Fixed point: Difference between revisions

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A '''Fixed point''' <math> L </math> of a [[functor]] <math> F </math> is a solution of equation
A '''fixed point''' is a point in the domain of a [[function (mathematics)|function]] that is mapped to itself. Thus, a fixed point of a function ''f'' is a point ''x'' such that <math>f(x) = x</math>.
: <math>F[L]=L</math>,
that is a point that is mapped to itself.


==Simple examples==
==Examples==


===Elementary functions===
The squaring function is the function that maps each number to its [[square (arithmetics)|square]], so a fixed point of the squaring function is a number that equals its square. There are two such numbers: 0 and 1.
In particular, functor can be elementaty function. For example, 0 and 1 are fixed points of function [[sqrt]], because <math>\sqrt{0}=0</math> and
<math>\sqrt{1}=1</math>.


In similar way, 0 is fixed point of [[sine]] function, because <math>\sin(0)=0</math> .
In similar way, 0 is fixed point of [[sine]] function, because <math>\sin(0)=0</math>.


===Operators===
The function ''f'' can also be a [[linear operator]]. In this case, the fixed point is an [[eigenvector]] with [[eigenvalue]] equal to unity. For instance, the [[exponential function]] is a fixed point of the [[differential operator]] because the derivative of e<sup>''x''</sup> is again e<sup>''x''</sup>. Similarly, the [[Gaussian exponential]] exp(−''x''<sup>2</sup>/2) is a fixed point of the [[Fourier transform]] operator <math>\mathcal{F}</math> defined by
The functor in the equation, defining a fixed point, can be a [[linear operator]]. In this case, the fixed point of the functor <math>F</math> is its [[eigenfunction]] with [[eigenvalue]] equal to unity.  
:<math> \mathcal{F}[f](p) = \frac{1}{\sqrt{2\pi}} \int_{-\infty}^{\infty} f(x) \exp(-{\rm i}px) \, {\rm d}x. </math> &nbsp;&nbsp;&nbsp;&nbsp;<ref>The expression <math>\mathcal{F}[f](p)</math> on the left-hand side means the value at ''p'' of the Fourier transform <math>\mathcal{F}[f]</math>; the Fourier transform is the result of applying the operator <math>\mathcal{F}</math> to the function ''f''.</ref>
 
[[Exponential]] if fixed point or [[operator of differentiation]] D,
because
<math>{\rm D}~ \exp(x) =\exp'(x)=\exp(x)</math>
 
The [[Gaussian exponential]]
:<math>L(x)=\exp(-x^2/2)</math> , with <math>x \in \mathbb{R}</math> and <math>\mathbb{R}</math> the [[real number|reals]],
is fixed point of the [[Fourier operator]], defined with its action on a function <math>g</math>:
:(3) <math>F(g)(p)=\frac{1}{\sqrt{2\pi}}\int_{-\infty}^{\infty}
g(x)\exp(-{\rm i}px) {\rm d}x </math>
in general, functors have no need to be linear, and there is no [[associativity]]
at application of several functors in row, and parenthesis are necessary in the left hand side of eapression (3).
<ref name="ambiguity">
Note that that there is certain [[ambiguity]] in commonly used writing of mathematical formulas, omiting sign * of multiplication; in equation (3), expression  
<math>F(g)(p)</math> does not mean that <math>F(g)</math> is multiplied to value of <math>p</math>; it means that result <math>F(g)</math> of action of operator <math>F </math> on function <math>g</math>, which is also a function, is [[evaluate]]d at argument <math>p</math>.
</ref>


==Fixed points of [[exponential]] and fixed points of [[logarithm]]==
==Fixed points of [[exponential]] and fixed points of [[logarithm]]==

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A fixed point is a point in the domain of a function that is mapped to itself. Thus, a fixed point of a function f is a point x such that .

Examples

The squaring function is the function that maps each number to its square, so a fixed point of the squaring function is a number that equals its square. There are two such numbers: 0 and 1.

In similar way, 0 is fixed point of sine function, because .

