721
Amante, C., and .B. W., Eakins (2009). ETOPO1 1 arc-minute global relief model:
722
procedures, data sources and analysis. In: NOAA Technical Memorandum NESDIS
723
NGDC-24, p. 19.
724
Asimow, P. D., and Langmuir, C. H. (2003). The importance of water to oceanic mantle
725
melting regimes. Nature, 421, 815-820. https://doi.org/10.1038/nature01429
726
Baba, K., and Seama, N. (2002). A new technique for the incorporation of seafloor
727
topography in electromagnetic modeling. Geophys. J. Int., 150, 392-402.
728
https://doi.org/10.1046/j.1365-246X.2002.01673.x
729
Baba, K., and A. D. Chave (2005), Correction of seafloor magnetotelluric data for
730
topographic effects during inversion, J. Geophys. Res., 110, B12105,
731
doi:10.1029/2004JB003463
24
732
Baba, K., Chave, A. D., Evans, R. L., Hirth, G., and Mackie, R. L. (2006). Mantle
733
dynamics beneath the East Pacific Rise at 17°S: Insights from the Mantle
734
Electromagnetic and Tomography (MELT) experiment. J. Geophys. Res., 111,
735
B02101. https://doi.org/10.1029/2004JB003598
736
Becker, N., Fryer, C., P., and Moore, G. F. (2010). Malaguan-Gadao Ridge: Identification
737
and implications of a magma chamber reflector in the southern Mariana Trough.
738
Geochem.
739
https://doi.org/10.1029/2009GC002719
740
741
Geophys.
11,
Geosyst.,
Q04X13.
Bird, P. (2003). An updated digital model of plate boundaries. Geochem. Geophys.
Geosyst., 4(3), 1027. https://doi.org/10.1029/2001GC000252
742
Brounce, M., Kelley, K. A., Stern, R., Martinez, F., and Cottrell, E. (2016). The Fina Nagu
743
volcanic complex: Unusual submarine arc volcanism in the rapidly deforming
744
southern Mariana margin. Geochem. Geophys. Geosyst., 17, 4078-4091.
745
https://doi.org/10.1002/2016GC006457
746
Cagnioncle, A.-M., Parmentier, E. M., and Elkins-Tanton, L. T. (2007). Effect of solid
747
flow above a subducting slab on water distribution and melting at convergent plate
748
boundaries. J. Geophys. Res., 112, B09402. https://doi.org/10.1029/2007JB004934
749
Chave, A. D., and Thomson, D. J. (2004). Bounded influence estimation of
750
magnetotelluric
751
https://doi.org/10.1111/j.1365-246X.2004.02203.x
response
functions.
Geophys.
J.
Int.,
157,
988–1006.
752
Conder, J. A. (2007). Temperature structure of the Mariana system from geodynamical
753
modeling. Joint NSF-MARGINS and IFREE Workshop: Subduction Factory
754
Studies in the Izu-Bonin-Mariana Arc System: Results and Future Plans, Honolulu,
755
Hawaii, (Available at http://www.nsf-margins.org/IBM07/index.html).
756
Conder, J. A., Wiens, D. A., and Morris, J. (2002). On the decompression melting
757
structure at volcanic arcs and back-arc spreading centers. Geophys. Res.
758
Lett., 29(15), https://doi.org/10.1029/2002GL015390
759
Constable, S., Shankland, T. J., and Duba, A. (1992). The electrical conductivity of an
760
isotropic
761
https://doi.org/10.1029/91JB02453
762
763
olivine
mantle. J.
Geophys.
Res., 97(B3), 3397-3404.
Constable, S. (2006). SEO3: A new model of olivine electrical conductivity. Geophys. J.
Int., 166, 435-437. https://doi.org/10.1111/j.1365-246X.2006.03041.x
25
764
Dalton, C. A, Langmuir, C. H., Gale, A. (2014). Geophysical and geochemical evidence
765
for deep temperature variations beneath mid-ocean ridges. Science, 344(6179), 80-
766
83. https://doi.org/10.1126/science.1249466
767
Dasgupta, R., and Hirschmann, M. M. (2010). The deep carbon cycle and melting in
768
Earth's
769
https://doi.org/10.1016/j.epsl.2010.06.039
770
interior.
Earth
Planet.
