basic principles of ultrafast lasers components of ultrafast laser system pump hr gain oc...
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Basic principles of ultrafast lasers
Components of ultrafast laser system Components of ultrafast laser system Pump
HR
Gain
OC
Mode-locking
Mechanism
Dispersion
Compensation
Cavity modesCavity modes
n= 2 L/n f = c/2 L
Concepts of Mode Locking
Out of phase
RANDOM phase for all the laser phase for all the laser modesmodes Irradiance vs. Time
TimeTime TimeTime
Out of phaseOut of phase Out of phaseOut of phaseIn phase
LOCKED phases for all the laser modes phases for all the laser modes
Mode locking is a method to obtain ultrafast pulses from lasers, which are then called mode-locked lasers mode
Basic principles of ultrafast lasers
Bandwidth vs PulsewidthBandwidth vs Pulsewidth
narrow spectrum
continuous wave (CW)
broader spectrum
pulses (mode-locked)
broadest spectrum
shortest pulses
bandwidth
duration
= const.
Active mode-locking Acousto-optic modulator Synchronous pump mode-locking
Passive mode-locking Saturable absorber (dye, solid state) Optical Kerr effect
Mode-locking Mechanisms
Pow
er
Time
Pow
er
Time
cwcw cw MLcw MLP
ower
Time
Q-switchQ-switch Pow
erTime
Q-sw.MLQ-sw.ML
Types of Laser Output
Low-intensity beam
High-intensity ultrashort pulse
Focused pulse
Kerr medium (n = n0 + n2I)
Kerr-Lensing
Intensity dependent refractive index: n = n0 + n2I(x,t)
Spatial (self-focusing)• provides loss modulation with suitable placement of gain medium (and a hard aperture)
Temporal (self-phase modulation)• provides pulse shortening mechanism with group velocity dispersion
Optical Kerr Effect
Refractive index depends on light intensity: n (I)= n + n2 I
self phase modulation dueto temporal intensity variation
self-focusing due totransversal mode profile
Optical Kerr Effect
Optical pulse in a transparent medium stretches because of GVD
Group Velocity Dispersion (GVD)
• v = c / n – speed of light ina medium
• n –depends on wavelength, dn/dl < 0 – normal dispersion
• v = c / n – speed of light ina medium
• n –depends on wavelength, dn/dl < 0 – normal dispersion
• High-intensity modes have smaller cross-section and are less lossy. Thus, Kerr-lens is similar to saturating absorber!
• Some lasing materials (e.g. Ti:Sapphire) can act as Kerr-media
• Kerr’s effect is much faster than saturating absorber allowing one generatevery short pulses (~5 fs).
• High-intensity modes have smaller cross-section and are less lossy. Thus, Kerr-lens is similar to saturating absorber!
• Some lasing materials (e.g. Ti:Sapphire) can act as Kerr-media
• Kerr’s effect is much faster than saturating absorber allowing one generatevery short pulses (~5 fs).
Prism compensator
Wavelengthtuning mask
“Red” component of the pulse propagates in glass where group velocity is smaller than for the “blue” component
GVD CompensationGVD can be compensated if optical pathlength is different for “blue” and “red”
components of the pulse.
Components of an Ultrafast Laser
Pulse shortening mechanism•Self phase modulation and group velocity dispersion
Dispersion Compensation
Starting Mechanism
Regenerative initiation•Cavity perturbation•Saturable Absorber (SESAM)
Cavity configuration of Ti:Sapphire laser
Tuning range 700-1000 nmPulse duration < 20 fs Pulse energy < 10 nJRepetition rate 80 – 1000 MHzPump power: 2-15 W
Tuning range 700-1000 nmPulse duration < 20 fs Pulse energy < 10 nJRepetition rate 80 – 1000 MHzPump power: 2-15 W
Typical applications:
• time-resolved emissionstudies• multi-photon absorptionspectroscopy
• imaging
Typical applications:
• time-resolved emissionstudies• multi-photon absorptionspectroscopy
• imaging
Amplification of fs Pulses
Oscillator Stretcher Amplifier Compressor
• Stretch femtosecond oscillator pulse by 103 to 104 times• Amplify• Recompress amplified pulse
• Stretch femtosecond oscillator pulse by 103 to 104 times• Amplify• Recompress amplified pulse
Concept:Concept:
Chirped pulse amplification
• Femtosecond pulses can be amplified to petawatt powers• Pulses so intense that electrons stripped rapidly from atoms
• Femtosecond pulses can be amplified to petawatt powers• Pulses so intense that electrons stripped rapidly from atoms