Sean Carroll's Mindscape: Science, Society, Philosophy, Culture, Arts, and Ideas - 167 | Chiara Marletto on Constructor Theory, Physics, and Possibility
Episode Date: October 4, 2021Traditional physics works within the "Laplacian paradigm": you give me the state of the universe (or some closed system), some equations of motion, then I use those equations to evolve the system thro...ugh time. Constructor theory proposes an alternative paradigm: to think of physical systems in terms of counterfactuals — the set of rules governing what can and cannot happen. Originally proposed by David Deutsch, constructor theory has been developed by today's guest, Chiara Marletto, and others. It might shed new light on quantum gravity and fundamental physics, as well as having applications to higher-level processes of thermodynamics and biology. Support Mindscape on Patreon. Chiara Marletto received her DPhil in physics from the University of Oxford. She is currently a research fellow at Wolfson College, University of Oxford. Her new book is The Science of Can and Can't: A Physicist's Journey Through the Land of Counterfactuals. Web site Oxford web page Google Scholar publications Wikipedia "How to Rewrite the Laws of Physics in the Language of Impossibility," Quanta
Transcript
Discussion (0)
Aging is real. And so are the benefits of adding vital proteins collagen peptides to your daily routine.
New vital proteins collagen sparkling water. Your daily glow-up now in three fresh flavors.
Strawberry blossom, lemon, lime, and blood orange. Improved skin health in as little as 30 days thanks to collagen peptides?
Cheers to that. Or go with our classic collagen peptides. So you can stay vital, stay you.
Visit vital proteins.com to learn more and where to buy.
These statements have not been evaluated by the Food and Drug Administration. This product is not intended to diagnose, treat, cure, or prevent any
disease. When I competed in track and field at the collegiate level, there were times I second
guessed myself. That's why it's important for female athletes to have a space to build confidence
and self-esteem. Colgate supports female athletes of all levels through the Colgate women's
games, the nation's longest running indoor track and field series for girls and women. By supporting
female athletes, Colgate hopes to put more smiles out into the world. Colgate, your smile is your
strength. Hello everyone and welcome to the Mindscape podcast.
I'm your host, Sean Carroll.
Very often here on the podcast, we talk about the laws of physics, right?
Both what they are and what they might be, you know.
We don't have all of the laws of physics completely settled yet,
so one of the ongoing things that physicists try to do
is suggest different kinds of laws of physics.
But there's different kinds and different kinds.
There are specific laws of physics,
like the standard model of particle physics is a very, very specific set of laws.
Or Einstein's theory of general relativity is a specific.
specific set of laws. But then there are broader frameworks within which we can think about
proposing laws. The obvious ones would be quantum mechanics is a broad framework. Classical
mechanics is also a broad framework. But even those two broad frameworks of classical and quantum
mechanics, they share a certain underlying paradigm, what in other contexts I've called the Laplacean
paradigm for doing physics. And the Laplocene paradigm is basically, you give me the state
of a system, either now or in the far past as initial conditions. There's something we call the
state of the system that has all the information you need. And then there are dynamical laws. The
dynamical laws say starting from that state, where does the system evolve to? And you can evolve it
forward in time, or if the theory is reversible, both forward and backward in time, if you like.
And that kind of paradigm is broader even than the ideas, the frameworks of classical mechanics
and quantum mechanics.
So what if that paradigm isn't right?
What if it's not the best way to think about physics
in either some contexts or even all contexts?
That's the suggestion made by something called constructor theory,
which was first proposed by David Deutsch at Oxford,
and has been picked up by some people,
most notably by today's guest, Kiara Marletto,
who is both a collaborator of Deutsch's
and also has moved the field forward herself
and with other collaborators quite a bit.
So the idea of constructor theory, very, very roughly,
you'll hear more about it later,
is that rather than being given conditions for the system
and how they evolve,
you tell me the complete set of things that can be done
and things that cannot be done
within the laws of physics, whatever they are.
And somehow, this set of things that can happen
and cannot happen,
so factual and counterfactual possibilities,
are enough to either, hopefully, maybe, ideally,
completely tell you the laws of physics,
or at least shed some explanatory light
on what actually happens in the world.
And this is potentially very interesting.
You know, as we'll talk near the end of the podcast,
Kiarra has come up with some ways to use this perspective
to propose things you might not have proposed
by doing physics the more conventional way,
like possible experimental tests of quantum gravity.
But also a completely new perspective says that you change what you think of
are the interesting and relevant puzzles and problems in your field.
Potentially you think about connections, for example,
between fundamental physics and emergent higher levels in different ways.
So it's clear why you might want to do something like this.
It's very, very ambitious, you know, you're trying to do big things.
it also is hopefully clear what the drawbacks of something like this is.
The more ambitious you are, the harder it is to get things right, you know?
I mean, the Laplacean paradigm has been around for a lot of years.
It was implicit in the work of Galileo and Newton, and Pierre Simone Laplace,
circa the year 1800, put it down quite explicitly.
So that's a long track record of success.
To try to start with physics on a completely different footing,
it's hard because you'll probably fail, right?
Most ways of doing physics are going to be wrong,
and you have some success in the current system,
so why not just stick with that and try to improve it?
But it's good that some people try to jump out
of the current way of doing things
and look at things from a brand-new angle.
The burden on them is to sort of come up
with some useful signposts along the way
that correspond to real advances
that we can all agree on or solving some puzzle.
So I will try to,
or rather we, because I really don't understand this stuff very well,
we, I and Kiara, will try to explain what constructor theory is,
why it might be useful, why it has things to say not about just fundamental physics,
like quantum gravity and quantum mechanics itself,
but also real-world stuff, heat engines, thermodynamics,
the physics of life and biology, and so forth.
So I think it's one of these fascinating conversations.
It goes a lot of places.
I will remind you, as I occasionally do, that you can see,
support the Mindscape podcast on Patreon.
If you go to patreon.com slash Sean M. Carroll, you can post a little pledge, rather, a little
donation once per episode, a dollar or a euro, or even more, if you'd like to do that.
Mostly, I think the reason to do this is just to express appreciation, but you also get
ad-free versions of the podcast.
And once a month, as you know, I do ask me anything episodes, and it's the Patreon
supporters that get to ask the questions that are answered on the Ask Me Anything episodes.
But mostly it's a little community of people who like the Mindscape podcast and support it.
And for whom I am extremely grateful, it really helps keep me going podcast-wise, which I hope
everyone is enjoying.
So with that, let's let Kiara take over and expand our minds a little bit.
Let's go.
Giarra Marletto, welcome to the Mindscape Podcast.
Great to be here.
So one thing that strikes me about what you're trying to do is it's super ambitious, right?
You're sort of rewriting the rules for how physics should be done.
So before we get into the actual ways in which you're doing that,
let me just ask the sort of more personal question.
I mean, if one of my graduate students said, yeah, I'm going to work on completely changing the way that we do physics,
I would say don't do that, or at least don't do that until you're a little bit older, right?
It's good to be ambitious, but it's also hard to get things right when you're that ambitious right from the start.
So, I mean, how do you think about that?
Do you think, well, you know, screw it.
I'm just going to be ambitious and we'll see what happens,
or is it a matter of going back and forth between being super ambitious and being more down to earth?
Yes.
So I think the – so, as I said, initially when I started working on this, this was during my PhD in Oxford.
And what happened is that I, so I attended this very interesting talk that David Deutsch gave on sketching or outlining what this program of constructor theory was about and how he envisaged this as being like a generalization of the quantum theory computation.
And so in a way, because my PhD was on the quantum zero computation, I was very intrigued by this.
this idea that there could be something more, something beyond that.
And since then my main question, the thing that interested me,
beside this, of course, bold vision of reformulating laws of physics in a different way and
so on, was, is there a way that we can find problems that are currently open and
tractable that we can address with this approach?
And so in a sense, my focus so far has been to find these problems and solve them in a way that this is in a way of convincing my own self that is actually a worthwhile good working approach.
