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config.toml

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base_url = "https://um-arm-lab.github.io/lucca"
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base_url = "https://um-arm-lab.github.io/claps"
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compile_sass = true
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build_search_index = false
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generate_feeds = false
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favicon = false
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large_card = true
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footer_text = "This website is built using <a href='https://www.getzola.org' target='_blank'>Zola</a> and the <a href='http://github.com/aterenin/academic-paper/' target='_blank'>Academic Paper</a> theme, which is <a href='https://jeffhuang.com/designed_to_last/' target='_blank'>designed to last</a>."
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server_side_katex = true
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server_side_katex = true

content/_index.md

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@@ -40,48 +40,27 @@ In this work, we rigorously analyze configuration errors using Lie groups, exten
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</div>
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# Problem Statement
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**Setting**: Let `$q\in \mathcal Q$` be the configuration of a
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robot, `$\dot q \in Tq \mathcal Q$` be
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the generalized velocity, and `$s := (q,\dot q) \in T\mathcal Q$` its state.
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We consider both holonomic systems and robots subject to
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*nonholonomic constraints*, i.e., non-integrable constraints on
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the allowable velocities. We observe
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the true dynamical system state at discrete points `$s_k := s(k\Delta t)$`, where `$\Delta t$` is the sampling time between
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measurements. We consider systems with time-invariant
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stochastic dynamics whose `$\mathcal Q$` can be represented by the
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matrix Lie group `$SE(2)$` and `$SE(3)$`. This class is broad,
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encompassing unicycles, differential drive vehicles, car-like
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systems, quadrotors, surface vessels, underwater vehicles,
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satellites, quadrupeds modeled by their center of mass,
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and so on. We write the true
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unknown dynamics of the observable discrete process as
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{% problem_columns() %}
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### Problem Setting
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Let `$q\in \mathcal Q$` be the robot configuration, `$\dot q \in T_q \mathcal Q$` the generalized velocity, and `$s := (q,\dot q) \in T\mathcal Q$` the state. We consider holonomic and *nonholonomic* systems whose `$\mathcal Q$` is the Lie group `$SE(2)$` or `$SE(3)$` (unicycles, car-like robots, quadrotors, surface/underwater vehicles, satellites, quadrupeds’ COM, ...). The *unknown dynamics* evolve as
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```
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$$
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s_{k+1} = f(s_k, u_k, w_k), w_k P_{noise},
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s_{k+1} = f(s_k, u_k, w_k), \qquad w_k \sim P_{noise},
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$$
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```
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where `$f$` is an *unknown* deterministic function, `$w_k$` is a
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stochastic term drawn iid from an *unknown* distribution `$P_{noise}$`, and `$u_k \in \mathbb R^m$` is the known control input. Inaccuracies in
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modeling `$f$` may arise e.g., from domain shifts between fitting
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and deployment, and result in *epistemic uncertainty*. On the
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other hand, `$w_k$` makes the dynamics stochastic, introducing
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*aleatoric uncertainty*, and may represent external disturbances
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such as wind gusts, wheel slippage, or terrain bumps.
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**Objective**: Our goal is to provide, for a given admissible action `$u_{des}$`, a C-Space prediction region `$C^q \subseteq \mathcal Q$` that provably contains the next true *unknown system configuration* `$q_1$` with, at
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least, a *user-defined probability* `$(1-\alpha)$`, i.e.
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where `$f$` is *unknown*, `$w_k$` is an iid disturbance drawn from an *unknown* distribution, and `$u_k \in \mathbb R^m$` is the control input. Inaccuracies
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in modeling `$f$` may arise e.g., from domain shifts between fitting and deployment, and result in *epistemic uncertainty*. Additionally,
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`$w_k$` introduces *aleatoric uncertainty*, and may represent external disturbances such as wind gusts, wheel slippage, or terrain bumps.
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---
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### Objective
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For a given admissible action `$u_{des}$`, provide a C-Space prediction region `$C^q \subseteq \mathcal Q$` that contains the resulting (unknown) configuration `$q_1$` with probability at least `$(1-\alpha)$`:
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```
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$$
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\mathbb{P}(q_1 \in \mathcal C^q ) \ge (1 − \alpha),
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\mathbb{P}(q_1 \in \mathcal C^q ) \ge 1 - \alpha, \quad \alpha \in (0,1).
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$$
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```
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where `$\alpha \in (0,1)$` is the user-set acceptable failure-probability.
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While purely achieving this is trivial, e.g., by predicting the
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entire space `$C^q =\mathcal Q$`, we additionally want `$C^q$` to be as
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*tight/volume-efficient* as possible to make it practical for
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downstream robotic tasks such as *safe control*. We do not make strong assumptions about the fidelity of `$\tilde f$`, or the nature of the stochastic disturbances.
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where `$\alpha$` is the user-set acceptable failure probability. While purely achieving this goal is trivial, e.g., by predicting the entire space `$(C^q = \mathcal Q)$`, we additionally want `$C^q$` to be as *tight/volume-efficient* as possible, to make it practical for downstream robotic tasks such as *safe control*. We do not make strong assumptions about the fidelity of `$\tilde{f}$`, or the nature of the stochastic disturbances.
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{% end %}
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# CLAPS
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**Method Figure.** **C**onformal **L**ie-Group **A**ction **P**rediction **S**ets | Offline: a dataset of state transitions is used jointly with an approximate dynamical model to derive a rigorous symmetry-aware probabilistic error bound on the configuration predictions. Online: our algorithm takes in a desired action `$u_{des}$` and computes a *calibrated C-Space prediction region* `$\mathcal{C}^q$` that is marginally guaranteed to contain the true configuration resulting from executing `$u_{des}$`.
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{% end %}
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The prediction region constructed by **CLAPS** `$(C^q \subseteq Q)$` can be used for probably-safe control in three main ways:
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- Configuration Check: a (sample) configuration `$g$` belongs in `$C^q$` if `$\sqrt{\log(\tilde{g}^{-1}g)^\top \tilde{\Sigma}^{-1}\log(\tilde{g}^{-1}g)} \le \chi^2_{\alpha}(\dim \mathfrak g)$` --- quick to evaluate in batch
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- C-space set: The `$C^q$` can be reconstructed by Alg. 2, for example to check if `$C^q \subseteq \mathcal Q_{safe}$`, for a known safe set `$\mathcal Q_{safe} \subseteq \mathcal Q$`.
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- Workspace set: `$C^q$` can be inflated by the robot's radius and mapped to the workspace `$(\mathbb R^2)$` to perform collision checks with known obstacles.
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For more details, please refer to Section `$\S$`V-C in the paper.
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The prediction region constructed by **CLAPS** `$(C^q \subseteq Q)$` can be used for probably-safe control in three main ways (for more details refer to Section `$\S$`V-C):
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1. Configuration Check: a (sample) configuration `$g$` belongs in `$C^q$` if `$\sqrt{\log(\tilde{g}^{-1}g)^\top \tilde{\Sigma}^{-1}\log(\tilde{g}^{-1}g)} \le \chi^2_{\alpha}(\dim \mathfrak g)$` --- quick to evaluate in batch
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2. C-space set: The `$C^q$` can be reconstructed by Alg. 2, for example to check if `$C^q \subseteq \mathcal Q_{safe}$`, for a known safe set `$\mathcal Q_{safe} \subseteq \mathcal Q$`.
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3. Workspace set: `$C^q$` can be inflated by the robot's radius and mapped to the workspace `$(\mathbb R^2)$` to perform collision checks with known obstacles.
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# Experiments
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We compare **CLAPS** in both simulation (JetBot) and hardware (MBot) against seven baselines to demonstrate its improved *efficiency* and *representation quality*.
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In both cases, we model the system as a second-order unicycle.
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We perform standard system identification to estimate the inertial properties (mass and inertia)
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## JetBot Experiments (Simulation)
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In Isaac Sim, we independently sampled perturbations to the commanded actions to introduce aleatoric uncertainty into the system. Additionally, epistemic uncertainty arose from unmodeled effects (see paper) and imperfections in the inertial property estimation.
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**JetBot Experiments (Simulation)**<br>
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&emsp;In Isaac Sim, we independently sampled perturbations to the commanded actions to introduce aleatoric uncertainty into the system. Additionally, epistemic uncertainty arose from unmodeled effects (see paper) and imperfections in the inertial property estimation.
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The Figure below demonstrates **CLAPS**' ability to represent the underlying dynamics uncertainty of the unknown system (MC particles).
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{% figure(alt=["Workspace method comparison plot"] src=["contour_comparison_val_isaac_0007_vs_val_isaac_0590_clear.png"] dark_invert=[true] style="width:80%") %}
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## MBot Experiments (Hardware)
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We also validated our method on an MBot, a differential-drive vehicle shown below.
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**MBot Experiments (Hardware)**<br>
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&emsp;We also validated our method on an MBot, a differential-drive vehicle shown below.
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Despite a relatively-small calibration dataset corresponding to `$\approx$`2 min of driving data `$(\lvert D_{cal}\rvert = 237)$`, our method provably satisfied the user-specified safety specifications, thanks to its *non-asymptotic guarantees*.
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**CLAPS** uses `$D_{cal}$` to derive data-driven provable (probabilistic) bounds on the uncertainty arising from both model mismatch, and inherent stochasticity.
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sass/_figures.scss