Lett.,
298(1-2),
1-13.
Dunn, R. A., and Martinez, F. (2011). Contrasting crustal production and rapid mantle
771
transitions
772
https://doi.org/10.1038/nature09690
773
Sci.
beneath
back-arc
ridges.
469, 198-202.
Nature,
England, P. C., and Katz, R. F. (2010). Melting above the anhydrous solidus controls the
774
location
775
https://doi.org/10.1038/nature09417
of
volcanic
arcs.
467, 700-703.
Nature,
776
Evans, R. L., Hirth, G., Baba, K., Forsyth, D., Chave, A., and Mackie, R. (2005).
777
Geophysical evidence from the MELT area for compositional controls on oceanic
778
plates. Nature, 437, 249-252. https://doi.org/10.1038/nature04014
779
Evans, R. L., Wannamaker, P. E., McGary, R. S., Elsenbeck, J. (2013). Electrical structure
780
of the central Cascadia subduction zone: The EMSLAB Lincoln Line revisited.
781
Earth Planet. Sci. Lett., 402, 265-274. https://doi.org/10.1016/j.epsl.2013.04.021
782
Forsyth, D. W. (1992). Geophysical constraints on mantle flow and melt generation
783
beneath mid-ocean ridges. In J. P. Morgan, D. K. Blackman, J. M. Sinton
784
(Eds.), Mantle flow and melt generation at mid-ocean ridges, Geophysical
785
Monograph Series (Vol. 71, pp. 183-280).
786
Geophysical Union. Htttps://doi.org/10.1029/GM071p0001
787
Washington, DC: American
Gardés, E., Gaillard, F., and Tarits, P. (2014), Toward a unified hydrous olivine electrical
788
conductivity
789
https://doi.org/10.1002/2014GC005496
law.
Geochem.
Geophys.
Geosyst.,
15,
4984-5000.
790
Gerya, T. V., and Yuen, D. A. (2003). Rayleigh-Taylor instabilities from hydration and
791
melting propel ‘cold plumes’ at subduction zones. Earth Planet. Sci. Lett., 212, 47-
792
62. https://doi.org/10.1016/S0012-821X(03)00265-6
793
Grove, T. L., Till, C. B., Lev, E., Chatterjee, N., and Médard, E. (2009). Kinematic
794
variables and water transport control the formation and location of arc volcanoes.
795
Nature, 459, 694-697. https://doi.org/10.1038/nature08044
26
796
Guo, X., Yoshino, T., and Katayama, I. (2011). Electrical conductivity anisotropy of
797
deformed talc rocks and serpentinites at 3 GPa. Phys. Earth Planet. Inter., 188, 69-
798
81. https://doi.org/10.1016/j.pepi.2011.06.012
799
Hayes, G. P., Wald, D. J., and Johnson, R. L. (2012). Slab1.0: A three-dimensional model
800
of global subduction zone geometries. J. Geophys. Res., 117, B01302.
801
https://doi.org/10.1029/2011JB008524
802
Hacker, B. R., Abers, G. A., and Peacock, S. M. (2003). Subduction factory, 1, Theoretical
803
mineralogy, densities, seismic wave speeds, and H2O contents. J. Geophys. Res.,
804
108(B1), 2029. https://doi.org/10.1029/2001JB001127
805
Hall, P. S., and Kincaid, C. (2001). Diapiric flow at subduction zones: A recipe for rapid
806
transport. Science, 292(5526), 2472-2475. https://doi.org/10.1126/science.1060488
807
Harmon, N., and Blackman, D. K. (2010). Effects of plate boundary geometry and
808
kinematics on mantle melting beneath the back-arc spreading centers along the Lau
809
Basin.
810
https://doi.org/10.1016/j.epsl.2010.08.004
Earth
Planet.
Sci.
Lett.,
298,
334-346.
811
Hashin, Z., and Shtrikman, S. (1962). A variational approach to the theory of the effective
812
magnetic permeability of multiphase materials, J. Appl. Phys., 33, 3125-3131.
