4845:
coordinate expression, and properties sections), and several book sources that are given as (unfootnoted) general references lack specific section or page numbers to guide readers to the material here that they source. Ideally, every separate claim in the article should have a specific footnote indicating where to find it in the sources, and each paragraph should have at least one footnote. Because it is so far from meeting criterion 2, I think this should be a quick fail, but (as usual) with no prejudice against re-nominating once this issue has been addressed.
3817:
798:
understanding, but their knowledge is incomplete, or they are searching for something related that was once known, but forgotten (e.g. the Picard-Lindelof or
Frobenius theorem) -- thus links and mentions like this are not "clutter" but are actually useful. Similarly, references to books or other online "tutorial" sources are important. There is a fairly strong feeling within WP that it is not a book or a tutorial, but a reference, although who knows what the future may bring. You are invited to debate issues of style and content at
4671:
namely that the vectors are to be treated as operators, specifically directional derivatives. The subsequent statement "the Lie derivative is the commutator" does not clarify this for the non-initiate, since the commutator does not define what product is involved; in this case it is evidently the operator composition. This can be especially confusing to someone who is thinking of vectors simply in terms of a basis, and is expecting, for example, tensor products, but is faced with an undefined juxtaposition in the article
129:
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21:
3812:{\displaystyle {\mathcal {L}}_{X}Y:=\left.{\frac {\mathrm {d} ^{2}}{2\mathrm {d} ^{2}t}}\right|_{t=0}\mathrm {Fl} _{-t}^{Y}\circ \mathrm {Fl} _{-t}^{X}\circ \mathrm {Fl} _{t}^{Y}\circ \mathrm {Fl} _{t}^{X}=\left.{\frac {\mathrm {d} }{\mathrm {d} t}}\right|_{t=0}\mathrm {Fl} _{-{\sqrt {t}}}^{Y}\circ \mathrm {Fl} _{-{\sqrt {t}}}^{X}\circ \mathrm {Fl} _{\sqrt {t}}^{Y}\circ \mathrm {Fl} _{\sqrt {t}}^{X}}
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novices in the field find themselves rather confused by all the different derivatives, (Lie, exterior, partial and covariant) and have trouble sorting out the relationships between them. It is important for this article to succinctly state what these relationships are. That some of this info is also duplicated in other articles is acceptable.
780:. It doesn't matter whether you get a particular flow through the point in question, only that there exists one with the required first order behavior. Those who know about such things (myself included) are aware of these theorems, but they add needless clutter to the article. Simply things as far as possible, and no further.
3209:
1983:
2790:{\displaystyle ({\mathcal {L}}_{A}T)(\alpha ,\beta ,\ldots ,X,Y,\ldots )\equiv \nabla _{A}T(\alpha ,\beta ,\ldots ,X,Y,\ldots )-\nabla _{T(\cdot ,\beta ,\ldots ,X,Y,\ldots )}\alpha (A)-\ldots +T(\alpha ,\beta ,\ldots ,\nabla _{X}A,Y,\ldots )+\ldots +s(\nabla \cdot A)T(\alpha ,\beta ,\ldots ,X,Y,\ldots )}
1943:
4670:
The statement "The Lie derivative along a vector field is the evaluation of the vector field on functions" in the lead gives very little indication of how the vectors are to be considered, and in particular what the "evaluation" means. This assumes context that is simply missing from the description,
827:
techniques are perfectly OK. One person's helpful aside is another's buzzword generator, so I doubt that there is any absolute criterion of what to include. But the main thing is to aim at a comprehensive treatment of a topic. Well, that's in the
Knowledge charter; of course little in mathematics can
4678:
I'm sure it would only take a few words to mention the interpretation of vectors (or at least their evaluation over a scalar field) as operators (specifically directional derivatives) and that the commutator relates to their use and composition as operators (functionals). This is not my field, and I
913:
A short question from a reader of this page: The definition of the Lie derivative given here makes it look like it eats vector fields (in both slots), but the function f that is introduced later on in the definition of the Lie derivative, and which the Lie derivative eats, is a function from M to R.
713:
Yep, it needs to go. I can recommend two possible approaches. The first is to define the Lie derivative as a derivation on the full tensor bundle of a differentiable manifold. This has the advantage of fitting into the overall algebraic tone of the article. The second is to define it by means of
797:
Silly Rabbit, do note that the general consensus is that WP is a reference rather than a tutorial. To learn a new topic, a reader should read a book on the topic. In general, WP articles usually assume that the reader already has some general familiarity with the topic, possibly even a rather good
3113:
It is more confusing that it begins with "One might..." which suggests that a line of faulty reasoning is about to be dismissed (c.f. covariant derivative vs simpler derivative and the need to compensate for metric variation). Why not simply say "One can... in several ways..." but choose carefully
679:
a function along a congruence, as this leads nicely into the definition of a Lie derivative (perhaps as a section further in the article, not necessarily in the intro.). Another suggestion is to have component expressions for the Lie derivative of a tensor field and explain why (or at least state)
446:
I just edited a bit of the "Lie derivative of tensor fields" section. I made a few clarifications in the first (and very long) sentence, and I converted the math to math-markup. I know this might be controversial, but in this case there is a really long tensorial equation at heart that is somewhat
3978:
I am wondering what the original source of the equations on the second line is. The reference given at these equations (Kolar,Michor,Slovak) indeed provides a proof for it, but it doesn't give the origin of the equation either, nor does the second expression (with the square roots of t) appear in
498:
sections of Λ. I'm not too worried; which is which is should always be clear from context. There's not enough letters in the Greek alphabet. If its not clear from context, look for the phrase "where ω is a ...". I've never seen vol used for the volume form, that seems like a rather non-standard
215:
Sorry, but this article was obviously written by mathematicians.... It describes exactly what a Lie derivative is, but gives no clue whatsoever why it was defined or its uses. I've been seeing references to Lie derivatives in differential geometry and thought I could get an idea of why I should
4875:
I have no explanation for the undo of the following lines. I will add them again. If somebody wants to erase them, first we should have a discussion. This notation exists and I personally believe it is much better. A good reference to find this notation is the following book (see introduction):
1502:
Disagree. Note that different authors and different texts define the Lie derivative in different ways. Thus, all of these ways of approaching the definition should be described. No one particular definition should be elevated as "more right" than the others. A second important point is that many
699:
The section on Lie derivatives of tensor fields is total garbage, and needs to be completely re-written. The connection should be banished. Somewhere in this article we should make clear that the connection is not required for any of this stuff; and explain why; since I think the interplay of a
693:
I don't have any books that mention Lie dragging, so I wouldn't know how to write that up. If its placed in its own section, that would be fine to me. This article already mentions three different definitions for a Lie derivative; having a fourth one is fine, as long as this definition is not
4844:
Unfortunately, despite what appears (on a very superficial reading, by a non-expert) to be a well-written description of this subject, it is a long way from meeting Good
Article criterion 2, on sourcing. Most of the article has no inline sources (including the entire motivation, definition,
1203:
216:
care to learn about them from
Knowledge, but instead got this dry definition more suitable for computers than humans. Could someone who knows more about the subject add sections on the history of the Lie derivative, its reasons for being singled out for definition by Lie, etc.
