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Multiscale imaging of plants: current approaches and challenges

Plant Methods volume 11, Article number: 6 (2015) Cite this article

Abstract

We review a set of recent multiscale imaging techniques, producing high-resolution images of interest for plant sciences. These techniques are promising because they match the multiscale structure of plants. However, the use of such high-resolution images is challenging in the perspective of their application to high-throughput phenotyping on large populations of plants, because of the memory cost for their data storage and the computational cost for their processing to extract information. We discuss how this renews the interest for multiscale image processing tools such as wavelets, fractals and recent variants to analyse such high-resolution images.

Introduction

Finding the good practices to perform high-throughput phenotyping of large populations of plants is a current challenge to meet the high-throughput capacity of genotyping and push forward the knowledge on the development of plants in different environments. Because they allow contactless and noninvasive measurements, imaging techniques are regarded as tools of highest interest in this context, to provide anatomical or physiological objective traits and outperform the limit of human vision either in terms of sensitivity, accuracy or throughput. Conversely, plant sciences constitute a new field of application for computer vision which traditionally, when applied in life sciences, used to focus more on biomedical imaging. Among the specificities of computer vision for plant sciences that are not found in biomedical imaging, is the possibility to monitor, continuously over the whole life cycle, the process of growth on structures possessing complex 3D multiscale organisation with a part visible in the air (shoot) and a part hidden in the soil (root).

There has been a significant increase in interest in plant imaging and image analysis methods in recent years, but most of the techniques proposed focus on measurements at a single scale - cell, organ, whole plant, etc. This is in contrast to modelling efforts which have stressed multiscale approaches. Such numerical models have been proposed at the scale of the entire structure of plants from iterated replication processes using L-systems (see [1,2] for reviews). Such replication processes have been shown able to reproduce the fractal organization of plant structures as measured on entire real plants. These can also serve to model the root systems [3] and have recently been used to validate image processing algorithms for root segmentation [4]. Multiple plant modeling coupled to agronomical models have also been developed [5] and allow the numerical validation of image processing algorithms at the scale of canopy. Replication processes have also been modeled at the cellular scale with possibilities of explanatory physical mechanisms for the shape of the plant at higher scales [6]. As another instance, the so-called dead leaves model takes inspiration from the foliage of plants, with leaves of different sizes and illumination which are reproduced at various scales with occlusions [7-9]. Such models have been shown to produce fractal patterns with controllable properties, and in return they offer models for the multiscale constitution of plants.

Due to the increase in size and resolution of the imaging sensors and to the development of efficient registration methods, the number of scales accessible in imaging is now ready to meet the multiscale structure of plants. In this review article, we present a set of recent high-resolution imaging techniques which cover the plant scales from molecules in the cell up to the field, and we detail how this renews the interest of scale-analysis tools for image processing.

Multiscale high-resolution imaging in plant sciences

We give in Table 1 a list of imaging techniques which have been shown in the recent literature to cover multiple scales of interest for plant sciences. At the smallest scales, single molecules up to the the entire cell are now also accessible for plants [10] with super-resolution imaging techniques [11] outperforming the classical diffraction limits such as photoactivated localization microscopy (PALM), stochastic optical resolution microscopy (STORM) [12], stimulated-emission depletion microscopy (STED) [13], three-dimensional structured illumation microscopy (3D-SIM) [14] and total internal reflection fluorescence microscopy (TIRF) [15]. At a higher range of scales, some recent microscopic imaging techniques now allow to discriminate cells of an entire organ. This is illustrated in Figure 1 with an example of optical coherence tomography (OCT) of a seedling of Arabidopsis thaliana during elongation with a resolution enabling to discriminate the cells of the seedling and the entire seedling. Other microscopic imaging techniques also have this capability and have been applied to plants like X-ray phase contrast imaging (X-ray PCT) [16] for microstructure analysis of the voids in an entire seed, light sheet fluorescence microscopy (LSFM) [17], multiangles confocal microscopy [18] to observe the entire seedling growth cell by cell, or optical projection tomography (OPT) [19] to image an entire leaf with possibility of cell resolution. At larger scales, inside the soil, imaging techniques give access to nodules on the root system up to the entire root system. This has been recently demonstrated in 3D in soil with absorption-based micro X-ray computed tomography [20-22], and with high-resolution imaging in 2D with rhizotron using reflectance imaging [23], or with bioluminescence imaging [24,25]. At the same metric scales but in the air, imaging techniques give access to a leaf in the shoot up to the entire shoot. This has been recently demonstrated with a variety of 3D imaging systems (see [26,27] for a recent reviews). At still larger metric scales, in field conditions, one can capture with high-resolution imaging setups embedded on an airplane or unmanned aerial vehicle (UAV) [28,29] the entire shoot from top view up to the canopy constituted by assemblies of shoots.

Figure 1
figure1

Images of a seedling of Arabidopsis thaliana acquired with optical coherence tomography (see [ 31 ] for another illustration of OCT with plants). Panel A: 3D view of an entire seedling. Panel B: 2D view in XY. Panel C: zoom in the solid rectangle of the 2D view of panel B.

