Apodized fiber Bragg gratings manufactured with the phase plate process

Christophe Martinez; Sylvain Magne; Pierre Ferdinand

doi:10.1364/AO.41.001733

Applied Optics
Vol. 41,
Issue 9,
pp. 1733-1740
(2002)
•https://doi.org/10.1364/AO.41.001733

Apodized fiber Bragg gratings manufactured with the phase plate process

Christophe Martinez, Sylvain Magne, and Pierre Ferdinand

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Christophe Martinez, Sylvain Magne, and Pierre Ferdinand, "Apodized fiber Bragg gratings manufactured with the phase plate process," Appl. Opt. 41, 1733-1740 (2002)

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Abstract

We present a manufacturing method based on the dynamic use of phase plates to photowrite Bragg gratings. This process allows for control of the local value of the index modulation envelope in the grating. The application to apodized fiber Bragg gratings is discussed.

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Apodization	Parameters	L (mm)	Δn _mod (10^-4)
None		4	4
Gaussian	p = 2; G = 1	7.2	5.1
Super Gaussian	p = 1.5; G = 2	6.2	4.2

Plate	Condition
Plate	0 ≤ t ≤ T[1 - exp(-p ^2 G)]/2	T[1 - exp(-p ^2 G)]/2 ≤ t ≤ T
1	$z_{π} (t) = \frac{L}{2} + {\frac{L}{2 p}}^{2 G} \sqrt{ln (\frac{T}{T - 2 t})}$	z_π(t)=L
2	$z_{π} (t) = \frac{L}{2} - {\frac{L}{2 p}}^{2 G} \sqrt{ln (\frac{T}{T - 2 t})}$	z _π(t)=0

Apodization	Parameters	L (mm)	Δn _mod (10^-4)
None		4	4
Gaussian	p = 2; G = 1	7.2	5.1
Super Gaussian	p = 1.5; G = 2	6.2	4.2

Plate	Condition
Plate	0 ≤ t ≤ T[1 - exp(-p ^2 G)]/2	T[1 - exp(-p ^2 G)]/2 ≤ t ≤ T
1	$z_{π} (t) = \frac{L}{2} + {\frac{L}{2 p}}^{2 G} \sqrt{ln (\frac{T}{T - 2 t})}$	z_π(t)=L
2	$z_{π} (t) = \frac{L}{2} - {\frac{L}{2 p}}^{2 G} \sqrt{ln (\frac{T}{T - 2 t})}$	z _π(t)=0

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Applied Optics