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03:02
are there any affordable materials that could be used as a filter to measure presence in air of diameter 2.5 μm particles?
 
3 hours later…
05:44
@ACuriousMind I feel like this sort of implies (even tho I know it doesn't) that there is some macroscopic properties about light that cannot be derived from each individual photon that makes up the light
 
2 hours later…
07:21
@LeakyNun there is a difference between "this property cannot be derived from the notion of individual photons" and "this property is a property of the collective state and not of the state of individual photons"
as an analogy: Temperature is a property of statistical systems, not of the individual particles of which they consist
but that doesn't mean "temperature cannot be derived from each individual particle" - the behaviour of the macroscopic systems is derived from the microscopic dynamics
likewise, definite phases are a property of coherent states, not of individual particle states. That doesn't mean you can't derive the properties of coherent states from the properties of the single-particle states
08:14
@PM2Ring yes. I think this experiment shows that mental states are different from what can be described using mathematical systems like physics models
But we shud also note that, as shown in the "responses" section, most physicalists agree with this. Those physicalists just differentiate between "linguistic physicalism" and "physicalism"
Physicalism generally means that everything, including mental states, is "physical stuff". So mental states can still b physical stuff while also not being contained in linguistic structures like information bits or physics models
But then, idk what the definition of "physical stuff" is supposes to b here. I think they're just defining "everything thay exists" as "physical stuff"
In that case, "physicalism vs idealism" is just a matter of semantics imo.
But the real meaningful conclusion here is that mental states are not contained in linguistic structures like mathematics. This is what even most physicalist agree with in their response to "Mary's room"
09:00
@JohnRennie hi
Sir do we require quantum transistor as well to make quantum computer
How the transmission of such wave work I mean it is quite confusing to understand how a computer will look like
09:15
@ACuriousMind hi
Anything to add?
@JackRod I don't know, sorry :-(
I know next to nothing about how quantum computers are built.
@JohnRennie ok
09:49
Looking into Puthoff's polarizable vacuum's theory of gravity for fun
Apparently invalidated by the earth rotation rate experiments
 
2 hours later…
12:00
fun part is, while crazy people have used his theories to push weird ideas, Puthoff didn't even think it was a serious theory?
He just considered it as a pedagogical tool
12:16
@RyderRude IMHO, even if we knew that the qualia of red happens when some particular chunk of brain hardware "runs" some specific chunk of software, that still doesn't help us to explain what the qualia of red feels like to someone who's never experienced it.
We have a similar problem with less abstract stuff, too. Eg, We could describe an apple as a list of different molecules in some geometrical arrangement. But that description is hard for a human to assimilate. It wouldn't be a very helpful way to describe an apple to someone who's never seen or tasted one.
So even though we can reduce stuff to fundamental physics, we generally need to look at stuff at a higher level of abstraction. Similarly, when we want to understand a piece of software we read the source code, not the machine code.
If we only knew more about the brain...
I'm a brain
you can ask me
Speaking of quantum computing, Scott Aaronson recently gave GPT-4 a quantum computing exam. It managed to score a "B", but made some weird mistakes that a human would be very unlikely to make. scottaaronson.blog/?p=7209
2
Oh apparently Eric Davies, crazy man, is a friend of Puthoff
So maybe Puthoff is to blame
What was so special about Einstein's 🧠
12:29
@user85795 Maybe. But my point is that explanations in terms of brain structure and function are of limited usefulness if they're too complicated for a human to understand.
We can't even understand the brain of a fruit fly.
