Abstract
The generation of phase-locked pulses with a well-defined electric field is essential for applications like high harmonic pulse generation [1] or precision metrology [2]. Active and passive locking schemes have been widely demonstrated utilizing Ti:sapphire technology. However, active stabilization requires cumbersome feedback loops and a locking of fCEO = 0 is very challenging at the full repetition rate of the laser.
© 2011 Optical Society of America
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