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PULSE LIMITED WAVEFORMS FROM
INTERLEAVED MODE: AN ANALYSIS ON
THE ACHIEVABLE SPECKLE REDUCTION
M. Scagliola1, L. Recchia1, D. Giudici1 , M. Kuschnerus2
(2)(1)
 Speckle, multilooking and range noise
 Interleaved mode
 Incoherent average strategy for LR waveforms
 Correlation model for LR waveforms
 Results for the achievable speckle reduction on LR waveforms
 Conclusions
Outline
Speckle, incoherent average and range noise
Speckle: radar echoes are the incoherent
summation of many randomly phased
echoes from small scattering regions of
the surface. This causes the speckle noise.
Incoherent average: speckle reduction can
be achieved by incoherent average,
assuming that single look echoes are only
partially correlated.
Range noise: the uncertainty on the range
measure is function of the number of
statistically independent looks (N) 








SNRNNg
p
h
2
1
8.0


)()()(  sXXs 
)()(
1
)(
1
 sX
N
X
MLN
lML
ml  
Single look echo:
Multilooked echo:
Range noise at the leading edge [1]
[1] Design of the Seasat-A radar altimeter, MacArthur J. L., OCEANS 1976, IEEE
Poseidon4 will be the first altimeter able to operate in a continuous high-
rate pulse mode, i.e. interleaved mode, that foresees that between any
two transmitted pulses, an echo is received.
 simultaneous production of low-resolution mode measurements on-
board as well as the processing of high-resolution echoes on-ground
 higher number of single looks waveforms in high-resolution mode w.r.t.
closed burst mode
Interleaved mode
Just like a Pulse
Limited altimeter
but at a much
higher rate (9
kHz for Ku-band)
…..
Tracking cycle
Tx
Rx
PRF
Incoherent average strategy for LR waveforms
Walsh limit Conventional LRM
instrument
Interleaved mode
instrument
PRF  1.8 kHz  2 kHz  9 kHz
Successive echoes are
partially correlated
Higher number of single look
echoes but more correlated
Echoes
@9kHz
Incoherent
average
Incoherent
average
Echoes
@1.8kHz5
Incoherent average of all pulses @9kHz:
waveforms not statistically equivalent to
conventional LRM instrument but higher
speckle reduction expected
Incoherent average of decimated pulses
@1.8kHz:
waveforms statistically equivalent to
conventional LRM instrument
Two possible strategies for incoherent average [2]:
Objective: quantifying the higher speckle reduction achievable @9kHz
[2] JASON‐CS SAR MODE ERROR BUDGET STUDY REVIEW OF STATE OF KNOWLEDGE FOR SAR
ALTIMETRY OVER OCEAN, EUM/RSP/REP/14/749304, 21 NOVEMBER 2013, VERSION 2.2
Exploiting the single look echo cross-product impulse response in
[3], we can compute the echo correlation coefficient as function of
the delay τ and of the along orbit displacement x
Correlation model for LR waveforms
Mean echo cross-product
over
Mean echo power)(
),(
*)()(
*),()(
),(





X
xx
xR


[3] Giles, K., D. J. Wingham, N. Galin, R. Cullen, W. Smith, 2012: Precise estimates of ocean
surface parameters from Cryosat. OSTST 2012, Venice, 27‐28 Sept 2012,
ENL is defined as the estimate of the
effective number of statistically
independent looks
Higher is the ENL and lower is the
speckle






