Physics:Quantum mechanics
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Quantum mechanics 

[math]\displaystyle{ i \hbar \frac{\partial}{\partial t}  \psi (t) \rangle = \hat{H}  \psi (t) \rangle }[/math] 
Quantum mechanics is a fundamental theory in physics that provides a description of the physical properties of nature at the scale of atoms and subatomic particles.^{[2]}^{:1.1} It is the foundation of all quantum physics including quantum chemistry, quantum field theory, quantum technology, and quantum information science.
Classical physics, the collection of theories that existed before the advent of quantum mechanics, describes many aspects of nature at an ordinary (macroscopic) scale, but is not sufficient for describing them at small (atomic and subatomic) scales. Most theories in classical physics can be derived from quantum mechanics as an approximation valid at large (macroscopic) scale.^{[3]}
Quantum mechanics differs from classical physics in that energy, momentum, angular momentum, and other quantities of a bound system are restricted to discrete values (quantization), objects have characteristics of both particles and waves (waveparticle duality), and there are limits to how accurately the value of a physical quantity can be predicted prior to its measurement, given a complete set of initial conditions (the uncertainty principle).
Quantum mechanics arose gradually from theories to explain observations which could not be reconciled with classical physics, such as Max Planck's solution in 1900 to the blackbody radiation problem, and the correspondence between energy and frequency in Albert Einstein's 1905 paper which explained the photoelectric effect. These early attempts to understand microscopic phenomena, now known as the "old quantum theory", led to the full development of quantum mechanics in the mid1920s by Niels Bohr, Erwin Schrödinger, Werner Heisenberg, Max Born and others. The modern theory is formulated in various specially developed mathematical formalisms. In one of them, a mathematical entity called the wave function provides information, in the form of probability amplitudes, about what measurements of a particle's energy, momentum, and other physical properties may yield.
Overview and fundamental concepts
Quantum mechanics allows the calculation of properties and behaviour of physical systems. It is typically applied to microscopic systems: molecules, atoms and subatomic particles. It has been demonstrated to hold for complex molecules with thousands of atoms,^{[4]} but its application to human beings raises philosophical problems, such as Wigner's friend, and its application to the universe as a whole remains speculative.^{[5]} Predictions of quantum mechanics have been verified experimentally to an extremely high degree of accuracy.^{[note 1]}
A fundamental feature of the theory is that it usually cannot predict with certainty what will happen, but only give probabilities. Mathematically, a probability is found by taking the square of the absolute value of a complex number, known as a probability amplitude. This is known as the Born rule, named after physicist Max Born. For example, a quantum particle like an electron can be described by a wave function, which associates to each point in space a probability amplitude. Applying the Born rule to these amplitudes gives a probability density function for the position that the electron will be found to have when an experiment is performed to measure it. This is the best the theory can do; it cannot say for certain where the electron will be found. The Schrödinger equation relates the collection of probability amplitudes that pertain to one moment of time to the collection of probability amplitudes that pertain to another.
One consequence of the mathematical rules of quantum mechanics is a tradeoff in predictability between different measurable quantities. The most famous form of this uncertainty principle says that no matter how a quantum particle is prepared or how carefully experiments upon it are arranged, it is impossible to have a precise prediction for a measurement of its position and also at the same time for a measurement of its momentum.
Another consequence of the mathematical rules of quantum mechanics is the phenomenon of quantum interference, which is often illustrated with the doubleslit experiment. In the basic version of this experiment, a coherent light source, such as a laser beam, illuminates a plate pierced by two parallel slits, and the light passing through the slits is observed on a screen behind the plate.^{[6]}^{:102–111}^{[2]}^{:1.1–1.8} The wave nature of light causes the light waves passing through the two slits to interfere, producing bright and dark bands on the screen – a result that would not be expected if light consisted of classical particles.^{[6]} However, the light is always found to be absorbed at the screen at discrete points, as individual particles rather than waves; the interference pattern appears via the varying density of these particle hits on the screen. Furthermore, versions of the experiment that include detectors at the slits find that each detected photon passes through one slit (as would a classical particle), and not through both slits (as would a wave).^{[6]}^{:109}^{[7]}^{[8]} However, such experiments demonstrate that particles do not form the interference pattern if one detects which slit they pass through. Other atomicscale entities, such as electrons, are found to exhibit the same behavior when fired towards a double slit.^{[2]} This behavior is known as waveparticle duality.
Another counterintuitive phenomenon predicted by quantum mechanics is quantum tunnelling: a particle that goes up against a potential barrier can cross it, even if its kinetic energy is smaller than the maximum of the potential.^{[9]} In classical mechanics this particle would be trapped. Quantum tunnelling has several important consequences, enabling radioactive decay, nuclear fusion in stars, and applications such as scanning tunnelling microscopy and the tunnel diode.^{[10]}
When quantum systems interact, the result can be the creation of quantum entanglement: their properties become so intertwined that a description of the whole solely in terms of the individual parts is no longer possible. Erwin Schrödinger called entanglement "...the characteristic trait of quantum mechanics, the one that enforces its entire departure from classical lines of thought".^{[11]} Quantum entanglement enables the counterintuitive properties of quantum pseudotelepathy, and can be a valuable resource in communication protocols, such as quantum key distribution and superdense coding.^{[12]} Contrary to popular misconception, entanglement does not allow sending signals faster than light, as demonstrated by the nocommunication theorem.^{[12]}
Another possibility opened by entanglement is testing for "hidden variables", hypothetical properties more fundamental than the quantities addressed in quantum theory itself, knowledge of which would allow more exact predictions than quantum theory can provide. A collection of results, most significantly Bell's theorem, have demonstrated that broad classes of such hiddenvariable theories are in fact incompatible with quantum physics. According to Bell's theorem, if nature actually operates in accord with any theory of local hidden variables, then the results of a Bell test will be constrained in a particular, quantifiable way. Many Bell tests have been performed, using entangled particles, and they have shown results incompatible with the constraints imposed by local hidden variables.^{[13]}^{[14]}
It is not possible to present these concepts in more than a superficial way without introducing the actual mathematics involved; understanding quantum mechanics requires not only manipulating complex numbers, but also linear algebra, differential equations, group theory, and other more advanced subjects.^{[note 2]} Accordingly, this article will present a mathematical formulation of quantum mechanics and survey its application to some useful and oftstudied examples.
Mathematical formulation
In the mathematically rigorous formulation of quantum mechanics, the state of a quantum mechanical system is a vector [math]\displaystyle{ \psi }[/math] belonging to a (separable) complex Hilbert space [math]\displaystyle{ \mathcal H }[/math]. This vector is postulated to be normalized under the Hilbert space inner product, that is, it obeys [math]\displaystyle{ \langle \psi,\psi \rangle = 1 }[/math], and it is welldefined up to a complex number of modulus 1 (the global phase), that is, [math]\displaystyle{ \psi }[/math] and [math]\displaystyle{ e^{i\alpha}\psi }[/math] represent the same physical system. In other words, the possible states are points in the projective space of a Hilbert space, usually called the complex projective space. The exact nature of this Hilbert space is dependent on the system – for example, for describing position and momentum the Hilbert space is the space of complex squareintegrable functions [math]\displaystyle{ L^2(\mathbb C) }[/math], while the Hilbert space for the spin of a single proton is simply the space of twodimensional complex vectors [math]\displaystyle{ \mathbb C^2 }[/math] with the usual inner product.
Physical quantities of interest — position, momentum, energy, spin — are represented by observables, which are Hermitian (more precisely, selfadjoint) linear operators acting on the Hilbert space. A quantum state can be an eigenvector of an observable, in which case it is called an eigenstate, and the associated eigenvalue corresponds to the value of the observable in that eigenstate. More generally, a quantum state will be a linear combination of the eigenstates, known as a quantum superposition. When an observable is measured, the result will be one of its eigenvalues with probability given by the Born rule: in the simplest case the eigenvalue [math]\displaystyle{ \lambda }[/math] is nondegenerate and the probability is given by [math]\displaystyle{ \langle \vec\lambda,\psi\rangle^2 }[/math], where [math]\displaystyle{ \vec\lambda }[/math] is its associated eigenvector. More generally, the eigenvalue is degenerate and the probability is given by [math]\displaystyle{ \langle \psi,P_\lambda\psi\rangle }[/math], where [math]\displaystyle{ P_\lambda }[/math] is the projector onto its associated eigenspace. In the continuous case, these formulas give instead the probability density.