851:
Ok, I retract my anti-buzzword prejudice. But I still believe that the article could use some clarification and simplification. The algebraic methods are quite useful in practice, but they don't provide much insight into the meaning of the Lie derivative.
875:
Dear Linas, Alrighty then. I have extensively revised the article. In my opinion, it is now clearer, more complete, better organized, and contains fewer errors. I hope that my revisions satisfy you and the rest of the wikipedia math community. Best,
3474:{\displaystyle ({\mathcal {L}}_{X}Y)_{x}:=\lim _{t\to 0}(\mathrm {T} (\mathrm {Fl} _{-t}^{X})Y_{\mathrm {Fl} _{t}^{X}(x)}-Y_{x})/t=\left.{\frac {\mathrm {d} }{\mathrm {d} t}}\right|_{t=0}\mathrm {T} (\mathrm {Fl} _{-t}^{X})Y_{\mathrm {Fl} _{t}^{X}(x)}}
3097:
The definition in the case of tensor densities (or field) is the following ... In the following particular cases this boils down to simpler expressions: (i) Functions (that is, (0,0)-tensors):... (ii) Vector fields (that is (1,0)-tensors): ... And so
2238:{\displaystyle ({\mathcal {L}}_{A}T)(\alpha ,\beta ,\ldots ,X,Y,\ldots )\equiv \nabla _{A}T(\alpha ,\beta ,\ldots ,X,Y,\ldots )-\nabla _{T(\cdot ,\beta ,\ldots ,X,Y,\ldots )}\alpha (A)-\ldots +T(\alpha ,\beta ,\ldots ,\nabla _{X}A,Y,\ldots )+\ldots }
3058:
4719:
A few days ago I added a new subsection with some examples. I think they are very useful, especially for people who are now learning about the Lie derivative and since the article is definitely not one of the most clear ones on
Knowledge.
1488:
1718:
4695:
Well, for somebody who is used to find clarity searching on wikipedia, this article is clearly written in mumbo jumbo language. So I've checked also the
Wolfram mathworld for some clue, any clue...and there really is one:
4383:
For me it's clear, see
William M. Boothy "An introduction to differentiable manifolds and Riemannian Geometry", Academic Press, second edition, ISBN: 0-12-116052-1, Orlando 1986, p. 117, where one can read: "the function
4379:
902:
I made some major revisions to Lie derivatives of tensor fields. There was some good stuff in there which I had to delete involving Lie derivatives of tensor densities. I have preserved it below in this talk page.
1396:
4174:. I would suggest that we change the definition of Lie derivative according to Khalil (see H.K.Khalil, Nonlinear Systems, Prentice Hall editions, 3rd edition, ISBN: 0-13-067389-7, London 2002, pp.509-501). So, let
3124:. I've removed all of the ugly "One" language. I haven't added any extra content providing some insight/value for each definition, but hopefully the more straight-forward presentations of each definition help. —
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article and am writing stuff on the Lie derivative in that article. I have links to this (Lie derivative) article, but can I suggest that there should be more information here regarding the concept of
4649:
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that the Lie derivative does not need a connection for its definition (as is indicated by the fact that the covariant derivatives can be replaced by partials). Comments appreciated. Thanks. ---
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Separately from this, and not a reason for a quick fail: I think a subject as geometric as this one could benefit from some illustrations, such as we already have (for instance) at
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Well, if you've "been seeing references to Lie derivatives in differential geometry" then surely the setting within which these references arise are themselves motivation!
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4700:. Also this wiki article lacks the importance and significance of this derivative in physics. So clearly it is just another strange expression in Mumbo jumbo language...
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No not exactly the push forward, T is the
Tangent functional (aka derivative) but the overall effect is push forward. Seems a pretty obscure way to write it to me.
