To recapitulate the basics of elliptic integral theory (details here) we have
K = K(k) = \int_{0}^{\pi/2}\frac{d\theta}{\sqrt{1 - k^{2}\sin^{2}\theta}} = \int_{0}^{1}\frac{dx}{\sqrt{(1 - x^{2})(1 - k^{2}x^{2})}}
E = E(k) = \int_{0}^{\pi/2}\sqrt{1 - k^{2}\sin^{2}\theta}\,d\theta = \int_{0}^{1}\frac{\sqrt{1 - k^{2}x^{2}}}{\sqrt{1 - x^{2}}}\,dx
We have here 0 \leq k \leq 1 and the complementary modulus k' = \sqrt{1 - k^{2}} or in other words k^{2} + k'^{2} = 1. Also we denote K' = K(k'), E' = E(k') and we have the Legendre's Identity KE' + K'E - KK' = \frac{\pi}{2}
From the above arguments it follows that the function K'/K is a strictly decreasing function of k. When k \to 0, K'/K \to \infty and as k \to 1, K'/K \to 0. Thus the function K'/K maps the interval (0, 1) to the interval (0, \infty). For any given positive number \alpha we have a unique positive k \in (0, 1) such that K'/K = \alpha. Let p be any positive number and then p\alpha is also positive and therefore there is a unique number l \in (0, 1) such that K(l')/K(l) = p\alpha. We traditionally denote L = K(l), L' = K(l'). Therefore we can write \frac{L'}{L} = p\alpha = p\,\frac{K'}{K}
Again let's think in the following way. Suppose a number k \in (0, 1) and a positive number p is given. From k we can calculate K'/K and hence pK'/K corresponding to which there is a unique number l \in (0, 1) such that L'/L = pK'/K. In this fashion l turns out to be a function of k. Therefore the equation L'/L = pK'/K determines l as a function of k which is one-one and invertible. From the continuity of K the function turns out to be continuous. To derive these results formally we need the fundamental formulas: \frac{dk'}{dk} = -\frac{k}{k'},\,\, \frac{dK}{dk} = \frac{E - k'^{2}K}{kk'^{2}},\,\, \frac{dE}{dk} = \frac{E - K}{k} (for the proofs of these results read here)
Using these we have \frac{dK'}{dk} = \frac{dk'}{dk}\frac{dK'}{dk'} = -\frac{k}{k'}\frac{E' - k^{2}K'}{k^{2}k'} = \frac{k^{2}K' - E'}{kk'^{2}} and therefore \begin{align}\frac{d}{dk}\left(\frac{K'}{K}\right) &= \dfrac{K\dfrac{dK'}{dk} - K'\dfrac{dK}{dk}}{K^{2}} = \frac{1}{K^{2}}\left(\frac{K(k^{2}K' - E')}{kk'^{2}} - \frac{K'(E - k'^{2}K)}{kk'^{2}}\right)\notag\\ &= \frac{KK' - KE' - K'E}{kk'^{2}K^{2}} = -\frac{\pi}{2kk'^{2}K^{2}}\notag\end{align} Thus we have finally another fundamental relation \frac{d}{dk}\left(\frac{K'}{K}\right) = -\frac{\pi}{2kk'^{2}K^{2}} which shows that K'/K is strictly decreasing. On differentiating the equation L'/L = pK'/K we get \frac{dl}{ll'^{2}L^{2}} = p\frac{dk}{kk'^{2}K^{2}} or \frac{dl}{dk} = p\,\frac{ll'^{2}}{kk'^{2}}\left(\frac{L}{K}\right)^{2} and therefore l is a strictly increasing function of k and maps (0, 1) to (0, 1). Also p <(=,>) 1 \Rightarrow l > (=,<) k. We also see that the ratio L/K is a function of k, l and we traditionally call it the multiplier and denote by M_{p}(l, k). Thus we have pM_{p}^{2}(l, k) = p\left(\frac{L}{K}\right)^{2} = \frac{kk'^{2}}{ll'^{2}}\frac{dl}{dk} Also it should be noted that if p < (=, >) 1 \Rightarrow M_{p}(l, k) > (=, <) 1.
