A wave function in quantum physics is a mathematical description of the quantum state of an isolated quantum system. The wave function is a complex-valued probability amplitude, and the probabilities for the possible results of measurements made on the system can be derived from it. The most common symbols for a wave function are the Greek letters ψ and Ψ (lower-case and capital psi, respectively).
The wave function is a function of the degrees of freedom corresponding to some maximal set of commuting observables. Once such a representation is chosen, the wave function can be derived from the quantum state.
For a given system, the choice of which commuting degrees of freedom to use is not unique, and correspondingly the domain of the wave function is also not unique. For instance, it may be taken to be a function of all the position coordinates of the particles over position space, or the momenta of all the particles over momentum space; the two are related by a Fourier transform. Some particles, like electrons and photons, have nonzero spin, and the wave function for such particles includes spin as an intrinsic, discrete degree of freedom; other discrete variables can also be included, such as isospin. When a system has internal degrees of freedom, the wave function at each point in the continuous degrees of freedom (e.g., a point in space) assigns a complex number for each possible value of the discrete degrees of freedom (e.g., z-component of spin) – these values are often displayed in a column matrix (e.g., a 2 × 1 column vector for a non-relativistic electron with spin 1⁄2).
According to the superposition principle of quantum mechanics, wave functions can be added together and multiplied by complex numbers to form new wave functions and form a Hilbert space. The inner product between two wave functions is a measure of the overlap between the corresponding physical states, and is used in the foundational probabilistic interpretation of quantum mechanics, the Born rule, relating transition probabilities to inner products. The Schrödinger equation determines how wave functions evolve over time, and a wave function behaves qualitatively like other waves, such as water waves or waves on a string, because the Schrödinger equation is mathematically a type of wave equation. This explains the name "wave function", and gives rise to wave–particle duality. However, the wave function in quantum mechanics describes a kind of physical phenomenon, still open to different interpretations, which fundamentally differs from that of classic mechanical waves.In Born's statistical interpretation in non-relativistic quantum mechanics,
the squared modulus of the wave function, |ψ|2, is a real number interpreted as the probability density of measuring a particle as being at a given place – or having a given momentum – at a given time, and possibly having definite values for discrete degrees of freedom. The integral of this quantity, over all the system's degrees of freedom, must be 1 in accordance with the probability interpretation. This general requirement that a wave function must satisfy is called the normalization condition. Since the wave function is complex valued, only its relative phase and relative magnitude can be measured—its value does not, in isolation, tell anything about the magnitudes or directions of measurable observables; one has to apply quantum operators, whose eigenvalues correspond to sets of possible results of measurements, to the wave function ψ and calculate the statistical distributions for measurable quantities.
Why shud one take the Fourier transform of a wavefunction and multiply the result with its conjugate to get the probability? Why can't it be Fourier transform of the probability directly?
thank you
Hi everyone,
This might belong in the quantum mechanics section, so I apologize if I placed this thread in the wrong place.
My question is: how do I calculate the gradient of a multiparticle wavefunction? For example, suppose that a wavefunction \psi describing the probability...
Problem
A free particle of mass m moving in one dimension is known to be in the initial state
\psi(x, 0) = \sin(k_0 x)
a) What is \psi(x, t)?
b) What value of p will measurement yield at the time t, and with what probabilities will these values occur?
c) Suppose that p is measured at...
Problem
Describe the evolution in time of \phi_1 = A \sin \omega t \cos k(x+ct).
Attempt at Solution
We have that
\partial^2 \phi_1 / \partial x^2 = -Ak^2 \sin \omega t \cos k(x+ct)
\partial \phi_1 / \partial t = A \sin \omega t (-kc \cdot \sin k(x+ct)) + A \omega \cos \omega t \cos...
Wavefunction collapse ==> increase in entropy??
I just read an article in Scientific American by Sean Carroll, called something like Does Time Run Backward in Other Universes. In it, he says that the reason wavefunctions only collapse and never un-collapse is because collapsing represents an...
