Abstract:A method to construct noncommutative instantons as deformations from commutative instantons was provided in [1]. Using this noncommutative deformed instanton, we investigate the spinor zero modes of the Dirac operator in a noncommutative instanton background on noncommutative R 4 , and we modify the index of the Dirac operator on the noncommutative space slightly and show that the number of the zero mode of the Dirac operator is preserved under the noncommutative deformation. We prove the existence of the Gree… Show more
“…We further prove one-to-one correspondence between the moduli space of the U(N) k-instantons and the moduli space of the ADHM data labeled by (N, k) [25]. In the proof, we apply Furuuchi's observation and several properties on noncommutative field theory (especially NC-deformed index theorem by Maeda and Sako [34]) to all the other ingredients of the ADHM construction and prove the existence of them in the operator sense. As a result, we obtain the following formula (a noncommutative version of the This directly shows an origin of the instanton number from the language of the ADHM data.…”
Section: Conclusion and Discussionmentioning
confidence: 99%
“…(A beautiful treatment can be also found in [11].) Noncommutative version of the ADHM duality is discussed in [25,34,41]. We start this section by giving a brief review on the Nahm transformation and then argue the ADHM/Nahm duality by taking certain limits.…”
Section: Nahm Transformation and Origin Of The Adhm Dualitymentioning
We discuss the Atiyah-Drinfeld-Hitchin-Manin (ADHM) construction of U(N) instantons in noncommutative (NC) space and prove the one-to-one correspondence between moduli spaces of the noncommutative instantons and the ADHM data, together with an origin of the instanton number for U(1). We also give a derivation of the ADHM construction from the viewpoint of the Nahm transformation of instantons on four-tori. This article is a composite version of [23] and [24].
“…We further prove one-to-one correspondence between the moduli space of the U(N) k-instantons and the moduli space of the ADHM data labeled by (N, k) [25]. In the proof, we apply Furuuchi's observation and several properties on noncommutative field theory (especially NC-deformed index theorem by Maeda and Sako [34]) to all the other ingredients of the ADHM construction and prove the existence of them in the operator sense. As a result, we obtain the following formula (a noncommutative version of the This directly shows an origin of the instanton number from the language of the ADHM data.…”
Section: Conclusion and Discussionmentioning
confidence: 99%
“…(A beautiful treatment can be also found in [11].) Noncommutative version of the ADHM duality is discussed in [25,34,41]. We start this section by giving a brief review on the Nahm transformation and then argue the ADHM/Nahm duality by taking certain limits.…”
Section: Nahm Transformation and Origin Of The Adhm Dualitymentioning
We discuss the Atiyah-Drinfeld-Hitchin-Manin (ADHM) construction of U(N) instantons in noncommutative (NC) space and prove the one-to-one correspondence between moduli spaces of the noncommutative instantons and the ADHM data, together with an origin of the instanton number for U(1). We also give a derivation of the ADHM construction from the viewpoint of the Nahm transformation of instantons on four-tori. This article is a composite version of [23] and [24].
“…Another method to construct noncommutative instantons as smooth deformations of commutative instantons was provided in [48,49,50]. The correspondence between the smooth deformation and the ADHM construction are discussed in [51]. On the other hand, there exist instanton solutions which are not smoothly connected to commutative instantons.…”
Section: B Noncommutative U (1) Instanton In the Fock Spacementioning
We show that Hermitian-Einstein metrics can be locally constructed by a map from (anti-)self-dual two-forms on Euclidean R 4 to symmetric two-tensors introduced in [1]. This correspondence is valid not only for a commutative space but also for a noncommutative space. We choose U (1) instantons on a noncommutative C 2 as the self-dual two-form, from which we derive a family of Hermitian-Einstein metrics. We also discuss the condition when the metric becomes Kähler.
“…(A beautiful treatment can be also found in [9].) Noncommutative version of the ADHM duality is discussed in [17,27,32]. We start this section by giving a brief review on the Nahm transformation and then argue the ADHM/Nahm duality by taking certain limits.…”
Section: Nahm Transformation and Origin Of The Adhm Dualitymentioning
We discuss the Atiyah-Drinfeld-Hitchin-Manin (ADHM) construction of U (N) instantons in noncommutative (NC) space and prove the one-to-one correspondence between moduli spaces of the noncommutative instantons and the ADHM data, together with an origin of the instanton number for U (1). We also give a derivation of the ADHM construction from the viewpoint of the Nahm transformation of instantons on four-torus.
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