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Jim
12:00 PM
@rob that's "literaRy" not "literaLLy"
 
lol
 
rob
@Jim ... in which Tom Sawyer is "literally rolling in wealth." I love the catalogue of gifts he's received, but I don't believe he rolls in them.
 
Jim
::Jim is done::
 
rob
descriptive linguistics for the win!
 
Jim
**Jim's express Dictionary**
Literally:
adv.
1) Exactly as expressed; not figurative.
2) Figuratively
 
12:04 PM
lol
@rob did you not realise he is a dog?
 
why are you people up so early
 
Jim
@0celoñe7 time zones
 
rob
@djsmiley2k Actually one of Tom's rewards is "a dog collar (but no dog)"
 
^^^
 
@Jim In Canadia it is \le 8
 
12:06 PM
So, what does that mean then ? :)
 
Jim
@0celoñe7 yeah, and I work for a living
8 isn't early
 
I started work at 7am :(
I think my brain has just had it with this office, i was fine on the drive in... got here, sleeep\zzzzzz
 
Jim
also, in canada it's anywhere from 5 to 9:30
 
@djsmiley2k are you a dj also?
 
@Jim yeah, well
I work too, but thank god I just show up whenever
and stay late
 
12:08 PM
lol
Do you work for OVH o_O
 
@djsmiley2k No, random
 
:D
@DawoodibnKareem I somehow flipped from one to the other, by changing jobs
I can only theorise that someone, somewhere, flipped the other way and is now wondering where their pens have gone.
As pens cannot be created, nor destroyed, they merely change form...
 
6 hours ago, by The Raiders of Las Vegas
There's a third type, namely those that don't know how to use a pen :P
 
Anonymous
 
Anonymous
Why doesn't netbeans give any output? :/
 
Anonymous
12:23 PM
@DawoodibnKareem do you know?
 
Anonymous
This is my first time with netbeans
 
Anonymous
I used bluej earlier
 
Anonymous
Should be some problem with the Settings
 
Anonymous
Can't figure it
 
Anonymous
12:30 PM
Phew
 
Anonymous
Got it fixed
 
[Random] Quantum sock:
Suppose you are in a dark closet filled with "quantum socks"
where all socks are pairs of entangled states such that when measured, the color of one sock and its pair always turned out different no matter what color it is
 
...
 
There are 20 socks, which makes 10 pairs of entangled socks in the closet
and when picked up and taken out of the dark closet (which we can assume that will be a measurement since the color will be determined) it can be either red or blue
Calculate the probability to get two socks of matching color
 
There is nothing quantum about just having ten pairs of differently colored socks.
 
12:44 PM
indeed, because we don't know whether the two socks we picked up are part of an entangled pair, the probabilities should be classical, I think
 
They are also not "entangled". They are just pairs of differently colored socks.
 
yup. The quantumness meter is at zero so far.
 
If you're talking about entangled states, there is no need to confuse the issue by calling these states socks. If you're talking about actual socks, there is no need to confuse the issue by calling them quantum or entangled.
 
Ditto for the entanglometer.
 
uh, the 10 pairs of socks are prepared in a way such that they basically act like 10 pairs of entangled qubits, such that when measured, their observables (in this case, red vs blue) always anticorrelate. Their color is not determined before being taken out of the closet
Here's a more rigorous version by taking out the obvious joke of finding socks in a dark closet in case it is confusing:
 
rob
12:48 PM
Entanglement turns interesting when you involve non-commuting observables.
There's a nice book by Bell where he compares entanglement to finding you only have one glove in your pocket.
If it's your left glove, you know right away that the glove on your countertop at home is a right glove. But that's not interesting.
For the socks, you could define three color axes, red, green, and blue
Measure the color along one axis by looking at it in a red light, or a blue light, or a green light --- the sock is either bright or dark
 
[Rigorous version]
Suppose there's a box containing 20 electrons, which they are entangled to form 10 entangled pairs. All of these are singlet states (thus there are 10 singlet states) thus whenever a pair is measured, their spins always anticorrelate. Now, calculate the probability to measure any two electrons from the box, such that you get them both spin up
 
rob
"Entangled socks" would also still be different colors under magenta lights, cyan lights, or yellow lights.
 
