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.
Hello i wonder if anyone here can explain to me, why the wavefunction as a function of position is defined like this:
$$\Psi(x,t) = \langle{x}|{\Psi(t)}\rangle$$
Why is it wise to use an inner product as a definition?
I propose a simple thpught experiment;
A scientist A measure the spin of an electron and finds it "up". After that he removes all evidence of his experiment and goes away, only to die in a road accident.
Another scientist, obviously unaware of the experiment done by A come and measures the...
Homework Statement
A wave function is given by:
\Psi (x) = a cos(2\pi x) + b sin (2\pi x) for\: x<0 \\
and\\
\Psi (x) = Ce^{-kx} for\: x>0 \\
Determine the constant k in terms of a, b and c using the boundary conditions and discuss the case a >> b.
Homework Equations...
If a baryon wavefunction is \Psi = \psi_{spatial} \psi_{colour} \psi_{flavour} \psi_{spin},
and we consider the ground state (L=0) only.
We know that the whole thing has to be antisymmetric under the interchange of two quarks. We know that colour is antisymmetric (always colourless) and...
Homework Statement
Solve for the wavefunctions and energy levels of an infinite square well potential extending between -L<x<L.
Hint: It may be worth noting that for a potential symmetric in x, then the observed probability density must also be symmetric in x, i. |ψ(x)|2 = |ψ(-x)|2.
Homework...
I understand that the variational method can give me the "best" approximate ground state wavefunction among the class of the function belongs to. It is the "best" wavefunction in a sense that its energy level is closest to the ground state among its own class.
Question: Is it also true that...
Homework Statement
The Hamiltonian for a rigid rotator which is confined to rotatei n the xy plane is
\begin{equation}
H=-\frac{\hbar}{2I}\frac{\delta^{2}}{\delta\phi^{2}}
\end{equation}
where the angle $\phi$ specifies the orientation of the body and $I$ is the moment of inertia...
Lets say we have a finite square potential well like below:
This well has a ##\psi## which we can combine with ##\psi_I##, ##\psi_{II}## and ##\psi_{III}##. I have been playing around and got expressions for them, but they are not the same for ODD and EVEN solutions but let's do this only...
I was reading Penrose's 1968 paper on twistor theory and it seems interesting.
Even upon reading around half the paper, I did not find the answer to one of the questions that came to my mind while reading the first few pages.
Somewhere in the first few pages (Section 0, 1 and 2), it was...
Problem:
Show that
\Theta_{20}=\frac{\sqrt{10}}{4}(3cos^{2}\theta-1)
is a normalized solution to
\frac{1}{sin\theta}\frac{d}{d\theta}(sin\theta \frac{d\Theta}{d\theta})+[l(l+1)-\frac{m_{l}^{2}}{sin^{2}\theta}]\Theta=0
Solution:
I know how to show it's a solution, but I'm stuck on showing...
Sometimes we see the wave function broken into specific parts, like $$\psi_{\rm total}=\psi_{\rm space}\psi_{\rm spin}\psi_{\rm isospin}.$$ What determines which parts you include in writing down the wavefunction? For instance, why or why wouldn't we include the isospin part? This has...
All the relevant information about the problem is in the attachment.
I just have a problem with the first step, my question it:
How is b true? I would have thought that the second part of the exponential function would be taken outside of the integral as well as A since you're taking the...
This isn't a homework question per se but it's a question that I had while reading through my textbook so I think it's appropriate here. I just started studying Quantum Mechanics and so am getting familiarized with the meaning of wave functions and their behavior. One question I can't seem to...
Have you recently came across and remember titles of papers about real experiments concerning the famous double slit electron behaviour?
I have found some about electron diffraction, but I'm still looking for those that showed how interference pattern is broken when we watch where the...
Does |\psi(\mathbf{x},t)|^2d^3\mathbf{x} or |\psi(\mathbf{x},t)|^2d^3\mathbf{x}dt give the probability of a particle to collapse at the point \mathbf{x} at time t?
Griffiths sides with the former, but I'm having doubts.
