If quantum mechanics is the solution, what should the problem be?

: The paper addresses the problem, which quantum mechanics resolves in fact. Its viewpoint suggests that the crucial link of time and its course is omitted in understanding the problem. The common interpretation underlain by the history of quantum mechanics sees discreteness only on the Plank scale, which is transformed into continuity and even smoothness on the macroscopic scale. That approach is fraught with a series of seeming paradoxes. It suggests that the present mathematical formalism of quantum mechanics is only partly relevant to its problem, which is ostensibly known. The paper accepts just the opposite: The mathematical solution is absolute relevant and serves as an axiomatic base, from which the real and yet hidden problem is deduced. Wave-particle duality, Hilbert space, both probabilistic and many-worlds interpretations of quantum mechanics, quantum information, and the Schrödinger equation are included in that base. The Schrödinger equation is understood as a generalization of the law of energy conservation to past, present, and future moments of time. The deduced real problem of quantum mechanics is: “What is the universal law describing the course of time in any physical change therefore including any mechanical motion?”

I have hinted the famous answer "42" as a metaphor of "The present situation in quantum mechanics", re-coining the title of a philosophical and critical review published by Schrödinger (1935) eighty years ago. The answer, i.e. quantum mechanics, is available, however the question, to which it should refer, is unknown yet and yet.
The present paper is an attempt to imagine or deduce the problem judging only by the answer rather than by the prejudice known as its interpretations. Perhaps, that intention would met sharp criticism for quantum mechanics is a tool working exceptionally well, on the one hand, and at least a few of the interpretations of quantum mechanics are accepted in the corpus of human knowledge, on the other hand. One can admit that the paper is skeptical to both and thus doubts them. This is not true. The text is skeptical only to that quantum mechanics and its interpretations are all truth rather than they are true.
This means that some crucial link is omitted in the picture of quantum mechanics so that its whole remains yet incomprehensible therefore imposing a functional and abstractly mathematical approach to quantum mechanics as to something, which works somehow... however works very well. the principle of complementarity, the principle of correspondence, quantum mechanics formulated in Hilbert space, etc.
However the collection of all those facts is often interpreted in a misleading way: The very small physical objects, the quantity of action of which is commeasurable with the Planck constant, are discrete. That discreteness is gradually transformed into the continuity of all quantities as to the physical bodies of our experience. The formalism of quantum mechanics based on Hilbert space represents this transformation. However it implies very ridiculous corollaries such as: both Born's and Hugh Everett III's (many-worlds) interpretations, Einstein-Podolsky-Rosen's "paradox", Schrödinger's "cat", Wigner's "friend" and many others, which should not be referred to reality by itself but to the mathematical model of quantum mechanics, which will be ostensibly perfected in the future.
Consequently, the mathematical solution involved by quantum mechanics is only partly relevant to its problem for the really relevant mathematical solution is forthcoming.
However, the expected relevant solution has not yet appeared, many of the ridiculous corollaries were ultimately confirmed experimentally and no one of them has be able to be refuted. Almost all physicians use just the standard mathematical formalism of quantum mechanics and escape to reflect on its metaphysical interpretations. So, the mathematical formalism seems to be the true unlike its philosophical interpretations being even redundant in a sense. The real solution is available, and the problem, to which it refers, seems to be unimportant and petty, but never mind. That is the situation in the philosophy of quantum mechanics, which can be designated by the metaphor "42": The answer is clear, but what on earth is the question?
3. The necessary and sufficient facts relevant to the hidden problem of quantum mechanics One can attempt another approach to the real problem of quantum mechanics starting from its formalism and thus from the ridiculous corollaries rather than from the presupposed interpretations of it. That approach would use the available mathematical formalism as the reliable base from which the true, but hidden yet problem of quantum mechanics might be deduced. This means that the mathematical formalism, i.e. the "answer", is equivalent to the problem, i.e. the "question", in a sense for both answer and question are interdeducible from each other. This is admissible as the "ridiculous corollaries" are granted as true in that approach. Furthermore, it hints the idea the problem to be not only deduced, but to be deduced even axiomatically from the formalism for the formalism is just mathematical and thus easily representable axiomatically. Even more, those axiomatic features necessary and sufficient for both "answer and question" to be deduced from them can be embedded in the real facts of the history of quantum mechanics thus interpreting. Those fundamental facts can be the following: (1) wave-particle duality; (2) the probabilistic (Max Born 1957) and many-worlds (Hugh Everett III 1957) interpretations of quantum mechanics; (3) Hilbert space as the basic mathematical formalism of quantum mechanics; (4) the "no hidden variables" theorems in quantum mechanics. The concept of (5) quantum information and the (6) Schrödinger equation linking these properties (1-4) of the formalism of quantum mechanics to its utilization and meaning will be considered a little latter and in detail.
