Notation by work
Arithmetic J-Space Training Lab
All notation · Glossary · Source coverage
22 symbol spellings in 10 mathematical passages across 3 selected source files. Subscripts and superscripts have their own entries alongside their base symbols.
The same symbol can have several meanings here. A passage classified as a definition may define another part of its expression. Read the linked context before assigning a meaning.
All 22 entries are available below.
+Use in source · 3 passages
Search aliases: +
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
=Use in source · 3 passages
Search aliases: =
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
BUse in source · 2 passages
Search aliases: B
Use in source · EXPERIMENT_DESIGN.md, line 183
G_o = E[gg^top] + λ I, B = G_c^1/2G_oG_c^1/2.
Exact mathematical passage
G_o = \mathbb{E}[gg^\top] + \lambda I, \qquad B = G_c^{1/2}G_oG_c^{1/2}.
cUse in source · 5 passages
Search aliases: c
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
\mathbb{E}Use in source · 3 passages
Search aliases: E mathbb
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
GUse in source · 6 passages
Search aliases: G
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
gUse in source · 1 passage
Search aliases: g
Use in source · EXPERIMENT_DESIGN.md, line 183
G_o = E[gg^top] + λ I, B = G_c^1/2G_oG_c^1/2.
Exact mathematical passage
G_o = \mathbb{E}[gg^\top] + \lambda I, \qquad B = G_c^{1/2}G_oG_c^{1/2}.
g^\topUse in source · 1 passage
Search aliases: g^top top
Use in source · EXPERIMENT_DESIGN.md, line 183
G_o = E[gg^top] + λ I, B = G_c^1/2G_oG_c^1/2.
Exact mathematical passage
G_o = \mathbb{E}[gg^\top] + \lambda I, \qquad B = G_c^{1/2}G_oG_c^{1/2}.
G_cUse in source · 2 passages
Search aliases: G_c
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
G_c^{1/2}Use in source · 3 passages
Search aliases: G_c^1/2
Use in source · EXPERIMENT_DESIGN.md, line 183
G_o = E[gg^top] + λ I, B = G_c^1/2G_oG_c^1/2.
Exact mathematical passage
G_o = \mathbb{E}[gg^\top] + \lambda I, \qquad B = G_c^{1/2}G_oG_c^{1/2}.
G_oUse in source · 4 passages
Search aliases: G_o
Use in source · EXPERIMENT_DESIGN.md, line 183
G_o = E[gg^top] + λ I, B = G_c^1/2G_oG_c^1/2.
Exact mathematical passage
G_o = \mathbb{E}[gg^\top] + \lambda I, \qquad B = G_c^{1/2}G_oG_c^{1/2}.
hUse in source · 3 passages
Search aliases: h
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
h^\topUse in source · 1 passage
Search aliases: h^top top
Use in source · WORKSPACE_PROTOCOL.md, line 176
G_c=E[Δ hΔ h^top]+λ I.
Exact mathematical passage
G_c=\mathbb{E}[\Delta h\Delta h^\top]+\lambda I.
h_\ellUse in source · 2 passages
Search aliases: h_ℓ ell
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
h_\ell^\topUse in source · 1 passage
Search aliases: h_ℓ^top ell top
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
IUse in source · 3 passages
Search aliases: I
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
oUse in source · 4 passages
Search aliases: o
Use in source · EXPERIMENT_DESIGN.md, line 183
G_o = E[gg^top] + λ I, B = G_c^1/2G_oG_c^1/2.
Exact mathematical passage
G_o = \mathbb{E}[gg^\top] + \lambda I, \qquad B = G_c^{1/2}G_oG_c^{1/2}.
\topUse in source · 3 passages
Search aliases: top
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
uUse in source · 1 passage
Search aliases: u
Use in source · EXPERIMENT_DESIGN.md, line 164
At upstream layer u, sealed random residual perturbations are propagated to candidate source layer ℓ. Their source-layer effects estimate
Exact mathematical passage
u
\DeltaUse in source · 2 passages
Search aliases: Δ Delta
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
\lambdaUse in source · 3 passages
Search aliases: λ lambda
Use in source · EXPERIMENT_DESIGN.md, line 167
G_c = E[Δ h_ℓΔ h_ℓ^top] + λ I.
Exact mathematical passage
G_c = \mathbb{E}[\Delta h_\ell\Delta h_\ell^\top] + \lambda I.
\ellUse in source · 3 passages
Search aliases: ℓ ell
Use in source · EXPERIMENT_DESIGN.md, line 165
At upstream layer u, sealed random residual perturbations are propagated to candidate source layer ℓ. Their source-layer effects estimate
Exact mathematical passage
\ell
Source coverage
Automatic extraction covers TeX and Markdown math delimiters and common equation environments in these selected files. It does not interpret diagrams, images, PDF text, program identifiers, or historical archives. Occurrences are navigation aids, not a proof review.
Download all entries, passages and source checksums (JSON) · Collection coverage
- experiments/arithmetic-jspace/EXPERIMENT_DESIGN.md · 6 mathematical passages
- experiments/arithmetic-jspace/README.md · 1 mathematical passage
- experiments/arithmetic-jspace/WORKSPACE_PROTOCOL.md · 3 mathematical passages