|
The
European Cenozoic Volcanic Province is
not caused by mantle plumes |
Romain Meyer1 & Gillian R. Foulger2
1Afd.
Geologie, Katholieke Universiteit Leuven,
Celestijnenlaan 200E , B-3001 Leuven, Belgium, mail@romain-meyer.eu
2Durham University, Durham DH1 3LE,
UK, g.r.foulger@durham.ac.uk
Click here to
download a PDF version of this webpage
Abstract
The European Cenozoic Volcanic
Province (ECVP) comprises several small volcanic
areas. Its formation is often genetically linked
to one or several mantle plumes, but there is no
convincing evidence for this. The primary observations
from the ECVP contradict every prediction of the
classical plume hypothesis and require major adaptations
of that model to explain them. The mantle
plume model thus is not an acceptable explanation
for ECVP formation. A more likely explanation
is that the volcanism is related to Alpine subduction
processes that affect stress, deformation and
flow in the European continental crust and underlying
shallow mantle, coupled with the influence of local
lithospheric conditions.
1. Introduction
The current geodynamic setting of
Central and Western Europe is dominated by the continental
collision of the European and the Adriatic plates during
the Alpine orogenesis. In the northern Alpine forelands
extensive lithospheric rift systems developed (e.g.,
Ziegler,
1990), closely linked both spatially and temporally
to the Alpine orogeny. Sedimentary basins developed
under extensional conditions in central Europe, and
their formation was accompanied locally by melt intrusion
and extrusion (Figure
1). The main graben structure, the NNE–SSW trending
Rhine graben, is essentially amagmatic with the exception
of Kaiserstuhl volcano in its southern part (Wilson & Downes,
1991). Magmas extend
over France (the Massif Central), central Germany (Eifel,
Westerwald, Vogelsberg, Rhön), the Czech Republic
(the Eger graben) and SW Poland (Lower Silesia), a
region ~1,200 km wide. This volcanic region is called
the European Cenozoic Volcanic Province (ECVP) in this
webpage.
Figure 1: Map of the
Cenozoic volcanic rocks of central Europe (green)
and rift-related sedimentary basins (red) in the
Alpine foreland. Volcanic sub-areas: S: Siebengebirge;
W: Westerwald; HD: Hessian Depression; R: Rhön/Heldburg;
UP: Upper Palatinate; DH: Doupovské Hory;
CS: Českè Středohoři;
LS: Lower Silesia. Rift systems: LG: Limagne
Graben; BG: Bresse Graben; URG: Upper Rhine Graben;
LRG: Lower Rhine (Roer Valley) Graben; HG: Hessian
grabens; EG: Eger (Ore) Graben. Age data from
Abratis
et al. (in press), Lustrino & Wilson
(2007) and references
therein.
The predominantly intraplate
magmatism of the ECVP has been attributed by different
authors to a variety of causes (e.g.,
Lustrino & Carminati,
2007, and references therein). These include one
or more mantle plumes and a partial melt layer representing
a “fossil
plume head” from which small plumes (also termed “baby
plumes” or “finger plumes”) rise.
Nevertheless, the province has essentially none of
the characteristics expected for classical Morgan-type
mantle plumes (Morgan,
1971). A source related
to Alpine subduction processes coupled with local lithospheric
conditions offers a much less astonishing explanation
for European Cenozoic volcanism than do mantle plumes.
Some primary observations from the ECVP are:
- The area covered with volcanic rocks is much too
small to be classified as a Large Igneous Province
(LIP);
- The spatial distribution of volcanism is not time-progressive;
- Some of the volcanic fields are located close
to Cenozoic rift systems (e.g., Kaiserstuhl, Vogelsberg),
whereas others are located on uplifted basement
massifs (e.g., the Westerwald, Eifel and Auvergne);
- The time-scale of uplift and volcanism is not what
is predicted by the mantle plume model;
- At least two different mantle xenolith types in
host magmas show that the subcontinental mantle of
the ECVP is heterogeneous. In general, ECVP magmas
have trace-element and isotopic characteristics that
resemble closely ocean-island basalts (OIB);
- 3He/4He ratios are homogeneous
(R/Ra = 6.32 ± 0.39;
Gautheron et al.,
2005) and lower than MORB values
(8 ± 1 Ra; Allègre
et al.,
1995);
- No high-Mg (picritic) magmas, often assumed to
indicate excess temperatures in the mantle, are reported,
and;
- Low-wave-speed seismic mantle anomalies are detected
beneath some, but not all, sub-areas. Where they
are observed, they are confined to the upper mantle.
These eight points are discussed in sequence and in
detail in Section 3 below.
2. Tectonic setting
The developing Alps and Pyrenees exerted
compressional stresses on the European plate during
the Paleocene and caused lithospheric buckling and
basin inversion out to distances of up to 1700 km north
of the Pyrenean and Alpine deformation fronts (Dèzes
et al., 2004).
This buckling was accompanied locally by the injection
of mafic melts into the European foreland crust. The
Paleogene geodynamic history of the Alpine orogen was
dominated by the subduction of the continental Briançonnais
block subduction after subduction of the South Penninic
Ocean was complete (well summarized by Schmid
et al., 1996).
