REVIEW 2 major objections 4 minor 5 cited by
Rotating two IRSs in unison yields a fourth-power SNR scaling in element count.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
T0 review · deepseek-v4-flash
2026-08-03 16:15 UTC pith:LM2OSV32
load-bearing objection Useful system-level study of double rotatable IRSs with a plausible PSO-based design, but the closed-form optimal azimuth in Proposition 1 is wrong as stated: the trig identity silently assumes nonnegative x-displacements and ignores constraint boundaries. the 2 major comments →
Cooperative Rotatable IRSs for Wireless Communications: Joint Beamforming and Orientation Optimization
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
For a cooperative double-IRS link with far-field propagation, the received SNR factorizes as the product of an aperture gain for IRS 1, an aperture gain for IRS 2, and a beamforming term that depends on phase shifts and transmit precoding. By optimizing the phases and the BS beamforming in closed form, the SNR reduces to maximizing the aperture-gain product F(Omega_1)F(Omega_2). Under line-of-sight channels and a planar deployment (both IRSs at z = 0), the paper proves that the optimal azimuth for IRS 1 is theta*_1 = (pi - Delta_1 - Delta_2)/2, where Delta_1 and Delta_2 are the angles of the BS-to-IRS-1 and IRS-1-to-IRS-2 directions, and that setting elevation to zero is optimal. This closed
What carries the argument
The central object is the aperture-gain factorization of Eq. (13), where the received SNR is written as (angle-dependent aperture gains of IRS 1 and IRS 2) times (a coherent beamforming gain). The aperture gains are products of the cosines of the incident and reflected elevation angles at each IRS, making the orientation angles Omega_1 and Omega_2 appear explicitly in the objective. The proof of the closed-form azimuth uses product-to-sum trigonometric identities to turn the aperture-gain product into a cosine that is minimized at the angle bisecting the two incident/reflected directions, yielding theta*_1. This factorization decouples orientation optimization from phase and beamforming opti
Load-bearing premise
The whole argument rests on the factorization of SNR in Eq. (13), which assumes far-field propagation and that all elements of each IRS have the same reflection amplitude, so that the aperture gain separates from the beamforming term; if near-field phase variations or element-dependent amplitudes matter, maximizing the aperture-gain product no longer maximizes SNR.
What would settle it
In a near-field setup or with a large IRS where element distances vary significantly, deploy two IRSs with the closed-form azimuth theta*_1 = (pi - Delta_1 - Delta_2)/2 and compare the measured SNR with the predicted maximum from the aperture-gain product; if the SNR does not track F(Omega_1)F(Omega_2), the factorization fails.
If this is right
- A planar double-IRS deployment needs only one rotational degree of freedom (azimuth) per IRS to achieve optimal SNR; elevation motors are unnecessary.
- The SNR with two rotatable IRSs scales as O(N^4), so doubling the element count from 900 to 1800 yields about 12 dB gain, compared with 6 dB for a single rotatable IRS.
- Enabling rotation lowers the total element count at which a double-IRS system beats a single-IRS system, making rotation a cost-effective alternative to adding more elements.
- An alternating-optimization plus particle-swarm algorithm handles the general Rician fading case, with closed-form optimal beamforming and phase shifts at each step.
- The aperture-gain product structure means orientation optimization can be performed independently of phase and beamforming optimization, simplifying deployment tuning.
Where Pith is reading between the lines
- The closed-form azimuth theta*_1 depends only on the geometry of the BS, IRS 1, and IRS 2, so orientation could be precomputed from known coordinates without any channel estimation, unlike phase shifts which require CSI.
- If the far-field equal-amplitude assumption fails in near-field or high-element-count regimes, the factorization breaks and orientation would need to be optimized jointly with element-wise phase and amplitude, likely requiring a different approach such as ray-tracing or full-wave simulation.
- The same aperture-gain product structure may generalize to IRS chains longer than two, suggesting that rotation optimization for multi-hop reflected links could follow the same pattern, with each hop contributing a cosine-product factor.
- The result suggests a simple deployment rule: align the normal of each IRS along the bisector of the incident and reflected directions; for a planar geometry this yields the optimal orientation without iterative search.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper considers a downlink system with two cooperative rotatable IRSs under an angle-dependent reflection model, and jointly optimizes BS transmit beamforming, passive beamforming at both IRSs, and the 2D rotations of the IRSs to maximize received SNR. Under LoS channels it proposes a PSO-based rotation search and derives a closed-form optimal azimuth for the planar case z1,1=z2,1=0; under Rician fading it proposes an AO-PSO algorithm. Numerical results claim substantial gains over fixed IRS schemes and show that double rotatable IRSs outperform a single rotatable IRS with O(N^4) versus O(N^2) scaling.
Significance. The motivating idea is timely: mechanically rotating IRSs to improve aperture alignment is a practically relevant degree of freedom. The O(N^4) versus O(N^2) comparison for double versus single rotatable IRSs is a useful quantitative claim, and the PSO/AO machinery, together with the closed-form beamforming and phase-shift steps, is sensible. However, the paper's headline analytical result—Proposition 1—contains a sign error in its trigonometric derivation and ignores the feasible-set boundary, so the advertised closed-form optimal azimuth is not generally correct. Since this result is advertised in the abstract and repeated in the conclusion, the central analytical contribution requires substantial repair. The paper does not provide code or multi-seed statistical analysis for the stochastic PSO runs, which further limits confidence in the numerical comparisons.
major comments (2)
- [Section III-A, Eqs. (21) and (24)] The proof of Proposition 1 uses the identity (a·u)/|a| = sin(theta+Delta) with Delta = arccos(a_y/|a|), but this identity is valid only when a_x >= 0; for a_x < 0 the correct expression is sin(theta-Delta). The paper applies the identity without tracking this sign. In the planar version of the paper's own geometry (p_{B,1}-p_{1,1}=(-7,-40), p_{2,1}-p_{1,1}=(5,-45)), one has Delta_1 ~ 169.9 deg and Delta_2 ~ 174.1 deg. Eq. (21) gives theta* ~ -81.9 deg, whereas the constrained maximizer of F_{theta1} is theta=-pi/2, which is larger by about 0.13 dB in F_{theta1}. Thus the closed-form azimuth in Eq. (21) is not generally optimal. The proof must use atan2-based piecewise expressions and must check the constraints (14)-(15): the unconstrained stationary point of the cosine can be outside the feasible interval, in which case the optimum is on the boundary.
