[HN Gopher] Understanding Gaussians
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       Understanding Gaussians
        
       Author : lapnect
       Score  : 133 points
       Date   : 2024-10-22 07:54 UTC (15 hours ago)
        
 (HTM) web link (gestalt.ink)
 (TXT) w3m dump (gestalt.ink)
        
       | youoy wrote:
       | Thanks for sharing! The Gaussian distribution never gets old. And
       | nice plot of this:
       | 
       | > 100 000 points drawn from a Gaussian distribution and passed
       | through a randomly initialized neural network.
       | 
       | It gives you a sense of how complex the folding of the space by
       | NNs can be. And also the complexity of the patterns that they can
       | pick up.
        
       | wodenokoto wrote:
       | > You can see that the data is clustered around the mean value.
       | Another way of saying this is that the distribution has a
       | definite scale. [..] it might theoretically be possible to be 2
       | meters taller than the mean, but that's it. People will never be
       | 3 or 4 meters taller than the mean, no matter how many people you
       | see.
       | 
       | The way the author defines definite scale is that there is a max
       | and a minimum, but that is not true for a gaussian distribution.
       | It is also not true that if we keep sampling wealth (an example
       | of a distribution without definite scale used in the article),
       | there is no limit to the maximum.
        
         | klysm wrote:
         | I think he's saying that the distribution of human heights has
         | definite scale, not the Gaussian?
        
           | deepnet wrote:
           | Jinlian (1964-1982) of China was 8 feet, 1 inch (2.46
           | centimeters) when she died, making her the tallest woman
           | ever. According to Guinness World Records, Zeng is the only
           | woman to have passed 8 feet (about 2.44 meters)
           | 
           | Mean from article 163.
           | 
           | So the facts check out.
           | 
           | Author is correct.
           | 
           | Also very interesting the suggestion that human height is not
           | Gaussian.
           | 
           | Snip :
           | 
           | " Why female soldiers only? If we were to mix male and female
           | soldiers, we would get a distribution with two peaks, which
           | would not be Gaussian.
           | 
           | "
           | 
           | Which begs the question what other human statistics are non
           | Gaussian if sexes are mixed and does this apply to other
           | strong differentiators like historical time, nutrition,
           | neural tribes ?
           | 
           | Statistics is highly non-trivial. "
        
           | nwnwhwje wrote:
           | Nothing is Gaussian then. What probability distribution
           | allows for Graham's Number to be a possibility?
        
           | dekhn wrote:
           | Human height (by gender) very nearly follows a gaussian
           | distribution- because height is determined (hand-wave away
           | complexity) by a sum of many independent random variables. In
           | reality it's not truly gaussian for a number of reasons.
        
         | shiandow wrote:
         | It's an oversimplification but at some point there is really no
         | difference between impossible and 'incredibly small
         | probability'.
         | 
         | I mean sure it is possible for all air molecules to randomly
         | all go to the same corner of the room at the same time (heck it
         | is inevitable in some sense), you can play it back in reverse
         | to check no laws of physics were broken, but practically that
         | simply _does not_ happen.
        
           | KK7NIL wrote:
           | > at some point there is really no difference between
           | impossible and 'incredibly small probability'.
           | 
           | This is not true.
           | 
           | Using your air molecules example: Every microstate (i.e.
           | location and speed of all the molecules) possible under the
           | given macrostate (temperature, number of molecules, etc) has
           | a probability of happening of 0, but aren't impossible,
           | simply because the microstates are real variables and real
           | numbers are uncountable. Impossible microstates also have 0
           | probability but are obviously not the same.
        
       | mhh__ wrote:
       | https://gregorygundersen.com/blog/2020/04/11/moments/
        
       | lamename wrote:
       | > The best way to do that, I think, is to do away entirely with
       | the symbolic and mathematical foundations, and to derive what
       | Gaussians are, and all their fundamental properties from purely
       | geometric and visual principles. That's what we'll do in this
       | article.
       | 
       | Perhaps I have a different understanding of "symbolic". The
       | article proceeds to use various symbolic expressions and
       | equations. Why say this above if you're not going to follow
       | through? Visuals are there but peppered in.
        
         | Torkel wrote:
         | Agree. This text relies heavily on traditional mathematics to
         | define and work through things. It's quite good at that! But it
         | does become weird when it starts out by declaring that it won't
         | do what it then does.
         | 
         | It also felt like this could be a good topic for a 3b1b
         | video... and... here's the 3b1b video on gaussians:
         | https://www.youtube.com/watch?v=d_qvLDhkg00
        
       | hughw wrote:
       | Gaussian, Gaussian, Gaussian. Important to understand Gaussians,
       | but also to recognize how profoundly non-Gaussian, in particular
       | multimodal, the world is. And to build systems that navigate and
       | optimize over such distributions.
       | 
       | (Not complaining about this article, which is illuminating).
        
         | photochemsyn wrote:
         | A particularly interesting case is Maxwell-Boltzmann
         | distributions of the speeds of molecules in a gas in a 3D
         | space. Even though the individual velocities of gas molecules
         | along the x, y and z directions do follow Gaussian
         | distributions, the distributions of scalar speeds do not (since
         | the speed is obtained from the velocities by a non-linear
         | transformation), resulting in a long tail of high velocities,
         | and a median value less than the mean value.
         | 
         | Incidentally human expertise and ability seems to follow the
         | Maxwell-Boltzmann model far more than the Gaussian 'bell curve'
         | model - there's a long tail of exceptional capabilities.
        
