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Unraveling the internal microstructure of biogenic and bioinspired calcite single crystals

Published online by Cambridge University Press:  03 June 2015

Anna S. Schenk
Affiliation:
Institute of Polymer Chemistry, University of Stuttgart, Germany; anna.schenk@ipoc.uni-stuttgart.de
Yi-Yeoun Kim
Affiliation:
School of Chemistry, University of Leeds, UK; y.y.kim@leeds.ac.uk

Abstract

Modern materials design is largely based on composite structures aimed at a synergistic integration of multiple components with a diverse range of properties. Biologically grown minerals provide an intriguing example of sophisticated organic–inorganic nanocomposite structures resulting in excellent mechanical characteristics. Among the mineral phases utilized by living organisms to generate hard tissues, calcium carbonate—especially the calcite polymorph—is ubiquitous and has been studied intensively. Biogenic calcite crystals often show hierarchical organization spanning multiple length scales, and the occluded organic phases are now known to be intimately associated with the mineral host. Here, we discuss the internal micro- and nanostructure of two selected types of calcite biominerals—the sea urchin spine and prismatic single crystals extracted from mollusk shells. This article highlights recent advances in translating the key principles of biological mineralization into design strategies for synthetic materials and presents analogies between biogenic and synthetic calcite single crystals.

Information

Type
Research Article
Copyright
Copyright © Materials Research Society 2015 
Figure 0

Figure 1. Examples of calcitic biominerals acting as skeletal elements in marine organisms. (a) Red coral skeleton, (b) sea urchin spine (left) and test (right), (c) mollusk shell (Atrina rigida), and (d) coccosphere. (c) Reproduced with permission from Reference 8. © 2006 Wiley.

Figure 1

Figure 2. The hierarchical structure of prismatic crystals extracted from the shell of a mollusk. (a) A cross section of an Atrina rigida shell imaged by scanning electron microscopy. Prismatic calcite crystals (lower part) and nacre tablets (upper part) are seen. (b) Three-dimensional reconstruction of x-ray microtomography data obtained from the prismatic layer of Pinna nobilis. The elongated prismatic shape of the grains is discernible. (c–d) Electron micrographs of individual prisms extracted from Atrina rigida presenting views of the side facets (c) and the basal plane (d). (e) Selective removal of the mineral phase uncovers a network of organic fibers penetrating the prism. The periodicity indicates a cyclic growth pattern. (f) Mineral grains in the size range of approximately 50 nm are tightly associated with the organic network. (g) Electron tomographic reconstruction of a thin section of an Atrina rigida prism. Isolated disc-like patches of lower density (organic material) are shown in blue. The yellow arrow indicates the direction of the crystallographic c-axis. (h–i) Annular dark-field scanning transmission electron microscope images of thin slices of a prismatic crystal cut parallel (h) or perpendicular (i) to the c-axis. Dark areas correspond to low-density organic occlusions. (a, e, f) Reproduced with permission from Reference 7. © 2007 Royal Society of Chemistry. (b) Reproduced with permission from Reference 21. © 2014 Nature Materials. (g–i) Reproduced with permission from Reference 27. © 2011 Wiley.

Figure 2

Figure 3. Nanostructure and lattice distortions in prismatic calcite from Pinna nobilis studied by x-ray scattering techniques. (a–d) Small- and wide-angle x-ray scattering (SAXS and WAXS) plots of individual calcite prisms. (a–b) Two-dimensional (2D)-detector images of simultaneously recorded SAXS and WAXS before (a) and after (b) annealing at 300°C. The SAXS signal (center of the 2D detector) is clearly anisotropic, and intensity streaks point toward the azimuthal position of specific Bragg spots (arrows), indicating non-homogenous incorporation of organic material aligned with the corresponding families of lattice planes. After annealing (decomposition of intracrystalline organics), the orientation of nanostructural features toward the [001]-direction of the mineral lattice becomes more pronounced. (c–d) Integral SAXS intensity plotted over the azimuthal angle χ before (c) and after (d) annealing. Drop lines indicate the angular position of (006) and (104) Bragg peaks. The yellow bar marks the region affected by the beamstop (BS). (e–f) Lattice parameters (a- and c-axes) calculated from high-resolution powder diffraction extracted from high-resolution powder diffraction data as a function of the annealing temperature. Significant anisotropic lattice distortions are seen with respect to a control sample. Mild annealing at temperatures above 200°C induces relaxation of the crystal lattice. (a–d) Reproduced with permission from Reference 22. © 2011 Wiley. (e–f) Reproduced with permission from Reference 14. © 2006 Elsevier.

