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Quantum Machine Learning for Remote Sensing: Exploring potential and challenges

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arxiv 2311.07626 v1 pith:ZIQWEAAL submitted 2023-11-13 quant-ph cs.LG

classification quant-phcs.LG
keywords quantumremotesensingchallengespotentialadvantageanalysisdata
verification ladder T0 review T1 audit T2 compute T3 formal
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The industry of quantum technologies is rapidly expanding, offering promising opportunities for various scientific domains. Among these emerging technologies, Quantum Machine Learning (QML) has attracted considerable attention due to its potential to revolutionize data processing and analysis. In this paper, we investigate the application of QML in the field of remote sensing. It is believed that QML can provide valuable insights for analysis of data from space. We delve into the common beliefs surrounding the quantum advantage in QML for remote sensing and highlight the open challenges that need to be addressed. To shed light on the challenges, we conduct a study focused on the problem of kernel value concentration, a phenomenon that adversely affects the runtime of quantum computers. Our findings indicate that while this issue negatively impacts quantum computer performance, it does not entirely negate the potential quantum advantage in QML for remote sensing.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Volcanic Clouds Detection through QCNN and Geostationary Satellite Multispectral Imagery

    cs.CV 2026-07 conditional novelty 5.0 of 10

    Hybrid QCNNs with 2–4 qubits classify SEVIRI volcanic-cloud scenes with F1 up to 1.00, matching or beating classical models with far fewer parameters.

  2. Hybrid Quantum CNN for Cross-Sensor Spaceborne Volcanic Thermal Activity Recognition Worldwide

    physics.geo-ph 2026-07 conditional novelty 5.0 of 10

    A hybrid quantum CNN with a 4-qubit parameterized circuit reached 92.5% accuracy on volcanic thermal-activity classification; a 2-qubit variant generalized best across sensors (F1 0.88).

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