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[GH-ISSUE #5489] [BUG]: thinking model goes outside bounds on 1.12.1 #5119

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opened 2026-06-05 14:52:06 -04:00 by yindo · 4 comments
yindo commented 2026-06-05 14:52:06 -04:00
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Originally created by @Anto79-ops on GitHub (Apr 23, 2026).
Original GitHub issue: https://github.com/Mintplex-Labs/anything-llm/issues/5489

Originally assigned to: @timothycarambat on GitHub.

How are you running AnythingLLM?

Docker (local)

What happened?

Hello,

Using AnythingLLM 1.12.1 on Docker using Ollama and Gemma4, and I noticed that the thinking text goes outside the box bounds.

Please see photo.

Image

Are there known steps to reproduce?

No response

LLM Provider & Model (if applicable)

Ollama Gemma4

Embedder Provider & Model (if applicable)

No response

Originally created by @Anto79-ops on GitHub (Apr 23, 2026). Original GitHub issue: https://github.com/Mintplex-Labs/anything-llm/issues/5489 Originally assigned to: @timothycarambat on GitHub. ### How are you running AnythingLLM? Docker (local) ### What happened? Hello, Using AnythingLLM 1.12.1 on Docker using Ollama and Gemma4, and I noticed that the thinking text goes outside the box bounds. Please see photo. <img width="1017" height="415" alt="Image" src="https://github.com/user-attachments/assets/cebb49a0-bf8d-4dfc-a25c-b39f36f67fd8" /> ### Are there known steps to reproduce? _No response_ ### LLM Provider & Model (if applicable) Ollama Gemma4 ### Embedder Provider & Model (if applicable) _No response_
yindo added the bugUI/UXneeds info / can't replicate labels 2026-06-05 14:52:06 -04:00
yindo closed this issue 2026-06-05 14:52:06 -04:00
yindo commented 2026-06-05 14:52:07 -04:00
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@timothycarambat commented on GitHub (Apr 23, 2026):

@Anto79-ops Can you please copy paste the actual response you got here (assuming nothing is proprietary) I am using Ollama + Gemma4 and I cannot for the life of me replicate this - must be something specific in the output doing this.

<!-- gh-comment-id:4307072537 --> @timothycarambat commented on GitHub (Apr 23, 2026): @Anto79-ops Can you please copy paste the actual response you got here (assuming nothing is proprietary) I am using Ollama + Gemma4 and *I cannot for the life of me* replicate this - must be something specific in the output doing this.
yindo commented 2026-06-05 14:52:07 -04:00
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@Anto79-ops commented on GitHub (Apr 23, 2026):

sure, nothing propeitary, but I asked it this question:

"hello create a power point presentation on the kohn sham equation" what came out was below:

I also logged into another computer and logged into where AnythingLLM is hosted, and the other computer also showed the same out of bounds problem (See screenshot).

Image

Full responce below:

Create a PowerPoint presentation on the Kohn-Sham equations. The user wants a structured outline/content for a PowerPoint presentation. The Kohn-Sham equations (Density Functional Theory - DFT).

*   *Introduction:* What is DFT? Why do we need it? (The many-body problem).
*   *The Core Concept:* Hohenberg-Kohn theorems (Density as the fundamental variable).
*   *The Problem with HK:* The unknown functional (Exchange-Correlation).
*   *The Kohn-Sham Approach:* Mapping the interacting system to a non-interacting system.
*   *The Equations:* The actual KS equations (effective potential, kinetic energy, etc.).
*   *The Components:* Kinetic energy, External potential, Hartree potential, Exchange-Correlation potential.
*   *The Self-Consistent Field (SCF) Method:* How to solve it (iterative process).
*   *Applications/Limitations:* Where it's used (chemistry, physics, materials science) and what's missing (self-interaction error, dispersion).
*   *Conclusion:* Summary.

*   *Slide 1: Title Slide*
    *   Title: The Kohn-Sham Equations
    *   Subtitle: Foundations of Density Functional Theory (DFT)

*   *Slide 2: Introduction - The Many-Body Problem*
    *   Problem: Solving the Schrödinger equation for $N$ interacting electrons.
    *   Complexity: Exponential scaling with $N$.
    *   Goal: Find a way to simplify the problem without losing accuracy.

*   *Slide 3: The Hohenberg-Kohn Theorems*
    *   Theorem 1: The ground-state density $\rho(\mathbf{r})$ uniquely determines the external potential and thus the entire Hamiltonian.
    *   Theorem 2: The energy is a functional of the density, and the true density minimizes this energy functional.
    *   *Crucial point:* We moved from $\Psi$ (wavefunction) to $\rho$ (density).