@Secret so? it is irrelevant whether they are entangled or not. For the observables you've specified so far, it's perfectly possible to provide a non-entangled model that will reproduce all the observations, and your observables will be unable to distinguish between the entangled and the non-entangled versions.
@Secret ^ ditto for that version, too
@Secret You should give some serious thought to a disciplined and thorough reading of Nielsen and Chuang.
 
rob
So what's interesting is if you look at a sock under red light, and I look at its partner under magenta light.
Entangled socks and classical socks have different correlations under those mixed tests.
 
Emilio: Exactly, this joke inspired question is in some sense really a demonstration of no communication theorem, if you don't know which are the correlated pair, then it is just an ordinary probability question (I think...)
Meanwhile, I think rob might be actually talking about the scenario where things gets interesting
 
rob
12:55 PM
@Secret I'm usually trying to make things more interesting.
 
@Secret what is the point of this.
 
@djsmiley2k Me attempt to put a quantum twist to the famous "find matching socks in a dark closet"
 
I know neither if this joke is funny, or not funny, and i've even observed it!
Boom, there's a joke.
 
Jul 21 at 15:42, by AccidentalFourierTransform
user image
 
@rob is that an allusion to measuring bell states along an axis somewhere between xyz axes, and show that the outcomes of their spins differ between classical and entangled states?
 
rob
1:01 PM
@Secret Just so
@Secret In Bell-type measurements, entanglement doesn't add anything if the two measurements are on parallel axes or on orthogonal axes.
 
ah, you are referring to that cos shaped correlation diagram, where in classical, it will just look like a sawtooth
 
rob
@Secret I think that you could construct such a correlation diagram in the experiments I have in mind, yes.
 
Quantum sock ver 2: (This time, I am pretty sure we can do quantum on it) Suppose you are in a dark closet, and there are 20 socks, which once again can be either red or blue if taken out of the closet. The socks are entangled in such a way such that the sock that is picked up always has a different color from the other 9 socks. Calculate the probability that two random socks taken out of the closet will have the same color
(Actually, I am not sure if such generalisation of GHZ state can be written down... need to check)
Let $\{red,blue\} = \{0,1\}$ Then
$$\lvert socks\rangle = \frac{1}{\sqrt{20}}(\lvert 1000...0\rangle + \lvert 0100...0\rangle + \cdots + \lvert 0000...1 \rangle)$$
uh, that does not look really entangled to me... hmm...
if it is 2 qubit, then we have the bell states:
$$\lvert socks\rangle = \frac{1}{\sqrt{2}}(\lvert 01\rangle \pm \lvert 10\rangle),\lvert socks\rangle = \frac{1}{\sqrt{2}}(\lvert 11\rangle \pm \lvert 00\rangle)$$
and then, the singlet state will ensure anticorrelation
o nvm then, it is all good, mistaken $\lvert abcdef...z\rangle$ as state vectors with many components and not tensor product of state vectors...
now to check entanglement...
 
1:22 PM
I hit a birb with my car :(
@Secret $\mathrm{div}\, B=0$ distributionally
 
Is it dead?
 
@skullpatrol idk I didn't stop to examine the carnage
my car seems fine
 
ok, by definition of entanglement in terms of tensor product, the state is entangled, as required
however, I think I might need some minus signs somewhere...
 
@0celoñe7 Here we have suicidal seagulls on the road. But of course I am mostly afraid of the moose.
 
Interestingly, I stopped asking that question
0
Q: What is a real world analog to spin?

