CONTROL SYSTEM AND PROCEDURE FOR CONTROLLED ACCESS BY MEANS OF AN OPTICAL DEVICE BASED ON FLAT BANDS

Abstract

A control system for controlled access to a user by means of verifying a physical element defined in an optical and low level of power context, which includes: a setup (1) for the creation of arbitrary spatial light patterns, with control of amplitude and phase; which includes: a source of light (9) which emits a Laser beam; toward a first microscope objective (11); a spatial light modulation set (2) which receives the light of the first microscope objective (11) and said spatial light modulator set (2) sends a profile modulated in amplitude and phase which form an image to a beam splitter BS (17) which divides the image into an initial CCD camera (6) and to a second microscope objective (12); a defined physical element (7) which receives the initial image from the second microscope objective (12), and transmits the image without diffracting it as a final image to a third microscope objective (13); a final CCD camera (8), that receives the final image of the third microscope objective (13) and sends it to a computer (300) which compares that final image with the initial image, and performs a calculation of similarity between both images to decide to grant access to the user, if the similarity is greater than a predefined value, and deny it if the similarity is less than a predefined value; a control procedure of controlled access which compares a pattern of dots transmitted through the defined physical element, which code the numbers 0 to 9 and decides to grant or deny access if it matches with the key entered by user.

Claims

1. A control system for controlled access to a user by means of verifying a defined physical element in an optical and low level of power context, wherein it comprises: a. a setup for the creation of arbitrary spatial light patterns, with control of amplitude and phase; including: b. a source of light which emits a LASER beam of light; toward a first microscope objective; c. a spatial light modulation set which receives the light of the first microscope objective and said spatial light modulator set sends a profile modulated in amplitude and phase which form an image to a beam splitter BS which divides the image onto an initial CCD camera and to a second microscope objective; d. a defined physical element which receives the initial image from the second microscope objective, and transmits the image without diffracting it as a final image to a third microscope objective; and e. a final CCD camera receives the final image of the third microscope objective and sends it to a computer which compares said final image with the initial image, and performs a calculation of similarity between both images to decide to grant access to the user, if the similarity is greater than a predefined value, and deny in case if the similarity is less than a predefined value.

2. The control system of claim 1, wherein the spatial light modulation set (SLM) consists of: a. a first amplitude modulation set, formed by polarizers, lens, an obturator, a spatial light modulator; b. a second phase modulation set, formed by waves retardants; the spatial light modulator, a lens and a mirrors, wherein the light that comes from the first microscope objective is directed to the first set of amplitude modulation wherein it is directed toward the obturator, crossing then the lens, and then the polarizer to reach the spatial modulator on which generates a profile modulated in amplitude, subsequently this profile modulated in amplitude is transmitted by the polarizer, crossing then the lens, the profile and modulated in amplitude is redirected in opposed direction by the mirrors, then said profile modulated in amplitude crosses the second phase modulator set wherein it passes through the wave retardants, to reach the spatial modulator which generates a profile modulated in phase, later this profile modulated in phase is transmitted by the wave retardants, and then passes through the lens in order to said image with modulated amplitude and phase be directed to the beam splitter BS.

3. The control system of claim 1, wherein the profile modulated in amplitude and phase generated in the SLM corresponds to a set of localized beams/spots.

4. The control system of claim 1, wherein the first, second, and third microscope objective have amplification 20?, 4?, 10?, respectively.

5. The system according to claim 1, wherein the defined physical element is a periodic system with non-conventional geometry selected from the group consisting of: photonic crystal, electronic system, system of cold atoms in optical lattices, spintronics, arrangements of quantum dots, arrangements of micro oscillators, arrangements of micropillars, chains of proteins.

6. The system according to claim 5, wherein the photonic crystal is selected from the group that consists of: Lieb, Kagome, Sawtooth, Stub, other unconventional photonic crystals.

7. The system according to claim 5, wherein the photonic crystal has at least one unitary cell.

8. The system according to claim 5, wherein at least a unitary cell of the photonic crystal is composed of at least two sites with different interactions at short range.

9. The system according to claim 5, wherein the non-conventional photonic crystal presents, at least, a flat band.

10. The system according to claim 1, wherein the physical element defined is contained inside a protective device and light transmitter.

