concept

Quantum superposition

Quantum superposition is a state where a quantum system exists in multiple distinct states simultaneously.
3 formulas · 4 who worked here

Description

Quantum superposition is not just a mix of pre-existing states, but a fundamental ability of nature to form their coherent combinations. Formally, such a state is written as a sum of basis vectors with complex weights: |ψ⟩ = c₁|φ₁⟩ + c₂|φ₂⟩ + ... . The probability of finding the system in a particular state after measurement is equal to the square of the modulus of the corresponding weight. That is why in the double-slit experiment, the particle demonstrates interference, as if passing through both slits at once. Superposition is preserved only with complete isolation from the environment; interaction with the surroundings destroys coherence, causing it to quickly vanish in macroscopic objects.

History

The idea of superposition was born from attempts to reconcile the wave behavior of matter, predicted by Louis de Broglie in 1924, with the particle picture. Erwin Schrödinger in 1926 constructed a wave equation for which, as with any linear differential equations, the sum of solutions is also a solution — thus the formal principle of superposition of states arose. In 1935, he also devised the paradox of 'Schrödinger's cat', demonstrating the problem of the transition from the micro-world to the macro-world. John Stewart Bell in 1964 showed that superposition leads to statistical correlations that cannot be explained classically (Bell's theorem); later, laboratory tests, initiated by Alain Aspect, brilliantly confirmed this prediction. Since the end of the 20th century, superposition has been actively used in quantum computing; the pioneer of this direction was David Deutsch, who described the universal quantum computer in 1985.

How it works

The state of a system is encoded as a vector |ψ⟩ in Hilbert space. According to the superposition principle, any linear combination of the form Σ c_i |φ_i⟩, where {|φ_i⟩} is a basis, and c_i are complex amplitudes, describes a physically realizable state. Time evolution obeys the Schrödinger equation, which preserves superposition: if the initial state was a superposition, then the subsequent state will remain a superposition as long as the system is isolated. Measurement, on the contrary, irreversibly projects the vector onto one of the eigenstates of the measured quantity; the probabilities are determined by the squared moduli of the amplitudes. In real conditions, the inevitable coupling to the heat bath entangles the system with a huge number of environmental degrees of freedom, quickly destroying coherence (decoherence) — that is why macroscopic superpositions are extremely difficult to create and maintain.

In practice

Quantum computers build superposition into the basis of computation: a qubit in a superposition of zero and one processes both values at once. This speeds up solving problems, such as modeling drugs or optimizing large systems.

Fun fact

A quantum bit, or qubit, in a superposition of 0 and 1 is capable of processing both states in parallel. This gives quantum computers an exponential advantage over classical ones in certain computational tasks.

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Formulas

$$|\text{cat}\rangle = \frac{1}{\sqrt{2}}(|\alpha\rangle + |-\alpha\rangle)$$
Quantum superposition of two coherent states.
What is in the formula
|cat⟩variablecat state vector — quantum state
|α⟩variablecoherent state with amplitude α — coherent state
|−α⟩variablecoherent state with amplitude −α — coherent state
|{cat}\rangle=\frac{1}{\sqrt{2}}(|α\rangle+|-α\rangle) · 2606.03293
$$a_k = \sum_n P_n |\langle \chi_k | n \rangle|^2$$
Probability amplitude as sum over Boltzmann-weighted overlaps.
What is in the formula
a_kvariableProbability amplitude for state k — probability amplitude
P_nvariableBoltzmann weight for state n — boltzmann weight
χ_kvariableEigenstate of observable — quantum state
nvariableEnergy eigenstate — quantum state
⟨ | ⟩operatorQuantum mechanical inner product — inner product
∑operatorSum over states — summation
a_k(t_i)=\sum_{n}p_n(t_i)|\langleχ_k|n\rangle|^2 · 2607.03845
$$F(\rho, \sigma) = \operatorname{Tr}\sqrt{\sqrt{\rho}\sigma\sqrt{\rho}}$$
Quantum fidelity measures similarity between two quantum states.
What is in the formula
FvariableQuantum fidelity between states — fidelity
ρvariableDensity matrix of first quantum state — density matrix
σvariableDensity matrix of second quantum state — density matrix
TroperatorSum of diagonal elements of a matrix — trace operator
√operatorPrincipal square root of a positive semidefinite matrix — matrix square root
k({x}_n,{x}_m)=\operatorname{tr}[ρ_a({x}_n)ρ_a({x}_m)] · 2607.10656

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