论文标题
客观崩溃方程保持保护法,没有新常数
Objective Collapse Equation Maintains Conservation Laws With No New Constants
论文作者
论文摘要
为了将测量过程的描述纳入量子理论的数学结构,已提出了Schrödinger方程的修改版本。通常,这些建议会引入新的物理常数,并暗示对动量和节能的侵犯很小。 可以通过假设波函数崩溃是由建立系统之间相关性的个体相互作用引起的,可以消除这些有问题的特征。波动函数的相互作用和非相互作用分支之间的足够数量的小型,随机的幅度随机移动会导致与我们的宏观体验一致的规模崩溃。两粒子相互作用的势能可以用作添加到schrödinger方程中的崩溃期限的基础。相互作用的范围设置了塌陷效应的距离尺度;势能与粒子的总相对论能量的比率决定了振幅变化的幅度,并且相互作用进行的速率固定了时序参数。 由于崩溃操作员会自动考虑到测量的系统与以前在交互过程中与之交换保守数量的系统之间的小而残余的纠缠,因此保持了与各个实验中的保护定律的一致性。保护对于动量和轨道角动量是精确的,并且在非依赖主义理论中可描述的有限的能量形式所允许的精度内,它具有能量。
Modified versions of the Schrödinger equation have been proposed in order to incorporate the description of measurement processes into the mathematical structure of quantum theory. Typically, these proposals introduce new physical constants, and imply small violations of momentum and energy conservation. These problematic features can be eliminated by assuming that wave function collapse is induced by the individual interactions that establish correlations between systems. The generation of a sufficient number of small, random shifts of amplitude between interacting and noninteracting branches of the wave function can bring about collapse on a scale consistent with our macroscopic experience. Two-particle interaction potential energies can be used as the basis for a collapse term added to the Schrödinger equation. The range of the interactions sets the distance scale of the collapse effects; the ratio of potential energies to the total relativistic energies of the particles determines the magnitude of the amplitude shifts, and the rate at which the interactions proceed fixes the timing parameters. Consistency with conservation laws in individual experiments is maintained because the collapse operator automatically takes into account the small, residual entanglement between the measured system and systems with which it has previously exchanged conserved quantities during interactions. Conservation is exact for momentum and orbital angular momentum, and it holds for energy within the accuracy allowed by the limited forms of energy describable in nonrelativistic theory.