Next let's understand that it is necessary only to study the case when p is a positive prime. For, if for positive prime p the relation L'/L = pK'/K is leading to an algebraic relation between l and k then we can show that the same kind of relation holds when p is any positive rational number. First suppose p is composite positive integer and p = p_{1}p_{2} where both p_{1}, p_{2} are primes. Then L'/L = pK'/K can be written L'/L = p_{1}\Gamma'/\Gamma = p_{1}(p_{2}K'/K). Since the relation between l, \gamma and \gamma, k is algebraic by assumption, the relation between l, k is algebraic. The same reasoning can be extended to the case when p is a product of any number of primes. Thus the case of positive integers is handled. In case of p = a/b where a, b are positive integers we can write L'/L = pK'/K as bL'/L = aK'/K = \Gamma'/\Gamma. Since the relation between \gamma, k and \gamma, l is algebraic therefore the relation between k, l is algebraic.
So from now on let's assume that p is a positive prime. The algebraic relation between l, k implied by the equation L'/L = pK'/K is called a modular equation of degree p. The way Jacobi obtained these modular equations is related to the transformation of elliptic integrals. Consider the differential \frac{dy}{\sqrt{(1 - y^{2})(1 - l^{2}y^{2})}} By suitable rational transformation y = f(x)/g(x) where f(x), g(x) are polynomials it is expected to reduce the differential to the form \frac{dx}{M\sqrt{(1 - x^{2})(1 - k^{2}x^{2})}} Thus in effect we wish to establish a relation of the form \frac{Mdy}{\sqrt{(1 - y^{2})(1 - l^{2}y^{2})}} = \frac{dx}{\sqrt{(1 - x^{2})(1 - k^{2}x^{2})}} where y is a rational function of x and M is some constant. That such a transformation is possible is not so obvious. Jacobi started his Fundamenta Nova by describing this elegant theory of transformation and showed that such a transformation exists for every value of the positive prime p which is called the order of the transformation. In what follows we shall assume that p is an odd prime ( p = 2 is covered by the famous Landen Transformations).
The constant M is called multiplier and depends upon the values of l, k and is related to the multiplier M_{p}(l, k). To simplify the process of transformation the rational function y = U(x)/V(x) is chosen to be of very specific form. With the requirement that y vanishes with x we take y = xf(x)/g(x) where f(x), g(x) are polynomials of degrees (p - 1). Also f(x), g(x) are supposed to be even functions so that they are functions of x^{2} and then we can write y = \frac{xN(1, x^{2})}{D(1, x^{2})} where N, D are homogeneous polynomials of degree (p - 1)/2. Another condition which we impose is that the relation between y and x does not change when (x, y) is replaced by (1/kx, 1/ly). That this is possible needs to be demonstrated. First of all we can see that N\left(1, \frac{1}{k^{2}x^{2}}\right) = \left(\frac{1}{kx}\right)^{p - 1}N(k^{2}x^{2}, 1) We can next choose D(1, x^{2}) such that N(k^{2}x^{2}, 1) = \Delta D(1, x^{2}) where \Delta is a constant. Thus the coefficients of D(1, x^{2}) are same as those of N(1, x^{2}), but in reverse order and multiplied by suitable powers of k. It thus follows that N\left(1, \frac{1}{k^{2}x^{2}}\right) = \Delta\left(\frac{1}{kx}\right)^{p - 1}D(1, x^{2}) Replacing x by 1/kx we get N(1, x^{2}) = \Delta x^{p - 1}D\left(1, \frac{1}{k^{2}x^{2}}\right) Multiplying the above two equations we get N(1, x^{2})N\left(1, \frac{1}{k^{2}x^{2}}\right) = \frac{\Delta^{2}}{k^{p - 1}}D(1, x^{2})D\left(1, \frac{1}{k^{2}x^{2}}\right) Now let's suppose that in the defining equation if we put 1/kx in place of x then the value of y changes to y_{1}. Thus y_{1} = \dfrac{\dfrac{1}{kx}N\left(1, \dfrac{1}{k^{2}x^{2}}\right)}{D\left(1, \dfrac{1}{k^{2}x^{2}}\right)} = \frac{1}{kx}\frac{\Delta^{2}}{k^{p - 1}}\frac{D(1, x^{2})}{N(1, x^{2})} = \frac{\Delta^{2}}{k^{p}}\frac{D(1, x^{2})}{xN(1, x^{2})} = \frac{\Delta^{2}}{k^{p}}\frac{1}{y} Clearly this reduces to 1/ly provided l = k^{p}/\Delta^{2}.
