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Oakfield Operator Calculus Function Reference Site

Stretched Exponential

For τ>0\tau > 0, α>0\alpha > 0, and tRt \in \mathbb{R},

f(t)=exp ⁣[(tτ)α]f(t) = \exp\!\left[-\left(\frac{|t|}{\tau}\right)^{\alpha}\right]

Defined for real tt (or t0t \ge 0 in time-dependent settings). Output lies in (0,1)(0,1) for t0t \neq 0 and equals 11 at t=0t=0.


f(t)f(t) decays monotonically in t|t|, with characteristic scale set by τ\tau.

f(t)=αταtα1sgn(t)exp ⁣[(tτ)α]f'(t) = -\frac{\alpha}{\tau^{\alpha}} |t|^{\alpha-1} \operatorname{sgn}(t)\, \exp\!\left[-\left(\frac{|t|}{\tau}\right)^{\alpha}\right]

  • α=1\alpha=1 recovers ordinary exponential decay.
  • α=2\alpha=2 yields a Gaussian in tt.
  • As tt\to\infty, f(t)0f(t)\to 0.
  • As α0+\alpha\to 0^+, f(t)e1f(t)\to e^{-1} for t0t\ne 0.

Stretched exponentials interpolate between exponential and Gaussian decay. They are closely connected to fractional dynamics, where memory kernels and anomalous relaxation often produce non-exponential tails.


Oakfield uses stretched-exponential forms as building blocks for fractional-time and colored-noise dynamics:

  • Subordination integrator: the subordination integrator uses a kernel of the form wα(s)exp(sα)w_\alpha(s)\propto \exp(-s^\alpha) in its quadrature rule when approximating subordinated evolution.
  • Stochastic noise: the stochastic_noise operator uses decays like exp((dt/τ)α)\exp(-(dt/\tau)^\alpha) when updating its internal (fractional OU–style) noise state, where α\alpha controls the “color”/memory.

Stretched-exponential relaxation laws appear in 19th-century work by Kohlrausch and were later widely used (often as the KWW form) to model non-exponential relaxation in complex media.

Stretched exponentials serve as flexible empirical decay models and as effective kernels in systems exhibiting heterogeneity or broad distributions of time scales.


  • NIST Digital Library of Mathematical Functions (DLMF), §4
  • Mainardi, Fractional Calculus and Waves in Linear Viscoelasticity