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img,
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video {
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margin-bottom: 0.5rem;
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margin-left: auto;
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margin-right: auto;
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display: block;
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}
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>div {

sass/main.scss

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flex: none;
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width: 100%;
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}
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}
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}
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/* Problem statement two-column cards */
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.problem-columns {
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display: grid;
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grid-template-columns: repeat(auto-fit, minmax(280px, 1fr));
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gap: 1.25rem;
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align-items: stretch;
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margin: 1.5rem 0 2rem;
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}
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.problem-card {
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background: var(--color-light);
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border: 1px solid var(--color-border);
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border-radius: 0.5rem;
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padding: 1.1rem 1.25rem;
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display: flex;
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flex-direction: column;
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height: 100%;
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hyphens: none;
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}
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.problem-card h3 {
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margin: 0 0 0.5rem;
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}
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.problem-card p,
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.problem-card ul {
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margin: 0 0 0.65rem;
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}
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.problem-card p,
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.problem-card li {
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hyphens: none;
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}
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.problem-card ul {
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padding-left: 1.2rem;
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}
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{% set parts = body | trim | split(pat="---") %}
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<div class="problem-columns">
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{% for part in parts %}
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{% if part | trim != "" %}
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<div class="problem-card">
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{{ part | trim | markdown | safe }}
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</div>
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{% endif %}
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{% endfor %}
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</div>

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