« first day (2147 days earlier)      last day (2787 days later) » 

6:00 PM
Because that also looks like the zealous hope of someone sceptical of quantum physics :P
 
@Danu If you calculate the optical chirality it gives zero, and the conclusion from the questions here was that higher-order chiralities reduce to this for monochromatic fields.
 
@DavidZ go for it
 
@EmilioPisanty Right
 
@Danu The global symmetry in principle would permit different mirror versions in the far field for the two enantiomers.
However, they also need to be able to have a chiral local interaction with the field
And that's where the zilches give zero, so no luck.
As far as I can tell.
 
@ACuriousMind In class, we showed that $Na^\dagger|n\rangle=(n+1)a^\dagger|n\rangle$. The prof then claimed that $a^\dagger|n\rangle=d|n+1\rangle$. Why?
 
6:02 PM
@DanielSank By the way, as far as your question, I think the biggest difference is that as a moderator, most of my time on the site is spent on "janitorial" work. My first stop when I come to the site is the moderator flag queue. It typically has about 10 flags, and I go through and handle the easy ones (~5), then think about the hard ones. Sometimes it takes 10-20 minutes to handle a difficult flag, not counting time spent waiting to confer with the other mods.
 
@0celo7 What's the definition of $\lvert n+1\rangle$?
 
@DavidZ Interesting. This feels more "different" than, say, people constantly pinging you in chat with whatever questions and comments?
 
@ACuriousMind It's a state s.t. $N|n+1\rangle=(n+1)|n+1\rangle$. But how do we know there's just one?
 
@0celo7 Aha, I thought that that was your underlying question!
Wait while I locate the relevant Qmechanic post
 
@DanielSank You mean, is this the janitorial work a more important/relevant difference to how I would use the site as a 10k user, than the repeated pings? Yes, I'd say so
 
6:05 PM
@DavidZ ok
 
@0celo7 Here.
 
@ACuriousMind uhhh, what
 
quantum guys: I still find it strange in about the interpretation that it is an uncertainty. From what I remember about the derivation, it is derived using cauchy schwartz and also terms like $\langle A^2 \rangle$ (which suggest variance), which when plugged into cauchy swartz gives the commutator term. But since a commutator [A,B] is an infintesimal unitary transformation of A by B (which act as a generator), then wouldn't the interpretation that the inequality is along the lines of the lower
 
@EmilioPisanty Invent allll the tensors :D
 
bound on how much A is being transformed by B?
 
6:07 PM
@DanielSank BTW the fact that I spend most of my time handling flags rather than posting questions and answers is a reflection of what I, personally, see as the best use of my time here - it's not an obligation of moderators in general.
 
@Danu No, my gut feeling is that if the simple tool says no then the simple tool is right.
 
@Secret Writing @quantum just pings QuantumBrick currently. Don't use @ unless you actually want to ping someone.
 
Here it's worth going up a single step in the ladder, because first-order contributions could conceivably cancel.
 
ok sorry about that
 
@ACuriousMind indeed.
 
6:08 PM
(e.g., take two co-propagating, counter-rotating fields at $\omega$ and $2\omega$ (another favourite of mine). Set the relative intensities right and the optical chirality / 000-zilch will vanish, but the field is still chiral.)
 
(cont.) so why there is no interpretation of a notion of a infitesimal transformation in HUP as hinted by the presence of the commutator?
 
but more than that is unlikely to give something new.
 
@ACuriousMind So we just assume there's only one eigenstate?
 
@DavidZ That's puzzling.
 
@EmilioPisanty My feeling is TENSORS
 
6:10 PM
are we quotienting out the various degenerate kets?
 
@Secret Well, that is a valid interpretation, but it's the more impractical one. That $\delta A$ is an uncertainty is not an interpretation however, since its definition is just the definition of the standard defination of a random variable
 
@Danu lol
@Danu your feeling is wrong
your feeling should be SYMMETRY
 
I see, makes sense
 
As always :'(
 
@Danu =P
 
6:11 PM
@DanielSank how so? (also note my edit to the previous message)
 
@0celo7 The "nicer" assumption is that the representation is an irreducible representation of the ladder algebra. If you have degenerate kets it would be reducible, so the system would fall apart into two disjoint, non-interacting pieces, which we certainly don't expact for a single HO.
 
@DavidZ Ah.
 
5
Q: In 2016 (pre-election) what activities are involved in being a Physics SE mod?

John RennieWith a moderator election looming it would be useful to hear from our current moderators how much the role affects their use of the site. Some obvious questions would be how many hours a day does it require, and what are are the day to day tasks you need to do in that time. However it would also ...

