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Pinching Discretization Efficiency

Updated 28 December 2025
  • Pinching discretization efficiency is defined as the ratio of the ergodic rate of a discrete PAS to that of a continuous PAS, capturing performance loss due to finite pinching points.
  • Analytical models using dielectric-waveguide PASs yield closed-form expressions for metrics like outage probability and ergodic rate, highlighting trade-offs between antenna density and throughput.
  • Design guidelines derived from the analysis recommend optimal PA counts for different spatial dimensions to balance hardware simplicity with near-continuous performance in programmable wireless environments.

Pinching discretization efficiency quantifies the loss—or efficiency—incurred when a theoretically continuous actuator (such as a pinching antenna capable of arbitrary placement along a waveguide) is constrained to operate on a discrete, finite set of positions. In programmable wireless environments (PWEs), this metric rigorously characterizes how well a practical two-state pinching-antenna system (PAS) with a finite number of fixed pinching points can approximate the ideal continuous limit in terms of achievable throughput or ergodic data rate. Pinching discretization efficiency has become a central analytic tool in evaluating and optimizing the design of PASs and in engineering trade-offs between hardware simplicity and communication performance (Tyrovolas et al., 21 Dec 2025, Tyrovolas et al., 3 Nov 2025).

1. Definition and Formalism

Pinching discretization efficiency, denoted ηr\overline\eta_r or ηd\eta_d in the literature, is defined as the ratio of the ergodic achievable data rate of a discrete (two-state) PAS to that of the ideal continuous PAS: ηr=RRc\overline\eta_r = \frac{\overline R}{R_c} where

  • R\overline R: Ergodic rate with MM fixed pinching-antenna (PA) locations, activating exactly one per slot.
  • RcR_c: Ergodic rate when PAs can be formed at any real-valued position along the waveguide.

This definition encapsulates, in a single normalized scalar, the degree to which the discrete hardware approaches the ideal propagation control promise of continuous reconfigurability. By construction, 0<ηr10 < \overline\eta_r \leq 1, and ηr1\overline\eta_r \rightarrow 1 as MM \to \infty (i.e., as the discretization becomes vanishingly fine) (Tyrovolas et al., 21 Dec 2025, Tyrovolas et al., 3 Nov 2025).

2. Analytical Framework and Key Assumptions

The canonical analysis is based on a dielectric-waveguide PAS, where radiation is produced by selectively exciting one of MM pre-placed PAs along a waveguide of length DxD_x. The main modeling assumptions are:

  • PAs are located at xk=(2k1)δ/2x_k = (2k-1)\delta/2, with grid spacing δ=Dx/M\delta = D_x/M.
  • Each user is randomly positioned in the xyxy-plane, and the optimal PA (maximizing user SNR) is chosen in each access.
  • The signal undergoes exponential attenuation along the waveguide (eαxe^{-\alpha x}), with additional path-loss effects from the antenna to the user.

The received SNR for user (xm,ym,0)(x_m, y_m, 0) from the kkth PA is: γ(k)=ηPtexp(αxk)σ2[(xmxk)2+ym2+h2]\gamma^{(k)} = \frac{\eta P_t \exp(-\alpha x_k)}{\sigma^2[(x_m - x_k)^2 + y_m^2 + h^2]} where η=λ2/(16π2)\eta = \lambda^2/(16\pi^2) and hh is the waveguide height.

With these assumptions, the ergodic rate R\overline R is computed by integrating the log-rate over the user distribution and the discrete PA serving regions partitioned by proximity (Tyrovolas et al., 21 Dec 2025, Tyrovolas et al., 3 Nov 2025).

3. Closed-form Expressions, Region Partitioning, and PDE Calculation

For two-state PASs, the discrete spatial structure allows the entire axis to be partitioned into MM serving rectangles, each associated with a PA and width δ\approx \delta. With uniform user distribution, key outcomes include:

  • Outage Probability:

Po=k=1M[LkDxPl(Lk)+RkDxPl(Rk)]P_o = \sum_{k=1}^M \left[\frac{L_k}{D_x} P_l(L_k) + \frac{R_k}{D_x} P_l(R_k)\right]

Pl()P_l(\cdot) is the 1D outage probability, detailed in five piecewise expressions parameterized by A0,kA_{0,k}.

  • Ergodic Rate:

R=k=1M[LkDxCl(Lk)+RkDxCl(Rk)]\overline R = \sum_{k=1}^M \left[\frac{L_k}{D_x} C_l(L_k) + \frac{R_k}{D_x} C_l(R_k)\right]

Cl(Δ)=2ΔDyln2[Ii(C0,k+h2)+Ij(C0,k+h2)Ii(h2)Ij(h2)]C_l(\Delta) = \frac{2}{\Delta D_y \ln 2} \left[ I_i(C_{0,k} + h^2) + I_j(C_{0,k} + h^2) - I_i(h^2) - I_j(h^2) \right]

Ii()I_i(\cdot) and Ij()I_j(\cdot) are computed in closed form, and C0,k=CeαxkC_{0,k} = C e^{-\alpha x_k}.

