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Ординатура / Офтальмология / Английские материалы / Retinal Development_Sernagor, Eglen, Harris, Wong_2006

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S. J. Eglen and L. Galli-Resta

Figure 10.1 Example mosaic of cholinergic amacrine cells from the inner nuclear layer of a postnatal day (P)3 rat retina. Cell bodies, clearly labelled by choline acetyltransferase, are regularly distributed across the sample area. Scale bar is 10 µm.

10.2.1 Interactions between homotypic (mosaic) cells

Given that many types of retinal neurons form mosaics during development, it is plausible to think that interactions between cells of different types may influence the formation of retinal mosaics. However, several lines of evidence outlined below indicate that in most cases interactions between different cell types do not guide the development of retinal cells. Instead, it seems that interactions between cells of the same type (homotypic interactions) are sufficient to guide mosaic formation.

First, computer simulations have demonstrated that a spatial distribution of retinal cells can be replicated by assuming that each cell is surrounded by an ‘exclusion zone’. In the

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model, neurons are positioned randomly into the array, subject only to the constraint that a cell cannot be placed within another cell’s exclusion zone. This model is known as the dmin model, where dmin is the parameter that specifies the diameter of the circular exclusion zone surrounding the cell body (Galli-Resta et al., 1997). A limitation of this model is that although it shows some form of exclusion zone acting on homotypic neurons is sufficient to generate mosaics, it does not suggest candidate biological mechanisms that might generate an exclusion zone. However, it does suggest that the mechanism can be fairly local, rather than long-ranging.

Experimental evidence against heterotypic interactions in forming retinal mosaics comes from cross-correlation studies. Rockhill et al. (2000) examined six different cell types in rabbit retina and tested for the existence of spatial correlation between pairs of mosaics. In each case, the cross-correlation analysis indicated that the positioning of one type of neuron was spatially independent of another type of neuron. To date, only one positive crosscorrelation between cell types, blue cones and blue-cone bipolar cells in the monkey, has been reported (Kouyama and Marshak, 1997). Likewise, only one negative cross-correlation between two cell types, horizontal and short-wavelength cones, has been reported (Ahnelt et al., 2000). Hence, cross-correlations between cell types are likely to be rare exceptions to the general principle of spatial independence between different classes of neuron.

In addition to the computer modelling and analysis of retinal mosaics, direct experimental manipulations have been performed to test for heterotypic interactions in mosaic formation. For example, since the cholinergic amacrine cells and retinal ganglion cells (RGCs) are synaptic partners, it might be possible that these two cell types influence each other during mosaic formation. However, spatial organization of cholinergic amacrine cells in the developing rodent retina was unaffected by either complete loss of RGCs or by doubling the density of RGCs (Galli-Resta, 2000). Likewise, in the case of the horizontal cells the loss of photoreceptor synaptic input, or the presence of a higher than normal cell density around these cells, did not alter their spatial regularity (Raven and Reese, 2003; Rossi et al., 2003). Taken together, these analytical and experimental results suggest that whatever mechanisms are involved in mosaic formation, heterotypic interactions are unlikely to play a major role.

10.2.2Cell fate

All of the different types of retinal cells originate from one population of postmitotic cells, with a stereotypical sequence in the birthdates of the different types of retinal neuron (see Chapter 3 and Chapter 5). For example, RGCs are born first, whereas bipolar cells are born among the latest (Livesey and Cepko, 2001). Although the fate of an individual postmitotic cell becomes restricted during development (Cepko et al., 1996), it has been suggested that a cell’s fate to become a certain type of neuron is influenced by environmental factors, perhaps from neighbouring cells. In analogy to the lateral inhibition process active in Drosophila, whereby R8 photoreceptors inhibit neighbouring cells to take the R8 fate, lateral inhibition has been proposed for different types of photoreceptor both in primates and goldfish (Wikler and Rakic, 1991; Stenkamp et al., 1997). It has also been suggested

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that RGCs secrete factors that inhibit neighbouring postmitotic cells from also becoming RGCs (Waid and McLoon, 1998). Furthermore, a diffusible signal acting as an inhibitory cue in cell fate processes is suggested to be responsible for the spatial arrangement of tyrosine hydroxylaseand 5-hydroxytryptamine-positive cells (Tyler et al., 2005). However, the chemical identity of such inhibitory factors has not yet been determined. In contrast, much is known about the molecular signals involved in the specification of the different classes of photoreceptor in each ommatidium of the Drosophila eye (Freeman, 1997). Given the similarities between vertebrate and invertebrate eye development (Jarman, 2000), mechanisms observed in Drosophila may well inform future vertebrate studies.

