Mathematics of Control, Signals, and Systems

, Volume 26, Issue 3, pp 339–374

# A compendium of comparison function results

• Christopher M. Kellett
Open Access
Original Article

## Abstract

The use of comparison functions has become standard in systems and control theory, particularly for the purposes of studying stability properties. The use of these functions typically allows elegant and succinct statements of stability properties such as asymptotic stability and input-to-state stability and its several variants. Furthermore, over the last 20 years several inequalities involving these comparison functions have been developed that simplify their manipulation in the service of proving more significant results. Many of these inequalities have appeared in the body of proofs or in appendices of various papers. Our goal herein is to collect these inequalities in one place.

## Keywords

Comparison functions Stability theory Nonlinear systems

## 1 History

Jose Massera appears to have been the first scholar to introduce comparison functions to the study of stability theory in 1956 [26]. In particular, to elegantly capture the notion of (local) positive definiteness he relied on a function $$a: \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ with

$$a(r)$$ being continuous and increasing when $$r > 0$$, $$a(0) = 0$$.”

To further describe a function having an infinitely small upper bound, he then used a function $$b: \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ “having the same properties of $$a(r)$$”.1

In his 1959 manuscript, Wolfgang Hahn [11] termed such functions as class-$$\mathcal {K}$$ functions2 and also introduced the terminology “decrescent” for what Lyapunov had originally termed “an infinitely small upper limit” [24]. However, in what remains a remarkably modern text, it was in his 1967 manuscript [12] where Hahn not only introduced the additional function classes of class-$$\mathcal {L}$$ and class-$$\mathcal {KL}$$, but also made significant use of these comparison functions and their properties.

Following Hahn’s text, functions of class-$$\mathcal {K}$$ appeared occasionally in works through the 1970s and 1980s. However, the use of these functions was largely limited to the characterization of positive definite and decrescent functions and the properties that Hahn elucidated in [12] were essentially ignored [21, 32, 34, 41, 42].

Sontag’s seminal 1989 paper [35] introducing the notion of input-to-state stability represented a return to the elegant formulations first presented in [12]. In particular, Sontag took as the definition of global asymptotic stability the formulation involving a class-$$\mathcal {KL}$$ function first proposed in [12, Equation 26.2]. To study systems under the influence of inputs, Sontag then augmented the class-$$\mathcal {KL}$$ formulation of global asymptotic stability with a class-$$\mathcal {K}$$ function of the input.

Since the appearance of [35], the use of comparison functions in the analysis of stability and robustness for nonlinear systems has become standard. Many useful inequalities and other relationships have been developed for comparison functions. Unfortunately, these results tend to be reported in appendices or within the context of proving some larger results relating to stability or robustness. Our goal here is a modest one: to collect some of the most useful comparison function inequalities and relationships in one place.

The manuscript is organized as follows: in Sect. 2 we provide the standard comparison function definitions and review some well-known facts. In Sect. 3, we provide lemmas that give upper bounds on a given comparison function. By contrast, in Sect. 4, we provide lemmas that give lower bounds on a given function. Section 5 provides lemmas on differential inequalities involving comparison functions. In an overlap of terminology that should cause no confusion, these lemmas are frequently referred to as comparison lemmas. In Sect. 6, we provide some other useful relationships involving comparison functions. In Sect. 7, we briefly mention a few recently defined function classes that we believe are likely to be more widely used in the future. Finally, in Sect. 8 we discuss a generalization of class-$$\mathcal {K}$$ functions, termed monotone aggregation functions, that are defined on $$\mathbb {R}^n_{\ge 0}$$ rather than $$\mathbb {R}_{\ge 0}$$. For the purpose of illustrating some of the proof techniques, proofs of selected results are included in the Appendix.

## 2 Definitions and obvious facts

In what follows, we denote integers by $$\mathbb {Z}$$ and real numbers by $$\mathbb {R}$$. Restrictions to subsets of $$\mathbb {Z}$$ or $$\mathbb {R}$$ will be denoted by subscripts such as $$\mathbb {R}_{\ge 0} \subset \mathbb {R}$$ for the nonnegative real half-line or by the standard notation $$[a,b) \subset \mathbb {R}$$ for the half-open interval. We denote $$n$$-dimensional Euclidean space by $$\mathbb {R}^n$$ and use $$|\cdot |$$ to denote the norm. We will use both parenthesis and the symbol $$\circ$$ to denote function composition; i.e., for functions $$\alpha _1,\alpha _2 : \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$, we will use either $$\alpha _1(\alpha _2(s))$$ or $$\alpha _1 \circ \alpha _2(s)$$ for all $$s \in \mathbb {R}_{\ge 0}$$, where the choice is always made to improve readability.

As previously mentioned, Hahn3 first defined functions of class-$$\mathcal {K}$$ in [11], though such functions had been previously used in stability analysis by Massera in [26]. In [12, Defn 2.5] this definition is immediately used to define the notion of a stable equilibrium point rather than as a precursor to using such functions to characterize positive definiteness (as done in [11, 26, 32, 41]).

### Definition 1

A function $$\alpha : \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ is said to be of class-$$\mathcal {K}$$ ($$\alpha \in \mathcal {K}$$) if it is continuous, zero at zero, and strictly increasing. For some $$a \in \mathbb {R}_{>0}$$, a function $$\alpha : [0,a) \rightarrow \mathbb {R}_{\ge 0}$$ is said to be of class-$$\mathcal {K}_{[0,a)},$$ if it is continuous, zero at zero, and strictly increasing.

As cited in the introduction, the first use of class-$$\mathcal {K}$$ functions was to characterize the concept of a locally positive definite function. To see that this is indeed the case, we follow the same argument as [12]. A positive definite function is understood as a function that is zero at the origin, and (strictly) positive at every other point. Given, then, a continuous locally positive definite function $$\rho :\mathbb {R}^n \rightarrow \mathbb {R}_{\ge 0}$$ on a closed ball of radius $$c$$ (denoted by $$\overline{\mathcal {B}}_c \subset \mathbb {R}^n$$), we can define a continuous nondecreasing function $$\hat{\alpha }: \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ by
\begin{aligned} \hat{\alpha }(s) \doteq \min _{\{x \in \overline{\mathcal {B}}_c : |x| \ge s\} } \rho (x), \quad \forall s \in [0,c]. \end{aligned}
Since $$\hat{\alpha }(s)$$ is strictly positive for $$(0,c]$$, it is possible to lower bound this nondecreasing function by one that is strictly increasing to obtain the desired result. Note that globally positive definite continuous functions that satisfy $$\lim _{s \rightarrow \infty } \rho (s) = 0$$ cannot be bounded from below by a class-$$\mathcal {K}$$ function. A comparison function lower bound for globally positive definite continuous functions is presented in Lemma 18.

Hahn [11] introduced the term radially unbounded and in [12] characterized a radially unbounded function as one that is lower bounded by a class-$$\mathcal {K}$$ function that approaches infinity as its argument approaches infinity. Hahn cites [4] for introducing the same notion under the terminology “$$\alpha$$ becomes infinitely large”. Sontag [35] introduced the now standard notation $$\mathcal {K}_{\infty }$$ for such functions.4

### Definition 2

A function $$\alpha : \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ is said to be of class-$$\mathcal {K}_{\infty }$$ ($$\alpha \in \mathcal {K}_{\infty }$$) if $$\alpha \in \mathcal {K}$$ and, in addition, $$\displaystyle \lim \nolimits _{s \rightarrow \infty } \alpha (s) = \infty$$.

One of the most useful properties of class-$$\mathcal {K}$$ and class-$$\mathcal {K}_{\infty }$$ functions is their invertibility. First consider $$\alpha \in \mathcal {K}\backslash \mathcal {K}_{\infty }$$; i.e., $$\alpha \in \mathcal {K}$$ but $$\alpha \notin \mathcal {K}_{\infty }$$. Since $$\alpha \in \mathcal {K}\backslash \mathcal {K}_{\infty }$$ is continuous and strictly increasing there exists a constant $$a \in \mathbb {R}_{>0}$$ such that $$\lim _{s \rightarrow \infty } \alpha (s) = a$$, the inverse function exists on $$[0,a)$$, and the inverse function is also continuous and strictly increasing; i.e., the function $$\alpha ^{-1}: [0,a) \rightarrow \mathbb {R}_{\ge 0}$$ is continuous, zero at zero, strictly increasing, and hence of class-$$\mathcal {K}_{[0,a)}$$. The inverse function also satisfies $$\lim _{s \rightarrow a} \alpha ^{-1}(s) = \infty$$. In the case where $$\alpha \in \mathcal {K}_{\infty }$$, we observe that the inverse function will be defined globally and consequently $$\alpha ^{-1} \in \mathcal {K}_{\infty }$$. We thus observe that class-$$\mathcal {K}_{\infty }$$ functions are the set of homeomorphisms on the nonnegative real half-line, $$\mathbb {R}_{\ge 0}$$.

Hahn [12] observed that if $$\alpha _1, \alpha _2 \in \mathcal {K}_{\infty }$$ and if $$\alpha _1(s) \le \alpha _2(s)$$ for all $$s \in \mathbb {R}_{\ge 0}$$, then $$\alpha _1^{-1}(s) \ge \alpha _2^{-1}(s)$$. This is straightforward to see by considering $$r = \alpha _1(s)$$ in the first inequality. This property also holds for two class-$$\mathcal {K}$$ functions, though only on $$[0,a)$$ where $$a = \lim _{s \rightarrow \infty } \min \{\alpha _1(s), \alpha _2(s)\}$$.

Three further useful and straightforward properties are related to the sum, maximum, or minimum of class-$$\mathcal {K}$$ functions. Suppose we have a finite number of functions $$\alpha _i \in \mathcal {K}$$ where $$i \in \{1, \ldots , N\}$$ for some finite $$N \in \mathbb {Z}_{>0}$$. Then, the function $$\alpha : \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ defined by any of
\begin{aligned} \begin{aligned} \alpha (s)&\doteq \sum _{i=1}^N \alpha _i(s) , \\ \alpha (s)&\doteq \max _{i \in \{1, \ldots , N\}} \alpha _i(s), \quad \mathrm{or} \\ \alpha (s)&\doteq \min _{i \in \{1, \ldots , N\}} \alpha _i(s), \end{aligned} \end{aligned}
for all $$s \in \mathbb {R}_{\ge 0}$$ is of class-$$\mathcal {K}$$. Furthermore, for the summation or maximum, if $$\alpha _i \in \mathcal {K}_{\infty }$$ for any $$i \in \{1, \ldots , N\}$$, then $$\alpha \in \mathcal {K}_{\infty }$$. Note that maximization and summation are specific instances of the monotone aggregation functions discussed in Sect. 8.

