CN2739606Y - Weak phase distortion phase difference amplifying hologram device - Google Patents

Weak phase distortion phase difference amplifying hologram device Download PDF

Info

Publication number
CN2739606Y
CN2739606Y CN 200420082615 CN200420082615U CN2739606Y CN 2739606 Y CN2739606 Y CN 2739606Y CN 200420082615 CN200420082615 CN 200420082615 CN 200420082615 U CN200420082615 U CN 200420082615U CN 2739606 Y CN2739606 Y CN 2739606Y
Authority
CN
China
Prior art keywords
lens
hologram
diaphragm
telescope
stage
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
CN 200420082615
Other languages
Chinese (zh)
Inventor
陈建文
高鸿奕
朱化凤
李儒新
徐至展
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shanghai Institute of Optics and Fine Mechanics of CAS
Shanghai Micro Electronics Equipment Co Ltd
Original Assignee
Shanghai Institute of Optics and Fine Mechanics of CAS
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shanghai Institute of Optics and Fine Mechanics of CAS filed Critical Shanghai Institute of Optics and Fine Mechanics of CAS
Priority to CN 200420082615 priority Critical patent/CN2739606Y/en
Application granted granted Critical
Publication of CN2739606Y publication Critical patent/CN2739606Y/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Landscapes

  • Holo Graphy (AREA)

Abstract

The utility model discloses a weak phase distortion phase difference amplifying hologram device, respectively comprising a laser source, a telescope, a hologram, a lens, a diaphragm, a lens and a hologram along the direction of optical axis. The laser source is a single mode operative He-Ne laser, and the telescope is an enlarged 100 times beam expanded system. The lens is a high quality aplanatic optical lens. The focal distance of a first lens is f1 and the focal distance of a second lens is f2, and nf1 =f2. The diaphragm is a space filtering device. After the hologram is expanded and illuminated by the laser source through the telescope, positive and negative diffracted waves of all levels are generated through the first lens. Diffracted focal points are generated on the diaphragm, and two apertures on the diaphragm respectively only permit diffracted waves of +M stage and-N stage to pass. The diffracted waves of +M stage-N and stage pass through the second lens and are interlapped on the focal plane of the second lends to generate a new hologram whose phase difference is amplified (M+N) times. The utility model has the advantage of being suited to the staff who are not in optics major.

