Gigantism in Unique Biogenic Magnetite at the Paleocene–Eocene Thermal Maximum

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Gigantism in Unique Biogenic Magnetite at the Paleocene–Eocene Thermal Maximum Gigantism in unique biogenic magnetite at the Paleocene–Eocene Thermal Maximum Dirk Schumann*†, Timothy D. Raub‡, Robert E. Kopp§, Jean-Luc Guerquin-Kern¶ʈ, Ting-Di Wu¶ʈ, Isabelle Rouiller†**, Aleksey V. Smirnov††, S. Kelly Sears†**, Uwe Lu¨ cken‡‡, Sonia M. Tikoo‡, Reinhard Hesse*, Joseph L. Kirschvink‡, and Hojatollah Vali*†**§§ *Department of Earth and Planetary Sciences, McGill University, 3450 University Street, Montre´al, QC, Canada H3A 2A7; †Facility for Electron Microscopy Research, and **Department of Anatomy and Cell Biology, McGill University, 3640 University Street, Montre´al, QC, Canada H3A 2B2; ‡Division of Geological and Planetary Sciences, California Institute of Technology, MC 170-25 1200 East California Boulevard, Pasadena, CA 91125; §Department of Geosciences and Woodrow Wilson School of Public and International Affairs, Princeton University, 210 Guyot Hall, Princeton, NJ 08544; ¶Imagerie Inte´grative de la Mole´cule a`l’Organisme, Institut National de la Sante´et de la Recherche Me´dicale, Unite´759, Institut Curie, 91405 Orsay, France; ʈLaboratoire de Microscopie Ionique, Institut Curie, 91405 Orsay, France; ††Department of Geological and Mining Engineering and Sciences, Michigan Technological University, Houghton, MI 49931-1295; and ‡‡Nanobiology Marketing, FEI Company, Eindhoven, 5600KA, Eindhoven, The Netherlands Edited by James Zachos, University of California, Santa Cruz, CA, and accepted by the Editorial Board August 29, 2008 (received for review April 15, 2008) ) ) We report the discovery of exceptionally large biogenic magnetite t % quartz sand (FMR) m m legend e e ( ( lithology crystals in clay-rich sediments spanning the Paleocene–Eocene h p d 0 25 50 0.30 0.35 0.40 164 g Thermal Maximum (PETM) in a borehole at Ancora, NJ. Aside from previously described abundant bacterial magnetofossils, electron g g silty clay g microscopy reveals novel spearhead-like and spindle-like magne- 165 165.20 tite up to 4 ␮m long and hexaoctahedral prisms up to 1.4 ␮m long. clay Manasquan Formation 165 .55 Similar to magnetite produced by magnetotactic bacteria, these 165. 81 166 sandy to single-crystal particles exhibit chemical composition, lattice per- clayey silt fection, and oxygen isotopes consistent with an aquatic origin. Electron holography indicates single-domain magnetization de- GEOLOGY 167 clay and spite their large crystal size. We suggest that the development of silty clay a thick suboxic zone with high iron bioavailability—a product of g 1 67 .70 g dramatic changes in weathering and sedimentation patterns glauconite 168 driven by severe global warming—drove diversification of mag- 168.1 7 netite-forming organisms, likely including eukaryotes. CIE 168.81 burrows 169 ͉ ͉ 169. 1 1 biomineralization electron microscopy magnetofossil bacterial 169 .53 magneto- fossils 169 .89 agnetofossils, geologically preserved magnetic particles PETM clay Marlboro-equivalent 170 170 .03 Mproduced most abundantly by magnetotactic bacteria, are 170. 41 elongated, 170. 56 prismatic recognized by distinctive physical and chemical traits and pro- full magnetic particle response vide a record of past microbial ecosystems (1–3). Two recent 171 171.22 papers (4, 5) report an extraordinary magnetofossil ‘‘Lager- onset magnetic spearhead sta¨tte’’in lowermost Eocene kaolinite-rich clay sediments de- response particle 171 .95 posited at subtropical paleolatitude in the Atlantic Coastal Plain 172 Ϸ spindle of New Jersey. The sediments were deposited 55.6 million shaped g g Vincentown Vincentown Formation particle years ago during the Paleocene–Eocene Thermal Maximum g 173 g (PETM), an Ϸ100- to 200-ky interval of Ϸ5–9°C abrupt global -2 0 2 sampling depth (m) and 13C type of magnetofossil warming (5, 6). Kopp et al. (4) and Lippert and Zachos (5) use inorg ferromagnetic resonance (FMR) spectroscopy (7), other rock Fig. 1. Lithological profile of late Paleocene and early Eocene strata of ODP magnetic methods, and transmission electron microscopy Leg 174AX, Ancora, NJ, plotted together with the fine quartz sand fraction, ␦13 ␣ (TEM) of magnetic separates to characterize sediments from Cinorganic, and FMR parameter . The profile shows the abundance of boreholes at Ancora (ODP Leg 174AX) (Fig. 1) and Wilson different types of magnetite particles at examined sample horizons [lithologi- Lake, NJ, respectively. These sediments contain abundant, Ϸ40- cal information from Miller et al. (37)]. Fine quartz sand fraction and ␦13 ␣ to 300-nm cuboidal, elongate-prismatic, and bullet-shaped mag- Cinorganic are from Kent et al. (38). FMR parameter were taken from Kopp netofossils, sometimes arranged in short chains, resembling et al. (4). crystals in living magnetotactic bacteria (4, 5). Despite scarcity of intact magnetofossil chains, the asymmetry ratios of the FMR and previously unknown types of magnetofossils and uniquely spectra reflect a profusion of elongate SD crystals and/or chains large exemplars of a more common morphology. The first type [FMR and Rock Magnetic Properties in supporting information of particle has a spearhead-like shape with flattened, bilateral (SI) Text]. It is not obvious whether the unusual abundance of magnetofossils reflects extraordinarily favorable preservation conditions or whether ecological changes enhanced growth of Author contributions: D.S. and H.V. designed research; D.S., J.