The general definition of a qubit as the quantum state of a two-level quantum system.
In quantum computing, a qubit (/ˈkjuːbɪt/) or quantum bit is a basic unit of quantum information—the quantum version of the classic binary bit physically realized with a two-state device. A qubit is a two-state (or two-level) quantum-mechanical system, one of the simplest quantum systems displaying the peculiarity of quantum mechanics. Examples include the spin of the electron in which the two levels can be taken as spin up and spin down; or the polarization of a single photon in which the two spin states (left-handed and the right-handed circular polarization) can also be measured as horizontal and vertical linear polarization. In a classical system, a bit would he to be in one state or the other. However, quantum mechanics allows the qubit to be in a coherent superposition of multiple states simultaneously, a property that is fundamental to quantum mechanics and quantum computing.
Etymology[edit]The coining of the term qubit is attributed to Benjamin Schumacher.[1] In the acknowledgments of his 1995 paper, Schumacher states that the term qubit was created in jest during a conversation with William Wootters.
Bit versus qubit[edit]A binary digit, characterized as 0 or 1, is used to represent information in classical computers. When eraged over both of its states (0,1), a binary digit can represent up to one bit of information content, where a bit is the basic unit of information. However, in this article, the word bit is synonymous with a binary digit.
In classical computer technologies, a processed bit is implemented by one of two levels of low direct current voltage, and whilst switching from one of these two levels to the other, a so-called "forbidden zone" between two logic levels must be passed as fast as possible, as electrical voltage cannot change from one level to another instantly.
There are two possible outcomes for the measurement of a qubit, usually taken to he the values "0" and "1", like a bit. However, whereas the state of a bit can only be binary (either 0 or 1), the general state of a qubit according to quantum mechanics can be an arbitrary coherent superposition of all computable states simultaneously.[2] Moreover, whereas a measurement of a classical bit would not disturb its state, a measurement of a qubit would destroy its coherence and irrevocably disturb the superposition state. It is possible to fully encode one bit in one qubit. However, a qubit can hold more information, e.g., up to two bits using superdense coding.
A bit is always completely in either one of its two states, and a set of n bits (e.g. a processor register or some bit array) can only hold a single of its 2n possible states at any time. A quantum state can be in a superposition state, which means that the qubit can he non-zero probability amplitude in both its states simultaneously (popularly expressed as "it can be in both states simultaneously"). A qubit requires two complex numbers to describe its two probability amplitudes, and these two complex numbers can together be viewed as a 2-dimensional complex vector, which is called a quantum state vector, or superposition state vector. Alternatively and equivalently, the value stored in a qubit can be described as a single point in a 2-dimensional complex coordinate space.
Furthermore, a set of n bits can be represented by n binary digits, simply by concatenating the representations of each of the bits, whereas a set of n qubits, which is also called a register, requires 2n complex numbers to describe its superposition state vector.[3][4]: 7–17 [2]: 13–17