@PM2Ring so, in ur opinion, the information about qualia has been conveyed in physics. It's just that it's not practically useful for a human to get an idea of qualia. But an extremely intelligent Mary would be able to assemble the information and get an idea of what the qualia is
I mean a fiction-level intelligent Mary. She wud be able the assemble the information
I personally believe that we can nevr get an idea of what shape something is by the information about the set of points. We can know the shape from the set of points only if we already know what shapes mean becuz we r familiar with shapes
Like, if u have an equation describing a set of points... there is no shape in there. U can only map it to a shape becuz u already know what shapes mean
"Shape" is an inexplicable qualia here
12:50
holy smokes
Is this bot activity
looks legit
What are the advantages and disadvantages of being Solipsist in your experience? @ACuriousMind @Slereah
I tried being Solipsist today. One disadvantage is that u can feel alone even in a room full of close people
One advantage is that u r more spontaneous
Solipsists feel alone imo
It can also lead to less empathy but im not sure. I think prolonged belief in solipsism may do that
@RyderRude I said "Even if". We can get a rough idea of brain regions associated with sensory experience via functional MRI, but it's still pretty crude. But my main point is that our brains can't understand stuff if its complexity is too high. In particular, we can only understand stuff that's simpler than our mind / brain. And even then the information has to be arranged carefully or we can't assimilate it.
@NiharKarve Extremely likely to be LLM output, not only because of the timing, but also because of several characteristic repeated formulations across different answers (e.g. watch out for last paragraphs starting with "In summary,")
13:03
@PM2Ring u r again talking about the Godel stuff :P. If the Godel stuff applies, this also means we shud be able to understand the qualia of less complex organisms, in principle. But in practice, it would still b impossible
@PM2Ring I personally believe that mental states are their own thing, and are only correlated to the mathematical models of the universe's ontology. But we shud also note that there may not be any final mathematical model. This would mean that any correlations are always approximate.
@RyderRude Kind of, but it's simpler than Gödel's theorem. This is just about the limitations of finite systems, whereas Gödel's theorem involves infinite sets. OTOH, Hofstadter discusses this stuff in Gödel, Eschet, Bach.
I mean that it may even be meaningless to talk about an exhaustive mathematical description of the brain
@ACuriousMind you're right, on closer reading
I mean that there is no reason to expect mathematics or language to exhaustively describe all that exists. Mathematics has its own place in real-world applications, but there has never been an indication that mathematics sits at the root of everything
@RyderRude Yeah, shapes is a good topic. I might understand a lot of the geometry of a tesseract (a 4D hypercube), and look at apps & anims illustrating it. chat.stackexchange.com/transcript/71?m=57912812#57912812 But I don't feel that I can understand what the shape of a 4D structure is really like.
13:12
@RyderRude I don't know what that means. I don't choose my beliefs about the world based on how they make me feel, I can't "try solipsism": Either I already believe solipsism is true and then I cannot stop believing it any more than I can stop breathing, or I don't believe in it and I can't "try believing" in it any more than I can start breathing water
That you can "try being solipsist today" suggests to me that you have a fundamentally different idea of what believing in something means than I do
Ooh yeah. Belief would mean something more permanent :P. Maybe i didnt believe in solipsism today. I just pretended
Becuz ofc, i doubt solipsism. So i dont believe in it
@PM2Ring yeah. That animation looks completely 3D to me
I've seen some mathematicians say that they've trained themselves to visualise 4D. But idk. I think they've bought into their own hype :P
The closest thing I can do to visualise 4D is to imagine four intersecting planes.
Like the corner of a room, but there are four planes
@ACuriousMind Well obviously you're not a pragmatist
I don't think there's technically any issue in visualizing 4D in your mind
I'm not sure it's possible but on a formal level there isn't really any objection to it
Your brain just receive discrete informations from your eyes, there's nothing fundamentally three dimensional about how you perceive vision
Yeah. Becuz the mind picture is 2D anyway. And still, it gives u an idea of 3D
All the 3D reconstruction is done at the processing level
@RyderRude ...what do you mean, "the mind picture is 2D anyway"
13:22
Although learning to manipulate 4D images, idk how you'd do it
This is the idea i use in visualising the room corner with four planes. I just use the trick my brain uses for 3D
are you one of these people who can't rotate a cube in your mind's eye
@ACuriousMind You're only seeing a cube on the projective plane you fool
I mean the picture is still 2D. It's like how you can draw a cuboid on paper
of your mind's eye
13:23
well, in that sense you could argue we never see 3d anyway
you don't even need to add "in our minds"
Yeah, this is y Slereah says there's no fundamental restriction to 4d
Different reason
What was ur reason? @Slereah
see above
U said something about discrete information. Do u mean bits?
