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Domal
uplift and volcanism in a collision zone without
a mantle plume:
Evidence
from Eastern Anatolia |
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| Abstract
The
Eastern Anatolia region is one of the best examples
of a continental collision zone in the world. It also
comprises one of the high plateaus of the Alpine-Himalaya
mountain belt with an average elevation of ~2 km above
sea level (Fig. 1). It displays
shallow and diffuse seismicity (Fig.
2), indicating that the lithosphere is still being
actively deformed as a result of diffuse north-south
shortening. This implies that the collision is still
in progress. Previous studies have shown that the Arabian
plate made its initial contact with the Eurasian plate
during the Late Eocene. The region underwent compressional
tectonic evolution subsequently, but most of it lay
beneath sea level during a period between the Late Eocene
(~50 Ma) and Serravalian (~13 Ma). At about 13 Ma, the
region was subjected to abrupt block uplift and consequently
elevated above sea level. Uplift was followed
by subaerial volcanic activity. Volcanism intensified
and had became widespread all over the region by about
7-8 Ma, while the region gradually acquired a regional
domal shape comparable to that of the
Ethiopian
High Plateau. However, the dome structure in Eastern
Anatolia has a north-south shortened asymmetrical shape,
due to the compressional tectonic regime created by
collision, in contrast to that of the Ethiopian High
Plateau. At present,
it is difficult to recognise the dome in topographic
maps since the topography of the region has been strongly
modified by volcanoes and river drainage systems.
Volcanism
migrated to the south/southeast over time. Great volumes
of volcanic material (i.e. lavas and pyroclastic units)
reaching over 1 km in thickness in places were erupted
onto the surface between 8 and 1.5 Ma, forming volcano-sedimentary
successions, and covering almost two-thirds of the region.
Thus, the Eastern Anatolia region can be regarded as
the site of a "melting anomaly" or "hotspot"
resembling closely the setting proposed for mantle plumes.
However, geologic and geochemical data provide evidence
against a plume origin. In addition, the results of
new geophysical studies, coupled with geologic and geochemical
findings, support the view that both domal uplift and
extensive magma generation can be linked to the mechanical
removal of a portion or the whole thickness of the mantle
lithosphere, accompanied by passive upwelling of normal-temperature
asthenospheric mantle to a depth as shallow as 50 km.
This process is argued to have occurred either by delamination,
slab-steepening and breakoff, or a combination of both.
Therefore, magma generation beneath Eastern Anatolia
may have been controlled by adiabatic decompression
of the asthenosphere. The presence of a subduction component
and thus water in the asthenospheric mantle wedge whould
have played an important role in this melting process.
In addition,
material derived from previously subducted slabs might
have contributed to the fertility of the mantle source
region.
The
Eastern Anatolian example is important in showing that
not
only plumes but also shallow plate tectonic processes
have the potential to generate regional domal structures
in the Earth's lithosphere as well as large volumes
of magma, as proposed by a number of recent studies. |
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Introduction
Orogenic belts formed by collisions between continents
contain invaluable records of the geological history
of the Earth and therefore have always attracted the
attention of Earth scientists. The Eastern Anatolia
Region, exhibiting plateau morphology with an elevation
1500 – 2000 m above sea level, is one of two regions
where active continent-continent collision is currently
taking place, the other being the Tibetan Plateau (Fig.
1). Therefore, the Eastern Anatolia region is a
spectacular natural laboratory where the early stages
of a continent-continent collision and their effects
can be thoroughly studied.

Figure
1. Plateaus in the Alpine/Himalayan mountain belt.
Black: thrust belts; yellow:
foreland and hinterland basins. Numbers refer to the
average height of the plateaus.
1: Western Anatolian plateau (1 km);
2: Eastern Anatolian Plateau (2 km);
3: Tien Shan (3 km);
5: Tibet (5 km)
[Fig. 1 from Dewey et al., 1986].
Figure
2. Distribution of earthquake epicentres, magnitudes
and depths across the Eastern Anatolia region. The map
includes recorded earthquakes from 1st December
1999 to 23rd March 2005. The figure is a
screenshot from the Earthquake Monitor program of Gezdirici
[2001]. Red circles are hypocentres which are shallower
than 20 km (see figure legend).
Previous
studies to date [e.g., Sengor & Kidd, 1979;
Dewey et al., 1986] have shown that collision
occurred between the Eurasian and Arabian continents,
resulting in the formation of an extensive (~ 150,000
km2) high plateau with an average elevation
of 2 km above sea level (Fig. 3).
These studies also revealed that the region has reached
this elevation as a block since the Serravalian (~ 13-11
Ma: Gelati, 1975), when the terminal collision
of Arabia with Eurasia started [Sengor & Kidd,
1979].

Figure
3. Topographic map showing the Eastern Anatolian plateau
with an average elevation of 2 km above sea level. See
Figs. 4, 5
and 6 for the main tectonic
lines and stratigraphic units.
Volcanic
activity initiated immediately after the rapid block
uplift of Eastern Anatolia and became widespread all
over the region, producing subaerial lava flows and
pyroclastic products which are very variable in their
composition and eruptive style [Pearce et al.,
1990; Keskin et al., 1998; Yilmaz et al.,
1998]. The volcanic activity initiated in the north
around the Erzurum-Kars Plateau and migrated to the
south-southeast [Keskin, 2003] (Fig.
7). A vast volume of volcanic material was produced
by this activity, covering almost two thirds of the
region and reaching over 1 km in thickness in some localities
(Figs. 4, 5
and 6).