After the measurement, if result [math]\displaystyle{ \lambda }[/math] was obtained, the quantum state is postulated to collapse to [math]\displaystyle{ \vec\lambda }[/math], in the nondegenerate case, or to [math]\displaystyle{ P_\lambda\psi/\sqrt{\langle \psi,P_\lambda\psi\rangle} }[/math], in the general case. The probabilistic nature of quantum mechanics thus stems from the act of measurement. This is one of the most difficult aspects of quantum systems to understand. It was the central topic in the famous Bohr–Einstein debates, in which the two scientists attempted to clarify these fundamental principles by way of thought experiments. In the decades after the formulation of quantum mechanics, the question of what constitutes a "measurement" has been extensively studied. Newer interpretations of quantum mechanics have been formulated that do away with the concept of "wave function collapse" (see, for example, the manyworlds interpretation). The basic idea is that when a quantum system interacts with a measuring apparatus, their respective wave functions become entangled so that the original quantum system ceases to exist as an independent entity. For details, see the article on measurement in quantum mechanics.^{[17]}
The time evolution of a quantum state is described by the Schrödinger equation:
 [math]\displaystyle{ i\hbar {\frac {d}{dt}} \psi (t) =H \psi (t). }[/math]
Here [math]\displaystyle{ H }[/math] denotes the Hamiltonian, the observable corresponding to the total energy of the system, and [math]\displaystyle{ \hbar }[/math] is the reduced Planck constant. The constant [math]\displaystyle{ i\hbar }[/math] is introduced so that the Hamiltonian is reduced to the classical Hamiltonian in cases where the quantum system can be approximated by a classical system; the ability to make such an approximation in certain limits is called the correspondence principle.
The solution of this differential equation is given by
 [math]\displaystyle{ \psi(t) = e^{iHt/\hbar }\psi(0). }[/math]
The operator [math]\displaystyle{ U(t) = e^{iHt/\hbar } }[/math] is known as the timeevolution operator, and has the crucial property that it is unitary. This time evolution is deterministic in the sense that – given an initial quantum state [math]\displaystyle{ \psi(0) }[/math] – it makes a definite prediction of what the quantum state [math]\displaystyle{ \psi(t) }[/math] will be at any later time.^{[18]}
Some wave functions produce probability distributions that are independent of time, such as eigenstates of the Hamiltonian. Many systems that are treated dynamically in classical mechanics are described by such "static" wave functions. For example, a single electron in an unexcited atom is pictured classically as a particle moving in a circular trajectory around the atomic nucleus, whereas in quantum mechanics, it is described by a static wave function surrounding the nucleus. For example, the electron wave function for an unexcited hydrogen atom is a spherically symmetric function known as an s orbital (Fig. 1).
Analytic solutions of the Schrödinger equation are known for very few relatively simple model Hamiltonians including the quantum harmonic oscillator, the particle in a box, the dihydrogen cation, and the hydrogen atom. Even the helium atom – which contains just two electrons – has defied all attempts at a fully analytic treatment.
However, there are techniques for finding approximate solutions. One method, called perturbation theory, uses the analytic result for a simple quantum mechanical model to create a result for a related but more complicated model by (for example) the addition of a weak potential energy. Another method is called "semiclassical equation of motion", which applies to systems for which quantum mechanics produces only small deviations from classical behavior. These deviations can then be computed based on the classical motion. This approach is particularly important in the field of quantum chaos.
Uncertainty principle
One consequence of the basic quantum formalism is the uncertainty principle. In its most familiar form, this states that no preparation of a quantum particle can imply simultaneously precise predictions both for a measurement of its position and for a measurement of its momentum.^{[19]}^{[20]} Both position and momentum are observables, meaning that they are represented by Hermitian operators. The position operator [math]\displaystyle{ \hat{X} }[/math] and momentum operator [math]\displaystyle{ \hat{P} }[/math] do not commute, but rather satisfy the canonical commutation relation:
 [math]\displaystyle{ [\hat{X}, \hat{P}] = i\hbar. }[/math]
Given a quantum state, the Born rule lets us compute expectation values for both [math]\displaystyle{ X }[/math] and [math]\displaystyle{ P }[/math], and moreover for powers of them. Defining the uncertainty for an observable by a standard deviation, we have
 [math]\displaystyle{ \sigma_X=\sqrt{\langle {X}^2 \rangle\langle {X}\rangle^2}, }[/math]
and likewise for the momentum:
 [math]\displaystyle{ \sigma_P=\sqrt{\langle {P}^2 \rangle\langle {P}\rangle^2}. }[/math]
The uncertainty principle states that
 [math]\displaystyle{ \sigma_X \sigma_P \geq \frac{\hbar}{2}. }[/math]
Either standard deviation can in principle be made arbitrarily small, but not both simultaneously.^{[21]} This inequality generalizes to arbitrary pairs of selfadjoint operators [math]\displaystyle{ A }[/math] and [math]\displaystyle{ B }[/math]. The commutator of these two operators is
 [math]\displaystyle{ [A,B]=ABBA, }[/math]
and this provides the lower bound on the product of standard deviations:
 [math]\displaystyle{ \sigma_A \sigma_B \geq \frac{1}{2}\left\langle[A,B]\rangle \right. }[/math]
Another consequence of the canonical commutation relation is that the position and momentum operators are Fourier transforms of each other, so that a description of an object according to its momentum is the Fourier transform of its description according to its position. The fact that dependence in momentum is the Fourier transform of the dependence in position means that the momentum operator is equivalent (up to an [math]\displaystyle{ i/\hbar }[/math] factor) to taking the derivative according to the position, since in Fourier analysis differentiation corresponds to multiplication in the dual space. This is why in quantum equations in position space, the momentum [math]\displaystyle{ p_i }[/math] is replaced by [math]\displaystyle{ i \hbar \frac {\partial}{\partial x} }[/math], and in particular in the nonrelativistic Schrödinger equation in position space the momentumsquared term is replaced with a Laplacian times [math]\displaystyle{ \hbar^2 }[/math].^{[19]}
Composite systems and entanglement
When two different quantum systems are considered together, the Hilbert space of the combined system is the tensor product of the Hilbert spaces of the two components. For example, let A and B be two quantum systems, with Hilbert spaces [math]\displaystyle{ \mathcal H_A }[/math] and [math]\displaystyle{ \mathcal H_B }[/math], respectively. The Hilbert space of the composite system is then
 [math]\displaystyle{ \mathcal H_{AB} = \mathcal H_A \otimes \mathcal H_B. }[/math]
If the state for the first system is the vector [math]\displaystyle{ \psi_A }[/math] and the state for the second system is [math]\displaystyle{ \psi_B }[/math], then the state of the composite system is
 [math]\displaystyle{ \psi_A \otimes \psi_B. }[/math]
Not all states in the joint Hilbert space [math]\displaystyle{ \mathcal H_{AB} }[/math] can be written in this form, however, because the superposition principle implies that linear combinations of these "separable" or "product states" are also valid. For example, if [math]\displaystyle{ \psi_A }[/math] and [math]\displaystyle{ \phi_A }[/math] are both possible states for system [math]\displaystyle{ A }[/math], and likewise [math]\displaystyle{ \psi_B }[/math] and [math]\displaystyle{ \phi_B }[/math] are both possible states for system [math]\displaystyle{ B }[/math], then
 [math]\displaystyle{ \tfrac{1}{\sqrt{2}} \left ( \psi_A \otimes \psi_B + \phi_A \otimes \phi_B \right ) }[/math]
is a valid joint state that is not separable. States that are not separable are called entangled.^{[22]}^{[23]}
If the state for a composite system is entangled, it is impossible to describe either component system A or system B by a state vector. One can instead define reduced density matrices that describe the statistics that can be obtained by making measurements on either component system alone. This necessarily causes a loss of information, though: knowing the reduced density matrices of the individual systems is not enough to reconstruct the state of the composite system.^{[22]}^{[23]} Just as density matrices specify the state of a subsystem of a larger system, analogously, positive operatorvalued measures (POVMs) describe the effect on a subsystem of a measurement performed on a larger system. POVMs are extensively used in quantum information theory.^{[22]}^{[24]}
As described above, entanglement is a key feature of models of measurement processes in which an apparatus becomes entangled with the system being measured. Systems interacting with the environment in which they reside generally become entangled with that environment, a phenomenon known as quantum decoherence. This can explain why, in practice, quantum effects are difficult to observe in systems larger than microscopic.^{[25]}
Equivalence between formulations
There are many mathematically equivalent formulations of quantum mechanics. One of the oldest and most common is the "transformation theory" proposed by Paul Dirac, which unifies and generalizes the two earliest formulations of quantum mechanics – matrix mechanics (invented by Werner Heisenberg) and wave mechanics (invented by Erwin Schrödinger).^{[26]} An alternative formulation of quantum mechanics is Feynman's path integral formulation, in which a quantummechanical amplitude is considered as a sum over all possible classical and nonclassical paths between the initial and final states. This is the quantummechanical counterpart of the action principle in classical mechanics.