Hahn introduced class-$$\mathcal {L}$$ functions in [12, Defn 2.6] as a precursor to defining attractivity of an equilibrium point.

### Definition 3

A function $$\sigma :\mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{> 0}$$ is said to be of class-$$\mathcal {L}$$ ($$\sigma \in \mathcal {L}$$), if it is continuous, strictly decreasing,5 and $$\displaystyle \lim \nolimits _{s \rightarrow \infty } \sigma (s) = 0$$.

Note that, similar to class-$$\mathcal {K}$$ functions, functions of class-$$\mathcal {L}$$ are invertible on their range and the inverse is itself (nearly) class-$$\mathcal {L}$$ on the range of the original function; i.e., for $$\sigma \in \mathcal {L}$$, the inverse $$\sigma ^{-1}:(0,\sigma (0)] \rightarrow \mathbb {R}_{\ge 0}$$ is continuous, strictly decreasing, and $$\lim _{s \rightarrow 0} \sigma ^{-1}(s) = +\infty$$.

In [12, Section 24], Hahn noted two somewhat obvious facts about the composition of comparison functions. Suppose $$\alpha , \alpha _1, \alpha _2 \in \mathcal {K}$$ and $$\sigma \in \mathcal {L}$$. Then
\begin{aligned} \begin{array}{l} \alpha _1 \circ \alpha _2 \in \mathcal {K}; \ \mathrm{and} \\ \alpha \circ \sigma \in \mathcal {L}. \end{array} \end{aligned}
In addition, we observe that for $$\sigma _1, \sigma _2 \in \mathcal {L}$$ and with $$c \doteq \sigma _1 \circ \sigma _2(0)$$ we have
\begin{aligned} \sigma _1 \circ \sigma _2 - c \in \mathcal {K}. \end{aligned}
As a final definition, Hahn [12, Defn 24.2] introduced the class of $$\mathcal {KL}$$ functions:

### Definition 4

A function $$\beta : \mathbb {R}_{\ge 0} \times \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ is said to be of class-$$\mathcal {KL}$$ ($$\beta \in \mathcal {KL}$$) if it is class-$$\mathcal {K}$$ in its first argument and class-$$\mathcal {L}$$ in its second argument. In other words, $$\beta \in \mathcal {KL}$$ if for each fixed $$t \in \mathbb {R}_{\ge 0}$$, $$\beta (\cdot ,t) \in \mathcal {K}$$ and for each fixed $$s \in \mathbb {R}_{\ge 0}$$, $$\beta (s,\cdot ) \in \mathcal {L}$$.

For consistency, we will generally use $$\alpha$$ or $$\varphi$$ for functions of class-$$\mathcal {K}$$ or class-$$\mathcal {K}_{\infty }$$, $$\sigma$$ for functions of class-$$\mathcal {L}$$, $$\beta$$ for functions of class-$$\mathcal {KL}$$, $$\rho$$ for positive definite functions, and $$a,b,c$$, or $$\lambda$$ for positive constants in $$\mathbb {R}_{>0}$$. For functions $$\alpha \in \mathcal {K}$$ that are differentiable, we will denote the derivative by $$\alpha '$$. We will denote the identity function by $$\mathrm{id}$$; i.e., $$\mathrm{id}(s) = s$$ for all $$s \in \mathbb {R}_{\ge 0}$$.

### 2.1 Example: Lyapunov functions and $$\mathcal {KL}$$-stability

As a brief example of the elegance enabled by the use of comparison functions, we demonstrate the proof that a Lyapunov function implies uniform global asymptotic stability of the origin for an autonomous system
\begin{aligned} \dot{x} = f(x). \end{aligned}
Here, we assume the existence and uniqueness of solutions and denote solutions to the above differential equation from an initial point $$x_0 = x(0) \in \mathbb {R}^n$$ by $$x(t)$$ for all $$t \in \mathbb {R}_{\ge 0}$$.

### Definition 5

The origin is globally asymptotically stable for $$\dot{x} = f(x)$$ if there exists a function $$\beta \in \mathcal {KL}$$ such that, for all $$x_0 \in \mathbb {R}^n$$,
\begin{aligned} |x(t)| \le \beta (|x_0|,t), \quad \forall t \in \mathbb {R}_{\ge 0} . \end{aligned}

It is obvious that the above definition is equivalent to the standard definition of global asymptotic stability as the combination of stability and attractivity (see [22, Proposition 2.5]).

### Definition 6

A Lyapunov function $$V:\mathbb {R}^n \rightarrow \mathbb {R}_{\ge 0}$$ for $$\dot{x} = f(x)$$ is a continuously differentiable function such that there exist $$\alpha _1,\alpha _2 \in \mathcal {K}_{\infty }$$, a continuous positive definite function $$\rho : \mathbb {R}^n \rightarrow \mathbb {R}_{\ge 0}$$ and, for all $$x \in \mathbb {R}^n$$,
\begin{aligned} \alpha _1(|x|) \le V(x) \le \alpha _2(|x|) \end{aligned}
(1)
\begin{aligned} \dot{V}(x) = \langle \nabla V(x), f(x) \rangle \le -\rho (x) . \end{aligned}
(2)
Assume the existence of a Lyapunov function for $$\dot{x}=f(x)$$. Lemma 18 in the sequel yields the existence of $$\alpha \in \mathcal {K}_{\infty }$$ and $$\sigma \in \mathcal {L}$$ such that
\begin{aligned} \rho (x) \ge \alpha (|x|) \sigma (|x|), \quad \forall x \in \mathbb {R}^n. \end{aligned}
(3)
Since the functions $$\alpha _1,\alpha _2 \in \mathcal {K}_{\infty }$$, they are both invertible and we define
\begin{aligned} \hat{\alpha } \doteq \alpha \circ \alpha _2^{-1} \in \mathcal {K}_{\infty }\quad \mathrm{and} \quad \hat{\sigma } \doteq \sigma \circ \alpha _1^{-1} \in \mathcal {L}. \end{aligned}
Finally, we define $$\hat{\rho }:\mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ by
\begin{aligned} \hat{\rho }(s) \doteq \hat{\alpha }(s) \hat{\sigma }(s), \quad \forall s \in \mathbb {R}_{\ge 0} \end{aligned}
(4)
and note that the product of a class-$$\mathcal {K}_{\infty }$$ function and a class-$$\mathcal {L}$$ function is a positive definite function and hence $$\hat{\rho }$$ is a positive definite function. Therefore, using (1), (3), and the definitions of functions $$\hat{\alpha }, \hat{\sigma }$$, and $$\hat{\rho }$$, we may bound the decrease condition (2) as
\begin{aligned} \dot{V}(x) \le - \alpha (|x|)\sigma (|x|) \le - \alpha \left( \alpha _2^{-1}(V(x))\right) \sigma \left( \alpha _1^{-1}(V(x)) \right) = -\hat{\rho }(V(x)). \end{aligned}
(5)
Using a comparison lemma from the sequel (Lemma 20) we have the existence of a function $$\hat{\beta } \in \mathcal {KL}$$ such that, for all $$x(0) = x_0 \in \mathbb {R}^n$$,
\begin{aligned} V(x(t)) \le \hat{\beta } (V(x_0),t), \quad \forall t \in \mathbb {R}_{\ge 0}. \end{aligned}
By manipulating the upper and lower bounds in (1) we obtain
\begin{aligned} |x(t)| \le \alpha _1^{-1}\left( \hat{\beta }\left( \alpha _2(|x_0|),t \right) \right) \doteq \beta (|x_0|,t), \end{aligned}
for all $$t \in \mathbb {R}_{\ge 0}$$ and $$x_0 \in \mathbb {R}^n$$, proving global asymptotic stability of the origin.
Furthermore, we note that any nonlinear scaling of a Lyapunov function by a continuously differentiable function $$\bar{\alpha }\in \mathcal {K}_{\infty }$$ satisfying $$\bar{\alpha }'(s) > 0$$ for all $$s \in \mathbb {R}_{>0}$$ yields a Lyapunov function6. To see this, given a Lyapunov function $$V$$, functions $$\alpha _1,\alpha _2 \in \mathcal {K}_{\infty }$$ and a continuous positive definite function $$\rho : \mathbb {R}^n \rightarrow \mathbb {R}_{\ge 0}$$ so that (1) and (2) hold, define
\begin{aligned} W(x) \doteq \bar{\alpha }(V(x)), \quad \forall x \in \mathbb {R}^n . \end{aligned}
We define $$\hat{\alpha }_1 \doteq \bar{\alpha }\circ \alpha _1 \in \mathcal {K}_{\infty }$$ and $$\hat{\alpha }_2 \doteq \bar{\alpha }\circ \alpha _2 \in \mathcal {K}_{\infty }$$ and see that (1) implies that $$W$$ satisfies the necessary upper and lower bounds
\begin{aligned} \hat{\alpha }_1(|x|) \le W(x) \le \hat{\alpha }_2(|x|), \quad \forall x \in \mathbb {R}^n. \end{aligned}
Since $$\bar{\alpha }\in \mathcal {K}_{\infty }$$ is continuously differentiable and $$\bar{\alpha }'(s) > 0$$ for all $$s \in \mathbb {R}_{>0}$$, we have
\begin{aligned} \langle \nabla W(x), f(x) \rangle = \bar{\alpha }'(V(x)) \langle \nabla V(x), f(x) \rangle \le -\bar{\alpha }'(V(x)) \rho (x) \end{aligned}
(6)
for all $$x \in \mathbb {R}^n \backslash \{0\}$$, where the right-hand side is a continuous positive definite function. In other words, the function $$W(x) = \bar{\alpha }(V(x))$$ is a Lyapunov function for any continuously differentiable $$\bar{\alpha }\in \mathcal {K}_{\infty }$$.
Finally, let the continuous positive definite function $$\hat{\rho }: \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ be defined as in (4) so that we have the decrease condition (5). Then for $$\hat{\rho }$$, Lemma 24 in the sequel yields an $$\bar{\alpha }\in \mathcal {K}_{\infty }$$ that is continuously differentiable on $$\mathbb {R}_{>0}$$ such that
\begin{aligned} \bar{\alpha }(s) \le \hat{\rho }(s) \bar{\alpha }'(s), \quad \forall s \in \mathbb {R}_{>0}. \end{aligned}
Repeating the calculations of (5) and (6) we see that, for $$W(x) \doteq \bar{\alpha }(V(x))$$ we have
\begin{aligned} \dot{W}(x) = \langle \nabla W(x), f(x) \rangle \le -\bar{\alpha }'(V(x))\hat{\rho }(x) \le - \bar{\alpha }(V(x)) = - W(x) \end{aligned}
for all $$x \in \mathbb {R}^n \backslash \{0\}$$. In other words, the Lyapunov function $$W(x) = \bar{\alpha }(V(x))$$ decreases exponentially.

