Steven Weinberg (1933) American theoretical physicist
Source: Lectures on Quantum Mechanics (2012, 2nd ed. 2015), Ch. 3: General Principles of Quantum Mechanics
Source: The End of Science (1996), p. 88
Steven Weinberg (1933) American theoretical physicist
Source: Lectures on Quantum Mechanics (2012, 2nd ed. 2015), Ch. 3: General Principles of Quantum Mechanics
“The most efficient and practical interpretation of quantum mechanics is… no interpretation at all.”
F. J. Duarte (1954) Chilean-American physicist
in [Quantum Optics for Engineers, CRC, New York, 2013, 978-1439888537, F. J. Duarte]
David Pearce (philosopher) (1959) British transhumanist
Dave's Diary https://www.hedweb.com/davdiary.htm, BLTC Research, May 1996
Steven Weinberg (1933) American theoretical physicist
"Testing Quantum Mechanics" http://www.sciencedirect.com/science/article/pii/0003491689902765, Annals of Physics (1989)
Steven Weinberg (1933) American theoretical physicist
Steven Weinberg, in " Science’s Path From Myth to Multiverse https://www.quantamagazine.org/20150317-sciences-path-from-myth-to-multiverse/" by Dan Falk (March 17, 2015)
Victor J. Stenger (1935–2014) American philosopher
In God and the Folly of Faith: The Incompatibility of Science and Religion (2012)
Gerardus 't Hooft (1946) Dutch theoretical physicist and Nobel Prize winner
Context: The usual no-go theorems telling us that hidden variables are irreconcilable with locality, appear to start with fairly conventional pictures of particle systems, detectors, space and time. Usually, it is taken for granted that events at one place in the universe can be described independently from what happens elsewhere. Perhaps one has to search for descriptions where the situation is more complex. Maybe, it needs not be half as complex as superstring theory itself. The conventional Copenhagen interpretation of quantum mechanics suffices to answer all practical questions concerning conventional experiments with quantum mechanics, and the outcome of experiments such as that of Aspect et al can be precisely predicted by conventional quantum mechanics. This is used by some to state that no additional interpretation prescriptions for quantum mechanics are necessary. Yet we insist that the axioms for any "complete" quantum theory for the entire cosmos would present us with as yet unresolved paradoxes.<br><br> Obstacles on the Way toward the Quantization of Space, Time and Matter — and possible resolutions — http://www.staff.science.uu.nl/~hooft101/gthpub/foundations.pdf
Sidney Coleman (1937–2007) American physicist
Quantum Mechanics in Your Face http://www.physics.harvard.edu/about/video.html, a lecture given by Sidney Coleman at the New England sectional meeting of the American Physical Society (Apr. 9, 1994)
Erwin Schrödinger (1887–1961) Austrian physicist
italics in the original
DISCUSSION OF PROBABILITY RELATIONS BETWEEN SEPARATED SYSTEMS (1935)
Hugh Everett (1930–1982) American physicist, author of the many-worlds interpretation of quantum mechanics
http://space.mit.edu/home/tegmark/everett/.