« first day (5090 days earlier)      last day (136 days later) » 
00:00 - 14:0014:00 - 23:00

14:00
@qwerty Basically anything involving the big python libraries
most of the learning for python is learning how the libraries you use work
pragmatic learning
for example, it seems like i can frame a physical theory as an estimator of parameters, say the position of a ball subject to a range of conditions.
I'm afraid I have no idea what you're talking about
@SillyGoose this sounds like model testing?
An estimator - in the sense I know the term - is a function that takes a sample that is supposed to follow a certain kind of probability distribution and then outputs an estimate for some characteristic of that distribution (e.g. the sample mean is a common estimator for the expected value of an underlying distribution)
I don't see how this is supposed to be related to physics outside of the cases where physics makes a probabilistic prediction and you compare the observed sample to the expected distribution by using appropriate estimators
14:11
@qwerty yesh
@ACuriousMind well in say newtonian mechanics, if I throw a ball with initial $(x_0, v_0)$ subject to constant acceleration $a_0$, then I get a predicted trajectory $x(t)$ for the ball. Is this not a model describing the parameter "position of the ball" as following a time-dependent, distribution that says: certainly the ball will occupy position $x(t)$ at time $t$.
@SillyGoose no I don't think so? your parameter here is a_0
@SillyGoose if you absolutely want to you can say that, but what does that have to do with estimators?
well maybe i can frame it more generally. experiments measure values. a physical theory is meant to reproduce these values. measurements and physical theories are assumed to be not perfect, so actually a physical theory should only be expected to estimate the experimentally measured values. In this sense, a physical theory should be able to be framed as a theory of systematically constructing parameter estimators that are related to the class of phenomena the physical theory hopes to study.
whether it makes certain predictions (e.g. newtonian mechanics) or whether it makes statistical predictions (e.g. statistical mechanics) does not matter for the above observation, to my understanding
this is similar to the discussion NI Slereah and ACM had with me on how science works and popper vs bayesianism
@SillyGoose I think you understand something different under "estimator" than I do
14:20
the other week
Again, an estimator is something which you apply to a sample in order to get back some property of the underlying probability distribution that produced that sample
it's just not just a name for anything that gives you an approximate value (which is what "estimate" would mean colloquially)
here i am identifying the experimentally measured values as "the sample".
no you're not - you're saying the theory "estimates the experimentally measured values" (you above, verbatim)
but the estimator does not "estimate the sample", it uses the sample as input in order to estimate properties of the underlying distribution
I agree with ACM that estimator is the incorrect choice of word
hm i thought that estimation theory includes constructing a probability distribution which is meant to spit out as similar as possible distributions to what is observed in a sample.
14:25
but I think a theory is more general than a model
in your description, I would also argue for replacing "theory" with model...
@SillyGoose I mean the use of estimators consists of (at least) two steps: 1. Write down a statistical model with some parameters that you think could describe the process that produces your samples. 2. Find estimators that can estimate the parameters of that model from your sample data.
oh i think i see what is being said now
I'm still puzzled how you think this applies to physics outside of the instances where we do statistics and are interested in reconstructing the underlying distribution from observations
Physics may be heavily involved in that first step, but estimators are just one very specific kind of "fitting models to data" that one may use in the course of doing physics
usually you don't have statistical models and distributions and work with estimators, you just have a theoretical prediction and a bunch of data points with error bars and you do some regression fit mimizing $\chi^2$ or whatever
hm well then i guess i am curious what maybe a generalization of "parameter estimation" would be in the following sense. say you define a physical theory to be a triplet (1) state space, (2) differential equation(s), (3) observable space. out of all of known math there are infinite ways to choose a triplet $(S, D, O)$. But squinting enough, this seems in the same spirit as parameter estimation where you are fitting a model to some data by tuning parameters appropriately.
