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en>CiaPan: /* Example calculation */ minor formatting, style and linking corrections

2014-06-12T13:08:44Z

Example calculation: minor formatting, style and linking corrections

← Older revision		Revision as of 15:08, 12 June 2014
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	~~{{Unreferenced\|date=December 2009}}~~		Hi there. Allow me start by [http://Articles.Baltimoresun.com/2011-02-21/specialsection/bs-hs-std-testing-20110221_1_std-testing-gonorrhea-and-chlamydia-chlamydia-cases introducing] the writer, her title is Myrtle Cleary. Hiring has been my profession for some time but I've already applied for an additional one. To collect cash is a thing that I'm completely addicted [http://Reinodoprazer.Com.br/index.php?do=/blog/326/tips-about-how-to-overcome-candidiasis-easily/ website] to. Years in the past we at home std test moved to North Dakota [http://apcbook.com.ng/index.php?do=/profile-446/info/ apcbook.com.ng] and std testing at home I adore each working day residing here.<br><br>Here is at home std test my web site :: at home std testing ([http://www.1A-pornotube.com/user/GCalvert mouse click the up coming article])
	~~In [[mathematics]], a '''doubly periodic function''' is a [[function (mathematics)\|function]] defined at all points on the [~~[complex plane]] and having two "periods", which are complex numbers ''u'' and ''v'' that are [[linear independence\|linearly independent]] as vectors over the [[field (mathematics)\|field]] of [[real number]]s. That ''u'' and ''v'' are periods of a function ''ƒ'' means that

	:~~<math>f(z + u) = f(z + v) = f(z)\, <~~/~~math>~~

	~~for all values of the complex number ''z''~~.

	~~The doubly periodic function is thus a two~~-dimensional extension of the simpler [[periodic function\|singly periodic function]], which repeats itself in a single dimension. Familiar examples of functions with a single period on the real number line include the [[trigonometric functions]] like cosine and ~~sine. In the [[complex plane]~~] the ~~[[exponential function]] ''e''<sup>''z''</sup>~~ is ~~a singly periodic function, with period 2''πi'~~'.

	~~As an arbitrary mapping from pairs of reals (or complex numbers) to reals,~~ a ~~doubly periodic function can be constructed with little effort. For example, assume~~ that ~~the periods are 1 and ~~'~~'i'', so that the repeating lattice is the set of unit squares with vertices at the~~ [~~[Gaussian integer]]s~~. ~~Values in the prototype square (i~~.e. ~~''x'' + ''iy'' where 0 ≤ ''x'' < 1 and 0 ≤ ''y'' < 1) can be assigned rather arbitrarily and then 'copied'~~ to ~~adjacent squares. This function will then be necessarily doubly periodic~~.

	~~If the vectors 1 and ''i''~~ in ~~this example are replaced by linearly independent vectors ''u'' and ''v''~~ the prototype square becomes a prototype parallelogram, which still [[tessellation\|tiles the plane]]. And the "origin" of the lattice of parallelograms does not have to be the point 0; the lattice can start from any point. In other words, we ~~can think of the plane and its associated functional values as remaining fixed, and mentally translate the lattice~~ to ~~gain insight into the function's characteristics.~~

	~~If a doubly periodic function is also a~~ [[Complex analysis\|''complex function'']] that satisfies the [[Cauchy–Riemann equations]] and provides an analytic function away from some set of isolated [[Pole (complex analysis)\|poles]] – in other words, a [[meromorphic function]] – then a lot of information about such a function can be obtained by applying some basic theorems from complex analysis.

	* A non-constant meromorphic doubly periodic function cannot be bounded on the prototype parallelogram. ~~For if it were it would be bounded everywhere, and therefore constant by [[liouville's theorem (complex analysis)\|Liouville's theorem]]~~.

	* Since the function is meromorphic, it has no essential singularities and its poles are isolated. ~~Therefore a translated lattice that does not pass through any pole can be constructed~~. ~~The [[line integral\|contour integral]~~] ~~around any parallelogram in the lattice must vanish, because the values assumed by the doubly periodic function along the two pairs of parallel sides are identical,~~ and the two pairs of sides are traversed in opposite directions as we move around the contour. Therefore, by the [[residue theorem]], the function cannot have a single simple pole inside each parallelogram – it must have at ~~least two simple poles within~~ each ~~parallelogram (Jacobian case), or it must have one or more poles of order greater than one (Weierstrassian case)~~.

	* A similar argument can be applied to the function ''g'' = 1/''ƒ'' where ''ƒ'' is meromorphic and doubly periodic. Under this inversion the [[zero (complex analysis)\|zeroes]] of ''ƒ'' become the poles of ''g'', and ''vice versa''. So the meromorphic doubly periodic function ''ƒ'' cannot have one simple zero lying within each parallelogram on the lattice—it must have at ~~least two simple zeroes, or it must have~~ at ~~least one zero of multiplicity greater than one~~. ~~It follows that ''ƒ'' cannot attain any value just once, since ''ƒ'' minus that value would itself be a meromorphic doubly periodic function with just one zero~~.