Standard representation[edit]In quantum mechanics, the general quantum state of a qubit can be represented by a linear superposition of its two orthonormal basis states (or basis vectors). These vectors are usually denoted as | 0 ⟩ = [ 1 0 ] {\displaystyle |0\rangle ={\bigl [}{\begin{smallmatrix}1\\0\end{smallmatrix}}{\bigr ]}} and | 1 ⟩ = [ 0 1 ] {\displaystyle |1\rangle ={\bigl [}{\begin{smallmatrix}0\\1\end{smallmatrix}}{\bigr ]}} . They are written in the conventional Dirac—or "bra–ket"—notation; the | 0 ⟩ {\displaystyle |0\rangle } and | 1 ⟩ {\displaystyle |1\rangle } are pronounced "ket 0" and "ket 1", respectively. These two orthonormal basis states, { | 0 ⟩ , | 1 ⟩ } {\displaystyle \{|0\rangle ,|1\rangle \}} , together called the computational basis, are said to span the two-dimensional linear vector (Hilbert) space of the qubit.[5]
![{\displaystyle |0\rangle ={\bigl [}{\begin{smallmatrix}1\\0\end{smallmatrix}}{\bigr ]}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/279f5336e8dcc639125e7dda2410319b81c9bf94)
and
|
1
⟩
=
[
0
1
]
{\displaystyle |1\rangle ={\bigl [}{\begin{smallmatrix}0\\1\end{smallmatrix}}{\bigr ]}}
![{\displaystyle |1\rangle ={\bigl [}{\begin{smallmatrix}0\\1\end{smallmatrix}}{\bigr ]}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/e788c1d112bf1312c0a7d6416782b66eecb0788b)
. They are written in the conventional Dirac—or "bra–ket"—notation; the
|
0
⟩
{\displaystyle |0\rangle }
and
|
1
⟩
{\displaystyle |1\rangle }
are pronounced "ket 0" and "ket 1", respectively. These two orthonormal basis states,
{
|
0
⟩
,
|
1
⟩
}
{\displaystyle \{|0\rangle ,|1\rangle \}}
, together called the computational basis, are said to span the two-dimensional linear vector (Hilbert) space of the qubit.[5]
Qubit basis states can also be combined to form product basis states. A set of qubits taken together is called a quantum register. For example, two qubits could be represented in a four-dimensional linear vector space spanned by the following product basis states:
| 00 ⟩ = [ 1 0 0 0 ] {\displaystyle |00\rangle ={\biggl [}{\begin{smallmatrix}1\\0\\0\\0\end{smallmatrix}}{\biggr ]}} , | 01 ⟩ = [ 0 1 0 0 ] {\displaystyle |01\rangle ={\biggl [}{\begin{smallmatrix}0\\1\\0\\0\end{smallmatrix}}{\biggr ]}} , | 10 ⟩ = [ 0 0 1 0 ] {\displaystyle |10\rangle ={\biggl [}{\begin{smallmatrix}0\\0\\1\\0\end{smallmatrix}}{\biggr ]}} , and | 11 ⟩ = [ 0 0 0 1 ] {\displaystyle |11\rangle ={\biggl [}{\begin{smallmatrix}0\\0\\0\\1\end{smallmatrix}}{\biggr ]}} .
![{\displaystyle |00\rangle ={\biggl [}{\begin{smallmatrix}1\\0\\0\\0\end{smallmatrix}}{\biggr ]}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/814b0d8fe628d367664121a8ca6476ab0d1e3eb1)
,
|
01
⟩
=
[
0
1
0
0
]
{\displaystyle |01\rangle ={\biggl [}{\begin{smallmatrix}0\\1\\0\\0\end{smallmatrix}}{\biggr ]}}
![{\displaystyle |01\rangle ={\biggl [}{\begin{smallmatrix}0\\1\\0\\0\end{smallmatrix}}{\biggr ]}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/82dd56d4009b20c6161c2766a23e9783733ee441)
,
|
10
⟩
=
[
0
0
1
0
]
{\displaystyle |10\rangle ={\biggl [}{\begin{smallmatrix}0\\0\\1\\0\end{smallmatrix}}{\biggr ]}}
![{\displaystyle |10\rangle ={\biggl [}{\begin{smallmatrix}0\\0\\1\\0\end{smallmatrix}}{\biggr ]}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/96d0f59de833b73b8e3df20ceae3b2fc94fc0231)
, and
|
11
⟩
=
[
0
0
0
1
]
{\displaystyle |11\rangle ={\biggl [}{\begin{smallmatrix}0\\0\\0\\1\end{smallmatrix}}{\biggr ]}}
![{\displaystyle |11\rangle ={\biggl [}{\begin{smallmatrix}0\\0\\0\\1\end{smallmatrix}}{\biggr ]}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/d90f338913e70a0f691593bed17c2da7a3752b81)
.
