2026 - Important Thesis - M-Layer on Scientific Law Verification, ODE to PDEs
Thomas, Jyrki, profs and Labs
End Goals
- pretty visuals
- M-Layer for discovering and verifying induced by scientific laws in
high-dimensional observationspace. - What might be missed in current Theoretical Laws?
Experiment test:
- Can the model determine whether X=(q,v,a) is xxx?
Key Index:
- Zero-shot / Systematic Generalization / (Out-of-Distribution (OOD) Generalization Ability)
Lorentz data
- 1D
gamma / energy
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|______/________________________> beta = v/c
0 0.5 0.9 1
- 2D
beta_y
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| high gamma near boundary
| ***********************
| *** ***
| ** low gamma **
| ** near center **
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+-------------------------------> beta_x
What Else Can be Verified?
| Frontier Problem | Core Open Question | Why | AI / M-Layer Direction |
|---|---|---|---|
| Quantum Gravity | How can general relativity and quantum mechanics be unified? | It asks what spacetime is at the Planck scale. | Learn whether observed dynamics lie on hidden constraint manifolds consistent with classical, semiclassical, or beyond-GR regimes. |
| Dark Matter | Is dark matter a particle, a field, primordial black holes, or modified gravity? | Most matter in the universe is gravitationally visible but physically unidentified. | Use high-dimensional classifiers to distinguish Newtonian gravity, dark matter halos, and modified-gravity trajectories from lensing and galaxy dynamics. |
| Dark Energy | Is cosmic acceleration caused by a cosmological constant or evolving dark energy? | Recent DESI results strengthen hints that dark energy may evolve over time. (DESI) | Learn deviations from ΛCDM as geometric constraints in cosmological trajectory space. |
| Black Hole Information Problem | Does black hole evaporation preserve quantum information? | It tests the consistency of quantum mechanics, thermodynamics, and gravity. | Use AI as a verifier for whether simulated black-hole dynamics obey conservation, entropy, and causal constraints. |
| Testing General Relativity | Does Einstein gravity remain exact in strong-field regimes? | Gravitational waves allow direct tests near merging black holes. Current LIGO-Virgo-KAGRA analyses remain consistent with GR. (aei.mpg.de) | Train physical-law verifiers on waveform manifolds to detect subtle beyond-GR deviations. |
| Gravitational-Wave Discovery | Can we extract weak, noisy, rare signals from detector data? | It opens a new observational channel for black holes, neutron stars, and early-universe physics. | AI is already used for denoising, waveform modeling, and parameter estimation in gravitational-wave pipelines. (Hep Journals) |
| Cosmic Structure Formation | How did galaxies, halos, filaments, and voids emerge from early fluctuations? | It connects gravity, dark matter, baryons, and cosmology across billions of years. | Learn compact latent laws from simulations and surveys; explainable ML has already found interpretable structure in dark-matter halo profiles. (mpa-garching.mpg.de) |
| Weak Lensing and Hidden Mass | Can we reconstruct invisible matter from distorted galaxy images? | Lensing is one of the cleanest probes of dark matter and dark energy. | Use AI-assisted simulation-based inference and constraint learning to map hidden mass fields from sparse observations. (Imperial College London) |
| Modified Gravity | Are cosmic anomalies caused by unseen matter or by a failure of GR at large scales? | It challenges the foundation of modern cosmology. | Build contrastive datasets: GR-valid trajectories vs modified-gravity trajectories, then learn the separating physical manifold. |
| From Galaxies to Cells | Can one learning principle discover lawful dynamics across scales? | It would unify scientific ML beyond domain-specific prediction. | M-Layer can be framed as a high-dimensional physical constraint learner: not predicting one trajectory, but verifying whether a system belongs to the lawful manifold. |
