In mathematics, the Simon problems (or Simon's problems) are a series of fifteen questions posed in the year 2000 by Barry Simon, an American mathematical physicist.[1][2] Inspired by other collections of mathematical problems and open conjectures, such as the famous list by David Hilbert, the Simon problems concern quantum operators.[3] Eight of the problems pertain to anomalous spectral behavior of Schrödinger operators, and five concern operators that incorporate the Coulomb potential.[1]
In 2014, Artur Avila won a Fields Medal for work including the solution of three Simon problems.[4][5] Among these was the problem of proving that the set of energy levels of one particular abstract quantum system was in fact the Cantor set, a challenge known as the "Ten Martini Problem" after the reward that Mark Kac offered for solving it.[5][6]
The 2000 list was a refinement of a similar set of problems that Simon had posed in 1984.[7][8]
Background definitions for the "Coulomb energies" problems (
Simon listed the following problems in 1984:[7]
No. | Short name | Statement | Status | Year solved |
---|---|---|---|---|
1st | (a) Almost always global existence for Newtonian gravitating particles | (a) Prove that the set of initial conditions for which Newton's equations fail to have global solutions has measure zero.. | Open as of 1984.[7][needs update] In 1977, Saari showed that this is true for 4-body problems.[9] | ? |
(b) Existence of non-collisional singularities in the Newtonian N-body problem | Show that there are non-collisional singularities in the Newtonian N-body problem for some N and suitable masses. | In 1988, Xia gave an example of a 5-body configuration which undergoes a non-collisional singularity.[10][11]
In 1991, Gerver showed that 3n-body problems in the plane for some sufficiently large value of n also undergo non-collisional singularities.[12] |
1989
~Duckmather --> | |
2nd | (a) Ergodicity of gases with soft cores | Find repulsive smooth potentials for which the dynamics of N particles in a box (with, e.g., smooth wall potentials) is ergodic.
Sinai once proved that the hard sphere gas is ergodic, but no complete proof has appeared except for the case of two particles, and a sketch for three, four, and five particles.[7] |
? | |
(b) Approach to equilibrium | Use the scenario above to justify that large systems with forces that are attractive at suitable distances approach equilibrium, or find an alternate scenario that does not rely on strict ergodicity in finite volume. | ? | ||
(c) Asymptotic abelianness for the quantum Heisenberg dynamics | Prove or disprove that the multidimensional quantum Heisenberg model is asymptotically abelian. | ? | ||
3rd | Turbulence and all that | Develop a comprehensive theory of long-time behavior of dynamical systems, including a theory of the onset of and of fully developed turbulence. | ? | |
4th | (a) Fourier's heat law | Find a mechanical model in which a system of size |
? | |
(b) Kubo's formula | Justify Kubo's formula in a quantum model or find an alternate theory of conductivity. | ? | ||
5th | (a) Exponential decay of |
Consider the two-dimensional classical Heisenberg model. Prove that for any beta, correlations decay exponentially as distance approaches infinity. | Open as of 1984.[needs update] | ? |
(b) Pure phases and low temperatures for the |
Prove that, in the | |||
(c) GKS for classical Heisenberg models | Let | |||
(d) Phase transitions in the quantum Heisenberg model | Prove that for | |||
6th | Explanation of ferromagnetism | Verify the Heisenberg picture of the origin of ferromagnetism (or an alternative) in a suitable model of a realistic quantum system. | ? | |
7th | Existence of continuum phase transitions | Show that for suitable choices of pair potential and density, the free energy is non- |
? | |
8th | (a) Formulation of the renormalization group | Develop mathematically precise renormalization transformations for |
Open as of 1984.[needs update] | ? |
(b) Proof of universality | Show that critical exponents for Ising-type systems with nearest neighbor coupling but different bond strengths in the three directions are independent of ratios of bond strengths. | |||
9th | (a) Asymptotic completeness for short-range N-body quantum systems | Prove that |
Open as of 1984.[7][needs update] | ? |
(b) Asymptotic completeness for Coulomb potentials | Suppose | |||
10th | (a) Monotonicity of ionization energy | (a) Prove that |
Open as of 1984.[needs update] | ? |
(b) The Scott correction | Prove that | |||
(c) Asymptotic ionization | Find the leading asymptotics of | |||
(d) Asymptotics of maximal ionized charge | Prove that | |||
(e) Rate of collapse of Bose matter | Find suitable | |||
11th | Existence of crystals | Prove a suitable version of the existence of crystals (e.g. there is a choice of minimizing configurations that converge to some infinite lattice configuration). | ? | |
12th | (a) Existence of extended states in the Anderson model | Prove that in |
Open as of 1984.[needs update] | ? |
(b) Diffusive bound on "transport" in random potentials | Prove that | |||
(c) Smoothness of |
Is | |||
(d) Analysis of the almost Mathieu equation | Verify the following for the almost Mathieu equation:
| |||
(e) Point spectrum in a continuous almost periodic model | Show that | |||
13th | Critical exponent for self-avoiding walks | Let |
? | |
14th | (a) Construct QCD | Give a precise mathematical construction of quantum chromodynamics. | Open as of 1984.[needs update] | ? |
(b) Renormalizable QFT | Construct a nontrivial quantum field theory that is renormalizable but not superrenormalizable. | |||
(c) Inconsistency of QED | Prove that QED is not a consistent theory. | |||
(d) Inconsistency of |
Prove that a nontrivial | |||
15th | Cosmic censorship | Formulate and then prove or disprove a suitable version of cosmic censorship. | ? |
In 2000, Simon claimed that five[which?] of the problems he listed had been solved.[1]
The Simon problems as listed in 2000 (with original categorizations) are:[1][13]
No. | Short name | Statement | Status | Year solved |
---|---|---|---|---|
Quantum transport and anomalous spectral behavior | ||||
1st | Extended states | Prove that the Anderson model has purely absolutely continuous spectrum for |
? | ? |
2nd | Localization in 2 dimensions | Prove that the spectrum of the Anderson model for |
? | ? |
3rd | Quantum diffusion | Prove that, for |
? | ? |
4th | Ten Martini problem | Prove that the spectrum of |
Solved by Puig (2003).[13][14] | 2003 |
5th | Prove that the spectrum of |
Solved by Avila and Krikorian (2003).[13][15] | 2003 | |
6th | Prove that the spectrum of |
? | ? | |
7th | Do there exist potentials |
Essentially solved by Denisov (2003) with only |
2003, 2005 | |
8th | Suppose that |
? | ? | |
Coulomb energies | ||||
9th | Prove that |
? | ? | |
10th | What are the asymptotics of |
? | ? | |
11th | Make mathematical sense of the nuclear shell model. | ? | ? | |
12th | Is there a mathematical sense in which one can justify current techniques for determining molecular configurations from first principles? | ? | ? | |
13th | Prove that, as the number of nuclei approaches infinity, the ground state of some neutral system of molecules and electrons approaches a periodic limit (i.e. that crystals exist based on quantum principles). | ? | ? | |
Other problems | ||||
14th | Prove that the integrated density of states |
| k(E1 + ΔE) - k(E1) | < ε | ? | |
15th | Lieb-Thirring conjecture | Prove the Lieb-Thirring conjecture on the constants |
? | ? |
![]() | Original source: https://en.wikipedia.org/wiki/Simon problems.
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