At the end of the Early Eocene the whole Briançonnais
zone, along with major parts of the North Penninic
Bündnerschiefer/Valais “ocean”, were
subducted. The following initial continent-continent
collision stage (Early Eocene, Ypresian to Oligocene,
Rupelian) is defined by the subduction of the Adula
nappe–the southern, distal margin of
the continent of Europe (Schmid
et al., 1996).
During the middle Eocene, the European
Cenozoic Rift System (ECRIS) began to form as a result
of the north-directed intraplate compressional stresses
that resulted from the processes described above. In
the north, the ECRIS is represented by the Rhine rift
system which comprises the northward-trending Upper
Rhine and Hessian (Wetterau, Leine) grabens and the
northwest-striking Roer Valley (Lower Rhine) graben.
The southern branch of the ECRIS includes the grabens
of the Massif Central (Limagne, Forez, Roanne) and
the Bresse Graben (Ziegler
& Dèzes,
2005; 2007 ). The northern and southern rift systems
are thought to involve tensional reactivation of Late
Hercynian fractures (Ziegler, 1992).
Tectonic events associated with
Alpine orogeny, which were important for ECVP magmatism
occurred during the Eocene-Oligocene transition. Major
parts of the Penninic units, including oceanic crust,
Briançonnais,
and distal European crust were subducted (Schmid
et al., 1996).
The European upper continental crust was accreted to
the orogenic wedge after the Eocene collision. This
excessively thickened the orogenic wedge whilst the
detached lower crust of the European foreland was subducted
from 36 Ma onward (P.A. Ziegler, pers. comm.). Around
34 Ma the subducting slab of the central Alps, comprising
the lower crust and the lithospheric mantle of the
distal European margin and the Briançonnais
and the lithosphere of the Valais and Penninic oceans,
broke off from the European foreland lithosphere (Dèzes
et al., 2004, 2005). Slab
break-off and tearing scenarios have also been described
for Anatolia and
Mexico.
3. Features
of the ECVP important to source models
3.1 The size of the ECVP
The ECVP covers a maximum total area
of 20,000 km2. This is much smaller than
the minimum areas of 50,000 km2 or 100,000
km2 that
have been suggested for LIPs.
Lava thicknesses and volumes are also small. LIPs such
as the North Atlantic
Igneous Province and the Deccan flood
basalts have thicknesses of several to many kilometres.
Volcanism in the ECVP, on the other hand, is characterized
by small, monogenetic centres (e.g., Eifel),
scattered necks and plugs (e.g., the Hessian
Depression), dykes (e.g., the Rhön/Heldburg
area) and a few central volcano complexes (e.g.,
Cantal and Vogelsberg). The sizes
of the different regions vary from large central volcano
systems (e.g., Vogelsberg–ca. 2500 km2)
to small isolated plugs.
3.2 Spatial and temporal patterns
One of the most important mantle plume
model predictions, time-progressive volcanism, is violated
in the ECVP. The volcanics are mainly restricted to
a belt 300 km wide surrounding the northern Alps. A
space-time correlation between the igneous sub-areas,
that might indicate a plume track, does not exist.
For example, magmatic activity in the Eger Graben and
the Eifel area started in the Eocene (in the Massif
Central, Vosges-Black Forest and Bohemian Massif even
as early as the Paleocene), but the major phase of
activity in western and central Europe occurred only
in the Neogene. Along with intervals of low activity,
eruptions continued locally to a few thousand years
BP, despite paleogeographic reconstructions that show
that activity in these areas started when they were
approximately 1000 km south of their present positions
(Torsvik
et al.,
2001). This cannot
be explained by one or more relatively stationary mantle
plumes, but suggests a phenomenon that traveled
with the lithosphere.
Volcanic activity ceased in some sub-areas,
whereas it continued or started in others with
the same chemistry (e.g., Abratis
et al.,
in press). An excellent example of this “jumping” of
activity is the area around the Vogelsberg (Figure
2). Volcanic activity ceased at 18 Ma in the Rhön
area whereas it continued in the Vogelsberg and in
the northern Hessian Depression in the WNW, and started
in the Grabfeld, farther SE, at 16 Ma. At present,
geologically recent magmatic activity as well as the
oldest igneous ECVP rocks (Paleogene), occur at both
the W and E ends of the ECVP.
Figure 2: Simplified geological
map of central Germany showing the ECVP sub-areas
Vogelsberg, Rhön and Heldburg Gangschar. Volcanics
and dykes are indicated by black coloured fields.
Age data from Abratis
et al. (in press) and references
therein.
3.3 Tectonic setting of the volcanic fields
ECVP eruptions occurred in two major
tectonic settings:
- the European Cenozoic Rift System,
and
- uplifted Variscan basement massifs (the Massif
Central, Rhenish Massif and Bohemian Massif).
Magmas
erupted in a volcanic belt from the French Massif
Central, through central Germany (Eifel, Westerwald,
Vogelsberg, Rhön),
to the Eger graben and SW Poland (Figure 1). This
belt runs perpendicular to the post-Alpine NNE-SSW
rift system of the Upper Rhine graben (Ziegler,
1992). The volcanic complex of the Vogelsberg is
located at the northern end of the Rhine Graben where
it splits into two branches. Other volcanic
fields associated with the Cenozoic rift systems
are the Eger graben and Hessian depression volcanic
areas. Examples of volcanic areas associated with
uplifted basement massifs are the Westerwald,
Eifel and the Massif Central.