In general, n qubits are represented by a superposition state vector in 2n dimensional Hilbert space.[5]
Qubit states[edit]
Polarization of light offers a straightforward way to present orthogonal states. With a typical mapping
|
H
⟩
=
|
0
⟩
{\displaystyle |H\rangle =|0\rangle }
and
|
V
⟩
=
|
1
⟩
{\displaystyle |V\rangle =|1\rangle }
, quantum states
(
|
0
⟩
±
|
1
⟩
)
/
2
{\displaystyle (|0\rangle \pm |1\rangle )/{\sqrt {2}}}
he a direct physical representation, both easily demonstrable experimentally in a class with linear polarizers and, for real
α
{\displaystyle \alpha }
and
β
{\displaystyle \beta }
, matching the high-school definition of orthogonality.[6]
and
|
V
⟩
=
|
1
⟩
{\displaystyle |V\rangle =|1\rangle }
, quantum states
(
|
0
⟩
±
|
1
⟩
)
/
2
{\displaystyle (|0\rangle \pm |1\rangle )/{\sqrt {2}}}
he a direct physical representation, both easily demonstrable experimentally in a class with linear polarizers and, for real
α
{\displaystyle \alpha }
and
β
{\displaystyle \beta }
, matching the high-school definition of orthogonality.[6]
A pure qubit state is a coherent superposition of the basis states. This means that a single qubit ( ψ {\displaystyle \psi } ) can be described by a linear combination of | 0 ⟩ {\displaystyle |0\rangle } and | 1 ⟩ {\displaystyle |1\rangle } :
| ψ ⟩ = α | 0 ⟩ + β | 1 ⟩ {\displaystyle |\psi \rangle =\alpha |0\rangle +\beta |1\rangle }
) can be described by a linear combination of
|
0
⟩
{\displaystyle |0\rangle }
where α and β are the probability amplitudes, and are both complex numbers. When we measure this qubit in the standard basis, according to the Born rule, the probability of outcome | 0 ⟩ {\displaystyle |0\rangle } with value "0" is | α | 2 {\displaystyle |\alpha |^{2}} and the probability of outcome | 1 ⟩ {\displaystyle |1\rangle } with value "1" is | β | 2 {\displaystyle |\beta |^{2}} . Because the absolute squares of the amplitudes equate to probabilities, it follows that α {\displaystyle \alpha } and β {\displaystyle \beta } must be constrained according to the second axiom of probability theory by the equation[4]
| α | 2 + | β | 2 = 1. {\displaystyle |\alpha |^{2}+|\beta |^{2}=1.}
and the probability of outcome
|
1
⟩
{\displaystyle |1\rangle }
. Because the absolute squares of the amplitudes equate to probabilities, it follows that
α
{\displaystyle \alpha }
The probability amplitudes, α {\displaystyle \alpha } and β {\displaystyle \beta } , encode more than just the probabilities of the outcomes of a measurement; the relative phase between α {\displaystyle \alpha } and β {\displaystyle \beta } is for example responsible for quantum interference, as seen in the double-slit experiment.
Bloch sphere representation[edit]
Bloch sphere representation of a qubit. The probability amplitudes for the superposition state,
|
ψ
⟩
=
α
|
0
⟩
+
β
|
1
⟩
,
{\displaystyle |\psi \rangle =\alpha |0\rangle +\beta |1\rangle ,\,}
are given by
α
=
cos
(
θ
2
)
{\displaystyle \alpha =\cos \left({\frac {\theta }{2}}\right)}
and
β
=
e
i
φ
sin
(
θ
2
)
{\displaystyle \beta =e^{i\varphi }\sin \left({\frac {\theta }{2}}\right)}
are given by
α
=
cos
(
θ
2
)
{\displaystyle \alpha =\cos \left({\frac {\theta }{2}}\right)}
and
β
=
e
i
φ
sin
(
θ
2
)
{\displaystyle \beta =e^{i\varphi }\sin \left({\frac {\theta }{2}}\right)}
It might, at first sight, seem that there should be four degrees of freedom in | ψ ⟩ = α | 0 ⟩ + β | 1 ⟩ {\displaystyle |\psi \rangle =\alpha |0\rangle +\beta |1\rangle \,} , as α {\displaystyle \alpha } and β {\displaystyle \beta } are complex numbers with two degrees of freedom each. However, one degree of freedom is removed by the normalization constraint |α|2 + |β|2 = 1. This means, with a suitable change of coordinates, one can eliminate one of the degrees of freedom. One possible choice is that of Hopf coordinates:
α = e i δ cos θ 2 , β = e i ( δ + φ ) sin θ 2 . {\displaystyle {\begin{aligned}\alpha &=e^{i\delta }\cos {\frac {\theta }{2}},\\\beta &=e^{i(\delta +\varphi )}\sin {\frac {\theta }{2}}.\end{aligned}}}
, as
α
{\displaystyle \alpha }
Additionally, for a single qubit, the global phase of the state e i δ {\displaystyle e^{i\delta }} has no physically observable consequences,[a] so we can arbitrarily choose α to be real (or β in the case that α is zero), leing just two degrees of freedom:
α = cos θ 2 , β = e i φ sin θ 2 , {\displaystyle {\begin{aligned}\alpha &=\cos {\frac {\theta }{2}},\\\beta &=e^{i\varphi }\sin {\frac {\theta }{2}},\end{aligned}}}
has no physically observable consequences,[a] so we can arbitrarily choose α to be real (or β in the case that α is zero), leing just two degrees of freedom:
where e i φ {\displaystyle e^{i\varphi }} is the physically significant relative phase.[7][b]
