Also have you tried training activations to any extent? I'm going through this DL course and it was mentioned that you could use leaky ReLU and optimize the "leakiness"...though I suppose that's technically more model selection than training. Sounded like an interesting concept though
Yeah it was more of the hyperparameter even though I called it training...I wonder if there's a way to systematically include it in the loss or something
And saying lol to them saying no...it was meant to be a league joke though
I'm almost done with the first DL course in the sequence, which has gone by fairly quickly. Though this one is pretty much just overexplaining linear algebra
I built an autoencoder as a stand in for a RBM...since the dl4j peeps didn't support RBMs anymore on account of "everybody just doing autoencoders now"
Yeah I imagine I probably won't be able to breeze through the other courses quite as easily. I do really like the jupyter notebooks instead of matlab in his other course
Slow science is part of the broader slow movement. It is based on the belief that science should be a slow, steady, methodical process, and that scientists should not be expected to provide "quick fixes" to society's problems. Slow science supports curiosity-driven scientific research and opposes performance targets.
== See also ==
"Publish or perish"
== References ==
== Further reading... ==
I cannot see what can go wrong other than research will be so slow to fix urgent world problems
Do mathematical physicists conjugate the scalar on their bra's or kets when they take it out of an inner product?
I know pure physicists conjugate the scalar on the bra, and pure mathematicians conjugate the scalar on the ket, but I've no clue what someone from both camps will do.
say we've got a dielectric in a cylinder of length L, which has uniform polarization P inside. if we straddle the boundary with a square path, the line integral is PL. however, I'm unsure how to extract what the curl would be AT the boundary, which is what I'm trying to extract
the curl is everywhere else zero, inside and out, so I'm pretty sure it must have a delta function dependence
and unnecessary for me to say dielectric in a cylinder. just consider the whole thing a dielectric.
what does "dimensionless" in "dimensionless gauge coupling" mean? I have seen two places in which this phrase is used.
"... through the dynamical Higgs mechanism the W,Z-bosons acquire a mass via the Higgs condensate and at energies below a couple of 100 GeV they can no longer be excited from the vacuum and consequently the corresponding weak interactions freeze out. We are then left with only the electro-magnetic interactions between the quarks, leptons and the photon described by Quantumelectrodynamics and the strong interactions between the quarks and the gluons described by Quantumchromodynamics (QCD).
The parameters of the latter theory are the masses of the six quark flavours and the dimensionless gauge coupling."
the above is one place where I see "dimensionless gauge coupling".
@JohnRennie you mean dimensionless gauge coupling means the coupling is described only by constants (without any variables) so there is no dimension/degree of freedom involved)?
@JohnRennie but in Wikipedia the running coupling seems to be referred to as dimensionless gauge coupling, as in "There are many quantum field theories which, while not being exactly scale invariant, remain approximately scale invariant over a long range of distances.
Such quantum field theories can be obtained by adding to free field theories interaction terms with small dimensionless couplings. For example, in four spacetime dimensions one can add quartic scalar couplings, Yukawa couplings, or gauge couplings. Scaling dimensions of operators in such theories can be expressed schematically as Δ = Δ 0 + γ ( g ) $\displaystyle \Delta =\Delta _{0}+\gamma (g)$...
Generally, due to quantum mechanical effects, the couplings g do not remain constant, but vary (in the jargon of quantum field theory, run) with the distance scale according to their beta-function."
Well yes, the fine structure constant, and the other coupling constants, aren't actually constant because they change with energy. However they are dimensionless, and I would guess they are what is being referred to in your quote.
@JohnRennie Hm, it seemed unclear to me - I mean, I thought there was no indication of why the asker is not able to understand that the expression given in the question represents a Lorentz-invariant quantity. But I suppose that's not such a slam-dunk case that it calls for a mod hammer.
I'll reopen it but in its current form I would very much like to see the community put it on hold.
Also your comment there should have been an answer ;-)
@DavidZ I guess the OP is a beginner and doesn't understand much about SR. The question seems rather lacking in effort, but it seems reasonable to me. You'll note I've found a similar Q/A though it isn't a duplicate.
@JohnRennie I agree that the OP seems to be a beginner and not to understand much about SR, but we differ in that I don't think it's a reasonable question (at least not for this site).
I guess it's not immediately obvious to me why the inner product of two four vectors is a Lorentz scalar. Well, it is but only because I already know the answer. I mean for someone who doesn't already know the answer it's not obvious.
I can get behind that, but I would expect a bare minimum level pf effort to look up the answer. Even just reading a relevant Wikipedia page, or whatever happens to come up in the top few search results, should give some information the asker could have used to define the question better.
