Ambient Seismic Noise Interferometry Using Rotational Ground Motion

Ambient Seismic Noise Interferometry Using Rotational Ground Motion

Ambient seismic noise interferometry using rotational ground motion Céline Hadziioannou, Paul Neumann University of Hamburg, Germany Joachim assermann, Heiner !gel "udwig$%aximilians-University %unich, Germany Ulrich 'chreiber Technical University %unich, Germany … and the *+%Y team - .ideo recording of presentation here 0or scan the QR code23 Note4 most references are lin5s to the publications2 - Ne# sensing technologies 6 beyond conventional seismic translation measurements- Here: rotational ground motion Can we detect the wea5 ocean-generated seismic noise with the e&isting rotation sensors7 Can we /erform ambient noise interferometry #ith rotational motions7 !nterferometry with rotations 8 strain4 Paitz, Sager, 9ichtner: GJI 2<=> +bserving rotations4 Ring lasers G meter Observatory instruments: Ring lasers Ring lasers o?er a point measurement of rotational ground motion @ RLAS in Wettzell Germany: vertical com/onent rotation =; meter most sensitive worldwide co-located seismometer4 A( @ RO"Y near Munich Germany: RLAS Brst 3-com/onent rotation RO"# co-located seismometer4 9U* D*+%,4 A Multi-Component Ring Laser for Geodesy and Geophysics”, earthAr&iv D"ord of the Rings”, Science, 2<=F +bserving rotations4 Ring lasers Observatory instruments: Ring lasers @ RLAS in Wettzell Germany: vertical com/onent rotation most sensitive worldwide co-located seismometer4 A( @ RO"Y near Munich Germany: Brst 3-com/onent rotation co-located seismometer4 9U* Here: focus on vertical component: 'H- and Love waves %an we pic' up the ocean microseism? PP'L for seismometer vs- ring laser Translations: Seismometer Rotations: RLAS Laser Primary Secondary 'econdary %icroseism %icroseism %icroseism !nstrument sensitivity limit H<-<J$<-= Hz] H<-=$<-; Hz] 0before 2<=K3 RLAS RO"# %an we pic' up the ocean microseism? PP'L for seismometer vs- ring laser Translations: Seismometer Rotations: RLAS Laser Primary Secondary Primary 'econdary %icroseism %icroseism %icroseism %icroseism !nstrument sensitivity limit H<-<J$<-= Hz] H<-=$<-; Hz] 0after 2<=K3 RLAS RO"# *"A' ring laser in ettzell im/roved in 20=F Here4 Primary microseism detected in January 20=K !s it really the primary microseism7 Combining Rotation and Translation 3C Translation @ 3C Rotation Ground acceleration *otation rate Seismometer Rotation sensor @ *otation rate and acceleration should be in phase @ am/litudes scaled by t&o times the horizontal phase velocity) *hase velocity → using single measurement of 6C in phase + waveforms similar → can Bnd source direction %an we pic' up the ocean microseism? PP'L for seismometer vs- ring laser Rotations: RLAS Laser Primary 'econdary %icroseism %icroseism !nstrument sensitivity limit 0after 2<=K3 RLAS RO"# *"A' ring laser in ettzell im/roved in 20=F Here4 Primary microseism detected in January 20=K !s it really the primary microseism7 !s it coming from a speci,c direction? 'ingle$point bac'azimuth determination *otation rate and acceleration should be in phase in phase → waveforms similar + can find source direction *rimary microseism: 0-<5 N 0-= Hz h t u m i z RLAS a ' RO"# c a b -. hours A//roach described: Hadziioannou et al- ;<=;, Jo' Sensitivity of ring laser sufficiently im/roved to detect primary microseism Rotations: RLAS Laser Primary Secondary Coherent #avefield coming from North4 %icroseism / %icroseism 0consistent #ith e-g. Juretze5 8 Hadziioannou, GJI 2<=F3 *rimary microseism detected/ <-<J N 0-= Hz !nstrument sensitivity limit h t 0after ;<=K3 u m i z RLAS a ' RO"# c a b -. hours A//roach described: Hadziioannou et al. 20=;, Jo' - Ne# sensing technologies 6 beyond conventional seismic translation measurements- Here: rotational ground motion Can we detect the wea5 ocean-generated seismic noise with the e&isting rotation sensors7 Yes/ + Sensitivity of ring laser sufficiently im/roved to detect primary microseism Can we /erform ambient noise interferometry #ith rotational motions7 Ambient noise interferometry 9rom seismic noise to useful signal4 noise interferometry 1deal case: ● noise sources illuminating medium from all sides ● Average recorded noise over long time ● Turns seismometers into 2virtual sources’ A correlation 0 time N time + 4oes this work for rotational motion( Noise *eceiver source ant to know more? D(utorial on seismic interferometryE, apenaar et al, Geo/hysics 20=< Seismic noise interferometry with rotational ground motion? h t u m i z a ' c a b 5 hours RLAS RO"# .)