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Put $m=\left(\genfrac{}{}{0ex}{}{k}{2}\right)$, take odd $q\equiv 1(\mathrm{mod}2m)$, and let $H$ be the index-$m$ multiplicative subgroup. If a $k$-set $A$ has its unordered pair differences in distinct $H$-cosets, choose $S\subset H$ containing exactly one element from each pair $\{h,-h\}$. Then $\{sA:s\in S\}$ is a difference family for a Steiner 2-design. Indeed one unordered pair supplies each coset, and its two difference orientations multiplied by $S$ cover that coset once. Translations yield a $2$-$(q,k,1)$ Steiner system. The cyclotomic pattern extension by a second-moment bound supplies suitable $A$ for all sufficiently large $q$ in this progression.

Use the pair-design convention: each pair of distinct points must lie in exactly one Steiner block of size $k$. With this convention the printed endpoint $k=1$ is false for every $v\ge 2$, since a singleton contains no pair. Thus the intended assertion requires $k\ge 2$. For $k=2$, take all pairs as Steiner blocks for any $v\ge 2$. We now give a finite-field construction for every fixed $k\ge 3$, without assuming the desired design-existence theorem.

Put $m=\left(\genfrac{}{}{0ex}{}{k}{2}\right)$ and take an odd prime power $q\equiv 1(\mathrm{mod}2m)$. By cyclicity of ${\mathbb{F}}_q^{\times }$, it has a subgroup $H$ of index $m$; its order $(q-1)/m$ is even, so $-1\in H$. We will find a $k$-set $A=\{a_1,\dots ,a_k\}$ such that its $m$ unordered pair differences occupy the $m$ distinct cyclotomic classes of a finite field modulo $H$. The following argument supplies that set for every sufficiently large compatible $q$.

First establish the required two-class intersection estimate by elementary character sums. Let $\chi$ be a multiplicative character of a finite field of order $m$, with $\chi (\gamma )={\zeta }_m$ for a generator $\gamma$. Extend every power ${\chi }^j$, including the trivial character, by zero at zero. For $C_i={\gamma }^{i}H$,For a nontrivial additive character $\psi$ of ${\mathbb{F}}_q$ and a nontrivial multiplicative character $\eta$, its Gauss sum of a finite-field character satisfiesHere the inner sum equals $q-1$ for $t=1$ and $-1$ otherwise, by additive-character orthogonality; multiplicative-character orthogonality gives the last equality. Such a nontrivial additive character exists by identifying the additive group with a vector space over its prime field and choosing a nonzero linear functional into that prime field.

If $\eta ,\xi ,\eta \xi$ are nontrivial, substituting $x=uz$, $y=(1-u)z$ in the product of their Gauss sums provesThe terms with $x+y=0$ sum to zero because $\eta \xi$ is nontrivial. Hence $|J|=\sqrt{q}$. If exactly one character is trivial, subtracting the excluded zero and one terms gives absolute value one. If both are nontrivial but their product is trivial, the substitution $u/(1-u)$ gives $J(\eta ,{\eta }^{-1})=-\eta (-1)$, again of absolute value one. If both are trivial, the sum is $q-2$. Expanding the two cyclotomic indicators and scaling a nonzero translate to one therefore gives, uniformly in $i,j$ and $t\ne 0$,All constants depend only on the fixed $m$.

To extend a prescribed difference pattern on $r$ coordinates, fix desired classes $D_1,\dots ,D_r$ for the new differences $x-a_i$ and setAverage over all $q^r$ tuples, allowing repeated coordinates just for this average. With $f=(q-1)/m$, counting choices for each $a_i$ independently givesFor the second moment, sum over the two potential extensions $x,y$. The $x=y$ terms contribute $q{f}^r/q^r$. For $x\ne y$, the choices of $a_i$ number $q/m^2+O_m(\sqrt{q})$ each, by the preceding intersection estimate. ThusThe Chebyshev inequality shows that the proportion of tuples with $M(a)<q/(2m^r)$ is $O_{m,r}(q^{-1/2})$. Inductively, any fixed compatible difference pattern on $r$ distinct coordinates is realized by at least $c_r{q}^r$ tuples, with $c_r>0$ independent of sufficiently large $q$. The assertion starts with $r=1$. Almost all tuples are outside the exceptional set, so at least half the realizing tuples have at least $q/(2m^r)$ extensions. Each extension is distinct from the old coordinates because its differences belong to nonzero classes. This proves the assertion for $r+1$. This cyclotomic pattern extension by a second-moment bound avoids the false assumption that every partial choice can be extended.

Prescribe a different one of the $m$ cosets to each pair $a_j-a_i$, $i<j$. Since $-1\in H$, changing an orientation does not change its coset, so the prescriptions are compatible. The preceding induction supplies $A$.

Choose $S\subset H$ containing one element from each pair $\{h,-h\}$. Form the Steiner blocksFor two distinct points $x,y$, their difference identifies exactly one unordered pair $\{a_i,a_j\}$ of $A$ having the same $H$-coset. Exactly one of $(x-y)/(a_i-a_j)$ and its negative lies in $S$. Choose the orientation $a,b$ of that pair making $s=(x-y)/(a-b)\in S$, and then set $t=x-sa$. This yields $x=sa+t$, $y=sb+t$. Both the oriented base pair and $(s,t)$ are unique, so precisely one Steiner block contains the pair. In particular different Steiner block parameters cannot produce repeated Steiner blocks. Equivalently, the Steiner blocks $sA$ form a difference family for a Steiner 2-design, and translation gives the cyclotomic construction of a Steiner 2-design.

There are infinitely many suitable field orders: choose one odd prime $\ell$ not dividing $2m$, and take $q={\ell }^{\phi (2m)u}$ for integers $u\ge 1$. Euler's congruence gives $q\equiv 1(\mathrm{mod}2m)$, and these orders become arbitrarily large. ConsequentlyThe qualification at $k=1$ is necessary for the standard pair-design definition.