"Introduction: John Bell and the second quantum revolution" (2004)
“The solution of the measurement problem is twofold. First, any observation or measurement requires a macroscopic measuring apparatus. A macroscopic object is also governed by quantum mechanics, but has a large number of constituents, so that each macroscopic state is a combination of an enormous number of quantum mechanical eigenstates. As a consequence the quantum mechanical interference terms between two macroscopic states virtually cancel and only probabilities survive. That is the explanation why our familiar macroscopic physics, concerned with billiard balls, deals with probabilities rather than probability amplitudes.”
The Scandal of Quantum Mechanics (2008)
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Nico van Kampen 3
Dutch theoretical physicist 1921–2013Related quotes
Principles of Modern Chemistry (7th ed., 2012), Ch. 4 : Introduction to Quantum Mechanics
On the problem of hidden variables in quantum mechanics (1966)
Ravi Gomatam's paper "How do Classical and Quantum Probabilities Differ?" http://www.bvinst.edu/gomatam1/pub-2011-01.pdf, delivered at the conference on Foundations of Probabilities and Physics - 6 (FPP-6), Vaxjo, Sweden, June 13-17, 2011.
Book Reviews, REVIEWER: JAKUB PALIDER, NANOSCALE COMMUNICATION NETWORKS STEPHEN F. BUSH, ARTECH HOUSE, 2010, ISBN-13: 978-1-60807-003-9, HARDCOVER, 308 PAGES, IEEE Communications Magazine, August 2011.
Source: The Emperor's New Mind (1989), Ch. 6, Quantum Magic and Quantum Mastery, p. 269.
Context: It seems to me that we must make a distinction between what is "objective" and what is "measurable" in discussing the question of physical reality, according to quantum mechanics. The state-vector of a system is, indeed, not measurable, in the sense that one cannot ascertain, by experiments performed on the system, precisely (up to proportionality) what the state is; but the state-vector does seem to be (again up to proportionality) a completely objective property of the system, being completely characterized by the results it must give to experiments that one might perform.
W. E. Lamb, Super classical quantum mechanics: the best interpretation of non relativistic quantum mechanics, Am. J. Phys. 69, 413-422 (2001).