is the physically significant relative phase.[7][b]
The possible quantum states for a single qubit can be visualised using a Bloch sphere (see picture). Represented on such a 2-sphere, a classical bit could only be at the "North Pole" or the "South Pole", in the locations where | 0 ⟩ {\displaystyle |0\rangle } and | 1 ⟩ {\displaystyle |1\rangle } are respectively. This particular choice of the polar axis is arbitrary, however. The rest of the surface of the Bloch sphere is inaccessible to a classical bit, but a pure qubit state can be represented by any point on the surface. For example, the pure qubit state ( | 0 ⟩ + | 1 ⟩ ) / 2 {\displaystyle (|0\rangle +|1\rangle )/{\sqrt {2}}} would lie on the equator of the sphere at the positive X-axis. In the classical limit, a qubit, which can he quantum states anywhere on the Bloch sphere, reduces to the classical bit, which can be found only at either poles.
would lie on the equator of the sphere at the positive X-axis. In the classical limit, a qubit, which can he quantum states anywhere on the Bloch sphere, reduces to the classical bit, which can be found only at either poles.
The surface of the Bloch sphere is a two-dimensional space, which represents the observable state space of the pure qubit states. This state space has two local degrees of freedom, which can be represented by the two angles φ {\displaystyle \varphi } and θ {\displaystyle \theta } .
Mixed state[edit] Main article: Density matrix
and
θ
{\displaystyle \theta }
.
A pure state is fully specified by a single ket, | ψ ⟩ = α | 0 ⟩ + β | 1 ⟩ , {\displaystyle |\psi \rangle =\alpha |0\rangle +\beta |1\rangle ,\,} a coherent superposition, represented by a point on the surface of the Bloch sphere as described above. Coherence is essential for a qubit to be in a superposition state. With interactions, quantum noise and decoherence, it is possible to put the qubit in a mixed state, a statistical combination or "incoherent mixture" of different pure states. Mixed states can be represented by points inside the Bloch sphere (or in the Bloch ball). A mixed qubit state has three degrees of freedom: the angles φ {\displaystyle \varphi } and θ {\displaystyle \theta } , as well as the length r {\displaystyle r} of the vector that represents the mixed state.
of the vector that represents the mixed state.
Quantum error correction can be used to maintain the purity of qubits.
Operations on qubits[edit] Further information: DiVincenzo's criteria and Physical and logical qubitsVarious kinds of physical operations can be performed on qubits.
Quantum logic gates, building blocks for a quantum circuit in a quantum computer, operate on a set of qubits (a register); mathematically, the qubits undergo a (reversible) unitary transformation described by multiplying the quantum gates unitary matrix with the quantum state vector. The result from this multiplication is a new quantum state vector. Quantum measurement is an irreversible operation in which information is gained about the state of a single qubit, and coherence is lost. The result of the measurement of a single qubit with the state | ψ ⟩ = α | 0 ⟩ + β | 1 ⟩ {\displaystyle |\psi \rangle =\alpha |0\rangle +\beta |1\rangle } will be either | 0 ⟩ {\displaystyle |0\rangle } with probability | α | 2 {\displaystyle |\alpha |^{2}} or | 1 ⟩ {\displaystyle |1\rangle } with probability | β | 2 {\displaystyle |\beta |^{2}} . Measurement of the state of the qubit alters the magnitudes of α and β. For instance, if the result of the measurement is | 1 ⟩ {\displaystyle |1\rangle } , α is changed to 0 and β is changed to 1, while the phase factor e i ϕ {\displaystyle e^{i\phi }} is no longer experimentally accessible. If measurement is performed on a qubit that is entangled, the measurement may collapse the state of the other entangled qubits. Initialization or re-initialization to a known value, often | 0 ⟩ {\displaystyle |0\rangle } . This operation collapses the quantum state (exactly like with measurement). Initialization to | 0 ⟩ {\displaystyle |0\rangle } may be implemented logically or physically: Logically as a measurement, followed by the application of the Pauli-X gate if the result from the measurement was | 1 ⟩ {\displaystyle |1\rangle } . Physically, for example, if it is a superconducting phase qubit, by lowering the energy of the quantum system to its ground state. Sending the qubit through a quantum channel to a remote system or machine (an I/O operation), potentially as part of a quantum network. Quantum entanglement[edit] Main articles: Quantum entanglement and Bell state
is no longer experimentally accessible. If measurement is performed on a qubit that is entangled, the measurement may collapse the state of the other entangled qubits.
