Table of spherical harmonics - Revision history

en>Bduke: Reverted 1 edit by 2601:1:8D00:21F:51AA:2DA5:C3F:967A (talk): Rv last change. Not according to Chisholm reference. (TW)

2014-12-14T20:38:05Z

Reverted 1 edit by 2601:1:8D00:21F:51AA:2DA5:C3F:967A (talk): Rv last change. Not according to Chisholm reference. (TW)

← Older revision		Revision as of 22:38, 14 December 2014
Line 1:		Line 1:
	~~The author~~ is ~~known as Irwin Wunder~~ but it's not the most ~~masucline name~~ out there. ~~Years ago we moved~~ to North Dakota. ~~Managing people is his occupation~~. ~~To gather cash is what his~~ family ~~members and him enjoy~~.<br><br>my ~~page ...~~ [http://~~riddlesandpoetry~~.~~com~~/~~?q=node~~/~~19209 home~~ std test ~~kit~~]		Marvella at home std testing is what you can call her but it's not the most feminine title out [http://www.biogids.nl/biobank/2014-06-13/how-can-1-especially-get-around-todays-diseases std home test] there. What I love doing is to collect badges but I've been taking on new things recently. Hiring has been my at home std test [http://Www.wvdhhr.org/hotlinenumbers.asp occupation] for some time but I've currently utilized for an additional 1. For many years he's been residing in North Dakota and his [http://Www.Healthcentral.com/genital-herpes/h/female-symptoms-herpes-pictures.html family loves] it.<br><br>Review [http://nxnn.info/user/G8498 at home std test] my blog post: [http://spermdonorinfo.co.uk/groups/eliminate-a-yeast-infection-with-one-of-these-tips/ over the counter std test]

en>Loudandras: Undid revision 594558158 by 18.189.97.183 (talk): 'align' exists, 'aligned' doesn't. The parser error came from the server side, edit was unnecessary.

2014-02-08T21:50:41Z

Undid revision 594558158 by 18.189.97.183 (talk): 'align' exists, 'aligned' doesn't. The parser error came from the server side, edit was unnecessary.

← Older revision		Revision as of 23:50, 8 February 2014
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	~~In [[mathematics]], a '''complex differential form''' is a [[differential form]] on a [[manifold]] (usually a [[complex manifold]]) which~~ is ~~permitted to have [[complex number\|complex]] coefficients.~~		The author is known as Irwin Wunder but it's not the most masucline name out there. Years ago we moved to North Dakota. Managing people is his occupation. To gather cash is what his family members and him enjoy.<br><br>my page ... [http://riddlesandpoetry.com/?q=node/19209 home std test kit]

	~~Complex forms have broad applications in [[differential geometry]]. On complex manifolds, they are fundamental and serve~~ as the basis for much of [[algebraic geometry]], [[Kähler metric\|Kähler geometry]], and [[Hodge theory]]. Over non-complex manifolds, they also play a role in the study of [[almost complex structure]]s~~, the theory of [[spinor]]s, and [[CR structure]]s.~~

	Typically, complex forms are considered because of some desirable decomposition that the forms admit. On a complex manifold, for instance, any complex ''k''-form can be decomposed uniquely into a sum of so-called '''(''p'',''q'')-forms''': roughly, wedges of ''p'' [[exterior derivative\|differentials]] of the holomorphic coordinates with ''q'' differentials of their complex conjugates. The ensemble of (''p'',''q'')-forms becomes the primitive object of study, and determines a finer geometrical structure on the ~~manifold than the ''k''-forms. Even finer structures exist, for example, in cases where [[Hodge theory]] applies.~~

	~~==Differential forms on a complex manifold==~~
	~~Suppose that ''M'' is a [[complex manifold]]. Then~~ there ~~is a local [[coordinate system]] consisting of ''n'' complex-valued functions ''z''<sup>1</sup>,.~~.~~.,z<sup>''n''</sup> such that the coordinate transitions from one patch~~ to another are [[holomorphic function]]s of these variables. The space of complex forms carries a rich structure, depending fundamentally on the fact that these transition functions are holomorphic, rather than just [[smooth manifold\|smooth]].

