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John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

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Page 1: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21
Page 2: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

“Antenna Technology For ATSC 3.0 – Boosting the Signal Strength”

Continuation

John L. Schadler

Page 3: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

4KUHDTV

Page 4: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 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 Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

Effect of heavy beam tilt Effect of heavy null fill

Addition of SFNs

Page 6: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

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

• Saturate in the vicinity of the main antenna by increasing the null fill

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

+ SFN

Page 7: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

• ATSC 3.0 MISO scheme – TDCFS• Transmitting two uncorrelated signals to a single receiver• Cost effective

• Increase the complexity of the transmitter – not the receiver• ATSC 3.0 SFN sites will serve many receivers

• Economical to add equipment cost at the transmit site rather than the receiver

• Receiver remains small and affordable

Page 8: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

• TDCFS can be deployed in either a co-located or distributed configuration

• Does not require any new RF equipment within the existing SFN

Co-located Distributed

• Diversity gain throughout the coverage area

Page 9: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

Diversity gain Boosting the RSS≡

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

M transmit antennas N receive antennas

1 ≤ 𝐺𝑑 ≤ 𝐺𝑚𝑎𝑥 = 𝑀 ∗ 𝑁

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

Page 10: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

• Traditionally• Spatial diversity

• Separate antennas• Difficult to implement

• Space limitations• Polarization diversity

• Co-located antenna elements• Orthogonal polarizations• Modes of operation

• Slant linear• 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 Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

• Max diversity gain depends on spreading the power evenly between the polarizations• Figure of merit

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

𝑋𝑃𝐷 =𝑅𝑣

2

𝑅ℎ2 For optimal diversity gain XPD=0dB

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

Page 12: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

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

Dipole modeling Channel modeling

Four channel links between the transmitter and receiver

𝑅ℎ𝑅𝑣

=Γ11𝑒

𝑗𝜙11 Γ12𝑒𝑗𝜙12

Γ21𝑒𝑗𝜙21 Γ22𝑒

𝑗𝜙22

𝑉ℎ𝑉𝑣

𝑉ℎ𝑉𝑣

=𝑠𝑖𝑛𝛼 −𝑐𝑜𝑠𝛼𝑐𝑜𝑠𝛼 𝑠𝑖𝑛𝛼

𝑉1𝑉2𝑒

−𝑗𝜃

Γ – random variable used to model the multipath fading

Φ- random phase introduced by the channel

Page 13: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

𝑋𝑃𝐷 =

𝑉12 Γ21

2𝑠𝑖𝑛2𝛼 + Γ222𝑐𝑜𝑠2𝛼 + 2Γ21Γ22𝑠𝑖𝑛𝛼𝑐𝑜𝑠𝛼𝑐𝑜𝑠 𝜙21 − 𝜙22 + 𝑉2

2 Γ222𝑠𝑖𝑛2𝛼 + Γ21

2𝑐𝑜𝑠2𝛼 + 2Γ21Γ22𝑠𝑖𝑛𝛼𝑐𝑜𝑠𝛼𝑐𝑜𝑠 𝜙21 − 𝜙22

+2𝑉1𝑉2𝑐𝑜𝑠𝜃 Γ21Γ22 𝑠𝑖𝑛2𝛼 − 𝑐𝑜𝑠2𝛼 𝑐𝑜𝑠 𝜙21 − 𝜙22 + Γ222 − Γ21

2 𝑠𝑖𝑛𝛼𝑐𝑜𝑠𝛼

𝑉12 Γ11

2𝑠𝑖𝑛2𝛼 + Γ122𝑐𝑜𝑠2𝛼 + 2Γ11Γ12𝑠𝑖𝑛𝛼𝑐𝑜𝑠𝛼𝑐𝑜𝑠 𝜙11 − 𝜙12 + 𝑉2

2 Γ122𝑠𝑖𝑛2𝛼 + Γ11

2𝑐𝑜𝑠2𝛼 + 2Γ11Γ12𝑠𝑖𝑛𝛼𝑐𝑜𝑠𝛼𝑐𝑜𝑠 𝜙11 − 𝜙12

+2𝑉1𝑉2𝑐𝑜𝑠𝜃 Γ11Γ12 𝑠𝑖𝑛2𝛼 − 𝑐𝑜𝑠2𝛼 𝑐𝑜𝑠 𝜙11 − 𝜙12 + Γ122 − Γ11

2 𝑠𝑖𝑛𝛼𝑐𝑜𝑠𝛼

The definition yields 𝑋𝑃𝐷 =𝑅𝑣

2

𝑅ℎ2=𝐴 Γ21

2 + 𝐵 Γ222

𝐴 Γ112 + 𝐵 Γ12

2

𝐴 = 𝑉12𝑠𝑖𝑛2𝛼 + 𝑉2

2𝑐𝑜𝑠2𝛼 − 2𝑉1𝑉2𝑠𝑖𝑛𝛼𝑐𝑜𝑠𝛼𝑐𝑜𝑠𝜃

𝐵 = 𝑉12𝑐𝑜𝑠2𝛼 + 𝑉2

2𝑠𝑖𝑛2𝛼 + 2𝑉1𝑉2𝑠𝑖𝑛𝛼𝑐𝑜𝑠𝛼𝑐𝑜𝑠𝜃where

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

Page 14: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 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 Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

• Analysis assumes• For CP we increased the transmitter power 3dB to maintain the same ERP• The receiver is stationary• Independent of any margin improvement observed by transmitting CP to a

linearly polarized receive antenna in motion

Page 16: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

𝑀𝐼 = 𝑆𝑁𝑅𝑐𝑝 − 𝑆𝑁𝑅𝑙𝑖𝑛𝑒𝑎𝑟

Page 17: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

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

• Controlled environments• Field tests in ME and FL• Indoor / Outdoor / Vehicle• Measurements based on RSS

and BER• Different amounts of VPOL

Page 18: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 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 Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

• Gd and MI are independent• 5-7dB MI is observed when transmitting a single CP signal to a linear

receiver in motion• 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 Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

• A new antenna specification to consider• So far we have assumed the transmit signals are completely uncorrelated• Imperfect antennas couple energy

SR/SL Linear RH/LH circular

𝐼 = 𝑓 𝑐𝑟𝑜𝑠𝑠 𝑝𝑜𝑙𝑎𝑟𝑖𝑧𝑎𝑡𝑖𝑜𝑛 𝐼 = 𝑓 𝑎𝑥𝑖𝑎𝑙 𝑟𝑎𝑡𝑖𝑜

• 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 Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

𝐼 = 10𝑙𝑜𝑔

12 +

𝐴𝑅𝐴𝑅2 + 1

12

1

𝐴𝑅 + 1𝐴𝑅 − 1

2 + 1 +𝐴𝑅

𝐴𝑅2 + 11

𝐴𝑅 + 1𝐴𝑅 − 1

2 − 1

SpecificationAR<1.7dB for RH/LH CP MISO

Page 22: John L. Schadler Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

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

average performance in a stationary MISO diversity system• This is independent of any margin improvement observed by transmitting CP to

a linearly polarized receive antenna in motion• Transmitting CP to a linearly polarized receiver in motion in a heavy scatter

environment can add 5 to 7 dB of margin improvement• 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.• 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 Continuation€¦ · 𝑋𝑃𝐷= 𝑉1 2Γ 21 2 𝑖 2𝛼+Γ 22 2𝑐 2𝛼+2Γ 21Γ22 𝑖 𝛼𝑐 𝛼𝑐 𝜙21−𝜙22 +𝑉2 2Γ 22 2 𝑖 2𝛼+Γ 21

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