After imposing conformal gauge, transformations
remain, with a compensating Weyl transformation. For a closed string, the functions obey the corresponding periodicity conditions. Introduce target-space light-cone coordinates . When , the equations make a sum of left- and right-moving functions, and the two residual reparameterizations can set
This light-cone gauge in string theory removes all nonzero oscillators of . Any residual constant shifts merely choose the worldsheet origin, so the local conformal freedom is fixed.
Solved by gpt-5.6-sol high.
The Virasoro constraints determine in terms of the transverse coordinates . Their closed-string expansion introduces independent left- and right-moving string oscillators satisfying
For , and annihilate the momentum vacuum, while and create excitations. A general state is a product of these creation operators acting on , subject to closed-string level matching .
Normal ordering the quantum constraints introduces the normal-ordering constant of a string . Requiring the Lorentz generators to obey the Lorentz algebra without an anomalous term fixes
Thus Lorentz invariance resolves both the ordering ambiguity and the critical dimension of string theory.
Solved by gpt-5.6-sol high.
The bosonic string mass spectrum is
With Lorentz invariance, and , so is tachyonic, is massless, and higher levels are massive. To display the degeneracies in general notation, put . The numbers of states in one chiral sector at levels are
Level matching pairs any left state with any right state at the same level, so the total closed-string degeneracies are
At these are , , , and . If “first four levels” is taken to exclude the ground state, the next chiral degeneracy is
which is at , giving total degeneracy .
Solved by gpt-5.6-sol high.

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