Step 1: Recall the Bragg condition for a fiber Bragg grating.
A fiber Bragg grating reflects light strongly at the Bragg wavelength \(\lambda_B\), which is fixed by the effective refractive index \(n_{eff}\) of the fiber core and the physical period \(\Lambda\) of the grating. The first-order Bragg condition is
\[ \lambda_B = 2\, n_{eff}\, \Lambda \]
This comes from requiring the light reflected from successive grating planes to add up in phase, so the round trip over one grating period must equal one wavelength as measured inside the fiber.
Step 2: Rearrange the formula for the grating period.
\[ \Lambda = \frac{\lambda_B}{2\, n_{eff}} \]
Step 3: Substitute the given values.
With \(\lambda_B = 1550\) nm and \(n_{eff} = 1.44\):
\[ \Lambda = \frac{1550}{2 \times 1.44} = \frac{1550}{2.88} \]
\[ \Lambda = 538.194\ldots \text{ nm} \]
Final Answer:
Rounded off to two decimal places, the grating period is \(538.19\) nm.
\[ \boxed{538.19 \text{ nm}} \]