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2 of the uppermost valence band (UVB) and the lowermost conduction band (LCB) in bulk and atomically t
3 lated that their ultimate destination is the lowermost few hundred kilometres of the mantle, known as
5 iple, piecewise continuous interfaces in the lowermost layer (D'') beneath Central and North America.
8 ents in a low-shear-velocity province in the lowermost mantle (D'' region) beneath the central Pacifi
9 ogical and electromagnetic properties of the lowermost mantle (D'') is important to understand the fo
10 ser than the surrounding solid phases in the lowermost mantle and that melts will be trapped above th
11 erential travel times of phases sensitive to lowermost mantle beneath the central Pacific reveals lat
13 ompositional variation should strengthen the lowermost mantle between 1,800 km depth and 2,000 km dep
17 gical observations provide evidence that the lowermost mantle contains superposed thermal and composi
18 modeling suggests a sharp transition in the lowermost mantle from a broad slow region to a broad fas
19 o-called ScS and SKKS waves, which probe the lowermost mantle from above and below, respectively, rev
22 tanding deformation of mineral phases in the lowermost mantle is important for interpreting seismic a
25 Seismic anomalies in the outer core and the lowermost mantle may be due to magnetic collapse of ferr
27 e perovskite (Pv) to postperovskite (pPv) at lowermost mantle pressure-temperature (P - T) conditions
31 ase to explain the seismic properties of the lowermost mantle through coupled ab initio and seismic m
33 decouple the mantle above 2,000 km from the lowermost mantle, and provide a rheological basis for th
34 ation for laterally varying viscosity in the lowermost mantle, as required by long-period geoid model
35 he basaltic materials are accumulated at the lowermost mantle, high electrical conductivity of these
36 estabilize high-temperature anomalies in the lowermost mantle, in disagreement with the seismic obser
38 compositions) at the P - T conditions of the lowermost mantle, searching for candidate rocks with a s
40 uated to reveal the thermal structure of the lowermost mantle, where no phase transitions were previo
41 and seismologically distinct regions of the lowermost mantle, which may organize global mantle flow
55 ix well-resolved plumes that extend into the lowermost mantle: Ascension, Azores, Canary, Easter, Sam
56 the uppermost mantle or lithosphere and the lowermost-mantle analogue of the lithosphere, the D" reg
62 ing associated with volcanic aerosols in the lowermost stratosphere (LMS) had not been considered.
63 approximately 50 kilometers, descend to the lowermost stratosphere and are followed by anomalous tro
64 from persistent circulation anomalies in the lowermost stratosphere and is greatest during boreal win
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