         | slashdave wrote:
         | There was an opportunity when heights of soldiers were
         | discussed. Gaussians have infinite extent, but soldier heights
         | must be positive.
        
           | hughw wrote:
           | Good example
        
       | mjhay wrote:
       | Great article, but I wish it would have made a more explicit
       | mention of the* central limit theorem (CLT), which I think is
       | what makes the normal distribution "normal." For those not
       | familiar, here is the jist: suppose you have `n` independent,
       | finite-variance random variables with support in the real numbers
       | (so things like count R.V.s work). Asymptotically, as
       | n->infinity, the distribution of the mean will approach a normal
       | distribution. Usually, n doesn't have to be big for this to be a
       | reasonable approximation. n~30 is often fine. The CLT extends in
       | a
       | 
       | To me, this is one of the most astonishing things about
       | probability theory, as well as one of the most useful.
       | 
       | The normal distribution is just one of a class of "stable
       | distributions," all sharing the properties of sums of their R.V.s
       | being in the same family.
       | 
       | The same idea can be generalized much further. The underlying
       | idea is the distribution of "things" as they get asymptotically
       | "bigger." The density of eigenvalues of random matrices with
       | I.I.D entries approach the Wigner Semicircle Distribution, which
       | is exactly what it sounds like. It plays the role of the normal
       | distribution in the very practically-promising theory of free
       | (noncommutative) probability.
       | 
       | https://en.wikipedia.org/wiki/Wigner_semicircle_distribution
       | 
       | Further reading:
       | 
       | https://terrytao.wordpress.com/2010/01/05/254a-notes-2-the-c...
       | 
       | *there's a few normal distribution CLTs, but this is the
       | intuitive one that usually matters in practice
        
         | abetusk wrote:
         | Good for you for stating the assumptions properly that go into
         | the CLT and for mentioning other stable distributions.
         | 
         | I disagree about the Gaussian being the "normal" case or the
         | "one that usually matters". Finite variance is a big assumption
         | and one that's routinely violated in practice.
         | 
         | For those that are interested, Levy-stable distributions are
         | the general class of convergent sums of random variables [0],
         | synonymously called "fat-tailed" or "heavy-tailed"
         | distributions and include Pareto [1] and the Cauchy
         | distributions [2].
         | 
         | Is there an intuitive explanation for why the Wigner
         | semicircular law is basically the "logarithm" the Gaussian in
         | some respect?
         | 
         | [0] https://en.wikipedia.org/wiki/L%C3%A9vy_distribution
         | 
         | [1] https://en.wikipedia.org/wiki/Pareto_distribution
         | 
         | [2] https://en.wikipedia.org/wiki/Cauchy_distribution
        
           | CrazyStat wrote:
           | "Normal" in the context of the normal distribution actually
           | derives from the technical meaning of normal as
           | perpendicular, like the normal map in computer graphics. The
           | linguistic overloading with normal in the sense of usual or
           | ordinary is an unfortunate coincidence.
        
         | mturmon wrote:
         | > ...most astonishing things about probability theory...
         | 
         | It's a core result, perhaps _the_ most useful core result of
         | standard probability theory.
         | 
         | But from some points of view, the CLT is not actually
         | astonishing.
         | 
         | If you know what Terry Tao (in the convenient link above) calls
         | the "Fourier-analytic proof", the CLT for IID variables can
         | seem inevitable, as long as the underlying distribution is such
         | that the moment generating function (density Fourier transform)
         | of the first summand exists.
         | 
         | I'd be interested to hear if you have sympathy with the
         | following reasoning:
         | 
         | The Gaussian distribution corresponds to a MGF with second-
         | order behavior like 1 - t^2/2 around the origin. You only care
         | about MGF behavior around the origin because, as N -> \infty,
         | that's all that matters.
         | 
         | Because of the way we normalized the sum (we subtracted the
         | mean), the first-order term in the MGF will vanish. We
         | purposely zeroed it out by centering the sum around zero. That
         | leaves the second-order term, which will give a Gaussian
         | distribution.
         | 
         | So in short:                   - MGF of one summand exists =>
         | MGF of (recentered) sum exists         - We have an expression
         | for the MGF of the recentered sum (convolution property)
         | - Only the MGF behavior around the origin matters         - We
         | re-center the sum, causing the first-order term to vanish
         | - We invert the resulting MGF and recover the Gaussian
         | 
         | I'm not being precise here, but I hope the idea comes through.
        
       | dian_hacks wrote:
       | > If we want to stretch a function f(x) vertically by a factor of
       | y, we should multiply its input by 1/y: f(1/y x)
       | 
       | I didn't quite follow this part.
        
         | FabHK wrote:
         | Possibly the author meant "horizontally".
        
       | brcmthrowaway wrote:
       | Now explain Gaussian splatting
        
         | CamperBob2 wrote:
         | He never gets as far as splatting, but if you follow the links
         | on the page you eventually end up at a really nice set of
         | lecture notes on Gaussian diffusion:
         | https://dlvu.github.io/pdfs/lecture11.diffusion.annotated.pd...
        
       | tylerneylon wrote:
       | I like the font, images, and layout of this article. Does anyone
       | happen to know if a tool (that I can also use) helped achieve
       | this look?
       | 
       | Or if not, does anyone know how to reach the author? I may have
       | missed it, but I didn't even see the author's name anywhere on
       | the site.
        
         | generuso wrote:
         | The author is Peter Bloem, and the html is compiled from these
         | sources: https://github.com/pbloem/gestalt.ink
         | 
         | with the help of mathjax: https://www.mathjax.org/
         | 
         | The font seems to be Georgia.
        
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