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How to split string with itself in python?

I would like to split a string with itself. My string is like this:
some_text=”Join(‘;”How to be a better developer, Ruby on Rails tutorial (‘>Rails Tutorial)’),”Hello world! This is blog post!”)”>

from there, I want to split this string to only get :
[‘Join(‘;How to be a better developer, Ruby on Rails tutorial (‘>Rails Tutorial)’),’, ”Hello world! This is blog post!”]

I’ve tried it and it doesn’t work.

The following seems to work:
>>> s = ‘Join(“;How to be a better developer, Ruby on Rails tutorial (Rails Tutorial)”),”Hello world! This is blog post!”;’
>>> [i[:-1] for i in s.split(‘;’)]
[‘Join(“;How to be a better developer, Ruby on Rails tutorial (Rails Tutorial)”),’, ‘Hello world! This is blog post!’]

Whereas your attempt:
>>> s.split(“;”)
[‘Join(“;’, ‘

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You can download the trial version of EControl Syntax Editor for a 30 day free trial. cases, showing that the number of the observations on a unit length scale should be a complicated non-monotonic function of the average velocity $\langle V(r)\rangle$ for $r\lesssim L/2$, where $L$ is the size of the observation domain. In the bulk case, this implies that the medium may be neither incompressible nor infinitely compressible. We show that our experimental observation is consistent with such predictions.

The fact that the concentration variance $C(r)$ at a scale $r$ is proportional to the velocity field $\bm{V}(r)$ that is perpendicular to $\bm{r}$ is reminiscent of the statistical *local structure theorem* for velocity increments [@C; @KSS; @S] where the scale invariance of the structure functions for velocity increments holds true. The anisotropy of the flow structures for $\delta\bm{u}$ and $\bm{V}$ is observed directly in our observation of the concentration field. This implies that the spatial structure of the flow fields for $\delta\bm{u}$ and $\bm{V}$ are different. This is consistent with the existing theoretical results on the anisotropic structure functions for velocity increments [@S; @XS]. The scale invariance of the concentration variance at a scale $r$ shows that the concentration field is statistically isotropic at a scale $r$, which is expected from the locally isotropic pressure distribution shown in Fig. \[rho-u-pressure\].

The fact that the non-Gaussian features of the concentration distribution function, such as $\beta$ and $\alpha$, are mainly determined by the average velocity field at a scale $r$ also leads to a remarkable consequence: The non-Gaussian features of the distribution of concentration should be the most vivid in the interior of the anisotropic flow structures, where the velocity is largest. This is because the velocity gradient, on which the effect of non-Gaussianity in the velocity field is reflected through the concentration gradient, is larger in the interior of the vortices than the exterior of the vortices. Therefore, the non-

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