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it seems linas that you have used omega for a 1-form here. This clashes with the supposed standard use of omega as the volume form. Perhaps we should start using
1938:{\displaystyle T(f_{1}\alpha ,f_{2}\beta ,\ldots ,f_{p+1}X,f_{p+2}Y,\ldots )=f_{1}f_{2}\cdots f_{p+1}f_{p+2}\cdots f_{p+q}T(\alpha ,\beta ,\ldots ,X,Y,\ldots )}
1408:
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This is an issue that I have been aware of for a long time, but have never gotten around to fixing. It should (and will... someday) be fixed. Thanks,
4298:
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The explanation of the last two equations of section "The Lie derivative of a vector field" is completely missing. I talk about these equations:
510:
I will read it. Why did you remove it? It is from there that my use of the notation stems. It may not be standard, but it is certainly clearer. -
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1198:{\displaystyle {\mathcal {L}}_{X}(\alpha \wedge \beta )=({\mathcal {L}}_{X}\alpha )\wedge \beta +\alpha \wedge ({\mathcal {L}}_{X}\beta )}
918:
The definition is extended so that it eats also functions. A function from M to R^n would still be a function and NOT a tangent vector. --
4539:. Your definition is "wrong". Remember, we are doing Differential Geometry. But I agree with you in that it is better to use the symbol
3986:
3921:
3856:
3079:
32:
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4608:(taking its flow), not with respect a function. Khalil's definition it's a particular one. It corresponds to taking the vector field
883:(P.S., I left the offending buzzwords intact, although I still believe that they ought to be removed or exported to an article like
672:
142:
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is hopelessly confused! (For those of you readers who don't know what the Lie derivative of a function is, it's just the ordinary
974:
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removed them without any discussion or explanation whatsoever though, so I reinstated them. Other articles like the one for the
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Second suggestion that we remove the definition and results concerning the interior product. These result are in the section
650:. Also, if there were any, they would not be more than one or two, so can be fixed by hand. Am I misunderstanding something?
3915:
Yes it's clear that it "Fl" is the flow and T is the pushforward. The only problem that this isn't mentioned in the article.
4728:
have a small subsection with examples so it's obvious that having the examples really helps people understand the material.
963:. This is correct if a connection is defined. However the Lie derivative is defined even if the connection is not defined.
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I believe this topic has something to do with the intersection between algebra and differential geometry, am I correct?
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I see that several forms of the definition are mentioned. I think it would be less confusing to say something like:
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For a general differential form, the Lie derivative is likewise a contraction, taking into account the variation in
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Is there any source that uses this axiom to define Lie derivative? If not, what is the meaning of the expression
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4852:. And, some parts of the article are fearsomely notation-heavy, so additional attention to making the material
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is the result of a calculation. The Lie derivative of any object is always defined with respect a vector field
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No reference whatsoever to the Picard-Lindelof or
Frobenius theorem is required. Please see the definition of
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What is "degree 0" derivation? This needs either an explanation, or a link to a page with an explanation.
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4952:. This notation is usually cleaner since it avoids the use of subindexes. This notation comes from prof.
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I'm not sure that's right. The prejudice is against getting confused between WP and a textbook. Various
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be changed? Then I will run the bot on the ones which should be changed, which are a majority. Thanks.
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Now that I've read it, I think the whole article should be scrapped. Even the Lie derivative of a
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on
Knowledge. If you would like to participate, please visit the project page, where you can join
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3053:{\displaystyle {\mathcal {L}}_{U}T={\frac {d}{dt}}\left(\psi _{t}^{*}T\right)\vert _{\psi (t)=p}}
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I dunno, ω is used for many things; often it is a representative member of Ω which is the set of
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I'm familiar with the notation. "Fl" is indeed the flow, and T is the "tangent functor" or the
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In the section "The Lie derivative of a function" it is not clear what is meant by the symbols
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1250:, the Lie derivative is just the contraction of the exterior derivative with the vector field
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4675:. Juxtaposition of two vectors can, for example, be interpreted as the geometric product.
1600:
1483:{\displaystyle {\mathcal {L}}_{fX}\omega =f{\mathcal {L}}_{X}\omega +df\wedge i_{X}\omega }
565:
To fix redirects with a bot is easy. The hard problem is that not all the pages linking to
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I have never seen that notation before, so this is just a guess. "Fl" might be short for
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tedious to read as HTML and gains a lot of clarity in the TeXed version. Hope that's OK.
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Shouldn't this be a function from M to R^n, where n is the dimension of the manifold?
573:. In some cases the link should certainly be changed, in some cases, like the article
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I am not sure. Could anybody knowing these things make a list of articles linking to
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under the one-parameter group of diffeomorphisms generated by a vector field: the
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and Lie derivatives can then be summarized as follows. For an ordinary function
1224:(Or should be) and should not be reproduced here. The section would now become:
929:
Some suggestions about the list of axioms for Lie derivative of tensor fields.
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4374:{\displaystyle (L_{f}g)(x)\triangleq ({\frac {\partial g}{\partial x}}f)(x)}
4817:. The edit link for this section can be used to add comments to the review.
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and an infinitesimal generator of a diffeomorphism given by a vector field
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Removal or major edit of section "The Lie derivative of differential forms"
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1391:{\displaystyle {\mathcal {L}}_{X}\omega =i_{X}d\omega +d(i_{X}\omega )}
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4134:) has different equivalent representations then instead of the symbol
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Axiom 3: I propose replacing axiom 3 with two more "primitive axioms":
722:. This has the advantage of saying what the Lie derivative actually
499:
notation. BTW, add your book reference to the article on Laplacian.
2854:
700:
connection is a stumbling block for mastering these concepts.
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and explain why each definition has particular value/insight.
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Now I am really confused. There are just a couple of links to
60:
15:
1064:{\displaystyle {\mathcal {L}}_{X}(\xi )(Y)=X(\xi (Y))-\xi ()}
241:
Added a motivation paragraph to the beginning of the article
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4856:(without, of course, oversimplifying it) would be welcome. —
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5043:{\displaystyle {\mathcal {L}}_{X}(T(Y_{1},\ldots ,T_{n}))}
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induced by ψ. Then the Lie derivative of the tensor field
346:{\displaystyle :={\mathcal {L}}_{A}B=-{\mathcal {L}}_{B}A}
41:
at the time (December 11, 2016). There are suggestions on
4679:
request someone more familiar with it to clarify this. —
3822:
It would be necessary to explain at least the meaning of
3168:
Lee. I have no reference to confirm this to you though. —
420:{\displaystyle :={\mathcal {L}}_{A}B-{\mathcal {L}}_{B}A}
259:
It seems that in the intro Lie derivate is used both for
726:. Both approaches should have a place in the article.
