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1 MORBs generally exhibit a relatively low and narrow rang
2 MORBs vary in their abundances of incompatible elements
3 primitive magmas outgassed volatiles with a MORB-like helium isotopic signature ((3)He/(4)He ratio);
4 r the formation of the Solar System, OIB and MORB mantle sources must have differentiated by 4.45 bil
5 opic compositions of abyssal peridotites and MORB do not appear to be in equilibrium, raising questio
6 mixing between subducted atmospheric Xe and MORB Xe, which obviates the need for a less degassed dee
8 s lower than that of mid-ocean ridge basalt (MORB) and comparable to the ultramobile pure carbonate m
9 tection of subducted mid-ocean ridge basalt (MORB) in the lower mantle is hindered by uncertainties i
10 re more oxidized than midocean ridge basalt (MORB) magmas, suggesting that the upper mantle sources o
11 wstone compared with mid-ocean ridge basalt (MORB) samples, this confirms that the deep plume and sha
13 otope variations in mid-ocean ridge basalts (MORB) are commonly attributed to compositional variation
14 more oxidized than mid-ocean ridge basalts (MORB), but it is debated whether this is a mantle featur
15 ces in the depleted mid-ocean ridge basalts (MORB)-source mantle, the enriched ocean island basalts (
18 differences between mid-ocean ridge basalts (MORBs) and ocean island basalts (OIBs) provide critical
20 d isotope space for mid-ocean ridge basalts (MORBs) converge on a single end-member component that ha
21 We also find that mid-ocean-ridge basalts (MORBs) have (238)U/(235)U ratios higher than does the bu
22 OIBs) compared with mid-ocean-ridge basalts (MORBs) have been used as evidence for the existence of a
23 y uniform values in mid-ocean-ridge basalts (MORBs), are thought to result from a well mixed upper-ma
28 he rheniumosmium isotope system, constituent MORB phases are shown to possess exceptionally high Re/O
30 lt from a well mixed upper-mantle source for MORB and a distinct deeper-mantle source for ocean islan
33 ange of noble-gas concentrations observed in MORB and OIB glasses, can self-consistently be explained
34 ow that a higher CO2 content in OIBs than in MORBs leads to more extensive degassing of helium in OIB
36 the first time that the inflow of the Indian MORB-type mantle has reached the southern tip of tectoni
39 that observed in OIBs worldwide and indicate MORB-like (3)He/(4)He ratios in OIBs cannot be used to p
41 tinct material, but do not account for lower MORB-like (3)He/(4)He ratios in OIBs, nor their observed
42 has led to a volatile-depleted upper mantle (MORB source) with low 3He concentrations and low 3He/4He
43 chondritic before 3.5 Ga and evolved to a N-MORB-like composition between approximately 3.5 and 2.7
44 +/- 0.006 per mille offset between BSE and N-MORBs requires that <30% of Earth's mantle equilibrated
46 i/(47)Ti ratios ranging from chondritic to N-MORBs compositions, indicating continuing disruption of
47 model basalt, hydrous model basalt and near-MORB to assess the effects of iron and water on the melt
48 ontrast, the uranium isotopic composition of MORB requires the convective stirring of recycled uraniu
49 reases its fO(2), and that the uniformity of MORB fO(2)s is a consequence of the melting process and
50 ope and incompatible-element geochemistry of MORBs by a component of recycled crust that is variably
52 Compositional variations in the sources of MORBs could reflect recycling of subducted crustal mater
53 of mantle melts (mid-ocean ridge basalts, or MORBs) and their presumed mantle sources (abyssal perido
55 his confirms that the deep plume and shallow MORB mantles have remained distinct from one another for
57 ng the plume source to be less degassed than MORBs, a conclusion that is independent of noble gas con
62 ingly, estimates of the H(2)O content of the MORB mantle source based on H(2)O in abyssal peridotites