The LPD truncation error of a layered Trotter circuit, in Pauli norm #
This file assembles the norm-level truncation-error bound for a Trotter step made of Γ
disjoint-support layers of Pauli rotations, with truncation to Pauli weight at most w* at the
end of every step. The main result is pauliNorm_layerStep_error_le_model_of_source_regime: for
a k_o-local observable O and r Trotter steps in the paper's parameter regime,
‖U^r(O) - O_r‖ ≤ (t / t₀)^(m+1) · (e (m+1))^(k_o / (k_h - 1)) · ‖O‖,
where ‖·‖ is the normalized Pauli 2-norm pauliNorm, U is the untruncated step
(layerBlockEnd), O_r is the LPD output (layerStepTraj), the cutoff is
w* = rungWeight ko kh (m + 1) = k_o + m (k_h - 1), and t₀ = 1 / (2 Γ (k_h - 1) α) is
tZeroModel Γ k_h α. This is the Pauli-norm counterpart of apd:thm:one_step_truncation_error
with the time condition apd:eq:time_condition.
Main definitions #
layerBlockTraj: the untruncated evolution through the firstilayers of a block.layerStepTraj: the LPD recurrence: a whole block ofΓlayers, then the weight cut.layerScheduledTraj: the same execution indexed by layers, as alayerTrajwith the scheduletrotterSchedule Γ wstar. Here the schedule counts layers, not individual rotations.discardedLayerStep: the discarded operatorX_{d+1}ofapd:eq:step_component.layerStepMass: the high-weight norm inside a step, before the cut.layerBlockEnd: one block as an additive endomorphism; its powers are the untruncated evolution.
Main results #
layerScheduledTraj_at_boundary: the layer-indexed and the step-indexed executions agree at step boundaries.pauliNorm_discardedLayerStep:‖X_{d+1}‖is the high-weight norm of the operator before the cut.layerStepMass_reset,layerStepMass_inflow: the two hypotheses ofMultiLadder.sum_block_inflow_le, proved for the Pauli model.sum_pauliNorm_discardedLayerStep_le_chain: the shifted-chain bound on∑_d ‖Õ^{(d)}_{≥w*+1}‖ofapd:eq:total_high_weight_norm.layerStep_telescoping,pauliNorm_layerStep_error_le: the telescoping identity and the norm-level triangle bound ofapd:thm:triangle, for layered steps.sum_pauliNorm_discardedLayerStep_le_cZero,pauliNorm_layerStep_error_le_cZero: the bound with the constantc₀ofapd:eq:c0.source_entry_inflation_le_one,source_beta_le_half: the paper's step-count condition gives4eβ ≤ 1andβ ≤ 1/2.pauliNorm_layerStep_error_le_model,pauliNorm_layerStep_error_le_model_of_source_regime: the final bound with the thresholdtZeroModel.
Implementation notes #
The discarded operator Õ^{(d)}_{≥w*+1} lives at a step boundary, and its norm is the high-weight
norm of
the operator before the cut. The kept trajectory, whose rung masses pauliMultiLadder
controls, has no mass above the cutoff right after a boundary. The bridge is layerStepMass:
within a step it starts from zero (layerStepMass_reset) and grows by the multi-jump inflow from
the lower rungs of the kept trajectory (layerStepMass_inflow). With these two facts,
MultiLadder.sum_block_inflow_le bounds ∑_d ‖Õ^{(d)}_{≥w*+1}‖ by the shifted-chain sum of
apd:eq:total_high_weight_norm, and MultiLadder.sum_block_epsJump_le_cZero by the c₀ form.
layerStepTraj and layerScheduledTraj are defined independently, and their agreement at step
boundaries is a theorem. Every hypothesis of the final theorems concerns the circuit (layer
structure, Hermiticity, sine bound), the observable (locality) or the parameters
(Admissible, 1 ≤ m, 5 ≤ r, the step-count condition); no recurrence, reset or intermediate
bound is assumed.
All bounds are in the normalized Pauli 2-norm. Expectation values in a state, and the comparison of the Trotter circuit with the Hamiltonian evolution, are not treated here.
In the paper's parameter regime, the step-count condition r ≥ 8e² w₂ A together with
a ≤ A / r gives B = 4eβ ≤ 1, where β = 2e w₂ a (apd:eq:multijump_factor; apd:eq:c0;
apd:thm:one_step_truncation_error). This is the hypothesis B ≤ 1 of cZero_le_two. The
proof multiplies through by r; no division by a occurs.
