# Tag Info

21

In order to avoid definiteness problems, I will consider $a$, $b$ and $c$ as independent variables in the field of rational fractions $\mathbb{C}(a,b,c)$, and I will seek some kind of a parametric representation of the solutions $(a,b,c)$ of the proposed equation as rational functions from $\mathbb{C}(u,v)$ where $u$ and $v$ are independent variables. ...

12

If $x_1,x_2,x_3$ are the roots of $x^3+2x^2+3x+4=0$ then $$x^3+2x^2+3x+4 = (x-x_1)(x-x_2)(x-x_3)$$ $$= x^3 - (x_1 + x_2 + x_3)x^2 + (x_1 x_2 + x_1 x_3 + x_2 x_3)x - x_1 x_2 x_3 = x^3 - e_1 x^2 + e_2 x - e_3.$$ So $e_1 = -2$, $e_2 = 3$ and $e_3 = -4$. Now the trick is to express the power sums $x_1^3 + x_2^3 = x_3^3$ and $x_1^4 + x_2^4 = x_3^4$ in terms of ...

8

Probably a simple general formula for your matrix $C_n=(C_{\lambda,\mu})_{\lambda,\mu\in\mathcal P_n}$, where $\mathcal P_n$ denotes the partitions of $n$ (ordered in decreasing lexicographic ordering) does not exist. However a number of things can be said, notably your above guesses can be confirmed. One thing that your examples suggest but which is false ...

6

Okay, I'll answer your question on the cross ratio: First of all, recall its definition $$\lambda = \lambda(z) = [z,z_2,z_3,z_4] = \frac{z-z_3}{z - z_4} : \frac{z_2 - z_3}{z_2 - z_4}$$ which is the unique Möbius transformation $z \mapsto \lambda(z)$ sending the ordered triple $(z_2,z_3,z_4)$ to $(1,0,\infty)$—it is a general and easy fact that ...

6

The trick it's just to add and subtract $1$ from each fraction and then to factorize: $$\frac{a}{b+c}+\frac{b}{c+a}+\frac{c}{a+b}=\frac{a+b+c}{b+c}-1+\frac{a+b+c}{c+a}-1+\frac{a+b+c}{a+b}-1=(a+b+c)(\frac{1}{a+b}+\frac{1}{b+c}+\frac{1}{a+c})-3=7\cdot 0.7 -3=1.9$$

6

$$\frac{c}{a+b}+\frac{a}{b+c}+\frac{b}{a+c}$$ $$=\frac{7-(a+b)}{a+b}+\frac{7-(b+c)}{b+c}+\frac{7-(a+c)}{a+c}$$ $$=\frac{7}{a+b}+\frac{7}{b+c}+\frac{7}{a+c}-3$$ $$=7\cdot 0.7-3=1.9$$

4

Not a general answer, but in this particular case you can write $$f(x_1,x_2,x_3,x_4)= \frac{(x_1-x_3)(x_2-x_4)}{(x_1-x_4)(x_2-x_3)}$$ which makes it easier to see the symmetries.

4

The claim is true. I find it convenient to state the problem in a "Boolean hypercube" form . The variables will be the $\binom{2d}{d}$ strings of length $2d$ over the alphabet $\{L,R\}$ with exactly $d$ Rs. For any string $x\in\{L,R\}^{2d}$ with exactly $d+1$ $R$'s, let $\partial(x)$ denote the sum of the variables labelled by strings obtained by ...

4

Ones first impression is that this is a set of three quadratic equations. So if we would proceed by eliminating two of the three variables, we would get a higher order equation that presumably can not be solved. However, in this case the functions are such that we can side-step these complications. With a nice trick we can work with linear equations! x*y - ...

4

One possibility is to compute $S$-polynomials from the given polynomials, namely $$25x + 9y + 16z - 12=0, \\ 24yz + 16z^2 - 32z + 5 =0.$$ Then we can eliminate $x$ and $y$ and substitute into the three original equations. We obtain $$(64z^3 - 80z^2 - 52z + 5)(4z - 1)=0.$$ Although we have all roots real here, we see that the only positive real solution ...

4

Simplify it to $$f(x)={{5a^2+6ax+9x^2}\over {a+3x}}=\frac{4a^2}{a+3x} + {{a^2+6ax+9x^2}\over {a+3x}}=\frac{4a^2}{a+3x} + {{(a+3x)^2}\over {a+3x}}\\ =\frac{4a^2}{a+3x} + (a+3x)$$ and substitute $y=a+3x$ then $$f(y)=\frac{4a^2}{y}+y$$ which has the following property: $$f(-y)=-\frac{4a^2}{y} -y = -f(y)$$ which means that $f(y)$ is an odd function, point ...

3

There is no nice way. This is, however, the theory of symmetrization which attempts to show that for some extremal problems the solutions have certain symmetry. It goes back at least to Steiner symmetrization of 19th century. Much is known, but many open problems remain, and there is no universal theorem with which one could hammer problems without looking ...

