Interview with Astrophysicist Adam Becker
Adam Becker is an astrophysicist and science writer whose first book “What Is Real?: The Unfinished Quest for the Meaning of Quantum Physics” just hit the bookshelves!
Table of Contents
Give us some background on how you got interested in physics and some experiences in youth/school that were formative.
I don’t remember a time when I wasn’t interested in science—some of my earliest memories are of going to the American Museum of Natural History in Manhattan and staring at the dinosaurs. Like a lot of little kids, I was obsessed with dinosaurs, but when I was six years old, a switch flipped. By that time, I’d read most of the dinosaur books in my elementary school library, and the shelf with the space books was right next to the shelf with the dinosaur books, so I tried one of the ones about space, and that was it—dinosaurs were out and space was in. (Though I still think dinosaurs are pretty cool.) My parents and my first grade teacher were very supportive, and helped me find more things to read. (My first grade teacher also set me on the path to become a science communicator by having me do a presentation in front of her class about the solar system — I talked about this on a Story Collider podcast, which you can listen to here: https://www.storycollider.org/stories/2016/12/30/adam-becker-the-solar-system)
I read absolutely everything I could get my hands on about space (a book called From Quarks to Quasars made a big impression, as did Tyson’s Universe Down To Earth). As I learned more about space, I learned more about physics too, and my interests slowly shifted to physics more generally as I got a little older. I taped the old Timothy Ferris PBS special “The Creation of the Universe” and practically wore out the VHS tape from rewatching it so many times. I watched Carl Sagan’s Cosmos, of course, and read the book too; that introduced me to the idea of a history of science, science as a process, ideas that people pieced together over time, rather than a monolithic set of facts. Similarly, Kip Thorne’s excellent book Black Holes and Time Warps brought to life some of the personalities behind the great scientific discoveries of the 20th century. By the time I was in high school, I knew I wanted to do physics—and I wanted to know more about the people who did physics.
Tell us a bit about what readers will find in your new book “What is Real?“
What is Real? is about the unfinished quest for the meaning of quantum physics. We have this beautiful theory, quantum mechanics, and it’s astonishingly accurate. But it’s not at all clear what that theory is saying about the nature of the world around us. It must be saying something about that world—there must be something in nature that resembles the mathematics of quantum mechanics, otherwise why would the theory work so well? But there’s no clarity or consensus among physicists about what, exactly, quantum physics is saying about reality. This is very strange, especially given that quantum mechanics is over 90 years old.
Even worse than that, there’s a problem at the heart of quantum physics that doesn’t have a generally accepted answer: the measurement problem. The Schrödinger equation does a beautiful job of describing what wave functions do when nobody’s looking, but when we do look, suddenly the Schrödinger equation is suspended and we have to use the Born rule instead. Why? How does that work? And what counts as a “measurement” anyhow? “What exactly qualifies some physical systems to play the role of ‘measurer’?”, John Bell asked in 1989. “Was the wavefunction of the world waiting to jump for thousands of millions of years until a single-celled living creature appeared? Or did it have to wait a little longer, for some better qualified system…with a PhD? If the theory is to apply to anything but highly idealized laboratory operations, are we not obliged to admit that more or less ‘measurement-like’ processes are going on more or less all the time, more or less everywhere? Do we not have jumping then all the time?”
The closest thing we have to a consensus about any of this is the Copenhagen interpretation. But the Copenhagen interpretation isn’t really a single coherent set of ideas about quantum mechanics—it’s a family of mutually-contradictory ideas, none of which adequately solve the measurement problem or answer the other questions at the heart of quantum theory. This is all the more strange given that reasonable alternatives to Copenhagen have existed for decades.
What is Real? is the history behind all of this—the history of quantum foundations. How did we end up with the Copenhagen interpretation? Why were superior alternatives ignored for so long? Why is the Copenhagen interpretation less popular than it once was? My book picks up where other books on the history of quantum physics leaves off—it starts with the Bohr-Einstein debates and goes all the way to the present day. What Is Real? also busts a lot of historical myths along the way, such as the true nature of Einstein’s qualms about quantum physics (it had little to do with indeterminism and more to do with locality), the real meaning of Bell’s theorem (realism is irrelevant to the theorem, and Bell hated Copenhagen), and more.
I understand that this may be controversial and that not everyone will agree with me. That’s fine. I’m happy to debate people on this subject—if you’d like me to do that at your university, drop me a line.
What was the inspiration and goal for writing “What is Real?”
Back when I was first learning about physics in all those popular science books I read when I was a kid, I noticed that explanations always got annoyingly vague whenever quantum physics came up. I figured that this would make more sense when I actually learned quantum physics. Once I did learn quantum physics in college, I was surprised to find that the vagueness got worse, not better—it was maddeningly unclear what a measurement was, or what part of the world obeyed the Schrödinger equation at all. And when I asked questions about this, some professors just shrugged, while others were sarcastic and dismissive of my questions. One professor made his disdain for my questions very clear, telling me in a witheringly haughty tone of voice that “if that’s the kind of questions you’re interested in, why don’t you go to the Philosophy Department!” I knew he meant it as an insult, but I did go over to the Philosophy Department, and ended up doing a double major in philosophy and physics at Cornell. At Cornell, and later at Michigan (where I went for my PhD in physics), I found that the philosophers actually cared about these questions, and had been thinking about them for a good long while and had developed some good ideas and arguments that most of the physicists didn’t know about. I also met some physicists (like David Mermin at Cornell) who didn’t think questions about the meaning of quantum physics were silly at all.
As a physicist, it’s nice to be able to explain asymmetries. And this asymmetry I’d found was a doozy: the philosophers of physics were, in general, quite well informed about physics, but the physicists were, by and large, wholly ignorant of philosophy, despite the fact that they were making philosophical claims when they dismissed questions about quantum foundations. As a result, the physicists were generally relying upon faulty philosophy when they answered such questions. (For example, say you ask “hey, what’s the electron doing when we’re not looking?” and you get the answer “that’s unobservable in principle, and it’s meaningless to talk about unobservable things.” That answer is dependent on an outdated and erroneous philosophy of science called “logical positivism,” and the flaws in that kind of reasoning are very well known to philosophers of science.) Where did this asymmetry come from? The answer had to be the history of quantum foundations. So I started digging into this field as a side project while I was in graduate school, and what I found there was this totally astonishing story about the history of physics in the 20th century. The story wasn’t exactly hidden—it’s easy to find out what happened by piecing together various papers and books on the history of physics, and by reading what John Bell and others actually said—but it was scattered, and most physicists didn’t seem to know the story. And it was an interesting story, one that physicists, philosophers, and the scientifically-minded public might find compelling reading. Hence the book.
In “What is Real?“, how do you balance the technicality of physics with the required accessibility for the general public?
That balancing act is hard, and it’s the central struggle of all science writing. (I’m not totally sure I pulled it off successfully, though I hope I did.) When I was writing What Is Real?, I had two basic rules that I kept in mind to try to keep things accessible.
First, people generally care more about other people than they do about ideas. That doesn’t mean people don’t care about ideas! It just means that people will care more about ideas if you can tie those ideas to a person, and use the story of that person to explain the ideas. So when I was writing the book, I generally tried to use personal stories from the history of quantum foundations to explain ideas that were new to the reader. This was also the animating principle behind the structure of the book as a whole: it’s structured as a history, so I can talk about the people in the story as a way into explanations of the ideas that we grapple with in quantum foundations. And focusing on the people also makes it easier for me to quote those people, and good quotations have a way of bringing a story to life.
Second, only explain the new concepts and jargon that are absolutely essential for telling the story. For example, despite the fact that quantum wave functions live in configuration space (when using the position basis), I don’t introduce the concept of configuration space in my book. That’s not because I think the average reader couldn’t understand the idea; I’m confident that they could, given a clear explanation. But there are already many other unfamiliar concepts that I’m throwing at readers in this book (wave functions and their collapse, entanglement, the measurement problem, decoherence, etc.) and I didn’t want to burden them with one more, especially if it wasn’t truly essential for explaining other things.
Should schools be trying to teach every kid physics or should they instead divert resources into the few that might have the potential to contribute?
I think that this question is based on a faulty premise: we don’t teach kids physics because we think they’re all going to become physicists, any more than we teach kids history because we think everyone’s going to become a historian. Instead, we teach kids history because a knowledge of history is vital to being an informed citizen of a democracy, and makes it possible to have a deeper understanding of other people, other cultures, and current events. We teach kids physics for exactly the same reasons. A basic understanding of physics gives a new and important perspective on the world, one that students will hopefully carry with them for the rest of their lives, whether or not they become physicists.
I’ll also add that any attempt to identify “the few that might have the potential to contribute” would run into insurmountable problems. There’s no good way to tell what a person’s future potential is in physics or in almost any other field. And if we tried to do it anyway, not only would we fail, but we’d most likely fail in ways that reinforce existing societal biases that favor white men, especially in the sciences. So yes, we should be teaching every kid at least some physics. We can’t know in advance where the next Einstein will be found, and finding the next Einstein isn’t the sole purpose of physics education anyhow.
What’s your opinion of still using ‘Apparent Magnitude’ in astronomy
I don’t feel strongly about this, but then again my background is in statistical cosmology, not observational astronomy.
What is considered an inertial frame in astronomy/cosmology and can you point one out?
I’m not sure what this question is driving at. The rest frame of the CMB is an inertial frame. And the rest frame of the sun is pretty close to an inertial frame; the acceleration it feels due to its orbit around the center of the Milky Way is very small. But the idea of “inertial frame” is an idealization; even if it turns out that it’s hard to define the rest frame of the CMB, it doesn’t mean there’s anything wrong with talking about inertial frames.
Is there anything you found particularly interesting about the evolution of the structure of the universe while working on your thesis? What about your thesis’ topic did you find particularly challenging?
One of the things I really liked best about my thesis was that I was trying to understand the inflationary epoch, a period so far back in the history of the universe that there’s no material of any kind left over from it—no atoms, no quarks or electrons, not even any photons. All that we have left from that time in history are the patterns in the distribution of stuff in the universe, and so our only hope of better understanding that period is to tease out statistical features of the cosmic microwave background radiation and large-scale structure. That kind of statistical work is where cosmological theory and observation and simulations all intersect, and that’s a great place to be when you’re doing science.
