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00:00 - 20:0020:00 - 00:00

00:01
@0celo7 You should be nice to people. I did something nice for some dude and it turns out he works for EA. Now he's offering me arbitrary games :D
I don't even have a computer that can play them XD
00:26
> The comments section is not for roleplaying as deities. – AncientSwordRage♦ 13 hours ago
^ not a problem we've had, fortunately
@DavidZ although to some extent I disagree
it's true your advisor's status in the field is really important but it's also important to be at a department with a rich physics atmosphere
both in terms of colloquia, caliber of students, number of post-docs etc.
and stuff like that tends to scale with ranking
00:43
@Danu: Like I said, you'll have to teach me.
@FenderLesPaul In my experience, the quality/motivation/helpfulness of the other students in your PhD program matters an order of magnitude more than anything else.
Specifically, those in your lab.
This is obviously correlated with having a good PI.
But anyway, you'll spend a lot more time with the other students in your lab than with anyone else.
0
Q: Contributations Lost in Time

JenWhat happens to good physic questions and answers lost by people who lost their accounts either which a way?

01:05
@DanielSank I just like being around a variety of really smart physics students
even if they aren't in your group
01:52
@FenderLesPaul Sure. I'm just telling your from experience what I've found actually matters.
Let me put it like this: there are a lot of people who go to highly ranked institutions but are literally miserable because they're in a crappy group with a crappy PI and crappy students.
I would rather be not miserable, instead of being miserable.
02:09
@DanielSank:
@DanielSank right I get what you're saying
seems very reasonable
@DanielSank ^
@FenderLesPaul you ruined it!
02:33
@DanielSank Up?
03:23
@DanielSank What?
Who was I not nice to
you should give me the games, I'm nice to you
@0celo7 That...doesn't sound very nice
@FenderLesPaul Harvard Applied Physics, Northwestern, USC, Wisconsin Madison
U Pittsburgh
@ACuriousMind whaaaaat
Emory
you know what's not nice
the length of The Revenant
that's a loooooooooong movie
03:30
I take it you just watched it?
yes
I liked it. She didn't.
Not sure Leo dying for 2 and a half hours is her thing :/
@ACuriousMind so what's wrong with "just take the maximum" as the proof of "every finite set contains its sup"?
its trivial to verify that if the maximum exists, it must be the sup
@ACuriousMind all of these proofs online use induction
@0celo7 Yeah, but how do you know it exists? It's "obvious", but you have to formally prove it once.
@ACuriousMind My prof said along the lines of "prove it if you want"
03:52
"Tis vain to tell, you wot full well"
Yes I fucking "wot" because I have no clue what you're talking about Mr. Wigglesworth
 
2 hours later…
06:01
@FenderLesPaul expect a small number monday/tuesday pick up on wednesday, and raining emails thursday/friday/saturday
particularly thurs/fri
06:12
@0celo7 I never said you're not nice. Just saying, karma works, apparently!
@BernardMeurer yeah
06:25
@DanielSank @ACuriousMind @DavidZ
http://www.feynmanlectures.caltech.edu/III_03.html

Couple of quantum conceptual questions:

1. Has there been any theoretical mechanisms being proposed by the literature that explains why indistinguishable states can interfere (besides it is an experimental fact from double slits, alpha particle, neutron diffraction etc.)?

2. (Will wrote this up in more detail and formally later) Suppose I have a double slit set up, where the hole detectors and the light source can be receded on the press of a button. Suppose I have increase the voltage and intensity of
(The questions are based on that from reading the Feynman lecture notes, I understood that if two states are indistinguishable, they can interfere, but they cannot if they are different (hence distinguishable). From the double slit experiments we knew that the interference pattern disappears when the detectors are triggered. But I am wondering it is sensible to ask about
how fast does the setup knows its state (described by $|detector\rangle \otimes |x\rangle$) are being changed, thus changing the way the pattern developed (from interfering to non interfering))
@ChrisWhite I have a question about rotation mechanics
Which radii I should use for the 3rd case?
06:58
@Secret:
> Has there been any theoretical mechanisms being proposed by the literature that explains why indistinguishable states can interfere
I don't know what you mean by "indistinguishable states can interfere".
In the same page of that feymann lecture feymann said

