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Tectonic Aneurysms occur in areas in which uplift is forced by surface erosion creating a weakness in the crust such as the Nanga Parbat. They result from a positive feedback mechanism caused by the interaction between meteorological erosion within tectonically active landscapes. Exhumation by fluvial or glacial processes results in localized crustal thinning and weakening which alters the deep crustal heat flow regimes. The thin crust acts as a weakness allowing greater geothermal heat flow than the surrounding areas driving localized deformation. Geographically, tectonic aneurysms can only occur in areas with intensive, continuous erosion that is sustained for long periods of time which can be fluvially or glacially derived. Modeled active systems must also occur in tectonically active areas with relatively shallow heat flow in order to drive the deformation. Moreover, the rheology of the crustal material must permit melting at relatively low temperatures characteristic of upper continental crust.These factors are met in several areas of young mountain belts on Earth which have areas with large relief over short distances.Most proposed tectonic aneurysms occur at syntaxial areas or bends which focus compressional stresses into a small region at plate boundaries.

Figure 1: A diagram of a young tectonic aneurysm. Isothermal gradient anticline caused by channel incision creating a thinner crust than the surrounding. Strain is focused into weakness forcing warm material into the zone thereby lifting isotherms locally
Figure 2: An advanced tectonic aneurysm. Isothermal gradient becomes more advanced than in the young stage. Material flow causes surface uplift of young rock on the peripheral edges of the erosion area. The uplift brings weak warm rocks to the surface and creates high relief. This causes accelerated mass wasting and easier erosion thereby enforcing the positive feedback


Figure 3: This diagram contrasts the crustal strength of a landscape with significant localized erosion(Blue Dashed Line) when compared to an unmodified landscape (Green Dashed Line). The strength profile illustrated in the diagram is only in the brittle zone with an assumed constant increase with depth on the basis of increased pressure with increased overlying mass.

Deformation Mechanism

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Deformation caused by tectonic aneurysms are similar to aneurysms in blood vessels in which weakening of the confining force allows for localized growth or uplift. However, in the geological setting, deformation occurs over millions of years with significant sustained erosion power ranging from 10s to 100s of kiloWatts per meter[1]. Incision or crustal thinning of an area on the surface relative to the background crust thickness causes two things to occur that allow for aneurysm formation. Firstly, due to the brittle nature of crustal rocks and their pressure dependent strength, the decrease in overlying material depresses the crustal strength when compared to surrounding areas. This occurs because the removal of crust decreases the overburden and thus the pressure which influences the strength. Secondly, the geothermal gradient increases vertically. Localized deep valleys create weakest areas that focus strain and thereby the movement of deep ductile material.

By weakening the crust in a localized area, a preferential region of strain can develop concentrating the flow of material. Ductile rocks deeper in the crust will be able to move towards the potential gradient, whereas brittle rocks near the surface will fracture when subject to increased strain. The transition between brittle deformation and ductile deformation is determined by the temperature which is generally controlled by depth as well as rheology. Weak hot minerals, below the ductile transition, with significant partial melt move into the area underlying the thinned crust as a result of the pressure gradient being decreased in the thin area. At a certain point, the pressure will decrease substantially moving from convergent basement rock into thinned crust. This causes rapid decompression at relatively stable and raised isotherms. Decompression melting occurs, which increases the proportion of partial melt within the material and causes rapid heat advection towards the surface. Continued convergent plate movement focuses the flow of material into the syntaxial areas with the localized weakness permitting upward escape as an accommodation mechanism. This process solves the fundamental problem of material being forced into a confined space by creating an outlet. The result of which creates a positive feedback with erosion focusing uplift which transports more weak rock vertically enhancing erosive capabilities. Areas of consistent elevation in river valleys and mountains with relief can be maintained by high exhumation rates of relatively young weak rocks. The ages of minerals in the area will be younger than the surrounding crust due to cooling occurring in an area with a steeper thermal gradient at shallower depths. Mature tectonic aneurysm systems, such as the Nanga Parbat, can have very high local reliefs of young rocks due to consistent erosion maintaining the elevation in the erosive area and vertical strain forcing material up along the proximal edges.

