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The recording grating is defined also by a weak probe beam from a continuous semiconductor laser (λ = 405 nm, the power is I 0 = 50 mW).
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The DNA-QD system is driven by a strong pump field and a weak probe field.
Except for that, the spatial beam multiplexing may be carried out by means of the diffraction of a weak probe beam on a stable phase grating.
By applying a strong pump laser and a weak probe laser to the QD simultaneously, one could probe the MFs via optical pump-probe technique [30, 31].
It is known that the absorption and the dispersion properties of a weak probe field can be modified effectively by atomic coherence and quantum interference [1 5].
The emerging two parallel beams with a diameter of approximately 3 mm, a strong pump and a weak probe, are focused on the same area on the sample surface by a convex lens of 50 mm focal length.
The optical pump-probe technology includes a strong pump laser and a weak probe laser [54], which provides an effective way to investigate the light-matter interaction.
The nearby MF is coupled to a semiconductor QD embedded in a nanomechanical resonator under a strong pump laser and a weak probe laser simultaneously.
Since photodetection technology is well developed, for instance with the assistance from quantum dot [14], we can expect to observe some properties of DNA molecules by detecting the weak probe beam.
The susceptibility of the compact double QWs to the weak probe field is determined by coherence term ρ 01 chi =frac{2Nwp }{E{varepsilon}_0}{rho}_{01}, (7).
Genes of this group (12 probe sets representing 9 genes) are closely related to the previous group and are characterized by a weak TNF-α inducibility.
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