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Analyzing URA Geometry for Enhanced Near-Field Beamfocusing and Spatial Degrees of Freedom

Ahmed Hussain, Asmaa Abdallah, Abdulkadir Celik, Emil Björnson, Ahmed M. Eltawil

Abstract

With the deployment of large antenna arrays at high-frequency bands, future wireless communication systems are likely to operate in the radiative near-field. Unlike far-field beam steering, near-field beams can be focused on a spatial region with a finite depth, enabling spatial multiplexing in the range dimension. Moreover, in the line-of-sight MIMO near-field, multiple spatial degrees of freedom (DoF) are accessible, akin to a scattering- rich environment. In this paper, we derive the beamdepth for a generalized uniform rectangular array (URA) and investigate how the array geometry influences near-field beamdepth and its limits. We define the effective beamfocusing Rayleigh distance (EBRD), to present a near-field boundary with respect to beamfocusing and spatial multiplexing gains for the generalized URA. Our results demonstrate that under a fixed element count constraint, the array geometry has a strong impact on beamdepth, whereas this effect diminishes under a fixed aperture length constraint. Moreover, compared to uniform square arrays, elongated configurations such as uniform linear arrays (ULAs) yield narrower beamdepth and extend the effective near-field region defined by the EBRD. Building on these insights, we design a polar codebook for compressed-sensing-based channel estimation that leverages our findings. Simulation results show that the proposed polar codebook achieves a 2 dB NMSE improvement over state-of-the-art methods. Additionally, we present an analytical expression to quantify the effective spatial DoF in the near-field, revealing that they are also constrained by the EBRD. Notably, the maximum spatial DoF is achieved with a ULA configuration, outperforming a square URA in this regard.

Analyzing URA Geometry for Enhanced Near-Field Beamfocusing and Spatial Degrees of Freedom

Abstract

With the deployment of large antenna arrays at high-frequency bands, future wireless communication systems are likely to operate in the radiative near-field. Unlike far-field beam steering, near-field beams can be focused on a spatial region with a finite depth, enabling spatial multiplexing in the range dimension. Moreover, in the line-of-sight MIMO near-field, multiple spatial degrees of freedom (DoF) are accessible, akin to a scattering- rich environment. In this paper, we derive the beamdepth for a generalized uniform rectangular array (URA) and investigate how the array geometry influences near-field beamdepth and its limits. We define the effective beamfocusing Rayleigh distance (EBRD), to present a near-field boundary with respect to beamfocusing and spatial multiplexing gains for the generalized URA. Our results demonstrate that under a fixed element count constraint, the array geometry has a strong impact on beamdepth, whereas this effect diminishes under a fixed aperture length constraint. Moreover, compared to uniform square arrays, elongated configurations such as uniform linear arrays (ULAs) yield narrower beamdepth and extend the effective near-field region defined by the EBRD. Building on these insights, we design a polar codebook for compressed-sensing-based channel estimation that leverages our findings. Simulation results show that the proposed polar codebook achieves a 2 dB NMSE improvement over state-of-the-art methods. Additionally, we present an analytical expression to quantify the effective spatial DoF in the near-field, revealing that they are also constrained by the EBRD. Notably, the maximum spatial DoF is achieved with a ULA configuration, outperforming a square URA in this regard.
Paper Structure (41 sections, 6 theorems, 46 equations, 19 figures, 2 tables, 1 algorithm)

This paper contains 41 sections, 6 theorems, 46 equations, 19 figures, 2 tables, 1 algorithm.

Key Result

Theorem 1

For a generalized URA, the $\unit[3]{dB}$ beamdepth $r_{\mathrm{\hbox{BD} }}$ obtained by focusing a beam at a distance $r_{\mathrm{\hbox{F}}}$ from the BS is given by

Figures (19)

  • Figure 1: URA setup and a single prospective user.
  • Figure 2: Near-field beam with finite beamdepth and beamwidth in the axial and lateral dimensions, respectively.
  • Figure 3: Numerical and analytical beamdepth for a $(256 \times 16)$URA operating at $\unit[30]{GHz}$. The zoom inset highlights the beamdepth for focus distances less than $2D = 5$.
  • Figure 4: Near-field boundary in terms of ERD and EBRD for a ULA. Here $f_c = \unit[28]{GHz}$, $N_{\mathrm{\hbox{BS} }}=256$, $r_{\mathrm{\hbox{RD} }}=\unit[348]{m}$.
  • Figure 5: Beamdepth with respect to azimuth angle $\varphi$ for different array configuration $\eta$ and elevation angle $\theta$.
  • ...and 14 more figures

Theorems & Definitions (10)

  • Theorem 1
  • proof
  • Theorem 2
  • proof
  • Corollary 1
  • Corollary 2
  • Theorem 3
  • proof
  • Theorem 4
  • proof