### 2.2 A word on regularity

Since class-$$\mathcal {K}$$ and class-$$\mathcal {L}$$ functions are monotonic, a theorem due to Lebesgue states that these functions must be differentiable almost everywhere (see, for example, [31, Section 2]) and this property holds without the functions necessarily being continuous.

While we have assumed that functions of class-$$\mathcal {K}$$ or class-$$\mathcal {L}$$ are continuous functions, it is sometimes useful to require functions with more regularity; for example, when discussing the nonlinear scaling of Lyapunov functions in the previous section we required the nonlinear scaling $$\alpha \in \mathcal {K}_{\infty }$$ to be continuously differentiable. In fact, we can always bound comparison functions from above and below by smooth functions on $$\mathbb {R}_{>0}$$. We here state [5, Lemma 2.5] as two lemmas to separately state the results for nondecreasing and nonincreasing functions.

### Lemma 1

Let $$\alpha : \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ be continuous, zero at zero, strictly positive on $$\mathbb {R}_{>0}$$, and nondecreasing. Then there exist functions $$\alpha _1, \alpha _2 \in \mathcal {K}$$, smooth on $$\mathbb {R}_{>0}$$, so that
\begin{aligned} \alpha _1(s) \le \alpha (s) \le \alpha _2(s), \quad \forall s \in \mathbb {R}_{\ge 0}. \end{aligned}
Furthermore, if $$\lim _{s \rightarrow \infty } \alpha (s) = \infty$$ then both functions may be chosen to satisfy $$\alpha _1, \alpha _2 \in \mathcal {K}_{\infty }$$.

### Lemma 2

Let $$\sigma : \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{>0}$$ be continuous, nonincreasing, and satisfying $$\lim _{s \rightarrow \infty } \sigma (s) = 0$$. Then, there exist functions $$\sigma _1, \sigma _2 \in \mathcal {L}$$, smooth on $$\mathbb {R}_{>0}$$, so that
\begin{aligned} \sigma _1(s) \le \sigma (s) \le \sigma _2(s), \quad \forall s \in \mathbb {R}_{\ge 0}. \end{aligned}

In contrast to the above results, when we assume that the function we wish to approximate is of class-$$\mathcal {K}$$ or class-$$\mathcal {L}$$, we may additionally control how close the smooth function is to the given function.

### Lemma 3

For $$\alpha \in \mathcal {K}$$ and any $$\varepsilon >0$$ there exist $$\alpha _1,\alpha _2 \in \mathcal {K}$$, smooth on $$\mathbb {R}_{>0}$$, so that, for all $$s \in \mathbb {R}_{\ge 0}$$
\begin{aligned} \alpha (s) - \varepsilon < \alpha _1(s) \le \alpha (s) \le \alpha _2(s) < \alpha (s) + \varepsilon . \end{aligned}
(7)

### Lemma 4

For $$\sigma \in \mathcal {L}$$ and any $$\varepsilon > 0$$ there exist $$\sigma _1, \sigma _2 \in \mathcal {K}_{\infty }$$, smooth on $$\mathbb {R}_{>0}$$ so that, for all $$s \in \mathbb {R}_{\ge 0}$$
\begin{aligned} \sigma (s) - \varepsilon < \sigma _1(s) \le \sigma (s) \le \sigma _2(s) \le \sigma (s) + \varepsilon . \end{aligned}

With a further requirement that the given function be of class-$$\mathcal {K}_{\infty }$$, we obtain the following two smooth approximation lemmas.

### Lemma 5

[9, Lemma B.2.1] Given $$\alpha \in \mathcal {K}_{\infty }$$ and $$\rho :\mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ is continuous and positive definite, there exists $$\tilde{\alpha }\in \mathcal {K}_{\infty }$$, smooth on $$\mathbb {R}_{>0}$$, so that
\begin{aligned} |\alpha (s) - \tilde{\alpha }(s)| \le \rho (\alpha (s)), \quad \forall s \in \mathbb {R}_{\ge 0}. \end{aligned}

### Lemma 6

[9, Lemma B.2.2] Given $$\alpha \in \mathcal {K}_{\infty }$$ and $$\rho :\mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ is continuous and positive definite, there exists $$\alpha _1,\alpha _2 \in \mathcal {K}_{\infty }$$, smooth on $$\mathbb {R}_{>0}$$, so that, for all $$s \in \mathbb {R}_{\ge 0}$$,
\begin{aligned} \alpha (s) - \rho (\alpha (s)) \le \alpha _1(s) < \alpha (s) < \alpha _2(s) \le \alpha (s) + \rho (\alpha (s)) . \end{aligned}

The proofs of all of the lemmas in this section follow a similar idea where a continuous piecewise linear function is constructed to bound the given function from above or below while giving the additional desired inequalities. Standard techniques can then be used to smooth these functions where they are pieced together. As an example, and because we have not seen the result previously in the literature, we present the proof of Lemma 3 in Appendix A.1 and provide a remark on the necessary modifications to obtain Lemma 4.

## 3 Upper bounds

Arguably the most useful lemma regarding $$\mathcal {KL}$$-functions is widely known as Sontag’s Lemma on $$\mathcal {KL}$$-Estimates which originally appeared as [36, Proposition 7]. The version given here is from [19] and provides some nice properties on one of the resulting $$\mathcal {K}_{\infty }$$ functions. The proof is provided in Appendix A.2.

### Lemma 7

[19, Lemma 5.3] Given $$\beta \in \mathcal {KL}$$ and $$\lambda \in \mathbb {R}_{>0}$$, there exist $$\alpha _1, \alpha _2 \in \mathcal {K}_{\infty }$$ such that $$\alpha _1(\cdot )$$ is Lipschitz on its domain, smooth on $$\mathbb {R}_{>0}$$, $$\alpha _1(s) \le s\alpha _1'(s)$$ for all $$s \in \mathbb {R}_{>0}$$ and
\begin{aligned} \alpha _1 \left( \beta (s,t)\right) \le \alpha _2(s)e^{-\lambda t}, \quad \forall (s,t) \in \mathbb {R}_{\ge 0} \times \mathbb {R}_{\ge 0}. \end{aligned}

A precursor to the above result was presented by Hahn [12]:

### Lemma 8

Let $$\alpha _1, \alpha _2 \in \mathcal {K}$$, $$\sigma \in \mathcal {L}$$, and either $$\alpha _1'$$ or $$\alpha _2$$ be bounded. Then, there exist $$\hat{\alpha } \in \mathcal {K}$$ and $$\hat{\sigma } \in \mathcal {L}$$ such that
\begin{aligned} \alpha _1 \left( \alpha _2(s) \sigma (t) \right) \le \hat{\alpha }(s) \hat{\sigma }(t), \quad \forall s,t \in \mathbb {R}_{\ge 0}. \end{aligned}

### Proof

If there exists a $$c \in \mathbb {R}_{>0}$$ so that $$\alpha _1'(s) \le c$$ for all $$s \in \mathbb {R}_{>0}$$, then the mean value theorem yields the desired result with $$\hat{\alpha }\doteq c \alpha _2$$ and $$\hat{\sigma }\doteq \sigma$$.

On the other hand, if there exists $$c \in \mathbb {R}_{>0}$$ so that $$\alpha _2(s) \le c$$ for all $$s \in \mathbb {R}_{>0}$$, then the result holds with $$\hat{\alpha }(s) \doteq \sqrt{\alpha _1(\sigma (0)\alpha _2(s))}$$ for all $$s \in \mathbb {R}_{\ge 0}$$ and $$\hat{\sigma }(t) \doteq \sqrt{\alpha _1(c\sigma (t))}$$ for all $$t \in \mathbb {R}_{\ge 0}$$. $$\square$$

The following result describes a class of functions that can be bounded from above by a class-$$\mathcal {KL}$$ function. This result was proved, though not formally stated, in [22].

### Lemma 9

[1, Lemma 4.1] Suppose a function $$\phi : \mathbb {R}_{\ge 0} \times \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}$$ satisfies
• for all $$r,\varepsilon \in \mathbb {R}_{>0}$$, there exists some $$T = T(r,\varepsilon ) \in \mathbb {R}_{>0}$$ such that $$\phi (s,t) < \varepsilon$$ for all $$s \le r$$ and $$t \ge T$$; and

• for all $$\varepsilon \in \mathbb {R}_{>0}$$ there exists $$\delta \in \mathbb {R}_{>0}$$ such that $$\phi (s,t) \le \varepsilon$$ for all $$s \le \delta$$ and all $$t \in \mathbb {R}_{\ge 0}$$.

Then there exists some $$\beta \in \mathcal {KL}$$ such that $$\phi (s,t) \le \beta (s,t)$$ for all $$s,t \in \mathbb {R}_{\ge 0}$$.
As in analysis more generally, the existence of a triangle inequality is extremely useful. In [35, Equation (12)], Sontag observed that for any function $$\alpha \in \mathcal {K}$$ and any $$a,b \in \mathbb {R}_{\ge 0}$$,
\begin{aligned} \alpha (a + b) \le \alpha (2a) + \alpha (2b) . \end{aligned}
(8)
A generalization of this was presented in [17] where an additional function $$\varphi \in \mathcal {K}_{\infty }$$ can be used to trade off the relative weighting on the first argument versus the second argument. The following is sometimes referred to as a weak triangle inequality. A proof is provided in Appendix A.3.

### Lemma 10

[17, Equation (6)] Given $$\alpha \in \mathcal {K}$$ and any function $$\varphi \in \mathcal {K}_{\infty }$$ such that $$\varphi - \mathrm{id} \in \mathcal {K}_{\infty }$$, then for any $$a,b \in \mathbb {R}_{\ge 0}$$
\begin{aligned} \alpha (a + b) \le \alpha (\varphi (a)) + \alpha \left( \varphi \circ (\varphi - \mathrm{id})^{-1}(b) \right) . \end{aligned}
(9)
Clearly, choosing $$\varphi (s) = 2s$$ for all $$s \in \mathbb {R}_{\ge 0}$$ regains the original form of the weak triangle inequality (8). More generally, we can select $$\varphi (s) = (1+c)s$$ with $$c \in \mathbb {R}_{>0}$$, which satisfies
\begin{aligned} \varphi \circ (\varphi - \mathrm{id})^{-1}(s) = \frac{1+c}{c}s . \end{aligned}
Consequently, choosing $$c < 1$$ puts a larger weighting on the $$b$$ term, whereas choosing $$c > 1$$ puts a larger weighting on the $$a$$ term.
We note that an alternate, more symmetric, form of (9) can be obtained by choosing $$\hat{\varphi } \doteq \varphi - \mathrm{id} \in \mathcal {K}_{\infty }$$ so that
\begin{aligned} \alpha (a+b) \le \alpha \circ \left( \hat{\varphi } + \mathrm{id} \right) (a) + \alpha \circ \left( \hat{\varphi }^{-1} + \mathrm{id} \right) (b), \quad \forall a,b \in \mathbb {R}_{\ge 0}. \end{aligned}
(10)
This form of the weak triangle inequality was presented in [33, Lemma 1.1.2].