*   *Slide 4: The Challenge - The Unknown Functional*
    *   Even though we know $E[\rho]$ exists, we don't know the exact form of the functional, especially the Exchange-Correlation ($E_{xc}$) part.
    *   The "Many-Body" difficulty remains hidden in $E_{xc}$.

*   *Slide 5: The Kohn-Sham Strategy*
    *   The "Trick": Map the complex system of *interacting* electrons onto a system of *non-interacting* electrons.
    *   Requirement: The non-interacting system must yield the *same* ground-state density $\rho(\mathbf{r})$ as the interacting system.
    *   This allows us to calculate the kinetic energy exactly for non-interacting particles.

*   *Slide 6: The Kohn-Sham Equations*
    *   The single-particle equation:
        $\left[ -\frac{1}{2}\nabla^2 + v_{eff}(\mathbf{r}) \right] \phi_i(\mathbf{r}) = \epsilon_i \phi_i(\mathbf{r})$
    *   Where the density is: $\rho(\mathbf{r}) = \sum_{i} |\phi_i(\mathbf{r})|^2$
    *   $v_{eff}$ is the effective potential.

*   *Slide 7: The Effective Potential ($v_{eff}$)*
    *   $v_{eff}(\mathbf{r}) = v_{ext}(\mathbf{r}) + v_{H}(\mathbf{r}) + v_{xc}(\mathbf{r})$
    *   $v_{ext}$: Nuclei-electron interaction.
    *   $v_{H}$ (Hartree Potential): Classical electron-electron repulsion.
    *   $v_{xc}$ (Exchange-Correlation Potential): The "everything else" term (quantum effects).

*   *Slide 8: The Self-Consistent Field (SCF) Method*
    *   The problem: $v_{eff}$ depends on $\rho$, but $\rho$ depends on the orbitals $\phi_i$, which are solutions to the equation containing $v_{eff}$.
    *   The Solution: Iterative loop.
        1. Guess initial $\rho$.
        2. Calculate $v_{eff}$.
        3. Solve KS equations for $\phi_i$.
        4. Compute new $\rho$.
        5. Check for convergence. If not converged, repeat.

*   *Slide 9: Applications and Impact*
    *   Computational Chemistry (molecular properties).
    *   Solid State Physics (band structures, lattice constants).
    *   Materials Science (new battery materials, catalysts).
    *   The "Workhorse" of modern quantum simulations.

*   *Slide 10: Limitations and Future Directions*
    *   Self-interaction error.
    *   Difficulty with Van der Waals (dispersion) forces.
    *   Strongly correlated systems.
    *   Development of more accurate functionals (Hybrid functionals, Meta-GGAs).

*   *Slide 11: Conclusion*
    *   Summary of the KS approach.
    *   The bridge between quantum reality and computational feasibility.

*   Check for clarity and technical accuracy.
*   Ensure the tone is professional.
*   Organize into a clear "Slide-by-Slide" format.
Since I am an-AI text model, I cannot generate a .pptx file directly, but I can provide you with a complete, professional slide-by-slide outline. You can copy and paste this content directly into PowerPoint.

Presentation Title: The Kohn-Sham Equations
Subtitle: The Foundation of Modern Density Functional Theory (DFT) Presenter Name: [Your Name]

Slide 1: Introduction – The Many-Body Problem
The Challenge: Solving the Schrödinger equation for a system of 
N
N interacting electrons.
The Complexity:
The wavefunction 
Ψ
(
r
1
,
r
2
,
.
.
.
,
r
N
)
Ψ(r
​1
​​ ,r
​2
​​ ,...,r
​N
​​ ) depends on 
3
N
3N variables.
Electron-electron repulsion (Coulomb interaction) makes the equation non-separable.
Computational cost scales exponentially with the number of electrons.
The Goal: Find a way to simplify the many-body problem without losing the essential physics.
Slide 2: The Hohenberg-Kohn Theorems (The Foundation)
Before Kohn-Sham, we need the Hohenberg-Kohn (HK) theorems (1964):

