TY - JOUR
T1 - Two-slit diffraction with highly charged particles
T2 - Niels Bohr's consistency argument that the electromagnetic field must be quantized
AU - Baym, Gordon
AU - Ozawa, Tomoki
PY - 2009/3/3
Y1 - 2009/3/3
N2 - We analyze Niels Bohr's proposed two-slit interference experiment with highly charged particles which argues that the consistency of elementary quantum mechanics requires that the electromagnetic field must be quantized. In the experiment a particle's path through the slits is determined by measuring the Coulomb field that it produces at large distances; under these conditions the interference pattern must be suppressed. The key is that, as the particle's trajectory is bent in diffraction by the slits, it must radiate and the radiation must carry away phase information. Thus, the radiation field must be a quantized dynamical degree of freedom. However, if one similarly tries to determine the path of a massive particle through an inferometer by measuring the Newtonian gravitational potential the particle produces, the interference pattern would have to be finer than the Planck length and thus indiscernible. Unlike for the electromagnetic field, Bohr's argument does not imply that the gravitational field must be quantized.
AB - We analyze Niels Bohr's proposed two-slit interference experiment with highly charged particles which argues that the consistency of elementary quantum mechanics requires that the electromagnetic field must be quantized. In the experiment a particle's path through the slits is determined by measuring the Coulomb field that it produces at large distances; under these conditions the interference pattern must be suppressed. The key is that, as the particle's trajectory is bent in diffraction by the slits, it must radiate and the radiation must carry away phase information. Thus, the radiation field must be a quantized dynamical degree of freedom. However, if one similarly tries to determine the path of a massive particle through an inferometer by measuring the Newtonian gravitational potential the particle produces, the interference pattern would have to be finer than the Planck length and thus indiscernible. Unlike for the electromagnetic field, Bohr's argument does not imply that the gravitational field must be quantized.
KW - Electromagnetism
KW - Gravitation
KW - Interferometry
KW - Quantum theory
UR - http://www.scopus.com/inward/record.url?scp=62549154017&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=62549154017&partnerID=8YFLogxK
U2 - 10.1073/pnas.0813239106
DO - 10.1073/pnas.0813239106
M3 - Article
AN - SCOPUS:62549154017
SN - 0027-8424
VL - 106
SP - 3035
EP - 3040
JO - Proceedings of the National Academy of Sciences of the United States of America
JF - Proceedings of the National Academy of Sciences of the United States of America
IS - 9
ER -