Initialization or re-initialization to a known value, often
|
0
⟩
{\displaystyle |0\rangle }
An important distinguishing feature between qubits and classical bits is that multiple qubits can exhibit quantum entanglement; the qubit itself is an exhibition of quantum entanglement. In this case, quantum entanglement is a local or nonlocal property of two or more qubits that allows a set of qubits to express higher correlation than is possible in classical systems.
The simplest system to display quantum entanglement is the system of two qubits. Consider, for example, two entangled qubits in the | Φ + ⟩ {\displaystyle |\Phi ^{+}\rangle } Bell state:
1 2 ( | 00 ⟩ + | 11 ⟩ ) . {\displaystyle {\frac {1}{\sqrt {2}}}(|00\rangle +|11\rangle ).}
Bell state:
In this state, called an equal superposition, there are equal probabilities of measuring either product state | 00 ⟩ {\displaystyle |00\rangle } or | 11 ⟩ {\displaystyle |11\rangle } , as | 1 / 2 | 2 = 1 / 2 {\displaystyle |1/{\sqrt {2}}|^{2}=1/2} . In other words, there is no way to tell if the first qubit has value "0" or "1" and likewise for the second qubit.
or
|
11
⟩
{\displaystyle |11\rangle }
, as
|
1
/
2
|
2
=
1
/
2
{\displaystyle |1/{\sqrt {2}}|^{2}=1/2}
. In other words, there is no way to tell if the first qubit has value "0" or "1" and likewise for the second qubit.
Imagine that these two entangled qubits are separated, with one each given to Alice and Bob. Alice makes a measurement of her qubit, obtaining—with equal probabilities—either | 0 ⟩ {\displaystyle |0\rangle } or | 1 ⟩ {\displaystyle |1\rangle } , i.e., she can now tell if her qubit has value "0" or "1". Because of the qubits' entanglement, Bob must now get exactly the same measurement as Alice. For example, if she measures a | 0 ⟩ {\displaystyle |0\rangle } , Bob must measure the same, as | 00 ⟩ {\displaystyle |00\rangle } is the only state where Alice's qubit is a | 0 ⟩ {\displaystyle |0\rangle } . In short, for these two entangled qubits, whatever Alice measures, so would Bob, with perfect correlation, in any basis, however far apart they may be and even though both can not tell if their qubit has value "0" or "1"—a most surprising circumstance that cannot be explained by classical physics.
Controlled gate to construct the Bell state[edit]Controlled gates act on 2 or more qubits, where one or more qubits act as a control for some specified operation. In particular, the controlled NOT gate (CNOT or CX) acts on 2 qubits, and performs the NOT operation on the second qubit only when the first qubit is | 1 ⟩ {\displaystyle |1\rangle } , and otherwise lees it unchanged. With respect to the unentangled product basis { | 00 ⟩ {\displaystyle \{|00\rangle } , | 01 ⟩ {\displaystyle |01\rangle } , | 10 ⟩ {\displaystyle |10\rangle } , | 11 ⟩ } {\displaystyle |11\rangle \}} , it maps the basis states as follows:
| 00 ⟩ ↦ | 00 ⟩ {\displaystyle |00\rangle \mapsto |00\rangle } | 01 ⟩ ↦ | 01 ⟩ {\displaystyle |01\rangle \mapsto |01\rangle } | 10 ⟩ ↦ | 11 ⟩ {\displaystyle |10\rangle \mapsto |11\rangle } | 11 ⟩ ↦ | 10 ⟩ {\displaystyle |11\rangle \mapsto |10\rangle } .
