Continuous function#Heine definition of continuity

{{Short description|Mathematical function with no sudden changes}}

{{Calculus}}

In mathematics, a continuous function is a function such that a small variation of the argument induces a small variation of the value of the function. This implies there are no abrupt changes in value, known as discontinuities. More precisely, a function is continuous if arbitrarily small changes in its value can be assured by restricting to sufficiently small changes of its argument. A discontinuous function is a function that is {{em|not continuous}}. Until the 19th century, mathematicians largely relied on intuitive notions of continuity and considered only continuous functions. The epsilon–delta definition of a limit was introduced to formalize the definition of continuity.

Continuity is one of the core concepts of calculus and mathematical analysis, where arguments and values of functions are real and complex numbers. The concept has been generalized to functions between metric spaces and between topological spaces. The latter are the most general continuous functions, and their definition is the basis of topology.

A stronger form of continuity is uniform continuity. In order theory, especially in domain theory, a related concept of continuity is Scott continuity.

As an example, the function {{math|H(t)}} denoting the height of a growing flower at time {{mvar|t}} would be considered continuous. In contrast, the function {{math|M(t)}} denoting the amount of money in a bank account at time {{mvar|t}} would be considered discontinuous since it "jumps" at each point in time when money is deposited or withdrawn.

History

A form of the epsilon–delta definition of continuity was first given by Bernard Bolzano in 1817. Augustin-Louis Cauchy defined continuity of y = f(x) as follows: an infinitely small increment \alpha of the independent variable x always produces an infinitely small change f(x+\alpha)-f(x) of the dependent variable y (see e.g. Cours d'Analyse, p. 34). Cauchy defined infinitely small quantities in terms of variable quantities, and his definition of continuity closely parallels the infinitesimal definition used today (see microcontinuity). The formal definition and the distinction between pointwise continuity and uniform continuity were first given by Bolzano in the 1830s, but the work wasn't published until the 1930s. Like Bolzano,{{cite web|url=http://dml.cz/handle/10338.dmlcz/400352|title=Rein analytischer Beweis des Lehrsatzes daß zwischen je zwey Werthen, die ein entgegengesetzetes Resultat gewähren, wenigstens eine reelle Wurzel der Gleichung liege |year=1817 |last1=Bolzano |first1=Bernard |publisher=Haase|location=Prague}} Karl Weierstrass{{Citation | last1=Dugac | first1=Pierre | title=Eléments d'Analyse de Karl Weierstrass | journal=Archive for History of Exact Sciences | year=1973 | volume=10 | issue=1–2 | pages=41–176 | doi=10.1007/bf00343406| s2cid=122843140 }} denied continuity of a function at a point c unless it was defined at and on both sides of c, but Édouard Goursat{{Citation | last1=Goursat | first1=E. | title=A course in mathematical analysis | publisher=Ginn | location=Boston | year=1904 | page=2}} allowed the function to be defined only at and on one side of c, and Camille Jordan{{Citation | last1=Jordan | first1=M.C. | title=Cours d'analyse de l'École polytechnique | publisher=Gauthier-Villars | location=Paris | edition=2nd |year=1893 | volume=1|page=46|url={{Google books|h2VKAAAAMAAJ|page=46|plainurl=yes}}}} allowed it even if the function was defined only at c. All three of those nonequivalent definitions of pointwise continuity are still in use.{{Citation|last1=Harper|first1=J.F.|title=Defining continuity of real functions of real variables|journal=BSHM Bulletin: Journal of the British Society for the History of Mathematics|year=2016|volume=31|issue=3|doi=10.1080/17498430.2015.1116053|pages=1–16|s2cid=123997123}} Eduard Heine provided the first published definition of uniform continuity in 1872, but based these ideas on lectures given by Peter Gustav Lejeune Dirichlet in 1854.{{citation|last1=Rusnock|first1=P.|last2=Kerr-Lawson|first2=A.|title=Bolzano and uniform continuity|journal=Historia Mathematica|volume=32|year=2005|pages=303–311|issue=3|doi=10.1016/j.hm.2004.11.003|doi-access=}}

Real functions

=Definition=

File:Function-1 x.svg defined on the reals.{{cite book |last1=Strang |first1=Gilbert |title=Calculus |year=1991 |publisher=SIAM|isbn=0961408820 |page=702|url={{Google books|OisInC1zvEMC|page=87|plainurl=yes}}}}]]

A real function that is a function from real numbers to real numbers can be represented by a graph in the Cartesian plane; such a function is continuous if, roughly speaking, the graph is a single unbroken curve whose domain is the entire real line. A more mathematically rigorous definition is given below.{{cite web | url=http://math.mit.edu/~jspeck/18.01_Fall%202014/Supplementary%20notes/01c.pdf | title=Continuity and Discontinuity | last1=Speck | first1=Jared | year=2014 | page=3 | access-date=2016-09-02 | website=MIT Math | quote=Example 5. The function 1/x is continuous on (0, \infty) and on (-\infty, 0),, i.e., for x > 0 and for x < 0, in other words, at every point in its domain. However, it is not a continuous function since its domain is not an interval. It has a single point of discontinuity, namely x = 0,, and an infinite discontinuity there. | archive-date=2016-10-06 | archive-url=https://web.archive.org/web/20161006014646/http://math.mit.edu/~jspeck/18.01_Fall%202014/Supplementary%20notes/01c.pdf | url-status=dead }}

Continuity of real functions is usually defined in terms of limits. A function {{math|f}} with variable {{mvar|x}} is continuous at the real number {{mvar|c}}, if the limit of f(x), as {{mvar|x}} tends to {{mvar|c}}, is equal to f(c).

There are several different definitions of the (global) continuity of a function, which depend on the nature of its domain.

A function is continuous on an open interval if the interval is contained in the function's domain and the function is continuous at every interval point. A function that is continuous on the interval (-\infty, +\infty) (the whole real line) is often called simply a continuous function; one also says that such a function is continuous everywhere. For example, all polynomial functions are continuous everywhere.