It is possible to weakly factor functions of two variables that are jointly of class-$$\mathcal {K}$$.

### Lemma 11

[3, Corollary IV.5] Suppose $$\alpha :\mathbb {R}_{\ge 0}^2 \rightarrow \mathbb {R}_{\ge 0}$$ is such that $$\alpha (\cdot ,s) \in \mathcal {K}$$ for each fixed $$s \in \mathbb {R}_{\ge 0}$$ and $$\alpha (r,\cdot ) \in \mathcal {K}$$ for each fixed $$r \in \mathbb {R}_{\ge 0}$$. Then there exists a function $$\hat{\alpha } \in \mathcal {K}$$ such that
\begin{aligned} \alpha (r,s) \le \hat{\alpha }(r)\hat{\alpha }(s) . \end{aligned}
(11)

We present a sketch of the proof in Sect. 7.4.

A precursor to the above appeared as [36, Corollary 10] where the relationship between the arguments is a product.

### Lemma 12

[36, Corollary 10] Given $$\alpha \in \mathcal {K}_{\infty }$$ there exist $$\alpha _1, \alpha _2 \in \mathcal {K}_{\infty }$$ such that
\begin{aligned} \alpha (rs) \le \alpha _1 (r) \alpha _2 (s), \quad \forall r,s \in \mathbb {R}_{\ge 0}. \end{aligned}
Hahn [12] made use of a similar upper bound in a fairly simple case. In particular, given $$\alpha \in \mathcal {K}$$ and constants $$c,\lambda \in \mathbb {R}_{> 0}$$ such that $$\alpha (s) \le c s^\lambda$$ for all $$s \in \mathbb {R}_{\ge 0}$$. Then
\begin{aligned} \alpha (r s) \le c r^\lambda s^\lambda , \quad \forall r,s \in \mathbb {R}_{\ge 0}. \end{aligned}
The following lemma provides an upper bound on a given class-$$\mathcal {K}$$ function in terms of the composition of convex and concave functions of class-$$\mathcal {K}$$.

### Lemma 13

[30, Lemma 14] Given $$\alpha \in \mathcal {K}$$ there exist continuously differentiable and convex $$\alpha _v \in \mathcal {K}$$ and continuously differentiable and concave $$\alpha _c \in \mathcal {K}$$ such that
\begin{aligned} \alpha (s) \le \alpha _c \circ \alpha _v(s), \quad \forall s \in \mathbb {R}_{\ge 0}. \end{aligned}
The key idea of the proof involves the fact that the integral of a class-$$\mathcal {K}$$ function is convex. On the one hand, the convex function required is directly defined by
\begin{aligned} \alpha _v(s) \doteq \frac{\alpha ^{-1}(s^*)}{s^*} \int \limits _0^{2s} \alpha (\tau ) d\tau + s, \quad \forall s \in \mathbb {R}_{\ge 0} \end{aligned}
where $$s^* \doteq \min \{1, \tfrac{a}{2}\}$$ and $$a = \lim _{s \rightarrow \infty } \alpha (s)$$. These latter points guarantee that the inverse $$\alpha ^{-1}$$ is well defined. On the other hand, the concave function is defined by specifying its inverse as the convex function
\begin{aligned} \alpha _c^{-1}(s) \doteq \left\{ \begin{array}{l@{\quad }l} \int _0^s \alpha ^{-1}(\tau ) d\tau , &{} \forall s \in [0,s^*] \\ \alpha _c^{-1}(s^*) + (s-s^*) \alpha ^{-1}(s^*) , &{} \forall s > s^*. \end{array} \right. \end{aligned}
An upper bound for class-$$\mathcal {L}$$ functions was presented in [12] as follows:

### Lemma 14

If $$\sigma \in \mathcal {L}$$ then there exist $$\sigma _1, \sigma _2 \in \mathcal {L}$$ such that
\begin{aligned} \sigma (r+s) \le \sigma _1(r)\sigma _2(s) , \quad \forall r,s \in \mathbb {R}_{\ge 0} . \end{aligned}

The proof of the above is provided in Appendix A.4.

Finally, we introduce the Legendre–Fenchel transform to present a general version of Young’s Inequality. Suppose $$\alpha \in \mathcal {K}_{\infty }$$ is continuously differentiable and that, in addition, $$\alpha ' \in \mathcal {K}_{\infty }$$. To ease the notation, denote $$(\alpha ')^{-1}(s) \doteq \varphi (s)$$ for all $$s \in \mathbb {R}_{\ge 0}$$. Then the Legendre–Fenchel transform of $$\alpha$$ is defined by
\begin{aligned} \ell \alpha (s) \doteq \int \limits _0^s \varphi (\tau ) d\tau , \quad \forall s \in \mathbb {R}_{\ge 0}. \end{aligned}
(12)
The Legendre–Fenchel transform appears to have first been used in conjunction with comparison functions in [29]. Several interesting properties of the Legendre–Fenchel transform were provided in [20].

### Lemma 15

[20, Lemma A.1] If $$\alpha , \alpha ' \in \mathcal {K}_{\infty }$$, then the Legendre–Fenchel transform (12) satisfies
\begin{aligned} \begin{array}{lll} \mathrm{(i)} \quad &{} \ell \alpha (s) = s \varphi (s) - \alpha \circ \varphi (s), &{} \forall s \in \mathbb {R}_{\ge 0}; \\ \mathrm{(ii)} &{} \ell \ell \alpha (s) = \alpha (s), &{} \forall s \in \mathbb {R}_{\ge 0}; \\ \mathrm{(iii)} &{} \ell \alpha ( \alpha '(s)) = s \alpha '(s) - \alpha (s), &{} \forall s \in \mathbb {R}_{\ge 0}; \ \mathrm{and} \\ \mathrm{(iv)} &{} \ell \alpha \in \mathcal {K}_{\infty }; . \end{array} \end{aligned}

Using the Legendre–Fenchel transform, the following general version of Young’s Inequality was presented in [29].

### Lemma 16

For any continuously differentiable $$\alpha \in \mathcal {K}_{\infty }$$ such that $$\alpha ' \in \mathcal {K}_{\infty }$$ and any $$x, y \in \mathbb {R}^n$$
\begin{aligned} x^T y \le \alpha (|x|) + \ell \alpha (|y|) \end{aligned}
with equality if and only if
\begin{aligned} y = \frac{\alpha '(|x|)}{|x|} x. \end{aligned}
The original version of Young’s inequality [13, Theorem 156] bounds the product of two nonnegative numbers as follows: for any $$\hat{\alpha }\in \mathcal {K}_{\infty }$$ and $$a,b \in \mathbb {R}_{\ge 0}$$,
\begin{aligned} ab \le \int \limits _0^a \hat{\alpha }(\tau ) d\tau + \int \limits _0^b \hat{\alpha }^{-1}(\tau )d\tau , \end{aligned}
(13)
with equality if and only if $$b = \hat{\alpha }(a)$$. The relationship of (13) to Lemma 16 is straightforward to see by considering $$\hat{\alpha }= \alpha '$$.

A useful result for bounding from above the product of two nonnegative numbers based on any given $$\mathcal {K}_{\infty }$$ function was presented in [30].

### Lemma 17

For any $$\alpha \in \mathcal {K}_{\infty }$$ and any $$p \in \mathbb {R}_{>0}$$,
\begin{aligned} ab \le \alpha ^{-1}(pa)a + \frac{\alpha (b)b}{p}, \quad \forall a,b \in \mathbb {R}_{\ge 0}. \end{aligned}

The proof is straightforward by considering the two cases of $$\alpha ^{-1}(pa) \ge b$$ and $$\alpha ^{-1}(pa) < b$$. Alternatively, this can be shown via Young’s inequality (13) by considering $$\alpha \doteq \frac{1}{p}\hat{\alpha }\in \mathcal {K}_{\infty }$$.

## 4 Lower bounds

As comparison functions are most frequently used in gain and stability estimates, they tend to be used to upper bound various quantities. As a consequence, the literature contains many more results for bounding functions from above than for bounding functions from below. Nonetheless, lower bounds have occasionally proved useful.

As previously noted, the initial use of class-$$\mathcal {K}$$ functions was for the characterization of locally positive definite functions. However, it is not possible to bound every globally positive definite function from below by a function of class-$$\mathcal {K}$$. A complete characterization of positive definite functions on $$\mathbb {R}_{\ge 0}$$ in terms of a lower bound depending on both a class-$$\mathcal {K}$$ function and a class-$$\mathcal {L}$$ function was given by in [3, Lemma IV.1]. The version presented here extends the characterization to positive definite functions defined on $$\mathbb {R}^n$$. A proof is provided in Appendix A.5.

### Lemma 18

Let $$\rho :\mathbb {R}^n \rightarrow \mathbb {R}_{\ge 0}$$ be a continuous positive definite function. Then, there exist functions $$\alpha \in \mathcal {K}_{\infty }$$ and $$\sigma \in \mathcal {L}$$ such that
\begin{aligned} \rho (x) \ge \alpha (|x|)\sigma (|x|), \quad \forall x \in \mathbb {R}^n . \end{aligned}

The following lower bound on functions of class-$$\mathcal {KL}$$ was introduced in [37] to separate the effect of the two arguments when considering the decrease condition for an input-to-output stability Lyapunov function.7 The main idea of the proof is discussed in Sect. 7.4.

### Lemma 19

[37, Lemma A.2] For any $$\beta \in \mathcal {KL}$$ there exist $$\alpha _1 \in \mathcal {K}$$, $$\alpha _2 \in \mathcal {K}_{\infty }$$ such that
\begin{aligned} \beta (s,t) \ge \frac{\alpha _1(s)}{1 + \alpha _2(t)} \end{aligned}
(14)
for all $$(s,t) \in \mathbb {R}_{\ge 0} \times \mathbb {R}_{\ge 0}$$.

## 5 The comparison principle

The comparison principle or comparison lemma makes use of a (usually solvable) scalar differential inequality to make statements about the nature of solutions to a scalar differential equation. An example application of this principle was provided in Sect. 2.1. In the case where the right-hand side of the scalar differential inequality is a continuous negative definite function, then solutions are bounded by a function of class-$$\mathcal {KL}$$. The following result was first demonstrated in a slightly more restrictive form by Hahn [12, Section 24E].

