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Spatial encoding brings high-density 3D shape sensing to a single-mode fibre


  • Light: Advanced Manufacturing  7, Article number: 130 (2026)
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  • Corresponding author:
    Huifang Gao (gaohuifang@cjlu.edu.cn)Qing Yang (qingyang@zju.edu.cn)
  • These authors contributed equally: Huirong Chen, Zhong Wen

  • Received: 31 July 2026
    Revised: 13 August 2026
    Accepted: 13 August 2026
    Published online: 23 September 2026

doi: https://doi.org/10.37188/lam.2026.130

  • Existing three-dimensional fibre shape-sensing systems involve trade-offs among compactness, spatial sampling density, and interrogation complexity. Luo et al. addressed these challenges by spatially encoding orthogonal curvature components using axially misplaced eccentric scatterers in a standard single-mode fibre, enabling millimetre-scale, single-channel reconstruction and scalable integration into robotic and minimally invasive devices.
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  • [1] Mengaldo, G. et al. A concise guide to modelling the physics of embodied intelligence in soft robotics. Nature Reviews Physics 4, 595-610 (2022). doi: 10.1038/s42254-022-00481-z
    [2] Wang, P. Y. et al. Sensing expectation enables simultaneous proprioception and contact detection in an intelligent soft continuum robot. Nature Communications 15, 9978 (2024). doi: 10.1038/s41467-024-54327-6
    [3] Lamb, E. S. et al. Shape sensing endoscope fiber. Optica 11, 1462-1467 (2024). doi: 10.1364/OPTICA.532250
    [4] Lee, B. Review of the present status of optical fiber sensors. Optical Fiber Technology 9, 57-79 (2003). doi: 10.1016/S1068-5200(02)00527-8
    [5] Pendão, C. & Silva, I. Optical fiber sensors and sensing networks: overview of the main principles and applications. Sensors 22, 7554 (2022). doi: 10.3390/s22197554
    [6] Zeng, K. B. et al. Synthesized complex-frequency excitation for ultrasensitive molecular sensing. eLight 4, 1 (2024). doi: 10.1186/s43593-023-00058-y
    [7] Tan, T. et al. Biomimetic acoustic perception via chip-scale dual-soliton microcombs. eLight 5, 22 (2025). doi: 10.1186/s43593-025-00099-5
    [8] Zhang, Z. L. et al. Structured light meets machine intelligence. eLight 5, 26 (2025). doi: 10.1186/s43593-025-00102-z
    [9] Tan, Z. Z. et al. A Mach-Zehnder-based optical fiber sensor enables multi-directional and wide-range curvature sensing with the assistance of CNN. Optical Fiber Technology 84, 103766 (2024). doi: 10.1016/j.yofte.2024.103766
    [10] Zhang, S. S. et al. Fiber-optic bending vector sensor based on Mach-Zehnder interferometer exploiting lateral-offset and up-taper. Optics Letters 37, 4480-4482 (2012). doi: 10.1364/OL.37.004480
    [11] Oliveira, R., Cardoso, M. & Rocha, A. M. Two-dimensional vector bending sensor based on Fabry-Pérot cavities in a multicore fiber. Optics Express 30, 2230-2246 (2022). doi: 10.1364/OE.445396
    [12] He, C. J. et al. Optical fiber shape sensing of flexible medical instruments with temperature compensation. Optical Fiber Technology 74, 103123 (2022). doi: 10.1016/j.yofte.2022.103123
    [13] Meng, L. X. et al. High-accuracy 3D shape sensor based on anti-twist packaged high uniform multicore fiber FBGs. Advanced Fiber Materials 5, 1467-1477 (2023). doi: 10.1007/s42765-023-00285-5
    [14] Fu, C. L. et al. High-spatial-resolution φ-OFDR shape sensor based on multicore optical fiber with femtosecond-laser-induced permanent scatter arrays. Optics Letters 48, 3219-3222 (2023). doi: 10.1364/OL.486644
    [15] Fu, C. L. et al. OFDR shape sensor based on a femtosecond-laser-inscribed weak fiber Bragg grating array in a multicore fiber. Optics Letters 49, 1273-1276 (2024). doi: 10.1364/OL.516067
    [16] Parent, F. et al. Enhancement of accuracy in shape sensing of surgical needles using optical frequency domain reflectometry in optical fibers. Biomedical Optics Express 8, 2210-2221 (2017). doi: 10.1364/BOE.8.002210
    [17] Luo, P. T. et al. Single-channel single-fiber 3D shape sensing based on cascaded cladding fiber Bragg gratings array. Laser & Photonics Reviews 19, e00668 (2025). doi: 10.1002/lpor.202500668
    [18] Waltermann, C. et al. Multiple off-axis fiber Bragg gratings for 3D shape sensing. Applied Optics 57, 8125-8133 (2018). doi: 10.1364/AO.57.008125
    [19] Luo, P. T. et al. Single-fiber three-dimensional shape sensing via femtosecond laser inscribed orthogonal eccentric scatterers. Light: Science & Applications 15, 343 (2026). doi: 10.1038/s41377-026-02425-z
    [20] Hadad, B. et al. Toward multimode-fiber shape sensing. Optics Letters 48, 1160-1163 (2023). doi: 10.1364/OL.479876
    [21] Manavi Roodsari, S. et al. Deep learning-based approach for high spatial resolution fibre shape sensing. Communications Engineering 3, 19 (2024). doi: 10.1038/s44172-024-00166-8
    [22] Meng, Y. J. et al. Wavelength-division-multiplexed and identical-weak Bragg grating arrays in multicore fiber for single-channel OFDR shape sensing. Optics Express 33, 39396-39405 (2025). doi: 10.1364/OE.569784
    [23] Qiu, G. C. et al. Spatial short-term Fourier transform based single-channel single-fiber 3D shape sensing. IEEE Robotics and Automation Letters 11, 5438-5445 (2026). doi: 10.1109/LRA.2026.3674026
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    [25] Jiang, Q., Li, J. H. & Masood, D. Fiber-optic-based force and shape sensing in surgical robots: a review. Sensor Review 43, 52-71 (2023). doi: 10.1108/SR-04-2022-0180
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Spatial encoding brings high-density 3D shape sensing to a single-mode fibre

