11.2 Neon
Until recently, neon was the most problematical
of the rare gases. Of its three isotopes, 21Ne and 22Ne
are nucleogenic and their variations are well understood. In contrast, 20Ne
is non nucleogenic, and the causes of its variation in the Earth were hotly
debated. However, the resolution of this debate has now made neon isotopes a
kind of ‘Rosetta Stone’ for understanding the behaviour of the other rare gases
in mantle sources.
11.2.1 Neon production
The principal nuclear reactions which generate
neon isotopes are n, " reactions on 24Mg and 25Mg, which produce 21Ne
and 22Ne respectively. Subsidiary pathways are ", n reactions on 18O and 19F
which produce 21Ne and 22Na, the latter undergoing $ decay to 22Ne. The ", n reaction on 17O to
yield 20Ne is unimportant, due to the low abundance of the parent.
All " particles
are derived from the U-series decay chains, while the neutrons are mostly
produced by secondary reactions from " particles.
These
reactions were first studied by Wetherill (1954), and have been refined in
subsequent work (e.g. Kennedy et al.,
1990). The net result of these reactions is to yield a trend towards lower 20Ne/22Ne
and higher 21Ne/22Ne ratios which is most clearly seen in
uranium-rich rocks such as granites. Figure 11.17 shows isotopic data for gas
wells from
Fig. 11.17. Neon three-isotope correlation
diagram showing well gases from the Alberta basin on a mixing line between
atmospheric and nucleogenic neon. After Kennedy et al. (1990).
Isotopic
analysis of exposed terrestrial rocks has also demonstrated the cosmogenic
production of 21Ne (Marty and Craig, 1987). This isotope is produced
by spallation reactions on Mg, Na, Si and Al, generating a sub-horizontal array
on the three-isotope plot. By analysing all three isotopes, the cosmogenic
component can resolved from trapped (magmatic) neon and nucleogenic neon. Graf et al. (1991) applied the cosmogenic
neon method to quartz separates from Antarctic rocks which had previously been
dated by 26Al and 10Be (section 14.6.2). They
demonstrated coherent behaviour of 21Ne with these other cosmogenic
isotopes, suggesting that neon will be a useful tool in determining cosmic
exposure ages of surficial rocks.
11.2.2 Solar neon in the Earth
The first evidence for non-atmospheric neon in
the mantle was presented by Craig and Lupton (1976) from samples of MORB and
volcanic gases. These are enriched in 20Ne, as well as nucleogenic 21Ne,
relative to 22Ne contents. Subsequently, Harding County well gas was
also found to have a composition well removed from atmosphere (Phinney et al., 1978). These 20Ne-enriched
components were attributed to exotic primordial rare gas components in the
Earth, possibly representing solar neon. In contrast, Kyser and Rison (1982)
speculated that 20Ne enrichment in the analysed samples might be due
to mass fractionation of neon from an original mantle composition similar to
that of the atmosphere. They compared a compilation of mantle-derived neon
analyses with neon data from geothermal gases in Japan (Nagao et al., 1979). These gases display a
mass-fractionation trend (Fig. 11.18) which is explained by preferential
diffusion of light neon through the soil to the sampling sites.
Fig. 11.18. Comparison of mantle samples ( ! ), and mass-fractionated geothermal
gases ( " ), on a neon three-isotope diagram. After Kyser and Rison (1982).
Elevated
20Ne abundances were also found in diamonds (Fig. 11.19) by Honda et al. (1987) and Ozima and Zashu (1988;
1991). These analyses disproved the 20Ne ‘enrichment’ model of Kyser
and Rison, since diamonds represent in
situ solid samples of the mantle. Therefore, Ozima and Zashu reversed the
mass fractionation argument of Kyser and Rison, suggesting that diamonds sample
a solar neon reservoir in the Earth, whereas the present-day atmosphere has
been depleted in 20Ne by
mass fractionation. They argued that bombardment of the early Earth by radiation
caused the massive blow-off of a primitive solar-type atmosphere, leaving a
residue enriched in heavy neon.