If in the case of two non-interacting particles, the wavefunction looks like (for bosons):
\psi(x_1, x_2) = \frac{1}{\sqrt{2}}[\phi_a(x_1)\phi_b(x_2) + \phi_a(x_2)\phi_b(x_1)
And to normalise the wavefunction, the modulus squared has to be found. I can do this when I can substitute...
Homework Statement
If \Psi = f(x, y) and x = g(t), y = h(t), then (d\Psi / dt) = (p\Psi / px)(dx / dt) + (p\Psi / py)(dy / dt), where "p" symbolizes the partial derivative here and throughout the rest of this posting.
Derive the phase velocity equation +/- v = -(p\Psi / pt) / (p\Psi / px)...
I'm not sure the double-slit experiment is one such example, maybe I have not understood it yet.
This experiment shows the wave nature of light due to the wavefunctions of photons. But how does it show a particle of zero size that is not just a burst of waves?
Hi,
I'm teaching myself quantum mechanics (so this isn't homework). I came across the following question:
\Phi(p) = A\Theta\left[\frac{\hbar}{d}-|p-p_{0}|\right]
I have to find the constant of normalization, \psi(x), and the coordinate space wave function \psi(x,t) in the limit...
[SOLVED] Perturbed Ground State Wavefunction with Parity
Homework Statement
A particle is in a Coulomb potential
H_{0}=\frac{|p|^{2}}{2m} - \frac{e^{2}}{|r|}
When a perturbation V (which does not involve spin) is added, the ground state of H_{0} + V may be written
|\Psi_{0}\rangle =...
Could anyone please help with the following, rather unusual, query?
I know that for spin 0 bosons, the Klein Gordon equation gives solutions that are similar to the solutions of the Schrodinger equation for a non-relativistic free particle, the only difference being that the energy used when...
I have read it said a few times that a photon cannot be described by a wave-function but I am not far enough along in my QFT to know why. What's the story here?
And is this the same thing as saying that one cannot answer the question "What is the probability of observing the photon in volume...
Homework Statement
Find the most likely position of the particle.
Homework Equations
\Psi = A[(x+1)^{2} - 1)]
between x = 0 and x = 1
\Psi = 0 anywhere else
The Attempt at a Solution
I found A to equal \sqrt{15 / 38}... but I am not sure how to do the rest of it
Homework Statement
At time t=0 hydrogen atom is in state
\psi(r,0)=\frac{4}{(2a)^{3/2}}[e^{-r/a}+iA\frac{r}{a}e^{-r/2a}(-iY^{1}_{1}+Y^{-1}_{1}+\sqrt{7}Y^{0}_{1})]
a) Is it possible to normalize wave function ?
b) Find \psi(r,t) if at time t=0 measuring L_{z} we find \hbar
Homework...
Can anyone help me understand what is meant by the "parity of a wavefunction"?
I know in terms of even/odd parity, that:
P \Psi(x,y,z) = \pm \Psi(x,y,z)
ie, P = +/- 1
But I don't know what "parity of a wavefunction" physically means...
Homework Statement
I'm trying to determine a normalization value, A, for the following wavefunction:
\Psi = Ax{^2}exp(-\alpha x)}, x>0
\Psi = 0, x<0
In the past, I've had an i term in my exponential, so when applying the Normalization Condition:
\int|\Psi(x)|^2 dx = \int\Psi{^*}(x)...
Hi there, i have been studying a bit about QM, but ther's one fundamental question
about the wavefunction i can't understand: why is the wavef. defined complex? I mean,
couldn't one work from the beginning with a real wave?
Thanks
[SOLVED] hydrogen atom
Homework Statement
My book says that
R_{1,0}(r) = 2(1/a_0)^{3/2} e^{-r/a_0}
is a normalized wavefunction. But if you integrate R_{1,0}(r)^2 over r from 0 to infinity, you do not get 1. What's wrong here?Homework Equations
The Attempt at a Solution
I faced a weird question:what is the requirement of having a wave equation for the QM systems?