"Now we would like to emphasize an important point so that you will avoid a common error. Suppose that you only want the amplitude that the electron arrives at xx, regardless of whether the photon was counted at D1D1 or D2D2. Should you add the amplitudes given in Eqs. (3.8) and (3.9)? No! You must never add amplitudes for different and distinct final states. Once the photon is accepted by one of the photon counters, we can always determine which alternative occurred if we want, without any further disturbance to the system. Each alter
Jan 19 at 18:52, by ACuriousMind
@Secret: You're probably confused about this: When you have the detector information, then you are asking "What's the probability to detect either $\lvert x,D_1\rangle$ or $\lvert x,D_2\rangle$?" Two states, two probabilities, just add them.
Jan 19 at 18:52, by ACuriousMind
When you don't have the detector information, all you're asking is "What's the probability to detect $\lvert x \rangle$?", where now you may in the calculation of this single probability, write $\lvert x\rangle = \lvert x,D_1\rangle+\lvert x,D_2\rangle$, and when you now evaluate $\langle x \vert \text{initial state}\rangle$, this gives the added amplitudes.
and in here
http://www.feynmanlectures.caltech.edu/III_04.html

"Now suppose, however, that aa and bb are identical Bose particles. Then the process of aa going into 11 and bb going into 22 cannot be distinguished from the exchanged process in which aa goes into 22 and bb goes into 11. In this case the amplitudes for the two different processes can interfere. The total amplitude to obtain a particle in each of the two counters is"
actually feymann repeated the same thing many times that indistinguishable particles their amplitudes will interfere from Ch. 3-7 in Vol III
NB: Acuriousmind elaborated Feymann's statement in terms of state vectors instead of amplitudes, thus the principle is the same

So then the interesting question is then on whether there are mechanisms that are proposed that explains why indistinguishable states can interfere
 
3 hours later…
10:42
@FenderLesPaul I have to stop checking it...it's tearing me apart
hey guys my custom dark theme is ready
it's on github: https://github.com/busukxuan/Stack-Exchange-TM-Custom-Dark-Theme/blob/master/physics.css
you'll need a User CSS browser extension/add-on to use it, the extension probably even needs to inject CSS rather than just inject a link to the stylesheet, or some stuff might break and look inconsistent
if you love dark themes, please feel free to try it out :-)
the code is pretty messy though...
user116211
11:32
I'm not getting the time-reversal transformation: $t\rightarrow -t$; suppose you are seeing a stroboscopic film with instances: 10, 20, 30, 40, 50. When you rewind the film (in backward direction of time): the instances would be: 50, 40, 30, 20, 10. Now, how can it be reversal of time; as time-reversal means $t\rightarrow -t$ but here only the instances are in reversed order; where is the minus sign of the transformation? Can anyone point me that?
It's the physical process that happened that is the subject of time reversal

suppose you have some physical process that is described by some relation with the parameter t. Time reversal means you replace t with -t. If you still get the same physics, (e.g. a ball rolling to the right when t is increasing corresponds to a ball rolling to the left when t is decreasing) then you have time reversal symmetry
If your video frames is actually describing the evolution of the system as it move forward in time (where each frame (the 10 20 30 40 50) is a snapshot of the system at that moment in time, then the - sign goes into reversing the order of the video frames, such that the system in the video evolve backwards
For example a ball rolling with constant speed v such that $$S=vt$$ will become $$S=v * (-t)=-vt$$ thus on reversing t it rolls backwards
 