Do you have an explanation for the Cosmic Axis of Evil and the Spin of Galaxies?
No. It’s unclear what’s going on with the “axis of evil.” To the best of my knowledge, it’s an open problem.
As a science historian, can you generalize your insights about the lines of inquiry that have enjoyed traditional success in approaching big questions tackled by astrophysicists, and how these compare or may apply to big questions surrounding dark matter and dark energy?
From a historical perspective, the modern idea of dark matter is in pretty good company. There are other kinds of “dark matter” that have been suggested in the past to explain different phenomena, and they have often met with success. When astronomers in the early 1800s noticed an anomaly in the motion of Uranus, they invoked “dark matter” in the form of another as-yet-unseen planet, and they were right—that’s how Neptune was discovered. And when beta decay seemed to violate the conservation of energy, Wolfgang Pauli suggested “dark matter” in the form of neutrinos, which weren’t seen for another quarter-century. Of course, this kind of strategy doesn’t always work. In the mid-19th century, “dark matter,” in the form of an unseen planet or asteroids, was suggested as an explanation for the extra precession of the perihelion of the orbit of Mercury. That turned out to be false—that extra precession is a result of general relativity, as Einstein found in 1915. But dark matter is certainly a reasonable idea from a historical perspective. And from a scientific perspective, I don’t really think we can reasonably doubt that dark matter is there. The evidence is truly overwhelming.
Dark energy is a little bit weirder, historically speaking—it’s hard to know what a good analogy is. Certainly there are many historical examples of a postulated thing permeating all of space, some of which we still accept (electromagnetic field) and some of which we don’t (luminiferous aether). As for the idea of dark energy itself, it’s got a long history, longer than dark matter. Einstein famously considered a cosmological constant and then dismissed it once Hubble discovered the distance-redshift relation, implying that the universe was expanding. And Einstein’s usage of a cosmological constant to keep the universe static wouldn’t have worked anyhow—it was an unstable equilibrium. So Einstein’s idea was abandoned for most of the 20th century. But although the first good evidence for dark energy showed up on the scene in the very late 1990s, it had been anticipated well before that. If you look in cosmology textbooks from the early 1980s, they’re already talking about the possibility of a cosmological constant quite seriously. And again, the cosmological evidence for dark energy is very good.
Do you think a consistent Bohmian formulation of QFT is possible?
That’s an open research question, and it’s not my area of expertise. I have heard that part of the difficulty people have encountered with developing a consistent Bohmian formulation of QFT comes from the fact that our best QFTs are questionably consistent, due to weirdness like Haag’s theorem and renormalization. But take that with a grain of salt—it’s really not my area.
Concerning the different interpretations of quantum mechanics... could one determine if one interpretation is more fundamental or more encompassing than another? An experimental test? A successful quantum theory of gravity or of unified fields?
Fundamentally, I don’t think we’re going to be able to determine which interpretation is closest to the mark until we have a theory that goes beyond quantum mechanics, like a theory of quantum gravity. But there’s a catch-22: I don’t think we’re going to be able to come up with such a theory if we’re stuck thinking about quantum mechanics in a fundamentally misguided way. So, since there’s no way to know which interpretation will lead to the insights that will yield a theory of quantum gravity, I think it’s important for researchers to be familiar with several different interpretations, even if they have a strong feeling about which interpretation is right.
Do you have a view on the ‘reality’ of the wave function?
I think that there must be something in nature that approximately resembles the wave function, or that directly gives rise to something like a wave function. That’s an intentionally broad statement. It could be that there really is a big wave function of the universe out there, constantly splitting in the way that the many-worlds interpretation posits. It could be that there’s something out there like a wave function, but it’s not the whole story, as pilot-wave theory (aka de Broglie-Bohm) posits. Or there’s any number of other possibilities: there’s something out there like the wave function but it doesn’t quite behave the way quantum mechanics dictates (spontaneous collapse); there’s something real out there that that isn’t much like the wave function, but it behaves in such a way that our information about it obeys the Schrödinger equation, and thus that information can be modeled with a wave function (information-theoretic interpretations); etc. But in all of these cases, there’s a real thing, out in the world, that guarantees that the Schrödinger equation will hold and that the Born rule applies in the usual way.
Why do I think this? Because quantum physics works phenomenally well. It explains a huge diversity of phenomena to a breathtaking degree of accuracy. How could quantum physics possibly work so well if there weren’t something out in the world that it was accurately describing? Why would the theory be so accurate if it bore no resemblance to nature at all? Remember, this is a theory that was initially developed to explain atomic spectra—that’s all. Now we use it to understand why the sun shines and how to build lasers. A theory that can do that has got to be latching on to some true fact about nature, even if it’s just in an indirect or approximate way.
Say we have a piece of matter with some temperature T, regarding it for now as a classical system. If we view it as a quantum system, does it still have a temperature?
Sure. The statistical mechanics definition of temperature still applies perfectly well to composite quantum systems.
Thanks so much for your time Adam! Now readers go out and buy his book!
Read the next interview with physicist Niels Tuning
I have a BS in Information Sciences from UW-Milwaukee. I’ve helped manage Physics Forums for over 22 years. I enjoy learning and discussing new scientific developments. STEM communication and policy are big interests as well. Currently a Sr. SEO Specialist at Shopify and writer at importsem.com
Indeed. Even the most appealing creative thought has to be confronted with observations and accurate measurements. If you cannot make contact to observables, it's a nice mathematical idea at best or just philosophical gibberish at worst. If your predictions are clearly countered by observation, it's a physical theory that's wrong and needs to be modified (at best) or abandoned (at worst)! As all natural sciences physics after all is an empirical science.
You have to find an answer for yourself to such a question. To my mind, it’s beyond the scope of "Physics" to answer this question or questions like “What is real?”.Sure
You can conceive that in course of experiments photographic plates have been blackened or that cloud droplets have been formed, without the intrusion of a conscious observer, but how should "Physics" prove your idea.Why should physics prove anything?
Nevertheless, "Modern physics" now indicates that one cannot arbitrarily cut “NATURE” into – so to speak – subjective or objective parts or – let’s say – into Descartes’ mind and matter. Here I follow Bohr who said: I consider those developments in physics during the last decades which have shown how problematical such concepts as "objective" and "subjective" are, a great liberation of thought.Science requires two things to do it. First, you have to have creative thinking to come up with possible explanations of phenomena. And second, you have to have critical thinking to throw away useless explanations.
"Great liberation of thought" is good for creative thinking, but if you loose the critical thinking part as a result of this liberation … well, it's just not going to work.
You have to find an answer for yourself to such a question. To my mind, it’s beyond the scope of "Physics" to answer this question or questions like “What is real?”. You can conceive that in course of experiments photographic plates have been blackened or that cloud droplets have been formed, without the intrusion of a conscious observer, but how should "Physics" prove your idea.
From an instrumentalist' point of view, such questions are idle ones. "In science we study the linkage of pointer readings with pointer readings." (Arthur Stanley Eddington). That’s all. The confusion begins when one tries on base of a schedule of pointer readings to draw conclusions as to the nature of “NATURE”.
Nevertheless, "Modern physics" now indicates that one cannot arbitrarily cut “NATURE” into – so to speak – subjective or objective parts or – let’s say – into Descartes’ mind and matter. Here I follow Bohr who said: I consider those developments in physics during the last decades which have shown how problematical such concepts as "objective" and "subjective" are, a great liberation of thought.I just finished Part I of Adam's book. Did you read it? It speaks precisely against this attitude.
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So do the records of experimental data and setup details have mind independent existence?You have to find an answer for yourself to such a question. To my mind, it’s beyond the scope of "Physics" to answer this question or questions like “What is real?”. You can conceive that in course of experiments photographic plates have been blackened or that cloud droplets have been formed, without the intrusion of a conscious observer, but how should "Physics" prove your idea.
From an instrumentalist' point of view, such questions are idle ones. "In science we study the linkage of pointer readings with pointer readings." (Arthur Stanley Eddington). That’s all. The confusion begins when one tries on base of a schedule of pointer readings to draw conclusions as to the nature of “NATURE”.
Nevertheless, "Modern physics" now indicates that one cannot arbitrarily cut “NATURE” into – so to speak – subjective or objective parts or – let’s say – into Descartes’ mind and matter. Here I follow Bohr who said: I consider those developments in physics during the last decades which have shown how problematical such concepts as "objective" and "subjective" are, a great liberation of thought.
So do the records of experimental data and setup details have mind independent existence?I'll mostly defer to vanhees71's account, comment #70. I think of triggers as a definite lossy data compression, but how the data is compressed is presumably decided by some committee, which hopefully has some minds. One could perhaps say that once an experiment has been constructed as an automated object, the data collected can be automated and be mostly independent of mind. Indeed, if human intervention is required to keep an experiment on track because of an error condition that lies outside the automation specified, one would expect that any data during the period during which human intervention was required ought to be discarded (unless, perhaps the human intervention can be formally modeled).
I'll paste in an account I wrote last night to a correspondent, which seems to be a propos:
Consider an Avalanche PhotoDiode, an APD: we set up an exotic state of matter so that the output signal is almost always near zero current, but occasionally it is some obviously non-zero value. Hardware is usually set up to record the time at which a transition from zero to non-zero current happens (we could instead record the current as a 14-bit output from an Analog-to-Digital Converter, an ADC, every nanosecond, say, but the record of current transition times is essentially a very compressed, very lossy record of the same information.) Also of interest in experiments is the dead time, the time it takes the hardware to restore the current to near zero so that another transition can be noticed and the time recorded.
Suppose we have this device. When it's set up in a dark room, there is a low rate of current transitions, called the dark rate; when we enter the room and turn on a dim light, the rate of current transitions changes; when we move around the room, the rate of current transitions changes; when we change the intensity of the light or introduce new lights, the rate of current transitions changes. If we set up some barriers, again the rate of current transitions changes, and again when we move the barriers around. If we set up two or more APDs, we can calculate more elaborate statistics, cross-correlations at the same or at different times.