Cell fate mechanisms are likely to be implicated in generating the correct density of each type of neuron, but whether they contribute to the ultimate spatial positioning of cells is unclear. In principle, mutual inhibition of neighbouring cells from adopting the same fate can contribute to spatial order in a population of neurons, as verified by computer models (Eglen and Willshaw, 2002). These theoretical arguments are supported by findings from RGCs in chick, which are seen to be regularly distributed early in development, before migration to their final layer (McCabe et al., 1999). However, since cell fate mechanisms occur relatively early in development, many other subsequent mechanisms (mentioned below) may interfere with any order generated by cell fate mechanisms. This seems to be the case at least for cholinergic amacrine cells; as they migrate to their destination layer, they do not observe minimal spacing constraints (Galli-Resta et al., 1997). This would suggest that if any minimal spacing constraints were created among cholinergic amacrines by early cell fate mechanisms, it is subsequently lost once cells migrate away from the ventricular zone. In contrast, cell fate mechanisms may be sufficient to create ordering in Drosophila, since cells do not migrate subsequent to the cell fate decision process.

10.2.3 Radial and lateral migration

The lack of good biochemical markers for identifying most types of retinal neuron early in development means that the extent to which cell fate mechanisms can aid mosaic formation is still largely unknown. However, even after cell fate specification, most types of retinal neuron need to migrate away from the ventricular zone into their final destination layer (described in Chapter 4). Depending on the extent of this movement, the initial ordering imposed by any cell fate mechanisms may be destroyed by subsequent migration. Hence, later acting mechanisms must also be involved.

Lineage tracing techniques were used to study the migration of groups of neurons that descended from individual retinal progenitors. These studies found that the cells originated from individual progenitors were organized into columns spanning across the depth of the retina, from which it was suggested that retinal cells migrate predominantly in a radial fashion from the ventricular zone (Turner and Cepko, 1987; Holt et al., 1988). Occasionally, labelled cells were found outside of the radial columns, but since they occurred rarely these were thought to be artefactual or ectopic (Reese and Galli-Resta, 2002). However, by using an X-inactivation transgenic mouse, 50% of all retinal projectors were labelled with the

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Figure 10.2 Lateral migration of certain classes of retinal neuron away from their clonal column of origin. (A) Retinal section from a female hemizygous transgenic mouse showing labelled cells arranged into columns passing through both the inner and outer nuclear layers (INL and ONL). Outside of these columns, tangentially dispersed cells are observed (indicated by arrows). These cells are horizontal cells (single arrowhead), amacrine cells (double arrowhead) and a ganglion cell (arrow) in the ganglion cell layer (GCL). (B) Retinal section from chimeric mouse (produced by blastocyst injection of embryonic stem cells) whereby a smaller fraction of cells is labelled, thus allowing easier visualization of the clonal columns. Again, tangentially displaced horizontal, amacrine, ganglion cells are observed, together with a blue cone in the ONL (arrow). Scale bar is 50 µm in (A) and 75 µm in (B). Modified from Reese and Galli-Resta (2002) with permission from Prog. Retin. Eye Research.

LacZ reporter and hence half of the subsequently generated retinal cells were labelled. In common with the earlier studies, most labelled cells were found in radial columns. However, in addition, many cells were observed outside of these columns, suggesting that some cells moved laterally away from their radial column of origin (Figure 10.2; Reese et al., 1995).

By studying the identity of the neurons that moved, it was found that only certain classes of retinal neuron (cone photoreceptors, horizontal, amacrine and ganglion cells) moved radially, but that for those classes, all cells in each class moved laterally (Reese et al., 1999). The extent of tangential movement away from the nearest column was around 45 to 150 µm. Furthermore, the cell classes that move radially are also the classes whose mosaics are the most regular. From these results, it is suggested that tangential migration of cells away from their radial clone of origin aids mosaic formation. The time at which cells undergo tangential migration has not been precisely determined for most cell types. In the case of mouse horizontal cells, tangential migration occurs around postnatal day (P)1 to P5, which is about the same time as when horizontal cells change from a radial to a horizontal morphology. This correlation between morphological changes and tangential migration hints at a possible mechanism underlying the lateral movements (see Section 10.2.5).