  • 1. State Key Laboratory of Extreme Photonics and Instrumentation, College of Optical Science and Engineering, International Research Center for Advanced Photonics, Zhejiang University, Hangzhou 310027, China
  • 2. ZJU-Hangzhou Global Scientific and Technological Innovation Center, Zhejiang University, Hangzhou 311200, China
  • 3. College of Optical and Electronic Technology, China Jiliang University, Hangzhou 310018, China
  • Corresponding author:

    Huifang Gao, gaohuifang@cjlu.edu.cn

    Qing Yang, qingyang@zju.edu.cn

  • These authors contributed equally: Huirong Chen, Zhong Wen

doi: https://doi.org/10.37188/lam.2026.130

Abstract: Existing three-dimensional fibre shape-sensing systems involve trade-offs among compactness, spatial sampling density, and interrogation complexity. Luo et al. addressed these challenges by spatially encoding orthogonal curvature components using axially misplaced eccentric scatterers in a standard single-mode fibre, enabling millimetre-scale, single-channel reconstruction and scalable integration into robotic and minimally invasive devices.

  • Shape sensing is increasingly important for soft robots, steerable endoscopes, and minimally invasive instruments, where real-time knowledge of three-dimensional deformation is required for navigation, manipulation, and closed-loop control in confined or delicate environments13. Optical fibre shape sensors are particularly well suited for this task because they are thin, flexible, lightweight, and immune to electromagnetic interference. In addition, they can be embedded in narrow instruments without substantially increasing the probe size47.

