diff --git a/docs/usage/dynamics/analytic-continuation.ipynb b/docs/usage/dynamics/analytic-continuation.ipynb
index 7151ad7dd..1a82cfe01 100644
--- a/docs/usage/dynamics/analytic-continuation.ipynb
+++ b/docs/usage/dynamics/analytic-continuation.ipynb
@@ -357,7 +357,7 @@
     "np_rho_cm = sp.lambdify((m, m_a, m_b), rho_cm.doit())\n",
     "np_breakup_momentum = sp.lambdify(\n",
     "    (m, m_a, m_b),\n",
-    "    ComplexSqrt(q_squared.subs(s, m**2).doit()) / (8 * sp.pi),\n",
+    "    2 * ComplexSqrt(q_squared.subs(s, m**2).doit()),\n",
     ")"
    ]
   },
@@ -417,7 +417,7 @@
     "for ax in [ax_rho_cm, ax_rho_ac]:\n",
     "    ax.set_yticks([])\n",
     "\n",
-    "ylim = (-0.002, 0.03)\n",
+    "ylim = (-0.1, 1.4)\n",
     "\n",
     "\n",
     "def func_imag(func, *args, **kwargs):\n",
@@ -547,8 +547,16 @@
    "name": "python3"
   },
   "language_info": {
+   "codemirror_mode": {
+    "name": "ipython",
+    "version": 3
+   },
+   "file_extension": ".py",
+   "mimetype": "text/x-python",
    "name": "python",
-   "version": "3.8.17"
+   "nbconvert_exporter": "python",
+   "pygments_lexer": "ipython3",
+   "version": "3.11.8"
   }
  },
  "nbformat": 4,
diff --git a/src/ampform/dynamics/phasespace.py b/src/ampform/dynamics/phasespace.py
index 1e5902b31..75a424a5d 100644
--- a/src/ampform/dynamics/phasespace.py
+++ b/src/ampform/dynamics/phasespace.py
@@ -92,9 +92,10 @@ def _latex_repr_(self, printer: LatexPrinter, *args) -> str:
 
 @unevaluated
 class PhaseSpaceFactor(sp.Expr):
-    """Standard phase-space factor, using :func:`BreakupMomentumSquared`.
+    r"""Standard phase-space factor, using :func:`BreakupMomentumSquared`.
 
-    See :pdg-review:`2021; Resonances; p.6`, Equation (50.9).
+    See :pdg-review:`2021; Resonances; p.6`, Equation (50.9). We ignore the factor
+    :math:`\frac{1}{16\pi}` as done in :cite:`chungPrimerKmatrixFormalism1995`, p.5.
     """
 
     s: Any
@@ -105,8 +106,7 @@ class PhaseSpaceFactor(sp.Expr):
     def evaluate(self) -> sp.Expr:
         s, m1, m2 = self.args
         q_squared = BreakupMomentumSquared(s, m1, m2)
-        denominator = _phase_space_factor_denominator(s)
-        return sp.sqrt(q_squared) / denominator
+        return 2 * sp.sqrt(q_squared) / sp.sqrt(s)
 
     def _latex_repr_(self, printer: LatexPrinter, *args) -> str:
         s_symbol = self.args[0]
@@ -136,8 +136,7 @@ class PhaseSpaceFactorAbs(sp.Expr):
     def evaluate(self) -> sp.Expr:
         s, m1, m2 = self.args
         q_squared = BreakupMomentumSquared(s, m1, m2)
-        denominator = _phase_space_factor_denominator(s)
-        return sp.sqrt(sp.Abs(q_squared)) / denominator
+        return 2 * sp.sqrt(sp.Abs(q_squared)) / sp.sqrt(s)
 
     def _latex_repr_(self, printer: LatexPrinter, *args) -> str:
         s_symbol = self.args[0]
@@ -163,8 +162,7 @@ class PhaseSpaceFactorComplex(sp.Expr):
     def evaluate(self) -> sp.Expr:
         s, m1, m2 = self.args
         q_squared = BreakupMomentumSquared(s, m1, m2)
-        denominator = _phase_space_factor_denominator(s)
-        return ComplexSqrt(q_squared) / denominator
+        return 2 * ComplexSqrt(q_squared) / sp.sqrt(s)
 
     def _latex_repr_(self, printer: LatexPrinter, *args) -> str:
         s_symbol = self.args[0]
@@ -212,7 +210,7 @@ def chew_mandelstam_s_wave(s, m1, m2):
     right_term = (m1**2 - m2**2) * (1 / s - 1 / (m1 + m2) ** 2) * sp.log(m1 / m2)
     # evaluate=False in order to keep same style as PDG
     return sp.Mul(
-        1 / (16 * sp.pi**2),
+        1 / sp.pi,
         left_term - right_term,
         evaluate=False,
     )
@@ -265,10 +263,6 @@ def _analytic_continuation(rho, s, s_threshold) -> sp.Piecewise:
     )
 
 
-def _phase_space_factor_denominator(s) -> sp.Mul:
-    return 8 * sp.pi * sp.sqrt(s)
-
-
 def _indices_to_subscript(indices: Sequence[int]) -> str:
     """Create a LaTeX subscript from a list of indices.