LOL, no, robjohn. Still in San Diego, recovering from a sinus infection. I leave for Ann Arbor Tuesday morning.
I taught the simplex method back in 1982, but I haven't thought about it since. But we didn't throw in extra variables. We just used the reduced echelon form to travel to the right vertex. But I've forgotten the algorithm.
@robjohn Who is us? I'll let you know about it privately. Never discuss here my published stuff for avoiding the discussions I had in the past with some users (like Ted, that is an example)
@robjohn: Perhaps you could privately explain to chris'ssis that most of us respect her mathematical abilities but do not share her taste or her unrelenting what comes across as bragging about her being God's gift (or Ramanujan's gift) to mathematics.
In mathematics, the Barnes G-function G(z) is a function that is an extension of superfactorials to the complex numbers. It is related to the Gamma function, the K-function and the Glaisher–Kinkelin constant, and was named after mathematician Ernest William Barnes. Up to elementary factors, it is a special case of the double gamma function.
Formally, the Barnes G-function is defined in the following Weierstrass product form:
where is the Euler–Mascheroni constant, exp(x) = ex, and ∏ is capital pi notation.
== Functional equation and integer arguments ==
The Barnes G-function satisfies t...
Professor Hari M. Srivastava has some nice stuff in his books about Barnes G-functions, limits, series and some integrals.
I should also mention here Professor Choi Junesang (they both wrote an amazing book).
@Khallil I'm here now. Unfortunately, simply connected domains in $\Bbb C$ are never defined with the minimal amount of machinery as I defined you above (except maybe in good complex analysis books), and homotopy are almost never introduced in complex analysis books. To learn some of these stuff, you need to have a look at algebraic topology textbooks.
Standard reference would be Munkres Topology part II, but you need to know a bit about topological spaces.
(by bit, I mean the basis plus quotient topology and various forms of connectedness, especially path connectedness and local connectedness).
But everything needed can be found in Munkres Topology part I :)
You can learn basic notions of homotopy and fundamental group using metric spaces, but it'd be preferable to learn some abstract topology first. Although if you want to I'd encourage you take a peek in Munkres Topology part II.
I put a password to the wireless network, I didn't have one before (or better say for a little while). My uncle tried to connect to internet (from a phone) and failed with the password, so I kept it a while like that.
It looks like all moves faster now (or does it just seem to me?).
@OFFSHARING I have a password and also allow only certain MAC ID on my wireless. Each time a new device comes in, I need to add its MAC ID to the list.
@MikeMiller Hmm, I've read a bit of Titchmarsh, but I don't remember simple connectedness defined in a formal way. Also, a book full of computations Lipschitz-Spiegel just defines it hand-wavingly ("every loop can be shrunk to a point")
With the standard field structure on a field of characteristic $p$ which isn't equal to its prime subfield, I believe I have an argument that Frobenius can't be represented by a multiplication map. But I know very little about the different ring structures on fields of char $p$...
It would be really helpful if anyone suggest places where harmonic analysis is done in more of a functional analysis approach rather than measure theoretric completely!!
@Ted: that's what I don't know, I suppose. :) If that's the case, then there's another example. For small enough values of $q$, if you require rings have unity, one can march through multiplication tables, but I don't know many stronger methods.
yeah, I looked up Cech cohomology. the nerve idea I also had when trying to capture the idea of local-possibility vs global-impossibility, but I was trying to define a fundamental group that way.
@anon By the way, one thing: Penrose's remark on $d_{ij}$ not depending on the choice of $A_{ij}$'s is actually correct and important, contrary to what you (and admittedly I) believed :)
my idea was to define the fundamental group to be the homotopies of an embedding of the disk into the picture which at all times during the homotopy has "possible" image
I'll have to reread my question to remember what the dijs even were
go ahead and start writing an answer if you haven't already
@BalarkaSen Say the picture is a space X, and we have an open cover {U} of all open sets which, when you restrict your attention to only the picture as it exists inside U, are "possible" (rather than impossible like the whole picture). Let *:D->X be an embedding of the open disk U into X whose image is "possible" set U. A "path" in the fundamental group of X should be a homotopy H:*->* such that H(t,-):D->X has image which is possible for all t.
basically, you're shining a light on the picture, and moving around your light but are restricted to making sure you're only shining light on a region which depicts something possible
You see, it's the group of symmetries of the figure which makes changes to your pieces $Q_i$, but the figure remains the same. In the tribar example, one can enlarge one piece by $\lambda$, enlarge (i.e., shrink) the other piece by $1/\lambda$ and leave the third as it is. This leaves the picture invariant. So collection of all such symmetries exactly forms the ambiguity group!
