III. BOHM: The Whole and the Implicate Order A. Bohm's Life. Understanding David Bohm's life will help us understand his philosophy. Bohm studied under Oppenheimer and completed his doctorate in 1943. Bohm taught at Princeton, where he wrote a book on quantum theory in 1951. The work is still considered one of the best treatments of the topic. At Princeton Bohm had a series of discussions with Einstein, who was opposed to what was to become the standard dual-property, non-deterministic interpretation of quantum physics. "God does not play dice with the universe," Einstein said. These conversations led Bohm to develop a new interpretation of quantum mechanics, one more consistent with determinism. Bohm resurrected some suggestions made by deBroglie, who had developed a "hidden variables" model in 1927, and in 1952, Bohm published his own model. During the McCarthy era, Bohm was called to testify before congress against Oppenheimer. Bohm refused, and though he was brought to trial and acquitted of contempt of congress, he was fired by Princeton and spent the rest of his life as an expatriate. In 1961 Bohm met Krishnamurti, whose spiritual agenda and unique brand of materialism influenced Bohm for the rest of his life. B. Bohm's Critical Approach to the Physical Sciences. Though his thought is revolutionary, Bohm's analytical method is conservative. He accepts axioms that have served the physical sciences since the time of Gallileo: (1) new empirical evidence should be treated with skepticism; (2) no new entities should be postulated as explanatory constructs unless necessary; (3) the ontology presupposed by the physical sciences should be changed only as a last resort. As is well known, quantum mechanics and relativity theory did force a change in the physical sciences that impacted each of these axioms. Initially skeptics ruled the day when the experimental evidence for these theories was presented. Lorentz, for example, rejected the idea that the Michelson-Morley experiment actually demonstrated the absence of the ether in the universe. Lorentz's interpretation was consistent with the experimental data and kept the ontology of physics, which included the ether, static. Likewise, quantum physics challenged both the perfect predictability of physical phenomena and the existence of descrete entities with clearly defined properties. The most widely-accepted resolution to the challenges of quantum mechanics, is that while the gross pheomena of nature remain statistically predicable, certain sub-atomic phenomena are unpredicable in their very nature and the entities responsible for these changes have a dual nature: in certain circumstances they behave as particles, and in others as waves. The ontology of physics is now generally understood to include these ambiguous entities. Bohm argued that this revolution in the physical sciences brought about by quantum mechanics was inconsistent. On the one hand, physics had, since Galileo and Newton, been historically committed to ontological foundationalism: the belief that there was a "bottom" to the physical sciences and that this foundation would not only be discoverable, but would also be firmly based on the pure determinism of mechanism and fully describable in terms of fundamental entities whose qualitative transformations would be fully predictable by inflexible laws of nature. Foundationalism in physics, as Bohm put it, was committed to the belief that there is a finite set of laws that "permit an exhaustive treatment of the whole of nature" (Bohm, 1957, p. 134). One the other hand, physics was now claiming to have discovered the bottom, in the form of quantum mechanics, but at the same time it claimed that the ultimate principles governing the fundamental entities were not fully predictable, but depended on chance. In his 1957 book Causality and Chance, Bohm listed five criticisms of contemporary physics (see Bohm, 1957, pp. 132-134). 1. If the prevailing interpretation of quantum physics were right, pure mechanism is wrong. 2. The belief is foundationalism is not necessary for physics. It is possible to have an evolutionary view of knowledge in the physical sciences. 3. Foundationalism does not reflect a scientific attitude. To accept any law as absolute and final closes the door to further inquiry. 4. Experiment shows that physical laws apply to a range of phenomena only. It is not possible to establish experiments that cover every possible condition. 