Hence a transformation of the form y = U(x)/V(x) with U of degree p and V of degree (p - 1) with U being odd function and V being even function is possible which remains invariant under the change of variables (x, y) \to (1/kx, 1/ly).
Next we would like to have further restrictions on the form of U and V. Putting y = U/V leads to dy = \frac{VU' - UV'}{V^{2}}\,dx,\,\, \sqrt{(1 - y^{2})(1 - l^{2}y^{2})} = \frac{1}{V^{2}}\sqrt{(V^{2} - U^{2})(V^{2} - l^{2}U^{2})} and hence \frac{dy}{\sqrt{(1 - y^{2})(1 - l^{2}y^{2})}} = \frac{VU' - UV'}{\sqrt{(V^{2} - U^{2})(V^{2} - l^{2}U^{2})}}\,dx If it is possible that V + U = (1 + x)A^{2}, V - U = (1 - x)B^{2} for some polynomials A, B then we can see that 1 + y = (1 + x)A^{2}/V,\, 1 - y = (1 - x)B^{2}/V and by invariance of relation between x and y under the transformation (x, y) \to (1/kx, 1/ky) we can see that we must also have the relations 1 + ly = (1 + kx)C^{2}/V,\, 1 - ly = (1 - kx)D^{2}/V or V +lU = (1 + kx)C^{2},\, V - lU = (1 - kx)D^{2} Now we can see that if (x - \alpha) is a factor of A then (x - \alpha)^{2} divides V + U and hence (x - \alpha) divides (V + U)U' - U(V + U)' = VU' - UV'. From the same logic it follows that A, B, C, D each divide VU' - UV' and since the degrees of VU' - UV' and ABCD are same (equal to (2p - 2)) it follows that the ratio ABCD/(VU' - UV') is a constant which we denote by M. Thus we arrive at \frac{Mdy}{\sqrt{(1 - y^{2})(1 - l^{2}y^{2})}} = \frac{dx}{\sqrt{(1 - x^{2})(1 - k^{2}x^{2})}} The idea is now to choose polynomials A, B in a suitable form. We keep A = P + Qx, B = P - Qx such that P, Q are even functions of x and the degree of P \pm Qx is (p - 1)/2. In general if p = (4n - 1) then the degrees of P, Q are (2n - 2) and if p = 4n + 1, degree of P is 2n and that of Q is (2n - 2).
Thus we arrive at the following transformation \frac{1 - y}{1 + y} = \frac{1 - x}{1 + x}\frac{(P - Qx)^{2}}{(P + Qx)^{2}} so that y = \frac{x(P^{2} + 2PQ + Q^{2}x^{2})}{P^{2} + 2PQx^{2} + Q^{2}x^{2}} and then we obtain \begin{align}1 - y &= \frac{(1 - x)(P - Qx)^{2}}{P^{2} + 2PQx^{2} + Q^{2}x^{2}}\notag\\ 1 + y &= \frac{(1 + x)(P + Qx)^{2}}{P^{2} + 2PQx^{2} + Q^{2}x^{2}}\notag\\ 1 - ly &= \frac{(1 - kx)(P' - Q'x)^{2}}{P^{2} + 2PQx^{2} + Q^{2}x^{2}}\notag\\ 1 + ly &= \frac{(1 + kx)(P' + Q'x)^{2}}{P^{2} + 2PQx^{2} + Q^{2}x^{2}}\notag\end{align} The actual methodology of finding the polynomials U, V (or P, Q) would be dealt with in next post by showing examples with p = 3 and p = 5. From the theoretical investigation above it is clear that the process of finding these polynomials (i.e. their coefficients) is totally algebraical and hence the relation between k and l is algebraic (note that l = k^{p}/\Delta^{2}, and that \Delta itself would be an algebraic function of l, k). It should also be observed that the multiplier M is also an algebraical function of l and k (calculation of M is easy if we observe that 1/M = dy/dx \text{ at } x = 0).
