Origin of Quantum Mechanics, of Physical Laws, and of the Physical World
 
Natural emergence
       of physical universes composed of quantum fields,
       of their spacetime, of initial conditions for their quantum evolution, and
       of their physical laws with local symmetries, yielding
              the standard interactions of elementary particles and quantum gravity

General multidimensional Gaussian distribution

 

My two latest papers[1,2] offer a simple and natural resolution to some of the most profound questions of particle physics and cosmology.

Skepticism about having found as early as in 2012 the correct answers to "most of the problems of modern physics" — which is how an eminent US physicist characterized the questions answered — is understandable and healthy. Nevertheless, please consider that:
My education and qualifications are well suited to explore the areas addressed.
My earlier work in theoretical particle physics and cosmology has consistently yielded acknowledged findings — several of which have been confirmed experimentally — about our real, physical world.
Derivation of the current results has been written up in detail. These results form a closed and natural picture that is remarkably straightforward. Quantum properties of our world, which are still puzzling to essentially everyone else, in this view are utmost natural and simple. So is natural and simple their origin.
At last, with the general picture available since 2012 and many opportunities to reexamine it, the obtained results have been verified and understood thoroughly in several equivalent descriptions.

Some of the fundamental questions answered in [1] and [2] are:

  1. Do the physical laws — including the postulates of quantum mechanics, quantum field theory, and general relativity — arise naturally from something much more elementary?
  2. Why does the physical evolution proceed by specific, unchanging fundamental laws?
  3. What laws govern the evolution on the shortest physical scales (at the Planck length), where the Standard Model of particle physics and canonically quantized general relativity[3] break down?
  4. Why do time and space unify in classical relativity but differ conceptually in quantum physics, even of relativistic systems? Why is the observed physical dynamics local? Why are its laws highly symmetric, e.g., have gauge symmetry and general covariance, yielding the electromagnetic, weak, strong and gravitational interactions?
  5. Which of the various "interpretations" of quantum mechanics (e.g., Copenhagen, many-world, hidden-variable, stochastic, super-deterministic, etc.) — some being different physical theories, predicting different outcomes of feasible experiments — is the correct one?
  6. Why do the observed large-scale cosmic structure and fluctuations in the cosmic microwave background indicate that our universe underwent cosmological inflation, despite convincing theoretical arguments by esteemed physicists [4, 5, 6, 7, 8, 9] that it is more probable to live in anthropically suitable matter configurations that have never inflated, e.g., in Boltzmann-brain worlds[10, 11]?
  7. How to reconcile the unitarity of quantum evolution with the apparent loss of information during the Hawking evaporation of a black hole? How does its evaporation end? What does an observer who falls in a black hole, see at its horizon? What physics applies to the singularity at its center?

The fundamentals of the physical world appear to be surprisingly simple. Their understanding requires no abstract mathematical or philosophical concepts. The only material structure behind the quantum-field worlds identified in [1] is the general distribution dN/(dQ1dQ2...) of a large number N of any material entities over many of their arbitrary independent properties Q1, Q2, ... that can be quantified with real numbers.

The nature of the material entities characterized by the quantities Q1, Q2, ... is irrelevant. If our universe originates as described, its material base is all the objectively existing information carriers, not limited to the objects in our or other emergent physical universes. The basic material entities are not expected to be embedded in any external spacetime or to evolve. It is sufficient for them just "to be".

The emergent physical worlds at sub-Planckian energies are succinctly described by effective quantum field theory, with all its standard mathematical machinery. The fields of the elementary particles of the emergent worlds undergo well-defined evolution, tractable on every physical scale.

The wave function of the emergent fields consists of alternate, equivalent presentations of the smoothly coarse-grained general distribution dN/(dQ1dQ2...) of the arbitrary basic material entities over their general properties Qn[1]. The elementary particles of the respective emergent physical worlds are quantized excitations of the fields. The general relativistic, quasiclassical spacetime of the worlds arises as detailed in [1].

The Born rule for the probabilities of alternate outcomes of quantum processes in the emergent worlds is not a postulate. It arises dynamically from the first principles. The worlds evolve naturally from cosmological inflation.

Unlike the previous theoretical approaches, we do not postulate fundamental physical principles, dynamics, or initial conditions. They all are what they are for the generically emerging quantum-field worlds, which actually and objectively exist in nature. The dynamics and initial conditions for a general class of the emergent systems appear, under their present understanding, to be indistinguishable from those observed in our universe.