1
0
1
0
,
2
/
N
n
N
m
mnRNENL
The correlation model has been verified by comparison with the results in
[4], where the coherence as function of the delay delay τ and of the lag
between CryoSat pulses has been measured from CryoSat FBR data
Verification of the correlation model
[4] W.Smith, R. Scharroo, Pulse-to-pulse correlation in CryoSat SAR echoes from ocean surfaces: implications
for optimal pseudo-LRM waveform averaging. 20 years of progress in radar altimetry symposium
Aresys’modelCryoSatdata[3]
The matching between the theoretical
coherence and the experimental one
allows to verify the correcteness of
the Aresys model
Achievable speckle reduction on LR waveforms
-50 0 50 100 150 200 250 300 350 400
0
0.2
0.4
0.6
0.8
1
Echo delay [ns]
Normalizedpower[0-1]
-50 0 50 100 150 200 250 300 350 400
60
65
70
75
80
85
90
Incoherent average @1.8 kHz
time [ns]Numberoflooks
ENL
Number of looks
-50 0 50 100 150 200 250 300 350 400
0
100
200
300
400
Incoherent average @9 kHz
time [ns]
Numberoflooks
ENL
Number of looks
The achievable ENL in case of
Low Resolution waveforms by
averaging echoes at 9 kHz or at
1.8 kHz is here shown:
 the ENL @1.8 kHz approaches
the number of averaged
echoes
 the ENL @9 kHz is far from
the number of averaged
echoes (echoes highly
correlated)
 Oscillations of the ENL as
function of τ can be noticed in
both the cases
SWH = 1 m and SWH = 2 m
250
300
350
400
450
SWH = 1 moflooks
ENL @9 kHz
Number of averaged echoes @9 kHz
ENL @1.8 kHz
Number of averaged echoes @1.8 kHz
0 100 200 300 400 500
0
50
100
150
200
250
300
350
400
450
SWH = 1 m
Echo delay [ns]
Numberoflooks
0 100 200 300 400 500
0
50
100
150
200
250
300
350
400
450
SWH = 2 m
Echo delay [ns]
Numberoflooks
 the ENL is comparable around the leading egde,
i.e same speckle
 the ENL @9 kHz is higher for the trailing edge,
i.e. higher speckle reduction
SWH = 4 m and SWH = 8 m
0 100 200 300 400 500
0
50
100
150
200
250
300
350
400
450
SWH = 4 m
Echo delay [ns]
Numberoflooks
0 100 200 300 400 500
0
50
100
150
200
250
300
350
400
450
SWH = 8 m
Echo delay [ns]
Numberoflooks
250
300
350
400
450
SWH = 1 moflooks
ENL @9 kHz
Number of averaged echoes @9 kHz
ENL @1.8 kHz
Number of averaged echoes @1.8 kHz
 the ENL @9 kHz increases as the SWH increases
 At high SWH, the ENL @9 kHz is higher than the
ENL @1.8 kHz also around the leading edge
 It has been evaluated the theoretical speckle reduction on Low
Resolution waveforms that is achievable by interleaved mode
acquisition in Sentinel-6/Poseidon-4
 By incoherent average of all the echoes at high pulse rate (9 kHz),
going beyond the Walsh limit, we have that
 a higher speckle reduction is achieved, even if the echoes are highly
correlated
 the speckle reduction is more effective in the trailing edge of the
waveform
 the speckle reduction increases as the SWH increases
 Incoherent average of all the available echoes has been verified to be
the best strategy from the speckle reduction point of view
Conclusions
The analysis here shown has been developed in the framework of
activities for the provision to ESA of the Sentinel-6 Poseidon-4 L1b
Simulator, a model-based simulator for Level1 altimeter products
To correctly simulate the LR waveforms, the speckle has to be injected
with the proper statistical properties.
For more details, please refer to FUT_002
presented at SAR Altimetry Workshop 2016, La-Rochelle, 31 October 2016
Sentinel-6 Poseidon-4 L1b Simulator

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PULSE LIMITED WAVEFORMS FROM INTERLEAVED MODE: AN ANALYSIS ON THE ACHIEVABLE SPECKLE REDUCTION