0
Q: 2016 moderator election README

DanielSank Election page Question pool for potential moderators Present (2016 September) moderators' thoughts on what it's like being a mod. Main Stack Exchange FAQ on what it means to be a moderator. This is important; in order to vote for a moderator we need to know how being a moderator differs from e.g...

 
^clickbaity title
 
Which?
 
6:14 PM
Why not just "General information concerning the 2016 moderator elections"
 
"read me"
 
Yours :P
 
That's standard notation...
Should I have not all-caps'd it?
 
Q2. Why measurement must sample from a spectrum of eigenvalues and project the state onto an eigenstate? Using the decoherence interpretation, why only eigenstates become entangled to the environment pointer states but no entangled states formed by a superposition state of the system entangled with one of the pointer states? That is, why entanglement with the environment must occur between eigenstates an not the superposition states?
 
@DanielSank Yes, because it's supposed to be clickbait. I don't think that's a bad thing.
 
6:14 PM
No "read me" in general, IMO.
 
@Danu A readme file is something you should read so other stuff makes more sense.
That's the point of that post.
 
We call these things "readme" for the same reason people call their virus executables "clickme" :P
 
@ACuriousMind True.
 
@DanielSank for people who are familiar with software, yes; outside that community, I'm not so sure.
 
@DanielSank I don't think it is a good title, because I personally for instance don't want/need to read that post.
 
6:15 PM
@DanielSank I'm with Danu on this one - standard in some conventions, but I don't really think it's one that applies
 
If you had just called it "general info concerning..." then I wouldn't have clicked
Now I clicked, for nothing.
 
So edit it.
 
I wanted to leave that to you, but sure
 
It's really frustrating that the software community has such good standards with regard to communication, but physics simply does not.
 
It has nothing to do with that, IMO. I understand what README means.
It's just not true that I need to read that post
So I don't want the title to say that I do
 
6:17 PM
@Danu omg
 
@Danu just edit it already :-P
 
@DavidZ I did :)
 
@ACuriousMind Geodesic balls tonight :D
 
OK cool
 
@DanielSank It's really not a big deal, don't get me wrong.
 
6:17 PM
I don't like the new title XD
 
@Danu I don't need to read the readmes of most software either, the title doesn't mean "everyone needs to read this"
 
lol
 
It's not general information, it's a set of links.
@ACuriousMind Yes.
Listen to ACM. He is wise.
 
@DanielSank ...which collect general information
 
It's to say "if you are confused about what's going on with this thing, read its readme first", not "read the readme at all costs"
 
6:18 PM
^ That
 
In short, why measurement can only project to eigenstates, but not superposition states made from nondegenerate eigenstates?
 
@ACuriousMind Meh. I think the current title is more accurate and more useful, at least for me personally.
 
@DanielSank I notice an uptick in flattery lately. Are you implementing your election "winning" strategy? ;)
 
lel
 
@ACuriousMind Sure, that's what readme means to a programmer. That's much too subtle a reading for an item on the yellow box on the front page, though.
 
6:20 PM
@ACuriousMind Partially I'm trying to highlight how incredibly good you are at stating what I'm thinking. This serves two purposes.
1) It might make you want to run for mod, because a key element of a community leader is understanding what other people want/think and distilling those thoughts into useful works.
 
@EmilioPisanty I agree with that, but the reason @Danu gave was "I don't need to read this thing so it shouldn't be called readme". Which I guess proves your point about subtlety, but is not a good reason in itself ;)
 
2) It helps me rationalize to myself that if you are elected, my opinions on policy will be well received, etc.
 
@ACuriousMind Not sure I agree with Danu's reasons, but I agree that the old title is clickbaity
Not 100% behind the new one though
 
@EmilioPisanty I feel like software community standards are pervading our entire culture though.
Surely the idea of a readme is well understood.
I'm delighted by this discussion.
 
@DanielSank "our entire culture" is a bit strong
 
6:22 PM
Communication is important.
@EmilioPisanty Is it?
If I say "the system crashed" you know what I mean.
 
that's a long way away from README
 
"entire culture" = hbar ;P
 
@Danu I think we're representative of the population at large.
 
What about the many hundreds of 300+ rep users who use the site occasionally and only rarely go to meta or chat?
 
@0celo7 With you in here, we've even got Trump voters!
 
6:23 PM
@0celo7 Bwhahahahahahahahahahahahahahahahahahahahahahahahahahahahahahahaha
 
@EmilioPisanty They've never seen a reaadme?
 