Symmetries and conservation laws
The Hamiltonian [math]\displaystyle{ H }[/math] is known as the generator of time evolution, since it defines a unitary timeevolution operator [math]\displaystyle{ U(t) = e^{iHt/\hbar} }[/math] for each value of [math]\displaystyle{ t }[/math]. From this relation between [math]\displaystyle{ U(t) }[/math] and [math]\displaystyle{ H }[/math], it follows that any observable [math]\displaystyle{ A }[/math] that commutes with [math]\displaystyle{ H }[/math] will be conserved: its expectation value will not change over time. This statement generalizes, as mathematically, any Hermitian operator [math]\displaystyle{ A }[/math] can generate a family of unitary operators parameterized by a variable [math]\displaystyle{ t }[/math]. Under the evolution generated by [math]\displaystyle{ A }[/math], any observable [math]\displaystyle{ B }[/math] that commutes with [math]\displaystyle{ A }[/math] will be conserved. Moreover, if [math]\displaystyle{ B }[/math] is conserved by evolution under [math]\displaystyle{ A }[/math], then [math]\displaystyle{ A }[/math] is conserved under the evolution generated by [math]\displaystyle{ B }[/math]. This implies a quantum version of the result proven by Emmy Noether in classical (Lagrangian) mechanics: for every differentiable symmetry of a Hamiltonian, there exists a corresponding conservation law.
Examples
Free particle
The simplest example of quantum system with a position degree of freedom is a free particle in a single spatial dimension. A free particle is one which is not subject to external influences, so that its Hamiltonian consists only of its kinetic energy:
 [math]\displaystyle{ H = \frac{1}{2m}P^2 =  \frac {\hbar ^2}{2m} \frac {d ^2}{dx^2}. }[/math]
The general solution of the Schrödinger equation is given by
 [math]\displaystyle{ \psi (x,t)=\frac {1}{\sqrt {2\pi }}\int _{\infty}^\infty{\hat {\psi }}(k,0)e^{i(kx \frac{\hbar k^2}{2m} t)}\mathrm{d}k, }[/math]
which is a superposition of all possible plane waves [math]\displaystyle{ e^{i(kx \frac{\hbar k^2}{2m} t)} }[/math], which are eigenstates of the momentum operator with momentum [math]\displaystyle{ p = \hbar k }[/math]. The coefficients of the superposition are [math]\displaystyle{ \hat {\psi }(k,0) }[/math], which is the Fourier transform of the initial quantum state [math]\displaystyle{ \psi(x,0) }[/math].
It is not possible for the solution to be a single momentum eigenstate, or a single position eigenstate, as these are not normalizable quantum states.^{[note 3]} Instead, we can consider a Gaussian wave packet:
 [math]\displaystyle{ \psi(x,0) = \frac{1}{\sqrt[4]{\pi a}}e^{\frac{x^2}{2a}} }[/math]
which has Fourier transform, and therefore momentum distribution
 [math]\displaystyle{ \hat \psi(k,0) = \sqrt[4]{\frac{a}{\pi}}e^{\frac{a k^2}{2}}. }[/math]
We see that as we make [math]\displaystyle{ a }[/math] smaller the spread in position gets smaller, but the spread in momentum gets larger. Conversely, by making [math]\displaystyle{ a }[/math] larger we make the spread in momentum smaller, but the spread in position gets larger. This illustrates the uncertainty principle.
As we let the Gaussian wave packet evolve in time, we see that its center moves through space at a constant velocity (like a classical particle with no forces acting on it). However, the wave packet will also spread out as time progresses, which means that the position becomes more and more uncertain. The uncertainty in momentum, however, stays constant.^{[27]}
Particle in a box
The particle in a onedimensional potential energy box is the most mathematically simple example where restraints lead to the quantization of energy levels. The box is defined as having zero potential energy everywhere inside a certain region, and therefore infinite potential energy everywhere outside that region.^{[19]}^{:77–78} For the onedimensional case in the [math]\displaystyle{ x }[/math] direction, the timeindependent Schrödinger equation may be written
 [math]\displaystyle{  \frac {\hbar ^2}{2m} \frac {d ^2 \psi}{dx^2} = E \psi. }[/math]
With the differential operator defined by
 [math]\displaystyle{ \hat{p}_x = i\hbar\frac{d}{dx} }[/math]
the previous equation is evocative of the classic kinetic energy analogue,
 [math]\displaystyle{ \frac{1}{2m} \hat{p}_x^2 = E, }[/math]
with state [math]\displaystyle{ \psi }[/math] in this case having energy [math]\displaystyle{ E }[/math] coincident with the kinetic energy of the particle.
The general solutions of the Schrödinger equation for the particle in a box are
 [math]\displaystyle{ \psi(x) = A e^{ikx} + B e ^{ikx} \qquad\qquad E = \frac{\hbar^2 k^2}{2m} }[/math]
or, from Euler's formula,
 [math]\displaystyle{ \psi(x) = C \sin(kx) + D \cos(kx).\! }[/math]
The infinite potential walls of the box determine the values of [math]\displaystyle{ C, D, }[/math] and [math]\displaystyle{ k }[/math] at [math]\displaystyle{ x=0 }[/math] and [math]\displaystyle{ x=L }[/math] where [math]\displaystyle{ \psi }[/math] must be zero. Thus, at [math]\displaystyle{ x=0 }[/math],
 [math]\displaystyle{ \psi(0) = 0 = C\sin(0) + D\cos(0) = D }[/math]
and [math]\displaystyle{ D=0 }[/math]. At [math]\displaystyle{ x=L }[/math],
 [math]\displaystyle{ \psi(L) = 0 = C\sin(kL), }[/math]
in which [math]\displaystyle{ C }[/math] cannot be zero as this would conflict with the postulate that [math]\displaystyle{ \psi }[/math] has norm 1. Therefore, since [math]\displaystyle{ \sin(kL)=0 }[/math], [math]\displaystyle{ kL }[/math] must be an integer multiple of [math]\displaystyle{ \pi }[/math],
 [math]\displaystyle{ k = \frac{n\pi}{L}\qquad\qquad n=1,2,3,\ldots. }[/math]
This constraint on [math]\displaystyle{ k }[/math] implies a constraint on the energy levels, yielding
[math]\displaystyle{ E_n = \frac{\hbar^2 \pi^2 n^2}{2mL^2} = \frac{n^2h^2}{8mL^2}. }[/math]
A finite potential well is the generalization of the infinite potential well problem to potential wells having finite depth. The finite potential well problem is mathematically more complicated than the infinite particleinabox problem as the wave function is not pinned to zero at the walls of the well. Instead, the wave function must satisfy more complicated mathematical boundary conditions as it is nonzero in regions outside the well. Another related problem is that of the rectangular potential barrier, which furnishes a model for the quantum tunneling effect that plays an important role in the performance of modern technologies such as flash memory and scanning tunneling microscopy.
Harmonic oscillator
As in the classical case, the potential for the quantum harmonic oscillator is given by
 [math]\displaystyle{ V(x)=\frac{1}{2}m\omega^2x^2. }[/math]
This problem can either be treated by directly solving the Schrödinger equation, which is not trivial, or by using the more elegant "ladder method" first proposed by Paul Dirac. The eigenstates are given by
 [math]\displaystyle{ \psi_n(x) = \sqrt{\frac{1}{2^n\, n!}} \cdot \left(\frac{m\omega}{\pi \hbar}\right)^{1/4} \cdot e^{  \frac{m\omega x^2}{2 \hbar}} \cdot H_n\left(\sqrt{\frac{m\omega}{\hbar}} x \right), \qquad }[/math]
 [math]\displaystyle{ n = 0,1,2,\ldots. }[/math]
where H_{n} are the Hermite polynomials
 [math]\displaystyle{ H_n(x)=(1)^n e^{x^2}\frac{d^n}{dx^n}\left(e^{x^2}\right), }[/math]
and the corresponding energy levels are
 [math]\displaystyle{ E_n = \hbar \omega \left(n + {1\over 2}\right). }[/math]
This is another example illustrating the discretization of energy for bound states.
Mach–Zehnder interferometer
The Mach–Zehnder interferometer (MZI) illustrates the concepts of superposition and interference with linear algebra in dimension 2, rather than differential equations. It can be seen as a simplified version of the doubleslit experiment, but it is of interest in its own right, for example in the delayed choice quantum eraser, the Elitzur–Vaidman bomb tester, and in studies of quantum entanglement.^{[28]}^{[29]}
We can model a photon going through the interferometer by considering that at each point it can be in a superposition of only two paths: the "lower" path which starts from the left, goes straight through both beam splitters, and ends at the top, and the "upper" path which starts from the bottom, goes straight through both beam splitters, and ends at the right. The quantum state of the photon is therefore a vector [math]\displaystyle{ \psi \in \mathbb{C}^2 }[/math] that is a superposition of the "lower" path [math]\displaystyle{ \psi_l = \begin{pmatrix} 1 \\ 0 \end{pmatrix} }[/math] and the "upper" path [math]\displaystyle{ \psi_u = \begin{pmatrix} 0 \\ 1 \end{pmatrix} }[/math], that is, [math]\displaystyle{ \psi = \alpha \psi_l + \beta \psi_u }[/math] for complex [math]\displaystyle{ \alpha,\beta }[/math]. In order to respect the postulate that [math]\displaystyle{ \langle \psi,\psi\rangle = 1 }[/math] we require that [math]\displaystyle{ \alpha^2+\beta^2 = 1 }[/math].
