We have made dual-frequency (1.67 and 5.00 GHz) VLBI observations of five c
ompact, presumably extragalactic radio sources in the Galactic plane in the
constellation of Cygnus. The lines of sight to these sources pass through
a part of the interstellar medium that is modified by the Cygnus OB1 associ
ation. The VLBI observations were processed to yield measurements of the sc
attering measure due to interstellar plasma turbulence. The dual-frequency
VLBI observations allowed estimates of the possible intrinsic structure con
tamination of the scattering measurements. Such an error is estimated to be
less than 5% of the scattering measure for our two best-observed cases, an
d 15% to as high as 30% for a more weakly scattered source. Modeling the sp
atial power spectrum of the turbulence by P-delta n(q) = C(N)(2)q(-alpha),
where a is the spatial wavenumber of the turbulent fluctuations, our observ
ations provide a measurement of integral(o)(L)C(N)(2)dz, where L is the thi
ckness of the scattering medium and z is a coordinate along the line of sig
ht. When combined with our earlier observations of the radio source 2013+37
0, we have a total of six lines of sight through the Cygnus OB1 association
. Our observations show that the scattering through the Cygnus OB1 associat
ion is heavy and that the scattering measures vary from 0.14 to 2.21 m(-20/
3) kpc on Lines of sight separated by as little as 1 degrees-2 degrees. Whe
n combined with measurements of the emission measure in the same directions
, our scattering-measure results constrain properties of the turbulence in
the Cygnus OB1 association. Specifically, if epsilon is the normalized ampl
itude of the density fluctuations, and l(o) is the outer scale to the Kolmo
gorov spectrum, then our combined scattering measure emission measure data
set constrains the quantity epsilon(2)/(1+epsilon(2))l(o)(2/3). The mean Va
lue is similar to 4.3 x 10(-13) cm(-2/3), with a range of about 0.5 in the
logarithm. We do-not have sufficient information to determine epsilon and l
(o) separately, but plausible ranges are epsilon<1 and l(o)<3 pc. For the m
ost heavily scattered lines of sight, the outer scale must be considerably
less than a parsec. In the case of two of our sources, 2005+372 and 2020+35
1, the observations are of sufficient quality to determine the spectral ind
ex cc of the density spectrum. In both cases our measurements are consisten
t within the errors with the Kolmogorov value of 3.67. These new measuremen
ts are in accord with a previous, similar measurement for 2013+370 and thus
suggest that the mechanism responsible for generating turbulence in the vi
cinity of stellar OB associations is similar to that operative in the diffu
se ionized gas (DIG) of the interstellar medium. Our observations also show
anisotropy of the scattering for 2005+-372 and 2020+351, with axial ratios
of 1.83+/-0.10 and 1.05-1.50, respectively. These observations are quantit
atively consistent with a handful of other such observations, and suggest t
hat the irregularities responsible for interstellar scintillations are exte
nded along the interstellar magnetic held.
We briefly and qualitatively discuss mechanisms by which the plasma shell s
urrounding Cygnus OB1 has become turbulent.