• Advanced Photonics Nexus
  • Vol. 3, Issue 5, 054001 (2024)
Zhiwei Guo†,*, Yang Xu, Shengyu Hu, Yuqian Wang..., Yong Sun* and Hong Chen*|Show fewer author(s)
Author Affiliations
  • Tongji University, School of Physics Science and Engineering, MOE, Key Laboratory of Advanced Micro-Structure Materials, Shanghai, China
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    DOI: 10.1117/1.APN.3.5.054001 Cite this Article Set citation alerts
    Zhiwei Guo, Yang Xu, Shengyu Hu, Yuqian Wang, Yong Sun, Hong Chen, "Metamaterial-enhanced magnetic resonance imaging: a review," Adv. Photon. Nexus 3, 054001 (2024) Copy Citation Text show less

    Abstract

    Magnetic resonance imaging (MRI), as a noninvasive and powerful method in modern diagnostics, has been advancing in leaps and bounds. Conventional methods to improve MRI based on increasing the static magnetic field strength are restricted by safety concerns, cost issues, and the impact on patient experience; as such, innovative approaches are required. It has been suggested that metamaterials featuring subwavelength unit cells can be used to take full control of electromagnetic waves and redistribute electromagnetic fields, achieve abundant counterintuitive phenomena, and construct versatile devices. Recently, metamaterials with exotic effective electromagnetic parameters, peculiar dispersion relations, or tailored field distribution of resonant modes have shown promising capabilities in MRI. Herein, we outline the principle of the MRI process, review recent advances in enhancing MRI by employing the unique physical mechanisms of metamaterials, and demystify ways in which metamaterial designs could improve MRI, such as by enhancing the imaging quality, reducing the scanning time, alleviating field inhomogeneities, and increasing patient safety. We conclude by providing our vision for the future of improving MRI with metamaterials.
    ω0=γB0,

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    θ=γB1τ.

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    SNRB02sin(γB1+τ)B1Rcoil+Rsample,

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    μ=1F(1ω02ω2)+iΓωandμ=1,

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    (jωL+jωC+R)In+jωM(In1+In+1)=Vn,

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    1ω02/ω2j/Q+κcos(ka)=0.

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    ε¯¯=(εxx000ε000ε)andεxx=ε0(1ωp2ω2).

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    εxx(ω,kx)=ε(1kp2k2kx2).

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    ε=ε(ω)=CR1ω2LLandμ=μ(ω)=LR1ω2CL.

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    θ=βl=(2πλ)(mλ2)=mπ,m=1,2,3,,

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    Zhiwei Guo, Yang Xu, Shengyu Hu, Yuqian Wang, Yong Sun, Hong Chen, "Metamaterial-enhanced magnetic resonance imaging: a review," Adv. Photon. Nexus 3, 054001 (2024)
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