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0.028403... | 0.007791 | -0.023715 | 0.060833 | 11.072457 | 0.021731 | [
0.01844937540216075,
0.024944031836051005
] | [
0.08640233799987246,
-0.22716026935787775,
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0.24604772533670888,
0.06115800250358281,
0.3854876981261752,
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0.23376307149882258,
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0.06483879802051543,
-0.08425983747988303,
-0.028653653242135244,
0.03696759450525775,
-0.2408866... | 0.023878 | [
0.019972927632609657,
0.02784350635545893
] | [
-0.0023204680361268992,
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0.1253751351654007,
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0.04240707397428742,
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0.06326520269760844,
0.06847987773743636,
0.06794267441564787,
0.0040156105664787695,
0.138954... | 0.037864 | [
0.031229933708360184,
0.045809735323434506
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-0.17725944322079135,
0,
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0.05902362969757492,
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0.2416089702282627,
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0.3604858333140384,
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0,
0... | 0.920271 | 0.114649 | 4 | 50 | globalZ | 0.029527 | e1/n04_L050.json |
Barren Plateaus from Scratch: results
Every data point behind the technical report Barren Plateaus from Scratch: A NumPy State-Vector Study of
Trainability in Variational Quantum Circuits (Thanatchon Chongmankhong, 2026). The numbers were produced with
qsim, a from-scratch NumPy state-vector simulator with exact adjoint gradients, on 2–16 qubits.
- 📄 Paper: read online · PDF
- 💻 Code: github.com/thanatchon36/bp-from-scratch (MIT)
- 📦 Archive: doi:10.5281/zenodo.23995487
The dataset comes in two forms:
data/: one tidy Parquet table per experiment. These are the configurations below, readable withdatasets, pandas or the dataset viewer.raw/: the JSON cache exactly as the experiment scripts wrote it, one file per configuration, plussummary.json. It is byte-identical toresults/in the code repository at v0.2.0.
Load
from datasets import load_dataset
e1 = load_dataset("thanatchon36/bp-from-scratch", "e1_variance_vs_n", split="train").to_pandas()
print(e1[["n", "L", "var_mid", "haar_two_sided"]].sort_values(["L", "n"]).head())
import pandas as pd
df = pd.read_parquet("hf://datasets/thanatchon36/bp-from-scratch/data/e5_training.parquet")
print(df.groupby(["cost", "shots", "n"]).fidelity_final.mean().unstack("n").round(3))
To regenerate every figure and table of the paper from this data, put raw/ in place of results/ in the code
repository and run make figures && make paper.
Configurations
| Config | Rows | One row is | What it measures |
|---|---|---|---|
e0_haar_check |
14 | Hamiltonian × n | Sampled gradient variance with Haar-random circuits before, after or on both sides of a rotation, against the closed-form values (Appendix A) |
e1_variance_vs_n |
40 | n × depth L | McClean random-axis hardware-efficient ansatz, H = Z⊗n: gradient variance, raw derivative samples and half-chain entropy |
e2_local_vs_global |
60 | cost × n × L | Alternating-layered ansatz with a global projector cost and a local cost (Cerezo et al.) |
e3_initialisation |
30 | strategy × n | Uniform, Gaussian (σ = 1, 0.3, 0.1) and identity-block initialisation, local cost (1/n)ΣXᵢ |
e4_variance_vs_depth |
13 | depth L at n = 12 | Fine depth grid of the E1 circuit: gradient variance and entanglement entropy |
e5_training |
330 | one Adam run | Preparing |0⟩⊗n from random angles with exact gradients or 10⁴-shot noise; full cost history |
e6_qaoa_variance |
28 | n × p | QAOA MaxCut on random 3-regular graphs: variance of ∂C/∂γ₁ and ∂C/∂β₁ |
e6_qaoa_training |
18 | p × graph at n = 10 | Approximation ratios reached by Adam from 4 random starts per graph |
e7_dla |
24 | family × n | Exact dynamical Lie algebra dimension, 𝔤-purities, predicted and measured Var[C] |
Columns
Gradient statistics (e1–e4). Every row samples n_samples random parameter vectors and computes the
full gradient with the adjoint method.