And I'm completely open to the fact that this may not work to the degree that in a way the whole program hopes.
but I think so far the results are promising enough that they entice me to work more on it.
And more broadly, I think there's one more point I wanted to make,
but I think in general, any work in foundational physics is about working out these bold questions.
So even though, yes, the kind of advice to students is to try to find tractable problems,
I think it's the case that what physics is about is to address these questions.
And so in that sense, I don't see what I'm doing as a particularly unusual or different thing
from what all physicists are interested in foundations are really doing.
It's just one of the various things that we're trying to move a step forward
and try to find new ways of solving these open problems.
Yeah, that sounds perfectly fair to me.
but I have noticed in my own writing papers, giving talks,
and getting responses to them,
that there's always a difficulty when you have to both convince the audience
that there exists a problem
and that you're making progress solving it, right?
Like, everyone has a list of actual existing problems in their head,
and if you say you're solving those, like, why is there more matter than antimatter?
People go, oh, yes, that's a good problem to be working on.
But is this the situation you find yourself in
where you have to convince people that there is an issue to be addressed,
or are people more or less sympathetic to that?
Well, it depends on the particular kind of problem.
I think I do recall having to elaborate on, you know,
why, you know, there is a problem with the quantum theory computation itself.
So I think this is because most people who are currently working in the field
are somewhat focused on the technological developments that stem from the field,
but they are not perhaps focusing on the more foundational aspect
that are actually the ones, you know,
the reasons why the quantum theory computation in a way came about in the first place.
And so in that sense, yes, sometimes you have to, you know, point out that there are these new problems.
But in broader terms, I think some of the other things,
other issues I've been working on, which have to do with this issue of making predictions in
cases where the dynamical laws that we have either fail or we don't quite know which particular
dynamical law we could apply. This is a problem that's recognized by most people who work
in foundations of physics in the sense that, you know, both in the, but for an example, it's the
quantum gravity community where, of course, this is a known issue. And likewise,
problems at the foundation of thermodynamics have some kind of open problems that I don't have to argue about because they're already somehow understood.
So yeah, I think it's the most challenging thing I've found myself tackling so far is really the, so showing that there is a kind of advantage in appealing to these principles that Constructed Theory has, which can lead us to
somehow supplement the dynamical laws as we currently know them.
So in that sense, this is more like a kind of challenging finding specific problems
where this approach makes a difference rather than in explaining why the problems are important,
which I think in a way it's understood at least in the foundational community.
Right.
And so I'm getting the impression that there's a grew out of thinking about quantum mechanics,
quantum foundations and quantum computation and information in particular.
So that's a pretty easy cell.
These days everyone agrees that quantum computing is something interesting.
So it may be if you are presenting a framework that will help us understand that,
that's a relatively tangible thing that people can hold on to.
Yes.
And I think perhaps the less widely known thing is that when you look at the quantum theory computation,
So you open a textbook where they are proving some theorems about channel capacity or other things.
Most of what's proven there is rooted completely in the formalism of quantum theory of non-relativistic quantum mechanics, really.
And this is a plus, of course, in the sense that it's great that we can prove these theorems.
But somehow, if you look at it from a purest point of view,
from the point of view of a person who's interested in information theory,
you would consider this as a slight deficiency,
in fact, as an important deficiency, I would say, of the approach,
because as a theory of information,
if you compare it to, say, Turing's theory of classical information,
it really relies a lot on the formalism of particular theory,
which we know will somehow have to be modified one way or another
by the next kind of dynamical law that will merge quantum theory and GR and general activity.
So in that sense, I think one of the aims of this program that I'm kind of developing
is to find a way of emancipating these results from the specific details of quantum theory
while still retaining all of the information theoretic reach of the results themselves.
So in a way, you know, still being able to talk about things like entanglement and superpositions and, you know, exponential speed up due to quantum effects without there being a specific formalism or which is the one of the formalism of quantum theory.
So this is one way in which the theory computation needs to be generalized.
And it's quite important, I think, because so in a way we haven't quite complete.
the program of formulating the quantum theory computation in this more general way.
And Constructed Theory is attempting this generalization.
Yeah, I want to get to the details of Constructor Theory, but you keep saying interesting
things that I need to follow up on. And the interesting things you just said was the
possibility or the prospect that standard quantum theory itself might need to be
modified in some way. Of course, that's always a possibility. But I,
I think a lot of other physicists would say, you know, there's no evidence that we need that
kind of thing, except maybe if you say that the fact that we haven't quantized gravity yet
should make us skeptical. But you seem more open to the fact that quantum theory itself is going
to not be up to the task of describing physics in the years to come.
Yeah, I think there are a number of reasons why I think this. So on the one hand, there is what you
said. There is the fact that we have a number of...
very well-crafted proposals for quantum gravity, both in the perturbative regime and in a non-perturative
regime and so on. But there is no somehow consensus on which one of these is the right one. And there
are some conceptual issues with some of them and difficulty in finding obvious predictions that stem
out of them and so on. So in that sense, I think in the absence of this one candidate, it's
quite important, I think, to emancipate the results that we have about the universality of
computation and various other things that pertain to the quantum theory computation from the
specific formal aspects of quantum theory, because some of them may stay, some of them may not
stay in the future. But whatever happens, I think my bet is that the information theoretic
structure of quantum theory will be maintained. So things like the quantum multiverse, the idea that
the kind of quantum computing mechanism will still be viable and the possibility of proving that
the universal quantum computer has modes of computation that are more general than those accessible
to a classical universal computer. All of these things will be
are true and we need a way of expressing them
without necessarily rooting them into quantum theory.
The other reason why I think quantum theory is somewhat problematic
or has some, you know, some kind of things
that are not so satisfactory about it
is that there is this field, which is called quantum field theory,
which is something that we effectively use
whenever we have to make a perform a calculation
to perform some kind of predictive,
statement about what happens in laboratory and so on. So in that sense, you know, it's a very
successful thing, formalism. But, you know, quantum field theory itself was at least
conceived by those who proposed it, especially in regard to the theory of electromagnetism,
a kind of work in progress. So it wasn't really supposed to stay as a fundamental theory
of nature. So, and it has issues. So it has various issues, mathematical issues, and it also has
conceptual issues to do with continuum and things of that kind. So in a way, I also find that
not such a satisfactory theoretical device from the foundational point of view. Of course, it's very
successful and, you know, it's great that we can use it to make predictions about things that we
we can test right now and so on. But the question is, we need a better theory. And so in all these
cases, I'd like to be able to build a more robust foundation for the edifice of quantum
tier computation so that it will survive no matter what the new dynamical law will be.
There are a few higher stakes activities that a company can do than to hire new people. You don't
have that many jobs, you need to find the right people, and Indeed.com is here to help you out.
Indeed is the job site that makes hiring incredibly simple. You can attract, you can interview,
and you can hire all on the same webpage. Indeed's hiring tools help you cut through the noise
to hire faster and smarter, and indeed instant match provides a list of quality candidates
whose resumes are on Indeed the moment you post a sponsor job. According to Talent Nest,
Indeed delivers four times more hires than all other job sites combined,
so you can join the more than 3 million businesses worldwide
that use Indeed to hire great talent fast.
Get started right now with a $75-sponsored job credit
to upgrade your job post at Indeed.com slash mindscape.
Get a $75 credit at Indeed.com slash mindscape.
That's indeed.com slash mindscape,
offer valid through October 31, terms and conditions apply.
Okay, that is a good set of motivations.
So now that we're motivated, I mean, maybe I want to ask about what exactly constructor theory says,
but is it first helpful to compare it to the standard paradigm?
If we have people listening in the audiences who are not professional physicists,
what is it about the standard way of doing physics that is there that you're considering
either altering or presenting an alternative to?
Yeah, so first let me just say one thing that is perhaps slightly related to the former question,
but it kind of prepares the answer to this one.
So the name Constructor Theory might make the people wonder why Constructed what is that.