,
|
01
⟩
{\displaystyle |01\rangle }
,
|
10
⟩
{\displaystyle |10\rangle }
,
|
11
⟩
}
{\displaystyle |11\rangle \}}
, it maps the basis states as follows:
|
01
⟩
↦
|
01
⟩
{\displaystyle |01\rangle \mapsto |01\rangle }
|
10
⟩
↦
|
11
⟩
{\displaystyle |10\rangle \mapsto |11\rangle }
|
11
⟩
↦
|
10
⟩
{\displaystyle |11\rangle \mapsto |10\rangle }
.
A common application of the CNOT gate is to maximally entangle two qubits into the | Φ + ⟩ {\displaystyle |\Phi ^{+}\rangle } Bell state. To construct | Φ + ⟩ {\displaystyle |\Phi ^{+}\rangle } , the inputs A (control) and B (target) to the CNOT gate are:
1 2 ( | 0 ⟩ + | 1 ⟩ ) A {\displaystyle {\frac {1}{\sqrt {2}}}(|0\rangle +|1\rangle )_{A}} ⊗ {\displaystyle \otimes } | 0 ⟩ B {\displaystyle |0\rangle _{B}} = 1 2 {\displaystyle {\frac {1}{\sqrt {2}}}} ( | 00 ⟩ + | 10 ⟩ ) {\displaystyle (|00\rangle +|10\rangle )} .
⊗
{\displaystyle \otimes }
|
0
⟩
B
{\displaystyle |0\rangle _{B}}
=
1
2
{\displaystyle {\frac {1}{\sqrt {2}}}}
(
|
00
⟩
+
|
10
⟩
)
{\displaystyle (|00\rangle +|10\rangle )}
.
After applying CNOT, the output is the | Φ + ⟩ {\displaystyle |\Phi ^{+}\rangle } Bell State: 1 2 ( | 00 ⟩ + | 11 ⟩ ) {\displaystyle {\frac {1}{\sqrt {2}}}(|00\rangle +|11\rangle )} .
Applications[edit]
.
The | Φ + ⟩ {\displaystyle |\Phi ^{+}\rangle } Bell state forms part of the setup of the superdense coding, quantum teleportation, and entangled quantum cryptography algorithms.
Quantum entanglement also allows multiple states (such as the Bell state mentioned above) to be acted on simultaneously, unlike classical bits that can only he one value at a time. Entanglement is a necessary ingredient of any quantum computation that cannot be done efficiently on a classical computer. Many of the successes of quantum computation and communication, such as quantum teleportation and superdense coding, make use of entanglement, suggesting that entanglement is a resource that is unique to quantum computation.[8] A major hurdle facing quantum computing, as of 2018, in its quest to surpass classical digital computing, is noise in quantum gates that limits the size of quantum circuits that can be executed reliably.[9]
Quantum register[edit]A number of qubits taken together is a qubit register. Quantum computers perform calculations by manipulating qubits within a register.
Qudits and qutrits[edit]The term qudit denotes the unit of quantum information that can be realized in suitable d-level quantum systems.[10] A qubit register that can be measured to N states is identical to an N-level qudit. A rarely used[11] synonym for qudit is quNit,[12] since both d and N are frequently used to denote the dimension of a quantum system.
Qudits are similar to the integer types in classical computing, and may be mapped to (or realized by) arrays of qubits. Qudits where the d-level system is not an exponent of 2 cannot be mapped to arrays of qubits. It is for example possible to he 5-level qudits.
In 2017, scientists at the National Institute of Scientific Research constructed a pair of qudits with 10 different states each, giving more computational power than 6 qubits.[13]
In 2022, researchers at the University of Innsbruck succeeded in developing a universal qudit quantum processor with trapped ions.[14] In the same year, researchers at Tsinghua University's Center for Quantum Information implemented the dual-type qubit scheme in trapped ion quantum computers using the same ion species.[15] In 2025, the Innsbruck team managed to simulate two-dimensional lattice gauge theories on their qudit quantum computer.[16]
Also in 2022, researchers at the University of California, Berkeley developed a technique to dynamically control the cross-Kerr interactions between fixed-frequency qutrits, achieving high two-qutrit gate fidelities.[17] This was followed by a demonstration of extensible control of superconducting qudits up to d = 4 {\displaystyle d=4} in 2024 based on programmable two-photon interactions.[18]
in 2024 based on programmable two-photon interactions.[18]
Similar to the qubit, the qutrit is the unit of quantum information that can be realized in suitable 3-level quantum systems. This is analogous to the unit of classical information trit of ternary computers.[19] Besides the advantage associated with the enlarged computational space, the third qutrit level can be exploited to implement efficient compilation of multi-qubit gates.[18][20][21]
Physical implementations[edit]Any two-level quantum-mechanical system can be used as a qubit. Multilevel systems can be used as well, if they possess two states that can be effectively decoupled from the rest (e.g., the ground state and first excited state of a nonlinear oscillator). There are various proposals. Several physical implementations that approximate two-level systems to various degrees he been successfully realized. Similarly to a classical bit, where the state of a transistor in a processor, the magnetization of a surface in a hard disk, and the presence of current in a cable can all be used to represent bits in the same computer, an eventual quantum computer is likely to use various combinations of qubits in its design.
All physical implementations are affected by noise. The so-called T1 lifetime and T2 dephasing time are a time to characterize the physical implementation and represent their sensitivity to noise. A higher time does not necessarily mean that one or the other qubit is better suited for quantum computing because gate times and fidelities need to be considered, too.
Different applications like quantum sensing, quantum computing and quantum communication use different implementations of qubits to suit their application.
The following is an incomplete list of physical implementations of qubits, and the choices of basis are by convention only.
Physical support Name Information support | 0 ⟩ {\displaystyle |0\rangle } | 1 ⟩ {\displaystyle |1\rangle } photon polarization encoding polarization of light horizontal vertical number of photons Fock state vacuum single-photon state time-bin encoding time of arrival early late coherent state of light squeezed light quadrature amplitude-squeezed state phase-squeezed state electrons electronic spin spin up down electron number charge no electron two electron nucleus nuclear spin addressed through NMR spin up down neutral atom atomic energy level spin up down trapped ion atomic energy level spin up down Josephson junction superconducting charge qubit charge uncharged superconducting island (Q = 0) charged superconducting island (Q = 2e, one extra Cooper pair) superconducting flux qubit current clockwise current counterclockwise current superconducting phase qubit energy ground state first excited state singly charged quantum dot pair electron localization charge electron on left dot electron on right dot quantum dot dot spin spin down up gapped topological system non-abelian anyons braiding of excitations depends on specific topological system depends on specific topological system vibrational qubit[22] vibrational states phonon/vibron | 01 ⟩ {\displaystyle |01\rangle } superposition | 10 ⟩ {\displaystyle |10\rangle } superposition van der Waals heterostructure[23] electron localization charge electron on bottom sheet electron on top sheet Qubit storage[edit]In 2008 a team of scientists from the U.K. and U.S. reported the first relatively long (1.75 seconds) and coherent transfer of a superposition state in an electron spin "processing" qubit to a nuclear spin "memory" qubit.[24] This event can be considered the first relatively consistent quantum data storage, a vital step towards the development of quantum computing. In 2013, a modification of similar systems (using charged rather than neutral donors) has dramatically extended this time, to 3 hours at very low temperatures and 39 minutes at room temperature.[25] Room temperature preparation of a qubit based on electron spins instead of nuclear spin was also demonstrated by a team of scientists from Switzerland and Australia.[26] An increased coherence of qubits is being explored by researchers who are testing the limitations of a Ge hole spin-orbit qubit structure.[27]
See also[edit]
Wikimedia Commons has media related to Qubit.
Ancilla bit
Electron-on-helium qubit
Physical and logical qubits
Unitary group
W state and Greenberger–Horne–Zeilinger state (GHZ state)
Notes[edit]
^ This is because of the Born rule. The probability of observing an outcome upon measurement is the modulus squared of the probability amplitude for that outcome (or basis state, eigenstate). The global phase factor
e
i
δ
{\displaystyle e^{i\delta }}
is not measurable, because it applies to both basis states, and is on the complex unit circle so
|
e
i
δ
|
2
=
1.
{\displaystyle |e^{i\delta }|^{2}=1.}
Note that by removing
e
i
δ
{\displaystyle e^{i\delta }}
it means that quantum states with global phase can not be represented as points on the surface of the Bloch sphere.
^ The Pauli Z basis is usually called the computational basis, where the relative phase he no effect on measurement. Measuring instead in the X or Y Pauli basis depends on the relative phase. For example,
(
|
0
⟩
+
e
i
π
/
2
|
1
⟩
)
/
2
{\displaystyle (|0\rangle +e^{i\pi /2}|1\rangle )/{\sqrt {2}}}
will (because this state lies on the positive pole of the Y-axis) in the Y-basis always measure to the same value, while in the Z-basis results in equal probability of being measured to
|
0
⟩
{\displaystyle |0\rangle }
or
|
1
⟩
{\displaystyle |1\rangle }
.Because measurement collapses the quantum state, measuring the state in one basis hides some of the values that would he been measurable in the other basis; See the uncertainty principle.
References[edit]
^
Schumacher, B. (1995). "Quantum coding". Physical Review A. 51 (4): 2738–2747. Bibcode:1995PhRvA..51.2738S. doi:10.1103/PhysRevA.51.2738. PMID 9911903.
^ a b Nielsen, Michael A.; Chuang, Isaac L. (2010). Quantum Computation and Quantum Information. Cambridge University Press. p. 13. ISBN 978-1-107-00217-3.
^ Shor, Peter (1997). "Polynomial-Time Algorithms for Prime Factorization and Discrete Logarithms on a Quantum Computer∗". SIAM Journal on Computing. 26 (5): 1484–1509. arXiv:quant-ph/9508027. Bibcode:1995quant.ph..8027S. doi:10.1137/S0097539795293172. S2CID 2337707.
^ a b Williams, Colin P. (2011). Explorations in Quantum Computing. Springer. pp. 9–13. ISBN 978-1-84628-887-6.
^ a b Yanofsky, Noson S.; Mannucci, Mirco (2013). Quantum computing for computer scientists. Cambridge University Press. pp. 138–144. ISBN 978-0-521-87996-5.
^ Seskir, Zeki C.; Migdał, Piotr; Weidner, Carrie; Anupam, Aditya; Case, Nicky; Dis, Noah; Decaroli, Chiara; Ercan, İlke; Foti, Caterina; Gora, Paweł; Jankiewicz, Klementyna; La Cour, Brian R.; Malo, Jorge Yago; Maniscalco, Sabrina; Naeemi, Azad; Nita, Laurentiu; Parvin, Nassim; Scafirimuto, Fabio; Sherson, Jacob F.; Surer, Elif; Wootton, James; Yeh, Lia; Zabello, Olga; Chiofalo, Marilù (2022). "Quantum games and interactive tools for quantum technologies outreach and education". Optical Engineering. 61 (8): 081809. arXiv:2202.07756. Bibcode:2022OptEn..61h1809S. doi:10.1117/1.OE.61.8.081809.{{cite journal}}: CS1 maint: article number as page number (link)
Note that by removing
e
i
δ
{\displaystyle e^{i\delta }}
will (because this state lies on the positive pole of the Y-axis) in the Y-basis always measure to the same value, while in the Z-basis results in equal probability of being measured to
|
0
⟩
{\displaystyle |0\rangle }
This article incorporates text from this source, which is ailable under the CC BY 4.0 license.
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Further reading[edit]
Nielsen, Michael A.; Chuang, Isaac (2000). Quantum Computation and Quantum Information. Cambridge, England: Cambridge University Press. ISBN 0521632358. OCLC 43641333.
Williams, Colin P. (2011). Explorations in Quantum Computing. Springer. ISBN 978-1-84628-887-6.
Yanofsky, Noson S.; Mannucci, Mirco (2013). Quantum computing for computer scientists. Cambridge University Press. ISBN 978-0-521-87996-5.
A treatment of two-level quantum systems, decades before the term "qubit" was coined, is found in the third volume of The Feynman Lectures on Physics (2013 ebook edition), in chapters 9–11.
A non-traditional motivation of the qubit aimed at non-physicists is found in Quantum Computing Since Democritus, by Scott Aaronson, Cambridge University Press (2013).
An introduction to qubits for non-specialists, by the person who coined the word, is found in Lecture 21 of The science of information: from language to black holes, by Professor Benjamin Schumacher, The Great Courses, The Teaching Company (4 DVDs, 2015).
A picture book introduction to entanglement, showcasing a Bell state and the measurement of it, is found in Quantum entanglement for babies, by Chris Ferrie (2017). ISBN 9781492670261.
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