Like the image converted to binary
13:25
no, just how vision is processed
you just have points of lights from the optic nerves being sent to your brain
Your brain doesn't know how those are positioned with respect to each other
@RyderRude without getting into details about vision you're just receiving "hey, there's this color here: <color information>" from a more-or-less 2-dimensional surface at the back of your eyes
the "3d" part is entirely constructed in the brain, that's why there's all these funny visual illusions where equally sized 2d objects can appear in different sizes because they trick the part of your brain that does the perspective processing
We're lucky enough that most objects in the world are rigid
I personally use the trick my brain uses to make me feel the 3D corner of the room. My brain uses 120 degree angles with some depth perception. So i use almost 90 degree angles with some depth stuff to visualise 4D corner of room @ACuriousMind @Slereah
Might be hard to reconstruct how space works otherwise
what
(to both preceeding messages :P)
13:29
Like u can get a feel for 3d co ordinate system on a 2d paper by drawing 3 lines at 120 degrees from a point
So they r never at 90 degrees.
If objects constantly deformed you'd have a hard time having a 3D idea of what they look like :p
But u gotta pretend they have some depth that makes them 90
Imagine trying to make a model of a cube in your mind if it deformed as you rotated it
@RyderRude oh, you're talking about an isometric projection
@ACuriousMind I know you're familiar with isometric 3D
13:31
Yeah. I use this stuff to get a feel for 4d room corner
But i cant manipulate 4d objects. Its just a static image
But perhaps we can have 4D dreams. It would b cool to navigate such a room
@Slereah sure, but I think if I think about 3d "abstractly" I actually see the typical projection from drawing 3d diagrams in vector algebra or whatever, i.e. oblique projections
I don't think my mind's eye operates in isometric projection :P
@ACuriousMind I just meant from RPGs
Don't you think in little scenes from Disco Elysium
the visuals are the least important part of the typical DE scene
I dunno
the voices in my head just use the textbox without accompanying visuals :P
more limbic system screaming at me, less Kim being supportive
13:36
@ACuriousMind Do you hear UPDATED MY JOURNAL in your brain
I heard it just now when I read your message
that and "you must gather your party before venturing forth" are seared into my brain
Planescape Torment was a tough game for me because I played it in the early 00's and the version that existed back then was sometimes unplayable on modern PCs
It would just flip the fuck out when particle effects appeared
crash the whole PC
Maybe I should give it another playthrough, it's been a while
Game kind of loses steam when you reach Carceri tho
Typical case of game running out of money/idea/time at the end so they just make you kill some monsters
13:55
yeah, see also everything Troika did
Ahah
I do think about them a lot for that too yes
Boy Vampire did not evolve nicely
Bloodlines is so good...for about the first half, and if you use the community patch that fixes a lot of gamebreaking bugs :P
it is also very bad because the first and second half are so different that you can really fuck yourself in spending your skills
I bought a bunch of skills for investigating urban mysteries and then I'm stuck in some dungeons fighting ghouls
Those skills do not transfer well
Had similar issues with Arcanum when you go to that big spooky castle
not enough XPs spent on being a big strong man
14:12
I don't think I ever played Arcanum more than an hour or so
It's an alright game
Did you get troubles at the bridge?
