Optical control system with modulated emitters

• US 8,227,742 B2
• Filed: 08/07/2009
• Issued: 07/24/2012
• Est. Priority Date: 08/07/2008
• Status: Active Grant

• Current Assignee: Beechrock Limited
• Original Assignee: Rapt Ip Limited
• Inventors: Drumm, Owen
• Primary Examiner(s): PYO, KEVIN K
• Application Number:
  US13/059,772
• Publication Number:
  US 20110147569A1
• Time in Patent Office: 1,082 Days
• Field of Search: 250/221, 250/216, 250/206.1, 345/156, 345/173, 345/175, 345/176, 178/18.03, 178/18.09, 341/31
• US Class Current: 250/221
• CPC Class Codes: G06F 2203/04109 FTIR in optical digitiser, i.e. touch detection by frustrating the total internal reflection within an optical waveguide due to changes of optical properties or deformation at the touch location
• CPC Class Codes: G06F 3/0421 by interrupting or reflecting a light beam, e.g. optical touch-screen

Abstract

An optical control system is described, which employs a series of optical emitters and detectors arranged about a touch area. The emitters are driven by a series of orthogonal functions, and the system is operable to correlate the signals received at the detectors with the modulation functions to determine the amount of energy received by the detectors from each of the emitters. This system means that all or many emitters can be modulated simultaneously, so the scanning process is accelerated. Also, the energy estimates arrived at by correlation with the modulating functions are largely unaffected by external interference signals as well by each other. An additional benefit of the present invention is that the correlation processing makes use of many detector samples and tends to yield results which have higher resolution than the sample values themselves, due to the averaging of noise over the sample set.

Claims

1. An optical control system comprising:

a plurality of optical emitters and a plurality of optical detectors defining therebetween an area of optical paths whereby the transmission of energy between an emitter and a detector may be modulated by an optical interaction occurring in the vicinity of said area, wherein at least one of said detectors is positioned to receive optical energy from more than one of said optical emitters;

drive circuitry for driving a plurality of said optical emitters simultaneously according to a modulation scheme in which each emitter is modulated with a different modulation function, said functions being orthogonal relative to one another;

correlation means associated with said at least one detector for receiving an output therefrom and for correlating said output with at least those modulation functions driving the emitters which said at least one detector is positioned to receive optical energy from, to thereby determine the amount of energy incident on said at least one detector from each of said emitters.

2. An optical control system as claimed in claim 1, further comprising a memory for storing said modulation scheme, said memory being accessible to said drive circuitry.

3. An optical control system as claimed in claim 2, wherein said modulation functions are selected to ensure that the number of emitters active at any given time according to said modulation scheme is below a predetermined maximum.

4. An optical control system as claimed in claim 3, wherein said modulation functions are selected as an optimum set of orthogonal functions of length N for driving said plurality of emitters through a sequence of N states, wherein the set is optimised to provide the minimum possible simultaneous number of active emitters during said sequence of N states.

5. An optical control system as claimed in claim 1, wherein said drive circuitry further comprises a variable timing mechanism for varying the timing of successive emitter activations to an aperiodic frequency.

6. An optical control system as claimed in claim 5, wherein the receipt of detector output samples is further timed according to the varied timing provided by said variable timing mechanism.

7. An optical control system as claimed in claim 1, further comprising a noise detection mechanism for sampling said detector output before and after one or more associated emitters are activated to determine noise levels before and after activation, and for interpolating a noise value at a point in time during said activation when the detector is sampled to determine the energy incident thereon from the one or more associated emitters.

8. An optical control system as claimed in claim 7, wherein said noise detection mechanism is operable to sample said detector output once before each activation of the emitters, the interpolation being carried out between the sample before two successive activations.

9. An optical control system as claimed in claim 7, wherein an output from said noise detection mechanism is used to determine an emitter power level.

10. An optical control system as claimed in claim 7, wherein an output from said noise detection mechanism is used to determine whether an error condition exists due to excessive noise.

11. A method of operating an optical control system having a plurality of optical emitters and a plurality of optical detectors defining therebetween an area of optical paths whereby the transmission of energy between an emitter and a detector may be modulated by an optical interaction occurring in the vicinity of said area, wherein at least one of said detectors is positioned to receive optical energy from more than one of said optical emitters, the method comprising the steps of:

driving a plurality of said optical emitters simultaneously according to a modulation scheme in which each emitter is modulated with a different modulation function, said functions being orthogonal relative to one another;

receiving an output from said at least one detector;

correlating said output with at least those modulation functions driving the emitters which said at least one detector is positioned to receive optical energy from, to thereby determine the amount of energy incident on said at least one detector from each of said emitters.