The problem of the origin of the upper-mantle Xe is discussed and a st
raightforward model of lower- and upper-mantle mass exchange is presen
ted. The upper-mantle Xe isotope composition is assumed to be that mea
sured in continental CO2 gases. This assumption is supported by a regr
ession analysis of isotope compositions of Xe in MORB glasses. The pos
sibility is investigated that the lower mantle contains Xe isotope abu
ndances that are similar to unfractionated solar Xe, as now appears to
be the case for both He and Ne. Abundances of the heavy isotopes in u
nfractionated Xe are relatively lower than in air Xe. A mixture of the
unfractionated Xe with plutogenic Xe-131-136(Pu) may yield Xe with re
lative abundances of heavy Xe isotopes similar to atmospheric Xe. This
makes Xe(Pu) invisible in so far as air Xe is used as a reference com
position. The abundance of Xe-131-136, solar-like Xe-130, and I-129-d
erived Xe-129 in mantle Xe are used to derive concentrations of fissi
on plutogenic these components in the lower mantle. A steady-state ass
umption for highly incompatible elements in the upper mantle with resi
dence times of 1 Ga is used to estimate the concentration of uranogeni
c fission Xe(U) Xe-136(U)/Xe-129(I)=0.357, inferred from Xe-136/Xe-130
-Xe-129/Xe-130 correlation for mantle-derived samples, allow a lower m
antle-upper mantle mass flux to be estimated. This flux is within the
range from 0.05 . 10(13) to 1.2 . 10(13) kg/a, the upper limit being s
imilar to independent estimates from U-He-Ne systematics. It is, howev
er, by two orders of magnitude lower than the present-day mass flux of
subducted slab.