I think I just got fed up with the strange combat system
My main isometric RPG strategy for combat is "Click attack and wait for it to be over"
It's not the most nuanced
the turn-based mode feels very slow and the non-turn-based version feels oddly sped up I think
It works better in some games than others
Still have nightmares about Jagged Alliance 2
aka "What if Baldur's Gate happened in Nicaragua"
14:34
If possible, pls try solipsism for a day and report ur experiences
Finally I can kill anyone I want
I wont b responsible for that :P
Try at ur own expense
Well you're not even a person so no
Tell that to the judge :P
14:49
@DIRAC1930 Again discussed in that section
15:45
hi - i want to clarify something about solving the schrodinger equation. so if we solve the equation, say for the hydrogen atom, my understanding is that what we get is basically the atomic orbitals, and that these are the possible states the electron could be in, but we need more techniques to determine which states are most probable, which states an electron is in for a given situation, etc.
[...] but I encountered a case recently where time evolving a hamiltonian showed the population transfer between states. my confusion is how we go from solving the schrodinger equation which defines our possible states to having a case where solving the schrodinger equation actually tells you how something is moving through these levels/states?
@Relativisticcucumber are you sure you're talking about the same "Schrödinger equation" in both of these cases
because when we look for the atomic orbitals, we're solving the time-independent Schrödinger equation, which is imo a silly name for "looking for the eigenstates of the Hamiltonian"
when you do time evolution, then you're solving the time-dependent Schrödinger equation, which is what I'd usually just call the Schrödinger equation
isnt time dep valid for stationary states + time dep term and we just dont see evolution
in formulae, the difference is $H\psi = E\psi$ (time-independent, looking for eigenfunctions, acts on a state $\psi\in \mathcal{H}$ in Hilbert spacd) and $\partial_t \psi = H\psi$ (time-dependent, looking for trajectories, acts on a trajectory $\psi : \mathbb{R}\to \mathcal{H}, t\mapsto \psi(t)$
I, too, was often confused about what was going on until I separated these two notions clearly in my head
yes what i mean is i thought stationary states with time dep term tacked on are solutions to time dep schrod equation
wait maybe im missing the point
@Relativisticcucumber they are a basis of solutions
15:50
right right so my thought is we can consider the time dep schrod equation to be what we are using for both cases i mentioned in my OG question
@ACuriousMind that is my response to this
@Relativisticcucumber okay, then the next question is: Was the Hamiltonian there the same in both cases?
because what you describe sounds to me like perturbation theory: You start with some $H_0$ and solve for its eigenstates, and then you look at time evolution of these states under a perturbed Hamiltonian $H_0 + \epsilon H_\text{int}$
no! in the case with the population transfer there was an interaction term added but i think this is what im misunderstanding. so i thought an interaction term should merely allow more states to be accessed but shouldnt really tell how they are populated?
@ACuriousMind that message was in response to this not the second message
@Relativisticcucumber what does "allow more states to be accessed" mean?
the Hilbert space doesn't change if you add an interaction term, both $H_0$ and $H_\text{int}$ are operators on the same Hilbert space and so is their sum
so the example i am thinking of is if i have a wavefunction for my hydrogen atom and it says im in one stationary state, we see nothing in the time evolution, but if we add a magnetic field i think then i should see something in the evolution, but what i thought is that this new hamiltonian (H0 + Hmag) just shows us that now the electron could be in more states than before, but it doesnt tell us what actually happens to this wavefunction? i think i am missing something though
I don't know what you mean by "more states"
the Hilbert space for a spinless single particle is $L^2(\mathbb{R}^3)$
15:55
i mean if originally it's in s1 maybe it can move to s2 or something like this
@Relativisticcucumber So the idea of this kind of perturbation theory is this: We start with the interaction turned off, the Hamiltonian is $H_0$. So the system starts in an eigenstate of $H_0$ (insert some general argument why systems will settle into energy eigenstates here) and time evolution is trivial
Then we turn the interaction on, the new Hamiltonian is $H = H_0 + H_\text{int}$, and in general the eigenstates of $H_0$ will not be eigenstates of $H$
so their time-evolution is no longer trivial, and they start to evolve into superpositions of the eigenstates of $H_0$ (they're no longer eigenstates of the time evolution but they still form a basis of the Hilbert space - the spectral theorem doesn't care whether the operator we're applying it to is the Hamiltonian or not)
I think what I am confused about is this: "So the system starts in an eigenstate of $H_0$".
i see this conceptually like we can have a system in any linear comb of eigenstates
but hmmmm
see physics.stackexchange.com/q/69559/50583 for an explicit discussion of my "insert some general argument" above
okay okay so is it like we independently solve for these eigenstates then we put our system in some linear combination of these states then the time evolution tells us how it moves from there on? and these are two entirely separate processes?
