Fiber Bragg Grating
A microscopic barcode burned into a glass thread that hears how hard you squeeze it.
A fiber Bragg grating (FBG) is a 1–20 mm long region inside a single-mode fiber's germanium-doped silica core where the refractive index has been periodically modulated, creating a wavelength-selective mirror at the Bragg wavelength λ_B = 2 n_eff Λ. The grating reflects a narrow band (~0.1–1 nm wide) and transmits all other wavelengths essentially unattenuated. Because λ_B shifts ~10 pm/°C with temperature and ~1.2 pm/µε with strain, FBGs are deployed as embedded distributed sensors in aircraft wings, wind-turbine blades, bridges, oil pipelines, and inside surgical catheters — and as low-loss wavelength-selective mirrors in fiber lasers and dispersion-compensation modules.
FBGs are typically inscribed by exposing photosensitive Ge-doped fiber to a periodic UV interference pattern from a 248 nm KrF or 193 nm ArF excimer laser, usually via a phase mask whose ±1 diffraction orders interfere on the fiber core. The UV-induced photochemistry breaks Ge–Si bonds and forms color centers, raising the refractive index by Δn ≈ 10⁻⁵–10⁻³ in the bright fringes. A 5 mm grating with Δn ≈ 10⁻⁴ achieves >90 % peak reflectivity. Reading is by an interrogator — a swept-wavelength laser or spectrometer with sub-picometer resolution. The Bragg shift versus measurand is Δλ_B/λ_B = (1−p_e)ε + (α+ξ)ΔT, where p_e ≈ 0.22 is the effective photoelastic coefficient, α ≈ 0.55 ppm/°C the thermal-expansion coefficient, and ξ ≈ 6.7 ppm/°C the thermo-optic coefficient. Hundreds of FBGs at distinct λ_B values can share a single fiber, addressed by wavelength-division multiplexing.
In plain terms
Imagine a glass straw with tiny rings etched inside at perfectly even intervals — like a microscopic xylophone. Blow one note in (one color of light) and only that note bounces back; everything else passes through. Now squeeze the straw: the rings get closer, so a slightly different note bounces back. By listening to which note returns, you can tell exactly how hard the squeeze was, or how hot the straw is, without touching it. That's a fiber Bragg grating.
Also called: FBG, in-fiber Bragg reflector, fiber grating sensor.
Why it matters
- Embeds nano-strain and temperature sensing into structures (aircraft, wind blades, bridges, oil wells) using a passive glass thread, immune to EMI.
- Standard low-loss narrowband mirror in fiber lasers and DFB/DBR fiber lasers — sub-kHz linewidth single-frequency outputs.
- Chirped FBGs compensate the chromatic dispersion of thousands of kilometers of installed submarine fiber in 10 cm of coiled grating.
- MRI-compatible medical sensing (catheter shape, pressure, temperature) — no metal in the patient.
Where it lives
- Embedded FBG arrays in Airbus A380 / Boeing 787 composite wings
- FBG strain monitors on long-span bridges (Akashi-Kaikyo, Stonecutters)
- Submarine telecom dispersion compensators (chirped FBGs)
- Surgical-catheter FBG shape sensors (Intuitive Surgical / academic)
Key numbers
- Typical λ_B: 1550 nm (C-band telecom)
- Grating period: ~528 nm (For 1550 nm, n_eff ≈ 1.468)
- Strain sensitivity: ~1.2 pm/µε
- Temperature sensitivity: ~10 pm/°C
- Reflection bandwidth: 0.1–1 nm
- Peak reflectivity: up to >99 %
Surprising facts
- A 5-mm grating inscribed by a single excimer-laser pulse can survive temperatures above 1,000 °C (with regenerated-FBG processing) and detect strains as small as one nanostrain — a length change of one part per billion.
- A single 1-meter length of fiber can host hundreds of FBGs at distinct Bragg wavelengths, each acting as an independent strain or temperature sensor — a massively parallel sensor array thinner than a human hair.
- Chirped FBGs perform the dispersion compensation of an entire transatlantic submarine fiber link in 10 cm of coiled fiber — replacing rooms of electronic dispersion-compensating modules.
Open questions
- Hydrogen-induced wavelength drift: FBGs deployed in subsea or fuel-cell environments absorb dissolved hydrogen, slowly altering the refractive index of the Ge-doped core and drifting λ_B over months without applied strain. Pre-annealing and hydrogen-free fiber selection mitigate but do not eliminate the effect.
- Polarization-dependent Bragg splitting: In slightly birefringent fiber, the two polarization eigenmodes have slightly different λ_B, producing a split or broadened reflection peak — typically 10–100 pm — that complicates picometer-scale wavelength tracking.
A short history
Photosensitivity in Ge-doped silica was discovered in 1978 by Hill, Fujii, Johnson, and Kawasaki at the Communications Research Centre Canada — they observed that a standing-wave Ar-ion laser pattern wrote a permanent grating in fiber. Phase-mask inscription (Hill et al. 1993) made FBGs reproducibly manufacturable. Erdogan's 1997 J. Lightwave Tech. paper standardized the analytical framework. By the 2000s FBGs had become standard components in fiber lasers, telecom dispersion compensation, and structural-health monitoring.
Sources
- Erdogan, J. Lightwave Technol. 15, 1277 (1997) — Fiber grating spectra (https://ieeexplore.ieee.org/document/618322)
- RP Photonics — Fiber Bragg gratings (https://www.rp-photonics.com/fiber_bragg_gratings.html)
- FBGS Technology — FBG Principle (https://fbgs.com/technology/fbg-principle/)
- Rao, Meas. Sci. Technol. 8, 355 (1997) — In-fiber Bragg grating sensors (https://iopscience.iop.org/article/10.1088/0957-0233/8/4/002)