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**|**PLoS Comput Biol**|**v.13(7); 2017 July**|**PMC5515450

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PLoS Comput Biol. 2017 July; 13(7): e1005615.

Published online 2017 July 3. doi: 10.1371/journal.pcbi.1005615

PMCID: PMC5515450

Alexandra Vormberg, Conceptualization, Data curation, Formal analysis, Methodology, Software, Visualization, Writing – original draft, Writing – review & editing,^{1,}^{2,}^{*} Felix Effenberger, Conceptualization, Formal analysis, Methodology, Software, Writing – original draft, Writing – review & editing,^{1,}^{2} Julia Muellerleile, Conceptualization, Software, Writing – original draft, Writing – review & editing,^{3} and Hermann Cuntz, Conceptualization, Formal analysis, Funding acquisition, Methodology, Software, Supervision, Writing – original draft, Writing – review & editing^{1,}^{2,}^{*}

Boris S. Gutkin, Editor^{}

École Normale Supérieure, College de France, CNRS, FRANCE

The authors have declared that no competing interests exist.

Received 2017 January 27; Accepted 2017 June 5.

Copyright © 2017 Vormberg et al

This is an open access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.

Dendrites form predominantly binary trees that are exquisitely embedded in the networks of the brain. While neuronal computation is known to depend on the morphology of dendrites, their underlying topological blueprint remains unknown. Here, we used a centripetal branch ordering scheme originally developed to describe river networks—the Horton-Strahler order (SO)–to examine hierarchical relationships of branching statistics in reconstructed and model dendritic trees. We report on a number of universal topological relationships with SO that are true for all binary trees and distinguish those from SO-sorted metric measures that appear to be cell type-specific. The latter are therefore potential new candidates for categorising dendritic tree structures. Interestingly, we find a faithful correlation of branch diameters with centripetal branch orders, indicating a possible functional importance of SO for dendritic morphology and growth. Also, simulated local voltage responses to synaptic inputs are strongly correlated with SO. In summary, our study identifies important SO-dependent measures in dendritic morphology that are relevant for neural function while at the same time it describes other relationships that are universal for all dendrites.

Similarly to river beds, dendritic trees of nerve cells form elaborate networks that branch out to cover extensive areas. In the 1940s, ecologist Robert E. Horton developed an ordering system for branches in river networks that was refined in the 1950s by geoscientist Arthur N. Strahler, the Horton-Strahler order (SO). Branches at the tips start with order 1 and increase their order in a systematic way when encountering new branches on the way to the root. SO relationships have recently become popular for quantifying dendritic morphologies. Various branching statistics can be studied as a function of SO. Here we describe that topological measures such as the number of branches, the branch bifurcation ratio and the size of subtrees exhibit stereotypical relations with SO in dendritic trees independently of cell type, mirroring universal features of binary trees. Other functionally more relevant features such as mean branch lengths, local diameters and simulated voltage responses to synaptic inputs directly correlate with SO in a cell type-specific manner, indicating the importance of SO for understanding dendrite growth as well as neural computation.

Neurons of the central nervous system have a variety of shapes and possess dendritic trees that exhibit complex branching patterns. Apart from providing neurons with adequate connectivity, dendritic trees are not just simple passive signal conductors but are thought to be involved in sophisticated signal processing and neural computation [1,2]. Theoretical studies have suggested that dendritic morphology alone is able to influence a neuron's functional properties such as its firing patterns [3,4]. In particular, the topology of dendrites has been associated with strong effects on the temporal structure in the spiking behaviour [5,6]. Furthermore, the size of a neuron's dendritic tree, its diameter and its branching properties are all factors that influence the decay of synaptic signals on their way to the soma [7,8]. Understanding the principles governing dendrite morphology is therefore important for understanding neural computation. In order to better characterise and quantify dendritic branching structure, a number of branching statistics have been proposed [9,10]. Yet, these quantities exhibit strong correlations that are mostly unexplored [11]. Even when taken together, a commonly used set of existing branching statistics is not sufficient to cluster morphologies according to their given cell types [12].

In the following, we explore how sorting branching statistics by the precise order of the occurrence of nodes in a tree can increase the interpretative power of these statistical measures. Different methods have been developed to sort branches in dendrites. They mainly divide into those that start ordering the branches from the root, i.e. at the soma (centrifugal), and those that start from the terminal branches (centripetal) [13]. The centrifugal branch ordering method assigns a lowest order of 0 (or 1 depending on the definition) to the root, and increases the order by 1 at each branch point. Centrifugal branch ordering has found common use in many tree-like structures and has been specifically applied to dendritic trees on many occasions [14–20]. Among others, the maximum and mean branch order of dendritic trees have been used to measure dendritic tree complexity [21].

Centripetal ordering schemes, on the other hand, have become increasingly common in recent years and we focus here on the so-called Horton-Strahler or Strahler order (SO), which was originally developed by Robert E. Horton as a stream ordering method for river networks [22]. This scheme was later refined and slightly modified to be objectively quantifiable by Arthur N. Strahler [23]. In Strahler's version, which we use in this study, all terminal branches are assigned order 1. The remaining orders are then constructed in an iterative way: When two branches of order *k* meet, the order of the parent branch is increased to order *k* + 1. When two branches of different order meet, the higher order prevails (see Fig 1A). The highest order of the tree always occurs at the root of the tree. The Strahler order of the root (or the maximal Strahler order assigned to a segment in the tree) is referred to as the Strahler number (SN) of the tree.