813
https://doi.org/10.1063/1.1728579
814
Hirschmann, M. M., Aubaud, C., and Withers, A. C. (2005). Storage capacity of H2O in
815
nominally anhydrous minerals in the upper mantle. Earth Planet. Sci. Lett., 236,
816
167-181. https://doi.org/10.1016/j.epsl.2005.04.022
817
Hyndman, R. D., and Peacock, S. M. (2003). Serpentinization of the forearc mantle. Earth
818
Planet. Sci. Lett., 212, 417-432. https://doi.org/10.1016/S0012-821X(03)00263-2.
819
Ikemoto, A., and H. Iwamori (2014). Numerical modeling of trace element transportation
820
in subduction zones: implications for geofluid processes. Earth Planets Space,
821
66:26, https://doi.org/10.1186/1880-5981-66-26
822
Ito, G., Lin, J., and Graham, D. (2003). Observational and theoretical studies of the
823
dynamics of mantle plume–mid-ocean ridge interaction. Rev. Geophys., 41, 4, 1017,
824
https://doi:10.1029/2002RG000117
825
Kato, T., Beavan, J., Matsushima, T., Kotake, Y., Camacho, J. T., and Nakao, S. (2003).
826
Geodetic evidence of back-arc spreading in the Mariana Trough. Geophys. Res.
827
Lett., 30(12), 1625. https://doi.org/10.1029/2002GL016757
27
828
Kawamoto, T., Kanzaki, M., Mibe, K., Matsukage, K. N., and Ono, S. (2012). Separation
829
of supercritical slab-fluids to form aqueous fluid and melt components in
830
subduction zone magmatism. Proc Natl Acad Sci USA., 109(46), 18695-18700.
831
https://doi.org/10.1073/pnas.1207687109
832
Key, K., Constable, S. Liu, L., and Pommier, A. (2013), Electrical image of passive
833
mantle upwelling beneath the northern East Pacific Rise, Nature, 495, 499-502.
834
https://doi.org/0.1038/nature11932
835
Kelley, K. A., Plank, T., Grove, T. L., Stolper, E. M., Newman, S., and Hauri, E. (2006).
836
Mantle melting as a function of water content beneath back-arc basins. J. Geophys.
837
Res., 111, B09208. https://doi.org/10.1029/2005JB003732
838
Kelley, K. A., Plank, T., Newman, S., Stolper, E. M., Grove, T. L., Parman, S., Hauri, E.
839
H. (2010). Mantle melting as a function of water content beneath the Mariana Arc, J.
840
Petrol., 51(8), 1711-1738. https://doi.org/10.1093/petrology/egq036
841
Kimura, J.-I., and Nakajima, J. (2014). Behaviour of subducted water and its role in
842
magma genesis in the NE Japan arc: A combined geophysical and geochemical
843
approach.
844
https://doi.org/10.1016/j.gca.2014.04.019
Geochim.
Cosmochim.
Acta,
143,
165-188.
845
Kitada, K., Seama, N., Yamazaki, T., Nogi, Y., and Suyehiro, K. (2006). Distinct regional
846
differences in crustal thickness along the axis of the Mariana Trough, inferred from
847
gravity
848
https://doi.org/10.1029/2005GC001119
anomalies.
Geochem.
Geophys.
Geosyst.,
7,
Q04011.
849
Ledo, J., Gueralt, P., Marti, A., and Jones, A. G. (2002). Two-dimensional interpretation
850
of three-dimensional magnetotelluric data: an example of limitations and resolution.
851
Geophys. J. Int., 150, 127-139. https://doi.org/10.1046/j.1365-246X.2002.01705.x
852
Lin, J., and Morgan, J. P. (1992). The spreading rate dependence of three-dimensional
853
mid-ocean
854
https://doi.org/10.1029/91GL03041
ridge
gravity
structure,
Geophys.
Res.
Lett., 19(1),
13-16.
855
Liu, C.-Z., Snow, J. E., Hellebrand, E., Brügmann, G., von der Handt, A., Büchl, A. and
856
Hofmann, A. W. (2008). Ancient, highly heterogeneous mantle beneath Gakkel
857
ridge, Arctic Ocean, Nature, 452, 311-316. https://doi.org/10.1038/nature06688
858
Macdonald, K. C., Scheirer, D. S., and Carbotte, S. M. (1991). Mid-ocean ridges:
859
Discontinuities, segments and giant cracks, Science, 253(5023), 986-994.