### Lemma 20

[37, Lemma A.4] For any continuous positive definite function $$\rho : \mathbb {R}_{\ge 0}\rightarrow \mathbb {R}_{\ge 0}$$ there exists $$\beta \in \mathcal {KL}$$ such that if $$y(\cdot )$$ is any locally absolutely continuous function defined on some interval $$[0,T]$$ with $$y(t) \ge 0$$ for all $$t \in [0,T]$$, and if $$y(\cdot )$$ satisfies the differential inequality
\begin{aligned} \dot{y}(t) \le - \lambda \rho (y(t)) \end{aligned}
(15)
for almost all $$t \in [0,T]$$ for some $$\lambda \ge 0$$ with $$y(0) = y_0 \in \mathbb {R}_{\ge 0}$$ then
\begin{aligned} y(t) \le \beta (y_0, \lambda t), \quad \forall t \in [0,T] . \end{aligned}

The above, with $$\lambda =1$$, first appeared in [22, Lemma 4.4]. A precursor to this where $$y(t)$$ satisfying a differential equation, rather than the inequality above, implies a $$\mathcal {KL}$$ bound appeared in [35, Lemma 6.1]. A proof of Lemma 20 is provided in Appendix A.6.

An extension to the above comparison principle allows the right-hand side of the differential inequality to also depend on an external input. This is particularly useful when considering robust stability in the context of input-to-state stability and its variants. The following two lemmas allow the input to enter via a maximization and a summation, respectively.

### Lemma 21

[3, Lemma IV.2] Given any continuous positive definite function $$\rho : \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ there exists $$\beta \in \mathcal {KL}$$ so that if, for some $$\bar{t} \in \mathbb {R}_{>0}$$, $$v:[0,\bar{t}) \rightarrow \mathbb {R}_{\ge 0}$$ is a continuous function and $$y:[0,\bar{t}) \rightarrow \mathbb {R}$$ is a (locally) absolutely continuous function with $$y(0) = y_0 \in \mathbb {R}_{\ge 0}$$, and if
\begin{aligned} \dot{y}(t) \le - \rho \left( \max \{ y(t) + v(t), 0\} \right) \end{aligned}
holds for almost all $$t \in [0,\bar{t})$$ then
\begin{aligned} y(t) \le \max \left\{ \beta (y_0,t), \sup _{\tau \in [0,t]} |v(\tau )| \right\} , \quad \forall t \in [0,\bar{t}). \end{aligned}

The proof relies on Lemma 18 applied to the positive definite function $$\rho$$ to obtain $$\alpha \in \mathcal {K}_{\infty }$$ and $$\sigma \in \mathcal {L}$$, so that, with the decreasing property of $$\sigma$$, $$\rho (s) \ge \alpha (s)\sigma (2s)$$ for all $$s \in \mathbb {R}_{\ge 0}$$. Without being overly precise, two time intervals are then considered: times such that $$y(t) \le \sup _{\tau \in [0,t]} |v(\tau )|$$ and times such that $$y(t)$$ exceeds this bound. The former set is invariant since $$y(t)$$ is decreasing and $$\sup _{\tau \in [0,t]} |v(\tau )|$$ is increasing. In the latter case, we see that $$y(t) > v(t)$$ so that $$y(t) \le y(t)+v(t) \le 2y(t)$$. Then, since $$\alpha \in \mathcal {K}_{\infty }$$, $$\dot{y}(t) \le \alpha (y(t))\sigma (2y(t))$$ and we can appeal to Lemma 20 to obtain the desired result. See [3] for a detailed proof.

### Lemma 22

[3, Corollary IV.3] Given any continuous positive definite function $$\rho :\mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ there exists $$\beta \in \mathcal {KL}$$ so that if, for some $$\bar{t} \in \mathbb {R}_{>0}$$, $$v:[0,\bar{t}) \rightarrow \mathbb {R}_{\ge 0}$$ is a measureable, locally essentially bounded function and $$y:[0,\bar{t}) \rightarrow \mathbb {R}_{\ge 0}$$ is (locally) absolutely continuous function with $$y(0) = y_0 \in \mathbb {R}_{\ge 0}$$, and if
\begin{aligned} \dot{y}(t) \le - \rho ( y(t)) + v(t) \end{aligned}
for almost all $$t \in [0,\bar{t})$$, then
\begin{aligned} y(t) \le \beta (y_0,t) + \int \limits _0^t 2v(\tau ) d\tau , \quad \forall t \in [0,\bar{t}). \end{aligned}
The proof follows by defining certain auxiliary functions and showing that these functions satisfy the requirements of Lemma 21. In particular, let $$w(t)$$ be the solution to the initial value problem
\begin{aligned} \dot{w}(t) = - \rho (w(t)) + v(t), \quad w(0) = y(0), \end{aligned}
let $$v_1(t) = \int _0^t v(\tau ) d\tau$$, and let $$w_1(t) = w(t) - v_1(t)$$. The function $$w_1$$ then plays the role of $$y$$ in Lemma 21. As before, see [3] for a detailed proof.

## 6 Other relationships

In addition to the previously presented lemmas providing upper and lower bounds and comparison principles, several results involving comparison functions are available that do not neatly fit into these categories. In this section, we summarize several such results.

Many factorizations of comparison functions are possible, with the derivations frequently relying on the invertibility of class-$$\mathcal {K}_{\infty }$$ functions. A proof of the following is in Appendix A.7.

### Lemma 23

[33, Lemma 1.1.3] For any $$\alpha \in \mathcal {K}$$, there exist $$\alpha _1, \alpha _2 \in \mathcal {K}$$ such that
\begin{aligned} \alpha + \mathrm{id} = \left( \alpha _1 + \mathrm{id} \right) \circ \left( \alpha _2 + \mathrm{id} \right) \!. \end{aligned}
Furthermore, if $$\alpha \in \mathcal {K}_{\infty }$$ then $$\alpha _1$$ and $$\alpha _2$$ can be chosen of class-$$\mathcal {K}_{\infty }$$ as well.

The next two lemmas presented were used to modify decrease conditions of Lyapunov functions in continuous time (Lemma 24) and discrete time (Lemma 25). The following is a combination of [30, Lemmas 11 and 12].

### Lemma 24

[19, Lemma 5.4] For each continuous, positive definite function $$\rho : \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ there exists $$\alpha \in \mathcal {K}_{\infty }$$ such that $$\alpha (\cdot )$$ is locally Lipschitz on its domain, continuously differentiable on $$(0,\infty )$$ and
\begin{aligned} \alpha (s) \le \rho (s) \alpha '(s), \quad \forall s \in \mathbb {R}_{> 0} . \end{aligned}
The form of the function $$\alpha \in \mathcal {K}_{\infty }$$ used in the proof of Lemma 24 is
\begin{aligned} \alpha (s) \doteq \exp \left( 2 \int \limits _1^s \frac{1}{\min \{\tau , \rho (\tau )\} } d\tau \right) , \quad \forall s \in \mathbb {R}_{>0} \end{aligned}
and $$\alpha (0) = 0$$.

### Lemma 25

[18, Lemma 19] If $$\lambda > 1$$ and if $$\alpha \in \mathcal {K}_{\infty }$$ satisfies $$(\alpha - \mathrm{id}) \in \mathcal {K}_{\infty }$$, then there exists $$\hat{\alpha } \in \mathcal {K}_{\infty }$$ such that
\begin{aligned} \hat{\alpha } \circ \alpha (s) = \lambda \hat{\alpha }(s), \quad \forall s \in \mathbb {R}_{\ge 0} . \end{aligned}
(16)
A proof of the above lemma is provided in Appendix A.8. While the proof is generally nonconstructive, for linear functions of class-$$\mathcal {K}_{\infty }$$
\begin{aligned} \alpha (s) = cs, \quad c>1 \end{aligned}
one choice for the $$\mathcal {K}_{\infty }$$ function of Lemma 25 can be seen to be
\begin{aligned} \hat{\alpha }(s) = s^m, \quad m = \frac{\log \lambda }{\log c} . \end{aligned}
Since $$\lambda , c > 1$$, we have that $$m>0$$ and
\begin{aligned} \hat{\alpha }\circ \alpha (s) = c^{\frac{\log \lambda }{\log c}} s^m = \lambda s^m = \lambda \hat{\alpha }(s). \end{aligned}
It is possible to derive a corollary to Lemma 25 to allow for positive constants less than one. The proof is provided in Appendix A.9.

### Corollary 1

If $$\lambda \in (0,1)$$ and if $$\alpha \in \mathcal {K}_{\infty }$$ satisfies $$(\mathrm{id} - \alpha ) \in \mathcal {K}_{\infty }$$ then there exists $$\hat{\alpha } \in \mathcal {K}_{\infty }$$ such that
\begin{aligned} \hat{\alpha } \circ (\mathrm{id} - \alpha )(s) = \lambda \hat{\alpha }(s), \quad \forall s \in \mathbb {R}_{\ge 0}. \end{aligned}
(17)

Given a function of class-$$\mathcal {K}$$, it is possible to find another function of class-$$\mathcal {K}$$ that upper bounds the given function away from the origin and is linear near the origin.

### Lemma 26

[16, Lemma 1] For any $$\alpha \in \mathcal {K}$$ and any $$\lambda \in \mathbb {R}_{> 0}$$, there exist two numbers $$\lambda _1, \lambda _2 \in \mathbb {R}_{>0}$$ and a smooth $$\hat{\alpha } \in \mathcal {K}_{\infty }$$ such that
\begin{aligned} \alpha (s)&\le \hat{\alpha }(s), \quad \forall s \ge \lambda \\ \hat{\alpha }(s)&= \lambda _1 s, \quad \forall s \in [0,\lambda _2) . \end{aligned}

The following lemma describes a condition under which the order of composition of two class-$$\mathcal {K}$$ functions can be reversed whilst maintaining a contraction principle.

### Lemma 27

[38, Fact A.2] Let $$\alpha _1, \alpha _2 \in \mathcal {K}$$ and let $$c \in \mathbb {R}_{>0}$$. Then
\begin{aligned} \alpha _1 \circ \alpha _2(s) \le s, \ \ \forall s \in [0,c] \quad \Longleftrightarrow \quad \alpha _2 \circ \alpha _1(s) \le s, \ \ \forall s \in [0,\alpha _2(c)]. \end{aligned}
(18)

We note that [38, Fact A.2] only proved one direction of the implication. The proof of Lemma 27 is provided in Appendix A.10.

As a corollary to the above, we obtain the following result when both functions are of class-$$\mathcal {K}_{\infty }$$.