A function is continuous on a semi-open or a closed interval; if the interval is contained in the domain of the function, the function is continuous at every interior point of the interval, and the value of the function at each endpoint that belongs to the interval is the limit of the values of the function when the variable tends to the endpoint from the interior of the interval. For example, the function f(x) = \sqrt{x} is continuous on its whole domain, which is the closed interval [0,+\infty).

Many commonly encountered functions are partial functions that have a domain formed by all real numbers, except some isolated points. Examples include the reciprocal function x \mapsto \frac {1}{x} and the tangent function x\mapsto \tan x. When they are continuous on their domain, one says, in some contexts, that they are continuous, although they are not continuous everywhere. In other contexts, mainly when one is interested in their behavior near the exceptional points, one says they are discontinuous.

A partial function is discontinuous at a point if the point belongs to the topological closure of its domain, and either the point does not belong to the domain of the function or the function is not continuous at the point. For example, the functions x\mapsto \frac {1}{x} and x\mapsto \sin(\frac {1}{x}) are discontinuous at {{math|0}}, and remain discontinuous whichever value is chosen for defining them at {{math|0}}. A point where a function is discontinuous is called a discontinuity.

Using mathematical notation, several ways exist to define continuous functions in the three senses mentioned above.

Let f : D \to \R be a function defined on a subset D of the set \R of real numbers.

This subset D is the domain of {{math|f}}. Some possible choices include

  • D = \R : i.e., D is the whole set of real numbers. or, for {{mvar|a}} and {{mvar|b}} real numbers,
  • D = [a, b] = \{x \in \R \mid a \leq x \leq b \} : D is a closed interval, or
  • D = (a, b) = \{x \in \R \mid a < x < b \} : D is an open interval.

In the case of the domain D being defined as an open interval, a and b do not belong to D, and the values of f(a) and f(b) do not matter for continuity on D.

==Definition in terms of limits of functions==

The function {{math|f}} is continuous at some point {{math|c}} of its domain if the limit of f(x), as x approaches c through the domain of f, exists and is equal to f(c).{{Citation | last1=Lang | first1=Serge | author1-link=Serge Lang | title=Undergraduate analysis | publisher=Springer-Verlag | location=Berlin, New York | edition=2nd | series=Undergraduate Texts in Mathematics | isbn=978-0-387-94841-6 | year=1997}}, section II.4 In mathematical notation, this is written as

\lim_{x \to c}{f(x)} = f(c).

In detail this means three conditions: first, {{math|f}} has to be defined at {{math|c}} (guaranteed by the requirement that {{math|c}} is in the domain of {{math|f}}). Second, the limit of that equation has to exist. Third, the value of this limit must equal f(c).

(Here, we have assumed that the domain of f does not have any isolated points.)

==Definition in terms of neighborhoods==

A neighborhood of a point c is a set that contains, at least, all points within some fixed distance of c. Intuitively, a function is continuous at a point c if the range of f over the neighborhood of c shrinks to a single point f(c) as the width of the neighborhood around c shrinks to zero. More precisely, a function f is continuous at a point c of its domain if, for any neighborhood N_1(f(c)) there is a neighborhood N_2(c) in its domain such that f(x) \in N_1(f(c)) whenever x\in N_2(c).

As neighborhoods are defined in any topological space, this definition of a continuous function applies not only for real functions but also when the domain and the codomain are topological spaces and is thus the most general definition. It follows that a function is automatically continuous at every isolated point of its domain. For example, every real-valued function on the integers is continuous.

==Definition in terms of limits of sequences==

File:Continuity of the Exponential at 0.svg

One can instead require that for any sequence (x_n)_{n \in \N} of points in the domain which converges to c, the corresponding sequence \left(f(x_n)\right)_{n\in \N} converges to f(c). In mathematical notation, \forall (x_n)_{n \in \N} \subset D:\lim_{n\to\infty} x_n = c \Rightarrow \lim_{n\to\infty} f(x_n) = f(c)\,.

==Weierstrass and Jordan definitions (epsilon–delta) of continuous functions==

File:Example of continuous function.svg

Explicitly including the definition of the limit of a function, we obtain a self-contained definition: Given a function f : D \to \mathbb{R} as above and an element x_0 of the domain D, f is said to be continuous at the point x_0 when the following holds: For any positive real number \varepsilon > 0, however small, there exists some positive real number \delta > 0 such that for all x in the domain of f with x_0 - \delta < x < x_0 + \delta, the value of f(x) satisfies

f\left(x_0\right) - \varepsilon < f(x) < f(x_0) + \varepsilon.

Alternatively written, continuity of f : D \to \mathbb{R} at x_0 \in D means that for every \varepsilon > 0, there exists a \delta > 0 such that for all x \in D:

\left|x - x_0\right| < \delta ~~\text{ implies }~~ |f(x) - f(x_0)| < \varepsilon.

More intuitively, we can say that if we want to get all the f(x) values to stay in some small neighborhood around f\left(x_0\right), we need to choose a small enough neighborhood for the x values around x_0. If we can do that no matter how small the f(x_0) neighborhood is, then f is continuous at x_0.

In modern terms, this is generalized by the definition of continuity of a function with respect to a basis for the topology, here the metric topology.

Weierstrass had required that the interval x_0 - \delta < x < x_0 + \delta be entirely within the domain D, but Jordan removed that restriction.

==Definition in terms of control of the remainder==

In proofs and numerical analysis, we often need to know how fast limits are converging, or in other words, control of the remainder. We can formalize this to a definition of continuity.

A function C: [0,\infty) \to [0,\infty] is called a control function if

  • C is non-decreasing
  • \inf_{\delta > 0} C(\delta) = 0

A function f : D \to R is C-continuous at x_0 if there exists such a neighbourhood N(x_0) that

|f(x) - f(x_0)| \leq C\left(\left|x - x_0\right|\right) \text{ for all } x \in D \cap N(x_0)

A function is continuous in x_0 if it is C-continuous for some control function C.