	~~===One-forms===~~
	We begin with the case of one-forms. First decompose the complex coordinates into their real and imaginary parts: ''z''<sup>''j''</sup>=''x''<sup>''j''</sup>+''iy''<sup>''j''</sup> for each ''j''. Letting
	~~:<math>dz^j=dx^j+idy^j,\quad d\bar{z}^j=dx^j-idy^j,</math>~~
	~~one sees that any differential form with complex coefficients can be written uniquely as a sum~~
	~~:<math>\sum_{j=1}^n f_jdz^j+g_jd\bar{z}^j.</math>~~

	Let Ω<sup>1,0</sup> be the space of complex differential forms containing only <math>dz</math>'s and Ω<sup>0,1</sup> be the space of forms containing only <math>d\bar{z}</math>'s. One can show, by the [[Cauchy-Riemann equations]], that the spaces Ω<sup>1,0</sup> and Ω<sup>0,1</sup> are stable under holomorphic coordinate changes. In other words, if one makes a different choice ''w''<sub>i</sub> of holomorphic coordinate system, then elements of Ω<sup>1,0</sup> transform [[tensor]]ially, as do elements of Ω<sup>0,1</sup>. Thus the spaces Ω<sup>0,1</sup> and Ω<sup>1,0</sup> determine complex [[vector bundle]]s on the complex manifold.

	~~===Higher degree forms===~~
	~~The wedge product of complex differential forms~~ is ~~defined in the same way as with real forms~~. ~~Let ''p'' and ''q'' be a pair of non-negative integers ≤ ''n''. The space Ω<sup>p,q</sup> of (''p'',''q'')-forms~~ is ~~defined by taking linear combinations of the wedge products of ''p'' elements from Ω<sup>1,0</sup>~~ and ~~''q'' elements from Ω<sup>0,1</sup>~~. ~~Symbolically,~~
	~~:<math>\Omega^{p,q}=\Omega^{1,0}\wedge\dotsb\wedge\Omega^{1,0}\wedge\Omega^{0,1}\wedge\dotsb\wedge\Omega^{0,1}</math>~~
	~~where there are ''p'' factors of Ω<sup>1,0</sup> and ''q'' factors of Ω~~<~~sup~~>~~0,1~~<~~/sup~~>. ~~Just as with the two spaces of 1-forms, these are stable under holomorphic changes of coordinates, and so determine vector bundles~~.

	If ''E''<sup>''k''</sup> is the space of all complex differential forms of total degree ''k'', then each element of ''E''<sup>''k''</sup> can be expressed in a unique way as a linear combination of elements from among the spaces Ω<sup>p,q</sup> with ''p''+''q''=''k''. ~~More succinctly, there is a [~~[~~direct sum of vector bundles\|direct sum]] decomposition~~
	~~:<math>E^k=\Omega^{k,0}\oplus\Omega^{k-1,1}\oplus\dotsb\oplus\Omega^{1,k-1}\oplus\Omega^{0,k}=\bigoplus_{p+q=k}\Omega^{p,q}.</math>~~
	~~Because this direct sum decomposition is stable under holomorphic coordinate changes, it also determines a vector bundle decomposition.~~

	~~In particular, for each ''k'' and each ''p'' and ''q'' with ''p''+''q''=''k'', there is a canonical projection of vector bundles~~
	~~:<math>\pi^{p,q}:E^k\rightarrow\Omega^{p,q}.</math>~~

	~~===The Dolbeault operators===~~
	~~The usual exterior derivative defines a mapping of sections ''d''~~:~~''E''<sup>''k''<~~/~~sup>→''E''<sup>''k+1''<~~/~~sup>~~. ~~Restricting this to sections of Ω<sup>''p,q''</sup>, one can show that in fact ''d'':Ω<sup>''p,q''</sup>→Ω<sup>''p''+1,''q''</sup> + Ω<sup>''p'',''q''+1<~~/~~sup>.{{clarify\|reason=This is an object. In fact, it exists~~? ~~Equals something?\|date=November 2011}} The exterior derivative does not in itself reflect the more rigid complex structure of the manifold.~~

