Talk:Poincaré metric

message: What's up with the random picture of the J-invariant?  The connection to this page is pretty opaque, although it's a beautiful picture. --Dylan Thurston (talk) 23:44, 4 June 2009 (UTC)
thread_title:  Picture of J-invariant 

message: There's a lot more information on the disk model over at Poincaré disk model. These two pages seem similar enough that I don't see a great need for two separate articles. --Dantheox 22:20, 30 April 2006 (UTC)
replies: text: I'm against the merger, for multiple reasons: 1) Its OK to duplicate some information across multiple articles. 2) Both articles are already rather long; merging them would make them unmanageably long. 3) Neither article has exhausted what one can say about either topic: much more can be said about the disk, and much more can be said about the metric. 4) The Poincare disk model is about the N-dimensional hyperbolic model. This article (Poincare metric) limits itself to two dimensions only.  Although we could generalize this article to N dimensions, there's actually a big difference between two and more than two dimensions: There's rigidity in three and higher dimensions, whereas in two, there is a very rich set of surfaces. One also looses some of the natural connections to number theory and modular forms and complex analysis. Etc. 5) combining them would lead to topic confusion, is the resulting combo about the disk or the metric? Suppose one wanted to talk about the metric on the half-plane? Does that mean we should merge with the half-plane article too? Before long, we'll end up merging a dozen articles because they all contain inter-related info. linas 01:59, 1 May 2006 (UTC)
replies: text:  That's fine.. perhaps a "Main article on this topic" link in the disk section of this article would be a more appropriate course of action. --Dantheox 04:52, 1 May 2006 (UTC)
replies: text: I think the merger tags should be removed from both articles, as this idea isn't going anywhere. As for a main article link, it isn't clear that the other article is the main article on the metric; it's an article on the model, and mentions the metric very briefly. I'll add a link to the "see also" section. Gene Ward Smith 06:15, 1 May 2006 (UTC)
thread_title:  Merger 

message: Currently the article defines cross-ratio as (z_1,z_2; z_3,z_4) = \frac{(z_1-z_2)(z_3-z_4)}{(z_2-z_3)(z_4-z_1)} which is inconsitent with the order defined in cross-ratio. I'll tag this inconsistency. I'm not sure whether the formula after that refers to the common definition of cross-ratio or actually relies on this non-standard definition. It might need adjustment as well. Someone should verify this. -- Martin von Gagern (talk) 15:31, 11 July 2011 (UTC)
thread_title:  Order in cross-ratio 

message: I inserted a factor of 2 in the formula for \rho(z_1,z_2).  With the old formula we would have \rho(x,0)=x+O(x^2) for small positive x, which is clearly inconsistent with the formula for ds^2.  The formula for ds^2 is the right one if we want to have curvature -1. Neil Strickland (talk) 13:07, 8 January 2015 (UTC)
thread_title:  Missing factor of 2 

message: Though Poincare's name is attached to two models of the hyperbolic plane, the metric in these planes is named after Arthur Cayley and Felix Klein. Appropriate use of references may preserve this article for some applications in Riemann surface theory, but the reference to the hyperbolic plane models is incorrect. Currently there are no in-line references. Inaccurate statements are subject to change. — Rgdboer (talk) 21:30, 10 January 2016 (UTC)
thread_title:  Cayley-Klein metric 

message: The Poincaré volume form (called "invariant volume element" in the page) is written as a tensor or symmetric product (depending on convention) of differential forms dxdy, instead of an antisymmetric product dx\wedge dy. One may assume that dxdy is implicitly antisymmetrized but higher in the page the wedge notation is used, which may cause confusion. Plm203 (talk) 22:46, 9 July 2023 (UTC)
thread_title:  Volume form notation