- 6 0)5 Hz Secondary microseism available on both sensors Dominant source to#ard N consistent #ith beamforming D here do ocean microseisms come from7E Juretze5 8 Hadziioannou, JGR ;<=M Seismic noise interferometry with rotational ground motion? Need long enough stacking time: 6 P one year of noise, <=-<=-;<=K – <=-=;-;<=K Ambient noise from the secondary microseism available on both sensors: 6 filter between <-= – <-2 Hz RLAS RO"# Seismic noise interferometry with rotational ground motion? "ove waves RLAS Ambient noise interferometry: RO"# @ blac': bet#een two seismometers near *+MY and *"A' 0QclassicR case) Seismic noise interferometry with rotational ground motion? "ove waves RLAS Ambient noise interferometry: RO"# @ blac'4 between t&o seismometers near *+%Y and *"AS 0Qclassic’ case) @ red4 between the t&o ring lasers *+MY and *"A' Seismic noise interferometry with rotational ground motion? "ove waves RLAS Ambient noise interferometry: RO"# @ blac'4 between t&o seismometers near *+%Y and *"AS 0Qclassic’ case) @ red4 between the t&o ring lasers *+MY and *"A' @ &aveform of vertical rotation rate 0red3 should be similar to the transverse acceleration 0blac'3 @ #ith long enough stac'ing time, the #aveforms match2 Seismic noise interferometry with rotational ground motion? "ove waves RLAS Ambient noise interferometry: RO"# @ blac': between t&o seismometers near *+%, and *"A' 0Qclassic’ case3 @ red4 between the t&o ring lasers *+%Y and *"AS @ blue: synthetic signal for =D model 0P*A%3 source at *"A' recorded at *+%, 'eismic noise analysis with rotational ground motion Ocean-generated noise can be detected at two ring laser sites: beside the secondary microseism, no# also the primary microseism + push limit towards weak motions *roof of concept: first case of 2rotational3 noise interferometry using ocean-generated noise recorded at t#o ring lasers + towards noise interferometry of 6-component displacement data. !eneral: + ambient noise applications with rotational motion What3s ne8t( 'lides 8 more4 celine-hadzii-com What does the future bring? 1nnovative $raining net&or' funded by <: H2.5. programme Started march 5.5-) integrate emerging ground$motion sensing technology into seismological /ractice A?ect of small-scale structure and changes on the seismic wave field $rain a ne# generation of researchers4 -= *h4 positions across <urope !ermany University of Hamburg (Coordinator3 "%U Munich GFS Potsdam S&itzerland A(H ZTrich 9rance !PGP Paris Université Grenoble Al/es 1reland L!AS Dublin :; University of Edinburgh Uritish Geological 'ervice %ore about 'PIN4 htt/4VVs/in-itn-eu 'lides 8 more4 celine-hadzii-com twitter-comV'PIN_itn References 1n this presentation: Hadziioannou, C-, Gaebler, P-, 'chreiber, U-, Wassermann, J-, & Igel, H- 0;<=;3- A&amining ambient noise using colocated measurements of rotational and translational motion. Journal of 'eismology, =M0G3, FKF$F>M- htt/4VVd&-doi-orgV=<-=<<FVs=<>J<$<=;$>;KK$J C- Juretze5, C- Hadziioannou, 0;<=F3- "in5ing source region and ocean #ave /arameters #ith the observed /rimary microseismic noise, Geo/hys- J- Int- ;== 0C3, =MG<$=MJG- htt/s4VVdoi-orgV=<-=<>CVgXiVgg&CKK C- Juretze5, C- Hadziioannou, 0;<=M3- here do ocean microseisms come from7 A study of "ove$to$*ayleigh #ave ratios, J- Geo/hys- *es- 'olid Earth =;=, MFG=$MFJM htt/4VVd&-doi-orgV=<-=<<;V;<=MJU<=C<=F D*+%,4 A Multi$Com/onent *ing "aser for Geodesy and Geo/hysicsE 0;<;=3 Geo/hysical Journal International, ;;J0=3, MKG – M>K- htt/s4VVdoi-orgV=<-=<>CVgXiVggaaM=G earthAr&iv htt/s4VVearthar&iv-orgVre/ository/vie#V=F;CV Y"ord of the *ingsY, 'cience ;= A/r ;<=F4 Vol- CJM, Issue MCCJ, //- ;CM$;CK L+!4 =<-==;MVscience-CJM-MCCJ-;CM Paitz, P-, 'ager, Z-, & 9ichtner, A- 0;<=>3- *otation and strain ambient noise interferometry. Geo/hysical Journal International, ;=M0C3, =>CK$=>J;- htt/s4VVdoi-orgV=<-=<>CVgXiVggy5;K a/enaar, Z-, Draganov, L-, 'nieder, *-, Cam/man, [-, & Verdel, A- 0;<=<3- (utorial on seismic interferometry: Part =\Uasic /rinci/les and a//lications- Geo/hysics, FJ0J3, FJA=>J$FJA;<>- htt/s4VVdoi-orgV=<-==><V=-CGJFGGJ References Rotational seismology database 'alvermoser, J-, Hadziioannou, C-, Hable, S-, Krischer, L-, Cho#, B-, Ramos, C-, Wassermann, J., Schreiber, U-, Gebauer, A & !gel, H- (;<=F3- An event database for rotational seismology- Seismological Research Letters. htt/s4VVrotations-database-geophysi5-uni$muenchen-deV !et started &ith rotational data seismo-live-org → rotational seismology 6 C introductory noteboo5s to re/roduce some figures from the rotational database presented in the lin5 above.

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