28
860
https://doi.org/10.1126/science.253.5023.986
861
Macpherson, C. G., Hilton, D. R., and Hammerschmidt, K. (2010). No slab-derived
862
CO2 in Mariana Trough back-arc basalts: Implications for carbon subduction and
863
for temporary storage of CO2 beneath slow spreading ridges. Geochem. Geophys.
864
Geosyst., 11, Q11007. https://doi.org/10.1029/2010GC003293
865
Manthilake, G., Bolfan-Casanova, N., Novella, D., Mookherjee, M., and Andrault, D.
866
(2016). Dehydration of chlorite explains anomalously high electrical conductivity
867
in
868
https://doi.org/10.1126/sciadv.1501631
the
mantle
wedges.
Advances, 2(5),
Science
e1501631.
869
Martínez, F., Fryer, P., and Becker, N. (2000). Geophysical characteristics of the
870
southern Mariana Trough, 11°50′N-13°40′N. J. Geophys. Res., 105(B7), 16591-
871
16607. https://doi.org/10.1029/2000JB900117
872
873
Martinez, F., and Taylor, B. (2002). Mantle wedge control on back-arc crustal accretion,
Nature, 416, 417-420. https://doi.org/10.1038/416417a
874
Masuda, H., and Fryer, P. (2015). Geochemical characteristics of active backarc basin
875
volcanism at the southern end of the Mariana Trough. In J. Ishibashi et al. (Eds.),
876
Subseafloor Biosphere Linked to Global Hydrothermal Systems; TAIGA Concept
877
(pp. 241-251). Tokyo: Springer Japan. https://doi.org/10.1007/978-4-431-54865-
878
2_21
879
Matsuno, T., Seama, N., and Baba, K. (2007). A study on correction equations for the
880
effect of seafloor topography on ocean bottom magnetotelluric data. Earth Planets
881
Space, 59, 981-986. https://doi.org/10.1016/j.pepi.2007.02.014
882
Matsuno, T., Seama, N., Evans, R. L., Chave, A. D., Baba, K., White, A., Goto, T.,
883
Heinson, G., Boren, G., Yoneda, A., and Utada, H. (2010). Upper mantle electrical
884
resistivity structure beneath the central Mariana subduction system. Geochem.
885
Geophys. Geosyst., 11, Q09003. https://doi.org/10.1029/2010GC003101
886
Matsuno, T., Evans, R. L., Seama, N., and Chave, A. D. (2012). Electromagnetic
887
constraints on a melt region beneath the central Mariana back-arc spreading ridge.
888
Geochem. Geophys. Geosyst., 13, Q10017. https://doi.org/10.1029/2012GC004326
889
Matsuno, T., Chave, A. D., Jones, A. G., Muller, M. R., and Evans, R. L. (2014). Robust
890
magnetotelluric
891
https://doi.org/10.1093/gji/ggt484
inversion.
Geophys.
29
J.
Int.,
196,
1365-1374.
892
McGary, R. S., Evans, R. L., Wannamaker, P. E., Elsenbeck, J., and Rondenay, S. (2014).
893
Pathway from subducting slab to surface for melt and fluids beneath Mount Rainier.
894
Nature, 511, 338-340. https://doi.org/10.1038/nature13493
895
Miller, M. S., Kennett, B. L. N., and Toy, V. G. (2006). Spatial and temporal evolution of
896
the subducting Pacific plate structure along the western Pacific margin. J. Geophys.
897
Res., 111, B02401. https://doi.org/10.1029/2005JB003705
898
Müller, R. D., M. Sdrolias, C. Gaina, and W. R. Roest (2008), Age, spreading rates, and
899
spreading asymmetry of the world’s ocean crust, Geochem. Geophys. Geosyst., 9,
900
Q04006. doi:10.1029/2007GC001743
901
Newman, S., Stolper, E., and Stern, R. (2000). H2O and CO2 in magmas from the Mariana
902
arc and back arc systems. Geochem. Geophys. Geosyst., 1(5), 1013.
903
https://doi.org/10.1029/1999GC000027
904
Nielsen, S. G., and Marschall, H. R. (2017). Geochemical evidence for mélange melting
905
in
906
https://doi.org/10.1126/sciadv.1602402
907
908
global
arcs.
Science
3(4),
Advances,
e1602402.