In general, the sub-provinces on uplifted
areas have been linked to arriving mantle plumes
(e.g.,
Granet
et al., 1995; Ritter
et al.,
2001). However other European
coeval uplifted massifs show no Cenozoic magmatic activity
(see Section 3.4).
The volcanic areas close to or within
the Cenozoic rift systems are clearly the result of
decompression melting processes due crustal extension.
On the other hand the Vogelsberg, situated at the triple
junction of the Upper Rhine Graben and the Hessian
grabens (Figure 1), has often been used as a textbook
example of a triple junction caused by the impact of
a mantle plume on the base of the lithosphere. It has
been suggested that the large volume of igneous material
at the Vogelsberg requires high mantle temperatures.
However, source temperatures higher than for other
ECVP sub-areas are not required for these (presumably)
higher melt fractions and volumes. Petrogenetically,
three different possible scenarios could result in
melting:
- Higher
temperatures;
- Decreasing pressure; and
- Changes in volatile content.
Lithosphere stretching and
thinning, coupled with consequentially induced local,
small-scale convection at this triple junction, negates
the need for high temperatures.
3.4 Vertical motions
Plume models predict uplift of the
surface prior to arrival of a plume head (Campbell,
2005). A maximum
elevation of ~500-1000 m is predicted for a temperature
anomaly of ~100°C. Uplift is expected to be
followed by subsidence as the plume head spreads beneath
the lithosphere, and the impingement site is transported
away from the plume stem. The lithosphere is expected
to stretch above the arriving plume. Vertical movements
associated with plume impingement are predicted to
place the lithosphere under stress, and zones of compression
and extension are predicted to result above the plume
head (Burov & Guillou-Frottier,
2005). Whether the resulting rift zones are expected
to be elongated, as in the ECRIS and its perpendicular
ECVP, is unknown.
The ECRIS is characterized by relatively
low crustal stretching factors (Cloetingh
et al.,
2005), hardly reaching values of 1.15 in the deepest
and narrowest parts of the Upper Rhine Graben (Dèzes
et al.,
2004; Ziegler & Dèzes, 2007), but
with a distinct uplift of the crust–mantle boundary.
Basement uplift in the ECVP area started during the
Neogene (e.g., the Massif Central: Early Miocene;
Vosges-Black Forest Arch: Middle Miocene)
extending over a period of ~20 Ma (Ziegler,
1990; 1992), which is 20 to 40 Ma after the beginning
of rifting (Ziegler, 1992). Stratigraphic
observations show that the Rhenish Massif, Eifel, and
the Massif Central were still close to sea level during
the Oligocene (Ziegler & Dèzes,
2005 and references therein) when volcanism had
already commenced. These areas were mainly uplifted
later, commencing during the Middle Miocene (Ziegler
& Dèzes, 2007).
Volcanic activity appears
to have been synchronous with the Late Oligocene minor
uplift of the Rhenish Massif (Meyer
et al., 1983).
During the Miocene, the Roer Valley graben continued
to subside due to the NW-directed compressional stress
field (Schumacher,
2002), in contrast with the
Rhenish Massif. This included the Hessian grabens,
which were gradually uplifted and became the site of
increased volcanic activity (e.g., Jung, 1999).
This can be related to progressive thinning of the
mantle lithosphere, and the related induction of small-scale
convection. The Bohemian Massif experienced a major
phase of volcanism during the Early and Middle Oligocene
which was succeeded by subsidence of the NE-striking
Eger Graben (e.g.,
Ulrych
et al.,
1999). It is beneath
this region that seismic imaging recently failed to
detect a plume-like structure in the mantle (Plomerová et
al.,
2007).
An additional observation relevant
to vertical movements in central Europe is that many
volcanic constructions were strongly eroded (e.g.,
Bücking, 1916) after
volcanic activity ceased. This suggests that uplift
still continued after the volcanic activity. Meyer
et al. (1983) concluded that uplift
in the western Rhenish Massif accelerated during the
Quaternary while volcanic activity resumed in Eifel
(0.7-0.01 Ma). Vertical movement continues to the present-day
(see Meyer & Stets, 2002; van
Balen et al., 2000
in Ziegler & Dèzes, 2007).
It is also interesting to note that
the uplifted Armorican Massif (NW France) and the Belgian
Ardennes have no volcanic activity at all. Clearly
uplift in the Alpine foreland has a complex history
and pattern and cannot simplistically be explained
by one or more mantle plumes. For more discussion of
uplift mechanism, see Ziegler & Dèzes (2007).
3.5 Petrogenesis
3.5.1 Rock types and melt fractions
In the ECVP basanites, nephelinites,
and alkali basalts dominate over tholeiitic basalts
(olivine to quartz; Figure 3). The higher partial melting
degrees presumed for the tholeiitic basalts (~10%; Meyer
et al., 2002)
compared with alkali basalts (2-3%; Meyer
et al., 2002)
cannot automatically be attributed to an abnormally
hot mantle. In a high-temperature mantle plume scenario,
a relationship in space and time between the alkaline
and tholeiitic melts would be expected. Abratis
et al. (in
press) conclude, however, that the different
magmas erupted more or less simultaneously within sub-areas.
