In string theory, a worldsheet is a two-dimensional manifold which describes the embedding of a string in spacetime. The term was coined by Leonard Susskind as a direct generalization of the world line concept for a point particle in special and general relativity. The type of string, the geometry of the spacetime in which it propagates, and the presence of long-range background fields (such as gauge fields) are encoded in a two-dimensional conformal field theory defined on the worldsheet. For example, the bosonic string in 26 dimensions has a worldsheet conformal field theory consisting of 26 free scalar bosons. Meanwhile, a superstring worldsheet theory in 10 dimensions consists of 10 free scalar fields and their fermionic superpartners.
Mathematical formulation
Bosonic string We begin with the classical formulation of the bosonic string. First fix a d {\displaystyle d} -dimensional flat spacetime ( d {\displaystyle d} -dimensional Minkowski space), M {\displaystyle M} , which serves as the ambient space for the string. A world-sheet Σ {\displaystyle \Sigma } is then an embedded surface, that is, an embedded 2-manifold Σ ↪ M {\displaystyle \Sigma \hookrightarrow M} , such that the induced metric has signature ( − , + ) {\displaystyle (-,+)} everywhere. Consequently it is possible to locally define coordinates ( τ , σ ) {\displaystyle (\tau ,\sigma )} where τ {\displaystyle \tau } is time-like while σ {\displaystyle \sigma } is space-like. Strings are further classified into open and closed. The topology of the worldsheet of an open string is R × I {\displaystyle \mathbb {R} \times I} , where I := [ 0 , 1 ] {\displaystyle I:=[0,1]} , a closed interval, and admits a global coordinate chart ( τ , σ ) {\displaystyle (\tau ,\sigma )} with − ∞ < τ < ∞ {\displaystyle -\infty <\tau <\infty } and 0 ≤ σ ≤ 1 {\displaystyle 0\leq \sigma \leq 1} . Meanwhile the topology of the worldsheet of a closed string is R × S 1 {\displaystyle \mathbb {R} \times S^{1}} , and admits 'coordinates' ( τ , σ ) {\displaystyle (\tau ,\sigma )} with − ∞ < τ < ∞ {\displaystyle -\infty <\tau <\infty } and σ ∈ R / 2 π Z {\displaystyle \sigma \in \mathbb {R} /2\pi \mathbb {Z} } . That is, σ {\displaystyle \sigma } is a periodic coordinate with the identification σ ∼ σ + 2 π {\displaystyle \sigma \sim \sigma +2\pi } . The redundant description (using quotients) can be removed by choosing a representative 0 ≤ σ < 2 π {\displaystyle 0\leq \sigma <2\pi } .
World-sheet metric In order to define the Polyakov action, the world-sheet is equipped with a world-sheet metric g {\displaystyle \mathbf {g} } , which also has signature ( − , + ) {\displaystyle (-,+)} but is independent of the induced metric. Since Weyl transformations are considered a redundancy of the metric structure, the world-sheet is instead considered to be equipped with a conformal class of metrics [ g ] {\displaystyle [\mathbf {g} ]} . Then ( Σ , [ g ] ) {\displaystyle (\Sigma ,[\mathbf {g} ])} defines the data of a conformal manifold with signature ( − , + ) {\displaystyle (-,+)} .
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