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Laser spectroscopy with nanometric cells containing atomic vapor of metal: influence of buffer gas

机译:包含金属原子蒸气的纳米池的激光光谱:缓冲气体的影响

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Comparison of absorption and fluorescence in a nano-cell containing Rb vapor with other Rb nano-cells with addition of neon gas is presented. It is shown that the effect of collapse and revival of Dicke-type narrowing occurs for Rb nano-cells containing N_2 as buffer gas under 6 and 20 Torr pressure for the thickness L = λ/2 and L = λ, where λ is the resonant laser wavelength 794 nm (D_1 line). Particularly for 6 Torr the line-width of the transmission spectrum for the thickness L = λ/2 is 2 times narrower than that for L = λ. For an ordinary Rb cell with L = 0.1 - 10 cm with addition of buffer gas, the velocity selective optical pumping/saturation (VSOP) resonances in saturated absorption spectra are fully suppressed when the buffer gas pressure > 0.5 Torr. A spectacular difference is that for L = λ, VSOP resonances located at the atomic transitions are still observable even when Ne pressure is > 6 Torr. Narrowband fluorescence spectra of a nano-cell with L = λ/2 can be used as a convenient tool for online buffer gas pressure monitoring for the conditions when ordinary pressure gauges are unusable. Comparison of electromagnetically induced transparency (EIT) effect in a nano-cell filled with pure (without a buffer gas) Rb with another nano-cell, where buffer gas nitrogen is added, is presented. The use of N_2 gas inside Rb nano-cells strongly extends the range of coupling laser detunings in which it is still possible to form EIT resonance.
机译:提出了在包含Rb蒸气的纳米电池中,与其他添加了氖气的Rb纳米电池相比,其吸收和荧光的比较。结果表明,在厚度为L =λ/ 2和L =λ的情况下,在6和20 Torr压力下,含有N_2作为缓冲气体的Rb纳米电池发生了Dicke型变窄的塌陷和恢复,其中λ为共振激光波长794 nm(D_1线)。特别是对于6 Torr,厚度L =λ/ 2时透射光谱的线宽比L =λ时窄2倍。对于添加缓冲气体的L = 0.1-10 cm的普通Rb电池,当缓冲气体压力> 0.5 Torr时,饱和吸收光谱中的速度选择光泵浦/饱和(VSOP)共振将被完全抑制。一个显着的差异是,对于L =λ,即使Ne压力> 6 Torr,仍然可以观察到位于原子跃迁处的VSOP共振。 L =λ/ 2的纳米单元的窄带荧光光谱可以用作在线缓冲气体压力监测的便捷工具,以监测普通压力表无法使用的情况。呈现了在填充有纯(无缓冲气体)Rb的纳米电池中,与另一种添加了缓冲气体氮气的纳米电池中的电磁感应透明度(EIT)效果的比较。 Rb纳米单元内部使用N_2气体极大地扩展了耦合激光失谐的范围,在该范围内仍可能形成EIT共振。

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