Pinching discretization efficiency is then evaluated as ηr=R/Rc\overline\eta_r = \overline R / R_c, with RcR_c determined by the same formalism but with δ0\delta \rightarrow 0 (continuous limit) (Tyrovolas et al., 21 Dec 2025, Tyrovolas et al., 3 Nov 2025).

4. Intuitive Interpretation and Limiting Behavior

The PDE quantifies how closely a discrete, grid-constrained PAS emulates the ideal PAS with continuous pinching. At small MM (larger δ\delta), the closest available PA may be far from the user-optimal xpx_p^*, incurring SNR and rate loss. As MM increases, the discretization penalty diminishes due to finer spatial granularity.

However, a notable artifact is that, under exponential waveguide attenuation, further densification of PAs may eventually overshoot the true optimum, so ηr\overline\eta_r plateaus below unity rather than increasing indefinitely. This characterizes a fundamental performance saturation dictated by combined grid alignment and physical channel effects (Tyrovolas et al., 21 Dec 2025).

5. Design Criteria and Performance Guidelines

A key utility of pinching discretization efficiency lies in enabling principled design of PAS topologies. Analytical forms for ηr\overline\eta_r provide explicit trade-offs between the number of PAs (MM), the physical environment dimensions (Dx,DyD_x, D_y), and the desired proximity to the continuous optimum.

Key design recommendations, validated both numerically and by closed-form analysis, are:

  • For room-scale environments (Dx10mD_x \le 10\,\text{m}), M=2M=2 suffices for ηr0.95\overline\eta_r \ge 0.95.
  • For Dx=20mD_x = 20\,\text{m}, M3M \simeq 3.
  • For Dx=30mD_x = 30\,\text{m}, M4M \simeq 4.
  • For Dx=50mD_x=50\,\text{m}, M=8M=8–$12$ achieves ηr0.95\overline\eta_r \ge 0.95.
  • Further increments in MM yield rapidly diminishing returns, so hardware cost and complexity can be minimized by targeting ηr\overline\eta_r thresholds (e.g., $0.95$ or $0.99$) (Tyrovolas et al., 21 Dec 2025, Tyrovolas et al., 3 Nov 2025).

The penalty scales as O(δ2/h2)O(\delta^2/h^2), motivating design of δ\delta (and thus MM) such that the expected PA-user misalignment is below the characteristic vertical dimension.

6. Relationship with Energy Efficiency and Dual-Scale Resolution

Beyond raw ergodic rate, discretization efficiency interacts with broader system energy efficiency, particularly under dual-scale deployment (DSD) strategies. Here, coarse and fine grid resolutions are jointly optimized against actuation power cost, RF combining gain, and deployment protocol.

  • Coarse resolution Δc\Delta_c impacts amplitude alignment and transmission efficiency. Excessive coarseness (Δc1m\Delta_c \gg 1\,\text{m}) can cause substantial efficiency loss—up to 30%30\% in multi-PA systems.
  • Fine resolution Δr\Delta_r controls phase alignment and can induce a 15%\sim15\% drop if too coarse.
  • Practical energy-efficient PAS designs emerge by tuning Δc\Delta_c and Δr\Delta_r to achieve less than 1dB1\,\text{dB} amplitude quantization and <10<10^\circ phase error, respectively (Gan et al., 31 Oct 2025).
  • Overall system energy efficiency (spectral efficiency per total consumed power) is maximized by balancing RF, positioning, and mechanical costs with discretization-induced rate penalties using PDE as a guiding metric.

7. Numerical Validation and Practical Implications

Simulations consistently confirm the analytic framework, indicating:

  • For typical PWEs (α=0.05\alpha = 0.05, γt=90dB\gamma_t = 90\,\text{dB}, Dy=10mD_y = 10\,\text{m}, h=3mh=3\,\text{m}), ηr\overline\eta_r saturates quickly with moderate MM.
  • Even with moderate MM, near-optimal performance is accessible; e.g., for Dx=30mD_x=30\,\text{m}, ηr0.93\overline\eta_r \approx 0.93 at M=3M=3, and 0.96\approx 0.96 at M=4M=4.
  • The impact of increased waveguide attenuation (α\alpha) mildly depresses the plateau in ηr\overline\eta_r but does not shift the saturation point (Tyrovolas et al., 21 Dec 2025).

The analytic approach, validated by Monte Carlo, supports hardware-efficient deployment of PAS in practical indoor scenarios, with the ability to a priori size the number of discrete antennas for a target throughput or energy efficiency constraint.


References:

(Tyrovolas et al., 21 Dec 2025, Tyrovolas et al., 3 Nov 2025, Gan et al., 31 Oct 2025)

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