Magnetic-nanoparticle-labeled antibodies flow over a capture surface printed directly on top of a giant-magnetoresistance (GMR) spin-valve sensor. Binding follows Langmuir kinetics for surface coverage θ (0–1):
dθ/dt = k_on·C·(1 − θ) − k_off·θ
An in-plane bias field Hbias magnetizes each superparamagnetic core to a moment m ≈ χ·V·Hbias (V = core volume, χ = susceptibility) that saturates at high field. Every bound particle sits a fixed height above the sensor's free layer and contributes a small dipole stray field there. The spin-valve's resistance responds to the total stray field through an approximately linear-then-saturating magnetoresistance transfer curve:
ΔR/R(H_sense) = ΔR/R_max · tanh(H_sense / H_sat)
H_sense ∝ N_bound · m / d³
- Analyte concentration C — sets the association rate k_on·C in the binding ODE; higher C drives θ toward saturation faster and to a higher plateau.
- Bias field Hbias — magnetizes the nanoparticle labels; too little field and each particle's stray signal is too weak to detect, too much saturates the sensor's transfer curve.
- Nanoparticle core size — sets the per-particle moment (moment scales with volume, i.e. size³), trading signal strength for particle diffusivity and steric crowding on the surface.
- Off-rate koff — how fast bound label falls back off; a low-affinity antibody (high k_off) caps the achievable signal even at high concentration.
Right panel: the top array is the capture surface viewed from directly above — drag to pan across the chip. Below it, the left strip shows the live ΔR/R trace and the right strip plots the sensor's tanh transfer curve with a moving dot marking the current operating point.
Real-world relevance: this is the operating principle behind lab-on-chip GMR/TMR biosensor platforms (e.g. MagArray-style point-of-care diagnostics) — the signal is a magnetic field measured electrically, largely immune to the optical scattering and autofluorescence that trip up colorimetric lateral-flow readouts.