Skip to content

Commit 6e8ad05

Browse files
committed
[AR1] Update editorial suggestions
1 parent 8d0822f commit 6e8ad05

File tree

2 files changed

+19
-12
lines changed

2 files changed

+19
-12
lines changed

lectures/ar1_processes.md

Lines changed: 18 additions & 12 deletions
Original file line numberDiff line numberDiff line change
@@ -19,7 +19,7 @@ kernelspec:
1919
```
2020

2121
(ar1_processes)=
22-
# AR1 Processes
22+
# AR(1) Processes
2323

2424
```{admonition} Migrated lecture
2525
:class: warning
@@ -44,7 +44,7 @@ These simple models are used again and again in economic research to represent t
4444
AR(1) processes can take negative values but are easily converted into positive processes when necessary by a transformation such as exponentiation.
4545

4646
We are going to study AR(1) processes partly because they are useful and
47-
partly because they help us understand important concepts.
47+
partly because they help us understand important concepts. Specifically, AR(1) processes are valuable as they can measure the persistence of shocks over time.
4848

4949
Let's start with some imports:
5050

@@ -54,7 +54,7 @@ import matplotlib.pyplot as plt
5454
plt.rcParams["figure.figsize"] = (11, 5) #set default figure size
5555
```
5656

57-
## The AR(1) Model
57+
## The AR(1) model
5858

5959
The **AR(1) model** (autoregressive model of order 1) takes the form
6060

@@ -73,11 +73,11 @@ This is called the **state process** and the state space is $\mathbb R$.
7373

7474
To make things even simpler, we will assume that
7575

76-
* the process $\{ W_t \}$ is IID and standard normal,
76+
* the process $\{ W_t \}$ is {ref}`IID <iid-theorem>` and standard normal,
7777
* the initial condition $X_0$ is drawn from the normal distribution $N(\mu_0, v_0)$ and
7878
* the initial condition $X_0$ is independent of $\{ W_t \}$.
7979

80-
### Moving Average Representation
80+
### Moving average representation
8181

8282
Iterating backwards from time $t$, we obtain
8383

@@ -105,7 +105,7 @@ Equation {eq}`ar1_ma` shows that $X_t$ is a well defined random variable, the va
105105
Throughout, the symbol $\psi_t$ will be used to refer to the
106106
density of this random variable $X_t$.
107107

108-
### Distribution Dynamics
108+
### Distribution dynamics
109109

110110
One of the nice things about this model is that it's so easy to trace out the sequence of distributions $\{ \psi_t \}$ corresponding to the time
111111
series $\{ X_t\}$.
@@ -116,7 +116,7 @@ This is immediate from {eq}`ar1_ma`, since linear combinations of independent
116116
normal random variables are normal.
117117

118118
Given that $X_t$ is normally distributed, we will know the full distribution
119-
$\psi_t$ if we can pin down its first two moments.
119+
$\psi_t$ if we can pin down its first two [moments](https://en.wikipedia.org/wiki/Moment_(mathematics)).
120120

121121
Let $\mu_t$ and $v_t$ denote the mean and variance
122122
of $X_t$ respectively.
@@ -179,7 +179,9 @@ ax.legend(bbox_to_anchor=[1.05,1],loc=2,borderaxespad=1)
179179
plt.show()
180180
```
181181

182-
## Stationarity and Asymptotic Stability
182+
## Stationarity and asymptotic stability
183+
184+
In Distribution Dynamics, stationarity and asymptotic stability ensure that a single long-term prediction remains valid over time.
183185

184186
Notice that, in the figure above, the sequence $\{ \psi_t \}$ seems to be converging to a limiting distribution.
185187

@@ -254,7 +256,7 @@ plt.show()
254256

255257
As claimed, the sequence $\{ \psi_t \}$ converges to $\psi^*$.
256258

257-
### Stationary Distributions
259+
### Stationary distributions
258260

259261
A stationary distribution is a distribution that is a fixed
260262
point of the update rule for distributions.
@@ -285,8 +287,8 @@ Thus, when $|a| < 1$, the AR(1) model has exactly one stationary density and tha
285287

286288
The concept of ergodicity is used in different ways by different authors.
287289

288-
One way to understand it in the present setting is that a version of the Law
289-
of Large Numbers is valid for $\{X_t\}$, even though it is not IID.
290+
One way to understand it in the present setting is that a version of the law
291+
of large numbers is valid for $\{X_t\}$, even though it is not IID.
290292

291293
In particular, averages over time series converge to expectations under the
292294
stationary distribution.
@@ -319,6 +321,10 @@ $$
319321
In other words, the time series sample mean converges to the mean of the
320322
stationary distribution.
321323

324+
In reality, if an economy is ergodic, its long-term average growth rate is stable. For example, observing an economy's behavior over time can give a reliable estimate of its long-term growth potential.
325+
326+
However, ergodicity fails when persistent shocks or structural changes affect growth dynamics, making past observations unreliable for predicting future growth.
327+
322328
As will become clear over the next few lectures, ergodicity is a very
323329
important concept for statistics and simulation.
324330

@@ -345,7 +351,7 @@ M_k =
345351
\end{cases}
346352
$$
347353
348-
Here $n!!$ is the double factorial.
354+
Here $n!!$ is the [double factorial](https://en.wikipedia.org/wiki/Double_factorial).
349355
350356
According to {eq}`ar1_ergo`, we should have, for any $k \in \mathbb N$,
351357

lectures/lln_clt.md

Lines changed: 1 addition & 0 deletions
Original file line numberDiff line numberDiff line change
@@ -167,6 +167,7 @@ $$
167167

168168
The next theorem is called Kolmogorov's strong law of large numbers.
169169

170+
(iid-theorem)=
170171
````{prf:theorem}
171172
If $X_1, \ldots, X_n$ are IID and $\mathbb E |X|$ is finite, then
172173

0 commit comments

Comments
 (0)