@Relativisticcucumber Yes, the eigenstates still form a basis of the Hilbert space - if you know how each of the eigenstates evolves, you know how any state evolves
16:03
somehow i am still confused. i feel these two processes have nothing to do with eachother so im not seeing how they follow the same formalism, namely that the time dep schrod equation achieves both, which is defining the eigenstates of the system as well as how things move through these eigenstates
there is no "eigenstate of the system"
there are only eigenstates of operators
it's just convenient to use the eigenbasis of the Hamiltonian instead of some other operator, because, as you already said, the eigenstates of $H_0$ evolve under time evolution by $H_0$ as $\mathrm{e}^{\mathrm{i}H_0t}\lvert E_i\rangle = \mathrm{e}^{\mathrm{i}E_i t}\lvert E_i\rangle$, which is very simple
So we usually start by writing the state of our system as $\lvert \psi\rangle = \sum_i c_i\lvert E_i\rangle$
okay i see so the hamiltonian defines the eigenstates and the wave function does indeed tell us where things will be found in terms of some combination of these eigenstates so the time evolution evolves the wave function across these states because they are built into the hamiltonian -- this is my updated view
that was meant to be stated as a question lol
I'm not really sure what you mean by that
maybe we should write down some formula
when we change the Hamiltonian to be $H$, we first figure out what $\mathrm{e}^{\mathrm{i}Ht}\lvert E_i\rangle$ is - it's no longer a stationary state, but we can compute what this is
this, by linearity, then also tells us what the evolution of any state under the new Hamiltonian is: $\mathrm{e}^{\mathrm{i}Ht}\lvert \psi\rangle = \sum_i c_i \mathrm{e}^{\mathrm{i}Ht}\lvert E_i\rangle$
so we don't lose anything by just focusing on the $H_0$ eigenstates and their time evolutions
I don't think there's anything more to this
okay maybe i should ask for a clarification. i was told today by my professor the exact statement "solving the schrodinger equation for a hydrogen atom tells you nothing about where you will find an electron, it only tells you where you, theoretically, could see an electron". this statement has thrown me into a great deal of confusion so i am wanting to confirm if it is even true.
i guess the issue is not about time evolution since i buy everything you said but is about the conceptual interpretation of this
maybe that quote is not even rigorous enough to discuss
I really don't know what that statement is supposed to mean
like, it's not wrong or right, I see they wanted to communicate something there but I have no idea what it was :P
16:21
i will think about this and return at some point
 
2 hours later…
18:51
@Relativisticcucumber this sounds ominous :D
19:24
@ACuriousMind but terribly relatable :P
19:38
It's not in chapter 1
20:22
It's on the third page, the paragraph "The momentum can figure in a consistent theory...", then the next paragraph has the $t \to \pm \infty$ thing
Mine just says this
Which is not very helpful because it doesn't explain anything
What's wrong with that
Well there's no calculation showing it
You just have to take their word
They explained it right above
It doesn't explain why the only observable quantities are free particles
20:31
you can prove that the scattering n-point functions define a quantum field theory fully, it's called the Wightman reconstruction theorem
Only for a free particle can you assume $\Delta t \to \infty$ i.e. $\Delta p \to 0$ i.e. the error in the measurement is zero where since the momentum is conserved the measured value is what we can assume the state of the particle was in the measurement
Thats fully understood. What's not understood is why asymptotic particles are free
Particles close together interact, particles far apart don't interact
How do I show this just from a field operator obeying field equations
Is there a list of the kind of sets to expect in borel sets of R^n
To get a general vibe of borel sets
20:37
Read the scattering section of any qft book
That doesn't help because they all start will the statement you said without explaining it
There's open sets, and since it's closed under complementation, I guess all kinds of elements you can remove to get open sets are also borel sets?