@DanielSank You betcha some of them haven't
 
@Danu exactly
 
Sorry to break the news
 
We've got like every segment of the population
 
6:24 PM
and if they did, they forgot about it
 
How about "2016 moderator election resources/links"
 
maybe they did read it
 
@danielsank @EmilioPisanty @ACuriousMind sorry some typo: Why measurement can only project to eigenstates (or for degenerate eigenstates, the subspace spanned by the degenerate eigenstates), but not superposition states made from nondegenerate eigenstates?
 
Well, our resident homeless person Chris White isn't here any more...
but other than that
 
@0celo7 Yeah what's his deal?
 
6:24 PM
Sorry, box-dweller.
not homeless
 
@DanielSank Better. I'd shy away from starting with a number
 
@DanielSank I'm sure some of them haven't.
 
particularly with the current font
 
@DanielSank JD annoyed him; he left.
 
I hate the numbers in this font
 
6:25 PM
@0celo7 wow
 
Deleted account.
 
Because of JD?
 
@DanielSank Not sure if that's why, but indeed the whole SE account is gone.
 
We don't know the full story.
 
@0celo7 Is there any relevant chat transcript that's still public?
 
6:25 PM
But something happened with JD, CW got suspended, then deleted his account.
 
Also CC @ACuriousMind
 
@EmilioPisanty AFAIK, no.
Chris's comments were deleted, and everything else was behind closed doors.
 
@DanielSank Something like that is fine too
 
@0celo7 suspended or chat-banned?
 
@EmilioPisanty Chat banned for a day.
 
6:26 PM
@EmilioPisanty There is no visible evidence left. CW made some Not Nice comments, was chat banned for a day, never returned and had his account deleted. We don't know anything more.
 
Can we remove a user for being extremely disruptive, even if there's no direct evidence of trolling?
 
@ACuriousMind OK. Were you present at the time?
 
@EmilioPisanty At the time of the comments? Yes
 
Let me ask that we avoid speculation about what happened to Chris. It's not a punishment imposed for something that happened on this site, but I don't know any details beyond that, and AFAIK nobody else here does either.
 
@DavidZ Sure. I've been pondering whether to write directly (just to say sorry you're gone), and I wanted to brush up on the public knowledge.
 
6:28 PM
9 page lab report
Still have to do analysis, problems, conclusion
when will it end??
 
@Secret That is way old
 
@Secret what?
 
cycle through all the letters of the alphabet to find all CW messages
 
@Secret that's basically the measurement problem, which I'm not going to discuss.
 
6:30 PM
Okay guys
I really need some help with my maths
@ACuriousMind Are you busy?
 
@ACuriousMind @Secret pretty much my position too.
 
@BernardMeurer Only busy with the other conversations in this chat :P
So go ahead and ask
 
@ACuriousMind <3
 
why not ask me?
 
@0celo7 You too
 
6:32 PM
Too busy
got a lab report due in 2 hours
I really need like 3
 
@EmilioPisanty Well I am not exactly sure if my question is really the measurement problem, because I am not asking whether the state do collapse, but rather, why it collapse on eigenstates and never superposition states of nondegenerate eigenstates... Or is that still part of the measurement problem?
 
I blame Kobayashi-nomizu
 
I forgot: Did we have any unresolved topic before the lengthy readme digression? :D
 
We started today by defining an Inductive set as: $$X\subset \mathbb{R}, X\text{ is inductive iff }x\in X \Rightarrow x+1\in X$$
 
For the love of the almighty potato, use \text for words that are meant to be words
6
 
6:34 PM
@DavidZ Also: while there's good reason for laying off the speculation, it is undeniably a relevant aspect of the site's life. Chris's departure has a clear and definite negative impact on the site's ability to address a broad swathe of astrophysics. If (if) it was caused by other users being disruptive-while-keeping-the-formal-rules, then that is a cause for concern.
 
@ACuriousMind thanks, didn't know how to do that :)
Okay, does that definition make sense?
 
@BernardMeurer Yes, although I have seen "$1\in X$" as an additional requirement to be called inductive
 
@BernardMeurer \text for longer stretches; \mathrm works but it kills any spaces.
 
@EmilioPisanty fair enough; I guess what I really want to ask is that everyone refrain from acting like they know what happened to Chris when they really don't.
 
@ACuriousMind Seems reasonable, but let's go with the one the old man gave
 
@BernardMeurer what the hell
what kind of class is that?
 
Continuing, we then proves that $\mathbb{R}, \mathbb{R}^{+},\mathbb{Q}$ are inductive
 
PhD level logic? I've never even seen that
 
@0celo7 Introduction to analysis
 
What the hell?
 
