diff --git a/res/paper.md b/res/paper.md
index 982eea9..6311310 100644
--- a/res/paper.md
+++ b/res/paper.md
@@ -30,24 +30,24 @@ A Cartesian impedance controller is a type of control strategy that is used in r
 
 In this package, we provide a C++ implementation of a controller that allows collaborative robots:
 
-1. To achieve compliance in its Cartesian task-frame coordinates.
-2. To allow for joint compliance in the nullspace of its task-frame coordinates.
-3. To be able to apply desired forces and torques to the environment of the robot, *e.g.*, for direct force control.
+1. To achieve compliance in Cartesian task-frame coordinates;
+2. To allow for joint compliance in the nullspace of task-frame coordinates; and
+3. To be able to apply desired forces and torques to their environments, e.g., for direct force control.
 
-This package can be used in any torque-controlled robotic manipulator. Its implementation in Robot Operating System (ROS) integrates it into `ros_control` [@ros_control] and can automatically utilize the URDF description of the robot's geometry.
+This package can be used in any torque-controlled robotic manipulator. Its implementation in Robot Operating System (ROS) integrates it into `ros_control` [@ros_control] and can automatically utilize the Unified Robot Description Format (URDF) description of the robot's geometry.
 
 # Statement of Need
-Modern robotics is moving more and more past the traditional robot systems that have hard-coded paths and stiff manipulators. Many use-cases require the robots to work in semi-structured environments. These environments impose uncertainties that could cause collisions. Furthermore, many advanced assembly, manufacturing and household scenarios such as insertions or wiping motions require the robot to excert a controlled force on the environment. Finally, the robot workspace is becoming increasingly shared with human workers in order to leverage both agents and allow them to complement each other.
+Modern robotics is moving more and more past the traditional robot systems that have hard-coded paths and stiff manipulators. Many use cases require the robots to work in semi-structured environments. These environments impose uncertainties that could cause collisions. Furthermore, many advanced assembly, manufacturing, and household scenarios such as insertions or wiping motions require the robot to excert a controlled force on the environment. Finally, the robot workspace is becoming increasingly shared with human workers to leverage both agents and allow them to complement each other.
 
 An implementation of compliant control for robotic manipulators is an attractive solution for robots in contact-rich environments. To cover the wide variety of tasks and scenarios, we think that it needs to fulfill the following criteria:
 
 1. Dynamically adapt the end-effector reference point.
-2. Dynamically adjust the robot's impedance (*i.e.*, its ability to resist or comply with external forces).
-3. Apply commanded forces and torques (*i.e.*, a wrench) with the end-effector of the robot.
+2. Dynamically adjust the robot's impedance (i.e., its ability to resist or comply with external forces).
+3. Apply commanded forces and torques (i.e., a wrench) with the end-effector of the robot.
 4. Command a joint configuration and apply it in the nullspace of the Cartesian robotic task.
 5. Execute joint-space trajectories.
 
-A complete implementation with respect to items 1-5 above of compliance for torque-commanded robotic manipulators is not available, and the existing solutions `franka_ros` [@franka_ros] and `libfranka` [@libfranka] as well as the `KUKA` FRI Cartesian impedance controller can only be used for a single type of robotic manipulator:
+A complete implementation with respect to items 1–5 above of compliance for torque-commanded robotic manipulators is not available, and the existing solutions `franka_ros` [@franka_ros] and `libfranka` [@libfranka] as well as the `KUKA` FRI Cartesian impedance controller can only be used for a single type of robotic manipulator:
 
 |                            | KUKA FRI controller | franka_ros | libfranka | **This package** |
 |----------------------------|:-------------------:|:----------:|:---------:|:------------:|
@@ -59,9 +59,9 @@ A complete implementation with respect to items 1-5 above of compliance for torq
 |    Trajectory Execution    |                     |            |           |     **x**    |
 |     Multi-Robot Support    |                     |            |           |     **x**    |
 