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Table 1 Multiple scale high-resolution imaging in plant sciences
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The list of imaging techniques given in Table 1 is not exhaustive (see [32-34] for recent reviews). This familly of new imaging systems bring some challenges that would be interesting to be discussed in the field of instrumentation when applied to plants. To point only one, the new microscopies of Table 1 have been introduced for applications of broad interest in life sciences and often demonstrated on organisms which serve as models for biology, such as C-elegans, zebra fish, mice, Drosophilae fly or Arabidopsis thaliana... Consequently, the non-invasiveness property of the light used to acquire images of such a variety of organisms is mainly expressed as nonphototoxic if it does not kill the organism on a time scale linked with the time required by instrumentation for image acquisition. For specific applications on plants however, imaging the development can necessitate long time-lapsed acquisitions. For instance, imbibition and germination of a seed take hours while elongation of a seedling several days. At these stages of development illustrated in Figure 1, plants are supposed to grow in dark conditions in the soil with no light exposure, as light strongly modifies the physiology of seedlings since it activates the process of photosynthesis. It would therefore be important to revisit, as recently done for seedling in [35], the concept of phototoxicity, by adapting wavelength, energy and duration of the light used by the family of mutiscale microscopies when applied to plants.

In this review, we rather put the stress on current approaches and challenges brought by new imaging systems at the level of image processing. The point here is that techniques of Table 1 have in common, although working at very different metric and biological scales, to produce images requiring a huge capacity of data storage. This is due to the increasing size, resolution and dynamic of imaging sensors, but also to the coupling of imaging systems with motorized scanning systems. By this coupling, multiple views can be acquired and registered to produce high-resolution imaging. Multiview imaging is common practice in remote sensing. This is now extending to the scale of a single plant with rotating plates, or at the scale of the cells with microscope scanners. For instance, the OCT system used to produce Figure 1 is associated to microstage translation systems, in such a way that the imaging technique can, after registration, capture in 3D and at the cell resolution, hundreds of such entire seedlings in a single run, resulting in some Giga bytes of data. This is 106 more than what has to be stored for one single plant imaged with a standard imaging resolution. Such large images can still be opened by a software like ImageJ but image processing, even some basic ones, can become very slow. This high memory cost, specially in the perspective of high-througput phenotyping for large population of plants, calls for adapted approaches. We propose a review of the most prominent of them in the following.

Image processing tools for multiscale imaging

Combining modalities with different scales

A problematic of current interest in multiscale imaging is to combine imaging modalities providing different scales and contrasts. This association has for instance been illustrated in plant sciences with electron microscopy combined with confocal microscopy [36], or magnetic resonance imaging (MRI) combined with positon emission tomography (PET) [37] or again depth imaging combined with thermal imaging [26]. In these examples one of the modality has a relative high spatial resolution (electron microscopy, MRI, depth imaging) which provides an anatomical information while the other modality (respectively confocal, PET, thermal imaging) gives a more functional information. The functional modality can be used to locate a region a interest to be further analysed from an anatomical point of view or the other way round. This is a useful way to reduce the amount of data to be explored at high resolution. Also, the high-resolution modality can be used to analyze separately different anatomical compartments, not clearly contrasted in the functional modality. This is illustrated in Figure 2 where a 3D image of sugar beet dry seed has been acquired with a high-resolution X-ray tomograph and a MRI sequence providing gray levels proportional to the content of lipid in the seed. This gives an image of the embryo of the dry seed. As shown in Figure 2, the high-resolution modality can be used to identify the position of the cotyledon and the radicle in the embryo. If the two modalities are registered, the landmark corresponding to the beginning of the separation between cotyledon and radicle can be applied onto the MRI images and then allowing a comparison of the lipid content of these two sub-organs of the seed. Specifically here, this shows the expected higher content of lipid in the cotyledon than in the radicle. The registration step is a key image processing step in this combination of modalities. Image registration is a problematic of image processing by itself [38] with various approaches (conventionnally classified as rigid versus non rigid, automatic versus manual,...) which have in common the calculation of a transformation matrix to be applied on one of the modality so as to be able to surperimpose both modalities with a locally accurate match all over the images. The development of high-resolution multiscale images has called for the design of approaches adapted to the computational cost due to the large size of the images to be registered. Instead of performing the computation of the registration on the whole image, the transformation matrix is computed on a region of interest containing landmarks and then applied on the entire image (this is available in the ImageJ Plugin TurboReg pointed in Table 2). These landmarks can be selected manually or detected automatically with scale invariant feature transforms (SIFT) [39] or variants implemented in the ImageJ Plugin TrakEM2 pointed in Table 2. Random local deformation can occur with electron microscopy due to slicing or with MRI due to the so-called blooming effect or also with thermal imaging due to the presence of mixed pixels on edges of structures. The compensation of these local deformations randomly occuring in one of the imaging modalities remains an open challenge for image registration.

