论文标题
中子返回时间线性电势
The neutron returning time in a linear potential
论文作者
论文摘要
在本文中,我们计算了中子散射地球线性重力电位的量子时间延迟。量子时间延迟是通过分别从Wigner时间,停留时间和重新定义Larmor时间从经典的返回时间(CRT)来获得的。与常规定义不同,我们的Larmor时间是通过沿中子传播方向对齐的磁场来定义的,并且该定义确实可以通过自由区域和方形屏障为运动提供合理的结果。值得注意的是,在零磁场限制中,Larmor时间与CRT良好相吻合,这是由于线性屏障的特殊形状,并且可能与弱等价原理有一定程度的相关性。还发现,经典的禁区对于与CRT相匹配的住宅时间$τ_ {_ \ Mathrm {dw}} $起着至关重要的作用。所有时间延迟都处于亚毫秒和表现出振荡行为的顺序,表达散射中子的自我干扰,并且只有当de broglie波长$λ_K=2π/k $与特征性的长度可比$ l_c = [2m^2g/\ hbar^1/3时,振荡才变得明显。如果时间延迟测量在实验上可以实现,则可以探测粒子在时间结构域中的重力电位散射的量子性质。
In this paper, we calculate the quantum time delays for neutron scattering off the Earth's linear gravitational potential. The quantum time delays are obtained by subtracting the classical returning time (CRT) from the Wigner time, the dwell time and the redefined Larmor time respectively. Different from the conventional definition, our Larmor time is defined by aligning the magnetic field along the neutron propagation direction, and this definition does give reasonable results for motions through a free region and a square barrier. It is worth noting that in the zero magnetic field limit, the Larmor time coincides well with the CRT, which is due to the special shape of linear barrier, and may have some relevance to the weak equivalence principle. It is also found that the classical forbidden region plays an essential role for the dwell time $τ_{_\mathrm{DW}}$ to match with the CRT, and the difference between the dwell and the phase times, \ie, the self-interference time delay, is barrier shape sensitive and clearly shows the peculiarity of the linear barrier. All the time delays are on the order of sub-millisecond and exhibit oscillating behaviors, signaling the self-interference of the scattering neutron, and the oscillations become evident only when the de Broglie wavelength $λ_k=2π/k$ is comparable to the characteristic length $L_c=[2m^2g/\hbar^2]^{-1/3}$. If the time delay measurement is experimentally realizable, it can probe the quantum nature for particle scattering off the gravitational potential in the temporal domain.