2 hours later…
user116211
13:33
@Secret: Thanks for the reply. Okay, when the film rewinds, would the time sequence be -10,-20,-30,-40,-50 or 50,40,30,20,10 or -50,-40,-30,-20,-10? I could get the physical implication of time reversal but still having problem with $t\rightarrow -t$. So, which of the above would be the correct sequence of reverse time?
14:04
@0celo7 : you know what motion is, a gradual change of position. Moreover, it's empirical. I can hold my hands up a foot apart and show you the gap, the space, between them. And I can waggle my hands to show you motion. But you can't show me spacetime, because it's an abstract "mathematical space" in which there is no motion.
14:21
@FenderLesPaul Stony Brook U seems like they're later than normal this year
@user36790 I am not very sure, I am guessing it will depend on where you set $t=0$

If you are doing a rewind directly at the 50 frame by $t\riaghtarrow -t$, then it will go like 0 -10 -20 -30 -40 -50

But (at least for something linear as indexing each frame with a time), you can always shift the position of the $t=0$ point such as adding 50 for each value of t so that it becomes 50 40 30 20 10

Since it is ultimately like a coordinate system, it does not matter where the origin is

I welcome anyone else that can point out anything I miss in this analysis
@GBeau Are you waiting the answers for Ph.D. applications? Do they now interview people before deciding about the scholarships?
user116211
14:43
@Secret: thanks, again; didn't want to post such a dumb question at the site; but want to like to hear others' view also; so willing to post it as a question:/
The Chat Crowd generally arrived 2-3 hours later, unless it is noon in your place, you might just have t check back later
@yuggib some do, some don't
@GBeau ah ok I see...SB didn't in my time
(almost ten years ago)
@yuggib pretty much everywhere doesn't, but then asks for them on a case by case basis as an exception
but seemingly more people are getting asked every year
I see
15:07
hey guys need some help here
Sicne I don't even know the name of that general formula (i.e. can aloow things like summation, integrations etc.) that relates $r_{eff}$ to v of an arbitrary rigid body, I don't know how to answer this question myself
0
Q: Trying to understand the physical intuition on finding/deriving effective rotation radii of a rigid body

SecretThis question is inspired from the answer of this If the rolling is assumed to be without slipping, we can solve the problem by conservation of energy: $$ mg \Delta h = \frac{1}{2}mv^2 + \frac{1}{2} I \omega^2 \tag{*} \,,$$ with the relationship between $v$ and $\omega$ set by the spacing...

@ChrisWhite I just had a random thought about that crazy star dimming thing. What is the potential for stars to develop really massive star-spots? Is there an upper bound on the size of star-spots for a given star?
@Secret How can the rods be unequally spaced around a sphere? I'm not sure I understand the setup
Any configuration I can think of will still end up being symmetric around the sphere for some axis, it just might not be the axis aligned vertically
You can have a track where one end is shorter than the other, then as long it is not too much, the ball will not tip over and will remain on the track
But any 2 points in contact with a sphere will always be symmetric about some axis of the sphere won't it? I am having a really hard time drawing something that isn't symmetric about some axis
And again, the axis of symmetry may not be aligned with the gravity vector in general
15:38
It will look something like this
(Sorry but it seems h bar takes forever for me to upload it directly)
@Secret I feel that the issue here is that Feynman talks about processes (probably because he thinks in terms of Feynman diagrams). But, formally, there is no notion of a "process" in quantum mechanics. You have an initial state $| i \rangle$ and a final state $|f\rangle$ and the time evolution operator $U$ and the probability to see the transition $i\to f$ is $| \langle i|U|f\rangle|^2$. There is no notion of a process "$|i\rangle$ goes into $|v_1\rangle$ and then into $|f\rangle$".
The idea of the path integral, however, is that you can sum up the amplitudes of "all possible ways" in which $i\to f$ "can happen" (which is basically just using that the identity can be resolved as $\sum_i|b_i\rangle\langle b_i|$ for an orthonormal basis), and this is what you try to express as "indistinguishable states can interfere".
The problem is that our thinking in terms of "processes" is not a sensible notion in the quantum theory itself - if you are not measuring $|v_1\rangle$ or $|v_2\rangle$, it makes no sense to speak of the processes $i\to v_1\to f$ and $i\to v_2\to f$ as distinct because the transition $i\to v_i$ doesn't happen if $v_i$ is not being measured.
Hmm... no wonder when I read it it so remind me of path integrals (at least the basic gist, as I have not learnt them formally yet)
But then the issue of measurement became more mysterious
If the notion of process is not defined in quantum mechanics, then how does the setup itself knows it has detected $v_i$ and thus the electrons started to pile up into the non interference pattern

