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About strings ?


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I don't think there is such a notion, or at least not one I have come across.

 

The states of an excited string correspond to particle and anti-particle states. So, the excitations describe particles and antiparticles. The string is still "just a string". You have "right and left movers" in string theory, these sectors do not talk to each other. They are not identified as particles and anti-particles.

 

A similar thing occurs in quantum field theory, you can decompose the excitations of the field into positive and negative frequencies, which you do identify with particles and anti-particles but one does not really talk of a field and and anti-field (in this context. There is a notion of an anti-field but this is a very different notion).

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Both.

 

The bosonic string is described classically in terms of commuting variables. Essentially one is thinking of embedding a 2-d world sheet in some higher dimensional bulk. You can think in terms of a 1+1 dimensional bosonic field theory. (Or bosonic sigma models) Such a string cannot describe the fermionic degrees of freedom as required for any reasonable phenomenologically useful model.

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Understood via perturbation theory 1 bosonic and 5 supersymmetric.

 

M-theory understands the supersymmetric string theories as expansions about different limits. Non-perturbatively there are (or should be?) string theories "in between" these limits.

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i new for this forum but i understand ur question but i really not know whats meaning for this

 

Welcome to the forum.

 

I don't think there is any notion of an anti-string. I have not come across anyone talking about anti-strings for sure.

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