Glossary
code: A code that uses n physical qubits to encode k logical qubits and will correct errors.
Abelian group: A group for which all elements commute.
Abelian subgroup: See Abelian Group, Subgroup
Adjoint (of a matrix): The transpose complex conjugate of an operator. (Also referred to as the conjugate or Hermitian conjugate.)
Ancilla: An ancillary (or extra) qubit not used directly in the computation, but used for other purposes, e.g. error correction.
Angular momentum: A vector quantity classically defined as the cross product of the instantaneous position vector and instantaneous linear momentum. In quantum mechanics, it is defined as the cross product of the position and momentum operators.
Anti-commutation: Two operators anti-commute when AB+BA=0.
Basis: Subset of a given vector space, V, that is both linearly independent and spans the vector space V. The number of elements in any basis are equal to the dimension of V.
Bath system: Describes a system that has had an unwanted interaction with an open quantum system. Environment.
Bell's theorem: "No physical theory of local hidden variables can ever reproduce all of the predictions of quantum mechanics." See Full Article
Bit flip error: An error which takes to and to . The operator which does this is the Pauli operator .
Bloch sphere: Unit sphere where a qubit can be represented as a point; geometrical representation of a two-level quantum system. Image
Block diagonal matrix: A matrix which has non-zero elements only in blocks along the diagonal.
Bra-ket notation: Used in quantum mechanics to describe quantum states, consisting of two distinct symbols: the left symbol, bra, and the right symbol, ket. Bra: ; Ket:
Centralizer:
Checksum: See Dot Product
Classical bit: A classical bit is represented by two different states of a classical system, which are represented by 1 and 0. (1.3)
Closed system:
Code:
Codewords:
Commutator: The commutator of and is denoted , which means . Its value may be found by implementing the operators of and on a test function. If the commutator of and is zero, they are said to commute.
Complex conjugate:
Complex number: A complex number has a real and imaginary part. A complex number can be represented in the form or, .
Controlled not (CNOT gate):
Controlled operation: An operation on a state or set of states that is conditioned on another state or set of states.
Coset of a group
CSS codes
Cyclic group
Dagger (see hermitian conjugate or adjoint)
Definite matrix (see matrix properties)
Degenerate: Having two or more eigenvalues that are equal.
Density matrix
Density operator
Depolarizing error
Determinant: When rows or columns of a matrix are taken as vectors, the determinant is the volume enclosed by those vectors and corresponding parallel vectors creating parallelograms. Determinants only exist for square matrices.
Diagonalizable: A matrix is diagonalizable when it can be put into the form , where and exist and are inverses.
Differentiable manifold
Dirac delta function
Dirac notation (see bra-ket notation)
Disjointness condition
Distance of a quantum error correcting code
DiVincenzo's requirements for quantum computing: See Section
Dot product: The scalar that results when two vectors have their corresponding components multiplied, and each of these products summed.
Dual matrix
Dual of a code
Eigenfunction, eigenvalue, eigenvector: If where is a matrix, is a scalar and is a vector, then is the eigenvector and is the eigenvalue. If is a function, it is called an eigenfunction.
Entangled state
Environment (see Bath system)
EPR paradox
Epsilon tensor
Equivalent representation
Error syndrome
Euler angle parametrization
Euler's law:
Expectation value:
Exponentiating a matrix (see matrix exponential)
Faithful representation
Field
Gate (see Quantum gate)
General linear group
Generators of a group
Generator matrix
Gram-Schmidt decomposition (see Schmidt decomposition)
Group
Grover's algorithm
bar (): Planck's constant divided by , is Planck's constant
Hadamard gate
Hamming bound
Hamming code
Hamming distance
Hamming weight
Hamiltonian: The Hamiltonian operator gives the total energy of the system.
Heisenberg exchange interaction (8.5.2):
Heisenberg uncertainty principle (see uncertainty principle)
Hermitian: An operator whose transpose equals its complex conjugate, i.e., the matrix is equal to its adjoint.
Hermitian conjugate: The transpose complex conjugate of an operator.
Hidden variable theory (see also local hidden variable theory):
Hilbert-Schmidt inner product (2.4)
Hilbert space
Homomorphism
: Denotes the square root of negative one
Identity matrix: A matrix of zeros except for the diagonal, where each element is 1. Multiplying any matrix of the same dimension by it leaves the original matrix unchanged.