-L.G.-K., T.-D.W., I.R., S.K.S., magnetotactic bacteria. Here we address both conundrums by U.L., and H.V. performed research; D.S., T.D.R., R.E.K., I.R., A.V.S., S.M.T., R.H., J.L.K., and reporting the discovery from these same sediments of excep- H.V. analyzed data; and D.S., T.D.R., R.E.K., S.M.T., J.L.K., and H.V. wrote the paper. tionally large and novel biogenic magnetite crystals unlike any The authors declare no conflict of interest. previously reported from living organisms or from sediments. This article is a PNAS Direct Submission. J.Z. is a guest editor invited by the Editorial Board. §§To whom correspondence should be addressed. E-mail: [email protected]. Results and Discussion This article contains supporting information online at www.pnas.org/cgi/content/full/ Scanning Electron Microscopy (SEM) and TEM. SEM and TEM 0803634105/DCSupplemental. analysis of the magnetic extracts reveals the presence of two large © 2008 by The National Academy of Sciences of the USA www.pnas.org͞cgi͞doi͞10.1073͞pnas.0803634105 PNAS Early Edition ͉ 1of6 Downloaded by guest on September 23, 2021 A B f tip is 3 (I) xa C D aix s2 a1xis (II) {31 1} (III) (IV) {31 1} {220} Fig. 2. SEM images and drawings showing the morphological features of the spearhead-like magnetite particles. (A and B) SEM images of spearhead-like magnetite particles with pronounced growth steps in the stalk and lower part and well developed crystal faces near the spearhead tip. (C) SEM image of the spearhead-like particle reveals bilateral symmetry. Note abundant conventional magnetofossils surrounding the gigantic spearhead-like particles. (D) Models of idealized crystal habits of the spearhead-like particle shown in A constructed on the basis of the lattice fringe data obtained by HRTEM. These models show the top view (I), lateral view (II), back view (III), and front view (IV). symmetry (Fig. 2 A–C). These particles were possibly disaggre- and c). The {111} lattice fringes have a d-spacing of 0.48 nm and gated from originally agglutinated, remarkable cellular armor are nearly parallel to the long axis (axis 1) of the particle (Fig. (Fig. S1 and Movie S1). Their morphology can be described by 3B and Fig. S2c). Another set of lattice fringes with d-spacing of a geometric three-axis coordinate system (Fig. 2D) that is not 0.296 nm are almost parallel to less-pronounced crystal faces at coincident with the crystallographic system. Length (axis 1) the tip (Fig. 3B) and tail sections of the particle and correspond ranges from 2.0 to 3.8 ␮m, width (axis 2) ranges from 1.0 to 1.4 to {220} fringes. HRTEM images show sets of lattice fringes with ␮m, and thickness (axis 3) ranges from 0.65 to 0.7 ␮m. The apex d-spacing of 0.25 nm parallel to four pyramidal sides that sector is characterized by well pronounced crystal faces resem- correspond to the {311} family of magnetite. The middle and bling a six-sided pyramid-like structure. ‘‘stalk’’ sectors of some particles show circumferential steps on High-resolution TEM (HRTEM) of whole particles and of an the crystal surfaces (Fig. 2 A, B, and DIand II) indicating ultrathin section prepared by focused ion beam (FIB) milling ontogenetic crystal growth from ‘‘stalk’’ toward crystal ‘‘tip’’ reveals that the spearhead-like particles are single, defect-free (Fig. 4). These steps, ranging from 10 to 29 nm, are pronounced crystals of magnetite (i.e., magnetofossils) (Fig. 3 and Fig. S2 b Spearhead-like magnetite allometry: lengthwise head growth at constant stalk width { A B 20}2 1.4 4.0 3.5 D 1.2 3.0 µ 1.0 µ 2.5 0.8 2.0 0.6 head width/ stalk width 1.5 0.48 nm field 0.4 spearhead width ( m) 1.0 spearhead length ( m) 0.2 0.5 0 0 0 0.1 0.2 0.3 0.4 00.1 0.2 0.3 0.4 stalk width (µ m) stalk width (µ m) Fig. 4. Allometry of the spearhead-like particles. Variance in stalk width and 1mµ 5 nm spearhead width are both Ϸ3.6% of those respective means. Variance in spearhead length, by contrast, is Ͼ15% of mean spearhead length, suggesting that spearhead-like particles continue to grow lengthwise after they reach a Fig. 3. Low-resolution TEM image of a random projection of a spearhead- (perhaps itinerantly) maximum width and maintain a constant proportion like particle (A) and a HRTEM image (B) of the tip of the same crystal showing between stalk and spearhead.
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