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Frequency doubled tunable diode laser for excitation of Rydberg states in Rb atoms

机译:频率加倍可调谐二极管激光器,用于rydberg状态在RB原子中的激励

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Nowadays tunable diode laser become main tool for high resolution atomic spectroscopy. The use of frequency doubled lasers extends available wavelength ranges from green to vacuum ultraviolet small linewidth (from 10kHz to tens of MHz) radiation tunable across range from tens to hundreds of nm. It makes possible application of single mode laser diodes in certain specific fields one of them - pumping and high resolution spectroscopy of highly excited long-lived atomic states and selective photo ionization of atoms. Recently studies of highly exited -^s"Rydberg atoms" have obtained second wind in the experiments with laser cooled atoms [1]. It has been pointed out that cold Rydberg atom are most likely candidate as logic gate for quantum computing modeling [2]. Such experiments build up new requirements to the lasers radiation. Because of relatively thin absorption lines of cold atoms the laser should have small linewidth. Furthermore laser radiation should be continuously tunable in certain wavelength range, while laser frequency is stable and have relatively high power of several mW of UV or blue radiation. The one of possible atoms for quantum computation are laser cooled Rb atoms having as alkali atoms simple atomic levels structure and relatively large atomic mass in comparison to lithium, sodium, and potassium, and therefore lower temperatures. There are several ways to excite Rb atoms into Rydberg states. One mostly possible is based on use cascade transition 5S{sub}(1/2)→5P{sub}(3/2)→n(S,D) using two lasers radiation. First pumping cycle is made by using external cavity laser diode working at 780 nm. Second cycle should be made using laser tunable between 479-481 nm. In the selected wavelength range it was possible use frequency doubled Ti:Sa and Dye-lasers, having certain disadvantages related to pumping lasers. Semiconductor lasers are devoid of such disadvantages. Unfortunately up to present day there were no laser diodes available for mentioned above spectral range. Possibly the GaN based laser diodes will extend lasing emission band to this range in nearest future, but in a current work we found only one way for solution. It was based on conventional frequency doubling technique of near infrared laser diode using nonlinear crystal inside a ring cavity [3].
机译:如今调谐二极管激光器成为高分辨率原子光谱主要工具。使用倍频激光器的从绿色延伸可用波长范围真空紫外线小线宽(从10kHz至几十MHz)跨越范围内的辐射可调谐从几十到几百纳米。这使得在某些特定领域它们中的一个单模式激光二极管的可能的应用 - 泵送和高度激发的长寿命原子态和原子的选择性光离子化的高分辨光谱。最近高度退出研究 - ^的“里德伯原子”与激光冷却原子[1]取得第二风在实验。已经指出,冷里德伯原子是最有可能的候选作为逻辑门,用于量子计算建模[2]。这样的实验建立新的要求,以激光辐射。因为冷原子的相对薄的吸收线的激光应当具有小的线宽。此外激光辐射应在一定的波长范围内连续可调,而激光频率是稳定的,并且具有UV或蓝色辐射的几个毫瓦的相对高的功率。用于量子计算可能的原子的一个是激光冷却具有如碱原子简单的原子水平的结构和相对大的原子质量相比于锂,钠,和钾,和因此较低的温度RB原子。有几种方法与Rb原子激发到里德堡态。一个可能的大多是基于使用级联过渡5S {子}(1/2)→5P {子}(3/2)→N使用两个激光器辐射(S,d)。第一泵送循环利用外空腔的激光二极管工作在780nm处取得。第二周期应该使用479-481纳米之间的可调谐激光进行。在所选择的波长范围内它可能使用倍频的Ti:Sa和染料激光器,具有与泵送激光器某些缺点。半导体激光器是没有这样的缺点。不幸的是高达至今没有可用于以上的光谱范围内提到的激光二极管。可能基于GaN激光二极管会延长激光发射带于该范围在最近的将来,但在目前的工作我们发现只有一种溶液的方法。使用环形空腔[3]内的非线性晶体它是基于近红外激光二极管的常规倍频技术。

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