The Cascaded Channel and the System Model

The Two-Hop Signal Path

An RIS does not transmit; it only reflects. So the signal reaching the user arrives via two hops: a first hop from the base station (BS) to the RIS, and a second hop from the RIS to the user equipment (UE). This two-hop geometry is not a detail β€” it is the reason RIS channels behave differently from conventional single-hop links, and it is the reason every optimization problem in this book takes the shape it does.

Definition:

Canonical RIS-Aided System Model

Consider a downlink narrowband system with:

  • a base station equipped with NtN_t antennas,
  • an RIS with NN passive reflecting elements,
  • a single-antenna user equipment (the extension to NrN_r receive antennas is straightforward and treated in Chapter 3).

Define the three physical channels:

  • H1∈CNΓ—Nt\mathbf{H}_1 \in \mathbb{C}^{N \times N_t}: BS-to-RIS channel (the incident wavefront at the RIS).
  • h2∈CN\mathbf{h}_2 \in \mathbb{C}^{N}: RIS-to-UE channel (one column, since the UE has a single antenna).
  • hd∈CNt\mathbf{h}_d \in \mathbb{C}^{N_t}: direct BS-to-UE channel (often blocked in RIS deployments).

Let v∈CNt\mathbf{v} \in \mathbb{C}^{N_t}, βˆ₯vβˆ₯=1\|\mathbf{v}\| = 1, be the BS beamforming vector, let Ξ¦=diag(ejΞΈ1,…,ejΞΈN)\boldsymbol{\Phi} = \text{diag}(e^{j\theta_1}, \ldots, e^{j\theta_N}) be the RIS phase-shift matrix, and let s∈Cs \in \mathbb{C} be the data symbol with E[∣s∣2]=Pt\mathbb{E}[|s|^2] = P_t. The received signal at the UE is

y=(hdH+h2HΦ H1)⏟heffHv s+w,w∼CN(0,Οƒ2).y = \underbrace{\big(\mathbf{h}_d^H + \mathbf{h}_2^H \boldsymbol{\Phi}\, \mathbf{H}_1\big)}_{\mathbf{h}_{\text{eff}}^H} \mathbf{v}\, s + w, \qquad w \sim \mathcal{CN}(0, \sigma^2).

The bracketed 1Γ—Nt1 \times N_t row vector

β€…β€ŠheffHβ€…β€Š=β€…β€ŠhdHβ€…β€Š+β€…β€Šh2HΦ H1β€…β€Š\boxed{\;\mathbf{h}_{\text{eff}}^H \;=\; \mathbf{h}_d^H \;+\; \mathbf{h}_2^H \boldsymbol{\Phi}\, \mathbf{H}_1\;}

is the effective end-to-end channel seen by the BS beamformer.

Notice the crucial structural fact: the RIS phase shifts enter heff\mathbf{h}_{\text{eff}} linearly via the diagonal matrix Ξ¦\boldsymbol{\Phi}, but Ξ¦\boldsymbol{\Phi} is constrained to the non-convex unit-modulus torus. The system is linear in v\mathbf{v}, linear in Ξ¦\boldsymbol{\Phi}, but the joint feasibility set of (v,Ξ¦)(\mathbf{v}, \boldsymbol{\Phi}) is not convex. This is the root of nearly every difficulty and nearly every algorithm in this book.