VegetableeggSpin is an elusive concept in physics which seems to have no "physical world" parallel -- that is, something that we can see to compare it to. We know spin can be defined as the quantifiable (it is quantized at 1/2 units) form of angular momentum. But, spin has direction too (because all particl...

spin is already something real, I think OP is asking what the classical analogue is, in which case there is none
(i think)
 
1:49 PM
Hello
Q. A thermometer is kept in air at direct sunlight. Whose temperature does the thermometer read, of air, of sun or something else?
 
@GerWyn the surface of the sun, no?
 
@Ocelone7, what does that mean?
 
Thanks for your advice , Does Griffith has textbook on EM? — user46899 2 mins ago
 
@GerWyn air
 
::facepalm::
somebody stop me from doing something rash
 
1:54 PM
@0celoñe7 What?
 
@user685252, how?
 
@GerWyn what is the thermometer in contact with?
 
does the amount of heat transfer by radiation enough to heat the thermometer to the surface of the sun, but I think convection should be quicker and dominating the process, right
 
Air, direct sunlight
 
so it should not be able to get to the surface of the sun temperature
 
1:57 PM
Can't it get tempretaure from sun rays?
 
What is "temperature?"
 
@EmilioPisanty stop!
 
@0celoñe7 Have you seen thermometers in sunlight go up to thousands of Kelvin? :P
 
::Throws cold water at Emilio to cool him down::
 
@user685252, temperature is degree of hotness or coldness of a body
 
Anonymous
1:59 PM
I guess some people don't know that electrodynamics and electromagnetics refer to the same thing. Maybe you could just point that out... (As Griffiths' book is named "Introduction to Electrodynamics")
 
@GerWyn and how is that hotness or coldness of a body transmitted to the thermometer?
 
Through contact
 
yes
the collisions of the air molecules
 
IIs "the collisions of the air molecules" another method?
 
@user685252 Objects in direct sunlight can get hotter than the surrounding air.
The transfer of heat is not solely from the air but also - obviously - through the radiation from the sun.
The temperature of the thermometer in direct sunlight is neither that of the air nor that of the sun.
 
2:06 PM
@ACuriousMind, could you please say why/how does that happen?
??
 
nvm
 
2:21 PM
@ACuriousMind no, I tend to not put thermometers in the sun for that very reason
 
@0celoñe7 In case they heat up to the temperature o the Sun? :-)
 
@JohnRennie yes -- or worse
 
2:48 PM
Hey hbar.
Are these all the physically acceptable conditions on a wavefunction?
I vaguely remember being told as an example, something about the indeterminacy of the normal component of $\nabla \psi$ at an infinite potential surface?
So long back, I don't even remember now.
 
@GerWyn I'm not sure what exactly you want to know - without the sunlight, the thermometer would have the temperature of the air. If it additionally absorbs sunlight, it becomes hotter than that.
 
Anonymous
@ACuriousMind That's a bit misleading imo. In presence of sunlight even the surrounding air will heat up. So the thermometer's temperature will be more or less equal to the surrounding's air's temperature. (Assumming similar specific heats)
 
@ACuriousMind What does $Z_q$ look like
Is it for, say, $q = 2$, just $-1, 0, 1, -1, ...$
 
The $V \rightarrow \infty$, $\psi \rightarrow 0$ argument looks fine, but is there any condition from the potential on the KE term of Schrodinger equation?
 
Or does it not go over negative values
Apparently it does not
nvm
 
2:58 PM
@Blue Well, of course the thermometer heats the air - but I don't think we consider "air temperature" here to be the temperature of the infinitesimally thin layer of air above the thermometer
 
@Blue Sunlight doesn't heat air directly. The sunlight will heat the thermometer and the thermometer will heat the air.
 
And the sunlight doesn't heat the air as much as the thermometer
 
@Slereah what
 
Anonymous
@JohnRennie I'm a bit confused. Are you saying that in absence of the thermometer the sunlight would not heat up the air?
 