If we ask what could be causing these events, one answer is that we've set up a ridiculously exotic state of matter, so of course weird stuff will happen. More than that, however, we notice that as we continuously change the conditions of the experiment, the current transition statistics change more-or-less continuously, if we collect enough data. Even though the events are discrete, the statistics change continuously. Historically, elementary physics has said that each current transition is caused by a particle, but more sophisticated physics works with a quantum field, which can be understood to make no claims about what happens outside the APD, nor about details of the APD current, but does discuss the statistics one would observe for a given theoretical model of an APD, and how those statistics would change continuously as we move the lights or the barriers or the APDs around.
For what it's worth, my YouTube video from last February, Quantum Mechanics: Event Thinking, deliberately short at 4'26", presents more-or-less this story.One additional note, keying in to vanhees71's account, is that triggers for large experiments are usually much more elaborate (and can slip into dangerously ad-hoc territory) than just whether one electrical signal transitions from zero to non-zero.
I think it's best not to get too hung up on the Bishop Berkeley problem. Ultimately I can't see that it helps much to be solipsist about the world. Go to the world of extreme positivism for a visit if you like, which I've found occasionally useful as a way to get out of the box, but best to come back. I've been peppering everything I've written on PF with links to my arXiv:1709.06711 (comment #30 has a more up to date version attached) because that's how I think about QM/QFT (for which sorry, I guess) and it's not yet well-known, but for this specific question, I think its mathematical derivation of a random field as a subalgebra of a free quantum field algebra more reconciles a classical perspective and a quantum field perspective than any other math I've seen in the literature (there's a parallel with the de Broglie-Bohm approach, deriving trajectory probabilities from the wave function, but there are also fundamental differences, that I keep to the mathematics of operators acting on Hilbert space as a model for signal analysis, manifest Poincaré invariance is maintained, and I keep to an operational interpretation of the math as far as possible). One significant point, however, is that the philosophy of classical probability has become significantly less settled than it used to be. I'm happy with an instrumental, construct-an-ensemble-and-compute-statistics approach, which I think is what physicists do, but philosophers have worries that I find significant about that approach, and physicists who want to construct a model for the whole observable universe obviously can't construct an ensemble (also, if we take away the background Minkowski space, constructing an ensemble becomes quite fraught, AFAICT —amongst other worries, of course).
I'd say, if anything is free of prejudices it's a "machine read" record of experimental results. Of course, these records are of no value, if one doesn't know, how the measurement devices and DAQ (i.e., both hard and software) has been constructed. E.g., at the LHC even the best DAQ technology cannot produce "raw data", i.e., there are hardware triggers already in the detectors before anything is stored to electronic storage. These triggers are to a certain extent constructed using models. It's not so clear to me, whether one really could perhaps through away interesting signals by such cuts. Recently there was an interesting article concerning the still mute search for particles beyond the Standard Model concerning possible long-lived candidates in the Quanta Magazine:
https://www.quantamagazine.org/how-the-hidden-higgs-could-reveal-our-universes-dark-sector-20170926/
So one should be aware that there is indeed a subjective element in objective observations, that cannot be eliminated, namely the "arbitrary choice" of the observational apparati. I you'd say, e.g., only the direct human senses are valid, you'd miss a lot of stuff, which objectively exists: e.g., of the electromagnetic spectrum, restricting yourself what can be seen by the human eye, you'd exclude all em. waves at wavelenths outside the one octave from about 400 too 800 nm that can be seen directly by the human eye.
Nevertheless there's some objective reality in observations (particularly those not related to direct involvement of the human senses), because they are reproducible everywhere and at any time independently from each other, given a precise enough description of what is observed in terms of possible setups for measuring the concerning quantities. That becomse, of course, the more convincing if two or more such setups are also using different technology to measure the very same observable.
In modern experiments, it will usually mean a record in a computer, not any direct experience, microsecond by microsecond. For experimental data to be really out there, it should be in "Supplementary Material", or at least available to other physicists on application. Where things get edgy is in the instrumental details of how the experimental apparatus was constructed, including how whatever exotic materials were used were exotically processed, where apparatus was sourced, what sources of noise were shielded and corrected for, et cetera, whchi all in all should be as much as is needed to reproduce the results.So do the records of experimental data and setup details have mind independent existence?
I'm not sure what do you mean with "pointer readings". Do you mean either:
1) direct experience of expermentalist;
2) any type of record from which one can learn about certain measurement result?In modern experiments, it will usually mean a record in a computer, not any direct experience, microsecond by microsecond. For experimental data to be really out there, it should be in "Supplementary Material", or at least available to other physicists on application. Where things get edgy is in the instrumental details of how the experimental apparatus was constructed, including how whatever exotic materials were used were exotically processed, where apparatus was sourced, what sources of noise were shielded and corrected for, et cetera, whchi all in all should be as much as is needed to reproduce the results.
The scope of physics and its operational formalism is limited to pointer readings (the experience of what is called “observations”), which physics can study and connect to other pointer readings. There is no need for any assumption of realism or anti-realism or anything else. All these assumption belong to the realm of beliefs, personal “hypotheses” about yourself and about your experiences of “observations”.I would use a slightly different wording but….yes, that is exactly correct.
The scope of physics and its operational formalism is limited to pointer readings (the experience of what is called “observations”), which physics can study and connect to other pointer readings.I'm not sure what do you mean with "pointer readings". Do you mean either:
1) direct experience of expermentalist;
2) any type of record from which one can learn about certain measurement result?
Scientific approach is based on assumption of realism…..The scope of physics and its operational formalism is limited to pointer readings (the experience of what is called “observations”), which physics can study and connect to other pointer readings. There is no need for any assumption of realism or anti-realism or anything else. All these assumption belong to the realm of beliefs, personal “hypotheses” about yourself and about your experiences of “observations”.
Einstein believed “that the notions of physics would refer to a real external world and that these ideas would be set by things that claim a "real existence" independent of the perceiving subjects.” And then he tried to force quantum physics into the corset of his conceptions. Everybody knows how successful he was. “Physics” cannot establish that such beliefs are true, but it can establish that such beliefs are not true. But, instead of learning from Einstein’s convoluted and ultimately entirely unsuccessful attempts, some are still on the quest to find some good elements of “objective reality” in quantum theory. And the “interpretative game” goes on. It’s not the word "reality" that has almost lost its usability, it’s the concept of a physical reality that has lost all its usability.Scientific approach is based on assumption of realism (defined as "there is mind independent reality" or as opposite of solipsism). So the realism is common basis for any meaningful scientific discussion (this applies to positivists too). If you reject realism there can be no meaningful discussion with you about any science topic.
Again, one of Einstein’s fallacies, merely based on his psychological predispositions and his desire to return to the ontology of materialism.
In his book “Chemistry, Quantum Mechanics and Reductionism: Perspectives in Theoretical Chemistry“ Hans Primas cites Fock:
“The deeper reason for the circumstance that the wave function cannot correspond to any statistical collective lies in the fact that the concept of the wave function belongs to the potentially possible (to experiments not yet performed), while the concept of the statistical collective belongs to the accomplished (to the results of experiments already carried out) (Fock 1952, 1957).”It's well known, why Fock wrote quite "interesting" philosophical articles concerning QT in Soviet times! I don't know, whether it's also in the English edition of Blokhintsev's famous QM textbook, but in the (then Eastern!) German edition there was also a "philosophical appendix"…
atyy's comment,
is perhaps too much a cute fussing about words, but I'll further note that there are no “objective reproducible quantitative observations in nature” insofar as events never repeat perfectly. Of course pragmatically a given experimenter makes their choice of what is close enough (perhaps quantitatively, a formal choice of a distance between events, but even in the most meticulous experiments there are also judgement calls), there are "good" experimenters who serve as exemplars of best practice, and there are social conventions that have been honed over centuries that make intersubjective seem objective to those who have been trained in those social conventions, but there is a gap. Research is arguably about getting "out of the box" —or, for some, the straightjacket— that we find ourselves trained into, and creating a new and beautiful box for students to have to get out of in their turn. All of us have some groups of outsiders, people who have been trained into different social conventions than those we have been trained into, to whom we pay some attention. We can and should make our own choices, and perhaps it's OK even to disdain some other groups, but, I suggest, philosophers of physics are too diverse a group, at least as I find them, for physicists to dismiss all of them.
I'll also add that there's no such thing as “pure qualitative "philosophical" thought”, except as a straw man. Most of the philosophers I pay attention to engage in quantitative mathematics of one kind or another.Well, particularly due to quantum mechanics we have some things that are really reproducible exactly. E.g., any electron is precisely as any other, they are even indistinguishable in a very strict sense. Thus to the best of our knowledge each electron has precisely the same mass, magnetic moment, and charges of the standard model as any other. Of course, these quantities can be measured only with some finite accuracy, but so far even by getting this accuracy down to up to 12 significant digits (for the magnetic moment), there's no deviation from the assumption of indistinguishability. In this sense we have objective reproducible quantitative observations in nature in much better approximation than within classical physics.
That natural sciences are not sheer convention within a science community can be seen that indepedent researchers find the same result, measuring, e.g., the properties of elementary particles.
Mathematics is not philosophy. The mathematicians for already some time like to group mathematics into the category of "structural sciences" rather than "philosophy". Of course, mathematical physics (like axiomatic QFT) is not philosophy but an important part of physics (maybe also mathematics, but that the mathematicians have to judge). If I was a mathematical physicist I'd consider it an insult to be named a philosopher of science!
How come it's not ok to talk about "reality", but it is ok to talk about "Nature"?
Is Nature different from reality?It's ok to talk about reality with physicists, but with philosophers you never know what they mean!
His view is concisely expressed as follows [Einstein (1949), quoted here without the supporting argument]:
“The attempt to conceive the quantum-theoretical description as the complete description of the individual systems leads to unnatural theoretical interpretations, which become immediately unnecessary if one accepts the interpretation that the description refers to ensembles of systems and not to individual systems.”Again, one of Einstein’s fallacies, merely based on his psychological predispositions and his desire to return to the ontology of materialism.
