Research ArticleResearch Article: New Research, Integrative Systems

Learning an Efficient Hippocampal Place Map from Entorhinal Inputs Using Non-Negative Sparse Coding

Yanbo Lian and Anthony N. Burkitt
eNeuro 23 June 2021, 8 (4) ENEURO.0557-20.2021; DOI: https://doi.org/10.1523/ENEURO.0557-20.2021

Abstract

Cells in the entorhinal cortex (EC) contain rich spatial information and project strongly to the hippocampus where a cognitive map is supposedly created. These cells range from cells with structured spatial selectivity, such as grid cells in the medial EC (MEC) that are selective to an array of spatial locations that form a hexagonal grid, to weakly spatial cells, such as non-grid cells in the MEC and lateral EC (LEC) that contain spatial information but have no structured spatial selectivity. However, in a small environment, place cells in the hippocampus are generally selective to a single location of the environment, while granule cells in the dentate gyrus of the hippocampus have multiple discrete firing locations but lack spatial periodicity. Given the anatomic connection from the EC to the hippocampus, how the hippocampus retrieves information from upstream EC remains unclear. Here, we propose a unified learning model that can describe the spatial tuning properties of both hippocampal place cells and dentate gyrus granule cells based on non-negative sparse coding from EC inputs. Sparse coding plays an important role in many cortical areas and is proposed here to have a key role in the hippocampus. Our results show that the hexagonal patterns of MEC grid cells with various orientations, grid spacings and phases are necessary for the model to learn different place cells that efficiently tile the entire spatial environment. However, if there is a lack of diversity in any grid parameters or a lack of hippocampal cells in the network, this will lead to the emergence of hippocampal cells that have multiple firing locations. More surprisingly, the model can also learn hippocampal place cells even when weakly spatial cells, instead of grid cells, are used as the input to the hippocampus. This work suggests that sparse coding may be one of the underlying organizing principles for the navigational system of the brain.

Significance Statement

The brain can perform extremely complex spatial navigation tasks, but how it does this remains unclear. Here, we show that the principle of sparse coding can be used to learn the hippocampal place map in a way that efficiently tiles the entire spatial environment using inputs from the entorhinal cortex (EC), namely either grid cells or weakly spatial cells. This demonstrates that the hippocampus can retrieve spatial information from the EC using an efficient representation and that sparse coding may be one of the underlying principles of the navigational system of the brain.

Introduction

Since the Nobel-prize-winning discovery of place cells in the hippocampus (O’Keefe and Dostrovsky, 1971; O’Keefe, 1976) and grid cells in the medial entorhinal cortex (MEC; Hafting et al., 2005; Rowland et al., 2016), brain regions involved in spatial awareness and navigation have attracted much attention from both experimental and computational neuroscientists.

In the hippocampus, place cells generally have a single specific firing location in a small environment (O’Keefe and Dostrovsky, 1971; Park et al., 2011), and neighboring cells have firing fields at different locations, such that the local cell population in the hippocampus can represent the whole spatial environment (O’Keefe, 1976). In contrast, granule cells in the dentate gyrus of the hippocampal formation have multiple discrete firing locations without spatial periodicity (Jung and McNaughton, 1993; Leutgeb et al., 2007).

However, in the EC, cells that carry spatial information range from cells with structured selectivity to weakly spatial cells that have spatial information but no structured selectivity. For example, MEC grid cells have hexagonal firing fields that cover the entire environment (Hafting et al., 2005). The hexagonal grid is characterized by three grid parameters: spacing, orientation, and phase (see Fig. 1A–C). Grid cells are organized into discrete modules according to their spacings because the progression in grid spacing along the dorsal-ventral axis is geometric, with ratio around 1.42 (Stensola et al., 2012). Also, grid cells in each module have similar orientations but random phases (Stensola et al., 2012). Nevertheless, there are also other cells such as weakly-tuned cells (Zhang et al., 2013) in the MEC and Diehl et al. (2017) found that, apart from the well-characterized spatial cells in the MEC, nearly all of the remaining 2/3 MEC cells have spatial selectivity. In addition, cells in the lateral EC (LEC) also display weak spatial selectivity (Hargreaves et al., 2005; Yoganarasimha et al., 2011).

Followed by the experimental studies that indicate that EC inputs, including both grid cells and weakly spatial cells, are the principal cortical input to the hippocampus (Steward and Scoville, 1976; Tamamaki and Nojyo, 1993; Leutgeb et al., 2007; Van Strien et al., 2009; Zhang et al., 2013), various models have been proposed to explain the emergence of place cells based on the feedforward connection from grid cells, from mathematical models that have no learning (Solstad et al., 2006; de Almeida et al., 2009) to models with plasticity (Rolls et al., 2006; Franzius et al., 2007a,b; Savelli and Knierim, 2010; Neher et al., 2017).

Among these learning models, Rolls et al. (2006) used a competitive learning procedure. However, only ∼10% of modelled hippocampal cells had a single firing location. Furthermore, the competition was introduced by manually setting the population activation to a small specified value. Similarly, Franzius et al. (2007a,b) applied independent component analysis (Hyvarinen, 1999) to learn place cells. However, the examples of learned place cells are mostly located at the border (Franzius et al., 2007a, their Fig 3C; Franzius et al., 2007b, their Fig. 1G). Additionally, the weights connecting grid and place cells can be positive or negative, and the place cell responses were manually shifted by a constant term to be kept non-negative, which puts into question the biological realization of the model. Furthermore, previous models do not investigate how well the learned hippocampal place map represents the entire spatial environment and how the weakly spatial cells in the EC can contribute to the formation of the place map.

Sparse coding (Olshausen and Field, 1996) provides a compelling explanation of many experimental findings of brain network structures. One particular variant, non-negative sparse coding (Hoyer, 2003), has recently been shown to account for a wide range of neuronal responses in brain areas (for review, see Beyeler et al., 2019). However, whether sparse coding can learn the hippocampal place map has not previously been investigated.

Here, we apply sparse coding with non-negative constraint, where neuronal responses and connection weights are restricted to be non-negative, to building a learning model of hippocampal cells using EC inputs. Our results show that, when grid cells are used as the entorhinal input, single-location hippocampal place cells that tile the entire environment can be learned, given the sufficient diversity in grid parameters. However, if there is a lack of diversity in any grid parameters, the learning of the hippocampal place cells is impeded; instead, more hippocampal cells with multiple firing locations are learned. Furthermore, a lower number of hippocampal cells in the network also results in learning hippocampal cells with multiple firing locations. Additionally, the competition generated by sparse coding naturally provides a global inhibition such that learned hippocampal place cells display single firing fields, suggesting that the proposed model can be implemented by biologically based neural mechanisms and circuits. Also, the learned hippocampal place cells tile the entire spatial environment efficiently by a hexagonal lattice, which is consistent with a recent study of conceptual state spaces (Mok and Love, 2019). Moreover, the model can still learn hippocampal place cells even when the grid inputs are replaced by the responses of weakly spatial cells, suggesting that sparse coding can retrieve information from EC inputs efficiently to form a cognitive map as long as there is sufficient spatial information in the upstream input. This also provides a plausible explanation of many experimental studies that suggest the emergence and maintenance of place cells does not require grid cells (Langston et al., 2010; Wills et al., 2010; Koenig et al., 2011; Brandon et al., 2014; Hales et al., 2014; Schlesiger et al., 2015).

Materials and Methods

The environment

The 2D spatial environment used in this study is a 1 × 1 m square box. A 32 × 32 grid with 1024 points is used to represent the entire environment. Therefore, a 1024 × 1 vector, denoted by r, with only one non-zero element of value 1 can be used to represent the spatial location of a virtual rat.

Model of entorhinal input

Since the environment is represented by a 32 × 32 grid, a 1024 × 1 vector, denoted by ei , can be used to represent the spatial firing field of the modelled entorhinal cell i over the entire environment. For a given position r in the environment, the response of modelled entorhinal cell i is simply eiTr . Next, we show how the entorhinal inputs, grid cells or weakly spatial cells, are modelled to provide information for modelled hippocampal cells.

Grid cells described by a mathematical model

The hexagonal firing fields of grid cells can be represented by the sum of three sinusoidal gratings (Solstad et al., 2006; Kropff and Treves, 2008; de Almeida et al., 2009), as described by E(r→)=23(13∑j=13cos(4π3λu→j·(r→−r→0)) + 12), (1)where E(r→) is the grid cell response at the spatial location r→=(x,y) , λ is the grid spacing, θ is the grid orientation, r→0=(x0,y0) represents the grid phase, and u→j=(cos(2πj/3+θ)),sin(2πj/3+θ)) is the unit vector with direction 2πj/3+θ . E(·) , described in Equation 1, is normalized to have a maximal value of 1 and minimum of 0. Because of the periodicity of the hexagonal pattern, the grid orientation, θ, lies in the interval of [0,π/3) , and the phases in both x- and y-axes are smaller than the grid spacing, i.e., 0≤x0,y0<λ .

Since grid cells have different spacings, orientations and phases, Equation 1 is used to generate diverse grid cells. The value of the grid spacing, λ, ranges in value from 28 cm (Hafting et al., 2005; Solstad et al., 2006) and increases by a geometric ratio 1.42 that is consistent with experimental results (Stensola et al., 2012) and the optimal grid scale derived by a mathematical study (Wei et al., 2015). For example, if there are Nλ different grid spacings, the spacings will be 28 cm, 28 × 1.42 = 39.76 cm, ⋯, and 28×1.42Nλ−1 cm. For each grid spacing, different values of grid orientation, θ, are uniformly taken from the interval [0 60°). For example, if there are three different grid orientations, the values will be 0°, 20°, and 40°. The number of different orientations for each grid spacing is denoted as Nθ. Furthermore, it is assumed here that there are Nx and Ny phases along x-axis and y-axis for each specific grid spacing and orientation. Similar to grid orientation, the value of the phase is taken uniformly from [0,λ) . For example, if there are two different phases along the x-axis, they will have the values x0=0 and λ/2 . The resulting total number of modelled entorhinal cells (grid cells), denoted as Ne , will be the product of numbers of spacings, orientations and phases: Ne=Nλ Nθ Nx Ny. (2)

Some examples of grid cells described by Equation 1 are shown in Figure 1D. These grid cells have diverse grid spacings, orientations and phases.

Figure 1.
Figure 1.