@ACuriousMind Hi, let me know when you're around for a tiny QM question. It's about how we compose Hilbert spaces, sometimes we have a macroscopic variable, say A, describing the properties of a subsystem S with Hilbert space H_S. The Hilbert space of the entire system can then be written as tensor product between H_S and H_R where H_R denotes the Hilbert space of the reservoir (i.e. remaining d.o.f's). But I've heard the composition is not always so. For example, (...)
@ACuriousMind (...) in a crystal, the long wavelength phonons can be considered as our subsystem S here, while the short wavelength phonons belong to the reservoir. Apparently, then, the Hilbert spaces are not just factors of the Hilbert space H of the entire space. Which begs to ask, why in this case we no longer have a relation like $H = H_S \otimes H_R$ ?
@danielunderwood I got a cool idea for something to do with GANs... could lead to a paper... you interested in working with me on it? You can be first author if we do write a paper and you do more of the work :P
My knowledge of them so far is pretty much "One NN generates samples and optimizes to create samples the other misclassifies"...or something like that?
I do have Goodfellow's section on generative algos open to read, but haven't read it yet
produce samples so real that it's impossible to distinguish
The issue that I have with a generic GAN though is that the input to the generator is just a noise matrix
you're supposed to generate an image starting with just noise
what I want to do, is to attach a RNN pre-processing pipeline to the input of the GAN so that instead I'm inputting some representation of a caption
and have the GAN reproduce the caption in an image
so basically reverse the image-captioning problem using RNN's attached to a GAN
I think it could be done, and I'm not aware of someone else doing it. Of course, we'd have to do a literature search to see if it's been done before...and if it has, we could improve on their architecture or something.
hmmm I've actually looked at a number of image classification resources in the captioning talk I'm looking through...though I didn't really know what I was doing at the time
All the cloud providers have some sort of new account credit (and I think AWS even has some sort of research credit)...though that will handle all of a day of GPU training
@user929304 I don't know anything about crystals, but if you e.g. just take the space of all photon states and partition it by wavelength, then the problem is that that space is already the sum of all finite tensor products of the one-photon space with itself
In that case, the total photons space is the sum of all finite tensor products of the "short wavelength one-photon space" with the "large wavelength one-photon space", but the one-photon space is not the tensor product of the two.
forget it then, I think it'd be too hard to come up with something more novel in that field atm lol
all my ideas are taken already grrr...I also thought up variational autoencoder for collaborative filtering...but lo-and-behold some research group already did it for netflix sonofabitch
Why is the scalar product of two four-vectors Lorentz-invariant?
For instance, given two four-vector $A^\mu$ and $B^\mu$, so their scalar product is $A\cdot B=A^\mu B_\mu=A^\mu g_{\mu\nu}B^{\nu}$.
Why is $A^\mu g_{\mu\nu}B^{\nu}$ Lorentz-invariant?
The formula should optimize for quality, on many sites it actually optimizes for controversy, and on ours it often optimizes for rather basic questions because many physicists love trying to explain the basic things in their own words...
I've told to come here by another user after my question was put on hold a few days ago for being "off-topic".
What does "conceptual" mean? It's a word I see floating around a lot on this site and it's never explained. Ever. I asked the aforementioned user what it meant and they directed me here...
With due apologies for the unilateral action - I really don't think that this is a duplicate. There's a lot to criticize here in AustereTiger's complete disregard to reading the site policies before going on to rudely dismiss and criticize things s/he hadn't even attempted to understand, despite explicit pointers to go and read $-$ but the way to deal with those flaws is to downvote. Or can the close-voters explain why they think that this is an exact duplicate? — Emilio Pisanty8 secs ago
@danielunderwood maybe we should be more ambitious and work on "sparse attention"...unfortunately it's a super vague concept and I don't see a clear path forward unlike the GAN concept lol.
the upshot is, because it's so vague, there's no chance someone already "did it"...since we can always just work on the part that's "not done"
I was gonna devote research to this area at openai, but since they rejected my application I guess that's not gonna happen
This is evidenced by games like montezuma's revenge where you have to take a lot of steps, get keys, find items, etc., before getting to your goal.
I think the current method to work around that problem is by "reward shaping" in the sense of putting intermediate rewards for intermediate actions that lead to the goal action.
guys, temperature is defined with the volume of the system held fixed. i'm confused then why the thermometer's operational definition works, since the liquid is expanding?
@ACuriousMind Hi, you've perfectly captured what I m trying to understand, and your photon example stands as equivalent to mine (for the purposes of these discussions). I'm still struggling to understand the part where we say "...is already the sum of all finite tensor products of the one-photon with itself." Could you please explain this part at a much more basic level? What is different about partitioning a space according to wavelength here, as opposed (...)