So I think the I think von Neumann, so this is a term that was coined by von Neumann.
So he was wondering whether there could be a more general device that can somehow supplement the notion of a computer.
So he was trying to find ways of saying that the way in which Turing had devised its universal computer was too limited.
And so in a way, while a universal fueling machine can simulate anything that is permitted by the dynamical model on which it runs, it may not be able to perform all the physically allowed transformations, not just computations, so more general transformations.
And the classic example that for Neumann gave in one of his brilliant lectures in the 50s was that there is this task, which is the task of self-reproduction, which was, which was,
of course, cells can implement very easily.
Now, this is a task that requires the device in question
to create a replica of itself.
And while a universal Turing machine can simulate
in its workspace, an ecosystem with cells,
self-reproducing and undergoing natural selection and so on,
it cannot itself be programmed to create a replica of itself.
So that's one, you know, slight,
kind of drawback of Turing's construction.
It's very unfortunate that I can kind of create a replica
of my computers just by programming in a suitable way.
But so in that sense, phenomenon thought,
we need to treat more general programmable machines.
And constructors, that's the term he coined,
were precisely used to kind of label this more general class
of programming machines, which include programable computers,
but also this more universal set of objects that can perform general physical transformations,
not just computations.
And the universal constructor is a machine that can perform any transformation that's physically
allowed.
So it's a kind of ultimate generalization of Turing's universal machine.
The reason why we use the term constructor is because
the key new step in Constructed Theory is that we would like to focus laws of physics
and the fundamental laws of physics, not just on what traditionally is considered to be
the most fundamental way of formulating laws of physics, which is to use a dynamical law
with some boundary condition or initial condition, however you want to call it.
But we'd like to enlarge the set of fundamental statements to include statements about
what physical transformations are impossible and what are possible and also why.
And I think when we talk about a possible transformation, there is where the notion of a
constructor is hidden because the statement that the transformation is possible means that given
a set of laws of physics, the performing that task to the transformation to arbitrarily high
accuracy with a device that works like a constructor so it can perform the task and work in a cycle
so it retains the ability of causing it again.
So this phenomenon that leads to the task to being performed by this constructor is allowed to arbitrary high accuracy.
That's what possible means.
And the fact that the task is impossible, on the other hand, means that there is a fundamental limitation to how well you can, you know, approximate the behavior of a constructor for a given transformation.
And the constructor is, in this case, an even more general.
notion than the one that was proposed by Phenomen, because it's really any system that can
enact enable the transformation on a different system and then retain the ability of causing it
again. So it's in a way it's something that can work in a cycle. So you can think of it as a
generalization of things like enzymes or thermal engines or computers. And of course it can be
programmed as well and so on, but I think it doesn't have to be programmable.
And in a way, the fact that it works in a cycle allows you to remove it from the statement about the law of physics.
And the law of physics are just then about what's possible and what's impossible without having to deal with the complexity of each particular constructor.
So that's perhaps the key step that distinguishes this approach from the traditional approach.
So these statements are supposed to be now the most fundamental statements.
And things like dynamical laws and boundary conditions should be explained in terms of them.
So that's the fundamental switch that you need to take when you try to formulate the laws in this way that we are proposing.
So good. So I think this is actually helpful to me anyway.
I hope to the rest of the audience.
So to restate that, yeah, the bringing up von Neumann is very, very helpful here.
So can I think about it as saying that the point that Turing made was that regardless of any individual computer you might build, I can imagine this universal computer.
And asking what it can and cannot do sheds light on the very idea of computation and the limits of that in the physical world.
And likewise, with von Neumann's constructors, you and David Deutsch and your collaborators are saying that if we knew,
the whole set of things that could or could not be performed,
the whole set of tasks that could or could not be performed
by the universal constructor or individual constructors,
that would be equivalent to what most physicists think of
as knowing the full laws of physics.
Is that the idea?
Yes, indeed.
And I think it would be, that's a very nice way of putting it.
And so here there are a few really exciting insights.
The first insight is what you said, that it's already implicit in the quantum theory computation,
that by studying limitations of programmable machines, which seem to be emergent,
and there's supposed to be something that isn't really at the foundations of physics,
according to the traditional way of looking at physics,
you can actually understand better the foundations of a very deep theory,
which in the case of quantum theory computation is quantum theory.
And in the case of constructive theory, we are hoping can be a more general set of laws,
dynamical laws that include quantum theory, but possibly its successors and so on.
And the other insight is that by switching to the study of these statements about possible and impossible transformations,
you are liberating, you're trying to, you know, you manage to escape this set of
philosophically problematic issues that the traditional conception of physics runs into.
For example, the fact that we put a lot of emphasis in the traditional way of doing physics
on dynamical laws, but somehow we always have, and you kind of have written very eloquently
about this, that we always had this issue of, you know, setting the theory of what are the
boundaries without the initial supplementary conditions for these laws.
And this is an issue that is still open in a sense because there are very many theories
that are proposed about cosmology and also there are issues about how to test them.
And the explanatory statements they make are somehow perhaps less established than
those that you can make with the purely set, the pure set of dynamical laws.
And by appealing to this additional set of principles, we are trying also to explain, to provide a kind of explanatory foundations for theories of cosmology.
So in a sense, we are trying to solve this issue of, okay, we've got the dynamical laws.
Now we have to fix initial conditions and theories about those seem to be a bit arbitrary or hard to pin down.
We want general principles that can help us understanding also what those theories,
could be. So in that sense, this is an additional bonus that comes from expanding the set of
statements that you take as fundamental in your physical picture of the universe. Yeah, I mean,
that would be great if we shed some light on the problem that from the traditional point of
view is what are the initial conditions for the universe, right? And it's very often true that if you
change perspectives, even if the formalism that you invent is completely equivalent, problems that
seemed hard in the original formalism become more illuminated and even easy in the new formalism.
So is your, is constructor theory supposed to be in principle equivalent to the standard way of
having initial conditions plus dynamical laws? Or do you think that it's possible the laws of
physics ultimately just can't be expressed in terms of initial conditions and dynamical laws?
And constructor theory will give you something better, bigger, different than that.
So this is something that will become clear in the future.
So we don't have results yet that can help us understand which one of these two options is the true one.
But the hope is that this approach can enlarge the set of things we can say about the universe.
So in a way, dynamical laws and initial conditions, if this approach works,
would still be true in some approximate domain in a way,
but they would be like emerging consequences of these deeper principles.
And I think you can understand perhaps in what sense this could be true
by considering a principle that, you know,
one of the principles that is most well known in a sense in physics,
which is this principle of conservation of energy,
which I know also you're quite interested in.
So if you take the principal conservation of energy
as a statement about the universe,
about the universe,
you can perhaps think of it in two different ways.
So one is to say, well,
I have this particular set of dynamical laws
and I've got a quantity that I call energy
or even a more general quantity doesn't have to be energy.
And then I can derive by using the symmetries of these laws,
that actually this quantity is conserved.
So it's one way of understanding what the law says.
But there is a different way of thinking about it,
which is to say that the law says that in all true laws of nature,
those that we already know and those that we may actually come up with in the future,
there must be a quantity called something, energy or more general quantity,
that has to be conserved.
Now, this latter statement, if you consider it, is more general than the former, in the sense that the former statement is always particular to a specific formalism of a particular dynamical law, and it doesn't really take a view on what we might want to conjecture tomorrow about a better dynamical law.
But the latter statement really is like a kind of draconian constraint on any law that we might come up with in the future really has to conform to this idea that the task of creating energy, auto-know energy, is really impossible.
And so in this latter statement, you could say any particular symmetry of a particular dynamical law that happens to conform to this principle is in a way explainable in terms of this more.
general way of formulating the conservation law in question.
And so this is the sense in which we expect that these principles of
constructor theory should play a role in deriving or explaining features of dynamics
in a deeper way than just saying, well, the dynamics is like this,
there are these symmetries and we expect these things to be conserved.