- [Section III-A, final paragraph; Section V; Abstract] The statement that elevation rotation is unnecessary is sound only for a fixed theta for which the two dot products in (22)-(23) are nonnegative; it does not fix the azimuth error. Because of the sign mistake, the advertised conclusion that 1D rotation is sufficient for optimal performance in the planar deployment is unsupported. The same incorrect sign convention is used for the analogous IRS-2 azimuth formula theta_2* = (pi - Delta_2 - Dtilde_1)/2. The authors should replace the claimed closed form with a corrected piecewise boundary-aware solution, or explicitly downgrade this to a heuristic and rely on the PSO result.
minor comments (4)
- [Throughout] There are several typos and formatting issues: "light-of-sight" should be "line-of-sight" in the abstract; the caption of Fig. 1 says "The norm vector of IRS"; Section II contains "m∈ Mand" and similar spacing errors; Eq. (19) has missing parentheses around the product.
- [Section III-A, Eq. (24)] The notation is confusing: Eq. (24) defines F_{theta1} as a product of unnormalized dot products, but the subsequent trigonometric reexpression uses normalized dot products. Please make the normalization denominators explicit to avoid ambiguity.
- [Section III-B, convergence claim] The statement that the AO-PSO algorithm 'is guaranteed to converge' is too strong. The global-best fitness is non-decreasing only if the update rule explicitly retains the best particle, and random PSO moves can still leave the swarm in a local region. The numerical results should report feasibility rates and statistics over multiple independent seeds.
- [Section II, Eq. (13) and the paragraph before it] The SNR factorization relies on the far-field approximations t_{n1,m} ~ t_{1,1}, d_{n2,n1} ~ d_{1,1}, r_{n2} ~ r_1 for amplitudes. Because rotating the IRS changes the element positions relative to the global frame, the authors should state the validity regime of this approximation (array size versus distances) and comment on when element-wise amplitude and near-field phase variations could break the factorization.
Circularity Check
No significant circularity; the derivation is self-contained and the only self-citation ([8]) is background context, not load-bearing.
full rationale
The paper's derivation chain is not circular. The SNR expression in Eq. (13) is a far-field factorization under stated approximations, with the aperture-gain factors taken from an external reference [12] and the passive-beamforming/transmit-beamforming optimal forms taken from external reference [3]. Proposition 1 solves the resulting aperture-gain optimization; even if its trigonometric sign handling is questionable, that is a correctness issue, not a circular reduction. The PSO-based methods optimize the same objective that is later reported, which is standard for algorithm papers and does not constitute fitting a parameter and then calling it a prediction. The only self-citation is [8], an arXiv preprint by the same author group, used merely to motivate rotatable IRSs as a concept; it is not used to justify the paper's optimality claims or to import a uniqueness theorem. The O(N^4) scaling follows algebraically from Eq. (19) after the external decomposition, and the numerical upper bound is an internal consistency check rather than a circular validation. Thus the central claims have independent mathematical and algorithmic content, and no load-bearing step reduces to its own inputs.
Axiom & Free-Parameter Ledger
axioms (5)
- domain assumption Far-field approximation: all IRS elements share one reflection coefficient amplitude and distances are approximated by first-element distances.
- domain assumption Aperture gain model F(Omega)=cos(incident angle)cos(reflected angle) from [12].
- domain assumption LoS channels can be decomposed into outer products of signature vectors as in [3].
- domain assumption Rician NLoS components are independent and have distance-dependent variance.
- standard math PSO global-best fitness is monotonically non-decreasing and bounded, implying convergence.
read the original abstract
Rotatable intelligent reflecting surfaces (IRSs) introduce a new degree of freedom (DoF) for shaping wireless propagation by adaptively adjusting the orientation of IRSs. This paper considers an angle-dependent reflection model in a wireless communication system aided by two rotatable IRSs. Specifically, we study the joint design of the base station transmit beamforming, as well as the cooperative passive beamforming and orientation of the two IRSs, to maximize the received signal-to-noise ratio (SNR). Under the light-of-sight (LoS) channels, we first develop a particle swarm optimization (PSO) based method to determine the IRS rotation and derive an optimal rotation in a closed-form expression for a two-dimensional IRS deployment. Then, we extend the design to the general Rician fading channels by proposing an efficient alternating optimization and PSO (AO-PSO) algorithm. Numerical results validate the substantial gains achieved by the IRS rotation over fixed-IRS schemes and also demonstrate the superior performance of the double rotatable IRSs over a single rotatable IRS given a sufficient total number of IRS elements.
Figures
Forward citations
Cited by 5 Pith papers
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Multi-User MIMO with Rotatable Antennas and IRS: Joint Antenna Boresight and IRS Orientation Design
Coordinated rotation of BS antennas and IRS panel yields higher sum-rate than fixed-orientation or single-rotation baselines in an IRS-assisted multi-user MIMO setup.
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Movable antenna systems exhibit a fundamental tradeoff between movement duration for improved channels and transmission time, optimized via 1D search or a fitting method that yields a closed-form speed threshold below...
Reference graph
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