imaging with non-aliased seismic wavefields large n (and not just sensors) john hole, iris active...

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Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) n Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL ALIASING resolution resolution resolution WAVEFIELDS NOT JUST WAVEFORMS

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Page 1: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

Imaging with Non-Aliased Seismic WavefieldsLarge N (and not just sensors)

John Hole, IRIS Active Source Workshop, 2014

John HoleVirginia Tech

SPATIALALIASING

resolutionresolutionresolution

WAVEFIELDSNOT JUST WAVEFORMS

Page 2: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

Non-Aliased Seismic Wavefields

seismic reflection uses non-aliased wavefields since the 1950’s

continuity of arrivals=> unwrap statics problem, cycle skips

data redundancy improves S/N => “fold”enables wavefield imaging (stacking, migration, etc.)

need for both shots and receivers to be non-aliased

rest of this presentation: - imaging examples using non-traditional wavefield imaging- description of IRIS’s Large N initiative

Page 3: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

structure of the San Andreas fault zonecontext for $20M drill hole

1999:4.9 km straight line10 m shots, 1 kg5 m stations

2003: 46 km straight line0.5 km shots, 25 kg dense, but aliased 50 m stations (3-component telemetered MEMS)

not funded:3-D multichannal + VSP proposed ($2.7M) rejected due to cost

SAFOD

Page 4: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

SAFOD: Waveform Inversion

travel time tomography

waveform inversion

Bleibinhaus et al., 2007

Page 5: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

requirements:- non-aliased stations- not/weakly aliased at shots- excellent starting model- low frequencies => dense spacing + long offsets => Large N

SAFOD: Waveform Inversion

Bleibinhaus et al., 2007

Page 6: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

SAFOD: Steep-Dip Migration

Bleibinhaus et al., 2007

Hole et al., 2001

requirements:- non-aliased stations- not/weakly aliased at shots- wide-angle offsets and times- excellent velocity model=> dense spacing + long offsets => Large N

Hole et al., 1996

Page 7: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

lithology!

SAF

SAF

SAFOD: Three Component Vp & Vs

Ryberg et al., 2012

requirements:- S waves, ideally from 3-component stations

Page 8: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

SAFOD: Low-Fold Energy Stack

Bleibinhaus et al., 2007

dense receiversmigrated shot gathers

Page 9: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

SAFOD: Low-Fold Energy Stack

dense receiversmigrated shot gathers

much worse than multichannel

aliased shotscannot stack waveforms=> low-fold energy stack

Bleibinhaus et al., 2007

Page 10: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

several 30-50 km lines 2-4 km shots aliased100 m stations

not sufficient for multi-channel reflection=> low-fold energy stack in progress

maybe(?) sufficient for waveform inversion, but only where surface geology is very uniform

=> in progress

perhaps(??) sufficient for steep-dip pre-stack migration=> only line-segment migration to date

SSIP

Page 11: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

Batholiths 2009

SSIP 2011

IDOR 2012

John Hole, IRIS Active Source Workshop, 2014

Continuous Recording

continuous recording on Texans limited by power, RAM, to ~75 hours at 4 msallows flexibility to shoot when readyrecords ambient noise, including earthquakes

AIDA 2011

Page 12: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

Shot Gather Receiver Gather

Surface waveSurface wave

P-waveP-wave

John Hole, IRIS Active Source Workshop, 2014

SSIP: Ambient Noisenoise sources:- geothermal plants (surface and pumping)- 2 highways, 1 railroad- micro-earthquakes (tectonic and induced)- agricultural operations- waves in Salton Sea

Sabey et al., 2013

excellent information about shallow subsurface but does not replace active sources for deeper imaging

10-50 Hz, to 4 km distancereflections in progress; <1 km depth

0.4-8 Hz (on 4.5 Hz phones) to 600 m depth

surface waves

body waves

Page 13: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

P

PcP

0.5-5.0 Hz

60 s

PmS

29-station broadband array - vertical

IDOR: M7.7 Eastern Russia Earthquake

Stanciu et al., 2013

John Hole, IRIS Active Source Workshop, 2014

Page 14: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

P

PcP

0.1-1.0 Hzon 4.5 Hz geophones!

