The Euler-Lagrange equation of the gauge-fixed Polyakov action is the two-dimensional wave equation
Its general solution is a sum of left- and right-moving functions. Periodicity in and a Fourier expansion give the closed-string mode expansion
The zero modes satisfy . Here and are the center-of-mass position and momentum, while the nonzero string oscillators describe shape excitations.
A classical string must also satisfy the equations obtained by varying the worldsheet metric before imposing conformal gauge. Vanishing of the worldsheet stress-energy tensor gives
In modes these are the Virasoro constraints
for every integer . Reality of also requires
Together with periodicity and the wave equation, these conditions remove the unphysical longitudinal worldsheet excitations.
For a target circle of radius , maps may wind, so the boundary condition is
Single-valued target-space wavefunctions quantize the center-of-mass momentum as , with . The compact boson expansion becomes
Equivalently, its left- and right-moving zero-mode momenta are
The integers and are the momentum and winding modes.
Let be the mass measured in the uncompactified 25-dimensional spacetime. The quantum zero-mode constraints are
The string level operators
have nonnegative integer eigenvalues. Adding the constraints and using gives
Their difference gives closed-string level matching, with the present left-right convention. The normal-ordering constant of a string is the regularized zero-point energy generated when oscillator products are normal ordered.

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