Abelian sandpile model

The Abelian sandpile model, also known as the Bak–Tang–Wiesenfeld model, was the first discovered example of a dynamical system displaying self-organized criticality. It was introduced by Per Bak, Chao Tang and Kurt Wiesenfeld in a 1987 paper.
The model is a cellular automaton. In its original formulation, each site on a finite grid has an associated value that corresponds to the slope of the pile. This slope builds up as "grains of sand" (or "chips") are randomly placed onto the pile, until the slope exceeds a specific threshold value at which time that site collapses transferring sand into the adjacent sites, increasing their slope. Bak, Tang, and Wiesenfeld considered process of successive random placement of sand grains on the grid; each such placement of sand at a particular site may have no effect, or it may cause a cascading reaction that will affect many sites.
The model has since been studied on the infinite lattice, on other (non-square) lattices, and on arbitrary graphs (including directed multigraphs). It is closely related to the dollar game, a variant of the chip-firing game introduced by Biggs.
Definition (rectangular grids).
The sandpile model is a cellular automaton originally defined on a formula_1 rectangular grid ("checkerboard") formula_2 of the standard square lattice formula_3.
To each vertex ("side", "field") formula_4 of the grid, we associate a value ("grains of sand", "slope", "particles") formula_5, with formula_6 referred to as the (initial) configuration of the sandpile.
The dynamics of the automaton at iteration formula_7 are then defined as follows:
The toppling of several vertices during one iteration is referred to as an "avalanche". Every avalanche is guaranteed to eventually stop, i.e. after a finite number of topplings some stable configuration is reached such that the automaton is well defined. Moreover, although there will often be many possible choices for the order in which to topple vertices, the final stable configuration does not depend on the chosen order; this is one sense in which the sandpile is "abelian". Similarly, the number of times each vertex topples during each iteration is also independent of the choice of toppling order.
Definition (undirected finite multigraphs).
To generalize the sandpile model from the rectangular grid of the standard square lattice to an arbitrary undirected finite multigraph formula_23, a special vertex formula_24 called the "sink" is specified that is not allowed to topple. A "configuration" (state) of the model is then a function formula_25 counting the non-negative number of grains on each non-sink vertex. A non-sink vertex formula_26 with 
is unstable; it can be toppled, which sends one of its grains to each of its (non-sink) neighbors:
The cellular automaton then progresses as before, i.e. by adding, in each iteration, one particle to a randomly chosen non-sink vertex and toppling until all vertices are stable.
The definition of the sandpile model given above for finite rectangular grids formula_2 of the standard square lattice formula_3 can then be seen as a special case of this definition: consider the graph formula_23 which is obtained from formula_35 by adding an additional vertex, the sink, and by drawing additional edges from the sink to every boundary vertex of formula_35 such that the degree of every non-sink vertex of formula_37 is four. In this manner, also sandpile models on non-rectangular grids of the standard square lattice (or of any other lattice) can be defined: Intersect some bounded subset formula_38 of formula_39 with formula_3. Contract every edge of formula_3 whose two endpoints are not in formula_42. The single remaining vertex outside of formula_42 then constitutes the sink of the resulting sandpile graph.
Transient and recurrent configurations.
In the dynamics of the sandpile automaton defined above, some stable configurations (formula_44 for all formula_45) appear infinitely often, while others can only appear a finite number of times (if at all). The former are referred to as "recurrent configurations", while the latter are referred to as "transient configurations". The recurrent configurations thereby consist of all stable non-negative configurations which can be reached from any other stable configuration by repeatedly adding grains of sand to vertices and toppling. It is easy to see that the "minimally stable configuration" formula_46, where every vertex carries formula_47 grains of sand, is reachable from any other stable configuration (add formula_48 grains to every vertex). Thus, equivalently, the recurrent configurations are exactly those configurations which can be reached from the minimally stable configuration by only adding grains of sand and stabilizing.
Not every non-negative stable configuration is recurrent. For example, in every sandpile model on a graph consisting of at least two connected non-sink vertices, every stable configuration where both vertices carry zero grains of sand is non-recurrent. To prove this, first note that the addition of grains of sand can only increase the total number of grains carried by the two vertices together. To reach a configuration where both vertices carry zero particles from a configuration where this is not the case thus necessarily involves steps where at least one of the two vertices is toppled. Consider the last one of these steps. In this step, one of the two vertices has to topple last. Since toppling transfers a grain of sand to every neighboring vertex, this implies that the total number of grains carried by both vertices together cannot be lower than one, which concludes the proof.
Sandpile group.
Given a configuration formula_49, formula_50 for all formula_45, toppling unstable non-sink vertices on a finite connected graph until no unstable non-sink vertex remains leads to a unique "stable" configuration formula_52, which is called the "stabilization" of formula_49. Given two stable configurations formula_49 and formula_55, we can define the operation formula_56, corresponding to the vertex-wise addition of grains followed by the stabilization of the resulting sandpile.