60 s

PmS

2555-station Texan array - vertical

correlation => signal

Davenport et al., 2013

John Hole, IRIS Active Source Workshop, 2014

IDOR: M7.7 Eastern Russia Earthquake

Page 15: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

AIDA Virginia

Davenport et al., in press

148 stations 200-400 m spacing12x12 km array of lines

several thousand aftershocks

John Hole, IRIS Active Source Workshop, 2014

Page 16: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

AIDA Virginia: Aftershocks

Davenport et al., in press

magnitude 2.0

John Hole, IRIS Active Source Workshop, 2014

Page 17: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

1 km

0 s

0.10 s

0.05 s

0 s0 s

0.05 s0.05 s

0.10 s0.10 s

1 km 1 km

Wang et al., 2013

AIDA Virginia: Aftershocks

magnitude 3.7

source back-projection (3-D reverse time migration)

smallest point-source migrated: M(-2)

John Hole, IRIS Active Source Workshop, 2014

Page 18: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

1 km

0 s

0.10 s

0.05 s

0 s0 s

0.05 s0.05 s

0.10 s0.10 s

1 km 1 km

AIDA Virginia: Aftershocks

Wang et al., 2013

magnitude 3.7

source back-projection (3-D reverse time migration)

smallest point-source migrated: M(-2)smallest slip propagation resolved: M2.5

John Hole, IRIS Active Source Workshop, 2014

Page 19: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

Current Status of (Onshore) Academic Community

seismographs:

2-D not aliased (thanks to the Texans)

3-D 10’s of stations x 10’s of stations => usually aliased

3-C a few hundred stations => usually aliased

sources:

=> horribly aliased

Page 20: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

IRIS’s current instrumentation and field procedures are 20+ years oldlimits the science that we can do

past decades have seen rapid improvements in technologyimproved instruments are possible

improving technology enables new science

IRIS’s Large N Initiative

Page 21: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

IRIS’s Large N Initiative

“Large N” = arrays recording non-aliased wavefields

instruments:- much less expensive- much simpler to deploy & retrieve- much simpler to retrieve useful data (dirt to desktop)- high quality signals- broadest possible range of applications, from 1 m to 10,000 km

transform how we acquire data to

enable wavefield imaging methodsSPATIALALIASING

resolutionresolutionresolution

WAVEFIELDSNOT JUST WAVEFORMS

Page 22: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

broadband ~$35k>100 kg3-6-hour deploymentsolar power

long periodhigh sensitivity3-componentlarge memoryGPS

Texan~$4k<2 kg3-minute deployment2 D cells power

high frequencymodest sensitivity1-componentsmall memoryinternal clock

combine the best of bothprobably some compromises

efficiency capacity

John Hole, IRIS Active Source Workshop, 2014

IRIS’s Large N Initiative

Page 23: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

in IRIS’s FY2014-2018 NSF Cooperative Agreement:

continue providing existing instrument services

and

development of Large N

IRIS’s Large N Initiative

Page 24: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

Large N Working Group (chair: John Hole)task: compile…

What new science could be enabled by Large N?

not the focus: technical instrument needs

series of online workshops February-April 2014 single seismic community per workshop

controlled-source: February, hosted by Katie Keranenmarine, OBSIP: use recent workshop (Van Avendonk)

glossy white paper report: Scientific Potential=> NSF, DOE, DOD, USGS, Industry, …

IRIS’s Large N Initiative

Page 25: Imaging with Non-Aliased Seismic Wavefields Large N (and not just sensors) John Hole, IRIS Active Source Workshop, 2014 John Hole Virginia Tech SPATIAL

John Hole, IRIS Active Source Workshop, 2014

Sources

sources are not in IRIS’s Large N…

budget is a major issuenon-aliased shots are too expensive during NSF review process the last onshore deep reflection survey was CD-ROM (1999) marine seismic reflection is currently at risk

possible solution: a facility that removes the source cost from the PI budgetenables science that a PI-driven proposal cannot performa community facility, not just a community projecta virtual facility via standing contracts, rather than instrumentation