Most tektite strewn fields have now been associated with a particular impact structure with an established age directly relating the tektite to its corresponding ejecta deposit: Moldavites with the Ries Crater in Germany, Ivory Coast tektites with the Bosumtwi crater in Ghana, and the North American tektites with the Chesapeake Bay Impact Crater. The largest known strewn field, encompassing the Austalasian tektites, has yet to be identified with a particular impact structure, but it has been suggested that this event may reflect an aerial burst similar to the event over Tunguska, Siberia, and that which produced Libyan Desert Glass in Egypt. Still, recent gravity and topography data from Seasat and Geosat has identified an ~100-km circular feature off the coast of Vietnam in the South China Sea centered at 13.6° N., 110.5° E., which could prove to be the elusive crater. Geochemical data suggest that these tektites sample typical post-Archean sedimentary, upper crustal rocks.
Lechatelierite, a form of fused quartz, and other relict mineral inclusions showing evidence of shock metamorphism, are found inside tektites, consistent with an impact origin rather than one based on igneous volcanism. Moreover, the high-pressure polymorph of quartz known as coesite has been identified in tektites, indicating pressures greater than 2 GPa. Elemental abundance patterns, along with size and shape characteristics of the mineral inclusions, suggest that the typical parent material for tektites was a terrestrial, fine-grained, sedimentary deposit similar to a graywacke or loess.
One revealing fact in the origin debate is that no tektites have ever been found in Antarctica, where meteorites from most all classes have previously been recovered, including many lunar specimens. A major point of contention held by the lunar-origin theorists (Futrell and O'Keefe, 1997) has been the very low content of water in tektites compared to the terrestrial source rock. A recent study into the physics and chemistry of impact melting and vaporization explains this lack of water as a natural outcome of the thermodynamics associated with shock pressures in excess of 100 GPa and temperatures in excess of 50,000°C. Under these conditions, volatile-containing bubbles would carry all of the water vapor out of the silicate droplets, along with free oxygen, leading to reduction of Fe and the formation of the dark green to black colors associated with tektites. Furthermore, lunar rocks contain still less water than tektites do.
Recoveries of some Indochinite tektites with signs of stretching during flight provide more evidence for an impact origin rather than an extraterrestrial origin. If these features had been the result of etching by soil acids, as some have argued, the stretch areas would have been etched to a similar degree as
the rest of the tektite, which is not the case. This leads to the conclusion that these features were formed by aerodynamic sculpting instead. The internal heating demonstrated by the plastic stretching is also further evidence that the tektites did not arrive on Earth as individuals, in which case the only heating effects would be those on the exterior caused by heating during entry. Instead, these features were the result of spallation on a large, rapidly rotating body within the atmosphere.
The photo above shows four members of the ~803 t.y. old Australasian strewn field, which covers at least one-tenth of the Earth's surface. Other tektite sources likely encompasssed by this strewn field include those from Tibet, the Phillipines (Rizalite, Bikolite, Anda) and Java. Based on the spatial variation in microtektite concentrations from deep-sea drilling cores, the probable location for the source crater is determined to be in eastern Cambodia (12° N., 106° E.), in agreement with previous predictions. The diameter of the source crater is estimated to be 90116 km.
The button/lens-shaped Australite above, which was the first type of tektite described in the literature by naturalist Charles Darwin, exhibits typical concentric ring-wave flow ridges on the forward face emanating from the stagnation point, consistent with aerodynamically stable hypervelocity ablation during descent. The Muong Nong-type layered tektites are thought to have formed close to the source crater, consistent with their lack of ablation features and a recovery location very near that predicted for the source crater. Also pictured above is a tektite-like glass, a Colombianite (or Amerikanite), which is now thought to be of terrestrial volcanic origin due to its high water content, in spite of its strong resemblance to a tektite.