,

Theorem: Diagonal Factorization of the Cascaded Channel

For any h2∈CN\mathbf{h}_2 \in \mathbb{C}^N and any diagonal Ξ¦=diag(Ο•1,…,Ο•N)\boldsymbol{\Phi} = \text{diag}(\phi_1, \ldots, \phi_N),

h2HΞ¦H1β€…β€Š=β€…β€ŠΟ•T(h2βˆ—βŠ™H1)β€…β€Š=β€…β€ŠΟ•Tdiag(h2βˆ—) H1,\mathbf{h}_2^H \boldsymbol{\Phi} \mathbf{H}_1 \;=\; \boldsymbol{\phi}^T \big( \mathbf{h}_2^* \odot \mathbf{H}_1 \big) \;=\; \boldsymbol{\phi}^T \text{diag}(\mathbf{h}_2^*)\, \mathbf{H}_1,

where Ο•=[Ο•1,…,Ο•N]T\boldsymbol{\phi} = [\phi_1, \ldots, \phi_N]^T and βŠ™\odot denotes row-wise element-wise multiplication (i.e., h2βˆ—\mathbf{h}_2^* is broadcast against the rows of H1\mathbf{H}_1).

This identity is a simple but pivotal algebraic rearrangement: it turns the expression h2HΦH1\mathbf{h}_2^H \boldsymbol{\Phi} \mathbf{H}_1, which looks trilinear in (h2,ϕ,H1)(\mathbf{h}_2, \boldsymbol{\phi}, \mathbf{H}_1), into something linear in ϕ\boldsymbol{\phi}. Every RIS optimization algorithm exploits this.

Key Takeaway

The RIS channel is linear in Ο•\boldsymbol{\phi} β€” even though the optimization is non-convex. The difficulty of RIS beamforming does not come from the objective (which is a simple quadratic form in Ο•\boldsymbol{\phi}) but from the feasibility set {βˆ£Ο•n∣=1}\{|\phi_n| = 1\}. This separation of "easy objective" and "hard constraint" is why SDR, manifold optimization, and alternating methods all apply.

Example: Received SNR for a Single-User MISO-RIS Link

A BS with NtN_t antennas transmits ss with beamformer v\mathbf{v}, βˆ₯vβˆ₯=1\|\mathbf{v}\| = 1, transmit power PtP_t. The direct path hd\mathbf{h}_d is blocked (hd=0\mathbf{h}_d = \mathbf{0}). The RIS has NN elements with phase-shift matrix Ξ¦\boldsymbol{\Phi}. Noise is CN(0,Οƒ2)\mathcal{CN}(0, \sigma^2). Derive an expression for the received SNR.

Common Mistake: The Ο•T\boldsymbol{\phi}^T vs Ο•H\boldsymbol{\phi}^H Trap

Mistake:

A student writes h2HΦH1=ϕHM\mathbf{h}_2^H \boldsymbol{\Phi} \mathbf{H}_1 = \boldsymbol{\phi}^H \mathbf{M} and proceeds to optimize in ϕH\boldsymbol{\phi}^H.

Correction:

The factorization uses Ο•T\boldsymbol{\phi}^T, not Ο•H\boldsymbol{\phi}^H. This is because Ξ¦\boldsymbol{\Phi} is a diagonal matrix of the non-conjugated phase shifts, so the sum βˆ‘n(h2)nβˆ—Ο•nβ‹―\sum_n (\mathbf{h}_2)_n^* \phi_n \cdots pulls out Ο•n\phi_n (not Ο•nβˆ—\phi_n^*). Getting the transpose wrong flips the sign of the phase-compensation term and sends the optimization in the opposite direction. Always double-check: is the symbol you are extracting conjugated in the original expression, or not?

Effective Channel Gain vs. RIS Phase Alignment

Visualize how the magnitude βˆ£Ο•Ta∣2|\boldsymbol{\phi}^T \mathbf{a}|^2 varies as the RIS phases progressively align with the coefficient vector a\mathbf{a}. At the "aligned" end (Ο•n⋆=eβˆ’jarg⁑(an)\phi_n^\star = e^{-j\arg(a_n)}) the magnitude equals βˆ₯aβˆ₯12\|\mathbf{a}\|_1^2, the peak achievable by any unit-modulus Ο•\boldsymbol{\phi}.

Parameters
32

More elements widen the gap between random and aligned.

0.5

$0$ = random phases, $1$ = matched-filter phases.