diff --git a/doc/src/pair_ylz.rst b/doc/src/pair_ylz.rst
index 744a868cb6..cb59385579 100644
--- a/doc/src/pair_ylz.rst
+++ b/doc/src/pair_ylz.rst
@@ -27,47 +27,58 @@ Description
 
 .. versionadded:: TBD
 
-The *ylz* (Yuan-Li-Zhang) style computes an anisotropic interaction between pairs of 
-coarse-grained particles considering the relative particle orientations. This potential
-was originally developed as a particle-based solvent-free model for biological membranes
-:ref:`(Yuan2010a) <Yuan>`. Unlike the :doc:`pair_style gayberne <pair_gayberne>` whose 
-orientation dependence is strictly derived from the closest distance between two 
-ellipsoidal rigid bodies, the orientation-dependence of this pair style is mathematically
-defined such that the particles can self-assemble into one-particle-thick 
-fluid membranes. The potential of this pair style is described via the formulas
+The *ylz* (Yuan-Li-Zhang) style computes an anisotropic interaction
+between pairs of coarse-grained particles considering the relative
+particle orientations. This potential was originally developed as a
+particle-based solvent-free model for biological membranes
+:ref:`(Yuan2010a) <Yuan>`.  Unlike :doc:`pair_style gayberne
+<pair_gayberne>`, whose orientation dependence is strictly derived from
+the closest distance between two ellipsoidal rigid bodies, the
+orientation-dependence of this pair style is mathematically defined such
+that the particles can self-assemble into one-particle-thick fluid
+membranes.  The potential of this pair style is described by:
 
 .. math::
 
    U ( \mathbf{r}_{ij}, \mathbf{n}_i, \mathbf{n}_j ) =\left\{\begin{matrix} {u}_R(r)+\left [ 1-\phi (\mathbf{\hat{r}}_{ij}, \mathbf{n}_i, \mathbf{n}_j ) \right ]\epsilon, ~~ r<{r}_{min} \\ {u}_A(r)\phi (\mathbf{\hat{r}}_{ij}, \mathbf{n}_i, \mathbf{n}_j ),~~  {r}_{min}<r<{r}_{c} \\ \end{matrix}\right.\\\\ \phi (\mathbf{\hat{r}}_{ij}, \mathbf{n}_i, \mathbf{n}_j )=1+\left [  \mu (a(\mathbf{\hat{r}}_{ij}, \mathbf{n}_i, \mathbf{n}_j )-1) \right ] \\\\a(\mathbf{\hat{r}}_{ij}, \mathbf{n}_i, \mathbf{n}_j )=(\mathbf{n}_i\times\mathbf{\hat{r}}_{ij} )\cdot (\mathbf{n}_j\times\mathbf{\hat{r}}_{ij} )+{\beta}(\mathbf{n}_i-\mathbf{n}_j)\cdot \mathbf{\hat{r}}_{ij}-\beta^{2}\\\\  {u}_R(r)=\epsilon \left [ \left ( \frac{{r}_{min}}{r} \right )^{4}-2\left ( \frac{{r}_{min}}{r}\right )^{2} \right ] \\\\ {u}_A(r)=-\epsilon\;cos^{2\zeta }\left [ \frac{\pi}{2}\frac{\left ( {r}-{r}_{min} \right )}{\left ( {r}_{c}-{r}_{min} \right )} \right ]\\
 