This approach leads naturally to refining the notion of continuity by restricting the set of admissible control functions. For a given set of control functions \mathcal{C} a function is {{nowrap|\mathcal{C}-continuous}} if it is {{nowrap|C-continuous}} for some C \in \mathcal{C}. For example, the Lipschitz, the Hölder continuous functions of exponent {{mvar|α}} and the uniformly continuous functions below are defined by the set of control functions

\mathcal{C}_{\mathrm{Lipschitz}} = \{C : C(\delta) = K|\delta| ,\ K > 0\}

\mathcal{C}_{\text{Hölder}-\alpha} = \{C : C(\delta) = K |\delta|^\alpha, \ K > 0\}

\mathcal{C}_{\text{uniform cont.}} = \{C : C(0) = 0 \}

respectively.

==Definition using oscillation==

File:Rapid Oscillation.svg.]]

Continuity can also be defined in terms of oscillation: a function f is continuous at a point x_0 if and only if its oscillation at that point is zero;[http://ramanujan.math.trinity.edu/wtrench/texts/TRENCH_REAL_ANALYSIS.PDF Introduction to Real Analysis], updated April 2010, William F. Trench, Theorem 3.5.2, p. 172 in symbols, \omega_f(x_0) = 0. A benefit of this definition is that it {{em|quantifies}} discontinuity: the oscillation gives how {{em|much}} the function is discontinuous at a point.

This definition is helpful in descriptive set theory to study the set of discontinuities and continuous points – the continuous points are the intersection of the sets where the oscillation is less than \varepsilon (hence a G_{\delta} set) – and gives a rapid proof of one direction of the Lebesgue integrability condition.[http://ramanujan.math.trinity.edu/wtrench/texts/TRENCH_REAL_ANALYSIS.PDF Introduction to Real Analysis], updated April 2010, William F. Trench, 3.5 "A More Advanced Look at the Existence of the Proper Riemann Integral", pp. 171–177

The oscillation is equivalent to the \varepsilon-\delta definition by a simple re-arrangement and by using a limit (lim sup, lim inf) to define oscillation: if (at a given point) for a given \varepsilon_0 there is no \delta that satisfies the \varepsilon-\delta definition, then the oscillation is at least \varepsilon_0, and conversely if for every \varepsilon there is a desired \delta, the oscillation is 0. The oscillation definition can be naturally generalized to maps from a topological space to a metric space.

==Definition using the hyperreals==

Cauchy defined the continuity of a function in the following intuitive terms: an infinitesimal change in the independent variable corresponds to an infinitesimal change of the dependent variable (see Cours d'analyse, page 34). Non-standard analysis is a way of making this mathematically rigorous. The real line is augmented by adding infinite and infinitesimal numbers to form the hyperreal numbers. In nonstandard analysis, continuity can be defined as follows.

{{block indent|em=1.5|text=A real-valued function {{math|f}} is continuous at {{mvar|x}} if its natural extension to the hyperreals has the property that for all infinitesimal {{math|dx}}, f(x + dx) - f(x) is infinitesimal{{cite web| url=http://www.math.wisc.edu/~keisler/calc.html |title=Elementary Calculus|work=wisc.edu}}}}

(see microcontinuity). In other words, an infinitesimal increment of the independent variable always produces an infinitesimal change of the dependent variable, giving a modern expression to Augustin-Louis Cauchy's definition of continuity.

=Construction of continuous functions=

File:Brent method example.svg has no jumps or holes. The function is continuous.]]

Checking the continuity of a given function can be simplified by checking one of the above defining properties for the building blocks of the given function. It is straightforward to show that the sum of two functions, continuous on some domain, is also continuous on this domain. Given

f, g \colon D \to \R,

then the {{em|sum of continuous functions}}

s = f + g

(defined by s(x) = f(x) + g(x) for all x\in D) is continuous in D.

The same holds for the {{em|product of continuous functions}},

p = f \cdot g

(defined by p(x) = f(x) \cdot g(x) for all x \in D)

is continuous in D.

Combining the above preservations of continuity and the continuity of constant functions and of the identity function I(x) = x {{nowrap|on \R,}} one arrives at the continuity of all polynomial functions {{nowrap|on \R,}} such as

f(x) = x^3 + x^2 - 5 x + 3

(pictured on the right).

File:Homografia.svg. The function is not defined for x = -2. The vertical and horizontal lines are asymptotes.]]

In the same way, it can be shown that the {{em|reciprocal of a continuous function}}

r = 1/f

(defined by r(x) = 1/f(x) for all x \in D such that f(x) \neq 0)

is continuous in D\setminus \{x : f(x) = 0\}.

This implies that, excluding the roots of g, the {{em|quotient of continuous functions}}

q = f / g

(defined by q(x) = f(x)/g(x) for all x \in D, such that g(x) \neq 0)

is also continuous on D\setminus \{x:g(x) = 0\}.

For example, the function (pictured)

y(x) = \frac{2x-1}{x+2}

is defined for all real numbers x \neq -2 and is continuous at every such point. Thus, it is a continuous function. The question of continuity at x = -2 does not arise since x = -2 is not in the domain of y. There is no continuous function F : \R \to \R that agrees with y(x) for all x \neq -2.

File:Si cos.svg

Since the function sine is continuous on all reals, the sinc function G(x) = \sin(x)/x, is defined and continuous for all real x \neq 0. However, unlike the previous example, G {{em|can}} be extended to a continuous function on {{em|all}} real numbers, by {{em|defining}} the value G(0) to be 1, which is the limit of G(x), when x approaches 0, i.e.,

G(0) = \lim_{x\to 0} \frac{\sin x}{x} = 1.

Thus, by setting

:

G(x) =

\begin{cases}

\frac {\sin (x)}x & \text{ if }x \ne 0\\

1 & \text{ if }x = 0,

\end{cases}

the sinc-function becomes a continuous function on all real numbers. The term {{em|removable singularity}} is used in such cases when (re)defining values of a function to coincide with the appropriate limits make a function continuous at specific points.