-This implementation offers a base library that can easily be integrated into other software and also implements a `ros_control` controller on top of the base library for the popular ROS middleware. The base library can be used with simulation software such as DART [@Lee2018]. It is used for contact-rich applications such as wiping a surface @mayr23wiping. Furthermore it is utilized in several research papers such as @mayr22skireil, @mayr22priors, @ahmad2022generalizing and @ahmad23generalization that explore reinforcement learning as a strategy to accomplish contact-rich industrial robot tasks.
+This implementation offers a base library that can easily be integrated into other software and also implements a `ros_control` controller on top of the base library for the popular ROS middleware. The base library can be used with simulation software such as DART [@Lee2018]. It is used for contact-rich applications such as wiping a surface @mayr23wiping. Furthermore it is used in several research papers such as those by @mayr22skireil; @mayr22priors; @ahmad2022generalizing; and @ahmad23generalization that explore reinforcement learning as a strategy to accomplish contact-rich industrial robot tasks.
 
-The Robot Operating System (ROS) is an open-source middleware that is widely used in the robotics community for the development of robotic software systems [@quigley:2009]. Within ROS, an implementation of compliant control is available for position-commanded and velocity-commanded robotic manipulators with the `cartesian_controllers` package [@FDCC]. However, if a robotic manipulator supports direct control of the joint torques, *e.g.*, the `KUKA LBR iiwa` or the `Franka Emika Robot (Panda)`, torque-commanded Cartesian impedance control is often the preferred control strategy, since a stable compliant behavior might not be achieved for position-commanded and velocity-commanded robotic manipulators [@lawrence:1988].
+The Robot Operating System (ROS) is an open-source middleware that is widely used in the robotics community for the development of robotic software systems [@quigley:2009]. Within ROS, an implementation of compliant control is available for position-commanded and velocity-commanded robotic manipulators with the `cartesian_controllers` package [@FDCC]. However, if a robotic manipulator supports direct control of the joint torques, e.g., the `KUKA LBR iiwa` or the `Franka Emika Robot (Panda)`, torque-commanded Cartesian impedance control is often the preferred control strategy, since a stable compliant behavior might not be achieved for position-commanded and velocity-commanded robotic manipulators [@lawrence:1988].
 
 # Control Implementation
 
@@ -69,9 +69,9 @@ The gravity-compensated rigid-body dynamics of the controlled robot can be descr
 \begin{equation}\label{eq:rigbod_q}
     M(q)\ddot{q} + C(q,\dot{q})\dot{q} = \tau_{\mathrm{c}} + \tau^{\mathrm{ext}}
 \end{equation}
-where $M(q)\in  \mathbb{R}^{n\times n}$ is the generalized inertia matrix, $C(q,\dot{q})\in  \mathbb{R}^{n\times n}$ captures the effects of Coriolis and centripetal forces, $\tau_{\mathrm{c}}\in  \mathbb{R}^{n}$ represents the input torques, and $\tau^{\mathrm{ext}}\in  \mathbb{R}^{n}$ represents the external torques, with $n$ being the number of joints of the robot. Since the proposed controller was evaluated using robots that are automatically gravity-compensated (`KUKA LBR iiwa` and `Franka Emika Robot (Panda)`), the gravity-induced torques have not been included in (\autoref{eq:rigbod_q}). However, the proposed controller can be used in robots that are not automatically gravity-compensated by adding a gravity-compensation term to the commanded torque signal, $\tau_{\mathrm{c}}$.
+where $M(q)\in  \mathbb{R}^{n\times n}$ is the generalized inertia matrix, $C(q,\dot{q})\in  \mathbb{R}^{n\times n}$ captures the effects of Coriolis and centripetal forces, $\tau_{\mathrm{c}}\in  \mathbb{R}^{n}$ represents the input torques, and $\tau^{\mathrm{ext}}\in  \mathbb{R}^{n}$ represents the external torques, with $n$ being the number of joints of the robot. Since the proposed controller was evaluated using robots that are automatically gravity-compensated (`KUKA LBR iiwa` and `Franka Emika Robot (Panda)`), the gravity-induced torques have not been included in \autoref{eq:rigbod_q}. However, the proposed controller can be used in robots that are not automatically gravity-compensated by adding a gravity-compensation term to the commanded torque signal, $\tau_{\mathrm{c}}$.
 