5. Although new laws appear to converge on "the truth," we have no reason to expect that this will always happen. New conditions may introduce new laws and new physical qualities that are not expected. We have no reason, other than blind belief, to assume that there is a finite set of laws that "permit an exhaustive treatment of the whole of nature" (Bohm, 1957, p. 134). Bohm concluded, in my opinion correctly, that physicists should assume that the kinds of significant qualities in the universe is unlimited. The idea of the "qualitative infinity of nature" is both scientifically and philosophically sound. It opens the door to further research, urging us to continue to discover more complex structures in nature. At the same time, however, Bohm also realized that is was necessary to preserve, as far as possible, some of the useful, conservative impulses that have guided the history of physics. Bohm employed a mixture of pragmatism and instrumentalism. He argued that although a proper scientific attitude implied an infinity of possibilities, there is still a place for the notion of substances in nature: all things must have some "degree of autonomy and stability in their modes of being" (Bohm, 1957, p. 139). This is necessary (a) in order to allow things to preserve their identity for some time; and (b) in order for things to be distinguished from other things. After all, if "things" do not "exist," it will be impossible to formulate laws that describe their qualitative transformations under a range of experimental conditions. These experimental conditions establish simultaneously not only a set of substances and their properties but also a set of background conditions that allow the properties to be described. That is to say, experimental conditions only capture an aspect of a system. But because there is, potentially, an infinite number of aspects to the whole of nature,no system of determinate law can ever attain perfect validity. For every such system works with only a finite number of things (Bohm, 1957, p. 141). This system Bohm later called the Whole. It alone was ultimately real. Experimental conditions, then, capture only a part of the Whole, and it is a always matter of interpretation to decide which elements in an experimental condition are due to the characteristics substances, and which are due some other aspect of the Whole that is not captured by the experiment. When it comes to interpreting which aspects of experiments were due to chance and which were due to laws, Bohm argued that we cannot always be sure. Might it not be that "chance" is simply used as an "explanation" to cover over what is due to some undiscovered law that operates at a deeper level of the Whole? Since we may presume that the Whole has an infinite number of aspects, it is incumbent upon us to consider such a possibility. With these guidelines, Bohm sought to provide an interpretation of quantum mechanics that he felt was both consistent with the history of physics (conservative) and his idea of the Whole. Before turning to Bohm's quantum interpretation, it may be instructive to consider how Bohm's style of thinking might be applied to a more familiar case. (Be it noted, physicists may have a difficult time accepting this analogy, finding it factually flawed; but that is irrelevant to the point of the analogy.) C. The "Baseball" Analogy. Consider the path followed by a baseball when thrown from the pitcher's mound to the catcher. As everyone knows, the path followed by this baseball, all other things being equal (such as air resistance, spin on the ball, and so on) is precisely determined by the law of gravity. The path of a thrown baseball is represented below. P ----> X X X X C ^Catcher catches ball here. Assume that scientists have investigated this phenomenon many times, and that the law is verified each time and the predictions are always fulfilled. Now let us suppose that we one day discover that although our predictions are always fulfilled, if we measure more precisely we discover that the ball is in fact oscillating, in a somewhat random manner, during its flight. The actual path, with all the positions filled in, is more like that shown below. X P ----> X X X X X X X X X X X X C ^Catcher catches ball here. There is one way to easily explain this phenomenon. As a statistical generalization, the average path of the ball still remains the same. The "law" of gravity, as a predicting tool, is not invalidated. We do have, apparently, another, NEW phenomenon that operates within the parameters of the "law" of gravity. At present, the source of these random variations is unexplained. One might now object, anticipating our conclusion, that this is not at all what happens in quantum physics. At this point, it does not matter. We are only concerned with establishing that a "law" of motion may turn out to be a statistical average caused by the influence of TWO factors: 1. a field of force, and 2. random variations of an object moving within that field of force. Let us change our thought experiment to more closely approximate the situation in quantum mechanics. Suppose we are now using what, for all practical purposes, seems to be a very "baseball-like" object in similar experiments. But we soon discover that now the Catcher, UNDER CERTAIN CONDITIONS, actually is found to catch the ball in different spots, even though it is pitched the same each time. Sometimes he catches it higher than expected, sometimes lower. X P ----> X X X X X X X X X X X < Catcher sometimes catches ball here X X