602:
I was very modestly thinking only of "all" the links on
2877:, as given above. Note that ψ is a local 1-parameter
1673:, …), such that for any collection of smooth functions
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4644:{\displaystyle X=f{\frac {\partial }{\partial x}}\,}
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for the volume form. I think it is less confusing. -
146:, a collaborative effort to improve the coverage of
429:The first equation is correct. The second is not.
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47:for improving the article. If you can improve it,
4083:. If it is simply meant that the defined entity (
1231:. In this context, it is closely related to the
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4882:"Another notation to denote the Lie derivative
4698:http://mathworld.wolfram.com/LieDerivative.html
4510:
4102:
3122:definition of the Lie derivative for a function
4878:http://matematicas.unex.es/~navarro/degree.pdf
4494:" and p. 226, where one can find the formula:
527:Has somebody a bot who could fix all links to
4971:The Lie derivative of a tensor field: axiom 3
694:presented as the first or primary definition.
8:
4651:, in a particular chart and representation.
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4666:Non-intuitive definition in lead for layman
4242:{\displaystyle D\subseteq \mathbb {R} ^{n}}
3151:BTW - how is "Lie" pronounced? Lye or Lee?
2307:In other words, if you have a tensor field
1402:The derivative of products is distributed:
1303:{\displaystyle {\mathcal {L}}_{X}f=i_{X}df}
4746:
4127:{\displaystyle ({\mathcal {L}}_{\!X}f)(p)}
1227:The Lie derivative can also be defined on
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271:Where is the sign = ? where is the true ?
4532:{\displaystyle {\mathcal {L}}_{\!X}f=Xf}
2401:under the infinitesimal diffeomorphism.
1949:and if further we have a differentiable
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1583:(which we consider as a differentiable
94:
64:
800:Knowledge talk:WikiProject Mathematics
4915:{\displaystyle {\mathcal {L}}_{X}(Y)}
4214:be sufficiently smooth functions and
4207:{\displaystyle f,g:D\to \mathbb {R} }
828:actually be treated that thoroughly.
20:
7:
2833:Alternately, given the vector field
263:and for elements of the range of . -
140:This article is within the scope of
2374:{\displaystyle {\mathcal {L}}_{U}T}
1514:Lie derivatives of tensor densities
83:It is of interest to the following
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761:that things become interesting.)
472:
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5084:Mid-priority mathematics articles
3120:Please review the updates to the
673:mathematics of general relativity
160:Knowledge:WikiProject Mathematics
4458:{\displaystyle (Xf)(p)=X_{p}f\,}
275:(sorry for my very bad English)
203:Insufficiently explained concept
163:Template:WikiProject Mathematics
127:
117:
96:
65:
19:
3842:{\displaystyle \mathrm {Fl} \,}
2881:of local diffeomorphisms. Let
180:This article has been rated as
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2819:{\displaystyle \nabla \cdot A}
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705:14:06, 29 September 2005 (UTC)
688:07:05, 29 September 2005 (UTC)
531:by adding (abstract algebra)?
479:{\displaystyle \mathrm {vol} }
374:
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1:
5060:03:54, 25 November 2020 (UTC)
4866:22:46, 11 December 2016 (UTC)
4840:22:46, 11 December 2016 (UTC)
3084:03:03, 11 November 2005 (UTC)
2404:More generally, if we have a
1508:21:33, 16 December 2005 (UTC)
1497:12:36, 16 December 2005 (UTC)
1211:13:17, 15 December 2005 (UTC)
908:03:00, 11 November 2005 (UTC)
881:06:10, 11 November 2005 (UTC)
636:derivation (abstract algebra)
571:derivation (abstract algebra)
154:and see a list of open tasks.
5079:B-Class mathematics articles
5074:Former good article nominees
4966:13:49, 16 January 2018 (UTC)
4954:Juan Bautista Sancho Guimerá
4738:10:03, 16 January 2015 (UTC)
4710:20:15, 29 January 2013 (UTC)
4661:17:45, 3 November 2011 (UTC)
3995:23:48, 1 December 2012 (UTC)
3875:which is a related concept.
2260:. This tensor is called the
956:{\displaystyle \nabla _{Y}f}
923:13:17, 31 October 2005 (UTC)
857:02:07, 9 November 2005 (UTC)
833:15:45, 8 November 2005 (UTC)
807:14:50, 8 November 2005 (UTC)
785:06:45, 8 November 2005 (UTC)
766:06:22, 8 November 2005 (UTC)
731:06:09, 8 November 2005 (UTC)
671:I'm currently rewriting the
4922:, although less common, is
4147:{\displaystyle \triangleq }
3973:21:31, 11 August 2008 (UTC)
3949:21:16, 12 August 2008 (UTC)
3930:21:22, 11 August 2008 (UTC)
3911:12:47, 11 August 2008 (UTC)
3885:12:27, 11 August 2008 (UTC)
3865:06:17, 11 August 2008 (UTC)
646:. I don't see any links to
5100:
4036:{\displaystyle X_{p}(f)\,}
3893:pushforward (differential)
233:12:07, 5 August 2008 (UTC)
37:, but it did not meet the
4871:Sancho Guimerá's notation
4854:as accessible as possible
4686:11:32, 24 June 2012 (UTC)
4554:{\displaystyle \equiv \,}
4076:{\displaystyle (Xf)(p)\,}
3188:18:35, 22 July 2009 (UTC)
3161:15:36, 22 July 2009 (UTC)
3144:18:35, 22 July 2009 (UTC)
2901:{\displaystyle \psi ^{*}}
2252:∇ used; as long as it is
1242:The relationship between
490:15:56, 27 Apr 2005 (UTC)
450:- Thomas, 131.111.231.27
434:05:23, 22 July 2006 (UTC)
267:14:19, 27 Apr 2005 (UTC)
179:
112:
91:
4870:
3109:for more than one reason
933:Axiom 1 should not have
749:. It's when you get to
655:21:59, 11 May 2005 (UTC)
618:21:48, 11 May 2005 (UTC)
590:20:17, 11 May 2005 (UTC)
557:14:43, 11 May 2005 (UTC)
543:22:20, 10 May 2005 (UTC)
503:00:33, 29 Apr 2005 (UTC)
439:Using math sections etc.