	~~Using ''d'' and the projections defined in the previous subsection, it is possible to define the '''Dolbeault operators''':~~
	~~:<math>\partial=\pi^{p+1,q}\circ d:\Omega^{p,q}\rightarrow\Omega^{p+1,q},\quad \bar{\partial}=\pi^{p,q+1}\circ d:\Omega^{p,q}\rightarrow\Omega^{p,q+1}</math>~~
	~~To describe these operators in local coordinates, let~~
	~~:<math>\alpha=\sum_{\|I\|=p,\|J\|=~~q~~}\ f_{IJ}\,dz^I\wedge d\bar{z}^J\in\Omega^{p,q}</math>~~
	~~where ''I'' and ''J'' are [[multi-index\|multi-indices]]. Then~~
	~~:<math>\partial\alpha=\sum_{\|I\|,\|J\|}\sum_\ell \frac{\partial f_{IJ}}{\partial z^\ell}\,dz^\ell\wedge dz^I\wedge d\bar{z}^J</math>~~
	~~:<math>\bar{\partial}\alpha=\sum_{\|I\|,\|J\|}\sum_\ell \frac{\partial f_{IJ}}{\partial \bar{z}^\ell}d\bar{z}^\ell\wedge dz^I\wedge d\bar{z}^J.</math>~~

	~~The following properties are seen to hold:~~
	~~:<math>d~~=~~\partial+\bar{\partial}<~~/~~math>~~
	~~:<math>\partial^2=\bar{\partial}^2=\partial\bar{\partial}+\bar{\partial}\partial=0.</math>~~

	~~These operators and their properties form the basis for [[Dolbeault cohomology]] and many aspects of [[Hodge theory]].~~

	~~===Holomorphic forms===~~
	~~For each ''p'', a holomorphic ''p''-form is a holomorphic section of the bundle Ω<sup>''p,0''</sup>. In local coordinates, then, a holomorphic ''p''-form can be written in the form~~

	~~:<math>\alpha=\sum_{\|I\|=p}f_I\,dz^I</math>~~

	~~where the ''f''<sub>''I''</sub> are holomorphic functions. Equivalently, the (''p'',0)-form α is holomorphic if and only if~~
	~~:<math>\bar{\partial}\alpha=0.</math>~~
	The [[sheaf (mathematics)\|sheaf]] of holomorphic ''p''-forms is often written Ω<sup>''p''</sup>, although this can sometimes lead to confusion so many authors tend to adopt an alternative notation.

	~~==See also==~~

	*[[Dolbeault complex]]
	*[[Frölicher spectral sequence]]
	*[[Differential of the first kind]]

	~~==References==~~
	* {{cite book\|last=Wells\|first=R.O.\|authorlink=Raymond O. Wells, Jr.\|title=Differential analysis on complex manifolds\|year=1973\|publisher=Springer-Verlag\|isbn=0-387-90419-0}}

	~~[[Category:Complex manifolds]]~~
	~~[[Category:Differential forms]~~]

en>Susilehtola: /* Real spherical harmonics */ - Restore atomic orbital symbols

2014-01-18T09:31:47Z

Real spherical harmonics: - Restore atomic orbital symbols

← Older revision		Revision as of 11:31, 18 January 2014
Line 1:		Line 1:
	~~She~~ is ~~known~~ by the ~~title~~ of ~~Myrtle Shryock~~. ~~Bookkeeping~~ is ~~what I do~~. He is ~~really fond~~ of ~~doing ceramics but he~~ is ~~struggling~~ to ~~discover time for~~ it. ~~Years~~ in the ~~past we moved~~ to ~~North Dakota~~ and I ~~adore every day living here.~~<br><br>~~Feel free~~ to ~~surf to my homepage~~ :: ~~at home std testing - [http~~://~~www~~.~~alemcheap.fi~~/~~show~~/the-~~way~~-to-~~cure~~-an-~~unpleasant~~-~~candidiasis Suggested Internet site~~],		In [[mathematics]], a '''complex differential form''' is a [[differential form]] on a [[manifold]] (usually a [[complex manifold]]) which is permitted to have [[complex number\|complex]] coefficients.

