Reconstruction of polarization-shaped laser pulses after a hollow-core fiber using backreflection

Georg Achazi; Alexander Patas; Fabian Weise; Monika Pawłowska; Albrecht Lindinger

doi:10.1364/AO.50.000915

Reconstruction of polarization-shaped laser pulses after a hollow-core fiber using backreflection

Georg Achazi, Alexander Patas, Fabian Weise, Monika Pawłowska, and Albrecht Lindinger

Applied Optics
Vol. 50,
Issue 6,
pp. 915-923
(2011)
•https://doi.org/10.1364/AO.50.000915

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Georg Achazi, Alexander Patas, Fabian Weise, Monika Pawłowska, and Albrecht Lindinger, "Reconstruction of polarization-shaped laser pulses after a hollow-core fiber using backreflection," Appl. Opt. 50, 915-923 (2011)

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Related Topics
Table of Contents Category
- Ultrafast Optics
Optics & Photonics Topics
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The topics in this list come from the OSA Optics and Photonics Topics applied to this article.
Previously assigned OCIS codes
- Fiber optics (060.2310)
- Pulse shaping (320.5540)
- Ultrafast technology (320.7160)

About this Article
History
- Original Manuscript: November 10, 2010
- Revised Manuscript: January 5, 2011
- Manuscript Accepted: January 7, 2011
- Published: February 17, 2011

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Abstract

We present a method to reconstruct the pulse shape of polarization-shaped femtosecond laser pulses after a hollow-core photonic crystal fiber by reflecting the pulses back through the fiber. First, a procedure is introduced to receive the optical fiber properties and generate parametrically shaped pulses after propagation through the fiber. Changes of the fiber’s birefringence by mechanical stress are examined to investigate the correlation between the pulse shapes after one and two passes through the fiber. Finally, we demonstrate the characterization of the pulse after one pass through the fiber by calculating the pulse shape from the measured pulse after two passes.

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Parameter	s Pulse	f Pulse
Pulse position	$- 570 fs$	$+ 570 fs$
Linear chirp	$- 8250 {fs}^{2}$	$8250 {fs}^{2}$
Quadratic chirp	$- 8.0 \times 10^{5} {fs}^{3}$	$- 4.5 \times 10^{5} {fs}^{3}$
Cubic chirp	$- 5.5 \times 10^{6} {fs}^{4}$	$3.2 \times 10^{6} {fs}^{4}$

Parameter	Pulse 1	Pulse 2	Pulse 3
Polarization	f	s	s
Zero-order phase	$0.535 \times π$	0	0
Pulse position	$- 390 fs$	$818 fs$	$187 fs$
Linear chirp	$- 11, 000 {fs}^{2}$	$7320 {fs}^{2}$	$7320 {fs}^{2}$
Quadratic chirp	$7.56 \times 10^{5} {fs}^{3}$	$5.75 \times 10^{5} {fs}^{3}$	$5.75 \times 10^{5} {fs}^{3}$
Cubic chirp	$- 5.23 \times 10^{6} {fs}^{4}$	$6.4 \times 10^{6} {fs}^{4}$	$6.4 \times 10^{6} {fs}^{4}$

Parameter	s Pulse	f Pulse
Pulse position	$- 570 fs$	$+ 570 fs$
Linear chirp	$- 8250 {fs}^{2}$	$8250 {fs}^{2}$
Quadratic chirp	$- 8.0 \times 10^{5} {fs}^{3}$	$- 4.5 \times 10^{5} {fs}^{3}$
Cubic chirp	$- 5.5 \times 10^{6} {fs}^{4}$	$3.2 \times 10^{6} {fs}^{4}$

Parameter	Pulse 1	Pulse 2	Pulse 3
Polarization	f	s	s
Zero-order phase	$0.535 \times π$	0	0
Pulse position	$- 390 fs$	$818 fs$	$187 fs$
Linear chirp	$- 11, 000 {fs}^{2}$	$7320 {fs}^{2}$	$7320 {fs}^{2}$
Quadratic chirp	$7.56 \times 10^{5} {fs}^{3}$	$5.75 \times 10^{5} {fs}^{3}$	$5.75 \times 10^{5} {fs}^{3}$
Cubic chirp	$- 5.23 \times 10^{6} {fs}^{4}$	$6.4 \times 10^{6} {fs}^{4}$	$6.4 \times 10^{6} {fs}^{4}$

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