Grid parameters and example grid cells defined by Equation 1. A–C, Schematic plots that illustrate grid spacing, orientation, and phase (re-generated from Moser et al., 2014). D, Grid cells generated by Equation 1 that have different grid spacings, orientations and phases. Each block represents the hexagonal firing field of a grid cell in a 1 × 1 m environment. Values in each block are normalized to [0 1] in this plot.

The number of different grid parameters (Nλ, Nθ, Nx, and Ny) of grid cells defined above are assigned to different values to investigate the effect of the diversity of grid cells on the formation of place cells.

Although the firing fields of grid cells can be represented by the sum of three sinusoidal gratings (Eq. 1) given grid spacings, orientations, and phases and are used in many studies (Solstad et al., 2006; Kropff and Treves, 2008; de Almeida et al., 2009), this mathematical model cannot capture the variability in individual grid fields of the grid cells as reported by Ismakov et al. (2017). Therefore, in this article, we also adopt a more realistic model of grid cells that characterizes grid fields individually and embraces the variability between individual grid fields. This model of grid cells is used to investigate the robustness of our results obtained by using the mathematical model of grid cells (Eq. 1).

Grid cells described by a more realistic model

MEC grid cells have different spacings, orientations and phases, and are separated into discrete modules where grid cells are anatomically adjacent and have similar grid spacings, which is supported by experimental evidence (Hafting et al., 2005; Stensola et al., 2012). Moreover, grid cells in the same spacing module tend to have similar orientations and random phases (Stensola et al., 2012). Because of these properties of grid cells, we model grid cells using a similar approach in a previous study (Neher et al., 2017) as described below.

Values of the grid spacing in each module are randomly sampled from normal distributions: there are four discrete modules for grid spacings (λ) with mean of 38.8, 48.4, 65, and 98.4 cm, and a same SD of 8 cm. For grid orientation (θ), since grid cells in the same spacing module tend to have similar orientations, grid cells in the four discrete modules also have mean orientations 15°, 30°, 45°, and 0°, and a common SD of 3°. Because grid phases, (x0, y0), are random in each module, grid phase is randomly sampled from a uniform distribution between 0 and λ. Stensola et al. (2012) showed that 87% of grid cells belong to the two modules with small spacings based on their recordings. Therefore, we have 43.5%, 43.5%, 6.5%, and 6.5% of grid cells in the modules with mean spacings 38.8, 48.4, 65, and 98.4 cm, respectively (unless otherwise noted).

The firing field of each grid cell is modelled as the sum of multiple grid fields whose centers are located at the vertices of the hexagonal grid. The grid field at vertex (xv, yv) is described by a function with the following form (Neher et al., 2017) Qv(x,y)=γve−ln(5)(x−xv)2 + (y−yv)2σ2, (3)where γv is the amplitude, σ determines the radius of the grid field, and the response will be γv/5 at a distance σ away from the center. σ is determined by the grid spacing, λ, with σ = 0.32 λ (Neher et al., 2017). To incorporate the variability of individual grid fields, the amplitude of the grid field at every vertex of the hexagonal pattern, γv, is chosen from a normal distribution with mean 1 and SD 0.1 (Neher et al., 2017). The locations of all vertices of the hexagonal grid are determined by grid spacing, λ, grid orientation, θ, and grid phase, (x0, y0).

After the mathematical model of grid cells are used as the input, the more realistic model of grid cells is then used to verify the results and investigate the robustness of the model.

Weakly spatial cells

Apart from grid cells in the MEC, other cells such as weakly-tuned cells (Zhang et al., 2013) and non-grid cells (Diehl et al., 2017) in the MEC, and LEC cells that contains spatial information (Hargreaves et al., 2005; Yoganarasimha et al., 2011), can also contribute to the formation of hippocampal place cells. In this article, we model these cells as weakly spatial cells. The firing field of weakly spatial cells is generated in the simulation by first assigning a random activation, sampled from a uniform distribution between 0 and 1, to each location, then smoothing the map with a Gaussian kernel with SD 6 cm, and normalizing the map such that the values are between 0 and 1 (Neher et al., 2017).

Weakly spatial cells are used as another type of entorhinal input to investigate how they contribute to the formation of the hippocampal place map.

Sparse coding with non-negative constraint

Sparse coding was originally proposed by Olshausen and Field (1996) to demonstrate that simple cells in the primary visual cortex represent their sensory input using an efficient neuronal representation, namely that their firing rates in response to natural images tend to be sparse (rarely attain large values) and statistically independent. In addition, sparse coding finds a reconstruction of the sensory input through a linear representation of features with minimal error, which can be understood as minimizing the following cost function G(A,s)=12||I−As||22 + β∑iQ(si), (4)where the matrix I is the input, columns of A are basis vectors (universal features) from which any input can be constructed from a weighted sum, the vector s represents the neural responses and each element, si, is the coefficient for the corresponding basis vector, the function Q(·) is a function that penalizes high activity of model units, and β is a sparsity constant that scales the penalty function (Olshausen and Field, 1996, 1997). Implemented in a neural network, A represents the connection between layers and s represents the neuronal responses. The term As in Equation 4 represents the model reconstruction of the input, so this cost function represents the sum of squared reconstruction error and response penalty. Therefore, the model finds a sparse representation for the input by solving this minimization problem. By taking the partial derivatives of Equation 4 in terms of the elements of A and s, and then applying gradient descent, the dynamic equation and learning rule are given by s.=AT(I−As)−βQ′(s), (5)and ΔA∝〈(I−As)sT〉, (6)respectively. Q′(·) is the derivative of Q(·) , the dot notation represents differentiation with regard to time, and 〈·〉 is the average operation.

One common choice of Q(·) is the l1 norm, i.e., the absolute value function. In this case, Rozell et al. (2008) shows that the dynamics in Equation 5 can be implemented via thresholding and local competition in neural circuits, as described by τu.=−u+ATI−(ATA−1)ss={max(u−β,0),ifu>0min(u+β,0),ifu<0, (7)where 1 is the identity matrix, τ is the time constant, u can be interpreted as the membrane potential, and β is the positive sparsity constant in Equations 4, 5 and becomes the threshold of the thresholding function in Equation 7. In this article, we will use Equation 7 (Rozell et al., 2008) to implement sparse coding and use the learning rule in Equation 6 to update the entorhinal-hippocampal connection A.

Non-negative sparse coding is simply sparse coding with non-negative constraint, i.e., the connection weights A and model responses s are restricted to non-negative values in the cost function Equation 4. Note that, when β in Equation 4 is set to zero, the cost function of non-negative sparse coding reduces to the cost function of non-negative matrix factorization (Lee and Seung, 1999).

Structure of the model

In this study, a two-layer network is proposed to model the activities of entorhinal cells (first layer) and hippocampal cells (second layer), respectively. Given a spatial location in the environment, modelled entorhinal cells respond according to their firing fields. Modelled entorhinal cell responses then feed into modelled hippocampal cells and the entorhinal-hippocampal network implements a sparse coding model with non-negative constraint. The model structure is shown in Figure 2.

Figure 2.
Figure 2.

Graphical representation of the model. Red arrows represent non-negative connection. Notation is defined in the main text. E represents the firing fields of modelled entorhinal cells, and A represents the connection between the EC and hippocampus. r represents the spatial location, s_e represents the response of entorhinal cells, and s_h represents the responses of hippocampal cells.

Denote E as a 1024×Ne matrix that represents the firing fields for Ne modelled entorhinal cells in the network, i.e., each column of E, ei (i=1, 2,....,Ne ), is a 1024 × 1 vector that represents the firing field of modelled entorhinal cell i. For a spatial location r in the environment, modelled entorhinal cell responses (firing rates), se , are given by se=ETr . Modelled hippocampal cell responses (firing rates), sh , are computed by a sparse coding model for the entorhinal-hippocampal network with non-negative connection A. Assume there are Nh modelled hippocampal cells in the network. Then A is a Ne×Nh matrix and sh is a Nh×1 vector. Denote uh as a Nh×1 vector that represents membrane potentials of modelled hippocampal cells. Based on Equation 7, the dynamics of the model is given by se=ETrτuh.=−uh + ATse−Wshsh=max(uh−β,0), (8)where τ is the time constant for modelled hippocampal cells, β is the threshold of the rectifying function of firing rates, and W can be interpreted as the matrix of recurrent connection between modelled hippocampal cells determined by W=ATA−1 , where 1 is a Nh×Nh identity matrix. The dynamics of modelled hippocampal cells described in Equation 8 is derived from the local competitive algorithm (LCA) proposed by Rozell et al. (2008) that solves sparse coding efficiently. However, modelled hippocampal cell responses, sh , and connection matrix, A, are taken to be non-negative in this study.

The code to run the model is available at https://github.com/lianyunke/Learning-Efficient-Hippocampal-Place-Map-from-Entorhinal-Inputs-Using-Nonnegative-Sparse-Coding.

Learning rule

The learning rule for updating the connection strength matrix A is similar to that in previous studies of sparse coding (Olshausen and Field, 1997; Zhu and Rozell, 2013), as given by ΔA=η(se−Ash)shT, (9)where η is the learning rate. Elements of A are kept non-negative during training, i.e., the element will be set to 0 if it becomes negative after applying the learning rule described in Equation 9. Then, each column of A is normalized to unit length, similar to previous studies (Olshausen and Field, 1997; Rolls et al., 2006; Zhu and Rozell, 2013; Lian et al., 2019).

The model dynamics and learning rule described in Equations 8, 9 can be implemented in a biologically realistic network (Lian et al., 2019). Here, we simply use the equations described above to demonstrate that the principle of non-negative sparse coding can learn hippocampal cells with both single and multiple firing locations.

Training

For modelled entorhinal cells, when using grid cells described by a mathematical model (Eq. 1 in Materials and Methods) as the entorhinal input, the smallest grid spacing and grid ratio are taken to be 28 cm and 1.42, respectively. Since the environment used in this study is 1 × 1 m, the maximal grid spacing is taken to be smaller than 1 m, which leads to 1≤Nλ≤4 . Therefore, all possible grid spacings are 28, 39.76, 56.46, and 80.17 cm. For grid orientation, we have 1≤Nθ≤7 . For grid phase, we have the same number of phases in each direction and the maximal number is 5, i.e., 1≤Nx=Ny≤5 . After investigating the effect of grid diversity on modelled hippocampal cells for the learning model, more realistic grid cells (defined in Materials and Methods) are then used to investigate the robustness of the model. Furthermore, weakly spatial cells (defined in Materials and Methods) are also used as the entorhinal input to investigate what weakly spatial cells in the EC contribute to place cells’ firing. For both cases of realistic grid cells and weakly spatial cells, the number of modelled entorhinal cells is taken to be 600 (Ne = 600).