I know that in the maths the difference between the case where $v_i$ is measured (i.e. the detector detects something) and not measured (i.e. the detectors failed to detect something, or fail to determine which hole the electron came from) lies in the information avaliable for us to let us work out what scenarios we are dealing with thus co
15:55
@Secret The setup doesn't "know". The setup is different whether there is a detector present or not. It's not the same setup in the case where we can detect the $v_i$ and in the case where we can't.
There's nothing mysterious here. Adding a detector means there's the interaction between the detector and the particle that wasn't there before, which changes the time evolution operator, and hence the probability of $i\to f$.
The setup has feelings too
hmm, in that case this brought me to the 2nd question

Based on the settings of the voltage of the electron gun and the lamp mentioned earlier (so that the stream of electrons are packed close enough to effectively build up a pattern on the screen within a time interval $t_0$), and (from previous message) that we know that slotting in the detector or out will effectively switch the setup between two different ones. Will we expect no time delay (correct to the nearest $t_0$) that the interference pattern become a non interfering one?
correction: slotting in the detector or out will effectively switch the setup between two different ones (because The setup is different whether there is a detector present or not)
@Secret Well, go ahead and do some time-dependent perturbation theory to determine that, given a characteristic function $f(t)$ with $f(t\geq t_\text{switch}) = 0$ for the detector Hamiltonian $H_\text{int}$ and full Hamiltonian $H = H_0 + f(t)H_\text{int}$. It's gonna get ugly, but it's pretty obvious that you should expect the propagation of the change to be $\sim c$ without any calculation, since there's nothing in the system to have memory of the switch.
16:26
And the beautiful thing is that in quantum mechanics (in QFT one has to be a bit careful), every observable has a measuring process (at least theoretically) i.e. an apparatus such that the interaction with it measures the observable giving an output on the apparatus pointer, and "collapsing the system" (very bad words) to the proper subspace corresponding to the measured value.
So I don't see anything mysterious in the measuring process, as described à la von Neumann...everything behaves as it should, and it is always theoretically possible to measure an observable (even very "bad" observables such as unbounded ones and with continuous spectrum)
user54412
@tpg2114 You know, I don't know of any formal upper bound, though this would be a lot more extreme than I've ever imagined. Star spots are complex phenomena emerging from strong convection and magnetic fields. At this point, though, I'm kind of hoping the star unexpectedly goes supernova. Then we'd have no choice but to conclude supernovae are weapons used by interstellar civilization.
@yuggib The problem is that people don't introduce measurements as von Neumann measurements. Most treatments seem to just state the rule that a measured state collapses into an eigenstate, and never talk about the measurement itself or decoherence, which leads students to believe there's a mystery there.
indeed
16:48
@Secret Yeah, so that's still symmetric but it's rotated
@GBeau yeah I'm expecting people to get a flurry of emails thursday/friday
@ChrisWhite I guess you missed the article by some guy who said the reason we haven't found aliens yet is because they are all extinct
it'll be quite a blizzard
@tpg2114 but isn't the weight pointing striaght down?
@GBeau I'm hoping to be caught in the eye of the storm and not left out of it
@GBeau also stop checking dude
I stopped checking and I've been way more relaxed
still anxious but not nearly so
it's not going to do you any good to check anyways
so just relax
16:49
@Secret Yes, but like I said in my comments about it -- there will always be an axis of symmetry but that axis may not be aligned with gravity
@GBeau at the end of the day your apps are already in so it is what it is, it's out of your hands so just wait it out; good things will come :)
worst case scenario you'll learn to love wherever you end up
The weight will be distributed onto one or the other rail based on the dot product between the gravity vector and the axis of symmetry or something like that. But given two points of contact and a sphere, one can always find a symmetric axis so the notion of an asymmetric set of rails you asked about doesn't exist
Or at the very least is unclear
@FenderLesPaul Nice to see you finally adopted reasonable fatalism :)
@FenderLesPaul or you can always refuse and try next time if you don't want to compromise...
So in that case the $r_{eff}$ will be at an angle wrt the weight vector and thus we solve the problem as in the symmetric case?
16:53
@Secret That's the approach I would take. That said, I haven't done it so I can't verify
I don't even know how to verify because I cannot find the formula for the most general case, unlike how we have the moment of inertia formula as $$I=\int_V \rho r^2dr$$