@Blue Yes. Air does not absorb sunlight.
 
3:02 PM
@Slereah I'm not sure I understand the question
 
lolwut Google !!
 
what prevents the sunlight exposed thermometer to go up thousand degrees (because it will theoretically be if it absorbs every single photon emitted from the photosphere), is it because the convection to the surrounding air draws the heat away fast enough?
 
Hi @heather
 
Ooooo, infrared emitted from the thermometer and the sun's distance
 
@Secret It doesn't absorb every single photon from the photosphere, it absorbs a very tiny fraction of the radiation.
 
Anonymous
3:09 PM
@JohnRennie I knew that air doesn't absorb most visible wavelengths. But it obviously does absorb infrared. And sunlight does contain infrared radiation too. Also, sunlight will be absorbed by the ground which will heat up the air above.
 
hello
 
right, makes sense
 
@Blue ...if air absorbs infrared, how do infrared cameras work?
 
@ACuriousMind residual radiation
 
If you want to be pointlessly pedantic, then the visible light we see is also "residual radiation" that the air didn't absorb :P
 
3:12 PM
^
 
Anonymous
@ACuriousMind Ok. Some part of air (around 10%) absorbs while the other 90% doesn't (mostly N2 and O2).
 
@Blue Air has effectively zero absorptance at wavelengths where the intensity of light from the Sun is significant.
 
@ACuriousMind: Any comments?
18 mins ago, by The Dark Side
The $V \rightarrow \infty$, $\psi \rightarrow 0$ argument looks fine, but is there any condition from the potential on the KE term of Schrodinger equation?
 
@TheDarkSide Can you prove that psi goes to zero at infinity?
 
Some guy in a physics facebook group suggest a mix of EM field tensor and the einstein tensor. Surely, T is where the F is (because the field is considered part of the energy momentum and hence part of T), thus making this redundant?
 
3:15 PM
@JohnRennie Well...significant depends on what you're looking at. E.g. $CO_2$'s infrared-absorbent properties are sometimes significant...but not when we are looking at a thermometer ;)
 
@0celoñe7 You are obviously contemplating some mathematical argument, but I'll say that if $\psi$ does not $\rightarrow 0$ as $x \rightarrow \infty$, the wavefunction won't be $L_2$ normalizable.
 
@ACuriousMind how the hell do you know about infrared properties of CO2
 
In physics, Maxwell's equations in curved spacetime govern the dynamics of the electromagnetic field in curved spacetime (where the metric may not be the Minkowski metric) or where one uses an arbitrary (not necessarily Cartesian) coordinate system. These equations can be viewed as a generalization of the vacuum Maxwell's equations which are normally formulated in the local coordinates of flat spacetime. But because general relativity dictates that the presence of electromagnetic fields (or energy/matter in general) induce curvature in spacetime, Maxwell's equations in flat spacetime should be...
yes, source term
 
@ACuriousMind $CO_2$ absorbs at relatively long IR wavelengths. That's why it absorbs black body radiation emitted by the Earth. It does not absorb much of the light from the Sun.
 
So, that's a physical argument, a smaller subset of maths that way.
 
3:17 PM
@TheDarkSide That is absurd.
 
@TheDarkSide I have never seen a physical argument for the $\psi\to 0$ property other than "it gives nicer functions"
Nothing in the basic structure of quantum mechanics restricts function that way
 
Nvm I was being dumb
 
Anonymous
@JohnRennie I agree with that. My point was that in presence of sunlight the surrounding land/ground will also heat up and thus the air above. The thermometer temperature won't be much different from the surrounding air's anyway. You are correct in saying that air won't absorb much of the shorter wavelength IR that sun emits.
 
One can make an argument that it might not be possible to prepare the state corresponding to functions without that property in finite time, but that just makes them difficult to realize, not forbidden
@Blue I've seen thermometers show 60° C on a hot day in sunlight. I'm reasonably certain the air wasn't 60° C hot.
 
