Atomic-Scale Structure of Biogenic Materials by Total X-Ray Diffraction: a Study of Bacterial and Fungal Mnox V

Atomic-Scale Structure of Biogenic Materials by Total X-Ray Diffraction: a Study of Bacterial and Fungal Mnox V

ARTICLE Atomic-Scale Structure of Biogenic Materials by Total X-ray Diffraction: A Study of Bacterial and Fungal MnOx V. Petkov,†,* Y. Ren,‡ I. Saratovsky,§ P. Paste´n,Ќ S. J. Gurr,¶ M. A. Hayward,§ K. R. Poeppelmeier,# and J.-F. Gaillardp †Department of Physics, 203 Dow Science, Central Michigan University, Mt. Pleasant, Michigan 48859, ‡Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, §Inorganic Chemistry Laboratory, University of Oxford, Oxford, U.K. OX1 3QR, ЌPontificia Universidad Cato´lica de Chile, Santiago, Co´digo Postal 690441, Chile, ¶Department of Plant Sciences, Oxford University, Oxford, U.K. OX1 3RB, #Department of Chemistry, Northwestern University, Evanston, Illinois 60202, and pDepartment of Civil and Environmental Engineering, Northwestern University, Evanston, Illinois 60208 urrently, technology is looking for C smaller scale, ordered materials ABSTRACT Biogenic materials are produced by microorganisms and are typically found in a nanophase state. with well-defined properties. As such, they are difficult to characterize structurally. In this report, we demonstrate how high-energy X-ray Nanophase materials are, therefore, being diffraction and atomic pair distribution function analysis can be used to determine the atomic-scale structures of manufactured in increasing numbers.1Ϫ3 MnO produced by bacteria and fungi. These structures are well-defined, periodic, and species-specific, built of Nature is also a prolific producer of x ؊ nanophase materials. A typical example of Mn O6 octahedra forming birnessite-type layers and todorokite-type tunnels, respectively. The inherent this is the microorganism assisted, or bio- structural diversity of biogenic material may offer opportunities for practical applications. genic, oxidation of water-soluble metal ions into insoluble oxides.4 Indeed this process KEYWORDS: biogenic materials · structure determination · X-ray has been taking place for millions of years diffraction · manganese oxides leaving its signature all around: in the sedi- ments on the ocean floor and in the soil on land. Nature‘s evident success is inspiring rials freshly produced by living microorgan- and scientists are trying to employ its tools isms. As an example we consider MnOx pro- for applications including manufacturing of duced by bacteria and fungi. These magnetic nanoparticles5 and capturing of biogenic materials show a length of struc- contaminant metal ions.6Ϫ8 Thus under- tural coherence of about 2Ϫ3 nm only and, standing the way living microorganisms in this sense, are in a nanophase state. Nev- produce materials, in particular nanophase ertheless, their atomic-scale structure is pe- metal oxides, is becoming important not riodic and can be described in simple crys- only for the advance of today’s technology tallographic terms. Surprisingly the crystal but also for remediating some of its un- structures of fungal and bacterial MnOx turn wanted consequences such as metal out to be substantially different indicating pollution. that biogenic materials are inherently struc- One of the most important prerequi- turally diverse. sites to understanding a physicochemical Manganese oxides are ubiquitous in na- process, such as the formation of a ture13 and have been used by mankind for nanophase material, is the knowledge of many thousands of yearsOfirst as pigments the atomic-scale structure of its product. Re- and today as catalysts and battery materi- cently, good progress has been made in de- als. This has generated a long-lasting inter- termining the structure of synthetic (i.e., est in their genesis. Several studies on MnOx man-made) nanophase materials by em- produced by microorganisms have been *Address correspondence to ploying total X-ray diffraction (XRD) involv- carried out but no complete structural de- [email protected]. ing a combination of high-energy XRD and termination has yet been performed. The Received for review October 3, 2008 atomic pair distribution function (PDF) studies have only suggested that bacterial and accepted December 30, 2008. analysis.9Ϫ11 This nontraditional approach MnO is likely to possess a layered-type x Published online January 13, 2009. has also been applied to nanophase materi- structure of the type found in the mineral 10.1021/nn800653a CCC: $40.75 als of geological interest, such as ores.12 birnessite.14,15 Even less is known about fun- 16,17 The approach can also be applied to mate- gal MnOx. © 2009 American Chemical Society www.acsnano.org VOL. 3 ▪ NO. 2 ▪ 441–445 ▪ 2009 441 ARTICLE Figure 2. Fragments from the structures of manganosite (a), lithiophorite (b), chalcophanite (c), birnessite (d), and -birnessite-like “slabs” of Mn؊O6 octahedra separated by re gions scarcely populated with Mn ions and water (lightly shaded) (e). The unit cells in birnessite and bacterial MnOx are outlined with thin solid lines. fuse diffraction patterns are very difficult