you approach will clearly gave a different ans to mine, but the issue is I don't know how to check which approach is the correct one
@Secret The answer that agrees with both limiting cases will be the right one. So when the symmetry axis aligns with the gravity vector, you have the original formula. When it is exactly 90 degrees to the gravity vector, you just have a ball rolling down a ramp
If you have a formula that works in both those limits then it is likely to be correct. But not a guarantee
And it will almost definitely involve the dot product of the gravity vector and the symmetry axis unit vector
hi guys
i'm a little bit fan of @ACuriousMind , deep knowledge in so many physics fields always a pleasure to read his answers
Acuriousmind is especially good at quantum mechanics, a field I love so much but struggle so hard on it
4
i see
i think he's even good at engineering stuffs
17:04
other quantum guys include yuggib and danielsank (who actually work with quantum information systems)
@no_choice99 Thanks ;) (There are many people with deeper knowledge about things though)
yeah danieksank is another physics monstah
3
@no_choice99 Definitely not, my whole practical experience consists of obligatory lab courses, and I've never done something that would really be engineering
@ACuriousMind @DanielSank ahahah it surely is one of the sock-puppets of the master speaking here.... >:-D
self-promotion...
17:07
who is the master? :)
Psssssssst
For the uninformed ones, I'm just kidding
Ohh, I forgot about the sock puppet/master post
That was a good one
@tpg2114 "the"? There were like, hundred, until that user finally gave up
the "supposed" master (obviously it is not true) was DS
and ACM was one of his supposed sock-puppets actually
17:09
@ACuriousMind I just considered them all one.
@yuggib Well, have you seen us in the same physical room? ;)
@ACuriousMind of course not
So you cannot exclude there is one very sophisticated puppet master at work.
I can't
Perhaps physics.SE has only a dozen of users, all thinking they're the sole puppet master
17:11
In theory, on the beginning of february me and @Danu could be on the same room
(but probably he won't attend the seminar)
What are you talking about?
I am giving a seminar at LMU
I meant what is the topic of the seminar...I see "what are you talking about" wasn't the best way to say that :D
:D
Bohr's correspondence principle for the Nelson model
that (or a small variation of it) should be the title
I know one of those two things ;)
17:14
@tpg2114
but maybe not in its full mathematical majesty
@yuggib I know the correspondence principle as a vague statement, and I have no idea what the Nelson model is
The limiting cases seemed to agree, it seems we need something more stringent to test them apart
Searching for "Nelson model physics" gives surprisingly useless results :P
17:16
@ACuriousMind yeah, I figured that out...Nelson model $\simeq$ non-relativistic quantum particles in a phonon/KG field
with linear coupling
because it is a name used mostly by mathematicians
the model was not invented by Nelson, but introduced by him to the mathematical community
(in the paper where he proves that it has a non-perturbative renormalization)
I see. Having non-relativistic particles and a quantum field in the same theory seems a bit strange to me, though
@ACuriousMind Your definition of dimension was a nerd trap
@ACuriousMind that happens often, e.g. in condensed matter or quantum optics and the alike
Ah, that explains why I haven't seen that before
Never did QO, and the only condensed matter course I had was the very basic obligatory one
originally, it was used also for nuclear physics
e.g. nucleons interacting with a meson field
of course the nucleons are only approximatively non-relativistic
17:29
@0celo7 lol, what happened?
@yuggib Ew, filthy effective theories
:-D
at least it is possible to define a renormalized self-adjoint dynamics in (3+1)d
the rest is just physical taste, and I am a mathematician now...
@ACuriousMind he came up with some crazy counterexample
@yuggib Well, that sounds indeed nice.
basically showed that the trace need not be defined on the identity
I don't know enough functional analysis to know what exactly happened
@0celo7 For a finite-dimensional vector space?
I was aware that the identity on infinite-dimensional spaces is not trace-class
17:32
we didn't have a notion of finite vs. infinite
in any case, he proved the thing using induction without the AoC
Hm, well, if there was "functional analysis" involved, the c.e. was probably infinite-dimensional.
it was
he looked at the vector space $\mathcal{F}(I):=\{f:I\to\mathbb{R}\}$
we also ran out of time
damn physics lecture
Well, @yuggib had already said that my definition fails for the infinite case:
Jan 21 at 22:19, by yuggib
I don't think you can define the trace that way for $V$s that are not finite dimensional
yes, Denzler proved that
or maybe he didn't, I can't functional analysis
Well, the physicist's "proof" is easy: We know that $1 = \mathrm{i}\hbar[x,p]$, but the trace of a commutator is zero, and the trace of the identity can't be zero, so it has to be undefined.
17:39
lol
eh, modulo constants. I can never remember the sign of the $\mathrm{i}$
