FACTS ABOUT BIREFRINGENT CRYSTAL REVEALED

Facts About Birefringent Crystal Revealed

Facts About Birefringent Crystal Revealed

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各向异性透明晶体如方解石、石英等的折射率,是其固有的特性,称为永久双折射。

In each body of Determine 8, the axis in the microscope polarizer is indicated through the capital letter P and is also oriented in an East-West (horizontal) way. The axis of your microscope analyzer is indicated because of the letter A which is oriented in the North-South (vertical) path. These axes are perpendicular to each other and end in a very dark industry when noticed throughout the eyepieces with no specimen over the microscope stage.

The birefringence of nonlinear crystal resources permits birefringent phase matching of nonlinear interactions. Primarily, Consequently birefringence compensates the wavelength dependence with the refractive index.

The optical path big difference is usually a classical optical notion connected with birefringence, and both are defined with the relative section shift among the regular and incredible rays since they emerge from an anisotropic content. On the whole, the optical route change is computed by multiplying the specimen thickness from the refractive index, but only once the medium is homogeneous and won't incorporate sizeable refractive index deviations or gradients.

The ordinary and extraordinary wavefronts in uniaxial crystals coincide at possibly the gradual or perhaps the rapidly axis with the ellipsoid, dependent upon the distribution of refractive indices inside the crystal (illustrated in Figure six). The optical route big difference or relative retardation among these rays is determined by the lag of one wave behind one other in floor wavefronts alongside the propagation direction.

一些激光器晶体(例如,钒酸盐晶体和钨酸盐晶体)本身就具有双折射。这在需要无去极化损耗的线偏振输出时非常有用。 

For bulk optical products, It's also common to contemplate the primary difference of refractive indices for the two polarization Instructions. The larger that big difference, the bigger the attained retardance for each millimeter of propagation size.

文献中,双折射通常包含两种不同的含义。经典光学中,就是下面所说的双折射(double refraction)。

Non-polarized white mild from your illuminator enters the polarizer over the still left and is particularly linearly polarized with here an orientation during the course indicated via the arrow (adjacent for the polarizer label), and is particularly arbitrarily represented by a crimson sinusoidal light-weight wave. Subsequent, the polarized gentle enters the anisotropic crystal (mounted on the microscope stage) the place it is refracted and divided into two different components vibrating parallel on the crystallographic axes and perpendicular to one another (the pink open up and filled light waves).

双折射现象的明显例子是方解石。透过方解石的菱面体就可以看到明显重影。

而在非线性光学和激光器技术中,双折射则是一些非各向同性透明介质的折射率依赖于偏振方向(即电场方向)的性质。后者的性质时非偏振光束入射到该材料上时产生双折射。 

Alternatively, by measuring the refractive indices of the anisotropic specimen and calculating their big difference (the birefringence), the interference colour(s) is often identified with the birefringence values together the best of the chart. By extrapolating the angled strains again for the ordinate, the thickness from the specimen may also be approximated.

The strategy allows segregation of an individual refractive index for measurement. Subsequently, the remaining refractive index of the birefringent material can then be measured by rotation in the polarizer by 90 levels.

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在激光器技术和非线性光学中,双折射现象通常发生在非各向同性晶体中: 

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