There are 100 modelled hippocampal cells at the second layer in our simulations (unless otherwise noted), i.e., Nh=100 . The dynamical system described by Equation 8 is implemented by the first-order Euler method, where the membrane time constant is τ = 10 ms, consistent with the physiological value (Dayan and Abbott, 2001), the threshold is β = 0.3, and there are 200 integration time steps with a time step of 0.8 ms, which we found to provide numerically stable solutions. We use 20,000 epochs in our training. In each epoch, a random location, r, is presented to the entorhinal cells and the model responses are computed using Equation 8 and the matrix of connection strengths, A, is updated by Equation 9. The learning rate, η, is chosen to be 0.03. The parameters above were chosen to ensure a stable solution in a reasonable time scale, but the results were found to be robust to moderate changes of these parameters.

Recovering the firing fields of modelled hippocampal cells

Because the response of modelled hippocampal cells is computed by the dynamic equations in Equation 8, ATse=(EA)Tr cannot simply represent the response corresponding to the spatial location r because of the recurrent connection W, i.e., EA cannot represent the firing field of modelled hippocampal cells. Therefore, after training, we use the method of reverse correlation to recover the firing fields, denoted as F, of modelled hippocampal cells. We present K uniformly sampled random locations, r1,⋯,rK , to the model, compute according to Equation 8 the neural responses of a modelled hippocampal cell, s1,⋯,sK , and then compute the firing field, F, of this modelled hippocampal cell by F=s1r1 +⋯+ sKrKs1 +⋯+ sK. (10)

K = 105 is used in this article.

Fitting firing fields to functions

In order to obtain the center and size of the firing field of the modelled hippocampal cell, F is fitted by a function Q(x, y) of the form Q(x,y)=γe−ln(5)(x−xc)2 + (y−yc)2σ2, (11)where γ is the amplitude, σ is the breadth of the firing field, and (xc, yc) represents the center of the function. The built-in MATLAB (version R2020a) function, lsqcurvefit, is used to fit these parameters. The fitting error is defined as the square of the ratio between the fitting residual and firing field. After fitting, the fitting error and σ are used to determine whether a modelled hippocampal cell meets the criteria of place cell described below.

Selecting place cells

Some firing fields of modelled hippocampal cells have multiple firing locations and noise in the background, while others have a single location of firing. After fitting firing fields into the function described in Equation 11, a modelled hippocampal cell is categorized as a place cell if the following two criteria are satisfied for the firing field: (1) the fitting error is smaller than 15%; (2) the breadth, σ, is larger than 5 cm. These two rules exclude any modelled hippocampal cells with no obvious firing field or with multiple-location firing field. The firing field of a place cell is called place field.

Measuring the uniformity of place cell representation

For place cells that meets the criteria defined above, the field center (xc, yc) fitted by Equation 11 indicates the spatial location that the place cell responds to. We measured how well all place cells represent the entire environment using two measures.

The first measure is distance to place field, dPF, which indicates the Euclidean distance between each spatial location (px, py) in the environment and the nearest place field, described as dPF=mini((xi−px)2 + (yi−py)2). (12)

If the distance to a place field is large for a location, it means that there are no place fields near this location. Therefore, the distribution of this measure can tell us how well place fields of all place cells tile the entire spatial environment. When all spatial locations have small values of dPF, the entire environment is tiled by the place cells.

The second measure is nearest distance, dND. We define dND of place cell j as the maximal Euclidean distance of two nearest centers, described as dND(j)=max(mini,i≠j2((xi−xj)2 + (yi−yj)2)), (13)where (xj, yj) is the center of the place field, min2 returns a set of two smallest values. The distribution of dND for all centers shows the uniformity of place cells in the environment. However, this measure alone provides little information about the coverage of all place cells because place cells with small nearest distance might only lie in a small sub-region of the entire environment, which would give a small value of this measure but would not represent a good tiling of the entire environment.

The distance to place field, dPF , together with nearest distance, dND , provide quantitative measures of how well the place cells code for the spatial environment. Small values of both measures indicate that place cells can tile the entire environment fairly evenly. For example, if 100 place cells are organized on a 10 × 10 grid that evenly tile the 1m×1m environment, the nearest distance will be 100/(10−1)≈11.11 cm for each place cell and the distance to place field for every location is smaller than 11.11/2≈5.56 cm.

Results

When diverse grid cells are used as the entorhinal input, the model can learn place cells that tile the entire environment efficiently

The results shown in this section use grid cells described by the mathematical model as the entorhinal input. Our simulation shows that the non-negative sparse coding model proposed here can learn single-location place cells given diverse grid cells as the input. Grid cells with four different spacings (Nλ = 4), six different orientations (Nθ = 6), and five different phases in both x- and y-axes (Nx=Ny=5 ) are used here, i.e., there are 600 grid cells in total used as the entorhinal input (Ne=NλNθNxNy=600 ).

After learning, all 100 modelled hippocampal cells meet the criteria of a place cell (as defined in Materials and Methods). The firing fields, F (defined by Eq. 10), for 100 modelled hippocampal cells are shown in Figure 3A. The firing fields of modelled hippocampal cells are ordered by their spatial locations. All place cells have a single-location firing field. Furthermore, different place cells have spatially different firing fields.

Figure 3.
Figure 3.

A, Firing fields, F (defined by Eq. 10), for 100 place cells. All 100 modelled hippocampal cells learn a place field at different spatial locations and meet the criteria of a place cell. Each block represents the firing field of a cell in a 1 × 1 m environment. Values in each block are normalized to [0 1]. The radii of all place cells have mean 8.92 cm and SD 0.49 cm. B, Centers of the place cells plotted together in the environment, showing that they evenly tile the whole spatial environment with a hexagonal pattern. C, Box plot of distance to place field for all spatial locations in the spatial environment. The black lines at the bottom and top indicate the minimum and maximum, and the bottom edge of the blue box, red line inside the blue box, and top edge of the blue box represent 25th, 50th (median), and 75th percentiles of the data. In this box plot, there are no outliers. D, Histogram of nearest distance for all place cells.

The learned place cells tile the environment efficiently

The centers of all the place cells are displayed together in the 1 × 1 m spatial environment represented by a 32 × 32 pixel-like image (Fig. 3B), which shows that the centers of the 100 place cells tile the entire environment without any overlap. In addition, the box plot in Figure 3C shows that any location within the space is within a distance of no more than 8.2 cm from the nearest place fields. The histogram of nearest distance of all 100 place cells is displayed in Figure 3D, which shows that the distribution is centered around a mean value of 10.70 cm and SD 0.75 cm. Given that the learned place cells have mean radius 8.92 cm with SD 0.49 cm, Figure 3B–D illustrates that the learned place cells tile the whole environment rather evenly, i.e., the model learned by non-negative sparse coding can give an accurate neural representation of the spatial location in the environment.

Moreover, centers of all learned place cells (Fig. 3B) are positioned into a hexagonal pattern, which can be explained by the principle of the model. Because our model is based on sparse coding that finds an efficient representation of the input, the fact that all learned place cells altogether form a hexagonal pattern is efficient because the triangular lattice of the hexagonal pattern is known to be the optimal solution to the circle packing problem (Thue, 1892). The recurrent connection W, described in Equation 8 might provide the inhibition needed for generating an efficient population code of the space. This result is also consistent with a cluster learning method of concept learning in both spatial and conceptual domains (Mok and Love, 2019), suggesting that sparse coding might be an underlying principle of processing conceptual information as well.

The competition introduced by sparse coding provides the inhibition for place cells

The connectivity profile between 600 grid cells and 100 place cells is plotted in Figure 4A, which shows that each place cell selects a group of particular grid cells with different weights. As a result, the overall feedforward connection from the spatial environment to the place cells, namely the matrix product EA, has the spatial structure plotted in Figure 4B, which shows that each place cell is selective to one spatial location similar to the firing fields (Fig. 3A). However, EA has strong average offsets, which can be seen from the gray background in Figure 4B. The model of place cells proposed by Solstad et al. (2006) has an inhibition term to balance the excitation so that the place fields are responsive to a single location. As for the model of place cells proposed by Franzius et al. (2007b), an offset constant is added and signs of model units are adjusted to achieve single location place fields. Nevertheless, comparing Figures 3A and 4B, we can conclude that the network implemented by sparse coding naturally introduces the competition to inhibit place cells such that they have firing fields similar to those found in experiments. As stated earlier in Materials and Methods, the sparse coding model used in this article can be implemented by a biologically realistic network (Lian et al., 2019), suggesting that principle used here can be a potential mechanism used in the navigational system of the brain. The results presented in this study are not sensitive to different parameter values as long as there are diversities in spacing, orientation, and phase. Even 81 grid cells (Nλ = 3, Nθ = 3, and Nx=Ny=3 and Nx=Ny=5 ) are sufficient for the model to learn place cells that tile the whole environment.

Figure 4.
Figure 4.

Feedforward connection of the model. A, Connection strengths between grid and place cells, A. Each block represents the connection between 600 grid cells and a place cell on a 24 × 25 matrix. B, Feedforward connection strengths from the spatial environment to place cells, EA. Each block shows the selective spatial structure of a place cell. For both A, B, values in each block are normalized to [0 1] for plotting.

In addition, the principle of sparse coding forces the model to learn an efficient representation of the entorhinal input. The average percentage of active modelled hippocampal cells in response to a spatial location is 5.59%. The sparse population activity is consistent with the experimental study that shows sparse ensemble activities in the macaque hippocampus (Skaggs et al., 2007).

The model can learn cells with multiple firing locations

In this section, we still use grid cells described by the mathematical model as the entorhinal input and show that the lack of diversity in any grid parameters or the lack of modelled hippocampal cells in the network will prevent the model from learning place cells and cells with multiple firing locations start to emerge, i.e., the same model can learn cells similar to dentate gyrus cells that have multiple firing locations.

