Absolute scaling exponents | ![]() |
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CVI SFs (10243 sol) | 0.62 | 1.20 | 1.73 | 2.21 | 2.65 | 3.05 |
CVI SFs (10243 comp) | 0.62 | 1.13 | 1.52 | 1.82 | 2.05 | 2.22 |
Relative Scaling Exponents |
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CVI SFs using ESSa (10243 sol) | 0.36 | 0.70 | 1.00 | 1.27 | 1.51 | 1.72 |
CVI SFs using ESSa (10243 comp) | 0.38 | 0.72 | 1.00 | 1.23 | 1.41 | 1.56 |
Polaris Flareb | 0.37 | 0.70 | 1.00 | 1.27 | 1.53 | 1.77 |
Polaris Flarec | 0.38 | 0.71 | 1.00 | 1.28 | 1.54 | 1.80 |
Intermittency Model SL94d | 0.36 | 0.70 | 1.00 | 1.28 | 1.54 | 1.78 |
Intermittency Model B02e | 0.42 | 0.74 | 1.00 | 1.21 | 1.40 | 1.56 |
Notes. (a) Using
extended self-similarity (ESS) (Benzi
et al. 1993).
(b) Measurement of
CVI structure functions by Hily-Blant
et al. (2008).
(c) Measurement of
CVI structure functions by Hily-Blant
et al. (2008) using 12CO(2-1) data
by Bensch
et al. (2001).
(d) Intermittency
model
defined in Eq. (28)
using a fractal co-dimension
(She & Leveque 1994),
which corresponds to filamentary structures (
).
(e) Same as d,
but for co-dimension
(Boldyrev
2002; Boldyrev et al.
2002) corresponding to sheet-like structures (
).
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