I have seen that the schrodinger wave equation is derived from the assumption that every wavefunction is of the form
ψ(x,t)=A(cos(2πx/λ-2πηt)+isin(2πx/λ-2πηt))
where η is the frequency
I can understand the real part of the equation. However, I am not able to understand the complex part...
Hey guys,
I was reading a book about the philosophy of science, and in the chapter about QM the author uses a well known example in order to explain quantum entaglement and illustrate the non-separability of individual system in QM. He describes a system composed of two spin-1/2 particles...
Homework Statement
I need to find the momentum space wavefuntion Phi(p,t) for a particle in the first excited state of the harmonic oscillator using a raising operator.
Homework Equations
Phi_1(p,t)= "raising operator" * Phi_0 (p,t)The Attempt at a Solution
In position space, psi_1 (x) =...
Determine scattering amplitude for atomic charge which is "spread" as wavefunction
Homework Statement
Derive the scattering amplitude and differential cross section for Rutherford scattering (done this). Now rederive the same quantities for the atomic charge which is "spread" with the...
Homework Statement
See the attachment for question and solutionHomework Equations
See the hint in the questionThe Attempt at a Solution
In part (c), it asks about the probability of finding the particle in ground state.
As far as I know, we need to write the wave function in terms of...
As the title suggests, I am interested in symmetries of QM systems.
Assume we have a stationary nonrelativistic quantum mechanical system H\psi = E\psi where we have a unique ground state.
I am interested in the conditions under which the stationary states of the system inherit the...
Homework Statement
The wave function Ψ of a quantum mechanical system described by a Hamiltonian H ̂ can be written as a linear combination of linear combination of Φ1 and Φ2 which are eigenfunctions of H ̂ with eigenvalues E1 and E2 respectively. At t=0, the system is prepared in the state...
A. Given the exact locations of N electrons - can we find out the total wave function and the individual wave functions by some law of nature?
B. Given the exact total wave function - can we find out the coordinates of each electron and the indiviual wave function of each electron by some law...
Homework Statement
Given the wavefunction, \psi(x) = Cx for 0 < x < 10 and \psi(x) = 0 for all other values.
What is the normalization constant of C? I got \sqrt{3/1000}.
What is <x>? I got 30/4.
What is <p>? Here is where I'm confused.Homework Equations
\langle p \rangle = C^2...
Homework Statement
Show that ψ(x) = Acos(kx) is not an eigenfunction of the momentum operator. If you were to measure the momentum of a particle with this wavefunction, what possible values would you get and what would the probability be of obtaining these values?
Homework Equations...
Basically, the problem gives me a wave function and asks me to find the wave function in momentum space. It then asks me to find the expected value. Namely <p> and <p^2>. The problem is, when I try to calculate <p> it blows up to infinity. What am I doing wrong? Here is my work...
Neumann's Principle states:
If a crystal is invariant with respect to certain symmetry elements, any of its physical properties must also be invariant with respect to the same symmetry elements.
So, does this apply to the wavefunction of an electron in a crystal? Or, stated another way, if...
Homework Statement
Suppose that there is a wavefunction \Psi (x,0) where 0 is referring to t. Let us also say that a(k) = (C\alpha/\sqrt \pi )exp(-\alpha^2k^2) is the spectral contents (spectral amplitudes) where k is defined as wavenumber k. \alpha and C is some constant
My question is, why...
Hi there!
I have tried to apply time reversal (which makes t -> -t) to a free particle wavefunction:
Exp[i(p.r-Et)/\hbar]
and got:
Exp[-i(p.r-Et)/\hbar]
I got this by flipping the sign of p since it has a d/dt part, and flipping the t in the Et part. However I think this is wrong...
All I need to evaluate the normalization coefficient. I need a step by step guide. It will be a great help if someone please tell me where can i get the solution (with intermediate steps). I think the solution can be done using the orthogonal properties of associated Laguerre polynomial. I need...
So, in QM making a measurement collapses the state into an eigenstate of that observable. Thus, if the system is properly isolated, then the same measurement should return the same value. But the eigenvalue for that state is degenerate, then does that mean the state might actually collapse to a...