here, the parameters would be mathematical structures
Now that I think about it, the $\chi^2$ technique and other goodness-of-fit methods do conceive of the theoretical model as a kind of random distribution, i.e. "doing a $\chi^2$-minimizing fit" is an estimator
but this is an implementation detail of how we do experimental tests of theories, not an inherent property of the theory
@SillyGoose If I squint that much, my eyes are just closed :P
also that "definition" of physical theory is deeply questionable
we're not doing physics by having hundreds of highly mathematical models compete against each other to see who can fit the data best
14:41
well it seems quite hard to come up with just one that accomplishes that goal :P. but i am thinking if we did have two we would choose between them by seeing which fits empirical observations best
as much as I love mathematical physics, trying to pretend physical theories - the ones that actually exist in the world not the ones you wish there were - are anywhere close to being mathematical objects in any rigorous sense strikes me as deeply misguided
Hello,

A static load or a gradual load where the weight start from zero to 2 tonnes to break long bone and a sudden load or an impact load where we instantly put a 1 tonne load on a long bone, the force of both of these are the same. Correct?
@ACuriousMind well the triplet constructed I intended to be some toy model of the situation to see if any interesting insight could be gained, not so much to faithfully reconstruct reality
@SillyGoose yes, but...how often does that happen? The history of science is not the history of people developing theories in a vacuum then testing them against each other during experiment. For most of history, we've had a plethora of observations no one could explain and all the physicists were doing was trying to come up with any model that correctly predicted the strange things we observed
and then the great controversies were often things we can't even really follow today, such as the vis viva discussion where I still don't really understand what the philosophical hang-up was about "true quantities of motion".
@SillyGoose Yes, but even for a toy model I should have some chance of seeing how to extend it to reality
but in reality a physical theory is not an algorithmic thing, there is so much choice and ambiguity involved in when to do what kind of approximation and what to assume about the systems under consideration etc. that I think any attempt to pretend a physical theory is just some kind of mathematical object is just...wrong
it's not an oversimplification, it's a fundamental misunderstanding about how science is practiced
15:16
anyone wanna friendly debate on consciousness philosophies?
i will argue for the "consciousness is fundamental" side and u can argue for a different side
@SnoopyKid if the time interval is the same and the impulse is the same, the average force is the same
implulse = total momentum imparted to the long bone
15:45
If you want to see some actual examples of "Trying to fit theoretical values to experiments", you can look at the PPN approximation
That's basically how it works in GR
Alternatives to general relativity are physical theories that attempt to describe the phenomenon of gravitation in competition with Einstein's theory of general relativity. There have been many different attempts at constructing an ideal theory of gravity. These attempts can be split into four broad categories based on their scope. In this article, straightforward alternatives to general relativity are discussed, which do not involve quantum mechanics or force unification. Other theories which do attempt to construct a theory using the principles of quantum mechanics are known as theories o...
^example
In physics, precisely in the study of the theory of general relativity and many alternatives to it, the post-Newtonian formalism is a calculational tool that expresses Einstein's (nonlinear) equations of gravity in terms of the lowest-order deviations from Newton's law of universal gravitation. This allows approximations to Einstein's equations to be made in the case of weak fields. Higher-order terms can be added to increase accuracy, but for strong fields, it may be preferable to solve the complete equations numerically. Some of these post-Newtonian approximations are expansions in a smal...
^and the experimental values
@ACuriousMind At least a big part of it is the "permanence of conservation" kind of arguments coming from not realising that energy has extra ways to be transferred away, which is only to be expected from them being ignorant of. But that then leads to all kinds of "how can you say that something that is only sometimes conserved as being of any fundamental importance?" and then it goes into the argument over "fundamental"
@SnoopyKid no, and that is not how questions of that kind arise.
@SillyGoose even your statement here already assumes that there is time-independence, and just one single distribution to choose from.
@qwerty I don't understand why that ought to make you less patient with code than physics. SQL is not an ugly language; it can be quite nice to use even in raw form. However, you need to have its mindset, and the data must already be organised in a way that naturally fits the database. That is, if you already have the mindset for SQL, then the vast majority of the headaches come from someone having the data stored in a stupid architecture, rather than something inherent to SQL itself.
@qwerty oh dBeaver is quite new! It shouldn't be terrible to use?
16:11
@RyderRude thanks ryder
I think this is a good answer "if the time interval is the same and the impulse is the same, the average force is the same
implulse = total momentum imparted to the long bone"
@SnoopyKid that's an illusion of an answer, of course.
