RF Leakage Investigations & Atomic Clock Signal Phase Drift Analysis

RF Leakage Investigations &
Atomic Clock Signal Phase Drift
Analysis
John Schaefer
Mentor: Dick Gustafson
RF Signals and the IFO
LIGO Radio Frequency (RF) roughly ranges from 100 kHz to 150 MHz
RF signals used to derive control signals for achieving resonance in
our optical cavities
Tells cavities whether they’re too short or too long and steers changes in
cavity length accordingly
RF leakages can contaminate signals in other electronics
Suspected to be a reason behind some losses of lock and source of
noise
DC Ground Isolation Units (“Baluns”)
Decouples DC grounds using a
transformer and shields leakage with
enclosure
RF leakages observed when
measuring ground to ground across
the balun
Largest leakage seen on balun
mounted on PSL electronics rack with
-22 dBV (~79 mV
rms
) at 80 MHz
Typical Spectrum Analysis using RF Analyser
Measured from cabling
ground to cabling ground
across balun
This balun transmits a
35.5 MHz current
-29 dBV is about 35 mV
rms
Other peaks are
suspected to be due to
leakages from
neighboring baluns
Circuit Diagram & Solutions
DCC: LIGO-D1101077-v1
Future Plans
Improve and test further modifications to the baluns (i.e. add more
capacitors?)
Identify other baluns that are candidates for replacement
Investigate “big picture” impact on IFO
Atomic Clock Phase Drift
We use an atomic clock as well as GPS for timing on the IFO
When triggering a signal from a rubidium clock on a 1 PPS GPS signal,
the signal seems to wander in phase
Small phase shifts may not matter in small timescale measurements,
but algorithms that use long integration times would see the effect
i.e. Algorithms that perform continuous wave searches
Phase Drift Sped Up
Long Term Measurement of Horizontal Shift
Mean drift of
213.55 ps per
second
We can likely
tune the clock to
get rid of linear
drift
But Not Perfectly Linear…
Observed Periodicity in Residuals
Test for Periodicity
Creating periodogram we find the two most interesting peaks are
5.02 mHz (~200 s period)
1.205 mHz (~14 min period)
Future Plans
Tune atomic clock to get rid of linear phase drift
Investigate the sources of these periodicities
Perform same analysis on an atomic clock more identical to the one
use on H1
Take two identical RF Oscillator Sources and have one disciplined by
GPS and the other by an atomic clock and analyze the difference
Questions?
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RF signals ranging from 100 kHz to 150 MHz are utilized for achieving resonance in optical cavities. DC Ground Isolation Units help decouple DC grounds and shield leakage. Spectrum analysis using RF analyzers reveals peaks possibly from neighboring balun leakages. Solutions involve increasing capacitance to reduce RF leakage. Future plans include testing modifications to baluns and assessing their impact on the IFO's performance. Atomic clock phase drift affects long integration time measurements, highlighting the importance of signal stability.

  • RF Signals
  • Atomic Clock
  • Phase Drift
  • Spectrum Analysis
  • Capacitance

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  1. RF Leakage Investigations & Atomic Clock Signal Phase Drift Analysis John Schaefer Mentor: Dick Gustafson

  2. RF Signals and the IFO LIGO Radio Frequency (RF) roughly ranges from 100 kHz to 150 MHz RF signals used to derive control signals for achieving resonance in our optical cavities Tells cavities whether they re too short or too long and steers changes in cavity length accordingly RF leakages can contaminate signals in other electronics Suspected to be a reason behind some losses of lock and source of noise

  3. DC Ground Isolation Units (Baluns) Decouples DC grounds using a transformer and shields leakage with enclosure RF leakages observed when measuring ground to ground across the balun Largest leakage seen on balun mounted on PSL electronics rack with -22 dBV (~79 mVrms) at 80 MHz

  4. Typical Spectrum Analysis using RF Analyser Measured from cabling ground to cabling ground across balun This balun transmits a 35.5 MHz current -29 dBV is about 35 mVrms Other peaks are suspected to be due to leakages from neighboring baluns

  5. Circuit Diagram & Solutions Solution: Increase capacitance! Recall that ? = Modifications: Replace cap with conductor (copper) Add more capacitors in parallel on the other cap Results: Peak goes from -22 dBV (~79 mVrms) to -50 dBV (~3.2 mVrms) at 80 MHz 1 ??? DCC: LIGO-D1101077-v1

  6. Future Plans Improve and test further modifications to the baluns (i.e. add more capacitors?) Identify other baluns that are candidates for replacement Investigate big picture impact on IFO

  7. Atomic Clock Phase Drift We use an atomic clock as well as GPS for timing on the IFO When triggering a signal from a rubidium clock on a 1 PPS GPS signal, the signal seems to wander in phase Small phase shifts may not matter in small timescale measurements, but algorithms that use long integration times would see the effect i.e. Algorithms that perform continuous wave searches

  8. Phase Drift Sped Up

  9. Long Term Measurement of Horizontal Shift Mean drift of 213.55 ps per second We can likely tune the clock to get rid of linear drift

  10. But Not Perfectly Linear

  11. Observed Periodicity in Residuals

  12. Test for Periodicity Creating periodogram we find the two most interesting peaks are 5.02 mHz (~200 s period) 1.205 mHz (~14 min period)

  13. Future Plans Tune atomic clock to get rid of linear phase drift Investigate the sources of these periodicities Perform same analysis on an atomic clock more identical to the one use on H1 Take two identical RF Oscillator Sources and have one disciplined by GPS and the other by an atomic clock and analyze the difference

  14. Questions?

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