{"title":"Sixty years of nonlinear optics","authors":"S. Grechin, A. Savel’ev","doi":"10.1070/QEL18010","DOIUrl":null,"url":null,"abstract":"Apparently, the concept of ‘nonlinear optics’ was first introduced by S.I. Vavilov when analysing the results of absorption saturation in uranium glasses obtained in 1926. In particular, he noted that “In an absorbing medium ‘nonlinearity’ should be observed not only in relation to absorption. The latter is related to dispersion, so the speed of light propagation in a medium, generally speaking, must also depend on the light power”. One of the defining criteria for nonlinear optics, according to S.I. Vavilov, is the violation of the superposition principle. Sixteen years later, in 1942, E. SchrÖdinger, considering the problem of light scattering by electrons, also defined the processes as nonlinearly optical. Nonlinear optics, as an independent branch of physics, dates back to the work by Franken et al. in 1961, when the generation of the second harmonic of ruby laser radiation was obtained at an extremely low efficiency (~10–12) in terms of the number of photons: only 106 second harmonic photons. But already in 1962, second harmonic generation was realised in the phase-matched regime with a conversion efficiency that was several orders of magnitude higher. Then, literally within a few years, it was possible to obtain effective generation of the third and fourth harmonics and of the sum frequency, to implement parametric amplification and generation, and to observe stimulated Raman scattering, two-photon absorption, and other nonlinear effects. The works of Pockels, Kerr, Faraday and others, performed back in the 19th century, turned out to be the basis for understanding the essence of the effects observed, and research on nonlinear optics itself became a logical continuation of work on radiophysics, nonlinear electrodynamics of the microwave range, optics, hydrodynamics and acoustics, the theory of oscillations, etc. As with many other branches of physics, it is difficult to give an exact definition of nonlinear optics by specifying its boundaries. In 1965 one of the founders of nonlinear optics, R.V. Khokhlov, divided nonlinear wave processes into two groups: dispersive and nondispersive, in each of which these effects are possible in reactive and absorbing media. Such a definition does not raise the question that nonlinear optical processes are possible only under high-intensity irradiation, which is not infrequently done even today. R. Boyd adheres to the same approach in his 2020 monograph, with clarification for parametric and nonparametric processes in dispersive media. It is difficult to say to what extent the existing definitions correspond to the problems of nonlinear optics of tomorrow, but even now the rapid development of quantum nonlinear optics clearly indicates the importance of nonlinear optical processes occurring with single quanta, i.e., in the regime of extremely low intensities. Research in the field of nonlinear optics is carried out by many teams of scientists around the world. An invaluable contribution to the formation and development of the theory of nonlinear wave processes was made by N. Blombergen, D.A. Kleinman, J.A. Armstrong, R. Byer, J. Ducuing, P.S. Pershan, and many others. In the USSR, the scientific school formed back in the late 1950s under the leadership of R.V. Khokhlov and S.A. Akhmanov largely determined the development of nonlinear optics in our country. One of the key tasks of nonlinear optics is the frequency conversion of laser radiation, which significantly expands the functionality of lasers. This made it possible to ensure the efficient generation of radiation in a wide range of wavelengths: from soft X-rays (due to the generation of high harmonics) to millimetre and terahertz (due to optical rectification) radiation with pulse durations down to a few femtoseconds in the optical range, and an order of magnitude shorter attosecond pulses in the X-ray range and with a peak power of several PW. The fields of application of lasers with frequency conversion are very wide. These are spectroscopy, environmental monitoring, diagnostics, medicine, various types of material processing, information and telecommunication systems, including the problems of quantum optics and quantum computing, etc. Significant progress is being observed in the study of fast-flowing processes, within the framework