Fractionation
of the proposed magnitude between mantle and atmosphere should be accompanied
by fractionation of the non-radiogenic isotopes of argon, krypton and xenon.
Therefore, it should be possible to test the atmospheric fractionation model by
isotopic analysis of the heavy rare gases. However, two factors make such tests
difficult to perform. Firstly, the heavier rare gases respond to fractionation
effects to a lesser degree; and secondly, the heavy rare gases are more likely
to be recycled back into the mantle, masking the effect of any
mantle–atmosphere fractionation of such gases. This subject will be re-examined
below.
Fig. 11.19. Neon isotope data for diamonds
compared with the composition of other solar system components. (The solar-wind
composition was determined by analysis of Lunar soil). For data sources, see
text.
Additional
insights into terrestrial neon systematics have been sought from the analysis
of submarine basaltic glasses. Sarda et
al. (1988) demonstrated the existence of a MORB correlation line passing
through the atmosphere point, which has been confirmed by several subsequent
studies (e.g. Marty, 1989; Hiyagon et al.,
1992; Moreira et al., 1998). This
array (Fig. 11.20) can be explained by three-component mixing of solar-type,
atmosphere-type and nucleogenic neon, as discussed below.
Fig. 11.20. Compilation of MORB neon data ( ! ) on a 3-isotope plot. A and B represent
the ‘planetary’ neon compositions seen in some meteorites. After Hiyagon
(1992).
Sarda
et al. (1988) also determined neon
isotope ratios in several Loihi glasses which fell within error of the
atmospheric composition. They believed that these signatures represented a
genuine primordial mantle signature, consistent with this reservoir being the
principal source of atmospheric neon. However, subsequent analyses of submarine
basalt glasses from Loihi and nearby Kilauea revealed a wider range of neon isotope
ratios, stretching from the atmospheric composition towards 20Ne-enriched
compositions (Honda et al., 1991;
Hiyagon et al., 1992). The enriched
end of this array approaches the solar wind composition, but the array has a
slope intermediate between the pure mass-fractionation line and the MORB
correlation line (Fig. 11.21). In order to explain these results, Honda et al. and Hiyagon et al. attributed all neon in the Earth’s interior to mixing
between solar and nucleogenic isotopes. The sloping arrays of MORB and OIB were
then attributed to variable atmospheric contamination of this solar plus
radiogenic mantle neon, whereas the Loihi neon samples originally analysed by
Sarda et al. (1988) were attributed
almost entirely to atmospheric contamination.
Fig. 11.21. Compilation of Hawaiian neon data
on a three-isotope plot. ( " ) = Loihi; ( ! ) = Kilauea. After Hiyagon et al.
(1992).
Allegre
et al. (1993) attempted to reinstate
the ‘planetary model’ for neon in the deep mantle by invoking a new mechanism
to explain high 20Ne/22Ne ratios of solar type in the
earth’s mantle. They attributed these signatures to the subduction of cosmic
dust particles accumulated in deep-sea sediments. These dust particles become implanted
with neon from the solar wind during their exposure in space. Analysis of this
material in the atmosphere and in deep sea sediment reveals 20Ne/22Ne
ratios which span the range between atmospheric and solar compositions (e.g.
Nier and Schlutter, 1990). Matsuda et al.
(1990) suggested that these particles could survive the ‘noble gas subduction
barrier’ and deliver cosmic (solar) neon to the deep mantle. This could explain
the high 20Ne/22Ne ratios of submarine glasses without
having to invoke solar-type primordial neon in the Earth. However, experimental
studies by Hiyagon (1994) suggested that neon would be completely extracted
from cosmic dust within three years at 500 oC, which is insufficient
to sustain this model.