A more involved construction of continuous functions is the function composition. Given two continuous functions

g : D_g \subseteq \R \to R_g \subseteq \R \quad \text{ and } \quad f : D_f \subseteq \R \to R_f \subseteq D_g,

their composition, denoted as

c = g \circ f : D_f \to \R, and defined by c(x) = g(f(x)), is continuous.

This construction allows stating, for example, that

e^{\sin(\ln x)}

is continuous for all x > 0.

=Examples of discontinuous functions=

File:Discontinuity of the sign function at 0.svg).]]

An example of a discontinuous function is the Heaviside step function H, defined by

H(x) = \begin{cases}

1 & \text{ if } x \ge 0\\

0 & \text{ if } x < 0

\end{cases}

Pick for instance \varepsilon = 1/2. Then there is no {{nowrap|\delta-neighborhood}} around x = 0, i.e. no open interval (-\delta,\;\delta) with \delta > 0, that will force all the H(x) values to be within the {{nowrap|\varepsilon-neighborhood}} of H(0), i.e. within (1/2,\;3/2). Intuitively, we can think of this type of discontinuity as a sudden jump in function values.

Similarly, the signum or sign function

\sgn(x) = \begin{cases}

\;\;\ 1 & \text{ if }x > 0\\

\;\;\ 0 & \text{ if }x = 0\\

-1 & \text{ if }x < 0

\end{cases}

is discontinuous at x = 0 but continuous everywhere else. Yet another example: the function

f(x) = \begin{cases}

\sin\left(x^{-2}\right)&\text{ if }x \neq 0\\

0&\text{ if }x = 0

\end{cases}

is continuous everywhere apart from x = 0.

File:Thomae function (0,1).svg

Besides plausible continuities and discontinuities like above, there are also functions with a behavior, often coined pathological, for example, Thomae's function,

f(x)=\begin{cases}

1 &\text{ if } x=0\\

\frac{1}{q}&\text{ if } x = \frac{p}{q} \text{(in lowest terms) is a rational number}\\

0&\text{ if }x\text{ is irrational}.

\end{cases}

is continuous at all irrational numbers and discontinuous at all rational numbers. In a similar vein, Dirichlet's function, the indicator function for the set of rational numbers,

D(x)=\begin{cases}

0&\text{ if }x\text{ is irrational } (\in \R \setminus \Q)\\

1&\text{ if }x\text{ is rational } (\in \Q)

\end{cases}

is nowhere continuous.

=Properties=

==A useful lemma==

Let f(x) be a function that is continuous at a point x_0, and y_0 be a value such f\left(x_0\right)\neq y_0. Then f(x)\neq y_0 throughout some neighbourhood of x_0.{{citation|last=Brown|first=James Ward|title=Complex Variables and Applications|year=2009|publisher=McGraw Hill|edition=8th|page=54|isbn=978-0-07-305194-9}}

Proof: By the definition of continuity, take \varepsilon =\frac

y_0-f(x_0)
{2}>0 , then there exists \delta>0 such that

\left|f(x)-f(x_0)\right| < \frac{\left|y_0 - f(x_0)\right|}{2} \quad \text{ whenever } \quad |x-x_0| < \delta

Suppose there is a point in the neighbourhood |x-x_0|<\delta for which f(x)=y_0; then we have the contradiction

\left|f(x_0)-y_0\right| < \frac{\left|f(x_0) - y_0\right|}{2}.

==Intermediate value theorem==

The intermediate value theorem is an existence theorem, based on the real number property of completeness, and states:

:If the real-valued function f is continuous on the closed interval [a, b], and k is some number between f(a) and f(b), then there is some number c \in [a, b], such that f(c) = k.

For example, if a child grows from 1 m to 1.5 m between the ages of two and six years, then, at some time between two and six years of age, the child's height must have been 1.25 m.

As a consequence, if f is continuous on [a, b] and f(a) and f(b) differ in sign, then, at some point c \in [a, b], f(c) must equal zero.

==Extreme value theorem==

The extreme value theorem states that if a function f is defined on a closed interval [a, b] (or any closed and bounded set) and is continuous there, then the function attains its maximum, i.e. there exists c \in [a, b] with f(c) \geq f(x) for all x \in [a, b]. The same is true of the minimum of f. These statements are not, in general, true if the function is defined on an open interval (a, b) (or any set that is not both closed and bounded), as, for example, the continuous function f(x) = \frac{1}{x}, defined on the open interval (0,1), does not attain a maximum, being unbounded above.

==Relation to differentiability and integrability==

Every differentiable function

f : (a, b) \to \R

is continuous, as can be shown. The converse does not hold: for example, the absolute value function

:f(x)=|x| = \begin{cases}

\;\;\ x & \text{ if }x \geq 0\\

-x & \text{ if }x < 0

\end{cases}

is everywhere continuous. However, it is not differentiable at x = 0 (but is so everywhere else). Weierstrass's function is also everywhere continuous but nowhere differentiable.

The derivative f′(x) of a differentiable function f(x) need not be continuous. If f′(x) is continuous, f(x) is said to be continuously differentiable. The set of such functions is denoted C^1((a, b)). More generally, the set of functions

f : \Omega \to \R

(from an open interval (or open subset of \R) \Omega to the reals) such that f is n times differentiable and such that the n-th derivative of f is continuous is denoted C^n(\Omega). See differentiability class. In the field of computer graphics, properties related (but not identical) to C^0, C^1, C^2 are sometimes called G^0 (continuity of position), G^1 (continuity of tangency), and G^2 (continuity of curvature); see Smoothness of curves and surfaces.

Every continuous function

f : [a, b] \to \R

is integrable (for example in the sense of the Riemann integral). The converse does not hold, as the (integrable but discontinuous) sign function shows.

==Pointwise and uniform limits==

File:Uniform continuity animation.gif

Given a sequence

f_1, f_2, \dotsc : I \to \R

of functions such that the limit

f(x) := \lim_{n \to \infty} f_n(x)

exists for all x \in D,, the resulting function f(x) is referred to as the pointwise limit of the sequence of functions \left(f_n\right)_{n \in N}. The pointwise limit function need not be continuous, even if all functions f_n are continuous, as the animation at the right shows. However, f is continuous if all functions f_n are continuous and the sequence converges uniformly, by the uniform convergence theorem. This theorem can be used to show that the exponential functions, logarithms, square root function, and trigonometric functions are continuous.

