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Copy file name to clipboardExpand all lines: src/correlations.jl
+2-2Lines changed: 2 additions & 2 deletions
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C::QuantumObject;
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kwargs...)
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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``.
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Returns the two-time 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``.
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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)).
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"""
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reverse::Bool=false,
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kwargs...)
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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``.
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Returns the two-time 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``.
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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)).
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