1996
DOI: 10.1134/1.567138
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Erratum: Radiative corrections to the pion beta decay [JETP 59, No. 10, 671–676 (25 May 1994)]

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Cited by 4 publications
(5 citation statements)
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“…First, it was found during lower hybrid heating (LHH). An abrupt drop of H β radiation and MHD activity, an increase of the plasma density and stored energy as well as broadening of the ion temperature profile were observed after the RF pulse was switched on and after the post heating phase [2]. After an L-H transition the energy confinement time increased by a factor of two to three.…”
Section: Introductionmentioning
confidence: 98%
“…First, it was found during lower hybrid heating (LHH). An abrupt drop of H β radiation and MHD activity, an increase of the plasma density and stored energy as well as broadening of the ion temperature profile were observed after the RF pulse was switched on and after the post heating phase [2]. After an L-H transition the energy confinement time increased by a factor of two to three.…”
Section: Introductionmentioning
confidence: 98%
“…It is difficult to investigate the ECEC process because one only detects the low energy x-rays. It is interesting to search for transitions to the excited states of daughter nuclei, which are easier to detect given the cascade of higher energy gammas [7]. One can foresee that with improvement in the experimental techniques and increasing the mass of the detectors, the search for β + β + , β + EC and ECEC processes will be considerably extended.…”
Section: Introductionmentioning
confidence: 99%
“…Note, that this term is currently considered [5,6] among other ones in line of phenomenological analysis of possible gauge boson interactions. Interaction (1) defines a vertex in the momentum space, which according to the approach acts in the region p 2 i < Λ 2 , where p i are three momenta of the vertex legs and the effective cut-off Λ is of the order of magnitude of few T eV [7,8]. The vertex has the form Γ abc µνρ (p, q, k) = ǫ abc λg M 2 W Γ µνρ (p, q, k) ; Γ µνρ (p, q, k) = g µν (p ρ (qk) − q ρ (pk)) + g νρ (q µ (pk) − k µ (pq)) +…”
mentioning
confidence: 99%
“…However, we are to remember, that the basic vertex (2) has cut-off Λ. In previous calculations [3,7,8] we have used Pauli-Villars type of formfactor on each gauge boson leg. Following this line let us define the following integrals…”
mentioning
confidence: 99%
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