Theorem 1 (Existence): The ground-state electron density 
ρ
(
r
)
ρ(r) uniquely determines the external potential 
v
e
x
t
(
r
)
v
​ext
​​ (r) and thus all properties of the system.
Theorem 2 (Variational Principle): There exists a universal functional of the density, 
E
[
ρ
]
E[ρ], such that the global minimum of this functional is the true ground-state energy.
The Catch: While we know a functional exists, the HK theorems do not tell us what the functional is.
Slide 3: The Kohn-Sham Strategy (The “Big Idea”)
The Problem with HK: The kinetic energy of interacting electrons is extremely difficult to calculate directly from density.
The Solution (1965): Map the complex system of interacting electrons onto a simpler system of non-interacting electrons.
The Constraint: The non-interacting system must be constructed such that it yields the exact same ground-state density 
ρ
(
r
)
ρ(r) as the real, interacting system.
Result: This allows us to treat the kinetic energy exactly (as a single-particle problem) and relegate the complex interactions to a small “correction” term.
Slide 4: The Kohn-Sham Equations
The core mathematical formulation:

We solve a set of single-particle Schrödinger-like equations:
[
−
1
2
ϕ
i
∇
2
+
v
e
f
f
(
r
)
]
ϕ
i
(
r
)
=
ϵ
i
ϕ
i
(
r
)
[−
​2
​
​1
​​ ϕ
​i
​​ ∇
​2
​​ +v
​eff
​​ (r)]ϕ
​i
​​ (r)=ϵ
​i
​​ ϕ
​i
​​ (r)

Where:
ϕ
i
(
r
)
ϕ
​i
​​ (r) are the Kohn-Sham orbitals.
ϵ
i
ϵ
​i
​​  are the orbital energies.
The total density is reconstructed from the orbitals: \rho(\mathbfroll) = \sum_{i=1}^{N} |\phi_i(\mathbf{r})|^2.
Slide 5: The Effective Potential (
v
e
f
f
v
​eff
​​ )
The “magic” happens in the effective potential, which is split into three parts:

v
e
f
f
(
r
)
=
v
e
x
t
(
r
)
+
v
H
(
r
)
+
v
x
c
(
r
)
v
​eff
​​ (r)=v
​ext
​​ (r)+v
​H
​​ (r)+v
​xc
​​ (r)

v
e
x
t
(
r
)
v
​ext
​​ (r) (External Potential): Interaction between electrons and nuclei.
v
H
(
r
)
v
​H
​​ (r) (Hartree Potential): The classical electrostatic repulsion between the electron density and itself.
v
x
c
(
r
)
v
​xc
​​ (r) (Exchange-Correlation Potential): The “everything else” term. It contains all the complex quantum mechanical effects (Pauli exclusion principle and electron correlation).
Slide 6: The Exchange-Correlation (
E
x
c
E
​xc
​​ ) Term
This is the only part of the functional that must be approximated.

Exchange (
E
x
E
​x
​​ ): Accounts for the Pauli Exclusion Principle (electrons of the same spin avoid each other).
Correlation (
E
c
E
​c
​​ ): Accounts for the dynamical avoidance of electrons due to Coulomb repulsion.
Common Approximations:
LDA (Local Density Approximation): Depends only on the density at a specific point.
GGA (Generalized Gradient Approximation): Depends on the density and its gradient (e.g., PBE functional).
Hybrid Functionals: Incorporate a portion of exact exchange from Hartree-Fock theory (e.g., B3LYP).
Slide 7: The Self-Consistent Field (SCF) Method
The KS equations cannot be solved in one step because 
v
e
f
f
v
​eff
​​  depends on 
ρ
ρ, and 
ρ
ρ depends on the solution to the equation. The Iterative Loop:

Guess: Start with an initial trial density 
ρ
i
n
i
t
i
a
l
ρ
​initial
​​ .
Construct: Calculate 
v
e
f
f
v
​eff
​​  using the current density.
Solve: Solve the KS equations to find new orbitals 
ϕ
i
ϕ
​i
​​ .
Update: Calculate a new density 
ρ
n
e
w
ρ
​new
​​  from the new orbitals.
Check Convergence: Is 
ρ
n
e
w
≈
ρ
o
l
d
ρ
​new
​​ ≈ρ
​old
​​ ?
No: Use 
ρ
n
e
w
ρ
​new
​​  to repeat the loop.
Yes: The system has reached “Self-Consistency.”
Slide 8: Summary and Applications
Summary:
Kohn-Sham equations transformed DFT from a theoretical concept into a practical computational tool.
They replaced the 
3
N
3N-dimensional wavefunction problem with a 3-dimensional density problem.
Applications:
Materials Science: Predicting crystal structures and band gaps.
Chemistry: Calculating molecular geometries and reaction energies.
Nanotechnology: Designing new catalysts and semiconductor devices.
Drug Discovery: Modeling protein-ligand interactions.
Slide 9: Limitations and Future Frontiers
Current Challenges:
Self-Interaction Error: Electrons “seeing” themselves in the Hartree potential.
Van der Waals Forces: Standard functionals struggle with long-range dispersion.
Strongly Correlated Systems: Systems where the 
E
x
c
E
​xc
​​  approximation fails (e.g., transition metal oxides).
The Future:
Development of “Machine Learning” functionals.
Higher-accuracy Meta-GGAs.
Integrating DFT with many-body perturbation theory (GW approximation).
Slide 10: Q&A
Thank You!
Questions?
Pro-Tips for your Presentation:
Visuals: On Slide 1, add a graphic of a complex cloud of electrons. On Slide 7, use a flowchart to show the “loop” of the SCF method.
Equations: If using PowerPoint, use the “Insert > Equation” tool to make the math look professional.
Analogy: When explaining the Kohn-Sham “trick” (Slide 3), use the analogy of “Replacing a crowded, chaotic room of people (interacting electrons) with a room of ghosts (non-interacting) that move in a way that creates the same crowd density.”
<!-- gh-comment-id:4307284125 --> @Anto79-ops commented on GitHub (Apr 23, 2026): sure, nothing propeitary, but I asked it this question: "hello create a power point presentation on the kohn sham equation" what came out was below: I also logged into another computer and logged into where AnythingLLM is hosted, and the other computer also showed the same out of bounds problem (See screenshot). <img width="1149" height="596" alt="Image" src="https://github.com/user-attachments/assets/22757ca7-8900-4937-acfd-bbd18e146577" /> Full responce below: ``` Create a PowerPoint presentation on the Kohn-Sham equations. The user wants a structured outline/content for a PowerPoint presentation. The Kohn-Sham equations (Density Functional Theory - DFT). * *Introduction:* What is DFT? Why do we need it? (The many-body problem). * *The Core Concept:* Hohenberg-Kohn theorems (Density as the fundamental variable). * *The Problem with HK:* The unknown functional (Exchange-Correlation). * *The Kohn-Sham Approach:* Mapping the interacting system to a non-interacting system. * *The Equations:* The actual KS equations (effective potential, kinetic energy, etc.). * *The Components:* Kinetic energy, External potential, Hartree potential, Exchange-Correlation potential. * *The Self-Consistent Field (SCF) Method:* How to solve it (iterative process). * *Applications/Limitations:* Where it's used (chemistry, physics, materials science) and what's missing (self-interaction error, dispersion). * *Conclusion:* Summary. * *Slide 1: Title Slide* * Title: The Kohn-Sham Equations * Subtitle: Foundations of Density Functional Theory (DFT) * *Slide 2: Introduction - The Many-Body Problem* * Problem: Solving the Schrödinger equation for $N$ interacting electrons. * Complexity: Exponential scaling with $N$. * Goal: Find a way to simplify the problem without losing accuracy. * *Slide 3: The Hohenberg-Kohn Theorems* * Theorem 1: The ground-state density $\rho(\mathbf{r})$ uniquely determines the external potential and thus the entire Hamiltonian. * Theorem 2: The energy is a functional of the density, and the true density minimizes this energy functional. * *Crucial point:* We moved from $\Psi$ (wavefunction) to $\rho$ (density). * *Slide 4: The Challenge - The Unknown Functional* * Even though we know $E[\rho]$ exists, we don't know the exact form of the functional, especially the Exchange-Correlation ($E_{xc}$) part. * The "Many-Body" difficulty remains hidden in $E_{xc}$. * *Slide 5: The Kohn-Sham Strategy* * The "Trick": Map the complex system