Hurst Noah, Harilal S S
Hyperion Scientific, Inc., 455 Science Dr., Madison, Wisconsin 53711, USA.
Rev Sci Instrum. 2009 Mar;80(3):035101. doi: 10.1063/1.3079698.
The pulse from a transversely excited atmospheric CO(2) laser consists of a sharp spike followed by a long, drawn out tail region spanning about 2-5 micros caused by the nitrogen gas in the laser cavity. The nitrogen tail is undesirable in many applications because it decreases the average power of the laser pulse. We employ a pinhole plasma shutter for eliminating the nitrogen tail and shortening the pulse width. The pinhole shutter optically triggers plasma at a certain point in time with respect to the temporal profile of the laser pulse. This way, a good portion of the sharp spike is transmitted, while the energy stored in the nitrogen tail is consumed in heating the plasma. This simplistic plasma shutter is easy to build and inexpensive compared to other existing plasma shutter designs.
横向激励大气压二氧化碳激光器发出的脉冲由一个尖锐的尖峰以及随后一个长长的拖尾区域组成,拖尾区域持续约2至5微秒,是由激光腔内的氮气造成的。在许多应用中,氮气拖尾是不理想的,因为它会降低激光脉冲的平均功率。我们采用针孔等离子体快门来消除氮气拖尾并缩短脉冲宽度。针孔快门在相对于激光脉冲时间轮廓的特定时刻光学触发等离子体。通过这种方式,大部分尖锐尖峰被传输,而氮气拖尾中存储的能量则消耗于加热等离子体。与其他现有的等离子体快门设计相比,这种简单的等离子体快门易于构建且成本低廉。