Geodetic VLBI experiment BRD01. Schedule notes.
Introduction
A dedicated 4-stations 24 hours experiment is proposed. One of the stations:
MEDICINA will swap RCP<-->LCP many times during the experiment while two
other stations will observe RCP. A set of RR and RL scans will be produced.
Background
Polarization test conducted on 14-DEC-98 showed
that European geodetic VLBI stations have considerable polarization
impurity. It was found that
-
RL fringes were found at all baselines, and the fringe amplitude
for RL scans was at the level 0.08-0.20 of the fringe amplitude for
RR scans. It means that the effect of polarization impurity in
normal RR scans is at the level 0.01-0.04, roughly 10 times smaller
than in RL scans.
-
Individual fringe amplitudes vary up to 3 times within the band
of registration (360MHz at X-band and 80MHz at S-band)
-
Bandwidth synthesis for RL scans at X-band failed: residual phases
scattered up to 2 radians. Bandwidth synthesis for RL scans at S-band
was poor: residual phases scattered up to 0.5 radians. The ratio of
residual phase scattering at X-band and S-band is 4. This ratio is
about the ratio of frequencies - 8.2/2.2 . It is an indication that
the effect which caused phase scattering is a path-like but not
phase-like.
We expect that
- Almost all stations have instrumental polarization exceeding 1%
and some stations have instrumental polarization exceeding 10%.
- Instruments polarization is depends on time relatively weak,
but may change after any manipulation with appliances.
- Instrumental polarization shows strong frequency dependence at many
stations. Dependence of instrumental polarization on frequency has
quasi-sinusoidal modulation with periods about the physical scales of
the antenna: tens MHz.
Motivation
Residual phase scattering at X-band after wideband synthesis for RL scans
is about 1 radian. Why?
If the factor which caused this scattering is related to instrumental
polarization we can expect that it affects normal RR scans with
the magnitude 10 times less what correspond to 0.1 radian. It is a typical
residual phase scattering which we have but it is larger than it
should be based on SNR. Excessive residual phase scattering was noticed
in early 80-s, was picturesquely described by T. Herring in his Ph.D.
theses dated in 1983 but was not explained up to now. Can polarization
impurity be a reason?
Objectives
- To measure polarization impurity on stations participating in
the experiment.
- To investigate dependence of instrumental polarization on
- time
- frequency
- parallactic angle
- To investigate how residual phases depend on
- time
- frequency
- parallactic angle
- To determine relative jumps in group and phase delays for RR and
RL scans.
- To make phase connection of RR and RL scans.
- To investigate misclosure for RR and RL scans for
- group delays
- multiband fringe phases
- individual phases
Schedule
Stations
Station MEDICINA is able to
swap RCP and LCP automatically and therefore was chosen as a key station.
Two other stations are
MATERA and
WETTZELL. Triangle: MATERA
MEDICINA WETTZELL has baselines 522, 597 and 990 kilometers.
Station TIGOWTZL is added to all
scans. SNR for cross-polarized RL scans at the baseline TIGOWTZL/MEDICINA is
allowed to be below a detection limit and fringes for 75% of such scans will
not be detected. Purpose of station TIGOWTZL participation is to investigate
the differences group delay minus phase delay at the 59 meter long baseline
WETTZELL/TIGOWTZL.
Sources
Expected fringe amplitudes in RL scans are only 10% of the amplitudes
in RR scans. Therefore only the strongest sources can be scheduled. The
information about fluxes of the strongest sources is taken from the file
Physical
characteristics ICRF and from the
UMRAO database.