-Moreover, the torque signal commanded by the proposed controller to the robot, $\tau_{\mathrm{c}}$ in (\autoref{eq:rigbod_q}), is composed by the superposition of three joint-torque signals:
+Moreover, the torque signal commanded by the proposed controller to the robot, $\tau_{\mathrm{c}}$ in \autoref{eq:rigbod_q}, is composed by the superposition of three joint-torque signals:
 \begin{equation}\label{eq:tau_c}
     \tau_{\mathrm{c}} = \tau_{\mathrm{c}}^\mathrm{ca} + \tau_{\mathrm{c}}^\mathrm{ns} + \tau_{\mathrm{c}}^\mathrm{ext}
 \end{equation}
@@ -81,13 +81,13 @@ where
     \begin{equation}\label{eq:tau_sup}
         \tau_{\mathrm{c}}^\mathrm{ca} = J^{\mathrm{T}}(q)\left[-K^\mathrm{ca}\Delta \xi-D^\mathrm{ca}J(q) \dot{q}\right]
     \end{equation}
-    with $J(q)\in \mathbb{R}^{m \times n}$ being the Jacobian relative to the end-effector (task) frame of the robot, and $K^\mathrm{ca}\in \mathbb{R}^{m \times m}$ and $D^\mathrm{ca}\in \mathbb{R}^{m \times m}$ being the virtual Cartesian stiffness and damping matrices, respectively. Also, the Cartesian pose error, $\Delta \xi$ in (\autoref{eq:tau_sup}) is defined as $\Delta \xi_{\mathrm{tr}} = \xi_{\mathrm{tr}}-\xi_{\mathrm{tr}}^{\mathrm{D}}$ for the translational degrees of freedom of the Cartesian pose and as \mbox{$\Delta \xi_{\mathrm{ro}} = \xi_{\mathrm{ro}}\left(\xi_{\mathrm{ro}}^{\mathrm{D}}\right)^{-1}$} for the rotational degrees of freedom.
+    with $J(q)\in \mathbb{R}^{m \times n}$ being the Jacobian relative to the end-effector (task) frame of the robot, and $K^\mathrm{ca}\in \mathbb{R}^{m \times m}$ and $D^\mathrm{ca}\in \mathbb{R}^{m \times m}$ being the virtual Cartesian stiffness and damping matrices, respectively. Also, the Cartesian pose error, $\Delta \xi$ in \autoref{eq:tau_sup} is defined as $\Delta \xi_{\mathrm{tr}} = \xi_{\mathrm{tr}}-\xi_{\mathrm{tr}}^{\mathrm{D}}$ for the translational degrees of freedom of the Cartesian pose and as \mbox{$\Delta \xi_{\mathrm{ro}} = \xi_{\mathrm{ro}}\left(\xi_{\mathrm{ro}}^{\mathrm{D}}\right)^{-1}$} for the rotational degrees of freedom.
 
 * $\tau_{\mathrm{c}}^\mathrm{ns}$ is the torque commanded to achieve a joint impedance behavior with respect to a desired configuration and projected in the null-space of the robot's Jacobian, to not affect the Cartesian motion of the robot's end-effector [@ott:2008]:
     \begin{equation}\label{eq:tau_ns}
         \tau_{\mathrm{c}}^\mathrm{ns} = \left(I_n-J^{\mathrm{T}}(q)(J^{\mathrm{T}}(q))^\mathrm{\dagger}\right)\tau_0
     \end{equation}
-    with the superscript $^\mathrm{\dagger}$ denoting the Moore-Penrose pseudoinverse matrix [@khatib:1995]\footnote{The Moore-Penrose pseudoinverse is computationally cheap and allows a null-space projection disregarding the dynamics of the robot. However, not using the dynamics of the robot to fomulate a pseudoinverse matrix for null-space projection may cause that a non-zero arbitrary torque, $\tau_0$ in (\autoref{eq:tau_ns}), generates interfering forces in the Cartesian space if the joint of the robot are not in a static equilibrium ($\dot{q} = \ddot{q} = 0$).} given by \mbox{$J^\dagger = (J^\mathrm{T}J)^{-1}J^\mathrm{T}$} [@ben:2003], and $\tau_0$ being an arbitrary joint torque formulated to achieve joint compliance, 
+    with the superscript $^\mathrm{\dagger}$ denoting the Moore-Penrose pseudoinverse matrix [@khatib:1995]\footnote{The Moore–Penrose pseudoinverse is computationally cheap and allows a null-space projection disregarding the dynamics of the robot. However, not using the dynamics of the robot to fomulate a pseudoinverse matrix for null-space projection may cause that a non-zero arbitrary torque, $\tau_0$ in \autoref{eq:tau_ns}, generates interfering forces in the Cartesian space if the joint of the robot are not in a static equilibrium ($\dot{q} = \ddot{q} = 0$).} given by \mbox{$J^\dagger = (J^\mathrm{T}J)^{-1}J^\mathrm{T}$} [@ben:2003], and $\tau_0$ being an arbitrary joint torque formulated to achieve joint compliance, 
     \begin{equation}\label{eq:tau_0}
         \tau_0 = -K^\mathrm{ns}(q-q^{\mathrm{D}}) - D^\mathrm{ns} \dot{q}
     \end{equation}
@@ -103,7 +103,7 @@ where
 As described in \autoref{fig:flowchart}, there are several safety measures that have been implemented in the controller to achieve a smooth behavior of the robot:
 