While SO started out in the field of geology as a stream classification scheme for river networks, it has since found use in many other scientific fields. For example, SO has been employed to quantitatively describe other tree-like structures such as bronchial trees or pulmonary arteries [24–27], as well as actual botanical trees [28–30]. Yet, it is important to note that certain findings that have been reported using Strahler orders have little descriptive power if the underlying structure is a binary tree. Most prominently this applies to the so-called “Horton’s law of stream numbers” [22], a power law between the counts of branches of a given SO and the SO itself. The slope of this distribution corresponds to the tree’s overall bifurcation ratio (i.e. the ratio of the number of branches between any two consecutive orders). This power law asymptotically approaches 4^{1−k} for SO *k* [31] and the corresponding bifurcation ratio converges to 4 [32,33]. The fact that its descriptive power is weak was only discovered much later in the 1990s using Monte Carlo methods [34]. These findings caused some discussions in the field and, interestingly, seem to be less known to the scientific community outside of hydrology. We will therefore comment on them in the following and distinguish results that are close to the expected case from ones carrying more descriptive power.

To our knowledge, Strahler’s method was first applied to the analysis of neuronal morphologies by Hollingworth and Berry, who used it to quantify and compare the branching structures of Purkinje and pyramidal cell dendrites in rats [35]. Later it was used to analyse the growth patterns of axons in cat visual cortex [36]. In recent years, SO also became popular as a measure of branching complexity in *Drosophila* dendritic arborisation (da) neurons of different classes [37–42]. Despite its wide applicability and relative simplicity, SO has not been studied in detail especially in relation to larger samples of neuronal cell types. Hence, this study uses Strahler's centripetal branch ordering method to investigate and describe the morphology of a variety of reconstructions of real dendrites as well as of synthetic model dendrites. We observe that other SO-sorted distributions of topological measures apart from Horton’s law are also nearly invariant to cell types and reflect universal features of binary trees. However, the metric measures that we studied exhibit differences between distinct cell types and may thus be used to quantify, categorise and better understand dendritic tree structure.

Topological measures of dendritic trees can be calculated without any metric information, simply by analysing the succession of branch points (BPs) and termination points (TPs) in the tree. In the following, we first describe topological relationships with Strahler order (SO) while distinguishing between either segments (from BP—BP or BP—TP) or branches (consecutive segments) of a given SO *k* (Fig 1B). In order to better interpret results from SO-sorted relationships in dendritic trees, we first obtained results from the set of all possible binary trees with a given number of nodes (Fig 2A–2E). After calculating all unsorted binary trees with 16 terminal nodes, we also calculated the reduced set of all sorted binary trees in which the ordering of subtrees at each node is discarded by allowing permutations at all BPs to identify topologically equivalent trees (see Methods; the two trees in the green box in Fig 2A are topologically equivalent since they can be transferred into one another by rotations of subtrees). For such small trees (enumerating this set quickly becomes computationally expensive for larger trees as it grows exponentially with tree size) that are typical for some real dendrites (e.g. dentate gyrus granule cells), the distributions of SO-sorted segments (Fig 2B) and branches (Fig 2C) could vary widely in different binary trees. At one extreme, the so-called “herringbone” tree that is maximally asymmetric (Fig 2A, sample trees in the green box) showed a flat line with SO-sorted segment number (Fig 2B, green bold line) with SO values restricted to 1 and 2. At the other extreme, the complete binary tree (CBT), which is completely filled with nodes on every level (Fig 2A, sample tree in the magenta box), doubled the number of nodes at every step that decreased SO, leading to a 2^{−k} trend (Fig 2B, magenta bold line). By contrast, the mean values for these distributions (Fig 2D and 2E) followed much clearer trends. With increasing SN (the maximal SO assigned to a segment in the tree), the average number of segments per SO for all possible trees of degree 16 was well described by the same 2^{−k} trend predicted by the complete binary tree (Fig 2D, magenta dashed line). This is partly explained by the fact that we grouped trees according to their SN: Maximally asymmetric herringbone trees are characterised by an SN of 2. By contrast, symmetric CBTs exhibit maximal SN values for their respective number of nodes with distributions of 2^{−k}. Asymmetric trees naturally have lower SN values, therefore groups of trees with larger SN will be more symmetric and behave more like the complete binary tree.

The possible distributions for the number of branches per SO also varied widely (Fig 2C) while the averages (Fig 2E) tended to a specific trend, in this case 4^{1−k} (Fig 2E, grey dashed line). This is a consequence of Horton’s law and the 4^{1−k} power described in the introduction.

Generally, their topology has previously linked dendritic trees to certain classes of random binary trees [43]. We therefore compared our results from the set of all possible binary trees of degree 16 with a set of random trees produced by a critical Galton-Watson (GW) random branching process [44] that generates a distribution of trees of different sizes (Fig 2F). Such a GW process has been used in the past to generate a number of topologically distinct binary trees and to model dendrite branching patterns [45]. We obtained a large number of GW binary trees by randomly choosing to either terminate or branch further at every new terminal node in an iterative manner. The branching process was terminated when no further branching occurred or when a total number of 800 nodes was reached. The number of segments distribution grouped by SN (Fig 2G) again followed the 2^{−k} trend that would be expected for the CBT and was very similar to that seen in Fig 2D (see above). As expected from Kirchner [34], the number of branches per SO (Fig 2H) tightly approximated the same relationship as observed for all possible binary trees of degree 16 (Fig 2E). Due to the larger magnitude of GW random binary trees compared to the set of all possible binary trees of degree 16, the trends were much more pronounced. The 4^{1−k} trend in SO-sorted branch numbers can further be observed in the branch bifurcation ratios (Fig 2I), a related topological measure that compares the number of branches of SO *k* with that of the next higher order *k* + 1. Since bifurcations do not allow ratios lower than 2, this lower limit value is true for the CBT where SO increases at every single branch point (Fig 2I, magenta line; see also Fig 2C where the line is an upper bound). In this representation, most data points are evenly scattered around the average bifurcation ratio of 4 (coefficient of determination *R*^{2} = 0.9925), the asymptotic bifurcation ratio calculated previously for a large number of nodes [32–34] (see Discussion). Finally, we studied the topological subtree sizes capturing the number of daughter BPs and TPs for all BPs of a given SO in our GW random binary trees (Fig 2J). Since all nodes with SO 1 are TPs, the values here start at SO 2. We found an exponential increase in subtree size with SO that was not well described by the topological subtree sizes expected for a CBT (Fig 2J, magenta dashed line, root node SN 6) but was rather well approximated by 4^{k−SN} (Fig 2J, grey dashed line shown for all segment SN values), a mirror image of the relation that we found for the number of branches.