=Directional Continuity=

Image:Right-continuous.svg|A right-continuous function

Image:Left-continuous.svg|A left-continuous function

Discontinuous functions may be discontinuous in a restricted way, giving rise to the concept of directional continuity (or right and left continuous functions) and semi-continuity. Roughly speaking, a function is {{em|right-continuous}} if no jump occurs when the limit point is approached from the right. Formally, f is said to be right-continuous at the point c if the following holds: For any number \varepsilon > 0 however small, there exists some number \delta > 0 such that for all x in the domain with c < x < c + \delta, the value of f(x) will satisfy

|f(x) - f(c)| < \varepsilon.

This is the same condition as continuous functions, except it is required to hold for x strictly larger than c only. Requiring it instead for all x with c - \delta < x < c yields the notion of {{em|left-continuous}} functions. A function is continuous if and only if it is both right-continuous and left-continuous.

= Semicontinuity=

{{Main|Semicontinuity}}

A function f is {{em|lower semi-continuous}} if, roughly, any jumps that might occur only go down, but not up. That is, for any \varepsilon > 0, there exists some number \delta > 0 such that for all x in the domain with |x - c| < \delta, the value of f(x) satisfies

f(x) \geq f(c) - \epsilon.

The reverse condition is {{em|upper semi-continuity}}.

==Continuous functions between metric spaces==

{{anchor|Metric spaces}}

The concept of continuous real-valued functions can be generalized to functions between metric spaces. A metric space is a set X equipped with a function (called metric) d_X, that can be thought of as a measurement of the distance of any two elements in X. Formally, the metric is a function

d_X : X \times X \to \R

that satisfies a number of requirements, notably the triangle inequality. Given two metric spaces \left(X, d_X\right) and \left(Y, d_Y\right) and a function

f : X \to Y

then f is continuous at the point c \in X (with respect to the given metrics) if for any positive real number \varepsilon > 0, there exists a positive real number \delta > 0 such that all x \in X satisfying d_X(x, c) < \delta will also satisfy d_Y(f(x), f(c)) < \varepsilon. As in the case of real functions above, this is equivalent to the condition that for every sequence \left(x_n\right) in X with limit \lim x_n = c, we have \lim f\left(x_n\right) = f(c). The latter condition can be weakened as follows: f is continuous at the point c if and only if for every convergent sequence \left(x_n\right) in X with limit c, the sequence \left(f\left(x_n\right)\right) is a Cauchy sequence, and c is in the domain of f.

The set of points at which a function between metric spaces is continuous is a G_{\delta} set – this follows from the \varepsilon-\delta definition of continuity.

This notion of continuity is applied, for example, in functional analysis. A key statement in this area says that a linear operator

T : V \to W

between normed vector spaces V and W (which are vector spaces equipped with a compatible norm, denoted \|x\|) is continuous if and only if it is bounded, that is, there is a constant K such that

\|T(x)\| \leq K \|x\|

for all x \in V.

=Uniform, Hölder and Lipschitz continuity=

File:Lipschitz continuity.png

The concept of continuity for functions between metric spaces can be strengthened in various ways by limiting the way \delta depends on \varepsilon and c in the definition above. Intuitively, a function f as above is uniformly continuous if the \delta does

not depend on the point c. More precisely, it is required that for every real number \varepsilon > 0 there exists \delta > 0 such that for every c, b \in X with d_X(b, c) < \delta, we have that d_Y(f(b), f(c)) < \varepsilon. Thus, any uniformly continuous function is continuous. The converse does not generally hold but holds when the domain space X is compact. Uniformly continuous maps can be defined in the more general situation of uniform spaces.{{Citation | last1=Gaal | first1=Steven A. | title=Point set topology | publisher=Dover Publications | location=New York | isbn=978-0-486-47222-5 | year=2009}}, section IV.10

A function is Hölder continuous with exponent α (a real number) if there is a constant K such that for all b, c \in X, the inequality

d_Y (f(b), f(c)) \leq K \cdot (d_X (b, c))^\alpha

holds. Any Hölder continuous function is uniformly continuous. The particular case \alpha = 1 is referred to as Lipschitz continuity. That is, a function is Lipschitz continuous if there is a constant K such that the inequality

d_Y (f(b), f(c)) \leq K \cdot d_X (b, c)

holds for any b, c \in X.{{Citation | last1=Searcóid | first1=Mícheál Ó | title=Metric spaces | url=https://books.google.com/books?id=aP37I4QWFRcC | publisher=Springer-Verlag | location=Berlin, New York | series=Springer undergraduate mathematics series | isbn=978-1-84628-369-7 | year=2006}}, section 9.4 The Lipschitz condition occurs, for example, in the Picard–Lindelöf theorem concerning the solutions of ordinary differential equations.

{{anchor|Continuous map (topology)}}Continuous functions between topological spaces

Another, more abstract, notion of continuity is the continuity of functions between topological spaces in which there generally is no formal notion of distance, as there is in the case of metric spaces. A topological space is a set X together with a topology on X, which is a set of subsets of X satisfying a few requirements with respect to their unions and intersections that generalize the properties of the open balls in metric spaces while still allowing one to talk about the neighborhoods of a given point. The elements of a topology are called open subsets of X (with respect to the topology).

A function

f : X \to Y

between two topological spaces X and Y is continuous if for every open set V \subseteq Y, the inverse image

f^{-1}(V) = \{x \in X \; | \; f(x) \in V \}

is an open subset of X. That is, f is a function between the sets X and Y (not on the elements of the topology T_X), but the continuity of f depends on the topologies used on X and Y.

This is equivalent to the condition that the preimages of the closed sets (which are the complements of the open subsets) in Y are closed in X.

