ARMA models with a mean. The following are candidate ways to write an ARMA(p,q) model with mean μ. [A1]Yn=μ+ϕ1Yn−1+ϕ2Yn−2+⋯+ϕpYn−p+ϵn+ψ1ϵn−1+⋯+ψqϵn−q[A2]Yn=μ+ϕ1(Yn−1−μ)+ϕ2(Yn−2−μ)+⋯+ϕp(Yn−p−μ)+ϵn+ψ1ϵn−1+⋯+ψqϵn−q[A3]ϕ(B)Yn=ψ(B)ϵnϕ(x)=1−ϕ1x−ϕ2x2−⋯−ϕpxpψ(x)=1+ψ1x+ψ2x2+⋯+ψqxq. Are both [A1] and [A2] reasonable alternative models? Is there a reason to prefer one to the other? Which one matches [A3]?
Two equivalent MA models. Consider the following moving average models, defined in terms of a Gaussian white noise process ϵn∼iidN(0,σ2). [B1]Yn=ϵn+2ϵn−1,σ2=1.[B2]Yn=ϵn+0.5ϵn−1,σ2=4. Why can data never tell us which of [B1] and [B2] is preferable for a particular situation? Is there a practical reason to prefer [B1] or [B2]?
Over-damped AR(2) models. In Chapter 4, we saw
that AR(2) models can describe quasi-periodic oscillatory behavior, with
an autocorrelation function (ACF) that is an exponentially decaying
sinusoid. You could experiment with ARMAacf()
to find
parameter values ϕ1 and ϕ2 for a causal AR(2) model that does
not have a sinusoidal oscillation in its ACF. Instead, the ACF should
decay to zero similar to an AR(1) model. Can you say anything about the
class of all AR(2) models that do not have any oscillatory behavior? In
other words, can you find a mathematical expression for the set of
values of ϕ1 and ϕ2? One way to address this in the
context of Chapter 4 is to work out when a deterministic skeleton decays
with no oscillations. In physics and engineering, this is called an
over-damped system.