Locations

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Tectonic aneurysms are found in areas with localized high relief of relatively young rocks when compared to their surroundings. Actively observed systems that have been studied the most are located in 2 main regions of the Himalaya, the Nanga ParbatHaramosh Massif and Namche BarwaGyala Peri which occur on the Eastern and Western edges respectively. The Indus River is the mechanism responsible for crustal removal in the Nanga Parbat region, and the Tsangpo River is active in the Namche Barwa region.

Proposed tectonic aneurysms are located in the Saint Elias region of Alaska, the Kongur Shan and Muztagh Ata in China, and The Lepontine Dome in the Swiss Alps. These locations show incipient or similar, less significant characteristics to actively observed systems. Glacial mechanisms of erosion and transport are believed to be responsible in many alpine areas including the Saint Elias system.

Nanga Parbat-Haramosh Tectonic Aneurysm

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The Nanga Parbat-Haramosh is the most studied region in the context of tectonic aneurysms. The region has extreme relief over very short distances with the Indus River valley approximately 7 kilometers lower in elevation than the peak of the mountain. Within the study area, Biotite cooling ages (280°C ± 40°C) are consistently less than 10 million years old indicating rapid exhumation rates in the area[1]. Studies of composition and structure of the rocks in the area suggest exhumation of depths below 20 kilometers[1] .Exhumation rates from the massif and the valley are significantly higher than background rates. Calculations of peak exhumation rates range from 5 to 12 mm per year [1] depending on the location.The mountain top has a lower rate than the bottom of the valley yet both are significantly higher when compared to background rates outside of the syntax. Exposed granulite within the central aneurysm area represents low-pressure melting and advection as material moved into areas with decreasing pressure. Up to 20 kilometers of domal unroofing over a very short period of time has been inferred based on the sample ages ranging from 1 to 3 million years [1].

Namche Barwa-Gyala Peri

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The Namche Barwa-Gayla Peri tectonic aneurysm is located on the Eastern side of the Himalaya with the active Tsangpo River flowing down the valley between the mountains. Many researchers conclude the tectonic aneurysm model is the best explanation of the observed structures and tectonic arrangement of the region. The Argon-Argon Biotite ages and Zircon fission track ages of rocks from the area are 10 million years old or less[1], which is young compared to the surrounding rocks. Similar high reliefs seen in the Nanga Parbat are also evident with the Namche Barwa region, with approximately 4 kilometers of vertical elevation change over a short horizontal distance[1]. High and low-grade metamorphic rocks are found in the region with evidence to suggest a variation of metamorphic activity between regions from the strain center and the edges. The exhumation occurs in a circular area with young, high-grade decompression melts focused in the center[1]. Around the outside of the focus rubidium to strontium ratios suggest melting with fluid present[2]. The presence of fluid within melt has been modeled to occur as a result of immense precipitation allowing water to penetrate into shallow crustal rocks over long periods of time. Ages and barometric regimes of the rocks were used to calculate the volume of overburden removed, which was used to determine 3 millimeters of annual incision over the last 10 million years[1].

Saint Elias

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The proposed 4 million years old tectonic aneurysm system in the St. Elias Mountains in Alaska was formed by glacial erosion on the mountains developed by underthrusting of the Yakutat microplate beneath the North American margin. The aneurysm occurs in the Northern plate corner in which transitions from dextral strike-slip motion to thrust sense motion thereby focusing strain. The interpreted relationship between erosion mountain development has more variations between researchers than Himalayan systems due to the age of the system and constraints regarding field work due to glacier cover. In the St. Elias range collision and underthrusting caused surface uplift forming mountains. The elevation increase climate regime allowed glacier development resulting in extreme glacial erosion potential. Since its inception, glacial erosion transported sediments West into the Pacific Ocean and onto the continental margin. After which, approximately 2 million years ago, the formation of a decollement caused the locus of strain to propagate South☃☃. The shift in strain focus resulted in mountain development farther South which disrupted the climatic system thereby decreasing precipitation in Northern regions of the St. Elias[3]. The erosion and exhumation are now concentrated on the Southern portion of the mountain range which produces young cooling ages associated with the current tectonic aneurysm center.

Young detrital zircon fission track(240°C ± 40°C) and apatite fission track and Uranium -Thorium/ Helium (110°C ± 10°C) cooling ages of sediments in glacial catchment areas[3] support the theory of erosive influence on the St. Elias tectonic system. Rates of exhumation were inferred by calculating the difference between detrital zircon and apatite ages in sediments. The smaller the difference between zircon and apatite ages represents a faster movement of material through the isotherms and faster cooling. In the northern corner of contact between the plates, the zircon and apatite ages do not differ significantly, thereby providing evidence of rapid exhumation. The proximity to the depositional environment along the coastal margin and within fjords preserves a record of sedimentation rate which is used to interpret exhumation rates of 0.3mm year originally and approximately 1.3mm/year for the last million years[3]. The sediment age and thickness are used to track the movement of the focus of erosion from the North to the South.

The presence of a definitive tectonic aneurysm system in the region is widely disputed with many researchers concluding insufficient focused exhumation is occurring to support the hypothesis. Significant glacial cover limits the number of field samples and geological observations that can be made directly on the surface thereby adding uncertainty to interpretations. Alternative theories argue tectonic transpressional control of exhumation with little erosive influence on the overall system. Younger ages are explained by focused strain areas resulting from faulting.

Field Work in Proposed Regions

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By comparing the depth in Earth at which particular minerals crystallize and the elevation at which they were sampled, the age of minerals can be used to determine the rate which the strain zone moved material vertically. Various dating methods on specific fluid inclusions and minerals were used in order to provide chronological data of the exhumation rate of rocks in the area. The age dates were used to reconstruct the history of exhumation and thermal regimes by comparing them to pressure and temperature crystallization boundaries of the minerals. Uranium-Thorium and Uranium-Helium [1] [4] [2] [3] cooling ages of samples of apatite indicate the timing of 70°C cooling. Higher closure temperatures were dated using Argon-Argon methods for biotite samples (300°C) [1]and zircon fission-track (230°C - 250°C)[1] methods. By analyzing the ages of minerals with various closure temperatures, researchers can infer the speed at which they moved through the isotherms. When the difference between the age of a mineral that cooled at a high temperature and one that cooled at a low temperature are relatively similar, then exhumation is inferred to be rapid. The geothermobarometry is obtained using garnet-biotite plagioclase in order to constrain higher pressure metamorphic regimes[2]. Shallower exhumation rates (low-temperature cooling ages) alone can not realistically be used to describe tectonic aneurysms as deep isothermal gradient changes may not significantly affect shallower depths. Furthermore, shallow low-temperature cooling can be more largely related to erosion dominated exposure rather than tectonic driven uplift. Sample ages from minerals with higher cooling temperatures signify exhumation of deeper material which is the modeled function of a tectonic aneurysm.

Seismic velocity profiles are often used over large study areas in order to identify possible isothermal irregularities[1]. Low-velocity data is indicative of hotter rocks with a higher degree of the partial melt which slows P waves when compared to the surroundings. Magnetotelluric sampling is done to test the resistivity of the rocks which is used to infer the amount of fluid in the rocks[1].

References

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[5] [6] [7] [8] [9] [10] [11] [12] [13] [14] [15]