Nolasco, R., Tarits, P., Filloux, J. H., and Chave, A. D. (1998). Magnetotelluric imaging
of the Society Islands hotspot. J. Geophys. Res., 103(B12), 30287-30309
909
Pearce J. A., Stern, R. J., Bloomer, S. H., and Fryer, P. (2005). Geochemical mapping of
910
the Mariana arc-basin system: Implications for the nature and distribution of
911
subduction
912
https://doi.org/10.1029/2004GC000895
913
components.
Geochem.
Geophys.
Geosyst.,
6,
Q07006.
Pommier, A., Gaillard, F., Pichavant, M., and Scaillet, B. (2008). Laboratory
914
measurements of electrical conductivities of hydrous and dry Mount Vesuvius
915
melts under pressure. J. Geophys. Res., 113, B05205.
916
https://doi.org/10.1029/2007JB005269
917
Reynard, B., Mibe, K., and Van de Moortèleet, B. (2011). Electrical conductivity of the
918
serpentinised mantle and fluid flow in subduction zones. Earth Planet. Sci. Lett.,
919
307, 387-394. https://doi.org/10.1016/j.epsl.2011.05.013
920
Ribeiro, J. M., Stern, R. J., Kelley, K. A., Martinez, F., Ishizuka, O., Manton, W. I., and
921
Ohara, Y. (2013). Nature and distribution of slab-derived fluids and mantle sources
922
beneath the Southeast Mariana forearc rift. Geochem. Geophys. Geosyst., 14.
923
https://doiorg/10.1002/ggge.20244
30
924
Rodi, W., and Mackie, R. L. (2001). Nonlinear conjugate gradients algorithm for 2-D
925
magnetotelluric
926
https://doi.org/10.1190/1.1444893
inversion.
Geophysics,
66,
174-187.
927
Sato, T., Mizuno, M., Takata, H., Yamada, T., Isse, T., Mochizuki, K., Shinohara, M., and
928
Seama, N. (2015). Seismic structure and seismicity in the southern Mariana Trough
929
and their relation to hydrothermal activity. In J. Ishibashi et al. (Eds.), Subseafloor
930
Biosphere Linked to Global Hydrothermal Systems; TAIGA Concept (pp. 241-251).
931
Tokyo: Springer Japan. https://doi.org/10.1007/978-4-431-54865-2_18
932
Schmidt, M. W., and Poli, S. (1998). Experimentally based water budgets for dehydrating
933
slabs and consequences for arc magma generation. Earth Planet. Sci. Lett., 163,
934
361-379. https://doi.org/10.1016/S0012-821X(98)00142-3
935
936
Sdrolias, M., and Müller, R. D. (2006). Controls on back-arc basin formation, Geochem.
Geophys. Geosyst., 7, Q04016. https://doi.org/10.1029/2005GC001090
937
Seama, N., and Okino, K. (2015). Asymmetric seafloor spreading of the southern Mariana
938
Trough back-arc basin. In J. Ishibashi et al. (Eds.), Subseafloor Biosphere Linked
939
to Global Hydrothermal Systems; TAIGA Concept (pp. 241-251). Tokyo: Springer
940
Japan. https://doi.org/10.1007/978-4-431-54865-2_20
941
Seama, N., Sato, H., Nogi, Y., and Okino, K. (2015). The mantle dynamics, the crustal
942
formation, and the hydrothermal activity of the southern Mariana Trough back-arc
943
basin. In J. Ishibashi et al. (Eds.), Subseafloor Biosphere Linked to Global
944
Hydrothermal Systems; TAIGA Concept (pp. 241-251). Tokyo: Springer Japan.
945
https://doi.org/10.1007/978-4-431-54865-2_17
946
Shimizu, H., Yoneda, A., Baba, K., Utada, H., and Palshin, N. A. (2011). Sq effect on the
947
electromagnetic response functions in the period range between 104 and 105 s.
948
Geophys.
949
246X.2011.05036.x
J.
Int.,
186(1),
193-206.
https://doi.org/10.1111/j.1365-
950
Sifré, D., Gardés, E., Massuyeau, M., Hashim, L., Hier-Majumder, S., and Gaillard, F.
951
(2014). Electrical conductivity during incipient melting in the oceanic low-velocity
952
zone. Nature, 509, 81-85. https://doi.org/10.1038/nature13245
953
Stern, R. J., Tamura, Y., Masuda, H., Fryer, P., Martinez, F., Ishizuka, O. and Bloomer, S.