Figure 2
figure2

Bimodal imaging of the embryo of a dry seed of sugar beet with a low spatial resolution of 0,187 mm per isotropic voxel in MRI (A external 3D view and C medial 2D slice) and high spatial resolution of 7,84 μ m per isotropic voxel in X-ray tomography (B external 3D view and D medial 2D slice). The MRI is a spin-echo sequence giving gray-level propotional to the lipid content of the embryo. The red line in panel D is positionned manually on the X-ray at the separation between cotyledon and radicle. Red line in panel C is automatically positioned after registration of both imaging modalities with the ImageJ plugin TrakEM2 of Table 2.

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Table 2 Multiple scale image processing tools available under the free and open software ImageJ
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Selecting scales

The selection of structures appearing in the images at given scales can be realized with filters. The design of these filters has to incorporate some prior knowledge on the shape of the objects to be found at each scale. Among the strategies for the design of bank of filters, wavelets have shown to be a very powerful approach for application in plant sciences, see [40] for a review of the late 90’s, which continue to be investigated to select patterns on leaves [41-44] or on canopies [45,46]. The wavelet approach is versatile since a large panel of wavelet functions have been designed. A wavelet is a wave-like oscillation with an amplitude that begins at zero, increases, and then decreases back to zero on a scale which can be defined by the user. Such functions are expected to constitute good filters when they share common features with the shape of the objects to be extracted. Some familly of filters have specifically been developed to extract given shapes. Let us shortly underline the vesselness filter [47] which enhances area in images where the gradient in the image is almost null in one direction and much higher in the other perpendicular directions. This situation is found with any tubular structures. Therefore, although initially developed to enhance biomedical images with vascular vessels the vesslness filter is also very much suited to enhance tubular structures met in plant sciences such as cell walls, leaf veins or branches in trees. Based on the same philosophy, enhancing areas with high gradient in all directions extract the blob-like structures [48] (cells, nodules, spherical fruits, …), or also enhancing areas with high gradient in only one direction in space extracts surface-like structures (cellular layers, plant leaves,…). These familly of filters are available under ImageJ as mentioned in Table 2.

When no prior knowledge on the shapes or scales of the objects of interest in the image is available, it is necessary to use self-adaptive methods to automatically select the appropriate scales of interest. Such methods are known as wavelet packets decomposition. However, in this case, the choice of the wavelet and of the range of scales to be analysed still have to be performed by the user. Another self-adaptive method, of more recent introduction, is the empirical mode decomposition also called Hilbert-Huang transform, where the scale analysis is purely based on the data itself. Data-dependent modes, corresponding to the local frequency data, are extracted by the analysis to decompose the signal, instead of a decomposition on preexisting elemental functions such as wavelets. Introduced for monodimensional signals [49], empirical mode decomposition has then been extended to images [50] and successfully applied to texture characterization [51]. The dominant modes of the decomposition single out the main scales in the signals or images under analysis, and keeping only the dominant modes offers natural methods for parsimonious representation and for data compression. Efficient compression schemes have been developed for landscapes captured in remote sensing for scales from canopy to field [52]. Such compression approaches by scale selection remain open for investigation for the other scales of Table 1.

Another active field of image processing associated to the selection of scales is image denoising. Benchmark are found in the litterature [53] so as to identify the best techniques. However, such benchmarks are mostly organized on natural images not specifically suited for a given scientific field. It is very likely that the ranking of best practices may vary depending on the specific type of images. A specificity of multiscale images in plant sciences is the presence of replicated structures. This is visible in Figure 1 with cells or in Figure 3 with leaves. This replication process found in plant architecture constitutes a prior which is not found in all natural images. This observation motivates the choice of the so-called nonlocal mean [54] as interesting denoising methods. Nonlocal mean denoising is realized by averaging pixel content weighted by how similar these pixels are to the target pixel. In its principle, this non local averaging process, available under ImageJ plugin given in Table 2, will be very efficient if a lot of pixels are similar to the target pixel like in the self-similar structures found in plant sciences.

Figure 3
figure3

Bimodal RGB-depth representation of a forestery scene (first row) and a single plant (second row). Panels A and E: RGB luminance. Panels B and F: corresponding RGB histogram. Panels C and G: depth map expressed in meter. Panels D and H: corresponding point cloud of the depth map.

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Characterizing multiscale signatures

Instead of selecting specific scales of interest, another approach is to characterize the global organization over multiple scales in the images. Nontrivial regularities developing in a self-similar way across a significant range of scales usually identify the existence of a fractal organization. Fractal concepts have been shown relevant to the description of plants, of their roots and shoots, which often show self-similar organizations across scales [55-59]. Especially, such organizations lead to high surface areas at the interfaces with the environment, ensuring for the plant efficient capture of nutrients and energy.