Figure
4. Simplified geological map of the Eastern Anatolia
region showing tectonic units, collision-related volcanic
products and volcanic centres (compiled by Keskin, 2003).
A-A’: direction of the cross section given in Fig.
8. E-K-P: the Erzurum-Kars Plateau;
NATF and EATF: North and East Anatolian Transform Faults.
Volcanic centers: Ag: Mt. Agri (Ararat), Al1:
Mt. Aladag (SE of Agri), Al2: Mt. Aladag
(NW of Horasan), Bi: Mt. Bingol, Bl: Mt. Bilicandagi,
D: Mt. Dumanlidag, E: Mt. Etrusk, H: Mt. Hamadag, K:
Mt. Karatepe, Ki: Mt. Kisirdag, M: Mt. Meydandag, N:
Mt. Nemrut, S: Mt. Suphan, T: Mt. Tendürek, Y: Mt. Yaglicadag,
Z: Mt. Ziyaretdag.
Although
fissure eruptions dominated the volcanic activity, there
are over 20 volcanic centres (e.g., Mt. Nemrut,
Mt. Ararat, Mt. Tendurek) in the region, corresponding
basically to central eruption sites (Figs.
4 and 9). The erupted volumes
may represent only a small fraction of the melt generated
beneath the region, because a greater proportion presumably
was emplaced deeper in the crust as plutonic intrusions.
Thus, there must have been enormous magma generation
beneath the whole region related to the collision of
Arabia with Eurasia. As a result, Eastern Anatolia can
be regarded as one of the Earth's major “hotspots”
or a "melting anomalies".

Figure 5. Major tectonic
blocks of the Eastern Anatolia region. The borders are
modified from Sengor et al. [2003]. I: Rhodope-Pontide
fragment, II: Northwest Iranian fragment, III: Eastern
Anatolian Accretionary Complex (EAAC), IV: Bitlis-Poturge
Massif, V: Arabian foreland. Dark green areas: outcrops
of ophilitic melange, Pink and red areas: collision-related
volcanic units, white areas: undifferentiated units
or young cover formations. EKP: the Erzurum-Kars Plateau
in the north.

Figure 6. Topographic
map of the Eastern Anatolia Collision Zone (EACZ) over
which the main tectonic units as well as collision-related
volcanics are superimposed. NIF: Northwest Iranian Fragment,
BPM: Bitlis-Poturge massif, EAAC: Eastern Anatolian
Accretionary Complex, AF: Arabian Foreland. For more
explanation, see Figs. 4 and
5.

Figure
7. Distribution of the oldest radiometric ages of the
volcanic units. Ages are from Pearce et al. [1990],
Ercan et al. [1990] and Keskin et al. [1998]. Initiation
ages of the volcanism are contoured in 1-Myr intervals.
PS: Pontide suture, BPS: Bitlis-Poturge suture, CS:
inferred cryptic suture between the EAAC and BPS. Figure
from Keskin [2003].

Figure
8. Cross section summarizing the crustal structure and
petrologic/geochemical properties of the collision-related
volcanic units across the Eastern Anatolia Region [Keskin,
2003]. The crustal and lithospheric thicknesses are
from Sengor et al. [2003] and Zor et al. [2003]. The
direction of the cross section (A-A’) is shown in Fig.
4 . Source of geochemical data: *Ercan et al. [1990],
**Pearce et al. [1990], ***Keskin et al. [1998]. SC:
subduction component, AFC: Assimilation combined with
fractional crystallization process, r: ratio of the
rates of mass assimilation and mass crystallization.
F: strike-slip faults.


