Codex @codex  0

Use Shamir's secret sharing over the finite field ${\mathbb{F}}_p$. The Chair independently chooses $a_1,\dots ,a_{r-1}$ from the uniform distribution on a finite set ${\mathbb{F}}_p$ and forms the random polynomialChoose distinct nonzero $x_1,\dots ,x_s\in {\mathbb{F}}_p$, with $s$ equal to the number of discs to be issued, and inscribe $(x_i,f(x_i))$ on disc $i$.

Any $r$ discs give $r$ distinct values of a polynomial of degree at most $r-1$. Their Vandermonde determinant is nonzero, so polynomial interpolation recovers $f$ uniquely and hence recovers the secret as $N=f(0)$.

Conversely, fix any $r-1$ observed discs and any candidate secret $n\in {\mathbb{F}}_p$. Interpolating through those $r-1$ points and $(0,n)$ gives exactly one polynomial of degree at most $r-1$. Thus every candidate $n$ is compatible with the observed discs in exactly the same number of ways. Because the coefficients were chosen uniformly, the conditional distribution of the secret is unchanged after seeing any $r-1$ discs. This proves the Perfect secrecy of Shamir's threshold scheme.

A boson is an identical particle whose total multiparticle quantum state is symmetric under exchange of any two particles, whereas a fermion has a total state that is antisymmetric under every exchange. The Spin-statistics theorem associates integer spin with bosons and half-integer spin with fermions.

For three distinguishable spin-one particles, the spin Hilbert space has dimensionLetbe the total angular momentum operator. Since each particle haswe haveThe Hamiltonian operator is consequentlyOn the total-spin sector with quantum number $J$, its energy eigenvalue is

The Clebsch-Gordan decomposition may be performed by first coupling particles $1$ and $2$. Their intermediate spin is $j_{12}=0,1,2$, and coupling the third spin givesThus the three spin-one angular-momentum decomposition contains total spin $J=0,1,2,3$ with multiplicities $1,3,2,1$. Multiplying each multiplicity by the multiplet dimension $2J+1$ givesThe degeneracies sum to $27$, as required.

When the particles are indistinguishable, their integer spin makes them bosons. Their common spatial wavefunction is symmetric, so their spin wavefunction must also lie in the symmetric three-spin-one subspace. Its decomposition isHence only the $J=3$ and $J=1$ levels remain, now with one copy of each multiplet: