Abstract
We add non-linear and state-dependent terms to quantum field theory. We show that the resulting low-energy theory, non-linear quantum mechanics, is causal, preserves probability and permits a consistent description of the process of measurement. We explore the consequences of such terms and show that non-linear quantum effects can be observed in macroscopic systems even in the presence of de-coherence. We find that current experimental bounds on these non-linearities are weak and propose several experimental methods to significantly probe these effects. The locally exploitable effects of these non-linearities have enormous technological implications. For example, they would allow large scale parallelization of computing (in fact, any other effort) and enable quantum sensing beyond the standard quantum limit. We also expose a fundamental vulnerability of any non-linear modification of quantum mechanics - these modifications are highly sensitive to cosmic history and their locally exploitable effects can dynamically disappear if the observed universe has a tiny overlap with the overall quantum state of the universe, as is predicted in conventional inflationary cosmology. We identify observables that persist in this case and discuss opportunities to detect them in cosmic ray experiments, tests of strong field general relativity and current probes of the equation of state of the universe. Non-linear quantum mechanics also enables novel gravitational phenomena and may open new directions to solve the black hole information problem and uncover the theory underlying quantum field theory and gravitation.
Highlights
Quantum mechanics is the bedrock of physics
III C 3). (4) In [5], the concept of measurement in nonlinear quantum mechanics was discussed but not fully developed. We have developed this framework and pointed out that there is a consistent interpretation of measurement phenomena in nonlinear quantum mechanics, albeit at the expense of accepting a fundamental source of error in all measurement processes
We have shown that field theory permits a natural way to introduce causal nonlinear time evolution into quantum mechanics
Summary
Quantum mechanics is the bedrock of physics. Its seemingly ad hoc and phenomenologically derived axioms have proven to be remarkably resistant to parametrized deviation. Probability allows quantum mechanics to retain a finite set of energy states with the existence of continuous symmetries and observables by sacrificing deterministic measurement. We will adopt the view that measurement arises as the result of an interaction between a measuring device and a quantum system, with the interaction being described by the timeevolution equations that govern any other interaction in the theory.1 Using this concept of measurement, while causally consistent, we will find it to be fundamentally in conflict with the notion of a measuring device whose measurements are accurate and repeatable. II, we develop a transparent framework to show that the modification can be implemented in a causal and gauge-invariant manner We show that this modification allows for the existence of stationary states (Sec. II B), an essential element of quantum systems and we develop a consistent notion of.
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