So that's somehow the switching perspective and that's why we expect that,
Structed theory statements should be somehow more general than any particular statement you can make within a specific low motion that you happen to know.
Okay, I think this is all very helpful, but maybe I'm cheating because I know a little bit, because you wrote a book and I've read much of the book, et cetera, but the audience hasn't.
So let's bring it really down to earth.
A traditional paradigmatic thing that physicists do, physics problem that we explain is the motion of,
planets around the sun, right? Kepler's laws. Kepler came up with the laws. There's ellipses
and then Newton explained them using this paradigm, this old-fashioned paradigm of dynamical equations
plus initial conditions. How would I explain Kepler's laws from a constructive theory point of view?
Is that even a fair question? Is that the kind of thing that you would think about addressing?
Yes, I think in a way this is a very interesting example because it's specifically, so this is exactly one of those cases where you could explain the phenomenon in question in two different ways.
So one is to say, well, I have these laws, Newton's laws and I've got some initial conditions.
And I know that for certain initial conditions, I will end up having certain kinds of trajectories for these objects.
And then I can put in values for masses and various other constants and find out exactly something that matches the structure of the sort of system as we know it right now.
But there is a different way, which is to say, let's now list all the constraints about.
quantities that are conserved and things that are impossible to create out of nothing and so on.
And now you wouldn't quite get the prediction, the quantitative prediction about how a particular
feature of the orbit of a given planet should be. So you wouldn't get the quantitative aspects of
the dynamical predictions, but you would narrow down the set of allowed dynamical laws and
initial conditions that are compatible with these general constraints.
And now, within these laws, there would be Newton's laws, but also, of course, Einstein's
general relativity equations and perhaps future laws that will also be able to describe by
taking appropriate limits the current structure of the solar system.
them. And of course, to make quantitative predictions, you would need those dynamical laws,
but to explain all of their features, you would have to appeal to these more general statements
about what's conserved and what are the things that you can't change and what are the transformation
that you cannot or can perform. So that's the idea. So the bet is that just by confining yourself
to the dynamical laws, you can't express all of the reasons, why.
say the solar system is the way it is.
And most importantly, you can't capture all of the other possible dynamical laws that you could use in order to describe it.
And so you need to somehow enlarge the set of statements that you appeal to in order to explain a certain dynamical motion that you happen to be able to verify in your vicinity in the universe.
and perhaps a good example here has also to do with the information principles that you can construct
in the Inconstructed theory.
So in a way, maybe we can discuss this in a next question or a bit later.
Yeah, no, we can be.
I do want to dig into this one a little bit more because I may or may not have understood
what you said, but are you saying that knowing all of the principles of what can and cannot happen,
so energy is conserved, angular momentum is conserved, et cetera.
This is not enough to derive Kepler's laws.
Is that true?
We need something else.
Well, you wouldn't be able to derive the exact quantitative statements about,
for example, the certain geometry of a particular orbit
and the given, let's say, all the features of the sun,
and of the planets and of the things that are orbiting around the sun and so on.
So in that sense, the dynamical laws, in specific case, Newton's laws are quantitative about
some of these predictions.
And this is something that you can't get just by stating a set of possible and impossible
transformations because that is a qualitative set of statements.
So in that sense, I think the predictions you would get,
out of a set of statements about possible
impossible transformations are
compatible with
Newton's laws and
Kepler's laws, but
also with other laws that
are more general, and we may not
have conjectured yet,
and also include, of
course, Einstein's
general relativity, which is
a kind of improvement on those
laws. So in
this sense, I think it's
not enough to just constant
on the statements about, you know, on statements that say what transformations are possible
and impossible to derive all the statements that you can derive from, say, things like
Newton's laws. But the statement I'm making, and we are kind of making generally in this research
program, is that there are things in the reality that you can describe with dynamical laws,
such as Newton's, that can't be explained within just Newton's laws.
and therefore to have a complete picture, you need both the dynamical law approach supplemented
with these more general principles.
And then we make the statement that we believe that these more general principles are actually
in a way you can think of them as more fundamental because in a sense they are more general
than any specific law motion.
So these are the two logical steps involved in thinking about the principles and their
relations to dynamical laws.
Okay, so good.
I think this is helping me out, but let me just check that I have not fooled myself into thinking
I understand what's going on.
So in the standard picture, when we have Newton's laws, we can derive the fact that energy
is conserved and momentum is conserved, et cetera, but they seem a little bit parasitic on the
underlying dynamical laws.
And you're making the case that it would be better to consider that.
as, you know, at least on an equal footing, if not a more fundamental footing, than those
dynamical laws for reasons of explanatory power? Is that fair? Yes. Yes, correct. And in general,
as I said, once you have derived the conservation of energy within a specific law on motion,
that isn't very explanatory about possible other laws of motion. So in a way, in this framework where,
you're considering the fact that this law motion may be modified.
And you want to use these principles actually guidelines to help you out in guessing future laws,
which is actually what we do in physics ultimately, because that's how we use principles.
The thinking of the conservation of a certain quantity as being just an implication of a particular law motion isn't very helpful.
So in a way, this logic I'm advocating isn't that new because it's something that we have been informally using for,
for quite a bit in physics.
So principles are helpful when we want to conjecture
fusion laws of physics.
It's just here we were pointing out
that there are some phenomena
which are described by some of these dynamical laws
that we know that can't quite be exactly
captured within just those laws.
So you kind of need these other additional set of statements
to fully explain them.
And so conservation laws are an example.
There are other examples.
And yeah, so I think this is,
kind of, but what you said is exactly it.
Good. That's very helpful. I'm just going to keep heading on this one example a couple more times
because I'm really, this is very, very helpful to me. And it is putting it in these concrete
terms is making me understand. But if I understood what you said, then, you know,
Newton says that the force due to gravity obeys an inverse square law, right? The force
fades away as the inverse of the square of the distance between the objects. I could imagine
other possible worlds in which it obeyed an inverse cube law or something like that.
And energy would still be conserved and angular momentum would still be conserved.
So what I'm guessing, and you'll correct me if I'm wrong, is that constructor theory is sort of silent on which one is right.
And the full theory of the world would include, in your view, both these general principles and some specific addendum that says they're in
instantiated in the following way in the actual world.
Is that correct or did I go too far?
Yes, I think this is correct.
There is one interesting thought there that one could explore,
and this is to do with, could one then explain
even the particular scaling of a particular dynamical law
in terms of some other counterfactual principle,
which we don't perhaps yet know.
Likewise, this is similar in the, you know,
there's a similar question.
let's say in quantum theory where we have this certain rule that, well, we call the
born rule, which has to do with how to compute probabilities from given, say, the quantum
state of a given object.
And there are other assignments that could be in principle, other assignments for computing
this kind of probability rule.
And the question is, well, in this case, we're just postulating that the rule has to be like
that, at least this is what you're doing in textbook quantum mechanic.
But so there could be more general principles that you can conjecture, which would then pin down
the exact scaling that the one rule conjectures for the probability law in quantum theory.
So this is a similar question, so this is a similar issue to the one you pointed out.
And I think this can be said about, for example, constants of nature.
They are also currently unexplained in general in events.
a specific dynamical law.
So why a given value and not another?
So if the program works in the way we expect,
you could then link all of these apparently accidental features
of laws that we currently use in order to predict things successfully
to actually a more explanatory principle
that ultimately can be expressed in terms of these statements
about what's possible and what's impossible
on a given subsystem of the universe
when you're trying to perform a transformation on it.
But of course, it's a conjecture.
So it's a kind of work in progress
proving all of this.
And it's certainly true that just from the conservation laws,
you can't, of course, pin down some of these features alone.
But there should be more general principles.
Now, that makes a lot of sense.
So it seems as if there's sort of a weaker claim
that taking these principles as more fundamental
than the dynamical laws provides insight
and helps us explain things.