Given an arbitrary but fixed ordering of the non-sink vertices, multiple toppling operations, which can e.g. occur during the stabilization of an unstable configuration, can be efficiently encoded by using the graph Laplacian formula_57, where formula_58 is the degree matrix and formula_59 is the adjacency matrix of the graph.
Deleting the row and column of formula_60 corresponding with the sink yields the "reduced graph Laplacian" formula_61. Then, when starting with a configuration formula_49 and toppling each vertex formula_63 a total of formula_64 times yields the configuration formula_65, where formula_66 is the contraction product. Furthermore, if formula_67 corresponds to the number of times each vertex is toppled during the stabilization of a given configuration formula_49, then
In this case, formula_67 is referred to as the "toppling" or "odometer function" (of the stabilization of formula_49).
Under the operation formula_72, the set of recurrent configurations forms an abelian group isomorphic to the cokernel of the reduced graph Laplacian formula_61, i.e. to formula_74, whereby formula_75 denotes the number of vertices (including the sink). More generally, the set of stable configurations (transient and recurrent) forms a commutative monoid under the operation formula_72. The minimal ideal of this monoid is then isomorphic to the group of recurrent configurations.
The group formed by the recurrent configurations, as well as the group formula_74 to which the former is isomorphic, is most commonly referred to as the "sandpile group". Other common names for the same group are "critical group", "Jacobian group" or (less often) "Picard group". Note, however, that some authors only denote the group formed by the recurrent configurations as the sandpile group, while reserving the name Jacobian group or critical group for the (isomorphic) group defined by formula_74 (or for related isomorphic definitions). Finally, some authors use the name Picard group to refer to the direct product of the sandpile group and formula_79, which naturally appears in a cellular automaton closely related to the sandpile model, referred to as the chip firing or dollar game.
Given the isomorphisms stated above, the order of the sandpile group is the determinant of formula_61, which by the matrix tree theorem is the number of spanning trees of the graph.
Self-organized criticality.
The original interest behind the model stemmed from the fact that in simulations on lattices, it is attracted to its critical state, at which point the correlation length of the system and the correlation time of the system go to infinity, without any fine tuning of a system parameter. This contrasts with earlier examples of critical phenomena, such as the phase transitions between solid and liquid, or liquid and gas, where the critical point can only be reached by precise tuning (e.g., of temperature). Hence, in the sandpile model we can say that the criticality is self-organized.
Once the sandpile model reaches its critical state there is no correlation between the system's response to a perturbation and the details of a perturbation. Generally this means that dropping another grain of sand onto the pile may cause nothing to happen, or it may cause the entire pile to collapse in a massive slide. The model also displays 1/"ƒ" noise, a feature common to many complex systems in nature.
This model only displays critical behaviour in two or more dimensions. The sandpile model can be expressed in 1D; however, instead of evolving to its critical state, the 1D sandpile model instead reaches a minimally stable state where every lattice site goes toward the critical slope.
For two dimensions, it has been hypothesized that the associated conformal field theory consists of symplectic fermions with a central charge "c" = −2.
Properties.
Least action principle.
The stabilization of chip configurations obeys a form of "least action principle": each vertex topples no more than necessary in the course of the stabilization. 
This can be formalized as follows. Call a sequence of topples "legal" if it only topples unstable vertices, and "stabilizing" if it results in a stable configuration. The standard way of stabilizing the sandpile is to find a maximal legal sequence; i.e., by toppling so long as it is possible. Such a sequence is obviously stabilizing, and the Abelian property of the sandpile is that all such sequences are equivalent up to permutation of the toppling order; that is, for any vertex formula_63, the number of times formula_63 topples is the same in all legal stabilizing sequences. According to the least action principle, a minimal stabilizing sequence is also equivalent up to permutation of the toppling order to a legal (and still stabilizing) sequence. In particular, the configuration resulting from a minimal stabilizing sequence is the same as results from a maximal legal sequence.
More formally, if formula_83 is a vector such that formula_84 is the number of times the vertex formula_63 topples during the stabilization (via the toppling of unstable vertices) of a chip configuration formula_49, and formula_87 is an integral vector (not necessarily non-negative) such that formula_88 is stable, then formula_89 for all vertices formula_63.
Scaling limits.
The animation shows the recurrent configuration corresponding to the identity of the sandpile group on different formula_91 square grids of increasing sizes formula_92, whereby the configurations are rescaled to always have the same physical dimension. Visually, the identities on larger grids seem to become more and more detailed and to "converge to a continuous image". Mathematically, this suggests the existence of scaling-limits of the sandpile identity on square grids based on the notion of weak-* convergence (or some other, generalized notion of convergence). Indeed, existence of scaling limits of recurrent sandpile configurations has been proved by Wesley Pegden and Charles Smart
. In further joint work with Lionel Levine, they use the scaling limit to explain the fractal structure of the sandpile on square grids.
