1996
DOI: 10.1142/s0217732396000072
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Valley Instanton in the Gauge-Higgs System

Abstract: The instanton configuration in the SU(2)-gauge system with a Higgs doublet is constructed by using the new valley method. This method defines the configuration by an extension of the field equation and allows the exact conversion of the quasi-zero eigen-mode to a collective coordinate. It does not require ad hoc constraints used in the current constrained instanton method and provides a better mathematical formalism than the constrained instanton method. The resulting instanton, which we call “valley instanton… Show more

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Cited by 16 publications
(48 citation statements)
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“…(2.15a)-(2.15c) ff.) However, as in the N = 2 models considered in [26,47,81], it turns out that the integrations can nevertheless be accomplished using Gauss's law, and that only the asymptotic expressions (2.31) are actually needed. Here are the details.…”
Section: Construction Of the Multi-instanton Actionmentioning
confidence: 99%
“…(2.15a)-(2.15c) ff.) However, as in the N = 2 models considered in [26,47,81], it turns out that the integrations can nevertheless be accomplished using Gauss's law, and that only the asymptotic expressions (2.31) are actually needed. Here are the details.…”
Section: Construction Of the Multi-instanton Actionmentioning
confidence: 99%
“…First instanton tests of pure N = 2 supersymmetric SU(2) theories were performed in [54] at a one-instanton level and in [25] at a two-instanton level. Two-instanton contributions to the prepotential in SU(2) theories with N F fundamental hypermultiplets were calculated in [48,61,78] and the general expression for the k-instanton contribution to the prepotential as an integral over the ADHM moduli space was derived in [48]. The relation of Matone [80] between the prepotential and the condensate u 2 in SU(2) was tested at a two-instanton level in [81] and derived to all orders in instantons in [82].…”
mentioning
confidence: 99%
“…For a recent careful treatment of these issues see [92]. In addition to these effects, explicit instanton calculations are also necessary in order to fix the dictionary between the quantum moduli used in constructing exact solutions and the gauge-invariant VEVs u n , see [20,58,61,84,[91][92][93][94] for more detail. A completely new technique for evaluating the instanton contributions to the prepotential has been pioneered in [95,96] leading to the first calculations of instanton effects for all instanton number (beyond the large-N calculations reported in Chapters VII and IX) and the first test of Seiberg-Witten theory to all orders in the instanton expansion.…”
mentioning
confidence: 99%
“…Note that there is an ambiguity in the relation between u and z due to the integration constant u 0 . It is constrained to zero, either by an explicit 2-instanton computation [9,10,11,12] or by imposing invariance under the discrete R-transformations φ → e 2πi/3 φ [2].…”
Section: Solution Of the Modelmentioning
confidence: 99%
“…Here we show that, in conjunction with the SL(2, Z)-structure, the superconformal anomaly determines the low-energy effective Lagrangian and completely parametrises the quantum moduli space. What distinguishes the 4-dimensional model is that the non-perturbative contributions are not computable by other means (except for 1 and 2 instantons contributions [8,9,10,11,12]). …”
Section: Introductionmentioning
confidence: 99%