(...) to partitioning according position and spin where then we can take a tensor product of the two (assuming here there are position and spin operators, even though they can be tricky matters for photons).
uhm, I know the definition of enthalpy, and.. all I know is that when we consider internal energy in our thermal physics course, we usually think of thermal energies, because we want to work with the equipartition thm
but I think free energies will be treated soon, I think I saw it somewhere
@user929304 Alright, I'll try: 1. There is a one-photon space of states $H_1$, with a momentum (=frequency=wavelength, for photons) basis $\lvert p\rangle$.
2. The space of "all photons states" is $H_\text{tot} = \sum_{i = 1}^\infty \left( H_1^{\otimes i} \right)$, which is the space of states with arbitrarily (but finitely) many photons.
3. We may partition the one-photons space at some arbitrary momentum $p = p_0$ into two summands $H_1 = H_{1+} \oplus H_{1-}$, where $H_{1+}$ has as its basis all states $\lvert p\rangle$ with $p>p_0$ and $H_{1-}$ all states with $p<p_0$ (I don't care what you do with $p=p_0$, put it whereever ;) ).
then hypermarameter tuning is good for learning how to generally go about training the models, and there's a course on structuring ML projects to learn how to do that
4. Note that it is not the case that $H_1 = H_{1+}\otimes H_{1-}$. This is because $H_{1+},H_{1-}$ are not subsystems of the one-photon system - if you measure a single photon's momentum, it's always either in $H_{1+}$ or in $H_{1-}$. For true subsystems, you should be able to measure a state of both subsystems for every measurement.
well, I haven't seen how to compute the temperature of a liquid anyways. we've only treated (einstein) solids, low-density (monatomic) gases, and paramagnetic materials, because we can find explicit expressions for $S$
@Semiclassical yea, I'm getting this idea that heat capacity is partly defined just because it's so useful in experiments
as opposed to some of the more theoretical definitions
5. However, the tensor product is distributive: $H_\text{tot} = \bigoplus_{i = 1}^\infty \left( H_1^{\otimes i} \right) = \bigoplus_{i = 1}^\infty \left( (H_{1+} \oplus H_{1-})^{\otimes i} \right) = \bigoplus_{i = 1}^\infty$ Now $\left( H_{1+} \oplus H_{1-}\right)^{\otimes i} $ expands to a sum of $i$-fold tensor products where $H_{1+}$ and $H_{1-}$ occur in all possible orders. The sum over those then is the "sum of all possible tensor products of the short and long wavelength space".
@enumaris yeah I'm really interested in the structuring one. Like I'm comfortable with structuring normal software, but ML stuff always seems to not really fit into the same type of structure
It's not nearly as structured as software dev though...like agile or sprint or w/e other models you're gonna try to use. I suppose you could implement those models to ML, but that's not really what is gone over in that course.
@ACuriousMind point 5. will take me a while to digest, but if I may already go back to what was said upto point 4.: what is the meaning of \oplus? I only knew about \otimes (tensor prod) for composing Hilbert spaces, (e.g. Hilbert space of 3d position of a particle being written $H= H_x \otimes H_y \otimes H_z$ where $H_i$ is the space of the ith position component. I understand now what was meant by "that kind of partition not being really a partition into true subsystems".
@user929304 It's the direct sum. It's the more straightforward way to combine vector spaces - the direct sum of an n-dimensional and an m-dimensional vector space is just an $(m+n)$-dimensional vector space.
Andrew goes over like the stages of a ML project - inception, getting a data set to work with, building a simple model, refining, diagnosing the model...stuff like that
how to actually structure the code is not gone over
@ACuriousMind simple example: If you think of your first vector space as "degree n-1 polynomials in x" (an n-dim vector space) and your second as "degree m-1 polynomials in y" (an m-dim vector space)
@ACuriousMind ah I see! I still don't get (from a very naive pov) why $H_1 = H_{1+}\oplus H_{1-}$ and not $H_1 = H_{1+}\otimes H_{1-}$ ... :( in other words, what kinds of partitionings of a space lead to an $\oplus$ composition as opposed to $\otimes?$ (in the context of QM and Hilbert spaces)
My code is structured into the level of classes...but I haven't actually had to deal with class inheritance much for example. Since I haven't had to write a whole framework like Keras. I expect that as I write more of my RL library, I will have to get into that game more.
@user929304 Maybe it helps to think in terms of bases: If you take a space $H$ and a basis $v_i$, then you can split the basis into two sets (e.g. by taking one set to be the $v_i$ up to $i < i_0$ for some $i_0$, and the other the $v_i$ starting from $i \geq i_0$.). The two sets span two subspaces and the total space is their direct sum. Take for instance $\mathrm{R}^3$ - it is the direct sum of the 2d space spanned by the $x$ and $y$ basis vectors and the 1d space spanned by the $z$ basis vector.