-where :math:`\mathbf{r}_{i}` and :math:`\mathbf{r}_{j}` are the center position vectors
-of particles i and j, respectively, :math:`\mathbf{r}_{ij}=\mathbf{r}_{i}-\mathbf{r}_{j}` 
-is the inter-particle distance vector, :math:`r=\left|\mathbf{r}_{ij} \right|` and 
-:math:`{\hat{\mathbf{r}}}_{ij}=\mathbf{r}_{ij}/r`. The unit vectors :math:`\mathbf{n}_{i}` 
-and :math:`\mathbf{n}_{j}` represent the axes of symmetry of particles i and j, respectively,
-:math:`u_R` and :math:`u_A` are the repulsive and attractive potentials, :math:`\phi` is an
-angular function which depends on the relative orientation between pair particles, :math:`\mu` 
-is the parameter related to the bending rigidity of the membrane, :math:`\beta` is the parameter 
-related to the spontaneous curvature, and :math:`\epsilon` is the energy unit, respectively. 
-The :math:`\zeta` controls the slope of the attractive branch and hence the diffusivity of the 
-particles in the in-plane direction of the membrane. :math:`{r}_{c}` is the cutoff radius, 
-:math:`r_{min}` is the distance which minimizes the potential energy :math:`u_{A}(r)` and 
-:math:`r_{min}=2^{1/6}\sigma`, where :math:`\sigma` is the length unit.
+where :math:`\mathbf{r}_{i}` and :math:`\mathbf{r}_{j}` are the center
+position vectors of particles i and j, respectively,
+:math:`\mathbf{r}_{ij}=\mathbf{r}_{i}-\mathbf{r}_{j}` is the
+inter-particle distance vector, :math:`r=\left|\mathbf{r}_{ij} \right|`
+and :math:`{\hat{\mathbf{r}}}_{ij}=\mathbf{r}_{ij}/r`.  The unit vectors
+:math:`\mathbf{n}_{i}` and :math:`\mathbf{n}_{j}` represent the axes of
+symmetry of particles i and j, respectively, :math:`u_R` and :math:`u_A`
+are the repulsive and attractive potentials, :math:`\phi` is an angular
+function which depends on the relative orientation between pair
+particles, :math:`\mu` is the parameter related to the bending rigidity
+of the membrane, :math:`\beta` is the parameter related to the
+spontaneous curvature, and :math:`\epsilon` is the energy unit,
+respectively.   The :math:`\zeta` controls the slope of the attractive
+branch and hence the diffusivity of the particles in the in-plane
+direction of the membrane.  :math:`{r}_{c}` is the cutoff radius,
+:math:`r_{min}` is the distance which minimizes the potential energy
+:math:`u_{A}(r)` and :math:`r_{min}=2^{1/6}\sigma`, where :math:`\sigma`
+is the length unit.
 
-This pair style is suited for solvent-free coarse-grained simulations of biological systems 
-involving lipid bilayer membranes, such as vesicle shape transformations :ref:`(Yuan2010b) <Yuan>`,
-nanoparticle endocytosis :ref:`(Huang) <Huang>`, modeling of red blood cell membranes :ref:`(Fu) <Fu>`,
-:ref:`(Appshaw) <Appshaw>`, and modeling of cell elasticity :ref:`(Becton) <Becton>`.
+This pair style is suited for solvent-free coarse-grained simulations of
+biological systems involving lipid bilayer membranes, such as vesicle
+shape transformations :ref:`(Yuan2010b) <Yuan>`, nanoparticle
+endocytosis :ref:`(Huang) <Huang>`, modeling of red blood cell membranes
+:ref:`(Fu) <Fu>`, :ref:`(Appshaw) <Appshaw>`, and modeling of cell
+elasticity :ref:`(Becton) <Becton>`.
 
-Use of this pair style requires the NVE, NVT, or NPT fixes with the *asphere* extension 
-(e.g. :doc:`fix nve/asphere <fix_nve_asphere>`) in order to integrate particle rotation. 
-Additionally, :doc:`atom_style ellipsoid <atom_style>` should be used since it defines 
-the rotational state of each particle.
+Use of this pair style requires the NVE, NVT, or NPT fixes with the
+*asphere* extension (e.g. :doc:`fix nve/asphere <fix_nve_asphere>`) in
+order to integrate particle rotation.  Additionally, :doc:`atom_style
+ellipsoid <atom_style>` should be used since it defines the rotational
+state of each particle.
 
-The following coefficients must be defined for each pair of atoms types via the 
-:doc:`pair_coeff <pair_coeff>` command as in the examples above, or in the data file 
-or restart files read by the :doc:`read_data <read_data>` or 
-:doc:`read_restart <read_restart>` commands, or by mixing as described below:
+The following coefficients must be defined for each pair of atoms types
+via the :doc:`pair_coeff <pair_coeff>` command as in the examples above,
+or in the data file or restart files read by the :doc:`read_data
+<read_data>` or :doc:`read_restart <read_restart>` commands, or by
+mixing as described below:
 
 * :math:`\epsilon` = well depth (energy units)
 * :math:`\sigma` = minimum effective particle radii (distance units)
@@ -112,16 +123,17 @@ The *ylz* style is part of the ASPHERE package.  It is only enabled if
 LAMMPS was built with that package.  See the :doc:`Build package
 <Build_package>` page for more info.
 