An extreme example: if a set X is given the discrete topology (in which every subset is open), all functions

f : X \to T

to any topological space T are continuous. On the other hand, if X is equipped with the indiscrete topology (in which the only open subsets are the empty set and X) and the space T set is at least T0, then the only continuous functions are the constant functions. Conversely, any function whose codomain is indiscrete is continuous.

= Continuity at a point =

File:continuity topology.svg

The translation in the language of neighborhoods of the (\varepsilon, \delta)-definition of continuity leads to the following definition of the continuity at a point:

{{Quote frame|A function f : X \to Y is continuous at a point x \in X if and only if for any neighborhood {{mvar|V}} of f(x) in {{mvar|Y}}, there is a neighborhood {{mvar|U}} of x such that f(U) \subseteq V.}}

This definition is equivalent to the same statement with neighborhoods restricted to open neighborhoods and can be restated in several ways by using preimages rather than images.

Also, as every set that contains a neighborhood is also a neighborhood, and f^{-1}(V) is the largest subset {{mvar|U}} of {{mvar|X}} such that f(U) \subseteq V, this definition may be simplified into:

{{Quote frame|A function f : X \to Y is continuous at a point x\in X if and only if f^{-1}(V) is a neighborhood of x for every neighborhood {{mvar|V}} of f(x) in {{mvar|Y}}.}}

As an open set is a set that is a neighborhood of all its points, a function f : X \to Y is continuous at every point of {{mvar|X}} if and only if it is a continuous function.

If X and Y are metric spaces, it is equivalent to consider the neighborhood system of open balls centered at x and f(x) instead of all neighborhoods. This gives back the above \varepsilon-\delta definition of continuity in the context of metric spaces. In general topological spaces, there is no notion of nearness or distance. If, however, the target space is a Hausdorff space, it is still true that f is continuous at a if and only if the limit of f as x approaches a is f(a). At an isolated point, every function is continuous.

Given x \in X, a map f : X \to Y is continuous at x if and only if whenever \mathcal{B} is a filter on X that converges to x in X, which is expressed by writing \mathcal{B} \to x, then necessarily f(\mathcal{B}) \to f(x) in Y.

If \mathcal{N}(x) denotes the neighborhood filter at x then f : X \to Y is continuous at x if and only if f(\mathcal{N}(x)) \to f(x) in Y.{{sfn|Dugundji|1966|pp=211–221}} Moreover, this happens if and only if the prefilter f(\mathcal{N}(x)) is a filter base for the neighborhood filter of f(x) in Y.{{sfn|Dugundji|1966|pp=211–221}}

= Alternative definitions =

Several equivalent definitions for a topological structure exist; thus, several equivalent ways exist to define a continuous function.

== Sequences and nets {{anchor|Heine definition of continuity}}==

In several contexts, the topology of a space is conveniently specified in terms of limit points. This is often accomplished by specifying when a point is the limit of a sequence. Still, for some spaces that are too large in some sense, one specifies also when a point is the limit of more general sets of points indexed by a directed set, known as nets. A function is (Heine-)continuous only if it takes limits of sequences to limits of sequences. In the former case, preservation of limits is also sufficient; in the latter, a function may preserve all limits of sequences yet still fail to be continuous, and preservation of nets is a necessary and sufficient condition.

In detail, a function f : X \to Y is sequentially continuous if whenever a sequence \left(x_n\right) in X converges to a limit x, the sequence \left(f\left(x_n\right)\right) converges to f(x). Thus, sequentially continuous functions "preserve sequential limits." Every continuous function is sequentially continuous. If X is a first-countable space and countable choice holds, then the converse also holds: any function preserving sequential limits is continuous. In particular, if X is a metric space, sequential continuity and continuity are equivalent. For non-first-countable spaces, sequential continuity might be strictly weaker than continuity. (The spaces for which the two properties are equivalent are called sequential spaces.) This motivates the consideration of nets instead of sequences in general topological spaces. Continuous functions preserve the limits of nets, and this property characterizes continuous functions.

For instance, consider the case of real-valued functions of one real variable:{{cite book |title=Calculus and Analysis in Euclidean Space |edition=illustrated |first1=Jerry |last1=Shurman |publisher=Springer |year=2016 |isbn=978-3-319-49314-5 |pages=271–272 |url=https://books.google.com/books?id=wTmgDQAAQBAJ}}

{{math theorem|name=Theorem|note=|style=|math_statement=A function f : A \subseteq \R \to \R is continuous at x_0 if and only if it is sequentially continuous at that point.

}}

{{collapse top|title=Proof|left=true}}

Proof. Assume that f : A \subseteq \R \to \R is continuous at x_0 (in the sense of \epsilon-\delta continuity). Let \left(x_n\right)_{n\geq1} be a sequence converging at x_0 (such a sequence always exists, for example, x_n = x, \text{ for all } n); since f is continuous at x_0

\forall \epsilon > 0\, \exists \delta_{\epsilon} > 0 : 0 < |x-x_0| < \delta_{\epsilon} \implies |f(x)-f(x_0)| < \epsilon.\quad (*)

For any such \delta_{\epsilon} we can find a natural number \nu_{\epsilon} > 0 such that for all n > \nu_{\epsilon},

|x_n-x_0| < \delta_{\epsilon},

since \left(x_n\right) converges at x_0; combining this with (*) we obtain

\forall \epsilon > 0 \,\exists \nu_{\epsilon} > 0 : \forall n > \nu_{\epsilon} \quad |f(x_n)-f(x_0)| < \epsilon.

Assume on the contrary that f is sequentially continuous and proceed by contradiction: suppose f is not continuous at x_0

\exists \epsilon > 0 : \forall \delta_{\epsilon} > 0,\,\exists x_{\delta_{\epsilon}}: 0 < |x_{\delta_{\epsilon}}-x_0| < \delta_\epsilon \implies |f(x_{\delta_{\epsilon}})-f(x_0)| > \epsilon

then we can take \delta_{\epsilon}=1/n,\,\forall n > 0 and call the corresponding point x_{\delta_{\epsilon}} =: x_n: in this way we have defined a sequence (x_n)_{n\geq1} such that

\forall n > 0 \quad |x_n-x_0| < \frac{1}{n},\quad |f(x_n)-f(x_0)| > \epsilon

by construction x_n \to x_0 but f(x_n) \not\to f(x_0), which contradicts the hypothesis of sequential continuity. \blacksquare

{{collapse bottom}}

== Closure operator and interior operator definitions ==

In terms of the interior and closure operators, we have the following equivalences,

{{math theorem|name=Theorem|note=|style=|math_statement=Let f: X \to Y be a mapping between topological spaces. Then the following are equivalent.