@Blue try the experiment.
The thermometer will get a lot hotter than the air around it.
 
3:20 PM
@ACuriousMind In all fairness there are potentials for which the $C^\infty$-eigenfunctions have decay at infinity.
I had a discussion with yugibb about this.
 
@0celoñe7 Physical states are not restricted to be eigenfunctions
 
Ah, he is talking about a generic state?
 
I think there's also something like being able to make all 1d solutions to the Schrödinger equations continuous or differentiable for nice potentials, I remember a Qmechanic post about that
 
@DawoodibnKareem i can swear to the truth of this, except it's also true with pencils, and the true-ness of this goes up in an exponential fashion as you approach a middle or high school.
 
Anonymous
@JohnRennie Okay. But I still didn't get a reasonable explanation as to why :/ Is it because the specific heat of mercury much lesser than air ?
 
3:23 PM
@DawoodibnKareem Actually I used to lose pens before Grade 6. Now I tend to acumulate pens from the various conferences and events I joined
 
Here's an astronomy question, motivated by today's XKCD.
 
@ACuriousMind Please help me understand this. What about the global conservation of probability without this?
 
@ACuriousMind That should just be Picard-Lindelof, no?
 
@Blue thermometers heat up fast because they absorb the sunlight directly. Air heats up slowly because it has to be heated indirectly, and air currents carry the hot air away and replace it with cooler air.
 
@0celoñe7 Oh! How?
 
3:25 PM
question: @Mithrandir24601 said the other day that the matrix that represents a measurement is $\begin{bmatrix}0&0\\0&1\end{bmatrix}$, but how can a measurement be represented by a matrix? Measurement is probabilistic.
 
@TheDarkSide Consider a function $\phi\in C^\infty(\Bbb R)$ with support in $[-1,1]$, $\int_\Bbb R \phi^2=1$.
 
How 'sharp' will the shadow cast by the upcoming solar eclipse be? The map in the first panel and the image in the last panel of the aforementioned XKCD strip makes it look like the boundary will be pretty well-defined, but I wonder how realistic that is.
 
Measurements are represented by projectors (unless you consider the full system-device), and thus it is nonunitary
 
By squeezing $\phi$ one can make a function $\phi_h$ with support in $[-1,1]$ and $\int_\Bbb R\phi_h^2=h$.
 
@0celoñe7 I don't know that much maths. What's $C^{\infty}$?
 
3:26 PM
@TheDarkSide Continuously differentiable to all orders
 
I see. Let me think. And what's "support" in wawa?
 
wawa?
 
@Semiclassical The area where the eclipse is total is actually pretty narrow because the Sun and Moon are about the same angular size. There is only a small region where they overlap perfectly.
 
@Semiclassical Feynman slang for whatever.
 
Hmm, interesting.
Ah. @TheDarkSide
 
3:28 PM
@TheDarkSide $\mathrm{supp}\, f=\overline{\{x:f(x)\ne 0\}}$
@TheDarkSide I have to get back to work, but @Semiclassical or @ACuriousMind can finish my thought
 
cya
 
@TheDarkSide What about it?
 
Anonymous
@JohnRennie I see. I just now looked up the values of specific heats of air and mercury. It seems that mercury's is around 0.140 J/gmK while air's is around 1 J/gK. That's probably another reason in addition to yours because $\Delta T = \frac{Q}{mc}$. And yup, your reasoning seems to make sense to me.
 
I'm not sure what "global conservation of probability" means in the first place, or why it would require $\psi(x)\to 0$ as $x\to\infty$.
 
3:29 PM
@JohnRennie I imagine there's pictures out there which would settle things more definitively
This is pretty cool:
 
@ACuriousMind See, I am not as skilled as you guys are in Maths, but lets say we are addressing basic level introductory QM, where we are addressing $\psi (x)$ over one-D with $x$ allowed to vary to the infinities.
 
