Multiplicative cascade

In mathematics, a multiplicative cascade^{[1] [2]} is a fractal/multifractal distribution of points produced via an iterative and multiplicative random process.

The plots above are examples of multiplicative cascade multifractals.

To create these distributions there are a few steps to take. Firstly, we must create a lattice of cells which will be our underlying probability density field.

Secondly, an iterative process is followed to create multiple levels of the lattice: at each iteration the cells are split into four equal parts (cells). Each new cell is then assigned a probability randomly from the set ${\displaystyle \lbrace p_{1},p_{2},p_{3},p_{4}\rbrace }${\displaystyle \lbrace p_{1},p_{2},p_{3},p_{4}\rbrace } without replacement, where ${\displaystyle p_{i}\in [0,1]}${\displaystyle p_{i}\in [0,1]}. This process is continued to the Nth level. For example, in constructing such a model down to level 8 we produce a 4⁸ array of cells.

Thirdly, the cells are filled as follows: We take the probability of a cell being occupied as the product of the cell's own p_i and those of all its parents (up to level 1). A Monte Carlo rejection scheme is used repeatedly until the desired cell population is obtained, as follows: x and y cell coordinates are chosen randomly, and a random number between 0 and 1 is assigned; the (x, y) cell is then populated depending on whether the assigned number is lesser than (outcome: not populated) or greater or equal to (outcome: populated) the cell's occupation probability.

To produce the plots above, the probability density field is filled with 5,000 points in a space of 256 × 256.

An example of the probability density field:

The fractals are generally not scale-invariant and therefore cannot be considered standard fractals. They can however be considered multifractals. The Rényi (generalized) dimensions can be theoretically predicted. It can be shown ^[3] that as ${\displaystyle N\rightarrow \infty }${\displaystyle N\rightarrow \infty },

${\displaystyle D_{q}={\frac {\log _{2}\left(f_{1}^{q}+f_{2}^{q}+f_{3}^{q}+f_{4}^{q}\right)}{1-q}},}${\displaystyle D_{q}={\frac {\log _{2}\left(f_{1}^{q}+f_{2}^{q}+f_{3}^{q}+f_{4}^{q}\right)}{1-q}},}

where N is the level of the grid refinement and,

${\displaystyle f_{i}={\frac {p_{i}}{\sum _{i}p_{i}}}.}${\displaystyle f_{i}={\frac {p_{i}}{\sum _{i}p_{i}}}.}

• Fractal dimension
• Hausdorff dimension
• Scale invariance

• Fractals

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