When grid cells are less diverse

A lack of diversity in grid spacing results in the emergence of multiple firing locations of the modelled hippocampal cells, as illustrated in Figure 5A compared with Figure 3A. Similarly, compared with Figure 3B,C, the lack of diversity in grid orientation or grid phase will also cause the model to learn more cells with multiple firing locations (Fig. 5B,C). These modelled hippocampal cells are similar to dentate gyrus cells that are found to have multiple firing locations in experimental studies (Jung and McNaughton, 1993; Leutgeb et al., 2007).

Recall that the principle of sparse coding finds a linear representation of the input, namely the grid cell responses. Our results suggest that grid cells with less diversity in grid parameters are not sufficient to well represent the whole environment, so that the system gives an ambiguous representation of the spatial location. Therefore, the diverse grid cells found in the MEC are crucial to the emergence of hippocampal place cells if grid cells are the only entorhinal input to the hippocampus. The lack of diversity in afferent grid cells may be one possible factor explaining how cells with multiple firing locations emerge in the dentate gyrus.

When there are fewer modelled hippocampal cells

Simulations also show that a smaller number of modelled hippocampal cells, Nh, can also cause the model to learn cells with multiple firing locations, although the grid cells are diverse. This is illustrated in Figure 6, which shows the firing fields of modelled hippocampal cells when there are different numbers of modelled hippocampal cells in the network. The values of the remaining parameters are exactly the same as ones used in Figure 5, which shows well-learned place cells, except the number of modelled hippocampal cells, Nh. Figure 6 demonstrates that as the number of modelled hippocampal cells, Nh, decreases, cells with more firing-locations start to emerge. The less cells, the larger the proportion of cells with multiple firing locations that emerge. When Nh = 10 all modelled hippocampal cells have more than one firing location. When Nh = 20 there are five cells that are categorized as place cells. When Nh is larger than 30, almost all cells are found to have single-location firing fields.

Figure 5.
Figure 5.

Modelled hippocampal cells with multiple firing locations start to emerge because of the lack of diversity in any of the grid parameters. Each block represents the firing field, F (Eq. 10), of a modelled hippocampal cell in a 1 × 1 m environment. Values in each block are normalized to [0 1]. A, Lack of diverse grid spacings: one grid spacing, six orientations, and 25 phases (Nλ=1, Nθ=6 and Nx=Ny=5 ). B, Lack of diverse grid orientations: four grid spacing, one orientation, and 25 phases (Nλ=4, Nθ=1 and Nx=Ny=5 ). C, Lack of diverse grid phases: four grid spacing, six orientations, and one phase (Nλ=4, Nθ=6 and Nx=Ny=1 ).

Figure 6.
Figure 6.

The firing fields, F (recovered by Eq. 10), as the number of cells (Nh ) increases from 10 to 60 (separated by dash lines). A smaller number of cells, Nh, leads to more cells with multiple firing fields after learning. The yellow box highlights the only cells with multiple firing locations when Nh>=40 . Each block represents the firing field of a cell in a 1 × 1 m environment. Values in each block are normalized to [0 1]. Results shown in this figure have the same parameters as Figure 3 except the number of cells, Nh.

Consequently, although a network with diverse grid cells can represent the spatial environment well, having less modelled hippocampal cells does not result in a unique representation of the spatial location with single-location place cells and the animal’s location might need to be encoded using more than one cell. This suggests more generally that hippocampal cells with multiple firing locations may be generated by having a small number of modelled hippocampal cells in the population that implements sparse coding.

The spatial resolution of the hippocampal place map increases as more place cells are used to represent the environment

As discussed above, when Nh is larger than 30, almost all modelled hippocampal cells have a single-location firing field. In addition, the learned place cells tile the whole environment rather well with small values of the nearest distance (Eq. 13). Furthermore, as Nh increases, the mean nearest distance and field breadth of the place field decreases (Fig. 7) with relatively small variations, indicating that the spatial resolution of the neural representation by place cells improves.

Figure 7.
Figure 7.

Nh versus mean radius and Nh versus mean nearest distance. As Nh increases, the mean radius and mean nearest distance decrease, indicating that a place map with higher spatial resolution is obtained. The error bars represent the SDs of radius and nearest distance.

Model results are robust to realistic grid fields

When 600 more realistic grid cells sampled from four discrete grid modules (Materials and Methods) are used as the entorhinal input that incorporate the observed biological variability, the model can still learn a robust representation of the spatial location of the entire environment, as shown in Figure 8.

Figure 8.
Figure 8.

Results are robust when realistic grid cells are used. A, Learned place cells evenly tile the entire spatial environment (similar to Fig. 3). B, The lack of diversity in grid spacing, orientation or phase (left, middle, and right plots) leads to cells with multiple firing locations (similar to Fig. 5). C, The model with fewer modelled hippocampal cells leads to cells with multiple firing locations (similar to Fig. 6). The yellow box highlights the only modelled hippocampal cell with multiple firing locations when Nh = 60. D, Spatial resolution of the neural representation increases as Nh increases (similar to Fig. 7). The error bars represent the SDs of radius and nearest distance.

Figure 8A shows that when grid fields are diverse in grid spacing, orientation, and phase, each modelled hippocampal cell learns a single-location firing field such that centers of all place fields tile the entire spatial environment rather evenly. Furthermore, these place cells are positioned into a hexagonal pattern that packs the environment efficiently. The box plot of distance to place field shows fairly small values and indicates the whole environment is covered well. The distribution of nearest distance has mean 10.76 cm and SD 0.62 cm, qualitatively consistent with results shown in Figure 3C (mean 10.70 cm and SD 0.75 cm). Therefore, the learned place cells evenly tile the entire environment. Additionally, 600 grid cells sampled only from the two smallest grid modules are sufficient for place cells to emerge, as illustrated in Figure 9.

Figure 9.
Figure 9.

Place cells can be learned using grid cell inputs sampled only from the two smallest grid modules. A total of 96 (out of 100) modelled hippocampal cells are place cells after learning. The parameters of the model are the same as Figure 8A except that grid cells are only sampled from the two smallest grid modules whose mean grid spacings are 38.8 and 48.4 cm. Each block represents the firing field (recovered by Eq. 10) of a place cell in a 1 × 1 m environment. Values in each block are normalized to [0 1].

Figure 8B shows that realistic grid fields with less diversity will cause the model to learn hippocampal cells with multiple firing locations. The left plot displays the firing fields of 100 modelled hippocampal cells with less diversity in grid spacing. The SD of spacing in four grid modules is set to 0 cm instead of 8 cm while the SD of orientation is still 3° and the phase is random. The middle plot shows firing fields when there is less diversity in grid orientation, where in each grid module the SD of spacing is 4 cm, the SD of orientation is 0° and phase is random. The right plot is for the case of less diversity in grid phase, where in each grid module the SD of spacing is 8 cm, the SD of orientation is 3° and phase is (0, 0) for all grid cells. Although the model learns hippocampal cells with multiple locations when there is less diversity in grid parameters, the learned place cells still tile the entire environment.

Figure 8C shows that having fewer modelled hippocampal cells causes the model to learn cells with multiple firing locations. The six plots separated by dashed lines in Figure 8C represent the firing fields of modelled hippocampal cells when the number of modelled hippocampal cells, Nh, is 10, 20, 30, 40, 50, and 60, respectively. When Nh=10 and 20, there is no place cell. When Nh≥40 , most modelled hippocampal cells are place cells. The yellow box indicates the only modelled hippocampal cell that is not a place cell when Nh = 60.

Similar to Figure 7, the neural representation of the spatial environment has better resolution (smaller radius and smaller nearest distance) as Nh increases, as seen from Figure 8D.

The model can generate large place fields using grid cells

As discussed in a previous study (Neher et al., 2017), most existing models of place cells cannot produce large place fields, such as CA3 place cells with size around 1225 cm2. The model proposed here can generate large place fields by simply having grid cells with large grid spacings as the input to modelled hippocampal cells.

In this part of the study, more realistic grid cells are used as the entorhinal input to the hippocampus. In addition, only grid cells with grid spacings in the fourth module are used, i.e., the grid spacing is sampled from the normal distribution with mean 98.4 cm and SD 8 cm, grid orientation is sampled from the distribution with mean 0° and SD 3°, and grid phases are randomly chosen from a uniform distribution. Similarly, 600 grid cells are used. The number of modelled hippocampal cells, Nh, is set to 20.

After learning, each modelled hippocampal cell pools a particular group of grid cells, similar to Figure 4A, 18 out of 20 modelled hippocampal cells satisfy the criteria of place cells defined Materials and Methods. Figure 10A shows the 18 learned place cells. Figure 10C shows that these place cells have radius from 18.71 to 21.22 cm (mean 19.68 cm and SD 0.75 cm). Therefore, the size of place fields ranges from 1099.76 to 1414.62 cm2. Figure 10B,D,E shows that these 18 place cells with large size cover the entire environment rather evenly in a hexagonal pattern.

Figure 10.
Figure 10.

Large place fields emerge. A, Firing fields, F (recovered by Eq. 10), for 18 learned place cells. A total of 18 out of 20 modelled hippocampal cells learn a place field at different spatial locations. Each block represents the firing field of a modelled hippocampal cell in a 1 × 1 m environment. Values in each block are normalized to [0 1]. B, Centers of place cells plotted together in the environment. Place cells evenly tile the whole spatial environment. C, Histogram of radius for all place cells. D, Box plot of distance to place field for all spatial locations in the spatial environment. The black lines at the bottom and top indicate the minimum and maximum, and the bottom edge of the blue box, red line inside the blue box and top edge of the blue box represent 25th, 50th (median), and 75th percentiles of the data while outliers are excluded and represented as red dots. E, Histogram of nearest distance for all place cells.

Above all, the model can learn large place cells if the afferent grid cells have large grid spacings, consistent with experimental evidence that the sizes of grid cells and place cells increase along the dorsal-ventral axis (Fyhn et al., 2007; Kjelstrup et al., 2008) and with topographic entorhinal-hippocampal projections along the dorsal-ventral axis (Dolorfo and Amaral, 1998).

Weakly spatial cells in the EC are sufficient for hippocampal place cells to emerge

Recent experimental evidence shows that the emergence of hippocampal place cells happens earlier in development than grid cells (Langston et al., 2010; Wills et al., 2010). In addition, other experimental studies suggest that hippocampal place cells can still maintain their place fields even after grid cells are inactivated (Koenig et al., 2011; Brandon et al., 2014; Hales et al., 2014; Schlesiger et al., 2015). Although weakly spatial cells are more abundant than grid cells in the EC, how they contribute to the place fields of hippocampal place cells is still unclear. Here, we show that even weakly spatial cells can provide sufficient spatial information for the emergence of place cells that have an accurate representation of spatial locations. This suggests that place cells can emerge throughout the development of MEC grid cells, from the initial weakly-tuned spatial pattern to the fully developed hexagonal grid pattern.

