Photonica

Graded-index fiber

An optical fiber whose core refractive index varies smoothly with radial position, typically following a near-parabolic profile. Equalizes the group velocity of different modes, dramatically increasing the bandwidth-distance product of multimode fiber.

A graded-index (GI) fiber has a refractive-index profile n(r)n(r) that varies continuously with radial position rr, rather than the abrupt step of step-index fiber. The standard profile is a power-law:

n(r)  =  {n112Δ(r/a)αr<an2=n112Δr>an(r) \;=\; \begin{cases} n_1 \sqrt{1 - 2\Delta (r/a)^\alpha} & r < a \\ n_2 = n_1 \sqrt{1 - 2\Delta} & r > a \end{cases}

where Δ=(n12n22)/(2n12)\Delta = (n_1^2 - n_2^2)/(2n_1^2) is the relative index difference and α\alpha is the profile parameter. For α=2\alpha = 2 the profile is parabolic; for α\alpha \to \infty it degenerates to step-index.

Why graded-index reduces modal dispersion. In step-index multimode fiber, the highest-order modes propagate at angles close to the critical angle, traveling longer geometric paths than the fundamental mode. This produces large modal dispersion — pulse broadening from differential mode delay.

In a graded-index fiber, light traveling at angles to the fiber axis spends more time in regions of lower refractive index (toward the cladding). Lower index means higher phase velocity (v=c/nv = c/n), which compensates for the longer geometric path. For the special case of α2\alpha \approx 2 (parabolic profile), this compensation is nearly exact: all bound modes propagate with the same group velocity to leading order.

The remaining modal dispersion in optimally-designed graded-index fiber comes from higher-order corrections; the dispersion residual is approximately:

Δτ/L    Δ28c/n1.\Delta \tau / L \;\approx\; \frac{\Delta^2}{8c/n_1}.

For Δ=0.01\Delta = 0.01 (n1=1.50n_1 = 1.50, n2=1.485n_2 = 1.485): residual modal dispersion 0.06\sim 0.06 ns/km — about 100× smaller than step-index multimode fiber.

Optimum profile parameter. The exact α\alpha that minimizes modal dispersion is wavelength-dependent and slightly less than 2:

αopt    2(12λn1N1ΔdN1dλ),\alpha_\text{opt} \;\approx\; 2 \left(1 - \frac{2 \lambda \, n_1}{N_1 \, \Delta} \frac{dN_1}{d\lambda}\right),

where N1N_1 is the group index. For silica-based fibers at 850 nm: αopt2.03\alpha_\text{opt} \approx 2.03. At 1300 nm: αopt2.01\alpha_\text{opt} \approx 2.01. Standard OM3/OM4/OM5 multimode fiber is manufactured with α2.0\alpha \approx 2.0, optimized as a compromise across the operating wavelength range.

Standard graded-index multimode fibers.

StandardCore diameterNABandwidth at 850 nmBandwidth at 1300 nm
OM1 (62.5/125, legacy)62.5 μm0.275200 MHz·km500 MHz·km
OM2 (50/125)50 μm0.20500 MHz·km500 MHz·km
OM3 (50/125, laser-optimized)50 μm0.202000 MHz·km500 MHz·km
OM4 (50/125, enhanced)50 μm0.204700 MHz·km500 MHz·km
OM5 (50/125, wide-band)50 μm0.203500 MHz·km (850 nm) + 1850 MHz·km (953 nm)

OM3 and OM4 are designed specifically for 850 nm VCSEL-launched applications (10G-SR, 40G-SR4, 100G-SR4 Ethernet). OM5 extends usable wavelength range to enable short-wavelength wavelength-division multiplexing (SWDM).

Refractive-index profile measurement. Standard techniques:

  • Refracted near-field (RNF): probe fiber with HeNe laser; measure refracted intensity from each radial position
  • Transmitted near-field with image processing: image the core under illumination with edge-detection
  • Spatial spectral interferometry: white-light interferometer scan reveals profile

Modern multimode fibers achieve α=2.0±0.005\alpha = 2.0 \pm 0.005 tolerance.

Manufacturing. Graded-index fibers are produced by varying the dopant concentration during preform deposition:

  1. Inside-tube deposition (MCVD) or outside-tube deposition (OVD) builds up the preform with controlled GeO₂ dopant concentration
  2. Concentration is varied across the core to produce the desired index profile
  3. Standard SiO₂ tubes serve as preform cladding
  4. Preform is collapsed and drawn into fiber

Manufacturing tolerances of Δα±0.005\Delta \alpha \pm 0.005 require very precise dopant concentration control. The challenge of achieving the exact optimum profile is the primary reason graded-index fiber is more expensive than step-index single-mode fiber.

Why single-mode is still step-index. Single-mode operation requires V<2.405V < 2.405; the mode shape is the LP01 Gaussian-like distribution that does not benefit from index grading. There's no advantage to graded-index in single-mode systems, so step-index is universally used.

Why multimode persists in datacom. Graded-index multimode fiber, paired with low-cost 850 nm VCSELs, provides cost-effective 10G/40G/100G short-reach (up to 100 m) interconnect in data centers. Compared to single-mode fiber (which requires expensive cooled DFBs or external modulators), multimode is dramatically cheaper for short distances. Single-mode dominates for >100> 100 m.

References: Saleh & Teich, Fundamentals of Photonics (3rd ed., 2019), Ch. 9; Snyder & Love, Optical Waveguide Theory (Chapman & Hall, 1983), Ch. 13 (graded-index modal analysis); TIA-492AAAD for OM4 specifications; IEC 60793-2-10 for international multimode standards.