Description

Weak position phase distortion phasic difference amplifying holographic device
Technical field:
The utility model is about a kind of weak position phase distortion phasic difference amplifying holographic device, the holographic phase difference amplifying technique that particularly relates to phase distortion corrugated, weak position, be mainly used in the face shape detection of the reconstruct of electron hologram, high-accuracy optical element, the amplification test in the weak distortion corrugated or the like, enlargement factor can reach more than 30 times.
Background technology:
The holographic phase difference amplifying technique has obtained to use widely in the electronic holographic reconfiguration technique, owing to adopted this technology, advantageously promotes the development of electronic holographic technology.Undoubtedly, this high-accuracy corrugated measuring technology has great application market potentiality in fields such as the industry of China, national defence, scientific researches.
The high power holographic phase difference amplifying device (application number 03115177.9) that the inventor Gao Hongyi of Shanghai Optics and Precision Mechanics institute, Chinese Academy of Sciences, Chen Jianwen, Xie Honglan, Xu Zhizhan etc. are provided, as Fig. 1 (a) (b) shown in, by two the part form.First is a hologram recording apparatus, and principle is shown in Fig. 1 (a); Second portion is the reconstruct multiplying arrangement, shown in Fig. 1 (b).
First's pen recorder mainly is made up of LASER Light Source 1, telescope 2, beam splitter 3, catoptron 5,6,7, testing sample 4 and recording medium 8; The second portion multiplying arrangement mainly is made up of helium-Ne laser light source 1, beam expanding telescope 2, semi-transparent semi-reflecting lens 9,12, total reflective mirror 10,11, negative rack 13, lens 14, diaphragm 15 and receiver 16.
LASER Light Source 1 output beam is divided into two by beam splitter 3 after telescope 2 expands bundle, and a branch of is reference wave Cb, and another bundle is object wave Wb.
The light beam Wb that reflects from beam splitter 3 reflexes on the dry plate 8 through sample 4 arrival catoptrons 5, and as object wave, the light beam Cb that sees through beam splitter 3 also reflexes on the holographic dry plate 8 through catoptron 6 and 7, as the reference ripple.Object wave and reference wave interfere the back to form hologram, and record is on the plate 8.When behind the good hologram of the device photographs shown in Fig. 1 (a), holographic dry plate 8 is handled, dried up through dark place, be placed on then on the negative rack 13 shown in Fig. 1 (b) and carry out optics phasic difference amplification and reconstruct.
Phasic difference is amplified by your interferometer of optics Mach-Chen Te and is undertaken, and principle is shown in Fig. 1 (b).Mach-Chen Te that interferometer contains helium-Ne laser light source 1, semi-transparent semi-reflecting lens 9,12, total reflective mirror 10,11, negative rack 13, lens 14, diaphragm 15 and receiver 16.
By output wavelength is helium-Ne laser light source 1 emitted light beams of 632.8nm, behind first semi-transparent semi-reflecting lens 9, is divided into A, B two-beam.Light beam A behind the total reflective mirror 11 and second semi-transparent semi-reflecting lens 12, the hologram of illumination on the dry plate 8; Light beam B behind total reflective mirror 10 and semi-transparent semi-reflecting lens 12, the hologram on the dry plate 8 that also throws light on.
A, the B bundle is respectively by the hologram diffraction, produce 0 grade separately, ± 1, ± M, ± N ... order diffraction, adjust completely reflecting mirror 10 respectively, 11, allow A bundle produce on the hologram 8+M level (or-N level) diffracted wave and B bundle produce on hologram 8-N order diffraction ripple, overlapping on the focal plane of lens 14, use the non-overlapped part of diaphragm 15 eliminations again, because from the object wave of reconstruct on the hologram 8 and its ripple of gripping altogether is that the position is mutually opposite, be that A restraints after generation+M order diffraction ripple and the generation of B bundle-N order diffraction ripple stack, to produce interference, phasic difference is amplified to original (M+N) doubly, repeats said process n time, and then phasic difference amplifies 2 M+NDoubly.
It is higher that the weak point of this high power holographic phase difference amplifying device is to adjust the technical requirement of interferometer.
Summary of the invention:
The technical problems to be solved in the utility model is to overcome above-mentioned the deficiencies in the prior art, and a kind of weak position phase distortion phasic difference amplifying holographic device is provided, and does not need accurate especially adjustment, and the staff who is particularly suitable for non-optical specialty uses.
Technical solution of the present utility model is as follows:
A kind of weak position phase distortion phasic difference amplifying holographic device, its formation is: it comprises LASER Light Source, telescope, hologram, lens, diaphragm, lens and hologram successively along optical axis direction, and said LASER Light Source is the He-Ne laser instrument of a single mode running; Said telescope is a beam-expanding system that amplifies 100 times; Said first and second lens are the aplanatic optical lenses of a kind of high-quality; The focal length of first lens is f 1, the focal length of second lens is f 2, and nf 1=f 2Said diaphragm is a kind of spatial filter arrangement; After hologram is expanded Shu Zhaoming by LASER Light Source by telescope, behind first lens, produce positive and negative diffracted waves at different levels, and on diaphragm, produce diffractive spots, two apertures on the diaphragm, only allow respectively+the M level and-N order diffraction ripple passes through, then should+the M level and-N order diffraction ripple is again through second lens and overlapped on the focal plane of second lens, produces new hologram, this hologram has amplified (M+N) times with the phasic difference of hologram.
The utility model is compared with technology formerly, and following advantage is arranged:
Do not need to adopt Mach-Chen Teer to carry out precision adjustment, be applicable to the staff of non-optical specialty.
Description of drawings
Fig. 1 a is the technical notes hologram apparatus formerly
Hologram and reconstruct hologram apparatus are amplified in Fig. 1 b technology phasic difference formerly
The weak position of Fig. 2 the utility model phase distortion phasic difference amplifying holographic device structural representation
Embodiment:
See also Fig. 2, Fig. 2 is the weak position of a utility model phase distortion phasic difference amplifying holographic device structural representation, as seen from the figure, the weak position of the utility model phase distortion phasic difference amplifying holographic device, it comprises LASER Light Source 1, telescope 2, hologram 8, first lens 17, diaphragm 18, second lens 19 and holographic Figure 20 successively along optical axis direction.
Said LASER Light Source 1 is the He-Ne laser instrument of a single mode running, and output power is 5mW; Said telescope 2 is beam-expanding systems that amplify 100 times, and its function is that with diameter be the light beam that the light beam of 1mm is expanded into diameter 100mm; Said hologram 8 is the holograms that obtain with conventional method, as the optical hologram of electron hologram or phasic difference amplification.Said lens 17 and 19 are the aplanatic optical lenses of a kind of high-quality, and the focal length of lens 17 is f 1, the focal length of lens 19 is f 2, and nf 1=f 2, this is a gordian technique of the present utility model, hologram is amplified in the phasic difference that it can be taken under any angle.
Said diaphragm 18 is a kind of spatial filter arrangement, and its function is can be by diffracted wave to be amplified and conjugate wave thereof.After hologram 8 is expanded Shu Zhaoming by LASER Light Source 1 by telescope 2, can produce positive and negative diffracted waves at different levels through lens 17, and on diaphragm 18, produce diffractive spots.If on diaphragm 18, opened two apertures, only allow+the M level and-the N level passes through, so+the M level and-N order diffraction ripple is again through lens 19, so on the focal plane of lens 14, two train waves are overlapped, produce new hologram, this hologram has amplified (M+N) doubly with the phasic difference of hologram 8, and this process can be carried out repeatedly.
As mentioned above, the course of work of the present utility model is: at first will take, contain the hologram 8 of object phase information, and after handling in dark place, drying up, be placed on and carry out the phasic difference amplification on the negative rack shown in Figure 2, and take new holographic Figure 20.
Expand Shu Yihou through LASER Light Source 1 and telescope 2, beam lighting hologram 8, the diffracted wave of its generation produce in the focal plane of lens 17 0 grade, ± 1 ... ± M, ± N order diffraction focus, with the unwanted diffracted wave of diaphragm 18 eliminations, only allow needed+M level ,-the N level passes through, again after lens 19, on the focal plane of lens 19, + M level and-N level overlaid, produces new holographic Figure 20, just can be with new holographic Figure 20 reconstruct or continuation amplification again.
Adopt this technology can obtain the above measuring accuracy in λ/100, λ is used laser wavelength.