954
H. (2013). How the Mariana Volcanic Arc ends in the south. Island Arc, 22, 133-
955
148. https://doi.org/10.1111/iar.12008
31
956
957
958
959
Tatsumi, Y. (1986). Formation of the volcanic front in subduction zones. Geophys. Res.
Lett., 13(8), 717-720. https://doi.org/ 10.1029/GL013i008p00717
Taylor, B., Martinez, F. (2003). Back-arc basin basalt systematics, Earth Planet. Sci. Lett.,
210, 481-497. https://doi.org/10.1016/S0012-821X(03)00167-5
960
Thebault, E. et al. (2015). International Geomagnetic Reference Field: the 12th
961
generation. Earth Planets Space, 67:79. https://doi.org/10.1186/s40623-015-0228-
962
963
Tyburczy, J. A., and Waff, H. S. (1983). Electrical conductivity of molten basalt and
964
andesite to 25 kilobars pressure: Geophysical significance and implications for
965
charge transport and melt structure, J. Geophys. Res., 88(B3), 2413-2430.
966
https://doi.org/10.1029/JB088iB03p02413
967
Turner, A. J., Katz, R. F., and Behn, M. D. (2015). Grain-size dynamics beneath mid-
968
ocean ridges: Implications for permeability and melt extraction, Geochem. Geophys.
969
Geosyst., 16, 925-946. https://doi.org/10.1002/2014GC005692
970
Usui, Y. (2015). 3-D inversion of magnetotelluric data using unstructured tetrahedral
971
elements: applicability to data affected by topography. Geophys. J. Int., 202(2):
972
828-849. https://doi.org/10.1093/gji/ggv186
973
Usui, Y., T. Kasaya, Y. Ogawa, and H. Iwamoto (2018). Marine magnetotelluric inversion
974
with an unstructured tetrahedral mesh. Geophys. J. Int., 214(2): 952-
975
974. https://doi.org/10.1093/gji/ggy171
976
van Keken, P. E., Hacker, B. R., Syracuse, E. M., and Abers, G. A. (2011). Subduction
977
factory: 4. Depth-dependent flux of H2O from subducting slabs worldwide. J.
978
Geophys. Res., 116, B01401. https://doi.org/10.1029/2010JB007922
979
Wada, I., and Wang, K. (2009). Common depth of slab-mantle decoupling: Reconciling
980
diversity and uniformity of subduction zones. Geochem. Geophys. Geosyst., 10,
981
Q10009. https://doi.org/10.1029/2009GC002570
982
Wada, I., and Behn, M. D. (2015). Focusing of upward fluid migration beneath volcanic
983
arcs: Effect of mineral grain size variation in the mantle wedge. Geochem. Geophys.
984
Geosyst., 16, 3905-3923. https://doi.org/10.1002/2015GC005950
985
Wallace, L. M., R. McCaffrey, J. Beavan, and S. Ellis (2005). Rapid microplate rotations
986
and back-arc rifting at the transition between collision and subduction, Geology, 33,
987
857-860. doi:10.1130/G21834.1
32
988
Wallace, L. M., S. Ellis, and P. Mann (2009). Collisional model for rapid fore-arc block
989
rotations, arc curvature, and episodic back-arc rifting in subduction settings,
990
Geochem. Geophys. Geosyst., 10, Q05001. doi:10.1029/2008GC002220
991
Wang, D., Mookherjee, M., Xu, Y., and Karato, S. (2006). The effect of water on the
992
electrical
993
https://doi.org/10.1038/nature05256
994
995
conductivity
of
olivine.
Nature,
443,
977-980.
Wannamaker, P. E., Hohmann, G. W., and Ward, S. H. (1984). Magnetotelluric responses
of three-dimensional bodies in layered earths. Geophysics, 49, 1517-1533
996
Wessel, P., Smith, W. H. F., Scharroo, R., Luis, J., and Wobbe, F. (2013). Generic Mapping
997
Tools: Improved version released. Eos, trans. AGU, 94(45), 409-420.
998
https://doi.org/10.1002/2013EO450001
999
Wiens, D. A., Kelley, K. A., and Plank, T. (2006). Mantle temperature variations beneath
1000
back-arc spreading center inferred from seismology, petrology, and bathymetry.