### Corollary 2

Let $$\alpha _1, \alpha _2 \in \mathcal {K}_{\infty }$$. Then
\begin{aligned} \alpha _1 \circ \alpha _2(s) \le s, \ \ \forall s \in \mathbb {R}_{\ge 0} \quad \Longleftrightarrow \quad \alpha _2 \circ \alpha _1(s) \le s \ \ \forall s \in \mathbb {R}_{\ge 0}. \end{aligned}
A simple example shows that, for more than two functions, we cannot change the order of composition and maintain a contraction condition. For all $$s \in \mathbb {R}_{\ge 0}$$, let
\begin{aligned} \alpha _1(s) \doteq \sqrt{s}, \quad \alpha _2(s) \doteq \frac{3}{2}s, \quad \mathrm{and} \quad \alpha _3(s) \doteq \frac{1}{2}s^2. \end{aligned}
Then, for all $$s \in \mathbb {R}_{>0}$$, $$\alpha _1 \circ \alpha _2 \circ \alpha _3(s) = \frac{\sqrt{3}}{2}s < s$$ but $$\alpha _3 \circ \alpha _2 \circ \alpha _1(s) = \frac{9}{8}s > s$$.

Finally, in [23], the following characterization of growth rates of some class-$$\mathcal {K}_{\infty }$$ functions was provided.

### Lemma 28

[23, Proposition 5] The following are equivalent:
• A function $$\alpha \in \mathcal {K}_{\infty }$$ satisfies, for every $$\varepsilon \in \mathbb {R}_{>0}$$
\begin{aligned} \lim _{s \rightarrow \infty } \left\{ \alpha \left( (1+\varepsilon ) s \right) - \alpha (s) \right\} = \infty ; \end{aligned}
(19)
• For every $$\varepsilon \in \mathbb {R}_{>0}$$ there exists $$\varphi _\varepsilon \in \mathcal {K}_{\infty }$$ such that
\begin{aligned} \alpha (s-t) \le \alpha \left( (1+\varepsilon )s\right) - \varphi _\varepsilon (t), \quad \forall s\ge t \ge 0. \end{aligned}

It was noted in [23] that $$\mathcal {K}_{\infty }$$ functions of the form $$\alpha (s) = s^\lambda$$ for $$\lambda \in \mathbb {R}_{>0}$$ satisfy the growth condition of (19). By contrast, $$\mathcal {K}_{\infty }$$ functions of the form $$\alpha (s) = \lambda \log (1+s)$$ for $$\lambda \in \mathbb {R}_{>0}$$ do not satisfy (19).

## 7 Other function classes

Functions of class-$$\mathcal {K}$$, $$\mathcal {K}_{\infty }$$, $$\mathcal {L}$$, and $$\mathcal {KL}$$ have been used in stability theory for over 40 years going back to the original work of Massera and Hahn. Other useful classes have been introduced more recently.

### 7.1 Functions of class-$$\mathcal {KLD}$$

In [9], Grüne defined a subset of class-$$\mathcal {KL}$$ functions, which he called class-$$\mathcal {KL}\mathcal {D}$$.

### Definition 7

A function $$\mu : \mathbb {R}_{\ge 0} \times \mathbb {R}\rightarrow \mathbb {R}_{\ge 0}$$ is said to be of class-$$\mathcal {KLD}$$ if its restriction to $$\mathbb {R}_{\ge 0} \times \mathbb {R}_{\ge 0}$$ is class-$$\mathcal {KL}$$ and, in addition,
\begin{aligned} \mu (r,0) = r \quad \mathrm{and} \quad \mu \left( \mu (r,t),s\right) = \mu (r,t+s) \end{aligned}
(20)
for all $$r \in \mathbb {R}_{\ge 0}, \ s,t \in \mathbb {R}$$.

The $$\mathcal {D}$$ in $$\mathcal {KL}\mathcal {D}$$ above denotes dynamical and refers to the fact that, as a consequence of (20), a function of class-$$\mathcal {KL}\mathcal {D}$$ defines a dynamical system on $$\mathbb {R}_{\ge 0}$$. Class-$$\mathcal {KL}\mathcal {D}$$ functions were introduced in [9, 10] to characterize the notion of input-to-state dynamical stability (ISDS). ISDS is a robust stability concept equivalent to input-to-state stability and, as such, it is useful to know that any function of class-$$\mathcal {KL}$$ can be bounded from above by a function of class-$$\mathcal {KL}\mathcal {D}$$ as follows.

### Lemma 29

[9, Lemma B.1.4] For any $$\beta \in \mathcal {KL}$$, there exist functions $$\mu \in \mathcal {KL}\mathcal {D}$$ and $$\alpha \in \mathcal {K}_{\infty }$$ such that
\begin{aligned} \beta (s,t) \le \mu \left( \alpha (s), t \right) , \quad \forall s,t \in \mathbb {R}_{\ge 0} . \end{aligned}

### 7.2 Extended real-valued functions

As was earlier noted, functions of class-$$\mathcal {K}$$ are invertible only on their range. Hence, when using functions of class-$$\mathcal {K}$$, if their inverses are required, a certain level of notational overhead is necessary. To reduce this notational burden and to provide approximate inverses for functions that are not strictly increasing (see class-$$\mathcal {G}$$ functions below), Ito [14] considered extended real-valued functions (see also [15]); that is, functions on $$\overline{\mathbb {R}}_{\ge 0} \doteq \mathbb {R}_{\ge 0} \cup \{\infty \}$$.

For continuity at infinity of a function $$\alpha : \overline{\mathbb {R}}_{\ge 0} \rightarrow \overline{\mathbb {R}}_{\ge 0}$$ we intend that the usual limit condition $$s_n \rightarrow s$$ implies $$\alpha (s_n) \rightarrow \alpha (s)$$ including for sequences $$s_n \rightarrow \infty$$ as well as for any $$s \in \mathbb {R}_{>0}$$ such that $$\alpha (s) = \infty$$.

### Definition 8

A function $$\alpha : \overline{\mathbb {R}}_{\ge 0} \rightarrow \overline{\mathbb {R}}_{\ge 0}$$ is said to be of class-$$\overline{\mathcal {K}}$$ if it is continuous, zero at zero, strictly increasing on the range $$\mathbb {R}_{\ge 0}$$ and infinite otherwise.

By strictly increasing on the range $$\mathbb {R}_{\ge 0}$$ we mean that on the set
\begin{aligned} \{ s \in \overline{\mathbb {R}}_{\ge 0} : \alpha (s) \ne \infty \} \end{aligned}
the function $$\alpha$$ is strictly increasing. An example of a function $$\alpha \in \overline{\mathcal {K}}$$ is
\begin{aligned} \alpha (s) = \left\{ \begin{array}{l@{\quad }l} \mathrm{arctan}(s), &{} s \in \mathbb {R}_{\ge 0} \\ \frac{\pi }{2}, &{} s = \infty . \end{array} \right. \end{aligned}
(21)
Another example of a function $$\varphi \in \overline{\mathcal {K}}$$ is
\begin{aligned} \varphi (s) = \left\{ \begin{array}{l@{\quad }l} \mathrm{tan}(s) , &{} s \in \left[ 0, \frac{\pi }{2} \right) \\ \infty , &{} s \in \left[ \frac{\pi }{2}, \infty \right] . \end{array} \right. \end{aligned}
(22)
Ito defined the pseudo-inverse of a function $$\alpha \in \overline{\mathcal {K}}$$ as
\begin{aligned} \alpha ^\ominus (s) \doteq \left\{ \begin{array}{l@{\quad }l} \alpha ^{-1}(s) , &{} s \in [0, \lim _{\tau \rightarrow \infty } \alpha (\tau )) \\ \sup \{ s \in \mathbb {R}_{\ge 0} : \alpha (s) < \infty \}, &{} \mathrm{otherwise}. \end{array} \right. \end{aligned}
(23)
We note that, with these definitions, if a function $$\alpha \in \overline{\mathcal {K}}$$ then $$\alpha ^\ominus \in \overline{\mathcal {K}}$$. Furthermore, we may state the following result.

### Lemma 30

Let $$\alpha \in \overline{\mathcal {K}}$$. If
\begin{aligned} \sup \{ s \in \mathbb {R}_{\ge 0} : \alpha (s) < \infty \} = \infty \end{aligned}
(24)
then, for all $$s \in \overline{\mathbb {R}}_{\ge 0}$$,
\begin{aligned} \alpha ^\ominus \circ \alpha (s) = s \quad \mathrm{and} \quad \alpha \circ \alpha ^\ominus (s) \le s. \end{aligned}
(25)
On the other hand, if
\begin{aligned} \sup \{ s \in \mathbb {R}_{\ge 0} : \alpha (s) < \infty \} = c < \infty \end{aligned}
(26)
then, for all $$s \in \overline{\mathbb {R}}_{\ge 0}$$,
\begin{aligned} \alpha ^\ominus \circ \alpha (s) \le s \quad \mathrm{and} \quad \alpha \circ \alpha ^\ominus (s) = s. \end{aligned}
(27)

### Proof

Let $$a = \lim _{\tau \rightarrow \infty } \alpha (\tau )$$ so that $$\alpha : \overline{\mathbb {R}}_{\ge 0} \rightarrow [0,a]$$ and $$\alpha ^{-1}: [0,a) \rightarrow [0,\infty )$$. If (24) holds then
\begin{aligned} \alpha ^\ominus (s) = \left\{ \begin{array}{l@{\quad }l} \alpha ^{-1}(s), &{} s \in [0, a) \\ \infty , &{} s \ge a \end{array} \right. \end{aligned}
so that
\begin{aligned} \alpha ^\ominus \circ \alpha (s) = \left\{ \begin{array}{l@{\quad }l} s , &{} s \in [0,\infty ) \\ \infty , &{} s = \infty \end{array} \right. \quad \mathrm{and} \quad \alpha \circ \alpha ^\ominus (s) = \left\{ \begin{array}{l@{\quad }l} s , &{} s \in [0,a) \\ a , &{} s \ge a. \end{array} \right. \end{aligned}
Therefore, (25) holds.
If (26) holds then $$\lim _{s \nearrow c} \alpha (s) = \infty$$ (i.e., $$\alpha (c) = \infty$$) and
\begin{aligned} \alpha ^\ominus (s) = \left\{ \begin{array}{l@{\quad }l} \alpha ^{-1}(s), &{} s \in [0, \infty ) \\ c , &{} s = \infty \end{array} \right. \end{aligned}
so that
\begin{aligned} \alpha ^\ominus \circ \alpha (s) = \left\{ \begin{array}{l@{\quad }l} s , &{} s \in [0,c) \\ c , &{} s \ge c \end{array} \right. \quad \mathrm{and} \quad \alpha \circ \alpha ^\ominus (s) = \left\{ \begin{array}{l@{\quad }l} s , &{} s \in [0,\infty ) \\ \infty , &{} s = \infty . \end{array} \right. \end{aligned}
Therefore, (27) holds. $$\square$$

We observe that $$\alpha , \varphi \in \overline{\mathcal {K}}$$ from (21) and (22) are pseudo-inverses of each other; i.e., $$\alpha ^\ominus = \varphi$$ and $$\varphi ^\ominus = \alpha$$. Furthermore, $$\alpha \in \overline{\mathcal {K}}$$ satisfies (24) while $$\varphi \in \overline{\mathcal {K}}$$ satisfies (26).

