Authors' Reply

Abstract— Jull et al. propose an alternative interpretation of our depth vs. ¹⁴C data measured on a peat core from the central Tunguska impact site (Rasmussen et al., 1999). We find that the proposed alternative is untenable.     

Die Bedeutung der Süddeutschen Großscholle in der Geodynamik Westeuropas

The crustal plate of Southern Germany models, in a highly instructive way, the real behaviour of continental crustal plates in the immediate foreland of an active orogenic mountain belt. The frontier line between alpidic and outer-alpine strain pattern crossed this first order tectonic unit. During Upper Tertiary times, the crustal plate of Southern Germany shows an anticlockwise rotation of the direction of maximal principal stress (from NNE/SSW through NNW/SSE to NW/SE), nearly contemporaneous to the transition from alpine Flysch-to Molasse-to postorogenic sedimentation. From prae-Upper Cretaceous to Oligocene, NNE-SSW-plate movement follows a direction more or less parallel — not perpendicular — to the North Atlantic midocean ridge. Since the Pliocene, the axis of tectonic transport (a in rock fabrics nomenclature) turns to a more northwesterly-southeasterly position, so nearly becoming to the well known sea-floor spreading concept. But, at that time, alpine orogenesis comes to an end. Today, neither in the Alps nor in their foreland, any adequate subduction zone to counterbalance the opening of the North Atlantic (as supposed by means of paleomagnetic data) still exists. Since early Pliocene time, the Southern Germany crustal plate shows, in spite of the overburden by thick Molasse sediments, neither any subsidence nor underthrusting the Alps, but, on the contrary, uplifting in a magnitude up to more than fivehundred meters, while the opening of the North Atlantic seems to continue. So we find some serious inconsistencies between the so called new global tectonics and the tectonic evolution of the Southern Germany crustal plate.     

Kontinentale und marine Senkungsbecken als Ausdruck epirogener Bewegungen

Zusammenfassung Wir unterscheiden innerhalb der Geosynklinalen langgestreckte, schmale kontinentale Stenosynklinalen (besonders der Permzeit) im Gegensatz zu den aus ihnen herauswachsenden breiten, flächenhaften Eurysynklinalen. Während bei der ersten Form keine eigentlichen Geantiklinalen zu beobachten sind, können die Flanken der Eurysynklinalen als Kippungsflächen um eine oder mehrere Achsen (bzw. Achsenbündel) mit aufsteigendem Geantiklinal-Hebelarm und absteigendem Geosynklinalarm aufgefa\t werden.Der Betrag der Senkung wird ausgedrückt durch den stets nur zu errechnenden, niemals zu messenden absoluten oder relativen Senkungswinkel. Der Höchstbetrag der Senkung wird bezeichnet durch den Trogwinkel, d. h. die Abweichung der ganzen Beckenfläche von der ursprünglichen Horizontalebene. Der Durchschnitts-Senkungswinkel ist bei den Eurysynklinalen nur durch Bogenminuten oder -Sekunden auszudrücken. Senkungs- und Trogwinkel sind in der Mitte der Senke am kleinsten, wachsen dann nach den Rändern hin etwas an, um nach den Rändern hin schlie\lich wieder abzunehmen; nur bei den Stenosynklinalen kann der Trogwinkel auf wenige Grade anwachsen.Das Wachsen der Sedimentationsräume ist bedingt durch Zunahme des Senkungswinkels. Verschiebt sich die Kippungsachse gegen das Senkentiefste, so steigt bei gleichbleibender Kippungstendenz das zwischen der alten und neuen Achse gelegene Stück wieder auf, es beginnt das Schwinden des Sedimentationsraumes, das bei den Stenosynklinalen zu einem völligem Verschwinden durch Zuschüttung wird.Im Bereich der Kippungsachse findet, sofern diese nicht gerade untermeerisch liegt, weder Ablagerung noch Abtragung statt, während mit wachsender Entfernung von ihr im sinkenden Hebelarm Vermehrung der Ablagerungen, im aufsteigenden Hebelarm Verstärkung der Abtragung eintritt.     

Synthetic seismograms from generalized ray tracing1

A new method of numerical computation of elastic wavefields in regions containing caustics is tested. The method is an extension of the asymptotic ray theory (ART). The essential features of the method consist of the application of expressions which are well defined at caustics and expressed in terms of ray tracing combined with complex ray tracing in caustic shadows. The method and an outline of the underlying theory are briefly presented, followed by a comparison with finite differences on a test model involving a caustic cusp. The comparison reveals the unexpectedly high degree of accuracy of the new method.     

Estimating Deep Seafloor Interface and Volume Roughness Parameters Using the Multibeam-Hydrosweep System

Utilizing a hull-mounted, multinarrow beam echosounder onboard RV Polarstern, we measured variation of acoustic backscatter with incidence angles at two different sites in the Southern Oceans (Agulhas Plateau and the Riiser Larsen Sea). We modeled the data, using a composite roughness model, including water-sediment interface roughness and sediment volume roughness parameters. The model effectively uses the near normal incidence angle backscatter to determine the seafloor interface roughness parameters employing Helmholtz-Kirchhoff theory. Beyond 20° incidence angles, an application of Rayleigh-Rice theory is made by using a necessary splicing technique (combining both of the theories at 20° incidence angle). The estimated interface and volume roughness parameters are found to be in accordance with the known area geology.     