1001
Earth Planet. Sci. Lett., 248, 30-42. https://doi.org/10.1016/j.epsl.2006.04.011
1002
Wilson, C. R., Spiegelman, M., van Keken, P. E., and Hacker, B. R. (2014). Fluid flow in
1003
subduction zones: The role of solid rheology and compaction pressure. Earth Planet.
1004
Sci. Lett., 401, 261-274. https://doi.org/10.1016/j.epsl.2014.05.052
1005
Yoshino, T., Matsuzaki, T., Shatskiy, A., and Katsura, T. (2009), The effect of water on
1006
the electrical conductivity of olivine aggregates and its implications for the
1007
electrical structure of the upper mantle. Earth Planet. Sci. Lett., 288, 291-300.
1008
https://doi.org/10.1016/j.epsl.2009.09.032
33
1009
Table
1010
Station
Latitude
Longitude
Water
E-field
Remote B-
ID
(N)
(E)
Depth [m]
EM1
13°19.25’
143°02.80’
3924
Available
EM6
EM2
13°10.92’
143°15.09’
3749
Available
EM10
EM3
13°06.69’
143°21.56’
3567
Available
EM7
EM4
13°02.37’
143°28.05’
3255
EM5
12°58.00’
143°34.53’
3086
EM8
N/A
EM6
12°56.74’
143°36.41’
2868
Available
EM5
EM7
12°55.43’
143°38.18’
3123
Available
EM5
EM8
12°53.47’
143°41.21’
3316
Available
EM5
EM9
12°49.13’
143°47.57’
2569
++
++
EM10
12°45.09’
143°53.96’
3685
Available
N/A
EM11
12°40.82’
144°00.47’
3751
EM10
EM6
field
1011
1012
Table 1
1013
Station information. Station ID is numbered from the northwesternmost station to the
1014
southeasternmost one; see also Figure 1. Latitude and longitude is the location of the ship
1015
at the time of deployment of the instrument, and water depth is derived from the multi-
1016
narrow beam bathymetric data (Kitada et al., 2006). The symbol “+” for EM4 means that
1017
EM field data were obtained by the experiment, but the MT response estimated from the
1018
data had a low squared coherency between the electric field observed and that predicted
1019
from the MT response estimated and the magnetic field observed, and were not used in
1020
the inversion. The symbol “++” for EM9 means that this instrument has not yet been
1021
recovered.
34
1022
Figures
1023
1024
1025
Figure 1
1026
(a) Bathymetric map, which derives from multi-narrow beam data (Kitada et al., 2006)
1027
and the ETOPO1 data (Amante and Eakins, 2009), with depth contours of the surface of
1028
the subducted Pacific slab (colored dotted lines; Hayes et al., 2012) and the location of
1029
the Mariana Trench (light green dotted line; Bird, 2003), as well as ridge centers of the
1030
back-arc spreading in the Mariana Trough (black dash-dotted line; Kitada et al., 2006).
1031
The white box represents the range of the map in Figure 1b, and the range of this map is
1032
shown by the black rectangle in the right-top inset showing the plate boundaries (Bird,
1033
2003). White dots at around 18°N indicate MT stations used for obtaining an electrical
1034
resistivity structure in the central Marianas (Matsuno et al., 2010).
1035
(b) Bathymetric map with marine MT observational stations (symbols). Circles and
1036
crosses indicate locations of magnetic field data and electric field data, respectively. The
1037
colors red, black, and gray for the symbols indicate stations from which the data were
1038
used in the inversion, stations from which data were obtained but not used in inversion,
35
1039
and stations at which the instrument was not recovered, respectively. The station names
1040
are numbered from northwest to southeast (the northwesternmost station is called EM1,
1041
and the southeasternmost one is called EM11); see also Table 1. The abbreviations in this
1042
map are as follows: MGR: Malaguana-Gadau Ridge, PMVC: Patgon-Masala Volcanic
1043
Chain, FNVC: Fina Nagu Volcanic Chain, ASVP: Alphabet Seamount Volcano Province,
1044
WSRBF: West Santa Rosa Bank Fault, SEMFR: Southeast Mariana Forearc Rift (Stern
1045
et al., 2013; Masuda and Fryer, 2015).