Ozima
and Igarashi (2000) also rejected the ‘solar neon’ model. Their argument was
based on the distribution of data in a histogram of 20Ne/22Ne
ratios from MORB, OIB and diamonds (Fig. 11.22). They argued that since the
distribution tailed away to nothing at the solar wind composition, solar neon
could not be a major component of the terrestrial rare gas inventory. However,
it should be noted that the tailing effect in Fig. 11.23 is mainly due to OIB
data. The MORB distribution is essentially flat, indicating relatively equal
mixing of solar and atmospheric neon in these samples. The distribution of OIB
data in Fig. 11.23 is mainly a historical artefact, representing the great
difficulties encountered in excluding atmospheric contamination in earlier
work. However, improved methods to combat atmospheric contamination have
gradually been developed, as seen in recent data presented by Harrison et al. (1999) while the paper by Ozima
and Igarashi was under revision. These new neon isotope data from
Fig. 11.22. Histogram of neon isotope data for
MORB (hatched); diamonds (stipple) and OIB (clear) to show the distribution of
data between the atmospheric and Solar Wind values. After Ozima and Igarashi
(2000).
Further
evidence from Iceland in support of the Solar Neon model was provided by Dixon et al. (2000) and Moreira et al. (2001). For the first time, these
studies revealed a correlation steeper than the L–K line on the three-isotope
plot, falling within error of the mass fractionation line between atmospheric
and solar neon (Fig. 11.23). This discovery provides important support for the
two-reservoir model for terrestrial noble gases (section 11.1.4), because it
implies that the Earth does contain an essentially primordial neon reservoir.
Fig. 11.23. Neon three-isotope plot showing new
11.2.3 Neon and helium
Following widespread acceptance of the solar
neon model for the Earth, neon and helium isotope data can now be placed in a
unified model. This is because helium does not suffer significant atmospheric
contamination, while atmospheric contamination of neon can be corrected using
the three isotope plot. Relationships between neon and heavy rare gases will be
discussed in the next section.
One
way of correcting for atmospheric neon contamination is to calculate the slopes
of data arrays on the three-isotope plot by forcing a regression line through
the atmosphere composition. The gradient of this regression line is then equal
to the ratio *20Ne/*21Ne. Poreda and Farley (1992) used this notation
to compare the neon compositions of various mantle sources, categorised
according to 3He/4He ratio (expressed as R/RA). The results of this
analysis are presented in Fig. 11.24. In addition to data from Loihi and MORB,
new data were obtained from ultramafic xenoliths from
Fig. 11.24. Correlation of neon and helium
isotope signatures in mantle sources, expressed as histograms of *20Ne/*21Ne, categorised by R/RA ratio.
Different OIB samples are distinguished by hatching. After Poreda and Farley
(1992).
An
alternative way of correcting for atmospheric neon contamination is to project data
away from the atmosphere point to the solar 20Ne/22Ne
ratio, whereupon the neon data are presented as normalised 21Ne/22Ne
ratios. Porcelli and Wasserburg (1995b) used this notation to compare neon and helium
data for depleted mantle, lower mantle plumes, and meteorites (representing the
initial Earth). These reservoirs form an approximately linear growth curve on a
diagram of 21Ne/22Ne against 4He/3He.
This is consistent with the common progenitors U and Th, which produce
radiogenic helium and nucleogenic neon. Porcelli and Wasserburg (1995b) also
argued that the linear Ne–He growth curve is consistent with a steady state
model for mantle rare gases.
The
atmospheric contamination model successfully explains the neon isotope arrays
in submarine glasses, but it brings us back to the problem of explaining the
origin of the atmospheric neon signature itself. Most workers now support the
hypothesis that neon fractionation occurred during the burn-off of an early
terrestrial atmosphere of solar composition (as proposed by Ozima and Zashu,
1988; 1991). This question was re-evaluated by Pepin (1997), who argued that a
giant impact in the early history of the Earth would have fractionated all rare
gas isotope ratios, including those of neon and the heavy rare gases.
Nevertheless, he argued that atmospheric burn-off powered by extreme
ultra-violet solar radiation was still necessary to explain the observed
atmospheric neon signatures. An alternative model proposed by Marty (1989) is
that the atmosphere was formed by late accretion of gas-rich meteorites with
planetary neon (e.g. neon A in Fig. 11.20). These could have been accreted to
the surface of the Earth subsequent to the formation of the mantle with a solar
neon budget.
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