@SnoopyKid in general, we have : average force x time interval= momentum imparted
16:42
so what do you all think physics is all about :P
@SillyGoose ...describing the world around us?
constructing working models of nature
Does anybody know how exactly does the Wick's theorem change for complex scalar field?
Also, I know that the Feynman rules of complex scalar field theory have an orientation but I don't understand why: it wasn't the case for real scalar fields
@NairitSahoo I refuse to believe that any text would just state the Feynman rules with orientation without explaining what the orientation represents
@ACuriousMind It does. It just says that one represents the field and the other one is just the complex conjugate of that.
The incoming lines are the field and the outgoing ones are the complex conjugate of the field
I just don't see how that comes about...
What do you mean? You have to visually distinguish $\phi$ and $\phi^\dagger$, no?
choosing to do so by attributing an orientation to the diagrams is as arbitrary as choosing to represent the perturbative integrals with diagrams in the first place
16:53
@ACuriousMind do you think most participants of physics research today have their work centered around describing the world around us?
@SillyGoose usually a very specific and small part of it, but sure
well, I guess for some it's rather a very unspecific and big part of it if you're doing stuff like cosmology :P
most of them are just working on very down to earth stuff
like semiconductor or thermal isolation or optics
working on the theory of the mechanical properties of hot dogs
it has been challenging to find an idea that i can personally believe is worth pursuing. almost everything can be interesting, but few things seem to matter in the end.
but the average physics research is less about grand questions and more like "let's see if we can observe this weird prediction for some specific material", "let's see if we can make our laser pulses even shorter" or stuff like that
If you want things to matter you should have become an engineer :p
or work on something important and boring like meteorology
17:11
you're not gonna do anything to help mankind short-term by working on QFT or GR I fear
@SillyGoose for meow meow, physics is the study of how things move. How things actually move. Which includes how things stay stationary. But think about it, every phenomenon in physics is involved.
17:24
@ACuriousMind Hmm. Thanks. I was wording it wrong. I had a different problem actually: In real scalar $\phi^4$ interaction theory the term in the Lagrangian is $\lambda \phi^4/4!$, but for complex $\phi^4$ the term is $\frac{\lambda}{4} \phi^4$. Where does the factorial go? Is it because we can interchange four real $\phi~$s in $4!$ ways but for complex since there should always be two $\phi~$s and two $\phi^\dagger ~$ s, the total number of ways of indistinguishability is 2C1 * 2C1=4??
@NairitSahoo Your explanation is correct; the prefactor in the Lagrangian is chosen such that the diagram that consists only of the interaction vertex has amplitude $\mathrm{i}\lambda$ without prefactor - the factors $4!$ and $2\cdot 2$ are hence the symmetry factors associated with the interaction vertex as a Feynman diagram
18:09
@naturallyInconsistent Late reply, but I think part of the reason is that many students (myself included) are taught QM before Hamiltonian mechanics. Which is bizarre and makes the entire subject feel like a different beast from familiar classical physics
Add on to that the new linear algebra formalism (which some books like Townsend don't bother explaining in terms of linalg terminology) and it becomes pretty intimidating at first
Honestly I don't know how I only learned the Hamiltonian formalism when I got to grad school. It should've been a prerequisite to stat mech and QM
19:01
@SillyGoose i would say physics is expressing the patterns in the observable properties of the external world
observable is the key word. we experience the external world through the distorted lens of a human life. so we shouldn't expect to know everything about the external world
and we know that there do also exist unobservable things, e.g. the minds of other humans
 
1 hour later…
20:18
@naturallyInconsistent my issue isn't with the programming language. the only thing I've hated is excel :p. what I mean in general is that you can spend a lot of time optimising or learning how to optimise what already works "fine". not just the code itself but your workflow or tools too. it won't change the result but maybe it's easier to catch bugs or maintain or read. and there won't just be one or two ways but likely many ways. so if you just want it done rather than nice it can feel tedious.