Self-similarity accross scales, i.e. fractal features, can thus be found in various properties of images from plants. For instance, they have been reported in the spatial organization of gray-level luminance images from outdoor scenes of woods and plants [60,61]. This is manifested by scale-free power-law evolutions present in the frequency spectrum of luminance images or also in their spatial correlation functions. Also, the colorimetric organization of natural images including landscapes with plants has been reported to carry self-similarity and fractal properties [62-64]. More recently, multiscale analysis has been undertaken for plant images obtained from another imaging technique delivering depth images of a physical scene [65]. The depth map images from outdoor scenes of woods and plants as in [60,61] were shown in [65] to also reveal self-similarity and fractal properties. Such multiscale image analyses revealing and characterizing fractal properties in plants are important to contribute to their understanding, since the fractal and multiscale organization of plants has a direct impact on their functioning, for instance for efficient interactions with their environment as evoked above [58,66-68]. Also, fractal characterization of plants is useful to devise synthetic models of plants with sufficient realism [1].

For illustration, we proceed to the scale analysis of several images from a forestry scene and from a single plant, as shown in Figure 3, acquired with a bimodal RGB-depth camera [69]. Figure 3 shows four possible ways of vizualizing such data, with an RGB luminance image, with a 3D RGB histogram, with depth map or with a 3D depth point cloud. We analyze the scale organization in each of these four representations. The spatial frequencies of the RGB luminance images in Figure 3 are analyzed with the power spectrum computed via the periodogram method, through the squared modulus of the two-dimensional Fourier transform, expressed in polar coordinates in the plane of spatial frequencies from a single plant, as shown in Figure 3, acquired with a bimodal RGB-depth camera [65]. An average is then realized over the angular coordinate to yield the orientationally averaged spectrum. This power spectrum is computed on a gray-level version of the RGB image of Figure 3 and on the depth image of Figure 3 as a function of the spatial frequency. The results shown in Figure 4 demonstrate for both the forestry scene and for the single plant, and with both imaging modalities, scale-invariant power-law signatures over a significant range of scales, represented by the spatial frequency. Also, in Figure 4 we implemented the box counting method [65] on the point clouds constituted by the RGB histogram of Figure 3 and by the depth image of Figure 3. The box counting values are obtained in terms of scales represented by the side length of the various boxes. For each side length, we compute the number of boxes with this side length which are needed to cover all the point cloud. Here again the results shown in Figure 4 demonstrate, for both scenes and both modalities, power-law signatures over a significant range of scales, represented by the size of the covering boxes. As shown in Figure 4, the measures computed in luminance space, in RGB space as well as in depth space, all display scale-invariant power-law signatures over significant ranges of scales. Such fractal signatures are interesting in the context of multiscale imaging since they constitute an efficient and concise way to characterize a complex organization. Fractal image processing tools have been widely applied to characterize plants (see [70] for a review) at the scales of leaf [67,71], canopy [72]. So far the fractal characterization of plants at the microscopic scale is open for investigation. Fractal analyses of root systems have been undertaken but mainly from plants taken out of the soil [73-75]. The new high-resolution X-ray CT reported in [20-22] therefore opens new perspectives for the fractal characterization of the root system directly in 3D and in the soil.

Figure 4
figure4

First and second rows: multiscale analysis of RGB-depth images of first and second rows of Figure 3 . First column: average spectrum of RGB luminance image as a function of spatial frequency on a log-log plot. Second column: box counting in the RGB histogram as a function of the box size on a log-log plot. Third column: average spectrum of depth map image as a function of spatial frequency on a log-log plot. Fourth column: box counting in the point cloud of the depth map as a function of the box size on a log-log plot. In each graph, the dotted line with its slope indicated represents a model to appreciate a power-law evolution to match the data. The slopes reveal noninteger exponents for the power-law evolutions matching the data over a significant range of scales. This indicates nontrivial self-invariance of the data across scales, i.e. a fractal organization.

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Conclusion

High-resolution multiscale imaging in plant sciences was until recently limited to the domain of remote sensing. It is now also possible to capture entire roots or shoots of plants, at various stages of development, with cellular or subcellular spatial resolution. These high-resolution imagings are producing huge amounts of data, specially when they are applied to large populations of plants in high-throughput phenotyping. In this framework, we have highlighted here some current approaches connected to the multiscale analysis of plants and pointed toward efficient computational implementation under the free and open software ImageJ in Table 2. Open problems emerge for image compression and image characterization. Multiscale approaches are specifically relevant for the new microscopies such as those presented in Table 1; these are more recent and have received so far, in a multiscale perspective, less attention than remote-sensing imaging or than proximal detection in the field.

References

  1. 1

    Prusinkiewicz P, Lindenmayer A. The Algorithmic Beauty of Plants. Berlin: Springer; 2004.

    Google Scholar 

  2. 2

    Godin C. Representing and encoding plant architecture: a review. Ann Forest Sci. 2000; 57(5):413–38.

    Article  Google Scholar 

  3. 3

    Leitner D, Klepsch S, Bodner G, Schnepf A. A dynamic root system growth model based on L-systems. Plant and Soil. 2010; 332(1-2):177–92.

    Article  CAS  Google Scholar 

  4. 4

    Benoit L, Rousseau D, Belin É, Demilly D, Chapeau-Blondeau F. Simulation of image acquisition in machine vision dedicated to seedling elongation to validate image processing root segmentation algorithms. Comput Electron Agric. 2014; 104:84–92.

    Article  Google Scholar 

  5. 5

    Dufour-Kowalski S, Pradal C, Donès N, Barbier De Reuille P, Boudon F, Chopard J, et al. OpenAlea: An open-software plateform for the integration of heterogenous FSPM components. In: 5th International Workshop on Functional-Structural Plant Models, FSPM07, November, 2007. Napier, New Zealand: The Horticulture and Food Research Institute of New Zealand Ltd.: 2007. p. 1–2.

    Google Scholar 

  6. 6

    Mirabet V, Das P, Boudaoud A, Hamant O. The role of mechanical forces in plant morphogenesis. Annu Rev Plant Biol. 2011; 62:365–85.

    Article  CAS  PubMed  Google Scholar 

  7. 7

    Lee AB, Mumford D, Huang J. Occlusion models for natural images: A statistical study of a scale-invariant dead leaves model. International Journal of Computer Vision. 2001; 41:35–59.

    Article  Google Scholar 

  8. 8

    Bordenave C, Gousseau Y, Roueff F. The dead leaves model: A general tessellation modeling occlusion. Adv Appl Probability. 2006; 38:31–46.

    Article  Google Scholar 

  9. 9

    Gousseau Y, Roueff F. Modeling occlusion and scaling in natural images. SIAM Journal of Multiscale Modeling and Simulation. 2007; 6:105–34.

    Article  Google Scholar 

  10. 10

    Langhans M, Meckel T. Single-molecule detection and tracking in plants. Protoplasma. 2014; 251(2):277–91.

    Article  CAS  PubMed  Google Scholar 

  11. 11

    Elgass K, Caesar K, Schleifenbaum F, Stierhof Y-D, Meixner AJ, Harter K. Novel application of fluorescence lifetime and fluorescence microscopy enables quantitative access to subcellular dynamics in plant cells. PLoS One. 2009; 4(5):5716.

    Article  Google Scholar 

  12. 12

    Gutierrez R, Grossmann G, Frommer WB, Ehrhardt DW. Opportunities to explore plant membrane organization with super-resolution microscopy. Plant Physiol. 2010; 154(2):463–6.

    Article  PubMed Central  CAS  PubMed  Google Scholar 

  13. 13

    Sparkes I, Graumann K, Martinière A, Schoberer J, Wang P, Osterrieder A. Bleach it, switch it, bounce it, pull it: using lasers to reveal plant cell dynamics. J Exp Bot. 2010:351. doi:10.1093/jxb/erq351.

  14. 14

    Fitzgibbon J, Bell K, King E, Oparka K. Super-resolution imaging of plasmodesmata using three-dimensional structured illumination microscopy. Plant Physiol. 2010; 153(4):1453–63.

    Article  PubMed Central  CAS  PubMed  Google Scholar 

  15. 15

    Wan Y, Ash WM, Fan L, Hao H, Kim MK, Lin J. Variable-angle total internal reflection fluorescence microscopy of intact cells of Arabidopsis thaliana. Plant Methods. 2011; 7(1):27.

    Article  PubMed Central  CAS  PubMed  Google Scholar 

  16. 16

    Cloetens P, Mache R, Schlenker M, Lerbs-Mache S. Quantitative phase tomography of Arabidopsis seeds reveals intercellular void network. Proc Nat Acad Sci USA. 2006; 103(39):14626–30.

    Article  PubMed Central  CAS  PubMed  Google Scholar 

  17. 17

    Costa A, Candeo A, Fieramonti L, Valentini G, Bassi A. Calcium dynamics in root cells of Arabidopsis thaliana visualized with selective plane illumination microscopy. PLoS ONE. 2013; 8:75646.

    Article  Google Scholar 

  18. 18

    Fernandez R, Das P, Mirabet V, Moscardi E, Traas J, Verdeil J, et al. Imaging plant growth in 4D: robust tissue reconstruction and lineaging at cell resolution. Nat Methods. 2010; 7:547–53.

    Article  CAS  PubMed  Google Scholar 

  19. 19

    Leea K, Avondob J, Morrisonc H, Blotb L, Starkd M, Sharpec J, et al. Visualizing plant development and gene expression in three dimensions using optical projection tomography. Plant Cell. 2006; 18:2145–56.

    Article  Google Scholar 

  20. 20

    Mairhofer S, Zappala S, Tracy SR, Sturrock C, Bennett M, Mooney SJ, et al. RooTrak: automated recovery of three-dimensional plant root architecture in soil from X-ray microcomputed tomography images using visual tracking. Plant Physiol. 2012; 158(2):561–9.

    Article  PubMed Central  CAS  PubMed  Google Scholar 

  21. 21

    Zappala S, Mairhofer S, Tracy S, Sturrock CJ, Bennett M, Pridmore T, et al. Quantifying the effect of soil moisture content on segmenting root system architecture in X-ray computed tomography images. Plant and Soil. 2013; 370(1-2):35–45.

    Article  CAS  Google Scholar 

  22. 22

    Mairhofer S, Zappala S, Tracy S, Sturrock C, Bennett MJ, Mooney SJ, et al. Recovering complete plant root system architectures from soil via X-ray micro-computed tomography. Plant Methods. 2013; 9(8):1–7.

