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Nuclear physics without high-momentum potentials: Constructing the nuclear effective interaction directly from scattering observables

机译:没有高动量势的核物理:直接从散射可观察物构建核有效相互作用

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The traditional approach to nuclear physics encodes phase shift information in a nucleon-nucleon (NN) potential, producing a nucleon-level interaction that captures the sub-GeV consequences of QCD. A further reduction to the nuclear scale is needed to produce an effective interaction for soft Hilbert spaces, such as those employed in the shell model. Here we describe an alternative construction of the effective interaction that is simple and quite precise, proceeding from the QCD scale directly to the nuclear scale. This eliminates the need for constructing and renormalizing the high-momentum NN potential. Instead, continuum phase shifts and mixing angles are used directly at the nuclear scale. The method exploits the analytic continuity in energy of HOBET (Harmonic-Oscillator-Based Effective Theory) to connect bound states to continuum solutions at specific energies. The procedure is systematic, cutoff independent, and convergent, yielding keV accuracy at NNLO or N3LO, depending on the channel. Lepage plots are provided.
机译:传统的核物理方法将相移信息编码为核子-核子(NN)势,产生核子级相互作用,从而捕获QCD的次GeV后果。为了使软希尔伯特空间(例如在壳模型中使用的空间)产生有效的相互作用,还需要进一步减小核的规模。在这里,我们描述了一种简单有效的相互作用的替代构造,该构造简单且十分精确,从QCD规模直接发展到核规模。这消除了构造和重新规范高动量NN电位的需要。相反,连续相移和混合角直接在核尺度上使用。该方法利用了HOBET(基于谐波振荡器的有效理论)的能量分析连续性,将束缚态与特定能量下的连续体解联系起来。该过程是系统的,独立于截止且收敛的,根据通道的不同,在NNLO或N3LO处可获得keV精度。提供了渗漏图。

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