### Definition 9

A function $$\sigma : \overline{\mathbb {R}}_{\ge 0} \rightarrow \overline{\mathbb {R}}_{\ge 0}$$ is said to be of class-$$\overline{\mathcal {L}}$$ if it is continuous, strictly decreasing, and $$\sigma (\infty ) = 0$$.

For $$\sigma : \overline{\mathbb {R}}_{\ge 0} \rightarrow \overline{\mathbb {R}}_{\ge 0}$$, it is understood that strictly decreasing allows $$\sigma (0) = \infty$$ but requires $$\sigma (s) < \infty$$ for all $$s \in \overline{\mathbb {R}}_{>0}$$.

We define the pseudo-inverse of a function $$\sigma \in \overline{\mathcal {L}}$$ as
\begin{aligned} \sigma ^\dag (s) \doteq \left\{ \begin{array}{l@{\quad }l} \infty , &{} s = 0 \\ \sigma ^{-1}(s), &{} s \in (0, \sigma (0)) \\ 0, &{} s \in [\sigma (0), \infty ]. \end{array} \right. \end{aligned}
(28)
Similar to the fact that the inverse of a function $$\sigma \in \mathcal {L}$$ is nearly of class-$$\mathcal {L}$$ (see Section 2), the pseudo-inverse of a function $$\sigma \in \overline{\mathcal {L}}$$ is nearly of class-$$\overline{\mathcal {L}}$$; i.e., $$\sigma ^\dag : \overline{\mathbb {R}}_{\ge 0} \rightarrow \overline{\mathbb {R}}_{\ge 0}$$ is continuous, strictly decreasing for $$s \in [0,\sigma (0))$$, and $$\sigma ^\dag (\infty ) = 0$$.
We observe that, for all $$s \in \overline{\mathbb {R}}_{\ge 0}$$,
\begin{aligned} \sigma ^\dag \circ \sigma (s) = s \quad \mathrm{and} \quad \sigma \circ \sigma ^\dag (s) \le s . \end{aligned}
Constraining $$\sigma \in \overline{\mathcal {L}}$$ so that $$\sigma (0) = \infty$$ yields that $$\sigma ^\dag \in \overline{\mathcal {L}}$$ is a true inverse of $$\sigma \in \overline{\mathcal {L}}$$. For example, the function
\begin{aligned} \sigma (s) = \left\{ \begin{array}{l@{\quad }l} \infty , &{} s = 0 \\ \frac{1}{s}, &{} s \in (0, \infty ) \\ 0, &{} s = \infty \end{array} \right. \end{aligned}
is of class-$$\overline{\mathcal {L}}$$ and is its own pseudo-inverse.

### 7.3 Functions of class-$$\mathcal {G}$$

The function class-$$\mathcal {G}$$ was defined in [40] by enlarging the class-$$\mathcal {K}$$ to include functions that are not strictly increasing.8

### Definition 10

A function $$\alpha : \mathbb {R}_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ is said to be of class-$$\mathcal {G}$$ if it is continuous, nondecreasing, and $$\alpha (0) = 0$$.

It is clear that any class-$$\mathcal {G}$$ function can be bounded from above by a function of class-$$\mathcal {K}$$. However, it is not the case that every class-$$\mathcal {G}$$ function can be bounded from below by a function of class-$$\mathcal {K}$$. For example, a function which is identically zero for all $$s \in [0,1]$$ and equal to $$s-1$$ for all $$s >1$$ is of class-$$\mathcal {G}$$, but cannot be bounded from below by a function of class-$$\mathcal {K}$$.

Since class-$$\mathcal {G}$$ functions are not strictly increasing, they may fail to be invertible. This shortcoming can typically be circumvented by allowing set-valued inverses or by the introduction of class-$$\mathcal {K}$$ upper and lower bounds, where especial care is required to properly deal with any lower bound.

An alternative approach is to make use of the extended real-valued functions defined in the previous section to construct approximate inverses. Define class-$$\overline{\mathcal {G}}$$ as the enlargement of class-$$\overline{\mathcal {K}}$$ to include functions that are not strictly increasing.

### Lemma 31

[15, Proposition 1] Suppose $$\gamma \in \overline{\mathcal {G}}$$ is positive definite and $$\alpha \in \overline{\mathcal {K}}$$. Let $$c \in \overline{\mathbb {R}}_{\ge 0}$$ be given by $$c = \sup \{ s \in \overline{\mathbb {R}}_{\ge 0} : \alpha (s) < \infty \}$$ and assume
\begin{aligned} c < \infty \, \Rightarrow \, \gamma (\infty ) < c. \end{aligned}
(29)
Then, for all $$s \in \overline{\mathbb {R}}_{\ge 0}$$,
\begin{aligned} \alpha \circ \gamma (s) \le s \quad \mathrm{if \ and \ only \ if} \quad \gamma \circ \alpha (s) \le s. \end{aligned}
(30)

The proof of the above lemma is provided in Appendix A.11.

As an example, suppose we wish to derive an approximate inverse for the positive definite function $$\gamma \in \overline{\mathcal {G}}$$ defined by
\begin{aligned} \gamma (s) = \mathrm{sat}(2s) \doteq \left\{ \begin{array}{ll@{\quad }l} 2s, &{} &{} s \in \left[ 0,\tfrac{1}{2}\right] \\ 1, &{} &{} s > \tfrac{1}{2} \end{array}. \right. \end{aligned}
A well-defined inverse exists on $$[0,1)$$ but we encounter an obvious difficulty at the value of one. One possible approximation of an inverse for $$\gamma$$ is given by $$\alpha \in \overline{\mathcal {K}}$$ defined as
\begin{aligned} \alpha (s) \doteq \left\{ \begin{array}{ll@{\quad }l} \tfrac{1}{2} s, &{} &{} s \in [0,1] \\ \frac{a-1}{2(a-s)}, &{} &{} s \in [1,a) \\ \infty , &{} &{} s \ge a \end{array} \right. \end{aligned}
for some $$a > 1$$. We see that this extended real-valued function is the expected inverse on $$[0,1]$$ and goes to infinity arbitrarily close to one. It is straightforward to see that, for all $$s \in \overline{\mathbb {R}}_{\ge 0}$$, both $$\alpha \circ \gamma (s) \le s$$ and $$\gamma \circ \alpha (s) \le s$$, indicating that Lemma 31 captures a property of reasonable approximations of inverses of class-$$\overline{\mathcal {G}}$$ functions.

### 7.4 Functions of class-$$\mathcal {N}$$

The nomenclature of class-$$\mathcal {N}$$ has been used to denote two different function classes9. We here adopt the definition in [3].

### Definition 11

A function $$\nu : \mathbb {R}\rightarrow \mathbb {R}$$ is said to be of class-$$\mathcal {N}$$ if it is continuous, nondecreasing, and unbounded below (that is, $$\inf \nu = -\infty$$).

The following lemma is the key element in the proofs of Lemma 11 and Lemma 19.

### Lemma 32

[3, Proposition IV.4] Suppose $$\phi : \mathbb {R}^2 \rightarrow \mathbb {R}$$ is class-$$\mathcal {N}$$ in each of its arguments; i.e., $$\phi (\cdot ,y) \in \mathcal {N}$$ for each fixed $$y \in \mathbb {R}$$ and $$\phi (x,\cdot ) \in \mathcal {N}$$ for each fixed $$x \in \mathbb {R}$$. Then there exists $$\kappa \in \mathcal {N}$$ such that
\begin{aligned} \phi (x,y) \le \kappa (x) + \kappa (y), \quad \forall (x,y) \in \mathbb {R}^2 . \end{aligned}
To prove Lemma 11, given $$\alpha : \mathbb {R}^2_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ of class-$$\mathcal {K}$$ in each of its arguments independently, the function
\begin{aligned} \phi (x,y) \doteq \log \left( \alpha \left( e^x, e^y\right) \right) , \quad \forall x, y \in \mathbb {R}, \end{aligned}
where $$\log$$ denotes the natural logarithm, can be shown to be of class-$$\mathcal {N}$$. Applying Lemma 32, Lemma 1, and taking an exponential on both sides of the resulting inequality gives the desired result with $$\hat{\alpha }\in \mathcal {K}$$ bounding $$\varphi (s) \doteq e^{k(\log (s))}$$ from above.
The core idea of the proof of Lemma 19 similarly requires defining an appropriate function $$\phi$$. Define $$|x|_+ \doteq \max \{0, x\}$$ and
\begin{aligned} \phi (x,y) \doteq - \log \left( \tilde{\beta }\left( \tfrac{1}{|x|_+},|y|_+\right) \right) - |-x|_+ - |-y|_+, \quad \forall x,y \in \mathbb {R}, \end{aligned}
for a function $$\tilde{\beta }\in \mathcal {KL}$$ that is a lower bound for the given $$\beta \in \mathcal {KL}$$ with certain desirable properties. Again we apply Lemma 32, Lemma 1, and take exponentials on both sides of the resulting inequality. Some straightforward manipulations then yield the desired result.

## 8 Monotone aggregation functions

To compare two vectors $$x,y \in \mathbb {R}^n_{\ge 0}$$, we use $$x > \!\! > y$$ if and only if $$x_i > y_i$$ for all $$i \in \{1, \ldots , n\}$$. In other words, each element of $$x \in \mathbb {R}^n_{\ge 0}$$ must be greater than the corresponding element in $$y \in \mathbb {R}^n_{\ge 0}$$.

A generalization of class-$$\mathcal {K}$$ functions allowing a domain of $$\mathbb {R}^n_{\ge 0}$$, rather than a domain of $$\mathbb {R}_{\ge 0}$$, was introduced in [33] (see also [6]). These so-called monotone aggregation functions are defined as follows:

### Definition 12

A continuous function $$\mu : \mathbb {R}^n_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$ is a monotone aggregation function (MAF $$_n$$) if it is positive definite and strictly monotone; i.e., for any $$x, y \in \mathbb {R}^n_{\ge 0}$$, if $$x > \!\! > y$$ then $$\mu (x) > \mu (y)$$. The class of unbounded monotone aggregation functions on $$\mathbb {R}^n_{\ge 0}$$ is denoted by MAF$$_{n,\infty }$$.

Together with gain matrices describing the interconnection structure of large-scale systems, monotone aggregation functions were used in [33] and subsequent works to provide results on stability of large-scale systems, particularly through the use of small-gain theorems.