|--------------------|----------------|--------------|--------------|
| IAU name name | 8.0GHz 4.8GHz | 6cm 15cm | P-8.0 P-4.8 |
| (1) (2) | (3) (4) | (5) (6) | (7) (8) |
|--------------------|----------------|--------------|--------------|
| 0316+413 3C84 | 21.15 21.35 | 18.72 24.80 | 0.14 0.25 |
| 0538+498 3C147 | 4.64 7.92 | 8.18 12.98 | 0.10 0.21 |
| 0552+398 DA193 | 5.77 5.74 | 5.43 3.40 | 2.22 0.87 |
| 0923+392 4C39.25 | 10.64 12.53 | 7.57 4.20 | 1.09 1.08 |
| 1226+023 3C273B | 38.84 43.27 | 43.41 41.44 | 3.59 3.67 |
| 1253-055 3C279 | 24.83 17.82 | 15.34 11.80 | 2.23 3.93 |
| 1641+399 3C345 | 8.53 8.37 | 5.65 7.60 | 3.51 3.01 |
| 1921-293 OV-236 | 11.67 14.43 | 10.00 4.60 | 3.00 1.04 |
| 2134+004 2134+00 | 8.80 8.52 | 11.49 6.50 | 1.92 0.30 |
| 2251+158 3C454.3 | 11.78 12.92 | 10.03 10.50 | 1.37 2.57 |
|--------------------|----------------|--------------|--------------|
where
| (1) |
IAU source name;
|
| (2) |
alias source name;
|
| (3) |
Flux in Jy at 8.0 GHz from UMRAO at the nearest date to 01-JUL-99;
|
| (4) |
Flux in Jy at 4.8 GHz from UMRAO at the nearest date to 01-JUL-99;
|
| (5) |
Flux in Jy at 6 cm from ICRF physical characteristics;
|
| (6) |
Flux in Jy at 15 cm from ICRF physical characteristics;
|
| (7) |
SPX: degree of polarization at 8.0GHz in percents taken from UMRAO
at the nearest date to 01-JUL-99;
|
| (8) |
SPX: degree of polarization at 4.8GHz in percents taken from UMRAO
at the nearest date to 01-JUL-99;
|
These 10 sources are taken for BRD01 experiment. "Fluxes" for RL scans are
taken 10-times less than fluxes for RR scans.
Frequencies
Frequency setups
| SX | B1 | B2 | B3 |
B4 | B5 | B6 |
| 8210.99 | 8208.99 | 8207.99 | 8205.99 |
8213.99 | 8216.99 | 8218.99 |
| 8220.99 | 8218.99 | 8217.99 | 8215.99 |
8223.99 | 8226.99 | 8228.99 |
| 8250.99 | 8248.99 | 8247.99 | 8245.99 |
8253.99 | 8256.99 | 8258.99 |
| 8310.99 | 8308.99 | 8307.99 | 8305.99 |
8313.99 | 8316.99 | 8318.99 |
| 8420.99 | 8418.99 | 8417.99 | 8415.99 |
8423.99 | 8426.99 | 8428.99 |
| 8500.99 | 8498.99 | 8497.99 | 8495.99 |
8503.99 | 8506.99 | 8508.99 |
| 8550.99 | 8548.99 | 8547.99 | 8545.99 |
8553.99 | 8556.99 | 8558.99 |
| 8570.99 | 8568.99 | 8567.99 | 8565.99 |
8573.99 | 8576.99 | 8578.99 |
| 2212.99 | 2211.99 | 2209.99 | 2206.99 |
2200.99 | 2198.99 | 2191.99 |
| 2222.99 | 2221.99 | 2219.99 | 2216.99 |
2210.99 | 2208.99 | 2201.99 |
| 2237.99 | 2236.99 | 2234.99 | 2231.99 |
2225.99 | 2223.99 | 2216.99 |
| 2267.99 | 2266.99 | 2264.99 | 2261.99 |
2255.99 | 2253.99 | 2246.99 |
| 2292.99 | 2291.99 | 2289.99 | 2286.99 |
2280.99 | 2278.99 | 2271.99 |
| 2297.99 | 2296.99 | 2294.99 | 2291.99 |
2285.99 | 2283.99 | 2276.99 |
Observing scenarios
- Scenario a ("band scan")
A pair of sources: 0316+413, 0923+392 is observed from
182.10:00 till 182.12:15 and a pair of sources: 0923+392, 2251+158
is observed from 183.07:20 183.09:43.
