Authors: Vinayak Sharma, Lord Sen, Ashish Padhy, Sourav Behera, Gennaro De Luca, Shyamapada Mukherjee, Aviral Shrivastava
Organizations: School of Computing and Augmented Intelligence Arizona State University, Tempe, AZ 85281 · National Institute of Technology, Rourkela Sector 1, Rourkela, Odisha - 769008
The 2N dimensions of Hilbert space give quantum metric learning exponentially many mutually orthogonal states with which to separate classes, but the same exponential dimension also degrades its optimization landscape and the tractability of evaluating its metric. By letting a classical network predict all gate parameters of a fixed ansatz, we isolate the reachable state manifold and its fidelity metric. We prove that this separability is already present on the unentangled manifold Munentangled=(CP1)N, which saturates the 2N maximal orthogonal capacity needed for classification, while entanglement adds states only at intermediate separations, which are costly to resolve under finite sampling. The same size carries costs. Global fidelity causes exponential gradient collapse across both unentangled (Θ(c−N)) and entangled (Θ(4−N)) manifolds; as fidelities concentrate, the fidelity signal-to-noise ratio at a fixed shot budget also decays exponentially in N; and because Munentangled already holds 2N orthogonal states, expressive, unconstrained encoders under contrastive losses reach trivial minima by geometric shattering even without entanglement. We introduce Quantum Projective Metric Learning (QPMeL), an exact O(N) closed-form kernel on Munentangled that circumvents circuit simulation. QPMeL resolves gradient collapse via a curriculum annealing from a 1-local observable regime (restoring Θ(1/N2) polynomial variance) to the global product kernel. Empirically, QPMeL as a complete design exceeds eight and matches two of 11 published quantum few-shot designs.
Figures & tables
Figure 1: QPMeL architecture. A domain metric encoder maps the input to a latent vector, and an angle head projects it through bounded activations to N coordinate pairs (θq,γq) , one per qubit.
Figure 2: QPMeL training flow, shown for an MS-COCO image and caption. The PMeF (shaded) projects the encoder’s angles onto real coordinate vectors Cq and computes each qubit’s fidelity with the CKF, and the metric loss on the resulting kernel sends gradients back to the encoder. Every block is classical, and no circuit runs during training.
Model
Circuit
Protocol
Baseline
QPMeL
MNIST
Thumwanit et al. (2021)
E-VQC
Binary (3,6)
91.7 (9)
99.80±0.20 (5)
NQE ( Hur et al., 2023 )
CPQK
Binary (0,1)
99.50 (12)
99.60±1.71 (5)
Huang et al. (2025)
E-VQC
2w-10s (3,5)
89.69 (9)
99.00±1.01 (5)
Wang et al. (2024)
E-VQC
3w-1s (0,1,2)
50.5 (6)
98.27±1.86 (5)
Wang et al. (2024)
E-VQC
3w-10s (0,1,2)
82.5 (6)
99.73±0.37 (5)
Table 1: Few-shot classification against published quantum models.
QSTConv
QNervFormer
QNervFormer (dropout)
Head
Similarity
L
Train
Held-out
Train
Held-out
Train
Held-out
Chen et al.
⟨Z⟩ cosine
4
–
3.2
–
4.3
–
–
E-VQC
Fidelity
4
1.5±0.9
1.2±0.4
10.1±2.6
0.2±0.3
2.8±0.4
2.3±1.4
DR
Fidelity
1
13.1±6.5
12.3±5.2
65.0±17.9
1.0±0.9
7.9±6.2
6.6±4.6
DR
Fidelity
2
2.9±1.8
3.7±1.2
43.0±8.0
0.3±0.6
2.9±2.4
2.3±2.0
DR
Fidelity
4
0.6±0.7
0.7±0.4
6.5±1.7
0.5±0.4
0.9±1.0
0.9±0.7
Table 2: THINGS-EEG2 200-way top-1 accuracy (%) with only the head changed; L circuit layers.
Dataset
Task
SWAP 2q gates
Shots
Exact
IBM-Prague model
IBM Marrakesh
MNIST
10w-1s
73
128
96.7±0.6
96.3±0.8
97.6±3.4
Fashion-MNIST
10w-1s
93
128
85.03±0.4
80.9±1.5
74.8±4.2
Omniglot
5w-3s
184
128
93.9±0.7
93.4±1.2
84.0±6.0
Table 3: Few-shot accuracy (%) on IBM hardware and under a device noise model.