Both beam splitters are modelled as the unitary matrix [math]\displaystyle{ B = \frac1{\sqrt2}\begin{pmatrix} 1 & i \\ i & 1 \end{pmatrix} }[/math], which means that when a photon meets the beam splitter it will either stay on the same path with a probability amplitude of [math]\displaystyle{ 1/\sqrt{2} }[/math], or be reflected to the other path with a probability amplitude of [math]\displaystyle{ i/\sqrt{2} }[/math]. The phase shifter on the upper arm is modelled as the unitary matrix [math]\displaystyle{ P = \begin{pmatrix} 1 & 0 \\ 0 & e^{i\Delta\Phi} \end{pmatrix} }[/math], which means that if the photon is on the "upper" path it will gain a relative phase of [math]\displaystyle{ \Delta\Phi }[/math], and it will stay unchanged if it is in the lower path.
A photon that enters the interferometer from the left will then be acted upon with a beam splitter [math]\displaystyle{ B }[/math], a phase shifter [math]\displaystyle{ P }[/math], and another beam splitter [math]\displaystyle{ B }[/math], and so end up in the state
 [math]\displaystyle{ BPB\psi_l = ie^{i\Delta\Phi/2} \begin{pmatrix} \sin(\Delta\Phi/2) \\ \cos(\Delta\Phi/2) \end{pmatrix}, }[/math]
and the probabilities that it will be detected at the right or at the top are given respectively by
 [math]\displaystyle{ p(u) = \langle \psi_u, BPB\psi_l \rangle^2 = \cos^2 \frac{\Delta \Phi}{2}, }[/math]
 [math]\displaystyle{ p(l) = \langle \psi_l, BPB\psi_l \rangle^2 = \sin^2 \frac{\Delta \Phi}{2}. }[/math]
One can therefore use the Mach–Zehnder interferometer to estimate the phase shift by estimating these probabilities.
It is interesting to consider what would happen if the photon were definitely in either the "lower" or "upper" paths between the beam splitters. This can be accomplished by blocking one of the paths, or equivalently by removing the first beam splitter (and feeding the photon from the left or the bottom, as desired). In both cases there will be no interference between the paths anymore, and the probabilities are given by [math]\displaystyle{ p(u)=p(l) = 1/2 }[/math], independently of the phase [math]\displaystyle{ \Delta\Phi }[/math]. From this we can conclude that the photon does not take one path or another after the first beam splitter, but rather that it is in a genuine quantum superposition of the two paths.^{[30]}
Applications
Quantum mechanics has had enormous success in explaining many of the features of our universe, with regards to smallscale and discrete quantities and interactions which cannot be explained by classical methods.^{[note 4]} Quantum mechanics is often the only theory that can reveal the individual behaviors of the subatomic particles that make up all forms of matter (electrons, protons, neutrons, photons, and others). Solidstate physics and materials science are dependent upon quantum mechanics.^{[31]}
In many aspects modern technology operates at a scale where quantum effects are significant. Important applications of quantum theory include quantum chemistry, quantum optics, quantum computing, superconducting magnets, lightemitting diodes, the optical amplifier and the laser, the transistor and semiconductors such as the microprocessor, medical and research imaging such as magnetic resonance imaging and electron microscopy.^{[32]} Explanations for many biological and physical phenomena are rooted in the nature of the chemical bond, most notably the macromolecule DNA.
Relation to other scientific theories
Modern physics 

[math]\displaystyle{ \hat{H}  \psi_n(t) \rangle = i \hbar \frac{\partial}{\partial t}  \psi_n(t) \rangle }[/math] [math]\displaystyle{ \frac { 1 }{ { c }^{ 2 } } \frac { { \partial }^{ 2 }{ \phi }_{n} }{ { \partial t }^{ 2 } } { { \nabla }^{ 2 }{ \phi }_{n} }+{ \left( \frac { mc }{ \hbar } \right) }^{ 2 }{ \phi }_{n}=0 }[/math] 
Classical mechanics
The rules of quantum mechanics assert that the state space of a system is a Hilbert space and that observables of the system are Hermitian operators acting on vectors in that space – although they do not tell us which Hilbert space or which operators. These can be chosen appropriately in order to obtain a quantitative description of a quantum system, a necessary step in making physical predictions. An important guide for making these choices is the correspondence principle, a heuristic which states that the predictions of quantum mechanics reduce to those of classical mechanics in the regime of large quantum numbers.^{[33]} One can also start from an established classical model of a particular system, and then try to guess the underlying quantum model that would give rise to the classical model in the correspondence limit. This approach is known as quantization.
When quantum mechanics was originally formulated, it was applied to models whose correspondence limit was nonrelativistic classical mechanics. For instance, the wellknown model of the quantum harmonic oscillator uses an explicitly nonrelativistic expression for the kinetic energy of the oscillator, and is thus a quantum version of the classical harmonic oscillator.
Complications arise with chaotic systems, which do not have good quantum numbers, and quantum chaos studies the relationship between classical and quantum descriptions in these systems.
Quantum decoherence is a mechanism through which quantum systems lose coherence, and thus become incapable of displaying many typically quantum effects: quantum superpositions become simply probabilistic mixtures, and quantum entanglement becomes simply classical correlations. Quantum coherence is not typically evident at macroscopic scales, except maybe at temperatures approaching absolute zero at which quantum behavior may manifest macroscopically.^{[note 5]}
Many macroscopic properties of a classical system are a direct consequence of the quantum behavior of its parts. For example, the stability of bulk matter (consisting of atoms and molecules which would quickly collapse under electric forces alone), the rigidity of solids, and the mechanical, thermal, chemical, optical and magnetic properties of matter are all results of the interaction of electric charges under the rules of quantum mechanics.^{[34]}
Special relativity and electrodynamics
Early attempts to merge quantum mechanics with special relativity involved the replacement of the Schrödinger equation with a covariant equation such as the Klein–Gordon equation or the Dirac equation. While these theories were successful in explaining many experimental results, they had certain unsatisfactory qualities stemming from their neglect of the relativistic creation and annihilation of particles. A fully relativistic quantum theory required the development of quantum field theory, which applies quantization to a field (rather than a fixed set of particles). The first complete quantum field theory, quantum electrodynamics, provides a fully quantum description of the electromagnetic interaction. Quantum electrodynamics is, along with general relativity, one of the most accurate physical theories ever devised.^{[35]}^{[36]}
The full apparatus of quantum field theory is often unnecessary for describing electrodynamic systems. A simpler approach, one that has been used since the inception of quantum mechanics, is to treat charged particles as quantum mechanical objects being acted on by a classical electromagnetic field. For example, the elementary quantum model of the hydrogen atom describes the electric field of the hydrogen atom using a classical [math]\displaystyle{ \textstyle e^2/(4 \pi\epsilon_{_0}r) }[/math] Coulomb potential. This "semiclassical" approach fails if quantum fluctuations in the electromagnetic field play an important role, such as in the emission of photons by charged particles.
Quantum field theories for the strong nuclear force and the weak nuclear force have also been developed. The quantum field theory of the strong nuclear force is called quantum chromodynamics, and describes the interactions of subnuclear particles such as quarks and gluons. The weak nuclear force and the electromagnetic force were unified, in their quantized forms, into a single quantum field theory (known as electroweak theory), by the physicists Abdus Salam, Sheldon Glashow and Steven Weinberg.^{[37]}
Relation to general relativity
Even though the predictions of both quantum theory and general relativity have been supported by rigorous and repeated empirical evidence, their abstract formalisms contradict each other and they have proven extremely difficult to incorporate into one consistent, cohesive model. Gravity is negligible in many areas of particle physics, so that unification between general relativity and quantum mechanics is not an urgent issue in those particular applications. However, the lack of a correct theory of quantum gravity is an important issue in physical cosmology and the search by physicists for an elegant "Theory of Everything" (TOE). Consequently, resolving the inconsistencies between both theories has been a major goal of 20th and 21stcentury physics. This TOE would combine not only the models of subatomic physics but also derive the four fundamental forces of nature from a single force or phenomenon.
