity

โ€ข Co-located antenna elementsโ€ข Orthogonal polarizationsโ€ข Modes of operation

โ€ข Slant linearโ€ข RH / LH CP

Which mode of polarization diversity operation is best for ATSC 3.0 MISO?

Dual input broadcast antenna array

X

Page 11: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

โ€ข Max diversity gain depends on spreading the power evenly between the polarizationsโ€ข Figure of merit

โ€ข Cross Polarization Discrimination (XPD)โ€ข The ratio between the available power in the vertical and horizontal polarizations

๐‘‹๐‘ƒ๐ท =๐‘…๐‘ฃ

2

๐‘…โ„Ž2 For optimal diversity gain XPD=0dB

Compare the static response XPD for slant linear and RH/LH CP

Page 12: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

Pair of orthogonal crossed dipoles oriented in space by a tilt angle ฮฑ

Dipole modeling Channel modeling

Four channel links between the transmitter and receiver

๐‘…โ„Ž๐‘…๐‘ฃ

=ฮ“11๐‘’

๐‘—๐œ™11 ฮ“12๐‘’๐‘—๐œ™12

ฮ“21๐‘’๐‘—๐œ™21 ฮ“22๐‘’

๐‘—๐œ™22

๐‘‰โ„Ž๐‘‰๐‘ฃ

๐‘‰โ„Ž๐‘‰๐‘ฃ

=๐‘ ๐‘–๐‘›๐›ผ โˆ’๐‘๐‘œ๐‘ ๐›ผ๐‘๐‘œ๐‘ ๐›ผ ๐‘ ๐‘–๐‘›๐›ผ

๐‘‰1๐‘‰2๐‘’

โˆ’๐‘—๐œƒ

ฮ“ โ€“ random variable used to model the multipath fading

ฮฆ- random phase introduced by the channel

Page 13: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

๐‘‹๐‘ƒ๐ท =

๐‘‰12 ฮ“21

2๐‘ ๐‘–๐‘›2๐›ผ + ฮ“222๐‘๐‘œ๐‘ 2๐›ผ + 2ฮ“21ฮ“22๐‘ ๐‘–๐‘›๐›ผ๐‘๐‘œ๐‘ ๐›ผ๐‘๐‘œ๐‘  ๐œ™21 โˆ’ ๐œ™22 + ๐‘‰2

2 ฮ“222๐‘ ๐‘–๐‘›2๐›ผ + ฮ“21

2๐‘๐‘œ๐‘ 2๐›ผ + 2ฮ“21ฮ“22๐‘ ๐‘–๐‘›๐›ผ๐‘๐‘œ๐‘ ๐›ผ๐‘๐‘œ๐‘  ๐œ™21 โˆ’ ๐œ™22

+2๐‘‰1๐‘‰2๐‘๐‘œ๐‘ ๐œƒ ฮ“21ฮ“22 ๐‘ ๐‘–๐‘›2๐›ผ โˆ’ ๐‘๐‘œ๐‘ 2๐›ผ ๐‘๐‘œ๐‘  ๐œ™21 โˆ’ ๐œ™22 + ฮ“222 โˆ’ ฮ“21

2 ๐‘ ๐‘–๐‘›๐›ผ๐‘๐‘œ๐‘ ๐›ผ

๐‘‰12 ฮ“11

2๐‘ ๐‘–๐‘›2๐›ผ + ฮ“122๐‘๐‘œ๐‘ 2๐›ผ + 2ฮ“11ฮ“12๐‘ ๐‘–๐‘›๐›ผ๐‘๐‘œ๐‘ ๐›ผ๐‘๐‘œ๐‘  ๐œ™11 โˆ’ ๐œ™12 + ๐‘‰2

2 ฮ“122๐‘ ๐‘–๐‘›2๐›ผ + ฮ“11

2๐‘๐‘œ๐‘ 2๐›ผ + 2ฮ“11ฮ“12๐‘ ๐‘–๐‘›๐›ผ๐‘๐‘œ๐‘ ๐›ผ๐‘๐‘œ๐‘  ๐œ™11 โˆ’ ๐œ™12

+2๐‘‰1๐‘‰2๐‘๐‘œ๐‘ ๐œƒ ฮ“11ฮ“12 ๐‘ ๐‘–๐‘›2๐›ผ โˆ’ ๐‘๐‘œ๐‘ 2๐›ผ ๐‘๐‘œ๐‘  ๐œ™11 โˆ’ ๐œ™12 + ฮ“122 โˆ’ ฮ“11