In the paper's parameter regime, the same step-count condition gives β ≤ 1/2, the regime
of the entry-factor bound entryFactor_le
(apd:eq:multijump_factor; apd:eq:entry_bound).
The untruncated evolution through the first i layers of a fixed block, as used to define
Õ^{(d)}_{≥w*+1} in apd:eq:step_component.
Equations
- Lean4LPD.PauliString.layerBlockTraj layers O 0 = O
- Lean4LPD.PauliString.layerBlockTraj layers O i.succ = Lean4LPD.PauliString.layerConj (layers i) (Lean4LPD.PauliString.layerBlockTraj layers O i)
Instances For
The LPD recurrence: evolve through a whole block of Γ layers, then keep Pauli weights at
most wstar. This is the recurrence of the kept operator in apd:eq:step_component. It is
defined directly, not as a subsequence of layerScheduledTraj.
Equations
- One or more equations did not get rendered due to their size.
- Lean4LPD.PauliString.layerStepTraj layers Γ wstar O 0 = O
Instances For
One complete step: evolve through the block, then cut (apd:eq:step_component).
Execute the repeated fixed block with a cut after each multiple of Γ layers.
This uses the boundary convention of apd:thm:triangle.
Equations
- Lean4LPD.PauliString.layerScheduledTraj layers Γ wstar O = Lean4LPD.PauliString.layerTraj (fun (T : ℕ) => layers (T % Γ)) (Lean4LPD.PauliString.trotterSchedule Γ wstar) O
Instances For
A single scheduled layer: conjugation by the layer, then the scheduled projection
(apd:thm:triangle).
Before a boundary, the scheduled execution is the untruncated prefix of the fixed block,
started from the scheduled operator at the previous boundary (apd:eq:step_component).
Over one full block, the scheduled execution evolves without truncation and is then cut
(apd:eq:step_component).
The layer-indexed and the step-indexed executions agree at step boundaries
(apd:eq:step_component). Both sides are defined independently, so this is a theorem.
Inside a step, the untruncated prefix of the block equals the scheduled trajectory at the
corresponding layer. This identification lets the rung masses of pauliMultiLadder be used in
apd:eq:total_high_weight_norm. The endpoint i = Γ is excluded: there the scheduled
trajectory has already been cut.
The discarded operator X_{d+1} of apd:eq:step_component: the operator at the end of
step d + 1 before the cut, minus the kept operator. The index d is zero-based.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The Pauli norm of the discarded operator is the high-weight norm of the operator before
the cut (apd:thm:triangle; apd:eq:step_component).
After every completed step the kept operator has no mass above the cutoff. This gives the
reset condition in apd:eq:total_high_weight_norm. It is a statement about the kept operator,
not about the discarded one.
The high-weight norm inside step d + 1, after i untruncated layers and before the cut,
as used in apd:eq:total_high_weight_norm. It is defined from the matrix evolution; its
recurrence is layerStepMass_inflow.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Reset at the start of every step, as required by apd:eq:total_high_weight_norm: the
mass above the cutoff vanishes at layer 0 of each step. For the first step this follows from
k_o-locality of the input and k_o ≤ wstar; for later steps from the preceding cut.
Inflow inside a step. One more layer increases the mass above the cutoff by at most the
multi-jump inflow from the lower rungs of the kept trajectory layerN, plus the entry factor
times the Pauli norm of the input. This is the inflow hypothesis of
MultiLadder.sum_block_inflow_le for apd:eq:total_high_weight_norm, derived here from
highNorm_layerConj_le_multi.
The sum of the discarded Pauli norms obeys the shifted-chain bound.
This is the step of apd:eq:total_high_weight_norm that sums the per-step inflows over the
layer slots, with X_{d+1} defined by apd:eq:step_component: a chain with k + 1 jumps
carries the factor ((r + 1) Γ)^(k+1) / (k+1)!. The reset and the inflow recurrence required by
MultiLadder.sum_block_inflow_le are supplied by layerStepMass_reset and
layerStepMass_inflow, so they are not hypotheses.
Layer conjugation preserves zero, the additive-map helper for
apd:thm:triangle.
A zero input stays zero through a block of layers (apd:thm:triangle).