High-Dimensional Constraints Induced by Scientific Laws
| Domain | Scientific Law / Equation | Formula | Physical Meaning | What M-Layer Can Verify or Learn | ||||
|---|---|---|---|---|---|---|---|---|
| Special Relativity | Mass-energy equivalence | $E = mc^2$ | Mass and energy are equivalent; rest mass is a form of energy. | Verify whether generated particle or event data preserve relativistic energy relations. | ||||
| Special Relativity | Relativistic energy-momentum relation | $E^2 = p^2c^2 + m^2c^4$ | Energy, momentum, and mass are constrained by spacetime geometry. | Check whether simulated high-energy particles lie on the relativistic mass shell. | ||||
| Special Relativity | Lorentz factor | $\gamma = \frac{1}{\sqrt{1 - v^2/c^2}}$ | Time dilation and length contraction depend on velocity. | Detect impossible trajectories where $v > c$ or relativistic timing becomes inconsistent. | ||||
| Special Relativity | Time dilation | $\Delta t’ = \gamma \Delta t$ | Moving clocks are measured differently by different observers. | Verify relativistic time-series data, such as satellite timing or high-speed motion. | ||||
| Special Relativity | Length contraction | $L = \frac{L_0}{\gamma}$ | Moving objects contract along the direction of motion. | Detect violations in generated relativistic geometry. | ||||
| Special Relativity | Four-velocity normalization | $u^\mu u_\mu = -c^2$ | Physical worldlines have a fixed spacetime norm. | Learn the lawful manifold of admissible relativistic trajectories. | ||||
| General Relativity | Einstein field equations | $G_{\mu\nu} + \Lambda g_{\mu\nu} = \frac{8\pi G}{c^4}T_{\mu\nu}$ | Matter-energy determines spacetime curvature, and curvature determines motion. | Verify whether a proposed metric $g_{\mu\nu}$ and stress-energy tensor $T_{\mu\nu}$ are mutually consistent. | ||||
| General Relativity | Einstein tensor | $G_{\mu\nu} = R_{\mu\nu} - \frac{1}{2}Rg_{\mu\nu}$ | Curvature is summarized by the Einstein tensor. | Test whether learned geometric fields satisfy curvature consistency. | ||||
| General Relativity | Vacuum Einstein equation | $R_{\mu\nu} = 0$ | Empty spacetime can still contain curvature, such as gravitational waves or black holes. | Verify whether simulated vacuum spacetime solutions are physically admissible. | ||||
| General Relativity | Geodesic equation | $\frac{d^2x^\mu}{d\tau^2} + \Gamma^\mu_{\alpha\beta}\frac{dx^\alpha}{d\tau}\frac{dx^\beta}{d\tau} = 0$ | Free-falling objects follow geodesics in curved spacetime. | Verify whether trajectories are consistent with an inferred gravitational field. | ||||
| General Relativity | Stress-energy conservation | $\nabla_\mu T^{\mu\nu} = 0$ | Energy and momentum are locally conserved in curved spacetime. | Verify whether field simulations preserve local conservation laws. | ||||
| General Relativity | Bianchi identity | $\nabla_\mu G^{\mu\nu} = 0$ | Geometric consistency condition underlying energy-momentum conservation. | Test whether learned curvature fields obey internal geometric consistency. | ||||
| Cosmology | Friedmann equation | $H^2 = \frac{8\pi G}{3}\rho - \frac{kc^2}{a^2} + \frac{\Lambda c^2}{3}$ | Describes the expansion rate of the universe. | Verify whether cosmological trajectories match GR-based expansion laws. | ||||
| Cosmology | Acceleration equation | $\frac{\ddot a}{a} = -\frac{4\pi G}{3}\left(\rho + \frac{3p}{c^2}\right) + \frac{\Lambda c^2}{3}$ | Determines whether cosmic expansion accelerates or decelerates. | Detect whether observed expansion history implies dark energy, modified gravity, or inconsistent dynamics. | ||||
| Cosmology | Critical density | $\rho_c = \frac{3H^2}{8\pi G}$ | Defines the density required for a spatially flat universe. | Verify whether inferred cosmological parameters lie in physically consistent regions. | ||||
| Gravitational Lensing | Weak deflection angle | $\alpha \approx \frac{4GM}{c^2b}$ | Massive objects bend the path of light. | Verify whether lensing patterns are consistent with visible mass, dark matter, or modified gravity. | ||||