36
1046
1047
Figure 2
1048
Apparent resistivities for all four elements and all stations before and after the correction
1049
of topographic distortions (black circle and red diamond, respectively). Error bars show
1050
one standard error of the observations. An annotation for the vertical axis is shown only
1051
in the upper-left-most panel but is common to all the other panels. The station names are
1052
shown in the upper-left corner in the leftmost panels.
37
1053
1054
Figure 3
1055
Phase values for all four elements and all stations before and after the correction of
1056
topographic distortions. The symbols and the error bars are the same as in Figure 2. Note
1057
that ranges of the phase values for off-diagonal elements and diagonal elements are
1058
different. Annotations for the vertical axis are shown only in the top panels but are
1059
common to each MT impedance element panel. The station names are shown in the upper-
1060
left corner in the leftmost panels.
38
1061
1062
Figure 4
1063
(a) RMS misfits and model roughness values for 2-D electrical resistivity models in the
1064
robust inversion processing. The model constraint in the inversion is only model
1065
smoothness. The robust inversion processing was applied two times, and the resulting
1066
values are shown by triangles, squares, and circles for the 0th, 1st, and 2nd robust inversion
1067
runs. At each run, 9 values for the regularization parameter of model smoothness (τs) were
1068
used: 300, 100, 30, 10, 3, 1, 0.3, 0.1, and 0.03. The optimal value of the regularization
1069
parameter is 0.3 for all robust runs, as shown by the filled symbols.
1070
(b) Quantile-quantile plot with 95% confidence limits for the results of the final inversion
1071
(the 2nd run).
39
1072
1073
Figure 5
1074
Optimal 2-D electrical resistivity inversion models (a) with constraints on only model
1075
smoothness and (b) with constraints on model smoothness and allowance for resistivity
1076
jumps surrounding the subducted Pacific slab. The tip of the subducted slab, which was
1077
taken into account for the resistivity jump in Figure 5b, terminates at 200 km depth.
1078
Stations are represented by inverted triangles with numbers near the top of each figure.
1079
Note that the seafloor spreading center is located at 0 km distance, and that the station
1080
located at the spreading center is EM6.
40
1081
1082
Figure 6
1083
TM mode MT responses observed (circles, with error bar representing one standard error)
1084
and predicted from two types of electrical resistivity inversion models (red and blue lines,
1085
which correspond to the Figure 5a model and Figure 5b model, respectively). The two
1086
lines are almost consistent. The station names are shown in the upper-left corner in each
1087
panel. The filled squares seen only in the EM10 response represent outliers that were
1088
excluded from the data set by the robust inversion processing. RMS misfits for each site
1089
and those for each period are tabulated in Tables S1 and S2, respectively, in the supporting
1090
information.
41
1091
1092
Figure 7
1093
Electrical resistivity as a function of temperature, component, and the amount of melt
1094
interconnected in solid phase and water (or hydrogen) dissolved in solid phase or melt.
1095
Comparing this figure and the inversion model (Figure 5) with an assumption for
1096
temperature of a focusing area, the amount of melt and water (or hydrogen) can be
1097
estimated. See details in text.
1098
(a) Electrical resistivity for several types of minerals and materials as a function of
1099
temperature, overlying the resistivity color scale used for drawing the inversion models
1100
in Figure 5. Black solid lines indicate dry olivine (1a: Yoshino et al., 2009; 1b: Gardés et
1101
al., 2014; 1c: Constable et al., 1992; 1d: Constable , 2006). Blue lines indicate wet olivine
1102
(2a and 2a’: Yoshino et al., 2009 for 0.01 wt.% and 0.1 wt.% water, respectively; 2b, 2b’’,
1103
and 2b’: Gardés et al., 2014 for 0.01 wt.%, 0.03 wt.%, and 0.1 wt.% water, respectively;
1104
2c and 2c’: Wang et al., 2006 for 0.01 wt.% and 0.1 wt.% water, respectively). Red line
1105
indicates basaltic melt (3) (Tyburczy and Waff, 1983 for tholeiite melt at 4.3 kbar). Purple
1106
line indicates hydrous basaltic melt with 1 wt.% water (4) (Sifré et al., 2014). For clarity,
1107
the hydrous melt line, 4, is cut at cross-point by the dry silicate melt line, ...