The simple continued fraction algorithm for begins with . Its complete quotients repeat after
Thus
The convergents through one period are
The last one gives the negative Pell equation solution
Therefore
The Mackey restriction formula says, for an -representation ,
Frobenius reciprocity says
Applying both with an irreducible character gives
The identity double coset contributes one, and all terms are nonnegative integers. Therefore Mackey irreducibility criterion says that is irreducible exactly when every term belonging to a nonidentity double coset is zero.
Now take . Write
so . For , commutators of with generate , because conjugation sends to and one can choose . Every degree-one character of is therefore trivial on and has the form
where is a multiplicative character.
The Bruhat decomposition of SL2 over a finite field has two double cosets,
and . Conjugation by inverts , so
The only nonidentity Mackey term vanishes exactly when these two one-dimensional characters differ. Consequently
Thus the trivial character is excluded, as is the unique quadratic character when is odd. All other degree-one characters of induce irreducibly; the induced representations have degree . This is the irreducible principal series of finite SL2.
In the Erdős-Rényi model , the vertex set is and every one of the possible edges is present independently with probability .
Let count isolated vertices. If , the union bound gives
Thus .
Chebyshev inequality states that
Now suppose . Monotonicity lets us use the largest allowed . With
the supplied lower exponential estimate shows
For distinct vertices ,
Hence
and
Chebyshev with gives , so .
For connectivity, the lower-threshold result is immediate because a connected graph has no isolated vertex:
For the upper threshold, if a graph is disconnected it has a component with vertex set of some size . In particular, every one of the edges from to its complement is absent. Therefore
Choose
For , the standard bound gives
The sum of these terms tends to zero. For , use and :
Thus above the threshold. Together,
This is the connectivity threshold in the Erdős-Rényi model.
The gravitational three-body Lagrangian is
Put and . Solving the definitions of the Jacobi coordinates for three particles gives
Substitution into the kinetic energy makes all cross terms cancel:
where
The pair separations are
Hence the gravitational potential energy is
which is independent of . Thus is an ignorable coordinate and
The center of mass moves uniformly because the isolated system has no external force.
Finally, substituting the inverse coordinate transformation into
again cancels every cross term and yields
This is the angular momentum decomposition in three-body Jacobi coordinates.
This is attenuation bias from classical measurement error, also called regression dilution. The latent predictor is , but and are noisy proxies. The noisier proxy produces a slope closer to zero.
For a regression with an intercept, the population slope is
Here all variables are centred and the noises are independent. Therefore
so regressing on has slope . For
we have
Thus
With the stated values, the slopes are
matching the simulation.
Under this independent additive measurement-error model, the magnitude of the -on- slope is generally smaller than the magnitude of the -on- slope whenever . Increasing does not change the population slope, because response noise contributes neither to nor to . It increases residual variance and the sampling variability of the estimate; with one million observations, doubling it should leave the displayed slope close to while increasing its standard error.

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