    Google Scholar 

  23. 23

    Salon C, Jeudy C, Bernard C, Mougel C, Coffin A, Bourion V, et al. Google Patents. EP Patent App. 2014:EP20,130,173,626. http://www.google.com/patents/EP2679088A1?cl=fr.

  24. 24

    Dinneny JR. Luciferase Reporter System for Roots and Methods of Using the Same. Google Patents. US Patent App. 2014; 13/970:960. http://www.google.com/patents/US20140051101.

    Google Scholar 

  25. 25

    Rellán Álvarez R. Growth and luminescence observatory for roots (glo-roots): A platform for the analysis of root structure and physiology in soil. In: Plant and Animal Genome XXII Conference. Plant and Animal Genome: 2014.

  26. 26

    Chéné Y, Belin E, Chapeau-Blondeau F, Boureau T, Caffier V, Rousseau D. Anatomo-functional bimodality imaging for plant phenotyping: An insight through depth imaging coupled to thermal imaging. In: Plant Image Analysis: Fundamentals and Applications. Boca Raton: CRC Press: 2014. Chap. 9.

    Google Scholar 

  27. 27

    Paulus S, Behmann J, Mahlein A-K, Plümer L, Kuhlmann H. Low-cost 3d systems: Suitable tools for plant phenotyping. Sensors. 2014; 14(2):3001–18.

    Article  PubMed Central  PubMed  Google Scholar 

  28. 28

    Jones HG, Vaughan RA. Remote Sensing of Vegetation: Principles, Techniques, and Applications. Oxford: Oxford University Press; 2010.

    Google Scholar 

  29. 29

    Zarco-Tejada PJ, González-Dugo V, Berni JA. Fluorescence, temperature and narrow-band indices acquired from a UAV platform for water stress detection using a micro-hyperspectral imager and a thermal camera. Remote Sensing Environ. 2012; 117:322–37.

    Article  Google Scholar 

  30. 30

    Hettinger JW, de la Pena Mattozzi M, Myers WR, Williams ME, Reeves A, Parsons RL, et al. Optical coherence microscopy. a technology for rapid, in vivo, non-destructive visualization of plants and plant cells. Plant Physiol. 2000; 123(1):3–16.

    Article  PubMed Central  CAS  PubMed  Google Scholar 

  31. 31

    Meglinski I, Buranachai C, Terry L. Plant photonics: application of optical coherence tomography to monitor defects and rots in onion. Laser Phys Lett. 2010; 7(4):307.

    Article  Google Scholar 

  32. 32

    Dhondt S, Wuyts N, Inzé D. Cell to whole-plant phenotyping: the best is yet to come. Trends Plant Sci. 2013; 18(8):428–39.

    Article  CAS  PubMed  Google Scholar 

  33. 33

    Ehrhardt DW, Frommer WB. New technologies for 21st century plant science. The Plant Cell Online. 2012; 24(2):374–94.

    Article  CAS  Google Scholar 

  34. 34

    Sozzani R, Busch W, Spalding EP, Benfey PN. Advanced imaging techniques for the study of plant growth and development. Trends in Plant Sci. 2014; 19(5):304–10.

    Article  CAS  Google Scholar 

  35. 35

    Benoit L, Belin É, Durr C, Chapeau-Blondeau F, Demilly D, Ducournau S, et al. Computer vision under inactinic light for hypocotyl-radicle separation with a generic gravitropism-based criterion. Comput Electron Agric. 2015; 111:12–7.

    Article  Google Scholar 

  36. 36

    Bell K, Mitchell S, Paultre D, Posch M, Oparka K. Correlative imaging of fluorescent proteins in resin-embedded plant material1. Plant Physiol. 2013; 161(4):1595–603.

    Article  PubMed Central  CAS  PubMed  Google Scholar 

  37. 37

    Jahnke S, Menzel MI, Van Dusschoten D, Roeb GW, Bühler J, Minwuyelet S, et al. Combined mri–pet dissects dynamic changes in plant structures and functions. The Plant J. 2009; 59(4):634–44.

    Article  CAS  Google Scholar 

  38. 38

    Zitova B, Flusser J. Image registration methods: a survey. Image Vision Comput. 2003; 21(11):977–1000.

    Article  Google Scholar 

  39. 39

    Lowe DG. Distinctive image features from scale-invariant keypoints. Int J Comput Vision. 2004; 60(2):91–110.

    Article  Google Scholar 

  40. 40

    Dale MRT, Mah M. The use of wavelets for spatial pattern analysis in ecology. Journal of Vegetation Science. 1998; 9(6):805–14.

    Article  Google Scholar 

  41. 41

    Gu X, Du J-X, Wang X-F. Leaf recognition based on the combination of wavelet transform and Gaussian interpolation. In: Advances In Intelligent Computing. Berlin: Springer: 2005. p. 253–62.

    Google Scholar 

  42. 42

    Prasad S, Kumar P, Tripathi R. Plant leaf species identification using curvelet transform. In: 2nd International Conference on Computer and Communication Technology (ICCCT). IEEE: 2011. p. 646–52.

