Scalar chain for the diagonal add-in-u transfer #
This module contains the selected and diagonal Q₀--Q₄ scalar chains used for the
projection-simplified diagonal add-in-u transfer, together with the endpoint
identifications needed by the helper strong-self-consistency proof.
References #
references/ldt-paper/self_improvement.texlines 247--252blueprint/src/chapter/ch07_self_improvement.tex
Scalar chain for the projection-simplified diagonal add-in-u transfer #
Strong self-consistency for the point measurement, pulled back to the second
coordinate of the independent (u, v) average used by the add-in-u scalar
chain.
This is the distributional self-consistency input for the A^v_{h(v)} moves in
self_improvement.tex, lines 255--297: the point measurement sampled at v
has the same 2δ left/right state-dependent distance after the product average
over (u, v).
The grouped tensor mass over a fiber h(v)=a is a contraction.
This is the submeasurement bound used inside the first Cauchy--Schwarz square
root in self_improvement.tex, lines 267--272: after grouping by the value
a = h(v), the selected operators
H^u_h ⊗ T_h are dominated by the total mass of the sandwiched polynomial
submeasurement at u, hence by I.
Selection-parametrized add-in-u scalar chain #
The paper proves lem:add-in-u for an arbitrary outcome family M and
selection S_u ⊆ 𝒪 × polyfunc. The diagonal helper strong-self-consistency
application below is one specialization of this statement. The following
definitions record the same five scalar quantities before specializing to the
diagonal case, so that the off-diagonal point-consistency selection can reuse
the Cauchy--Schwarz chain rather than restating the transfer hypothesis.
The selected-chain left endpoint Q₀.
For a selected pair (o, h) ∈ S_u, this is the expectation of
M^u_o ⊗ H^v_h, where H^v_h = A^v_{h(v)} T_h A^v_{h(v)}.
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Instances For
The selected-chain scalar Q₁, after moving the right point projector
A^v_{h(v)} to the left tensor factor once.
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The selected-chain scalar Q₂, after moving both right point projectors to
the left tensor factor.
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The selected-chain scalar Q₃, after replacing the first point projector
at v by the corresponding point projector at u.
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The selected-chain scalar Q₄, after replacing both point projectors at
v by the corresponding point projectors at u.
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The selected-chain endpoint Q₀ is the generic add-in-u left quantity when
the second measurement is the averaged sandwiched polynomial submeasurement.
The selected-chain endpoint Q₄ is the generic add-in-u right quantity.
The expanded left endpoint Q₀ of the four-step scalar chain in
self_improvement.tex, lines 247--252, after setting M^u = H^u and averaging
the second tensor factor H = E_v H^v.
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Instances For
The scalar Q₁ obtained from Q₀ by moving the right point projection
A^v_{h(v)} to the left tensor factor; this is the target of
eq:move-one.
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Instances For
The scalar Q₂ obtained from Q₁ by moving the second right point
projection to the left tensor factor; this is the target of eq:move-another.
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The scalar Q₃ obtained from Q₂ by replacing the first point projection
A^v_{h(v)} by A^u_{h(u)}; this is the target of eq:change-one.
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The scalar Q₄ obtained from Q₃ by replacing the second point projection
A^v_{h(v)} by A^u_{h(u)}; after the projection collapse, this is the
projection-simplified right endpoint of the diagonal add-in-u transfer.
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The expanded chain endpoint Q₀ is the existing diagonal match-mass left
side used by selfConsistencyDiagonalAddInU_of_simplifiedTransfer.
The raw chain endpoint Q₄ collapses to the projection-simplified scalar
right side used by selfConsistencyDiagonalAddInU_of_simplifiedTransfer.