Figure 3

Figure 4. Micrometer and submicrometer-scale structure of the sea urchin spine. (a) Scanning electron micrograph showing the spongy microstructure of a spine fractured perpendicular to the long axis. (b) Fracture surface imaged in higher detail revealing conchoidal fracture. (c) A substructure composed of elongated grains is seen in the transmission electron microscopy image obtained from a small section of the spine. Inset: selected area electron diffraction pattern comprising distinct diffraction spots. (d) High-resolution transmission electron microscopy shows defect structures (white arrows) around lattice fringes. (e) Small-angle x-ray scattering indicates a bimodal size distribution of the scattering objects, where larger objects (exceeding a size of 100 nm), which might represent the mineral grains observed in electron microscopy, dominate the scattering profile (Intensity (q) versus q, where q represents the modulus of the scattering vector) at low q (region 1). The intensity at higher q (region 2) indicates the presence of occluded organic material, with an estimated correlation length of 1.4 nm. (c–e) Reproduced with permission from Reference 6. © 2012 National Academy of Sciences.

Figure 4

Figure 5. Scanning electron microscope images showing internal surfaces of synthetic calcite single crystals grown in the presence of polymer-based particles and gels. (a) Polystyrene latex particles (focused ion beam cross-sectioned), (b) block copolymer micelles (fractured), (c) in xyloglucan gel matrix functionalized with Fe3O4 nanoparticles (fractured). (a) Reproduced with permission from Reference 51. © 2010 Wiley. (b) Reproduced with permission from Reference 46. © 2011 Nature Materials. (c) Reproduced with permission from Reference 68. © 2014 Royal Society of Chemistry.

Figure 5

Figure 6. Powder x-ray diffraction profile of synthetic calcite crystals with organic occlusions. (a) Profiles of the (104) reflection obtained from calcite crystals precipitated with aspartic acid. The effects of different amounts of aspartic acid on the peak positions are demonstrated. In red, blue, and violet—calcite powders grown from solutions with the addition of 0.5, 2, and 3 mg/ml aspartic acid, respectively, compared to the (104) reflection of pure calcite (black). (b) Profiles of the (104) reflection obtained from composite crystals precipitated with poly(4-styrenesulfonic acid-co-maleic acid) sodium salt)(red) showing broadening in the peak compared to that of pure calcite (black). (c) Profile of the (006) reflection obtained from calcite grown with block copolymer micelles. The peak is anisotropically distorted (described by two different HWHMs). (d) Schematic representation of the model used to evaluate the effect of particle incorporation on the crystal lattice, where a particle of radius a causes a strain gradient in the lattice to a distance b from its center (strain-affected zone). The green curve depicted below the particle and its strain-affected zone describes the distribution of compressive strain (in green). (a) Reproduced with permission from Reference 43. © 2012 Wiley. (b) Reproduced with permission from Reference 45. © 2014 Nature Publishing Company. (c–d) Reproduced with permission from Reference 46. © 2011 Nature Materials.

Figure 6

Figure 7. Microbeam small- (SAXS) and wide-angle x-ray scattering (WAXS) of single calcite-PSS crystals. (a, left) Two-dimensional SAXS/WAXS scattering pattern recorded during a 180° rotation of an individual calcite-PSS crystal. The anisotropic SAXS signal in the center of the image (white frame) indicates the presence of a pronounced nanostructure in the hybrid crystal. Diffraction spots are observed in the wide-angle region (white arrows: (104) plane, yellow arrows: (006) reflections). (a, right) The SAXS pattern was recorded at a fixed rotation angle (ω). The intensity streak points to (006) lattice planes of calcite (scale bar = 1 nm−1). The azimuthal angle χ is illustrated by the white arrow. (b) Profiles of the intensity of the scattering signal versus the azimuthal angle χ are plotted for two distinct sample rotation angles ω, where maxima appear in the anisotropy of the SAXS signal (blue bar = angular range affected by the beam stop). Reproduced with permission from Reference 61. © 2012 Wiley.