| Black Holes | Schwarzschild radius | $r_s = \frac{2GM}{c^2}$ | Defines the event horizon radius of a non-rotating black hole. | Verify whether generated black-hole parameters are physically admissible. | ||||
| Black Holes | Schwarzschild metric | $ds^2 = -\left(1-\frac{2GM}{rc^2}\right)c^2dt^2 + \left(1-\frac{2GM}{rc^2}\right)^{-1}dr^2 + r^2d\Omega^2$ | Exact GR solution for a spherical, non-rotating mass. | Test whether simulated or inferred spacetime geometry matches the Schwarzschild solution. | ||||
| Black Holes | Kerr spin bound | $a = \frac{J}{Mc}, \quad a \leq \frac{GM}{c^2}$ | Rotating black holes have bounded angular momentum. | Detect generated rotating black holes that violate physical spin constraints. | ||||
| Gravitational Waves | Linearized Einstein equation | $\Box \bar h_{\mu\nu} = -\frac{16\pi G}{c^4}T_{\mu\nu}$ | Weak gravitational waves are perturbations of spacetime. | Verify whether waveform data are consistent with GR wave propagation. | ||||
| Gravitational Waves | Vacuum wave equation | $\Box \bar h_{\mu\nu} = 0$ | Gravitational waves propagate through vacuum at light speed. | Detect non-GR waveform deviations or unphysical wave speeds. | ||||
| Gravitational Waves | Quadrupole radiation principle | $P \sim \frac{G}{5c^5}\left\langle \dddot Q_{ij}\dddot Q_{ij}\right\rangle$ | Gravitational waves are mainly emitted by changing mass quadrupoles. | Verify whether simulated binary systems radiate energy consistently. | ||||
| Electromagnetism / Field Theory | Gauss law for electricity | $\nabla \cdot \mathbf{E} = \frac{\rho}{\varepsilon_0}$ | Electric charge is the source of electric fields. | Verify whether learned electric fields are consistent with charge distributions. | ||||
| Electromagnetism / Field Theory | Gauss law for magnetism | $\nabla \cdot \mathbf{B} = 0$ | Magnetic monopoles are absent in classical Maxwell theory. | Detect unphysical magnetic fields with nonzero divergence. | ||||
| Electromagnetism / Field Theory | Faraday induction law | $\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t}$ | Time-varying magnetic fields induce electric fields. | Verify whether temporal field evolution obeys electromagnetic induction. | ||||
| Electromagnetism / Field Theory | Ampere-Maxwell law | $\nabla \times \mathbf{B} = \mu_0\mathbf{J} + \mu_0\varepsilon_0\frac{\partial \mathbf{E}}{\partial t}$ | Currents and time-varying electric fields generate magnetic fields. | Learn whether electromagnetic field simulations preserve Maxwell dynamics. | ||||
| Electromagnetic Waves | Wave equation in vacuum | $\Box A^\mu = 0$ | Light is a propagating electromagnetic field. | Verify whether generated wave fields propagate causally at speed $c$. | ||||
| Gauge Field Theory | Electromagnetic field tensor | $F_{\mu\nu} = \partial_\mu A_\nu - \partial_\nu A_\mu$ | Electromagnetic fields arise from a gauge potential. | Learn gauge-consistent field representations instead of only fitting raw fields. | ||||
| Quantum Mechanics | Schrodinger equation | $i\hbar\frac{\partial}{\partial t}\psi = \hat H\psi$ | Quantum states evolve under the Hamiltonian operator. | Verify whether learned quantum-state trajectories obey unitary evolution. | ||||
| Quantum Mechanics | Born rule | $P(x) = | \psi(x) | ^2$ | Measurement probabilities are given by wave-function amplitudes. | Check whether generated quantum states produce valid probability distributions. | ||
| Quantum Mechanics | Canonical commutation relation | $[\hat x, \hat p] = i\hbar$ | Position and momentum cannot both be sharply determined. | Verify whether learned latent operators preserve quantum structure. | ||||
| Quantum Field Theory | Klein-Gordon equation | $(\Box + m^2)\phi = 0$ | Relativistic scalar fields satisfy a wave-like mass-shell equation. | Verify whether generated scalar fields satisfy relativistic field constraints. | ||||
| Quantum Field Theory | Dirac equation | $(i\gamma^\mu\partial_\mu - m)\psi = 0$ | Relativistic spin-1/2 particles are described by spinor fields. | Learn physically admissible fermionic field dynamics. | ||||