  43. 43

    Casanova D, de Mesquita Sa Junior JJ, Martinez Bruno O. Plant leaf identification using Gabor wavelets. Int J Imaging Sys Technol. 2009; 19(3):236–43.

    Article  Google Scholar 

  44. 44

    Bours R, Muthuraman M, Bouwmeester H, van der Krol A. Oscillator: A system for analysis of diurnal leaf growth using infrared photography combined with wavelet transformation. Plant Methods. 2012; 8(1):29.

    Article  PubMed Central  PubMed  Google Scholar 

  45. 45

    Epinat V, Stein A, de Jong SM, Bouma J. A wavelet characterization of high-resolution NDVI patterns for precision agriculture. Int J Appl Earth Observation Geoinformation. 2001; 3(2):121–32.

    Article  Google Scholar 

  46. 46

    Strand EK, Smith AM, Bunting SC, Vierling LA, Hann DB, Gessler PE. Wavelet estimation of plant spatial patterns in multitemporal aerial photography. Int J Remote Sensing. 2006; 27(10):2049–54.

    Article  Google Scholar 

  47. 47

    Frangi AF, Niessen WJ, Vincken KL, Viergever MA. Multiscale vessel enhancement filtering. In: Medical Image Computing and Computer-Assisted Interventation-MICCAI’98. Berlin: Springer: 1998. p. 130–7.

    Google Scholar 

  48. 48

    Sage D, Neumann FR, Hediger F, Gasser SM, Unser M. Automatic tracking of individual fluorescence particles: Application to the study of chromosome dynamics. IEEE Trans Image Process. 2005; 14:1372–83.

    Article  PubMed  Google Scholar 

  49. 49

    Huang NE, Shen Z, Long SR, Wu MC, Shih HH, Zheng Q, et al. The empirical mode decomposition and the Hilbert spectrum for nonlinear and non-stationary time series analysis. Proc R Soc London Ser A: Math Phys Eng Sci. 1998; 454(1971):903–95.

    Article  Google Scholar 

  50. 50

    Nunes JC, Bouaoune Y, Delechelle E, Niang O, Bunel P. Image analysis by bidimensional empirical mode decomposition. Image Vision Comput. 2003; 21(12):1019–26.

    Article  Google Scholar 

  51. 51

    Nunes JC, Guyot S, Deléchelle E. Texture analysis based on local analysis of the bidimensional empirical mode decomposition. Machine Vision Appl. 2005; 16(3):177–88.

    Article  Google Scholar 

  52. 52

    Myers WL, Patil GP. Pattern-Based Compression of Multi-Band Image Data for Landscape Analysis. Berlin: Springer; 2006.

    Google Scholar 

  53. 53

    Buades A, Coll B, Morel J-M. A review of image denoising algorithms, with a new one. Multiscale Model Simul. 2005; 4(2):490–530.

    Article  Google Scholar 

  54. 54

    Buades A, Coll B, Morel J-M. A non-local algorithm for image denoising. In: Computer Vision and Pattern Recognition, 2005. CVPR 2005. IEEE Computer Society Conference On. vol. 2. IEEE: 2005. p. 60–5.

  55. 55

    Palmer MW. Fractal geometry: A tool for describing spatial patterns of plant communities. Vegetatio. 1988; 75:91–102.

    Article  Google Scholar 

  56. 56

    Critten DL. Fractal dimension relationships and values associated with certain plant canopies. J Agric Eng Res. 1997; 67:61–72.

    Article  Google Scholar 

  57. 57

    Alados CL, Escos J, Emlen JM, Freeman DC. Characterization of branch complexity by fractal analyses. Int J Plant Sci. 1999; 160:147–55.

    Article  Google Scholar 

  58. 58

    Morávek Z, Fiala J. Fractal dynamics in the growth of root. Chaos, Solitons & Fractals. 2004; 19:31–4.

    Article  Google Scholar 

  59. 59

    Alados CL, Pueyo Y, Navas D, Cabezudo B, Gonzalez A, Freeman DC. Fractal analysis of plant spatial patterns: A monitoring tool for vegetation transition shifts. Biodivers Conserv. 2005; 14:1453–68.

    Article  Google Scholar 

  60. 60

    Ruderman DL, Bialek W. Statistics of natural images: Scaling in the woods. Phys Rev Lett. 1994; 73:814–7.

    Article  PubMed  Google Scholar 

  61. 61

    Ruderman DL. Origins of scaling in natural images. Vision Res. 1997; 37(23):3385–98.

    Article  CAS  PubMed  Google Scholar 

  62. 62

    Chauveau J, Rousseau D, Richard P, Chapeau-Blondeau F. Multifractal analysis of three-dimensional histogram from color images. Chaos, Solitons & Fractals. 2010; 43(1):57–67.

    Article  Google Scholar 

  63. 63

    Chauveau J, Rousseau D, Chapeau-Blondeau F. Fractal capacity dimension of three-dimensional histogram from color images. Multidimensional Syst Signal Process. 2010; 21(2):197–211.