Figure 9. MrSID satellite view of (a) Mt. Nemrut
volcano in the south, (b) Mt. Ararat: a double-peaked
strato-volcano in the northeast, and (c) the Erzurum-Kars
Plateau (EKP) in the northernmost part of the Eastern
Anatolia region. On the Erzurum-Kars Plateau (i.e. c)
Reddish coloured areas marked EKP correspond to volcanic
units, while purple to pinkish areas are either basement
units (e.g., areas in the northwest) or young sedimentary
cover formations. Vegetation is represented by green
areas. For the exact regional locations of Mt. Nemrut
and Mt. Ararat, see Fig. 4.
The
East Anatolian topographic uplift resembles the Tibetan
Plateau and has been viewed as a younger version of
it in many studies [e.g., Sengor & Kidd,
1979; Dewey et al., 1986; Barazangi,
1989]. In these studies, the Eastern Anatolian lithosphere
is thought to have doubled in thickness (to ~ 250-300
km) as a result of collision (Fig.
10). However, recent geophysical studies have revealed
that the mantle lithosphere is almost completely absent
beneath a greater portion of the region [Gök et
al., 2000, 2003; Al-Lazki et al., 2003]
(Fig. 8).
Moreover, studies of receiver functions indicate that
the crust beneath the region ranges in thickness between
38 and 50 km, averaging ~ 40–45 km [Zor et
al., 2003]. This indicates that an almost normal-thickness
crust is underlain by an extremely thin mantle lithosphere
or perhaps almost directly by the asthenosphere. Such
a lithospheric thickness can be considered to be normal
in extensional areas, such as Iceland, but unusual in
a continental collision setting with a compressional
tectonic regime.
 |
Figure
10: Continental collision and subsequent thickening
of the Anatolian crust/lithosphere [Dewey et al.,
1986]. |
On
the basis of these results and the geology of the region,
Sengor et al. [2003] proposed that the East
Anatolian high plateau is a mantle-supported, north-south
shortened domal structure, whose E-W topographic
profile along the 40°N parallel is very similar
to that of the Ethiopian High Plateau (Fig.
11).
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Figure
11. Figure 4 from Sengor et al. [2003].
Comparison of the topography of Ethiopia with
an E-W profile along the 40° parallel in
Eastern Anatolia. The smooth lines represent
least squares simplifications of the topography.
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When
these findings and interpretations are taken into account,
it can be argued that Eastern Anatolia represents a
tectonically-deformed, N-S shortened lithospheric dome
structure, supported by an asthenospheric upwelling
(see cross section in Fig. 8).
Thus, Eastern Anatolia closely resembles a mantle plume
setting. However, geologic and geochemical data indicate
that a mantle plume setting cannot be a viable model
for the region as I discuss in the following sections.
The
rest of this web-page deals with a number of problems
including:
-
how great volumes
of collision-related magma were generated in the region,
-
how and why the region
gained its elevation and the aforementioned domal
shape in the absence of a mantle plume, and
-
what tectonic processes
are responsible for both magma generation and the
regional uplift.
It
is organized as follows:
- Section
I focuses on the geology of the region,
- Section
II deals with the geochemical characteristics of the
collision-related volcanic units,
- Section
III describes the results of the Eastern
Turkey Seismic Experiment project,
- Section
IV discusses ten competing geodynamic models proposed
for the region with emphasis on the inherent discrepancies
in each model.
- Section
V is a discussion.
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| 1.
Geology
There are two main plateaus in the Alpine-Himalayan
collision system (Fig. 1):
-
The Anatolian –
Iranian plateau (1 and 2 in Fig.
1),
- The
Tibetan plateau (5 in Fig. 1)
[Sengor & Kidd, 1979; Dewey et al.,
1986].
The Anatolian – Iranian Plateau extends from Eastern
Anatolia to Eastern Iran, and typically has an elevation
of about 1.5 – 2 km in Eastern Anatolia. The basement
of the Anatolian – Iranian Plateau is made up
of micro-continents, accreted to each other during the
Late Cretaceous to Early Tertiary [Sengor,
1990]. These micro-continents are separated from each
other by ophiolite belts and accretionary complexes.
Five different
tectonic blocks
are recognised in North-Eastern Anatolia (Fig.
5):
- The Eastern Rhodope-Pontide fragment
in the northwest of the region (I in Fig.
5). It underlies the south-western and
north-eastern parts of the Erzurum Kars Plateau (i.e.
EKP in Fig. 5).
- The Northwest
Iranian fragment (II in Fig. 5).
The eastern part of the Erzurum-Kars Plateau (i.e.
Horasan, Aladag, Kagizman, Kars areas and Mt. Ararat)
overlies this tectonic block [Keskin et
al., 1998],
-
The Eastern Anatolian Accretionary Complex in the
middle of the region located between the Aras River
and the Bitlis-Poturge Massif (III in Fig.
5),
-
The Bitlis-Pötürge unit which is exposed along the
Taurus belt (IV in Fig. 5),
and
-
Autochthonous units of the Arabian continent or foreland
(V in Fig. 5).
Except
for the EAAC, all the tectonic blocks correspond to
the aforementioned micro-continents.
The Eastern Rhodope-Pontide
unit is located in the northernmost part of the region.
Its basement is represented by a metamorphic massive
named the Pulur Complex [Topuz et al., 2004].
The Pulur complex is composed of a heterogeneous set
of granulite facies rocks, ranging from quartz-rich
mesocratic gneisses to silica- and alkali-deficient,
Fe-, Mg- and Al-rich melanocratic rocks [Topuz et
al., 2004]. A thick volcano-sedimentary arc sequence
overlies this metamorphic basement. This sequence is
regarded as an ensialic, south-facing magmatic arc,
formed by north-dipping subduction under the Eurasian
continental margin [Yilmaz et al., 1997] in
a period between the Albian and Oligocene [Sengor
et al., 2003].
The Northwest Iranian
fragment is masked by collision-related volcanic units
in Eastern Anatolia. It is exposed in Armenia around
the Tsakhkuniats basement outcrop and Hankavan-Takarly
and Agveran massifs [Karapetian et al., 2001].
The unit is composed of a heterogeneous rock sequence,
consisting of trondhjemitic, phyillitic, albite-plagiogranitic,
plagiogranite- and granite-migmatitic lithologies [Karapetian
et al., 2001].
The Eastern Anatolian
Accretionary Complex (EAAC) forms a 150-180 km wide,
NW-SE extending belt in the middle of the region. It
represents the remnant of a huge subduction-accretion
complex formed on a north-dipping subduction zone located
between the Rhodop-Pontide in the north and the Bitlis-Poturge
microcontinent in the south in a period between the
Late Cretaceous and Oligocene [Sengor et al.,
2003]. It consists of two contrasting rock units:
-
An
ophiolitic melange of Late Cretaceous age, and
-
Paleocene
to Late Oligocene flysch sequences incorporated
into the ophiolitic melange as north-dipping tectonic
slices. These flysch slices become younger from
north to south and shallower from the Cretaceous
to the Oligocene [Sengor et al., 2003].
This observation is consistent with the polarity
of the subduction zone that is thought to have created
the Eastern Anatolian accretionary prism by underthrusting.
The Bitlis-Poturge
Massif is exposed in a NW-SE extending belt along the
Eastern Taurus mountain range. It is regarded as the
easternmost extremity of the Menderes-Taurus block.
It consists of medium-to-highly metamorphosed units.
Shallow marine
deposits of Oligocene to Middle Miocene age unconformably
overlie these tectonic blocks in some places (not shown
in Figs. 4 and 5).
Collision-related volcanic units, on the other hand,
unconformably overlie both these five tectonic blocks
and the aforementioned marine deposits, masking the
basement units over great distances (Figs.
4, 5 and 6).
These volcanic units become younger to the south/southeast
[Keskin, 2003] (Fig. 7).
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| 2.
Lithospheric structure of the region based on the results
of the Eastern Turkey Seismic Experiment project
Results
from the Eastern Turkey
Seismic Experiment project [ETSE project:
Al-Lazki et al., 2003; Gök et al.,
2000; 2003; Sandvol et al., 2003] reveal that
the mantle lithosphere is either very thin or absent
beneath a considerable portion of the region between
the Aras river (broadly
corresponding to the southern border of the EKP)
in the north and the
Bitlis-Poturge Massif in the south (Fig.
12). Moreover, crustal thicknesses obtained from
receiver function studies indicate a gradual change
from < 38 km in the southeast around the southern
part of the Bitlis suture zone to 50 km in the north
beneath the Erzurum-Kars Plateau [Zor et al.,
2003], averaging some 45 km. This indicates that an
almost normal-thickness crust overlies an extremely
thin mantle lithosphere or perhaps it directly overlies
the asthenosphere (see also the cross section in Fig.
8).

