The stability and instability of relativistic matter

The stability and instability of relativistic matter
复制标题

相对论物质的稳定性和不稳定性

DOI:
10.1007/3-540-27056-6_34
复制
发表时间:
1988
影响因子:
2.4
通讯作者:
H. Yau
H. Yau
中科院分区:
物理与天体物理2区
文献类型:
--
作者:
E. Lieb;H. Yau

文献摘要

被引文献

相似文献

我们考虑了电子和固定核通过库仑力相互作用的量子力学多体问题,但在动能的相对论形式下,(P_2C_2+M_2C_4)1/2−_mC_2代替了2/2M。电子被允许有q个自旋态(q=2)。对于一个电子和一个核,如果z为α>2/π,则发生不稳定性,其中z为核电荷,α为精细结构常数。我们证明了在多体情况下,如果α≦2/π和α<1/(47q)是稳定的。对于Smallza,也给出了在α上更好的界。在另一个方向,我们证明了存在一个临界αc(不大于12 8/15π),使得如果α>α,当原子核数目足够大时,对于所有正的z(不一定是积分的),总是发生不稳定性。文中还给出了其他几个技术性质的结果,如相对论动能的局域化估计和界限。
We consider the quantum mechanical many-body problem of electrons and fixed nuclei interacting via Coulomb forces, but with a relativistic form for the kinetic energy, namelyp2/2mis replaced by (p2c2+m2c4)1/2−mc2. The electrons are allowed to haveqspin states (q= 2 in nature). For one electron and one nucleus instability occurs ifzα > 2/πwherezis the nuclear charge and α is the fine structure constant. We prove that stability occurs in the many-body case ifzα≦ 2/π and α < 1/(47q). For smallza better bound onαis also given. In the other direction we show that there is a critical αc(no greater than 128/15π) such that if α > αcthen instability always occurs forallpositivez(not necessarily integral) when the number of nuclei is large enough. Several other results of a technical nature are also given such as localization estimates and bounds for the relativistic kinetic energy.