| Quantum Field Theory | Yang-Mills field equation | $D_\mu F^{\mu\nu} = J^\nu$ | Non-Abelian gauge fields generalize electromagnetism. | Verify whether learned gauge fields obey local symmetry constraints. | ||||
| Standard Model | Gauge symmetry structure | $SU(3)_C \times SU(2)_L \times U(1)_Y$ | The Standard Model is organized by local gauge symmetries. | Learn whether high-dimensional particle interaction data respect symmetry-induced constraints. | ||||
| Higgs Mechanism | Higgs potential | $V(\phi) = \mu^2 | \phi | ^2 + \lambda | \phi | ^4$ | Spontaneous symmetry breaking gives particles mass. | Verify whether learned particle-field configurations lie near physically meaningful vacuum structures. |
| Statistical Physics | Boltzmann distribution | $p(x) = \frac{1}{Z}e^{-E(x)/(k_BT)}$ | Equilibrium probabilities depend exponentially on energy. | Check whether generated molecular or thermodynamic states obey equilibrium statistics. | ||||
| Brownian Motion | Einstein diffusion relation | $\langle x^2(t)\rangle = 2Dt$ | Microscopic random motion produces macroscopic diffusion. | Verify whether stochastic particle, cell, or molecular trajectories obey diffusion scaling. | ||||
| Statistical Physics | Einstein mobility-diffusion relation | $D = \mu k_BT$ | Diffusion and mobility are linked by temperature. | Test whether noisy dynamics respect thermodynamic constraints. | ||||
| Photoelectric Effect | Photon energy | $E = hf$ | Light energy is quantized into photons. | Verify whether photon-material interaction data obey quantum energy constraints. | ||||
| Photoelectric Effect | Photoelectric equation | $K_{\max} = hf - \phi$ | Electron kinetic energy depends on light frequency and material work function. | Verify whether simulated photoelectric data obey quantum threshold behavior. | ||||
| Atomic Radiation | Detailed balance condition | $N_1B_{12}\rho(\nu) = N_2B_{21}\rho(\nu) + N_2A_{21}$ | Radiation and matter reach equilibrium through balanced transitions. | Check whether learned atomic transition models preserve equilibrium physics. |
Toolkit
- [npzviewer]
1. ODE
- 2025 - Life at the boundary of chemical kinetics and program execution, physical constraints
- 1931 - Hamiltonian Systems and Transformation in Hilbert Space
- nonlinear dynamics can be represented as linear transformations on a Hilbert space of observables.
- 2024 - Soliton dynamics and multistability analysis of the Hamiltonian amplitude model
- 2026 - Paving the way for agents in biology
2.Hamiltonian Systems and Operators
- Hamiltonian system
- Hilbert space: Transition from state point to function space
- Weierstrass Approximation Theorem
- Universal Approximation Theorem, Bézier Curve
- Lie operator, Unitary operator
- Flow map
3. Topological Defect
- The data manifold is extremely distorted, dimensionally reduced, or has broken connectivity in this region.
4. PDE / MHD, or Benchmark paper
learning hidden physical fields from sparse multimodal observations
multimodal observation
magnetic-field inference
streamer reconstruction
MHD-constrained dynamics
future disk prediction
ALMA / MHD simulation infers hidden protostellar dynamics
→ export magnetic fields, streamers, and gas-flow trajectories
→ CesiumJS / Three.js visualizes magnetogravitational accretion beautifully
5. Activation Functions and Field Theories
Simulation
trajectory generation
mission scenario
orbit propagation
lunar / deep-space transfer
navigation analysis
GMAT / Basilisk generates trajectory
→ export trajectory points
→ CesiumJS / Three.js visualizes it beautifully
Visualization
- NASA Eyes / Eyes on the Solar System
3D scene
+ time controller
+ camera fly-through
+ mission trajectory
+ object labels
+ information panel
Web Interaction
- NASA/mission-viz
- link
- CesiumJS / Three.js
Bio Process Dynamics: High-Dimensional Constraints Induced by Biochemical Process Laws
| Domain | Scientific Law / Equation | Formula | Physical Meaning | What M-Layer Can Verify or Learn |
|---|---|---|---|---|
