Augmented Torsion

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Naive torsion is usually where gauge covariance goes to die. GU’s transport move is to stop trying to “fix torsion” after the fact and instead define torsion as a compensated difference from the outset. The augmented torsion
$$ T := \eta - \varepsilon^{-1} d_{A_0} \varepsilon $$
is engineered so the bad (inhomogeneous) terms cancel. This gives a torsion variable that transforms adjointly and can be pulled back to $X$ without illegal moves.
Definitions / Notation used
- $\omega = (\varepsilon, \eta) \in G = H \ltimes N$, with $\eta \in \Omega^1(Y, \mathrm{ad}(P_H))$.
- $A_0$ fixed; $d_{A_0}$ is the covariant exterior derivative.
- $B_{\omega} := A_0 \cdot \varepsilon$, curvature $F_B := dB_{\omega} + B_{\omega} \wedge B_{\omega}$.
- Augmented torsion:
$$ T(\omega) := \eta - \varepsilon^{-1} d_{A_0} \varepsilon \in \Omega^1\big(Y, \mathrm{ad}(P_H)\big). $$
Main technical argument
Lemma (covariance of augmented torsion).
Under the tilted right action by $h \in H$, augmented torsion transforms adjointly:
$$ T(\omega \cdot h) = h^{-1} T(\omega) h. $$
Explicit transformation line showing cancellation
Use the tilted ($A_0$-aware) bookkeeping where the components transform as
$$ \varepsilon^\prime = \varepsilon h, \eta^\prime = h^{-1} \eta h + h^{-1} d_{A_0} h. $$
Compute:
$$ T^\prime = \eta^\prime - (\varepsilon^\prime)^{-1} d_{A_0} (\varepsilon^\prime) $$
$$ = \big(h^{-1} \eta h + h^{-1} d_{A_0} h\big) - (h^{-1} \varepsilon^{-1}) d_{A_0}(\varepsilon h) $$
$$ = h^{-1} \eta h + h^{-1} d_{A_0} h - h^{-1} \varepsilon^{-1} (d_{A_0} \varepsilon) h - h^{-1} d_{A_0} h $$
$$ = h^{-1} \big( \eta - \varepsilon^{-1} d_{A_0} \varepsilon \big) h $$
$$ = h^{-1} T h. $$
The inhomogeneous term $h^{-1} d_{A_0} h$ cancels exactly.
Geometric meaning
$T$ is the affine difference between two connection-building routes from the same $\omega$:
- translate: $A_0 + \eta$
- rotate: $B_{\omega} = A_0 \cdot \varepsilon$
Then $T$ is the “difference” in the model space $N$:
$$ T = (A_0 + \eta) - (A_0 \cdot \varepsilon), $$
which is precisely $\eta - \varepsilon^{-1} d_{A_0} \varepsilon$.
Assumptions vs Consequences
Assumptions
- $A_0$ fixed, $d_{A_0}$ used in compensators.
- Tilted $H$-action includes the inhomogeneous $h^{-1} d_{A_0} h$ term on $\eta $.
Consequences
- $T$ transforms covariantly: $T \mapsto h^{-1} T h$.
- Therefore $\iota^\ast(T)$ is well-defined on $X$.
- $B_{\omega}$ and $F_B$ are operational objects compatible with transport bookkeeping.
Why this matters
$T$ is the first transport-native torsion variable that survives gauge covariance. It is linear (lives in $N$), pullback-safe (can be observed on $X$ via $\iota^\ast$), and built to avoid “connections-aren’t-tensors” pitfalls. Later, when we build Einstein-like curvature contractions, we will not take naive Ricci traces on $\mathrm{ad}$-valued curvature; those contractions are replaced by Shiab $\bullet_{\varepsilon}$. $T$ is designed to be compatible with that gauge-aware contraction discipline.
Key takeaway
Augmented torsion is the right torsion variable because it is covariant by construction.
Technical takeaway
$T := \eta - \varepsilon^{-1} d_{A_0} \varepsilon$ transforms as $T \mapsto h^{-1} T h$ because the inhomogeneous terms cancel line-by-line.