    Article  Google Scholar 

  64. 64

    Chapeau-Blondeau F, Chauveau J, Rousseau D, Richard P. Fractal structure in the color distribution of natural images. Chaos, Solitons & Fractals. 2009; 42(1):472–82.

    Article  Google Scholar 

  65. 65

    Chéné Y, Belin E, Rousseau D, Chapeau-Blondeau F. Multiscale analysis of depth images from natural scenes: Scaling in the depth of the woods. Chaos, Solitons & Fractals. 2013; 54:135–49.

    Article  Google Scholar 

  66. 66

    Ferraro P, Godin C, Prusinkiewicz P. Toward a quantification of self-similarity in plants. Fractals. 2005; 13:91–109.

    Article  Google Scholar 

  67. 67

    Martinez Bruno O, de Oliveira Plotze R, Falvo M, de Castro M. Fractal dimension applied to plant identification. Inf Sci. 2008; 178:2722–33.

    Article  Google Scholar 

  68. 68

    Da Silva D, Boudon F, Godin C, Sinoquet H. Multiscale framework for modeling and analyzing light interception by trees. Multiscale Model Simul. 2008; 7:910–33.

    Article  Google Scholar 

  69. 69

    Chéné Y, Rousseau D, Lucidarme P, Bertheloot J, Caffier V, Morel P, et al. On the use of depth camera for 3D phenotyping of entire plants. Comput Electron Agric. 2012; 82:122–7.

    Article  Google Scholar 

  70. 70

    Chandra M, Rani M. Categorization of fractal plants. Chaos Solitons & Fractals. 2009; 41(3):1442–7.

    Article  Google Scholar 

  71. 71

    Scheuring I, Riedi RH. Application of multifractals to the analysis of vegetation pattern. J Vegetation Sci. 1994; 5(4):489–496.

    Article  Google Scholar 

  72. 72

    Bradshaw G, Spies TA. Characterizing canopy gap structure in forests using wavelet analysis. J Ecol. 1992; 80:205–15.

    Article  Google Scholar 

  73. 73

    Tastumi J, Yamauchi A, Kono Y. Fractal analysis of plant root systems. Ann Bot. 1989; 64(5):499–503.

    Google Scholar 

  74. 74

    Izumi Y, Iijima M. Fractal and multifractal analysis of cassava root system grown by the root-box method. Plant Production Sci. 2002; 5(2):146–51.

    Article  Google Scholar 

  75. 75

    Ketipearachchi KW, Tatsumi J. Local fractal dimensions and multifractal analysis of the root system of legumes. Plant Production Sci. 2000; 3(3):289–95.

    Article  Google Scholar 

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Acknowledgements

This work received supports from the French Government supervised by the Agence Nationale de la Recherche in the framework of the program Investissements d’Avenir under reference ANR-11-BTBR-0007 (AKER program).

Author information

Affiliations

  1. Université de Lyon, Laboratoire CREATIS, CNRS, UMR5220, INSERM, U1044, Université Lyon 1, INSA-Lyon, Villeurbanne, France

    David Rousseau

  2. Laboratoire Angevin de Recherche en Ingénierie des Systèmes (LARIS), Université d’Angers, 62 avenue Notre Dame du Lac, Angers, 49000, France

    Yann Chéné, Etienne Belin, Georges Semaan & François Chapeau-Blondeau

  3. GEVES, Station Nationale d’Essais de Semences (SNES), rue Georges Morel, Beaucouzé, 49071, France

    Ghassen Trigui & Karima Boudehri

  4. La Plateforme d’Ingénierie et Analyses Moléculaires (PIAM), Université d’Angers, Angers, 49000, France

    Florence Franconi

Authors
  1. David Rousseau
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  2. Yann Chéné
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  3. Etienne Belin
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  4. Georges Semaan
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  5. Ghassen Trigui
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  6. Karima Boudehri
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  7. Florence Franconi
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  8. François Chapeau-Blondeau
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Corresponding author

Correspondence to David Rousseau.

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Competing interests

The authors declare that they have no competing interests.

Authors’ contributions

DR conceived and designed this review, carried out the acquisition of OCT and RGB-depth data, conceived and interpreted the whole data, wrote and revised the manuscript. YC realized the acquisition and data analysis of RGB-depth images. EB helped in the analysis of RX-MRI data and revised the manuscript. GS helped in the acquisition and carried out the analysis of MRI data. GT and KB carried out the acquisition and analysis of RX data. FF carried out the MRI acquisition. FCB helped in the analysis of RGB-depth images and contributed in the writing and revision of the manuscript. All authors read and approved the final manuscript.

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Rousseau, D., Chéné, Y., Belin, E. et al. Multiscale imaging of plants: current approaches and challenges. Plant Methods 11, 6 (2015). https://doi.org/10.1186/s13007-015-0050-1

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Keywords

  • Mutiscale imaging
  • Multiscale filtering
  • Wavelets
  • Fractal
  • ImageJ plugins

Plant Methods

ISSN: 1746-4811