Since dendrites serve the particular purpose of network connectivity, we investigated how their resulting branching pattern distributions compare to those of random binary trees. We have previously introduced a minimum spanning tree (MST) based growth algorithm that connects a set of target points to generate synthetic dendrites. Meeting the requirements for dendritic connectivity, such MST-based model trees guarantee short total dendritic lengths and with one parameter, the balancing factor (*bf*), also increasingly prohibit long paths along the tree towards the root to reduce conduction times in the neural circuit [46]. When the resulting synthetic dendrites are restricted to binary trees by ruling out more than two daughter branches at a branch point, MST-based model trees represent a specialised, optimally-wired distribution over the set of all possible binary trees: Since they are grown on the basis of random target points distributed within a specific area, they rely on metric information to produce the resulting topology. For this reason, the binary trees resulting from the MST process might be distributed in a highly selective manner. In order to test this, we examined two-dimensional circular morphologies that varied the two parameters *bf* and the number of target points (in order to obtain trees of SN 3–6, see Methods for details; Fig 3A). The results for such MST-based model trees were similar to the set of all possible binary trees of degree 16 and the GW random binary trees (Fig 3B–3E), indicating that the specific sample of binary trees that perform optimal wiring is not easily distinguishable from a set of random trees by the SO-based metrics we used here. The branch bifurcation ratio (Fig 3D) in MST-based model trees was also tightly scattered around a ratio of 4 (*R*^{2} = 0.9814, over all trees) in agreement with the results from the random binary Galton-Watson model trees. Overall, *bf* 0 –the pure minimum spanning tree—seemed to be a special case potentially because it represents the least symmetric tree.

We then investigated the same topological measures in six real reconstructed dendrite types (Fig 4A) and found that they, too, behaved very much like the binary tree models shown above (Fig 4B–4E). Firstly, the normalised number of segments per SO approximated 2^{−k} for SO *k* (Fig 4B) with a slope between -0.89 and -1.20 for a fit by linear regression in binary logarithmic space in the six groups of reconstructed dendrites (*R*^{2} > 0.9686 for slope fits in all groups). Secondly, the expected invariance of the SO-sorted number of branches matching a 4^{1−k} decay for SO *k* (Fig 4C) was pronounced and we found linear slopes ranging from -0.45 to -0.54 in the log10 scale (*R*^{2} > 0.996 for slope fits in all groups). Thirdly, the bifurcation ratios for reconstructions of real dendrites (Fig 4D) exhibited linear regression slopes varying between 2.23 for dentate gyrus granule cells and 3.77 for lobula plate tangential cells (LPTCs; Table 1), and the fit for all lumped data was 3.44. However, the coefficient of determination for a fit of 4 was *R*^{2} = 0.9387. Finally, the subtree sizes distributions (Fig 4E) followed the 4^{k−SN} increase with SO *k* observed previously, with linear slopes on the logarithmic average data ranging from 0.54 to 0.65 (*R*^{2} > 0.9898 for slope fits in all cases).

Taken together, these analyses show that the SO-sorted topological measures yielded very similar distributions over a wide range of possible binary tree samples including all real dendritic trees, rendering these measures unsuitable for morphological classification, cf. [34].

Dendritic trees in the brain are embedded in 3D tissue, adding metric information such as *X*, *Y* and *Z* coordinates as well as diameter values to the nodes in their tree structures that are not captured by the topologies of abstract binary trees. While any local branching statistics could exhibit interesting relationships with SO, we focused on the distributions of total dendritic length, mean segment lengths, mean branch lengths, and branch diameters, as well as basic passive electrotonic properties. The amount of total dendritic length as a function of SO followed an approximately exponential decay for all reconstructed dendrite types that we analysed, as seen by straight lines in the semi-logarithmic plots (Fig 5B). However, the slope of the decay was clearly different for dendrites of various types: The decay was slower for planar, 2D morphologies (e.g. LPTCs, Purkinje cells), for which 50–60% of the total dendritic length was SO 1 (terminal segment or branch length). By contrast, the decay was faster in 3D morphologies such as dentate gyrus granule cell dendrites and basal pyramidal dendrites with the combined terminal branch length making up more than 80% of the total wiring length. Linear regression fits on the semi-logarithmic data yielded slope values between -0.31 and -0.76 (*R*^{2} > 0.9892 in all cases).

Normalised mean segment length distributions with SO also varied pronouncedly with cell type (Fig 5C). Mean segment lengths in planar lobula plate tangential cell (LPTC) dendrites and Purkinje cells were nearly constant over all SOs. By contrast, the distributions for 3D cells featured longer mean segment lengths in the terminals, followed by a rapid decrease over the remaining SOs in dentate granule cells (linear regression fit slope -0.45, *R*^{2} = 0.9996), basal pyramidal dendrites (-0.43, *R*^{2} = 0.9894), apical pyramidal trees (-0.23, *R*^{2} = 0.9748), and motoneurons (-0.17, *R*^{2} = 0.9995). SO-sorted distributions of mean branch lengths varied even more strongly between different dendrite types (Fig 5D). Some distributions increased exponentially with SO up until a certain point; e.g. Purkinje cells and LPTCs (exponential increase until their peak in the second-to-last order with linear regression slopes in logarithmic space of 0.18 and 0.30, respectively; *R*^{2} = 0.9766 and *R*^{2} = 0.9978). Others decreased exponentially (granule cells -0.32, *R*^{2} = 0.9805, basal pyramidal dendrites -0.33, *R*^{2} = 0.9999), and yet others still were nearly constant (motoneuron dendrites and apical pyramidal dendrites).