One proposal for doing so is string theory, which posits that the pointlike particles of particle physics are replaced by onedimensional objects called strings. String theory describes how these strings propagate through space and interact with each other. On distance scales larger than the string scale, a string looks just like an ordinary particle, with its mass, charge, and other properties determined by the vibrational state of the string. In string theory, one of the many vibrational states of the string corresponds to the graviton, a quantum mechanical particle that carries gravitational force.^{[38]}^{[39]}
Another popular theory is loop quantum gravity (LQG), which describes quantum properties of gravity and is thus a theory of quantum spacetime. LQG is an attempt to merge and adapt standard quantum mechanics and standard general relativity. This theory describes space as an extremely fine fabric "woven" of finite loops called spin networks. The evolution of a spin network over time is called a spin foam. The characteristic length scale of a spin foam is the Planck length, approximately 1.616×10^{−35} m, and so lengths shorter than the Planck length are not physically meaningful in LQG.^{[40]}
Philosophical implications
Unsolved problem in physics: Is there a preferred interpretation of quantum mechanics? How does the quantum description of reality, which includes elements such as the "superposition of states" and "wave function collapse", give rise to the reality we perceive? (more unsolved problems in physics)

Since its inception, the many counterintuitive aspects and results of quantum mechanics have provoked strong philosophical debates and many interpretations. The arguments centre on the probabilistic nature of quantum mechanics, the difficulties with wavefunction collapse and the related measurement problem, and quantum nonlocality. Perhaps the only consensus that exists about these issues is that there is no consensus. Richard Feynman once said, "I think I can safely say that nobody understands quantum mechanics."^{[41]} According to Steven Weinberg, "There is now in my opinion no entirely satisfactory interpretation of quantum mechanics."^{[42]}
The views of Niels Bohr, Werner Heisenberg and other physicists are often grouped together as the "Copenhagen interpretation".^{[43]}^{[44]} According to these views, the probabilistic nature of quantum mechanics is not a temporary feature which will eventually be replaced by a deterministic theory, but is instead a final renunciation of the classical idea of "causality". Bohr in particular emphasized that any welldefined application of the quantum mechanical formalism must always make reference to the experimental arrangement, due to the complementary nature of evidence obtained under different experimental situations. Copenhagentype interpretations remain popular in the 21st century.^{[45]}
Albert Einstein, himself one of the founders of quantum theory, was troubled by its apparent failure to respect some cherished metaphysical principles, such as determinism and locality. Einstein's longrunning exchanges with Bohr about the meaning and status of quantum mechanics are now known as the Bohr–Einstein debates. Einstein believed that underlying quantum mechanics must be a theory that explicitly forbids action at a distance. He argued that quantum mechanics was incomplete, a theory that was valid but not fundamental, analogous to how thermodynamics is valid, but the fundamental theory behind it is statistical mechanics. In 1935, Einstein and his collaborators Boris Podolsky and Nathan Rosen published an argument that the principle of locality implies the incompleteness of quantum mechanics, a thought experiment later termed the Einstein–Podolsky–Rosen paradox.^{[note 6]} In 1964, John Bell showed that EPR's principle of locality, together with determinism, was actually incompatible with quantum mechanics: they implied constraints on the correlations produced by distance systems, now known as Bell inequalities, that can be violated by entangled particles.^{[50]} Since then several experiments have been performed to obtain these correlations, with the result that they do in fact violate Bell inequalities, and thus falsify the conjunction of locality with determinism.^{[13]}^{[14]}
Bohmian mechanics shows that it is possible to reformulate quantum mechanics to make it deterministic, at the price of making it explicitly nonlocal. It attributes not only a wave function to a physical system, but in addition a real position, that evolves deterministically under a nonlocal guiding equation. The evolution of a physical system is given at all times by the Schrödinger equation together with the guiding equation; there is never a collapse of the wave function. This solves the measurement problem.^{[51]}
Everett's manyworlds interpretation, formulated in 1956, holds that all the possibilities described by quantum theory simultaneously occur in a multiverse composed of mostly independent parallel universes.^{[52]} This is a consequence of removing the axiom of the collapse of the wave packet. All possible states of the measured system and the measuring apparatus, together with the observer, are present in a real physical quantum superposition. While the multiverse is deterministic, we perceive nondeterministic behavior governed by probabilities, because we don't observe the multiverse as a whole, but only one parallel universe at a time. Exactly how this is supposed to work has been the subject of much debate. Several attempts have been made to make sense of this and derive the Born rule,^{[53]}^{[54]} with no consensus on whether they have been successful.^{[55]}^{[56]}^{[57]}
Relational quantum mechanics appeared in the late 1990s as a modern derivative of Copenhagentype ideas,^{[58]} and QBism was developed some years later.^{[59]}
History
Quantum mechanics was developed in the early decades of the 20th century, driven by the need to explain phenomena that, in some cases, had been observed in earlier times. Scientific inquiry into the wave nature of light began in the 17th and 18th centuries, when scientists such as Robert Hooke, Christiaan Huygens and Leonhard Euler proposed a wave theory of light based on experimental observations.^{[60]} In 1803 English polymath Thomas Young described the famous doubleslit experiment.^{[61]} This experiment played a major role in the general acceptance of the wave theory of light.
During the early 19th century, chemical research by John Dalton and Amedeo Avogadro lent weight to the atomic theory of matter, an idea that James Clerk Maxwell, Ludwig Boltzmann and others built upon to establish the kinetic theory of gases. The successes of kinetic theory gave further credence to the idea that matter is composed of atoms, yet the theory also had shortcomings that would only be resolved by the development of quantum mechanics.^{[62]} While the early conception of atoms from Greek philosophy had been that they were indivisible units — the word "atom" deriving from the Greek for "uncuttable" — the 19th century saw the formulation of hypotheses about subatomic structure. One important discovery in that regard was Michael Faraday's 1838 observation of a glow caused by an electrical discharge inside a glass tube containing gas at low pressure. Julius Plücker, Johann Wilhelm Hittorf and Eugen Goldstein carried on and improved upon Faraday's work, leading to the identification of cathode rays, which J. J. Thomson found to consist of subatomic particles that would be called electrons.^{[63]}^{[64]}
The blackbody radiation problem was discovered by Gustav Kirchhoff in 1859. In 1900, Max Planck proposed the hypothesis that energy is radiated and absorbed in discrete "quanta" (or energy packets), yielding a calculation that precisely matched the observed patterns of blackbody radiation.^{[65]} The word quantum derives from the Latin, meaning "how great" or "how much".^{[66]} According to Planck, quantities of energy could be thought of as divided into "elements" whose size (E) would be proportional to their frequency (ν):
 [math]\displaystyle{ E = h \nu\ }[/math],
where h is Planck's constant. Planck cautiously insisted that this was only an aspect of the processes of absorption and emission of radiation and was not the physical reality of the radiation.^{[67]} In fact, he considered his quantum hypothesis a mathematical trick to get the right answer rather than a sizable discovery.^{[68]} However, in 1905 Albert Einstein interpreted Planck's quantum hypothesis realistically and used it to explain the photoelectric effect, in which shining light on certain materials can eject electrons from the material. Niels Bohr then developed Planck's ideas about radiation into a model of the hydrogen atom that successfully predicted the spectral lines of hydrogen.^{[69]} Einstein further developed this idea to show that an electromagnetic wave such as light could also be described as a particle (later called the photon), with a discrete amount of energy that depends on its frequency.^{[70]} In his paper "On the Quantum Theory of Radiation," Einstein expanded on the interaction between energy and matter to explain the absorption and emission of energy by atoms. Although overshadowed at the time by his general theory of relativity, this paper articulated the mechanism underlying the stimulated emission of radiation,^{[71]} which became the basis of the laser.
This phase is known as the old quantum theory. Never complete or selfconsistent, the old quantum theory was rather a set of heuristic corrections to classical mechanics.^{[72]} The theory is now understood as a semiclassical approximation^{[73]} to modern quantum mechanics.^{[74]} Notable results from this period include, in addition to the work of Planck, Einstein and Bohr mentioned above, Einstein and Peter Debye's work on the specific heat of solids, Bohr and Hendrika Johanna van Leeuwen's proof that classical physics cannot account for diamagnetism, and Arnold Sommerfeld's extension of the Bohr model to include specialrelativistic effects.
In the mid1920s quantum mechanics was developed to become the standard formulation for atomic physics. In 1923, the French physicist Louis de Broglie put forward his theory of matter waves by stating that particles can exhibit wave characteristics and vice versa. Building on de Broglie's approach, modern quantum mechanics was born in 1925, when the German physicists Werner Heisenberg, Max Born, and Pascual Jordan^{[75]}^{[76]} developed matrix mechanics and the Austrian physicist Erwin Schrödinger invented wave mechanics. Born introduced the probabilistic interpretation of Schrödinger's wave function in July 1926.^{[77]} Thus, the entire field of quantum physics emerged, leading to its wider acceptance at the Fifth Solvay Conference in 1927.^{[78]}
By 1930 quantum mechanics had been further unified and formalized by David Hilbert, Paul Dirac and John von Neumann^{[79]} with greater emphasis on measurement, the statistical nature of our knowledge of reality, and philosophical speculation about the 'observer'. It has since permeated many disciplines, including quantum chemistry, quantum electronics, quantum optics, and quantum information science. It also provides a useful framework for many features of the modern periodic table of elements, and describes the behaviors of atoms during chemical bonding and the flow of electrons in computer semiconductors, and therefore plays a crucial role in many modern technologies. While quantum mechanics was constructed to describe the world of the very small, it is also needed to explain some macroscopic phenomena such as superconductors^{[80]} and superfluids.^{[81]}
See also
 Bra–ket notation
 Einstein's thought experiments
 List of textbooks on classical and quantum mechanics
 Macroscopic quantum phenomena
 Phasespace formulation
 Regularization
 Twostate quantum system
Notes
 ↑ See, for example, Precision tests of QED. The relativistic refinement of quantum mechanics known as quantum electrodynamics (QED) has been shown to agree with experiment to within 1 part in 10^{8} for some atomic properties.