First two scans are made in RR then two scans in RL, then
frequencies of individual videoconverters are changed. Frequencies
are changed 6 times by adding an offset to all frequencies of
videoconverters with respect to initial (default) setup each time.
Sequence of offsets at X-band is
-2, -3, -5, +3, +6, +8 MHz and -1, -4, -6, -10, -15, -21 MHz
at S-band. Restriction: a) the frequencies of the individual vcs
should not cross the boundary 224MHz of local oscillator:
8304 = 8080 + 224MHz and 2244 = 2020 + 224MHz in order not to change
their setup: upper or lower was taken into account;
b) the frequencies of the individual vcs should not exceed 499 MHz.
- Scenario b ("pair connection")
A pair of sources is observed. Two observations in RR and two
observations in RL. Then the procedure is repeated. Pair 1226+023,
1253-055 is observed at 182.12:44 -- 182.14:00 and at
182.16:44 182.17:33. Pair 0538+508, 0552+398 is observed between
182.14:06 and 182.16:44
- Scenario c ("stay on source")
One source is observed, but polarization is swapped after each
scan. 1253-055 is observed at the baseline MEDICINA/MATERA from
182.17:33 till 182.20:00 while WETTZELL is engaged for NEOS
Intensive and temporarily does not observe BRD01.
- Scenario d ("full coverage")
All visible sources are observed during 2-3 hours, in normal
geodetic fashion to achieve full sky coverage, but polarization setup
is not changed during that period. Then polarization is swapped and
again 2-3 hours of observations.
RR: 182.20:04 182.23:11, RL: 182.23:11 183.02:04
RR: 183.02:04 183.04:05, RL: 183.04:05 183.07:17
Comments:
| 1. |
Additional 1-1.5 minutes is added to allow an operator in MEDICINA
to swap polarization.
|
| 2. |
10 additional "pseudosources" with L at the end of their name are added
to the schedule in order to distinguish RR and RL scans. Their fluxes are
set 10 times smaller than the fluxes of their RR counterparts.
|
| 3. |
SNR threshold 40 is used in order to get sure detection for all RL scans
and reliable estimates of group delays.
|
Predicted SNR
Average predicted SNR at the subnetwork MEDICINA/MATERA/WETTZELL:
| Source | Plrz | SNR(X) |
SNR(S) | Num |
| 0316+413 | RR | 662 |
418 | 57 |
| 0316+413 | RL | 62 |
41 | 63 |
| 0538+508 | RR | 184 |
87 | 30 |
| 0538+508 | RL | 24 |
13 | 15 |
| 0552+398 | RR | 131 |
152 | 24 |
| 0552+398 | RL | 19 |
25 | 13 |
| 0923+392 | RR | 301 |
239 | 70 |
| 0923+392 | RL | 36 |
27 | 60 |
| 1226+023 | RR | 1098 |
823 | 72 |
| 1226+023 | RL | 98 |
83 | 57 |
| 1253-055 | RR | 675 |
274 | 57 |
| 1253-055 | RL | 73 |
30 | 45 |
| 1641+399 | RR | 233 |
156 | 33 |
| 1641+399 | RL | 37 |
25 | 24 |
| 1921-293 | RR | 298 |
257 | 10 |
| 1921-293 | RL | 45 |
27 | 18 |
| 2134+004 | RR | 245 |
166 | 30 |
| 2134+004 | RL | 36 |
25 | 30 |
| 2251+158 | RR | 33 |
239 | 48 |
| 2251+158 | RL | 37 |
27 | 51 |
Average predicted SNR at the baseline TIGOWTZL/WETTZELL over all observations:
Back to Web page "Study of
systematic errors in VLBI caused by polarization impurity".
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This page was prepared by
Leonid Petrov.
Web-master:
petrov@kuestner.geod.uni-bonn.de
Last update: 22-JUN-99 14:13:12