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21 | 21 |
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22 | 22 | Returns the two-times correlation function of three operators ``\hat{A}``, ``\hat{B}`` and ``\hat{C}``: ``\left\langle \hat{A}(t) \hat{B}(t + \tau) \hat{C}(t) \right\rangle`` for a given initial state ``|\psi_0\rangle``. |
23 | 23 |
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24 | | -If the initial state `ψ0` is given as `nothing`, then the [`steadystate`] will be used as the initial state. Note that this is only implemented if `H` is constant ([`QuantumObject`](@ref)). |
| 24 | +If the initial state `ψ0` is given as `nothing`, then the [`steadystate`](@ref) will be used as the initial state. Note that this is only implemented if `H` is constant ([`QuantumObject`](@ref)). |
25 | 25 | """ |
26 | 26 | function correlation_3op_2t( |
27 | 27 | H::AbstractQuantumObject{DataType,HOpType}, |
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74 | 74 |
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75 | 75 | Returns the one-time correlation function of three operators ``\hat{A}``, ``\hat{B}`` and ``\hat{C}``: ``\left\langle \hat{A}(0) \hat{B}(\tau) \hat{C}(0) \right\rangle`` for a given initial state ``|\psi_0\rangle``. |
76 | 76 |
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77 | | -If the initial state `ψ0` is given as `nothing`, then the [`steadystate`] will be used as the initial state. Note that this is only implemented if `H` is constant ([`QuantumObject`](@ref)). |
| 77 | +If the initial state `ψ0` is given as `nothing`, then the [`steadystate`](@ref) will be used as the initial state. Note that this is only implemented if `H` is constant ([`QuantumObject`](@ref)). |
78 | 78 | """ |
79 | 79 | function correlation_3op_1t( |
80 | 80 | H::AbstractQuantumObject{DataType,HOpType}, |
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112 | 112 |
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113 | 113 | Returns the two-times correlation function of two operators ``\hat{A}`` and ``\hat{B}`` : ``\left\langle \hat{A}(t + \tau) \hat{B}(t) \right\rangle`` for a given initial state ``|\psi_0\rangle``. |
114 | 114 |
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115 | | -If the initial state `ψ0` is given as `nothing`, then the [`steadystate`] will be used as the initial state. Note that this is only implemented if `H` is constant ([`QuantumObject`](@ref)). |
| 115 | +If the initial state `ψ0` is given as `nothing`, then the [`steadystate`](@ref) will be used as the initial state. Note that this is only implemented if `H` is constant ([`QuantumObject`](@ref)). |
116 | 116 |
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117 | 117 | When `reverse=true`, the correlation function is calculated as ``\left\langle \hat{A}(t) \hat{B}(t + \tau) \right\rangle``. |
118 | 118 | """ |
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156 | 156 |
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157 | 157 | Returns the one-time correlation function of two operators ``\hat{A}`` and ``\hat{B}`` : ``\left\langle \hat{A}(\tau) \hat{B}(0) \right\rangle`` for a given initial state ``|\psi_0\rangle``. |
158 | 158 |
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159 | | -If the initial state `ψ0` is given as `nothing`, then the [`steadystate`] will be used as the initial state. Note that this is only implemented if `H` is constant ([`QuantumObject`](@ref)). |
| 159 | +If the initial state `ψ0` is given as `nothing`, then the [`steadystate`](@ref) will be used as the initial state. Note that this is only implemented if `H` is constant ([`QuantumObject`](@ref)). |
160 | 160 |
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161 | 161 | When `reverse=true`, the correlation function is calculated as ``\left\langle \hat{A}(0) \hat{B}(\tau) \right\rangle``. |
162 | 162 | """ |
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