In order to understand which features of the dendritic geometry led to the differences that we observed in SO-sorted metric measures, we designed simple MST-based model trees that reproduced the properties observed in Fig 5 (Fig 6). The MST results depended strongly on the spatial distribution of the target points that were to be optimally connected. We matched the results for SO-sorted measures seen in real dendrites by modulating basic parameters of the MST model such as hull shape, root node location, balancing factor *bf*, number of target points *pts* and the mode of target point distribution (Fig 6A, bottom row; Table 2). The slope of exponential decay observed previously for SO-sorted total dendritic length (Fig 5B) was replicated when using 2D vs 3D spanning hulls for the MST-generated trees (Fig 6B). However, the details of the distributions were not entirely captured in the 2D models (LPTC and Purkinje cell models), indicating that potentially more complex features of morphology determine the traits observed in Fig 5B. Both the nearly constant mean segment length distribution seen in LPTCs and Purkinje cells (Fig 6C) and the more complex relationships of branch length distributions there as well as in motoneurons and apical dendrites of pyramidal cells (Fig 6D) could be replicated easily by geometric adjustments to the MST models. However, granule cell and basal pyramidal dendrites with their similar distributions in Fig 5 required precise reconstruction also of the inhomogeneous quadratic target point density along the height of the cone in which the MST-based model trees were grown (Fig 6A, violet model). Even then, the model did not capture the exponential decrease of segment and branch length seen in Fig 5C and 5D very well. These findings suggest that complex cell type-specific differences in the geometry of the growth process determine the different SO-sorted distributions of metric branching statistics that we observed in Fig 5.

It is well known that terminal segments of dendritic trees exhibit the smallest diameters [8,47,48] and that this contributes to the local input resistance being highest there [47,49]. At the same time, even short branches in close proximity to the soma typically reach the smallest diameters, suggesting a centripetal increase in diameter rather than a regular taper away from the root. In the following, we investigate a potential relationship between SO and these features that are expected to be important for neuronal computation. The relationship between diameters and SO was striking and followed a similar trend in all cell types (Fig 7A). This increase of diameters with SO would be consistent with quadratic fits (*R*^{2} > 0.9956 for all morphologies), which is in agreement with our predictions that quadratic tapers optimise current transfer in dendritic trees [8,47]. Since we showed that SO correlated with subtree sizes (Fig 4E) it was not surprising that diameters also weakly correlated with subtree sizes (Fig 7B).

As mentioned above, local diameter values are influential in the processing of synaptic inputs and small diameters result in large local input resistances with strong voltage deflections for a given synaptic input. Additionally, electrotonic properties depend in part on dendritic topology [5,6,50]. We therefore also analysed simulated voltage responses to small steady-state synaptic currents (10 pA) in passive entire dendrites (see Methods) and indeed found strong relationships with SO (Fig 8A for Purkinje cells with different passive properties and Fig 8B for the different cell types and their respective passive properties). Interestingly, all cell types apart from Purkinje cells exhibited strong relationships with SO. This matches well with our previous finding that diameters in Purkinje cells were not optimised to transfer currents to the root [8] and could indicate a particular functional role of the Purkinje cell dendrite that is to date not understood.

In this study, we showed that the branching structures of real dendritic trees are indistinguishable from random binary trees when using four different Strahler order (SO) sorted topological measures. The universal relationships that we uncovered were only partly known for random binary trees and they are important for understanding general features of topological measures when used to characterise dendritic trees. By contrast, we showed that SO-sorted metric measures differ according to cell types and therefore may be useful to categorise or quantify dendritic tree structures and their respective functions.

Regardless of the method used to select samples out of the set of all binary trees, whether it was the average of all sorted or unsorted binary trees, randomly selected binary trees, or trees that guaranteed optimal wiring (MST-based model trees), we found that the relationships between topological measures and SO followed universal trends. This was also the case for all dendritic trees we studied, independently of cell type, and spanned measures from branch numbers distributions and bifurcation ratios to distributions of segment numbers and subtree sizes.

As mentioned above, it has previously been shown analytically that the mean number of branches of a given Strahler order *k* in random binary trees asymptotically tends to 4^{1−k} as the number of terminals goes to infinity [31], with a corresponding overall bifurcation ratio of 4 [32,33]. Additionally, most binary trees lie close to a bifurcation ratio of 4 [34], and it has been suggested that it is inherent to the definition of Strahler order that no binary tree can depart indefinitely far from this branch number power law [51]. In fact, Van Pelt et al. [52] have shown that there are only a few unique values that the overall branch bifurcation ratio (i.e., the averaged ratio between the number of branches of any two successive SOs) can take for the set of all possible binary trees of a given size (e.g. 7 unique values for the 98 sorted possible binary trees of degree 10, or 18 unique values for the 10,905 sorted trees of degree 16). It is therefore not surprising that we found this relation to be true in Galton-Watson (GW) random trees (Fig 2H, dashed grey line) and in the set of all possible binary trees of a given size (Fig 2E).

The universality of this distribution of branch numbers and bifurcation ratios extends to a wide range of tree-like structures in nature that most likely do not reach an exact bifurcation ratio of 4 because of their relatively small size. In our study, overall bifurcation ratios varied from 2.23–3.77 for different dendritic tree types. In river networks, they commonly range from 3–5 [22,32]. Similar bifurcation values as well as the general exponential decay relation with increasing SO have also been observed with bifurcation ratios between 3.05–3.61 in the dog bronchial system [24], 2.99–3.10 in the human pulmonary arteries [25], 3.41–4.12 in networks of conducting particles in a dielectric liquid [53], and 3–5.76 in social networks [54]. They are also present in several different species of botanical trees, with bifurcation ratios ranging from 3–5.18 [28–30]. As we demonstrated here, this general range is similar for neuronal dendritic trees. Previously, the number of branches per SO in Purkinje cell dendrites has been found to decay exponentially with a linear regression slope for log-transformed data of -0.52 for cells of SN 6 and -0.46 for cells of SN 7 [35], which are values in a range similar to what we find in the reconstructed dendrites investigated in this study. Furthermore, Binzegger et al. [36] investigated axonal branching in cat visual cortex and found it to be topologically self-similar, i.e. with a bifurcation ratio that is similar between each two consecutive orders and amounts to 3.32 for both spiny and smooth axons (*r* = 0.99).

