Notation

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Symbol Definition
Hilbert Space
The set of complex numbers
The set of real numbers
Chapter 2 - Qubits and Collections of Qubits
The Hadamard gate (see Section 2.3.2, Section 5.4, Eq. 2.16, and Eq. 5.10)
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The Pauli Y matrix (see Table 2.1)
The Pauli Z matrix (see Table 2.1)
Identity operator
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Epsilon (see Equation C.8)
The Tensor Product (see Section C.7)
Chapter 3 - Physics of Quantum Information
The Hamiltonian (see Eqs. 3.1 - 3.4)
H-bar (Planck's constant divided by )
The Unitary Matrix (see Eqs. 3.5 - 3.6)
The Density Matrix or Density Operator (see Appendix E - Density Operator: Extensions)
The trace of a matrix (see Section C.3.5)
The determinant of a matrix (see Section C.3.6)
A unit vector (see Section C.5.1)
Eigenvalues (see Section C.6)
The expectation value of an operator (see Eqs. 3.47 - 3.48)
Chapter 4 - Entanglement
A possible hidden variable (see Eqs. 4.4 - 4.9)
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Local transformations (see Eq. 4.12)
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Bell States (see Eq. 4.14)
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Chapter 5 - Quantum Information
The variance of an observable (see Eq. 5.4)
The Hadamard gate (see Section 2.3.2, Section 5.4, Eq. 2.16, and Eq. 5.10)
,
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Chapter 6 - Noise in Quantum Systems
, Linear mapping vectors (see Eqs. 6.1 - 6.14)
The mapping matrix (see Eqs. 6.6 - 6.12)
The Hamiltonian for the system alone (see Eq. 6.15)
The Hamiltonian for the bath alone (see Eq. 6.15)
Operator on the system (see Eq. 6.15)
Operator on the bath (see Eq. 6.15)
The initial density matrix of the (open) system (see Eq. 6.16)
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Chapter 7 - Quantum Error Correcting Codes
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The binomial coefficient (see Eq. 7.17)
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Classical parity check matrix (see Eq. 7.21)
The generator matrix (see Eq. 7.22)
Chapter 8 - Decoherence-Free/Noiseless Subsystems
Hamiltonian acting only on the system (see Eq. 8.1)
Hamiltonian acting only on the bath (see Eq. 8.1)
The interaction Hamilton (see Eqs. 8.1 and 8.2)
Denotes the "error algebra" generated by the set
Set of error operators acting only on the system (see Eq. 8.2)
Acts only on the bath (see Eq. 8.2)
A particular unitary transformation
Collective phase error Hamiltonian (see Eq. 8.3)
A phase operator which acts on the th qubit (see Eq. 8.3)
, , The three collective errors (see Eq. 8.9)
Unitary transformation corresponding to the collection of Wigner-Clebsch-Gordan coefficients
The orthogonal subspace (to the code) (see Eq. 8.17)
An encoded state
Basis for the noise operators
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The Hamiltonian
A complete set of Hermitian matrices in terms of which any Hermitian matrix can be expanded
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Arbitrary coefficients
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