to analyze by tra- ditional approaches. When considered in real space, in Figure 1. Experimental XRD patterns (upper part) and the terms of the corresponding atomic PDFs however, they corresponding atomic PDFs for crystalline, fungal, and bac- lend themselves to structure search and refinement.21 The terial MnOx. PDF peaks reflecting first neighbor Mn؊O and ؊ Mn Mn correlations are marked with arrows. A model PDF experimental PDFs G(r)ϭ 4␲r[␳(r) Ϫ␳o], where ␳(r) and (line in red) based on the structure of hexagonal birnessite is ␳ are the local and average atomic number density, re- shown as well. o spectively, extracted from the XRD patterns are also Traditionally the three-dimensional (3D) structure shown in Figure 1 (the bottom part). As can be seen in of materials is determined by measuring and analyzing the figure the G(r) for birnessite exhibits a series of well- the positions and intensities of the Bragg peaks in their defined peaks to high real-space distances reflecting the XRD patterns.18 Traditional (i.e. Bragg) XRD studies of presence of a long-range, periodic, atomic ordering. The biogenic materials are possible19 but are difficult and experimental data can be approximated well in terms of a are often imprecise. The reason is that biogenic materi- structure model based on a periodic, hexagonal type lat- als are usually highly dispersed and/or of very low crys- tice (space group, P63/mmc) with parameters a ϭ 2.84(1) tallinity, often contain water and, as such, show diffrac- Å and c ϭ 14.02(1) Å, and Mn at (0,0,0) and oxygen at 2/3, tion patterns with a very few, if any, Bragg peaks and a 1/3, 0.07 positions inside the unit cell. The structure fea- pronounced diffuse component (see Figure 1). Spec- tures layers of edge sharing MnϪO6 octahedra, as shown troscopy techniques like XANES/EXAFS are also widely in Figure 2. The excellent level of agreement between used for structural characterization of materials. For bio- the present and previous literature data23 for the crystal genic materials, spectroscopy techniques may deliver structure of birnessite demonstrate the fact that atomic important information about the valence state of metal PDFs very accurately reflect the 3D atomic ordering in ions and their immediate coordination, but are not ca- materials. pable of elucidating the atomic ordering beyond 5Ϫ6Å As can be seen in Figure 1 the PDFs for both bio- (e.g.,seeFigure1inKimet al.20). Total XRD is well suited genic manganese oxides too show several well-defined to study materials structured at the nanoscale, as dem- peaks but they decay to zero faster (i.e., already at 2Ϫ3 onstrated recently.9Ϫ11,21 nm) than those in the PDF for synthetic birnessite, re- flecting the limited length of structural coherence in the RESULTS AND DISCUSSION former materials. The first peak in the PDFs for bio- Biogenic MnOx studied here were produced by L. dis- genic MnOx is positioned at approximately 1.9 Å and cophora SP-6 bacteria15 and fungi from the Acremonium the second at approximately 2.85 Å. The first two peaks strictum family.22 High-energy XRD patterns for bacterial, in the PDF for polycrystalline birnessite are positioned fungal, and crystalline MnO2 (birnessite) standard are at the same distances. Here they reflect the first neigh- shown in Figure 1 (the upper part). Sharp Bragg peaks bor MnϪO and MnϪMn atomic pairs from edge shar- are present in the XRD pattern for synthetic birnessite, as ing MnϪO6 octahedra, respectively. The similarity be- can be expected for a material of good crystallinity. The tween the low-r parts of the experimental PDFs in XRD patterns for both bacterial and fungal MnOx, how- Figure 1 indicates that biogenic MnOx studied here, ever, show only a few broad Bragg-like peaks. Such dif- like synthetic birnessite, are built up from intercon- 442 VOL. 3 ▪ NO. 2 ▪ PETKOV ET AL. www.acsnano.org ARTICLE nected MnϪO6 octahedra. This conclusion would have been difficult to arrive at if the XRD patterns and not their Fourier transforms, the atomic PDFs, had been considered alone. The higher-r parts (i.e., above 5Ϫ6 Å) of the experimental PDFs in Figure 1, however, are dissimilar and demonstrate that the longer-range atomic ordering, that is, the way the MnϪO6 octahe- dral units connect together and fill up the space, is dis- tinctly different in the three different manganese oxides studied. Such a conclusion is difficult to arrive at on the basis of spectroscopy (e.g., EXAFS) data alone. To reveal the 3D structure of biogenic MnOx we tested several structural models as follows: In line with the suggestions of previous studies14,15 the PDF for bac- terial MnOx was approached with models featuring lay- ersofMnϪO6 octahedra. As such we considered the structures of lithiophorite, chalcophanite, and hexago- nal and triclinic birnessite (see Figure 2) that occur in MnOx minerals. As shown in Figure 2 lithiophorite may be viewed as a stack of alternating layers of octahedra, perfect and defect (dark shaded in Figure 2), with the latter layers having 33% of their octahedral sites vacant.

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