Infinity Laplacian
In mathematics, the infinity Laplace (or  -Laplace) operator is a 2nd-order partial differential operator, commonly abbreviated . It is alternately defined by

or

The first version avoids the singularity which occurs when the gradient vanishes, while the second version is homogeneous of order zero in the gradient. Verbally, the second version is the second derivative in the direction of the gradient. In the case of the infinity Laplace equation , the two definitions are equivalent. While the equation involves second derivatives, usually (generalized) solutions are not twice differentiable, as evidenced by the well-known Aronsson solution . For this reason the correct notion of solutions is that given by the viscosity solutions. Viscosity solutions to the equation  are also known as infinity harmonic functions. This terminology arises from the fact that the infinity Laplace operator first arose in the study of absolute minimizers for , and it can be viewed in a certain sense as the limit of the p-Laplacian as . More recently, viscosity solutions to the infinity Laplace equation have been identified with the payoff functions from randomized tug-of-war games. The game theory point of view has significantly improved the understanding of the partial differential equation itself. Discrete version and game theory

A defining property of the usual -harmonic functions is the mean value property. That has a natural and important discrete version: a real-valued function  on a finite or infinite graph  is discrete harmonic on a subset  if 
 
for all . Similarly, the vanishing second derivative in the direction of the gradient has a natural discrete version:

. In this equation, we used sup and inf instead of max and min because the graph  does not have to be locally finite (i.e., to have finite degrees): a key example is when  is the set of points in a domain in , and  if their Euclidean distance is at most . The importance of this example lies in the following. Consider a bounded open set  with smooth boundary , and a continuous function . In the -case, an approximation of the harmonic extension of f to D is given by taking a lattice  with small mesh size , letting  and  be the set of vertices with degree less than 2d, taking a natural approximation , and then taking the unique discrete harmonic extension of  to V. However, it is easy to see by examples that this does not work for the -case. Instead, as it turns out, one should take the continuum graph with all edges of length at most , mentioned above. Now, a probabilistic way of looking at the -harmonic extension of  from  to  is that 
,
where  is the simple random walk on  started at , and  is the hitting time of . For the -case, we need game theory. A token is started at location , and  is given. There are two players, in each turn they flip a fair coin, and the winner can move the token to any neighbour of the current location. The game ends when the token reaches  at some time  and location , at which point the first player gets the amount  from the second player. Therefore, the first player wants to maximize , while the second player wants to minimize it. If both players play optimally (which has a well-defined meaning in game theory), the expected payoff  to the first player is a discrete infinity harmonic function, as defined above. There is a game theory approach to the p-Laplacian, too, interpolating between simple random walk and the above random tug-of-war game. Sources

. Differential operators
Elliptic partial differential equations