Product Delivery Report for K&C Phase 2. Christian Thiel Friedrich-Schiller-University Jena

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Product Delivery Report for K&C Phase 2 Christian Thiel Friedrich-Schiller-University Jena Science Team meeting #15 JAXA TKSC/RESTEC HQ, Tsukuba/Tokyo, January 24-28, 2011

1. Published (please provide PDF file) K&C deliverables Papers and Reports K&C Phase-1 and Phase 2 reports, contribution to K&C Booklet CH. THIEL, CA. THIEL & C. SCHMULLIUS (2009): Operational Large Area Forest Monitoring in Siberia Using ALOS PALSAR Summer Intensities and Winter Coherence.-In: IEEE Trans. Geoscience and Remote Sensing 47(12), pp. 3993-4000. CH. THIEL & C. SCHMULLIUS (2009): Examination of Multi-Seasonal ALOS PALSAR Interferometric Coherence for Forestry Applications in the Boreal Zone.-In: Proceedings of 3rd Joint PI Symposium of ALOS Data Nodes for ALOS Science Program, 09. 13. November 2009, Kona, USA. THIEL, CH., M. SANTORO, O. CARTUS, CA. THIEL, T. RIEDEL & C. SCHMULLIUS (2009): Perspectives of SAR based Forest Cover, Forest Cover Change and Biomass Mapping. In: Christophe P. Vasser [Ed.], The Kyoto Protocol: Economic Assessments, Implementation Mechanisms, and Policy Implications, pp. 13-56, ISBN: 978-1-60456-983-4. THIEL, CA., CH. THIEL, J. REICHE, R. LEITERER & C. SCHMULLIUS (2009): Großflächige Waldüberwachung in Sibirien unter Verwendung von ALOS PALSAR Winter Kohärenzen und Sommer Intensitäten.-In: Proceedings of 29. DGPF Jahrestagung: 24.-26.03.2009, Jena, Germany. THIEL, C. & C. SCHMULLIUS (2010): Examination of Summer- and Winter ALOS PALSAR Interferometric Coherence and Phase in Siberia. Proceedings of the ESA Living Planet Symposium, 28 June - 2 July 2010, Bergen, Norway. THIEL, C. & C. SCHMULLIUS (2010): Seasonality of ALOS PALSAR Interferometric Coherence and Interferometric Phase in central Siberia and its implication on forest parameter retrieval. - Proceedings of the International Geoscience and Remote Sensing Symposium IGARSS 10: 25-30 July 2010, Hawaii, USA.

K&C deliverables Papers and Reports 1. Published (please provide PDF file) 2. Submitted/in preparation THIEL, C. (spring 2011) et. al: Seasonality of ALOS PALSAR Interferometric Coherence and Interferometric Phase in central Siberia and its implication on forest parameter retrieval.-in: IEEE Trans. Geoscience and Remote Sensing. Sen4Science, ALOS Symposium 2011 etc.

K&C deliverables Original idea of the phase 2 proposal was to use the information contained in the winter coherence additionally to the backscatter for land cover mapping in the boreal zone. This idea was based on the very promising results of phase one. So far, the data base in terms of coherence data strips could not be provided. However, the whole approach is pending and might be accomplished at phase 3, at least for a smaller demonstration area. New overall topic: investigate use of interferometric coherence for forest biomass estimation

ALOS-PALSAR coherence for biomass estimation in the boreal zone Background

ALOS-PALSAR coherence for biomass estimation in the boreal zone Background Assumption: Decreasing coherence caused by volume decorrelation and temporal decorrelation

Data

Winter vs. Summer coherence Winter coherence (46 days) Summer coherence (46 days) This behavior was found for all sites. Dependency of perpendicular baseline?

Forest coherence versus perpendicular baselines: summer Horizontal lines denote coherence (and its standard deviation) for decorrelated data

Forest coherence versus perpendicular baselines: summer Horizontal lines denote coherence (and its standard deviation) for decorrelated data

Forest coherence versus perpendicular baselines: summer Temporal baseline = 92 days (blue) and > 92 days (red), all perpendicular baselines

Forest coherence versus perpendicular baselines: winter

Forest coherence versus perpendicular baselines: winter Temporal baseline = 92 days (blue) and > 92 days (red), all perpendicular baselines Is volume decorrelation occurring?

