-
1
-
-
0009448302
-
Über den anschaulichen inhalt der quantentheoretischen Kinematik und mechanik
-
For an English translation of this article see Ref. 2
-
W. Heisenberg, "Über den anschaulichen Inhalt der quantentheoretischen Kinematik und Mechanik," Z. Phys. 43, 172-198 (1927). For an English translation of this article see Ref. 2.
-
(1927)
Z. Phys.
, vol.43
, pp. 172-198
-
-
Heisenberg, W.1
-
2
-
-
0004205622
-
-
Princeton U.P., Princeton, NJ
-
J. A. Wheeler and W. H. Zurek, Quantum Theory and Measurement (Princeton U.P., Princeton, NJ, 1983), p. 62.
-
(1983)
Quantum Theory and Measurement
, pp. 62
-
-
Wheeler, J.A.1
Zurek, W.H.2
-
3
-
-
0003429685
-
-
Princeton University, Princeton
-
John von Neumann, Mathematical Foundations of Quantum Mechanics (Princeton University, Princeton, 1955), pp. 353, 354. Translated from the original German edition: Johann von Neumann, Mathematische Grundlagen der Quantenmechanik (Springer-Verlag, Berlin, 1932), pp. 187 and 188. These two pages provide an easy reference for the views we want to criticize in this article, but similar views are widespread in the literature.
-
(1955)
Mathematical Foundations of Quantum Mechanics
, pp. 353
-
-
Von Neumann, J.1
-
4
-
-
0004008274
-
-
Springer-Verlag, Berlin, These two pages provide an easy reference for the views we want to criticize in this article, but similar views are widespread in the literature
-
John von Neumann, Mathematical Foundations of Quantum Mechanics (Princeton University, Princeton, 1955), pp. 353, 354. Translated from the original German edition: Johann von Neumann, Mathematische Grundlagen der Quantenmechanik (Springer-Verlag, Berlin, 1932), pp. 187 and 188. These two pages provide an easy reference for the views we want to criticize in this article, but similar views are widespread in the literature.
-
(1932)
Mathematische Grundlagen der Quantenmechanik
, pp. 187
-
-
Von Neumann, J.1
-
5
-
-
85033766345
-
-
In view of the difficulties that beset the definition of action and angle variables as self-adjoint operators in quantum mechanics we prefer the more general term "observable" to distinguish them from c numbers
-
In view of the difficulties that beset the definition of action and angle variables as self-adjoint operators in quantum mechanics we prefer the more general term "observable" to distinguish them from c numbers.
-
-
-
-
7
-
-
0000307666
-
Discussion with Einstein on epistemological problems in atomic physics
-
edited by P. A. Schilpp Open Court, La Salle, IL, Reprinted in Ref. 2, p. 22
-
Niels Bohr, "Discussion with Einstein on epistemological problems in atomic physics," in Albert Einstein: Philosopher-Scientist, edited by P. A. Schilpp (Open Court, La Salle, IL, 1949), p. 214. Reprinted in Ref. 2, p. 22.
-
(1949)
Albert Einstein: Philosopher-Scientist
, pp. 214
-
-
Bohr, N.1
-
8
-
-
33744655885
-
Canonical transformations with time as a coordinate
-
O. D. Johns, "Canonical transformations with time as a coordinate," Am. J. Phys. 57, 204-215 (1989).
-
(1989)
Am. J. Phys.
, vol.57
, pp. 204-215
-
-
Johns, O.D.1
-
9
-
-
0003284838
-
Classical dynamics
-
edited by S. Flügge Springer-Verlag, Berlin, Somewhat disappointingly, Synge confines his treatment of relativistic particle dynamics to one-particle systems, a most atypical case
-
J. L. Synge, "Classical Dynamics," in Vol. 3, Part 1 of Encyclopedia of Physics, edited by S. Flügge (Springer-Verlag, Berlin, 1960), p. 105. Somewhat disappointingly, Synge confines his treatment of relativistic particle dynamics to one-particle systems, a most atypical case.
-
(1960)
Encyclopedia of Physics
, vol.3
, Issue.1 PART
, pp. 105
-
-
Synge, J.L.1
-
10
-
-
0003437218
-
-
i and t are functions. It is then possible to find an appropriate Lagrangian for the system. From this Lagrangian the momentum conjugate to t may be calculated and it turns out to be - H. This would then be a ground for considering t and -H as forming a fourth canonical pair. However, the next step, the inversion of the Lagrangian to obtain the generalized velocities as functions of the generalized coordinates and momenta, turns out to be impossible, that is, the equations of motion cannot be written in the usual Hamiltonian form
-
i and t are functions. It is then possible to find an appropriate Lagrangian for the system. From this Lagrangian the momentum conjugate to t may be calculated and it turns out to be - H. This would then be a ground for considering t and -H as forming a fourth canonical pair. However, the next step, the inversion of the Lagrangian to obtain the generalized velocities as functions of the generalized coordinates and momenta, turns out to be impossible, that is, the equations of motion cannot be written in the usual Hamiltonian form.