			Complex forms have broad applications in [[differential geometry]]. On complex manifolds, they are fundamental and serve as the basis for much of [[algebraic geometry]], [[Kähler metric\|Kähler geometry]], and [[Hodge theory]]. Over non-complex manifolds, they also play a role in the study of [[almost complex structure]]s, the theory of [[spinor]]s, and [[CR structure]]s.

			Typically, complex forms are considered because of some desirable decomposition that the forms admit. On a complex manifold, for instance, any complex ''k''-form can be decomposed uniquely into a sum of so-called '''(''p'',''q'')-forms''': roughly, wedges of ''p'' [[exterior derivative\|differentials]] of the holomorphic coordinates with ''q'' differentials of their complex conjugates. The ensemble of (''p'',''q'')-forms becomes the primitive object of study, and determines a finer geometrical structure on the manifold than the ''k''-forms. Even finer structures exist, for example, in cases where [[Hodge theory]] applies.

			==Differential forms on a complex manifold==
			Suppose that ''M'' is a [[complex manifold]]. Then there is a local [[coordinate system]] consisting of ''n'' complex-valued functions ''z''<sup>1</sup>,...,z<sup>''n''</sup> such that the coordinate transitions from one patch to another are [[holomorphic function]]s of these variables. The space of complex forms carries a rich structure, depending fundamentally on the fact that these transition functions are holomorphic, rather than just [[smooth manifold\|smooth]].

			===One-forms===
			We begin with the case of one-forms. First decompose the complex coordinates into their real and imaginary parts: ''z''<sup>''j''</sup>=''x''<sup>''j''</sup>+''iy''<sup>''j''</sup> for each ''j''. Letting
			:<math>dz^j=dx^j+idy^j,\quad d\bar{z}^j=dx^j-idy^j,</math>
			one sees that any differential form with complex coefficients can be written uniquely as a sum
			:<math>\sum_{j=1}^n f_jdz^j+g_jd\bar{z}^j.</math>

			Let Ω<sup>1,0</sup> be the space of complex differential forms containing only <math>dz</math>'s and Ω<sup>0,1</sup> be the space of forms containing only <math>d\bar{z}</math>'s. One can show, by the [[Cauchy-Riemann equations]], that the spaces Ω<sup>1,0</sup> and Ω<sup>0,1</sup> are stable under holomorphic coordinate changes. In other words, if one makes a different choice ''w''<sub>i</sub> of holomorphic coordinate system, then elements of Ω<sup>1,0</sup> transform [[tensor]]ially, as do elements of Ω<sup>0,1</sup>. Thus the spaces Ω<sup>0,1</sup> and Ω<sup>1,0</sup> determine complex [[vector bundle]]s on the complex manifold.

			===Higher degree forms===
			The wedge product of complex differential forms is defined in the same way as with real forms. Let ''p'' and ''q'' be a pair of non-negative integers ≤ ''n''. The space Ω<sup>p,q</sup> of (''p'',''q'')-forms is defined by taking linear combinations of the wedge products of ''p'' elements from Ω<sup>1,0</sup> and ''q'' elements from Ω<sup>0,1</sup>. Symbolically,
			:<math>\Omega^{p,q}=\Omega^{1,0}\wedge\dotsb\wedge\Omega^{1,0}\wedge\Omega^{0,1}\wedge\dotsb\wedge\Omega^{0,1}</math>
			where there are ''p'' factors of Ω<sup>1,0</sup> and ''q'' factors of Ω<sup>0,1</sup>. Just as with the two spaces of 1-forms, these are stable under holomorphic changes of coordinates, and so determine vector bundles.

			If ''E''<sup>''k''</sup> is the space of all complex differential forms of total degree ''k'', then each element of ''E''<sup>''k''</sup> can be expressed in a unique way as a linear combination of elements from among the spaces Ω<sup>p,q</sup> with ''p''+''q''=''k''. More succinctly, there is a [[direct sum of vector bundles\|direct sum]] decomposition
			:<math>E^k=\Omega^{k,0}\oplus\Omega^{k-1,1}\oplus\dotsb\oplus\Omega^{1,k-1}\oplus\Omega^{0,k}=\bigoplus_{p+q=k}\Omega^{p,q}.</math>
			Because this direct sum decomposition is stable under holomorphic coordinate changes, it also determines a vector bundle decomposition.