And the stronger claim that maybe there's sort of a maximal set of these principles
that we don't know yet about what can be constructed, what can not be constructed,
that would suffice to pin down the exact laws of nature perfectly.
Yes, quite.
Or rather, I would say, explain them.
Explain it.
So I prefer to use that statement in the sense that it may not be the case that this pins on one specific single law.
In fact, my guess is that, as I said, this would at best explain the features of a number of viable dynamical laws that are compatible with these assignments of principles.
And of course, the bold conjecture is to say, well, any relevant feature of those laws, if we note it as physicists in a way that is a kind of relevant thing that we want to explain, ultimately can be explained in terms of these statements about what possible and impossible transformations you have.
and that's something that may or not be true
and it will become clear in the future whether it is.
It's kind of an interesting question.
Sure.
Okay.
Final question about the solar system before we move on to other topics.
And this is like the dumbest question just for clarifying purposes.
When I first heard about constructor theory, it's not that old, right?
It's just a few years ago.
I guess my question was like, what is the constructor that picks up the earth
and moves it to another point in its orbit.
But I think from everything you've said,
and I've read subsequently,
the point is not that there is a constructor
that is making this happen,
but that by contemplating the set of all constructors
that could do different things,
you can figure out how things happen.
Yes. Yes, exactly.
So this is a very nice question.
When you're thinking in the traditional way
that we all use when we approach physics,
as you said, the question is, okay, I see a kind of change in the universe somewhere, a movement of sorts.
And I want to explain this in terms of some, ultimately some low emotion and some kind of initial set of conditions for that low of motion.
But so in this sense, the question of one could say, well, okay, the questioning, okay, the constructive theory is to say, let's identify the constructor that does this or that, they implement this or that transformation.
As you said, this is not the logic.
Here, the logic is to state a kind of constraint
about what are the features of the possible allowed constructors
for this particular motion that I'm considering.
And of course, if you think of the orbits and the planets,
you could think of much better constructors
than just the laws of physics as they are, right?
because you could think of having a robot that corrects the trajectory of a given planet every so often
and makes it even closer to a specific geometry that you desire.
And of course, this is actually allowed by the laws of physics.
So it's a permitted kind of constructor.
It's just we haven't implemented one yet.
We may in the future, I don't know.
And so for the moment, we just are stuck with this particular shape of the solar system,
which is the one that is naturally implemented by the underlying elementary symmetries of the dynamical laws we have.
So they are in a way, you can think of them as the approximate constructors that are at work there,
because they in a way are unchanged after they have implemented one rotation of the given planet around its orbit.
But of course there are better constructors for the task of letting a given planet move around a specific
orbit with a given shape.
And we can think of ways in which, in principle,
these constructors could be allowed and could be built.
But that's not what you see in the conservation law.
The conservation law just says,
well, out of all these constructors
that you might think to implement this transformation,
surely you can't use those that violate this particular thing
and they create, say, given quantity out of something
that doesn't have that.
Good. All right.
I will let you go for the solar system now.
I think I understand it a lot better.
And I want to give you an opportunity to talk a little bit about, because we are shifting viewpoint, right?
I mean, that's a big aspect of this whole program.
Well, sorry, it seems to me right now that in the current state of the program, a shift of viewpoint is the more obvious thing than a particular new view on the theory of everything or anything like that.
And part of that viewpoint shift is this emphasis on counterfactuals.
I mean, your book is literally called the science of Ken and Can't.
What is the title of your book?
Yeah, that's right.
Yeah, the science of Ken and Can't.
The Science of Can and Can't.
So what is the role the counterfactuals play?
Because in some trivial sense, anytime you have a law of physics,
there are counterfactuals implicit there
because the law of physics says, here are things that can happen,
and there are things that can't.
The things that can't happen obey the laws of physics,
and those other things can't.
You are putting a slightly different spin on it, I think.
Yes.
So the term counterfactually is used in the book in a very specific way.
So it's really referring to these statements that I already mentioned earlier,
the statements about what transformations are, say, possible or impossible on a given system
in the sense that we discussed a bit earlier.
So in this sense, it's a kind of perhaps in our sense than say what you find in mathematics or philosophy.
But it's in common with those other notions, it has the fact that these statements are more general than a particular statement that you make when you say,
well, I have this particular dynamical laws in the described universe and these are the boundary conditions.
And this is what happens in the universe.
And that's all there is to it.
So this could be regarded as a, in a way, a kind of caricature version of the traditional way of formulating physics.
But ultimately, I think I would say this is the ultimate goal of the traditional physics program in a way that we are all hoping, as physicists, let's say, that we will find this ultimate dynamical law and this ultimate theory of the initial condition.
and this will tell us everything we want to know about what's going on in the universe.
And the idea here is to say that this specific statement,
the one that fixes the dynamical laws and initial conditions,
is really just a statement about what happens in a given universe.
So it cuts out all of the other counterfactuals because, you know, they're not happening.
So there are other possibilities that haven't been realized,
and therefore they're not of interest in a sense.
And here we're saying something different.
So we're trying to say that first,
that statement in itself wouldn't exhaust all the explanatory things that you can say about the universe.
For example, it would miss out, for example, on these conservation law statements that we mentioned earlier,
because of course in a given universe,
you may not find a particular perpetual motion machine,
but that doesn't mean that it's not allowed.
So, you know, it doesn't happen.
But, you know, whether it's allowed or not
with different perhaps initial conditions
or different dynamical laws, we wouldn't know.
Whereas the law that says that isn't allowed,
that's not possible, and there is an explanation for why that is,
rules out all such counterfactual words.
worlds and leaves us with a set of other possible worlds that are kind of in principle permitted.
So I think the term, the emphasis on counterfactuals is kind of to say that among the things
that we need to appeal to in order to explain particular features of objects that we encounter
in the universe are these counterfactual features.
And just like with all laws of physics, they appeal.
to things that are not directly observable in the sense that, you know, the explanatory part of,
you know, quantum theory or general activity is far from what we directly see, but nonetheless
is the best part of the explanatory set of statements that the theories can make.
And likewise, in this case, the counterintuitive fact is to say, well, a factual thing,
something to do with what happens in the universe as we can observe it, is actually due to
these counterfactual principles. And so in that sense, it's like adding or emphasizing,
let's say, a set of these unseen things in terms of which we explain what we see in a more
systematic and general way than it's been done so far, because in a way counterfactuals
have been used in thermodynamics and in other branches of physics in kind of an informal or
implicit way. And now we want to do it in a kind of proper way. And also including counterfactuals
from, say, information theory and other branches of what we now think of physics. Philosophers, obviously,
you've thought about counterfactuals quite a bit. You know, David Lewis had a whole metaphysics
of possible worlds and so forth. Is that work of any use to you, or do you read about it? Or are you
just more pragmatic about your counterfactuals? I think these works are useful.
to understand, you know, philosophical works are usually useful to categorize things in a very
proper and clear way. So in that sense, I think they are very useful to that degree. And they've been
useful for me as far as, you know, you can tell what kinds of counterfactuals I'm interested in
with this theory versus a more general sense of counterfactuals. It could be of interests of
of use within philosophy or mathematics and so on.
I think for the level of predictions and kind of statements
that we're making at this stage within constructive theory,
we don't necessarily need to appeal to the subtleties
that are mentioned in these works,
but they could be useful in the future.
In general, I think I quite like the work that some philosophers do
in clarifying some of these categories that perhaps in physics
we are slightly misusing.
And I find it kind of illuminating sometimes to read about those things.
I'm not sure I find directly an application for those yet in what I do.
So in a way, I'm kind of on the pragmatic side, I would say.
But open to sort of refining my notions if I need to.
It's a good place to be.
I didn't actually know what the answer was going to be to that question.
So I thought I would throw it out there.
So here's something maybe more up your alley.
it's very interesting to me, and I think to a lot of people who are physics-minded,
who first hear presentations about constructor theory,
that we have a standard conventional view of what fundamental physics is like, right?