In his book “Chemistry, Quantum Mechanics and Reductionism: Perspectives in Theoretical Chemistry“ Hans Primas cites Fock:
“The deeper reason for the circumstance that the wave function cannot correspond to any statistical collective lies in the fact that the concept of the wave function belongs to the potentially possible (to experiments not yet performed), while the concept of the statistical collective belongs to the accomplished (to the results of experiments already carried out) (Fock 1952, 1957).”
Physics is about objective reproducible quantitative observations in nature, and theoretical physics aims at a mathematical description and the derivation of the observable phenomena from as little assumptions (fundamental Laws of Nature, themselves finally always based on empirical evidence) as possible. This implies also the aim to adapt our intuitive sense for whatever ideas we have about nature. Locality and causality have a very clear and well-defined meaning in local microcausal relativistic QFT, which is the mathematical basis for the Standard Model of elementary particles. It in my opinion and open question, how to incorporate self-consistently gravitation and spacetime structure, i.e., some theory of "quantum gravity", but that's not a philosophical but purely scientific problem, which I doubt very much to be solvable by pure qualitative "philosophical" thought.atyy's comment,
How come it's not ok to talk about "reality", but it is ok to talk about "Nature"?is perhaps too much a cute fussing about words, but I'll further note that there are no “objective reproducible quantitative observations in nature” insofar as events never repeat perfectly. Of course pragmatically a given experimenter makes their choice of what is close enough (perhaps quantitatively, a formal choice of a distance between events, but even in the most meticulous experiments there are also judgement calls), there are "good" experimenters who serve as exemplars of best practice, and there are social conventions that have been honed over centuries that make intersubjective seem objective to those who have been trained in those social conventions, but there is a gap. Research is arguably about getting "out of the box" —or, for some, the straightjacket— that we find ourselves trained into, and creating a new and beautiful box for students to have to get out of in their turn. All of us have some groups of outsiders, people who have been trained into different social conventions than those we have been trained into, to whom we pay some attention. We can and should make our own choices, and perhaps it's OK even to disdain some other groups, but, I suggest, philosophers of physics are too diverse a group, at least as I find them, for physicists to dismiss all of them.
I'll also add that there's no such thing as “pure qualitative "philosophical" thought”, except as a straw man. Most of the philosophers I pay attention to engage in quantitative mathematics of one kind or another.
My criticism against philosophy in QT is not that it doesn't solve any problems, but that they pretend that there are problems, where there are none and then confusing the subject by unclear definitions of prime notions like "reality". Thanks to philosophy (starting with the unfortunate EPR paper, which according to Einstein has not brought out his main concerns with QT which was more about inseparability due to entanglement, as he wrote in his Dialectica article of 1948 [*]) the word "reality" has almost lost its usability, because it is not clear anymore what exactly an author using it wants to say ;-)).
[*] A. Einstein, Quanten-Mechanik und Wirklichkeit, Dialectica 2, 320 (1948)Einstein believed “that the notions of physics would refer to a real external world and that these ideas would be set by things that claim a "real existence" independent of the perceiving subjects.” And then he tried to force quantum physics into the corset of his conceptions. Everybody knows how successful he was. “Physics” cannot establish that such beliefs are true, but it can establish that such beliefs are not true. But, instead of learning from Einstein’s convoluted and ultimately entirely unsuccessful attempts, some are still on the quest to find some good elements of “objective reality” in quantum theory. And the “interpretative game” goes on. It’s not the word "reality" that has almost lost its usability, it’s the concept of a physical reality that has lost all its usability.
Physics is about objective reproducible quantitative observations in nature, and theoretical physics aims at a mathematical description and the derivation of the observable phenomena from as little assumptions (fundamental Laws of Nature, themselves finally always based on empirical evidence) as possible. This implies also the aim to adapt our intuitive sense for whatever ideas we have about nature. Locality and causality have a very clear and well-defined meaning in local microcausal relativistic QFT, which is the mathematical basis for the Standard Model of elementary particles. It in my opinion and open question, how to incorporate self-consistently gravitation and spacetime structure, i.e., some theory of "quantum gravity", but that's not a philosophical but purely scientific problem, which I doubt very much to be solvable by pure qualitative "philosophical" thought.How come it's not ok to talk about "reality", but it is ok to talk about "Nature"?
Is Nature different from reality?
My criticism against philosophy in QT is not that it doesn't solve any problems, but that they pretend that there are problems, where there are none and then confusing the subject by unclear definitions of prime notions like "reality".Philosophy, per se, is not confusing. It’s merely the person itself which gets confused when philosophy questions his/hers implicit assumptions.
Finally, you're right about the first Hegerfeldt paper I cited; in future I will cite only the second paper, which I think enough applies to the relativistic case as well as to the nonrelativistic case to be at least of historical interest to anyone who wishes to understand nonlocality/locality in QFT.By QFT I mean what's used in practice. Of course, I'm aware that QFT is not strictly defined in the mathematical sense, but renormalized perturbative QFT is well defined and obeys all the fundamental properties you expect, including locality of interactions and causality (in the sense of the linked-cluster theorem). In Hegerfeldt's paper it's not clear to me, how he defines his observables. You cannot define particles in transient states in the Heisenberg picture at all. A particle interpretation is only possible for asymptotic free states, which makes it pretty clear that relativistic particles are even less localizable as "little billard balls" than non-relativistic particles. This is all well known since Bohr and Rosenfeld and no contradiction to causality.
Author is Ballentine. The book is Quantum Mechanics A Modern Development (1998). p47:
In classical mechanics the word “state” is used to refer to the coordinates and momenta of an individual system, and so early on it was supposed that the quantum state description would also refer to attributes of an individual system. … However, such assumptions lead to contradictions (see Ch. 9), and must be abandoned.
The quantum state description may be taken to refer to an ensemble of similarly prepared systems. One of the earliest, and surely the most prominent advocate of the ensemble interpretation, was A. Einstein. His view is concisely expressed as follows [Einstein (1949), quoted here without the supporting argument]:
“The attempt to conceive the quantum-theoretical description as the complete description of the individual systems leads to unnatural theoretical interpretations, which become immediately unnecessary if one accepts the interpretation that the description refers to ensembles of systems and not to individual systems.”
and look at chapter 9.3. The Interpretation of a State VectorYes sure, that's the minimal interpretation, advocated by Ballentine in his famous RMP article and also in his excellent textbook. For me the probabilistic interpretation taking Born's rule as a fundamental postulate (the only logical way, because attempts to derive Born's rule from the other postulates failed so far; see Weinberg, Lectures on Quantum Mechanics, Cambridge University Press) implies that the predictions of QT can only be experimentally tested on ensembles. Formally, a state is defined as an equivalence class of preparation procedures and as such of course refers to individual systems, because in order to create ensembles the state has to refer to a preparation procedure on a single system, since each ensemble consists of many realizations of the same state (in the sense of a preparation procedure). E.g., at the LHC you have well-defined bunches of protons which in a well defined way collide at specified interaction points, where the detectors are located.
The way I read philosophers on this is that they are not so much questioning the precise quantitative descriptions as physics, as questioning whether they properly capture our intuitive sense of the ordinary language terms "locality", "causality", etc.Physics is about objective reproducible quantitative observations in nature, and theoretical physics aims at a mathematical description and the derivation of the observable phenomena from as little assumptions (fundamental Laws of Nature, themselves finally always based on empirical evidence) as possible. This implies also the aim to adapt our intuitive sense for whatever ideas we have about nature. Locality and causality have a very clear and well-defined meaning in local microcausal relativistic QFT, which is the mathematical basis for the Standard Model of elementary particles. It in my opinion and open question, how to incorporate self-consistently gravitation and spacetime structure, i.e., some theory of "quantum gravity", but that's not a philosophical but purely scientific problem, which I doubt very much to be solvable by pure qualitative "philosophical" thought.
I agree with you that the latter quest is, in the end, a fool's errand, because if our ordinary language intuitions conflict with the precise quantitative physics that has been confirmed to umpteen decimal places by experiment, then what needs to change is our ordinary language intuitions, not the physics. But philosophers don't seem to like that very much, which is not surprising, since our ordinary language intuitions are the basis of their entire discipline.Ordinary language is inadequate for any kind of physics in the natural sense. Already Galileo new that "the book of nature is written in terms of geometry…". This is still true today, even in a much narrower sense. Of course you have to use a modern idea of geometry, which reaches back to Klein's Erlanger program, but that's another story.
I'm very interested in foundations of physics, but I don't think that philosophy helps to formulate the foundations clearly. To the contrary, philosophy tends to obscure clearly-defined notions (as "locality", "causality", etc) which have a very clear meaning and quantitative description in physics in terms of the most fundamental theories (relativistic local and microcausal QFT and GR).You’re missing the point, quantum nonlocality and delayed choice experiments are analyzed within experimental limits using non-relativistic QM. So, obviously, Lorentz invariance does nothing to abate these mysteries. Now let’s look at some problems in physics that can actually be resolved with philosophy, i.e., the problematic initial conditions of big bang cosmology known as the low entropy problem, the horizon problem, and the flatness problem.
These are indeed problems in physics, as evidenced by the creation of inflationary cosmology whose practitioners are physics professors at highly regarded institutions. How could mere philosophy resolve these problems? We explain that at length in chapter 3 of our book, but the short answer is that all we have to do as physicists is move from dynamical explanation per the Newtonian Schema Univese to block universe explanation per the Lagrangian Schema Universe. Those problems are created by physicists’ dynamical bias, as pointed out by … philosophy of physics. You may not like the answer, but it is an answer from philosophy for a problem in physics. If you want to argue about it, we’ll have to take that to another thread. Let’s try to keep this thread on topic, i.e., Adam’s book.
So philosophy seems to be discussing the validity of language and scientific reasoning. For the latter, the exploration in the scientific reasoning for a science that has not had much deductive evidence seems worthwhile. To add to that statement with the change of language, the nuances of what was originally meant to what is understood today could affect the interpretation of what was the original intention. However this is just skimming the surface knowledge that I have gained.