{{ordered list|type=lower-roman

| f is continuous;

| for every subset B \subseteq Y, f^{-1}\left(\operatorname{int}_Y B\right) \subseteq \operatorname{int}_X\left(f^{-1}(B)\right);

| for every subset A \subseteq X,

f\left(\operatorname{cl}_X A\right) \subseteq \operatorname{cl}_Y \left(f(A)\right).

}}

}}

{{collapse top|title=Proof|left=true}}

Proof.{{spaces|em}}i ⇒ ii.{{spaces|en}}

Fix a subset B of Y. Since \operatorname{int}_Y B is open.

and f is continuous, f^{-1}(\operatorname{int}_Y B) is open in X.

As \operatorname{int}_Y B \subseteq B, we have f^{-1}(\operatorname{int}_Y B) \subseteq f^{-1}(B).

By the definition of the interior, \operatorname{int}_X\left(f^{-1}(B)\right) is the largest open set contained in f^{-1}(B). Hence f^{-1}(\operatorname{int}_Y B) \subseteq \operatorname{int}_X\left(f^{-1}(B)\right).

ii ⇒ iii.{{spaces|en}}

Fix A\subseteq X and let x\in\operatorname{cl}_X A. Suppose to the contrary that f(x)\notin\operatorname{cl}_Y\left(f(A)\right),

then we may find some open neighbourhood V of f(x) that is disjoint from \operatorname{cl}_Y\left(f(A)\right). By ii, f^{-1}(V) = f^{-1}(\operatorname{int}_Y V) \subseteq \operatorname{int}_X \left(f^{-1}(V)\right), hence f^{-1}(V) is open. Then we have found an open neighbourhood of x that does not intersect \operatorname{cl}_X A, contradicting the fact that x\in\operatorname{cl}_X A.

Hence f\left(\operatorname{cl}_X A\right) \subseteq \operatorname{cl}_Y \left(f(A)\right).

iii ⇒ i.{{spaces|en}}

Let N\subseteq Y be closed. Let M = f^{-1}(N) be the preimage of N.

By iii, we have f\left(\operatorname{cl}_X M\right) \subseteq \operatorname{cl}_Y \left(f(M)\right).

Since f(M) = f(f^{-1}(N)) \subseteq N,

we have further that f\left(\operatorname{cl}_X M\right) \subseteq \operatorname{cl}_Y N = N.

Thus \operatorname{cl}_X M \subseteq f^{-1}\left(f(\operatorname{cl}_X M)\right) \subseteq f^{-1}(N) = M.

Hence M is closed and we are done.

{{collapse bottom}}

If we declare that a point x is {{em|close to}} a subset A \subseteq X if x \in \operatorname{cl}_X A, then this terminology allows for a plain English description of continuity: f is continuous if and only if for every subset A \subseteq X, f maps points that are close to A to points that are close to f(A). Similarly, f is continuous at a fixed given point x \in X if and only if whenever x is close to a subset A \subseteq X, then f(x) is close to f(A).

Instead of specifying topological spaces by their open subsets, any topology on X can alternatively be determined by a closure operator or by an interior operator.

Specifically, the map that sends a subset A of a topological space X to its topological closure \operatorname{cl}_X A satisfies the Kuratowski closure axioms. Conversely, for any closure operator A \mapsto \operatorname{cl} A there exists a unique topology \tau on X (specifically, \tau := \{ X \setminus \operatorname{cl} A : A \subseteq X \}) such that for every subset A \subseteq X, \operatorname{cl} A is equal to the topological closure \operatorname{cl}_{(X, \tau)} A of A in (X, \tau). If the sets X and Y are each associated with closure operators (both denoted by \operatorname{cl}) then a map f : X \to Y is continuous if and only if f(\operatorname{cl} A) \subseteq \operatorname{cl} (f(A)) for every subset A \subseteq X.

Similarly, the map that sends a subset A of X to its topological interior \operatorname{int}_X A defines an interior operator. Conversely, any interior operator A \mapsto \operatorname{int} A induces a unique topology \tau on X (specifically, \tau := \{ \operatorname{int} A : A \subseteq X \}) such that for every A \subseteq X, \operatorname{int} A is equal to the topological interior \operatorname{int}_{(X, \tau)} A of A in (X, \tau). If the sets X and Y are each associated with interior operators (both denoted by \operatorname{int}) then a map f : X \to Y is continuous if and only if f^{-1}(\operatorname{int} B) \subseteq \operatorname{int}\left(f^{-1}(B)\right) for every subset B \subseteq Y.{{cite web|title=general topology - Continuity and interior|url=https://math.stackexchange.com/q/1209229|website=Mathematics Stack Exchange}}

== Filters and prefilters ==

{{Main|Filters in topology}}

Continuity can also be characterized in terms of filters. A function f : X \to Y is continuous if and only if whenever a filter \mathcal{B} on X converges in X to a point x \in X, then the prefilter f(\mathcal{B}) converges in Y to f(x). This characterization remains true if the word "filter" is replaced by "prefilter."{{sfn|Dugundji|1966|pp=211–221}}

=Properties=

If f : X \to Y and g : Y \to Z are continuous, then so is the composition g \circ f : X \to Z. If f : X \to Y is continuous and

The possible topologies on a fixed set X are partially ordered: a topology \tau_1 is said to be coarser than another topology \tau_2 (notation: \tau_1 \subseteq \tau_2) if every open subset with respect to \tau_1 is also open with respect to \tau_2. Then, the identity map

\operatorname{id}_X : \left(X, \tau_2\right) \to \left(X, \tau_1\right)

is continuous if and only if \tau_1 \subseteq \tau_2 (see also comparison of topologies). More generally, a continuous function

\left(X, \tau_X\right) \to \left(Y, \tau_Y\right)

stays continuous if the topology \tau_Y is replaced by a coarser topology and/or \tau_X is replaced by a finer topology.

