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A Phase Plate for Phase Contrast Microscopy

A phase contrast microscope and phase plate technology, applied in the field of phase plates, can solve the problems of long production process flow, difficult to guarantee coating accuracy, limited processing efficiency, etc., to achieve improved imaging effect, shortened coating process flow, and reduced light source energy attenuation. Effect

Active Publication Date: 2018-05-11
NINGBO YONGXIN OPTICS
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Problems solved by technology

Although a single layer of MgF2 can change the phase (such as a negative phase process), the single layer of MgF2 film can only form a phase difference of -1 / 4λ at a specific wavelength, which is not suitable for broadband light sources. When using broadband light sources, the contrast ratio will decrease Therefore, a monochromatic filter of a specific wavelength must be added in front of the light source; however, the introduction of the filter will inevitably lead to the loss of light source energy, resulting in a dim field of view
In addition, the phase absorbing film of the traditional phase plate has a ring-shaped junction with a height difference between the single-layer MgF2 film and the single-layer Cr12 film. It is difficult to guarantee the coating accuracy at the ring-shaped junction, resulting in a long production process and low yield , which limits the processing efficiency and makes the manufacturing cost higher

Method used

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  • A Phase Plate for Phase Contrast Microscopy
  • A Phase Plate for Phase Contrast Microscopy
  • A Phase Plate for Phase Contrast Microscopy

Examples

Experimental program
Comparison scheme
Effect test

Embodiment 1

[0032] The glass substrate 1 is selected as an N-BK7 substrate. The bottom layer 5 and surface layer 7 of the annular thin film layer 2 are metal Cr film layers, the physical thickness of the bottom layer 5 of the annular thin film layer 2 is 8 nm to 12 nm, the physical thickness of the surface layer 7 is 3 nm to 5.5 nm, and the interlayer 6 is MgF2 The physical thickness of the layer is 110 nm to 116 nm. Preferred values: the physical thickness of the bottom layer 5 of the annular thin film layer 2 is 10 nm, the physical thickness of the surface layer 7 is 4.12 nm, and the physical thickness of the interlayer 6 is 113.7 nm.

[0033] When the physical thickness of the bottom layer 5 of the ring-shaped thin film layer 2 that is metal Cr film layer and the surface layer 7 and the MgF2 layer are all preferred values, the phase value distribution of the broadband light beam that is 450nm-700nm through its wavelength is as follows Image 6 As shown, the beam transmittance distribu...

Embodiment 2

[0035] The glass substrate 1 is selected as an N-BK7 substrate. The bottom layer 5 and surface layer 7 of the annular thin film layer 2 are metal Nb film layers, the physical thickness of the bottom layer 5 of the annular thin film layer 2 is 8nm to 12 nm, the physical thickness of the surface layer 7 is 3.5 nm to 6nm, and the interlayer 6 is MgF2 layer The physical thickness is 80nm to 90nm. Preferred values: the physical thickness of the bottom layer 5 of the annular thin film layer 2 is 10 nm, the physical thickness of the surface layer 7 is 5 nm, and the physical thickness of the interlayer 6 is 86.63 nm.

[0036] When the physical thickness of the bottom layer 5 of the annular thin film layer 2 that is metal Nb film layer and the surface layer 7 and the interlayer 6 of the MgF2 layer are all preferred values, the phase value distribution of the broadband light beam that is 450nm-700nm through its wavelength is as follows Figure 9 shown.

Embodiment 3

[0038] The glass substrate 1 is selected as an N-BK7 substrate. The bottom layer 5 and the surface layer 7 of the annular thin film layer 2 are metal Ti film layers, the physical thickness of the bottom layer 5 of the annular thin film layer 2 is 8 nm to 12 nm, the physical thickness of the surface layer 7 is 3.5 nm to 6 nm, and the interlayer 6 is the MgF2 layer The physical thickness is 95nm to 105nm. Preferred values: the physical thickness of the bottom layer 5 of the annular film layer 2 is 10 nm, the physical thickness of the surface layer 7 is 5 nm, and the physical thickness of the interlayer 6 is 100.39 nm.

[0039] When the physical thicknesses of the bottom layer 5 and the surface layer 7 of the annular film layer 2 of the metal Ti film layer and the interlayer 6 of the MgF2 layer are all preferred values, the phase value distribution of the broadband beam of 450nm-700nm through its wavelength is as follows Figure 10 shown.

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Abstract

The invention relates to a phase plate for a phase contrast microscope. According to the phase plate, a glass substrate (1) is coated with an annular thin film layer (2); the annular thin film layer comprises a bottom layer (5) directly coating the glass substrate (1), an interlayer (6) and a surface layer (7); the interlayer (6) is a MgF2 layer; the bottom layer (5) and the surface layer (7) are metal film layers made of the same material; and the material of the metal film layers is one material selected from Cr, Nb, Ti and Ni. The phase plate has a plurality of functions such as a phase changing function and a light beam absorption function. The wide-band phase change of the phase plate is small, so that the phase value of a wide-band light beam of which the wavelength ranges from 450 nm to 700 nm can be about -90 degrees, wherein the wide-band light beam passes through the phase plate, and therefore, the phase plate can be used under wide-band light sources; and the phase plate is simple in film layer structure and is convenient to manufacture.

Description

technical field [0001] The invention relates to a phase plate for a phase contrast microscope, especially a phase absorption film of the phase plate. Background technique [0002] The human eye can only identify changes in the wavelength (color) and amplitude of visible light, but not phase changes. However, most biological specimens are highly transparent, and the amplitude of the light wave is basically unchanged after passing through, but there is a phase change, which cannot be felt by the human eye. Living cell samples and unstained specimens cannot be directly observed by the human eye because the wavelength and amplitude of light do not change, but the phase of the light passing through the sample has changed, so the interference and diffraction effects of light can be used to distinguish the difference between the passing samples. The optical path difference of the light at the site is converted into a difference in amplitude, enabling clear visualization between va...

Claims

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Application Information

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Patent Type & Authority Patents(China)
IPC IPC(8): G02B5/30G02B21/14
CPCG02B5/3083G02B21/14
Inventor 张克奇邱慧马浩斌杨勇
Owner NINGBO YONGXIN OPTICS
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