Figure 12.
Contours (red) displaying the mantle lid (i.e.
lithospheric mantle) thicknesses in km (contours
are taken from Fig. 2 of Sengor et al., 2003).
The light bluish-coloured triangular area surrounded
by the cities of Agri, Erzurum, Bingol and Van
in the centre of the figure represents the area
with no mantle lid. Thick, dotted dark-blue lines
represent the northern and southern borders of
the Eastern Anatolian Accretionary Complex (also
see Fig. 5). Note that
areas of inferred complete lithospheric detachment
almost exactly coincide with the extent of the
Eastern Anatolian Accretionary Complex (i.e. the
EAAC). |
These results are also consistent with the study of
Hearn & Ni [1994], Maggi et al.
[2002] and Maggi & Priestley [2005], suggesting
that the temperature of the mantle significantly increased
beneath this area. What all these findings may imply
is that a huge portion of the mantle lithosphere was
lost beneath Eastern Anatolia. As the collision-related
volcanic activity is almost coeval with the rapid regional
block uplift at ~ 11–13 Ma, catastrophic delamination
might have been responsible [Keskin et al.,
1998]. |
3.
Geochemical characteristics of the collision-related
volcanic units
One of the most striking
aspects of Eastern Anatolia is the volume and the compositional
variability of collision-related volcanic products erupted
during the Neogene and Quaternary. Over half of the
region is covered with young volcanic units (Figs.
4, 5 and 6),
exceeding 1 km in thickness in places and ranging in
age from 11 Ma to present (Figs.
7 and 8).
3.1.
Classification
Collision-related
volcanic rocks across the region span the whole compositional
range from basalts to rhyolites. There is significant
variation in lava chemistry in the N-S direction between
the Erzurum-Kars Plateau (EKP) in the north and the
Mus-Nemrut-Tendurek volcanoes in the south (Figs.
13 and 14). Volcanic units
of the Erzurum-Kars Plateau are calc-alkaline (they
follow a calc-alkaline trend on the AFM diagram, which
is not shown here), while those of the Mus-Nemrut-Tendurek
volcanoes are alkaline to mildly alkaline in character.
Lavas of the Bingol and Suphan volcanoes display transitional
chemical characteristics [Pearce et al., 1990].

|
 |
Figure
13. Classification of volcanic units of the Eastern
Anatolia region on the total alkali vs silica
diagram of Le Bas et al. [1986]. Data for Erzurum-Kars
Plateau are from Keskin et al. [1998], the rest
are taken from Pearce et al. [1990]. Diagrams
are arranged from north to south:
- Erzurum-Kars plateau
in the north,
- Bingol-Suphan areas
in the central-west,
- Mus-Nemrut-Tendurek
areas in the south.
Abbreviations:
B: basalt, BA: basaltic andesite, TB: trachybasalt,
BTA: basaltic trachyandesite, A: andesite, TA:
trachyandesite, D: dacite, TD: trachydacite, T:
trachite, R: rhyolite, IB: alkaline/subalkaline
divide of Irvine and Baragar [1971], Ku:
alkaline/sub-alkaline divide of Kuno [1966]. Note
that alkalinity increases from north to the south. |
 
Figure
14. Classification of the volcanic units of the Eastern
Anatolia region on the K2O vs silica diagram
of Peccerillo & Taylor [1976]. Data for Erzurum-Kars
Plateau are from Keskin et al. [1998] and the rest are
from Pearce et al. [1990].
3.2.
Multi-element patterns
Calc-alkaline volcanic units on the EKP and Mt. Ararat
display MORB-normalised patterns typical of continental
arc volcanics. They are likely to have been derived
from an enriched mantle source containing a distinct
subduction signature (SC) (Figs.
15 and 16). This signature
decreases to the south and diminishes around Mus-Nemrut-Tendurek
volcanoes (Figs. 16 and 8),
where the lavas are alkaline and display an intraplate
signature [Pearce et al., 1990].
|
ERZURUM - KARS
PLATEAU

 |
Figure
15. MORB-normalised patterns for volcanic samples
from the Eastern Anatolia collision zone. Normalisation
values are from Sun & McDonough (1989).
The data from the Erzurum-Kars Plateau are taken
from Keskin et al. [1998], while the data from
the Mus-Nemrut-Tendurek areas are obtained from
Pearce et al. [1990].
Numbers in brackets
are SiO2 wt. % values.
Note that
the samples from the Erzurum-Kars Plateau in the
north contain a distinct subduction signature,
while lavas of the Mus-Nermrut-Tendurek areas
display an intraplate signature with or without
a slight subduction signature.
|

Figure
16. Th/Yb vs. Ta/Yb diagram [after Pearce, 1983] for
basic and intermediate lavas (SiO2 < 60%)
from the Eastern Anatolia Collision Zone. Data from
the Mus-Nemrut-Tendurek volcanoes are from Pearce et
al. [1990]. MM: mantle metasomatism array; SZE: subduction
zone enrichment; WPE: within-plate enrichment; UC: upper
crustal composition of Taylor & McLennan [1985];
FC: fractional crystallsation vector; AFC: assimilation
combined with fractional crsytallisation curve. The
FC curve has been modelled for 50% crystallsation of
an assemblage consisting of 50% plagioclase and 50%
amphibole from a basic magma. The AFC vector has been
drawn for an "r" value of 0.3. Note
that lavas of the Erzurum-Kars Plateau contain a distinct
subduction zone enrichment (SZE) signature.
3.3.
Petrologic modelling
3.3.1. Modelling of source-enrichment
On
a Ta/Yb vs. Th/Yb diagram, calc-alkaline
lavas of the Erzurum-Kars Plateau display a consistent
displacement from the mantle metasomatism array towards
higher Th/Yb ratios, forming a sub-parallel trend to
the main MM array (Fig. 16a).
This suggests that there was a contribution of a subduction
component to the EKP mantle source region. The alkaline
basic lavas of the Mus-Nemrut-Tendurek volcanoes show
a progressive shift from the MM array with increasing
SiO2 (Fig. 16b).
This implies that these lavas might have been derived
from an enriched source with or without a slight subduction
signature and then evolved through combined assimilation-fractional
crystallisation (AFC).
3.3.2.
Modelling fractional crystallisation
Crystallization assemblages in the collision-related
lavas of the Eastern Anatolia region also display variations
across the region. Lavas in the north contain hydrous
assemblages (e.g., amphibole) as well as anhydrous
minerals, whereas those in the south are dominated by
anhydrous minerals. This indicates that lavas are richer
in water in the north than in the south, consistent
with their subduction signature. Geochemical data are
also consistent with these petrographic observations:
the lavas containing hydrous minerals (e.g.,
amphiboles) display distinct depletion with increasing
Rb (Fig. 17a) in contrast to
the lavas of the southern areas (i.e. Mus-Nemrut-Tendurek;
Fig. 17b) which contain anhydrous
minerals that exhibit positive to flat gradients [Pearce
et al., 1990].

