[HN Gopher] New quantum algorithms finally crack nonlinear equat...
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       New quantum algorithms finally crack nonlinear equations
        
       Author : theastrowolfe
       Score  : 97 points
       Date   : 2021-01-06 14:59 UTC (8 hours ago)
        
 (HTM) web link (www.quantamagazine.org)
 (TXT) w3m dump (www.quantamagazine.org)
        
       | dls2016 wrote:
       | > The new approaches disguise that nonlinearity as a more
       | digestible set of linear approximations, though their exact
       | methods vary considerably.
       | 
       | The idea of reducing a nonlinear problem to a sequence of linear
       | problems is the bread and butter of nonlinear PDE, both
       | theoretical and numerical. The trick is always in the reduction
       | and I guess here you want the reduction to have a nice "quantum"
       | solution.
       | 
       | I'm not qualified to say what either of these papers have to do
       | with "chaos". You'll notice that this word only appears in one of
       | the papers and then only once in the intro.
        
       | ur-whale wrote:
       | The article seem to imply that quantum computers are a solution
       | to the problem that non-linear differential equations are chaotic
       | (as in: tiny changes in initial conditions lead to vastly
       | different solutions).
       | 
       | My impression of quantum computers are they will allow us to get
       | to solutions to algorithmic problems _faster_.
       | 
       | I fail to see how they could possibly work around the chaos
       | inherent to some diffeqs (e.g. N-body problems).
       | 
       | [edit]:and after reading the article more carefully, I'm still
       | not sure how QC has _any_ effect on the chaotic nature of non-
       | linear diffeqs . All I see in here is that they 're trying to map
       | non-linear diffeqs to linear systems via approximations so they
       | can run it on a QC.
        
         | meroes wrote:
         | If you can map non-linear eq's to linear, i.e. Schrodinger eq,
         | doesn't that dramatically reduce computation required? Non-
         | linearity is necessary for chaos. This seems like a big deal to
         | an layman like me. I don't know _how_ it 's done, but isn't the
         | fact that nonrelativistic QM and classical mechanics are nearly
         | identical at certain scales enough to say a mapping can be
         | done.
        
           | rowanG077 wrote:
           | Did you read the article? It's possible to write a non-linear
           | equation as an infinite set of lineair ones. They use this
           | fact in one of their solutions.
        
           | ur-whale wrote:
           | The mapping is not 1-to-1, it's done via approximation, which
           | means that what gets solved is not the original equation.
           | 
           | And ... as I believe poincare found out when he tried to
           | apply series expansion to the 3 body problem, the devil
           | (chaotic behavior) is in the long tail of the series
           | coefficients
           | 
           | [edit]:
           | 
           | https://en.wikipedia.org/wiki/Poincar%C3%A9_and_the_Three-
           | Bo...
           | 
           | http://www.bourbaphy.fr/chenciner.pdf
        
         | prof-dr-ir wrote:
         | I believe you are right, and that the Childs paper actually
         | beautifully quantifies your suspicion: they appear to show that
         | the speedup of the quantum algorithm disappears if 'R >
         | sqrt(2)', which intuitively means that the problem is 'too'
         | non-linear. (I would expect that truly chaotic systems fall
         | into this category.) This negative result does not seem to be
         | mentioned in the quanta article.
        
           | conformist wrote:
           | Yes, they even state that the "quantity R is qualitatively
           | similar to the Reynolds number", which supports this
           | intuition.
        
         | marius_k wrote:
         | I am not sure if this is related but during the past year I
         | noticed few articles describing about how quantum systems are
         | immune to butterfly effect [0]. I can't tell more details as
         | those articles are still on my backlog.
         | 
         | [0] https://news.ycombinator.com/item?id=24167691
        
           | sampo wrote:
           | Time-dependent Schrodinger equation for the time evolution of
           | a quantum system is a linear equation.
           | 
           | Essentially: d/dt Ps = H Ps
           | 
           | There is no second, or higher, powers of Ps. There is even no
           | constant term. It's linear.
           | 
           | https://en.wikipedia.org/wiki/Schr%C3%B6dinger_equation#Time.
           | ..
           | 
           | Now, how does nonlinear macroscopic world appear, if the
           | fundamental time evolution at quantum scale is linear? So
           | obviously Schrodinger equation alone is not enough to
           | describe the time evolution of the universe. One way is to
           | introduce wavefunction collapse, which is a nonlinear
           | process. But there is no physical theory (well, there are
           | propositions) of how and when collapse happens. It just
           | happens somehow, sometime. This problem is at the core of why
           | quantum mechanics is an incomplete theory.
        
             | btilly wrote:
             | Your comment presupposes that the Everett interpretation
             | cannot be true. But it offers an explanation of the
             | appearance of collapse without having a collapse.
             | 
             | Namely if a quantum mechanical observer observes a quantum
             | mechanical system in a superposition of states, we get a
             | superposition of quantum mechanical observers who can no
             | longer meaningfully interact, each of which observed a
             | different state of the quantum mechanical system. This is
             | exactly what the Schrodinger equation predicts MUST happen.
             | 
             | As a side note, this is the most popular interpretation of
             | quantum mechanics among cosmologists. It turns out that if
             | you're using quantum mechanics to explain things like the
             | birth of galaxies, taking seriously what quantum mechanics
             | says for human sized quantum mechanical systems becomes
             | very easy.
        