The magmas furthermore erupted continually in the same
small area of crust over millions of years on a moving
plate. The higher partial melting degrees thus seem
to be more easily explained by fertility heterogeneities
in the source.
Figure 3: Total alkali–silica
(TAS) diagram which outlines the compositional variability
of ECVP rocks. The corresponding geochemical data are
published in Lustrino & Wilson
(2007) in addition
to some personal (RM) unpublished data.
3.5.2 Mantle heterogeneity
Mantle homogeneity beneath a volcanic area can only
be directly studied using mantle xenoliths (e.g., Meyer & Hertogen,
2007). Two distinct suites of spinel peridotites (Stosch,
1987) found in mantle xenoliths from the ECVP testify
to a heterogeneous mantle:
- A high-temperature anhydrous suite–the
coarse-grained, high-T anhydrous Ib type. This
suite is characterized by the absence of hydrous
minerals. The texture of these xenoliths shows
a uniform grain size, suggesting that they formed
in the lithosphere under constant P-T conditions
over millions of years. They are spinel
harzburgite and olivine clinopyroxenites (Witt-Eickschen,
1993). The pyroxenites are also indicators
of a heterogeneous mantle, since they most likely
represent veins in the lherzolitic lithospheric
mantle (Witt-Eickschen & Kramm, 1998).
Geochemically these xenoliths range from REE chondritic
to moderately LREE depleted lherzolites, to
moderately LREE enriched harzburgites;
- A low-temperature hydrous suite–the tabular-mosaic
hydrous Ia type. These xenoliths contain pargasitic
amphibole in addition to olivine, orthopyroxene,
clinopyroxene, spinel and the breakdown products
of spinel. The hydrous Ia xenoliths show strong
enrichment of LREE and other incompatible elements
(Schmidt
et al.,
2003).
Based on P-T data it has been postulated
that the amphibole-bearing xenoliths came from just
below the Moho, and that the anhydrous
xenoliths came from greater depths. Following the earlier
ideas of Sleep (1984) and Fitton & Dunlop (1985),
a heterogeneous mantle containing lherzolite layers
with layers/veins of subducted eclogitic material has
been suggested, and termed “marble cake” mantle,
by Allègre & Turcotte (1986).
3.5.3 The OIB paradox,
and an asthenospheric or lithospheric source
The origin of intraplate magmas has been petrogenetically
linked to different sources:
- Partial melts of a metasomatized lithospheric
mantle (see, for example, Metasomatic
OIB page);
- Melts from a metasomatized asthenospheric mantle
source, and;
- Combined asthenospheric and lithospheric mantle
sources (e.g., Lustrino & Wilson, 2007 and references therein).
There are diverse opinions on this
issue, which may result in part from the difficulties
in distinguishing the trace-element and isotopic characteristics
of deep-mantle sources from those acquired by the involvement–either
as melt source or as contaminant–of the lithospheric
mantle and/or the continental crust. The OIB-like geochemistry
of ECVP magmas has been presented as “proof” of
a deep mantle plume source (e.g.,
Wörner
et al.,
1986; Hoernle
et al.,
1995; Wedepohl & Baumann,
1999; Haase
et al.,
2004). However, as Fitton (2007) recently
pointed out, OIB and OIB-like basalts are widespread
throughout the oceans and at many localities where
there is no evidence otherwise for, or expectation
of, mantle plumes, and where other observations rule
them out to a high degree of certainty. Such
observations include very small magma volumes and continual
volcanism as the locality is transported for thousands
of kilometres by plate movements. Many other continental
rift systems exhibit similar behaviour and magma compositions
e.g., the East African rift and the western
United States. See also Origin
of OIB pages.
3.6 3He/4He geochemistry
ECVP magmas contain enriched isotopic
OIB signatures of mainly HIMU type, mixed in variable
proportions with EM-1 (e.g., Vogelsberg) or
EM-2 (e.g., Massif
Central; Figure 4). This isotopic composition clearly
identifies the magmas as OIB-like. However, the occurrence
of OIB and OIB-like magmas cannot be petrogenetically
unambiguously explained using traditional geochemical
reasoning. Other tracers for a deep-mantle or core-mantle-boundary
origin have thus been proposed such as noble gases–in
particular 3He/4He ratios higher
than the common value of 8 ± 2 Ra generally
attributed to MORB (e.g.,
Allégre et al., 1995). This postulate has
nevertheless been challenged (see Helium
Fundamentals,
Noble Gases,
Pt-Os and Osmium
& Tungsten pages).
Figure 4: 143Nd/144Nd
vs. 87Sr/86Sr diagram for
ECVP magmas. Data from Lustrino & Wilson
(2007) in addition to some personal (RM) unpublished
data. Fields from Hart & Zindler (1989). Click here or
on figure for enlargement.
In contrast to the high 3He/4He signatures
reported from volcanic regions such as the Deccan,
Afar and Yellowstone (Basu et
al.,
1993; Marty, 1993;
Dodson et al.,
1997), 3He/4He ratios
from the ECVP are all lower than for MORB (R/Ra = 6.32 ± 0.39;
Gautheron et al.,
2005). The isotopic ratios
in each sub-area tend to be uniform and homogeneous,
with maximum values, for example, of R/Ra = 6.73 ± 0.11
for Eifel and 6.91 ± 0.3 for the Massif Central
(Gautheron et al.,
2005). In addition, the 3He/4He ratios do not vary as a function of distance from postulated “baby
plume” centres.