11. The system according to claim 10, wherein the protective device and light transmitter has the shape of a cylinder.

12. The system according to claim 10, wherein the protective device and light transmitter is flexible.

13. The system according to claim 10, wherein the transmitter of light of the protective device and transmitter is an optical fiber.

14. The system according to claim 13, wherein the protective device and light transmitter is a container box with a mobile part to let the light passing through.

15. The system according to claim 14, wherein the protective device and light transmitter is a container box is a card.

16. The system according to claim 15, wherein the card is a credit card or identification card.

17. A control procedure of controlled access to a user by means of verifying a defined physical element in an optical and low level of power context, wherein it consists of the following stages: a. deciding a desired initial image, which is formed in the spatial light modulator; b. observing with initial CCD camera the initial image generated in (a), and check that its structure of amplitude and phase matches the desired image. If they do not match, correct the image generated by the spatial light modulator until it matches the desired image; c. passing the modulated light beam through the defined physical element; d. observing with final CCD camera the output final image from the defined physical element; and e. comparing with a computer the coincidence of the final image captured with final CCD camera with the initial image captured with initial CCD camera by a calculation of similarity: if the similarity is >=P, allow access; if the similarity is <P, deny access.

18. A control procedure of controlled access according to claim 17, wherein the stage e) the similarity parameter P is =75%.

19. A control procedure for controlled access to a user by means of verifying a defined physical element in an optical and low level of power context through code, wherein it consists of the following stages: a. entering a defined physical element between the second microscope objective and the third microscope objective; b. typing numeric code in a keyboard of entrance; and c. comparing with a computer, if the pattern transmitted through the defined physical element coincides with the pattern of coded dots to numbers corresponding to the code typed in step (b), if match the access is granted, otherwise the access is denied.

Description

DESCRIPTION OF THE FIGURES

[0026] The group of FIGS. 1 shows the typical properties and phenomenology in conventional lattices without flat bands.

[0027] FIG. 1: (a) Three-dimensional outline of a photonic crystal of rectangular geometry. Waveguides are drawn in gray (cylindrical tubes), while the surrounding material in another shade of gray. Inset: Cross section of this crystalline structure, in which the horizontal and vertical distance between waveguides (circles) is identical (the lines are only visual aids for demarcating the interaction between closest waveguides). (b) First band for a photonic crystal of rectangular geometry. (c) Examples of global modes of the rectangular photonic crystal. (d) Profile of diffraction (below), for an arbitrary propagation distance, for two different initial conditions (above), for a rectangular photonic crystal. In (c) and (d) the scale of intensities grows from the black one through the gray one to the white one. The group of FIGS. 2 shows the properties and phenomenology of the non-conventional Lieb lattice.

[0028] FIG. 2. (a) Three-dimensional outline of a photonic crystal of isotropic Lieb geometry. The waveguides are drawn in gray (cylindrical tubes), while the surrounding material in another tone of gray. Inset: Cross section of this crystal. (b) Band structure for a photonic Lieb lattice. (c) Examples of global modes of photonic Lieb lattice, which cover a large part of the array, except the ring belonging to the flat band [flat surface at (b)]. (d) Profile of diffraction (below) for two different initial conditions (above), for a photonic Lieb lattice.

[0029] FIG. 3 shows a preferred configuration of setup for the physical element defined (7) in which this invention is implemented. The group of FIGS. 3 shows the experimental manufacture and setup technique for the photonic Lieb lattice in which this invention is implemented. FIG. 3. (A) Manufacturing technique of photonic crystals writing waveguides in arbitrary positions, when burning the surrounding material (silica) in defined places. Thus, the refractive index of the material changes and allows the creation of a waveguide for light conduction. (b) Microscope image of a Lieb array designed in Chile and manufactured in Germany, with 341 waveguides and a separation between neighboring waveguides of 20 micrometers. (c) Experimental setup for the creation of the initial image and the study of its propagation along a photonic Lieb lattice. The group of FIGS. 4 shows realistic numerical simulations of the propagation of different initial conditions in the photonic Lieb lattice.

[0030] FIG. 4. Numerical simulation of intensity patterns at the output of a Lieb lattice for different initial conditions: (a) Central excitation of a single waveguide, (b) Four sites with phase difference ? (Lieb ring), (c) Four sites without phase difference, and (d) two rings added. Wavelength ?=532 nm. The group of FIGS. 5 shows experimental images of the propagation of different initial conditions in the photonic Lieb lattice.

[0031] FIG. 5. Experimental observation of intensity patterns at the output of a Lieb lattice for different initial conditions: (a) Central excitation of a single waveguide, (b) Four sites with difference of phase ? (ring of Lieb), (c) Four sites with difference of phase 0, and (d) Two rings of Lieb added. Wavelength ?=532 nm. The group of FIGS. 6 shows the experimental observation of the propagation of different images (patterns) propagated without diffraction in the photonic Lieb lattice, as well as a coding example.

[0032] FIG. 6. Above: Experimental observation for combinations of Lieb rings in various configurations: (a) Two rings in diagonal, (b) 4 rings in sum, (c) 4 rings with horizontal sum and vertical subtraction, and (d) 4 rings with three added and one subtracted. Below: Example of a simplified outline of combinations (coding).

[0033] The group of FIGS. 7 shows an outline of combinations of four rings of Lieb, including the form of measurement of light (1) or no light (0) in four regions well demarcated. FIG. 7. Configuration of points in a pattern of 4 non-diffracting rings with different phase structure. (a) Combination of four localized rings; (b) Modes of the flat band (rings), one in each quadrant; (c) Combinations of 4 non-diffracting rings with different phase structure by coding the numbers from 0 to 9.

DETAILED DESCRIPTION OF THE INVENTION

[0034] A control system for controlled access to a user by means of verifying a defined physical element in an optical context and of low level of power, comprising:

[0035] A setup (1) for the creation of arbitrary spatial light patterns, with control of amplitude and phase; including:

[0036] A source of light (9) which emits a LASER beam; toward a first microscope objective (11);

[0037] A spatial light modulation set (2) that receives the light of the first microscope objective (11) and said spatial light modulation set (2) sends a profile modulated in amplitude and phase which form an image to a beam splitter BS (17) that divides the image onto an initial camera CCD (6) and to a second microscope objective (12);

[0038] A defined physical element (7) which receives the initial image from the second microscope objective (12), and transmits the image without diffracting it as a final image to a third microscope objective (13);

[0039] A final camera CCD (8), receives the final image of the third microscope objective (13) and sends it to a computer (300) which compares said final image with the initial image, and performs a calculation of similarity between both images to decide to grant access to the user, if the similarity is greater than a predefined value, and deny it in case if the similarity is less than a predefined value.

[0040] Wherein the whole spatial light modulation (SLM) (2) consists of:

[0041] A first amplitude modulation set (3), formed by polarizers (30, 31), lens (14A, 14b), an obturator (15), a spatial light modulator (16);

[0042] A second phase modulation set (4), formed by wave retardants (40, 41, 42, 43, 44, 45); the spatial light modulator (16), a lens (14C) and mirrors (5b, 5c), wherein the light that comes from the first microscope objective (11) is directed to the first modulator amplitude set (3) wherein it is directed toward the obturator (15), crossing then the lens (14a), and then the polarizer (30) to reach the spatial modulator (16) in which a profile modulated in amplitude is generated. Subsequently this profile modulated in amplitude is transmitted by the polarizer (31), crossing then the lens (14b), the profile modulated in amplitude is redirected in opposite direction by the mirrors (5b, 5c), then said profile modulated in amplitude passes through the second phase modulation set (4) wherein it passes through the wave retardants (45, 44, 43), to reach the spatial light modulator for phase modulation (16) which generates a modulated profile in phase. Later this profile modulated in phase is transmitted by the wave retardants (42, 41, 40), and then it passes through the lens (14c) in order for this image with modulated amplitude and phase is directed to the beam splitter BS (17).

[0043] The profile modulated in amplitude and phase generated in the SLM (2) corresponds to a localized set of beams/points and the first, second, and third microscope objective have an amplification of 20?, 4?, 10?, respectively.

[0044] The defined physical element is a periodic system with non-conventional geometry selected from the group consisting of: photonic crystal, electronic system, cold atoms system in optical lattices, spintronics, quantum dot arrays, micro oscillators arrays, micropillar arrays, chains of proteins.

[0045] In a preferred configuration the photonic crystal (7) is selected from the group that consists of: Crystal of: Lieb, Kagome, Sawtooth, Stub, other non-homogeneous photonic crystals, wherein the photonic crystal (7) which has at least one unitary cell, wherein at least one unitary cell of the photonic crystal (7) is constituted by at least two sites with different interactions at short range. The non-conventional photonic crystal (7) presents, at least, one flat band.

[0046] In another preferred configuration the defined physical element (7) is contained inside of a protective device and light transmitter, which has the form of a cylinder and preferably is flexible, such as an optical fiber.

[0047] In another preferred configuration the protective device and light transmitter is a container box with a mobile part to let the light pass through, which can have various sizes, ideally transportable such as a card, which can be a credit card or identification card.

[0048] A control procedure for controlled access to a user by means of verifying a defined physical element in an optical and low power level context, which consists of the following stages:

[0049] (a) to decide a desired initial image, which is formed in the spatial light modulator (2),

[0050] (b) observing with initial CCD camera (6) the initial image generated in (a), and check that its structure of amplitude and phase matches the desired image. If they do not match, correct the image generated by the spatial light modulator (2) until it matches the desired image;

[0051] (c) passing the modulated light beam through the defined physical element (7);

[0052] (d) observing with final CCD camera (8) the output image from the defined physical element (7);

[0053] (e) comparing with a computer (300) the coincidence of the final image captured with final CCD camera (8) with the initial image captured with initial CCD camera (6) by a calculation of similarity:

[0054] If the similarity is >=P, allow access;

[0055] If the similarity is <P, deny access; and

[0056] Wherein P=75%.

[0057] In another preferred configuration the control procedure for controlled access to a user by means of verifying a defined physical element in an optical and low level of power context is through code, comprising the following stages:

[0058] (a) Entering a defined physical element (7) between the second microscope objective (12) and the third microscope objective (13);

[0059] (b) Typing numeric code in an entry keyboard;

[0060] (c) Comparing with a computer (300), if the pattern transmitted through the defined physical element (7) coincides with the pattern of dots coded into numbers corresponding to the code typed in step (b), if match, the access is granted, otherwise the access is denied.

EXAMPLES OF APPLICATION

Example 1

[0061] Transmission of optically coded information. By the propagation of different images, it is possible to establish a language/code, whose coding and decoding can generate different types of security systems with different levels of reliability.

Example 2

[0062] Transmission of optically coded information. By the propagation of different images, it is possible to establish a logical language/code, which could serve as a basis for generating an optical information stream which will lay the foundations for a hypothetical optical computer.

Example 3

[0063] Locking plate. Associating each propagating light pattern to a letter or a number, it is possible to send and recognize a password, giving way to any security system, in particular a door lock plate, the alarm of a house, a safety deposit box, etc.

Example 4

[0064] Anti-piracy system. Similarly to example 3, it would be possible to use a code to check the veracity of a video game, a movie, etc. If the game disc would have an incorporated photonic crystal, to be inserted in the console might prove the veracity of the game. Illegally copied games would not possess this extra photonic crystal and would not be reproduced.

Example 5

[0065] ATM: Using the present invention as an interface between the user and the Automatic Teller Machine (ATM). To operate a security system using the present invention requires two basic components, an access key and a photonic crystal. Only with the presence of both components an access to ATM could be achieved. The advantage of the photonic crystal is that it could be smaller, and practically cannot be reproduced by any forger. In addition, as it does not have active components as the current magnetic cards, it would be impossible to copy or read the information contained in the crystal at the time of its use.

[0066] It is not possible by the observation of the light propagated without crystal determining the photonic crystal needed to obtain access. Advanced additional information is required in terms of geometries of crystals in physics in order to elucidate and get to deduct the needed crystal to be installed in order to achieve the propagation of the corresponding images. In fact, it is the inventors experience that in dynamics of waves in photonic crystals and skilled persons in the art around the world, that it would be practically impossible to determine the needed particular geometry for the images to be correctly propagated and that can be recognized, without knowing the geometry of the specific lattice. Geometrical or dimensions errors would cause the destruction of the incident image and the non-recognition of the pattern.

[0067] In the exposed examples it can be appreciated a strong analogy between the system of creation of a specific light pattern and a key, and between a non-conventional crystal (having a flat band) and a padlock or lock plate. Through the spatial light modulator (16) we can configure many possible combinations of rings, for example in different zones of the same crystal, allowing a very large number of possible keys for a same crystal (padlock). This would allow coding the information in patterns as complex as required to increase the security of the actuator system.