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We have here 0 \leq k \leq 1 and the complementary modulus k' = \sqrt{1 - k^{2}} or in other words k^{2} + k'^{2} = 1. Also we denote K' = K(k'), E' = E(k') and we have the Legendre's Identity KE' + K'E - KK' = \frac{\pi}{2}
The Function K'/K
From the definition it is clear that K is a strictly increasing function of k and moreover K \to \infty as k \to 1. Thus function K(k) maps interval [0, 1) to [\pi/2, \infty). Similarly E is strictly decreasing and maps [0, 1] to [1, \pi/2]. Therefore it follows that K' is a strictly decreasing function of k and E' is a strictly increasing function of k.From the above arguments it follows that the function K'/K is a strictly decreasing function of k. When k \to 0, K'/K \to \infty and as k \to 1, K'/K \to 0. Thus the function K'/K maps the interval (0, 1) to the interval (0, \infty). For any given positive number \alpha we have a unique positive k \in (0, 1) such that K'/K = \alpha. Let p be any positive number and then p\alpha is also positive and therefore there is a unique number l \in (0, 1) such that K(l')/K(l) = p\alpha. We traditionally denote L = K(l), L' = K(l'). Therefore we can write \frac{L'}{L} = p\alpha = p\,\frac{K'}{K}
Again let's think in the following way. Suppose a number k \in (0, 1) and a positive number p is given. From k we can calculate K'/K and hence pK'/K corresponding to which there is a unique number l \in (0, 1) such that L'/L = pK'/K. In this fashion l turns out to be a function of k. Therefore the equation L'/L = pK'/K determines l as a function of k which is one-one and invertible. From the continuity of K the function turns out to be continuous. To derive these results formally we need the fundamental formulas: \frac{dk'}{dk} = -\frac{k}{k'},\,\, \frac{dK}{dk} = \frac{E - k'^{2}K}{kk'^{2}},\,\, \frac{dE}{dk} = \frac{E - K}{k} (for the proofs of these results read here)
Using these we have \frac{dK'}{dk} = \frac{dk'}{dk}\frac{dK'}{dk'} = -\frac{k}{k'}\frac{E' - k^{2}K'}{k^{2}k'} = \frac{k^{2}K' - E'}{kk'^{2}} and therefore \begin{align}\frac{d}{dk}\left(\frac{K'}{K}\right) &= \dfrac{K\dfrac{dK'}{dk} - K'\dfrac{dK}{dk}}{K^{2}} = \frac{1}{K^{2}}\left(\frac{K(k^{2}K' - E')}{kk'^{2}} - \frac{K'(E - k'^{2}K)}{kk'^{2}}\right)\notag\\ &= \frac{KK' - KE' - K'E}{kk'^{2}K^{2}} = -\frac{\pi}{2kk'^{2}K^{2}}\notag\end{align} Thus we have finally another fundamental relation \frac{d}{dk}\left(\frac{K'}{K}\right) = -\frac{\pi}{2kk'^{2}K^{2}} which shows that K'/K is strictly decreasing. On differentiating the equation L'/L = pK'/K we get \frac{dl}{ll'^{2}L^{2}} = p\frac{dk}{kk'^{2}K^{2}} or \frac{dl}{dk} = p\,\frac{ll'^{2}}{kk'^{2}}\left(\frac{L}{K}\right)^{2} and therefore l is a strictly increasing function of k and maps (0, 1) to (0, 1). Also p <(=,>) 1 \Rightarrow l > (=,<) k. We also see that the ratio L/K is a function of k, l and we traditionally call it the multiplier and denote by M_{p}(l, k). Thus we have pM_{p}^{2}(l, k) = p\left(\frac{L}{K}\right)^{2} = \frac{kk'^{2}}{ll'^{2}}\frac{dl}{dk} Also it should be noted that if p < (=, >) 1 \Rightarrow M_{p}(l, k) > (=, <) 1.
