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#quantummechanics

3 posts2 participants2 posts today

For anyone in the Fediverse who might be interested in #philosophy of #physics, I’m excited to share this #workshop I’ve been organising with some friends, on metaphysical and epistemological problems in #quantummechanics. Some very cool speakers will join us for interesting discussions, on the 28th of June at #usi in #lugano

usi.ch/en/feeds/31385

www.usi.chRatio Workshop: Metaphysical and Epistemological Perspectives on Quantum TheoryDate and time: Saturday, June 28th. From 9:30am to 5pm.   The Workshop “Metaphysical and Epistemological Perspectives on Quantum Theory” will focus on philosophical questions arising within fundamental physical theories, especially quantum mechanics. The workshop will host international speakers, fostering discussion with the local research community on key issues in the foundations of physics.   Location: Room A-23, Red Building.   Tim Maudlin (New York University) Title: Ontology and Epistemology in Quantum Context Abstract: A physical theory only acquires empirical content if its claims can be directly tested against observational data. But, as John Bell emphasized in “The Theory of Local Beables”, observational data is always (and seemingly must always be) reported in terms of what he called “local beables”: the shape, constitution, and motion of localized macroscopic objects in space-time. Therefore, the only obvious way for a physical theory to acquire empirical content is to postulate that there are such localized macroscopic objects. And the only way we have ever been able to account for localized macroscopic objects in physics is by postulating that they are composed of localized microscopic objects. But “plain vanilla” quantum theory, as presented in textbooks, not only does not postulate just things, it largely seems to positively deny there are such things. That leads at least an epistemic puzzle, if not an epistemic catastrophe. I will consider some of the ways out of the catastrophe.   Valia Allori (University of Bergamo) Title: Why is there no consensus on the foundations of quantum mechanics? Abstract: Quantum mechanics is regarded by many as problematic for the scientific realist (among other things) because it looks like the prototypical example of underdetermination of theory by data: there are so many quantum theories which are (effectively) empirically equivalent, so how could the realist choose which one to believe? In this paper, I argue that the disagreement about theory choice in the quantum domain can be tracked down to specific features a fundamental physical theory should have in order to be satisfactory. People disagree about these desiderata because they disagree about which explanatory schema one should look for in a theory. This is, I argue, what leads different people to favor different theories. First, I show that the proponents of the information-theoretic approach, since they focus on empirical adequacy, are naturally led to look for an explanation in terms of principles, which is provided by standard quantum theory. In contrast, primitive ontologists favor a constructive understanding, which requires a spatiotemporal microscopic fundamental ontology, which guides them towards favoring the pilot-wave theory. Instead, Everettian approaches, which center around physical practice, conceive of quantum theory as a framework, and this makes them prefer the many-worlds theory. Finally, I argue that the wave function realists’ requirement of a local and separable ontology leads them to think of quantum theories as interaction theories, which describe how the fundamental ontology, provided by the non-spatiotemporal wavefunction, behaves. Thus, if this reconstruction is correct, it is unlikely that the realist community will find an agreement on which is the best quantum theory.    Lorenzo Lorenzetti (USI) Title: Quantum Physics and Effective Realism Abstract: Three accounts of effective realism (ER) have been advanced to solve three problems for scientific realism: Fraser and Vickers develop a version of ER about non-relativistic quantum mechanics that they argue is compatible with all the main realist versions (‘interpretations’) of quantum mechanics avoiding the problem of underdetermination among them; Williams and Fraser propose ER about quantum field theory as a response to the problems facing realist interpretations; Robertson and Wilson propose ER to deal with the dubious ontological status of the entities belonging to superseded theories. We argue for the unification of these proposals based on realism about modal structure and the idea of scale relativity of ontology developed by ontic structural realists. This solves problems some or all the accounts of ER face, especially that of making explicit in what way they are realist. In this talk we focus in particular on how the ontic structural realist approach to effective realism can be helpful in the context of quantum physics. (based on joint work with James Ladyman)   Mario Hubert (Ludwig-Maximilians-University Munich) Title: The Multi-Time Multi-Field Abstract: According to the multi-field interpretation, the quantum mechanical wave-function exists as a physical field in three-dimensional space. Unlike a classical field that assigns values to each point in three-dimensional space, a multi-field assigns values to ordered collections of spatial points. This interpretation has been developed specifically for non-relativistic quantum mechanics, particularly within the non-relativistic de Broglie–Bohm theory (Hubert and Romano, 2018). It offers an alternative to both wave-function realism (Ney, 2021) and the nomological interpretation (Goldstein and Zanghì, 2013), allowing the wave-function to exist as a physical object in the same physical space as particles, similar to the electromagnetic field in classical electromagnetism.  I propose to generalize the multi-field concept further into a multi-time multi-field. While a standard multi-field assigns values to ordered collections of spatial points at the same time, a multi-time multi-field assigns values to ordered collections of events in four-dimensional space, where these events need not occur simultaneously and where the space-time structure may not even provide a unique objective time. In the relativistic context, multi-time wave-functions have been developed (Lienert et al., 2020). Following a physical analysis of how multi-time wave-functions work in a relativistic many-worlds theory and relativistic de Broglie–Bohm theory, I will present arguments for interpreting these multi-time wave-functions as multi-time multi-fields.   Cristian Mariani (USI) TBC   For any queries: associazione.ratio@usi.ch Organisers: Ratio.

#OTD in 1914.

The Franck–Hertz experiment, the first electrical measurement to clearly demonstrate the quantum nature of atoms, was presented to the German Physical Society.

Their experimental results proved to be consistent with the Bohr model for atoms that had been proposed the previous year by Niels Bohr.

en.wikipedia.org/wiki/Franck%E

Niels Bohr at PG:
gutenberg.org/ebooks/author/44

Many-worlds without necessarily many worlds?