@Semiclassical if the eclipse occurs when the Earth is nearest the Sun and the Moon is farthest from the Earth you get an annular eclipse and there is no point of the Earth where the eclipse is total.
 
In this case, with the probabilistic interpretation,
the particle gotta be somewhere.
 
If the Earth is at aphelion and the Moon at it closest point then the Moon has a significantly larger angular width than the Sun and you get a wide area of totality.
 
Huh, I hadn't thought of that but it makes sense. The closer the Moon is to the Earth, the larger the shadow it'll cast.
 
3:33 PM
So it's not that interesting a question. The answer is it depends.
 
and so we say $\int_{-\infty}^{\infty} \vert \psi(x) \vert^2 dx = 1$
 
@TheDarkSide Yes. But that is not equivalent to $\psi(x)\to 0$ as $x\to\infty$.
 
Now, one can always bring in continuity equation here for the probability current, and say something like $\partial_{\mu} j^{\mu} = 0$ holds.
@ACuriousMind In a minute, sir.
 
There are non-square-integrable functions that go to zero as we move to infinity, and there are square integrable functions that don't go to zero. See physics.stackexchange.com/q/331976/50583
 
3:38 PM
My example would have been smooth and unbounded!
@ACuriousMind I asked you to continue the thought!
 
@ACuriousMind The example given there of a square-integrable function which doesn't go to zero at infinity is kinda disgusting.
It's definitely an example, but ew.
 
@Semiclassical I came up with one that's not even bounded
 
@Semiclassical No one said this would be pretty business ;P
 
lolyes
 
@JohnRennie this SEM has a triple monitor setup
I think that's my destiny
 
3:40 PM
though as Emilio's answer notes, one is usually not interested in the wavefunction as just a generic function; rather, one usually wants it to be a solution to the Schrodinger equation.
(usually that'd be the 'time-independent Schrodinger equation', which is good because I remember that things can get weird once you allow time-dependence)
 
@Semiclassical Yeah, I think it has to be clear which properties are generic requirements for wavefunctions and which are special properties of solutions for particular potentials, though
 
@ACuriousMind While that's an informative link, continuing in the same spirit as the linked question, is that an example of "mathematical pathological conuterexample"? I mean, is there any physics connection with that?
 
Of course, this is all in the context of bound states.
 
@Semiclassical What's stranger to me is: does Lebesgue measure have physical meaning
 
@0celoñe7 That's over a finite range, no?
 
3:43 PM
Well, does the definition of the Riemann integral have a physical meaning?
 
@TheDarkSide Well...that depends what you mean. E.g. a plane wave solution is physically very important and it's not even square-integrable!
 
After all, if states are in $L^2$, we must identify those which differ on a null set
 
@ACuriousMind But a superposition is !! :P
 
@ACuriousMind just to emphasize the obvious, that's exactly the scattering case.
 
@TheDarkSide You can sum a bunch of translates with area $1/2^j$
the total area is $1$, and the peaks blow up as $x\to\infty$
 
3:46 PM
@0celoñe7 Again, does this arise somewhere in Physics, or is this only a mathematical artifact?
 
@TheDarkSide Yeah, so since these functions not vanishing at infinity are part of our Hilbert space, in principle some perfectly ordinary wavefunctions that do vanish at infinity might be written as superpositions of these.
 
@ACuriousMind But a superposition of plane waves, is !! No?
 
I guess a way to put it would be: If you're doing a time-independent bound state problem, can you require $\psi(x)\to0$ at $\infty$ on physical grounds?
 
We should note that there are no infinite plane waves in the real world ...
 
I guess those 'physical grounds' would correspond to some statement about the confining potentials.
 
3:50 PM
@Semiclassical No.
 
I'll be honest, though, this kind of thing (while certainly important for speaking correctly) is hard for me to stay interested in.
 