Hi!
I'm currently re-reading Griffiths introductory QM book and plan to do most of the exercises. I got stuck on one problem and had to look for some hints and found two solutions that both claim that:
\int_{-\infty} ^{\infty} \frac{\partial }{\partial x}\left[ \frac{\partial \Psi...
I was wondering why is the nucleus willing to confine itself in one place while the electrons are free to appear anywhere around the nucleus within the orbital.
Electrons have this wave function, is there one for the nucleus?
The wavefunction is defined on the domain of complex numbers. To find the probability of discovering a particle in a certain region, the amplitude of the wavefunction is integrated over that region. The problem is that you have an infinite set of complex numbers mapping to a single amplitude...
Homework Statement
Find the constant A such that the equation
\psi(r,\theta,\varphi)=\sqrt{6\pi}A\sqrt{r}e^{-r/a}
Wich describes one electron in a hydrogenatom, is normalized
The Attempt at a Solution
I figured this equation is seperable in the form...
I am having troubles finding anything online that reveals the conceptual concerns relating to the probability wavefunction in regards to the travel of a particle and then how that plays into the double-slit experiment. No math is required. I merely need to know the concepts involved.
1) exactly...
This question is not directly related to QM although my reason for asking it is I'm trying to compute wavefunctions on my PC -- please excuse me if this is the wrong place to ask. I am having trouble using the DFT in Mathematica although I don't think my problem is directly Mathematica related...
Forgive me for asking such a basic question but say for IDSW1 if we have a wavefunction that is a superposition of the first two energy eigenfunctions so:
ψ(x)=(1/√2)*(ψ1+ψ2)
then if we measured say E1 we can eliminate the inconsistent part of the wavefunction so the wavefunction collapses to...
My first response to the question is "No", since electron and positron are distinguishable by their charge, so it's not necessary the wavefunction remains the same(up to +/-) upon permutation of particles. However on second thought, in the quantized Dirac field electron and positron creation...
Hey, I have been churning the idea of Dirac notation around in my head and I am thinking about the position and momentum basis representation of a wavefunction in a Hilbert space.
Wikipedia mentions the following in the article 'Bra-ket notation' under the heading 'Position-space wave...
Homework Statement
Assuming the five basis atomic orbitals are normalised use the Huckel approximations to normalise the wavefunction for the cyclopentadienyl radical
Wavefunction = \phi_{1}+\phi_{2}+\phi_{3}+\phi_{4}+\phi_{5} .
Homework Equations
I know that \phi_{i}\phi_{j} = 1 if...
I've read that color was introduces as a degree of freedom nessecary to satisfy the pauli exclusion principle in the quark model of particles. For example for the omega minus which had an observed total spin of 3/2 and no angular momenta ment that the spin had to the the same for all of the...
Hi!
I've read a lot of posts about the photon wavefunction. I'd like to ask you if this statement is correct:
"It is possible to write down a wavefunction for the photon which correctly describes its dynamics. But this wavefunction cannot be interpreted as an object whose squared modulus...
So I bugged the folks in General Physics about the latter form of the question a while back, and got some rather unconvincing "can't be done" replies. To state the problem specifically (and my motivation):
Let's say that the probability density of finding a particle at any place/time is given...
Hi all,
I was wondering if anyone could help me with some general rules for which parts one should include in a wave function when trying to determine symmetry. In simple cases, we see things like $$\psi_{\rm space}\psi_{\rm spin},$$ and in more complicated cases we see $$\psi_{\rm...
Hello, destructive interference seems like an important part of quantum physics, but I'm finding it very hard to grasp it conceptually. For instance in the Elitzur–Vaidman bomb tester, destructive interference in the mirror is used to determine if one of the paths is blocked. What exactly is...
Homework Statement
Consider the nonstationary state:
\Psi = \sqrt{\frac{1}{3}}\Psi_{22-1} + \sqrt{\frac{2}{3}}\Psi_{110}
Where \Psi_{22-1} and \Psi_{110} are normalized, orthogonal and stationary states of some radial potential. Is \Psi properly normalized? Calculate the expectation value of...