I think unless we have it,we cannot predict the probabilistic time and space evolution of the wave function subjected to potential constraints.(dynamicity of the wave function will be lost)...
Homework Statement
If given, for instance, psi(phi, 0)=[1/sqrt(2pi)](cos^2(phi/2) + isin(phi)), which is the wavefunction at t=0, how do you go about finding the wavefunction at time t, psi(phi,t)??
Homework Equations
The Attempt at a Solution
Would it simply be psi(phi...
I am just beginning to understand this concept. Some help would be appreciated.
Let me know if I am wrong in saying the following:
"The wave function (say \Psi] collapses to an eigen vector of the operator corresponding to the physical quantity(say \lambda) being measured. This is because the...
Can the wavefunction collapse not be derived or is it really an axiom?
How can the answer to this question (yes or no) be proven?
If it is an axiom, is it the best formulation, is it not a dangerous wording?
Let's enjoy this endless discussion !
I won't debate on the "wavefunction collapse" ...
... since this is just a lazy debate started from a misunderstanding.
Clearly when a small system interacts with a measuring device, the wave function of the small system just loses any meaning.
There is only one "larger" wavefunction for...
some very beautiful experimental work, observing the progressive collapse of a a wavefunction.
beautiful illustrations too
I didn't see this discussed here so decided to start a thread on it
Here's the abstract
http://arxiv.org/abs/0707.3880
Progressive field-state collapse and...
some very beautiful experimental work, observing the progressive collapse of a a wavefunction.
beautiful illustrations too
I didn't see this discussed here so decided to start a thread on it
http://arxiv.org/abs/0707.3880
Near "Normalization" calculation for given wavefunction
Homework Statement
A wave function is given by Y(E) = CEexp(-E/kt)
1. Find C so that Y(E) becomes Y0 where Y0 is a constant.
2. Calculate the mean energy with respect to Y(E).
3. Find Y(t) as a function of wavelength and...
hey guys,
this is a silly question, I'm sure it's been answered in other threads many times before and for that I am sorry.
when we take a measurement on an electron (lets say position or velocity), do we change it's wavefunction? What I mean is, we have a wavefunction in time and space...
I have an infinite well from -a to with a particle in its ground. The initial wavefunction is then
\psi(x) = u_1^+(x;a) = cos(\pi x/ 2a)/\sqrt{a} for |x| < a.
In order to get the wavefunction for this particle when box that is instantaneously expanded to [-b,b] should I apply Fourier...
Hi all
I know I raised a similar question in the thread "Wave particle duality", but it is already so full of many other questions, that I'd not be able to discuss this topic fully there.
So, in the double slit experiment, if a photon observes an electron, the interference pattern...
"Inside the Wavefunction"
Hi,
I was thinking about the wavefunction when I intercepted an interesting thought experiment that I couldn't quite formulate the answer to:
Say that we imagine a small particle that is small enough so that it is about the size of an electron (the particle...
It seems likely- but is it true that the ground state many-body wf must have zero nodes?
Is there a general rule for the nodes as a fn of quantum numbers?
hey all!
does anyone know the conditions a well behaved wavefunction (phi) must satisfy for all x? and any physical justifications for them?
is it something to do with continuity at boundaries? or to do with the differential of the wavefunction?
cheers for any input
roc
Will the wave function of a particle be the same in the two cases:
1) When the particle is isolated i.e. as a free or independent particle.
2) When the particle is bonded with other similar particles to constitute a composite particle.
For example, consider an isolated quark and a quark...
Homework Statement
Consider the electron in an atom of the heavy isotope of hydrogen,
tritium. The nucleus has charge e, and, apart from a small correction due
to the reduced mass effect, the electron has energies and eigenfunctions that
are identical to those of an ordinary hydrogen atom...