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"content": "Naive torsion is usually where gauge covariance goes to die. GU’s transport move is to stop trying to “fix torsion” after the fact and instead define torsion as a compensated difference from the outset. The augmented torsion\n\n$$\nT := \\eta - \\varepsilon^{-1} d_{A_0} \\varepsilon\n$$\n\nis engineered so the bad (inhomogeneous) terms cancel. This gives a torsion variable that transforms adjointly and can be pulled back to $X$ without illegal moves.\n\n# Definitions / Notation used\n- $\\omega = (\\varepsilon, \\eta) \\in G = H \\ltimes N$, with $\\eta \\in \\Omega^1(Y, \\mathrm{ad}(P_H))$.\n- $A_0$ fixed; $d_{A_0}$ is the covariant exterior derivative.\n- $B_{\\omega} := A_0 \\cdot \\varepsilon$, curvature $F_B := dB_{\\omega} + B_{\\omega} \\wedge B_{\\omega}$.\n- Augmented torsion:\n\n\n$$\nT(\\omega) := \\eta - \\varepsilon^{-1} d_{A_0} \\varepsilon \\in \\Omega^1\\big(Y, \\mathrm{ad}(P_H)\\big).\n$$\n\n# Main technical argument\n**Lemma (covariance of augmented torsion).**\n\nUnder the tilted right action by $h \\in H$, augmented torsion transforms adjointly:\n\n$$\nT(\\omega \\cdot h) = h^{-1} T(\\omega) h.\n$$\n\n## Explicit transformation line showing cancellation\nUse the tilted ($A_0$-aware) bookkeeping where the components transform as\n\n$$\n\\varepsilon^\\prime = \\varepsilon h,\n\\eta^\\prime = h^{-1} \\eta h + h^{-1} d_{A_0} h.\n$$\n\nCompute:\n\n$$\nT^\\prime = \\eta^\\prime - (\\varepsilon^\\prime)^{-1} d_{A_0} (\\varepsilon^\\prime)\n$$\n\n$$\n= \\big(h^{-1} \\eta h + h^{-1} d_{A_0} h\\big) - (h^{-1} \\varepsilon^{-1}) d_{A_0}(\\varepsilon h)\n$$\n\n$$\n= h^{-1} \\eta h + h^{-1} d_{A_0} h - h^{-1} \\varepsilon^{-1} (d_{A_0} \\varepsilon) h - h^{-1} d_{A_0} h\n$$\n\n$$\n= h^{-1} \\big( \\eta - \\varepsilon^{-1} d_{A_0} \\varepsilon \\big) h\n$$\n\n$$\n= h^{-1} T h.\n$$\n\nThe inhomogeneous term $h^{-1} d_{A_0} h$ cancels exactly.\n\n# Geometric meaning\n$T$ is the affine difference between two connection-building routes from the same $\\omega$:\n- translate: $A_0 + \\eta$\n- rotate: $B_{\\omega} = A_0 \\cdot \\varepsilon$\n\n\nThen $T$ is the “difference” in the model space $N$:\n\n$$\nT = (A_0 + \\eta) - (A_0 \\cdot \\varepsilon),\n$$\n\nwhich is precisely $\\eta - \\varepsilon^{-1} d_{A_0} \\varepsilon$.\n\n# Assumptions vs Consequences\n## Assumptions\n- $A_0$ fixed, $d_{A_0}$ used in compensators.\n- Tilted $H$-action includes the inhomogeneous $h^{-1} d_{A_0} h$ term on $\\eta $.\n\n\n## Consequences\n- $T$ transforms covariantly: $T \\mapsto h^{-1} T h$.\n- Therefore $\\iota^\\ast(T)$ is well-defined on $X$.\n- $B_{\\omega}$ and $F_B$ are operational objects compatible with transport bookkeeping.\n\n\n# Why this matters\n$T$ is the first transport-native torsion variable that survives gauge covariance. It is linear (lives in $N$), pullback-safe (can be observed on $X$ via $\\iota^\\ast$), and built to avoid “connections-aren’t-tensors” pitfalls. Later, when we build Einstein-like curvature contractions, we will not take naive Ricci traces on $\\mathrm{ad}$-valued curvature; those contractions are replaced by Shiab $\\bullet_{\\varepsilon}$. $T$ is designed to be compatible with that gauge-aware contraction discipline.\n\n\n# Key takeaway\nAugmented torsion is the right torsion variable because it is covariant by construction.\n\n# Technical takeaway\n$T := \\eta - \\varepsilon^{-1} d_{A_0} \\varepsilon$ transforms as $T \\mapsto h^{-1} T h$ because the inhomogeneous terms cancel line-by-line.",
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