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Movable Antenna: Enhancing Near-Field ISAC

Updated 20 January 2026
  • Movable Antenna (MA) is a paradigm that introduces adjustable degrees of freedom via mechanical repositioning, enabling enhanced near-field channel probing and fine spatial sampling.
  • It employs advanced techniques such as Newtonized Orthogonal Matching Pursuit and subregion clustering (LSRC) for high-resolution angle estimation and robust geometric localization.
  • The MA framework significantly improves integrated sensing and communication (ISAC) performance, offering up to 2–5 dB NMSE improvements over baseline methods in multi-scatterer environments.

Movable Antenna (MA) introduces adjustable physical degrees of freedom to future wireless communication systems via mechanized repositioning of antenna ports. This paradigm shift facilitates transmission and sensing in the near-field regime, enhancing channel estimation, localization, and integrated sensing and communication (ISAC) capabilities. MA’s adaptive movement enables fine spatial sampling and manipulation of EM field patterns for multi-stage signal acquisition, estimation, and geometric inference. A recent MA-assisted broadband near-field ISAC framework applies structured subregion partitioning, high-resolution angle estimation (via Newtonized Orthogonal Matching Pursuit, NOMP), and a geometric clustering/localization pipeline termed LSRC (Localization via Subregion Ray Clustering), yielding notable performance improvements in multi-scatterer environments (Sun et al., 13 Jan 2026).

1. Mathematical Model of Movable Antenna Systems

The MA system consists of a base station (BS) equipped with NN movable antenna ports, each located at rn=[xn,0,zn]TR3\mathbf r_n=[x_n,0,z_n]^T \in \mathbb R^3, forming the set R={rn}n=1N\mathcal{R} = \{\mathbf r_n\}_{n=1}^{N}. The environment contains LL dominant scatterers, with each scatterer’s position encoded in spherical coordinates as pl=[rl,θl,ϕl]T\mathbf p_l=[r_l, \theta_l, \phi_l]^T, and its Cartesian counterpart sl=[rlsinθlcosϕl\mathbf s_l = [r_l\sin\theta_l\cos\phi_l, rlsinθlsinϕlr_l\sin\theta_l\sin\phi_l, rlcosθl]Tr_l\cos\theta_l]^T.

The frequency-selective channel vector on subcarrier kk (fk)(f_k) is

rn=[xn,0,zn]TR3\mathbf r_n=[x_n,0,z_n]^T \in \mathbb R^30

with rn=[xn,0,zn]TR3\mathbf r_n=[x_n,0,z_n]^T \in \mathbb R^31 the complex gain, rn=[xn,0,zn]TR3\mathbf r_n=[x_n,0,z_n]^T \in \mathbb R^32 the path delay, and the near-field steering vector

rn=[xn,0,zn]TR3\mathbf r_n=[x_n,0,z_n]^T \in \mathbb R^33

Stacking across rn=[xn,0,zn]TR3\mathbf r_n=[x_n,0,z_n]^T \in \mathbb R^34 subcarriers produces the composite measurement rn=[xn,0,zn]TR3\mathbf r_n=[x_n,0,z_n]^T \in \mathbb R^35, decomposable as

rn=[xn,0,zn]TR3\mathbf r_n=[x_n,0,z_n]^T \in \mathbb R^36

where rn=[xn,0,zn]TR3\mathbf r_n=[x_n,0,z_n]^T \in \mathbb R^37, rn=[xn,0,zn]TR3\mathbf r_n=[x_n,0,z_n]^T \in \mathbb R^38, and the delay vector rn=[xn,0,zn]TR3\mathbf r_n=[x_n,0,z_n]^T \in \mathbb R^39.