Figure
17. Rb vs. Y diagram displaying theoretical Rayleigh
fractionation vectors for 50% crystallisation of the
phase combinations (given below) from a common magma
composition. Tick marks on each vector correspond to
5% crystallisation intervals. The data for the Erzurum-Kars
Plateau are from Keskin et al. [1998], while those from
the Mus-Nemrut-Tendurek and Bingol-Suphan volcanoes
in the south are from Pearce et al. [1990]. Bulk partition
coefficient values used in the modelling are those given
in Table 2 of Keskin et al. [1998]. The
FC vectors have been modelled using the "FC-Modeler
program" of Keskin [2002].
Phase combinations for
the vectors:
1. plg.5+cpx.3+olv.2
(B); 2. plg.5+cpx.5
(B) or ~plg.5+cpx.3+olv.2
(I); 3. plg.5+amp.5
(B) or plg.5+cpx.5 (I)
4. plg.2+opx.1+cpx.6+olv.1
(I); 5. plg.5+cpx.5
(A); 6. plg.5+amp.5
(I); 7. plg.4+amp.4+gt.2
(I); 8. plg.5+amp.5
(A); 9. plg.4+amp.4+gt.2
(A).
plg: plagioclase,
cpx: clinopyroxene, opx: orthopyroxene, olv: olivine,
amp: amphibole, gt: garnet
B: basic, I: intermediate, and
A: acid magma compositions.
3.3.3.
Modelling AFC process
AFC modelling results indicate that the degree of magma-crust
interaction is larger in the south than in the north
(Fig.18). Radiometric dating
results indicate that volcanic activity began earlier
in the north than in the south, migrating south over
time (Figs. 7 and 8).

Figure
18. Diagrams showing the results of assimilation-fractional
crystallisation (AFC) modelling. The modelling was conducted
using the AFC equations of De Paolo [1981]. Bulk
partition coefficients are inset in the diagrams. Parental
magma compositions correspond to the basaltic sample
MK139 (Erzurum-Kars Plateau; Keskin et al., 1998) and
sample 2362 (Mus-Nemrut-Tendurek: Pearce et al., 1990),
and the average crustal composition of Taylor &
McLennan [1985].
3.3.4.
Modelling partial melting process
Melting modelling (Fig.
19) was carried out using the fractional and batch
melting equations of Shaw [1970], the bulk
partition coefficient values given in the inset of Fig.
19 (for the source of Kd values,
see the caption of Fig. 19)
and modal mineralogy of spinel- and garnet-peridotites
proposed by Wilson [1989] (see the caption
of Fig. 19). The trace element
composition of the garnet-peridotite is taken from Frey
[1980], while the composition of the spinel-peridotite
is the average composition of spinel peridotite xenoliths
(see C0 values in the inset of Fig.
19) in young (i.e., Miocene-Pliocene) alkaline
basalts from the Thrace region, NW Turkey [Esenli
& Genc, submitted]. Most of the lavas of the
EKP plot on the batch-melting curve of the spinel peridotite,
while two of them (MK144: the oldest, 11 Ma, sample
from the bottom of the Horasan area, and three lava
samples from the Middle Stage in the Dumlu area) fall
close to the beginning of the fractional melting curve.
Therefore, magmas that fed the volcanism on the Erzurum-Kars
Plateau seem to have been generated by partial batch
melting of a spinel peridotite mantle source. The degree
of melting might be quite high for the lavas clustering
around the end of the batch-melting curve.

Figure
19. La/Sm vs. Sm/Yb plot showing theoretical melting
curves plotted along with the basic samples (SiO2<57%)
from the Erzurum-Kars Plateau. Fractional and batch
melting equations of Shaw [1970] were used to construct
the melting model. F: weight fraction of melt produced.
Modal mineralogy for the spinel- and garnet-peridotites
are taken from Wilson [1989], and ol.66+opx.24+cpx.08+sp.02
and ol.63+opx.30+cpx.02+gt.05
respectively (ol: olivine, opx:orthopyroxene, cpx: clinopyroxene,
sp: spinel, gt: garnet). Trace element composition of
the spinel-peridotite (C0 values) is the
average composition of spinel peridotite xenoliths in
young (Miocene) alkaline basalts of the Thrace region,
NW Turkey [Esenli & Genc, submitted], while that
of garnet peridotite is from Frey [1980]. Kds
between the basaltic melts and minerals given in the
inset are compiled from Irving & Frey [1978], Fujimaki
et al. [1984], McKenzie & O'Nions [1991] and Rollinson
[1993]. Bulk partition coefficient (Ds) of each element
has been calculated for garnet and spinel peridotite
source rock compositions by taking the modal mineralogy
of these end members into consideration. The coefficients
are given in the inset.
Coherence
of the data points from different stages of the volcanism
in Fig. 19 indicates that the
nature of the mantle source and the mode of the melting
process varied little with time. This is also consistent
with the results obtained from chondrite-normalized
REE and MORB-normalized multi-element patterns (see
Fig. 15); basic lavas erupted
during the early and late stages display similar patterns
all over the EKP. Similar modelling was conducted for
the lavas of the Karacadag and Tendurek volcanoes in
the south by Sen et al. [2004], and produced
similar results.
3.4.
Summary of the geophysical and geochemical findings
The geochemical and geophysical findings are presented
together in the cross section in Fig.
8. The geochemical evidence presented so far indicates
that volcanic
products in the north around the EKP and Mt. Ararat
are calc-alkaline in character and likely to have been
derived from an enriched mantle source containing a
distinct subduction signature (Fig.
8). This signature decreases to the south and diminishes
around the Mus-Nemrut-Tendurek volcanoes, where the
lavas are alkaline and display an intraplate signature.
Results from AFC modelling show that the degree of magma-crust
interaction is larger in the south than in the north
(Fig. 18). Radiometric dating
results indicate that volcanic activity begin earlier
in the north than in the south, and migrated south over
time (Fig. 7).
The
striking results of the Eastern
Turkey Seismic Experiment project along
with the geochemical findings discussed above lead us
to question the validity of geodynamic models proposed
for the Eastern Anatolian Collision Zone in a number
of studies reported in the literature. Therefore, prior
to focusing on the issue of what process was responsible
for the loss of mantle lithosphere, I first review the
competing geodynamic models and their discrepancies. |
4.
Competing geodynamic models & their discrepancies
Ten different geodynamic
models have been proposed for the genesis of collision-related
magmatism beneath the Eastern Anatolian collision zone.
Some of the earlier studies
[e.g., the tectonic escape model of McKenzie,
1972, and the lithospheric thickening model of Dewey
et al., 1986] did not address the problem of why
and how huge volumes of magmas were generated beneath
the region. Any geodynamic model proposed for the Eastern
Anatolian collision zone should, however, answer this
critical question since the topographic expression,
tectonic elements and magma generation are clearly all
associated with the same mechanism.
There appear to be inconsistencies
in all models except for the delamination and the slab-steepening
& breakoff models. In what follows, each model is
discussed thoroughly with its weaknesses and strengths.
1.
The tectonic escape of micro-plates to the east
and west [McKenzie, 1972]. |

