The appearance of tracks, close to classical orbits, left by charged quantum particles propagating inside a detector, such as a cavity periodically illuminated by light pulses, is studied for a family of idealized models. In the semi-classical regime, which is reached when one considers highly energetic particles, we present a detailed, mathematically rigorous analysis of this phenomenon. If the Hamiltonian of the particles is quadratic in position- and momentum operators, as in the examples of a freely moving particle or a particle in a homogeneous external magnetic field, we show how symmetries, such as spherical symmetry, of the initial state of a particle are broken by tracks consisting of infinitely many approximately measured particle positions and how, in the classical limit, the initial position and velocity of a classical particle trajectory can be reconstructed from the observed particle track.

1.
M.
Ballesteros
,
T.
Benoist
,
M.
Fraas
, and
J.
Fröhlich
, “
The appearance of particle tracks in detectors
,”
Commun. Math. Phys.
385
(
1
),
429
463
(
2021
).
2.
M.
Ballesteros
,
N.
Crawford
,
M.
Fraas
,
J.
Fröhlich
, and
B.
Schubnel
, “
Non-demolition measurements of observables with general spectra
,” in
Mathematical Problems in Quantum Physics (QMATH 13)
, edited by
F.
Bonetto
,
D.
Borthwick
,
E.
Harrell
, and
M.
Loss
[
Contemp. Math.
717
,
241
256
(
2018
)].
3.
R.
Figari
and
A.
Teta
, “
Emergence of classical trajectories in quantum systems: The cloud chamber problem in the analysis of Mott (1929)
,”
Arch. Hist. Exact Sci.
67
,
215
234
(
2013
).
4.
R.
Figari
and
A.
Teta
,
Quantum Dynamics of a Particle in a Tracking Chamber
, Springer Briefs in Physics (
Springer-Verlag
,
Heidelberg, New York, Dordrecht, London
,
2014
).
5.
O.
Steinmann
, “
Particle localization in field theory
,”
Commun. Math. Phys.
7
,
112
137
(
1968
).
6.
E.
Schrödinger
, “
Der stetige übergang von der mikro- zur makromechanik
,”
Naturwissenschaften
14
,
664
666
(
1926
).
7.
K.
Hepp
, “
The classical limit for quantum mechanical correlation functions
,”
Commun. Math. Phys.
35
,
265
277
(
1974
).
8.
A.
Bouzouina
and
D.
Robert
, “
Uniform semiclassical estimates for the propagation of quantum observables
,”
Duke Math. J.
111
(
2
),
223
252
(
2002
).
9.
M.
Zworski
,
Semiclassical Analysis
(
American Mathematical Society
,
Providence, RI
,
2012
), Vol. 138.
10.
J.
Dereziński
and
C.
Gérard
,
Mathematics of Quantization and Quantum Fields
(
Cambridge University Press
,
Cambridge, UK
,
2013
).
11.
B.
Simon
,
Functional Integration and Quantum Physics
, 2nd ed. (
AMS Chelsea Publishing; American Mathematical Society
,
Providence, RI
,
2005
).
12.

Note that, in general, an abstract random variable is denoted by a capital letter, while its values are denoted by the corresponding lower-case letter. For example, the approximate position of a particle is a random variable denoted by Q and its measured values are denoted by q.

13.
B.
Russo
,
H.
Dye
 et al., “
A note on unitary operators in C*-algebras
,”
Duke Math. J.
33
,
413
416
(
1966
).
14.
P.-L.
Lions
and
T.
Paul
, “
Sur les mesures de Wigner
,”
Rev. Mat. Iberoam.
9
(
3
),
553
618
(
1993
).
15.

More precisely, that for any C > 0, there exists a finite n0N0 such that for any nn0, Σn > C.

16.
M.
Reed
and
B.
Simon
,
Methods of Modern Mathematical Physics. Vol. 1. Functional Analysis
(
Academic Press
,
New York
,
1980
), revised and enlarged edition.
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