Examples of monotone aggregation functions include maximization and all $$p$$-norms on $$\mathbb {R}^n$$. As such, they provide a general and elegant formulation encapsulating and expanding the standard input-to-state stability estimates for systems with inputs. In particular, for $$\dot{x} = f(x,w)$$, we can subsume both the estimate
\begin{aligned} |x(t)| \le \beta (|x(0)|,t) + \gamma (||w||_{\infty }) \end{aligned}
and the estimate
\begin{aligned} |x(t)| \le \max \left\{ \beta (|x(0)|,t), \gamma (||w||_{\infty }) \right\} \end{aligned}
by the use of a function $$\mu \in \mathrm{MAF}_2$$ and the estimate
\begin{aligned} |x(t)| \le \mu \left( \beta (|x(0)|,t), \gamma (||w||_{\infty }) \right) \!. \end{aligned}
There are several useful and straightforward relationships between functions of class-$$\mathcal {K}$$ and monotone aggregation functions:
• The function classes $$\mathcal {K}$$ and $$\mathrm{MAF}_1$$ are equivalent.

• If $$\alpha \in \mathcal {K}$$ and $$\mu \in \mathrm{MAF}_n$$, then $$\alpha \circ \mu \in \mathrm{MAF}_n$$.

• If $$\alpha _i \in \mathcal {K}$$ for $$i=1, \ldots , n$$, and $$\mu \in \mathrm{MAF}_n$$, then the function
\begin{aligned} \mu _\alpha (s_1, \ldots , s_n) \doteq \mu (\alpha _1(s_1),\ldots , \alpha _n(s_n)) \end{aligned}
is in $$\mathrm{MAF}_n$$.
• Denote the vector of all ones in $$\mathbb {R}^n$$ by $$\mathbf {1}_n$$. If $$\mu \in \mathrm{MAF}_n$$ then $$\mu (s \mathbf {1}_n)$$, $$s \in \mathbb {R}_{\ge 0}$$, is a function of class-$$\mathcal {K}$$.

Despite the equivalence of class-$$\mathcal {K}$$ and $$\mathrm{MAF}_1$$, monotone aggregation functions are in fact different to functions $$\alpha :\mathbb {R}^n_{\ge 0} \rightarrow \mathbb {R}_{\ge 0}$$, $$n \in \mathbb {Z}_{>1}$$, that are of class-$$\mathcal {K}$$ in each argument, or what might be termed jointly class-$$\mathcal {K}$$. For example, in the case of a jointly class-$$\mathcal {K}$$ function of two arguments, $$\alpha \in \mathcal {K}^2$$, we see that $$\alpha (s,0) = 0$$ for all $$s \in \mathbb {R}_{\ge 0}$$. On the other hand, a function $$\mu \in \mathrm{MAF}_2$$ is positive definite; i.e., $$\mu (s,0) > 0$$ for all $$s \in \mathbb {R}_{>0}$$.

### Lemma 33

Given $$\mu \in \mathrm{MAF}_n$$ and integers $$n_1,n_2$$ such that $$n_1 + n_2 = n$$, there exist $$\mu _1 \in \mathrm{MAF}_{n_1}$$ and $$\mu _2 \in \mathrm{MAF}_{n_2}$$ such that
\begin{aligned} \mu (s_1, \ldots , s_n) \le \mu _1\left( s_1, \ldots , s_{n_1}\right) + \mu _2 \left( s_{n_1 + 1}, \ldots , s_n\right) \end{aligned}
for all $$(s_1, \ldots , s_n) \in \mathbb {R}^n_{\ge 0}$$.

### Proof

Denote a ball of radius $$r\ge 0$$ in the positive orthant by $$\mathcal {B}_r^+$$ and let $$\alpha \in \mathcal {K}$$ be given by
\begin{aligned} \alpha (s) \doteq \max _{x \in \mathcal {B}_s^+} \mu (x). \end{aligned}
(31)
That $$\alpha \in \mathcal {K}$$ follows directly from the fact that $$\mu \in \mathrm{MAF}_n$$. We see that
\begin{aligned} \mu (s_1, \ldots , s_n)&\le \alpha (s_1) + \cdots + \alpha (s_n) \\&= \sum _{i=1}^{n_1}\alpha (s_i) + \sum _{i=n_1 + 1}^n \alpha (s_i) \\&=: \mu _1\left( s_1, \ldots , s_{n_1}\right) + \mu _2 \left( s_{n_1 + 1}, \ldots , s_n\right) . \end{aligned}
That $$\mu _1 \in \mathrm{MAF}_{n_1}$$ and $$\mu _2 \in \mathrm{MAF}_{n_2}$$ follow from the fact that the sum of $$n$$ functions of class-$$\mathcal {K}$$ is a function of class-$$\mathrm{MAF}_n$$. $$\square$$

The above result leads to the following result from [8] allowing a general monotone aggregation function to be bounded from above by a summation. We denote by $$\mathcal {K}_{\infty }\cup \{ 0 \}$$ those functions that are either class-$$\mathcal {K}_{\infty }$$ or identically zero.

### Lemma 34

For any $$\mu \in \mathrm{MAF}_{n+1}$$, $$\beta \in \mathcal {KL}$$, and $$\alpha _i \in \mathcal {K}_{\infty }\cup \{0\}$$, $$i = 1, \ldots , n$$ there exist $$\hat{\mu }\in \mathrm{MAF}_{n-1}$$, $$\hat{\beta }\in \mathcal {KL}$$, $$\hat{\alpha }_n \in \mathcal {K}_{\infty }\cup \{0\}$$ such that
\begin{aligned} \mu \left( \beta (s_0,t), \alpha _1(s_1), \ldots , \alpha _n(s_n) \right) \le \hat{\beta }(s_0,t) + \hat{\mu }\left( \alpha _1(s_1), \ldots , \alpha _{n-1}(s_{n-1}) \right) + \hat{\alpha }_n(s_n) \end{aligned}
for all $$t,s_0, \ldots , s_n \in \mathbb {R}_{\ge 0}$$.

### Proof

We apply Lemma 33 twice to the function $$\mu \in \mathrm{MAF}_{n+1}$$ to obtain $$\hat{\mu }_1 \in \mathrm{MAF}_1$$, $$\hat{\mu }_2 \in \mathrm{MAF}_1$$, and $$\hat{\mu }\in \mathrm{MAF}_{n-1}$$. With the equivalence of class-$$\mathcal {K}$$ and $$\mathrm{MAF}_1$$, we can define $$\hat{\beta } \doteq \hat{\mu }_1 \circ \beta \in \mathcal {KL}$$ and $$\hat{\alpha }_n \doteq \hat{\mu }_2 \circ \alpha _n \in \mathcal {K}$$. $$\square$$

## Footnotes

1. 1.

It is worth remarking that in his 1949 manuscript studying similar stability problems, Massera [25] does not use comparison functions, but instead uses the more classical $$\varepsilon {-}\delta$$ formulations, indicating their development sometime between 1949 [25] and 1956 [26].

2. 2.

It is known that Hahn was aware of Massera’s work [26] as Massera submitted an Erratum for [26] to Annals of Mathematics on 13 January 1958 where he cites Hahn as having brought an error in the original paper to his attention.

3. 3.

It has been speculated that Hahn’s usage of the letter $$\mathcal {K}$$ was in reference to Kamke, though Hahn himself never apparently stated this. Functions similar to class-$$\mathcal {K}$$ functions do appear in [28] and are, in fact, denoted by $$K(\cdot )$$. In a similar vein, [27] makes use of a bounding function that is continuous and monotonically decreasing to zero on $$(0,\infty )$$.

4. 4.

Observe that class-$$\mathcal {K}_{[0,\infty )}$$ and class-$$\mathcal {K}_{\infty }$$ are not the same. In fact, class-$$\mathcal {K}_{[0,\infty )}$$ is the same as class-$$\mathcal {K}$$ since the subscript interval refers to the domain of definition of a function. By contrast, the subscript of $$\mathcal {K}_{\infty }$$ refers to the behavior of the function in the limit as its argument goes to infinity.

5. 5.

Note that some authors only assume that functions of class-$$\mathcal {L}$$ are nonincreasing. In many cases, this is sufficient. However, we prefer the symmetry with the strictly increasing property of class-$$\mathcal {K}$$ functions and the clean results on class-$$\mathcal {L}$$ functions that the assumption of strictly decreasing enables. Note that, since functions of class-$$\mathcal {L}$$ are strictly decreasing and go to zero in the limit, these functions are also strictly positive. This is explicit in the definition in that the range of class-$$\mathcal {L}$$ functions is $$\mathbb {R}_{>0}$$.

6. 6.

Despite the fact that functions $$\alpha \in \mathcal {K}$$ are strictly increasing, it is possible that $$\alpha '(s) = 0$$ for isolated points $$s \in \mathbb {R}_{>0}$$. For example, $$\alpha (s) \doteq \int \nolimits _0^s (1 + \sin (\tau ))d\tau$$ is one such function.

7. 7.

We note that the statement of Lemma 19 in [37] was not entirely precise in two respects. The first is that the authors explicitly defined class-$$\mathcal {KL}$$ functions as nonincreasing, rather than strictly decreasing, in their second argument. However, this definition admits functions such that $$\beta (s,t) = 0$$ for some $$s,t \in \mathbb {R}_{>0}$$ finite, while the right-hand side of (14) is strictly positive. The second is that it is necessary that $$\alpha _2 \in \mathcal {K}_{\infty }$$ whereas in [37, Lemma A.2] it is only stated that $$\alpha _2 \in \mathcal {K}$$. However, if $$\alpha _2 \in \mathcal {K}$$ is not of class-$$\mathcal {K}_{\infty }$$, then the right-hand side of (14) may remain bounded away from zero as $$t \rightarrow \infty$$ while $$\lim _{t \rightarrow \infty } \beta (s,t) = 0$$.

8. 8.

These functions were introduced in [39] under the nomenclature of “gain functions”, leading to the natural function class name of $$\mathcal {G}$$ in [40]. In [7], these functions were defined as class-$$\overline{\mathcal {K}}$$ while in [15] such functions were denoted by class-$$\mathcal {J}$$.

9. 9.

In [2], the function class-$$\mathcal {N}$$ denotes those functions which map $$\mathbb {R}_{\ge 0}$$ to $$\mathbb {R}_{\ge 0}$$ and are continuous and increasing. In this case, class-$$\mathcal {K}$$ is the subset of class-$$\mathcal {N}$$ functions that are also zero at zero.

## Notes

### Acknowledgments

The author would like to thank Lars Grüne, Björn Rüffer, Andy Teel, and Fabian Wirth for comments on early drafts of this manuscript. The work of the anonymous reviewers is also gratefully acknowledged.

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