{"title":"腔内和频产生的光学参量振荡","authors":"G. Moore, K. Koch","doi":"10.1364/nlo.1992.we23","DOIUrl":null,"url":null,"abstract":"We present theoretical calculations of an optical parametric oscillator (OPO) containing, in addition to the OPO crystal, a crystal for intracavity sum-frequency generation (SFG). The latter crystal combines light at the pump frequency ω\n p\n with light at the OPO signal frequency ω\n s\n to produce the desired frequency ω\n d\n = ω\n p\n + ω\n s\n . Only the frequency ω\n s\n oscillates in the cavity. This system is modeled in the plane-wave approximation for both spatial orderings of the crystals. The pump power is ultimately converted to the desired radiation, to idler radiation of frequency ω\n i\n =2ω\n p\n – ω\n d\n , and to cavity losses at frequency ω\n s\n . Since the ω\n i\n and ω\n d\n radiation grows from zero on each pass, changes in the cavity length do not produce interference effects. The choice of crystal for the OPO is limited by the requirement that this crystal transmit the long-wavelength idler. With proper choice of design parameters, little pump power remains unconverted by the two crystals over an extended range of the incident pump intensity. In steady-state operation the ratio η of the photon flux emitted at ω\n d\n to the photon flux incident at ω\n p\n can be nearly 0.5.","PeriodicalId":219832,"journal":{"name":"Nonlinear Optics: Materials, Fundamentals, and Applications","volume":"65 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"7","resultStr":"{\"title\":\"Optical Parametric Oscillation with Intracavity Sum-Frequency Generation\",\"authors\":\"G. Moore, K. Koch\",\"doi\":\"10.1364/nlo.1992.we23\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We present theoretical calculations of an optical parametric oscillator (OPO) containing, in addition to the OPO crystal, a crystal for intracavity sum-frequency generation (SFG). The latter crystal combines light at the pump frequency ω\\n p\\n with light at the OPO signal frequency ω\\n s\\n to produce the desired frequency ω\\n d\\n = ω\\n p\\n + ω\\n s\\n . Only the frequency ω\\n s\\n oscillates in the cavity. This system is modeled in the plane-wave approximation for both spatial orderings of the crystals. The pump power is ultimately converted to the desired radiation, to idler radiation of frequency ω\\n i\\n =2ω\\n p\\n – ω\\n d\\n , and to cavity losses at frequency ω\\n s\\n . Since the ω\\n i\\n and ω\\n d\\n radiation grows from zero on each pass, changes in the cavity length do not produce interference effects. The choice of crystal for the OPO is limited by the requirement that this crystal transmit the long-wavelength idler. With proper choice of design parameters, little pump power remains unconverted by the two crystals over an extended range of the incident pump intensity. In steady-state operation the ratio η of the photon flux emitted at ω\\n d\\n to the photon flux incident at ω\\n p\\n can be nearly 0.5.\",\"PeriodicalId\":219832,\"journal\":{\"name\":\"Nonlinear Optics: Materials, Fundamentals, and Applications\",\"volume\":\"65 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"7\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nonlinear Optics: Materials, Fundamentals, and Applications\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/nlo.1992.we23\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nonlinear Optics: Materials, Fundamentals, and Applications","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/nlo.1992.we23","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 7
摘要
我们提出了一个光学参量振荡器(OPO)的理论计算,除了OPO晶体外,还包含一个腔内和频产生(SFG)晶体。后一种晶体将泵浦频率ω p的光与OPO信号频率ω s的光结合,产生所需的频率ω d = ω p + ω s。只有频率ω s在腔中振荡。该系统是在平面波近似晶体的两个空间顺序。泵功率最终转换为所需的辐射,频率为ω i =2ω p - ω d的空闲辐射和频率为ω s的腔损失。由于ω i和ω d辐射在每次通过时都从零开始增长,因此腔长的变化不会产生干扰效应。OPO晶体的选择受限于该晶体传输长波长闲散信号的要求。在适当选择设计参数的情况下,在较大的入射泵浦强度范围内,两个晶体未转换的泵浦功率很小。稳态运行时,在ω d处发射的光子通量与在ω p处入射的光子通量之比η可以接近0.5。
Optical Parametric Oscillation with Intracavity Sum-Frequency Generation
We present theoretical calculations of an optical parametric oscillator (OPO) containing, in addition to the OPO crystal, a crystal for intracavity sum-frequency generation (SFG). The latter crystal combines light at the pump frequency ω
p
with light at the OPO signal frequency ω
s
to produce the desired frequency ω
d
= ω
p
+ ω
s
. Only the frequency ω
s
oscillates in the cavity. This system is modeled in the plane-wave approximation for both spatial orderings of the crystals. The pump power is ultimately converted to the desired radiation, to idler radiation of frequency ω
i
=2ω
p
– ω
d
, and to cavity losses at frequency ω
s
. Since the ω
i
and ω
d
radiation grows from zero on each pass, changes in the cavity length do not produce interference effects. The choice of crystal for the OPO is limited by the requirement that this crystal transmit the long-wavelength idler. With proper choice of design parameters, little pump power remains unconverted by the two crystals over an extended range of the incident pump intensity. In steady-state operation the ratio η of the photon flux emitted at ω
d
to the photon flux incident at ω
p
can be nearly 0.5.