Solutions for Mixed States in Open Bosonic String Theory

We describe the family of normalizable solutions in linearized open string field theory, defined by $QΨ_0=0$ ($Q$ is BRST charge) understood in the sense $<<QΨ_0,Φ>>=0$ for an arbitrary string field $Φ$. The solutions depend on shifted partition numbers and are parametrized in terms of values of $ζ$-function at pairs of positive numbers greater than 2. We argue that the operators, defined by these solutions, create mixed quantum-mechanical states by acting on the vacuum (as opposed to standard vertex operators, creating the pure states with definite masses and spins).

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