In this section, 600 weakly spatial cells are used as the entorhinal input to the hippocampus and there are 100 modelled hippocampal cells. We use a smaller learning rate (η = 0.01) and more epochs (30,000) for the learning here. The firing fields of ten example weakly spatial cells are shown in Figure 11A.

Figure 11.
Figure 11.

Weakly spatial cells are sufficient for place cells to emerge. A, Examples of weakly spatial cells. Each block represents the firing field of a cell in a 1 × 1 m environment. B, Firing fields, F (recovered by Eq. 10), for 90 learned place cells. A total of 90 out of 100 modelled hippocampal cells learn a place field at different spatial locations. Each block represents the firing field of a modelled hippocampal cell in a 1 × 1 m environment. Values in each block are normalized to [0 1]. C, Centers of 90 place cells plotted together in the environment. Place cells evenly tile the whole spatial environment with an efficient hexagonal pattern. D, Box plot of distance to place field for all spatial locations in the spatial environment. The black lines at the bottom and top indicate the minimum and maximum, and the bottom edge of the blue box, red line inside the blue box and top edge of the blue box represent 25th, 50th (median), and 75th percentiles of the data. In this box plot, there are no outliers. E, Histogram of nearest distance for place cells.

An efficient hippocampal place map emerges

The firing fields of weakly spatial cells are very different from the periodic pattern of grid cells. Surprisingly, they can nevertheless provide sufficient spatial information such that the model based on sparse coding can decode entorhinal cell responses and give an accurate representation of the spatial location. Figure 11B shows the firing fields of learned place cells. Figure 11C–E shows that the centers of place cells evenly tile the entire spatial environment with an efficient hexagonal pattern.

Compared with Figures 3, 8A, using weakly spatial cells instead of grid cells results in learning a hippocampal place-map with less resolution. The mean radius of place fields using weakly spatial cells as the entorhinal input (mean 11.45 cm with SD 2.14 cm; Fig. 11B) is larger than Figure 3 (8.92 cm) and Figure 8A (8.75 cm). Furthermore, the nearest distance in Figure 11E (mean 11.50 cm and SD 0.94 cm) is also larger, compared with Figure 3 (mean 10.70 cm and SD 0.75 cm) and Figure 8A (mean 10.76 cm and SD 0.62 cm) when grid cells are used. The larger SD in Figure 11E suggests that the irregular fields of weakly spatial cells lead to the less even tiling of place cells. However, the learned place map still covers the entire environment well with small distance to place field (Fig. 11D) and efficiently with a hexagonal lattice (Fig. 11C).

The learned place map is robust to noise even when weakly spatial cells are used

Furthermore, the model is quite robust to noise and an efficient place map can still be learned, although a relatively strong noise is added to the modelled entorhinal cell responses in Equation 8: se=ETr + γnn, (14)where n is the Gaussian noise with mean 0 and variance 1, and γn is the amplitude of the noise. Note that the maximal value of ETr is 1 because E is normalized to have the maximum 1. We find that the model can still learn an efficient map when γn is 0.3 (Fig. 12).

Figure 12.
Figure 12.

The model is robust to noise even when weakly spatial cells are used, γn=0.3 in Equation 14. A, Firing fields, F (recovered by Eq. 10), for 80 learned place cells. A total of 80 out of 100 modelled hippocampal cells learn a place field at different spatial locations. Each block represents the firing field of a modelled hippocampal cell in a 1 × 1 m environment. Values in each block are normalized to [0 1]. B, Centers of 80 place cells plotted together in the environment. Place cells tile the whole spatial environment. C, Box plot of distance to place field for all spatial locations in the spatial environment. The black lines at the bottom and top indicate the minimum and maximum, and the bottom edge of the blue box, red line inside the blue box, and top edge of the blue box represent 25th, 50th (median), and 75th percentiles of the data while outliers are excluded and represented as red dots. D, Histogram of nearest distance for place cells.

Although there are places in the environment not covered by place cells, generally the modelled hippocampal cells learn place fields that efficiently tile the entire environment.

Above all, the model is consistent with the experimental evidence that place cells emerge earlier than grid cells during development and a possible explanation is that the neural system can learn a hippocampal map even when the hexagonal spatial field is not well developed, and place cells can maintain their place fields when grid cells are inactivated because weakly spatial cells in the EC can lead to the emergence of a hippocampal place map.

Sparse coding can learn hippocampal place cells although the input cells from the EC are weakly tuned to the spatial environment. Thus, input cells with stronger spatial selectivity can provide more spatial information so that unique place field can be decoded by sparse coding. Barry and Burgess (2007) used a learning model to learn place cells from responses of boundary vector cells that are selective to boundaries of the environment at particular angles and distances. Their result can be regarded as a special case of the results presented in this article, where boundary vector cells are simply entorhinal input cells with stronger tuning of the spatial environment.

These weakly spatial cells can arise from any form of sensory inputs, such as visual input and auditory input, that encode spatial information. For example, the visual input at different locations of the environment actually carries information about spatial locations and consequently the afferent visual information to the EC can lead to weakly spatial cells. Moreover, the principle of sparse coding can cause EC cells to generate a hippocampal place map. The conjecture proposed here can explain a recent experimental study that shows that place cell firings mainly reflect visual inputs (Chen et al., 2019) and another experimental study that suggests homing abilities of mice even in darkness may not need accurate grid cell firing (Chen et al., 2016).

The effect of environmental geometry on hippocampal cells may come from distorted entorhinal input

O’Keefe and Burgess (1996) found that place fields will be stretched following the environmental distortions. Later, Barry et al. (2007) found the same phenomenon for gird cells, namely that grid cells will be stretched along the distorted axis. Given the anatomic connection from the EC to hippocampus, it is natural to ask whether stretched place fields caused by the environment manipulation originate from stretched gird cells caused by the environment geometry. Our model shows that when grid fields are stretched along one axis of the environment, place fields will be stretched along that direction as well.

After the model is learned using 600 realistic grid cells as the entorhinal input to the hippocampus (Fig. 8A), the entorhinal-hippocampal connection (A) is kept fixed. Then the spatial environment is changed to 2 × 1 m, i.e., the environment is re-scaled along x-axis. In addition, gird fields are also stretched by a factor of 2 along x-axis. Next, we recover the firing fields of modelled hippocampal cells (described in Materials and Methods) with fixed connection and stretched grid cells. Figure 13 shows that modelled hippocampal cells are still selective to one location of the environment but their firing fields are stretched compared with the original place fields (Fig. 8A, left plot).

Figure 13.
Figure 13.

Firing fields of modelled hippocampal cells with distorted grid cells. Firing fields, F (recovered by Eq. 10), for all 100 modelled hippocampal cells after the grid fields are stretched by a factor of 2 along the x-axis. Each block represents the firing field of a modelled hippocampal cell in a 2 × 1 m environment. Values in each block are normalized to [0 1].

As grid cells are anchored to external landmarks (Hafting et al., 2005), grid fields are re-scaled by environmental changes (Barry et al., 2007). Our model suggests that the effect of environmental geometry on place cells may come from grid cells distorted by the environment manipulation. However, this does not rule out the possibility that the spatial selectivity of other entorhinal input to place cells is also altered by the environment, which causes the changes of place fields. If there is experimental data about the effect of environment geometry on other EC neurons that project to the hippocampus in the future, our model can be used to further explain what causes the change of hippocampal place fields.

Navigation trajectory versus random location

As described in Materials and Methods, the model is trained using random spatial locations uniformly sampled from the entire environment, so the spatial input to the model can uniformly cover the entire environment very quickly after some iterations. However, for a real navigation trajectory of a rat running freely in an environment, the route is continuous and there are spatial locations the rat has never been to. In this section, we used the same model as the one displayed in Figure 8A that has 600 realistic modelled grid cells as the entorhinal input to the model and 100 modelled hippocampal cells. Instead, the random spatial input to the model is replaced by a simulated running trajectory of a virtual rat. The trajectory is generated by a smoothed random walk using the method from D’Albis and Kempter (2017) with mean speed 0.25 m/s and 20 Hz of sampling positions. A simulated running trajectory of 3600 s is used to train the model. After learning, another simulated running trajectory of 1200 s is used to recover the firing fields of modelled hippocampal cells using the same method described in Equation 10.

Figure 14 shows the firing fields of 100 modelled hippocampal cells using the same realistic grid cells as Figure 8A but simulated running trajectory for training. Compared with Figure 8, firing fields trained and recovered by running trajectories are less circular because of non-uniform spatial locations used to train and recover the firing fields. Though the running trajectory of 3600 s contains 72,000 spatial locations (much >20,000 spatial locations that are uniformly sampled to train the model in Fig. 8), not all modelled hippocampal cells learn a place field. Positions along the running trajectory are continuous and are not sampled according to a uniform distribution, so the model has more data at some positions than others, causing the model to learn less place cells with less circular firing fields.

Figure 14.
Figure 14.

Firing fields of modelled hippocampal cells trained and recovered using simulated running trajectories. Firing fields, F (recovered by Eq. 10), for all 100 modelled hippocampal cells. Four out of 100 modelled hippocampal do not have an obvious firing field, while the other 96 modelled hippocampal cells learn place-like cells with one dominant firing location. Each block represents the firing field of a modelled hippocampal cell in a 1 × 1 m environment. Values in each block are normalized to [0 1].

Discussion

Summary

In this article, we applied sparse coding with non-negative constraint to a hierarchical model of entorhinal-hippocampal network. Our results show that sparse coding can learn an efficient hippocampal place map that represents the entire environment when grid cells are diverse in grid spacing, orientation, and phase. However, lack of diversity in grid cells or fewer modelled hippocampal cells leads to the emergence of cells with multiple firing locations, like those cells found in the dentate gyrus. In addition, weakly spatial cells in the EC are sufficient for sparse coding to learn hippocampal place cells.