The first cited paper investigates relativistic classical fields interpreting them in terms of first-quantized wave mechanics a la Schrödinger in the non-relativistic case. I don't think that in the year 2018 we still have to discuss why this doesn't work and why one has to employ relativistic quantum field theory to precisely cure this problem with apparent acausality. It's discussed in any textbook (see, e.g., Peskin-Schroeder).One can't talk about relativistic quantum field theory "precisely", at least in 3+1-dimensions, except about free quantum fields, because interacting relativistic QFTs, again in 3+1-dimensions, only exist as asymptotic expansions, for which discussion is necessarily imprecise. In 1+1- or 2+1-dimensions, where there are models of the Wightman axioms, the Reeh-Schleider theorem is effectively the same as Hegerfeldt nonlocality.
To discuss free Wightman fields in 3+1-dimensions, one can consider as a simplest example the variance ##hatphi_f^2## of an observable ##hatphi_f=hatphi_f^dagger## in the state ##frac{langle 0|hatphi_g^daggerhat Ahatphi_g|0rangle}{langle 0|hatphi_g^daggerhatphi_g|0rangle}##, that is, the expression ##frac{langle 0|hatphi_g^daggerhatphi_f^2hatphi_g|0rangle}{(g,g)}=(f,f)+2frac{(g,f)(f,g)}{(g,g)}##, where ##(f,g)=langle 0|hatphi_f^daggerhatphi_g|0rangle## is a vacuum expectation value (which is enough to fix the Gaussian free field.)
This expression shows that the variance of the observable ##hatphi_f## is modified by the absolute value ##|(f,g)|^2## in the vector state ##hatphi_g|0rangle/sqrt{(g,g)}##. Of course it is the case that measurements ##hatphi_f## and ##hatphi_g## commute if ##f## and ##g## are at space-like separation, but ##|(f,g)|^2## in general is non-zero. Another way to state this is that ##[hatphi_f,hatphi_g|0ranglelangle 0|hatphi_g]not=0## even if ##f## and ##g## are at space-like separation. This simple computation shows that the relationship of state preparation to measurement is different from the relationship between two measurements; it can be dismissed as about free fields, which can be said to be not physically relevant, and the Reeh-Schlieder theorem (which subsumes this simple computation) can be dismissed as about Wightman fields, which can also be said to be not physically relevant, however interacting QFT would agree that ##[hatphi_f,hatphi_g|0ranglelangle 0|hatphi_g]not=0## in general, so there seems to me to be a prima facie case for there being some value in identifying and characterizing different kinds of nonlocality, not only repeating "microcausality", powerful though that indubitably is.
Finally, you're right about the first Hegerfeldt paper I cited; in future I will cite only the second paper, which I think enough applies to the relativistic case as well as to the nonrelativistic case to be at least of historical interest to anyone who wishes to understand nonlocality/locality in QFT.
Who is "the author"? Please try to cite clearly; if possible, I guess many in the forums appreciate also a link to a legal source of the paper.Author is Ballentine. The book is Quantum Mechanics A Modern Development (1998). p47:
In classical mechanics the word “state” is used to refer to the coordinates and momenta of an individual system, and so early on it was supposed that the quantum state description would also refer to attributes of an individual system. … However, such assumptions lead to contradictions (see Ch. 9), and must be abandoned.
The quantum state description may be taken to refer to an ensemble of similarly prepared systems. One of the earliest, and surely the most prominent advocate of the ensemble interpretation, was A. Einstein. His view is concisely expressed as follows [Einstein (1949), quoted here without the supporting argument]:
“The attempt to conceive the quantum-theoretical description as the complete description of the individual systems leads to unnatural theoretical interpretations, which become immediately unnecessary if one accepts the interpretation that the description refers to ensembles of systems and not to individual systems.”
and look at chapter 9.3. The Interpretation of a State Vector
philosophy tends to obscure clearly-defined notions (as "locality", "causality", etc) which have a very clear meaning and quantitative description in physics in terms of the most fundamental theories (relativistic local and microcausal QFT and GR)The way I read philosophers on this is that they are not so much questioning the precise quantitative descriptions as physics, as questioning whether they properly capture our intuitive sense of the ordinary language terms "locality", "causality", etc.
I agree with you that the latter quest is, in the end, a fool's errand, because if our ordinary language intuitions conflict with the precise quantitative physics that has been confirmed to umpteen decimal places by experiment, then what needs to change is our ordinary language intuitions, not the physics. But philosophers don't seem to like that very much, which is not surprising, since our ordinary language intuitions are the basis of their entire discipline.
The first cited paper investigates relativistic classical fields interpreting them in terms of first-quantized wave mechanics a la Schrödinger in the non-relativistic case. I don't think that in the year 2018 we still have to discuss why this doesn't work and why one has to employ relativistic quantum field theory to precisely cure this problem with apparent acausality. It's discussed in any textbook (see, e.g., Peskin-Schroeder).
I've no clue what "Hegerfeldt nonlocality" is though. Do you have a reference (preferrable a physics one, where one has clear statements and a sufficient math density rather than some unclear philosophical gibberish) ;-)).From a few comments down the Facebook comment thread after the Facebook comment I mentioned above:
I'd offer either Hegerfedt's https://arxiv.org/abs/quant-ph/9809030 or his https://arxiv.org/abs/quant-ph/9806036, which link to the conference-published papers and which both cite what I think of as rather less clear papers from the 1970s and 1980s. These two papers include a helpfully more abstract presentation as a Theorem, with the conditions better stated.
My own take on this is that Hegerfeldt's nonlocality, by depending on analyticity deriving from a positive energy condition, is sui generis with the Reeh-Schlieder theorem, however it depends on much less mathematical structure than algebraic QFT, LQP, etc, so that even someone dismissive of the mathematics of algebraic QFT should have a hard time dismissing Hegerfeldt nonlocality.
However, as I say above [in the Facebook comment thread], we can face Hegerfeldt nonlocality with a reasonable degree of equanimity because it is compatible with Lorentz invariance. A further aspect, although this is not something that I would expect a QFTist to find compelling (but who knows?), is that boundary and initial conditions, which are by their very nature nonlocal, determine which (Lorentz invariant) propagator should be used in classical physics, with extensive consequences.I should add that the philosopher I was engaging with there, Max Maaneli Derakhshani, has more-or-less refused to engage subsequently on the more careful, indeed more-or-less axiomatic, characterization of different kinds of locality. Hegerfeldt is essential reading, IMO, although if you know of something that more satisfyingly characterizes different kinds of nonlocality, I'll be very pleased to hear of it. Of course axiomatization is often disdained by physicists as "too much mathematics", which can be almost as much a smear as "too much philosophy". On the other hand, the best philosophy of QFT literature is almost indistinguishable from axiomatic QFT.
Probably I should add that Hegerfeldt is essentially a physicist.
Define "physics itself". I think there is no such thing.Of course there are plenty of problems in physics completely unrelated to philosophy. If this was not the case there'd be no necessity for pure physics research anymore. Fortunately we are far from such a sad state!
Take as an example the discovery of quantum theory. There was a well-posed physics problem in the 19th century to find the spectral distribution of black-body radiation, whose solution lead to modern relativistic QFT (which is imho the first complete solution of the problem; Planck 1900 and Einstein 1917 being important steps towards this solution). This is a typical problem within the natural sciences with no philosophical pseudoproblem around: You simply didn't know the distribution of black-body radiation. Then it was measured with high accuracy at the PTR around 1900, and using the data Planck found the correct spectrum as an empirical formula. Then his problem was to derive it from theory, which was not possible using the then established classical electrodynamics, thermodynamics, and classical statistical physics. He found an ad-hoc explanation in terms of "energy quantization" (where energy is meant to be the exchange energy between the em. field and the cavity walls in Planck's idealized oscillator model). This left him (and also Einstein) quite unsatisfied. The next very important step was Einstein's kinetic-theory treatment of 1917, which lead to the discovery of spontaneous emission, which in fact we know today is not explainable other than by field quantization! This was finally the important notion for Dirac to come up with his annihilation-creation-operator formalism in 1927 (although Jordan had already quantized the em. field in the "Dreimännerarbeit" in 1926 before, but that was not noticed by the community; I've to read that paper carefully to figure out, to guess why).
Another example, which is more a theoretical problem, is the discovery of special relativity. The Maxwell theory of electromagnetism was more or less established at the end of the 19th century (mostly due to the creation and detection of electromagnetic waves by H. Hertz in 1887). There was, however, a theoretical problem, because the theory is not Galilei invariant. Of course, the common opinion at the time was the presence of a preferred frame of reference in terms of the restframe of the aether, but the attempts to empirically prove the latters existence failed. That's why many physicists and mathematicians like Fitzgerald, Lodge, Lorentz, Poincare, and finally Einstein were investigating this problem, which although purely theoretical is clearly a problem within physics as a natural science and not one of some philosophy.
I’ve been studying, researching, and teaching physics for nearly 40 years with one motive — to make ontological inferences and use those to create new theory. These motives are germane to foundations of physics, so I’ve been participating in that community for the past 24 years. Different physicists have different motives for putting in the hard work needed to do research in physics. Whether or not someone’s motives are “worthwhile” is purely a value judgment. If you’re not interested in foundations of physics, don’t participate in those discussions.I'm very interested in foundations of physics, but I don't think that philosophy helps to formulate the foundations clearly. To the contrary, philosophy tends to obscure clearly-defined notions (as "locality", "causality", etc) which have a very clear meaning and quantitative description in physics in terms of the most fundamental theories (relativistic local and microcausal QFT and GR).