-This pair style requires that atoms store torque and a quaternion to represent
-their orientation, as defined by the :doc:`atom_style <atom_style>`. It also 
-requires they store a per-atom :doc:`shape <set>`. The particles cannot store 
-a per-particle diameter. To avoid being mistakenly considered as point masses,
-the shape parameters ought to be non-spherical, like [1  0.99  0.99]. Unlike 
-the :doc:`pair_style gayberne <pair_resquared>` pair style for which the shape 
-directly determines the mathematical expressions of the potential, the shape 
-parameters for this pair style is only involved in the computation of the 
-moment of inertia and thus only play a role to the rotational dynamics of 
-individual particles.
+This pair style requires that atoms store torque and a quaternion to
+represent their orientation, as defined by the :doc:`atom_style
+<atom_style>`.  It also requires they store a per-atom :doc:`shape
+<set>`.  The particles cannot store a per-particle diameter.  To avoid
+being mistakenly considered as point particles, the shape parameters ought
+to be non-spherical, like [1 0.99 0.99].  Unlike the :doc:`resquared
+<pair_resquared>` pair style for which the shape directly determines the
+mathematical expressions of the potential, the shape parameters for this
+pair style is only involved in the computation of the moment of inertia
+and thus only influences the rotational dynamics of individual
+particles.
 
 This pair style requires that **all** atoms are ellipsoids as defined by
 the :doc:`atom_style ellipsoid <atom_style>` command.
@@ -144,7 +156,7 @@ none
 
 .. _Yuan:
 
-**(Yuan2010a)** Yuan, Huang, Li, Lykotrafitis, Zhang, Phys. Rev. E, 82, 011905(2010). 
+**(Yuan2010a)** Yuan, Huang, Li, Lykotrafitis, Zhang, Phys. Rev. E, 82, 011905(2010).
 
 **(Yuan2010b)** Yuan, Huang, Zhang, Soft. Matter, 6, 4571(2010).
 
@@ -154,12 +166,12 @@ none
 
 .. _Fu:
 
-**(Fu)** Fu, Peng, Yuan, Kfoury, Young, Comput. Phys. Commun, 210, 193-203(2017). 
+**(Fu)** Fu, Peng, Yuan, Kfoury, Young, Comput. Phys. Commun, 210, 193-203(2017).
 
 .. _Appshaw:
 
-**(Appshaw)** Appshaw, Seddonb, Hannaa, Soft. Matter,18, 1747(2022).  
+**(Appshaw)** Appshaw, Seddon, Hanna, Soft. Matter,18, 1747(2022).
 
 .. _Becton:
 
-**(Becton)** Becton, Averett, Wang, Biomech. Model. Mechanobiol, 18, 425-433(2019).
+**(Becton)** Becton, Averett, Wang, Biomech. Model. Mechanobiology, 18, 425-433(2019).
diff --git a/doc/utils/sphinx-config/false_positives.txt b/doc/utils/sphinx-config/false_positives.txt
index cc46fd01fe..61c1d45ba7 100644
--- a/doc/utils/sphinx-config/false_positives.txt
+++ b/doc/utils/sphinx-config/false_positives.txt
@@ -182,6 +182,7 @@ Avalos
 avalue
 aveforce
 Avendano
+Averett
 avi
 AVX
 awpmd
@@ -272,6 +273,7 @@ bilayers
 binsize
 binstyle
 binutils
+Biomech
 biomolecular
 biomolecule
 Biomolecules
@@ -926,6 +928,7 @@ Emmrich
 emol
 eN
 endian
+endocytosis
 energetics
 energyCorr
 eng
@@ -1157,6 +1160,7 @@ ftm
 ftol
 fuer
 fugacity
+Fu
 Fumi
 func
 funcs
@@ -1308,6 +1312,7 @@ Hamaker
 Hamel
 Hammerschmidt
 Hanley
+Hanna
 haptic
 Haque
 Hara
@@ -1659,6 +1664,7 @@ kepler
 keV
 Keyes
 keyfile
+Kfoury
 Khersonskii
 Khrapak
 Khvostov
@@ -2025,6 +2031,7 @@ MEAM
 meamf
 meanDist
 mech
+Mechanobiology
 Mecke
 mediumaquamarine
 mediumblue
@@ -3146,6 +3153,7 @@ seagreen
 Secor
 sectoring
 sed
+Seddon
 segmental
 Seifert
 Seleson