-
1
-
-
85038309302
-
-
H.A. Lorentz, Theory of Electrons (Dover, New York, 1952).
-
H.A. Lorentz, Theory of Electrons (Dover, New York, 1952).
-
-
-
-
3
-
-
85038286914
-
-
J.D. Jackson, Classical Electrodynamics (Wiley, New York, 1975).
-
J.D. Jackson, Classical Electrodynamics (Wiley, New York, 1975).
-
-
-
-
4
-
-
85038341681
-
-
F. Rohrlich, Classical Charged Particles (Addison-Wesley, Redwood City, CA, 1990).
-
F. Rohrlich, Classical Charged Particles (Addison-Wesley, Redwood City, CA, 1990).
-
-
-
-
7
-
-
85038309279
-
-
A.D. Yaghjian, Relativistic Dynamics of a Charged Sphere (Springer, Berlin, 1992).
-
A.D. Yaghjian, Relativistic Dynamics of a Charged Sphere (Springer, Berlin, 1992).
-
-
-
-
8
-
-
85038301454
-
-
L.D. Landau and E.M. Lifshitz, The Classical Theory of Fields (Pergamon, Oxford, 1962).
-
L.D. Landau and E.M. Lifshitz, The Classical Theory of Fields (Pergamon, Oxford, 1962).
-
-
-
-
10
-
-
85038290900
-
-
gr-qc/9912045
-
E. Poisson, “An introduction to the Lorentz-Dirac equation,” gr-qc/9912045.
-
-
-
Poisson, E.1
-
15
-
-
85038297070
-
-
C. Itzykson and J.-B. Zuber, Quantum Field Theory (McGraw-Hill, New York, 1980).
-
C. Itzykson and J.-B. Zuber, Quantum Field Theory (McGraw-Hill, New York, 1980).
-
-
-
-
16
-
-
85038347274
-
-
hep-th/9805083
-
B.L. Julia, “Dualities in the classical supergravity limits: Dualisations, dualities and a detour via 4k+2 dimensions,” in Cargèse 1997, Strings, branes and dualities, pp. 121–139, LPTENS-98-07, hep-th/9805083.
-
-
-
Julia, B.L.1
-
17
-
-
85038266040
-
-
quant-ph/9812036
-
A. Higuchi, “Radiation reaction in quantum mechanics,” quant-ph/9812036.
-
-
-
Higuchi, A.1
-
18
-
-
85038282772
-
-
M. Abraham, Theorie der Elektrizität (Springer, Leipzig, 1905), Vol. II.
-
M. Abraham, Theorie der Elektrizität (Springer, Leipzig, 1905), Vol. II.
-
-
-
-
19
-
-
85038284867
-
-
L.I. Schiff, Quantum Mechanics (McGraw-Hill, New York, 1968).
-
L.I. Schiff, Quantum Mechanics (McGraw-Hill, New York, 1968).
-
-
-
-
21
-
-
85038323714
-
-
A.S. Davydov, Quantum Mechanics (Pergamon, Oxford, 1965).
-
A.S. Davydov, Quantum Mechanics (Pergamon, Oxford, 1965).
-
-
-
-
22
-
-
85038292355
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The corresponding correction to the forward-scattering amplitude is of order (Formula presented) Since the imaginary part of (Formula presented) is of order (Formula presented) the correction to the potential does not have an imaginary part at leading order in (Formula presented)
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The corresponding correction to the forward-scattering amplitude is of order (Formula presented) Since the imaginary part of (Formula presented) is of order (Formula presented) the correction to the potential does not have an imaginary part at leading order in (Formula presented)
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23
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85038284884
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The wave packet (68) is narrowest at (Formula presented) when the position is measured. One can make this wave packet more general so that the case considered here, which is more realistic, is included by changing the factor (Formula presented) to (Formula presented) with (Formula presented) The position shift will be unchanged with this modification.
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The wave packet (68) is narrowest at (Formula presented) when the position is measured. One can make this wave packet more general so that the case considered here, which is more realistic, is included by changing the factor (Formula presented) to (Formula presented) with (Formula presented) The position shift will be unchanged with this modification.
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24
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85038319050
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Since the second term in Eq. (17) is the lowest-order term in (Formula presented) that grows linearly in (Formula presented) the fact that it is much larger than the first term, which is of lower order in (Formula presented) does not imply that our approximation breaks down since the latter is independent of (Formula presented)
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Since the second term in Eq. (17) is the lowest-order term in (Formula presented) that grows linearly in (Formula presented) the fact that it is much larger than the first term, which is of lower order in (Formula presented) does not imply that our approximation breaks down since the latter is independent of (Formula presented)
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