Let be the space of homogeneous degree- polynomials in . For and a column vector , define
Substitution preserves degree, and
so is a continuous representation of a topological group. This is the homogeneous polynomial representation of SU2.
To prove irreducibility, restrict to the diagonal circle
The monomials are its one-dimensional weight spaces, with distinct weights up to our harmless inverse-action convention. If is invariant, Fourier projection along this circle shows that contains a monomial. Differentiating the action of and complexifying gives the operators
Repeated applications of and connect every monomial to every other one. Hence contains the entire monomial basis, so .
Every is conjugate to with . Reading the eigenvalues on the monomial basis gives the character of the homogeneous polynomial representation of SU2
For this is
with the values at obtained by continuity.
For completeness, let be any finite-dimensional irreducible continuous complex representation of . Its restriction to the diagonal circle splits into integral weight spaces. Choose a vector of largest weight . The raising operator kills it, and the commutation relations show that is a nonnegative integer and that successive applications of the lowering operator form a string of weights
Their span is an invariant copy of ; irreducibility forces it to equal . Thus the classification of finite-dimensional representations of SU2 says
If the eigenvalues of are , then the eigenvalues on are for . Therefore the character of an exterior square is
The exterior square of an SU2 irreducible representation or the Clebsch-Gordan decomposition for SU2 with flip parity gives
The dimensions check the result.
The third elementary symmetric polynomial in the , together with Newton identities, gives
For the five-dimensional representation , the canonical duality
finishes the decomposition. The weights sum to zero, so is trivial, and every irreducible is self-dual. Consequently
At late time and . Define the elementary symmetric polynomials
Then part ii reduces to
where a prime removes the momentum-conserving Dirac delta distribution and
Expanding the product gives
Repeated integration by parts reduces every negative power to the supplied logarithmic integral. The power divergences are real and disappear when the imaginary part is taken. Writing
one obtains
Consequently the late-time parity-odd primordial trispectrum is
Its factor of is required by reality of a momentum-space scalar correlator: reversing all momenta complex-conjugates the correlator, while the scalar triple product changes sign.
Let denote the th elementary symmetric polynomial of . Expanding both sides of the Marsden identity in powers of and equating the coefficient of gives
Thus , while and are respectively the means of the interior knots and of their pairwise products.
Put , let
be the minimal polynomial of an algebraic element over , and let be the integral closure of in a finite normal extension containing all roots of . Since is integral over and is integrally closed domain, every belongs to .
Write with and . Every -embedding into the normal extension fixes the and sends each to an element integral over . Thus every conjugate of lies in the extended ideal . Each nonleading coefficient of is, up to sign, an elementary symmetric polynomial in those conjugates, so it lies in .
For an integral extension, extension followed by contraction preserves a prime ideal:
Indeed, the determinant trick gives for , and primality then gives . Hence for every .
The discriminant is a symmetric polynomial in the four roots, so the Fundamental theorem of symmetric polynomials expresses it polynomially in the elementary symmetric polynomial. For this depressed quartic they are , , . Scaling each root by multiplies the discriminant by , while scale by . Thus only weighted-degree-twelve monomials can appear, giving .
For , use and the monic discriminant identity . At this gives , so . For , the roots are zero together with those of . The cubic's discriminant is . The extra squared differences from zero multiply this by , giving . Hence
These computations are polynomial identities, so they extend to parameter values with repeated roots as well.
Realize the standard representation of the symmetric group on . The symmetric power sums , for , freely generate its polynomial invariant ring. To justify the description, average any polynomial lift from to over the symmetric group; the resulting symmetric lift is a polynomial in the elementary symmetric polynomials , and restriction sets . The remaining three generators are algebraically independent. The Newton identities express them equivalently through over the complex numbers. In coordinates , one has and .
For the polynomial , the root list is , not . Its elementary symmetric polynomials are
The zero coefficient of is accounted for by the cancellation in . Omitting one occurrence of the double root of a polynomial loses both the polynomial degree and the correct coefficients. Multiplicity of a root is part of the root data.
For the block-rotation maximal torus in the special orthogonal group , the Weyl group acts by permutations and independent inversions of . Its invariant Laurent polynomials are the symmetric polynomials in , hence the polynomial ring in their elementary symmetric polynomials . Restriction of the group representation ring of a compact group is injective because every group element is conjugate into the torus and characters distinguish virtual representations. For the defining complexified representation , the exterior-power characters satisfy . For , its coefficient is plus an integral linear combination of for . Induction puts every in the restriction image, proving equality with the invariant ring and giving polynomial generators .
On in characteristic of a field other than two, take the elementary symmetric polynomials of . If the line through is , its third intersection is , so coefficient comparison gives , , . Hence . This is an identity of rational functions; tangent cases follow by specialization, and coordinates at infinity are handled through the projective addition map.
Take the stipulated polynomial roots . Their first three elementary symmetric polynomials are
Their monic polynomial is therefore
The constant coefficient is , while the product of the three roots of a polynomial is : for a cubic polynomial, these have opposite signs. Expanding the factors directly verifies the same polynomial identity.
Figure 1.
The roots determine the signed coefficients of a cubic
. An original exact calculation: the graph shows the stipulated polynomial, and the ledger groups choices of one, two or three root positions into elementary symmetric polynomials. The alternating factors convert these values into monic polynomial coefficients. Details.
For the nonmonic polynomial , the same ratios give sum , pairwise-product sum , and product . It is times the monic polynomial above, so its roots of a polynomial are the same. Checking only the sum and product would leave the middle elementary symmetric polynomial unchecked; all three are needed to recover a monic polynomial of polynomial degree three.
Vieta's formulas Created 2026-10-18 Updated 2026-10-20
Vieta's formulas connect two descriptions of a polynomial: its coefficients and its roots of a polynomial. They let us read the sum and product of the roots of a polynomial without finding the individual roots of a polynomial, and turn a proposed factorization of polynomials into checkable coefficient identities. The key is that coefficients encode elementary symmetric polynomials, which are unchanged by a permutation of the roots of a polynomial.
For a polynomial of polynomial degree , with nonzero leading coefficient , write its factorization of polynomials in a splitting field as
List every root of a polynomial according to its multiplicity of a root. Then
In particular, and . With coefficients in the real numbers or complex numbers, the fundamental theorem of algebra ensures that a list of roots of a polynomial in the complex numbers exists when multiplicity of a root is counted.[ref]
For a monic polynomial, this is the familiar convention
where is the th elementary symmetric polynomial in the roots of a polynomial; in particular, . The ratio by in the general statement matters: multiplying every coefficient by the same nonzero scalar preserves both the roots of a polynomial and these ratios.
A short derivation explains every alternating sign. In the product , a term of polynomial degree arises by choosing from distinct factor positions and from the others. Summing the resulting products gives . Values at different positions may coincide: the selection is of positions, not distinct root values. Matching coefficients gives the formula. This is the distributive property organized by the number of chosen root factors.