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1
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- Chengquan Li, Eric Moon, Zuoliang Duan, Jason Tackett ,Zenghu Chang
- April-05th-2006
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2
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- Important for experiments utilizing identical few-cycle laser pulses
- CE Phase-dependent research
- Can use a stabilized frequency comb to perform spectroscopy.
- More applications to come!
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3
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4
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5
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6
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7
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8
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- The CE phase change can be controlled by locking the offset frequency, f0,
to a known frequency.
- In the case of the KLS, f0 is set equal to one-quarter of the
repetition rate of the oscillator.
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9
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- The KLS utilizes a Kerr-Lens Mode locked Ti:Sapphire oscillator emitting
a ~77 million pulses per second.
- The pulses are roughly 12 fs at the output of the laser and carry nJ
energy per pulse.
- The oscillator is the starting point for the self-referencing technique.
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10
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11
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12
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- A second f-2f interferometer after the KLS amplifier provides a means
for quantifying the CE phase stabilization stability.
- 10% of the KLS amplifier output is sent to the experimental setup.
- White-light is generated in a sapphire plate and a BBO crystal provides
second-harmonic generation.
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13
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14
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15
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16
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17
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18
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19
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20
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21
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22
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- Using f-to-2f, the CE phase of oscillator can be locked over 3 hours;
- Fast dynamics founded in the CE phase drift in amplified laser pulses;
- Low frequency quasi-periodic CE phase drift in amplified laser pulses.
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23
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24
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25
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26
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27
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28
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- Using f-to-2f interferometer, we stabilized the change of the
carrier-envelope phase of the KLS over 3 hours.
- The CE phase drift was measured using a second f-to-2f interferometer.
- Under the slow feedback control, the Ce phase drift was suppressed into
100 mrad range for several minutes.
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29
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- Dr. Zenghu Chang
- Al Rankin
- KLS Members: Mahendra Shakya, Shambhu Ghimire, Chris Nakamura, and Steve
Gilbertson
- Dr. Washburn and Dr. Corwin
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30
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