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The segment type light wave reflector which possesses the Bragg reflected property which is chosen and does not receive the influence of line breadth

机译:具有选择的布拉格反射特性且不受线宽的影响的分段型光波反射器

摘要

(57) Abstract The goods of the segment type which possesses the Bragg reflected property which for the input wavelength which is chosen is chosen make clear. It has the section which possesses the index of refraction which the contiguity section differs in order these goods consist of and being the section of the optical material which is lined up, the multiple kind of segments where at the same time each segment 1st consists of with the section of the optical material and 2nd the section of the optical material 1 to form super cycle little alternately. The traveling wave to the rear of the synthetic amplitude in the input wavelength where of super cycle as for the segment 1 optical path differs from another segment of that super cycle little, furthermore as for the surface between the sections of super cycle, is chosen is made. In super cycle, the surface of the odd number turn eye which is continued forms the 1st set surface, the surface of the even number turn eye which super cycle continues makes the 2nd set surface. As for this section, (1) when sum concerning the super cyclic section of the product of length of each section in alignment direction and index of refraction of this section, N z integer, designating as wavelength of the entry wave, as for the surface of tupple of odd number or the even number which the surface which almost is equal to N z/2, and (2) in super cycle continues, modulus of sum of the synthetic amplitude which was made by this tupple is zero, or in order to become 40% or less of modulus of sum of the synthetic amplitude which was made or by other tupple, interval it can be less crowded. The device where Bragg reflection from the Bragg reflector of this invention is used for the stabilization of laser source is disclosed.
机译:(57)<摘要>具有针对所选输入波长选择的具有布拉格反射特性的分段类型的商品要清楚。这些商品的构成具有具有连续度部分不同的具有折射率的部分,并且是排列的光学材料的部分,同时各部分1st由多种部分构成。光学材料的截面和第二光学材料1的截面几乎不交替地形成超循环。对于段1光路而言,在超级波长的输入周期中,在输入波长处的合成振幅的后面的行波与该超级周期的另一段几乎没有差别,此外,对于超级周期的各部分之间的表面,选择了行进波。制作。在超级循环中,连续的奇数转眼的表面形成第一设定表面,在超级循环中连续的偶数转眼的表面形成第二设定表面。关于该部分,(1)当关于各部分的取向方向的长度与该部分的折射率的乘积的超循环部分的和为N z 整数时,指定为该部分的波长。进入波,超级循环中几乎等于N z / 2,和(2)的表面连续的奇数或偶数的连音号的表面,由该波峰形成的合成振幅为零,或者为了成为由其他波峰形成的合成振幅的总和的模数的40%以下,可以使间隔不那么拥挤。公开了使用来自本发明的布拉格反射器的布拉格反射来稳定激光源的装置。

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