10.2.4 Cell death

Cell death is a process found throughout the developing nervous system, and the retina is no exception. For example, it has been estimated that across a range of mammalian

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species, 50% to 90% of RGCs that are born will die during development (Finlay and Pallas, 1989). This retinal cell death has largely been implicated in the refinement of the retinal projections to their targets (O’Leary et al., 1986; but see Chapter 11 for discussion of other roles for cell death). However, more recently cell death has been suggested to be involved in the formation of retinal mosaics. If a group of retinal neurons form an irregular mosaic early in development, cell death might kill those neurons that are too close to one another. This would increase the size of the exclusion zone around a cell and thus improve regularity (Galli-Resta, 1998; Cook and Chalupa, 2000). This cell death might be mediated by cells competing with each other for trophic support or contacts from their afferents (W¨assle and Riemann, 1978; Kirby and Steineke, 1996), or might even be triggered by neighbouring cells. Part of the difficulty of understanding the impact of cell death is that currently it is very difficult to directly observe its effects; instead we have to rely on indirect observations (after cell death has occurred) to infer what role cell death is playing.

Two recent studies have implicated a role of cell death in the formation of retinal mosaics. First, in cat retina, the mosaic of alpha RGCs increases its regularity during the first postnatal month as the density of alpha RGCs drops by around 20%. This death seems normally driven by mechanisms related to cell spacing, since when spiking activity in the RGCs is blocked the magnitude of cell death is not altered, but mosaic regularity is not improved (Jeyarasasingam et al., 1998). This suggests that the activity patterns of alpha cells influence which cells die during development in a way that improves mosaic regularity. Second, the Bcl-2 overexpressing mouse was used to study the influence of cell death upon mosaic formation. Bcl-2 is an anti-apoptotic gene, and its overexpression inhibits naturally occurring cell death, leading to an increase in density of most retinal cell types (Strettoi and Volpini, 2002). Out of all neuronal types, dopaminergic amacrine cells showed the largest (tenfold) increase in density compared with wild-type retinas. In the Bcl-2 mouse, the dopaminergic amacrine cells were less regular than in wild type, where many close pairs of dopaminergic cells were often observed (Raven et al., 2003). Since the Bcl-2 mouse inhibits naturally occurring cell death, the suggestion is that cell death would normally remove cells that are positioned too close to neighbouring cells of the same type. These two studies differ in the magnitude of cell death observed (20% versus 90%) in a population, and computermodelling studies suggest that 20% cell death is insufficient by itself to transform irregular into highly regular arrays (Eglen and Willshaw, 2002). By contrast, the magnitude of cell death observed in the dopaminergic amacrine cells is very large compared with the mild increase in regularity in wild-type animals, suggesting that the choice of which cells to eliminate need not be very selective.

Retinal cell death is also unlikely to be a universal mechanism by which mosaics are generated. In the developing rat retina, around 20% of cholinergic amacrine cells die from P4 to P12, without any increase in mosaic regularity (Galli-Resta and Novelli, 2000). Also, cell death was suggested to be too small to account for the creation of a spatial dependency between blue cones and blue-cone bipolar cells (Kouyama and Marshak, 1997). It is therefore likely that cell death is just one of several mechanisms used to create a regular

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distribution of neurons. Modelling work suggests for example that it can be used after early cell fate events to produce regular mosaics (Eglen and Willshaw, 2002).

All these studies refer to late waves of cell death, eliminating cells once they have been generated and positioned. Cell death also occurs earlier in retinal development, sculpting the pool of progenitor cells that are available (de la Rosa and de Pablo, 2000), or affecting single cell populations at the same time as new cells are also formed or migrating. An early phase of cell death has been recently shown to contribute to mosaic formation: blocking purinergic receptors in the retina of newborn rodents at P1 to P4 inhibits an early phase of cholinergic cell death and leads to typically a 30% increase in the density of cholinergic cells (Resta et al., 2005). In the treated retinas, many pairs of nearby cholinergic cells are observed, a feature absent from control retinas. Considering that cholinergic cells are thought to be sources themselves of extracellular adenosine triphosphate (e-ATP), and that e-ATP does not diffuse far beyond 50 µm (Newman 2001), it has been suggested that cholinergic cells could be releasing e-ATP in a local fashion to cause close-neighbouring cholinergic cells to die (Resta et al., 2005).