This fundamental view of quantum evolution is the middle ground between Everett's picture (where essentially all the futures compatible with the conservation laws are assumed real) and interpretations of quantum mechanics that suggest only one branch of macroscopic evolution. Ditto the popular today — and vigorously explored by physicists and sci-fi writers for the past half-century — multiverse paradigm. The described view permits a variety of non-communicating universes with different physical laws, perhaps justifying anthropic explanation[12] of the tiny but non-zero cosmological constant. Yet by it, the laws of the physically real emergent universes span an infinitesimally small subset of all conceivable anthropically suitable laws of dynamics. In particular, it offers concrete answers[2] to the notoriously difficult questions about black holes: their information paradox, physics at their horizon and center, and the final moments of their Hawking evaporation.

Basic structure that produces the emergent quantum-field worlds is very general. In particular, it is ubiquitous in our familiar physical world. Hence the described systems certainly exist in nature. They evolve by dynamics and from initial conditions that pass the strict constraints of the contemporary particle-physics experiments, cosmological observations, and other empirical data. Some of the identified systems — apparently indistinguishable from our observeed universe — should contain internal inhabitants like us. Some of these inhabitants are occupied with what we currently are. Some of them, in particular, are pondering if their world originated as it did. It may be presumptuous to insist that we are not them. After all, their universe — physically real in every sense — is general.

Emergence of the wave function of locally supersymmetric fields
Emergence of spacetime and physical objects in it

Resolution of the Black Hole Information Paradox

Black hole illustration (wallpaperswide.com)

My latest second paper studies complete Hawking evaporation[1] of gravitational black holes in the described above generically emergent quantum-field worlds[2], likely including our universe. The paper explains physics at the centers of the black holes and at the end of their evaporation. The revealed picture is free from the information paradox[3] and the firewall paradox.

The inherent dynamics of the typical emergent quantum-field worlds is generally covariant. Their physical observers who fall in a black hole detect nothing special when crossing its horizon. Near its center the emergent fields cease to exist. Their evolving wave function is composed of alternate presentations the smoothed general distribution. The physical evolution is the continuous transformation that relates these presentations. It does not have to extend regularly indefinitely. Being excitations of quantum fields, the observers who fall across the horizon also stop to exist near the center of the black hole. The evolution elsewhere remains well-defined. The overall picture is sufficiently tractable to understand in detail and describe by equations. Covariant energy-momentum conservation remains a strict law. It follows from the inherent symmetries of the emergent systems.

Spin and Orbital Angular Momentum of Quarks and Gluons

Proton spin decomposition illustration

Intuitively, the spin of a proton or of any other hadron should be equal to the sum of the spins and orbital angular momenta of the constituent quarks and gluons. The respective decomposition in terms of the QCD operators, however, is not straightforward. For example, for gluon field it is impossible to define separate gauge-invariant densities of spin and orbital angular momentum.

On the other hand, experimentalists have been measuring the distribution of the spin of gluons in a hadron as the polarized gluon structure function Δg. With my MIT graduate advisor R. L. Jaffe, we developed a systematic method[1] of constructing gauge-invariant quark and gluon parton distributions for a general physical quantity. The developed method confirmed that Δg describes the gluon spin. Moreover, the method allowed us to find gauge-invariant distributions of quark and gluon orbital angular momenta[1], which together with the distributions of quark and gluon spins add up to the overall spin of the hadron (Bashinsky-Jaffe QCD sum rule).

Quantum Soliton

Aivazovsky, "The Ninth Wave"

A quantum field soliton at rest has a definite 4-momentum (M,0). Therefore, by the Heisenberg uncertainty principle, it is not localized in space. This project analyzed how the non-locality of a soliton position affects numerical computations of quantum corrections to the soliton mass and shape.

From H dibaryon to Scattering on a Lattice

H dibaryon illustration

As my first graduate project, with R. L. Jaffe we explored the possibility for the doubly strange H dibaryon[1] — (uuddss)singlet — to be unbound to strong decays. Color-magnetic interaction reduces[1] the energy of this singlet of the SU(3) flavor symmetry of the strong interaction. Yet the experimental searches have not revealed a corresponding stable or weakly decaying particle. Anticipating that H may decay strongly, we calculated[2] its experimental signatures in the coupled two-baryon channels for every possible mass of H. The expected enhancement in Λ Λ invariant mass spectrum has since been experimentally observed[3, 4, 5] by KEK-PS E224 and E522 collaborations.

The developed techniques can, in principle, be also applied to computing a cross section of two-particle scattering on a lattice.