Like points and lines etc
@Slereah no
it is consistent with ZF that all subsets of $\mathbb{R}$ are Borel
@ACuriousMind that's some pretty big sigma algebra
so any non-Borel set will be a monstrosity that explicitly invokes the axiom of choice
which I guarantee will not give you any "feel" for it :P
20:40
well "any set I can think of" is good enough for a feel I guess
Is that also true for $\mathbb{R}^n$?
I think so?
You start with a state which is collection of free particles at $t = - \infty$, you then evolve the state under the Hamiltonian which involves fields that vanish at infinity so initially the system is free, and then at $t = + \infty$ the collection of particles is again a system of free particles under a free Hamiltonian because the fields again vanished at infinity, this is really really simple you are overcomplicating it
The assumption that you start off with free particles is not justified at all. It's already states that you can't switch off the interaction because actual particles in the world that we observe are part of the full interacting theory. Free particles do not exist in nature. This step needs to be justified
You are basically arguing with the assumption that the fields in a classical Lagrangian all vanish at infinity
This is physics where everything lives and dies by this assumption (until you get into funny GR stuff etc)
I haven't looked into that
That however is more easy to justify. If all sources are in a given volume, then the fields will be $0$ asymptoticaly
e.g. the electric/magnetic field
20:46
1
Q: Why does the electric field vanish at infinity?

user71646When $r \rightarrow \infty$, $E \rightarrow 0$ for a point charge or set of charges or a finite charge distribution. While this seems obvious, I cannot find a reason why this is true when inspecting Maxwell's equations and the Lorentz force law. I thought however that all of electrodynamics was c...

You can do things that don't vanish at infinity even classically but why make your life harder
Maybe you want this formal mumbo-jumbo rephrasing of the same idea
In physics, the cluster decomposition property states that experiments carried out far from each other cannot influence each other. Usually applied to quantum field theory, it requires that vacuum expectation values of operators localized in bounded regions factorize whenever these regions becomes sufficiently distant from each other. First formulated by Eyvind H. Wichmann and James H. Crichton in 1963 in the context of the S-matrix, it was conjectured by Steven Weinberg that in the low energy limit the cluster decomposition property, together with Lorentz invariance and quantum mechanics, inevitably...
It is good enough to describe local dynamic
Yes I need to look into the Cluster decomposition principle
Well is it the same I'm not sure
20:49
@DIRAC1930 wrong: Plane electromagnetic waves filling the entire vacuum without any sources are consistent solutions of Maxwell's equations
yesterday, by ACuriousMind
@DIRAC1930 I think what you want is the cluster decomposition principle
I haven't looked at classical field theory in a long time
So I'm probably wrong
@ACuriousMind Plane waves aren't real
Well I tried
21:11
Why are Borel measures defined on Hausdorff spaces
is there anything particularly unpleasant about measures otherwise
21:24
@Slereah you want compact sets to be Borel (because intuitively compact sets have finite volume and hence should be measureable)
Hausdorfness guarantees that compact sets are Borel
if you try to talk about Borel measures on non-Hausdorff spaces you'd need to carefully examine any theorem about them whether it uses that compact sets are Borel or not
probably true on manifolds, I guess?
Can't think of a counter example on the top of my head
but on the other hand I don't care to include them
yes, the usual manifold definition is that manifolds are locally compact and Hausdorff
I wonder who did the first modern definition of manifolds
Let's see
Veblen apparently
He sounds familiar, but maybe just because he sounds like vielbein
21:48
Oh wait Veblen was guy that worked on projective connections

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