Comparison with other learning models

Our work differs significantly from previous studies on learning place cells from grid cell input (Rolls et al., 2006; Franzius et al., 2007b; Monaco and Abbott, 2011; Neher et al., 2017). Most importantly, our model investigates different types of entorhinal input: grid cells and weakly spatial cells. Also, among these learning models, we systematically investigate the influence of the diversity in grid cells using knowledge of grid modules (Stensola et al., 2012) on the formation for hippocampal cells. Moreover, we demonstrate that learned hippocampal place cells can represent the entire spatial environment efficiently using a hexagonal lattice, consistent with a recent work in the conceptual state spaces (Mok and Love, 2019). Furthermore, the same model can produce cells with one firing location, multiple firing locations and large place field size, which can account for the emergence of a range of different observed hippocampal cell types. In addition, we demonstrate that weakly spatial cells in the EC can also provide sufficient spatial information for the emergence of the hippocampal place map after learning and the model is very robust to noise. Most importantly, all the results presented in this article are generated by the same model, namely sparse coding with non-negative constraint.

Although the principle of independent component analysis used by Franzius et al. (2007a,b) to learn place cells from grid cells is similar to the principle of sparse coding used here, the place cell examples in their paper are mostly near the boundary of the environment. However, our model can learn place cells at different places of the entire environment, generate a hippocampal place map that tiles the entire environment efficiently, and automatically provide the needed inhibition by the dynamics of sparse coding. One possible reason is that place cells in a population are not necessarily independent because nearby cells do overlap, so independent component analysis might put a too strong assumption. Also, the non-negativity introduced in this article makes the model more similar to the real neural system, which might help the model uncover important biological properties.

Properties of grid cells that are necessary for the emergence of place cells

Our model shows that the principle of sparse coding can learn an efficient place map using input from the EC, grid cells or weakly spatial cells. Although the model can learn place cells when only weakly spatial cells are used, it does not imply that grid cells are not necessary for the formation of place cells. Fiete et al. (2008) proposed that grid cells with different spacings and phases altogether form a residual system that efficiently encodes the spatial location. In addition, the triangular lattice of the grid pattern is known to be the solution to the optimal circle packing problem (Thue, 1892) and the geometric scale of grid spacings can represent the spatial environment efficiently (Wei et al., 2015). Our results are consistent with the concept that grid cells provide efficient information that can be retrieved to form a hippocampal place map. In our results, when 600 more realistic grid cells are used as the entorhinal input to hippocampal place cells, the ratio between the average of square of grid cell responses and the average of square of place cell responses is 0.31. However, this ratio becomes 0.84 when 600 weakly spatial cells are used as the entorhinal input, suggesting that grid cells are much more efficient for providing spatial information to the hippocampus. Another important property of grid cells that might be necessary for the emergence of place cells is the temporal property-phase precession. The experimental study conducted by Schlesiger et al. (2015) suggests that the MEC input to the hippocampus is necessary for the temporal property of hippocampal place cells. Therefore, although weakly spatial cells can provide sufficient spatial information to learn an efficient place map, grid cells that have phase precession might be required to account for the phase precession of hippocampal place cells. This is left for the future work.

Non-grid cells in the EC

Although grid cells in the MEC have structured firing fields that lie on a hexagonal lattice, they only account for <1/3 of MEC cells and nearly 2/3 of MEC cells have spatial selectivity without well-characterized firing fields (Diehl et al., 2017). In the LEC, cells also display weak spatial specificity and convey nonspatial information (Hargreaves et al., 2005; Yoganarasimha et al., 2011). Our model explains how these upstream non-grid cells that contain weak spatial information can be used to form a hippocampal place map, which is consistent with increasingly more experimental evidence that suggests grid cells are not required to form the spatial firing field of place cells (Langston et al., 2010; Wills et al., 2010; Koenig et al., 2011; Brandon et al., 2014; Hales et al., 2014; Schlesiger et al., 2015).

Also, more recent studies have been investigating the effect of sensory input such as visual input on the firing of place cells. Chen and colleagues find that visual input largely determines place cells firing (Chen et al., 2013, 2016, 2019). In addition, a recent study shows that some neurons in V1 display location-specific firing (Haggerty and Ji, 2015). Therefore, we conjecture that neurons that respond to external stimuli in a spatial environment must contain spatial selectivity in any form and all these neurons contribute to the formation of a cognitive map. EC, the gateway between the hippocampus and the neocortex of the brain, provides abundant information for the hippocampus and plays a crucial role here. Our results show that the principle of sparse coding can be one underlying principle that efficiently retrieves spatial information from the upstream. Furthermore, the efficient hexagonal pattern of the learned place map (Figs. 3B, 8A, 10B, 11C) is consistent with the hexagonal clusters in a recent work in conceptual state spaces (Mok and Love, 2019), suggesting that the principle of sparse coding can be used to explain more functions of the hippocampus.

Non-negativity

In recent computational studies of the navigational system of the brain, the concept of non-negativity is used several times. Dordek et al. (2016) applied non-negative principal component analysis to extract grid cells from place cell responses and the introduction of non-negativity pushes the model to converge to a hexagonal lattice from a square lattice when there is no non-negativity. D’Albis and Kempter (2017) build a single-cell spiking model for the grid cell and the non-linearity brought by the non-negative weights is sufficient for the emergence of a hexagonal lattice. Similarly, Sorscher et al. (2019) build a theory for the emergence of grid cells and the non-negativity constraint on the firing rates brings a symmetry-breaking effect that leads to the hexagonal firing fields. Unlike these studies that impose non-negativity into the model of grid cells, we use non-negative sparse coding to learn the hippocampal place cells. Non-negativity is introduced to account for some biological aspects such as non-negative firing rates and excitatory connection between cortical areas. In the original paper of non-negative sparse coding (Hoyer, 2003), the model learns Gabor-like V1 simple cells when trained on natural images; in other words, the non-negativity introduced is to account for the biological aspects and it is the principle of sparse coding that enables the model to learn V1 simple cells. The non-negative sparse coding used in this article demonstrates that the principle of sparse coding can be used in the navigational system of the brain even when non-negativity constraint is incorporated. For our model, the non-negativity on neuronal responses is required to have a meaningful firing fields for the modelled hippocampal cells. However, when the non-negativity constraint on the connection A is removed, the modelled hippocampal cells still learn place fields that are similar to results demonstrated in this article. Also, it is important to note that the non-negativity constraint on the entorhinal-hippocampal connection A does not prohibited the role of inhibition in the model. Instead, inhibition in the sparse coding model is vital to provide the competition needed to achieve the sparseness of the model. However, a very detailed model of how sparse coding can be implemented is still not very clear, which is discussed in the next section.

Underlying neural circuits

Our study examines the extent to which sparse coding is as an underlying principle in the navigational system of the brain. However, the current model implies no specific neural circuits for the implementation of sparse coding, rather it is one of the principles that underlies the formation of the neural circuits. Neurophysiological and anatomic studies suggest that the EC and the hippocampus interact via a loop (Tamamaki and Nojyo, 1995; Tamamaki, 1997; Witter et al., 2014). Therefore, feedforward connection from the EC to the hippocampus, recurrent connection within the hippocampus, and feedback connection from the hippocampus to the EC all play an important role, although their specific contributions to the overall function of the network have not been fully uncovered yet. Rennó-Costa and Tort (2017) and Agmon and Burak (2020) investigated the coupling relationship between MEC grid cells and hippocampal place cells and showed that the proposed models can account for some experimental observations. However, how the underlying neural circuits can be implemented is still unclear. The proposed model based on sparse coding in this study does not rule out any of the network structures mentioned above, as sparse coding can be implemented in neural circuits either in a feedforward network with recurrent connection (Zylberberg et al., 2011) or a network with feedforward-feedback loops (Lian et al., 2019).

Future work

The current study does not propose a specific biological neural circuit for implementing sparse coding in the entorhinal-hippocampal region, which is the study of ongoing work. Such a model of these neural circuits would need to take into account the experimentally known networks in this area. Also, other properties of place cells such as phase precession (O’Keefe and Recce, 1993), multiple place fields in large environments (Park et al., 2011) and place map in 3D environments (Grieves et al., 2020) will be investigated in the future. In addition, the model here used prefixed grid cells. We did not attempt here to provide a description for how grid cells emerge, but rather the grid cells are assumed to provide an efficient representation of the environment. It would be interesting to also investigate the role of sparse coding in how grid cells themselves emerge. It is hoped that such future work, which incorporates these aspects of the development process of both grid cells and place cells, will provide further insights into how the navigational system of the brain works. Sparse coding represents just one of a number of possible mechanisms that shape network structures, and much remains to be explored to incorporate other mechanisms, such as those associated with the complexities of metabotropic receptor effects, as discussed by Hasselmo et al. (2021).

Acknowledgments

Acknowledgements: We thank Kathrine Clarke and Dr. Ali Almasi and Dr. Catherine Davey for helpful comments on this manuscript.

Footnotes

  • The authors declare no competing financial interests.

  • This work was supported by the Australian Government Grant AUSMURIB000001 associated with the ONR MURI Grant N00014-19-1-2571.

This is an open-access article distributed under the terms of the Creative Commons Attribution 4.0 International license, which permits unrestricted use, distribution and reproduction in any medium provided that the original work is properly attributed.