of qualitatively new analysis capabilities, the search for “lost time”. Nevertheless, there are still many unsolved fundamental problems in nonlinear optics, a significant part of which is associated with the development of laser and nonlinear optical technologies. These, in particular, include theoretical and experimental studies of problems at the junction with modern quantum electrodynamics: polarisation and nonlinearity of vacuum and its breakdown under the action of laser radiation of extreme intensity. Works on nonlinear optics have always been among the most important and actual topics of the Quantum Electronics journal. The papers presented in this issue by no means reflect all the scientific areas of modern nonlinear optics, in which numerous scientific groups are actively working in Russia. We would like to express our deep gratitude to the authors of all papers who sent their work for publication. However, since the number of papers on this topic received by the journal exceeded the total volume of possible publications in one issue, some of the papers will be published in the next issue. Sixty years of nonlinear optics","PeriodicalId":20775,"journal":{"name":"Quantum Electronics","volume":"9 1","pages":"207 - 207"},"PeriodicalIF":0.9000,"publicationDate":"2022-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Quantum Electronics","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.1070/QEL18010","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"Engineering","Score":null,"Total":0}
引用次数: 0
Abstract
Apparently, the concept of ‘nonlinear optics’ was first introduced by S.I. Vavilov when analysing the results of absorption saturation in uranium glasses obtained in 1926. In particular, he noted that “In an absorbing medium ‘nonlinearity’ should be observed not only in relation to absorption. The latter is related to dispersion, so the speed of light propagation in a medium, generally speaking, must also depend on the light power”. One of the defining criteria for nonlinear optics, according to S.I. Vavilov, is the violation of the superposition principle. Sixteen years later, in 1942, E. SchrÖdinger, considering the problem of light scattering by electrons, also defined the processes as nonlinearly optical. Nonlinear optics, as an independent branch of physics, dates back to the work by Franken et al. in 1961, when the generation of the second harmonic of ruby laser radiation was obtained at an extremely low efficiency (~10–12) in terms of the number of photons: only 106 second harmonic photons. But already in 1962, second harmonic generation was realised in the phase-matched regime with a conversion efficiency that was several orders of magnitude higher. Then, literally within a few years, it was possible to obtain effective generation of the third and fourth harmonics and of the sum frequency, to implement parametric amplification and generation, and to observe stimulated Raman scattering, two-photon absorption, and other nonlinear effects. The works of Pockels, Kerr, Faraday and others, performed back in the 19th century, turned out to be the basis for understanding the essence of the effects observed, and research on nonlinear optics itself became a logical continuation of work on radiophysics, nonlinear electrodynamics of the microwave range, optics, hydrodynamics and acoustics, the theory of oscillations, etc. As with many other branches of physics, it is difficult to give an exact definition of nonlinear optics by specifying its boundaries. In 1965 one of the founders of nonlinear optics, R.V. Khokhlov, divided nonlinear wave processes into two groups: dispersive and nondispersive, in each of which these effects are possible in reactive and absorbing media. Such a definition does not raise the question that nonlinear optical processes are possible only under high-intensity irradiation, which is not infrequently done even today. R. Boyd adheres to the same approach in his 2020 monograph, with clarification for parametric and nonparametric processes in dispersive media. It is difficult to say to what extent the existing definitions correspond to the problems of nonlinear optics of tomorrow, but even now the rapid development of quantum nonlinear optics clearly indicates the importance of nonlinear optical processes occurring with single quanta, i.e., in the regime of extremely low intensities. Research in the field of nonlinear optics is carried out