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Neutron Halo Isomers in Stable Nuclei and their Possible Application for the Production of Low Energy, Pulsed, Polarized Neutron Beams of High Intensity and High Brilliance

机译:稳定核中的中子卤素异构体及其可能的应用   低能量,脉冲,偏振中子束的生产   强度和高度

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摘要

We propose to search for neutron halo isomers populated via $\gamma$-capturein stable nuclei with mass numbers of about A=140-180 or A=40-60, where the$4s_{1/2}$ or $3s_{1/2}$ neutron shell model state reaches zero binding energy.These halo nuclei can be produced for the first time with new $\gamma$-beams ofhigh intensity and small band width ($\le$ 0.1%) achievable via Comptonback-scattering off brilliant electron beams thus offering a promisingperspective to selectively populate these isomers with small separationenergies of 1 eV to a few keV. Similar to single-neutron halo states for verylight, extremely neutron-rich, radioactive nuclei\cite{hansen95,tanihata96,aumann00}, the low neutron separation energy andshort-range nuclear force allows the neutron to tunnel far out into free spacemuch beyond the nuclear core radius. This results in prolonged half lives ofthe isomers for the $\gamma$-decay back to the ground state in the 100ps-$\mu$s range. Similar to the treatment of photodisintegration of thedeuteron, the neutron release from the neutron halo isomer via a second,low-energy, intense photon beam has a known much larger cross section with atypical energy threshold behavior. In the second step, the neutrons can bereleased as a low-energy, pulsed, polarized neutron beam of high intensity andhigh brilliance, possibly being much superior to presently existing beams fromreactors or spallation neutron sources.
机译:我们建议搜索质量为大约A = 140-180或A = 40-60,其中$ 4s_ {1/2} $或$ 3s_ {1的质量稳定的核中填充的中子卤素异构体。 / 2} $中子壳模型状态达到零束缚能。这些晕环原子可通过Comptonback散射首次获得高强度,小带宽($ \ le $ 0.1%)的新$ \γ$光束来生产。因此,它们可以从明亮的电子束中分离出来,从而为以1 eV至几keV的小的分离能选择性地填充这些异构体提供了一个有希望的前景。类似于单中子的晕圈状态,它具有非常轻,极富中子的放射性核素核素{hansen95,tanihata96,aumann00},低中子分离能和短程核力使中子能够隧穿很远的自由空间进入核以外的自由空间核心半径。这导致异构体的半衰期延长,因为在100ps-us的范围内,γ衰变回到基态。与氘核的光崩解处理相似,中子通过第二个低能强光子束从中子晕轮异构体释放的中子的横截面也大得多,具有非典型的能量阈值行为。在第二步骤中,中子可以作为高强度和高亮度的低能量,脉冲,极化中子束释放,可能比目前存在的来自反应堆或散裂中子源的束要优越得多。

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