While a significant number of publications have explored branch number distributions and bifurcation ratios in detail, the universal trend of the SO-sorted subtree size distribution is more elusive. Subtree sizes at branch points of a given SO increased exponentially with SO in a similar manner for all groups of binary trees studied here, including those of real dendrites. Subtree sizes are connected to distributions of number of branches, since the number of TPs and BPs in a tree can never be lower than the number of branches. In fact, subtree sizes appeared to mirror the distributions of number of branches with a steady 4^{k−SN} for SO *k*. We assume that those relations could be proven analytically using similar methods as in [31–33].

Surprisingly, a distribution very similar to that of SO-sorted topological subtree size (Fig 4E) was found when calculating the ratio of total dendritic length contained in the subtree of topological nodes of a given SO (S1 Fig). Such an exponential increase of local subtree weight with SO may have functional implications for electrotonic compartmentalisation and synaptic current transfer, in particular since we also found a relationship between subtree sizes and local diameters (Fig 7B).

Furthermore, the distribution of segment numbers with SO was very similar for all binary trees we studied. It has previously been found to decay in an exponential manner in Purkinje cells [35,55], and we observed that this relation holds true for many additional dendrite types. Here, on average, binary trees behaved similarly to the complete binary tree (CBT), characterised by its doubling of segments at every level where SO decreases. This is explained by the fact that any tree of a given *SN* > 2 must necessarily contain a certain number of complete subtrees in order to increase SO at branch points until the corresponding SN is reached (see Results).

The apparent universality and low variability of the SO-sorted segment and branch numbers and the branch bifurcation ratio in reconstructed dendrites can thus be explained by the fact that these statistics are universal for most binary trees and therefore of low descriptive power, cf. [34]. But it is important to note that if dendrites had followed a particular given blueprint, the distributions could have been widely different (Fig 2B and 2C). In this way, however, the universal property of SO-sorted topology in binary trees renders those distributions essentially useless for quantifying dendritic trees in a meaningful way (see also “Concluding remarks on Strahler order and neuronal dendrites” below).

The results were very different for metric measures, which exhibited strong correlations with SO that were cell type-specific in many cases. For example, we found that SO-sorted distributions of total dendritic length followed a pronounced exponential decay that seemingly depended on the dimensionality of the dendrites, since planar dendritic trees (e.g. Purkinje cell dendrites) revealed more shallow slopes than dendrites that extended into 3D space (e.g. granule cells). In line with this, SO-sorted total length in frog retinal ganglion cell (RGC) axons has been reported to decrease in a mostly exponential fashion, with 40–50% of the total length contributed by terminal segments and with a slope that closely resembles our LPTC data (black line in Fig 5B) [56]. We were able to reproduce this dimensionality effect using simple MST-based model trees based on optimal wiring principles for the different dendrites, where the slope of decay was additionally related to the *bf* parameter (see Fig 6B). The total dendritic length distribution does not denote a universal relation as seen with the number of segments or branches but is reflective of specific morphological attributes such as how planar a dendrite is. Similar observations were made for SO-sorted mean segment and branch lengths. Interestingly, we were unable to accurately replicate the exponential decay of mean segment and branch lengths with SO in basal pyramidal and granule cell dendrites using simple MST models. This might indicate that these trends are a result of the particular features of these cells, and the measures that we studied here could indeed help to better classify dendrites of such cell types.

While dendritic trees followed Horton's law of stream numbers as expected, not all of them obeyed Horton's law of stream lengths, which expresses the mean branch length of SO *k* as a direct geometric series starting with the mean branch length at SO 1 [22]. In dendrites, we found highly varying SO-sorted distributions of mean branch lengths, as opposed to the exponential increase postulated by Horton's law. For real dendritic trees that are flat and were represented with a low balancing factor in our respective MST models (e.g. LPTCs and Purkinje cells), mean branch length did appear to follow Horton’s law of stream lengths to some extent: The distribution increased exponentially with SO until it peaked in the second-to-last order, i.e. close to the root. Similarly, Hollingworth and Berry [35] observed an exponential increase in the mean lengths of branches of successive SO in rat Purkinje dendrites, and an increase was also reported by Yen et al. in frog RGC axons [56]. For granule cell dendrites and basal pyramidal dendrites, however, the distribution exhibited an exponential decrease. Since river networks are planar, it is conceivable that Horton's law of stream lengths applies only to 2D trees. Meanwhile, motoneurons and apical pyramidal dendrites appeared to fall somewhere in between those extremes and did not exhibit clear trends.

The most striking correlation was found between local branch diameters and SO. While the general presence of a correlation may be reasonably expected in a centripetal ordering system since diameter has been well established to taper towards the terminals of neurons, there seems to be no precedent of an investigation of SO-sorted branch diameter in neurons, apart from a report that diameter increases with SO in frog RGC axons [56]. Because diameter values strongly determine electrotonic properties of neurons, we also studied the consequences for synaptic integration and found that simulated local voltage responses to synaptic currents correlated strongly with SO. Interestingly, similar correlations between diameters and SO have been observed in other tree structures in nature. Branch diameters appear to increase exponentially with SO in the bronchial tree of dogs [24] and in botanical trees [29,30]. Additionally, topological subtree size was strongly correlated with SO and to a lesser extent with diameter, showing a functional relevance of SO.