The last photo shown above is a mass of Libyan desert glass (LDG), melted silica glass thought to have been formed by the intense heat of a meteoric aerial burst over sand dunes of the Great Sand Sea in western Egypt, ~28.5 m.y. ago. However, a study of C and Cl in LDG indicates quenching upon impact of a carbon-rich projectile with silica-rich crustal rocks and sea-water, rather than impacting on dry land (Miura, 2009). It has been estimated that at least 10 million tons of LDG were created in a region extending over an area of ~8025 km², of which 20 tons has been collected (Pratesi et al., 2002). A small, extensively weathered fragment of oxidized iron showing remnants of an octahedral structure (named Great Sand Sea 003) is possibly associated with this event. The energy released during this explosion is calculated to have been equivalent to that of the Tunguska event.
Similar to LDG, the high-silica Dakhleh Glass (DG) from the Dakhleh Oasis in the Western Desert of Egypt, derives from a low-altitude airburst ~120 (±40) t.y. ago into Pleistocene lacustrine sediments (Osinski et al., 2008). Many of the black to dark-gray DG specimens are vesiculated on the upper surface, sometimes exhibiting impressions of grass and reed vegetation on the underside, some containing burnt sediments. Dakhleh Glass is predominantly a mixture of glass and crystallites.
Resulting high-temperature melt-products identified in LDG glass include lechatelierite and cristobalite from quartz, and baddeleyite from zircon. Cathodoluminescence imaging has identified previously unrecognized quenched flow textures in this glass, potentially useful for characterizing the temperature of formation (Gucsik et al., 2003); temperatures in the 17002100°C range have now been calculated (Pratesi et al., 2002). These rare brown to bluish (from Rayleigh scattering by 60 nm-sized or smaller particles) streaks have been resolved into discrete rounded glass spherules which constitute an immiscible liquid within the silica-glass matrix. These spherules are enriched in Al, Fe, and Mg, as well as Ir, Os, Cr, Co, and Ni, elements which may reflect a significant meteoritic component. Graphite ribbons, possibly derived from the impactor, have also been identified.
Brecciated sandstone samples from the LDG area show signs of fractures, mosaicism, undulatory extinction, and cleavage. Planar deformation features and other shock features provide persuasive evidence for a hypervelocity impact origin. Geochronological data and isotopic ratios of Sr and Nd indicate that the target material was sand, derived from Precambrian crustal granitic rock, rather than Lower Cretaceous sandstones of the Nubia Group.
The photo shown below is an artifact recovered from King Tutankhamun's tomb. This pectoral fearures a yellow-green gem in the image of a scarab, carved from a piece of Libyan Desert Glass. This demonstrates the special nature of this material to the early Egyptian civilization.
Pictured below is an olive-green, filigree-like moldavite, a member of the Central European strewn field associated with the 14.68 (±0.11) m.y. old, 24-km-wide Nördlinger Ries impact crater in Germany (Laurenzi et al., 2003; Vincenzo and Skála, 2008). The 3.8-km-wide Steinheim Basin crater, located 42 km west-southwest of the Ries crater, is considered to have been formed during the same event, attesting to a binary asteroid impact. Through 3-D hydrocode simulations (Stöffler et al., 2002), it was determined that the two impact projectiles, with diameters of 1.5 km and 0.15 km, impacted at an angle of 3050° from the horizontal at a velocity of ~20 km/s. The leading shock wave impacted the target material, consisting of both weathered and unweathered, unconsolidated, Middle Miocene silica-rich sands, with lesser amounts of clays and carbonates, generating temperatures of ~40,000°C (Skála et al., 2008). The superheated melt was distributed up to 400500 km away in a symmetrical, ~60° fan-shaped jet, the remnant of which today is represented by the moldavite strewn subfields of South Bohemia, Moravia, the Cheb Basin, northern Austria, and Lusatia. Rapid cooling and solidification of the melt ensued, leading to the formation of tektites.
Moldavites accumulated from melt particles of variable chemical composition. The ultimate shape of moldavites is a result of etching by groundwater in an acidic, permeable environment. They are virtually water-free and incorporate cations that reflect differentiation based on ionic size, a result of their formation (fractional condensation) at plasma temperatures (von Engelhardt et al., 2005). Shock forces from the Ries impact created shattercones in the limestone layer below.
The four photos below represent tektites from the two remaining recognized strewn fields, along with an impact glass similar in composition to the LDGs:
Still other impact glasses have been found to be associated with craters: