DE2324381A1 - FOURIER SYNTHETIC TRANSFORM HOLOGRAM - Google Patents
FOURIER SYNTHETIC TRANSFORM HOLOGRAMInfo
- Publication number
- DE2324381A1 DE2324381A1 DE19732324381 DE2324381A DE2324381A1 DE 2324381 A1 DE2324381 A1 DE 2324381A1 DE 19732324381 DE19732324381 DE 19732324381 DE 2324381 A DE2324381 A DE 2324381A DE 2324381 A1 DE2324381 A1 DE 2324381A1
- Authority
- DE
- Germany
- Prior art keywords
- transform hologram
- fourier transform
- hologram
- image
- basic pattern
- 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.)
- Pending
Links
- 230000003287 optical effect Effects 0.000 claims description 8
- 239000000463 material Substances 0.000 claims description 2
- 230000005540 biological transmission Effects 0.000 description 7
- 238000005520 cutting process Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000005553 drilling Methods 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 230000010363 phase shift Effects 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
- 238000003466 welding Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H1/00—Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
- G03H1/04—Processes or apparatus for producing holograms
- G03H1/08—Synthesising holograms, i.e. holograms synthesized from objects or objects from holograms
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/42—Diffraction optics, i.e. systems including a diffractive element being designed for providing a diffractive effect
- G02B27/46—Systems using spatial filters
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B5/00—Optical elements other than lenses
- G02B5/18—Diffraction gratings
- G02B5/1876—Diffractive Fresnel lenses; Zone plates; Kinoforms
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H1/00—Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
- G03H1/0005—Adaptation of holography to specific applications
- G03H2001/0094—Adaptation of holography to specific applications for patterning or machining using the holobject as input light distribution
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H1/00—Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
- G03H1/22—Processes or apparatus for obtaining an optical image from holograms
- G03H1/2249—Holobject properties
- G03H2001/2252—Location of the holobject
- G03H2001/2255—Holobject out of Fourier or hologram planes
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Holo Graphy (AREA)
- Laser Beam Processing (AREA)
Description
Turlabor AG, Geissacherstrasse B, 8126 Zumikon (Schweiz)Turlabor AG, Geissacherstrasse B, 8126 Zumikon (Switzerland)
Synthetisches Fourier-Transformations-HologrammSynthetic Fourier transform hologram
Die Erfindung betrifft ein synthetisches Fourier-Transformations-Hologramm, bei welchem ein Grundmuster durch ein wiederzugebendes Bild moduliert ist.The invention relates to a synthetic Fourier transform hologram, in which a basic pattern is modulated by an image to be displayed.
Die bekannten synthetischen Fourier-Transformations-Hologramme dieser Art haben ein schachbrettartiges Grundmuster. Um mittels eines solchen Filters das vorgegebene Bild zu erzeugen, sind ein monochromatisches Parallelstrahlenbündel und ein optisches System nötig. Dieses optische System muss ein hohes Auflösungsvermögen haben und ist daher teuer. Ausserdem ist die Justierung des optischen Systems schwierig und zeitraubend und es entstehen durch dasselbe Lichtverluste.The well-known synthetic Fourier transform holograms of this type have a checkerboard-like basic pattern. In order to generate the specified image by means of such a filter, a monochromatic parallel beam and an optical system are required. This optical system is required to have a high resolution and is therefore expensive. In addition, the adjustment of the optical system is difficult and time-consuming and there are light losses due to the same.
Die Erfindung gestattet, dieses optische System zu erübrigen, indem erfindungsgemäss die Frequenz des Grundmusters linear mit dem Abstand von der optischen Achse zunimmt. Die Erfindung betrifft auch die Verwendung dieses Fourier-Transformations-Hologrammes zur Materialbearbeitung.The invention makes it possible to dispense with this optical system in that, according to the invention, the frequency of the basic pattern is linear increases with the distance from the optical axis. The invention also relates to the use of this Fourier transform hologram for material processing.
— A —- A -
3098A7/09533098A7 / 0953
In der Zeichnung ist ein Ausführungsbeispiel des Erfindungsgegenstandes schematisch dargestellt. In perspektivischer Darstellung zeigen:An exemplary embodiment of the subject matter of the invention is shown schematically in the drawing. In perspective Show illustration:
Fig. 1 den Strahlengang durch eine FresnelzonenplatteiFig. 1 shows the beam path through a Fresnel zone plate
Fig. 2 den Strahlengang durch ein Fourier-Transformations-Hologramm nach der Erfindung;2 shows the beam path through a Fourier transform hologram according to the invention;
Ferner zeigenAlso show
Fig. 3 und 4 die Transmission der Fresnelzonenplatte nach Fig. 1 bzw. des Fourier-Transformations-Hologrammes nach Fig. 2.3 and 4 the transmission of the Fresnel zone plate according to Fig. 1 or the Fourier transform hologram according to Fig. 2.
Die in Fig. 1 gezeigte Fresnelzonenplatte (Fresnelbeugungslinse) 1vbesteht in bekannter Weise aus einer durchsichtigen Platte, auf der konzentrische, undurchsichtige Kreise aufgezeichnet sind, wobei der Abstand zwischen den Kreisen nach aussen hin abnimmt. Beleuchtet man die Platte 1 mit einer punktförrnigen monochromatischen Lichtquelle 2, so wird das gebeugte Licht in einem Punkt 3 einer ξ- Π-Bildebene fokussiert, die zur x-y-Ebene der Platte 1 parallel ist. In Fig. ist die Transmission t der Platte 1 in Funktion des Radius r dargestellt. Es handelt sich um eine Rechteckwelle, die sich zwischen den Werten t = 1 und t = 0 ändert und deren Raumfrequenz linear mit dem Radius zunimmt, wobei deren "Impulse" 4 mit zunehmendem Radius schmäler werden.The Fresnel zone plate shown in Fig. 1 (Fresnel diffraction lens) 1v consists in the known manner of a transparent plate on which concentric, opaque circles are drawn with the distance between the circles decreasing towards the outside. If you illuminate the plate 1 with a point-like monochromatic light source 2, so that is diffracted light focused in a point 3 of a ξ- Π image plane, which is parallel to the x-y plane of the plate 1. In FIG. 1, the transmission t of the plate 1 is a function of the radius r shown. It is a square wave that changes between the values t = 1 and t = 0 and its spatial frequency increases linearly with the radius, its "pulses" 4 becoming narrower with increasing radius.
Das in Fig. 2 gezeigte Fourier-Transformations-Hologramm kann man sich dadurch aus der Platte 1 entstanden denken, dass deren Rechteckwelle räumlich gemäss der Fouriertransformierten eines vorgegebenen Bildes moduliert worden ist, d.h. dass die einzelnen "Impulse" 4' gegenüber den Impulsen 4 in ihrer LageThe Fourier transform hologram shown in FIG one can imagine that it emerged from the plate 1 that its square wave spatially corresponds to the Fourier transform of a given image has been modulated, i.e. that the individual "pulses" 4 'in relation to the pulses 4 in their position
- 2 309847/0953 - 2 309847/0953
und Breite verändert worden sind. Die räumliche Modulation kann so berechnet werden, insbesondere mittels eines Computers, dass in der ^ ~ ^"Bildebene eine bestimmte Figur entsteht; im vorliegenden Fall wird das von der monochromatischen Lichtquelle 2 ausgehende Licht auf einen konzentrischen Kreis 6 fokussiert. Wenn sich in der Bildebene z.B. eine Metallplatte befindet, so kann man auf diese Weise ein Loch vom Radius des Kreises .6 herausschneiden.and width have been changed. The spatial modulation can calculated in such a way, in particular by means of a computer, that a certain figure is created in the ^ ~ ^ "image plane; in the present case In this case, the light emanating from the monochromatic light source 2 is focused on a concentric circle 6. If, for example, there is a metal plate in the plane of the picture, a hole with the radius of the circle can be made in this way .6 cut out.
Anstelle eines Kreises könnte das Licht auch auf irgend eine oder mehrere andere geschlossene oder offene Linienzöge konzentriert werden, je nach gewünschter Anwendung zum Bohren, Schneiden, Schweissen und dgl.Instead of a circle, the light could also point to any one or several other closed or open lines are concentrated are, depending on the desired application for drilling, cutting, welding and the like.
Das Grundmuster des Fourier-Transforrnations-Hologrammes muss nicht unbedingt demjenigen der Fresnelzonenplatte entsprechen. Allgemein kann das Grundmuster durch folgende Gleichung dargestellt werden:The basic pattern of the Fourier transformation hologram must does not necessarily correspond to that of the Fresnel zone plate. In general, the basic pattern can be represented by the following equation will:
t(x,y) = V-1Cn · Bxp.jnoc. 4(x-u)2 + (y-v)2 Vt (x, y) = V -1 C n * Bxp.jnoc. 4 (xu) 2 + (yv) 2 V
Darin bedeuten:Therein mean:
t(x,y) die Transmission in jedem Punkt der x-y-Ebenet (x, y) is the transmission at each point on the x-y plane
Cn Koeffizienten der ReihenentwicklungC n coefficients of the series expansion
©£, u und ν Konstanten.© £, u and ν constants.
Das modulierte Grundmuster wird dann dargestellt durch die GleichungThe basic modulated pattern is then represented by the equation
t(x,y) = p(x,y) · \ c · exp.jnoC 4 (x-u)2 + (y-v)2 rt (x, y) = p (x, y) · \ c · exp.jnoC 4 (xu) 2 + (yv) 2 r
n = - oc n = - oc
309847/0953309847/0953
worin p(x,y) die Fouriertransformierte des vorgegebenen Bildes in jedem Punkt der.x-y-Ebene ist.where p (x, y) is the Fourier transform of the given Image is at every point in the .x-y plane.
Obige allgemeine Gleichung umfasst auch Grundmuster, bei denen die Transmission nicht nur zwei extreme Werte t = 1 und t = 0 annimmt ("Binäre Muster"), sondern auch solche, bei denen die Transmission kontinuierlich wellenförmig variiert, Extremwerte der Transmission sind t = +1 und t = -1, wobei eine negative Transmission wie üblich eine Phasenverschiebung von 180° bedeutet.The above general equation also includes basic patterns in which the transmission is not just two extreme values t = 1 and assumes t = 0 ("binary pattern"), but also those in which the transmission varies continuously in a wavy manner, Extreme values of the transmission are t = +1 and t = -1, where one As usual, negative transmission means a phase shift of 180 °.
Im Gegensatz zu den bekannten synthetischen Fourier-Transformations-Hollogrammen ist zur Erzeugung des Bildes 6 kein optisches System-zwischen dem Hologramm 5 und der ^~^? -Bildebene notwendig. Um den fiasstab des Bildes 6 zu verändern, genügt es, den Abstand des Hologrammes 5 von der Lichtquelle 2 zu variieren, während bei Anwendung der bekannten Hologramme hierzu ein anderes optisches System notwendig ist. Ein weiterer Vorteil ist der, dass die Wellenlänge des monochromatischen Lichtes in ziemlich weiten Grenzen ("Fresnelbereich") variieren kann, ohne dass dies zu Verzerrungen des Bildes führt.In contrast to the well-known synthetic Fourier transform hollograms is there no optical system for generating the image 6 between the hologram 5 and the ^ ~ ^? Image layer necessary. To change the scale of Figure 6, it is sufficient to measure the distance between the hologram 5 and the light source 2, while using the known holograms this requires a different optical system. Another The advantage is that the wavelength of the monochromatic light is within fairly wide limits ("Fresnel range") can vary without distorting the image.
3098^7709533098 ^ 770953
Claims (2)
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CH752572A CH552224A (en) | 1972-05-19 | 1972-05-19 | SYNTHETIC FOURIER TRANSFORMANCE HOLOGRAM. |
Publications (1)
Publication Number | Publication Date |
---|---|
DE2324381A1 true DE2324381A1 (en) | 1973-11-22 |
Family
ID=4326509
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
DE19732324381 Pending DE2324381A1 (en) | 1972-05-19 | 1973-05-14 | FOURIER SYNTHETIC TRANSFORM HOLOGRAM |
Country Status (8)
Country | Link |
---|---|
JP (1) | JPS4956650A (en) |
CA (1) | CA978775A (en) |
CH (1) | CH552224A (en) |
DE (1) | DE2324381A1 (en) |
FR (1) | FR2185805B1 (en) |
GB (1) | GB1393662A (en) |
IT (1) | IT1006578B (en) |
NL (1) | NL7306560A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7995256B2 (en) | 2005-07-06 | 2011-08-09 | Dai Nippon Printing Co., Ltd. | Transparent card with hologram, and apparatus for recognizing transparent card with hologram |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1035494C (en) * | 1994-04-19 | 1997-07-23 | 南京师范大学 | Method for producing large visual-angle secondary rainbow hologram with computing holography |
US8324529B2 (en) | 2007-11-14 | 2012-12-04 | Hamamatsu Photonics K.K. | Laser machining device with a converged laser beam and laser machining method |
-
1972
- 1972-05-19 CH CH752572A patent/CH552224A/en not_active IP Right Cessation
-
1973
- 1973-05-10 NL NL7306560A patent/NL7306560A/xx unknown
- 1973-05-14 DE DE19732324381 patent/DE2324381A1/en active Pending
- 1973-05-15 CA CA171,464A patent/CA978775A/en not_active Expired
- 1973-05-15 JP JP48053238A patent/JPS4956650A/ja active Pending
- 1973-05-16 IT IT2414273A patent/IT1006578B/en active
- 1973-05-16 FR FR7317716A patent/FR2185805B1/fr not_active Expired
- 1973-05-17 GB GB2364273A patent/GB1393662A/en not_active Expired
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7995256B2 (en) | 2005-07-06 | 2011-08-09 | Dai Nippon Printing Co., Ltd. | Transparent card with hologram, and apparatus for recognizing transparent card with hologram |
DE102006030865B4 (en) * | 2005-07-06 | 2016-03-24 | Dai Nippon Printing Co., Ltd. | Transparent card with hologram |
Also Published As
Publication number | Publication date |
---|---|
GB1393662A (en) | 1975-05-07 |
NL7306560A (en) | 1973-11-21 |
CH552224A (en) | 1974-07-31 |
FR2185805A1 (en) | 1974-01-04 |
CA978775A (en) | 1975-12-02 |
FR2185805B1 (en) | 1976-11-12 |
JPS4956650A (en) | 1974-06-01 |
IT1006578B (en) | 1976-10-20 |
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