So, going back to your earlier comment,
do you consider that whatever nonlocality there is in QM/QFT is not a problem? Of course microcausality is satisfied, so there is not that kind of nonlocality, but still there is, say, Hegerfeldt nonlocality (for references relevant to that, please see https://www.facebook.com/max.derakshani/posts/10103068335632754?comment_id=10103069043593994 and the comments that follow). Personally, I agree that the modern focus of philosophers specifically on "reality", whatever that means beyond hammering the desk, is perhaps excessive — I prefer a rather heavier dose of empiricism and calibrated acceptance of current theories.I couldn't sympathise more with poor Gross. It's hopeless to discuss with philosophers about the fact that local and microcausal relativistic QFT (as is applied with more success than wanted in the Standard Model) do not imply "spooky action at a distance", as claimed about QT in the EPR paper (which in fact Einstein was not quite satisfied with since he felt that his problems with QT are not well represented in this paper; his view becomes much clearer in his article in Dialectica 2, 320 (1948)). In fact, it's the collapse hypothesis of (some flavors of the) Copenhagen interpretation, which clearly contradicts the very construction of standard QFT and the meaning of the S matrix (see the first few chapters in Weinberg, QT of Fields, vol. 1, particularly the chapter on the linked-cluster theorem). Gross is of course referring to the state-of-the-art QFT of the 21st century and has as much problems with making sense of the EPR paper.
I've no clue what "Hegerfeldt nonlocality" is though. Do you have a reference (preferrable a physics one, where one has clear statements and a sufficient math density rather than some unclear philosophical gibberish) ;-)).
I’ve been studying, researching, and teaching physics for nearly 40 years with one motive — to make ontological inferences and use those to create new theory. These motives are germane to foundations of physics, so I’ve been participating in that community for the past 24 years. Different physicists have different motives for putting in the hard work needed to do research in physics. Whether or not someone’s motives are “worthwhile” is purely a value judgment. If you’re not interested in foundations of physics, don’t participate in those discussions.
Well, in physics there are a lot of problems determined within physics itself and some are solved and some are unsolved. That there is a "measurement problem" in QT for me is disproven by evidence since experimentalists and theorists can very well design and analyze experiments using QT. If this is philosophy, that's fine with me ;-))).Define "physics itself". I think there is no such thing.
Scientific method can solve some problems, but scientific method, by itself, cannot determine what is a problem and what is not. Your criticism against philosophy in QT is a philosophy itself.Well, in physics there are a lot of problems determined within physics itself and some are solved and some are unsolved. That there is a "measurement problem" in QT for me is disproven by evidence since experimentalists and theorists can very well design and analyze experiments using QT. If this is philosophy, that's fine with me ;-))).
Maybe, there's a masochistic side in me :biggrin:Many great physicists turn into philosophers later. Maybe you are getting old. :biggrin:
My criticism against philosophy in QT is not that it doesn't solve any problems, but that they pretend that there are problems, where there are none and then confusing the subject by unclear definitions of prime notions like "reality".So, going back to your earlier comment,
The outcome is very clear: If there is a deterministic HV theory that could reproduce the probabilistic predictions of QT (which in fact were shown to be correct, and the Bell inequality is violated as predicted by QT!) it must be non-local, and it's obviously hard to produce non-local HV theories in accordance with Einstein causality.do you consider that whatever nonlocality there is in QM/QFT is not a problem? Of course microcausality is satisfied, so there is not that kind of nonlocality, but still there is, say, Hegerfeldt nonlocality (for references relevant to that, please see https://www.facebook.com/max.derakshani/posts/10103068335632754?comment_id=10103069043593994 and the comments that follow). Personally, I agree that the modern focus of philosophers specifically on "reality", whatever that means beyond hammering the desk, is perhaps excessive — I prefer a rather heavier dose of empiricism and calibrated acceptance of current theories.
My criticism against philosophy in QT is not that it doesn't solve any problems, but that they pretend that there are problems, where there are noneScientific method can solve some problems, but scientific method, by itself, cannot determine what is a problem and what is not. Your criticism against philosophy in QT is a philosophy itself.
This is strawman attack. Philosophy is not rival to physics. Philosophy of science is concerned about physics
solutions rather than physics problems.My criticism against philosophy in QT is not that it doesn't solve any problems, but that they pretend that there are problems, where there are none and then confusing the subject by unclear definitions of prime notions like "reality". Thanks to philosophy (starting with the unfortunate EPR paper, which according to Einstein has not brought out his main concerns with QT which was more about inseparability due to entanglement, as he wrote in his Dialectica article of 1948 [*]) the word "reality" has almost lost its usability, because it is not clear anymore what exactly an author using it wants to say ;-)).
[*] A. Einstein, Quanten-Mechanik und Wirklichkeit, Dialectica 2, 320 (1948)
https://doi.org/10.1111/j.1746-8361.1948.tb00704.x
It is interesting that the author of Statistical interpretation clearly differentiates his interpretation from Copenhagen and describes it the way that can be viewed as generic HV interpretation (wavefunction is not a complete description of individual system).Who is "the author"? Please try to cite clearly; if possible, I guess many in the forums appreciate also a link to a legal source of the paper.
The cut is in all flavours of Copenhagen.
True, the cut is subjective.
True, the cut can be shifted, so anything can be moved from the classical side of the cut to the quantum side of the cut.
However, you cannot put the whole universe, including all observers on the quantum side of the cut, with nothing left on the classical side. People try to do so, but that requires an attempted solution to the measurement problem, eg. Many Worlds or Bohmian Mechanics.Well, then you'd call the minimal interpretation not a Copenhagen flavor. Fine with with me, although I don't think that it is too much different from what's presented as "Copenhagen Interpretation" in standard textbooks. For me the minimal interpretation is mostly this "Copenhagen Interpretation" omitting the collapse (which is not needed and almost never realized in experiments, except it's necessary to take the effort to do so) and the classical-quantum cut, which is anyway not clearly defined as you agree about above. If you call to put a "classically" behaving macroscopic measurement device a "cut", it's just strange language, and that macroscopic measurement devices behave classically for me is rather explained by decoherence than by some fundamental quantum-classical cut.
Henry P. Stapp in “The Mindful Universe”:
“In the introduction to his book Quantum Theory and Reality the philosopher of science Mario Bunge (1967, p. 4) said:
The physicist of the latest generation is operationalist all right, but usually he does not know, and refuses to believe, that the original Copenhagen interpretation – which he thinks he supports – was squarely subjectivist, i.e., nonphysical.
Let there be no doubt about this point. The original form of quantum theory is subjective, in the sense that it is forthrightly about relationships among conscious human experiences, and it expressly recommends to scientists that they resist the temptation to try to understand the reality responsible for the correlations between our experiences that the theory correctly describes.”
The confusion arises when one begins to reason about “the experience of WHAT” – maybe, you can call the "WHAT" the "REALITY" in a metaphysical sense. Quantum theory is – so to speak – about that what’s in our head, the varying content of our consciousness. It has nothing to say about the WHAT. The WHAT is of inscrutable nature. And the tremendous fallacy to mistake the map – the content of our conscious – with the territory – the WHAT – leads to pseudo-questions at the heart of quantum theory.As Bell said, presumably, you do not buy life insurance.
Copenhagen usually assumes the existence of reality……Henry P. Stapp in “The Mindful Universe”:
“In the introduction to his book Quantum Theory and Reality the philosopher of science Mario Bunge (1967, p. 4) said:
The physicist of the latest generation is operationalist all right, but usually he does not know, and refuses to believe, that the original Copenhagen interpretation – which he thinks he supports – was squarely subjectivist, i.e., nonphysical.
Let there be no doubt about this point. The original form of quantum theory is subjective, in the sense that it is forthrightly about relationships among conscious human experiences, and it expressly recommends to scientists that they resist the temptation to try to understand the reality responsible for the correlations between our experiences that the theory correctly describes.”
And the confusion arises when one begins to reason about “the experience of WHAT”. Quantum theory is – so to speak – about that what’s in our head, the varying content of our consciousness. It has nothing to say about the WHAT. And the tremendous fallacy to mistake the map – the content of our conscious – with the territory leads to pseudo-questions at the heart of quantum theory.
Well, this review is, however, also a bit besides the point. I've not read Becker's book, but to think that any of the physics problems, some seem still to claim to be existent, could be solved by philosophy is wishful thinking. There's not a single example in the history of science in the modern sense (which with about 400 years is however not that old yet) where philosophical considerations have solved any physical problem.This is strawman attack. Philosophy is not rival to physics. Philosophy of science is concerned about physics solutions rather than physics problems.
The rest of the interpretation just reproduces the probabilistic statements of the (minimal) standard interpretation, and the minimal standard interpretation (also known as statistical interpretation) is just a flavor of Copenhagen where all the philosophical mumbo-jambo of some of its followers is stripped off bringing bare bones of physically observable facts into the focus, i.e., there is a theory that predicts the probabilistic outcomes of measurements in real-world labs very well, and that's it.It is interesting that the author of Statistical interpretation clearly differentiates his interpretation from Copenhagen and describes it the way that can be viewed as generic HV interpretation (wavefunction is not a complete description of individual system).
The cut is also only in certain flavors of Copenhagen!The cut is in all flavours of Copenhagen.
There's no clear definition of it,True, the cut is subjective.
and there's no known limit to the validity of quantum theory also for macroscopic systems. It's only a technical problem of state preparation preventing us from measuring "quantum properties" of macroscopic objects. In any case there are some empirical examples that prove the existence of predicted quantum effects like entanglement, as for example the experiment entangleling vibration modes of diamonds over some distance (working even at room temperature on a usual lab desk).True, the cut can be shifted, so anything can be moved from the classical side of the cut to the quantum side of the cut.
However, you cannot put the whole universe, including all observers on the quantum side of the cut, with nothing left on the classical side. People try to do so, but that requires an attempted solution to the measurement problem, eg. Many Worlds or Bohmian Mechanics.
The outcome is very clear: If there is a deterministic HV theory that could reproduce the probabilistic predictions of QT (which in fact were shown to be correct, and the Bell inequality is violated as predicted by QT!) it must be non-local, and it's obviously hard to produce non-local HV theories in accordance with Einstein causality.One way to do something about this, vanhees71, is to ask for a manifestly Lorentz invariantly constructed random field that is equivalent to a quantum field. One finds that Einstein locality is indeed violated, but it's hard to object to a construction that is Lorentz invariantly constructed and that is equivalent to an empirically successful quantum field (specifically, quantized EM). I'll upload to here a current draft of a paper that derives from my EPL 87, 31002(2009) (the arXiv version is a couple of months old, as of now, and there's been lots of useful feedback from people on Facebook and from other correspondents since then; I intend to submit the paper to JMathPhys soon).