2. Subregion Partitioning and Signal Acquisition

MA spatial sampling is structured by partitioning the R={rn}n=1N\mathcal{R} = \{\mathbf r_n\}_{n=1}^{N}0 ports into R={rn}n=1N\mathcal{R} = \{\mathbf r_n\}_{n=1}^{N}1 disjoint subregions, each visiting R={rn}n=1N\mathcal{R} = \{\mathbf r_n\}_{n=1}^{N}2 ports indexed by R={rn}n=1N\mathcal{R} = \{\mathbf r_n\}_{n=1}^{N}3 (R={rn}n=1N\mathcal{R} = \{\mathbf r_n\}_{n=1}^{N}4). Signal acquisition in subregion R={rn}n=1N\mathcal{R} = \{\mathbf r_n\}_{n=1}^{N}5 on a pilot set of R={rn}n=1N\mathcal{R} = \{\mathbf r_n\}_{n=1}^{N}6 subcarriers (R={rn}n=1N\mathcal{R} = \{\mathbf r_n\}_{n=1}^{N}7) is

R={rn}n=1N\mathcal{R} = \{\mathbf r_n\}_{n=1}^{N}8

where R={rn}n=1N\mathcal{R} = \{\mathbf r_n\}_{n=1}^{N}9 extracts rows in LL0, LL1 selects pilot subcarriers, and LL2 models AWGN.

3. High-Precision Angle Estimation via Newtonized OMP

To circumvent near-field atom correlation in the full LL3 dictionary, angle estimation exploits an angular-only grid: reference distance LL4 is selected, and grid points are assigned via

LL5

for LL6, LL7 (LL8). The dictionary LL9 with pl=[rl,θl,ϕl]T\mathbf p_l=[r_l, \theta_l, \phi_l]^T0 supports sparse recovery via the MMV-CS problem: pl=[rl,θl,ϕl]T\mathbf p_l=[r_l, \theta_l, \phi_l]^T1

Newtonized Orthogonal Matching Pursuit (NOMP) refines detected angular atoms off-grid, iteratively applying coarse correlation (argmax), Newton optimization of the quadratic form pl=[rl,θl,ϕl]T\mathbf p_l=[r_l, \theta_l, \phi_l]^T2, and residual updating. This yields angle estimates pl=[rl,θl,ϕl]T\mathbf p_l=[r_l, \theta_l, \phi_l]^T3 for each subregion pl=[rl,θl,ϕl]T\mathbf p_l=[r_l, \theta_l, \phi_l]^T4.

4. Subregion Ray Clustering and Geometric Localization

Candidate rays are constructed as unit direction vectors (DVs)

pl=[rl,θl,ϕl]T\mathbf p_l=[r_l, \theta_l, \phi_l]^T5

formally collected into the set pl=[rl,θl,ϕl]T\mathbf p_l=[r_l, \theta_l, \phi_l]^T6 as indexed by angle candidates across subregions.

Clustering proceeds under the angular consistency criterion (Condition 1), where a set pl=[rl,θl,ϕl]T\mathbf p_l=[r_l, \theta_l, \phi_l]^T7 is accepted if

pl=[rl,θl,ϕl]T\mathbf p_l=[r_l, \theta_l, \phi_l]^T8

for all pl=[rl,θl,ϕl]T\mathbf p_l=[r_l, \theta_l, \phi_l]^T9, with threshold sl=[rlsinθlcosϕl\mathbf s_l = [r_l\sin\theta_l\cos\phi_l0 (e.g., sl=[rlsinθlcosϕl\mathbf s_l = [r_l\sin\theta_l\cos\phi_l1). Greedy growth produces clusters sl=[rlsinθlcosϕl\mathbf s_l = [r_l\sin\theta_l\cos\phi_l2 of sl=[rlsinθlcosϕl\mathbf s_l = [r_l\sin\theta_l\cos\phi_l3 rays, each interpreted as originating from one scatterer.