251:17:26, 5 June 2016 (UTC)
186:project's priority scale
33:Mathematics good article
5050:on the left-hand side?
4815:Talk:Lie derivative/GA1
4487:{\displaystyle C^{r}\,}
4167:{\displaystyle \equiv }
3091:Definition is confusing
1977:, then the linear map
523:Fix links to derivation
515:13:36, 2 May 2005 (UTC)
143:WikiProject Mathematics
5044:
4946:
4945:{\displaystyle X^{L}Y}
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1620:{\displaystyle T^{*}M}
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747:directional derivative
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3196:Unexplained equations
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2459:{\displaystyle (p,q)}
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1576:{\displaystyle (p,q)}
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667:Proposals/suggestions
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39:good article criteria
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4726:covariant derivative
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4579:{\displaystyle Xf\,}
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4402:{\displaystyle Xf\,}
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2466:and density s, then
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2256:, and in fact, is a
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1244:exterior derivatives
1099:
1084:{\displaystyle \xi }
1075:
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550:User:Oleg Alexandrov
462:
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166:mathematics articles
4601:{\displaystyle X\,}
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644:Talk:Lie derivative
29:was nominated as a
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3873:Flow (mathematics)
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1654:{\displaystyle TM}
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1229:differential forms
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755:differential forms
642:, and a couple on
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135:Mathematics portal
79:content assessment
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4286:{\displaystyle f}
4266:{\displaystyle g}
3985:comment added by
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3855:comment added by
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3153:Julian I Do Stuff
3087:
3070:comment added by
2995:
2945:{\displaystyle p}
2925:{\displaystyle T}
2870:{\displaystyle U}
2846:{\displaystyle U}
2424:{\displaystyle T}
2394:{\displaystyle T}
2340:{\displaystyle U}
2320:{\displaystyle T}
2297:{\displaystyle A}
2277:{\displaystyle T}
1970:{\displaystyle A}
1541:{\displaystyle T}
552:, he has a bot. -
211:Motivation needed
200:
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51:; it may then be
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5052:StrokeOfMidnight
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4759:Copyvio detector
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4249:. We define the
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830:Charles Matthews
569:need to link to
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4154:one should use
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2436:
2435:
2413:
2412:
2383:
2382:
2354:
2349:
2348:
2329:
2328:
2309:
2308:
2286:
2285:
2266:
2265:
2201:
2107:
2052:
1990:
1982:
1981:
1959:
1958:
1877:
1858:
1842:
1829:
1819:
1788:
1766:
1744:
1728:
1717:
1716:
1711:
1698:
1688:
1679:
1640:
1639:
1604:
1599:
1598:
1594:α, β, … of the
1553:
1552:
1530:
1529:
1522:, if we have a
1516:
1467:
1438:
1412:
1407:
1406:
1372:
1347:
1327:
1322:
1321:
1284:
1264:
1259:
1258:
1218:
1175:
1137:
1102:
1097:
1096:
1073:
1072:
978:
973:
972:
940:
935:
934:
669:
652:Oleg Alexandrov
587:Oleg Alexandrov
525:
460:
459:
456:
441:
400:
380:
357:
356:
326:
303:
280:
279:
273:
213:
205:
165:
162:
159:
156:
155:
133:
126:
106:
77:on Knowledge's
74:
44:the review page
12:
11:
5:
5097:
5095:
5087:
5086:
5081:
5076:
5066:
5065:
5039:
5036:
5031:
5027:
5023:
5020:
5017:
5012:
5008:
5004:
5001:
4998:
4993:
4987:
4972:
4969:
4941:
4936:
4932:
4911:
4908:
4905:
4900:
4894:
4872:
4869:
4858:David Eppstein
4826:David Eppstein
4820:
4819:
4803:
4802:
4800:
4799:
4794:
4789:
4783:
4780:
4779:
4775:
4774:
4772:
4771:
4769:External links
4766:
4761:
4755:
4752:
4751:
4744:
4741:
4716:
4713:
4692:
4691:Mumbo jumbo...
