CN2798070Y - Accurate measurement device for extinction ratio of polarization splitting film - Google Patents

Abstract

A precise measuring device for the extinction ratio of a polarized light splitting film, comprising a light source, characterized in that the forward direction of the light beam emitted by the light source is a combined polarizer, a reflector, and a beam splitter formed by a first polarized light splitter and a second polarized light splitter in sequence, after the light beam is split by the beam splitter, its transmitted light beam enters the first energy meter through the sample to be tested, and its reflected light beam is received by the second energy meter, the output ends of the first energy meter and the second energy meter are connected to the input port of a computer, the computer processes the data from the first energy meter and the second energy meter, and displays or prints the transmittance, reflectivity and extinction ratio of the test sample, and the sample to be tested is placed on a fourth rotating platform. The utility model device has the characteristics of simple structure, convenient use, high reliability, high measurement accuracy and low cost.

Description

The device for accurately measuring of polarization spectro-film extinction ratio

Technical field

The utility model relates to the measurement of optical thin film, is specifically related to a kind of device for accurately measuring of polarization spectro-film extinction ratio.

Background technology

Polarization spectro-film is meant that the light when a certain specific wavelength can produce P polarized light height when inciding it surperficial at an angle and see through the film of the high reflection of S polarized light.The polarimetry of polarization spectro-film is meant measures its transmitance for a certain specific wavelength P polarized light and S polarized light when a certain angle incident, and calculates its extinction ratio.

In laser instrument, polarization spectro-film is an important optical element, plays a part polarized light and isolates, and its polarization spectro performance will directly have influence on the polarization characteristic of laser instrument output laser.

Now the polarimetry device that uses generally is by the measurement polarization state of light is adjusted in the rotation of monotectic, or adds half-wave plate playing a monotectic back, regulates polarization state by rotating half-wave plate.Because playing monotectic is to be used for the light of a broad wavelength band is risen partially, its extinction ratio is not high, if use the high monotectic of extinction ratio, price is very expensive, and owing to adopt manual adjustment polarizing angle degree, the actual polarizing angle degree and the desired polarization angle of measuring beam may have some deviations, so measuring accuracy is lower, is difficult to satisfy the requirement of high request, high precision laser.In fact how to study to invent out and a kind ofly can accurately measure the polarization spectro-film extinction ratio and the very low again measurement mechanism of cost is an important problem always.

Summary of the invention

The technical problems to be solved in the utility model is to overcome the difficulty of above-mentioned prior art, provide a kind of simple in structure, easy to use, reliability is high, measuring accuracy is high and the measurement mechanism of low-cost polarization spectro-film extinction ratio.It is mainly used in the measurement of 1064nm laser, but is not limited to 1064nm, also can expand to the measurement of 532nm, 355nm and other optical maser wavelength.

Technical solution of the present utility model is:

A kind of device for accurately measuring of polarization spectro-film extinction ratio, comprise light source, it is characterized in that along the working direction that this light source sends light beam be the combined type polarizer that first polarization spectroscope and second polarization spectroscope form successively, catoptron, beam splitter, described light beam is after this beam splitter beam splitting, its transmitted light beam enters first energy meter through testing sample, its folded light beam is received by second energy meter, the output terminal of described first energy meter and second energy meter links to each other with the input port of computing machine, this Computer Processing is from the data of first energy meter and second energy, the transmissivity of demonstration or printing test sample, reflectivity and extinction ratio, shown testing sample is placed on the 4th rotation platform.

Described first polarization spectroscope and second polarization spectroscope are placed on respectively on intermeshing first rotation platform and second rotation platform, this intermeshing first rotation platform and second rotation platform are positioned on the flat board, and this flat board is fixed on the 3rd rotation platform.

Described second rotation platform and the 3rd rotation platform corotation rotating shaft.

Described light source is the Nd-YAG laser instrument, or has frequency multiplication or frequency tripling crystal Nd-YAG laser instrument.

Advantage of the present utility model:

1, the introducing of the combination polarizer can acquire the polarized light of High Extinction Ratio, and eliminate the deviation of polarized light polarization angle.

2, the introducing of beam splitter is write down transmitted light and the spectroscopical reflected light that passes through testing sample respectively with two energy meters, has eliminated the influence that instability such as light source shake are brought to measurement result.

3, this device carries out data processing automatically by computer, and test result can directly show, and device performance is reliable and stable, accurately reads height.

4, the utility model installation cost is low, and the film polarization spectroscope is compared with playing monotectic, and its cost is much lower.

5, by in the output wavelength that changes laser instrument with select the first suitable polarization spectroscope and second polarization spectroscope for use, the utility model can also be used to the polarization characteristic of measuring samples to 532nm, 355nm and other wavelength light.

Description of drawings

Fig. 1 is the structure of device for accurately measuring of the utility model polarization spectro-film extinction ratio and the index path of measuring samples P component photosensitiveness

Fig. 2 is the measurement index path of the utility model measurement device sample S component photosensitiveness

Fig. 3 is the vertical view of the combined type polarizer

Embodiment

The utility model is described in further detail below in conjunction with embodiment and accompanying drawing, but should not limit protection domain of the present utility model with this.