3.1. Wave-particle duality addresses the dual behavior of any quantum object such as an atom, an electron, a photon, etc. according to the kind of experiment: One and the same thing can be considered both as a particle and as a wave. However this is not contradictory because it behaviors either as a particle or as a wave in any given experiment just according to its kind. One can say that being either a particle or a wave is an accidental feature depending only on the external circumstances rather than an essential property referring to its nature and definition. Wave-particle duality should be reformulated as the invariance of the physical laws to all discrete and smooth (being necessary continuous) motions in the usual three-dimensional Euclidean space. Thus, the duality can be considered as a generalization of Einstein's equivalence in general relativity (1918) to all reference frames corresponding to the smooth motions. Then wave-particle duality means for the Einstein equivalence to be extended including also all discrete motions, i.e. all quantum leaps.
3.2. Hilbert space as the basic mathematical formalism of quantum mechanics has been introduced after the merging of matrix and wave mechanics ultimately completed in John von Neumann's "Mathematical foundations of quantum mechanics" (1932): Any state of any quantum system can be represented by a wave function, which is a "point" in Hilbert space, and vice versa. Any physical quantity is a kind of linear operator in Hilbert space (a "hyper-maximal operator" according to Neumann's terminology).
Hilbert space is the simplest mathematical structure, which "points" can represent equally well a leap and a smooth motion in the three-dimensional Euclidean space and thus are invariant both to discrete and to smooth morphisms of it therefore satisfying the generalized Einstein principle above.
3.3. The probabilistic (Max Born 1957) and many-worlds (Hugh Everett III, 1957) interpretations of quantum mechanics connect the wave function with the statistical ensemble of observed results after measuring the quantum state possessing this wave function. The square of the module of the wave function corresponds unambiguously to the probability for the state to be measured according to the Max Born interpretation. Any state whether the observed or other can be considered as an actual member of a statistical ensemble of all states and thus as a "world" continuing to exist in parallel to ours according to the "many-worlds" interpretation. The measurement or observation, which has chosen somehow to be in our world, therefore has called the splitting between them at the same time.
Though the concept of wave function as a point in Hilbert space has been initially involved to satisfy the uniform description of quantum leaps and smooth motions (or "wave-particle duality"), it turns out to has additionally another symmetry or invariance after both probabilistic and many-world interpretations: It is able to describe uniformly a coherent state (which is unorderable in principle for the "no-hidden variables" theorems) and the corresponding statistical ensemble (which is always well-orderable). Thus, it involves necessarily: (1) the well-ordering theorem equivalent to the axiom of choice, in the mathematical model; and (2) furthermore, choice and information as the quantity of choices, in quantum mechanics. The same can be interpreted: (1) ontologically as the invariance of the possible and actual, (2) mathematically as a kind of set-theory invariance in relation to the axiom of choices, and (3) as an invariance embodied in the concept of information.
Nevertheless, the link between wave-particle duality and the newly formulated "possibilityactuality duality" in quantum mechanics needs some explanation for it should be not an accidental feature infused by the mathematical model but an essential part of the problem, which is researched and re-searched.
3.4. The meant "no hidden variables" theorems in quantum mechanics are that of John von Neumann (1932: 157-173) and that of Kochen and Specker (1968), which can be considered both as amplification and as generalization of the former. They show that the "unused half" of variables in comparison to classical mechanics for a mechanical system to be exhaustedly described is redundant in principle if the mathematical model is that of Hilbert space. They can be also considered as a corollary from the above statements (3.1-3.3) and thus are able not to be included within the corpus of necessary axioms. However, they are rather useful for the mentioned two dualities or invariances to be unified into a single one: Indeed any of both dualities "spares" the one half of variables as "dual" and thus "redundant".
In other words, classical mechanics accepts that a leap and a smooth motion are different, therefore each of them needs a proper description. Quantum mechanics involves their invariance and thus "spares" the one description. Classical mechanics accepts that a possible state and an actual one are different. So, each of them needs a relevant description. Analogically, quantum mechanics introduces their equivalence and thus goes without the one description. Consequently, that "economy" is the common base shared by both dualities. The essence of that "economy" is information, especially quantum information. Their units, correspondingly a bit and a qubit, are the "currency" of the "saving".

Quantum information and how it is able to help us
The concept of quantum information introduced by quantum mechanics may be used to describe uniformly future and past and thus the present as the frontier of time.