References

  1. ↵
    Agmon H, Burak Y (2020) A theory of joint attractor dynamics in the hippocampus and the entorhinal cortex accounts for artificial remapping and grid cell field-to-field variability. Elife 9:e56894. doi:10.7554/eLife.56894
    OpenUrlCrossRef
  2. ↵
    Barry C, Burgess N (2007) Learning in a geometric model of place cell firing. Hippocampus 17:786–800. doi:10.1002/hipo.20324 pmid:17598149
    OpenUrlCrossRefPubMed
  3. ↵
    Barry C, Hayman R, Burgess N, Jeffery KJ (2007) Experience-dependent rescaling of entorhinal grids. Nat Neurosci 10:682–684. doi:10.1038/nn1905 pmid:17486102
    OpenUrlCrossRefPubMed
  4. ↵
    Beyeler M, Rounds EL, Carlson KD, Dutt N, Krichmar JL (2019) Neural correlates of sparse coding and dimensionality reduction. PLoS Comput Biol 15:e1006908. doi:10.1371/journal.pcbi.1006908 pmid:31246948
    OpenUrlCrossRefPubMed
  5. ↵
    Brandon MP, Koenig J, Leutgeb JK, Leutgeb S (2014) New and distinct hippocampal place codes are generated in a new environment during septal inactivation. Neuron 82:789–796. doi:10.1016/j.neuron.2014.04.013 pmid:24853939
    OpenUrlCrossRefPubMed
  6. ↵
    Chen G, King JA, Burgess N, O’Keefe J (2013) How vision and movement combine in the hippocampal place code. Proc Natl Acad Sci USA 110:378–383. doi:10.1073/pnas.1215834110 pmid:23256159
    OpenUrlAbstract/FREE Full Text
  7. ↵
    Chen G, Manson D, Cacucci F, Wills TJ (2016) Absence of visual input results in the disruption of grid cell firing in the mouse. Curr Biol 26:2335–2342. doi:10.1016/j.cub.2016.06.043
    OpenUrlCrossRefPubMed
  8. ↵
    Chen G, Lu Y, King JA, Cacucci F, Burgess N (2019) Differential influences of environment and self-motion on place and grid cell firing. Nat Commun 10:630.
    OpenUrl
  9. ↵
    D’Albis T, Kempter R (2017) A single-cell spiking model for the origin of grid-cell patterns. PLoS Comput Biol 13:e1005782. doi:10.1371/journal.pcbi.1005782 pmid:28968386
    OpenUrlCrossRefPubMed
  10. ↵
    Dayan P, Abbott L (2001) Theoretical neuroscience: computational and mathematical modeling of neural systems. Cambridge: The MIT Press.
  11. ↵
    de Almeida L, Idiart M, Lisman JE (2009) The input–output transformation of the hippocampal granule cells: from grid cells to place fields. J Neurosci 29:7504–7512. doi:10.1523/JNEUROSCI.6048-08.2009 pmid:19515918
    OpenUrlAbstract/FREE Full Text
  12. ↵
    Diehl GW, Hon OJ, Leutgeb S, Leutgeb JK (2017) Grid and nongrid cells in medial entorhinal cortex represent spatial location and environmental features with complementary coding schemes. Neuron 94:83–92. doi:10.1016/j.neuron.2017.03.004 pmid:28343867
    OpenUrlCrossRefPubMed
  13. ↵
    Dolorfo CL, Amaral DG (1998) Entorhinal cortex of the rat: topographic organization of the cells of origin of the perforant path projection to the dentate gyrus. J Comp Neurol 398:25–48. doi:10.1002/(SICI)1096-9861(19980817)398:1<25::AID-CNE3>3.0.CO;2-B
    OpenUrlCrossRefPubMed
  14. ↵
    Dordek Y, Soudry D, Meir R, Derdikman D (2016) Extracting grid cell characteristics from place cell inputs using non-negative principal component analysis. Elife 5:e10094. doi:10.7554/eLife.10094 pmid:26952211
    OpenUrlCrossRefPubMed
  15. ↵
    Fiete IR, Burak Y, Brookings T (2008) What grid cells convey about rat location. J Neurosci 28:6858–6871. doi:10.1523/JNEUROSCI.5684-07.2008 pmid:18596161
    OpenUrlAbstract/FREE Full Text
  16. ↵
    Franzius M, Sprekeler H, Wiskott L (2007a) Slowness and sparseness lead to place, head-direction, and spatial-view cells. PLoS Comput Biol 3:e166. doi:10.1371/journal.pcbi.0030166 pmid:17784780
    OpenUrlCrossRefPubMed
  17. ↵
    Franzius M, Vollgraf R, Wiskott L (2007b) From grids to places. J Comput Neurosci 22:297–299. doi:10.1007/s10827-006-0013-7 pmid:17195112
    OpenUrlCrossRefPubMed
  18. ↵
    Fyhn M, Hafting T, Treves A, Moser MB, Moser EI (2007) Hippocampal remapping and grid realignment in entorhinal cortex. Nature 446:190–194. doi:10.1038/nature05601 pmid:17322902
    OpenUrlCrossRefPubMed
  19. ↵
    Grieves RM, Jedidi-Ayoub S, Mishchanchuk K, Liu A, Renaudineau S, Jeffery KJ (2020) The place-cell representation of volumetric space in rats. Nat. Commun 11:789.
    OpenUrlCrossRefPubMed
  20. ↵
    Hafting T, Fyhn M, Molden S, Moser MB, Moser EI (2005) Microstructure of a spatial map in the entorhinal cortex. Nature 436:801–806. doi:10.1038/nature03721 pmid:15965463
    OpenUrlCrossRefPubMed
  21. ↵
    Haggerty DC, Ji D (2015) Activities of visual cortical and hippocampal neurons co-fluctuate in freely moving rats during spatial behavior. Elife 4:e08902. doi:10.7554/eLife.08902
    OpenUrlCrossRefPubMed
  22. ↵
    Hales JB, Schlesiger MI, Leutgeb JK, Squire LR, Leutgeb S, Clark RE (2014) Medial entorhinal cortex lesions only partially disrupt hippocampal place cells and hippocampus-dependent place memory. Cell Rep 9:893–901. doi:10.1016/j.celrep.2014.10.009 pmid:25437546
    OpenUrlCrossRefPubMed
  23. ↵
    Hargreaves EL, Rao G, Lee I, Knierim JJ (2005) Major dissociation between medial and lateral entorhinal input to dorsal hippocampus. Science 308:1792–1794. doi:10.1126/science.1110449 pmid:15961670
    OpenUrlAbstract/FREE Full Text
  24. ↵
    Hasselmo ME, Alexander AS, Hoyland A, Robinson JC, Bezaire MJ, Chapman GW, Saudargiene A, Carstensen LC, Dannenberg H (2021) The unexplored territory of neural models: potential guides for exploring the function of metabotropic neuromodulation. Neurosci 456:143–158.
    OpenUrl
  25. ↵
    Hoyer PO (2003) Modeling receptive fields with non-negative sparse coding. Neurocomputing 52–54:547–552. doi:10.1016/S0925-2312(02)00782-8
    OpenUrlCrossRef
  26. ↵
    Hyvarinen A (1999) Survey on independent component analysis. Neural Comput Surv 2:94–128.
    OpenUrl
  27. ↵
    Ismakov R, Barak O, Jeffery K, Derdikman D (2017) Grid cells encode local positional information. Curr Biol 27:2337–2343. doi:10.1016/j.cub.2017.06.034 pmid:28756950
    OpenUrlCrossRefPubMed
  28. ↵
    Jung M, McNaughton B (1993) Spatial selectivity of unit activity in the hippocampal granular layer. Hippocampus 3:165–182. doi:10.1002/hipo.450030209 pmid:8353604
    OpenUrlCrossRefPubMed
  29. ↵
    Kjelstrup KB, Solstad T, Brun VH, Hafting T, Leutgeb S, Witter MP, Moser EI, Moser MB (2008) Finite scale of spatial representation in the hippocampus. Science 321:140–143. doi:10.1126/science.1157086
    OpenUrlAbstract/FREE Full Text
  30. ↵
    Koenig J, Linder AN, Leutgeb JK, Leutgeb S (2011) The spatial periodicity of grid cells is not sustained during reduced theta oscillations. Science 332:592–595. doi:10.1126/science.1201685 pmid:21527713
    OpenUrlAbstract/FREE Full Text
  31. ↵
    Kropff E, Treves A (2008) The emergence of grid cells: intelligent design or just adaptation? Hippocampus 18:1256–1269. doi:10.1002/hipo.20520 pmid:19021261
    OpenUrlCrossRefPubMed
  32. ↵
    Langston RF, Ainge JA, Couey JJ, Canto CB, Bjerknes TL, Witter MP, Moser EI, Moser MB (2010) Development of the spatial representation system in the rat. Science 328:1576–1580. doi:10.1126/science.1188210 pmid:20558721
    OpenUrlAbstract/FREE Full Text
  33. ↵
    Lee DD, Seung HS (1999) Learning the parts of objects by non-negative matrix factorization. Nature 401:788–791. doi:10.1038/44565 pmid:10548103
    OpenUrlCrossRefPubMed
  34. ↵
    Leutgeb JK, Leutgeb S, Moser MB, Moser EI (2007) Pattern separation in the dentate gyrus and CA3 of the hippocampus. Science 315:961–966. doi:10.1126/science.1135801 pmid:17303747
    OpenUrlAbstract/FREE Full Text
  35. ↵
    Lian Y, Grayden DB, Kameneva T, Meffin H, Burkitt AN (2019) Toward a biologically plausible model of LGN-V1 pathways based on efficient coding. Front Neural Circuits 13:13. doi:10.3389/fncir.2019.00013 pmid:30930752
    OpenUrlCrossRefPubMed
  36. ↵
    Mok RM, Love BC (2019) A non-spatial account of place and grid cells based on clustering models of concept learning. Nat Commun 10:5685.
    OpenUrl
  37. ↵
    Monaco JD, Abbott LF (2011) Modular realignment of entorhinal grid cell activity as a basis for hippocampal remapping. J Neurosci 31:9414–9425. doi:10.1523/JNEUROSCI.1433-11.2011 pmid:21697391
    OpenUrlAbstract/FREE Full Text
  38. ↵
    Moser EI, Roudi Y, Witter MP, Kentros C, Bonhoeffer T, Moser MB (2014) Grid cells and cortical representation. Nat Rev Neurosci 15:466–481. doi:10.1038/nrn3766 pmid:24917300
    OpenUrlCrossRefPubMed
  39. ↵
    Neher T, Azizi AH, Cheng S (2017) From grid cells to place cells with realistic field sizes. PLoS One 12:e0181618–27. doi:10.1371/journal.pone.0181618
    OpenUrlCrossRef
  40. ↵
    O’Keefe J (1976) Place units in the hippocampus of the freely moving rat. Exp Neurol 51:78–109.
    OpenUrlCrossRefPubMed
  41. ↵
    O’Keefe J, Dostrovsky J (1971) The hippocampus as a spatial map: preliminary evidence from unit activity in the freely-moving rat. Brain Res 34:171–175. doi:10.1016/0006-8993(71)90358-1 pmid:5124915
    OpenUrlCrossRefPubMed
  42. ↵
    O’Keefe J, Recce ML (1993) Phase relationship between hippocampal place units and the EEG theta rhythm. Hippocampus 3:317–330. doi:10.1002/hipo.450030307 pmid:8353611
    OpenUrlCrossRefPubMed
  43. ↵
    O’Keefe J, Burgess N (1996) Geometric determinants of the place fields of hippocampal neurons. Nature 381:425–428. doi:10.1038/381425a0 pmid:8632799
    OpenUrlCrossRefPubMed
  44. ↵
    Olshausen BA, Field DJ (1996) Emergence of simple-cell receptive field properties by learning a sparse code for natural images. Nature 381:607–609. doi:10.1038/381607a0 pmid:8637596
    OpenUrlCrossRefPubMed
  45. ↵
    Olshausen BA, Field DJ (1997) Sparse coding with an overcomplete basis set: a strategy employed by V1? Vision Res 37:3311–3325. doi:10.1016/s0042-6989(97)00169-7 pmid:9425546
    OpenUrlCrossRefPubMed
  46. ↵
    Park E, Dvorak D, Fenton AA (2011) Ensemble place codes in hippocampus: CA1, CA3, and dentate gyrus place cells have multiple place fields in large environments. PLoS One 6:e22349. doi:10.1371/journal.pone.0022349 pmid:21789250
    OpenUrlCrossRefPubMed
  47. ↵
    Rennó-Costa C, Tort AB (2017) Place and grid cells in a loop: implications for memory function and spatial coding. J Neurosci 37:8062–8076. doi:10.1523/JNEUROSCI.3490-16.2017 pmid:28701481
    OpenUrlAbstract/FREE Full Text
  48. ↵
    Rolls ET, Stringer SM, Elliot T (2006) Entorhinal cortex grid cells can map to hippocampal place cells by competitive learning. Network 17:447–465. doi:10.1080/09548980601064846 pmid:17162463
    OpenUrlCrossRefPubMed
  49. ↵
    Rowland DC, Roudi Y, Moser MB, Moser EI (2016) Ten years of grid cells. Annu Rev Neurosci 39:19–40. doi:10.1146/annurev-neuro-070815-013824 pmid:27023731
    OpenUrlCrossRefPubMed
  50. ↵
    Rozell CJ, Johnson DH, Baraniuk RG, Olshausen BA (2008) Sparse coding via thresholding and local competition in neural circuits. Neural Comput 20:2526–2563. doi:10.1162/neco.2008.03-07-486 pmid:18439138
    OpenUrlCrossRefPubMed
  51. ↵
    Savelli F, Knierim JJ (2010) Hebbian analysis of the transformation of medial entorhinal grid-cell inputs to hippocampal place fields. J Neurophysiol 103:3167–3183. doi:10.1152/jn.00932.2009 pmid:20357069
    OpenUrlCrossRefPubMed
  52. ↵
    Schlesiger MI, Cannova CC, Boublil BL, Hales JB, Mankin EA, Brandon MP, Leutgeb JK, Leibold C, Leutgeb S (2015) The medial entorhinal cortex is necessary for temporal organization of hippocampal neuronal activity. Nat Neurosci 18:1123–1132. doi:10.1038/nn.4056 pmid:26120964
    OpenUrlCrossRefPubMed
  53. ↵
    Skaggs WE, McNaughton BL, Permenter M, Archibeque M, Vogt J, Amaral DG, Barnes CA (2007) EEG sharp waves and sparse ensemble unit activity in the macaque hippocampus. J Neurophysiol 98:898–910. doi:10.1152/jn.00401.2007 pmid:17522177
    OpenUrlCrossRefPubMed
  54. ↵
    Solstad T, Moser EI, Einevoll GT (2006) From grid cells to place cells: a mathematical model. Hippocampus 16:1026–1031. doi:10.1002/hipo.20244 pmid:17094145
    OpenUrlCrossRefPubMed
  55. ↵
    Sorscher B, Mel G, Ganguli S, Ocko S (2019) A unified theory for the origin of grid cells through the lens of pattern formation. Adv Neural Inf Process Syst 32:10003–10013.
    OpenUrl
  56. ↵
    Stensola H, Stensola T, Solstad T, Frøland K, Moser MB, Moser EI (2012) The entorhinal grid map is discretized. Nature 492:72–78. doi:10.1038/nature11649 pmid:23222610
    OpenUrlCrossRefPubMed
  57. ↵
    Steward O, Scoville SA (1976) Cells of origin of entorhinal cortical afferents to the hippocampus and fascia dentata of the rat. J Comp Neurol 169:347–370. doi:10.1002/cne.901690306 pmid:972204
    OpenUrlCrossRefPubMed
  58. ↵
    Tamamaki N (1997) Organization of the entorhinal projection to the rat dentate gyrus revealed by Dil anterograde labeling. Exp Brain Res 116:250–258. doi:10.1007/pl00005753 pmid:9348124
    OpenUrlCrossRefPubMed
  59. ↵
    Tamamaki N, Nojyo Y (1993) Projection of the entorhinal layer II neurons in the rat as revealed by intracellular pressure-injection of neurobiotin. Hippocampus 3:471–480. doi:10.1002/hipo.450030408 pmid:8269038
    OpenUrlCrossRefPubMed
  60. ↵
    Tamamaki N, Nojyo Y (1995) Preservation of topography in the connections between the subiculum, field CA1, and the entorhinal cortex in rats. J Comp Neurol 353:379–390. doi:10.1002/cne.903530306 pmid:7538515
    OpenUrlCrossRefPubMed
  61. ↵
    Thue A (1892) Om nogle geometrisk talteoretiske Theoremer. Fordhl Skand Naturforsk 14:352–353.
    OpenUrl
  62. ↵
    Van Strien N, Cappaert N, Witter M (2009) The anatomy of memory: an interactive overview of the parahippocampal–hippocampal network. Nat Rev Neurosci 10:272–282. doi:10.1038/nrn2614 pmid:19300446
    OpenUrlCrossRefPubMed
  63. ↵
    Wei XX, Prentice J, Balasubramanian V (2015) A principle of economy predicts the functional architecture of grid cells. Elife 4:e08362. doi:10.7554/eLife.08362 pmid:26335200
    OpenUrlCrossRefPubMed
  64. ↵
    Wills TJ, Cacucci F, Burgess N, O’Keefe J (2010) Development of the hippocampal cognitive map in preweanling rats. Science 328:1573–1576. doi:10.1126/science.1188224 pmid:20558720
    OpenUrlAbstract/FREE Full Text
  65. ↵
    Witter MP, Canto CB, Couey JJ, Koganezawa N, O’Reilly KC (2014) Architecture of spatial circuits in the hippocampal region. Philos Trans R Soc Lond B Biol Sci 369:20120515. doi:10.1098/rstb.2012.0515 pmid:24366129
    OpenUrlCrossRefPubMed
  66. ↵
    Yoganarasimha D, Rao G, Knierim JJ (2011) Lateral entorhinal neurons are not spatially selective in cue-rich environments. Hippocampus 21:1363–1374. doi:10.1002/hipo.20839 pmid:20857485
    OpenUrlCrossRefPubMed
  67. ↵
    Zhang SJ, Ye J, Miao C, Tsao A, Cerniauskas I, Ledergerber D, Moser MB, Moser EI (2013) Optogenetic dissection of entorhinal-hippocampal functional connectivity. Science 340:1232627. doi:10.1126/science.1232627 pmid:23559255
    OpenUrlAbstract/FREE Full Text
  68. ↵
    Zhu M, Rozell CJ (2013) Visual nonclassical receptive field effects emerge from sparse coding in a dynamical system. PLoS Comput Biol 9:e1003191. doi:10.1371/journal.pcbi.1003191 pmid:24009491
    OpenUrlCrossRefPubMed
  69. ↵
    Zylberberg J, Murphy J, DeWeese M (2011) A sparse coding model with synaptically local plasticity and spiking neurons can account for the diverse shapes of V1 simple cell receptive fields. PLoS Comput Biol 7:e1002250. doi:10.1371/journal.pcbi.1002250 pmid:22046123
    OpenUrlCrossRefPubMed