=Homeomorphisms=

Symmetric to the concept of a continuous map is an open map, for which {{em|images}} of open sets are open. If an open map f has an inverse function, that inverse is continuous, and if a continuous map g has an inverse, that inverse is open. Given a bijective function f between two topological spaces, the inverse function f^{-1} need not be continuous. A bijective continuous function with a continuous inverse function is called a {{em|homeomorphism}}.

If a continuous bijection has as its domain a compact space and its codomain is Hausdorff, then it is a homeomorphism.

=Defining topologies via continuous functions=

Given a function

f : X \to S,

where X is a topological space and S is a set (without a specified topology), the final topology on S is defined by letting the open sets of S be those subsets A of S for which f^{-1}(A) is open in X. If S has an existing topology, f is continuous with respect to this topology if and only if the existing topology is coarser than the final topology on S. Thus, the final topology is the finest topology on S that makes f continuous. If f is surjective, this topology is canonically identified with the quotient topology under the equivalence relation defined by f.

Dually, for a function f from a set S to a topological space X, the initial topology on S is defined by designating as an open set every subset A of S such that A = f^{-1}(U) for some open subset U of X. If S has an existing topology, f is continuous with respect to this topology if and only if the existing topology is finer than the initial topology on S. Thus, the initial topology is the coarsest topology on S that makes f continuous. If f is injective, this topology is canonically identified with the subspace topology of S, viewed as a subset of X.

A topology on a set S is uniquely determined by the class of all continuous functions S \to X into all topological spaces X. Dually, a similar idea can be applied to maps X \to S.

Related notions

If f : S \to Y is a continuous function from some subset S of a topological space X then a {{em|{{visible anchor|continuous extension|Continuous extension}}}} of f to X is any continuous function F : X \to Y such that F(s) = f(s) for every s \in S, which is a condition that often written as f = F\big\vert_S. In words, it is any continuous function F : X \to Y that restricts to f on S. This notion is used, for example, in the Tietze extension theorem and the Hahn–Banach theorem. If f : S \to Y is not continuous, then it could not possibly have a continuous extension. If Y is a Hausdorff space and S is a dense subset of X then a continuous extension of f : S \to Y to X, if one exists, will be unique. The Blumberg theorem states that if f : \R \to \R is an arbitrary function then there exists a dense subset D of \R such that the restriction f\big\vert_D : D \to \R is continuous; in other words, every function \R \to \R can be restricted to some dense subset on which it is continuous.

Various other mathematical domains use the concept of continuity in different but related meanings. For example, in order theory, an order-preserving function f : X \to Y between particular types of partially ordered sets X and Y is continuous if for each directed subset A of X, we have \sup f(A) = f(\sup A). Here \,\sup\, is the supremum with respect to the orderings in X and Y, respectively. This notion of continuity is the same as topological continuity when the partially ordered sets are given the Scott topology.{{cite book |last=Goubault-Larrecq |first=Jean |title=Non-Hausdorff Topology and Domain Theory: Selected Topics in Point-Set Topology |publisher=Cambridge University Press|year=2013 |isbn=978-1107034136}}{{cite book |last1=Gierz |first1=G. |last2=Hofmann |first2=K. H. |last3=Keimel |first3=K. |last4=Lawson |first4=J. D. |last5=Mislove |first5=M. W. |last6=Scott |first6=D. S. |title=Continuous Lattices and Domains |volume=93 |series=Encyclopedia of Mathematics and its Applications |publisher=Cambridge University Press |year=2003 |isbn=0521803381 |url-access=registration |url=https://archive.org/details/continuouslattic0000unse}}

In category theory, a functor

F : \mathcal C \to \mathcal D

between two categories is called {{em|continuous}} if it commutes with small limits. That is to say,

\varprojlim_{i \in I} F(C_i) \cong F \left(\varprojlim_{i \in I} C_i \right)

for any small (that is, indexed by a set I, as opposed to a class) diagram of objects in \mathcal C.

A {{em|continuity space}} is a generalization of metric spaces and posets,{{cite journal | title = Quantales and continuity spaces | citeseerx=10.1.1.48.851 | first = R. C. | last =Flagg | journal = Algebra Universalis | year = 1997 | volume=37 | issue=3 | pages=257–276 | doi=10.1007/s000120050018 | s2cid=17603865 }}{{cite journal | title = All topologies come from generalized metrics | first = R. | last = Kopperman | journal = American Mathematical Monthly | year = 1988 |volume=95 |issue=2 |pages=89–97 |doi=10.2307/2323060 | jstor = 2323060 }} which uses the concept of quantales, and that can be used to unify the notions of metric spaces and domains.{{cite journal | title = Continuity spaces: Reconciling domains and metric spaces | first1 = B. | last1 = Flagg | first2 = R. | last2 = Kopperman | journal = Theoretical Computer Science |volume=177 |issue=1 |pages=111–138 |doi=10.1016/S0304-3975(97)00236-3 | year = 1997 | doi-access = free }}

In measure theory, a function f : E \to \mathbb{R}^k defined on a Lebesgue measurable set E \subseteq \mathbb{R}^n is called approximately continuous at a point x_0 \in E if the approximate limit of f at x_0 exists and equals f(x_0). This generalizes the notion of continuity by replacing the ordinary limit with the approximate limit. A fundamental result known as the Stepanov-Denjoy theorem states that a function is measurable if and only if it is approximately continuous almost everywhere.{{cite book |last=Federer |first=H. |title=Geometric measure theory |publisher=Springer-Verlag |series=Die Grundlehren der mathematischen Wissenschaften |volume=153 |location=New York |year=1969 |isbn= |pages=}}

See also

References

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Bibliography

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