    Accurate three-dimensional shape reconstruction requires continuous or densely sampled measurements of both the local curvature and the bending direction along the sensing fibre8. Point bending sensors, such as those employing Mach–Zehnder interferometers9,10 and Fabry–Pérot interferometers11, can provide high sensitivity; however, their sparse sensing locations limit the reconstruction of complex, continuous shapes. Quasi-distributed sensing based on fibre Bragg gratings (FBGs)12,13 and distributed sensing based on optical frequency domain reflectometry (OFDR)14-16 have emerged as the two principal approaches for three-dimensional fibre shape sensing. However, recovering both the magnitude and direction of the local curvature generally requires axial-strain measurements at multiple spatially separated positions across the fibre cross section. Therefore, conventional systems rely on multiple fibres or multicore fibres, requiring each sensing channel to be interrogated separately. This increases the sensor size, interconnection and packaging complexity, and overall system cost.

    Femtosecond-laser inscription of multiple off-axis or cladding FBGs in a standard single-mode fibre provides a compact single-fibre solution, in which the relative intensities of spectrally distinguishable gratings are used to determine the bending direction17,18. However, the finite interrogation bandwidth limits the number of gratings that can be resolved in a single channel, restricting the system's capacity to simultaneously achieve a high sensing-point count and fine spatial resolution. While OFDR, provides densely distributed strain sampling, a conventional single-core fibre core does not provide sufficient independent transverse information to recover both the bending magnitude the and direction15,16. Achieving direction-resolved, densely sampled three-dimensional shape sensing in a standard single-core fibre using only one interrogation channel thus remains a central challenge.

    Against this backdrop, Luo et al. developed a three-dimensional deformation-encoding and shape-sensing approach based on misplaced orthogonal eccentric scatterers (MOESs) inscribed in a standard single-mode fibre19. The MOESs consist of femtosecond-laser-written, micrometre-scale Rayleigh scattering-enhancement structures positioned in the fibre cladding along alternating orthogonal azimuthal directions. Fibre bending changes the overlap between the guided mode and each eccentric scatterer, modulating its backscattered intensity according to the local curvature component along the corresponding direction. Unlike orthogonal FBGs, which are distinguished by their wavelengths, these scatterers have no intrinsic spectral labels. Therefore, they are axially staggered such that each generates a distinct peak in the spatial OFDR trace. The orthogonal eccentric positions encode the two transverse curvature components, whereas the axial displacement assigns each response a distinct spatial address within a single OFDR channel. Therefore, each adjacent orthogonal pair forms an effective sensing point that encodes the local directional-curvature information required for three-dimensional reconstruction into a one-dimensional sequence of scattering-peak intensities.

    Using a reel-to-reel femtosecond-laser writing system, the authors inscribed 450 scatterers along a 1.13-m fibre, corresponding to 449 sensing locations at 2.5-mm spacing, with a total added loss of only about 0.38 dB. Three-dimensional reconstruction was demonstrated over an approximately 9-cm section containing 36 scatterers and 35 sensing points. The two orthogonal scatterer sets showed approximately sinusoidal responses with bending direction, a phase offset of about 90°, and an average maximum sensitivity of approximately 0.05 dB·m. The three-dimensional trajectory was then reconstructed using the Frenet–Serret equations. For circular arcs with radii of 6–12 cm, the relative error remained below approximately 6% and the endpoint error was below 8%. The crossed, S-shaped, and spiral configurations were qualitatively reproduced. Temperature and axial-strain tests further indicated robustness to uniform environmental perturbations. Although weak-signal fluctuations and cumulative reconstruction errors remain important limitations, this study establishes a distinct spatial-encoding strategy for dense, direction-resolved three-dimensional shape sensing in a standard single-core fibre using only one interrogation channel.