IAI has a brief interview of David Deutsch on his advocacy for the many-worlds interpretation of quantum mechanics. (Warning: possible paywall.) Deutsch has a history of showing little patience with other interpretations, and this interview is no different. A lot of the discussion centers around his advocacy for scientific realism, the idea that science is actually telling us about the world, rather than just providing instrumental prediction frameworks.

Quick reminder. The central mystery of quantum mechanics is that quantum systems seem to evolve as waves, superpositions of many states, with the different states interfering with each other, all tracked by a mathematical model called the wave function. But when measured, these systems behave as localized particles, with the model only able to provide probabilities on the measurement result. Although the measurement results as a population show the interference patterns from the wave function. This is often called the “wave function collapse”.

Various interpretations attempt to make sense of this situation. Many deny the reality of what the wave function models. Others accept it, but posit the wave function collapse as a real objective event. Some posit both a wave and particle existing throughout. The Everett approach rejects wave function collapse and argues that if we just keep following the mathematical model, we get decoherence and eventually the same observations. But that implies that quantum physics apply at all scales, meaning that it’s not just particles in superpositions of many states, but measuring equipment, labs, people, planets, and the entire universe.

Reading Deutsch’s interview, it occurred to me that my own structural realist outlook, a more cautious take on scientific realism, is reflected in the more cautious acceptance I have of Everettian quantum mechanics. People like Deutsch are pretty confident that there is a quantum multiverse. I can see the reasoning steps that get them there, and I follow them, to a point. But my own view is that the other worlds remains a possibility, but far from a certainty.

I think this is because we can break apart the Everettian proposition into three questions.

  1. Does the mathematical structure of quantum theory provide everything necessary to fit the current data?
  2. If so, can we be confident that there won’t be new data in the future that drives theorists to make revisions or add additional variables?
  3. What effect would any additions or changes have on the broader predictions of the current bare theory?

My answer to 1 is yes, with a moderately high credence, maybe around 80%. I know people like Deutsch and Sean Carroll have this much higher. (I think Carroll says his is around 95% somewhere on his podcast.) And I think they have defendable reasons for it. Experimentalists have been stress testing bare quantum theory for decades, with no sign of a physical wave function collapse, or additional (hidden) variables. Quantum computing seems to have taken it to a new level.

But there remain doubts, notably about how to explain probabilities. I personally don’t see this as that big an issue. The probabilities reflect the proportion of outcomes in the wave function. But I acknowledge that lot of physicists do. I’m not a physicist, and very aware of the limitations of my very basic understanding of the math, so it’s entirely possible I’m missing something, which is why I’m only at 80%.

(Often when I make the point about the mathematical structures, it’s noted that there are multiple mathematical formalisms: wave mechanics, matrices, path integrals, etc. But while these are distinct mental frameworks, they reportedly always reconcile. These theories are equivalent, not just empirically, but mathematically. They always provide the same answer. If they didn’t, we’d see experimental physicists trying to test where they diverge. We don’t because there aren’t any divergences.)

If our answer to 1 is yes, it’s tempting to jump from that to the broader implications, the quantum multiverse. (Or one universe with a much larger ontology. Some people find that a less objectionable description.)

But then there are questions 2 and 3. I have to say no to 2. The history of science seems to show that any claims that we’ve found the final theory of anything is a dubious proposition, a point Deutsch acknowledges in the interview. All scientific theories are provisional. And we don’t know what we don’t know. And there are the gaps we do know about, such as how to bring gravity into the quantum paradigm. It seems rational to wonder what kind of revisions they may eventually require.

Of course 3 is difficult to answer until we get there. I do doubt any new discoveries would drive things toward the other interpretations people currently talk about, or overall be less bonkers than the current predictions. Again given the history of science, it seems more likely it would replace the other worlds with something even stranger and more disconcerting.

So as things stand, there’s no current evidence for adding anything to the structure of raw quantum theory. That does imply other worlds, but the worlds remain untestable for the foreseeable future.

To be clear, I don’t buy that they’re forever untestable. We can’t rule out that some clever experimentalist in the future won’t find a way to detect interference between decohered branches, to recohere them (which has been done but only very early in the process), or some other way we haven’t imagined yet.

My take is the untestability of the other worlds means that Everettian quantum mechanics, in the sense of pure wave mechanics, shouldn’t be accepted because we like the worlds, or rejected because we dislike them. For now, the worlds should be irrelevant for a scientific assessment. The only question is whether anything needs to be added to the bare theory, a question, it should be noted, we can ask regardless of whether we’re being realist or antirealist about any of this.

All of which means that while my credence in austere quantum mechanics is 80%, the credence for the other worlds vacillates somewhere around 50%. In other words I’m agnostic. This resonates with the views I’ve seen from a number of physicists, such as Stephen Hawking, Sidney Coleman, John Preskill, and most recently, Brian Cox, which accept the Everett view but downplay the other worlds. Even Sean Carroll notes in one of his AMAs that he doesn’t really care so much about the other worlds, but the physics at the core of the theory.

But maybe I’m missing something. Are the questions I raised above as easy to separate as I’m thinking? Or are there problems with pure wave mechanics I’m overlooking?

Continued thread

a jumble of Feynman diagrams and coloured shapes with a Bauhaus feel.

#linocut #printmaking #physics #Bauhaus #quantumMechanics #FeynmanDiagram #penguinDiagram #particlePhysics #sciart #WorldQuantumDay

*I am somewhat dubious of this date because a) I was trained to use the metric convention day/month/year and b) physicists use the reduced constant h-bar (that’s h divided by 2 pi) and then, cause it’s easier they just change units such that h-bar = 1 but it’s as good an excuse as any

🧵3/3