| Bioprocess Dynamics | General process ODE manifold | $\dot z = f(z,u;\theta)$ | A bioprocess trajectory is governed by state-dependent kinetic and control laws. | Verify whether a candidate point $(z,u,\dot z)$ lies on the learned dynamic process manifold rather than only matching observed trajectories. |
| Bioprocess Dynamics | Bioprocess residual constraint | $r(z,u,\dot z)=\dot z-f(z,u;\theta)=0$ | Physical consistency is encoded as zero residual between measured rates and governing equations. | Learn the zero-set of biochemical dynamics and reject rate-shuffled or direction-wrong samples. |
| Batch Fermentation | Biomass-substrate-product dynamics | $\frac{dX}{dt}=\frac{30.87XS}{(X+121.87)(S+105.4)}$ | Biomass growth depends jointly on biomass and substrate through saturating kinetics. | Verify whether biomass-rate data satisfy the learned fermentation growth law. |
| Batch Fermentation | Substrate consumption law | $\frac{dS}{dt}=-\frac{440.99XS}{(X+121.87)(S+105.4)}$ | Substrate is consumed as biomass grows, with a rate linked to the same kinetic denominator. | Detect unphysical trajectories where substrate decreases too slowly, too fast, or inconsistently with biomass growth. |
| Batch Fermentation | Product formation law | $\frac{dP}{dt}=\frac{73.65XS}{(X+121.87)(S+105.4)}$ | Product accumulates as a coupled consequence of biomass growth and substrate conversion. | Verify whether product-generation data lie on the same kinetic manifold as biomass and substrate dynamics. |
| Microbial Growth | Monod growth law | $\mu(S)=\mu_{\max}\frac{S}{K_S+S}$ | Specific growth rate saturates with substrate concentration. | Learn whether observed growth rates follow substrate-limited biological kinetics rather than arbitrary nonlinear trends. |
| Enzyme Kinetics | Michaelis-Menten law | $v(S)=\frac{V_{\max}S}{K_M+S}$ | Enzyme-catalyzed reaction rates saturate as substrate becomes abundant. | Verify whether enzyme-rate data lie on the Michaelis-Menten kinetic manifold. |
| Population Dynamics | Logistic growth | $\frac{dX}{dt}=rX\left(1-\frac{X}{K}\right)$ | Biomass grows exponentially at low density but saturates due to carrying capacity. | Detect unphysical biomass curves that violate growth saturation constraints. |
| Bioprocess Dynamics | Biomass inhibition | $\mu(X,S)=\mu_{\max}\frac{S}{K_S+S}\left(1-\frac{X}{K_\mu+X}\right)$ | High biomass can inhibit further growth due to crowding, toxicity, or resource limitations. | Test whether M-Layer learns full inhibitory dynamics instead of only a Monod substrate shell. |
| Temperature-Dependent Kinetics | Arrhenius activation | $k(T)=A\exp\left(-\frac{E_A}{RT}\right)$ | Reaction and growth rates depend exponentially on temperature. | Verify whether temperature-dependent process data obey thermodynamic rate scaling. |
| Bioreactor Control | Chemostat biomass balance | $\dot X=(\mu(S)-D)X$ | Biomass changes according to biological growth minus dilution washout. | Learn the admissible manifold of continuous bioreactor operation under dilution control. |
| Bioreactor Control | Chemostat substrate balance | $\dot S=D(S_{\mathrm{in}}-S)-\frac{1}{Y_{X/S}}\mu(S)X$ | Substrate concentration changes due to feed, outflow, and biological consumption. | Verify whether feed-substrate-growth data are mutually consistent. |
| Fed-Batch Processing | Volume balance | $\dot V=F$ | Reactor volume increases according to the feed rate. | Detect generated fed-batch trajectories with inconsistent feed-volume dynamics. |
| Fed-Batch Processing | Dilution relation | $D=\frac{F}{V}$ | Dilution rate is determined by feed rate and reactor volume. | Verify whether control inputs and reactor states satisfy process-operating constraints. |
| Product Formation | Luedeking-Piret law | $\dot P=\alpha\mu X+\beta X-DP$ | Product formation can be growth-associated and non-growth-associated, with dilution loss in continuous systems. | Learn whether product trajectories are consistent with biomass growth and process dilution. |
| Yield Constraints | Biomass yield relation | $-\dot S=\frac{1}{Y_{X/S}}\dot X$ | Substrate consumption and biomass formation are linked by a yield coefficient. | Test whether M-Layer learns stoichiometric yield constraints rather than only fitting each variable separately. |