Potentially, the variations in SO-sorted statistics could also reflect differences in the growth process: While some neurons such as granule cells could “blossom” like flowers, elongating mainly the branches close to the soma, others such as Purkinje cells could mostly develop by growing new terminal branches and densifying the fixed space they occupy. In line with this, Van Pelt et al. [43] demonstrated that the geometry of guinea pig Purkinje cells can be replicated using a dendritic growth model that favours branching at distal locations.

SO has advantages as well as disadvantages when compared to other branch ordering systems. Uylings et al. [13] reviewed different ordering methods for dendrite branching and concluded that the Strahler method should preferentially be used when studying branching patterns that are very asymmetric, or when studying tree structures with a very extensive branching pattern such as Purkinje cells, because the tree's Strahler number SN is not as high as the maximum branch order in the centrifugal system. A caveat of the method is its sensitivity especially to the addition or loss of terminal segments, as these can alter the order of many branches in the tree. It has furthermore been suggested that centripetal ordering schemes are superior when examining branch probabilities in distal regions of the dendrite, but that centrifugal ordering of branches is useful for branching structures near the soma or root of the tree [16].

The main usage of Strahler ordering applied to neuronal morphology in the literature so far is concerned with the distribution of the SO-sorted number of branches. It has been used for classification of branching complexity of Drosophila da neurons, as mentioned in the Introduction (e.g. [37,38,40–42]), and various other studies used that distribution to ascertain differences in “branching complexity” in various cell types, mostly aforementioned da neurons or Purkinje cells, between different conditions such as wild-type vs. knock-out cells (e.g. [38,40,57–60]). In all of these studies, the authors used the actual number of branches, which would have varied compared to the normalised number. However, since the normalised branch numbers distribution is on average very similar in different groups of trees (dendritic or otherwise), it is quite redundant to compare the number of branches of different orders between cells because the slope of the curve is not likely to differ very much, as discussed above. In fact, in most of those studies, it would have been enough to compare just the number of terminal segments without using any branch ordering system (or, perhaps, with the additional information of the SN): Where actual numbers were given in various publications [38,57–59,61,62], we plotted the number of branches per SO and saw that they did indeed follow the characteristic exponential decay that was close to a 4^{1-k} slope for SO *k* if values were normalised to the total number of branches. In most of the publications surveyed, significant differences in branch numbers appeared only in SO 1, i.e. the number of terminals. We argue that using SO only in this way is limiting and redundant, and that more interesting results might emerge if Strahler ordering were used more often in conjunction with metric measures such as total length per SO (only seen in one publication pertaining to axonal morphology; [56]). Some studies, e.g. [60], did investigate total length between two groups of cells, but there may be benefits to looking at the SO-sorted total length distribution as well as it might offer information regarding the dendritic locations where the length changes most significantly. Further metric SO-sorted measures such as mean branch and segment length might also be of use to quantify differences in morphology and branching complexity.

Our study demonstrates that one has to take great care when interpreting the topology of trees using SO because of the many universal features that make such quantification potentially useless. This stresses the importance of using computational models to better interpret the results from quantitative measures that are commonly used in neuroscience. Finally, we observe that SO can be a useful tool to classify tree structures and their functional relevance when used in conjunction with adequate metric information.

All analyses were performed using the TREES toolbox, an open-source software package for MATLAB (Mathworks, Natick, MA, USA), which provides tools for analysing and generating neuronal morphologies [46,63] (www.treestoolbox.org). We used functions of the TREES toolbox as well as additional custom MATLAB code to generate model dendritic trees, to pre-process reconstructed real dendrites, and to determine and visualise the various Strahler order-sorted branching statistics. A function *strahler_tree* to calculate Strahler order (SO) values for each node in a tree was implemented and will be made available in the TREES toolbox package.

In order to obtain the set of all possible binary trees of a given maximal size, we calculated all possible instances using a formal language defined in the following way: We started with the string ‘BTT’ representing a binary tree on 3 nodes, where ‘B’ stands for branch point and is followed by two subtrees and ‘T’ is a termination point. Recursively, all ‘T’ elements were then replaced by new branches ‘BTT’, one by one resulting in as many next generation trees with each two additional nodes. After calculating all trees of a given generation, all exact duplicates were removed. This procedure was then continued until the target tree size was obtained. Notice that the number of binary trees of a given size grows exponentially with the number of nodes (yielding 1, 2, 5, 14, 42, 132, 429, 1,430, etc. as the number of trees in each generation). For example there exist 9,694,845 binary trees on 31 nodes (16 ‘T’s), which was at the limit of the computing power available to us. We chose the set of all possible binary trees of degree 16 because we wanted to investigate a set that would include a complete binary tree. See Fig 2A for resulting sample binary trees. Note though that many of these trees were equivalent in terms of the topological structure since permutations of subtrees at every branch point are actually equivalent (for example a tree ‘BBTTT’ is equivalent to ‘BTBTT’; see also green box in Fig 2A for two topologically equivalent binary trees). Apart from the unsorted set of trees described above (i.e., the set which allows multiple topologically equivalent binary trees with differing ‘B’-and-‘T’ strings), we therefore calculated the reduced (sorted) subset that contained only topologically unique trees. To determine this sorted subset, the *sort_tree* function from the TREES toolbox was used to arrange all trees of a newly generated generation such that heavy subtrees would always be represented first in the ‘B’-and-‘T’ strings, thus enabling us to exclude duplicates. A few remaining duplicates were identified by an exhaustive search comparing all permutations of all subtrees at each branch point in the remaining trees. In this way, we obtained all 10,905 [52,64] sorted binary trees on 31 nodes (16 ‘T’s). Finally, tree structures were generated from the resulting ‘B’-and-‘T’ strings using the TREES toolbox function *BCT_tree*. The resulting trees were then analysed further using the TREES toolbox.