Gautheron
et al. (2005) concluded
that helium, neon and argon ratios argue against
a lower-mantle plume as the driving force for ECVP
magmatism, but support rift-related melting of
the lithospheric mantle. Dunai & Baur (1995) explained
Massif Central and Eifel helium systematics by
1-2% of recycled continental crust in the mantle
source. They calculated model ages ranging from 350
Ma to 800 Ma for this contamination process. They concluded
that contamination of the ECVP mantle source occurred
during and/or shortly prior to the Variscan orogeny.
The Variscan orogeny lasted from the Upper Devonian
to the Lower Carboniferous (~375 to ~330 Ma). An alternative
orogeny could be the Cadomian orogeny which took place
in the Late Proterozoic and Early Cambrian (~570
to ~540 Ma).
3.7 Source temperature indicators
Throughout the entire ECVP no picritic
magmas, commonly cited as evidence for high source
tempeatures, have been found. Rocks with relatively
high Mg contents (up to 16 wt.%; e.g., Meyer et
al., 2002) have been reported in the Rhön
for primitive basanites. These rocks are not picrites,
however, because their Na2O+K2O
contents exceed 3 wt.%. The petrogenesis of these rocks
does not require anomalously high temperatures.
Adopting the mantle plume model, Ritter
et al. (2001) explains
the maximum tomographic P-wave-speed anomaly
of ~2% down to depths of 400 km by a 150–200°C
temperature anomaly in the mantle. However alternative
scenarios involving the presence of partial melt or
other fluid, mineralogy and bulk-rock chemistry
of the mantle can also explain this anomaly (Lustrino & Carminati,
2007). Keyser
et al. (2002) explains
the –5% S-wave-speed
anomaly between 31-170 km depth below Eifel as a temperature
anomaly of 100°C plus ~1% of partial melt. Low
or absent temperature anomalies are more consistent
with the observed absence of picrites.
Due to shallow local Moho
depths, the temperature fluxes are higher
in thinned crustal segments (e.g., the
Rhine graben). The typical surface temperature flux
in Germany is 50-80 mW/m2. In contrast,
higher fluxes ranging from 80 to 120 mW/m2 have
been observed in the Rhine graben (Blundell
et al.,
1992). Recent geothermal
work shows a higher temperature
gradient for Eifel, but not for any other German, Czech
or Polish ECVP sub-area.
3.8 Mantle tomography
The classical plume model (e.g.,
Morgan,
1971; Griffiths & Campbell,
1990; 1991; Campbell & Griffiths,
1990; Farnetani & Samuel,
2005) assumes that plumes originate at the core-mantle
boundary and have a head-tail structure. Seismic
tomography images are expected to show this morphology.
Teleseismic tomography experiments have been performed
around the French Massif Central and Eifel (e.g.,
Granet
et al.,
1995; Ritter
et al.,
2001; several papers in Ritter
& Christensen,
2007) and the Eger graben (Plomerová et
al.,
2007).
Results from the Massif Central showed a low P-wave-speed
anomaly extending from the surface deep into the
upper mantle. The Eifel
Plume Project reveals a similar P-wave
structure, though there is poor agreement with the S-wave-speed
result. The P-wave model shows a columnar
low-velocity anomaly beneath the Eifel volcanic area,
extending down 400 km into the upper mantle. The S-wave
model (Keyser
et al.,
2002), on the other
hand, detects no anomaly in the depth range ~170
to 240 km depth. If the P-wave anomaly is
due to high temperature, then the S-wave
anomaly should be similar but stronger. The P-wave
anomaly is strongly attenuating in the lithosphere,
but weaker in the mantle (Ritter
et al.,
2002).
The Eifel lithospheric anomaly has been interpreted
as a zone of magmatic intrusions. In contrast, the
asthenospheric anomaly has been interpreted as representing
high temperature (e.g., Achauer
et al.,
2003). There
is no evidence that either the Eifel or the Central
Massif anomalies extend through the transition zone
and into the lower mantle. There is thus no evidence
that they represent
diapirs rising by thermal buoyancy from a thermal
boundary layer within or at the base of the deep
mantle. They may arise from the transition zone in
the upper mantle, between 410 and 650 km depths,
but there is no evidence that this is a thermal boundary
layer. These anomalies resemble that which underlies
Iceland, which has robustly been shown to not extend
through the transition zone and into the lower mantle
(see Iceland webpages).
Low-wave-speed seismic P- and S-wave
anomalies are often automatically assumed simply
to correspond to high mantle temperatures, with no
influence from other factors. However, temperature
is far from the only physical property that influences
seismic velocities. Partial melt and compositional
variations can also produce low seismic wave-speed
anomalies, and their effects may be stronger. The
presence of partial melt is particularly powerful
in lowering seismic wave speed. A trace
of partial melt, even < 1%,
could account for the low-seismic-wave-speed anomalies
detected beneath virtually all “hot spots”,
including the sub-areas of the ECVP. Such a trace
of melt could result, for example, from a trace of
CO2 (e.g., Presnall
& Gudfinsson,
2005).
