- Source: Simon problems
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. Inspired by other collections of mathematical problems and open conjectures, such as the famous list by David Hilbert, the Simon problems concern quantum operators. Eight of the problems pertain to anomalous spectral behavior of Schrödinger operators, and five concern operators that incorporate the Coulomb potential.
In 2014, Artur Avila won a Fields Medal for work including the solution of three Simon problems. 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.
The 2000 list was a refinement of a similar set of problems that Simon had posed in 1984.
Context
Background definitions for the "Coulomb energies" problems (
N
{\displaystyle N}
non-relativistic particles (electrons) in
R
3
{\displaystyle \mathbb {R} ^{3}}
with spin
1
/
2
{\displaystyle 1/2}
and an infinitely heavy nucleus with charge
Z
{\displaystyle Z}
and Coulombic mutual interaction):
H
f
(
N
)
{\displaystyle {\mathcal {H}}_{f}^{(N)}}
is the space of functions on
L
2
(
R
3
N
;
C
2
N
)
{\displaystyle L^{2}(\mathbb {R} ^{3N};\mathbb {C} ^{2N})}
which are asymmetrical under exchange of the
N
{\displaystyle N}
spin and space coordinates. Equivalently, the subspace of
(
L
2
(
R
3
)
⊗
C
2
)
⊗
N
{\displaystyle (L^{2}(\mathbb {R} ^{3})\otimes \mathbb {C} ^{2})^{\otimes N}}
which is asymmetrical under exchange of the
N
{\displaystyle N}
factors.
The Hamiltonian is
H
(
N
,
Z
)
:=
∑
i
=
1
N
(
−
Δ
i
−
Z
|
x
i
|
)
+
∑
i
<
j
1
|
x
i
−
x
j
|
{\displaystyle H(N,Z):=\sum _{i=1}^{N}(-\Delta _{i}-{\frac {Z}{|x_{i}|}})+\sum _{i
. Here
x
i
∈
R
3
{\displaystyle x_{i}\in \mathbb {R} ^{3}}
is the coordinate of the
i
{\displaystyle i}
-th particle,
Δ
i
{\displaystyle \Delta _{i}}
is the Laplacian with respect to the coordinate
x
i
{\displaystyle x_{i}}
. Even if the Hamiltonian does not explicitly depend on the state of the spin sector, the presence of spin has an effect due to the asymmetry condition on the total wave-function.
We define
E
(
N
,
Z
)
:=
min
H
f
H
(
N
,
Z
)
{\displaystyle E(N,Z):=\min _{{\mathcal {H}}_{f}}H(N,Z)}
, that is, the ground state energy of the
(
N
,
Z
)
{\displaystyle (N,Z)}
system.
We define
N
0
(
Z
)
{\displaystyle N_{0}(Z)}
to be the smallest value of
N
{\displaystyle N}
such that
E
(
N
+
j
,
Z
)
=
E
(
N
,
Z
)
{\displaystyle E(N+j,Z)=E(N,Z)}
for all positive integers
j
{\displaystyle j}
; it is known that such a number always exists and is always between
Z
{\displaystyle Z}
and
2
Z
{\displaystyle 2Z}
, inclusive.
The 1984 list
Simon listed the following problems in 1984:
In 2000, Simon claimed that five of the problems he listed had been solved.
The 2000 list
The Simon problems as listed in 2000 (with original categorizations) are:
See also
Almost Mathieu operator
Lieb–Thirring inequality
External links
"Simon's Problems". MathWorld. Retrieved 2018-06-13.
References
Kata Kunci Pencarian:
- Herbert Simon
- Britania Raya
- Tantrum
- Bahasa Inggris
- Globalisasi
- Perang Dunia II
- Alberht dari Anglia Timur
- Idris Elba
- Rusia
- Rishi Sunak
- Simon problems
- Simon's problem
- Smale's problems
- List of unsolved problems in mathematics
- Simon Reeve (British TV presenter)
- Deutsch–Jozsa algorithm
- Problem solving
- Simon Cowell
- Simon & Garfunkel
- Herbert A. Simon