Ultra-low CEP noise
Integrated phase noise of the DFC CORE +
![](https://www.toptica-china.com/fileadmin/_processed_/4/5/csm_toptica_dfc-core-plus_1200x350_w_01_335037a592.jpg)
- 34 mrad [70 mHz – 2 MHz]
- 61 mrad [70 mHz – 20 MHz]
- 135 mrad [70 mHz – 40 MHz]
The carrier envelope offset frequency fCEO of the DFC CORE + is zero because of the DFG process implemented in the CERO-Technology . Since it is hard to measure a signal at the frequency origin (0 Hz) we use a method first described by Liehl at al. to characterize the carrier envelope phase (CEP) noise.
An fCEO-free output of the DFC CORE + is amplified and broadened to an octave spanning supercontinuum to implement a modified f-2f setup like shown in figure 1. The long-wave part of the spectrum is frequency doubled and overlapped with the short-wave part at 950 nm. The resulting interference fringes are then filtered with optical bandpass filters and detected with a balanced photo detector. The resulting sinusoidal signal can be sampled up to high frequencies .
![](https://www.toptica-china.com/fileadmin/_processed_/4/1/csm_toptica_f-2f_interferometer_TL21PL22_99dd5b6138.png)
Figure 2 shows the ultra-low phase noise of the DFC CORE + measured according to Liehl et al. The long-term CEP stability can be characterized if the bandpass filters and balanced detection from figure 1 is replaced by a spectrometer (spectral interferometry). The interference fringes do show a very high modulation contrast of 97 %.
![](https://www.toptica-china.com/fileadmin/_processed_/c/e/csm_toptica_CEP_Phase_noise_70mHz_20MHz_61mrad_5feef77bea.png)
Figure 3 shows a time trace of the fringes over 25 seconds and the CEP which has been extracted by Fourier transformation.
We deduce 12 mrad phase stability in 25 seconds.
![](https://www.toptica-china.com/fileadmin/Editors_English/05_technology/02_frequency_combs/toptica_traces_24s_RMS_12_mrad.png)
- high modulation contrast -> 97 %
- high degree of CEP short term stability
- Stability limited by slow drift of the interferometer
- 12 mrad (rms) phase stability in 20 s