{"title":"Tuning a terahertz wire laser","authors":"Q. Hu","doi":"10.1109/PHOTWTM.2010.5421991","DOIUrl":null,"url":null,"abstract":"Lasers that can be continuously tuned over a broad wavelength range are essential components for sensing and spectroscopy. The frequency of a conventional tunable laser is changed similarly to a musical instrument such as the violin, whose pitch is varied by changing the length (the longitudinal component of wave vector) and the tension (the refractive index) of a string. However, such a method is difficult to implement at terahertz (THz) frequencies, where many important bio-chemical species have distinctive spectral fingerprints, because of the relatively long wavelength λ compared to the cross section w of semiconductor lasers. Continuous frequency tuning using an external-cavity grating has yet to be achieved, and changing the refractive index by temperature produces only small fractional tuning (<1%). Here we demonstrate a novel tuning mechanism that qualitatively differs from all the other methods. This mechanism is based on the unique feature of an unusual device termed “wire laser”, which is defined as a laser whose dimension in the transverse direction w is much smaller than λ. As such, a large fraction of the mode propagates outside the solid core. Placing a movable object close to the wire laser allows direct manipulation of the evanescent laser field, and consequently the lasing frequency. Based on this mechanism, continuous frequency tuning has been unambiguously demonstrated with single-mode operation free from mode hopping. Both red-shift and blue-shift tuning can be achieved from the same device by using either a dielectric or metallic movable object. In combination, a total tuning of ~137 GHz (3.6%) has been demonstrated from a single laser device at ~3.8 THz. Furthermore, these results demonstrate a mechanism for tuning wire lasers at all wavelengths.","PeriodicalId":367324,"journal":{"name":"2010 IEEE Photonics Society Winter Topicals Meeting Series (WTM)","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2009-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"134","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2010 IEEE Photonics Society Winter Topicals Meeting Series (WTM)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PHOTWTM.2010.5421991","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 134

Abstract

Lasers that can be continuously tuned over a broad wavelength range are essential components for sensing and spectroscopy. The frequency of a conventional tunable laser is changed similarly to a musical instrument such as the violin, whose pitch is varied by changing the length (the longitudinal component of wave vector) and the tension (the refractive index) of a string. However, such a method is difficult to implement at terahertz (THz) frequencies, where many important bio-chemical species have distinctive spectral fingerprints, because of the relatively long wavelength λ compared to the cross section w of semiconductor lasers. Continuous frequency tuning using an external-cavity grating has yet to be achieved, and changing the refractive index by temperature produces only small fractional tuning (<1%). Here we demonstrate a novel tuning mechanism that qualitatively differs from all the other methods. This mechanism is based on the unique feature of an unusual device termed “wire laser”, which is defined as a laser whose dimension in the transverse direction w is much smaller than λ. As such, a large fraction of the mode propagates outside the solid core. Placing a movable object close to the wire laser allows direct manipulation of the evanescent laser field, and consequently the lasing frequency. Based on this mechanism, continuous frequency tuning has been unambiguously demonstrated with single-mode operation free from mode hopping. Both red-shift and blue-shift tuning can be achieved from the same device by using either a dielectric or metallic movable object. In combination, a total tuning of ~137 GHz (3.6%) has been demonstrated from a single laser device at ~3.8 THz. Furthermore, these results demonstrate a mechanism for tuning wire lasers at all wavelengths.
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调谐太赫兹线激光器
可以在宽波长范围内连续调谐的激光器是传感和光谱学的重要组成部分。传统可调谐激光的频率变化类似于小提琴等乐器,其音高是通过改变弦的长度(波矢量的纵向分量)和张力(折射率)来改变的。然而,这种方法很难在太赫兹(THz)频率下实现,因为与半导体激光器的横截面w相比,波长λ相对较长,因此许多重要的生物化学物质具有独特的光谱指纹。使用外腔光栅的连续频率调谐尚未实现,并且通过温度改变折射率仅产生很小的分数调谐(<1%)。在这里,我们展示了一种新的调谐机制,它在质量上不同于所有其他方法。这种机制是基于一种被称为“线激光器”的不寻常装置的独特特征,它被定义为在横向方向上的尺寸w比λ小得多的激光器。因此,很大一部分模态在固体核外传播。将一个可移动的物体靠近线激光器,可以直接操纵倏逝的激光场,从而控制激光频率。基于这一机制,连续频率调谐已经明确地证明了单模操作无模式跳变。红移和蓝移调谐都可以通过使用电介质或金属可移动物体来实现。最后,在3.8太赫兹的单激光器件上实现了~137 GHz(3.6%)的总调谐。此外,这些结果证明了在所有波长下调谐线激光器的机制。
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