             | tagrun wrote:
             | H can depend on Ps, which is why Bose-Einstein condensates
             | referred in the new article are nonlinear.
        
             | pontus wrote:
             | While the Schrodinger equation is linear, that doesn't mean
             | that the time evolution of various derived quantities are
             | also linear. For example, the expectation value of position
             | follows a nonlinear equation of motion even though the
             | schrodinger equation is linear.
             | 
             | This is known as Ehrenfest's theorem:
             | https://en.m.wikipedia.org/wiki/Ehrenfest_theorem
             | 
             | In other words, nonlinear time evolution is natural in
             | quantum mechanics for quantities other than the wave
             | function and does not require collapse.
        
               | prof-dr-ir wrote:
               | As your link shows, the time evolution of the expectation
               | value of position does in fact _not_ generally obey a
               | closed-form non-linear differential equation; instead one
               | needs the expectation value of V '(x) which is a
               | different quantity altogether. But the easiest way to
               | compute that quantity is of course to solve the
               | Schrodinger equation...
               | 
               | Edit: removed an accusation because I misread the
               | original comment.
        
               | pontus wrote:
               | Yes, that's right: you need <V'(x)> rather than V'(<x>).
               | It's still the case that <x> does not follow a linear DE.
               | 
               | My point was that while the SE is linear, that does not
               | mean that everything derived from it is also linear. The
               | original comment was asking where all the nonlinearities
               | in the world could come from since the SE is linear. It
               | was suggested that either QM is incomplete because it is
               | linear or that we need wave function collapse to
               | introduce nonlinearities. I think my counterexample shows
               | that both of those suggestions are incorrect.
        
             | Lichtso wrote:
             | I am quite sure chaos can be an emergent property.
             | 
             | E.g. think of Conways game of life: One could build a
             | contraption which amplifies a very small event into a
             | gigantic one (like a Geiger-Muller tube) and spawn a few
             | gliders (as particles). Now, a very small change in the
             | initial configuration changes the outcome drastically, even
             | though all the rules of the simulation are still perfectly
             | deterministic and linear.
        
             | prof-dr-ir wrote:
             | I do not think that you need to introduce wave-function
             | collapse here, because there is no need for the universe to
             | be fundamentally non-linear - it suffices for the Poincare
             | recurrence time to be extremely large.
             | 
             | Like phase transitions in statistical mechanics, could it
             | no be that chaos is just an emergent effect that arises
             | from the quantum dynamics of infinitely many particles?
             | (The appearance of non-linearities in that limit happens to
             | also be discussed in the MIT paper of the quanta article.)
        
           | btilly wrote:
           | This is true. My favorite such article is https://michaelberr
           | yphysics.files.wordpress.com/2013/07/berr....
           | 
           | In classical mechanics, small initial perturbations can have
           | an ever widening effect with exponential growth in
           | consequences without bound.
           | 
           | In quantum mechanics, the Schrodinger equation is linear.
           | There cannot be any exponential growth lasting forever -
           | there is a linear bound!
           | 
           | The field of quantum chaos is devoted to resolving this
           | apparent paradox.
           | 
           | The answer for a closed system is that the quantum mechanical
           | system can approximate the classical system very well for a
           | limited time. After that the quantum mechanical system will
           | start repeating itself and show some decidedly non-classical
           | behavior. This time is sometimes called the "quantum break
           | time".
           | 
           | The answer for an open system is that every interaction with
           | the outside environment can change the state of the quantum
           | mechanical system, and the appearance of chaos can then be
           | maintained for unlimited times.
        
         | conformist wrote:
         | Yes, essentially that's right (regarding Child's paper), as far
         | as I can tell. Child's article seems to be about a smart way to
         | approximate sufficiently dissipative, non-linear, n-dimensional
         | ODEs (or spatially discretised PDEs for that matter), such that
         | you can apply good old forward Euler. They do that in such a
         | manner that you end up solving a linear system for time-
         | stepping for which a log(n) quantum algo is known. This is
         | pretty cool, because they basically use standard numerical
         | analysis tools and manage to plug in the quantum computing part
         | to show that, e.g., as you increase the spatial "resolution"
         | with which you solve a PDE, the cost only increases
         | logarithmically. This feels useful from a computational fluid
         | dynamics perspective, say, if you're not interested in super
         | turbulent flows. So this is more about "how do we make solving
         | hard PDEs faster" than "finally cracking non-linear PDEs".
        
         | CyberRabbi wrote:
         | Right, even if they have implemented an accurate solver for
         | non-linear problems, that doesn't fundamentally get around the
         | chaos problem for a lot of real world applications.
         | 
         | For instance, even if you could 100% accurately model the most
         | complex turbulent flow models, your predictions are still
         | limited in their applicability because any small inaccuracy in
         | your initial data will cause the long term results to look
         | completely different from what may really happen.
        
