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I am wondering about the exact approach to use the energy dissipation form of the Spin-Boson model, as described in the tutorial, for both time-dependent and time-independent forms. Specifically, in the interaction Hamiltonian, instead of considering the system operator as ( \sigma_z ), I want to use the raising and lowering operators ( \sigma_+ ) and ( \sigma_- ), such that:
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I am wondering about the exact approach to use the energy dissipation form of the Spin-Boson model, as described in the tutorial, for both time-dependent and time-independent forms. Specifically, in the interaction Hamiltonian, instead of considering the system operator as ( \sigma_z ), I want to use the raising and lowering operators ( \sigma_+ ) and ( \sigma_- ), such that:
[
H_{I} = \frac{1}{2}\sum_{k}g_{k}(\sigma_{-}a^{\dag} + \text{hc})
]
Can I write the code like this?
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