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2 his relationship, we focused analyses on the lowermost 500 kilometers of the Mississippi River, where
4 of the uppermost valence band (UVB) and the lowermost conduction band (LCB) in bulk and atomically t
6 ly thinned high-velocity (Vp ~ 7.3-7.4 km/s) lowermost crust, which extends over >350 km distance.
8 (50-70%) transformation of part of the mafic lowermost crustal layer into eclogite facies during Pale
10 lated that their ultimate destination is the lowermost few hundred kilometres of the mantle, known as
12 'interglacial period'(1,3) during which the lowermost latitude LDM ice(4-6) was etched and removed,
13 iple, piecewise continuous interfaces in the lowermost layer (D'') beneath Central and North America.
16 ents in a low-shear-velocity province in the lowermost mantle (D'' region) beneath the central Pacifi
17 ogical and electromagnetic properties of the lowermost mantle (D'') is important to understand the fo
18 ser than the surrounding solid phases in the lowermost mantle and that melts will be trapped above th
19 Low Shear Velocity Provinces (LLSVPs) in the lowermost mantle are key to understanding the chemical c
20 erential travel times of phases sensitive to lowermost mantle beneath the central Pacific reveals lat
22 ompositional variation should strengthen the lowermost mantle between 1,800 km depth and 2,000 km dep
26 gical observations provide evidence that the lowermost mantle contains superposed thermal and composi
27 modeling suggests a sharp transition in the lowermost mantle from a broad slow region to a broad fas
28 o-called ScS and SKKS waves, which probe the lowermost mantle from above and below, respectively, rev
31 tanding deformation of mineral phases in the lowermost mantle is important for interpreting seismic a
34 Seismic anomalies in the outer core and the lowermost mantle may be due to magnetic collapse of ferr
37 calized material flows and the region of the lowermost mantle possesses a separate layer circulation.
38 e perovskite (Pv) to postperovskite (pPv) at lowermost mantle pressure-temperature (P - T) conditions
43 ase to explain the seismic properties of the lowermost mantle through coupled ab initio and seismic m
47 decouple the mantle above 2,000 km from the lowermost mantle, and provide a rheological basis for th
48 ation for laterally varying viscosity in the lowermost mantle, as required by long-period geoid model
49 he basaltic materials are accumulated at the lowermost mantle, high electrical conductivity of these
50 estabilize high-temperature anomalies in the lowermost mantle, in disagreement with the seismic obser
52 compositions) at the P - T conditions of the lowermost mantle, searching for candidate rocks with a s
54 MgCO(3) under reducing conditions of Earth's lowermost mantle, these observations allow us to predict
55 uated to reveal the thermal structure of the lowermost mantle, where no phase transitions were previo
56 and seismologically distinct regions of the lowermost mantle, which may organize global mantle flow
57 to monitor dynamic processes in the Earth's lowermost mantle, yet no related seismic observations we
73 s of decadal-scale structural changes in the lowermost mantle: (1) a 10s km-scale shrinkage or moveme
74 ix well-resolved plumes that extend into the lowermost mantle: Ascension, Azores, Canary, Easter, Sam
75 the uppermost mantle or lithosphere and the lowermost-mantle analogue of the lithosphere, the D" reg
77 g that BMO fractional crystallization yields lowermost-mantle densities much higher than those of LLV
87 ing associated with volcanic aerosols in the lowermost stratosphere (LMS) had not been considered.
88 approximately 50 kilometers, descend to the lowermost stratosphere and are followed by anomalous tro
89 from persistent circulation anomalies in the lowermost stratosphere and is greatest during boreal win
93 experiment and inter-model variability that lowermost stratospheric water vapor decreases local temp