-
(1980)
Classical Mechanics
-
-
Goldstein, H.1
-
12
-
-
0343188122
-
Ueber die Jacobischen transformationen der quantenmechanik
-
F. London, "Ueber die Jacobischen Transformationen der Quantenmechanik," Z. Phys. 37, 915 (1926).
-
(1926)
Z. Phys.
, vol.37
, pp. 915
-
-
London, F.1
-
13
-
-
85033758104
-
-
Pauli has already remarked that if the spectrum of t is the whole real axis and t and H satisfy the commutation relation in (1), then the spectrum of H cannot contain discrete eigenvalues. In fact, the restrictions following from H≥0 are even more severe
-
Pauli has already remarked that if the spectrum of t is the whole real axis and t and H satisfy the commutation relation in (1), then the spectrum of H cannot contain discrete eigenvalues. In fact, the restrictions following from H≥0 are even more severe.
-
-
-
-
14
-
-
0004082161
-
-
Prentice-Hall, Englewood Cliffs, NJ, Chap. 3
-
See Ref. 5, Sec. 25. For a modern treatment: L. E. Ballentine, Quantum Mechanics (Prentice-Hall, Englewood Cliffs, NJ, 1990), Chap. 3.
-
(1990)
Quantum Mechanics
-
-
Ballentine, L.E.1
-
15
-
-
21144468595
-
The rate of evolution of a quantum state
-
J. Uffink, "The rate of evolution of a quantum state," Am. J. Phys. 61, 935-936 (1993).
-
(1993)
Am. J. Phys.
, vol.61
, pp. 935-936
-
-
Uffink, J.1
-
16
-
-
0002048908
-
A new view on the uncertainty principle
-
edited by A. I. Miller Plenum, New York
-
J. Hilgevoord and J. Uffink, "A new view on the uncertainty principle," in Sixty-Two Years of Uncertainty, Historical and Physical Inquiries into the Foundations of Quantum Mechanics, edited by A. I. Miller (Plenum, New York, 1990), pp. 121-139.
-
(1990)
Sixty-two Years of Uncertainty, Historical and Physical Inquiries into the Foundations of Quantum Mechanics
, pp. 121-139
-
-
Hilgevoord, J.1
Uffink, J.2
-
17
-
-
0040063076
-
Uncertainty in prediction and in inference
-
J. Hilgevoord and J. Uffink, "Uncertainty in prediction and in inference," Found. Phys. 21, 323-341 (1991).
-
(1991)
Found. Phys.
, vol.21
, pp. 323-341
-
-
Hilgevoord, J.1
Uffink, J.2
-
18
-
-
0002376722
-
The mathematical expression of the uncertainty principle
-
edited by A. van der Merwe, F. Selleri, and G. Tarozzi Kluwer, Dordrecht
-
J. Hilgevoord and J. Uffink, "The mathematical expression of the uncertainty principle," in Microphysical Reality and Quantum Formalism, edited by A. van der Merwe, F. Selleri, and G. Tarozzi (Kluwer, Dordrecht, 1988), pp. 91-114.
-
(1988)
Microphysical Reality and Quantum Formalism
, pp. 91-114
-
-
Hilgevoord, J.1
Uffink, J.2
-
19
-
-
0003580854
-
-
Pergamon, Oxford, 2nd ed., Sec. 44
-
L. D. Landau and E. M. Lifshitz, Quantum Mechanics, Volume 3 of Course of Theoretical Physics (Pergamon, Oxford, 1975), 2nd ed., Sec. 44.
-
(1975)
Quantum Mechanics, Volume 3 of Course of Theoretical Physics
, vol.3
-
-
Landau, L.D.1
Lifshitz, E.M.2
-
20
-
-
0001134465
-
The uncertainty relation between energy and time in nonrelativistic quantum mechanics
-
L. Mandelstam and I. Tamm, "The uncertainty relation between energy and time in nonrelativistic quantum mechanics," J. Phys. (USSR) 9, 249-254 (1945).
-
(1945)
J. Phys. (USSR)
, vol.9
, pp. 249-254
-
-
Mandelstam, L.1
Tamm, I.2
-
21
-
-
0008333857
-
On the energy-time uncertainty relation
-
P. Busch, "On the energy-time uncertainty relation," Part I and II, Found. Phys. 20, 1-43 (1990).
-
(1990)
Found. Phys.
, vol.20
, Issue.1-2 PART
, pp. 1-43
-
-
Busch, P.1
|