The conception of quantum information was introduced in the theory of quantum information studying the phenomena of entanglement in quantum mechanics. The entanglement was theoretically forecast in the famous papers of Einstein, Podolsky, and Rosen (1935) and independently by Shrödinger (1935) deducing it from Hilbert space. However, the former three demonstrated the forecast phenomenon as the proof of the alleged "incompleteness of quantum mechanics". John Bell (1964) deduced a sufficient condition as an experimentally verifiable criterion in order to distinguish classical from quantum correlation (entanglement). Aspect, Grangier, andRoger (1981, 1982) confirmed experimentally the existence of quantum correlations exceeding the upper limit of the possible classical correlations. The theory of quantum information has thrived since the end of the last century in the areas of quantum computer, quantum communication, and quantum cryptography.
The fundament of quantum information is the concept of 'quantum bit', "qubit" definable as the normed superposition of any two orthogonal subspaces of complex Hilbert space as follows: 'Qubit' is: |0⟩+ |1⟩ where , are complex numbers such that | | 2 + | | 2 =1, and |0⟩, |1⟩ are any two orthonormal vectors (e.g. the orthonormal bases of any two subspaces) in any vector space (e.g. Hilbert space, Euclidean space, etc.). Thus Hilbert space underlying quantum mechanics is representable as the quantity of quantum information and any wave function, i.e. any state of any quantum system being a point in it can be seen as a value of that quantity. Consequently, all physical processes turn out to be quantum-informational, and nature or the universe may be interpreted as a quantum computer processing quantum information.
The qubit is also isomorphic to a ball in Euclidean space, in which two points are chosen: the one chosen within the ball, and the other being the orthogonal projection on its surface, i.e. as a mapping of a unit ball onto its surface (or any other unit sphere).
Quantum information can be interpreted as the transfinite generalization of information. Its unit, a qubit, can be interpreted as a choice among an infinite set of alternatives. It generalizes the unit of classical information, a bit, which refer to a finite set of alternatives.
If one uses the notion of "length of now" defined as the period of the de Broglie (1925) wave associable to any physical item, the "length of now" of the apparatus can be visualized as a random chosen point onto the segment of the "length of now" of the measured quantum entity. Thus quantum mechanics is forced to describe uniformly the future, present and past of the investigated system. Future is represented as a coherent whole, present as a choice among infinitely many alternatives, and past as a well-ordering obtained as a result of a series of choices. The concept of quantum information unifies the future, present, and past as a measurable physical quantity. It describes the frontier of time, that "now", which transforms future into past.
The theorems about the absence of hidden variables in quantum mechanics (Neumann 1932;Kochen, Specker 1968) demonstrate that the mathematical formalism of quantum mechanics implies that no well-ordering of any coherent state might exist before measurement. However, the same coherent state is transformed into a well-ordered series of results in time after measurement. In order to be equated the state before and after measurement, the well-ordering theorem equivalent to the axiom of choice is necessary. The measurement mediating between them should be interpreted as an absolutely random choice of an element of the coherent state, for which no constructive way (equivalent to some "hidden variable") can exist in principle. The quantity of quantum information can describe uniformly the state before and after measurement (equivalent to a choice among an infinite set). Any wave function, being a given value of quantum information, "bounds" an unorderable and a well-ordered state as the quantity of qubits (i.e. the "infinite choices") necessary for the latter to be obtained from the former.
The quantity of quantum information is also the ordinal corresponding to the infinity series of finite choices. Both definitions of 'ordinal' (Cantor 1897;Neumann 1923) are applicable as the ordinals are relatively "small". The ordinal number defined in Cantor -Russell (Whitehead, Russell [any edition] : ) generates a statistical ensemble while that in Neumann, a well-ordering. Both correspond one-to-one to a coherent state as the one and same quantity of quantum information containing in it. One can accept that both definitions of "ordinal" are equivalent to where both definitions are applicable, i.e. to relatively "small" transfinite ordinals. Furthermore, that equivalence in turn corresponds to the equivalence of both definitions of the quantity of information: (1) as mutual entropy, i.e. as the functional of some probability distribution on the basis of another; (2) as the minimal length of an algorithm, which is able to reorder a well-ordering into another, i.e. the transfinite generalization of the Kolmogorov (1965Kolmogorov ( , 1968 definition of information. In fact, the concept of quantum information rests on the latter equivalence therefore corresponding thus to the equivalence of the ways for "ordinal" to be defined. Even more, one can offer the hypothesis that quantum information and thus the equivalence of the well-ordered and "statistical-ensemble" ordinals underlies the fundamental equation of quantum mechanics: the Schrödinger equation, therefore elucidating its meaning. The concept of quantum information allows of a large-scale synthesis: It links the physical processes studied by quantum mechanics to the theory of information, and by meditation of it, both to set theory and to the ontology of time in philosophy. The core of that synthesis is just "quantum information", which explains the course of time as ordering and relations of orderings (i.e. in terms of information)

The Schrödinger equation
We suggest that the Schrödinger equation is well-known in all modifications. So, it will be sufficient and more suitable to describe it only qualitatively for the present objectivity: It equates the first time derivative (therefore the change in time) of the wave function (therefore a value of quantum information) of any quantum system to the algebraic sum of (1, with sign minus sign) the second space derivative (laplacian and thus the tensor product of two changes in space) of the same wave function (and the same value of quantum information) corresponding to kinetic energy in classical mechanics and of (2, with a plus sign) the product of a potential function and the same wave function, corresponding to potential energy in classical mechanics. Both sides of the equation have the physical dimension of energy. The coefficients involved in the equation are the Planck constant, the mass of the system (more exactly, the reduced mass of the system), and the imaginary unit, i, which is very important for the information interpretation of the equation.