6:37 PM
Get over it @0celo7
 
@0celo7 can you show me your lab report i'm curious how the quality of our reports differ
 
I've never even heard of these things
@Obliv Mine is literal trash
@Danu Get over what?
 
Which is fine I got that
 
vzn
for makers/ hackers/ "experimenters" etc like @Bernard :)
 
I've never heard of these things
 
6:37 PM
@Secret It's still "why do projective measurements work like they do instead of otherwise", which is much too close to the MP for me to wade into at the moment.
 
ok then
 
then he showed us something called (Literal translation) Principle of the finite induction (dunno if this is the name in english)
which says:
 
@0celo7 give it to me...
 
vzn
@EmilioPisanty plz do contact him & let him know he is missed & ask/ urge him to rethink/ reconsider
 
If $A$ is an inductive subset of $\mathbb{N}$, and $0\in A$, then $A=\mathbb{N}$
 
6:39 PM
o.o
Is this actual math?
 
what is a subconj.
 
@BernardMeurer "subconj."? Do you mean subset?
 
@0celo7 Yes, this is how a European first semester rolls :P
 
@Obliv If in a parallel circuit, the currents add up to more than the current in the power supply, wtf went wrong
 
6:40 PM
Proof: $$A\subset \mathbb{N};\mathbb{N}\subset A \Rightarrow \mathbb{N}=A$$
 
@ACuriousMind @EmilioPisanty Q3. Why do classical observables cannot be operators, is it because the classical state space is a set hence there is nothing it can act on? (thus we don't see something like a poisson bracket acting on some function like e.g. $\{A,B\}f(q,p)$)?
 
Don't say measurement error
or human error
 
that's the only possible option if you're not gonna give any detail about the procedure
 
@Secret I'm not sure why you think I'm the guy to answer your questions.
 
b/c $\mathbb{N}$ is the intesection of all inductive subsets of $\mathbb{R}$ than contain 0
 
6:41 PM
@Secret Koopman-von Neumann mechanics makes your question non-sensical.
 
Literally hooked up 3 resistors in parallel, measured the current in the power supply, measured the current around each resistor, added them up, got more than the power supply
like 1% more
 
All of this makes a lot of sense to me
until this goof started showing "Proof by induction method"
 
@ACuriousMind Crazy
 
Which was like this (this will take a while):
 
@BernardMeurer now knows more math than me
I don't get it
 
6:42 PM
@0celo7 you sure you did the math right 8^)
 
@Obliv Yes.
 
@DanielSank : no, not because of JD. He posted a comment calling for downvote collusion and banning, I said that's not very nice and flagged it, then he got some kind of chatban, 1 day I think, then he decided he wanted to leave PSE.
 
Literally addition
 
> I'm a PhD student at the CDT in Controlled Quantum Dynamics at Imperial College London, and at the Max Born Institute in Berlin. My research is on strong-field and ultrafast physics, and I study tunnel ionization and high-harmonic generation.
=>This fit the description of a "quantum guy"
 
incorrect.
 
6:43 PM
@Obliv for the current, you add them
what is wrong with that?
 
@Secret May I point out that you never really interacted with Emilio in chat before and now just started pinging him with your questions?
Just because people may be qualified to answer your questions they still can get rather irritated if you ping them with those questions without any sort of prior rapport.
 
$$P(n) = \sum\limits_{k=0}^{n}\frac{k}{(k+1)!}=1-\frac{1}{(n+1)!};\forall_{n\in\mathbb{N}‌​}$$
 
@Secret Not sure how to put this, but I'm going to pass on your question.
 
@0celo7 physics.bu.edu/py106/notes/Circuits.html you have to get the equivalent resistance and then divide the voltage by this quantity and you'll get the current
not just addition
 
6:45 PM
The resistors adding inversely is equivalent to the current adding simply @Obliv
 
but nvm, that's all my quantum questions for today
 
yea but instead of measuring the current maybe you should try this method
you'd only need to know the voltage & resistances
 
Okay, fine, we then show that the solution set for this is $$A=\{n\in\mathbb{N}:P(n)\}$$
 
maybe u made a mistake measuring the currents
 
Does that make sense @ACuriousMind?
 