  1. ^ a b c d e f g h i j k l m n Zeitler, P., Hallet, B., & Koons, P. (2013). Tectonic aneurysms and mountain building
  2. ^ a b c Booth, A. L., Chamberlain, C. P., Kidd, W. S. F., & Zeitler, P. K. (2009). Constraints on the metamorphic evolution of the eastern himalayan syntaxis from geochronologic and petrologic studies of namche barwa. GSA Bulletin, 121(3-4), 385-407. doi:10.1130/B26041.1
  3. ^ a b c d Spotila, J. A., & Berger, A. L. (2010). Exhumation at orogenic indentor corners under long-term glacial conditions: Example of the st. elias orogen, southern alaska. Tectonophysics, 490(3), 241-256. doi:10.1016/j.tecto.2010.05.015
  4. ^ Finnegan, N. J., Hallet, B., Montgomery, D. R., Zeitler, P. K., Stone, J. O., Anders, A. M., & Yuping, L. (2008). Coupling of rock uplift and river incision in the namche barwa-gyala peri massif, tibet. GSA Bulletin, 120(1-2), 142-155. doi:10.1130/B26224.1
  5. ^ Zeitler, P., Hallet, B., & Koons, P. (2013). Tectonic aneurysms and mountain building
  6. ^ Ernst, W. G. (2006). Preservation/exhumation of ultrahigh-pressure subduction complexes. Lithos, 92(3), 321-335. doi:10.1016/j.lithos.2006.03.049
  7. ^ Garzanti, E., & Malusà, M. G. (2008). The oligocene alps: Domal unroofing and drainage development during early orogenic growth. Earth and Planetary Science Letters, 268(3), 487-500. doi:10.1016/j.epsl.2008.01.039
  8. ^ Spotila, J. A., & Berger, A. L. (2010). Exhumation at orogenic indentor corners under long-term glacial conditions: Example of the st. elias orogen, southern alaska. Tectonophysics, 490(3), 241-256. doi:10.1016/j.tecto.2010.05.015
  9. ^ Enkelmann, E., Koons, P. O., Pavlis, T. L., Hallet, B., Barker, A., Elliott, J., Garver, J., Gulick, S. P. S., Headley, R. M., Pavlis, G.L., Ridgway, K.D., Ruppert, N., Van Avendonk, Harm J. A. (2015). Cooperation among tectonic and surface processes in the st. elias range, earth's highest coastal mountains. Geophysical Research Letters, 42(14), 5838-5846. doi:10.1002/2015GL064727
  10. ^ Finnegan, N. J., Hallet, B., Montgomery, D. R., Zeitler, P. K., Stone, J. O., Anders, A. M., & Yuping, L. (2008). Coupling of rock uplift and river incision in the namche barwa-gyala peri massif, tibet. GSA Bulletin, 120(1-2), 142-155. doi:10.1130/B26224.1
  11. ^ Booth, A. L., Chamberlain, C. P., Kidd, W. S. F., & Zeitler, P. K. (2009). Constraints on the metamorphic evolution of the eastern himalayan syntaxis from geochronologic and petrologic studies of namche barwa. GSA Bulletin, 121(3-4), 385-407. doi:10.1130/B26041.1
  12. ^ Whipp, D. M., Beaumont, C., & Braun, J. (2014). Feeding the “aneurysm”: Orogen-parallel mass transport into nanga parbat and the western himalayan syntaxis: HIMALAYAN STRAIN PARTITIONING. Journal of Geophysical Research: Solid Earth, 119(6), 5077-5096. doi:10.1002/2013JB010929
  13. ^ Koons, P. O., Zeitler, P. K., Chamberlain, C. P., Craw, D., & Meltzer, A. S. (2002). Mechanical links between erosion and metamorphism in nanga parbat, pakistan himalaya. American Journal of Science, 302(9), 749-773. doi:10.2475/ajs.302.9.749
  14. ^ Zeitler, P. K., Koons, P. O., Bishop, M. P., Chamberlain, C. P., Craw, D., Edwards, M. A., . . . Shroder, J. F. (2001). Crustal reworking at nanga parbat, pakistan: Metamorphic consequences of thermal‐mechanical coupling facilitated by erosion. Tectonics, 20(5), 712-728. doi:10.1029/2000TC001243
  15. ^ Finlayson, D. P., Montgomery, D. R., & Hallet, B. (2002). Spatial coincidence of rapid inferred erosion with young metamorphic massifs in the himalayas. Geology, 30(3), 219. doi:10.1130/0091-7613(2002)030<0219:SCORIE>2.0.CO;2