nanoscale infrared spectroscopy Nanoscale infrared spectroscopy of light harvesting proteins, amyloid structures and collagen fibres Andrzej J. Kulik,1 Francesco Simone Ruggeri,1 Wieslaw I. Gruszecki 2 and Giovanni Dietler1 1. Laboratory of Physics of Living Matter, Ecole Polytechnique Fédérale de Lausanne, Lausanne, Switzerland 2. Department of Biophysics, Maria-Curie Sklodowska University, Lublin, Poland Introduction Several analytical methods have been developed that apply scanning probe microscopy to extract information about local physical or chemical properties of biological macromolecules. Most of these are very application specific, tedious or difficult to use, which limits their popularity. Kelvin probe microscopy and Piezoelectric probe microscopy are among the most commonly used now. The mapping of local mechanical properties is quite popular in biology, although there are reproducibility problems related to methodology and the non-reproducibility of commercially available cantilevers. Chemical force microscopy [1-3] measures tip-sample friction, or pull-off force, and is influenced heavily by the chemical properties of the sample. This method is very specific but does not fully deliver quantitative analytical information. nano Infrared analysis A recently developed infrared spectroscopy technique by Dazzi [4] and its subsequently commercialized version, the nanoIR system from Anasys Instruments, appears to offer an easy-touse solution for local chemical analysis with the spatial resolution of an atomic force microscope (AFM). The nanoIR technique uses thermomechanical detection. A pulsed, tunable laser beam is passed through a ZnSe prism and undergoes total internal reflection from the upper face of the crystal (Figure 1). An evanescent wave interacts with the sample, mounted as a thin layer on the ZnSe prism. If a given wavelength is absorbed by the sample, its temperature rises and its height subsequently changes through thermal expansion. This ‘kicks’ the AFM cantilever in contact with the sample surface. The cantilever resonates at several Eigen frequencies. One mode is chosen and its amplitude is proportional to IR absorption within the specimen. The user may change the wavelength (or wavenumber) by tuning the laser. It is possible to record IR spectra at one location of the sample, or alternatively map IR absorption at a single wavenumber. Additionally, wide band excitation with a short pulse excites simultaneously many Eigen frequencies of the cantilever. This ability gives the technique a strong advantage over other analytical methods in that it measures several cantilever resonant frequencies which can be related to the local stiffness of the specimen [5]. In this article we review the application of the nanoIR technique to the study of several biologically important macromolecules. materials and methods LHCII was isolated from spinach chloroplasts as described in [6] Samples were deposited at the surface of the attenuated total internal reflection element prism made of ZnSe monocrystals and dried overnight. Then, they were scanned in contact mode by a nano-IR system from Anasys Instruments with a rate line within 0.02-0.1 Hz. We used a silicon (AppNano) cantilever with a nominal radius of 10 nm and a nominal spring elastic constant of 0.5 N/m. All images MicroscopyandAnalysis | May 2014 Compositional Analysis have a resolution within 256x256 and 1024x1024 pixels for line. Spectra were collected with a sampling of 1-2 cm-1, within the range 1200-1800 cm-1. Measurements were done within 5-100% of the instrument maximum laser power. All measurements were performed at room temperature. FIGURE 1 Schematic of the nanoIR system. See text for explanation. (Courtesy of Anasys Instruments.) results photosynthetic pigmentprotein complex As a first application of the system, we performed a study on the molecular organization of the major plant photosynthetic pigment-protein, the light-harvesting complex of photosystem II (LHCII), in the environment of chloroplast lipid membranes [6]. This complex is the most abundant membrane protein in the biosphere and is estimated to comprise half of the chlorophyll pool on Earth. Its main physiological function is to collect light quanta and to transfer excitation energy towards the reaction centres where electric charge separation 11 nanoscale infrared spectroscopy takes place. The lipid membranes of the photosynthetic apparatus of plants are exceptionally enriched with proteins which occupy more than 70% of the membrane surface. Owing to this fact the structural aspects of the LHCII presence in the lipid phase are expected to be important determinants of the molecular architecture of the chloroplasts membranes. With the application of the nanoIR