| Column | Meaning |
|---|---|
n, L |
Qubits and circuit depth (layers) |
n_params |
Number of circuit parameters |
var_first, var_mid, var_last |
Variance of the derivative with respect to a probe parameter in the first, middle (middle qubit) and last layer |
*_ci |
95% percentile-bootstrap interval of that variance (400 resamples) |
raw_first, raw_mid, raw_last |
The individual derivative samples behind the variances |
var_per_param |
Variance of the derivative with respect to every parameter, in circuit order |
var_mean_over_params, var_median_over_params |
Mean and median of var_per_param |
grad_mean_abs, cost_mean, cost_var |
Mean absolute derivative, mean and variance of the cost |
entropy_mean, entropy_std |
Half-chain von Neumann entropy of U(θ)|0⟩ in nats (E1, E4) |
haar_two_sided |
Closed-form variance for a unitary 2-design on both sides of the probe (Eq. 2 of the paper) |
ham, cost, variant |
Cost operator, global or local cost (E2), initialisation strategy (E3) |
seconds |
Wall-clock time of the configuration on one CPU core |
E5 training runs. cost is global or local; shots = 0 means exact gradients, otherwise Gaussian noise of
standard deviation noise_sigma is added to every cost and gradient entry. grad_norm_init is the exact gradient
norm at the random start, fidelity_final is |⟨0|ψ⟩|² after steps Adam steps at learning rate lr, and
history is the cost after every step.
E6. var_gamma1 and var_beta1 are variances of the derivative of the cut operator C with respect to the
first QAOA angles γ₁ and β₁, and raw_gamma1, raw_beta1 are the samples. The paper's figure divides them by
|E|² = (3n/2)². A new random graph is drawn for every sample. In e6_qaoa_training, edges is the graph, max_cut its exact maximum cut, and the ratios are
⟨C⟩/C_max.
E7. family is hea_full {Xᵢ, Yᵢ, ZᵢZᵢ₊₁}, hea_real {Yᵢ, ZᵢZᵢ₊₁}, hva_tfim {ΣXᵢ, ΣZᵢZᵢ₊₁} or qaoa
(random 3-regular graph, edges). dim is the exact DLA dimension, capped marks closures stopped at the size
limit, purity_rho and purity_H are the 𝔤-purities, predicted_var is P𝔤(ρ)P𝔤(H)/dim 𝔤 (Ragone et al.), and
measured_var is the cost variance over samples uniformly random parameters of an L-layer circuit.
E0. Columns {two_sided,left_only,right_only}_{measured,predicted} for hamiltonian Z⊗n (globalZ) or
|0⟩⟨0|⊗n (projector), with G = Y on qubit 0.
Every table has a source_file column that names its file in raw/.
Conventions
Qubit 0 is the most significant bit, and rotations are exp(−i·θ·G/2), as in PennyLane and Qiskit. All seeds are
fixed in the experiment scripts, so make results in the code repository reproduces this data (about one CPU
hour).
Citation
@techreport{chongmankhong2026barren,
author = {Chongmankhong, Thanatchon},
title = {Barren Plateaus from Scratch: A NumPy State-Vector Study of Trainability in Variational Quantum Circuits},
year = {2026},
type = {Technical report},
url = {https://thanatchon36.github.io/bp-from-scratch/paper/}
}
@software{chongmankhong2026bpfromscratch,
author = {Chongmankhong, Thanatchon},
title = {bp-from-scratch: a NumPy state-vector simulator and a reproducible study of barren plateaus},
year = {2026},
version = {0.2.0},
doi = {10.5281/zenodo.23995487},
url = {https://doi.org/10.5281/zenodo.23995487}
}
License: MIT, the same as the code.
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