by many teams of scientists around the world. An invaluable contribution to the formation and development of the theory of nonlinear wave processes was made by N. Blombergen, D.A. Kleinman, J.A. Armstrong, R. Byer, J. Ducuing, P.S. Pershan, and many others. In the USSR, the scientific school formed back in the late 1950s under the leadership of R.V. Khokhlov and S.A. Akhmanov largely determined the development of nonlinear optics in our country. One of the key tasks of nonlinear optics is the frequency conversion of laser radiation, which significantly expands the functionality of lasers. This made it possible to ensure the efficient generation of radiation in a wide range of wavelengths: from soft X-rays (due to the generation of high harmonics) to millimetre and terahertz (due to optical rectification) radiation with pulse durations down to a few femtoseconds in the optical range, and an order of magnitude shorter attosecond pulses in the X-ray range and with a peak power of several PW. The fields of application of lasers with frequency conversion are very wide. These are spectroscopy, environmental monitoring, diagnostics, medicine, various types of material processing, information and telecommunication systems, including the problems of quantum optics and quantum computing, etc. Significant progress is being observed in the study of fast-flowing processes, within the framework of qualitatively new analysis capabilities, the search for “lost time”. Nevertheless, there are still many unsolved fundamental problems in nonlinear optics, a significant part of which is associated with the development of laser and nonlinear optical technologies. These, in particular, include theoretical and experimental studies of problems at the junction with modern quantum electrodynamics: polarisation and nonlinearity of vacuum and its breakdown under the action of laser radiation of extreme intensity. Works on nonlinear optics have always been among the most important and actual topics of the Quantum Electronics journal. The papers presented in this issue by no means reflect all the scientific areas of modern nonlinear optics, in which numerous scientific groups are actively working in Russia. We would like to express our deep gratitude to the authors of all papers who sent their work for publication. However, since the number of papers on this topic received by the journal exceeded the total volume of possible publications in one issue, some of the papers will be published in the next issue. Sixty years of nonlinear optics
显然,“非线性光学”的概念是由S.I. Vavilov在分析1926年获得的铀玻璃的吸收饱和度结果时首先引入的。他特别指出,“在吸收介质中,‘非线性’不仅应该在吸收方面被观察到。后者与色散有关,因此光在介质中的传播速度,一般来说也必须取决于“光功率”。根据S.I.瓦维洛夫的说法,非线性光学的定义标准之一是违反叠加原理。16年后的1942年,E. SchrÖdinger考虑到电子散射光的问题,也将这一过程定义为非线性光学。非线性光学作为物理学的一个独立分支,可以追溯到1961年Franken等人的工作,当时以极低的效率(~ 10-12)获得了红宝石激光辐射的二次谐波的产生,就光子数量而言,只有106个二次谐波光子。但早在1962年,二次谐波产生就在相位匹配状态下实现了,转换效率提高了几个数量级。然后,在短短几年内,就有可能获得第三次和第四次谐波以及和频率的有效产生,实现参数放大和产生,并观察受激拉曼散射,双光子吸收和其他非线性效应。波克尔斯、克尔、法拉第等人早在19世纪就完成的工作,为理解所观察到的效应的本质奠定了基础,对非线性光学本身的研究成为辐射物理学、微波范围的非线性电动力学、光学、流体力学和声学、振荡理论等工作的合乎逻辑的延续。与物理学的许多其他分支一样,通过指定非线性光学的边界来给它一个精确的定义是很困难的。1965年,非线性光学的创始人之一R.V. Khokhlov将非线性波过程分为两组:色散和非色散,在每一组中,这些效应在反应介质和吸收介质中都是可能的。这样的定义并没有提出非线性光学过程只有在高强度照射下才可能发生的问题,即使在今天,这种情况也并不罕见。R. Boyd在他2020年的专著中坚持了同样的方法,澄清了分散介质中的参数和非参数过程。很难说现有的定义在多大程度上与未来的非线性光学问题相对应,但即使是现在,量子非线性光学的迅速发展也清楚地表明,单量子非线性光学过程的重要性,即在极低强度的情况下。非线性光学领域的研究是由世界各地的许多科学家团队进行的。非线性波动过程理论的形成和发展是由N. Blombergen, d . Kleinman, J. a . Armstrong, R. Byer, J. Ducuing, P.S. Pershan和许多其他人做出的宝贵贡献。在苏联,20世纪50年代末在R.V. Khokhlov和S.A. Akhmanov领导下形成的科学学派在很大程度上决定了我国非线性光学的发展。非线性光学的关键任务之一是激光辐射的频率转换,这大大扩展了激光器的功能。这使得确保在宽波长范围内有效产生辐射成为可能:从软x射线(由于产生高谐波)到毫米和太赫兹(由于光学精流)辐射,其脉冲持续时间在光学范围内降至几飞秒,在x射线范围内的脉冲时间缩短了一个数量级,峰值功率为几PW。变频激光器的应用领域非常广泛。这些是光谱学、环境监测、诊断、医学、各种类型的材料加工、信息和电信系统,包括量子光学和量子计算等问题。在新的定性分析能力框架内,在研究快速流动过程,寻找“失去的时间”方面取得了重大进展。然而,非线性光学仍有许多尚未解决的基本问题,其中很大一部分与激光和非线性光学技术的发展有关。这些,特别是,包括理论和实验研究的问题在现代量子电动力学的结合点:极化和非线性真空及其击穿的激光辐射的作用下的极端强度。非线性光学的研究一直是《量子电子学》杂志最重要和最实际的课题之一。 本期发表的论文并不能反映现代非线性光学的所有科学领域,在俄罗斯,许多科学团体都在积极地研究这一领域。我们要对所有投稿的论文作者表示深深的感谢。但是,由于本刊收到的关于该主题的论文数量超过了一期可能发表的论文总量,因此部分论文将在下期发表。六十年的非线性光学
期刊介绍:
Quantum Electronics covers the following principal headings
Letters
Lasers
Active Media
Interaction of Laser Radiation with Matter
Laser Plasma
Nonlinear Optical Phenomena
Nanotechnologies
Quantum Electronic Devices
Optical Processing of Information
Fiber and Integrated Optics
Laser Applications in Technology and Metrology, Biology and Medicine.