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The Hasse-Minkowski theorem says that a nondegenerate quadratic form over a number field has a nonzero isotropic vector over that field if and only if it has one over every completion. In particular, over $\mathbb{Q}$ one tests $\mathbb{R}$ and every ${\mathbb{Q}}_{\ell }$. For the present integral form, a rational isotropic vector can be multiplied by a common denominator to give an integer one. This is the Hasse-Minkowski principle.

Write $P=p$, $R=p+12$ and $S=p+24$. All three primes are odd and exceed three: $p=2$ or $3$ would make $p+12$ composite. The second supplementary law for quadratic reciprocity gives

Necessity at $P$. Scale any nonzero vector over ${\mathbb{Q}}_P$ so that its coordinates lie in ${\mathbb{Z}}_P$ and at least one is a unit. Reduction of its equation modulo $P$ gives $y^2=2z^2$, since twelve is invertible modulo $P$. If the Legendre symbol $(2/P)$ is $-1$, this forces $P\mid y,z$. The original equation then forces $P\mid x$, because its other two terms are divisible by $P^2$. This contradicts the normalization. Thus

Sufficiency at the coefficient primes. Suppose $(2/P)=1$. A nonzero solution modulo $P$ is $(x,y,z)=(0,\sqrt{2},1)$. Its $y$-derivative is nonzero modulo $P$, so fixing the other two coordinates and applying the Hensel lemma lifts it to ${\mathbb{Q}}_P$.

Since $S\equiv P(\mathrm{mod}8)$, the same Legendre symbol criterion gives $(2/S)=1$. Modulo $S$, the equation reduces to $y^2=2x^2$, and the vector $(1,\sqrt{2},0)$ is a simple zero in the $y$ coordinate. It lifts to ${\mathbb{Q}}_S$. Modulo $R$, the coefficients of $x^2$ and $z^2$ are respectively $-12$ and $12$, so $(1,0,1)$ is a zero with nonzero $x$-derivative. It lifts to ${\mathbb{Q}}_R$.

The remaining odd primes. If $\ell$ is odd and divides none of $PRS$, the reduced ternary quadratic form is nondegenerate. An elementary finite-field argument finds a zero with $z=1$: if its coefficients are $A,B,C$, the setsboth have $(\ell +1)/2$ elements, so intersect. The resulting vector has nonzero $z$-derivative $2C$, and the Hensel lemma lifts it. This isotropy of nondegenerate ternary quadratic forms over finite fields verifies every remaining odd completion without an extra congruence condition.

The dyadic and real places. Setting $y=1,z=2$ reduces the dyadic problem toThe right side is a 2-adic unit congruent to $-3-4=1$ modulo eight. The unit square classes of the p-adic integers computed above show that it is a square in ${\mathbb{Q}}_2$. This also explains the printed hint: its integer can be taken as $m=-(p+21)/2$. Over $\mathbb{R}$, the positive and negative coefficients make the form indefinite; for instance $x=0,z=1,y=\sqrt{S/R}$ gives a nonzero zero.

All completions now have a nonzero isotropic vector. The Hasse-Minkowski theorem, followed by clearing denominators, proves

For an odd prime $p$, the Legendre symbol isEuler criterion states that

The Gauss lemma says that, for $p\nmid a$, if $m$ of the least positive residues oflie in $(p/2,p)$, thenTo prove it, replace every residue above $p/2$ by its negative. The resulting absolute residues are distinct up to sign and therefore form a permutation ofMultiplying the congruences givesCancel the nonzero factorial and apply Euler's criterion.

For $a=2$, the residues are $2,4,\dots ,p-1$. The number above $p/2$ iswhose parity gives the second supplementary law for quadratic reciprocityConsequently, for odd primes,The congruence is also soluble for $p=2$.

Because $I$ and $A$ commute, the matrix binomial theorem givesFor prime $p$, every intermediate coefficient $\left(\genfrac{}{}{0ex}{}{p}{j}\right)$ is divisible by $p$, proving the prime-power binomial congruence for a matrix

Forone has $(I+A{)}^2=2A$ and $(I+A{)}^4=-4I$. If $p=4k+1$, thenso $(-4{)}^k\equiv 1(\mathrm{mod}p)$. If $p=4k-1$, then $A^p=-A$ andso $(-4{)}^k\equiv 2(\mathrm{mod}p)$.

By Euler criterion, $(\frac{2}{p})\equiv 2^{(p-1)/2}(\mathrm{mod}p)$. In either case the preceding congruence gives $(\frac{2}{p})=(-1{)}^k$. Since $(p^2-1)/8$ has the same parity as $k$ for $p=4k\pm 1$, this is the second supplementary law for quadratic reciprocity