Inner product (see dot product)
Inverse of a matrix: The inverse of a square matrix is the matrix, denoted , such that , where is identity matrix. (When the matrix is not square, it is possible to have a left and/or right inverse which does not satisfy both of these relations, but only one or the other.)
Invertible matrix: A matrix for which an inverse exists.
Isolated system (see Closed system): A system which does not interact with any other system.
Isomorphism: A one-to-one and onto mapping.
Isotropy group or Isotropy subgroup (see stabilizer)
Jacobi identity
Ket: See bra-ket notation
Kraus representation (or Kraus decomposition) (see SMR representation)
Kronecker delta
Levi-Civita symbol (see epsilon tensor)
Lie algebra
Lie group
Linear code
Linear combination: A set of vectors each multiplied by a scalar and summed.
Linear map:
Little group (see stabilizer)
Local actions
Local hidden variable theory (see also hidden variable theory):
Logical bit
Matrix exponential
Matrix properties
Matrix transformation
Measurement
Minimum distance
Modular arithmetic: When a number is divided into another and does not go evenly, there is left a remainder. Modular arithmetic takes the information about what number was used to divide and what remainder is left to calculate how it will interact with another number. For example, 13 can go into 5 twice with remainder 3, so its representation is 3mod 5, (pronounced "three modulo 5) which it has in common with any number satisfying 3+5x where x is an integer. This usage of modulo has nothing to do with the physics usage of modulus.
Modulus
n,k,d code (see [n,k,d] code)
No cloning theorem: There is no universal copying machine. See Section 5.2.
Noise
Non-degenerate code
Normalizer:
Normalization: A process of scaling some set of numbers or functions in order that an operation including them returns a desired value. For instance the set of all possible probabilities is usually scaled or normalized so they sum to one.
One-to-one: A mapping where each domain element is mapped to exactly one range element, and each range element is mapped from one domain element.
Onto: A mapping where each domain element mapped to at most one range element.
Open system
Operator
Operator-sum representation (see SMR representation)
Order of a group
Ordered basis
Orthogonal: Two vectors are orthogonal when their dot product is zero.
Outer product
P gate (not the phase gate):
Parity
Parity check (see inner product)
Parity check matrix
Partial trace
Partition of a group
Pauli group
Pauli matrices: The X,Y,Z gates.
Permutation:
Phase flip error
Phase gate: See Z gate
Planck's constant:
Polarization
Positive definite and semidefinite matrix: A positive definite matrix is one whose eigenvalues are all greater than zero. A positive semidefinite matrix has no negative eigenvalues.
Probability for existing in a state:
Projector: A transformation such that .
Projection postulate
Pure state
QKD: See quantum key distribution
Quantum bit: See Qubit
Quantum cryptography
Quantum dense coding
Quantum gate: A unitary transformation applied to one or more qubits.
Quantum hamming bound
Quantum key distribution:
Quantum NOT gate: see X gate, but be careful, the NOT gate is only defined for qubits.
Qubit: A Qubit is represented by two states of a quantum mechanical system. (1.3)
Rank
Rate of a code
Reduced density operator
Representation space
Reversible quantum operation: An operation is reversible if for every state on which the operator can act, there exists an operation which restores the state to its original.
RSA encryption
Schmidt decomposition
Schrodinger's Equation
Set: Any mathematical construct.
Shor's algorithm
Shor's nine-bit quantum error correcting code
Similarity transformation
Singular values
Singular value decomposition
SMR representation
Special unitary matrix
Spin
Spooky action at a distance
Stabilizers of a group
Stabilizer code
Standard deviation
Stationary subgroup (see stabilizer)
Stirling's formula
Subgroup
Superposition: A qubit state in superposition, may be written as where and are complex numbers.
Syndrome measurement
Taylor expansion
Teleportation
Tensor product
Trace: The sum of the diagonal elements of a matrix.
Transpose
Trivial representation
Turing machine
Uncertainty principle
Unitary matrix
Unitary transformation: A transformation which leaves the magnitude of any object it transforms the same.
Universal quantum computing
Universal set of gates (universality) (2.6)
Variance
Vector: A directed quantity.
Vector space
Weight of a vector (see Hamming weight)
Weight of an operator: The number of non-identity elements in the tensor product.
Wigner-Clebsch-Gordon Coefficients
X gate (2.3.2)
Y gate
Z gate, or phase-flip gate (2.3.2)