diff --git a/lectures/scalar_dynam.md b/lectures/scalar_dynam.md
index 486ea954..2c0bdaed 100644
--- a/lectures/scalar_dynam.md
+++ b/lectures/scalar_dynam.md
@@ -235,6 +235,7 @@ Analyzing the dynamics of this model requires a different method (see below).
 Consider a fixed dynamic system consisting of set $S \subset \mathbb R$ and
 $g$ mapping $S$ to $S$.
 
+(scalar-dynam:steady-state)=
 ### Steady states
 
 A **steady state** of this system is a
@@ -254,6 +255,7 @@ definition to check that
 
 
 
+(scalar-dynam:global-stability)=
 ### Global stability
 
 A steady state $x^*$ of the dynamic system is called
diff --git a/lectures/solow.md b/lectures/solow.md
index ff2efdbd..484f7664 100644
--- a/lectures/solow.md
+++ b/lectures/solow.md
@@ -100,8 +100,7 @@ given an exogenous initial capital stock  $k_0$.
 
 ## A graphical perspective
 
-To understand the dynamics of the sequence $(k_t)_{t \geq 0}$ we use a 45
-degree diagram.
+To understand the dynamics of the sequence $(k_t)_{t \geq 0}$ we use a 45-degree diagram.
 
 To do so, we first
 need to specify the functional form for $f$ and assign values to the parameters.
@@ -109,8 +108,7 @@ need to specify the functional form for $f$ and assign values to the parameters.
 We choose the Cobb--Douglas specification $f(k) = A k^\alpha$ and set $A=2.0$,
 $\alpha=0.3$, $s=0.3$ and $\delta=0.4$.
 
-The function $g$ from {eq}`solow` is then plotted, along with the 45
-degree line.
+The function $g$ from {eq}`solow` is then plotted, along with the 45-degree line.
 
 
 Let's define the constants.
@@ -128,7 +126,7 @@ def g(A, s, alpha, delta, k):
     return A * s * k**alpha + (1 - delta) * k
 ```
 
-Let's plot the 45 degree diagram of $g$.
+Let's plot the 45-degree diagram of $g$.
 
 ```{code-cell} ipython3
 def plot45(kstar=None):
@@ -145,7 +143,7 @@ def plot45(kstar=None):
 
     lb = r'$g(k) = sAk^{\alpha} + (1 - \delta)k$'
     ax.plot(xgrid, g_values,  lw=2, alpha=0.6, label=lb)
-    ax.plot(xgrid, xgrid, 'k-', lw=1, alpha=0.7, label='45')
+    ax.plot(xgrid, xgrid, 'k-', lw=1, alpha=0.7, label='$45^{\circ}$')
 
     if kstar:
         fps = (kstar,)
@@ -175,7 +173,7 @@ def plot45(kstar=None):
 plot45()
 ```
 
-Suppose, at some $k_t$, the value $g(k_t)$ lies strictly above the 45 degree line.
+Suppose, at some $k_t$, the value $g(k_t)$ lies strictly above the 45-degree line.
 
 Then we have $k_{t+1} = g(k_t) > k_t$ and capital per worker rises.
 
@@ -183,7 +181,7 @@ If $g(k_t) < k_t$ then capital per worker falls.
 
 If $g(k_t) = k_t$, then we are at a **steady state** and $k_t$ remains constant.
 
-(A steady state of the model is a [fixed point](https://en.wikipedia.org/wiki/Fixed_point_(mathematics)) of the mapping $g$.)
+(A {ref}`steady state <scalar-dynam:steady-state>` of the model is a [fixed point](https://en.wikipedia.org/wiki/Fixed_point_(mathematics)) of the mapping $g$.)
 
 From the shape of the function $g$ in the figure, we see that
 there is a unique steady state in $(0, \infty)$.
@@ -198,7 +196,7 @@ If initial capital is below $k^*$, then capital increases over time.
 
 If initial capital is above this level, then the reverse is true.
 
-Let's plot the 45 degree diagram to show the $k^*$ in the plot.
+Let's plot the 45-degree diagram to show the $k^*$ in the plot.
 
 ```{code-cell} ipython3
 kstar = ((s * A) / delta)**(1/(1 - alpha))
@@ -209,7 +207,7 @@ plot45(kstar)
 From our graphical analysis, it appears that $(k_t)$ converges to $k^*$, regardless of initial capital
 $k_0$.
 
-This is a form of global stability.
+This is a form of {ref}`global stability <scalar-dynam:global-stability>`.
 
 
 The next figure shows three time paths for capital, from
@@ -387,7 +385,7 @@ linear differential equation
     x'_t = (1-\alpha) (sA - \delta x_t)
 ```
 
-This equation has the exact solution
+This equation, which is a [linear ordinary differential equation](https://math.libretexts.org/Bookshelves/Calculus/Calculus_(Guichard)/17%3A_Differential_Equations/17.01%3A_First_Order_Differential_Equations), has the solution
 
 $$
     x_t