The untruncated evolution through a fixed block of Γ layers, as an additive endomorphism
of matrices. Its powers are the untruncated whole-step evolutions in apd:thm:triangle.
Equations
- One or more equations did not get rendered due to their size.
Instances For
layerBlockEnd applies the matrix evolution layerBlockTraj through Γ layers
(apd:thm:triangle).
The operator telescope for layered steps. This is the identity in apd:thm:triangle:
the untruncated evolution minus the LPD output after r steps is the sum of the discarded
operators discardedLayerStep, each evolved through the remaining whole blocks.
A whole Hermitian layer block preserves the normalized Pauli norm, supporting the
norm-level triangle counterpart of apd:thm:triangle.
Every power of the block evolution preserves the normalized Pauli norm, for Hermitian
generators (apd:thm:triangle).
The truncation error is at most the sum of the discarded Pauli norms.
This is the norm-level part of apd:thm:triangle, in the normalized Pauli 2-norm. It is neither
a bound on expectation values nor a bound in the matrix operator norm.
The truncation error obeys the shifted-chain bound.
This composes the norm-level triangle bound of apd:thm:triangle with the shifted-chain bound
sum_pauliNorm_discardedLayerStep_le_chain of apd:eq:total_high_weight_norm. Besides 0 < Γ
and 1 ≤ m, the hypotheses concern only the generators (layer structure, Hermiticity, sine
bound, betaOf < 1) and the locality of the observable.
The sum of the discarded Pauli norms obeys the c₀ bound.
MultiLadder.sum_block_epsJump_le_cZero (apd:eq:total_high_weight_norm; apd:eq:c0) applied
to pauliMultiLadder, with reset and inflow supplied by layerStepMass_reset and
layerStepMass_inflow. The conclusion has the form of the hypothesis hstep of
total_truncation_error, which is therefore a theorem for the Pauli model. Here A stands for
the product α t, the cutoff is rung m + 1, and B = 4eβ.
The truncation error obeys the c₀ bound
(apd:thm:triangle; apd:eq:total_high_weight_norm; apd:eq:c0).
This is a statement in the normalized Pauli norm, not about expectation values.
The truncation error with the threshold tZeroModel.
This is the Pauli-norm counterpart of apd:thm:one_step_truncation_error and
apd:eq:time_condition: the error is at most q^(m+1) (e (m+1))^(k_o/(k_h-1)) ‖O‖ with
q = decayBase Γ k_h α t = t / tZeroModel Γ k_h α, a threshold that depends only on Γ, k_h
and α. The hypotheses 1 ≤ m and 5 ≤ r, under which c₀ ≤ 2 (cZero_le_two), are explicit,
as is B = 4eβ ≤ 1, which also implies β ≤ 1/2. Since c₀ ≤ 2 under these hypotheses,
tZeroModel is at most the threshold tZero with the constant c₀ (tZeroModel_le_tZero), so
t < tZeroModel is the more restrictive time condition. The hypothesis hstep of the scalar
theorem total_truncation_error_product_bound is supplied by
pauliNorm_layerStep_error_le_cZero.
The norm-level truncation bound in the paper's parameter regime.
This is apd:thm:one_step_truncation_error with apd:eq:time_condition at the level of the
normalized Pauli norm. Let O be k_o-local, let each step consist of Γ disjoint-support
layers of Hermitian rotations of weight at most k_h, 2 ≤ k_h, with
|sin θ| ≤ a ≤ α t / r, and let the cutoff be w* = k_o + m (k_h - 1). If Admissible r m Γ
(in particular m ≤ r and 8 (m + 1)² ≤ r Γ), 1 ≤ m, 5 ≤ r and
r ≥ 8e² (k_o + k_h - 1) α t, then
‖U^r(O) - O_r‖ ≤ (t / t₀)^(m+1) · (e (m+1))^(k_o/(k_h-1)) · ‖O‖, t₀ = tZeroModel Γ k_h α.
The step-count condition gives B = 4eβ ≤ 1 (source_entry_inflation_le_one) and hence
β ≤ 1/2, so neither is a separate hypothesis. The base t / t₀ is below one whenever
t < tZeroModel Γ k_h α, by decayBase_lt_one. Nothing is asserted about expectation values in
a state or about the Trotter approximation of the Hamiltonian evolution.