6:48 PM
??? Three messages over a time span of over a year don't even mean he remembers you. I certainly don't keep track of users I spoke that rarely, and I would be rather confused if they started pinging me with their questions. As a matter of fact, I've ignored some particularly obnoxious variants of these.
@BernardMeurer I think you may have messed up what exactly $P(n)$ there is supposed to be
What is meant to be going on is this: We have the proposition $P(n)$, which is true for a given $n$ if $\sum_{k=0}^n \frac{k}{(k+1)!} = 1-\frac{1}{(n+1)!}$ holds and false otherwise.
 
and we can prove this to be true $\forall_{n\in\mathbb{N}}$ by proving: $$\begin{cases} 0\in A, & P(0)\text{is true} \\ A\text{ is inductive}, & \forall_{n} P(n) \Rightarrow P(n+1)\end{cases}$$
 
@0celo7 I want to do cool derivations and use beyond basic algebra in my lab reports but the procedures rely on such simple theory it's not fair :(
 
@BernardMeurer You're using too few }'s in the subscripts
 
@Obliv how?
it's a digital ammeter
 
Your set $A=\{n\in\mathbb{N}\mid P(n)\}$ is then the set of all numbers for which that equation is true. The idea is now to show that $A$ is an inductive set containing $0$, since then you've shown that $A=\mathbb{N}$ without checking the truth of $P(n)$ for every $n$ individually.
 
6:51 PM
ACM: Noted, I will try to gain some rapport for future cases like these
 
@ACuriousMind yeah, I got it this far
this all makes sense to me
then comes his proof
which I copied from the board verbatim and will paste here
and that I did not understand one bit
 
So he shows it for 0, then shows that the case $n$ implies the $n+1$ case (hopefully)
 
@0celo7 idk dude maybe the wires at the end of the circuit had less resistance.
 
@BernardMeurer Okay :) Then let me just point out that the $P(n) = $ further up was bad notation because $P(n)$ is a logical proposition which is not equal to the sum you wrote it is equal to
 
The base case (checking $P(0)$ in this case is usually easy)
@ACuriousMind He should've written brackets around the second quality
 
6:54 PM
@ACuriousMind Bad notation on my part there, he denoted it differently but idk how to do it on LaTeX and was lazy :P
 
(I'm commenting for Bernard, not for you ACM ;) )
 
@BernardMeurer Okay. I just thought you were confused about what $P(n)$ is because that is a frequent source of confusion if not stated clearly.
 
$$\sum\limits_{k=0}^{n}\frac{k}{(k+1)!}=\sum\limits_{k=0}^{n}\frac{k}{(k+1)!}+(n‌​+1)/((n+2)!)=1-\frac{1}{(n+1)!}+\frac{n+1}{(n+2)!}=1-\frac{1}{(n+2)}$$
 
that's a beautiful line of latex there @bernard
 
$$\sum\limits_{k=0}^{n}\frac{k}{(k+1)!}=\sum\limits_{k=0}^{n}\frac{k}{(k+1)!}+\fr‌​ac{n+1}{(n+2)!}=1-\frac{1}{(n+1)!}+\frac{n+1}{(n+2)!}=1-\frac{1}{(n+2)}
\sum\limits_{k=0}^{n}\frac{k}{(k+1)!}=\sum\limits_{k=0}^{n}\frac{k}{(k+1)!}+\fr‌​ac{n+1}{(n+2)!}=1-\frac{1}{(n+1)!}+\frac{n+1}{(n+2)!}=1-\frac{1}{(n+2)}
\sum\limits_{k=0}^{n}\frac{k}{(k+1)!}=\sum\limits_{k=0}^{n}\frac{k}{(k+1)!}+\fr‌​ac{n+1}{(n+2)!}=1-\frac{1}{(n+1)!}+\frac{n+1}{(n+2)!}=1-\frac{1}{(n+2)} $$
 
6:58 PM
forgetting a { or } somewhere
 
@BernardMeurer you forgot the slashes before the "sum" so the \limits doesn't know what to do
 
Background for my trio of questions today: I have just finished reading the two Susskind books yestdy. I then became curious of the mathematical analogies and difference between classical and quantum (but unlike most, being slightly more familar with QM since I learn that first in uni, I tend to ask the opposite question on why classical behave that way, why classical does not behave like QM, why QM behave this way etc.). That way I can identify the quantum only things to better study about them
 
In other news, it's unnecessary to use \limits after \sum in display mode.
$$\sum_{hi}^{there}$$ works just fine
Lol ironic
 
6:59 PM
(In the photo I am going to post is a summary of the content of the 2 Susskind books)
 
@BernardMeurer Want me to edit for you?
(I can do it if you like)
 
$\sum\limits_{k=0}^{n}\frac{k}{(k+1)!}=\sum\limits_{k=0}^{n}\frac{k}{(k+1)!}+\fr‌​‌​ac{n+1}{(n+2)!}=1-\frac{1}{(n+1)!}+\frac{n+1}{(n+2)!}=1-\frac{1}{(n+2)}$
 

« first day (2147 days earlier)      last day (2787 days later) »