Appendix figures & tables6 assets
Supplementary material from the paper’s appendix.
Appendix
Top-1
Top-5
Final loss
Collapsed
Encoder
Curr.
Add.
Curr.
Add.
Curr.
Add.
Curr.
Add.
QSTConv
23.96±5.2
19.11±3.9
56.82±7.6
48.56±5.5
4.81
5.38
0
0
QNervFormer
0.92±0.8
0.73±0.5
4.92±2.0
3.93±1.4
0.50
1.40
0
0
Appendix
Table E.1: QPMeL kernel schedule on THINGS-EEG2, 10 subjects and 5 seeds: 200-way held-out accuracy (%), final training loss, and runs whose final loss stays above 6.9 of 50 . Here, Curr. is Curriculum and Add. is Additive.
Kernel at initialization
Head
Similarity
Mean
Range (nats)
Structure ρ
Encoder gradient
Train (%)
E-VQC
⟨Z⟩ cosine
−3.9×10−3
6.57
0.19
10.6
3.2
E-VQC
Fidelity
8.8×10−4
0.09
0.79
0.010
10.1
E-VQC
log fidelity
8.8×10−4
–
0.79
955
0.3
DR
Fidelity
1.0×10−3
0.02
0.06
0.021
6.5
QPMeL
PMeF, product
9.9×10−4
0.07
n/m
0.62
96.5
Appendix
Table E.2: Kernel and gradient diagnostics on THINGS-EEG2 with QNervFormer; four-layer circuits.
Layers L
Head
1
2
4
8
16
DR
Rings in the kernel
0
1
3
7
15
Structure ρ
0.64
0.46
0.06
0.00
0.00
Encoder gradient
1.4×10−4
8.3×10−3
0.022
0.041
0.068
Train (%)
65.0±17.9‡
43.0±8.0
7.0±3.1
1.0±0.0
2.0±0.9
Held-out, QSTConv
12.3±5.2
3.7±1.2
0.7±0.4
n/r
n/r
Appendix
Table E.3: Circuit depth under the fidelity readout on THINGS-EEG2. Structure is measured at initialization within one tower on inputs uniform in [−π,π] , and the encoder gradient is the RMS at the first epoch on QNervFormer. Train is the fit to 200 training images on QNervFormer after 200 epochs, three seeds ( ‡ ten). Held-out rows are on QSTConv and on QNervFormer with branch dropout, with the checkpoint selection of Table , five seeds ( † four); QPMeL reaches 19.9 and 11.8% there. n/r, not run.
QSTConv
QNervFormer, branch dropout
Head
L
Matched
Unmatched
<0.01
Matched
Unmatched
<0.01
E-VQC, fidelity
4
0.057
0.034
0.39
0.127
0.072
0.18
DR
1
0.282
0.161
0.02
0.214
0.121
0.22
DR
2
0.188
0.117
0.06
0.123
0.072
0.28
DR
4
1.3×10−3
1.2×10−3
0.99
0.047
0.029
0.60
DR
8
n/r
n/r
n/r
0.019
8.9×10−3
0.87
Appendix
Table E.4: Trained kernels on THINGS-EEG2: mean fidelity of matched and of unmatched pairs, and the fraction of unmatched pairs below 0.01 , on 1024 training pairs at the checkpoint of Table ; five seeds ( † four). ‡ QNervFormer without branch dropout at epoch 200, three seeds. Haar-random states give 9.8×10−4 , 9.8×10−4 and 1.00 . n/r, not run.
Image → text
Text → image
Way
PMeF
Simulated
PMeF
Simulated
3
99.6±0.6
98.7±1.9
98.9±1.0
98.0±2.3
5
98.5±0.9
98.8±1.4
98.5±0.8
98.0±1.7
7
97.8±0.9
96.3±2.1
97.5±1.1
96.3±2.4
9
98.1±0.8
95.3±2.1
97.0±1.0
95.1±2.4
11
96.5±0.9
94.4±2.1
96.8±0.8
95.1±1.7
Appendix
Table E.5: MS-COCO cross-modal matching on training pairs (%), 20 qubits: closed-form PMeF and statevector simulation of the same circuit. Chance is 100/n for n -way.