Figure
20
|
Discrepancies:
A
close examination of the model of McKenzie
[1972] reveals that it does not account entirely
for the strain induced by the 2.5 cm/yr convergence
of the Arabian and Eurasian plates [Dewey
et al., 1986]. In addition,
this model cannot
explain why and how huge volumes of magma were
generated beneath the region and how the region
was elevated to form an extensive plateau now
2 km above sea level. It also does not provide
an answer to why the lithospheric mantle is absent
beneath a greater portion of Eastern Anatolia. |
2.
Renewed subduction of the Arabian plate beneath
the Pontides and Eastern Anatolia [Rotstein
& Kafka, 1982].
|

Figure
21
|
| Discrepancies:
this model is not supported by any seismic evidence.
There are no seismic data for a north-dipping Benioff
zone beneath the Eastern Anatolia region. Tomographic
images obtained from the ETSE project [Al-Lazki
et al., 2003] indicate that a slab beneath
the region does not exist. |
3.
Detachment and northward movement of a subducting
slab beneath Eastern Anatolia [Innocenti et
al., 1982a,b]. |

Figure
22
|
|
On
the basis of their dating results and chemical
zonation in volcanic units across the collision
zone, Innocenti et al. [1982a,b] suggested
that the andesitic volcanic front migrated northward
by 150-200 km during the Pliocene. According to
them, this is evidence for detachment of the subducted
slab immediately after continental collision.
According to their model, the detached slab moved
northward while it was sinking in the asthenosphere.
They suggest that this movement generated progressively
lower intensity magmatism from south to the north.
In their view, volcanism becomes younger from
south to north. In this model, calc-alkaline magmas
that formed the Plio-Quaternary volcanic belt
in the north were generated above the subducting
slab, while the alkaline magmas representing the
Miocene volcanic belt in the south were derived
from the asthenosphere upwelling through the gap
behind the detached subducting slab.
Although
the model of Innocenti et al. [1982a,b]
is one of the earliest, it is remarkable in that
the possibility of slab detachment and consequential
effects in the Eastern Anatolian Collision Zone
were envisaged 13 years earlier than the "slab-breakoff
model" was proposed by Davies & von
Blanckenburg [1995]. The latest geodynamic
model,"slab-steepening & breakoff beneath
a large subduction-accretion complex", by
Keskin [2003] also proposes a similar
slab-detachment process, although the slab in
the model of Keskin [2003] does not move
northward after breakoff but instead steepens
beneath a large subduction-accretion complex until
it breaks off, creating a gradually widening mantle
wedge beneath the region.
Discrepancies: A more detailed study
of collision-related volcanism on the Erzurum-Kars
Plateau [Keskin, 1994], which comprises
the northernmost part of the Eastern Anatolian
volcanic province, has shown that volcanism initiated
at ~ 11 Ma in the north [Keskin et al.,
1998] and then migrated south over time [Keskin,
2003]. These findings are the opposite of what
is proposed by Innocenti et al. [1982a,b].
In addition, there is no seismic evidence for
a currently subducting slab beneath the region. |
|
4.
Rifting along E-W oriented Late Miocene-Pliocene
basins [Tokel, 1985] possibly accompanied
by decompression melting of "normal asthenosphere"
due to extension [McKenzie & Bickle,
1988]. |

Figure
23
|
|
Tokel [1985] cited
data from drilling cores gathered from E-W oriented
Upper Miocene-Pliocene basins in Eastern Anatolia.
He argued that these basins are bounded by gravity
faults and are filled with at least 2000 m of
limnic and fluvial deposits intercalated with
voluminous “tholeiitic” and “alkaline” volcanic
products. He suggested that recent tectonics in
Eastern Anatolia were dominated by an extensional
stress regime. On the basis of the mathematical
model of Turcotte [1983], he proposed
that these depressions and the sediments deposited
therein were related to a "rifting event"
in the region.
Discrepancies:
The fault plane solutions of earthquakes in the
region indicate that the faults are either strike
slip or reverse, which is inconsistent with extension(i.e.
a rift setting). A close examination of the E-W
oriented basins in the region reveals that the
they are not rift-related but are, instead, dominantly
pull-apart basins related to strike slip fault
systems.
Decompression melting
of normal asthenosphere as a result of regional
extension [McKenzie & Bickle, 1988]
requires a stretching factor of about 2.5 to generate
melts in dry asthenosphere at a depth of 50 km
and a temperature of around 1280°C. As is
well known the region is not being stretched so
at first sight this does not seem to be a likely
scenario. However, it is now almost certain that
nearly all the mantle lithosphere was detached
from beneath the region and thus, at present,
the lithosphere is much thinner than normal (~
38-50 km). Even if this is the case, however,
it is theoretically difficult to melt dry asthenosphere
in the absence of extension. The asthenospheric
mantle beneath the region is not completely dry,
but instead it contains a distinct subduction
component which increases in importance from
south to north as deduced from the chemistry of
collision-related volcanics in the region [Pearce
et al., 1990; Keskin, 1998]. The
existence of a subduction component (with water)
in the asthenospheric mantle may thus significantly
decrease the melting temperature and permit the
generation of voluminous basic magma at
this depth (38 to 45 km). |
|
5.
Continental collision and subsequent thickening
of the Anatolian crust/lithosphere [Dewey
et al., 1986]. |