Least-squares localization of cluster sl=[rlsinθlcosϕl\mathbf s_l = [r_l\sin\theta_l\cos\phi_l4 solves

sl=[rlsinθlcosϕl\mathbf s_l = [r_l\sin\theta_l\cos\phi_l5

where sl=[rlsinθlcosϕl\mathbf s_l = [r_l\sin\theta_l\cos\phi_l6 is the subregion center of ray sl=[rlsinθlcosϕl\mathbf s_l = [r_l\sin\theta_l\cos\phi_l7. Setting the gradient to zero yields

sl=[rlsinθlcosϕl\mathbf s_l = [r_l\sin\theta_l\cos\phi_l8

with

sl=[rlsinθlcosϕl\mathbf s_l = [r_l\sin\theta_l\cos\phi_l9

Algorithmic steps are summarized in Algorithm 2, encompassing clustering, labeling, solving for rlsinθlsinϕlr_l\sin\theta_l\sin\phi_l0, and conversion to rlsinθlsinϕlr_l\sin\theta_l\sin\phi_l1 coordinates.

5. Sensing-Assisted Near-Field Channel Estimation

Recovered scatterer positions rlsinθlsinϕlr_l\sin\theta_l\sin\phi_l2 facilitate enhanced channel modeling. The refined dictionary rlsinθlsinϕlr_l\sin\theta_l\sin\phi_l3 is constructed from estimated positions. Aggregated pilot measurements from all subregions yield

rlsinθlsinϕlr_l\sin\theta_l\sin\phi_l4

with rlsinθlsinϕlr_l\sin\theta_l\sin\phi_l5, and

rlsinθlsinϕlr_l\sin\theta_l\sin\phi_l6

producing path gains. Delay and gain estimation refine channel parameters via delay-domain gridding and MMV least-squares, followed by path pruning and final channel synthesis

rlsinθlsinϕlr_l\sin\theta_l\sin\phi_l7

This closed-loop refinement improves the NMSE by rlsinθlsinϕlr_l\sin\theta_l\sin\phi_l8–rlsinθlsinϕlr_l\sin\theta_l\sin\phi_l9 dB over baseline methods.

6. Computational Complexity and Empirical Performance

The computational complexity analysis yields:

  • NOMP per subregion: rlcosθl]Tr_l\cos\theta_l]^T0 for correlation, with rlcosθl]Tr_l\cos\theta_l]^T1 per Newton refinement. Multiplied by rlcosθl]Tr_l\cos\theta_l]^T2 subregions;
  • Ray clustering: rlcosθl]Tr_l\cos\theta_l]^T3 (worst case);
  • Position LS per cluster: rlcosθl]Tr_l\cos\theta_l]^T4.

Total operational complexity approximates rlcosθl]Tr_l\cos\theta_l]^T5. Simulation results demonstrate that angle MAE and radial-distance MAE are typically halved compared to full-region OMP for SNR rlcosθl]Tr_l\cos\theta_l]^T6 dB, and that the NMSE of reconstructed channels achieves rlcosθl]Tr_l\cos\theta_l]^T7 dB at rlcosθl]Tr_l\cos\theta_l]^T8 dB SNR (versus rlcosθl]Tr_l\cos\theta_l]^T9 dB baseline). Optimal sensing has been observed for a kk0 subregion grid (kk1), with port measurement compression ratio kk2 exerting greater influence than pilot subcarrier ratio kk3.

7. Significance and Implications for ISAC

The movable antenna paradigm provides a substantive new degree of freedom for future ISAC systems: by leveraging large-range mechanical movement, near-field channel structure can be adaptively probed, revealing detailed geometric and electromagnetic scattering properties. The LSRC methodology demonstrates an efficient pipeline for fusing sparse multi-region angle estimates into robust 3D localization and refined channel estimation. This technique enables higher sensing resolution and augments communication reliability in multi-scatterer, near-field environments, supporting future broadband, location-aware wireless networks (Sun et al., 13 Jan 2026). A plausible implication is that further refinement of MA movement and sensing protocols could extend practical ISAC capabilities in urban or dense multipath scenarios.

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