Photonic generation of impulse ultrawideband signals with switchable shapes and polarities based on frequency-to-time mapping

H.-Y. Jiang; L.-S. Yan; J. Ye; W. Pan; B. Luo; Z.-Y. Chen; X.-H. Zou; X. Steve Yao

doi:10.1364/OL.37.005052

Optics Letters
Vol. 37,
Issue 24,
pp. 5052-5054
(2012)
•https://doi.org/10.1364/OL.37.005052

Photonic generation of impulse ultrawideband signals with switchable shapes and polarities based on frequency-to-time mapping

H.-Y. Jiang, L.-S. Yan, J. Ye, W. Pan, B. Luo, Z.-Y. Chen, X.-H. Zou, and X. Steve Yao

Not Accessible

Your library or personal account may give you access

Get PDF
Email
Share
Get Citation
Copy Citation Text
H.-Y. Jiang, L.-S. Yan, J. Ye, W. Pan, B. Luo, Z.-Y. Chen, X.-H. Zou, and X. Steve Yao, "Photonic generation of impulse ultrawideband signals with switchable shapes and polarities based on frequency-to-time mapping," Opt. Lett. 37, 5052-5054 (2012)

Export Citation
- BibTex
- Endnote (RIS)
- HTML
- Plain Text
Citation alert
Save article

Related Topics
Table of Contents Category
- Fourier Optics and Signal Processing
Optics & Photonics Topics
?

The topics in this list come from the Optics and Photonics Topics applied to this article.

About this Article
History
- Original Manuscript: August 22, 2012
- Revised Manuscript: October 23, 2012
- Manuscript Accepted: November 2, 2012
- Published: December 5, 2012

Abstract

A photonic approach to generate impulse ultrawideband (UWB) signals with switchable shapes and polarities based on the frequency-to-time mapping technique is proposed and demonstrated. UWB monocycle, doublet, and triplet signals with two polarities can be obtained by adjusting the switchable spectrum shaper.

Full Article | PDF Article

More Like This

Photonic ultrawideband impulse radio generation and modulation over a fiber link using a phase modulator and a delay interferometer

Jing Shao and Junqiang Sun
Opt. Lett. 37(16) 3471-3473 (2012)

Photonic ultrawideband impulse radio shape modulation based on dual-filter tuning

Jing Shao and Junqiang Sun
Opt. Lett. 38(2) 232-234 (2013)

Optical generation of polarity- and shape-switchable ultrawideband pulses using a chirped intensity modulator and a first-order asymmetric Mach–Zehnder interferometer

Shilong Pan and Jianping Yao
Opt. Lett. 34(9) 1312-1314 (2009)

Previous Article Next Article

Cited By

You do not have subscription access to this journal. Cited by links are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Figures (6)

You do not have subscription access to this journal. Figure files are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Tables (3)

You do not have subscription access to this journal. Article tables are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Types	Positive	Negative
Monocycle	$Δ λ \approx F$ ; $CS = 1 / 8 F$ ; $RA = 0.7$ ;	$Δ λ \approx F$ ; $CS = 1 / 8 F$ ; $RA = 0.7$ ;
Doublet	$Δ λ = 1 / 2 F$ ; $CS = 0$ ; $RA = 0.5$ ;	$Δ λ = 1 / 2 F$ ; $CS = 1 / 4 F$ ; $RA = 1$ ;
Triplet	$Δ λ = 2 / 5 F$ ; $CS = 1 / 8 F$ ; $RA = 0.6$ ;	$Δ λ = 2 / 5 F$ ; $CS = 1 / 8 F$ ; $RA = 0.6$ ;

	Polarity	DGD	${VOA}_{upper}$	${VOA}_{lower}$
Monocycle	P	$\sim 7.9 ps$	$\sim 3 dB$	$\sim 1.5 dB$
Monocycle	N	$\sim 7.5 ps$	$\sim 3 dB$	$\sim 1.5 dB$
Doublet	P	$\sim 14.7 ps$	$\sim 2 dB$	$\sim 0.9 dB$
Doublet	N	$\sim 14.4 ps$	$\sim 3.9 dB$	$\sim 0.2 dB$
Triplet	P	$\sim 18.1 ps$	$\sim 2 dB$	$\sim 0.9 dB$
Triplet	N	$\sim 18.5 ps$	$\sim 2 dB$	$\sim 0.9 dB$

	Monocycle		Doublet		Triplet
Polarity	P.	N.	P.	N.	P.	N.
$λ_{c} (GHz)$	$\sim 4$	$\sim 4$	$\sim 6$	$\sim 5$	$\sim 7$	$\sim 7$
${BW}_{10 dB} (GHz)$	$\sim 4$	$\sim 5$	$\sim 4$	$\sim 3$	$\sim 5$	$\sim 5$

Types	Positive	Negative
Monocycle	$Δ λ \approx F$ ; $CS = 1 / 8 F$ ; $RA = 0.7$ ;	$Δ λ \approx F$ ; $CS = 1 / 8 F$ ; $RA = 0.7$ ;
Doublet	$Δ λ = 1 / 2 F$ ; $CS = 0$ ; $RA = 0.5$ ;	$Δ λ = 1 / 2 F$ ; $CS = 1 / 4 F$ ; $RA = 1$ ;
Triplet	$Δ λ = 2 / 5 F$ ; $CS = 1 / 8 F$ ; $RA = 0.6$ ;	$Δ λ = 2 / 5 F$ ; $CS = 1 / 8 F$ ; $RA = 0.6$ ;

	Polarity	DGD	${VOA}_{upper}$	${VOA}_{lower}$
Monocycle	P	$\sim 7.9 ps$	$\sim 3 dB$	$\sim 1.5 dB$
Monocycle	N	$\sim 7.5 ps$	$\sim 3 dB$	$\sim 1.5 dB$
Doublet	P	$\sim 14.7 ps$	$\sim 2 dB$	$\sim 0.9 dB$
Doublet	N	$\sim 14.4 ps$	$\sim 3.9 dB$	$\sim 0.2 dB$
Triplet	P	$\sim 18.1 ps$	$\sim 2 dB$	$\sim 0.9 dB$
Triplet	N	$\sim 18.5 ps$	$\sim 2 dB$	$\sim 0.9 dB$

Abstract

Cited By

Figures (6)

Tables (3)

Optics Letters