 ↑ Physicist John C. Baez cautions, "there's no way to understand the interpretation of quantum mechanics without also being able to solve quantum mechanics problems — to understand the theory, you need to be able to use it (and vice versa)".^{[15]} Carl Sagan outlined the "mathematical underpinning" of quantum mechanics and wrote, "For most physics students, this might occupy them from, say, third grade to early graduate school—roughly 15 years. [...] The job of the popularizer of science, trying to get across some idea of quantum mechanics to a general audience that has not gone through these initiation rites, is daunting. Indeed, there are no successful popularizations of quantum mechanics in my opinion—partly for this reason."^{[16]}
 ↑ A momentum eigenstate would be a perfectly monochromatic wave of infinite extent, which is not squareintegrable. Likewise, a position eigenstate would be a Dirac delta distribution, not squareintegrable and technically not a function at all. Consequently, neither can belong to the particle's Hilbert space. Physicists sometimes introduce fictitious "bases" for a Hilbert space comprising elements outside that space. These are invented for calculational convenience and do not represent physical states.^{[19]}^{:100–105}
 ↑ See, for example, the Feynman Lectures on Physics for some of the technological applications which use quantum mechanics, e.g., transistors (vol III, pp. 14–11 ff), integrated circuits, which are followon technology in solidstate physics (vol II, pp. 8–6), and lasers (vol III, pp. 9–13).
 ↑ see macroscopic quantum phenomena, Bose–Einstein condensate, and Quantum machine
 ↑ The published form of the EPR argument was due to Podolsky, and Einstein himself was not satisfied with it. In his own publications and correspondence, Einstein used a different argument to insist that quantum mechanics is an incomplete theory.^{[46]}^{[47]}^{[48]}^{[49]}
References
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 ↑ ^{2.0} ^{2.1} ^{2.2} Feynman, Richard; Leighton, Robert; Sands, Matthew (1964). The Feynman Lectures on Physics. 3. California Institute of Technology. ISBN 9780201500646. https://www.feynmanlectures.caltech.edu/III_01.html. Retrieved 19 December 2020.
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 ↑ Bub, Jeffrey (2019). "Quantum entanglement". in Zalta, Edward N.. Stanford Encyclopedia of Philosophy. Metaphysics Research Lab, Stanford University. https://plato.stanford.edu/entries/qtentangle/.
 ↑ ^{12.0} ^{12.1} Caves, Carlton M. (2015). "Quantum Information Science: Emerging No More". OSA Century of Optics. The Optical Society. pp. 320–323. ISBN 9781943580040. Bibcode: 2013arXiv1302.1864C.
 ↑ ^{13.0} ^{13.1} Wiseman, Howard (October 2015). "Death by experiment for local realism" (in en). Nature 526 (7575): 649–650. doi:10.1038/nature15631. ISSN 00280836. PMID 26503054.
 ↑ ^{14.0} ^{14.1} Wolchover, Natalie (7 February 2017). "Experiment Reaffirms Quantum Weirdness" (in enUS). Quanta Magazine. https://www.quantamagazine.org/20170207belltestquantumloophole/.
 ↑ Baez, John C. (20 March 2020). "How to Learn Math and Physics". https://math.ucr.edu/home/baez/books.html.
 ↑ Sagan, Carl (1996). The DemonHaunted World: Science as a Candle in the Dark. Ballentine Books. p. 249. ISBN 0345409469.
 ↑ Greenstein, George; Zajonc, Arthur (2006). The Quantum Challenge: Modern Research on the Foundations of Quantum Mechanics (2nd ed.). Jones and Bartlett Publishers, Inc. p. 215. ISBN 9780763724702. https://books.google.com/books?id=5t0tm0FB1CsC&pg=PA215., Chapter 8, p. 215
 ↑ Weinberg, Steven (2010). Dreams Of A Final Theory: The Search for The Fundamental Laws of Nature. Random House. p. 82. ISBN 9781407063966. https://books.google.com/books?id=OLrZkgPsZR0C.
 ↑ ^{19.0} ^{19.1} ^{19.2} ^{19.3} CohenTannoudji, Claude; Diu, Bernard; Laloë, Franck (2005). Quantum Mechanics. John Wiley & Sons. ISBN 047116433X.
 ↑ Quantum Mechanics: NonRelativistic Theory. 3 (3rd ed.). Pergamon Press. 1977. ISBN 9780080209401. OCLC 2284121. https://archive.org/details/QuantumMechanics_104.
 ↑ Section 3.2 of Ballentine, Leslie E. (1970), "The Statistical Interpretation of Quantum Mechanics", Reviews of Modern Physics 42 (4): 358–381, doi:10.1103/RevModPhys.42.358, Bibcode: 1970RvMP...42..358B. This fact is experimentally wellknown for example in quantum optics; see e.g. chap. 2 and Fig. 2.1 Leonhardt, Ulf (1997), Measuring the Quantum State of Light, Cambridge: Cambridge University Press, ISBN 0521497302, https://archive.org/details/measuringquantum0000leon
 ↑ ^{22.0} ^{22.1} ^{22.2} Nielsen, Michael A.; Chuang, Isaac L. (2010). Quantum Computation and Quantum Information (2nd ed.). Cambridge: Cambridge University Press. ISBN 9781107002173. OCLC 844974180.
 ↑ ^{23.0} ^{23.1} Rieffel, Eleanor G.; Polak, Wolfgang H. (4 March 2011) (in en). Quantum Computing: A Gentle Introduction. MIT Press. ISBN 9780262015066.
 ↑ Wilde, Mark M. (2017). Quantum Information Theory (2nd ed.). Cambridge University Press. doi:10.1017/9781316809976.001. ISBN 9781107176164. OCLC 973404322.
 ↑ Schlosshauer, Maximilian (October 2019). "Quantum decoherence" (in en). Physics Reports 831: 1–57. doi:10.1016/j.physrep.2019.10.001. Bibcode: 2019PhR...831....1S.
 ↑ Rechenberg, Helmut (1987). "Erwin Schrödinger and the creation of wave mechanics" (PDF). Acta Physica Polonica B 19 (8): 683–695. http://www.actaphys.uj.edu.pl/fulltext?series=Reg&vol=19&page=683. Retrieved 13 June 2016.
 ↑ Mathews, Piravonu Mathews; Venkatesan, K. (1976). "The Schrödinger Equation and Stationary States". A Textbook of Quantum Mechanics. Tata McGrawHill. p. 36. ISBN 9780070965102. https://books.google.com/books?id=_qzs1DD3TcsC&pg=PA36.
 ↑ Paris, M. G. A. (1999). "Entanglement and visibility at the output of a Mach–Zehnder interferometer". Physical Review A 59 (2): 1615–1621. doi:10.1103/PhysRevA.59.1615. Bibcode: 1999PhRvA..59.1615P.
 ↑ Haack, G. R.; Förster, H.; Büttiker, M. (2010). "Parity detection and entanglement with a MachZehnder interferometer". Physical Review B 82 (15): 155303. doi:10.1103/PhysRevB.82.155303. Bibcode: 2010PhRvB..82o5303H.
 ↑ Vedral, Vlatko (2006). Introduction to Quantum Information Science. Oxford University Press. ISBN 9780199215706. OCLC 442351498.
 ↑ Cohen, Marvin L. (2008). "Essay: Fifty Years of Condensed Matter Physics". Physical Review Letters 101 (25): 250001. doi:10.1103/PhysRevLett.101.250001. PMID 19113681. Bibcode: 2008PhRvL.101y0001C. http://prl.aps.org/edannounce/PhysRevLett.101.250001. Retrieved 31 March 2012.
 ↑ Matson, John. "What Is Quantum Mechanics Good for?". Scientific American. http://www.scientificamerican.com/article/everydayquantumphysics/. Retrieved 18 May 2016.
 ↑ Tipler, Paul; Llewellyn, Ralph (2008). Modern Physics (5th ed.). W.H. Freeman and Company. pp. 160–161. ISBN 9780716775508.
 ↑ "Atomic Properties". Academic.brooklyn.cuny.edu. http://academic.brooklyn.cuny.edu/physics/sobel/Nucphys/atomprop.html.
 ↑ Hawking, Stephen; Penrose, Roger (2010). The Nature of Space and Time. ISBN 9781400834747. https://books.google.com/books?id=6aagBFWuyQC&pg=PA61.
 ↑ Tatsumi Aoyama; Masashi Hayakawa; Toichiro Kinoshita; Makiko Nio (2012). "TenthOrder QED Contribution to the Electron g2 and an Improved Value of the Fine Structure Constant". Physical Review Letters 109 (11): 111807. doi:10.1103/PhysRevLett.109.111807. PMID 23005618. Bibcode: 2012PhRvL.109k1807A.
