| Literature DB >> 26640454 |
Zheng Wang1, Jerome Busemeyer2.
Abstract
Central to quantum theory is the concept of complementarity. In this essay, we argue that complementarity is also central to the emerging field of quantum cognition. We review the concept, its historical roots in psychology, and its development in quantum physics and offer examples of how it can be used to understand human cognition. The concept of complementarity provides a valuable and fresh perspective for organizing human cognitive phenomena and for understanding the nature of measurements in psychology. In turn, psychology can provide valuable new evidence and theoretical ideas to enrich this important scientific concept.Entities:
Keywords: Niels Bohr; William James; commutativity; compatibility; complementarity; order effects; quantum cognition; quantum probability
Year: 2015 PMID: 26640454 PMCID: PMC4661229 DOI: 10.3389/fpsyg.2015.01822
Source DB: PubMed Journal: Front Psychol ISSN: 1664-1078
FIGURE 1Sets representation of events. Classical probability theory has difficulty explaining order effects because events are represented as sets and are commutative, so the joint probability of events A and B is the same for the order of “A and B” and the order of “B and A.”
FIGURE 2A “toy” example of quantum probability model of sequential judgments. (A) Illustrates how quantum model provides a natural account for question order effects of the Clinton-Gore example in terms of incompatibility (Wang and Busemeyer, 2013; Wang et al., 2014). First, consider the probability of a person’s answering “yes” to both questions when Clinton is judged first. This is obtained by first projecting (following the black dotted lines) the magenta-colored state S to the blue Cy (“yes” to Clinton) axis and then projecting the result up to the red Gy (“yes” to Gore) axis, which produces a small probability (as illustrated by the short length of the black projection on the Gy axis). Next, consider the probability of a person’s answering “yes” to both questions when Gore is judged first. This is obtained by first projecting (following the green dash-dotted lines) the state S down to the red Gy (“yes” to Gore) axis and then projecting the result to the blue Cy (“yes” to Clinton) axis, which produces a much higher probability. In addition, note that the probability of saying “yes” to Gore in this Gore-Clinton order is much higher than it is in the Clinton-Gore order (as illustrated by the long length of the green projection on the Gy axis), producing the order effect for the Gore question when the question is asked before, as opposed to after, the Clinton question. (B) Illustrates similar order effects, but the order effects are much smaller because the basis vectors (i.e., the red and blue axes), which form the subspace for evaluating the Gore and Clinton questions, are more aligned with each other. This means that the rotation required to change from one evaluation basis (e.g., the blue Clinton axes) to the other (e.g., the red Gore axes) is smaller. In a sense, in psychology we could understand this as “reduced incompatibility” of the two questions, or the two sets of projectors as “more nearly commutative,” although in quantum physics, the original concept of complementarity does not have the notion of degrees of complementarity (events can be differentiated only by being complementary or not).