TY - JOUR
T1 - Ages and magnetic structures of the South China Sea constrained by deep tow magnetic surveys and IODP Expedition 349
AU - Li, Chun Feng
AU - Xu, Xing
AU - Lin, Jian
AU - Sun, Zhen
AU - Zhu, Jian
AU - Yao, Yongjian
AU - Zhao, Xixi
AU - Liu, Qingsong
AU - Kulhanek, Denise K.
AU - Wang, Jian
AU - Song, Taoran
AU - Zhao, Junfeng
AU - Qiu, Ning
AU - Guan, Yongxian
AU - Zhou, Zhiyuan
AU - Williams, Trevor
AU - Bao, Rui
AU - Briais, Anne
AU - Brown, Elizabeth A.
AU - Chen, Yifeng
AU - Clift, Peter D.
AU - Colwell, Frederick S.
AU - Dadd, Kelsie A.
AU - Ding, Weiwei
AU - Almeida, Iván Hernández
AU - Huang, Xiao Long
AU - Hyun, Sangmin
AU - Jiang, Tao
AU - Koppers, Anthony A.P.
AU - Li, Qianyu
AU - Liu, Chuanlian
AU - Liu, Zhifei
AU - Nagai, Renata H.
AU - Peleo-Alampay, Alyssa
AU - Su, Xin
AU - Tejada, Maria Luisa G.
AU - Trinh, Hai Son
AU - Yeh, Yi Ching
AU - Zhang, Chuanlun
AU - Zhang, Fan
AU - Zhang, Guo Liang
N1 - Publisher Copyright:
© 2014. American Geophysical Union. All Rights Reserved.
PY - 2014/12/1
Y1 - 2014/12/1
N2 - Combined analyses of deep tow magnetic anomalies and International Ocean Discovery Program Expedition 349 cores show that initial seafloor spreading started around 33 Ma in the northeastern South China Sea (SCS), but varied slightly by 1-2 Myr along the northern continent-ocean boundary (COB). A southward ridge jump of ∼20 km occurred around 23.6 Ma in the East Subbasin; this timing also slightly varied along the ridge and was coeval to the onset of seafloor spreading in the Southwest Subbasin, which propagated for about 400 km southwestward from ∼23.6 to ∼21.5 Ma. The terminal age of seafloor spreading is ∼15 Ma in the East Subbasin and ∼16 Ma in the Southwest Subbasin. The full spreading rate in the East Subbasin varied largely from ∼20 to ∼80 km/Myr, but mostly decreased with time except for the period between ∼26.0 Ma and the ridge jump (∼23.6 Ma), within which the rate was the fastest at ∼70 km/Myr on average. The spreading rates are not correlated, in most cases, to magnetic anomaly amplitudes that reflect basement magnetization contrasts. Shipboard magnetic measurements reveal at least one magnetic reversal in the top 100 m of basaltic layers, in addition to large vertical intensity variations. These complexities are caused by late-stage lava flows that are magnetized in a different polarity from the primary basaltic layer emplaced during the main phase of crustal accretion. Deep tow magnetic modeling also reveals this smearing in basement magnetizations by incorporating a contamination coefficient of 0.5, which partly alleviates the problem of assuming a magnetic blocking model of constant thickness and uniform magnetization. The primary contribution to magnetic anomalies of the SCS is not in the top 100 m of the igneous basement.
AB - Combined analyses of deep tow magnetic anomalies and International Ocean Discovery Program Expedition 349 cores show that initial seafloor spreading started around 33 Ma in the northeastern South China Sea (SCS), but varied slightly by 1-2 Myr along the northern continent-ocean boundary (COB). A southward ridge jump of ∼20 km occurred around 23.6 Ma in the East Subbasin; this timing also slightly varied along the ridge and was coeval to the onset of seafloor spreading in the Southwest Subbasin, which propagated for about 400 km southwestward from ∼23.6 to ∼21.5 Ma. The terminal age of seafloor spreading is ∼15 Ma in the East Subbasin and ∼16 Ma in the Southwest Subbasin. The full spreading rate in the East Subbasin varied largely from ∼20 to ∼80 km/Myr, but mostly decreased with time except for the period between ∼26.0 Ma and the ridge jump (∼23.6 Ma), within which the rate was the fastest at ∼70 km/Myr on average. The spreading rates are not correlated, in most cases, to magnetic anomaly amplitudes that reflect basement magnetization contrasts. Shipboard magnetic measurements reveal at least one magnetic reversal in the top 100 m of basaltic layers, in addition to large vertical intensity variations. These complexities are caused by late-stage lava flows that are magnetized in a different polarity from the primary basaltic layer emplaced during the main phase of crustal accretion. Deep tow magnetic modeling also reveals this smearing in basement magnetizations by incorporating a contamination coefficient of 0.5, which partly alleviates the problem of assuming a magnetic blocking model of constant thickness and uniform magnetization. The primary contribution to magnetic anomalies of the SCS is not in the top 100 m of the igneous basement.
KW - International Ocean Discovery Program Expedition 349
KW - South China Sea tectonics
KW - crustal evolution
KW - deep tow magnetic survey
KW - magnetic anomaly
KW - modeling
UR - http://www.scopus.com/inward/record.url?scp=84983508821&partnerID=8YFLogxK
U2 - 10.1002/2014GC005567
DO - 10.1002/2014GC005567
M3 - 期刊論文
AN - SCOPUS:84983508821
SN - 1525-2027
VL - 15
SP - 4958
EP - 4983
JO - Geochemistry, Geophysics, Geosystems
JF - Geochemistry, Geophysics, Geosystems
IS - 12
ER -