Hierarchical integrals are the inverse operators of hierarchical derivatives.
Rank \(0\) accumulates additively, rank \(1\) accumulates multiplicatively (relative scale),
and rank \(2\) accumulates in the \(\ln\!\ln\) space (structural / double-exponential form).
Notation rule: we always write derivatives with explicit rank and degree:
\(\;D_r^n\). On this page we focus on the most used case: \(\;D_n^{1}\).
Concept DOI:
10.5281/zenodo.17917302
Version DOI (v1.0.0):
10.5281/zenodo.17917303
The rank-\(n\) hierarchical integral \(\mathcal{I}_n\) is defined as an inverse of the rank-\(n\), degree-1 derivative \(D_n^{1}\) on a suitable domain:
If \(F\) satisfies \(D_n^{1}F=f\), then \(\mathcal{I}_n[f]\) reproduces \(F\) up to a rank-\(n\) constant:
| Rank | “Constant” lives in | Equivalent form |
|---|---|---|
| 0 | \(F\) | \(F + C\) |
| 1 | \(\ln F\) | \(F\cdot C_\times\) where \(C_\times=e^C>0\) |
| 2 | \(\ln(\ln F)\) | \(\ln(\ln F)\mapsto \ln(\ln F)+C\) (structural constant) |
Because higher ranks use iterated logarithms, every integration formula must state its domain.
| Rank | Required conditions | Reason |
|---|---|---|
| 0 | Classical domain of \(f\) | No iterated logs |
| 1 | \(x>0\), and outputs satisfy \(y(x)>0\) | \(\ln x\), \(\ln y\) are used |
| 2 | \(x>1\), and outputs satisfy \(y(x)>1\) | \(\ln(\ln x)\), \(\ln(\ln y)\) must exist |
Since \(D_{1}^{1}y=\dfrac{d\ln y}{d\ln x}\), solving \(D_1^{1}y=f(x)\) gives:
| \(f(x)\) | \(\mathcal{I}_1[f](x)\) | Check |
|---|---|---|
| \(1\) | \(x\) | \(D_{1}^{1}(x)=1\) |
| \(a\) (constant) | \(x^a\) | \(D_{1}^{1}(x^a)=a\) |
| \(\ln x\) | \(\exp\!\big((\ln x)^2/2\big)\) | \(D_{1}^{1}(\cdot)=\ln x\) |
| \(x^k\) | \(\exp\!\big(x^k/k\big)\ \ (k\neq0)\) | \(D_{1}^{1}(\cdot)=x^k\) |
| \(\dfrac{1}{\ln x}\) | \(\ln x\) | \(D_{1}^{1}(\ln x)=\dfrac{1}{\ln x}\) |
Rank-1 integration naturally produces controlled relative growth: power-laws and exponentials appear automatically because the integrator is built in \(\ln\)-space.
Since \(D_{2}^{1}y=\dfrac{d\ln(\ln y)}{d\ln(\ln x)}\), solving \(D_2^{1}y=f(x)\) gives:
| \(f(x)\) | \(\mathcal{I}_2[f](x)\) | Check |
|---|---|---|
| \(1\) | \(x\) | \(D_{2}^{1}(x)=1\) |
| \(a\) (constant) | \(\exp\!\big((\ln x)^a\big)\) (up to a structural constant) | \(D_{2}^{1}(\cdot)=a\) |
| \(\ln\ln x\) | \(\exp\!\big(\exp((\ln\ln x)^2/2)\big)\) | \(D_{2}^{1}(\cdot)=\ln\ln x\) |
| \(\ln x\) | \(\exp(x)\) | \(D_{2}^{1}(e^x)=\ln x\) |
| \((\ln\ln x)^n\) | \(\exp\!\Big(\exp\big((\ln\ln x)^{n+1}/(n+1)\big)\Big)\) | \(D_{2}^{1}(\cdot)=(\ln\ln x)^n\) |
GOSSA AHMED. Hierarchical Calculus — Hierarchical Integrals. Official Website. Zenodo DOI: 10.5281/zenodo.17917302 (2025).