of *interacting* electrons onto a system of *non-interacting* electrons. * Requirement: The non-interacting system must yield the *same* ground-state density $\rho(\mathbf{r})$ as the interacting system. * This allows us to calculate the kinetic energy exactly for non-interacting particles. * *Slide 6: The Kohn-Sham Equations* * The single-particle equation: $\left[ -\frac{1}{2}\nabla^2 + v_{eff}(\mathbf{r}) \right] \phi_i(\mathbf{r}) = \epsilon_i \phi_i(\mathbf{r})$ * Where the density is: $\rho(\mathbf{r}) = \sum_{i} |\phi_i(\mathbf{r})|^2$ * $v_{eff}$ is the effective potential. * *Slide 7: The Effective Potential ($v_{eff}$)* * $v_{eff}(\mathbf{r}) = v_{ext}(\mathbf{r}) + v_{H}(\mathbf{r}) + v_{xc}(\mathbf{r})$ * $v_{ext}$: Nuclei-electron interaction. * $v_{H}$ (Hartree Potential): Classical electron-electron repulsion. * $v_{xc}$ (Exchange-Correlation Potential): The "everything else" term (quantum effects). * *Slide 8: The Self-Consistent Field (SCF) Method* * The problem: $v_{eff}$ depends on $\rho$, but $\rho$ depends on the orbitals $\phi_i$, which are solutions to the equation containing $v_{eff}$. * The Solution: Iterative loop. 1. Guess initial $\rho$. 2. Calculate $v_{eff}$. 3. Solve KS equations for $\phi_i$. 4. Compute new $\rho$. 5. Check for convergence. If not converged, repeat. * *Slide 9: Applications and Impact* * Computational Chemistry (molecular properties). * Solid State Physics (band structures, lattice constants). * Materials Science (new battery materials, catalysts). * The "Workhorse" of modern quantum simulations. * *Slide 10: Limitations and Future Directions* * Self-interaction error. * Difficulty with Van der Waals (dispersion) forces. * Strongly correlated systems. * Development of more accurate functionals (Hybrid functionals, Meta-GGAs). * *Slide 11: Conclusion* * Summary of the KS approach. * The bridge between quantum reality and computational feasibility. * Check for clarity and technical accuracy. * Ensure the tone is professional. * Organize into a clear "Slide-by-Slide" format. Since I am an-AI text model, I cannot generate a .pptx file directly, but I can provide you with a complete, professional slide-by-slide outline. You can copy and paste this content directly into PowerPoint. Presentation Title: The Kohn-Sham Equations Subtitle: The Foundation of Modern Density Functional Theory (DFT) Presenter Name: [Your Name] Slide 1: Introduction – The Many-Body Problem The Challenge: Solving the Schrödinger equation for a system of N N interacting electrons. The Complexity: The wavefunction Ψ ( r 1 , r 2 , . . . , r N ) Ψ(r ​1 ​​ ,r ​2 ​​ ,...,r ​N ​​ ) depends on 3 N 3N variables. Electron-electron repulsion (Coulomb interaction) makes the equation non-separable. Computational cost scales exponentially with the number of electrons. The Goal: Find a way to simplify the many-body problem without losing the essential physics. Slide 2: The Hohenberg-Kohn Theorems (The Foundation) Before Kohn-Sham, we need the Hohenberg-Kohn (HK) theorems (1964): Theorem 1 (Existence): The ground-state electron density ρ ( r ) ρ(r) uniquely determines the external potential v e x t ( r ) v ​ext ​​ (r) and thus all properties of the system. Theorem 2 (Variational Principle): There exists a universal functional of the density, E [ ρ ] E[ρ], such that the global minimum of this functional is the true ground-state energy. The Catch: While we know a functional exists, the HK theorems do not tell us what the functional is. Slide 3: The Kohn-Sham Strategy (The “Big Idea”) The Problem with HK: The kinetic energy of interacting electrons is extremely difficult to calculate directly from density. The Solution (1965): Map the complex system of interacting electrons onto a simpler system of non-interacting electrons. The Constraint: The non-interacting system must be constructed such that it yields the exact same ground-state density ρ ( r ) ρ(r) as the real, interacting system. Result: This allows us to treat the kinetic energy exactly (as a single-particle problem) and relegate the complex interactions to a small “correction” term. Slide 4: The Kohn-Sham Equations The core mathematical formulation: We solve a set of single-particle Schrödinger-like equations: [ − 1 2 ϕ i ∇ 2 + v e f f ( r ) ] ϕ i ( r ) = ϵ i ϕ i ( r ) [− ​2 ​ ​1 ​​ ϕ ​i ​​ ∇ ​2 ​​ +v ​eff ​​ (r)]ϕ ​i ​​ (r)=ϵ ​i ​​ ϕ ​i ​​ (r) Where: ϕ i ( r ) ϕ ​i ​​ (r) are the Kohn-Sham orbitals. ϵ i ϵ ​i ​​ are the orbital energies. The total density is reconstructed from the orbitals: \rho(\mathbfroll) = \sum_{i=1}^{N} |\phi_i(\mathbf{r})|^2. Slide 5: The Effective Potential ( v e f f v ​eff ​​ ) The “magic” happens in the effective potential, which is split into three parts: v e f f ( r ) = v e x t ( r ) + v H ( r ) + v x c ( r ) v ​eff ​​ (r)=v ​ext ​​ (r)+v ​H ​​ (r)+v ​xc ​​ (r) v e x t ( r ) v ​ext ​​ (r) (External Potential): Interaction between electrons and nuclei. v H ( r ) v ​H ​​ (r) (Hartree Potential): The classical electrostatic repulsion between the electron density and itself. v x c ( r ) v ​xc ​​ (r) (Exchange-Correlation Potential): The “everything else” term. It contains all the complex quantum mechanical effects (Pauli exclusion principle and electron correlation). Slide 6: The Exchange-Correlation ( E x c E ​xc ​​ ) Term This is the only part of the functional that must be approximated. Exchange ( E x E ​x ​​ ): Accounts for the Pauli Exclusion Principle (electrons of the same spin avoid each other). Correlation ( E c E ​c ​​ ): Accounts for the dynamical avoidance of electrons due to Coulomb repulsion. Common Approximations: LDA (Local Density Approximation): Depends only on the density at a specific point. GGA (Generalized Gradient Approximation): Depends on the density and its gradient (e.g., PBE functional). Hybrid Functionals: Incorporate a portion of exact exchange from Hartree-Fock theory (e.g., B3LYP). Slide 7: The Self-Consistent Field (SCF) Method The KS equations cannot be solved in one step because v e f f v ​eff ​​ depends on ρ ρ, and ρ ρ depends on the solution to the equation. The Iterative Loop: Guess: Start with an initial trial density ρ i n i t i a l ρ ​initial ​​ . Construct: Calculate v e f f v ​eff ​​ using the current density. Solve: Solve the KS equations to find new orbitals ϕ i ϕ ​i ​​ . Update: Calculate a new density ρ n e w ρ ​new ​​ from the new orbitals. Check Convergence: Is ρ n e w ≈ ρ o l d ρ ​new ​​ ≈ρ ​old ​​ ? No: Use ρ n e w ρ ​new ​​ to repeat the loop. Yes: The system has reached “Self-Consistency.” Slide 8: Summary and Applications Summary: Kohn-Sham equations transformed DFT from a theoretical concept into a practical computational tool. They replaced the 3 N 3N-dimensional wavefunction problem with a 3-dimensional density problem. Applications: Materials Science: Predicting crystal structures and band gaps. Chemistry: Calculating molecular geometries and reaction energies. Nanotechnology: Designing new catalysts and semiconductor devices. Drug Discovery: Modeling protein-ligand interactions. Slide 9: Limitations and Future Frontiers Current Challenges: Self-Interaction Error: Electrons “seeing” themselves in the Hartree potential. Van der Waals Forces: Standard functionals struggle with long-range dispersion. Strongly Correlated Systems: Systems where the E x c E ​xc ​​ approximation fails (e.g., transition metal oxides). The Future: Development of “Machine Learning” functionals. Higher-accuracy Meta-GGAs. Integrating DFT with many-body perturbation theory (GW approximation). Slide 10: Q&A Thank You! Questions? Pro-Tips for your Presentation: Visuals: On Slide 1, add a graphic of a complex cloud of electrons. On Slide 7, use a flowchart to show the “loop” of the SCF method. Equations: If using PowerPoint, use the “Insert > Equation” tool to make the math look professional. Analogy: When explaining the Kohn-Sham “trick” (Slide 3), use the analogy of “Replacing a crowded, chaotic room of people (interacting electrons) with a room of ghosts (non-interacting) that move in a way that creates the same crowd density.” ```
yindo commented 2026-06-05 14:52:07 -04:00
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@angelplusultra commented on GitHub (Apr 23, 2026):

@Anto79-ops Closing this for now as we can't reproduce this bug.

<!-- gh-comment-id:4308568311 --> @angelplusultra commented on GitHub (Apr 23, 2026): @Anto79-ops Closing this for now as we can't reproduce this bug.
yindo commented 2026-06-05 14:52:07 -04:00
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@Anto79-ops commented on GitHub (Apr 23, 2026):

Okay sounds good it may have been just a one-off on that particular workspace.

It doesn't seem to do it with agent mode.

<!-- gh-comment-id:4308610323 --> @Anto79-ops commented on GitHub (Apr 23, 2026): Okay sounds good it may have been just a one-off on that particular workspace. It doesn't seem to do it with agent mode.
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Reference: Mintplex-Labs/anything-llm#5119
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