or the power of $\hbar$ :P
Oh, yes. Might be $\hbar^{-1}$
It's 1, anyway :P
$(\mathrm{i}\hbar)^{-1}$
Well, $\mathrm{i}^{-1}$ is just a sign
17:41
@ACuriousMind he was talking about a nuclear theorem or something
crazy stuff
I really need to pick a mentor now
What's not clear is if this person will be the same one overseeing my undergrad thesis
What function does this mentor have then?
Don't say "mentoring me" :P
Meet once a month for at least 30 minutes and talk about stuff
And oversee the thesis (probably)
So I can throw out all of the algebraists
They're useless
Number theory, too
@ACuriousMind the problem with the guy I originally had in mind is he WAY overestimates my abilities
wtf I can't be expected to know what my thesis will be on right now
I need someone who knows everything about GR, curvature flow, symplectic geometry, gauge theory, K theory, Riemannian geometry, PDE, functional analysis, algebraic topology
that probably captures everything I could write the thing on
oh also differential topology and measure theory
@0celo7 I thought the mentor need not supervise your thesis, so why would you decide now?
I don't know if they do or not!
I'm meeting with the director tomorrow, he'll tell me
@0celo7 that...seems like really relevant information that should be easily accessible
17:54
Dude I can't even Google
What makes you think I can look that up??
Hm, good point
> In addition, every student has a faculty mentor and eventually a thesis advisor.
Ok
@ACuriousMind it's the 5 stages of grief haha
so this means the mentor can be whoever
anxiety -> acceptance
17:57
@0celo7 See, you can do it!
@FenderLesPaul Wisconsin Madison sending out a bunch today
>.>
dude stop checking lol
@yuggib no, they should be someone that knows about stuff I enjoy reading about
just wait until the end of the week
did you apply to WM?
No
17:59
@yuggib also I was told not to ask postdocs to do it
yes, but not necessarily someone who would supervise your thesis; so it's not so important
well I don't want to get one of these algebraic geometers and start bugging them about Riemannian geometry
@0celo7 that seems reasonable...postdocs are not yet able to mentor
@GBeau I hope there aren't any new UMich admits
18:17
for some reason, this expression reminds me of the transition moment integral...
18:30
Hmm, an iterative procedure, no wonder they said it is nasty...
Guess I should boot my matlab or mathematica to crunch through it
@yuggib and I wouldn't mind learning some category theory...I don't think anyone who knows category theory also knows geometry, twistor theory, etc
So really I need my mentor to be Urs Schreiber
@ACuriousMind ::sigh::
@DanielSank you should pick a mentor for me
@0celo7 k what are my options?
also I wrote a few lines on the TeX file, you should take a look overleaf.com/read/rkwznvjqqwwp
from "motivation" to where I start on the tangent space and then the "some review" near the bottom
Ok lemme handle a small crisis in the lab and then I will sit down and read the whole thing again.
Looking forward to it.
ok thanks
@ACuriousMind German detected. It's "a hundred."
19:00
what the fuck
you wrote up stuff on index notation?
:p
@FenderLesPaul it's not nearly finished
it will be very good once it's done
in 20 years
19:38
Yo @0celo7 I'm reading your thing now.
fyi
I woke up thinking about electricity and motors, and soon identified a confusion I had. Photons are the carriers of the electromagnetic force, but I've seen/heard that electrons are excitations of the electromagnetic field (e.g. MinutePhysics) --
@El'endiaStarman That's incorrect.
Upon watching that video, he actually says that electrons are excitations of the quantum field, not the electromagnetic field. Confusion (mostly) gone. :P
Electrons are not excitations of the EM field.
Photons are excitations of the EM field.
Electrons are excitations of the electron field.
@El'endiaStarman EM field is a quantum field
19:42
@FenderLesPaul Indeed. All quantum fields are quantum fields :D
Ha, okay. Why does it make sense to talk about an "electron field", though?
Are these fields different representations/manifestations of the underlying most-fundamental field (quantum?)?
@El'endiaStarman There is no single thing called "the quantum field".
Anyone who says "the quantum field" is guaranteed to be not a physicist.
@DanielSank :D
There are many types of things in the Universe: electrons, photons, etc.
@DanielSank: But you just did!
19:44
I am the quantum
I am the field
I am
@MikeMiller ಠ_ಠ
Anyway....
@El'endiaStarman Each of these things was once thought of as little balls flying around.
It's a pretty good picture, but in the end it fails.
We find that these things have two peculiar properties:
1) they exhibit interference
2) They are indistinguishable in a very deep sense.
Item 2 is rather important and very often misunderstood.
Indistinguishible between electrons, say? (So only between particles of the same kind.)
@El'endiaStarman Correct.
@El'endiaStarman There was a question on the site about the relation between fields and particles a while back, and actually, I wrote what I thought was a good answer:
40
Q: Which is more fundamental, Fields or Particles?