Once one knows how, one can say that it's not so hard.
I gotta say that I think philosophy does something more than nothing for physics, though as in anything there's a lot that doesn't do much for me.
Copenhagen usually assumes the existence of reality. There is the classical/quantum cut, and the classical side (measurement outcomes) is reality. The terminology is bad, so one could also call the cut the macro/micro cut or the real/non-real cut.The cut is also only in certain flavors of Copenhagen! There's no clear definition of it, and there's no known limit to the validity of quantum theory also for macroscopic systems. It's only a technical problem of state preparation preventing us from measuring "quantum properties" of macroscopic objects. In any case there are some empirical examples that prove the existence of predicted quantum effects like entanglement, as for example the experiment entangleling vibration modes of diamonds over some distance (working even at room temperature on a usual lab desk).
To say that "quantum theory describes a tremendous part of the real world" is your personal "interpretation". That was my point.No, it's a well-established fact by a plethora of high-accuracy measurements of all kinds of systems from the high-energy-particle experiments at the LHC over quantum optics, atomic, nuclear physics to condensed-matter physics. That's not simply a personal interpretation of a single physicist!
To say that "quantum theory describes a tremendous part of the real world" is your personal "interpretation". That was my point…. expressing it with a machine that relies on QM and is on the brink of a revolution, which will rely even more on it.
What is here very strange? It is strange that still today many try to squeeze something REAL out of the “quantum physics” tube. Quantum physics has nothing to say about the nature per se of the world around us. It’s about object-subject relations. And why should there be consensus among physicists? To ask “What, exactly, is quantum physics saying about reality?” is a biased question. It implicitly assumes – without trying to go to the bottom – that there is something like REALITY.Copenhagen usually assumes the existence of reality. There is the classical/quantum cut, and the classical side (measurement outcomes) is reality. The terminology is bad, so one could also call the cut the macro/micro cut or the real/non-real cut.
Quantum theory describes a tremendous part of the real world (or at least that part we can observe and objectively investigate, anyway).To say that "quantum theory describes a tremendous part of the real world" is your personal "interpretation". That was my point.
Quantum theory describes a tremendous part of the real world (or at least that part we can observe and objectively investigate, anyway). To say it's "not real" is simply rediculous. The word "real" is spoiled by philosophers to a degree that you cannot use it anymore in scientific discussions since its meaning has been put into the state of maximum entropy (mess) ;-)). SCNR.
In the interview, Adam Becker says:
“What is Real? is about the unfinished quest for the meaning of quantum physics. We have this beautiful theory, quantum mechanics, and it’s astonishingly accurate. But it’s not at all clear what that theory is saying about the nature of the world around us. It must be saying something about that world—there must be something in nature that resembles the mathematics of quantum mechanics, otherwise why would the theory work so well? But there’s no clarity or consensus among physicists about what, exactly, quantum physics is saying about reality. This is very strange, especially given that quantum mechanics is over 90 years old.”
What is here very strange? It is strange that still today many try to squeeze something REAL out of the “quantum physics” tube. Quantum physics has nothing to say about the nature per se of the world around us. It’s about object-subject relations. And why should there be consensus among physicists? To ask “What, exactly, is quantum physics saying about reality?” is a biased question. It implicitly assumes – without trying to go to the bottom – that there is something like REALITY.
In the interview, Adam Becker says:
"The closest thing we have to a consensus about any of this is the Copenhagen interpretation. But the Copenhagen interpretation isn’t really a single coherent set of ideas about quantum mechanics—it’s a family of mutually-contradictory ideas, none of which adequately solve the measurement problem or answer the other questions at the heart of quantum theory. This is all the more strange given that reasonable alternatives to Copenhagen have existed for decades.“
What questions are at the heart of quantum theory? To my mind, such questions merely arise when people have the feeling that quantum theory “threatens” their personal psychological predispositions or philosophical beliefs. The “Copenhagens” were clearly aware of this.
Maybe, there's a masochistic side in me :biggrin:Blame it on the heritage. :cool:
Maybe, there's a masochistic side in me :biggrin:
@vanhees71 – congratulations on such a long post on philosophy! I think you are addicted to philosophy :biggrin:
Well, this review is, however, also a bit besides the point. I've not read Becker's book, but to think that any of the physics problems, some seem still to claim to be existent, could be solved by philosophy is wishful thinking. There's not a single example in the history of science in the modern sense (which with about 400 years is however not that old yet) where philosophical considerations have solved any physical problem. The progress has been made by a mutual interaction between experiments/observations, model and theory building as well as, in my opinion often underpreciated, progress in mathematics.
There is, as far as I can see, no measurement problem, because quantum theory is successfully used to predict experimental results and to suggest new experiments to test and clarify it. The philosophical quibbles between Bohr and Einstein haven't lead to anything interesting in physics before Bell hasn't found a way to reformulate the philosophical opinions of the two in terms of a scientifically well-defined theoretical statement (Bell's inequality must hold if a local deterministic hidden-variable theory can reproduce the probabilities of QT), which in turn lead to high-precision experiments due to technological progress in AMO physics. The outcome is very clear: If there is a deterministic HV theory that could reproduce the probabilistic predictions of QT (which in fact were shown to be correct, and the Bell inequality is violated as predicted by QT!) it must be non-local, and it's obviously hard to produce non-local HV theories in accordance with Einstein causality. All we have that is compatible with experiment and in accordance with causality in the sense of SRT is relativistic local QFT (and classical relativistic field theories of continua, which however are to be seen as effective theories of macroscopic systems), but no non-local relativistically causal HV theory.
The case of Bohm is in a way indeed tragic, and of course one should not intermingle political opinions with scientific questions. That said, however, it should be pretty clear that Bohmian-de-Broglie pilot wave theory is not very much appreciated in the physics community because Bohm had unwanted political views in his time, but because it is of not much use. The point is that it works to a certain extent for non-relativistic QT but there's no satisfactory reinterpretation of relativistic local QFT in its sense. Also the claimed Bohmian trajectories seem not to be observable, at least it's not unambigously clear how to measure them. The rest of the interpretation just reproduces the probabilistic statements of the (minimal) standard interpretation, and the minimal standard interpretation (also known as statistical interpretation) is just a flavor of Copenhagen where all the philosophical mumbo-jambo of some of its followers is stripped off bringing bare bones of physically observable facts into the focus, i.e., there is a theory that predicts the probabilistic outcomes of measurements in real-world labs very well, and that's it.
It's also not clear to me, why one makes Bohr the main culprit. Although guilty of having produced a lot of philosophical gibberish with notions as "complementarity", he usually was the one who argued with the hard physics facts. It's, e.g., not so clear to me, whether he agreed to the collapse conjecture, which is the most problematic ingredient, in clear contradiction to Einstein causality (and thus rightfully criticized by Einstein as "spooky action at a distance"). Interestingly Einstein also did not think very favorably about the Bohm-de-Broglie pilot-wave idea. If there is a main culprit of the "Copenhagen gang" it was Heisenberg, who was pretty dogmatic too. Ironically he got the interpretation of the uncertainty relation wrong. Bohr had to correct him, but unfortunately Heisenberg's first paper on the subject somehow stuck, and even today statements are made in textbooks that the uncertainty relatation is about the impossibility of accurately measure observables rather than the impossibility to prepare states for which the standard deviations of incompatible observables are small for all of them.
So the main problems with QT today, if there are any, are because of philosophical gibberish and imprecisely formulated claims. The real problem with QT today from a physics point of view, still is the unsolved problem to find a compatible quantum theory of gravitation rather than artificial philosophical issues on some apparent measurement problem.
There's a (positive) review on Becker's book in today's issue of Nature
https://www.nature.com/articles/d41586-018-03793-2There's a (mixed, but overall positive) review by Mélanie Frappier on Becker's Book in today's Science.
http://science.sciencemag.org/content/359/6383/1474.1
""… nontechnical primers are not the place for fastidious philosophical distinctions. They should, however, be careful not to create straw men. …
By suggesting that, for all practical purposes, these physicists defended the same position, Becker—like so many before him—ends up portraying the Copenhagen interpretation as a single, internally inconsistent doctrine. His uncharitable account makes it difficult not to conclude that these physicists were at best unsophisticated instrumentalists, at worst self-serving hypocrites. …
Despite an oversimplified treatment of the philosophical issues at play, What Is Real? offers an engaging and accessible overview … who like Einstein, wonder if the Moon is still there when no one is looking."
From The Quantum Times review:
“The truth, of course, is that (contrary to what many people, even many physicists, seem to believe) quantum mechanics does not describe electrons in this way. Instead of N wave-like disturbances in a field, the theory describes a system of N electrons as a single wave-like disturbance in an abstract, 3N-dimensional space whose connection to ordinary three-dimensional physical reality is, at best, completely obscure.”
This is another issue that the Lagrangian, block universe approach to QM clears up easily. By computing a probability amplitude for a specific outcome (path integral uses future boundary conditions), the formalism is moved out of configuration space and into spacetime. Now you can understand QM as providing distributional frequencies in spacetime, i.e., the relative frequencies of experimental outcome patterns in the block universe. And the confusing nature of the time-evolved wavefunction mentioned above is revealed as nothing more than an epistemological constraint of the ant’s-eye view. In other words, as ants we don’t know which particular outcome will occur in any given trial, thus the need for configuration space in a time-evolved approach.
A more interesting review, more philosophically academic, from the APS Division of Quantum Information, March 16th: http://thequantumtimes.org/2018/03/book-review-what-is-real-by-adam-becker/. This makes me more interested in seeing his lecture on April 3rd.
https://www.wsj.com/articles/what-is-real-review-quarks-and-quandaries-1521234605"Whether he has chosen to wear the right uniform will be for future readers to judge."