@naturallyInconsistent it was ok til I ran into this github.com/dbeaver/dbeaver/issues/20866 where if you have a CTE then it doesn't tell you what line the error is in, which has made debugging slower
@naturallyInconsistent I've sometimes wondered to what extent the study of dynamical systems (applied to the observable world) and physics are synonymous. but I guess you can write DEs for non physical systems
@ACuriousMind specifically unspecific and narrowly big!
21:25
Could I have some confirmation that I'm not talking rubbish in this answer?
5
A: If we imagine tachyons do exist, then can they seem to travel slower than speed of light from a reference frame traveling slower than speed of light?

PM 2RingTachyon geodesics are space-like. Lorentz transformations always preserve the quality of a spacetime interval. Therefore, in any inertial frame, time-like geodesics are always time-like, light-like (null) geodesics are always light-like, and space-like geodesics are always space-like. So shifting...

Also,
@ShauryaKad Fair point. But if one tachyon has zero kinetic energy relative to another, their relative speed is infinite. But I Could Be Wrong. :D — PM 2Ring 7 hours ago
@PM2Ring the entire question is ill-founded because tachyons do not move faster than light, cf. physics.stackexchange.com/q/166095/50583
actually, that's a duplicate
@ACuriousMind Yeah, ok. I'm just working with the naive definition of tachyon, as given by the OP.
reading the answer to the original q reminds me I still need to figure out what the difference is between what people call "nonlocal" in different fields
en.wikipedia.org/wiki/Tachyon > A tachyon (/ˈtækiɒn/) or tachyonic particle is a hypothetical particle that always travels faster than light. Physicists believe that faster-than-light particles cannot exist because they are inconsistent with the known laws of physics.
@PM2Ring the thing is, this definition is simply inconsistent, as the answers to the question I linked show - QFT does not give you particles that follow spacelike geodesics in this way even hypothetically
21:41
@ACuriousMind I know it's inconsistent. And I'm not concerned about any quantum issues. I'm just attempting to give some kind of consistent answer about a body that follows a spacelike geodesic. Even though my brain rebels at the very notion of a body following a spacelike geodesic. :)
I mean the part where you say that because your tachyons have space-like geodesics, and being space-like is an invariant, every observer should see them as spacelike is right
the part where you talk about what a tachyon sees is questionable, because observers by definition follow time-like geodesics - we can't even really talk about what "a photon sees" in mainstream physics because there is no Lorentz transformation that would connect a momentarily co-moving frame with the frame of any other observer
@ACuriousMind Oh, good.
@ACuriousMind Yeah. I added that stuff later, just before going to sleep. I'll add a disclaimer based on your remark. Do you want me to mention your name?
don't worry about it, perhaps rather link to physics.stackexchange.com/q/29082/50583 for a demonstration that what a photon sees is also a debatable concept
21:58
@ACuriousMind Ok
perhaps, put quotes around "see"s
It seems strange that photons would not have a well defined reference frame
it is like how em fields due to a particle are not well defined at the location of the particle. Something we just work around but seemingly kind of a flaw 0.o
@SillyGoose NASA astrophysicist Marina Brozović works on solar system dynamics. Her latest work improves the precision in our model of the orbit of Pluto & its satellites. iopscience.iop.org/article/10.3847/1538-3881/ad39f0
Does that really matter? Maybe not. But Marina also works on asteroids, and her work may help to warn us if we're going to be hit by a killer asteroid.
@SillyGoose well, photons are all sorts of weird - as fully relativistic "particles" you can't localize them fully and they do not have a non-relativistic wavefunction; one of the annoying insights of particle physics is that the non-relativistic idea of a particle as being definitely localizable with some attached rest frame is just that - a non-relativistic idea :P
2
22:17
> First and foremost, never listen to anybody who tells you what you can and cannot do. Second, never pass up an opportunity for an interesting research project even if it takes you out of your "comfort zone." Careers span many decades these days and you want to remain curious and to keep on growing as a researcher.
22:38
An unusually colourful xkcd:
If any of you want to meet some cool local oxygen atoms, I can introduce you!
2
00:00 - 14:0014:00 - 23:00

« first day (5090 days earlier)      last day (136 days later) »