  • 1. PULSE LIMITED WAVEFORMS FROM INTERLEAVED MODE: AN ANALYSIS ON THE ACHIEVABLE SPECKLE REDUCTION M. Scagliola1, L. Recchia1, D. Giudici1 , M. Kuschnerus2 (2)(1)
  • 2.  Speckle, multilooking and range noise  Interleaved mode  Incoherent average strategy for LR waveforms  Correlation model for LR waveforms  Results for the achievable speckle reduction on LR waveforms  Conclusions Outline
  • 3. Speckle, incoherent average and range noise Speckle: radar echoes are the incoherent summation of many randomly phased echoes from small scattering regions of the surface. This causes the speckle noise. Incoherent average: speckle reduction can be achieved by incoherent average, assuming that single look echoes are only partially correlated. Range noise: the uncertainty on the range measure is function of the number of statistically independent looks (N)          SNRNNg p h 2 1 8.0   )()()(  sXXs  )()( 1 )( 1  sX N X MLN lML ml   Single look echo: Multilooked echo: Range noise at the leading edge [1] [1] Design of the Seasat-A radar altimeter, MacArthur J. L., OCEANS 1976, IEEE
  • 4. Poseidon4 will be the first altimeter able to operate in a continuous high- rate pulse mode, i.e. interleaved mode, that foresees that between any two transmitted pulses, an echo is received.  simultaneous production of low-resolution mode measurements on- board as well as the processing of high-resolution echoes on-ground  higher number of single looks waveforms in high-resolution mode w.r.t. closed burst mode Interleaved mode Just like a Pulse Limited altimeter but at a much higher rate (9 kHz for Ku-band) ….. Tracking cycle Tx Rx PRF
  • 5. Incoherent average strategy for LR waveforms Walsh limit Conventional LRM instrument Interleaved mode instrument PRF  1.8 kHz  2 kHz  9 kHz Successive echoes are partially correlated Higher number of single look echoes but more correlated Echoes @9kHz Incoherent average Incoherent average Echoes @1.8kHz5 Incoherent average of all pulses @9kHz: waveforms not statistically equivalent to conventional LRM instrument but higher speckle reduction expected Incoherent average of decimated pulses @1.8kHz: waveforms statistically equivalent to conventional LRM instrument Two possible strategies for incoherent average [2]: Objective: quantifying the higher speckle reduction achievable @9kHz [2] JASON‐CS SAR MODE ERROR BUDGET STUDY REVIEW OF STATE OF KNOWLEDGE FOR SAR ALTIMETRY OVER OCEAN, EUM/RSP/REP/14/749304, 21 NOVEMBER 2013, VERSION 2.2
  • 6. Exploiting the single look echo cross-product impulse response in [3], we can compute the echo correlation coefficient as function of the delay τ and of the along orbit displacement x Correlation model for LR waveforms Mean echo cross-product over Mean echo power)( ),( *)()( *),()( ),(      X xx xR   [3] Giles, K., D. J. Wingham, N. Galin, R. Cullen, W. Smith, 2012: Precise estimates of ocean surface parameters from Cryosat. OSTST 2012, Venice, 27‐28 Sept 2012, ENL is defined as the estimate of the effective number of statistically independent looks Higher is the ENL and lower is the speckle       1 0 1 0 , 2 / N n N m mnRNENL
  • 7. The correlation model has been verified by comparison with the results in [4], where the coherence as function of the delay delay τ and of the lag between CryoSat pulses has been measured from CryoSat FBR data Verification of the correlation model [4] W.Smith, R. Scharroo, Pulse-to-pulse correlation in CryoSat SAR echoes from ocean surfaces: implications for optimal pseudo-LRM waveform averaging. 20 years of progress in radar altimetry symposium Aresys’modelCryoSatdata[3] The matching between the theoretical coherence and the experimental one allows to verify the correcteness of the Aresys model
  • 8. Achievable speckle reduction on LR waveforms -50 0 50 100 150 200 250 300 350 400 0 0.2 0.4 0.6 0.8 1 Echo delay [ns] Normalizedpower[0-1] -50 0 50 100 150 200 250 300 350 400 60 65 70 75 80 85 90 Incoherent average @1.8 kHz time [ns]Numberoflooks ENL Number of looks -50 0 50 100 150 200 250 300 350 400 0 100 200 300 400 Incoherent average @9 kHz time [ns] Numberoflooks ENL Number of looks The achievable ENL in case of Low Resolution waveforms by averaging echoes at 9 kHz or at 1.8 kHz is here shown:  the ENL @1.8 kHz approaches the number of averaged echoes  the ENL @9 kHz is far from the number of averaged echoes (echoes highly correlated)  Oscillations of the ENL as function of τ can be noticed in both the cases
  • 9. SWH = 1 m and SWH = 2 m 250 300 350 400 450 SWH = 1 moflooks ENL @9 kHz Number of averaged echoes @9 kHz ENL @1.8 kHz Number of averaged echoes @1.8 kHz 0 100 200 300 400 500 0 50 100 150 200 250 300 350 400 450 SWH = 1 m Echo delay [ns] Numberoflooks 0 100 200 300 400 500 0 50 100 150 200 250 300 350 400 450 SWH = 2 m Echo delay [ns] Numberoflooks  the ENL is comparable around the leading egde, i.e same speckle  the ENL @9 kHz is higher for the trailing edge, i.e. higher speckle reduction
  • 10. SWH = 4 m and SWH = 8 m 0 100 200 300 400 500 0 50 100 150 200 250 300 350 400 450 SWH = 4 m Echo delay [ns] Numberoflooks 0 100 200 300 400 500 0 50 100 150 200 250 300 350 400 450 SWH = 8 m Echo delay [ns] Numberoflooks 250 300 350 400 450 SWH = 1 moflooks ENL @9 kHz Number of averaged echoes @9 kHz ENL @1.8 kHz Number of averaged echoes @1.8 kHz  the ENL @9 kHz increases as the SWH increases  At high SWH, the ENL @9 kHz is higher than the ENL @1.8 kHz also around the leading edge
  • 11.  It has been evaluated the theoretical speckle reduction on Low Resolution waveforms that is achievable by interleaved mode acquisition in Sentinel-6/Poseidon-4  By incoherent average of all the echoes at high pulse rate (9 kHz), going beyond the Walsh limit, we have that  a higher speckle reduction is achieved, even if the echoes are highly correlated  the speckle reduction is more effective in the trailing edge of the waveform  the speckle reduction increases as the SWH increases  Incoherent average of all the available echoes has been verified to be the best strategy from the speckle reduction point of view Conclusions
  • 12. The analysis here shown has been developed in the framework of activities for the provision to ESA of the Sentinel-6 Poseidon-4 L1b Simulator, a model-based simulator for Level1 altimeter products To correctly simulate the LR waveforms, the speckle has to be injected with the proper statistical properties. For more details, please refer to FUT_002 presented at SAR Altimetry Workshop 2016, La-Rochelle, 31 October 2016 Sentinel-6 Poseidon-4 L1b Simulator