			In particular, for each ''k'' and each ''p'' and ''q'' with ''p''+''q''=''k'', there is a canonical projection of vector bundles
			:<math>\pi^{p,q}:E^k\rightarrow\Omega^{p,q}.</math>

			===The Dolbeault operators===
			The usual exterior derivative defines a mapping of sections ''d'':''E''<sup>''k''</sup>→''E''<sup>''k+1''</sup>. Restricting this to sections of Ω<sup>''p,q''</sup>, one can show that in fact ''d'':Ω<sup>''p,q''</sup>→Ω<sup>''p''+1,''q''</sup> + Ω<sup>''p'',''q''+1</sup>.{{clarify\|reason=This is an object. In fact, it exists? Equals something?\|date=November 2011}} The exterior derivative does not in itself reflect the more rigid complex structure of the manifold.

			Using ''d'' and the projections defined in the previous subsection, it is possible to define the '''Dolbeault operators''':
			:<math>\partial=\pi^{p+1,q}\circ d:\Omega^{p,q}\rightarrow\Omega^{p+1,q},\quad \bar{\partial}=\pi^{p,q+1}\circ d:\Omega^{p,q}\rightarrow\Omega^{p,q+1}</math>
			To describe these operators in local coordinates, let
			:<math>\alpha=\sum_{\|I\|=p,\|J\|=q}\ f_{IJ}\,dz^I\wedge d\bar{z}^J\in\Omega^{p,q}</math>
			where ''I'' and ''J'' are [[multi-index\|multi-indices]]. Then
			:<math>\partial\alpha=\sum_{\|I\|,\|J\|}\sum_\ell \frac{\partial f_{IJ}}{\partial z^\ell}\,dz^\ell\wedge dz^I\wedge d\bar{z}^J</math>
			:<math>\bar{\partial}\alpha=\sum_{\|I\|,\|J\|}\sum_\ell \frac{\partial f_{IJ}}{\partial \bar{z}^\ell}d\bar{z}^\ell\wedge dz^I\wedge d\bar{z}^J.</math>

			The following properties are seen to hold:
			:<math>d=\partial+\bar{\partial}</math>
			:<math>\partial^2=\bar{\partial}^2=\partial\bar{\partial}+\bar{\partial}\partial=0.</math>

			These operators and their properties form the basis for [[Dolbeault cohomology]] and many aspects of [[Hodge theory]].

			===Holomorphic forms===
			For each ''p'', a holomorphic ''p''-form is a holomorphic section of the bundle Ω<sup>''p,0''</sup>. In local coordinates, then, a holomorphic ''p''-form can be written in the form

			:<math>\alpha=\sum_{\|I\|=p}f_I\,dz^I</math>

			where the ''f''<sub>''I''</sub> are holomorphic functions. Equivalently, the (''p'',0)-form α is holomorphic if and only if
			:<math>\bar{\partial}\alpha=0.</math>
			The [[sheaf (mathematics)\|sheaf]] of holomorphic ''p''-forms is often written Ω<sup>''p''</sup>, although this can sometimes lead to confusion so many authors tend to adopt an alternative notation.

			==See also==

			*[[Dolbeault complex]]
			*[[Frölicher spectral sequence]]
			*[[Differential of the first kind]]

			==References==
			* {{cite book\|last=Wells\|first=R.O.\|authorlink=Raymond O. Wells, Jr.\|title=Differential analysis on complex manifolds\|year=1973\|publisher=Springer-Verlag\|isbn=0-387-90419-0}}

			[[Category:Complex manifolds]]
			[[Category:Differential forms]]

71.235.181.6: /* Real spherical harmonics with l = 2 */

2012-02-24T04:26:45Z

Real spherical harmonics with l = 2

New page

She is known by the title of Myrtle Shryock. Bookkeeping is what I do. He is really fond of doing ceramics but he is struggling to discover time for it. Years in the past we moved to North Dakota and I adore every day living here.<br><br>Feel free to surf to my homepage :: at home std testing - [http://www.alemcheap.fi/show/the-way-to-cure-an-unpleasant-candidiasis Suggested Internet site],