 ↑ "The Nobel Prize in Physics 1979". Nobel Foundation. http://nobelprize.org/nobel_prizes/physics/laureates/1979/index.html.
 ↑ Becker, Katrin; Becker, Melanie; Schwarz, John (2007). String theory and Mtheory: A modern introduction. Cambridge University Press. ISBN 9780521860697.
 ↑ Zwiebach, Barton (2009). A First Course in String Theory. Cambridge University Press. ISBN 9780521880329.
 ↑ Rovelli, Carlo; Vidotto, Francesca (13 November 2014) (in en). Covariant Loop Quantum Gravity: An Elementary Introduction to Quantum Gravity and Spinfoam Theory. Cambridge University Press. ISBN 9781316148112. https://books.google.com/books?id=w6z0BQAAQBAJ.
 ↑ Feynman, Richard (1967) (in en). The Character of Physical Law. MIT Press. pp. 129. ISBN 0262560038.
 ↑ Weinberg, Steven (2012). "Collapse of the state vector". Physical Review A 85 (6): 062116. doi:10.1103/PhysRevA.85.062116. Bibcode: 2012PhRvA..85f2116W.
 ↑ Howard, Don (December 2004). "Who Invented the "Copenhagen Interpretation"? A Study in Mythology" (in en). Philosophy of Science 71 (5): 669–682. doi:10.1086/425941. ISSN 00318248. https://www.journals.uchicago.edu/doi/10.1086/425941.
 ↑ Camilleri, Kristian (May 2009). "Constructing the Myth of the Copenhagen Interpretation" (in en). Perspectives on Science 17 (1): 26–57. doi:10.1162/posc.2009.17.1.26. ISSN 10636145. http://www.mitpressjournals.org/doi/10.1162/posc.2009.17.1.26.
 ↑ Schlosshauer, Maximilian; Kofler, Johannes; Zeilinger, Anton (1 August 2013). "A snapshot of foundational attitudes toward quantum mechanics". Studies in History and Philosophy of Science Part B 44 (3): 222–230. doi:10.1016/j.shpsb.2013.04.004. Bibcode: 2013SHPMP..44..222S.
 ↑ Harrigan, Nicholas; Spekkens, Robert W. (2010). "Einstein, incompleteness, and the epistemic view of quantum states". Foundations of Physics 40 (2): 125. doi:10.1007/s1070100993470. Bibcode: 2010FoPh...40..125H.
 ↑ Howard, D. (1985). "Einstein on locality and separability". Studies in History and Philosophy of Science Part A 16 (3): 171–201. doi:10.1016/00393681(85)900019.
 ↑ Sauer, Tilman (1 December 2007). "An Einstein manuscript on the EPR paradox for spin observables" (in en). Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 38 (4): 879–887. doi:10.1016/j.shpsb.2007.03.002. ISSN 13552198. Bibcode: 2007SHPMP..38..879S. http://philsciarchive.pitt.edu/3222/.
 ↑ Einstein, Albert (1949). "Autobiographical Notes". in Schilpp, Paul Arthur. Albert Einstein: PhilosopherScientist. Open Court Publishing Company.
 ↑ Bell, J. S. (1 November 1964). "On the Einstein Podolsky Rosen paradox" (in en). Physics Physique Fizika 1 (3): 195–200. doi:10.1103/PhysicsPhysiqueFizika.1.195.
 ↑ Goldstein, Sheldon (2017). "Bohmian Mechanics". Stanford Encyclopedia of Philosophy. Metaphysics Research Lab, Stanford University. https://plato.stanford.edu/entries/qmbohm/.
 ↑ Barrett, Jeffrey (2018). "Everett's RelativeState Formulation of Quantum Mechanics". in Zalta, Edward N.. Stanford Encyclopedia of Philosophy. Metaphysics Research Lab, Stanford University. https://plato.stanford.edu/entries/qmeverett/.
 ↑ Everett, Hugh; Wheeler, J. A.; DeWitt, B. S.; Cooper, L. N.; Van Vechten, D.; Graham, N. (1973). The ManyWorlds Interpretation of Quantum Mechanics. Princeton Series in Physics. Princeton, NJ: Princeton University Press. p. v. ISBN 069108131X.
 ↑ Wallace, David (2003). "Everettian Rationality: defending Deutsch's approach to probability in the Everett interpretation". Stud. Hist. Phil. Mod. Phys. 34 (3): 415–438. doi:10.1016/S13552198(03)000364. Bibcode: 2003SHPMP..34..415W.
 ↑ Ballentine, L. E. (1973). "Can the statistical postulate of quantum theory be derived?—A critique of the manyuniverses interpretation". Foundations of Physics 3 (2): 229–240. doi:10.1007/BF00708440. Bibcode: 1973FoPh....3..229B.
 ↑ Landsman, N. P. (2008). "The Born rule and its interpretation". Compendium of Quantum Physics. Springer. ISBN 9783540706229. http://www.math.ru.nl/~landsman/Born.pdf. "The conclusion seems to be that no generally accepted derivation of the Born rule has been given to date, but this does not imply that such a derivation is impossible in principle."
 ↑ Kent, Adrian (2010). "One world versus many: The inadequacy of Everettian accounts of evolution, probability, and scientific confirmation". in S. Saunders. Many Worlds? Everett, Quantum Theory and Reality. Oxford University Press. Bibcode: 2009arXiv0905.0624K.
 ↑ Van Fraassen, Bas C. (April 2010). "Rovelli's World" (in en). Foundations of Physics 40 (4): 390–417. doi:10.1007/s1070100993265. ISSN 00159018. Bibcode: 2010FoPh...40..390V. http://link.springer.com/10.1007/s1070100993265.
 ↑ Healey, Richard (2016). "QuantumBayesian and Pragmatist Views of Quantum Theory". in Zalta, Edward N.. Stanford Encyclopedia of Philosophy. Metaphysics Research Lab, Stanford University. https://plato.stanford.edu/entries/quantumbayesian/.
 ↑ Born, Max; Wolf, Emil (1999). Principles of Optics. Cambridge University Press. ISBN 0521642221. OCLC 1151058062.
 ↑ Scheider, Walter (April 1986). "Bringing one of the great moments of science to the classroom" (in en). The Physics Teacher 24 (4): 217–219. doi:10.1119/1.2341987. ISSN 0031921X. Bibcode: 1986PhTea..24..217S. http://www.cavendishscience.org/phys/tyoung/tyoung.htm.
 ↑ Feynman, Richard; Leighton, Robert; Sands, Matthew (1964). The Feynman Lectures on Physics. 1. California Institute of Technology. ISBN 9780201500646. https://www.feynmanlectures.caltech.edu/I_40.html. Retrieved 30 September 2021.
 ↑ Martin, Andre (1986), "Cathode Ray Tubes for Industrial and Military Applications", in Hawkes, Peter, Advances in Electronics and Electron Physics, Volume 67, Academic Press, p. 183, ISBN 9780080577333, ""Evidence for the existence of "cathoderays" was first found by Plücker and Hittorf ...""
 ↑ Dahl, Per F. (19970101) (in en). Flash of the Cathode Rays: A History of J J Thomson's Electron. CRC Press. pp. 4757. ISBN 9780750304535. https://books.google.com/books?id=xUzaWGocMdMC&newbks=0.
 ↑ Mehra, J.; Rechenberg, H. (1982). The Historical Development of Quantum Theory, Vol. 1: The Quantum Theory of Planck, Einstein, Bohr and Sommerfeld. Its Foundation and the Rise of Its Difficulties (1900–1925). New York: SpringerVerlag. ISBN 9780387906423.
 ↑ "Quantum – Definition and More from the Free MerriamWebster Dictionary". Merriamwebster.com. http://www.merriamwebster.com/dictionary/quantum.
 ↑ Kuhn, T. S. (1978). Blackbody theory and the quantum discontinuity 1894–1912. Oxford: Clarendon Press. ISBN 9780195023831.
 ↑ Kragh, Helge (1 December 2000). "Max Planck: the reluctant revolutionary". https://physicsworld.com/a/maxplanckthereluctantrevolutionary/.
 ↑ Stachel, John (2009). "Bohr and the Photon". Quantum Reality, Relativistic Causality and the Closing of the Epistemic Circle. The Western Ontario Series in Philosophy of Science. 73. Dordrecht: Springer. pp. 69–83. doi:10.1007/9781402091070_5. ISBN 9781402091063.
 ↑ Einstein, A. (1905). "Über einen die Erzeugung und Verwandlung des Lichtes betreffenden heuristischen Gesichtspunkt". Annalen der Physik 17 (6): 132–148. doi:10.1002/andp.19053220607. Bibcode: 1905AnP...322..132E. Reprinted in Stachel, John, ed (1989) (in de). The Collected Papers of Albert Einstein. 2. Princeton University Press. pp. 149–166. See also "Einstein's early work on the quantum hypothesis", ibid. pp. 134–148.