4689:
4667:
4664:
4635:
4632:
4628:
4623:
4620:
4617:
4595:
4573:
4570:
4548:
4528:
4525:
4522:
4519:
4514:
4506:
4479:
4475:
4465:, is of class
4452:
4447:
4443:
4439:
4436:
4433:
4430:
4427:
4424:
4421:
4418:
4409:, defined by
4396:
4393:
4370:
4367:
4364:
4361:
4358:
4352:
4349:
4344:
4341:
4335:
4332:
4329:
4326:
4323:
4320:
4317:
4312:
4308:
4304:
4282:
4262:
4251:Lie derivative
4236:
4231:
4226:
4223:
4202:
4198:
4195:
4192:
4189:
4186:
4183:
4163:
4143:
4123:
4120:
4117:
4114:
4111:
4106:
4098:
4092:
4070:
4067:
4064:
4061:
4058:
4055:
4052:
4030:
4027:
4024:
4019:
4015:
4002:
3999:
3976:
3975:
3955:
3954:
3953:
3952:
3951:
3919:
3918:
3917:
3916:
3888:
3887:
3835:
3832:
3820:
3819:
3806:
3800:
3794:
3791:
3786:
3781:
3775:
3769:
3766:
3761:
3756:
3749:
3744:
3739:
3736:
3731:
3726:
3719:
3714:
3709:
3706:
3699:
3696:
3693:
3688:
3682:
3678:
3672:
3666:
3662:
3657:
3652:
3647:
3644:
3639:
3634:
3629:
3624:
3621:
3616:
3611:
3606:
3603:
3598:
3595:
3590:
3585:
3580:
3577:
3572:
3569:
3562:
3559:
3556:
3551:
3545:
3540:
3535:
3530:
3524:
3519:
3512:
3508:
3505:
3500:
3494:
3481:
3468:
3465:
3462:
3457:
3452:
3447:
3444:
3438:
3434:
3429:
3424:
3421:
3416:
3413:
3408:
3404:
3398:
3395:
3392:
3387:
3381:
3377:
3371:
3365:
3361:
3358:
3354:
3350:
3345:
3341:
3337:
3332:
3329:
3326:
3321:
3316:
3311:
3308:
3302:
3298:
3293:
3288:
3285:
3280:
3277:
3272:
3268:
3264:
3259:
3256:
3253:
3249:
3245:
3240:
3236:
3232:
3227:
3221:
3215:
3203:
3197:
3194:
3193:
3192:
3191:
3190:
3149:
3148:
3147:
3146:
3110:
3107:
3092:
3089:
3062:
3061:
3047:
3044:
3041:
3038:
3035:
3032:
3028:
3023:
3019:
3014:
3009:
3005:
3000:
2993:
2990:
2986:
2981:
2978:
2973:
2967:
2941:
2921:
2895:
2891:
2866:
2842:
2815:
2812:
2809:
2798:
2797:
2786:
2783:
2780:
2777:
2774:
2771:
2768:
2765:
2762:
2759:
2756:
2753:
2750:
2747:
2744:
2741:
2738:
2735:
2732:
2729:
2726:
2723:
2720:
2717:
2714:
2711:
2708:
2705:
2702:
2697:
2693:
2689:
2686:
2683:
2680:
2677:
2674:
2671:
2668:
2665:
2662:
2659:
2656:
2653:
2650:
2647:
2642:
2639:
2636:
2633:
2630:
2627:
2624:
2621:
2618:
2615:
2612:
2609:
2606:
2603:
2599:
2595:
2592:
2589:
2586:
2583:
2580:
2577:
2574:
2571:
2568:
2565:
2562:
2559:
2556:
2553:
2548:
2544:
2540:
2537:
2534:
2531:
2528:
2525:
2522:
2519:
2516:
2513:
2510:
2507:
2504:
2501:
2498:
2495:
2490:
2484:
2478:
2455:
2452:
2449:
2446:
2443:
2420:
2409:tensor density
2406:differentiable
2390:
2370:
2365:
2359:
2336:
2316:
2293:
2273:
2262:Lie derivative
2246:
2245:
2234:
2231:
2228:
2225:
2222:
2219:
2216:
2213:
2208:
2204:
2200:
2197:
2194:
2191:
2188:
2185:
2182:
2179:
2176:
2173:
2170:
2167:
2164:
2161:
2158:
2153:
2150:
2147:
2144:
2141:
2138:
2135:
2132:
2129:
2126:
2123:
2120:
2117:
2114:
2110:
2106:
2103:
2100:
2097:
2094:
2091:
2088:
2085:
2082:
2079:
2076:
2073:
2070:
2067:
2064:
2059:
2055:
2051:
2048:
2045:
2042:
2039:
2036:
2033:
2030:
2027:
2024:
2021:
2018:
2015:
2012:
2009:
2006:
2001:
1995:
1989:
1966:
1955:tangent bundle
1947:
1946:
1934:
1931:
1928:
1925:
1922:
1919:
1916:
1913:
1910:
1907:
1904:
1901:
1898:
1895:
1890:
1887:
1884:
1880:
1876:
1871:
1868:
1865:
1861:
1855:
1852:
1849:
1845:
1841:
1836:
1832:
1826:
1822:
1818:
1815:
1812:
1809:
1806:
1801:
1798:
1795:
1791:
1787:
1784:
1779:
1776:
1773:
1769:
1765:
1762:
1759:
1756:
1751:
1747:
1743:
1740:
1735:
1731:
1727:
1724:
1703:
1693:
1684:
1677:
1650:
1647:
1637:tangent bundle
1616:
1611:
1607:
1572:
1569:
1566:
1563:
1560:
1537:
1524:differentiable
1515:
1512:
1511:
1510:
1491:
1490:
1479:
1474:
1470:
1466:
1463:
1460:
1457:
1454:
1449:
1443:
1437:
1434:
1431:
1426:
1423:
1417:
1400:
1399:
1387:
1384:
1379:
1375:
1371:
1368:
1365:
1362:
1359:
1354:
1350:
1346:
1343:
1338:
1332:
1311:
1310:
1299:
1296:
1291:
1287:
1283:
1280:
1275:
1269:
1217:
1214:
1194:
1191:
1186:
1180:
1174:
1171:
1168:
1165:
1162:
1159:
1156:
1153:
1148:
1142:
1136:
1133:
1130:
1127:
1124:
1121:
1118:
1113:
1107:
1080:
1060:
1057:
1054:
1051:
1048:
1045:
1042:
1039:
1036:
1033:
1030:
1027:
1024:
1021:
1018:
1015:
1012:
1009:
1006:
1003:
1000:
997:
994:
989:
983:
970:
969:
965:
964:
952:
947:
943:
928:
926:
925:
911:
910:
899:
898:
897:
896:
895:
894:
893:
892:
885:tangent bundle
866:
865:
864:
863:
862:
861:
860:
859:
842:
841:
840:
839:
838:
837:
836:
835:
814:
813:
812:
811:
810:
809:
790:
789:
788:
787:
771:
770:
769:
768:
736:
735:
734:
733:
708:
707:
696:
695:
668:
665:
664:
663:
662:
661:
660:
659:
658:
657:
640:Lie derivative
625:
624:
623:
622:
621:
620:
595:
594:
593:
592:
560:
559:
524:
521:
520:
519:
518:
517:
505:
504:
474:
471:
468:
455:
452:
440:
437:
416:
411:
405:
399:
396:
391:
385:
379:
376:
373:
370:
367:
364:
342:
337:
331:
325:
322:
319:
314:
308:
302:
299:
296:
293:
290:
287:
272:
269:
257:
256:
255:
254:
253:
236:
235:
212:
209:
204:
201:
198:
197:
194:
193:
190:
189:
178:
172:
171:
169:
152:the discussion
139:
138:
122:
110:
109:
101:
89:
88:
82:
71:
57:
56:
27:Lie derivative
24:
13:
10:
9:
6:
4:
3:
2:
5096:
5085:
5082:
5080:
5077:
5075:
5072:
5071:
5069:
5062:
5061:
5057:
5053:
5029:
5025:
5021:
5018:
5015:
5010:
5006:
4999:
4991:
4970:
4968:
4967:
4963:
4959:
4955:
4939:
4934:
4930:
4906:
4898:
4880:
4879:
4868:
4867:
4863:
4859:
4855:
4851:
4846:
4842:
4841:
4837:
4834:
4831:
4827:
4824:
4818:
4816:
4812:
4807:
4806:
4798:
4795:
4793:
4790:
4788:
4785:
4784:
4782:
4781:
4776:
4770:
4767:
4765:
4762:
4760:
4757:
4756:
4754:
4753:
4748:
4742:
4740:
4739:
4735:
4731:
4727:
4723:
4714:
4712:
4711:
4707:
4703:
4702:Theodore Yoda
4699:
4690:
4688:
4687:
4684:
4682:
4676:
4674:
4665:
4663:
4662:
4658:
4654:
4633:
4621:
4618:
4615:
4593:
4571:
4568:
4546:
4526:
4523:
4520:
4517:
4512:
4477:
4473:
4450:
4445:
4441:
4437:
4431:
4422:
4419:
4394:
4391:
4381:
4365:
4356:
4350:
4342:
4330:
4324:
4315:
4310:
4306:
4294:
4280:
4260:
4252:
4234:
4224:
4221:
4193:
4190:
4187:
4184:
4181:
4161:
4141:
4118:
4109:
4104:
4065:
4056:
4053:
4025:
4017:
4013:
4000:
3998:
3996:
3992:
3988:
3987:94.224.97.175
3984:
3974:
3970:
3962:
3956:
3950:
3946:
3942:
3938:
3937:
3936:
3935:
3934:
3933:
3932:
3931:
3927:
3923:
3922:89.135.19.155
3914:
3913:
3912:
3908:
3900:
3894:
3890:
3889:
3886:
3882:
3878:
3874:
3870:
3869:
3868:
3866:
3862:
3858:
3857:89.135.19.155
3854:
3804:
3798:
3784:
3779:
3773:
3759:
3754:
3747:
3742:
3729:
3724:
3717:
3712:
3697:
3694:
3691:
3686:
3680:
3660:
3655:
3650:
3637:
3632:
3627:
3614:
3609:
3604:
3601:
3588:
3583:
3578:
3575:
3560:
3557:
3554:
3549:
3543:
3538:
3528:
3522:
3506:
3503:
3498:
3482:
3463:
3455:
3450:
3436:
3427:
3422:
3419:
3396:
3393:
3390:
3385:
3379:
3359:
3356:
3352:
3343:
3339:
3335:
3327:
3319:
3314:
3300:
3291:
3286:
3283:
3257:
3251:
3243:
3238:
3230:
3225:
3206:
3205:
3204:
3201:
3195:
3189:
3185:
3181:
3177:
3173:
3172:
3167:
3166:
3165:
3164:
3163:
3162:
3158:
3154:
3145:
3141:
3137:
3133:
3129:
3128:
3123:
3119:
3118:
3117:
3116:
3115:
3108:
3106:
3105:
3102:
3099:
3090:
3088:
3085:
3081:
3077:
3073:
3072:Silly rabbit
3069:
3045:
3042:
3036:
3030:
3021:
3017:
3012:
3007:
3003:
2998:
2991:
2988:
2984:
2979:
2976:
2971:
2955:
2954:
2953:
2939:
2932:at the point
2919:
2911:
2893:
2889:
2880:
2864:
2856:
2840:
2831:
2829:
2813:
2810:
2781:
2778:
2775:
2772:
2769:
2766:
2763:
2760:
2757:
2754:
2751:
2745:
2739:
2736:
2727:
2724:
2721:
2718:
2712:
2709:
2706:
2703:
2700:
2695:
2687:
2684:
2681:
2678:
2675:
2672:
2666:
2663:
2660:
2657:
2651:
2645:
2637:
2634:
2631:
2628:
2625:
2622:
2619:
2616:
2613:
2610:
2607:
2601:
2593:
2587:
2584:
2581:
2578:
2575:
2572:
2569:
2566:
2563:
2560:
2557:
2551:
2546:
2538:
2532:
2529:
2526:
2523:
2520:
2517:
2514:
2511:
2508:
2505:
2502:
2493:
2488:
2469:
2468:
2467:
2450:
2447:
2444:
2434:
2418:
2410:
2407:
2402:
2388:
2368:
2363:
2334:
2314:
2305:
2291:
2271:
2263:
2259:
2255:
2251:
2232:
2229:
2223:
2220:
2217:
2214:
2211:
2206:
2198:
2195:
2192:
2189:
2186:
2183:
2177:
2174:
2171:
2168:
2162:
2156:
2148:
2145:
2142:
2139:
2136:
2133:
2130:
2127:
2124:
2121:
2118:
2112:
2104:
2098:
2095:
2092:
2089:
2086:
2083:
2080:
2077:
2074:
2071:
2068:
2062:
2057:
2049:
2043:
2040:
2037:
2034:
2031:
2028:
2025:
2022:
2019:
2016:
2013:
2004:
1999:
1980:
1979:
1978:
1964:
1956:
1952:
1929:
1926:
1923:
1920:
1917:
1914:
1911:
1908:
1905:
1902:
1899:
1893:
1888:
1885:
1882:
1878:
1874:
1869:
1866:
1863:
1859:
1853:
1850:
1847:
1843:
1839:
1834:
1830:
1824:
1820:
1816:
1810:
1807:
1804:
1799:
1796:
1793:
1789:
1785:
1782:
1777:
1774:
1771:
1767:
1763:
1760:
1757:
1754:
1749:
1745:
1741:
1738:
1733:
1729:
1722:
1715:
1714:
1713:
1710:
1706:
1702:
1696:
1692:
1687:
1683:
1676:
1672:
1668:
1664:
1648:
1645:
1638:
1634:
1630:
1614:
1609:
1605:
1597:
1593:
1590:
1586:
1567:
1564:
1561:
1551:
1535:
1528:
1525:
1521:
1513:
1509:
1506:
1501:
1500:
1499:
1498:
1495:
1477:
1472:
1468:
1464:
1461:
1458:
1455:
1452:
1447:
1435:
1432:
1429:
1424:
1421:
1405:
1404:
1403:
1382:
1377:
1373:
1366:
1363:
1360:
1357:
1352:
1348:
1344:
1341:
1336:
1320:
1319:
1318:
1316:
1297:
1294:
1289:
1285:
1281:
1278:
1273:
1257:
1256:
1255:
1253:
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778:tangent space
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759:tensor fields
756:
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751:vector fields
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584:
581:which should
580:
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28:
25:
18:
17:
4974:
4881:
4874:
4850:vector field
4847:
4843:
4832:
4822:
4821:
4808:
4797:Instructions
4730:129.194.8.73
4718:
4694:
4677:
4669:
4382:
4295:
4250:
4004:
3981:— Preceding
3979:this book.
3977:
3960:siℓℓy rabbit
3920:
3898:siℓℓy rabbit
3821:
3202:
3199:
3169:
3150:
3125:
3112:
3096:
3094:
3066:— Preceding
3063:
2952:is given by
2832:
2799:
2403:
2306:
2261:
2254:torsion-free
2247:
1951:vector field
1948:
1708:
1704:
1700:
1694:
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1685:
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1674:
1670:
1666:
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1527:tensor field
1517:
1492:
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1312:
1251:
1247:
1241:
1226:
1219:
1206:
1095:
1092:
971:
927:
912:
905:Silly rabbit
889:vector field
878:Silly rabbit
854:Silly rabbit
824:
782:Silly rabbit
763:Silly rabbit
742:
728:Silly rabbit
723:
677:Lie dragging
676:
670:
643:
603:
582:
575:dual numbers
526:
495:
457:
449:
445:
442:
428:
354:
277:
274:
260:
258:
218:
214:
206:
182:Mid-priority
181:
141:
107:Mid‑priority
85:WikiProjects
42:
31:
30:
26:
4811:transcluded
4653:Mgvongoeden
3851:—Preceding
1635:, … of the
720:vector flow
157:Mathematics
148:mathematics
104:Mathematics
53:renominated
5068:Categories
4764:Authorship
4750:GA toolbox
4673:commutator
4561:, because
2828:divergence
2250:connection
1665:(α, β, …,
1661:, written
1585:linear map
648:derivation
579:derivation
567:derivation
529:derivation
4823:Reviewer:
4787:Templates
4778:Reviewing
4743:GA Review
3877:JRSpriggs
3171:TedPavlic
3127:TedPavlic
243:David9550
49:please do
4958:JBecerra
4836:contribs
4792:Criteria
4715:Examples
3983:unsigned
3941:Billlion
3853:unsigned
3080:contribs
3068:unsigned
2910:pullback
1712:we have
1592:sections
1494:Mungbean
1235:and the
1208:Mungbean
825:tutorial
743:function
716:pullback
4681:Quondum
3180:contrib
3136:contrib
2908:be the
2826:is the
2347:, then
443:Hello,
184:on the
75:B-class
4273:along
2855:curves
2800:where
2411:field
2258:tensor
1589:smooth
920:MarSch
757:, and
685:(talk)
682:Mpatel
606:page.
554:MarSch
512:MarSch
496:smooth
488:MarSch
265:MarSch
81:scale.
4813:from
2879:group
1699:, …,
1680:, …,
1505:linas
804:linas
724:means
702:linas
501:linas
454:omega
355:+ :
278:- :
5056:talk
4962:talk
4956:"".
4862:talk
4830:talk
4734:talk
4706:talk
4657:talk
4293:as:
4043:and
3991:talk
3967:talk
3945:talk
3926:talk
3905:talk
3881:talk
3861:talk
3176:talk
3157:talk
3132:talk
3076:talk
2433:rank
1550:rank
1239:.
1093:and
615:Talk
604:this
548:ask
540:Talk
247:talk
229:talk
4253:of
3849:.
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3098:on.
3082:)
2857:of
2431:of
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1697:+ 1
1587:of
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1518:In
887:or
638:on
611:MFH
583:not
536:MFH
176:Mid
5070::
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