Quantum mechanics, quantum field theory, even, you know, a few hundred years ago,
Maxwell's equations, Newton's laws.
And many of your examples when you talk about constructor theory are already at the
macroscopic emergent level, right? enzymes or thermodynamic engines or something like that.
And I get the impression that you treat these, what I would think of as an emergent level of physics,
sort of macroscopic approximation to what's going on, you know, with equal dignity to the more
fundamental things that are going on. Is that a fair reading? Or is there something new and special
about the relationship between these different levels from the constructor theory point of view?
Yes, I think that's a great question.
It's a very important thing that I think it's already implicit in this work on the quantum theory of information.
So the divide between what's macroscopic and non-fundamental and what's considered as microscopic and fundamental is something that, well, I would say somewhat blurred.
or at least arbitrary in a way because we can for sure tell what's clearly macroscopic
and what's clearly microscopic.
But then there are all of these things in between that we, you know, it's a bit like
a question what constitutes something that's alive.
You know, clearly a bacterium is, an electron isn't, but there are lots of things in between
and one might put the dividing line in various places.
Now, the laws that we are talking about in Constructed Theory
try to capture regularities that are true, independent of the scale.
So they would be true within, say, you know,
a set of objects that we would label as microscopic, like a bunch of atoms, let's say,
not particularly aggregating in any specific way.
But also, it could be true of a more macroscopics,
object, which, for example, displays some information
theoretic regularities, such as a flag, which
can instantiate some bit of information or something like that.
And this is not an unusual thing in the sense
that although I think, as you said, most traditional physics
wouldn't think of laws of this kind as fundamental.
In the case of quantum computing, we already
encountered these kinds of things, because when we talk about
a qubit and what a qubit does,
does and what are the laws that kind of underlies behavior and so on, we're not really worried
about which specific system is embodying, I mean, embodies the cubit. Of course, we can think
of an electron spin, which is pretty microscopic. But then, of course, as Schrodinger did, we could think
of a cat being dead or alive, that, you know, if we were able to manipulate a cat in a quantum
mechanical way, the relevant degrees of freedom of it would also behave.
according to the laws of qubits.
And so in that sense, the examples I'm referring to bring in possible instances of both
microscopic and macroscopic objects, all of which conform to these general principles
because the principles are scale independent.
This is something that doesn't quite, so this is maybe an element of novelty, if you
like. And the principles are not about saying what is the most probable behavior of a given
aggregate of atoms above a certain scale, let's say, in the thermodynamic limit. They're
really about just stating that a certain transformation is impossible. And then it's up to you in a sense
to work out what this implies for a given aggregated atom with a given specification, which could
be approximating the behavior of an enzyme or a heat engine or something else.
So in that sense, I think it challenges the idea, the approach that we are pursuing,
challenges the classic divide between macroscopic and microscopic.
And tries to find these principles that are not rooted in either of the domain.
So it's not just, they're not just macroscopic or microscopic,
but somehow they are valid across scales.
And in a sense, you know, we're hoping that this unifies our understanding of objects
that we regard as emergent and objects as we, that we traditionally regard.
other's fundamental and more elementary.
Yeah, I mean, let me, let's continue in that vein a little bit because I am a little bit
confused about, you know, what is approximate and what is exact. And even if that's a sensible
notion in some way, because you make some provocative statements about the arrow of time
and irreversibility. And this sort of standard way of thinking about that. By standard, I mean
what I wrote in my book about the arrow of time is to say that at the microscopic
level, all processes are reversible. The laws of physics do not tell the difference between
forward and backward in time. But at the macroscopic level, when you add in some past
initial condition of low entropy, you find that certain things happen and certain things don't. So
the world looks irreversible. I mean, a classic example is the car no cycle back in the 19th century.
This is probably one of the first examples of one of what you're thinking of, you know,
it's just stating that certain things are impossible. An engine.
that has a certain efficiency is impossible.
But I take that to be a purely macroscopic statement.
And you're sort of shifting the ground underneath our feet a little bit to, to, I don't know,
undo the connection, I guess, between, in my mind anyway, between that kind of macroscopic
statement and the idea that it's an approximation of more exact microscopic statements.
you're sort of putting it on equal footing. Is that fair?
Yes. I think this is a very nice way of expressing what we're trying to do.
Okay, this is a very interesting topic.
So the first thing I want to say is that I see the statements about irreversibility to do with, say, the second law
and the issue of the hour of time as different or distinct.
So in a way, what I'm going to say has to do a lot with irreversibility and less so with the arrow of time, which is something that I see as a separate problem.
And so in regard to irreversibility and what, say, the second law says, the second law of thermodynamics says, I think I agree with the kind of general view that the second law of thermodynamics is a law that in the current formulations,
least holds in an just in approximate sense so in a way we know that it holds for certain systems
that we call macroscopic what that exactly means we don't want to go into really because when you know
asked for a specific characterization of what are the systems for which the second law holds
even philosophers having kind of quite quite an issue there so it's very hard
hard to say to pin down exactly what the exact boundary of applicability, domain of applicability
of the second laws, as we know them, is.
But let's say we are fairly happy pragmatically that they work in a certain case and not
in others.
And then we take the dynamical laws as the fundamental things.
They are reversible.
And then there are some ways in which we can make an argument that typically involves,
you know, quite ingenious.
ideas that were pioneered by Boltzmann and others to connect the general, the general sort of
statement that the second laws make with the particular dynamical laws, which are not,
which are not irreversible. Now, this is the general view. And what we think can happen with this,
new kind of approach in terms of counterfactuals is that there could be a way of reformulated
the second law in a way that doesn't rely on these approximation schemes. So in a sense, it's
no longer scale dependent. And it would be about certain transformations being possible in one
direction and not in the reverse direction. And by this, I mean not that the given dynamical trajectory
is allowed in one direction, not in the other. Otherwise, this would just say that we are thinking
that dynamical laws are irreversible, which isn't what we expect. But I'm saying a transformation
is possible in one direction and not in the other, which means a constructor, if you like,
is allowed in one direction, not in the other. And this is a much more plausible statement
in a sense.
And if you think about it,
it could actually hold at all scales
because it's not a surprise
that if you want to perform
a certain transformation
to arbitrarily high accuracy
in one direction,
you can use a given constructor
that has certain features
and operates according to some means.
But then if you try to use the same machine
to perform the opposite transformation,
it may actually stop working altogether
in the sense that there's no guarantee
the machine that performs a task in one direction
should actually be able
to perform the transport task, the reverse task.
So in this sense, we expect that by taking these statements about possibly impossible
as fundamental, you can somehow see a possible resolution between this conflict between, like,
the laws that are microscopic and reversible, and these general statements that hold in
thermodynamics and other domains, which prescribe the kind of irreversibility, because you can think of
this irreversibility as regarding constructors and their usability in one direction or another,
rather than trajectories, dynamical trajectories of isolated systems not being reversible,
which are obviously in conflict with the understanding of the microscopic physics that we currently have at the moment.
because all of the dynamical laws we know that are fundamental are kind of expected to be time-reversymmetric.
So in this sense, we are somehow proposing a third way out from this notorious clash.
So, you know, we would like not to use statistical mechanics methods because this leads to an emergent set of laws,
which is somehow only approximate and not really fundamental, I would say.
But we're still leaving the possibility open for the fact that the second law and like similar laws could be fundamental and exact, just that they have to be formulated in terms of these other statements.
And there you can see that there is a compatibility between those statements and the fact that the dynamical trajectories of elementary constituents of the objects that obey these general laws are actually time-reversosometric.
Okay. Yeah, this sounds worth trying to do, but still a little aspirational, right? Like, we don't have the full story yet played out. But I do want to give you an opportunity because I think there are examples where you have used this kind of way of thinking about things to sort of be specific and make some claims about physics that you might not otherwise have reached. For example,
in the case of hybrid quantum classical systems and maybe even quantum gravity and experimental tests.
Is this too dramatic or is that a fair way of putting it?