Generalizations and related models.
Sandpile models on infinite grids.
There exist several generalizations of the sandpile model to infinite grids. A challenge in such generalizations is that, in general, it is not guaranteed anymore that every avalanche will eventually stop. Several of the generalization thus only consider the stabilization of configurations for which this can be guaranteed.
A rather popular model on the (infinite) square lattice with sites formula_93 is defined as follows:
Begin with some nonnegative configuration of values formula_94 which is finite, meaning
Any site formula_96 with
is "unstable" and can "topple" (or "fire"), sending one of its chips to each of its four neighbors:
Since the initial configuration is finite, the process is guaranteed to terminate, with the grains scattering outward.
A popular special case of this model is given when the initial configuration is zero for all vertices except the origin. If the origin carries a huge number of grains of sand, the configuration after relaxation forms fractal patterns (see figure). When letting the initial number of grains at the origin go to infinity, the rescaled stabilized configurations were shown to converge to a unique limit.
Sandpile models on directed graphs.
The sandpile model can be generalized to arbitrary directed multigraphs. The rules are that any vertex formula_63 with 
is unstable; toppling again sends chips to each of its neighbors, one along each outgoing edge:
and, for each formula_104:
where formula_106 is the number of edges from formula_63 to formula_108.
In this case the Laplacian matrix is not symmetric. If we specify a sink formula_109 such that there is a path from every other vertex to formula_109, then the stabilization operation on finite graphs is well-defined and the sandpile group can be written
as before.
The order of the sandpile group is again the determinant of formula_61, which by the general version of the matrix tree theorem is the number of oriented spanning trees rooted at the sink.
The extended sandpile model.
To better understand the structure of the sandpile group for different finite convex grids formula_2 of the standard square lattice formula_3, Lang and Shkolnikov introduced the "extended sandpile model" in 2019. The extended sandpile model is defined nearly exactly the same as the "usual sandpile model" (i.e. the original Bak–Tang–Wiesenfeld model ), except that vertices at the boundary formula_115 of the grid are now allowed to carry a non-negative real number of grains. In contrast, vertices in the interior of the grid are still only allowed to carry integer numbers of grains. The toppling rules remain unchanged, i.e. both interior and boundary vertices are assumed to become unstable and topple if the grain number reaches or exceeds four.
Also the recurrent configurations of the extended sandpile model form an abelian group, referred to as the "extended sandpile group", of which the usual sandpile group is a discrete subgroup. Different to the usual sandpile group, the extended sandpile group is however a continuous Lie group. Since it is generated by only adding grains of sand to the boundary formula_115 of the grid, the extended sandpile group furthermore has the topology of a torus of dimension formula_117 and a volume given by the order of the usual sandpile group.
Of specific interest is the question how the recurrent configurations dynamically change along the continuous geodesics of this torus passing through the identity. This question leads to the definition of the sandpile dynamics
respectively 
induced by the integer-valued harmonic function formula_120 at time formula_121, with formula_122 the identity of the sandpile group and formula_123 the floor function. 
For low-order polynomial harmonic functions, the sandpile dynamics are characterized by the
smooth transformation and apparent conservation of the patches
constituting the sandpile identity. For example, the harmonic dynamics induced by formula_124 resemble the "smooth stretching" of the identity along the main diagonals visualized in the animation. The configurations appearing in the dynamics induced by the same harmonic function on square grids of different sizes were furthermore conjectured to weak-* converge, meaning that there supposedly exist scaling limits for them. This proposes a natural renormalization for the extended and usual sandpile groups, meaning a mapping of recurrent configurations on a given grid to recurrent configurations on a sub-grid. Informaly, this renormalization simply maps configurations appearing at a given time formula_125 in the sandpile dynamics induced by some harmonic function formula_120 on the larger grid to the corresponding configurations which appear at the same time in the sandpile dynamics induced by the restriction of formula_120 to the respective sub-grid.
The divisible sandpile.
A strongly related model is the so called divisible sandpile model, introduced by Levine and Peres in 2008, in which, instead of a discrete number of particles in each site formula_128, there is a real number formula_129 representing the amount of mass on the site. In case such mass is negative, one can understand it as a hole. The topple occurs whenever a site has mass larger than 1; it topples the excess evenly between its neighbors resulting in the situation that, if a site is full at time formula_125, it will be full for all later times.
Cultural references.
The Bak–Tang–Wiesenfeld sandpile was mentioned on the Numb3rs episode "Rampage," as mathematician Charlie Eppes explains to his colleagues a solution to a criminal investigation.
The computer game Hexplode is based around the Abelian sandpile model on a finite hexagonal grid where instead of random grain placement, grains are placed by players.