 ### Filtering  \label{filt}
-The proposed controller allows the online modification of relevant variables: $\xi^{\mathrm{D}}$, $K^\mathrm{ca}$ and $D^\mathrm{ca}$ in (\autoref{eq:tau_sup}), $K^\mathrm{ns}$ and $D^\mathrm{ns}$ in (\autoref{eq:tau_0}), and $F_{\mathrm{c}}^\mathrm{ext}$ in (\autoref{eq:tau_ext}). However, for a smoother behavior of the controller, the values of these variables are low-pass filtered. The update law at each time-step $k$ is:
+The proposed controller allows the online modification of relevant variables: $\xi^{\mathrm{D}}$, $K^\mathrm{ca}$ and $D^\mathrm{ca}$ in \autoref{eq:tau_sup}, $K^\mathrm{ns}$ and $D^\mathrm{ns}$ in \autoref{eq:tau_0}, and $F_{\mathrm{c}}^\mathrm{ext}$ in \autoref{eq:tau_ext}. However, for a smoother behavior of the controller, the values of these variables are low-pass filtered. The update law at each time-step $k$ is:
 \begin{equation}
     \alpha_{k+1} = (1-a)\alpha_k + a \alpha^\mathrm{D}
 \end{equation}
@@ -118,13 +118,13 @@ where $\alpha^\mathrm{D}$ is the desired new variable value and $a\in(0,1]$ is d
 being $\delta t$ the time between samples of the controller, *i.e.*, the inverse of the sampling frequency of the controller.) -->
 
 ### Saturation
-To increase safety in the controller, some of the filtered variables (the stiffness and damping factors $K^\mathrm{ca}$, $D^\mathrm{ca}$, $K^\mathrm{ns}$ and $D^\mathrm{ns}$, and the desired external force command $F_{\mathrm{c}}^\mathrm{ext}$) can be saturated between user-defined maximum and minimum limits, *i.e.*, for an example variable $\alpha$:
+To increase safety in the controller, some of the filtered variables (the stiffness and damping factors $K^\mathrm{ca}$, $D^\mathrm{ca}$, $K^\mathrm{ns}$, and $D^\mathrm{ns}$, and the desired external force command $F_{\mathrm{c}}^\mathrm{ext}$) can be saturated between user-defined maximum and minimum limits, i.e., for an example variable $\alpha$:
 \begin{equation}
     \alpha_\mathrm{min} \leq \alpha \leq \alpha_\mathrm{max} 
 \end{equation}
 
 ### Rate Limiter
-The rate of the commanded torque, $\tau_\mathrm{c}$ in (\autoref{eq:tau_c}), can be limited. For two consecutive commands at times $k$ and $k+1$:
+The rate of the commanded torque, $\tau_\mathrm{c}$ in \autoref{eq:tau_c}, can be limited. For two consecutive commands at times $k$ and $k+1$:
 \begin{equation}
     \Delta \tau_\mathrm{max} \geq \|\tau_{\mathrm{c},k+1} - \tau_{\mathrm{c},k}\|
 \end{equation}