Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Bandwidth-limited pulse
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
{{short description|Type of wave pulse}} {{refimprove|date=December 2009}} [[File:Duration-bandwidth product.gif|upright=2|thumb|right|The duration-bandwidth product depends on the shape of the power spectrum of the pulse.]] A '''bandwidth-limited pulse''' (also known as '''Fourier-transform-limited pulse''', or more commonly, '''transform-limited pulse''') is a [[pulse_(physics)|pulse]] of a [[wave]] that has the minimum possible duration for a given [[power spectrum|spectral]] [[Bandwidth (signal processing)|bandwidth]]. Bandwidth-limited pulses have a constant [[phase (waves)|phase]] across all frequencies making up the pulse. [[Optics|Optical]] pulses of this type can be generated by [[modelocking|mode-locked]] [[laser]]s. Any waveform can be disassembled into its [[spectral component]]s by [[Fourier analysis]] or [[Fourier transform]]ation. The length of a pulse thereby is determined by its {{em|[[Complex value|complex]]}} spectral components, which include not just their relative intensities, but also the relative positions ([[spectral phase]]) of these spectral components. For different pulse shapes, the minimum duration-bandwidth product is different. The duration-bandwidth product is minimal for zero phase-modulation. For example, <math>\mathrm{sech^2}</math> pulses have a minimum duration-bandwidth product of 0.315 while gaussian pulses have a minimum value of 0.441. A bandwidth-limited pulse can only be kept together if the [[dispersion (optics)|dispersion]] of the medium the wave is travelling through is zero; otherwise [[dispersion management]] is needed to revert the effects of unwanted spectral phase changes. For example, when an [[ultrashort pulse]] passes through a block of glass, the glass medium broadens the pulse due to [[group velocity dispersion]]. Keeping pulses bandwidth-limited is necessary to compress information in time or to achieve high field densities, as with [[ultrashort pulse]]s in [[Kerr-lens modelocking|modelocked lasers]]. ==Further reading== * {{cite book |title=Ultrashort Laser Pulse phenomena |author=J. C. Diels and W. Rudolph |isbn=978-0-12-215493-5 |year=2006 |publisher=New York, Academic}} {{DEFAULTSORT:Bandwidth-Limited Pulse}} [[Category:Optics]] [[Category:Nonlinear optics]] [[Category:Laser science]]
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)
Pages transcluded onto the current version of this page
(
help
)
:
Template:Cite book
(
edit
)
Template:Em
(
edit
)
Template:Refimprove
(
edit
)
Template:Short description
(
edit
)