No, I think that's correct.
And it's quite exciting.
I think it's another thing that currently I'm focused on.
So this is, well, ties in well with what we said earlier at the start of conversation.
about, you know, why would you want to have more general principles?
I mean, after all, you know, you go in the lab, you just want a dynamic law that kind of, you know,
conjecture to describe something and then maybe a rival law and then you'd kind of test them against
each other and that's how we do physics.
Now, the specific situation that you're referring to is this situation where this logic
doesn't seem to work as straightforwardly as it usually does.
and this is the case of systems that one way or another have dynamical laws that are either
interactable or worse, they are not even completely settled.
And the case of gravity, in interaction with a probe that is quantum mechanical fits
the second scenario.
So in the sense that we've got many suggested proposals to describe what's going on.
I think this goes back to kind of Feynman and other scientists who already at the time were wondering about how do we describe this kind of system.
But we don't really have a watertight way of just making predictions in these domains that are then testable and at least can help us rule out a class of models for gravity.
So it would be nice, at least from my point of view as well, because I'm one of those people who,
expects gravity to be modified in a way they will become quantum rather than quantum theory
becoming classical, it would be nice to be able to rule out a class of classical models for
gravity. And we haven't been able to do this yet in terms of just an experiment. So in this domain,
even though we don't have specific dynamical models that can unambiguously work for making
predictions, we can use principles. So in the same way that we can use, we could in the past use
thermodynamic principles to, for example, conjecture the existence of new particles that were not
known yet and so on. Here, too, we can appeal to these general principles that are about
counterfactuals and specifically about information, which is one of the works have been
developing also with David and others, to set up a kind of witness for testing whether a given
system is classical or not. Now, this is a very binary choice. So we are not really trying to say,
what is the dynamical law that gravity obeys? That's not the kind of question we're asking. We're asking
a much, much more modest question, which is, can we just say if gravity has some non-classical
elements? So something that makes it completely impossible for a classical theory, one that
doesn't have a multiverse in a sense, to quantum multiverse, to describe this object, to describe gravity.
Not just gravity, it could be any object, but gravity is the most exciting application, I would say.
And with these general principles, you can set up a theorem, kind of a theoretical argument that says that if you can use gravity to generate entanglement between two quantum masses in some experiment, you know, some kind of laboratory setting, and you can rule out other forces, other means of interaction between these two masses, then gravity has to be non-classical.
And note that while this is in a way obvious and trivial within quantum theory, because if you have three systems, then you can use one of them to entangle the other two, then in a way it's a kind of obvious consequence of quantum theory of information to say that this system that you use to entangle the other two should be quantum.
In the case where you cannot assume that this mediator is, obeys a given dynamical law, this statement is non-trivial at all.
And it's very interesting that you can still make this very strong statement by just assuming that this system that mediates the entanglement obeys these general principles.
And this is something that I developed with Vladkovedro.
We were both really excited that you could make this general claim because also it reminded us a bit of this, of the generality that you have in these theorems like Bell's theorem in quantum information,
you can use this theorem to just rule out if certain correlations are observed on given systems,
a whole class of dynamical models for a quantum system, sorry, for the system in question,
so you can rule out the local hidden variable models.
And likewise in this case, if you can set up an experiment where you're really sure,
and this is hard, but in principle,
where you can argue that the only mediator is gravity
between these two masses and they become entangled through it.
No matter what dynamical law specifically you want to use
in order to describe this mediator,
then you can rule out a whole class of classical theories for it,
which obey these general principles,
one being locality, in the sense of the locality of quantum field,
if you like, and the other one being the interoperability of information, which is this
constructed theoretic information principle that somewhat captures some intuitive properties
of information like systems that we expect to be true of bits and similar systems.
So that's quite exciting.
And I think it's kind of maybe the first example of a theorem that kind of goes beyond quantum
information in a genuine way.
So it's sort of fulfilling this expectation that was mentioned earlier.
that we've been asked to have this general set of theorems
that are actually more general,
the quantum information theory,
in the sense that they don't assume quantum theory,
specifically or any other dynamical theory,
just these general principles.
Good. So let me, I think I actually understood everything you just said,
but to check, let me try to say it back,
and you can tell me whether I got it.
I mean, there's a long-standing worry about quantizing gravity.
We haven't been able to do it, right?
People don't understand the full theory of quantum gravity.
And so some people have said, well,
maybe it's because gravity still is classical while everything else is quantum.
And one of the problems with testing that proposal experimentally is that nobody knows what it means.
Like no one has a theory, really, where gravity is classical and everything else is quantum.
So what you're saying is that even in the absence of a specific theory of classical gravity, quantum, everything else,
you can still test the idea based on these general principles.
and again, in principle, even if in practice it's very hard,
you've actually proposed a setup in which it could be done.
Yes, exactly.
And I think that's the, you emphasize the right things,
that it's precisely because there is such skepticism about the fact that,
you know, the laws that can describe gravity must be quantum or classical,
that it's important that we don't make any commitment to a specific dynamical model
to make a prediction, or at least to make this general.
statement. Then, of course, to make a specific prediction about the particular masses that you need
in such an experiment and so on, you can use a number of models. But you would like your conclusions
that you, you know, by observing entanglement, you are witnessing some non-classical effects in gravity
to be as kind of independent of these specific assumptions as possible. And I think we got
quite far in terms of how general these principles are because locality is a pretty general
principle, and it's weighed by both with quantum theory and by general activity and other theories
that we might expect plausibly to describe nature.
And then the interoperability of information is really obeyed by any theory that allows for
observables.
And we surely want a theory to be testable to allow for observers.
So in a sense, that's kind of also a general principle that we hold quite dear.
And you were honest about this, but just in case people didn't catch it, the particular
experiment that you're proposing, you're not necessarily saying is feasible in the short term,
but it's in principle thing that maybe some clever experimentalist can figure out a better way
to do something analogous to it. Yes, I think so this is about the particular realization
of this experiment. There have been a number of proposals in addition to ours. This proposal
was put forward by Sugato Bowes and his team in London.
And now a number of others are being, you know, investigated.
So in that sense, it's a non-trivial enterprise.
And in a way, it's exciting for that reason.
So the experimentalists are kind of now taking it seriously
and really trying to think hard of ways in which this could be brought into being feasible.
But the encouraging thing is, which was also something that excited people in the quantum gravity community,
is that the masses that you need for this kind of, to display this entanglement are smaller than Planck's mass,
which is the usual scale at which you expect quantum effects in gravity to become relevant.
And so in a way that was a surprise.
So it's 10 to minus 12 kilograms, which is a bit smaller than Planck's mass, not that small,
but still quite close to the current threshold of, you know,
what's the size of objects that we can put in quantum superpositions?
So in the sense, it's tantalizing.
And I think, you know, this might require a long-term effort,
but it's somewhat within reach, and that's very exciting to me.
Yeah, no, absolutely.
I'm like a big believer in trying to be.
figure out what is possible when it comes to quantum gravity in principle first experimentally,
but any kind of experiments that we can even contemplate are worth taking seriously and trying
to improve. And then I want to ask about one other domain of application to these ideas,
which is more macroscopic, this thermodynamics and information and work extraction story.
This is one I'm very interested in, but the idea that there are fluctuations on the microscopes,
on the microscopic scale, and somehow, I don't think we've talked about it in detail on the podcast,
and maybe this is not the place to get into it, but there's a set of claims going back to Maxwell's
demon that you can sort of interchange information for work, for, you know, extracting energy from a
system or for doing something useful. And I apologize for not having a better understanding of what
you've said about this, but I mean, I have the vague impression that Constructed theory is relevant here
somehow. Yes. So this is related to this generalization of the second law that I mentioned earlier.
So the general statement that's usually made when talking about the connection between
information theory and thermodynamics is, as you said, through the idea of Maxel's Demon
or more recently Silat-Engine and the work by Benetian.
and Lundauer.