Recent teleseismic tomography and seismic anisotropy
results for the upper mantle beneath the Eger rift
do not detect a low seismic wave-speed anomaly beneath
that magmatically active ECVP sub-area (Plomerová et
al.,
2007). It seems that such anomalies exist beneath
some sub-areas of the ECVP (e.g., the Massif
Central and Eifel), but not beneath other recently
active areas with similar geochemistry (e.g., Vosges-Black
Forest Arch: Achauer & Masson, 2002).
4. Discussion and proposed
geodynamic model for ECVP formation
Top-down tectonic processes provide a much more
reasonable explanation for ECVP magmatism than bottom-up,
thermally driven ones. The observations suggest that
several relatively small passive diapiric upwellings
occurred at various times beneath the ECVP. Alpine
orogenesis and rifting, inducing small-scale
flow, is the most likely explanation for the magmatism.
Subduction of the European lower continental crust
lithospheric mantle had a major influence
on the ECVP The continental crust was detached in
the Alpine region, and the lower crust was subducted.
Such a process, where the lithosphere including the
lower crust is subducted, must clearly have influenced
the crustal stress field to the north. The sinking
slab before break-off may have introduced extensional
stresses in the lower crust and lithosphere beneath
the foreland, while collision of the upper crust
reflected the compressional tectonic setting of the
orogeny. The more ductile lower crust may have been
strongly thinned locally in the Alpine foreland (ECVP
areas), allowing hot asthenosphee to rise. Later
slab break-off would have influenced mantle dynamics
300 km to the north, and small-scale convection would
have developed as a result of the ongoing deformation.
Most ECVP sub-areas are perpendicular to the main
NNE-SSW trending rift system of the Upper Rhine Valley
(Figure 1). That rift has been explained as the result
of post-Alpine extension. The Miocene to Pliocene
basins in central Europe also record this continental
rifting phase. The observation that most
Cenozoic rift faults cross-cut older Variscan sutures
has often been interpreted as evidence that rift
development was related to plume activity (Ritter,
1999, and references therein), but the rationale
for this is unclear.
In the northern Alpine foreland, there is geophysical
evidence for localized thermal attenuation of the
lithospheric mantle, presumably in response to small-scale
convection. Babuska & Plomerova (1992) find
that lithosphere thickness beneath western and central
Europe is uniform and typically 100-140 km. In contrast,
it is only ~60 km thick
below the SE Rhenish Massif (Babuska & Plomerova,
1992), 60-70 km thick beneath the Massif Central
(Sobolev et al., 1997) and 80 km thick beneath
the Eger Graben (Babuska & Plomerova, 2001).
The greatest shallowing of the Moho in western and
central Europe follows the northern Rhine graben
(see Moho
map).
Crustal thickness beneath the Vogelsberg is less
than 30 km. The lower crust is intruded by a strongly
reflective zone of basalt dykes at ~20 km depth and
crustal underplating may have also occurred (Braun & Berckhemer,
1993). Uplift of the asthenosphere–lithosphere
boundary may have been caused by local thinning
of the ductile lower crust by extension resulting
from lower-continental-crust Alpine subduction (Figure
5). The location of the thinned lithosphere is related
to older Variscan sutures. For example, the Vogelsberg
is located to the NW of the Rheno-Hercynian suture.
Buoyant asthenosphere migrated into the thinned lithosphere
and probably along the reactivated sutures.
Figure 5: Sketch
of the geodynamic model proposed here to explain
the origin of the ECVP. Alpine subduction of the
European lower continental crust thins the crust
in the Alpine foreland at Variscan sutures. This
thinning allows the upwelling of asthenosphere
and the initiation of small-scale convection
below ECVP localities.
This crustal setting favours the development of
small-scale convection. Uplift is expected
to result when thick cratonic lithosphere is positioned
next to asthenosphere upwelling below a rift (Vågnes & Amundsen,
1993; Kelemen & Holbrook,
1995). As a result,
small-scale convection could enhance melt production
during rifting and might be responsible for uplift
(Figure 5). Such uplift would start after development
of the rift. This contrasts with the predictions
of the mantle plume model, which expects uplift
to precede volcanism by several Ma. Partial melting
of the mantle in all ECVP areas was likely induced
by adiabatic decompression of the asthenosphere.
The jumps and onsets of magmatism suggest a common,
possibly geochemically similar, fertile mantle source
below the sub-areas. For example, in the Rhön,
this fertile mantle domain was tapped for ~2 Ma (20-18
Ma), prior to the tapping of a virtually identical
reservoir in the Grabfeld area for a comparable
period of time (16-14 Ma; Figure 2).
A fertile package in the mantle could arise
from old, possibly Variscian, buoyant slab material
that was not subducted into the deeper mantle (e.g.,
a similar situation to that beneath NE China). This
slab material thermally equilibrated with the surrounding
mantle and the resulting mantle is heterogeneous
and contains both depleted and enriched parts. Such
material, residing and slowly re-equilibrating in
or near the mantle transition zone for a long time,
then being drawn up passively in small-scale
convection, and melting to a small degree, could
also explain the tomographic anomaly beneath
Eifel.