We generated random binary trees by using a critical Galton-Watson random branching process [44]. This growth process starts with one terminal node at generation 1. For each successive generation, each terminal node of the previous generation is treated in one of the following two ways: (1) with probability *P*_{st}, growth stops there; (2) with probability *P*_{br}, the node becomes a branch point, and edges are added with two new terminal nodes (Fig 2F). Terminal growth was previously found to be compatible with the observed topologies in real dendrites [65]. A Galton-Watson process is called critical if *P*_{st} = 0.5 and *P*_{br} = 0.5. We used custom MATLAB code to generate 10,000 random topological trees, terminating each growth process in the cases when the tree size reached 800 nodes.

Spatially embedded minimum spanning trees (MST) take into account optimal wiring considerations that are important for real neurons. MST models (here we use the *MST_tree* function from the TREES toolbox) were previously used successfully to model a large palette of dendrites [7,46,47,66–68] and axons [69]. These models generate tree structures that connect a set of target nodes to minimise the total dendrite length as well as the cost for short paths from the target nodes to the root along the tree. Target nodes are given to the algorithm and may be chosen to be distributed inside specified two- or three-dimensional areas according to certain rules (e.g. uniform distribution when coordinates for target nodes are generated as uniformly distributed random numbers on a specified interval), and will end up being the branch points, termination points, and continuation points of the tree. The cost for short paths from target nodes to the root is weighted with the balancing factor (*bf*), with typical values between 0 and 0.9 in real dendrites. When *bf* is low, the total wiring cost is kept to a minimum and the resulting tree approaches a minimum spanning tree. When *bf* is high, direct paths from target points to the root are given more importance than the pure conservation of wiring.

To study topological measures in MST models (Fig 3), we uniformly distributed a number of random target points (30, 150, 500 or 1,200, in order to obtain as many trees as possible for SN 3, 4, 5, and 6, respectively) in a two-dimensional circular area of 10,000 μm^{2} with a root node located in the centre. 1,000 MST-based model trees were generated for each combination of *bf* (between 0 and 0.9, in steps of 0.1) and target point number. Here, the *MST_tree* function was constrained to bifurcations (option *‘-b’*), enforcing the generation of binary trees. The resulting trees were repaired using the *repair_tree* function, which assigns a number to every node in the tree according to a predefined standard, and all nodes from the root to the first branch point were deleted, forcing every tree to start with a branch point to best match the concept of binary trees. If nodes were deleted in the process, the *repair_tree* function was applied once again to update node indices accordingly.

In order to investigate the source of the cell type-specific differences in SO-sorted metric measures of real dendrites (Fig 5), we modelled the SO-sorted distributions by finding the simplest MST model parameters necessary to approximate those distributions (Fig 6). The initial model conditions were similar to the model described above with simple two- or three-dimensional (depending on the real cells) round spanning fields and a root node located in its centre. The complexity of the hull, the root location and the statistics of the target point distributions were adjusted manually in a trial-and-error procedure in an attempt to best reproduce—with as few modifications as possible—all SO-sorted branching statistics as seen in the real dendrites. In all cases, the balancing factor and number of target points were varied to best match the real dendrite statistics and SN values. Specific parameters for each of the five models are described in Table 2 and Fig 6A (bottom row). Binary synthetic trees were obtained in a similar manner as described above. 100 synthetic trees were generated for each of the models.

Reconstructions of real dendritic morphologies (examples see Fig 4A) were taken from the *NeuroMorpho*.*Org* database (accessed on 26/11/2015) with the exception of the blowfly LPTCs [66], which were taken directly from the set of sample cells in the TREES toolbox (see Table 3 for details). A preselection of neurons was conducted according to metadata filtering on the *NeuroMorpho*.*Org* website (Table 4). In brief, we restricted the dataset to neurons with complete dendrites that were part of the control conditions in any given experiment. All preselected neurons were manually inspected in three-dimensional view. Since the metadata is self-reported by the contributing labs, the quality of “complete” reconstructions may differ from dataset to dataset. Many reconstructions exhibited sudden step-like jumps in depth, a common problem in three-dimensional reconstructions. We excluded such dendrite reconstructions with insufficient quality by visual inspection but no objective criteria to appropriately quantify the quality of the tracings were used. Reconstructions of typically three-dimensional neurons (e.g. granule cells, pyramidal cells) that did not or did only slightly extend into the third dimension were also excluded from the analysis. The number of suitable cells left for each cell type can be found in Table 3. Despite the fact that our *NeuroMorpho*.*Org* metasearch required diameter information, we found that some of the remaining cells had poorly reconstructed diameter values (i.e., nearly constant diameter for all nodes). These cells were still used for most analyses in this study but were excluded from the SO-sorted branch diameter computation, which was therefore performed on a lesser number of dendritic trees per cell type (see Table 3).

We then deleted all cell regions that were not labelled “dendrite” (i.e., axon and soma regions). Deletion of a single cell's soma resulted in multiple dendritic trees (Table 3) if there were several primary dendrites emerging from the soma. We pooled data for all dendritic trees of a cell type for analysis, with the exception of pyramidal cells, where we analysed apical and basal trees as separate groups due to their very different morphologies. All dendritic trees were then repaired with the TREES toolbox function *repair_tree*, replacing branch points with more than two daughters with multiple consecutive bifurcations to restrict ourselves to binary trees (no multifurcations allowed). Furthermore, we identified the first branch point following the root (if it was not the root node already) and deleted all previous nodes. A deletion was followed by another application of the *repair_tree* function. This deletion step was performed to ensure that all analysed dendritic trees were binary trees that started with a branch point. However, it must be noted that this is an alteration of the original morphology and leads to exclusion of data concerning the length and presence of small branches of higher Strahler orders (e.g. dendrites that emerge from the soma as a single branch before they first bifurcate).