10.2.5 Dendritic interactions

So far we have seen that several mechanisms are implicated in the formation of retinal mosaics. Out of these mechanisms, lateral cell migration seems to play a major role in rearranging cells into a regular array. Computer modelling has been instructive to help our understanding of how mosaics might form. For example, the dmin model has shown that interactions need only be between cells of the same type to produce regular arrays similar to those observed experimentally. Furthermore, the dmin model also suggests that an exclusion zone mechanism local to each cell is sufficient to generate global order in the array. Following up on a hypothesis suggested by W¨assle and Riemann (1978), another computer model suggested that interactions between dendrites of neighbouring cells might cause cells to repel each other and rearrange the cell bodies from a random into a regular array (Eglen et al., 2000). What evidence is there for a role of dendritic interactions driving lateral cell migration and hence mosaic formation?

Two experimental studies provide indirect evidence in favour of dendritic interactions. First, horizontal cells in the mouse migrate to their destination layer, the inner nuclear layer (INL), by P1. At this stage they have a radial morphology. Within the next few days, the cells then displace laterally within their layer at the same time as the cell’s morphology changes from radial to horizontal, forming an initial dendritic tree (Reese et al., 1999). Second, when cholinergic cells first arrive in their destination layer, either the INL or ganglion cell layer (GCL), at around embryonic day (E)21, the cell bodies are irregularly spaced and there are many holes in the dendritic network. Soon afterwards (P0) the cell bodies form regular arrays at the same time as the network of dendrites becomes more complete (Galli-Resta et al., 2002).

These findings correlate the emergence of dendritic trees with the formation of retinal mosaics, but do not directly show a role for dendrites upon mosaic formation. However,

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Figure 10.3 Dependence of dendritic network upon mosaic formation. (A) At P0, cholinergic amacrine cell bodies in the rat are regularly spaced, and their dendrites interconnect to form a network. (B) A few days earlier, at E21, the dendritic network is poor and the somas are not so regularly positioned. (C, D, E) State of the network of cholinergic amacrine cells before (C), during (D) and after (E) disruptions of the dendritic network by treatments that affect the microtubule-associated proteins within the dendrites. During the treatment, the regular arrangement of neurons collapses; after the treatment wears off (a few days later), a regular mosaic returns. Scale bars: 10 µm. Figure reproduced from Galli-Resta (2002) with permission from Trends Neurosci. For colour version, see Plate 9.

Galli-Resta et al. (2002) provided direct evidence by manipulating the dendritic trees during development. Microtubules form the scaffold of both axonal and dendritic processes. Selective perturbation of the microtubules in the cholinergic and horizontal cells, either pharmacologically or with antisense oligonucleotides, disrupted the dendritic network leading to a collapse in the regular spacing of cell bodies within a layer and also to cells moving out of their normal layer (Figure 10.3; Galli-Resta et al., 2002). Remarkably, these effects were reversible, and after around two days, when the experimental treatments had worn off, both the dendritic network and regular mosaic returned. Similar effects were found for both cholinergic and horizontal cells, suggesting this mechanism is not specific to one cell type.

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To explain these findings Galli-Resta (2002) has proposed a micromechanical hypothesis of mosaic assembly. As neurons migrate to their destination layer they begin to form connections with dendrites from other neurons of the same type, creating a mechanical network. The microtubules in the dendrites provide a rigid skeleton that counteracts an elastic component to keep the net together. After the net is first formed, cells within the network are positioned at different depths in the retina, but still respect the minimal distance constraints (in 3-d) to neighbouring cells. Shortly afterwards, the cells move such that they are all positioned in the same layer, again respecting minimal distance constraints. From here, the network settles at equilibrium into a regular array of cells. Disruption of the microtubules causes local disturbances in the network, from which cells lose their regular spacing.