Jacobi's Transformation Theory
Jacobi showed that the relation between l and k is algebraic when p is rational. First of all as an example we can take p = 2. Then by Landen's transformation l = (1 - k')/(1 + k') < k we see that L'/L = 2K'/K. Clearly here the relation between l and k is algebraic and is also given by k = 2\sqrt{l}/(1 + l). Also \frac{dl}{dk} = \frac{(1 + k')(k/k') + (1 - k')(k/k')}{(1 + k')^{2}} = \frac{2k}{k'(1 + k')^{2}} and therefore 2M_{2}^{2}(l, k) = \frac{kk'^{2}}{ll'^{2}}\frac{dl}{dk} = kk'^{2}\frac{1 + k'}{1 - k'}\frac{(1 + k')^{2}}{4k'}\frac{2k}{k'(1 + k')^{2}} = \frac{k^{2}}{2}\frac{(1 + k')^{2}}{1 - k'^{2}} so that L/K = M_{2}(l, k) = (1 + k')/2 = 1/(1 + l) as should have been the case.Next let's understand that it is necessary only to study the case when p is a positive prime. For, if for positive prime p the relation L'/L = pK'/K is leading to an algebraic relation between l and k then we can show that the same kind of relation holds when p is any positive rational number. First suppose p is composite positive integer and p = p_{1}p_{2} where both p_{1}, p_{2} are primes. Then L'/L = pK'/K can be written L'/L = p_{1}\Gamma'/\Gamma = p_{1}(p_{2}K'/K). Since the relation between l, \gamma and \gamma, k is algebraic by assumption, the relation between l, k is algebraic. The same reasoning can be extended to the case when p is a product of any number of primes. Thus the case of positive integers is handled. In case of p = a/b where a, b are positive integers we can write L'/L = pK'/K as bL'/L = aK'/K = \Gamma'/\Gamma. Since the relation between \gamma, k and \gamma, l is algebraic therefore the relation between k, l is algebraic.
So from now on let's assume that p is a positive prime. The algebraic relation between l, k implied by the equation L'/L = pK'/K is called a modular equation of degree p. The way Jacobi obtained these modular equations is related to the transformation of elliptic integrals. Consider the differential \frac{dy}{\sqrt{(1 - y^{2})(1 - l^{2}y^{2})}} By suitable rational transformation y = f(x)/g(x) where f(x), g(x) are polynomials it is expected to reduce the differential to the form \frac{dx}{M\sqrt{(1 - x^{2})(1 - k^{2}x^{2})}} Thus in effect we wish to establish a relation of the form \frac{Mdy}{\sqrt{(1 - y^{2})(1 - l^{2}y^{2})}} = \frac{dx}{\sqrt{(1 - x^{2})(1 - k^{2}x^{2})}} where y is a rational function of x and M is some constant. That such a transformation is possible is not so obvious. Jacobi started his Fundamenta Nova by describing this elegant theory of transformation and showed that such a transformation exists for every value of the positive prime p which is called the order of the transformation. In what follows we shall assume that p is an odd prime ( p = 2 is covered by the famous Landen Transformations).
The constant M is called multiplier and depends upon the values of l, k and is related to the multiplier M_{p}(l, k). To simplify the process of transformation the rational function y = U(x)/V(x) is chosen to be of very specific form. With the requirement that y vanishes with x we take y = xf(x)/g(x) where f(x), g(x) are polynomials of degrees (p - 1). Also f(x), g(x) are supposed to be even functions so that they are functions of x^{2} and then we can write y = \frac{xN(1, x^{2})}{D(1, x^{2})} where N, D are homogeneous polynomials of degree (p - 1)/2. Another condition which we impose is that the relation between y and x does not change when (x, y) is replaced by (1/kx, 1/ly). That this is possible needs to be demonstrated. First of all we can see that N\left(1, \frac{1}{k^{2}x^{2}}\right) = \left(\frac{1}{kx}\right)^{p - 1}N(k^{2}x^{2}, 1) We can next choose D(1, x^{2}) such that N(k^{2}x^{2}, 1) = \Delta D(1, x^{2}) where \Delta is a constant. Thus the coefficients of D(1, x^{2}) are same as those of N(1, x^{2}), but in reverse order and multiplied by suitable powers of k. It thus follows that N\left(1, \frac{1}{k^{2}x^{2}}\right) = \Delta\left(\frac{1}{kx}\right)^{p - 1}D(1, x^{2}) Replacing x by 1/kx we get N(1, x^{2}) = \Delta x^{p - 1}D\left(1, \frac{1}{k^{2}x^{2}}\right) Multiplying the above two equations we get N(1, x^{2})N\left(1, \frac{1}{k^{2}x^{2}}\right) = \frac{\Delta^{2}}{k^{p - 1}}D(1, x^{2})D\left(1, \frac{1}{k^{2}x^{2}}\right) Now let's suppose that in the defining equation if we put 1/kx in place of x then the value of y changes to y_{1}. Thus y_{1} = \dfrac{\dfrac{1}{kx}N\left(1, \dfrac{1}{k^{2}x^{2}}\right)}{D\left(1, \dfrac{1}{k^{2}x^{2}}\right)} = \frac{1}{kx}\frac{\Delta^{2}}{k^{p - 1}}\frac{D(1, x^{2})}{N(1, x^{2})} = \frac{\Delta^{2}}{k^{p}}\frac{D(1, x^{2})}{xN(1, x^{2})} = \frac{\Delta^{2}}{k^{p}}\frac{1}{y} Clearly this reduces to 1/ly provided l = k^{p}/\Delta^{2}.