 ↑ Einstein, Albert (1917). "Zur Quantentheorie der Strahlung" (in de). Physikalische Zeitschrift 18: 121–128. Bibcode: 1917PhyZ...18..121E. Translated in Einstein, A. (1967). "On the Quantum Theory of Radiation". The Old Quantum Theory. Elsevier. pp. 167–183. doi:10.1016/b9780080121024.500188. ISBN 9780080121024.
 ↑ ter Haar, D. (1967). The Old Quantum Theory. Pergamon Press. pp. 206. ISBN 9780080121017. https://archive.org/details/oldquantumtheory0000haar.
 ↑ "Semiclassical approximation". https://www.encyclopediaofmath.org/index.php?title=Semiclassical_approximation.
 ↑ Sakurai, J. J.; Napolitano, J. (2014). "Quantum Dynamics". Modern Quantum Mechanics. Pearson. ISBN 9781292024103. OCLC 929609283.
 ↑ David Edwards,The Mathematical Foundations of Quantum Mechanics, Synthese, Volume 42, Number 1/September, 1979, pp. 1–70.
 ↑ D. Edwards, The Mathematical Foundations of Quantum Field Theory: Fermions, Gauge Fields, and Supersymmetry, Part I: Lattice Field Theories, International J. of Theor. Phys., Vol. 20, No. 7 (1981).
 ↑ Bernstein, Jeremy (November 2005). "Max Born and the quantum theory" (in en). American Journal of Physics 73 (11): 999–1008. doi:10.1119/1.2060717. ISSN 00029505. Bibcode: 2005AmJPh..73..999B.
 ↑ Pais, Abraham (1997). A Tale of Two Continents: A Physicist's Life in a Turbulent World. Princeton, New Jersey: Princeton University Press. ISBN 0691012431. https://archive.org/details/taleoftwocontine00pais.
 ↑ Van Hove, Leon (1958). "Von Neumann's contributions to quantum mechanics". Bulletin of the American Mathematical Society 64 (3): Part 2:95–99. doi:10.1090/s000299041958102062. https://www.ams.org/journals/bull/19586403/S000299041958102062/S000299041958102062.pdf.
 ↑ Feynman, Richard. "The Feynman Lectures on Physics III 214". California Institute of Technology. http://www.feynmanlectures.caltech.edu/III_21.html#Ch21S5. "...it was long believed that the wave function of the Schrödinger equation would never have a macroscopic representation analogous to the macroscopic representation of the amplitude for photons. On the other hand, it is now realized that the phenomena of superconductivity presents us with just this situation."
 ↑ Packard, Richard (2006). "Berkeley Experiments on Superfluid Macroscopic Quantum Effects". http://physics.berkeley.edu/sites/default/files/_/lt24_berk_expts_on_macro_sup_effects.pdf.
Further reading
The following titles, all by working physicists, attempt to communicate quantum theory to lay people, using a minimum of technical apparatus.
 Chester, Marvin (1987) Primer of Quantum Mechanics. John Wiley. ISBN 0486428788
 Cox, Brian; Forshaw, Jeff (2011). The Quantum Universe: Everything That Can Happen Does Happen. Allen Lane. ISBN 9781846144325.
 Richard Feynman, 1985. QED: The Strange Theory of Light and Matter, Princeton University Press. ISBN 0691083886. Four elementary lectures on quantum electrodynamics and quantum field theory, yet containing many insights for the expert.
 Ghirardi, GianCarlo, 2004. Sneaking a Look at God's Cards, Gerald Malsbary, trans. Princeton Univ. Press. The most technical of the works cited here. Passages using algebra, trigonometry, and bra–ket notation can be passed over on a first reading.
 N. David Mermin, 1990, "Spooky actions at a distance: mysteries of the QT" in his Boojums all the way through. Cambridge University Press: 110–76.
 Victor Stenger, 2000. Timeless Reality: Symmetry, Simplicity, and Multiple Universes. Buffalo NY: Prometheus Books. Chpts. 5–8. Includes cosmological and philosophical considerations.
More technical:
 Bernstein, Jeremy (2009). Quantum Leaps. Cambridge, Massachusetts: Belknap Press of Harvard University Press. ISBN 9780674035416. https://books.google.com/books?id=j0Me3brYOL0C.
 Bohm, David (1989). Quantum Theory. Dover Publications. ISBN 9780486659695. https://archive.org/details/quantumtheory0000bohm.
 Eisberg, Robert; Resnick, Robert (1985). Quantum Physics of Atoms, Molecules, Solids, Nuclei, and Particles (2nd ed.). Wiley. ISBN 9780471873730. https://archive.org/details/quantumphysicsof00eisb.
 Bryce DeWitt, R. Neill Graham, eds., 1973. The ManyWorlds Interpretation of Quantum Mechanics, Princeton Series in Physics, Princeton University Press. ISBN 069108131X
 Everett, Hugh (1957). "Relative State Formulation of Quantum Mechanics". Reviews of Modern Physics 29 (3): 454–462. doi:10.1103/RevModPhys.29.454. Bibcode: 1957RvMP...29..454E. https://semanticscholar.org/paper/066c796be96aaec3ed3e77b99f5589f8847bf34f.
 Feynman, Richard P.; Leighton, Robert B.; Sands, Matthew (1965). The Feynman Lectures on Physics. 1–3. AddisonWesley. ISBN 9780738200088.
 D. Greenberger, K. Hentschel, F. Weinert, eds., 2009. Compendium of quantum physics, Concepts, experiments, history and philosophy, SpringerVerlag, Berlin, Heidelberg.
 Griffiths, David J. (2004). Introduction to Quantum Mechanics (2nd ed.). Prentice Hall. ISBN 9780131118928. OCLC 40251748. A standard undergraduate text.
 Max Jammer, 1966. The Conceptual Development of Quantum Mechanics. McGraw Hill.
 Hagen Kleinert, 2004. Path Integrals in Quantum Mechanics, Statistics, Polymer Physics, and Financial Markets, 3rd ed. Singapore: World Scientific. Draft of 4th edition.
 L.D. Landau, E.M. Lifshitz (1977). Quantum Mechanics: NonRelativistic Theory. 3 (3rd ed.). Pergamon Press. ISBN 9780080209401. Online copy
 Liboff, Richard L. (2002). Introductory Quantum Mechanics. AddisonWesley. ISBN 9780805387148.
 Gunther Ludwig, 1968. Wave Mechanics. London: Pergamon Press. ISBN 0082032041
 George Mackey (2004). The mathematical foundations of quantum mechanics. Dover Publications. ISBN 0486435172.
 Merzbacher, Eugen (1998). Quantum Mechanics. Wiley, John & Sons, Inc. ISBN 9780471887027.
 Albert Messiah, 1966. Quantum Mechanics (Vol. I), English translation from French by G.M. Temmer. North Holland, John Wiley & Sons. Cf. chpt. IV, section III. online
 Omnès, Roland (1999). Understanding Quantum Mechanics. Princeton University Press. ISBN 9780691004358. OCLC 39849482. https://archive.org/details/understandingqua00omne.
 Scerri, Eric R., 2006. The Periodic Table: Its Story and Its Significance. Oxford University Press. Considers the extent to which chemistry and the periodic system have been reduced to quantum mechanics. ISBN 0195305736
 Shankar, R. (1994). Principles of Quantum Mechanics. Springer. ISBN 9780306447907.
 Stone, A. Douglas (2013). Einstein and the Quantum. Princeton University Press. ISBN 9780691139685. https://archive.org/details/einsteinquantumq0000ston.
 Transnational College of Lex (1996). What is Quantum Mechanics? A Physics Adventure. Language Research Foundation, Boston. ISBN 9780964350410. OCLC 34661512.
 Veltman, Martinus J.G. (2003), Facts and Mysteries in Elementary Particle Physics.
On Wikibooks
External links
 J. O'Connor and E.F. Robertson: A history of quantum mechanics.
 Introduction to Quantum Theory at Quantiki.
 Quantum Physics Made Relatively Simple: three video lectures by Hans Bethe
 Course material
 Quantum Cook Book and PHYS 201: Fundamentals of Physics II by Ramamurti Shankar, Yale OpenCourseware
 The Modern Revolution in Physics – an online textbook.
 MIT OpenCourseWare: Chemistry and Physics. See 8.04, 8.05 and 8.06
 5½ Examples in Quantum Mechanics
 Imperial College Quantum Mechanics Course.
 Philosophy
 Ismael, Jenann. "Quantum Mechanics". in Zalta, Edward N.. Stanford Encyclopedia of Philosophy. https://plato.stanford.edu/entries/qm/.
 Krips, Henry. "Measurement in Quantum Theory". in Zalta, Edward N.. Stanford Encyclopedia of Philosophy. https://plato.stanford.edu/entries/qtmeasurement/.
Original source: https://en.wikipedia.org/wiki/ Quantum mechanics.
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