Primitive
Setting
Qubits
2-qubit gates
Depth
Inversion test
N=5
5
0
6
Inversion test
N=6
6
0
6
Inversion test
N=10
10
0
6
SWAP test
N=5
11
73
187
SWAP test
N=6
13
93
232
SWAP test
N=10
21
167
394
Appendix
Table E.6: Transpiled cost of the two fidelity primitives, targeting the ibm_marrakesh coupling map and basis at optimization level 1 . Two-qubit counts are native cz gates after routing; the pre-routing logical count is 8N .
Quantum machine learning is often motivated by the exponentially large state space of quantum systems, but this promise leaves a basic generalization problem unresolved: how can a learner assign different meanings to unseen quantum directions when the training data provide no preferred basis, measurement frame, or other orienting structure? We address this identifiability problem by formulating supervised learning without an external quantum reference frame, so that predictions cannot depend on an arbitrary choice of Hilbert-space coordinates. This requirement forces the learned classifier to preserve every unitary symmetry left unbroken by the training data. We prove that whenever the training states fail to span the full Hilbert space, all pure states orthogonal to their span must receive the same prediction -- even when those states are mutually orthogonal and perfectly distinguishable once an appropriate measurement is supplied. The limitation is therefore not caused by state discrimination, optimization, or computational power, but by missing reference information. We further establish a robust version under weak symmetry breaking and show that learning generic unstructured concepts on multiqubit systems requires exponentially many independently oriented training directions. Numerical illustrations visualize the resulting prediction collapse and its controlled relaxation. Our results identify feature maps, measurement bases, Hamiltonians, locality, symmetry priors, architectures, and sufficiently diverse training states as operational resources for generalization. The central implication is that Hilbert-space dimension alone is not a learnable feature space: successful QML must specify the physical structure that gives unseen quantum directions semantic meaning.
Jeongho Bang
Institute for Convergence Research and Education in Advanced Technology, Yonsei University, Seoul 03722, Republic of Korea · Department of Quantum Information, Yonsei University, Incheon 21983, Republic of Korea
In supervised quantum machine learning with classical data, classification performance critically depends on the geometry induced by quantum data embedding. Existing data-adaptive approaches rely on pairwise fidelity evaluations between samples, which scale as O(B2) for B samples and create a computational bottleneck in iterative embedding optimization. To address this issue, we propose a prototype-guided framework for efficient data-adaptive quantum embedding. Using class-prototype separation and sample-to-prototype compactness, we derive a measurable lower certificate for class-ensemble distinguishability and construct a prototype-based objective requiring only O(B) fidelity evaluations. We integrate this objective into an end-to-end pipeline that combines task-specific quantum circuit architecture optimization with continuous refinement of the data-embedding parameters. Across five benchmark datasets with up to 20 qubits, our method retains competitive quantum kernel support vector machine (SVM) performance while reducing fidelity-evaluation cost, with particularly strong gains over budget-matched pairwise optimization on T-MNIST. Geometric analyses examine how the learned embeddings relate to kernel alignment and classification margins, revealing dataset-dependent benefits and limitations. We further derive a prototype-based classifier in the reproducing kernel Hilbert space that provides an explicit witness for the SVM objective and a low-cost proxy for model selection, and extend the framework to multiple prototypes for multimodal class structures.
Seokhoon Jeong, Daniel K. Park
Department of Statistics and Data Science Yonsei University Republic of Korea · Department of Statistics and Data Science Department of Applied Statistics Department of Quantum Information Yonsei University Republic of Korea
Learning with data in the form of quantum states is of current interest and has led to a variety of problems that boil down to interaction with the available data via quantum measurement and classical post-processing of observed classical outcomes. In quantum measurement PAC learning, one is given a sequence of unknown, prepared quantum states and classical labels, along with a hypothesis class of candidate measurements. The task is to select a measurement from the hypothesis class that minimizes a fixed notion of error in prediction of the classical labels via measurement of a new state by the selected hypothesis. In this work, we consider the advantage of interacting with the given data in the measurement learning framework using learning rules given by measurements that cannot be implemented using local operations and classical communication (LOCC), as opposed to single-copy learning rules. We provide a construction showing that there exist learning scenarios wherein single-copy learning rules are asymptotically suboptimal compared to optimal ones. We then show that learning rules based on entangled measurements enjoy at most a polynomial sample complexity advantage over single-copy learning rules in the PAC learning setting (under a natural joint measurability covering assumption).
Arka Prabha Das, Abram Magner
Department of Computer Science University at Albany, State University of New York Albany, NY, USA · AI Plus Institute at UAlbany