	~~== See also ==~~
	* [[Elliptic function]]
	* [[Fundamental pair of periods]]
	* [[Jacobi's elliptic functions]]
	* [[Period mapping]]
	* [[Weierstrass's elliptic functions]]

	~~==External links==~~
	* {{springer\|title=Double-periodic function\|id=p/~~d033930}}~~

	~~{{DEFAULTSORT:Doubly-Periodic Function}}~~
	~~[[Category:Analytic functions]~~]

en>Bhny: copy edit

2013-12-27T21:53:55Z

copy edit

← Older revision		Revision as of 23:53, 27 December 2013
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			In [[mathematics]], a '''doubly periodic function''' is a [[function (mathematics)\|function]] defined at all points on the [[complex plane]] and having two "periods", which are complex numbers ''u'' and ''v'' that are [[linear independence\|linearly independent]] as vectors over the [[field (mathematics)\|field]] of [[real number]]s. That ''u'' and ''v'' are periods of a function ''ƒ'' means that

			:<math>f(z + u) = f(z + v) = f(z)\, </math>

			for all values of the complex number ''z''.

			The doubly periodic function is thus a two-dimensional extension of the simpler [[periodic function\|singly periodic function]], which repeats itself in a single dimension. Familiar examples of functions with a single period on the real number line include the [[trigonometric functions]] like cosine and sine. In the [[complex plane]] the [[exponential function]] ''e''<sup>''z''</sup> is a singly periodic function, with period 2''πi''.

			As an arbitrary mapping from pairs of reals (or complex numbers) to reals, a doubly periodic function can be constructed with little effort. For example, assume that the periods are 1 and ''i'', so that the repeating lattice is the set of unit squares with vertices at the [[Gaussian integer]]s. Values in the prototype square (i.e. ''x'' + ''iy'' where 0 ≤ ''x'' < 1 and 0 ≤ ''y'' < 1) can be assigned rather arbitrarily and then 'copied' to adjacent squares. This function will then be necessarily doubly periodic.

			If the vectors 1 and ''i'' in this example are replaced by linearly independent vectors ''u'' and ''v'' the prototype square becomes a prototype parallelogram, which still [[tessellation\|tiles the plane]]. And the "origin" of the lattice of parallelograms does not have to be the point 0; the lattice can start from any point. In other words, we can think of the plane and its associated functional values as remaining fixed, and mentally translate the lattice to gain insight into the function's characteristics.

			If a doubly periodic function is also a [[Complex analysis\|''complex function'']] that satisfies the [[Cauchy–Riemann equations]] and provides an analytic function away from some set of isolated [[Pole (complex analysis)\|poles]] – in other words, a [[meromorphic function]] – then a lot of information about such a function can be obtained by applying some basic theorems from complex analysis.

			* A non-constant meromorphic doubly periodic function cannot be bounded on the prototype parallelogram. For if it were it would be bounded everywhere, and therefore constant by [[liouville's theorem (complex analysis)\|Liouville's theorem]].

			* Since the function is meromorphic, it has no essential singularities and its poles are isolated. Therefore a translated lattice that does not pass through any pole can be constructed. The [[line integral\|contour integral]] around any parallelogram in the lattice must vanish, because the values assumed by the doubly periodic function along the two pairs of parallel sides are identical, and the two pairs of sides are traversed in opposite directions as we move around the contour. Therefore, by the [[residue theorem]], the function cannot have a single simple pole inside each parallelogram – it must have at least two simple poles within each parallelogram (Jacobian case), or it must have one or more poles of order greater than one (Weierstrassian case).

			* A similar argument can be applied to the function ''g'' = 1/''ƒ'' where ''ƒ'' is meromorphic and doubly periodic. Under this inversion the [[zero (complex analysis)\|zeroes]] of ''ƒ'' become the poles of ''g'', and ''vice versa''. So the meromorphic doubly periodic function ''ƒ'' cannot have one simple zero lying within each parallelogram on the lattice—it must have at least two simple zeroes, or it must have at least one zero of multiplicity greater than one. It follows that ''ƒ'' cannot attain any value just once, since ''ƒ'' minus that value would itself be a meromorphic doubly periodic function with just one zero.

			== See also ==
			* [[Elliptic function]]
			* [[Fundamental pair of periods]]
			* [[Jacobi's elliptic functions]]
			* [[Period mapping]]
			* [[Weierstrass's elliptic functions]]

			==External links==
			* {{springer\|title=Double-periodic function\|id=p/d033930}}

			{{DEFAULTSORT:Doubly-Periodic Function}}
			[[Category:Analytic functions]]

119.154.130.170: /* Process */

2012-06-16T10:29:00Z

Process

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