Claims (1)

1, a kind of weak position phase distortion phasic difference amplifying holographic device, it is characterized in that it comprises LASER Light Source (1), telescope (2), hologram (8), first lens (17), diaphragm (18), second lens (19) and hologram (20) successively along optical axis direction, said LASER Light Source (1) is the He-Ne laser instrument of a single mode running; Said telescope (2) is a beam-expanding system that amplifies 100 times; The said lens first (17) and second lens (19) are the aplanatic optical lenses of a kind of high-quality; The focal length of lens (17) is f 1, the focal length of lens (19) is f 2, nf 1=f 2Said diaphragm (18) is a kind of spatial filter arrangement.
CN 200420082615 2004-09-07 2004-09-07 Weak phase distortion phase difference amplifying hologram device Expired - Fee Related CN2739606Y (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN 200420082615 CN2739606Y (en) 2004-09-07 2004-09-07 Weak phase distortion phase difference amplifying hologram device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN 200420082615 CN2739606Y (en) 2004-09-07 2004-09-07 Weak phase distortion phase difference amplifying hologram device

Publications (1)

Publication Number Publication Date
CN2739606Y true CN2739606Y (en) 2005-11-09

Family

ID=35354672

Family Applications (1)

Application Number Title Priority Date Filing Date
CN 200420082615 Expired - Fee Related CN2739606Y (en) 2004-09-07 2004-09-07 Weak phase distortion phase difference amplifying hologram device

Country Status (1)

Country Link
CN (1) CN2739606Y (en)

Similar Documents

Publication Publication Date Title
WO2019044336A1 (en) Holographic imaging device and data processing method therefor
CN214747811U (en) Light path of composite hologram with two groups of orthogonal interference fringes
CN104457611A (en) Dual-wavelength shearing interference digital holography microscope measuring device and method thereof
CN1614457A (en) Confocal interference microscope with high-space resolution imaging ability
CN112013791B (en) Three-wavelength variable-scale interference microscopic imaging system, imaging method and three-phase restoration method
CN1313847C (en) Holographic phase difference amplifying restructuring device based on sagnac interferometer
US9658114B1 (en) Device for measuring point diffraction interferometric wavefront aberration and method for detecting wave aberration
CN110160624B (en) Optical fiber point diffraction device for three-dimensional vibration measurement and measurement method
CN1200325C (en) Amplifying holographic device for axle recorded phase difference
CN2739606Y (en) Weak phase distortion phase difference amplifying hologram device
CN2655297Y (en) Coaxial recording phase difference amplifying holographing apparatus
CN110375641B (en) Circular carrier frequency digital holographic detection device and method based on improved Michelson structure
WO2024007674A1 (en) Method and apparatus for realizing ultra-high-speed structured illumination microscopy
CN1670639A (en) Lens-less coaxial recording holographic phase difference amplifying device
CN116448728A (en) Dual-beam field interference light sheet microscopic imaging method and device based on galvanometer scanning
KR100712708B1 (en) Rapid acquisition fused off-axis illumination direct-to-digital holography
CN2788230Y (en) Non-lens coaxial-recording holographic phase difference amplifying device
CN108562225A (en) Reflective railway digital holographic apparatus and method altogether based on light splitting pupil
CN100373270C (en) Holographic phasic difference amplifying and reconfiguration unit
CN1243952C (en) Position phase-difference enlarger of combined interferometer
CN2828742Y (en) Holographic phase difference amplification reconstructing device based on sagnae interferometer
CN2638108Y (en) Dynamic holography device for He-Ne laser shooting
CN117705001B (en) Digital holographic object morphology measuring device and method based on concave mirror
CN1431463A (en) High power holographic phase difference amplifying device
CN1560706A (en) High-resolution large field digital holographic device

Legal Events

Date Code Title Description
C14 Grant of patent or utility model
GR01 Patent grant
C19 Lapse of patent right due to non-payment of the annual fee
CF01 Termination of patent right due to non-payment of annual fee