Figure
24 |
| Dewey
et al. [1986] argued that the Eastern Anatolia
region owes its high elevation to a doubled (~
300 km) lithospheric thickness. According to them,
this thickening occurred as a result of continental
collision between the Arabian and Eurasian continents.
They also point out that the lavas were erupted
through both N-S cracks that extend into the Arabian
foreland and through transcurrent pull-aparts.
In this model magma generation is linked to local
extension and small-scale delamination events
beneath the pull-apart basins (e.g,.
the Erzincan, Karasu-Pasinler-Horasan and Mus
basins).
Following the model
of Dewey et al. [1986], Yilmaz et
al. [1987] suggested that the young volcanism
in Eastern Anatolia could be linked to heating
of the lower continental crust and mantle lithosphere
which had been subjected to lithospheric thickening.
Similarly, on the basis of their geochemical data,
Koronovskiy & Demina [1996] argued
that heating due to crustal thickening may explain
the young volcanism of the Lesser Caucasus, adjacent
to the Eastern Anatolia region.
Discrepancies: It is now well understood
that the region would not have been isostatically
elevated to ~ 2 km if a 250-300 km thick and dense
(3.2-3.3 g/cm3) mantle lithosphere
had been attached to the base of a lighter (2.7-2.8
gr/cm3) crust [Sengor et al.,
2002; Sengor et al., 2003]. The model
is not supported by recent tomographic data either
[e.g., Al-Lazki et al., 2003; Gok
et al., 2003]. Results of the Eastern
Turkey Seismic Experiment
project indicate that mantle lithosphere beneath
the region is very thin or completely absent over
a great distance in the middle of the region (Fig.
8).
Collision-related
volcanic units are not confined to pull-apart
basins. Instead, they cover a much greater area
away from these basins. This indicates that volcanism
in the region cannot be explained by the pull-apart
model alone.
Pearce et al.
[1990] discuss the point that a 50% increase in
thickness of the metasomatised mantle lithosphere
lowers a significant portion of this layer to
a depth below that of amphibole breakdown, forming
garnet and releasing water. This may initiate
localised melting but it also lowers the geotherm.
When this happens, most of the metasomatised layer
remains significantly below the solidus and thus
does not produce magma [Pearce et al.,
1990]. Therefore, it is difficult to explain the
huge volumes of magma generated in the region
by the models of Yilmaz et al. [1987]
and Koronovskiy & Demina [1996]. |
|
6.
Hot spot activity related to a mantle plume [discussed
by Pearce et al., 1990]. |

Figure
25 |
|
The possibility of plume-related
"hot spot" activity in Eastern Anatolia
was previously discussed by Pearce et al.
[1990]. They point out that the remarkable correlation
between topographic and volcanic expressions in
Eastern Anatolia. The Eastern Anatolia topographic
uplift has an asymmetric (i.e. deformed)
dome shape [Sengor et al., 2003] whose
long-axis aligns approximately E-W. The overall
volcanic expression is also asymmetric, extending
about 300 km in the direction of compression but
900 km perpendicular to it [Pearce et al.,
1990]. This remarkable correlation between the
topography and volcanic expression brings into
question whether there is a mantle plume beneath
the Eastern Anatolia Collision Zone.
Sengor et al.
[2003] compared the E-W topographic profile of
the Eastern Anatolian Plateau along the
40° parallel with the plume-generated Ethiopian
High Plateau [Sengor, 2001] and
found a striking similarity between them (Fig.
11). They low-pass filtered both profiles
at 125 km to remove plastic effects. On the basis
of the similarity of the profiles, they argued
that the cause of the domal uplift in both regions
was the same: hot, rising asthenosphere beneath
crust bereft of underlying mantle lithosphere
[Sengor et al., 2003].
Although domal uplift related to
a mantle plume is expected to have a symmetrical
shape, in theory, it may acquire an asymmetrical
shape in a collision setting due to compression.
However, there is no modern or ancient example
anywhere in the world of a plume-related dome
structure deformed by shortening in a collision
zone.
Discrepancies:
Dome structures formed by plumes
are expected to contain fault systems and dyke
swarms distributed radially. Such faults and dykes
are absent in Eastern Anatolia. Fault plane solutions
of earthquakes imply that the faults are either
transform or reverse; not normal as would be expected
in a plume-related domal structure. A plume model
cannot explain why volcanic units contain a distinct
subduction component in the north of Eastern Anatolia,
and why this component gradually diminishes to
the south. It is also difficult to explain by
a plume model why volcanism migrated south with
time, and why there is a gradual change in magma
chemistry from calc-alkaline in the north to alkaline
in the south. As pointed out by Pearce et
al. [1990], volcanic activity over the last
6 Myr displays a temporal change from more regional-scale
activity to localised activity on a set of aligned
central volcanoes. Such an evolutionary sequence
is the reverse of what is expected in plume-related
volcanic activity.
On the basis
of these discrepancies, I argue that a plume setting
is not a viable model for the Eastern Anatolian
Collision Zone. |
|
7.
Delamination of mantle lithosphere beneath the
region [Pearce et al., 1990; Keskin
et al., 1998]. |

Figure
26 |
|
Delamination of a thickened
thermal boundary layer is plausible since it is
colder and hence denser than the underlying asthenosphere
[Ed: See also Lithospheric
Delamination page]. It could therefore be
convectively replaced by asthenosphere [Houseman
et al., 1981; England & Houseman,
1988]. Platt & England [1993] argue
that magmatism in mountain belts could be evidence
of delamination of the lower part of the thickened
mantle lithosphere. Figs.
27a and b illustrate
the delamination model in a three-dimensional
block diagram for the Eastern Anatolia region
[modified from Keskin, 1994]. This process
is likely to be an effective mechanism for generating
large volumes of collision-related magma across
the region, since asthenosphere is brought into
close contact with the thickened layer of metasomatised
lithosphere [Pearce et al., 1990]. When
delamination occurs, it causes a perturbation
in what is left of the mantle lithosphere, raising
some parts of it above its solidus. While sinking
into the asthenosphere, the delaminated block
of the mantle lithosphere may release water that
also promotes melting. These two mechanisms play
an important role in the generation of extensive
partial melting in the mantle, and can produce
widespread volcanism in the region (Fig.
27b).
Pearce
et al. [1990] argue that the region is characterised
by a set of mantle domains that run parallel to
the collision zone. They suggest that each domain
has yielded magmas of particular composition since
the beginning of the magmatism in the region.
This may also be regarded as supporting evidence
for the delamination model.

