Phenomenological phenomena and quantum phenomena belonging to different domains have rather similarities that the concept of phenomena include the activities of appearances,entities themselves and their evolutions.Methodologically,phenomenology and quantum mechanics describe phenomena using the similar concepts of possibility and probability,the similar principles of free variety and complementarity.
Phenomenological phenomena and quantum phenomena belonging to different domains have rather similarities that the concept of phenomena include the activities of appearances,entities themselves and their evolutions.Methodologically,phenomenology and quantum mechanics describe phenomena using the similar concepts of possibility and probability,the similar principles of free variety and complementarity.
While quantum mechanics has proven successful in its calculations and predictions, a debate persists regarding its understanding. This chapter considers the fundamental concepts of phenomenology and its connection to early quantum mechanics, including the exploration of quantum mechanics by F. London & E. Bauer using phenomenology. Phenomenological investigations of quantum mechanics in recent years have evolved. For instance, the informational interpretation of quantum mechanics, introduced by C. Rovelli in 1996 and advanced by Fuchs and C. M. Caves, offers a new perspective on quantum mechanics and possesses phenomenological tendencies which provide new insights into the problem of quantum measurement. Interestingly, phenomenology has its strong ties to hermeneutics. Therefore, this chapter sheds new light on quantum mechanics via hermeneutical analyses, and bridges the gap between the humanities and the natural sciences. In hermeneutics, interpretation encompasses two key aspects: Erklärung (Explanation) and Auslegung (Explication), where the former establishes clear and objective descriptions, similar to the “shuo ming” (说明) concept in Chinese, and the latter unveils deeper meanings and context, similar to the “chan shi” (阐释) concept in Chinese. The iterative process of explanation and explication plays a crucial role in the development of quantum mechanics. Hermeneutics allows us to view quantum matter with a new perspective, and new features are revealed such as “fusion of horizons” and “history of effects”, where the former is the merging of observer and observed realities in the context of quantum mechanics, while the latter means that the past, present, and future of a quantum system influence its overall reality. For this reason, the photon’s past, in the delayed-choice experiment, becomes an unfinished entity, a superposition waiting to be defined by measurement. This measurement collapses the possibilities and merges the photon’s past and present realities into a single, unified “whole”.
It is shown that quantum mechanics is, like thermodynamics, a phenomenological theory i.e., not a causal theory, ( not because it is a statistical theory - statistical theories with caused probability distributions can be regarded as causal) but because pure states, i.e., probability distributions of measurement values, cannot inhere in elementary particles and therefore cannot change when their world tubes intersect and hence they cannot be regarded as interacting causally. By a causal theory is meant a theory that specifies the changes in time of the states of causally interacting entities in its domain. The areas in quantum mechanics in which causal interactions are relevant include, though not explicitly, measurement and therefore the Born rule, and, explicitly, the unitary Schrodinger time development of states. The Born rule probabilities are shown to to refer not to conjoint superpositions of eigenstates but to classical mixtures of mutually exclusive eigenvalues and the Schrodinger time development of states is shown to refer to the time development of the states of non-causally interacting elementary particles and hence cannot be regarded as as a causal time development equation, appearances to the contrary notwithstanding. The recognition that quantum mechanics is not a causal theory but a phenomenological theory like thermodynamics does not affect the way it is employed to calculate an predict and hence preserves its empirical success but it does allow a typically simple phenomenological theory explanation of entanglement and other apparently non-local phenomena.
A short exposition is given of the foundation of the causal description in classical physics and the failure of the principle of causality in coping with atomic phenomena. It is emphasized that the individuality of the quantum processes excludes a separation between a behaviour of the atomic objects and their interaction with the measuring instruments denning the conditions under which the phenomena appear. This circumstance forces us to recognize a novel relationship, conveniently termed complementarity, between empirical evidence obtained under different experimental conditions. An appropriate tool for a complementary mode of description is provided by the quantum-mechanical formalism which allows us to account for regularities of definite or statistical character beyond the grasp of classical physical explanation. – N. B.
This article explores Bohr's argument, advanced under the heading of 'complementarity,' concerning quantum phenomena and quantum mechanics, and its physical and philosophical implications.In Bohr, the term complementarity designates both a particular concept and an overall interpretation of quantum phenomena and quantum mechanics, in part grounded in this concept.While the argument of this article is primarily philosophical, it will also address, historically, the development and transformations of Bohr's thinking, under the impact of the development of quantum theory and Bohr's confrontation with Einstein, especially their exchange concerning the EPR experiment, proposed by Einstein, Podolsky and Rosen in 1935.Bohr's interpretation was progressively characterized by a more radical epistemology, in its ultimate form, which was developed in the 1930s and with which I shall be especially concerned here, defined by his new concepts of phenomenon and atomicity.According to this epistemology, quantum objects are seen as indescribable and possibly even as inconceivable, and as manifesting their existence only in the effects of their interactions with measuring instruments upon those instruments, effects that define phenomena in Bohr's sense.The absence of causality is an automatic consequence of this epistemology.I shall also consider how probability and statistics work under these epistemological conditions.
One can construct the model conception of quantum phenomena (MCQP) which relates to the axiomatic conception of quantum phenomena (ACQP), (i.e. to the conventional quantum mechanics) in the same way, as the statistical physics relates to thermodynamics. Such a possibility is based on a new conception of geometry, which admits one to construct such a deterministic space-time geometry, where motion of free particles is primordially stochastic. The space-time geometry can be chosen in such a way that statistical description of random particle motion coincides with the quantum description. Methods of MCQP in investigation of quantum phenomena appear to be more subtle and effective than, that of ACQP. For instance, investigation of the free Dirac equation in framework of MCQP shows that the Dirac particle is in reality a rotator, i.e. two particles rotating around their common center of inertia. In the framework of MCQP one can discover the force field, responsible for pair production, that is impossible in the framework of ACQP.