Contrasting rifted margin styles south of Greenland: implications for mantle plume dynamics

We present new and reprocessed seismic reflection data from the area where the southeast and southwest Greenland margins intersected to form a triple junction south of Greenland in the early Tertiary. During breakup at 56 Ma, thick igneous crust was accreted along the entire 1300-km-long southeast Greenland margin from the Greenland Iceland Ridge to, and possibly 100 km beyond, the triple junction into the Labrador Sea. However, highly extended and thin crust 250 km to the west of the triple junction suggests that magmatically starved crustal formation occurred on the southwest Greenland margin at the same time. Thus, a transition from a volcanic to a non-volcanic margin over only 100–200 km is observed. Magmatism related to the impact of the Iceland plume below the North Atlantic around 61 Ma is known from central-west and southeast Greenland. The new seismic data also suggest the presence of a small volcanic plateau of similar age close to the triple junction. The extent of initial plume-related volcanism inferred from these observations is explained by a model of lateral flow of plume material that is guided by relief at the base of the lithosphere. Plume mantle is channelled to great distances provided that significant melting does not take place. Melting causes cooling and dehydration of the plume mantle. The associated viscosity increase acts against lateral flow and restricts plume material to its point of entry into an actively spreading rift. We further suggest that thick Archaean lithosphere blocked direct flow of plume material into the magma-starved southwest Greenland margin while the plume was free to flow into the central west and east Greenland margins. The model is consistent with a plume layer that is only moderately hotter, 100–200°C, than ambient mantle temperature, and has a thickness comparable to lithospheric thickness variations, 50–100 km. Lithospheric architecture, the timing of continental rifting and viscosity changes due to melting of the plume material are therefore critical parameters for understanding the distribution of magmatism.     

Coeval argon‐40/argon‐39 ages of moldavites from the Bohemian and Lusatian strewn fields

Abstract— ⁴⁰Ar/³⁹Ar ages of four tektites (moldavites) from southern Bohemia (near ?eské Budějovice, Czech Republic) and a tektite from Lusatia (near Dresden, Germany) have been determined by 11 step‐degassing experiments. The purpose of the study was to enlarge the ⁴⁰Ar/³⁹Ar data base of moldavites and to check the age relations of the Bohemian and Lusatian samples. The mean plateau‐age of the Bohemian samples, which range from 14.42 to 14.70 Ma, is 14.50 ± 0.16 (0.42) (2σ) Ma (errors in parentheses include age error and uncertainty of standard monitor age). The plateau age of the Lusatian sample of 14.38 ± 0.26 (0.44) (2σ) Ma confirms the previously published ⁴⁰Ar/³⁹Ar age of 14.52 ± 0.08 (0.40) (2σ) Ma, and demonstrates that the fall of Lusatian and Bohemian tektites were contemporaneous. Because of their geochemistry and their ages there is no doubt that the Lusatian tektites are moldavites. Accepting that moldavites are ejecta from the Nördlinger Ries impact, the new ages also date the impact event. This age is slightly younger (about 0.2–0.3 Ma) than the age suggested by earlier K‐Ar determinations.     

Effects of groundwater flow on mineral diagenesis, with emphasis on carbonate aquifers

 This article provides a critical synopsis of the effects of groundwater flow on mineral diagenesis. Emphasis is placed on those aspects and processes that change porosity and permeability in carbonate aquifers, because they are of particular importance to human societies as sources of supplies of water for human consumption (drinking, irrigation) and of crude oil and natural gas. Diagenetic settings in carbonates as well as clastics are generally ill defined. This paper proposes a new comprehensive classification of diagenetic settings into near-surface, shallow-, intermediate-, and deep-burial diagenetic settings; hydrocarbon-contaminated plumes; and fractures. These settings are defined on the basis of mineralogy, petroleum, hydrogeochemistry, and hydrogeology. This classification is applicable to all sedimentary basins. Diagenesis is governed by various intrinsic and extrinsic factors that include thermodynamic and kinetic constraints, as well as microstructural factors that may override the others. These factors govern diagenetic processes, such as dissolution, compaction, recrystallization, replacement, and sulfate–hydrocarbon redox-reactions. Processes such as cementation, dissolution, and dolomitization require significant flow of groundwater driven by an externally imposed hydraulic gradient. Other processes, such as stylolitization and thermochemical sulfate reduction, commonly take place without significant groundwater flow in hydrologically nearly or completely stagnant systems that are geochemically "closed." Two major effects of groundwater flow on mineral diagenesis are enhancement and reduction of porosity and permeability, although groundwater flow can also leave these rock properties essentially unchanged. In extreme cases, an aquifer or hydrocarbon reservoir rock can have highly enhanced porosity and permeability due to extensive mineral dissolution, or it can be plugged up due to extensive mineral precipitation. Received, April 1998 · Revised, July 1998 · Accepted, September 1998