@TheDarkSide Here's another terrible thought: Since functions in $L^2$ are merely equivalence classes, it's not even clear what it means for "a wavefunction" to occur physically. I can declare that my wavefunction has the value 4.323524 at all rational numbers and I don't change the physics one bit.
 
@JohnRennie Sure. But all finite length/duration wavepackets can be written as superposition of them, no?
 
@Semiclassical It's not true -- there are Hamiltonians for which negative energy eigenstates do not decay.
 
So I consider it pretty pointless to try and decide whether or not certain wavefunctions are "physical" or not.
 
3:51 PM
So when you write your eigenbasis some of the functions don't decay.
 
@TheDarkSide No, you cannot construct a wavepacket that requires a superposition of infinite plane waves - just an approximation to such a wavepacket.
 
@ACuriousMind I literally said that
 
@ACuriousMind I have a naive definition when this won't make sense, maybe you can tell me in less mathy terms why this naive argument fails.
 
@0celoñe7 Yes, but probably not in a way that The Dark Side understood :P
 
@0celoñe7 Eh, that doesn't necessarily contradict my point. Are those Hamiltonians physically reasonable? (though that feels like weasel words)
 
3:52 PM
@JohnRennie Maybe I should get a 4K monitor for general use, a Gsync 1440p mintor for gaming, and my current 1080p monitor as another one
@Semiclassical No. I'd have to check Reed and Simon to be sure, but for lots of reasonable potentials, the functions do decay.
 
What I'm wondering is what the confining potential would be like in that case.
 
Reasonable being like $V\in L^p+L^\infty$ for some $p$ depending on the dimension of space.
 
mmkay. That's what I'm getting at with 'physical grounds.'
 
@0celoñe7 three monitors ... and an overdraught :-)
 
Though that again is a bit weasally.
 
3:55 PM
@ACuriousMind If your function is $f(x) = 4.323524 \ \forall x \ \in ]-\infty, \infty[$
 
No, that's not what I said :P
I said at all rationals
 
@Semiclassical This is all related to the question of when the Hamiltonian is legitimately self-adjoint.
 
Yeah, I can buy that.
 
@ACuriousMind Ah.
 
Fun fact: I'll be TAing for a quantum mechanics course this fall.
So this is probably good review for me.
 
3:57 PM
I pick any "normal" wavefunction $\psi(x)$ with $\int \lvert \psi\rvert^2 = 1$, and then I compare it to $\phi(x) = \begin{cases} 4 & x\in\mathbb{Q} \\ \psi(x) & x\in\mathbb{R}-\mathbb{Q}\end{cases}$
 
Now I am moving into less familiar grounds, ACM
 
@Semiclassical Please make it a course on operator theory and whatnot
I want to see the reaction
 
Not my choice :P
 
@Semiclassical Dang.
 
Anonymous
@Semiclassical Are you a graduate student?
 
3:57 PM
Yeah.
 
Physically, $\psi(x)$ and $\phi(x)$ encode the exact same quantum state.
 
Anonymous
@Semiclassical Which subject?
 
I want to teach a class "mathematical physics"
 
What?
 
Condensed matter theory, though my specific interest is semiclassical methods.
 
3:58 PM
What what?
 
@ACuriousMind OK. I see what you mean.
 
Anonymous
@Semiclassical ....and hence your name :P
 
So this makes asking which sorts of wavefunctions are "physical" pretty pointless imo - $\phi$ is just a horrible function, yet it is "physical". The more interesting question to ask is when we can ensure that every state has at least one "nice function" that represents it.
 
It's been suggested I change it to "Semicynical". I'm mulling it over.
 
3:59 PM
nah
Semi Tough was a good movie
 
@ACuriousMind Perfectly valid point. Except for, any physical process where $\phi(x)$ occurs ? :P :P
 
@ACuriousMind aka "measure zero sets are annoying"
 
@Semiclassical $d^2/dx^2-x^4$ is not self-adjoint.
 

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