    Table 1 compares the present results with those reported in a representative, though non-exhaustive, selection of prior studies in the field9,11,13,15,17,19-23. Existing approaches generally involve trade-offs among the sensor size, number of interrogation channels, spatial sampling density, and three-dimensional reconstruction capability. Local interferometric sensors cannot readily support axial shape reconstruction9,11, whereas multicore or multi-fibre schemes increase the system integration and demodulation complexity13,15,22. Existing single-fibre approaches are often constrained by the wavelength-multiplexing capacity17,21 or by application-specific sensing geometries with limited effective spatial sampling20,23. By introducing MOESs into a standard single-mode fibre, Luo et al. unified directional-information encoding and axial signal addressing in the spatial domain, thereby enabling high-density three-dimensional shape sensing with a single fibre and interrogation channel. The significance of this work lies not only in improving an individual sensing metric but also in establishing a deformation-encoding paradigm that avoids reliance on multicore structures and wavelength labels. Combined with reel-to-reel femtosecond-laser writing, this approach also provides a potential route toward long-length, high-density, and scalable manufacturing of shape-sensing systems.

    Work Sensing fibre / element Sampling / sensing length Capability / range Accuracy Readout Channel(s) Main comment
    Tan et al., 20249 Mach–Zehnder interferometer 1 local point 0–10.42 m−1;4 directions Transmission spectra + CNN 1 Directional local sensing only
    Oliveira et al., 202211 FP cavities in a seven-core fibre 1 local plane 2D vector bend;
    0–6.4 m−1
    <4% Reflection spectra Multicore Directional local sensing only
    Hadad et al., 202320 Step-index
    multimode fibre
    3 points over 2 m 1D position tracking ≈97% step accuracy Proximal reflected speckle + CNN 1 Sparse point tracking
    Roodsari et al., 202421 Five eccentric-FBG triplets in SMF 5 planes;
    5-cm spacing;
    30 cm
    3D shape;
    0.58–33.5 m−1
    2.1-mm median tip error Reflection spectra + CNN 1 DL-enhanced but data-dependent
    Meng et al., 202313 FBG arrays in anti-twist seven-core fibre 6 planes;
    3-cm spacing;
    15 cm
    Real-time 3D shape 3.33% max median tip error FBG reflection spectra Multicore Accurate but multichannel
    Fu et al., 202415 Weak-FBG arrays in seven-core fibre 60 points;
    1-cm spacing;
    60 cm
    2D/3D shape 1.08%/1.07% OFDR + cross-correlation Multicore,
    switched
    Dense but multichannel
    Meng et al., 202522 WDM/IW-FBG arrays in seven-core fibre 20 planes;
    2-cm spacing;
    40 cm
    2D/3D shape 2.61%/2.75% OFDR 1, seven-core synchronous Single-channel but wavelength-coded
    Qiu et al., 202623 Helically wrapped SMF 2.6-mm strain sampling;
    1.45 m
    2D/3D shape + twist 2.15%/5.32%; twist 7.90% OFDR + SSTFT 1 Twist-aware but geometry-dependent
    Luo et al., 202517 Cascaded orthogonal cl-FBGs in SMF 26 points;
    1-cm spacing;
    25 cm
    2D/3D shape <8%/≈3% OFDR intensity 1 Four wavelength labels; twist-sensitive
    Luo et al., 202619 MOESs in SMF 449 points;
    2.5-mm spacing;
    1.13 m
    2D/3D shape 3D End/relative errors <8%/<6% OFDR intensity 1 Dense single-core sensing; noise/twist limits

    Table 1.  Representative comparison of optical-fibre-based bending and three-dimensional shape-sensing approaches9,11,13,15,17,19-23. Note: SMF, single-mode fibre.

    Possible extensions may include improving robustness against signal fluctuations, fibre twisting, and sharp-bend loss, as well as validating the approach under dynamic deformation. Its compact architecture may also facilitate the integration of force sensing, intraoperative imaging, or closed-loop control in continuum robots and minimally invasive instruments24,25.

Acknowledgements
  • Financial support was provided by the National Key Research and Development Program of China (Grant Nos. 2022ZD011941, 2024YFF1206701, 2024YFF1206700, and 2024YFF1206705), the National Natural Science Foundation of China (Grant Nos. T2525010, T2293751, and T2293750), Leading Innovative and Entrepreneur Team Introduction Program of Zhejiang (Grant No. 2024R01001), and Zhejiang University Global Partnership Fund.

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