technique, we studied lipid multibilayers containing incorporated LHCII. We found that LHCII proteins self-organized into oligomeric structures in the plane of the membrane. Moreover the protein formed pillar-like transmembrane structures stabilized by hydrogen bonds between the peripheral (polar) protein fragments of the complexes anchored in the adjacent lipid bilayers. Formation of these type of complexes was found to be strongly dependent on the protein phosphorylation state (which is light intensity-controlled in vivo). Such a finding led to several specific conclusions on the role of molecular organization of LHCII in response of the photosynthetic apparatus of plants to stress conditions associated with strong light. Figure 2 Light-harvesting complex II. Model of the lipoprotein multibilayer composed of lipids and integrated LHCII. The model is based on the crystallographic structure of LHCII (coordinates downloaded from the PDB-database, PDB ID:2bhw. The horizontal dimension of the LHCII trimer is close to 10 nm [8]. For more details of the model, see [6]. a Figure 3 Light-harvesting complex II. (a) Surface topography, (b) mechanical stiffness map and (c) IR absorption pattern of the lipoprotein multibilayer, recorded simultaneously on a 1x1 µm area of the sample, the thickness of which was approximately 1.2 µm. Data contributing to the IR-absorption map were acquired at a wavenumber of 1650 cm-1. Scan resolution: X = 512 points, Y = 256 points; scan rate: 0.4 Hz, 8 co-averages. amyloid structures One of greatest benefits of nanoIR is that the nanoscale chemical analysis can be performed with very small quantities of biological samples. Purification and high throughput production of proteins is extremely expensive and time consuming; for this reason, the reduction of sample quantity required to perform routine FTIR measurements and secondary structure analysis are problems of primary importance which nanoIR can solve. This is the case of proteins aggregating into amyloid structures, which are involved in neurodegenerative disorders. Amyloids are insoluble proteins that form fibrillar aggregates. During aggregation, initially monomeric proteins undergo internal structural rearrangement forming amyloid fibrils with a universal cross b-sheet quaternary structure. This structure is independent on the monomeric initial one and it is the fingerprint of amyloid fibrils. FTIR is a key method for studying their structural conversion during amyloid formation. Nevertheless, during fibrillation, several coexisting amyloidogenic species are formed. So, conventional FTIR is only able to give average spectra of the heterogeneous solution. Sub-micrometer chemical characterization of amyloidogenic structures as oligomers and fibrils is central to understanding how proteins misfold and aggregate. In this work, the nanoIR system was initially used to analyze proteins deposited as patterned microdroplets 12 b c Compositional Analysis May 2014 | MicroscopyandAnalysis nanoscale infrared spectroscopy d a b c Figure 4 NanoIR imaging and spectra acquisition of lysozyme microdroplets containing amyloid structures. (a) AFM height channel of a monomeric droplet. (b) IR absorption of monomers at 1620 cm-1. (c) IR absorption of monomers at 1530 cm-1. (d) Spectra of monomers and fibrils. by means of a microfluidic system [7] (Figure 4). The instrument allowed us to distinguish spectra of lysozyme droplets (Figures 4 a,b,c) containing amyloids from ones containing native globular proteins. In particular, the shift in the amide I band allowed us to identify an a-to-b secondary structure transition which is associated with amyloid formation (Figure 4d). No other technique had been available to give chemical analysis at this sub-micrometer scale. The same approach was used to study a-synuclein macromolecular aggregates. The protein was deposited as droplets on the ZnSe substrate in two forms: monomeric and fibrillar (Figure 5). A first macro-observation showed that monomers formed a uniform layer on the surface, while fibrils were strongly organized (Figure 5 a-d). The monomeric layer is chemically and mechanically homogeneous, in contrast to the tubular fibrillar macro-aggregate (Figure 5 b,c,e,f). This difference was confirmed by the spectra acquisition of the two samples which are quite different and show a random-coil to b-sheet transition, typical of the formation of amyloids from unordered proteins. Spectra modification during amyloid formation is in very good agreement with the previous ones for lysozyme. g collagen fibres Finally, as last example of the versatility of the nanoIR technique, other measurements were realized on collagen MicroscopyandAnalysis | May 2014 Compositional Analysis FIGURE 5 NanoIR imaging