Our morphometric analysis distinguishes between dendrite segments and branches. A segment is defined as a piece of dendrite connecting two consecutive topological nodes in the tree (BP—BP or BP—TP). Consecutive segments (moving from terminals towards the root) of the same SO form one branch of that order. A branch may consist of only one segment (e.g., all terminal segments are also terminal branches), but often consists of multiple segments, especially for higher orders (Fig 1B, the tree contains three SO 2 segments, but only two SO 2 branches, one of which is composed of two segments). We additionally distinguish between node and segment SO to determine the highest order in a tree, its Strahler number (SN). We call the highest SO assigned to a segment in a tree its segment Strahler number. The highest SO of any node in a tree is its node Strahler number. In most cases, these two are interchangeable. However, when two segments of the same order meet at the root node of the tree, they are different (e.g. in Fig 1A: segment SN = 2, but node SN = 3). For node-based measures (subtree size, branch diameter, local voltage response), we forced functions to consider the root node’s SO as equal to the tree’s segment SN in the few cases where node and segment SN differed. This step did not significantly alter the resulting SO-sorted measures but was performed to ensure that all trees sharing a common segment SN would also display a common number of data points (from SO 1 to the order corresponding to the segment SN) that were averaged for visualisation in the figures.

The **topological measures** we analysed are the number of segments, number of branches, branch bifurcation ratio, and the size of topological subtrees. These measures do not require any metric information and therefore they enable us to compare these distributions across not only reconstructed neurons and synthetic MST morphologies, but also Galton-Watson random branching model trees as well as the set of all possible binary trees of degree 16. Except for Fig 2B and 2C, SO-sorted distributions of number of segments and branches were normalised (to the total number of segments and branches in the tree, respectively) to be able to compare distributions of trees of different sizes. The branch bifurcation ratio was obtained by visualising the number of branches of any SO *k* with the number of branches at SO *k* + 1. When bifurcation ratios between all consecutive orders in a tree are similar, the tree is said to be topologically self-similar. Hence, the bifurcation ratio provides information about the fractal degree of a structure. We calculated overall bifurcation ratios by performing a linear regression on the number of branches of SO *k* against the number of branches of SO *k* +1 for all trees of a dendrite type. Topological subtree sizes counting the number of BPs and TPs for any BP in the tree should intuitively increase for centripetal branch ordering schemes such as SO. Topological subtree sizes were also normalised (to the total number of topological nodes in the tree) and used for Figs Figs2,2, ,33 and and44.

The following **metric measures** were determined as a function of SO for reconstructions of real neurons and for their respective MST models: total dendritic length, mean branch length, and mean segment length. Also, branch diameters were investigated in the reconstructed morphologies where diameter values were available. Normalised total lengths per SO express the proportion of total dendritic length in each SO. Normalised mean branch and segment lengths per SO were obtained by dividing the total length value for a given SO by the total number of branches or segments respectively for that given SO value. These values were further divided by the sum of the average branch or segment length values of all SO (integral under the curve is then 1 in all cases) to keep the resulting distributions in the same range. Mean branch diameters per SO were calculated by taking the sum of the diameters of all nodes with a given SO and dividing that by the number of nodes of that given SO. Normalised relative values between 0 and 1 were obtained by setting the lowest mean diameter value for any order (this was always SO 1) to 0 and the highest mean diameter value (this was always the order corresponding to the tree’s SN) to 1.

**Electrotonic measures** in passive dendritic trees were calculated on a slightly differently pre-processed dataset because we took values for *R*_{i} and *R*_{m} from the literature that described whole cells instead of dendritic trees that were once part of a bigger dendritic field. We therefore took all neurons with reasonable diameter information (see Table 3, “Number, with diameter”), removed soma and axon regions in such a way that the dendrite would stay connected and not result in multiple dendritic trees, and repaired the dendrite with the *repair_tree* function, which may result in a small change of morphology and topology.

To simulate the average local voltage response to an injection of 10 pA into a topological node of SO *k*, the dendritic tree’s electrotonic signature given its specific membrane conductance *G*_{m} = 1/*R*_{m} and specific internal resistivity *R*_{i} was determined using the *sse_tree* function. *R*_{m} and *R*_{i} for the different cell types were taken from the literature [70–73] for Fig 8B. The diagonal of the resulting matrix contained the local input resistances in MΩ of every node in the tree. These values were averaged between all topological nodes that shared the same SO. In order to simulate the local voltage response to a small steady-state synaptic current injection of 10 pA, the values were divided by 100 and the unit became mV. For normalisation, all values were divided by the average value for the terminal nodes (SO 1). Three motoneurons (‘Alvarez-Control-Cell-1.CNG’, ‘Alvarez-Control-Cell-2.CNG’, and ‘Alvarez-Control-Cell-3.CNG’) had to be excluded from this simulation because of their high number of nodes.

All figures of SO-sorted distributions show averages of trees that share the same segment SN. In this way, patterns in the data are not skewed by averaging over model trees or real dendrites in a sample that have different SN values. For reconstructed morphologies, we chose the most abundant SN value for each cell type for visualisation, hence only the subset of the data where all trees share that SN value was plotted (e.g. see Fig 4B: for granule cells (in red), there were 59 dendritic trees analysed, but the graph shows only the average of those 53 trees in the subset of all granule cell dendritic trees that had segment SN 3).

Average (lines with markers) and standard deviations (shaded areas) of normalised subtree lengths for all topological nodes as a function of SO in real dendritic trees. Colours indicate cell types (for legend see Fig 4A). Values were normalised by expressing them as a ratio of total dendritic length. Grey dashed lines same as in Fig 4E.

(TIF)

Click here for additional data file.^{(362K, tif)}

We are grateful to A. D. Bird and P. Jedlicka for helpful discussions.

This work was funded by the German Federal Ministry of Education and Research grant 01GQ1406 https://www.bmbf.de/en/index.html. The funders had no role in study design, data collection and analysis, decision to publish, or preparation of the manuscript.

Data Availability

Data are available at www.neuromorpho.org. Table 3 details which archives the cells we analysed were taken from and Table 4 provides the exact filtering steps of our NeuroMorpho.Org database metadata search.

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