A few preliminary comments are necessary: 5.1. The Schrödinger equation is a generalization of the fundamental law of energy conservation in classical mechanics: Indeed the former implies the latter if the wave function is a constant as a particular case. In turn, the generalization involves just complex functions being inapplicable as to any real functions. One may suggests then that quantum information corresponds to a relevant generalization of energy already definable as to complex values therefore involving a second, i.e. just imaginary dimension of energy. That dimension is interpretable as time energy unlike kinetic and potential energy both space energies. Unfortunately the suitable term of "space-time energy" as equivalent to quantum information would call a series of messes for special and general relativity. Another option for them is to be designated correspondingly as temporal and spatial energy. Then, one of the possible meanings of the Schrödinger equation would be their equating. Furthermore the spatial energy would correspond to quantum information defined as a statistical ensemble (or as an ordinal in Cantor -Russell), and the temporal energy, defined as a transfinite ordinal (in Neumann).
5.2. The potential and kinetic energy are clearly distinguished from each other in classical mechanics: Kinetic energy corresponds to the real motion depending only on its velocity, and potential energy describes the force in each spatial point acting on a tentative reference unit (e.g. a body or a material point) depending only on its position. The law of energy conservation means the way for the acting of the force to be transformed into the motion of some real item. The Schrödinger equation generalizes the classical understanding as follows: The wave function corresponds to space in a different way in the cases of kinetic and potential energy: The tensor product of two identical and complementary (or "conjugate") wave functions is mapped into space if the energy is kinetic, and a single wave function is mapped into space in the case of potential energy. Indeed the latter can be interpreted as the action on an energymomentum unit thus depending only on the spatial coordinates. However this representation closer to the ideas of classical mechanics is "paraphrased" at present (and particularly in the Standard model) as a few kinds of fundamental symmetries: any symmetry is a relation between a set of symmetric elements as different and the same set as a single element being a class of equivalence to the symmetry in question. Thus, the concept of symmetry expresses differently but equivalently the underlying idea of quantum information: the choice of an element among a set of equivalent, but different alternatives. Nevertheless the form of the Schrödinger equation is universal referring to all possible symmetries rather than to the ones really observed in experiments until now or to the ones included in the Standard model. 5.3. The invariance of discrete leaps and smooth motions allows of the Schrödinger equation to be represented by the corresponding units: bits and qubits. Furthermore, one can introduce a new distinction between real (or kinetic) and potential qubits: the formers for kinetic energy, the laters for potential energy. Then, the Schrödinger equation can be formulated so: The energy of a (trans)finite bit is equal to the subtraction of the energy of a potential and a kinetic qubit. The necessary equivalence of potential and kinetic qubits is implied by the equivalence of the probabilistic and many-worlds interpretation (3.3 above) and in turn implies the equivalence of a bit of a transfinite position ("transfinite bit") and a bit of a finite position ("finite bit").
5.4. The Kochen -Specker (1968) theorem helps us to avoid a mess: the equation of the energies as above does not mean that a qubit can be equivalent to a bit, which would contradict to the direct corollary (Kochen, Specker 1968: 70), which is immediately after the main theorem of their paper (ibid., a few lines above). In fact the concept of energy conservation (only generalized in the Schrödinger equation), as Emmy Noether's (1918) fundamental theorem shows, implies the equality of all moments of time. Consequently, the equation of energies implies that the past moment corresponding to a bit, the present moment: to a kinetic qubit, and the future moment: to a potential qubit are already presupposed as equivalent, but this does not refer to the bits and qubits themselves: They are fundamentally different, and only the quantity of their corresponding energy can be equated.
Summarizing all consideration above, one can suggest the following meaning of the Schrödinger equation in terms of quantum information: It generalizes energy conservation to past, present, and future moments of time rather than only to present and future moments as this does the analogical law in classical mechanics. Thus, it is the universal law of how "time flows" or in other words, about the course of time. Furthermore, resolving its problem, the Schrödinger equation suggests the proportionality (or even equality if the units are relevantly chosen) of the