Abstract
In this chapter, we describe a unified quantum mechanical description for the generation and detection of coherent optical phonons using a simple model. Two electronic states coupled with displaced harmonic oscillators, which represent phonons, are used. The dipole interaction between an optical pulse and the system is assumed and treated as a perturbation interaction. Time evolution of the density operator is calculated using the second-order perturbation approximation.
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Notes
- 1.
- 2.
\(\alpha ^2\) is the Huang–Rhys factor, which is considered to be small (\(\alpha ^2 <1 \)) in a bulk solid.
- 3.
When we set \(\hat{B} = |e\rangle \langle e|\), the exponential \(\exp (\hat{H}_e \hat{B} t)\) is expressed by \(\exp (\hat{H}_e \hat{B} t) = \sum _n (\hat{A} t)^n \hat{B}^n\). Since \(\hat{B}^2 = (|e\rangle \langle e|)(|e\rangle \langle e|)= |e\rangle \langle e| = \hat{B}\), then \(\hat{B}^n = \hat{B} \) for \(n \ge 1\). Finally, we get \(\exp (\hat{H}_e |e\rangle \langle e| t) |e\rangle \langle g| = \exp (\hat{H}_e t) |e\rangle \langle g|\).
- 4.
The harmonic potential can be deformed under a long-range external field such as the surface-charge field. Supposing a uniform electric field (\(F(x)=-\mathrm{d}x\)) acting along the phonon coordinate (x), the effective charge field can be treated as uniform in such a short scale. When the external field potential is applied to a harmonic potential \(U(x)= kx^2/2\), the potential changes to \(U'(x)=U(x)+F(x) = k(x-\mathrm{d}/k)^2/2 -\mathrm{d}^2/(2k)\). Then, the potential minimum position and energy shift are \(\mathrm{d}/k\) and \(-\mathrm{d}^2/(2k)\), respectively. The slope d of the external fields in the electronic excited state is lower than that in the ground state, because the surface screening is suppressed by a electron–hole pair or electronic polarization. Then, the effective harmonic potential in the excited state is displaced from that in the ground state.
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Nakamura, K. (2019). Coherent Phonons: Quantum Theory. In: Quantum Phononics. Springer Tracts in Modern Physics, vol 282. Springer, Cham. https://doi.org/10.1007/978-3-030-11924-9_6
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DOI: https://doi.org/10.1007/978-3-030-11924-9_6
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