Summary of coherence behavior (averaged over 10 sites)

Summary of coherence behavior (averaged over 10 sites) Average coherence for stem volume 250-350 m³/ha 23 24 08 04 11 01 67 17 37 Number of samples 1 sample = 1 coherence image w = winter s = summer 1,2,3 = Δ cycle = mean over scenes - = min/max B>2km B>2km B>2km

Summary of coherence behavior (averaged over 10 sites) Saturation level [m³/ha] 23 24 08 04 11 01 67 17 37 Number of samples 1 sample = 1 coherence image w = winter s = summer 1,2,3 = Δ cycle = mean over scenes - = min/max B>2km B>2km B>2km

Summary of coherence behavior (averaged over 10 sites) R² stem volume vs. coherence (@ 10 m³/ha biomass class level) 23 24 08 04 11 01 67 17 37 Number of samples 1 sample = 1 coherence image w = winter s = summer 1,2,3 = Δ cycle = mean over scenes - = min/max B>2km B>2km B>2km

Investigation of interferometric phase Clear-cuts visible at shaded relief based on SRTM elevation data (Chunsky N)

Investigation of interferometric phase Clarification of high summer coherence phenomenon Investigation of interferometric phase (comparison of winter against summer phase centre) Summer INSAR Phase RGB = φhhφhvφhh

Investigation of interferometric phase Forest Clear-cut Forest B Δφ HH φ HH HH φ HV A RGB = φ HH φ HV φ HH Δφ HV HV A B

Investigation of interferometric phase Forest Clear-cut Forest B Δφ HH φ HH HH φ HV A RGB = φ HH φ HV φ HH Δφ HV HV A B

Investigation of interferometric phase Biased by topography (this bias can unfortunately not be corrected for, as no topographic surface model is available) Absolute offset (difference) is unaffected Difference in summer is about two times larger than in winter Only wanes considered, were the SRTM data features greater elevation for forest as for the related clear-cut, merely positive offsets emerge (320 entities)

Investigation of interferometric phase (320 entities)

Summer Coherence Remarkable examples (summer only) How much coherence is produced by the trees without ground interaction?

Summary Overall ALOS PALSAR data have high potential for forest stem volume estimation in Siberia Midwinter FBS coherence provides the most powerful measure Summer FBD coherence can provide additional information (e.g. for forest cover mapping), however, temporal baseline must be enlarged to increase temporal decorrelation This approach is very susceptible to variable environmental conditions (weather, soil moisture) Computation of coherence based on FBS (winter) and FBD (summer) images is possible, but not very useful; it might be used to support forest cover mapping At forests scattering processes in summer and winter are entirely different This fact must be considered when developing biomass estimation models

Summary Scientific Issues In summer overall temporal decorrelation is not larger than in winter (consecutive cycle coherence) This applies in particular to high stem volume classes In winter, decorrelation of high stem volume areas is interpreted as effect of volume decorrelation, temporal decorrelation is assumed to have minor effect (extremely stable environmental conditions) However independency of perp. baseline! Contradictionary to volume decorrelation assumption In summer, the decrease of penetration depth Remarkable examples (increasing coherence with increasing stem volume): Changing soil moisture impacts areas with low stem volume

Summary Scientific Issues For winter coherence no impact of spatial baseline evident One possible explanation (in accordance with all above results): Frozen forest, represented by stems and canopy, is a semitransparent layer on top of the surface. This layer introduces a noise component to the coherent signal coming from the ground (point- and surface scattering) Amount of noise driven by the density and the depth of this forest layer Basing on this assumption the coherence modelling over forest becomes rather simple

Summary Scientific Issues For winter coherence no impact of spatial baseline evident One possible explanation (in accordance with all above results): Frozen forest, represented by stems and canopy, is a semitransparent layer on top of the surface. This layer introduces a noise component to the coherent signal coming from the ground (point- and surface scattering) Amount of noise driven by the density and the depth of this forest layer Basing on this assumption the coherence modelling over forest becomes rather simple ɤ for = ɤ ground + noise noise = density depth Density Depth

Thank you! 1 no stretching applied on image data 0 20jun07_05aug07 21dec07_05feb08 05nov07_20jun07 Coherence Images Examples Chunsky N (Temp. Baseline 46 d)