Show that this dephasing operation is Markovian

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In summary, the dephasing operation is Markovian when ##E_gE_h = E_{g+h}## and can be simplified using hyperbolic trigonometric functions. The composition of the functions can be expressed as ##E_gE_h = \frac{1+e^{-g}}{2}\frac{1+e^{-h}}{2} \rho^2 + \frac{1-e^{-g}}{2}\frac{1-e^{-h}}{2}Z\rho ZZ\rho Z + \frac{1+e^{-g}}{2}\frac{1-e^{-h}}{2} = \rho Z \rho Z + \frac{1+e^{-g}}
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Show that this dephasing operation is Markovian
$$E_t(\rho)=\left(\frac{1+e^{-t}}{2}\right)\rho + \left(\frac{1-e^{-t}}{2}\right)Z\rho Z$$

The operation is supposed to be Markovian when
$$E_g E_h = E_{g+h}$$

So this is what I get when I apply this multiplication
$$
E_g E_h=\frac{1+e^{-g}}{2}\frac{1+e^{-h}}{2} \rho^2 + \frac{1-e^{-g}}{2} \frac{1-e^{h}}{2}Z\rho ZZ\rho Z + \frac{1+e^{-g}}{2} \frac{1-e^{-h}}{2} = \rho Z \rho Z + \frac{1+e^{-g}}{2} \frac{1-e^{-h}}{2} Z \rho Z \rho
$$
We can lose ZZ because
$$ZZ=I$$
but I can't see what else can be done. ρ after all only commutes with Z if it's diagonal but we can't assume that for ρ in general?
 
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  • #2
You have misunderstood the question. ##E_gE_h## means the composition of those functions.
The algebra might be a bit simpler using hyperbolic trig - if you know the formulae for ##\cosh(x+y)## etc.
 
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FAQ: Show that this dephasing operation is Markovian

What is a dephasing operation in quantum mechanics?

A dephasing operation in quantum mechanics refers to a process that causes a loss of coherence between the quantum states of a system. This typically affects the off-diagonal elements of the system's density matrix, reducing them over time while leaving the diagonal elements (the populations) unchanged. The result is a transition from a pure state to a mixed state, effectively introducing classical noise into the quantum system.

What does it mean for a dephasing operation to be Markovian?

A dephasing operation is considered Markovian if the process lacks memory effects, meaning the future evolution of the system's state depends only on its present state and not on its past history. In mathematical terms, this is often described by a Lindblad master equation, which provides a time-local description of the system's dynamics.

How can you mathematically show that a dephasing operation is Markovian?

To show that a dephasing operation is Markovian, one typically demonstrates that the system's dynamics can be described by a Lindblad master equation. This involves expressing the time evolution of the density matrix in the form \( \frac{d\rho(t)}{dt} = \mathcal{L}[\rho(t)] \), where \( \mathcal{L} \) is the Lindblad superoperator. For dephasing, this often takes the form \( \mathcal{L}[\rho] = \gamma (L\rho L^\dagger - \frac{1}{2}\{L^\dagger L, \rho\}) \), where \( \gamma \) is the dephasing rate and \( L \) is the Lindblad operator.

What are some common examples of Markovian dephasing processes?

Common examples of Markovian dephasing processes include phase damping in qubits, where the coherence between the |0⟩ and |1⟩ states is lost over time, and optical dephasing in atoms or molecules interacting with a fluctuating electromagnetic field. These processes can typically be modeled using a Lindblad master equation with appropriate dephasing terms.

What are the implications of a dephasing operation being Markovian for quantum computing and information?

If a dephasing operation is Markovian, it simplifies the analysis and control of quantum systems, as the lack of memory effects allows for straightforward predictions of system behavior. This is beneficial in quantum computing and information, where understanding and mitigating decoherence is crucial for maintaining quantum coherence and achieving reliable quantum operations. Markovian dephasing models enable the design of error correction schemes and noise-resilient quantum algorithms.

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