There's a book signing in New York on April 3rd, https://www.facebook.com/events/420267451764873/, which is part of a regular lecture series, https://nyphilsci.wordpress.com/201…ation-doesnt-work-and-why-its-popular-anyhow/. I know at least one other person who's going, so I'm toying with going myself. Anyone else interested? Frankly, I need a little impetus, because the story I'm seeing, particularly what seems an excessive focus on Copenhagen, doesn't do much for me (Copenhagen is interesting as history, but not much as a basis for new work, particularly for me, working on QFT).
And although it is not the source you'd normally go to for suggestions on a science book, this review of Adam's book appeared a few days ago… in the Wall Street Journal. :smile:
https://www.wsj.com/articles/what-is-real-review-quarks-and-quandaries-1521234605
There's a (positive) review on Becker's book in today's issue of Nature
https://www.nature.com/articles/d41586-018-03793-2
I agree, we don't want to discuss blockworld per se here, that would be off topic. And, I agree that for most physics blockworld has nothing new to offer. I've purchased Adam's book on audio and will start listening to it this weekend. I'll post any of my responses here. Of course, in that context adynamical thinking is highly relevant, as you'll see.
The dynamical bias runs deep, even those who interpret QM via future boundary conditions resort to terminology such as “retrocausality,” “completed transactions” and “backwards causation.”Bringing in retrocausality takes the discussion even further away from topic of this thread. I'm not going to discuss it in this thread.
Such ideas can take decades to mature.I agree that it takes decades for philosophical ideas to mature, but then it takes more decades to find out if they can contribute for development of scientific knowledge.
But I do not think that blockworld by itself changes anything just like switching from cartesian coordinates to spherical coordinates won't give any new statements about physical configuration we describe with these coordinate systems. There are other features in your approach that you exclusively associate with blockworld. But I don't. As this can open some offtopic discussion I rather stop here.
Have there been similar discussions about adynamical/dynamical thinking among philosophers?The philosophy of QFT seems generally more open to thinking about a block world than is the philosophy of non-relativistic QM, because dynamical evolution has to be equally describable in any boosted frame (not everyone feels forced to a block world by Lorentz invariance, but it's not easy to dismiss it as a possible ontology.)
Have there been similar discussions about adynamical/dynamical thinking among philosophers?The dynamical bias runs deep, even those who interpret QM via future boundary conditions resort to terminology such as “retrocausality,” “completed transactions” and “backwards causation.” I just attended special sessions on foundations of physics at the APS March Meeting earlier this month where Ken Wharton and I gave the only talks on the adynamical approach. [Aside: Ken only recently himself replaced the term “retrocausality” with “all-at-once view.”] Since philosophers of physics tend to follow physicists, there are very few of them who study adynamical approaches. Huw Price is a notable exception, having written a book on retrocausality (Price, H. (1996). Time’s Arrow and Archimedes Point: New Directions for the Physics of Time. Oxford University Press, Oxford) and used the term “global constraint” in a spatiotemporal sense in Price, H. (2008). Toy models for retrocausality. Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics, 39(4):752–61. David Albert worked with Aharonov and Vaidman on weak values corresponding to the Two-State Vector Formalism (Y. Aharonov, et al., Phys. Rev. Lett. 60, 1351 (1988)). Peter Evans is another philosopher who has written on this topic (Evans, P. (2015). Retrocausality at no extra cost. Synthese, 192(4):1139–55). I’m sure there are more, sorry I don’t have their names. [Aside: Ruth Kastner has reanimated (if you will) the use of future boundary conditions in her approach: Kastner, R. (2013). The Transactional Interpretation of Quantum Mechanics: The Reality of Possibility. Cambridge University Press, Cambridge.] Replacing the so-called Newtonian Schema Universe (current way we explain, term from Smolin) with the Lagrangian Schema Universe (block universe way to explain, term from Wharton) is an enormous change in what it means to explain something; probably rivaling the change from Aristotelian to Newtonian thinking. Such ideas can take decades to mature. Aharonov et al. introduced the Two-State Vector Formalism in 1964 and according to Wikipedia that idea originated with Watanabe in 1955. Fifty years later (we introduced Relational Blockworld in 2005 at New Directions) time-symmetric QM finally evolved to fully adynamical thinking (block universe patterns per adynamical global constraints). So, adynamical thinking is relatively nascent.
In short, we lay the blame for the current impasse of fundamental physics and foundations of physics at the feet of dynamical thinking. We also argue that, as Adam found himself, there is a need for collaboration between physicists and philosophers on these matters.Adam is arguing against positivism. And positivism has been discussed among philosophers and so there are things that philosophers can bring to the table.
Have there been similar discussions about adynamical/dynamical thinking among philosophers?
My experience with foundations of physics parallels Adam's, "And this asymmetry I’d found was a doozy: the philosophers of physics were, in general, quite well informed about physics, but the physicists were, by and large, wholly ignorant of philosophy, despite the fact that they were making philosophical claims when they dismissed questions about quantum foundations. As a result, the physicists were generally relying upon faulty philosophy when they answered such questions." In the nine courses I took on quantum mechanics, solid state physics, nuclear physics, quantum field theory, string theory, and particle physics, never once did any textbook or professor use the terms EPR paradox, Bell inequality, entanglement, measurement problem, delayed choice, quantum eraser, which-way twin-slit experiment, or quantum nonlocality. I received my PhD in physics in 1987, so hopefully things are better for young physicists today, but the asymmetry extends even here to PF today.
I've been researching, publishing and teaching in foundations of physics at Etown College for 30 years. I've given dozens of conference and public lectures on topics in this area, so I was particularly excited to see an online outlet become available for dissemination of "the cool stuff" in physics, i.e., PF Insights. I use these for my students in my GR and QM courses, and Ruth Kastner is currently writing a paper referencing two of them, but all of my PF Insights on foundations of physics topics were postdated (to hide them) and had the comments disabled. This sanction even included my Insights explaining papers published in Phys Rev Lett and Nature Comm. This is precisely the attitude towards foundations of physics in the physics community Adam decries.
As to Adam's particular take on the measurement problem, I hope he acknowledges in his book (which I will certainly read!) that the measurement problem is a non-starter for block universe views. For example, there is no "collapse of the wave function" or "non-unitary evolution of the wave function" in the block universe, since one is computing the probability amplitude in spacetime rather than the time evolution of a the wave function in configuration or Hilbert space. This is a psi-epistemic view rather than a psi-ontic view. I have a series of PF Insights explaining the implications of the block universe on foundations of physics starting with https://www.physicsforums.com/insig…ions-part-1-time-dilation-length-contraction/. These Insights have thousands of hits despite being duly"hidden" by the PF Admin.
My colleagues in philosophy and mathematics (Silberstein and McDevitt) and I have a book forthcoming with Oxford UP on a block universe approach to physics called "Beyond the Dynamical Universe" (already available in the UK, available in the US next month). Here is a link to a low-level introduction on the OUP authors' blog https://blog.oup.com/2018/03/gods-eye-view-of-reality/. Besides resolving the puzzle of the Big Bang, the flatness problem, the horizon problem, the low entropy problem, and the conundrums of quantum nonlocality, block universe physics denies the need for non-baryonic dark matter and dark energy. This also allows for an empirical approach to quantum gravity and unification. In short, we lay the blame for the current impasse of fundamental physics and foundations of physics at the feet of dynamical thinking. We also argue that, as Adam found himself, there is a need for collaboration between physicists and philosophers on these matters. This interview on PF is at least a small step in that direction.
Excellent read his new book. I become too intrigued so read it on my phone with kindle app.
It describes the path from the early days of quantum mechanics to the more modern times when questioning Bohr and Copenhagen interpretation become safer for professional career. He gives contexts for different periods and characters in his story that makes his book more interesting to read not to mention the sense of deeper understanding of historical context.
I will add one quote of Einstein that was new for me:
"When Philip Frank, a founding member of the Vienna Circle, asked Einstein about his philosophy of science, he was astonished to find that Einstein was not a positivist. Frank protested that Einstein had invented the positivist approach to physics in his theories of relativity. "A good joke should not be repeated too often." Einstein replied, much as he had to Heisenberg several years before."
An excellent interview, Greg. Thanks.
I look forward to Dr. Becker's book showing up here in the boondocks. It seems I need a lot of historical background to see how the theories first developed to understand what they are and Dr. Becker seems to recognize this key to comprehension.
I don't possess any higher math than some dusty trig. In that unfortunate aspect, I've seemed to reach a plateau with my layman's understanding of the relativities. Most quantum principles seem a lot more difficult to understand and especially incorporate into what might seem to be a simpler mechanical rendition like gravity. I hope to someday see a simpler natural explanation for atomic mechanism too. I ever harbor a secret suspicion that Nature is lazy and not so complicated after all.
So far I've read some info by Asimov and what might be a similar, but dated book, Quantum Reality: Beyond the New Physics by Nick Herbert. Herbert describes several perspectives that may lend themselves to simpler nucleic structure models; I hope more like the electron cloud and maybe even a incorporate a gravitational base.
Wes
…
fyi, we should be receiving a few copies of his new book to give away very soon!
Do you have a view on the ‘reality’ of the wave function?
I think that there must be something in nature that approximately resembles the wave function, or that directly gives rise to something like a wave function.
[..]
Why do I think this? Because quantum physics works phenomenally well. It explains a huge diversity of phenomena to a breathtaking degree of accuracy. How could quantum physics possibly work so well if there weren’t something out in the world that it was accurately describing?
[..]
A theory that can do that has got to be latching on to some true fact about nature, even if it’s just in an indirect or approximate way.I found your response to this question thought provoking, thank you.
Reference https://www.physicsforums.com/insights/interview-with-astrophysicist-adam-becker/
We should make his book a mandatory read for all who want to debate or turn a debate into the 1,001st take of a Bohemian Rapsody – introduction test to prove it included! The last one which started by a harmless attempt by Shoshany to bring QM nearer to school kids:
just turned into the obviously inevitable confrontation (post #8 fffff.)
I think it is weak on interpretation.