You have a natural composition. First do one symmetry operation, then do another.
So it's precisely the set $\{\lambda \in \Bbb R: \lambda > 0\}$ under multiplication. Namely, $\Bbb R^+$ under multiplication.
Ultimately, the group's meant to detect "ambiguity", not impossibility.
In the Necker cube, note that ambiguity is in the choice of a linking point/vertex to point outwards or inwards. So two choices. Choosing one vertex to be pointing outwards makes the figure "unambigous", as all others are automatically pointing outwards. Choosing it to be pointing inwards makes the figure unambigous again. So choice is in that single vertex. Reflection is our symmetry here.
@anon Here's how I think it's related to Cech cohomology. Let $X$ be your ambiguous figure. $\{Q_i\}$ be a good cover (good cover means every open set and all intersections are contractible). Declare $C_0(X)$ to be collection of functions $\{Q_i\} \to \{q_i\}$ (these are the 0-cochains). Declare $C_1(X)$ to be collection of functions $\{Q_i \cap Q_j\} \to \{d_{ij}\}$ such that $d_{ij} = d_{ji}^{-1}$.
Coboundary map $C_0(X) \to C_1(X)$ is just takes a 0-cochain assigning $q_i$ to $Q_i$ to the 1-cochain assigning $q_i/q_j$ to $Q_i \cap Q_j$.
@L33ter BTW, you were asking for smash product above. Here's what it is. Take $S^1 \times S^1$, where $S^1$ is the circle. This is a torus. Now a torus has a "meridian" (the circle which wraps around it and is tight around the handle) and a "longitude" (the circle going around the donut hole). These two intersect at a point. Now collapse (i.e., quotient) this subspace consisting of two circles touching at a point. You get $S^2$.
Thus, we say "smash" of two circles is $S^2$. Similar construction works for arbitrary spaces.
What tools would you recommend me for evaluating this integral?
$$\int_{0}^{\pi/4} \log(\sin(x)) \log(\cos(x)) \log(\cos(2x)) \,dx$$
My first thought was to use the beta function, but it's hard to get such a form because
of $\cos(2x)$. What other options do I have?
Suppose that a unit-speed curve $\gamma$ with curvature $\kappa>0$ and principal normal $n$ is a parametrization of the intersection of two oriented surfaces $S_1$ and $S_2$ with unit normals $N_1$ and $N_2$.
Suppose that $\alpha$ is the angle between the two surfaces.
How can we calculate $\|(N_1 \times N_2)\times n\|^2$ ?
(I may be imagining it incorrectly, but I reckon $n$ will point either in the same or opposite direction to the cross product of $N_1$ and $N_2$, so it'd just be $0$?)
Oh wait, I used the wrong word. I meant they would be perpendicular so the cross product of $N_1$ and $N_2$ would be parallel to the tangent to the intersection of the surfaces, @MaryStar. ^_^"
So in the picture, the cross product of $N_1$ and $N_2$ would point along the red line.
And why is $N_1 \times N_2$ parallel to the tangent along the curve of intersection? @Khallil
$N_1$ is perpedicular to the surface $S_1$, $N_2$ is perpedicular to the surface $S_2$. We have that $N_1\times N_2$ is perpendicular to both surfaces, right?
HINT: Your integral can be brought to this form $$\int_{-1}^1 \frac{\log \left((1-x)^s+(1+x)^s\right)-s \log (2)}{x+1} \, dx$$ and then you can split the interval and calculate each integral separately. Use on the positive side that $\frac{1-x}{1+x}\mapsto x$ and $\frac{1+x}{1-x}\mapsto x$ on the...
@robjohn I don't need the bounty but I'm curious to know why the other answer received the bounty (half of the bounty).
@SuperstarMonica Your answer was posted before the bounty was placed, and for an automatic award of bounties, only answers that were posted during the bounty period are eligible.