See also Fig. 1 earlier, as seen from the figure, the device for accurately measuring of the utility model polarization spectro-film extinction ratio, comprise light source 1, the working direction that it is characterized in that sending along light source 1 light beam is the combined type polarizer that is formed by the first polarization spectroscope 2-1 and the second polarization spectroscope 2-2 successively, catoptron 3, beam splitter 4, described light beam is after these beam splitter 4 beam splitting, its transmitted light beam enters first energy meter 6 through testing sample 5-1, its folded light beam is received by second energy meter 7, the output terminal of described first energy meter 6 and second energy meter 7 links to each other with the input port of computing machine 8, and described testing sample 5-1 is placed on the 4th rotation platform 5-2.The first polarization spectroscope 2-1 of the described combined type polarizer and the second polarization spectroscope 2-2 are placed on respectively on intermeshing first a rotation platform 2-3 and the second rotation platform 2-4, this the intermeshing first rotation platform 2-3 and the second rotation platform 2-4 are positioned on the dull and stereotyped 2-5, this flat board 2-5 is fixed on the 3rd rotation platform 2-6, as shown in Figure 3.

Described second rotation platform 2-2 and the 3rd rotation platform 2-6 are coaxial.

Described light source 1 is the Nd-YAG laser instrument, and it is the monochromatic light of 1064nm that wavelength is provided.

The described first polarization spectroscope 2-1 and the second polarization spectroscope 2-2 be on the K9 substrate of glass, be coated on the P of 1064nm place component transmitance greater than 99%, extinction ratio is greater than 100: 1 polarization spectro-film, its fundamental purpose provides the polarized light with higher polarization characteristic.

This intermeshing first rotation platform 2-3 and the second rotation platform 2-4 are positioned on the dull and stereotyped 2-5, this flat board 2-5 is fixed on the 3rd rotation platform 2-6, two polarization spectroscopes pass through gearing mesh, make their anglec of rotation equal and opposite in direction, direction is opposite, in substrate, reflect the space displacement that is brought to be used for compensating light beam, can also provide higher extinction ratio simultaneously.This combination is placed on the first rotation platform 2-3 and the second rotation platform 2-4 that can accurately control, and can select the needed anglec of rotation by the characteristic of polarization spectroscope.

Testing sample 5-1 is placed on the 4th rotation platform 5-2, also can accurately control the anglec of rotation, the polarization characteristic of testing sample 5-1 when being used for measuring different angles incident.

Beam splitter 4, by its accurate dichroism, the contrast light beam that can provide and measuring beam to compare for us, can also eliminate simultaneously since the instability such as shake of light source to the influence of measurement result.

The test philosophy of the utility model device is as follows:

When measuring the transmitance of P light components of testing sample 5-1, we measure with the transmitted light of polarization spectroscope, and light path as shown in Figure 1.If the extinction ratio of each sheet polarization spectroscope at the 1064nm place is N: 1 (by spectrophotometer lambda900 preliminary surveying, the polarization spectroscope that we are coated with is about 100: 1 in the extinction ratio at 1064nm place).When depolarized YAG laser passes through the first polarization spectroscope 2-1, just can obtain preliminary polarized light.The ratio of the energy of its P component and S component is:

$\frac{I_{P1}}{I_{S1}}=\frac{N}{1}$

I wherein _P1, I _S1Be respectively the P that sees through, the energy of S light components.

When light beam sees through 1064nm place extinction ratio is M: behind second polarization spectroscope 2-2 of 1, the ratio of the energy of its P component and S component is:

$\frac{I_{P2}}{I_{S2}}=\frac{N\×M}{1\×1}=(N\×M):1$

In this way, total extinction ratio of the utility model measuring system just is (N * M): 1.When N, M were 100, total extinction ratio can reach 10000: 1.If add several groups of polarization spectroscopes, we can obtain the more polarized light of High Extinction Ratio.

Simultaneously, because this polarized light is produced by polarization spectroscope self, its polarization direction and the plane of incidence are absolute parallel, and light beam is exactly the P polarized light of High Extinction Ratio when inciding on the sample, can not introduce the deviation of polarization angle.

With same principle, when we measure the transmitance of S component, reflected light with polarization spectroscope is measured, its light path as shown in Figure 2, Fig. 2 compares with Fig. 1, difference is that the 3rd rotation platform 2-6 has rotated an angle, forms highly purified S polarized light after making the light beam that sent by light source 1 through the combined type polarizer, also can not introduce the deviation of polarization angle.

After obtaining the polarized light of P component and S component, we just can measure the transmitance of testing sample 5-1 with beam splitter 4 and first energy meter 6 and second energy meter 7.

