450 likes | 477 Views
Explore the dynamics of group velocities associated with light pulses and the manipulation of light speed in dispersive media for fast light effects. Learn about phase sensitivity amplification, group delay, and applications in mode-locked lasers.
E N D
Group Velocity and Ultrafast Optics Ultrafast 2016 James Hendrie
Velocities Associated with Light Pulses Phase Ray Group Envelope
Derivation of Group Velocity t z z = ct z = vt
Slow/Fast Light Manipulation of the Group Velocity within a dispersive medium
(dk/dΩ) ≡ Group Delay/L • Choosing materials that manipulate the speed at which light propagates Small (dk/dΩ) ≡ “Fast Light” • The idea that light travels much faster in materials with these small values of dk/dΩ “Fast Light”≡ Phase Sensitivity is Amplified • Large group delays amount to additional phase shift as light travels through the material.
Group Delay NOT GROUP VELOCITY!!!
Carrier Envelope Offset Beat Note
IPI Schematic Beat Note Measurement Phase Alteration D
Nested Fabry-Perot in Mode-Locked Lasers to Monitor Minute Changes of Index James Hendrie, Koji Masuda, Adam Hecht, Jean-Claude Diels, and Ladan Arissian CLEO 2015 Ultrafast Class 2016
Motivation • Mode-locked lasers generate frequency combs which are sensitive to their parent cavities. • Inserting an etalon into the cavity generates a nested comb comprised of two repetition rates. • The ratio of these repetition rates can be used as an accurate measure of the optical path within the etalon.
Bunch Generation Pics from pics from latest paper
Bunch Generation Normalized Pulse Energy Time (nano-sec) t
Bunch Generation 0 Center of Gravity Shift (s) • Pulse bunch reaches steady state condition after many roundtrips Number of Pulses 0 100 200 300 400 500 600 700 800 900 1000 Number of Round Trips NRT = 1000 a = 0.0002 R = 0.05
Gaussian in the Steady State Regime 0.15 20 100 500 Laser Cavity Round Trips 80 15 0.1 60 Normalized Pulse Energy 10 Center of Gravity Number of Pulses 40 0.05 5 20 0 0 200 300 400 500 600 700 800 900 1000 100 20 30 40 50 60 Laser Cavity Round Trips Fabry-Perot Cavity Round Trips Koji Masuda, James Hendrie, Jean Claude Diels and Ladan Arissian; Envelope, Group and Phase velocities in a nested frequency comb, Under Review.
Fourier Transformation 146 ps 6.4 ns 1 ns Time 155 MHz 6.8 GHz 1 GHZ Frequency
Pump Power Effect on Repetition Rate ML Cavity FP Cavity
Resonant Frequencies The central optical frequency, is resonant with both cavities Cavity and FP frequencies are defined via group indices
Frequency Ratio Want to measure this!! Group indices must be constant at each point
Three Experiments Temperature Radiation Ring Laser Gyroscope
Temperature By changing the applied temperature of an intra-cavity Fabry-Perot etalon, one observes a change in frequency ratio.
Experimental Example SMALL Index changes due to applied heat SMALL
Temperature Diffusion in Glass Cap View Side View x z y
Center Line • Temperature change in the center of the etalon is very small
Fabry-Perot Angle Scan Internal Angle (milli radians)
Radiation K. Masuda, E. I. Vaughan, L. Arissian, J. P. Hendrie, J. Cole, J. -C. Diels, and A. A. Hecht, Novel techniques for high precision refractive index measurements, and application to assessing neutron damage and dose in crystals, Nuclear Instruments and Methods A (2014).
Gyro Explanation • Counter propagating beams sharing a single cavity see equal and opposite phase shifts throughout the duration of any applied rotation to that cavity
Three Descriptions • Standing wave created by counter propagating beams • Doppler Shift • Counter propagating beams see different perimeters These descriptions hold true in both cw and pulsed operations!! The Gyro effect is inherently due to phase velocity!!
Enhanced Gyro Derivation Taylor Expansion
Current Results Blue -> With FP Red -> Without FP