Major, trace element and Sr–Nd–Pb isotopic
data from ECVP igneous rocks define a common sub-lithospheric
mantle source component. This mantle source has geochemical
affinities to HIMU oceanic island basalts and is
often referred as the European Asthenospheric Reservoir
(EAR) and/or the Low Velocity Component (LVC). Meyer
et al. (2002) proposed metasomatically overprinted
sub-continental lithosphere as source. However, the
whole mantle may be heterogeneous (e.g., Meibom
& Anderson, 2004;
Albarède,
2005) and these heterogeneities may be the source
of ECVP magmas. In both models the mantle is a heterogeneous
source, but in the second model the “finger
plumes” or “baby plumes” observed
tomographically may be due to more fertile packages
from the mantle transition zone. In response to extensional
processes in the continental crust resulting from
the Alpine orogenesis, these packages upwell. A similar
model has been proposed for Iceland in the North
Atlantic Igneous Province (Korenaga,
2004).
In this model, continental break-up triggered the
upwelling of old, deep, large, fertile packages which
cause the tomographic signal commonly interpreted
as a mantle plume.
Acknowledgements
“Merci” to the government of Luxembourg
for funding RM BFR 05/133. We thank Prof. Peter A.
Ziegler for advice that enabled us to improve an earlier
version of this webpage.
References
-
Abratis,
M., Mädler, J.,
Hautmann, S., Leyk, H.-J., Meyer, R., Lippolt,
H.J., and Viereck-Götte,L.,
in press, Two distinct Miocene age ranges of basaltic
rocks from the Rhön and Heldburg areas (Germany)
based on 40Ar/39Ar step heating
data, Chemie der Erde-Geochemistry, doi:10.1016/j.chemer.2006.03.003.
-
-
-
-
-
-
-
-
Basu, S., Renne, P., DasGupta,
D., Teichmann, F., and Poreda, R., 1993, Early
and late alkali igneous pulses and a high 3He
plume origin for the Deccan Flood Basalts. Science, 261,
902–906.
-
-
Blundell, D., Freeman, R., and Mueller, S., 1992, A Continent Revealed. The European
Geotraverse, Cambridge
University Press, 73+275.
-
Bücking, H., 1916, Geologischer
Führer
durch die Rhön, Sammlung
geologischer Führer 21. Bornträger, 1–262.
-
Cloetingh,
S., Ziegler, P.A., Beekman, F., Andriessen, P.A.M.,
Hardebol, and Dèzes, P., 2005, Intraplate
deformation and 3D rhheological structure of
the Rhine Rift System and adjacent areas of the
northern Alpine foreland, Int. J. Earth Sciences
(Geologische Rundschau), 94, 758-778.
-
-
-
-
- Dèzes, P., Schmid, S.M. and Ziegler, P.A.,
2005, Reply to comments by L. Michon and O. Merle
on “Evolution of the European Cenozoic Rift
System: interaction of the Alpine and Pyrenean orogens
with their foreland lithosphere” by P. Dèzes,
S.M. Scmid and P.A. Ziegler, Tectonophysics 389 (2004)
1-33. Tectonophysics, 401, 257-262.
-
Dodson, A., Kennedy, M.B., DePaolo,
D.J., 1997, Helium and neon isotopes in the Imnaha
Basalt, Columbia River Basalt Group: evidence for
a Yellowstone plume source, Earth Planet.
Sci. Lett., 150, 443– 451.
-
-
-
Fitton, J.G. and Dunlop, H.M., 1985, The Cameroon
line, West Africa, and its bearing on the origin
of oceanic and continental alkali basalt, Earth
Planet. Sci. Lett., 72,
23–38.
-
Fitton,
J.G., 2007, The OIB paradox, In: Foulger, G.R.
& Jurdy, D.M. (Eds.) Plates, Plumes,
and Planetary Processes,
Geol. Soc. Am. Spec. Paper. 430, 387-415.
-
Gautheron,
C., Moreira, M., and Allègre,
C., 2005, He, Ne and Ar composition of the European
lithospheric mantle, Chem. Geol., 217, 97-112.
-
-
Griffiths,
R.W., and Campbell, I.H., 1991, Interaction of
mantle plume heads with the Earth’s surface
and onset of small-scale convection, J.
Geophys. Res., 96, 18,295-18,310.
-
Haase,
K.M., Goldschmidt, B., Garbe-Schönberg,
D., 2004. Petrogenesis of Tertiary continental
intra-plate lavas from the Westerwald region, J,
Pet,, 45, 883–905.
-
-
-
Kelemen,
P.B., and Holbrook, W.S., 1995, Origin of thick,
high-velocity igneous crust along the U.S. East
Coast margin, J. Geophys.
Res.,
100, 10,077-10,094.
-
Keyser,
M., Ritter, J.R.R. and Jordan, M., 2002, 3D shear-wave
velocity structure of the Eifel plume, Germany, Earth
Planet. Sci. Lett., 203,
59-82.
-
-
-
Lustrino,
M., Carminati, E., 2007, Phantom plumes in Europe
and neighbouring areas: In: Foulger, G.R. & Jurdy,
D.M. (Eds.) Plates,
Plumes, and Planetary Processes, Geol. Soc.
Am. Spec. Paper. 430, 723-746.
-
Marty, B., 1993, He, Ar, Sr,
Nd and Pb isotopes in the volcanic rocks from Afar:
evidence for a primitive mantle component and constraints
on magmatic sources, Geochem.