The function f can also be a linear operator. In this case, the fixed point is an eigenvector with eigenvalue equal to unity. For instance, the exponential function is a fixed point of the differential operator because the derivative of ex is again ex. Similarly, the Gaussian exponential exp(−x2/2) is a fixed point of the Fourier transform operator defined by

    [1]

Fixed points of exponential and fixed points of logarithm

FIg.1. is shown with levels , , , , , in the complex -plane
Fig.2. The same as FIg.1 for function

Fixed points can be searched graphically. Fig.1 shows the graphical search of fixed points of logarithm, i.e., solutions of the equation

(10)

There are no real solutions for this equation, but there are two complex-congjugated solutions and . However, the value of cannot be estimated well from the figure (1), but the straigtgorward iteration allows the precise estimate. Few hundreds of iterations are sufficient to get error of order of last significant figure in the approximation

(11)

Fixed points of exp are not the same as those of ln

Fixed points of logarithm should not be confised with fixed points of exponential, shown in FIgure 2. These fixed points are solutions of equations

(12)

They can be expressed also as solution of equation

(13) for some integer

For example, at

(13)

is fixed point of the exponential, but is not fixed point of natural logarithm.

In the case of exponential and natural logarithm, all fixed points are complex. However, the real fixed points exist at . For example, at , number e is fixed point of both, and ; and at , numbers 2 and 4 are their fixed points.

FIg.3. Example of graphic solution of equation for (two real solutions, and ), (one real solution ) (no real solutions).

Finding of real fixed points is presented graphically in Figure 3. The black curve represents the identical function in the left hand side of equation

(14)

the colored curves represent the function in the right hand side for , , and . In the last case, there are no real solutions, but the complex fixed points are complex numbers and . Within few hundred iterations of equation (14), they can be approcimated with many decimal digits;

(15).

Such evaluation can be performed in real time with any high level algorithmic language – Maple, Mathematica, that allow to specify number of correct decimal digits desirable in the result.

The mathematical proof of existence of the fixed points of the exponential can be found in the old paper by Helmuth Kneser [2]. Recently, Henryk Trappmann had generalized this proof for the exponentiation of arbitrary real base, but his theorem is not yet uploaded.

Tetration

FIg.4. parameters of asymptotic of tetration versus logarithm of the base

The fixed points of logarithm determine the asymptotic properties of analytic extension of tetration . In some range of the complex -plane, the tetration can be approximated with asymptotic

(32) 

where

(33) 

and are fixed complex numbers, dependent on . Possible values of fixed points are shown with thin black curves versus logarithm on base . At , the fixed points are complex; the real part is shown with solid curve, the imaginary part is shown with dashed curve.

Green curves in Figure 4 represent the parameter in (33), again, the dased curve shows the imaginary part, and real and imaginary parts of the asymptotic period . See article tetration for details.

Projectors

Functor on the space is called Projector, if for all .

Any function of subset of functions is fixed point of projector .

In common use are projectors of the 3-dimensional space to 2-dimensional space. Such projectors allow to make flat pictures of 3-dimensional objects. Any point at the plane of image is fixed point of such a projector.

Common fixed points

The same element may be fixed point of several projectors.

Sometimes, such common fixed points can be approximated using iterations. If there are two projectors and , then the sequence of elements, approximating the common fixed point of these projectors can be constructed in the following way:

Such a sequence is used to approximate the amplitude-phase behavior of ultra-short pulses in the FROG systems [3][4]. Amplitide and phase in ultra-short pulses can be measured only with another ultra-short pulse; so, some nonlinear interaction is used to recover the temporal behavior of the pulse. The set of equations (usually two) is solved numerically, projecting the probe function to the spaces of solutions of each equation sequentially.</ref>.

Notes

  1. The expression on the left-hand side means the value at p of the Fourier transform ; the Fourier transform is the result of applying the operator to the function f.
  2. Helmuth Kneser. "Reelle analytische Lösungen der Gleichung und verwandter Funktionalgleichungen". Journal für die reine und angewandte Mathematik 187: 8-67.
  3. Rick Trebino, Kenneth W. DeLong, David N. Fittinghoff, John N. Sweetser, Marco A. Krumbügel, and Bruce A. Richman. Measuring ultrashort laser pulses in the time-frequency domain using frequency-resolved optical gating. Rev. Sci. Instrum. 68, 3277 (1997); DOI:10.1063/1.1148286
  4. Giulio Cerullo and Sandro De Silvestri. Ultrafast optical parametric amplifiers. Rev. Sci. Instrum. 74, 1 (2003); DOI:10.1063/1.1523642

See also