ANATAC Meeting - PowerPoint PPT Presentation

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ANATAC Meeting

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The fiber stretcher voltage has a scale of 165 microns per volt. ... be due to the polarization or birefringent effect of the coarse fiber stretcher. ... – PowerPoint PPT presentation

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Title: ANATAC Meeting


1
ANATAC Meeting
  • Line Length Correction Status
  • 2004-Apr-23

2
  • In November,
  • Tests and theory indicated that phase change
    occured when the two lightwave polarizations were
    not fully aligned when the fiber (antenna) moves
  • Further tests indicated that
  • Misalignment of the polarizations can be added
    by either fiber or other components
  • Effect of fiber optic circulators on
    polarization alignment is large
  • Effect of 25km of fiber is fairly small

3
  • Optical Circulator - Polarization Independent
    Input Type
  • From US Patent 4,650,289 Mar 17, 1987
  • A ? B ? C ? D
  • Any path length difference on the split-path
    causes a wavelength dependent polarization change

4
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5
  • Polarization Requirement
  • Depends on relative polarization alignment
  • Misalignment must be minimized
  • Alignment must be done at the central building,
    before the two lightwaves are combined
  • Fiber introduces a misalignment that is
    unavoidable in the present baseline
  • Maximum angular misalignment introduced was
    measured for 25 km benchtop spool, about
    equivalent to 15 deg of arc on the Poincare
    sphere, or 97 alignment.
  • This is enough to cause a 3 amplitude reduction
    (compared to perfect alignment)
  • The phase change induced (with no circulators)
    was below 0.5 deg at 20 GHz, the limit of the
    measurement (about 100 fsec)
  • Since the spec is 12.2 fsec, we have not retired
    the risk, we need to measure to better precision
  • A reason to be optimistic the phase change was
    unmeasurable for a 300 degree rotation of a
    fairly crude azimuth mock wrap. This is a much
    worse case than for ALMA, which will have a
    carefully engineered wrap and will in general
    make much smaller angular moves.

6
New Block Diagram with Optical Circulators
Removed
Line Length Corrector (64 ea.)
At Each Antenna
50 MHz
Master laser stability 1e-11 short term (gt30km
coherence) 1e-10 long term
?
Separate photodetector for each band, output in
waveguide.
PD
Laser Synthesizer (4 ea.)
Loop Filter
Master (stabilized) Laser
1556.21 nm
Reference out 27 to 142 GHz
PD
Fiber Stretcher
up to 14 km of fiber
PBS
Slave (tunable) laser
OFS
Faraday Mirror
PD
1556.41557.4 nm
Harmonic Mixer
Loop Filter
?
25 MHz
Not shown optical signal distribution and
switching.
9 to 11 GHz
50 MHz
PD photodetector PBS polarization beam
splitter OFS optical frequency shifter
optical signals electrical signals
7
References 1 L. Ma, P. Jungner, J. Ye, J.L.
Hall, , Delivering the same Optical Frequency at
two places accurate cancellation of phase noise
introduced by an optical fiber or other
time-varying path, Optics Letters, Vol. 19, No.
21, Nov. 1, 1994, pp. 1777-1779 2 M.
Martinelli, A Universal Compensator for
Polarization Changes Induced By Birefringence on
a Retracing Beam, Optics Communication, Vol. 72,
No. 6, 15 Aug 1989, pp. 341-344
8
  • Prototype Master laser was delivered and accepted
  • Coherence was adequate to close the loop on a 5
    km spool of fiber. Longer lengths of 10km and 15
    km have now also been successfully tested
  • Some initial tests were conducted on a 5km length
    of fiber, transmitting a 20 GHz beatnote

9
Test Setup for measurement of phase drift between
the near and far end of the fiber. The fiber
length is actively corrected by means of an
optical interferometer servoed off of the
round-trip phase of a highly stable and coherent
master laser.
10
Phase Drift of 18.6 GHz signal going through 5
km of fiber. The fiber length correction is "ON"
for 660 seconds and then is turned "OFF".
11
Same test as previous figure, showing a closeup
of the measured residual phase with the
correction "ON"
12
Phase Drift of 18.6 GHz signal going through 5
km of fiber. The fiber length correction is "ON"
for 400 seconds and then is turned "OFF". This
plot also shows the correction voltage to the
fiber stretcher, which has a scale of 165 microns
per volt. (Right vertical scale is volts)
Figure 5 - Zoom of corrected portion of Figure 4.
13
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14
10 km
15
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16
Plot of Phase Drift of 18.6 GHz signal going
through 0 km of fiber. The fiber length
correction is "ON" for 800 seconds and then is
turned "OFF". The fiber stretcher voltage has a
scale of 165 microns per volt.
17
  • The preliminary experiments have successfully
    demonstrated the transmission of a 18 GHz
    reference over 5 km with a residual phase
    fluctuation lower than 0.22 degrees RMS (33 fs
    RMS) over 10 sec. These short term fluctuations
    are at the limit of our measuring system.
  • Further measurements are planned at higher
    frequency in order to further reduce the measured
    RMS phase residual.
  • Over a longer period of time, 600 sec, the total
    peak-to-peak drift was less than 100 fsec.
    However, this was similar or only slightly larger
    than what was measured for a zero-length of
    fiber, so we conclude that part of the source of
    the drift is in the test setup.
  • Additional drift may be due to the polarization
    or birefringent effect of the coarse fiber
    stretcher.

18
  • This is the first demonstration of the ALMA line
    length correction technique to instrument-limited
    accuracy. The main remaining objectives are
  • To prove the technique to greater accuracy
  • To prove the technique with a moving fiber wrap
  • To prove the technique in a field-system, such
    as the prototype antennas, esp. with buried fiber
    rather than a spool
  • To improve the master laser coherence so that up
    to 18 km of fiber can be stabilized and better
    immunity to environmental perturbations results.
  • Other subsystem issues
  • Polarization maintaining components, or
    polarization alignment servo on the source end
  • Minimization of polarization dispersion of the
    other compoents and the fiber, esp. fiber
    isolators required at the antenna end
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