Hence a transformation of the form y = U(x)/V(x) with U of degree p and V of degree (p - 1) with U being odd function and V being even function is possible which remains invariant under the change of variables (x, y) \to (1/kx, 1/ly).
Next we would like to have further restrictions on the form of U and V. Putting y = U/V leads to dy = \frac{VU' - UV'}{V^{2}}\,dx,\,\, \sqrt{(1 - y^{2})(1 - l^{2}y^{2})} = \frac{1}{V^{2}}\sqrt{(V^{2} - U^{2})(V^{2} - l^{2}U^{2})} and hence \frac{dy}{\sqrt{(1 - y^{2})(1 - l^{2}y^{2})}} = \frac{VU' - UV'}{\sqrt{(V^{2} - U^{2})(V^{2} - l^{2}U^{2})}}\,dx If it is possible that V + U = (1 + x)A^{2}, V - U = (1 - x)B^{2} for some polynomials A, B then we can see that 1 + y = (1 + x)A^{2}/V,\, 1 - y = (1 - x)B^{2}/V and by invariance of relation between x and y under the transformation (x, y) \to (1/kx, 1/ky) we can see that we must also have the relations 1 + ly = (1 + kx)C^{2}/V,\, 1 - ly = (1 - kx)D^{2}/V or V +lU = (1 + kx)C^{2},\, V - lU = (1 - kx)D^{2} Now we can see that if (x - \alpha) is a factor of A then (x - \alpha)^{2} divides V + U and hence (x - \alpha) divides (V + U)U' - U(V + U)' = VU' - UV'. From the same logic it follows that A, B, C, D each divide VU' - UV' and since the degrees of VU' - UV' and ABCD are same (equal to (2p - 2)) it follows that the ratio ABCD/(VU' - UV') is a constant which we denote by M. Thus we arrive at \frac{Mdy}{\sqrt{(1 - y^{2})(1 - l^{2}y^{2})}} = \frac{dx}{\sqrt{(1 - x^{2})(1 - k^{2}x^{2})}} The idea is now to choose polynomials A, B in a suitable form. We keep A = P + Qx, B = P - Qx such that P, Q are even functions of x and the degree of P \pm Qx is (p - 1)/2. In general if p = (4n - 1) then the degrees of P, Q are (2n - 2) and if p = 4n + 1, degree of P is 2n and that of Q is (2n - 2).
Thus we arrive at the following transformation \frac{1 - y}{1 + y} = \frac{1 - x}{1 + x}\frac{(P - Qx)^{2}}{(P + Qx)^{2}} so that y = \frac{x(P^{2} + 2PQ + Q^{2}x^{2})}{P^{2} + 2PQx^{2} + Q^{2}x^{2}} and then we obtain \begin{align}1 - y &= \frac{(1 - x)(P - Qx)^{2}}{P^{2} + 2PQx^{2} + Q^{2}x^{2}}\notag\\ 1 + y &= \frac{(1 + x)(P + Qx)^{2}}{P^{2} + 2PQx^{2} + Q^{2}x^{2}}\notag\\ 1 - ly &= \frac{(1 - kx)(P' - Q'x)^{2}}{P^{2} + 2PQx^{2} + Q^{2}x^{2}}\notag\\ 1 + ly &= \frac{(1 + kx)(P' + Q'x)^{2}}{P^{2} + 2PQx^{2} + Q^{2}x^{2}}\notag\end{align} The actual methodology of finding the polynomials U, V (or P, Q) would be dealt with in next post by showing examples with p = 3 and p = 5. From the theoretical investigation above it is clear that the process of finding these polynomials (i.e. their coefficients) is totally algebraical and hence the relation between k and l is algebraic (note that l = k^{p}/\Delta^{2}, and that \Delta itself would be an algebraic function of l, k). It should also be observed that the multiplier M is also an algebraical function of l and k (calculation of M is easy if we observe that 1/M = dy/dx \text{ at } x = 0).
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y=x*f(x)/g(x) Why f(x),g(x) should be polynomials of degrees p-1?
pokhkitro
December 20, 2021 at 6:09 PM