弦の場の理論
出典: フリー百科事典『ウィキペディア（Wikipedia）』 (2024/05/11 16:32 UTC 版)
弦の場の理論（げんのばのりろん、英語: String Field Theory）とは、相対論的な弦の力学が場の量子論の言葉で再定式化されるような弦理論の定式化である。弦のプロパゲーター (propagator) のように、ファインマン・ダイアグラムを拡張することで、弦の散乱振幅を弦の結合と分岐の頂点の様子として見ることにより、この定式化は摂動論のレベルで完成している。大半の弦理論では、自由弦と加えられた相互作用項を第二量子化することにより得られる古典的作用に、この定式化がエンコードされている。普通の（場の理論の）第二量子化の場合と同様に、その定式化の古典場の構成は、元々の理論の波動函数により与えられる。このことは、弦の場の理論の場合も 弦の場 と呼ばれる古典的構成が、自由弦の作るフォック空間の元で与えられることを意味する。
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