         | tagrun wrote:
         | Physicists here. I'm having a hard time believing that you read
         | it carefully, because that's the Childs preprint, which is only
         | mentioned "in passing", and the true focus of this new article
         | is the Palmer (MIT) preprint, which is about mapping nonlinear
         | differential equations to nonlinear Bose-Einstein condensates.
         | BECs are modeled by the Gross-Pitaevskii equation, which
         | contains a potential term that is proportional to particle
         | density (basically a potential that depends on the
         | wavefunction), causing nonlinearity.
         | 
         | From the news article:
         | 
         | > The MIT-led paper took a different approach. It modeled any
         | nonlinear problem as a Bose-Einstein condensate. This is a
         | state of matter where interactions within an ultracold group of
         | particles cause each individual particle to behave identically.
         | Since the particles are all interconnected, each particle's
         | behavior influences the rest, feeding back to that particle in
         | a loop characteristic of nonlinearity.
        
           | gnulinux wrote:
           | > I'm having a hard time believing that you read it carefully
           | 
           | Excuse me, but I find this uncalled for. Not everyone has a
           | formal physics education. People who last studied physics in
           | high school 10 years ago will make mistakes even if they read
           | things carefully.
        
           | prof-dr-ir wrote:
           | There are two paragraphs dedicated to the Childs preprint and
           | then two to the Palmer preprint. As far as I can see, the
           | rest of the article consistently refers to 'both papers'. So
           | I do not think it reasonable to claim that the Childs
           | preprint 'is only mentioned in passing'.
           | 
           | Second, you missed a key quote: "So by imagining a pseudo
           | Bose-Einstein condensate tailor made for each nonlinear
           | problem, this algorithm deduces a useful linear
           | approximation." From this I conclude that the MIT paper does
           | reduce the computation to a linear system after all, as OP
           | suggested.
           | 
           | Third, let me offer some unsolicited feedback on the tone of
           | your comment: the phrase "I'm having a hard time believing
           | that you read it carefully" came across as needlessly off-
           | putting to me.
        
             | tagrun wrote:
             | I'll give you that it's a rather long passing, but title
             | and the overall news article is actually about Palmer's
             | work, and Childs paper is "in passing" in the sense that
             | it's a relevant recent work that parallels Palmer's work
             | ---I don't believe Childs preprint would be newsworthy on
             | its own.
             | 
             | Regarding the editorial "key qoute", if you read the
             | preprint https://arxiv.org/pdf/2011.06571.pdf you can see
             | this conflates two things: the mapping of nonlinear
             | differential equations onto BECs, and the emulation of a
             | BEC on a typical quantum computer (which introduces
             | additional limitations). Note that the latter step isn't
             | truly necessary, because one can use a BEC directly to do
             | it.
             | 
             | Third, I'm sorry about how you feel about it, but I stand
             | by my dissent that this can be a coherent statement:
             | 
             | > and after reading the article more carefully, I'm still
             | not sure how QC has any effect on the chaotic nature of
             | non-linear diffeqs . All I see in here is that they're
             | trying to map non-linear diffeqs to linear systems via
             | approximations so they can run it on a QC.
             | 
             | which mischaracterizes Palmer's work at best. I don't
             | believe anyone would be happy to have their work (be it
             | physics or software development) disparaged like this,
             | would you?
        
         | cosmiccatnap wrote:
         | No big deal, all they gotta do is solve p=np first!
        
       | fchu wrote:
       | I find it fascinating that we're using an overall linear model
       | (Quantum Physics) of our non-linear reality, particularly the
       | bits that are less linear (Bose Einstein condensates) to
       | approximate linear solutions to non-linear models (flow dynamics,
       | etc) of said non-linear reality.
        
         | ur-whale wrote:
         | To be fair, we're using a linear model (Schrodinger's Equation)
         | but in an _infinite dimensional_ vector space and linear
         | operators on these infinite dimensional vector spaces.
         | 
         | These aren't your grandfather matrices and there are things in
         | infinite dimension that are rather weird, specifically when it
         | comes to eigenvalues, which QM makes extensive use of.
         | 
         | The spectrum of an operator, for example can be a weird mix of
         | discrete values, discrete sets of intervals and/or the entire
         | real line.
        
           | selimthegrim wrote:
           | The typical paradox that leads to consideration of trace
           | class matrices is usually to consider the trace of the
           | commutator of putatively traceless operators.
        
         | adamnemecek wrote:
         | The inner space of our reality is linear.
        
       | GistNoesis wrote:
       | What is the mesmerizing image at the top of the article ?
        
         | r34 wrote:
         | I was just about to write a comment stating that Quanta (and
         | Nautilus as well) have amazing art in almost every article. One
         | of the best visualisations I encounter.
        
         | mankyd wrote:
         | Olena Shmahalo
         | 
         | https://twitter.com/natureintheory?lang=en
        
           | GistNoesis wrote:
           | Following your link I found the place where, in a few days,
           | the author will presumably post the description of what
           | Quanta requested a depiction of :
           | https://natureintheory.artstation.com/albums/762329
        
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