So the idea would be that when you want to delete or erase information,
there has to be some fundamental thermodynamic cost to that task,
which is a logically reversible task,
because you want to send all possible states into one blank state.
And this particular step is actually fundamental in creating,
a thermodynamic cycle within things like the maxil-simon set up or the Ceylon engine set up.
And so somehow it was conjectured by Landauer and then more accurately proven by Bennett
that there is indeed an irreducible thermodynamic cost to the task of erasing a bit.
Now this goes through, it's a connection that somehow implies the number of assumptions.
and these assumptions could be spelled out in various ways.
And now there is a sense in which on the one hand,
if you describe everything in a completely reversible way,
so if you have a fully detailed dynamical model of the Silat engine or of Maxwell's demon,
then this statement, of course, if the dynamical laws are time-reversymmetric,
which usually are as far as phantom series concerned,
and you're not adding any other irreversibility,
then the statement almost follows from the simple fact that the laws are time revolves asymmetric.
So in that sense, when you're not putting heat anywhere by hand when you make an account
or what's going on in these kind of cycles,
then perhaps you don't need to appeal to Landau's principle to claim that this connection
between erasure and irreversibility is like an additional principle on top of whatever
else we have. And at the same time, if you then assume that you are in a macroscopic domain where
there is some fuzziness about, you know, your knowledge of the dynamical laws and you have some
heat source at any point during this cycle in the Cilad engine, then you just apply the second law
and it seems like you can obtain the same conclusion as Lundauer's principle. So in a way,
although this idea of connecting information theory and thermodynamics has been discussed,
a lot, there's still a lot of controversy there about how fundamental it is and whether it's
even useful because, you know, if we know all the dynamics, we don't need it. And if we know the
second law and we think it applies, we also don't need it. Now, in the case of this work that
I've been doing, you can connect information to your internal dynamics in a different way. And it remains
to be understood whether this other way that Landauer and Bennett were proposing,
could somehow be derived or understood in terms of this other way that I'm suggesting.
So it's kind of an interesting open question.
So the way that I'm suggesting there is a connection is that if you define a task,
which is to extract thermodynamic work out of a given system prepared in a number of possible states.
So, you know, you've got like, I don't know, a flywheel and it's got different possible.
dynamical states and these are your possible states out of which you want to extract work.
Or alternative, you've got an atom with different energy levels and you want to extract work
out of those.
Or more generally, a different system that we don't have to specify necessarily.
Then you can prove by using these general principles of constructor theory an interesting
statement, which is that these states out of which you can extract work must
be perfectly distinguishable. So distinguishable in the sense of single shot distinguishability
of quantum theory. So they must be for those who like quantum jargon, they must be orthogonal
or orthogonal subspaces or things like that. And this has to do with the fact that when you talk
about work extraction in the way that I'm envisaging here, you're thinking of the work extraction
to happen reliably. So there's a key element in the proof, which is that
you're thinking that the task of extracting work out of these possible set of states of a given system is actually possible,
which means that there is a constructor, which can be presented repeatedly with the substrate and do this task reliably.
And so there is an interesting connection between a set of states that you can use to perform what informally is called useful work in thermodynamics,
and a set of states that you can distinguish perfectly.
So any set of states that you can extract work from in this deterministic reliable way must also be a set of distinguishable states.
And that's, so that's a novel connection.
And it's interesting that it doesn't, to prove this result, you don't have to appeal to any entropy-like consideration or any scale-related consideration.
So it seems like this statement is free of the problems, let's say, that the other connection between information.
information and the thermodynamics has.
And perhaps, as I said, it would be interesting to investigate
whether the second law connection could be somehow rooted into this other connection.
And this is an open problem, which I'm kind of thinking about right now.
So it's kind of exciting.
Well, we like open problems.
We like being able to inspire the young kids in the audience to take all of their physics
and not just physics, but all of their academic projects inspired by the Mindscape podcast.
And the other thing, the other reason why I like this whole connection, one of the reasons why I like this whole connection between thermodynamics and information theory and work extraction is that there are at least claims or hopes that something like this happens in living cells, right, in living beings.
Like there's many attempts, including recent podcasts I've done, to link physics principles to how life works.
And this might be an example.
Is that too crazy or are you on that train also?
No, this is not crazy at all, at least from my point of view.
This was, I think, the original motivation of phenomenes.
So the view of envisaging a theory of universal constructors
or more special purpose constructors was indeed to,
define a set of principles that in the same way as thermodynamic principles can set limitations to thermal engines,
could also set limitations to biological systems.
So, and explain to us what both natural selection and artificial selection can do when exploring the possibilities of organisms that are fit for a specific environment.
And so we don't have a theory of that kind yet.
And it's a shame, I think, because there is a lot of physics in physics assumptions and physics considerations to be made within the theoretical biology studies that we've been, you know, as a scientific community in general, advancing so far.
in a way, I would say it's the next step to merge together the theory of information,
as we know it, quantum and classical, with the theory of thermodynamics,
would be like the next step in this program of building an overarching general theory for biological entities,
which you can regard in the most general way as programmable machines
that happen to have been produced by natural selection.
But of course, the forms of things that we see in a given biosphere right now are by no means exhaustive of what can be done.
And so the question is it would be very important also for technological developments to have a set of principles that can tell us exactly what are the limitations for machines that we might be able to synthesize artificially.
And so this kind of goes into the direction of artificial life.
all of these other things that are very interesting.
And although they're not my direct concern,
I'm hoping that some of these principles that we are conjecturing now
could be used for kind of a scope of this kind,
which was ultimately what phenomenon envisage.
So I'm hoping that he'd be happy if he could see this.
Well, I'm glad you're not being too ambitious,
just trying to understand quantum gravity and the origin of life.
You know, it's something to keep ourselves busy during our off hours.
Now, this is great. I think that, you know, it's wonderful to, when we're faced with these big problems,
sometimes you solve them just by being, just by persevering, right? Just by putting your nose down
and moving forward step by step. But sometimes you solve them by like trying to take a big leap sideways
and looking at things from a very different angle and maybe some new insights come out of that.
And you have to try it. You don't know it until you give it a shot. Yes. And on this note, I think
although some of these problems we mentioned,
I mean, they do sound as being very different from each other
and perhaps going in different directions.
There is a sense in which the way I see them,
they all stem from the same perhaps misconception
or the efficiency of the current way in which we look at things.
So in a way, it's one example,
if this thing that we're doing succeeds,
of finding how there is a common,
root to a number of problems that appear different. And once you shift, as you said, the perspective,
the logic of the solution is always the same. It just happens to be applied in different subfields.
And it's not the first time that this has happened. I think, again, I mean, the quantum theory
computation is always my reference because it's kind of the thing I know best. It's true that
methods of proof within the quantum theory computation often refer to this universality of
cubits.
So, you know, you have very different systems.
Maybe one is a many-body system in condensed matter physics.
There's a different system which involves photons and so on.
But once you reduce all of these different systems into a system of cubits, you can then solve
the problem there and then imply, you know, this is very far-reaching implications for all these
different fields.
And you may not even know about the details of those fields, but you can still make statements that are useful and quite far-reaching.
And I think in this case, we are noticing a similar pattern here.
And so counterfactual is helping us in a way in identifying commonalities between open problems and hoping to solve them in a way of just by switching to this different mode of looking and things.
Well, I think that's an inspirational place to wind up the conversation with the prospects of really making progress on some big problems.
So, Kiara Marlato, thanks so much for being on the Weinscape podcast.
Yeah, thank you so much for having me.
Free is great, but only if it's useful.
Free credit scores from some apps can differ by as much as 100 points from your actual FICO score that 90% of top lenders use when you apply for a credit card, personal loan, car loan or mortgage.
That can meet a higher interest rate, a bigger monthly payment, or
worse. Denied. My FICO gives you your actual FICO score. The score lenders use straight from the
company that created it. For the moments that matter, get the score that matters, your FICO
score. Visit MyFICO.com and get started for free today.