Synthesis

Reviewing Editor: Arvind Kumar, KTH Royal Inst of Technology

Decisions are customarily a result of the Reviewing Editor and the peer reviewers coming together and discussing their recommendations until a consensus is reached. When revisions are invited, a fact-based synthesis statement explaining their decision and outlining what is needed to prepare a revision will be listed below. The following reviewer(s) agreed to reveal their identity: Will de Cothi. Note: If this manuscript was transferred from JNeurosci and a decision was made to accept the manuscript without peer review, a brief statement to this effect will instead be what is listed below.

This manuscript was a transfer from J. Neurosci. We managed to get the same reviewers to review the revised version. Both reviewers have agreed that the revised manuscript has addressed all their concerns.

As noted by one of the reviewer, in line 420-421 you have mentioned that data is not shown. You should provide this figure. In addition, there are some typos.

Finally, please provide a more suitable visual abstract.

Author Response

Dear eNeuro Editor,

Please find attached the response to the reviews of our manuscript, “Learning an efficient hippocampal place map from entorhinal inputs using non-negative sparse coding” that was submitted to eNeuro (eN-TNWR-0557-20X).

In response to the comments of Reviewers:

1. A github link to the code is provided but the link is not correct.

•Response: We have corrected the code link and uploaded the code onto it.

2. The figure 3 is suggested as the visual abstract. While this a good illustrative figure, this figure does not constitute visual abstract. Please submit a new figure for this which explains the method and results in a visual manner.

•Response: We have created a visual abstract that visually shows the method and results.

3. In line 420-421 you have mentioned that data is not shown. You should provide this figure.

•Response: We have included another figure to show this, which is Figure 9 in the revised manuscript.

4. There are some typos.

•Response: We have performed a thorough proofreading. Following changes are made:

oThe spelling was changed to be consistent with British spelling.

oSome typos are corrected (see the highlighted revised manuscript).

Thank you for your consideration and we look forward to hearing from you.

Yours sincerely,

Anthony N. Burkitt

On behalf of the authors: Yanbo Lian, Anthony N. Burkitt

Back to top

In this issue

eneuro: 8 (4)
eNeuro
Vol. 8, Issue 4
July/August 2021
Email
Print
View Full Page PDF
Citation Tools
Respond to this article
Learning an Efficient Hippocampal Place Map from Entorhinal Inputs Using Non-Negative Sparse Coding
Yanbo Lian, Anthony N. Burkitt
eNeuro 23 June 2021, 8 (4) ENEURO.0557-20.2021; DOI: 10.1523/ENEURO.0557-20.2021
del.icio.us logo Digg logo Reddit logo Twitter logo Facebook logo Google logo Mendeley logo

Jump to section

Keywords

Responses to this article

Respond to this article

Jump to comment:

No eLetters have been published for this article.

Subjects