Description
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Description
Switching times are a critical component of scheduling a
phase-referencing observation with the VLBA. Beasley and Conway
(1995) give two equations for the longest allowable switching
time
, depending on whether
the time scale is less than or greater than that for fluctuations
to cross a distance equal to the scale height of the
troposphere:
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Here,
is in minutes,
is the wavelength in
centimeters, z is the zenith angle,
is the strength of the tropospheric turbulence
(
is the amplitude of the
structure function), and is in units of
m
, v is the
velocity of the turbulence in meters per second, and L is
the scale height of the troposphere. See Beasley and Conway
(1995) for more detailed discussion.
Below, we provide tables and plots that can be used to
estimate the phase-referencing switching time (or ``cycle time'')
as a function of observing wavelength, elevation, and
tropospheric conditions. Here, the switching time is defined as
the time between the midpoints of the two calibrator observations
before and after the target observation. A ``typical'' value of
m
is assumed, while a ``good'' troposphere (similar to
some winter nights) is assumed to have
m
, and a ``bad''
troposphere (similar to some summer days) has
m
. For all cases, the
maximum switching time is assumed to saturate at a value of 10
minutes. At the longest wavelengths, ionospheric effects will
become dominant, while at intermediate wavelengths, model errors
(e.g., source position errors) may limit the integrations to
about this value. Note that (1) the difference between 10-minute
and 20-minute cycle times is only about 6% in total on-source
integration time, or 3% in signal-to-noise; and (2) elevation
angles greater than
will be uncommon
except for the shortest baselines.

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