2 ๐‘ ๐‘–๐‘›๐›ผ๐‘๐‘œ๐‘ ๐›ผ

The definition yields ๐‘‹๐‘ƒ๐ท =๐‘…๐‘ฃ

2

๐‘…โ„Ž2=๐ด ฮ“21

2 + ๐ต ฮ“222

๐ด ฮ“112 + ๐ต ฮ“12

2

๐ด = ๐‘‰12๐‘ ๐‘–๐‘›2๐›ผ + ๐‘‰2

2๐‘๐‘œ๐‘ 2๐›ผ โˆ’ 2๐‘‰1๐‘‰2๐‘ ๐‘–๐‘›๐›ผ๐‘๐‘œ๐‘ ๐›ผ๐‘๐‘œ๐‘ ๐œƒ

๐ต = ๐‘‰12๐‘๐‘œ๐‘ 2๐›ผ + ๐‘‰2

2๐‘ ๐‘–๐‘›2๐›ผ + 2๐‘‰1๐‘‰2๐‘ ๐‘–๐‘›๐›ผ๐‘๐‘œ๐‘ ๐›ผ๐‘๐‘œ๐‘ ๐œƒwhere

The different types of polarization diversity can be described by the coefficients A and B

Page 14: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

Since the A and B coefficients are the same in all 6 cases, the equations that describe the XPD are identical in all 6 cases

Slant linear and circularly polarized antennas transmit the same average performance in a static MISO system. The expected diversity gain of SL / SR linear and RH / LH CP are on average the same.

Page 15: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

โ€ข Analysis assumesโ€ข For CP we increased the transmitter power 3dB to maintain the same ERPโ€ข The receiver is stationaryโ€ข Independent of any margin improvement observed by transmitting CP to a

linearly polarized receive antenna in motion

Page 16: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

๐‘€๐ผ = ๐‘†๐‘๐‘…๐‘๐‘ โˆ’ ๐‘†๐‘๐‘…๐‘™๐‘–๐‘›๐‘’๐‘Ž๐‘Ÿ

Page 17: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

Starting over a decade ago โ€“ extensive testing to quantify the benefit of transmitting CP to a linearly polarized receiver in motion

โ€ข Controlled environmentsโ€ข Field tests in ME and FLโ€ข Indoor / Outdoor / Vehicleโ€ข Measurements based on RSS

and BERโ€ข Different amounts of VPOL

Page 18: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

All measurements have confirmed that transmitting circular polarization to a linearly polarized receiver in motion in a heavy scatter environment provides 5 to 7 dB of margin improvement (MI) over transmitting a linearly polarized signal to the same receiver.

Page 19: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

โ€ข Gd and MI are independentโ€ข 5-7dB MI is observed when transmitting a single CP signal to a linear

receiver in motionโ€ข Adding a second independent path (MISO) does not change this but

adds 3dB of Gd

The total system gain of dual RH / LH CP MSIO diversity system transmitting to a linearly polarized mobile receiver in motion in a heavy scatter environment is as high as 8-10dB.

Page 20: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

โ€ข A new antenna specification to considerโ€ข So far we have assumed the transmit signals are completely uncorrelatedโ€ข Imperfect antennas couple energy

SR/SL Linear RH/LH circular

๐ผ = ๐‘“ ๐‘๐‘Ÿ๐‘œ๐‘ ๐‘  ๐‘๐‘œ๐‘™๐‘Ž๐‘Ÿ๐‘–๐‘ง๐‘Ž๐‘ก๐‘–๐‘œ๐‘› ๐ผ = ๐‘“ ๐‘Ž๐‘ฅ๐‘–๐‘Ž๐‘™ ๐‘Ÿ๐‘Ž๐‘ก๐‘–๐‘œ

โ€ข Studies : 17 dB of cross pol isolation is sufficient to reach 99% of desired data rate

All waves can be decomposed into two components with orthogonal polarization states

Page 21: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

๐ผ = 10๐‘™๐‘œ๐‘”

12 +

๐ด๐‘…๐ด๐‘…2 + 1

12

1

๐ด๐‘… + 1๐ด๐‘… โˆ’ 1

2 + 1 +๐ด๐‘…

๐ด๐‘…2 + 11

๐ด๐‘… + 1๐ด๐‘… โˆ’ 1

2 โˆ’ 1

SpecificationAR<1.7dB for RH/LH CP MISO

Page 22: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

โ€ข Employing MISO diversity gain can add up to 3 dB in the system gainโ€ข On average slant linear and circularly polarized antennas transmit the same

average performance in a stationary MISO diversity systemโ€ข This is independent of any margin improvement observed by transmitting CP to

a linearly polarized receive antenna in motionโ€ข Transmitting CP to a linearly polarized receiver in motion in a heavy scatter

environment can add 5 to 7 dB of margin improvementโ€ข Total ATSC 3.0 system gains employing RH/LH CP diversity can be 8 to 10dB if

you choose to increase your TPO by 3dB.โ€ข The axial ratio specification of a RH / LH co-located system considered for

diversity should be < 1.7dB.

* The use of LH CP will require an FCC rule change

Page 23: John L. Schadler Continuationโ‚ฌยฆย ยท ๐‘‹๐‘ƒ๐ท= ๐‘‰1 2ฮ“ 21 2 ๐‘– 2๐›ผ+ฮ“ 22 2๐‘ 2๐›ผ+2ฮ“ 21ฮ“22 ๐‘– ๐›ผ๐‘ ๐›ผ๐‘ ๐œ™21โˆ’๐œ™22 +๐‘‰2 2ฮ“ 22 2 ๐‘– 2๐›ผ+ฮ“ 21

Come visit us at Booth # C2613