玻色弦理論

玻色弦理論是最早的弦論版本，約在1960年代晚期發展。其名稱由來是因為粒子譜中僅含有玻色子。1980年代，在弦論的範疇下發現了超對稱；一個稱作超弦理論的新版本弦論成為了研究主題。儘管如此，玻色弦理論仍然是瞭解微擾弦理論的有用工具，並且超弦理論中的一些理論困難之處在玻色弦理論中已然現身。疑難.雖然玻色弦理論有許多吸引人的特質，其在成為物理模型理論有兩大缺陷：型別.有四種可能的玻色子弦理論，取決於是否允許開弦以及弦是否具有指定的可定向性。四種可能理論的光譜示意圖如下：請注意，所有四種理論都有一個負能量快子 (formula_1) 和一個無質量引力子。數學表示.路徑積分表述.玻色子弦理論可以由路徑積分定義：formula_2已隱藏部分未翻譯內容，歡迎參與[ 翻譯]。formula_3 is the field on the worldsheet describing the embedding of the string in 25+1 spacetime; in the Polyakov formulation, formula_4 is not to be understood as the induced metric from the embedding, but as an independent dynamical field. formula_5 is the metric on the target spacetime, which is usually taken to be the Minkowski metric in the perturbative theory. Under a Wick rotation, this is brought to a Euclidean metric formula_6. M is the worldsheet as a topological manifold parametrized by the formula_7 coordinates. formula_8 is the string tension and related to the Regge slope as formula_9.formula_10 has diffeomorphism and Weyl invariance. Weyl symmetry is broken upon quantization (Conformal anomaly) and therefore this action has to be supplemented with a counterterm, along with a hypothetical purely topological term, proportional to the Euler characteristic:formula_11The explicit breaking of Weyl invariance by the counterterm can be cancelled away in the critical dimension 26.Physical quantities are then constructed from the (Euclidean) partition function and N-point function:formula_12formula_13The discrete sum is a sum over possible topologies, which for euclidean bosonic orientable closed strings are compact orientable Riemannian surfaces and are thus identified by a genus formula_14. A normalization factor formula_15 is introduced to compensate overcounting from symmetries. While the computation of the partition function corresponds to the cosmological constant, the N-point function, including formula_16 vertex operators, describes the scattering amplitude of strings.The symmetry group of the action actually reduces drastically the integration space to a finite dimensional manifold. The formula_4 path-integral in the partition function is "a priori" a sum over possible Riemannian structures; however, quotienting with respect to Weyl transformations allows us to only consider conformal structures, that is, equivalence classes of metrics under the identifications of metrics related byformula_18Since the world-sheet is two dimensional, there is a 1-1 correspondence between conformal structures and complex structures. One still has to quotient away diffeomorphisms. This leaves us with an integration over the space of all possible complex structures modulo diffeomorphisms, which is simply the moduli space of the given topological surface, and is in fact a finite-dimensional complex manifold. The fundamental problem of perturbative bosonic strings therefore becomes the parametrization of Moduli space, which is non-trivial for genus formula_19.h = 0.At tree-level, corresponding to genus 0, the cosmological constant vanishes: formula_20.The four-point function for the scattering of four tachyons is the Shapiro-Virasoro amplitude:formula_21Where formula_22 is the total momentum and formula_23, formula_24, formula_25 are the Mandelstam variables.h = 1.Genus 1 is the torus, and corresponds to the one-loop level. The partition function amounts to:formula_26formula_27 is a complex number with positive imaginary part formula_28; formula_29, holomorphic to the moduli space of the torus, is any fundamental domain for the modular group formula_30 acting on the upper half-plane, for example formula_31. formula_32 is the Dedekind eta function. The integrand is of course invariant under the modular group: the measure formula_33 is simply the Poincaré metric which has PSL(2,R) as isometry group; the rest of the integrand is also invariant by virtue of formula_34 and the fact that formula_32 is a modular form of weight 1/2.This integral diverges. This is due to the presence of the tachyon and is related to the instability of the perturbative vacuum.