We are illustrated measuring method with the light of P component equally.Do not put into testing sample 5-1 in the beginning light path, directly read the data I of first energy meter 5 and second energy meter 6 ₁' and I ₂', we just can obtain the splitting ratio α of beam splitter 4 at the 1064nm place like this:

$\mathrm{\α}=\frac{I_1^{\′}}{I_2^{\′}}$

These data only need be measured once, deposit the transmitance that computer comes calculation sample as a parameter after measuring in.

During measurement, put into testing sample 5-1, and be adjusted to the angle that to measure.The data that first energy meter 6 and second energy meter 7 are measured are respectively I ₁And I ₂, we can obtain:

$\frac{I_1}{I_2}=T_P\×\frac{I_1^{\′}}{I_2^{\′}}=T_P\×\mathrm{\α}$

That is:

$T_P=\frac{I_1}{I_2\mathrm{\α}}=\frac{I_1}{I_2}\×\frac{I_2^{\′}}{I_1^{\′}}$

T in the formula _PIt is the transmitance of P polarized light.

As a same reason, when we measure with the reflected light of polarization spectroscope, can measure the transmissivity T of S light components _S, we go out the extinction ratio T of sample at the 1064nm place with regard to passable like this _P/ T _S

Measuring the P polarized light by the angle of rotating the 3rd rotation platform 2-6 with selection still is the S polarized light; Sample 5-1 is placed on the 4th rotation platform 5-2, can be by changing the anglec of rotation of the 4th rotation platform 5-2, but the transmitance of measuring beam during with different angles incident testing sample 5-1.The data input computing machine 8 of first energy meter 6 and second energy meter 7 carries out data processing, just can calculate the transmitance Tp of sample P polarized light.

Fig. 2 is the measurement index path of the device for accurately measuring S light components of the utility model polarization spectro-film extinction ratio, as seen from the figure, its formation is similar with the P polarized light measurement, also be to be along main optical path: the laser of the 1064nm that light source 1 sends produces high-quality S polarized light by two secondary reflections of the second polarization spectroscope 2-2 and the first polarization spectroscope 2-1, light path directly is divided into two bundles by beam splitter 4 with light beam then, wherein transmitted light path is by sample 5-1, accepted by first energy meter 6 then, reflected light is directly accepted by second energy meter 7.When measuring the S polarized light, as long as the 4th rotation platform 2-6 is rotated to an angle of having calibrated, shared identical measurement light path when making when measuring the S polarization with measurement P polarization, placing simultaneously a baffle plate 2-7 on the 4th rotation platform 2-6 blocks by the second polarization spectroscope 2-2) see through light, avoid it that the measurement light path of back is impacted.By the energy of computing machine 8 collection first energy meters 6 and second energy meter 7, just can try to achieve the transmitance Ts of the S polarized light of testing sample through data processing.

Like this, measure the transmitance of P component and S polarized light after, computing machine 8 will automatically be calculated testing sample 5-1, i.e. the extinction ratio Tp/Ts of polarization spectro-film, and automatically being presented on the display screen.

By analysis and probationary certificate, characteristics simple in structure, easy to use, that reliability is high, measuring accuracy is high and cost is low that the utility model device has.

Claims (5)

1. An accurate measuring device for the extinction ratio of a polarizing beam splitting film, comprising a light source (1), characterized in that the forward direction of the light beam emitted by the light source (1) is followed by a first polarizing beam splitter (2-1) and a second polarizing beam splitter A combined polarizer formed by a beam splitter (2-2), a reflector (3), and a beam splitter (4). After the beam is split by the beam splitter (4), the transmitted beam passes through the sample to be tested. (5-1) enters the first energy meter (6), and its reflected light beam is received by the second energy meter (7), and the output terminals of the first energy meter (6) and the second energy meter (7) are connected with the computer The input port of (8) is connected, and the sample to be tested (5-1) is placed on the fourth rotating platform (5-2). 2. The device for accurately measuring the extinction ratio of a polarization splitting film according to claim 1, characterized in that said light source (1) is a Nd-YAG laser. 3. The device for accurately measuring the extinction ratio of the polarizing beam splitting film according to claim 1, characterized in that the first polarizing beam splitter (2-1) and the second polarizing beam splitter (2-2) are respectively placed in a On the mutually engaged first rotating platform (2-3) and the second rotating platform (2-4), the mutually engaging first rotating platform (2-3) and the second rotating platform (2-4) are located on a flat plate (2-5), the flat plate (2-5) is fixed on the third rotating platform (2-6). 4. The device for accurately measuring the extinction ratio of a polarization splitting film according to claim 3, characterized in that the second rotating platform (2-2) is coaxial with the third rotating platform (2-6). 5. The device for accurately measuring the extinction ratio of a polarization splitting film according to any one of claims 1 to 4, characterized in that the light source (1) is a crystal Nd-YAG laser with frequency doubling or triple frequency, corresponding Applicable wavelengths of the first polarizing beam splitter (2-1) and the second polarizing beam splitter (2-2) are 532nm and 355nm respectively.

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