jpbrooks-user153707I hope that I am using appropriate terminology. My confusion about quantum theory (beyond my obvious unfamiliarity with its terminology) is basically twofold: I lack an adequate understanding of how the mathematics of quantum theory is supposed to correspond to phenomena in the physical world ...

I hate trying to find copies of theses.
It's impossible.
@MikeMiller Physical copies?
19:53
Any copies.
If a group doesn't post their students' theses on their website, I don't know how to save the world from disaster.
Hello @DanielSank, @MikeMiller, @El'endiaStarman, @FenderLesPaul :)
@privetDruzia Hello.
@privetDruzia Hi
Remember, everything varies between disciplines. "A group posting theses on their website" barely even parses in math.
19:55
@privetDruzia Kak dela?
xorosho a y tibya? :)
@MikeMiller Oh :(
@privetDruzia normalno
hahaha)
@privetDruzia shto?
nichivo
)
19:56
In retrospect I feel like QFT would be so much better to teach from a CMT point of view
than a particle physics point of view
ya zanimalsya s'ryskim yazikom v'yniversitete
could anybody tell me:
If is force the cause for a certain potential energy or is it the other way around?
^ Horrible attempt to spell Russian with English characters :(
@DanielSank kryta
s okay)
@privetDruzia eeehhhhhh that's kind of ambiguous.
I wouldn't really say one causes the other.
19:58
based on the formula $ \frac{-dU}{dx} = F(x)$
@privetDruzia Yeah, in a sense that's a definition of potential energy.
But you can take different points of view.
@privetDruzia (Ti Rysskui?)
so is my point of vieuw, based on this formula, incorrect?
niet prosto tam rabotal i zhil
@privetDruzia ehhhhh, I dunno. That equation has an equals sign, right? Equality isn't really directional. It's more saying that those things are "the same".
ya v evrope zshivy
mhm yes right
but
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