Click
on the figure for enlargement.

Click
on the figure for enlargement.

Figure
27. Block diagrams illustrating the delamination
model for the Eastern Anatolian Collision Zone.
Modified from Keskin [1994].
On the basis
of estimates of the active slip rates, total convergence
and timing of collision-related deformation across
the Arabia-Eurasia collision zone, coupled with
the interpretation of a cross-section produced
by the National Iranian Oil Company [1977],
Allen et al. [2004] suggest that the
collision-related magmatism, which initiated at
~ 11 Ma [Keskin et al., 1998] pre-dates
shortening of the crust in the region. Therefore,
they argue, a sudden and regional delamination
event is not be a viable model. However, results
obtained from two independent seismic studies:
-
the Eastern
Turkey Seismic Experiment
Project [Al-Lazki et al., 2003; Gök
et al., 2000; 2003; Sandvol et al.,
2003] and
-
the
Surface Waveform Tomography study of Maggi
& Priestley [2005]
reveal
that most of the Eastern Anatolian Collision Zone
is devoid of a mantle lithosphere. Therefore,
geophysical findings support a major lithospheric
detachment beneath the region and contradict the
interpretation of Allen et al. [2004].
Discrepancies: As
discussed in Section 2, new data obtained from
the Eastern
Turkey Seismic Experiment
indicate that there appears to be no lithospheric
mantle over a greater portion of the area beneath
the region. If this is the case, then the delamination
must have been a shallow event involving the whole
lithospheric mantle and perhaps even the lower
crust. In the absence of metasomatised lithospheric
mantle, the source region would then be asthenospheric
mantle.
Sengor
et al. [2003] point out that the basement
of a great portion of the Eastern Anatolia Region
between the Aras River in the north and Lake Van
in the south is represented by a subduction-accretion
complex (i.e. EAAC in Fig.
12). This area also coincides with the area
under which a lithospheric mantle lid is missing
[Sengor et al., 2003]. In contrast to
continental blocks, large subduction-accretion
complexes are devoid of their own lithospheric
roots, as they are produced on, and supported
by, subducting oceanic slabs. Therefore, in theory,
this area should have been underlain by a subducting
slab, not by sub-continental mantle lithosphere,
before the lithospheric detachment event.
As the delamination
process requires the presence of mantle lithosphere,
what took place beneath the region could not have
been a delamination event. As tomography provides
no evidence for a mantle lid beneath the region,
then the underlying slab must have detached and
sunk into the asthenosphere possibly immediately
prior to the domal uplift of the region at ~ 13
Ma. In view of these arguments, a model
involving steepening and breakoff of a subducting
slab beneath a huge subduction-accretion complex
can explain better the geodynamic evolution of
the Eastern Anatolian Collision Zone [Keskin,
2003; Sengor et al., 2003]. As discussed
below, this model is not only consistent with
the geology of the region but also explains better
the variations in magma age and chemistry across
the region (Fig. 8). |
|
8.
Localized extension associated with pull-apart
basins in strike-slip systems [Pearce et al.,
1990; Keskin et al., 1998]. |

Figure
28 |
|
In
their pioneering study, Dewey et al.
[1986] highlighted the connection between the
formation of pull-apart basins and volcanism.
They pointed out that there are two different
neotectonic magmatic suites in the region:
- the
nepheline-hypersthene normative alkaline basalts
of mantle origin, and
- the
silicic-to-mafic calc-alkaline suite.
They suggested that
both suites occur in pull-apart basins in strike
slip regimes and N-S extensional fissures. They
argue that the position and shape of magmatic
intrusions might have been controlled by "flaking
of the elastic lid" particularly beneath
the pull-apart basins. They argue that rapid lithospheric
stretching and small-scale delamination beneath
pull-apart basins can generate melting in the
mantle.
Although Pearce
et al. [1990] consider delamination to be
the dominant process that caused voluminous magma
generation beneath the region, they also argue
that it might have been accompanied by other stretching
mechanisms, such as the creation of pull-apart
basins. They also suggested that deviatoric stress
perpendicular to the principal direction of compression
might also have some effect.
Keskin et al.
[1998] emphasised the role of strike-slip faulting
in pull-apart basins in focussing magmas on the
Erzurum-Kars Plateau, north of the region. They
point out that, compared to nearby areas, a much
thicker (2-4 km) sequence of volcanic/volcano-clastic
rocks was deposited in these gradually subsiding
basins. However, it is not clear whether these
faults simply provide fractures that enable magma
to reach the surface or whether the associated
localised extension in pull-apart basins also
encourages melting in the mantle.
More recently Cooper
et al. [2002] suggested a similar model for
the origin of mafic magmas beneath northwestern
Tibet and argued that these lavas might have been
created by mantle upwelling beneath the releasing
bends of the strike-slip fault systems [Ed: see
also Ridge-transform
intersections page].
Discrepancies:
As mentioned the Introduction, collision-related
volcanic units in the region are not confined
to pull-apart basins, but cover a much greater
area. Therefore, it is plausible that a pull-apart
model cannot explain the genesis of all the collision-related
magmatism in the region. Some other mechanism
must also have been operational. |
|
9.
Inflow of lower crust driven by the isostatic
response to denudation and sedimentation in surrounding
areas [Mitchell & Westaway, 1999]. |

Figure
29 |
|
On the basis of their study
of Neogene-Quaternary uplift and magmatism in
the Greater Caucasus, Mitchell & Westaway
[1999] proposed an alternative model to explain
the formation of high mountain ranges and plateaus
such as the Greater and Lesser Caucasus including
the Armenian highlands adjacent to Northeastern
Anatolia. They argue that the rate and spatial
scale of uplift of the Caucasus are too great
to be the result of plate convergence alone, and
therefore some other processes must have been
operational.
Mitchell &
Westaway [1999] argue that when crustal material
is hotter than 300°C, it starts to behave
in a ductile way, deforming plastically. The depth
at which this temperature is reached (~ 15-20
km) broadly corresponds to the boundary between
the plastic lo | | | |