3

A function $f$ is radially symmetric if $f(Ax) = f(x)$ for all orthogonal $A$. Thus, if $f$ and $g$ are radially symmetric, and the convolution exists, we have for any $A\in O(n)$ \begin{align} (f\ast g)(Ax) &= \int_{\mathbb{R}^n} f(y) g(Ax-y)\,dy\\ &= \int_{\mathbb{R}^n} f(y) g(A(x-A^T y))\,dy\\ &= \int_{\mathbb{R}^n} f(y) g(x-A^T ... 3 First of all notice that a and b appear "symmetrically": if you exchange a with b, the system doesn't change. In these cases, settingx=a+b,\quad y=ab$$usually helps. Indeed, you can note now that the left hand side of the second equation is just x/y, while$$ a^3+b^3 = x^3 -3xy $$The first equation already tells you what x is; so the ... 3 Note that |e_n| is dominated by \left(\sum_j|x_j|\right)^n/(n!), so yes, everything like what you wrote converges and pretty fast. 3 Beside the very nice answer by Marc, I found this Introduction to Symmetric Functions by Mike Zabrocki:$$ e_\mu = \sum_\lambda B_{\lambda \mu} m_\lambda\tag{2.28} $$where B_{\lambda \mu} is the number of matricies with entries in \{0, 1\} whose column sum is \mu and row sum is equal to \lambda.$$\dots$$B_{\lambda \mu}is the number of ... 3 You have four symbols x_1,x_2,x_3 and x_4. If you have two different permutations which fix your function, then they will fix it if applied consecutively. The identity fixes the function, as does the inverse of any permutation which fixes it. The permutations fixing the function therefore form a group. Since there are four objects being permuted, the ... 3 eliminating y,z we get for x:$$125 x^4-60 x^3-58 x^2+18 x=1$$3 From the first equation we have$$y=\frac6x.$$Plugging this into the second equation yields$$x^{\tfrac6x}+\left(\frac6x\right)^x=17.$$Call this expression on the left hand side f(x). We want to solve the equation f(x)=17. It is obvious that x=2 and x=3 solve this equation. It remains to show that there are no other solutions. To see this, first ... 3 Take$$\|(x_1,x_2)\|^2 = x_1^2+x_1x_2+x_2^2.$$This relation defines a norm on \Bbb R^2. Clearly,$$\|(x_1,x_2)\|=\|(x_2,x_1)\|\ne \|(x_1,-x_2)\|.$$edit Write this norm in terms of a matrix A=\frac 12 \begin{pmatrix}2&1\\1&2\end{pmatrix} and scalar product:$$\|\vec x\|^2 = \vec x^TA\vec x = (A\vec x,\vec x).$$The matrix A is positive ... 3 Let I be the value of your integral. Use the substitution u=\pi/2-x to get a new integral, call it J=I. Then I+J = \int_0^{\pi/2} 1 ~ dx therefore 2I = \frac{\pi}{2}. 2 I think what you need is Newton's identities, in particular the section about their application to the roots of a polynomial. 2 Do this$$f(x) = 2(x^2 + 4x) + 5 = 2(x^2 + 4x + 4) + 5 - 8 = 2(x + 2)^2 - 3.$$Note that f is insensitive to the sign of x + 2 so f is symmetric about the line x = -2 2 It is natural to try to manipulate symmetric polynomials as one does polynomials, representing them as a sum of monomials, and to take advantage of the symmetry by representing a whole orbit of monomials only once, as a minimal symmetric polynomial~m_\lambda. Also one can now leave the number of indeterminates unspecified, and thus effectively manipulate ... 2 This solution is similar to what you are saying, but not phrased in your language of implicit function theorem. Consider the polynomial$$ \sum_{i=1}^n \left[ x_i ^m \prod_{j < k, j\neq i, k\neq i} (x_j-x_k)\right] $$If x_i = x_j, then you should verify that the polynomial is equal to 0 (many terms with x_i-x_j) are zero, and then ensure that the ... 2 We have$$\begin{align} a+b+c & = 3 \\ \frac{1}{a} + \frac{1}{b} + \frac{1}{c} &= \frac{5}{12} \\ a^3 + b^3 + c^3 & = 45 \\ \end{align} $$The second equation tells us that \frac{ab+bc+ca}{abc} = \frac{5}{12} , or that 12(ab+bc+ca) = 5(abc). Using (a+b+c)^3 - a^3 - b^3 - c^3 = 3(a+b)(b+c)(c+a) = 3(3-a)(3-b)(3-c), we get that 27-45 = ... 2 In order to see the "correct" behavior of the Schur polynomials and to be able to compare different formulas for the Schur polynomials, the number of variables you need is equal to the total number of boxes in the partition (the value d, in the Wikipedia notation), not just the number of (nonzero) parts in the partition. Try taking n=d=4 in both of your ... 2 I'll suppose R is an integral domain, and therefore contained in an algebraically closed field K (one can do without this assumption, but it simplifies the argument). Suppose p(s_1,\ldots,s_n)=0 but p is not the zero polynomial; then certainly there exist constants a_1,\ldots,a_n\in K such that p(a_1,\ldots,a_n)\neq0. Now consider$$ ...

2

I think your assumption is right. In the Introduction to Symmetric Functions by Mike Zabrocki there is a nice table on page 18, that relates all kinds of symmmetric functions. There $m_\mu$ is related to $e_\lambda$ by the same coefficients $G_{\lambda\mu}$ as $f_\mu$ and $h_\lambda$ are, but he leave[s] it as an exercise to determine some sort of formula ...

2

I'm not sure if this is exactly what you're looking for, but I recently worked on a paper regarding just this question (http://arxiv.org/abs/1403.8139). We were generalizing Tokuyama's deformation formula (http://projecteuclid.org/euclid.jmsj/1230129805) for the Schur polynomial, so we used Gelfand-Tsetlin patterns rather than Young tableaux. Tokuyama's ...

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