and spectra acquisition of a-synuclein film of monomers and of a supramolecular aggregate. (a) AFM height channel. (b) IR absorption at 1620 cm-1. (c) Mechanical response of the cantilever at 1620 cm-1 for a film of monomers. (d) AFM height channel. (e) IR absorption at 1620 cm-1. (f) Mechanical response of the cantilever at 1620 cm-1 for a supramolecular aggregate. (g) Spectra of the monomeric film and the supramolecular rod. 13 nanoscale infrared spectroscopy biography a Andrzej J. Kulik has worked as scientist at EPFL in Switzerland since 1981. He has developed several new methods for non-destructive material testing, quantitative acoustic microscopy, nanoscale measurements applied to nanoscale objects, AFM-based nanomanipulation and optical tweezers-based 3D nanomanipulation. Recently, he has been using a nanoIR system to study biomolecules. He is the co-author of over 110 papers, seven book chapters, and has two patents with more than 4000 citations. b c abstract d fibres. The system allowed us to acquire the spectral chemical composition of a single collagen fibril with a diameter of about 100 nm (Figure 6). conclusions In conclusion, we have demonstrated that the nanoIR technique is stable and easy-to-use, giving novel and meaningful results from studies of biologically important macromolecules that were previously not available. References: 1. Frisbie, C. D., Rozsnyai, L. F., Noy, A., Wrighton, M. S., Lieber, C. M. Functional group imaging by chemical force microscopy.Science 265:2071-2074, 1994. 2. Noy, A. C., Frisbie, C. D., Rozsnyai, L. F., Wrighton, M. S., Lieber, C. M. Chemical force microscopy: Exploiting chemically modified tips to quantify adhesion, friction, and functional group distributions in molecular assemblies. Journal of the American Chemical Society 117:7943-7951, 1995. 3. Beaussart, A., Ngo, T. C., Derclaye, S., Kalinova, R., Mincheva, R., Dubois, 14 FIGURE 6 NanoIR imaging and spectra acquisition of a bundle of collagen fibrils. (a) AFM height channel. (b) IR absorption at 1655 cm-1. (c) Mechanical response of the cantilever as a function of sample stiffness at 1655 cm-1. (d) Spectrum of typical collagen fibril with a diameter of about 100 nm. (Sample courtesy of L. Kreplak, Dalhousie University, Canada.) P., Leclère, P., Dufrêne, Y. F. Chemical force microscopy of stimuli-responsive adhesive copolymers. Nanoscale 6(1):565571, 2013. 4. Dazzi, A., Prazeres, R., Glotin, E., Ortega, J. M. Local infrared microspectroscopy with subwavelength spatial resolution with an atomic force microscope tip used as a photothermal sensor. Optics Letters 30(18):2388-2390, 2005. 5. Dupas, E., Gremaud, G., Kulik, A., Loubet, J.-L. High-frequency mechanical spectroscopy with an atomic force microscope. Review of Scientific Instruments 72(10): 3891-3897, 2001. 6. Janik, E., Bednarska, J., Zubik, M., Puzio, M., Luchowski, R., Grudzinski, W., Mazur, R., Garstka, M., Maksymiec, W., Kulik, A., Dietler, G., Gruszecki, W. I. Molecular architecture of plant thylakoids under physiological and light stress conditions: A study of lipid–light-harvesting complex II model membranes. Plant Cell 25(6):2155-2170, 2013. 7. Müller, T., Ruggeri, F. S., Kulik, A. J., Shimanovich, U., Mason, T. O., Knowles, By combining atomic force microscopy with photo-thermal induced resonance detection of infrared spectra (nanoIR), extraordinary high nanoscale spatial resolution can be obtained. This method is very useful to study inhomogeneous samples by functional imaging at a single wavenumber. This allows the detection of the distribution of chemical properties of the constituents of the sample. As well, the method provides meaningful infrared spectra of very small quantities of sample (e.g. proteins). Studies of light harvesting complex II, amyloid and collagen samples are presented. acknowledgements We would like to thank the Swiss National Foundation for Science for funding, Tuomas Knowles’ lab in Cambridge, who worked with us on lysozyme, and Lashuel Hilal’s lab for alpha-synuclein. Corresponding author details Dr Andrzej J. Kulik, Laboratory of Physics of Living Matter, Ecole Polytechnique Fédérale de Lausanne, BSP/Cubotron, CH-1015 Lausanne, Switzerland Tel: +41 21 693 3359 Email: [email protected] Microscopy and Analysis 28(4):11-15 (EU), May 2014 ©2014 John Wiley & Sons, Ltd T. P. J., Dietler, G. Nanoscale spatially resolved infrared spectra from single microdroplets. Lab on a Chip 14(7), 13151319, 2014. 8. Barros, T., Royant, A., Standfuss, J., Dreuw, A., Kühlbrandt, W. Crystal structure of plant light-harvesting complex shows the active, energytransmitting state. The EMBO Journal 28(3):298-306, 2009. Compositional Analysis May 2014 | MicroscopyandAnalysis
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