This model of mosaic assembly accounts for the results observed disrupting microtubules in the cholinergic and horizontal cells, however, it still requires further testing. For example, what are the mechanisms by which neighbouring neurons of the same type can recognize each other? One requirement of the model is that homotypic neurons must be able to create a network via their dendrites. While dendritic nets are observed in development for the horizontal cells and cholinergic amacrine cells, other types of retinal neuron have little dendritic contact with neighbouring neurons of the same type. For example, beta RGCs form few, if any, contacts with neighbouring beta RGCs, instead forming contacts with presynaptic amacrine and bipolar cells. It is thus to be seen whether this mechanical model of mosaic assembly can account for the regular arrangement of different types of RGCs.

10.3 Mathematical methods for quantifying regularity of retinal mosaics

Once a group of neurons has been labelled by using a specific chemical marker, visual inspection of the tissue may already tell us that the cells are regularly ordered. However, quantitative methods are normally required to evaluate the degree of regularity in retinal mosaics, and to allow comparisons between mosaics from different types of retinal neuron. Several methods have been developed, which are described in this section.

The earliest, and still dominant, technique for quantifying the regularity in the spatial distribution of cells has been the regularity index (RI), based upon finding the distance to nearest neighbours (W¨assle and Riemann, 1978; Cook, 1996). For each neuron, we measure the distance to the nearest neighbouring neuron of the same type (Figure 10.4a,b). We then define the RI as the mean of these nearest-neighbour distances divided by their standard deviation. The higher the RI, the more regular the population is. As a rough guideline, an RI around 2 or less typically indicates that the mosaic is randomly arranged. Higher values of the RI indicate that the mosaic is non-randomly arranged. Regularity index values in the range 3 to 9 are typical for regular retinal mosaics from different species.

The RI measure is dominant today because of its relative simplicity to calculate. However, since it measures only the nearest-neighbour distance, it clearly does not capture all the spatial information in a mosaic. For example, a group of cells equally spaced along a (one-dimensional) line will have the same RI as a group of cells positioned in a regular (two-dimensional) grid. Other methods have therefore been developed to capture the relative

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Figure 10.4 Example of a population of cells forming a retinal mosaic. (a) Example mosaic of horizontal cell somas from adult mouse retina. Cell bodies (10 µm diameter) are drawn to scale. Scale bar: 50 µm. (b) Nearest-neighbour histogram computed by finding the distance from each cell in (a) to its nearest neighbour. The regularity index here is 5.2. (c) Autocorrelation plot of the field shown in (a). Each annulus is 10 µm wide. (d) Density recovery profile of the field. Each histogram bar shows the density of cells in the corresponding annulus from the autocorrelation in (c). If cells were randomly positioned, the profile would be flat (shown by dotted line). The ‘well’ in the histogram out to around 20 µm (vertical line) indicates the size of the exclusion zone for this field. See Section 10.3 for details of the analysis methods used for determining mosaic regularity.

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Figure 10.5 Voronoi tessellation of a population of cells. Each retinal cell from a simulated population has been drawn as a circle; each cell is surrounded by its Voronoi polygon, denoting all points of space that are closest to that cell. For one central cell, dashed lines indicate the Delaunay segments to its neighbouring cells.

positioning of many neighbouring neurons. One popular approach has been to study the autocorrelation plot (Figure 10.4c), from which various measures can be calculated (Figure 10.4d; Rodieck, 1991). The autocorrelation plot is created by positioning each neuron at the centre of the plot, and then plotting the relative position of all other neurons. A common feature of the autocorrelation plot for retinal neurons is that there is a central ‘exclusion zone’ where few, if any, cells can be found. This indicates that no two neurons tend to come closer than some minimal distance from each other. Furthermore, this minimal distance is often much larger than the relatively small distance that is imposed by ‘steric hindrance’, since two somas cannot overlap in the same layer. A cross-correlation plot is similar to the autocorrelation plot (Figure 10.4c) except that for each cell of type A we plot the relative position of type B cells (Rodieck, 1991).

More recently, measures based on the Voronoi tessellation have been used to evaluate mosaic regularity (Figure 10.5). The Voronoi tessellation divides the retinal surface into nonoverlapping polygons, with one retinal neuron inside each polygon; the polygon encloses all points in the plane that are closest to that cell. Equivalently, the Delaunay triangulation