J., 27, 219–228.
-
-
Meyer, R., Abratis, M., Viereck-Gotte,
L., Madler, J., Hertogen, J., Romer, R.L., 2002,
Mantelquelen des vulkanismus in der thuringischen
Rhön, Beitr. Geol. Thüringen, 9,
75–105.
-
-
Meyer, W., Albers, H.J., Berners,
H.P., von Gehlen, K., Glatthaar, D., Löhnertz, W., Pfeffer, K.H.,
Schnütgen, A., Wieneke, K., and Zakosek, H.,
1983, Pre-Quaternary uplift in the central part of
the Rhenish Massif. In: Fuchs, K., von Gehlen, K.,
Mälzer, H., Murawski, H. and Semmel, A. (Eds.) Plateau Uplift, Springer-Verlag, Berlin, 9-38.
-
-
Plomerová,
J., Achauer, U., Babuška,
Vecsey, L., and BOHEMA working group, 2007, Upper
mantle beneath the Eger Rift (Central Europe):
plume or astenosphere upwelling?, Geophys.
J. Int., 169, 675-682.
-
Presnall, D. C., and Gudfinnsson, G. H., 2005,
Carbonatitic melts in the oceanic low-velocity zone
and deep mantle, in Foulger, G. H., Natland, J. H.,
Presnall, D. C., and Anderson, D. L., Plates,
Plumes, and Paradigms, Geol. Soc. Am. Spec. Paper 388, 207-216.
- Ritter, J.R.R. 1999, Rising Through Earth's Mantle, Science, 286,
1865 – 1866.
-
Ritter, J.R.R., Jordan, M.,
Christensen, U.R., Achauer, U., 2001, A mantle
plume below the Eifel volcanic fields, Germany,
Earth Planet. Sci. Lett., 186,
7–14.
-
Ritter,
J.R.R., Jordan, M., Achauer, U., Christensen,
U.R., and The Eifel Plume Team, 2002, Seismic structure
and physical state of the Eifelplume, Germany, Geophys.
Res. Abs., 4, 01661.
-
Ritter, J.R.R. and Christensen, U.R. (eds.), 2007,
Mantle Plumes - A Multidisciplinary
Approach, Springer
Verlag, Heidelberg, 502 pp.
-
Schmid,
S.M., Pfiffner, O.A., Froitzheim, N., Schönborn,
G. and Kissling, E. 1996, Geophysical-geological
transect and tectonic evolution of the Swiss-Italian
Alps, Tectonics, 15,
1036–1064.
-
Schmidt, G., Witt-Eickschen,
G., Palme, H., Seck, H., Spettel., and Kratz, K.-L.,
2003, Highly siderophile elements (PGE, Re and
Au) in mantle xenoliths from the West Eifel volcanic
field (Germany), Chem. Geol., 196, 77-105.
-
-
Sleep, N.H.,1984, Tapping of magmas from ubiquitous
mantle heterogeneities - an alternative to mantle
plumes, J. Geophys. Res., 89,
29–41.
-
Sobolev,
S.V., Zeyen, H., Granet,M., Achauer, U., Bauer,
C.,Werling, F., Altherr, R., Fuchs, K., 1997. Upper
mantle temperatures and lithosphere–asthenosphere
system beneath the French Massif Central constrained
by seismic, gravity, petrologic and thermal observations. Tectonophysics, 275,
143–164.
-
Stosch,
H.-G., 1987, Constitution and evolution of subcontinental
upper mantle and lower crust in areas of young
volcanism: differences and similaries between the
Eifel (F.R. Germany) and Tariat Depression (central
Mongolia) as evidenced by peridotite and granulite
xenoliths, Fortschritte der
Mineralogie, 65, 49–86.
-
-
Ulrych, J, Pivec E., Lang. M.,
Balogh. K., and Kropacek. V., 1999, Cenozoic intraplate
volcanic rocks series of the Bohemian Massif: a
review, Geolines, 9,
123–129.
-
-
-
-
-
-
Wörner,
G., Zindler, A., Staudigel, H., Schmincke, H.-U.,
1986, Sr, Nd, and Pb isotope geochemistry of
Tertiary and Quaternary alkaline volcanics from
West Germany, Earth
Planet. Sci. Lett., 79,
107–119.
-
-
Ziegler, P.A., 1990, Geological Atlas of Western
and Central Europe, Shell Internat. Petrol. Mij.,
Dist. Geol. Soc. Publ. House, Bath, 2nd ed. 239 pp.
and 56 encl.
-
Ziegler, P.A., 1992. European
Cenozoic rift system, Tectonophysics, 208,
91–111.
-
Ziegler, P.A. and Dèzes,
P., 2007, Cenozoic uplift of Variscan Massifs in
the Alpine foreland: Timing and controlling mechanisms. Global
Planetary Change, 58, 237-269.
-
Ziegler, P.A., Schumacher, M.E.,
Dèzes, P., van
Wees, J-D. and Cloetingh, S., 2004. Post-Variscan
evolution of the lithosphere in the Rhine Graben
area: constraints from subsidence modeling. In:
Wilson M. et al., (eds.) Permo-Carboniferous Magmatism
and Rifting in Europe.
Geol. Soc. Spec. Publs. 223, 289-317.
-
last updated 14th
September, 2007 |