| Yield Constraints | Product yield relation | $\dot P=Y_{P/S}(-\dot S)$ | Product generation is constrained by substrate conversion. | Verify whether product formation is physically coupled to substrate use. |
| Metabolic Networks | Stoichiometric flux balance | $\dot c=Nv(c)$ | Metabolite concentrations evolve according to stoichiometric reaction networks. | Learn whether metabolic trajectories satisfy network-level mass-conservation constraints. |
| Metabolic Networks | Steady-state flux constraint | $Nv=0$ | At metabolic steady state, internal metabolite accumulation vanishes. | Verify whether inferred flux vectors lie in the stoichiometric null space. |
| Bioreactor Thermodynamics | Reactor energy balance | $\rho C_pV\dot T=-\Delta H_rVr+UA(T_c-T)$ | Temperature evolves due to reaction heat and heat exchange with the coolant. | Verify whether concentration and temperature trajectories obey coupled mass-energy constraints. |
| Oxygen-Limited Bioprocesses | Oxygen transfer law | $\dot C_O=k_La(C_O^*-C_O)-q_OX$ | Dissolved oxygen changes due to gas-liquid transfer and cellular uptake. | Detect oxygen trajectories that violate transfer-uptake balance. |
| Maintenance Metabolism | Pirt relation | $q_S=\frac{\mu}{Y_{X/S}}+m_S$ | Substrate uptake supports both growth and cellular maintenance. | Learn whether substrate consumption decomposes into growth-associated and maintenance-associated components. |
| Process Optimization | Productivity objective | $\mathcal{P}=\frac{P(t_f)}{t_f}$ | Bioprocess performance depends on final product concentration per unit time. | Verify whether optimized trajectories remain dynamically feasible while improving productivity. |
| Sustainable Bioprocessing | Carbon conversion efficiency | $\eta_C=\frac{\text{carbon in product}}{\text{carbon in substrate}}$ | Sustainable bioprocesses should convert substrate carbon efficiently into desired product. | Learn whether generated process designs respect both kinetic feasibility and carbon-efficiency constraints. |
| Dynamic Equation Discovery | Symbolic kinetic recovery | $\dot z=f_{\mathrm{symbolic}}(z)$ | Interpretable process models aim to recover compact closed-form kinetic laws from dynamic data. | Use M-Layer as a verifier of candidate symbolic equations learned from bioprocess time series. |
| M-Layer Bioprocess Verifier | Learned physicality score | $\Psi_\theta(z,u,\dot z)\approx 0$ if $\dot z=f(z,u)$ | A low score means the point lies on the learned biochemical process manifold. | Distinguish true bioprocess states from derivative-shuffled, norm-preserving, or yield-preserving fake samples. |
References
- 2019 - SO(8) Supergravity and the Magic of Machine Learning
- 2023 - On backpropagating Hessians through ODEs
- 2007 - A systematic approach to multiphysics extensions of finite-element-based micromagnetic simulations: Nmag, Operator-based Abstraction
Bio process
- 📍 1 2012, Analysis, Synthesis, and Design of Chemical Processes.
Lie Group, ODE, and Chaos
- 1 Georgi, Howard. Lie Algebras in Particle Physics. 2nd ed. Boca Raton: CRC Press, 2018.
- 📍 2 Hairer, Ernst, and Gerhard Wanner. Solving Ordinary Differential Equations II: Stiff and Differential-Algebraic Problems. 2nd rev. ed. Berlin: Springer, 2010.
- 3 Sussman, Gerald Jay, and Jack Wisdom. Structure and Interpretation of Classical Mechanics. 2nd ed. Cambridge, MA: MIT Press, 2015.
- 📍 4 Strogatz, Steven H. Nonlinear Dynamics and Chaos: With Applications to Physics, Biology, Chemistry, and Engineering. 2nd ed. Boulder: Westview Press, 2018. (Nonlinear Dynamics / Benchmark ODE)
- 5 Hall, Brian C. Lie Groups, Lie Algebras, and Representations: An Elementary Introduction. 2nd ed. Cham: Springer, 2015.
References 2
- 2026 - High-Dimensional Probability
- 2023 - Seeing a Rose in Five Thousand Ways
- 2025 - Visual Chronicles: Using Multimodal LLMs to Analyze Massive Collections of Images
- 2026 - Reward-Conditioned Reinforcement Learning