Homework Statement
a)Write Complete wave function for an electron in a 2s orbital of hydrogen
b)find the probability that the electron is at a distance from the nucleus that is outside the radius of the node.
c)graph the radial distribution function for this system.
Homework Equations...
When you study in a book basic quantization of the string lagrangian you can see two basic ways.
On ne hand you can see the X^\nu(\sigma,\tau) coordinates of the worldsheet as fields and to make canonical quantization with them. On the other hand there is teh polyakov path integral.
But...
Sorry, another quick question. If I have a particle confined in a region of space -4 <= Z <=6 where
psi(x)= A(4+z), -4<= z <=1
A(6-z), 1<= z <=6
0 , everywhere else
And I sketch the wavefunction based on the above definitions, what is the actual equation for...
In this problem I am given a function a(k) = \frac{C \alpha}{\sqrt{ \pi}} e^{-\alpha ^2 k^2}
where alpha and C are both constants
Now I am supposed to construct \psi (x,t)
My work:
\psi (x,t) = \int_{-\inf}^{\inf} a(k) e^{i[kx - \omega (k) t]} dk
pull out the constants from our...
I am not a scientist - I am a retired software engineer. But I find the current interpretations in quantum physics rather unsatisfying. This leads me to some questions.
My main concern is over the need for a wave function. I've recently been reading the transactional interpretation but it...
For those who have the book, this is problem 1.4 from Griffiths, 2nd ed.
\psi (x,0) = \left\{ \begin{array}{rcl}
A\frac{x}{a} & \mbox{for} & 0 \leq x \leq a \\
A\frac{b-x}{b-a} & \mbox{for} & a \leq x \leq b \\
0 & otherwise
\end{array}\right.
a) Normalise the wavefunction.
I found...
I start with calculating psi(x,0). Then i use fft(psi(x,0)) to get the Fourier coefficients. and with fftshift i get the terms with negative index in the beginning. Then i multiply with the timedependent factor and use ifftshift and ifft to get the wavefunction psi(x,t).
Here is the code...
Well, the question goes like this,
A particle of mass m is trapped in an infinitely deep one-dimensional potential well between x = 0 and x = a and at a time t=0,, the wave fuction is given as
Φ(x,t=0)=sin(((πx)/a))cos(((2πx)/a))
(i) What possible values may be found for energy of...
OK - the question gives me two bosons with 0 spin (and the wavefunctions/energy levels) and tells me to find the total wavefunction and energy for the ground state and first excited state.
Now, I know the total wavefunction must be symmetric. I know the symmetric spatial part. But the spin...
Hi all,
we know that the state of material particles (like electron) can be described by a wavefunction and that the wavefunction has a probabilistic interpretation. I have studied at very introductory level the quantum theory of electromagnetic radiation and it seems that it is built up in a...
Hello, I'm writing a program, and while I have a decent understanding of wavefunctions and atomic orbitals, this one appears to be a problem I can't beat.
I'm graphing various properties of atomic orbitals (wavefunction, wavefunction squared, radial probability distribution, and a cross...
I have a wavefunction given by:
\psi = \sqrt{\frac{2}{L}}\sin \frac{n\pi x}{L}
With boundary conditions 0<x<L.
When I compute the expectation value for the momentum like this:
\overline{p_x} = \int_0^L \sqrt{\frac{2}{L}}\sin \frac{n\pi x}{L} \left(-i\hbar \frac{\partial}{\partial...
For this given wavefunction of a hydrogen atom in 2s state, verify if the function is normalized:
\psi_{200} = \frac{1}{\sqrt{32\pi a^3}}\left(2 - \frac{r}{a}\right)e^{\frac{-r}{2a}}
My work:
I have to verify:
\int_{all space} \psi_{200}^2 dV = 1
dV = 4\pi r^2dr
So,
\int_{all space}...