초록 ▼

Rapid calibration of a TOF system uses a stationary target object and electrically introduces phase shift into the TOF system to emulate target object relocation. Relatively few parameters suffice to model a parameterized mathematical representation of the transfer function between measured phase an

Rapid calibration of a TOF system uses a stationary target object and electrically introduces phase shift into the TOF system to emulate target object relocation. Relatively few parameters suffice to model a parameterized mathematical representation of the transfer function between measured phase and Z distance. The phase-vs-distance model is directly evaluated during actual run-time operation of the TOF system. Preferably modeling includes two components: electrical modeling of phase-vs-distance characteristics that depend upon electrical rather than geometric characteristics of the sensing system, and elliptical modeling that phase-vs-distance characteristics that depending upon geometric rather than electrical characteristics of the sensing system.

대표청구항 ▼

What is claimed is: 1. A method of calibrating a time-of-flight (TOF) system of the type that emits optical energy of a known phase, detects a portion of said optical energy reflected from a target object a distance Z away, and determines Z by examining phase shift in detected reflected optical ene

What is claimed is: 1. A method of calibrating a time-of-flight (TOF) system of the type that emits optical energy of a known phase, detects a portion of said optical energy reflected from a target object a distance Z away, and determines Z by examining phase shift in detected reflected optical energy relative to said known phase of emitted optical energy, the method comprising the following steps: (a) disposing a target object a distance Zx from said TOF system, said distance Zx being within operating distance range of said TOF system; (b) altering said known phase of said emitted optical energy by at least two known phase values; (c) for each known phase value of said emitted optical energy, determining from detected reflected optical energy a corresponding phase shift relative to said known phase; (d) using corresponding relative phase shift determined at step (c) to form an electrical model of detection characteristics of said TOF system; (e) storing data representing said electrical model; wherein data stored at step (e) is useable during run-time operation of said TOF system to provide calibrated values of Z responsive to phase shift in detected reflected optical energy. 2. The method of claim 1, where said Zx is a shortest distance Zf whereat elliptical error arising from geometry of phase detection of said TOF system is negligible. 3. The method of claim 1, wherein step (b) includes sweeping said first phase with incremental values of phase having at least one characteristic selected from a group consisting of (i) increments between each of said phase values are equal in magnitude, (ii) increments between at least some of said phase values have different magnitude, and (iii) sweeping encompasses substantially a range of about 0° to about 360°. 4. The method of claim 1, wherein step (e) includes storing said data representing said electrical model within said TOF system. 5. The method of claim 1, wherein step (d) includes forming said electrical model as a parametric function characterized by at least two parameters. 6. The method of claim 1, wherein step (b) includes sweeping said known phase with incremental values of phase exceeding 360°, and wherein step (d) includes unwrapping relative phase shift determined at step (c) to avoid distance ambiguity. 7. The method of claim 1, wherein said model formed at step (d) includes a linear factor and a sinusoid factor. 8. The method of claim 1, wherein: said TOF system includes an array of detectors; said model formed at step (d) approximates Z =ZUDij·[p+mij+Aijsin(sijp+2πfp)], where at least two parameters of ZUDij, mij, Aij, and sij are per detector parameters, f is a global TOF system parameter, and p is phase. 9. The method of claim 1, further including a step of dealiasing phase shift in said detected reflected optical energy, whereby said electrical model formed at step (d) is useable during run-time operation of said TOF system for unwrapped phase exceeding 360°. 10. The method of claim 1, wherein step (d) further includes forming an elliptical error model to correct phase-vs-distance data for geometric characteristics of said TOF system. 11. The method of claim 10, wherein said elliptical model formed at step (d) is useable when Z<Zf, where Zf is a shortest distance at which elliptical error for said TOF system is negligible. 12. The method of claim 10, wherein forming an elliptical error model includes the following steps: (i) disposing a target object at at least one distance ZyZ<f from said TOF system, where Zf is a shortest distance whereat elliptical error arising from geometry of phase detection of said TOF system is negligible; (ii) for each said distance Zy, determining from detected reflected optical energy a corresponding phase shift relative to said known phase; (iii) for each said distance Zy, obtaining a phase value from said electrical model formed at step (d); (iv) obtaining a difference in phase value between phase determined at step (ii) and phase obtained from step (iii), and using said difference in phase to form an elliptical error model; wherein said elliptical error model is useable during run-time operation of said TOF system to provide improved calibrated values of Z<Zf responsive to phase shift in detected reflected optical energy. 13. The method of claim 12, wherein step (iv) includes forming said elliptical error model as a parametric function. 14. A method of improving elliptical error calibration in a time-of-flight (TOF) system of the type that emits optical energy of a known phase, detects a portion of said optical energy reflected from a target object a distance Z away, and determines Z by examining phase shift in detected reflected optical energy relative to said known phase of emitted optical energy, the method comprising the following steps: (i) disposing a target object at at least one distance Zy<Zf from said TOF system, where Zf is a shortest distance whereat elliptical error arising from geometry of phase detection of said TOF system is negligible; (ii) for each said distance Zy determining from detected, reflected optical energy a corresponding phase shift relative to said known phase; (iii) for each said distance Zy, obtaining a phase value from an electrical model of phase-vs-distance formed for said TOF system; (iv) obtaining a difference in phase value between phase determined at step (ii) and phase obtained from step (iii), and using said difference in phase to form an elliptical error model; wherein said elliptical error model is useable during run-time operation of said TOF system to provide improved calibrated values of Z<Zf responsive to phase shift in detected reflected optical energy. 15. The method of claim 14, wherein step (iv) includes forming said elliptical error model as a parametric function. 16. The method of claim 14, wherein step (iv) includes storing said elliptical error model in memory useable by said TOF system during run-time operation of said TOF system. 17. A time-of-flight (TOF) system of the type that emits optical energy of a known phase, detects a portion of said optical energy reflected from a target object a distance Z away, and determines Z by examining phase shift in detected reflected optical energy relative to said known phase of emitted optical energy, the TOF including means for altering known phase emitted by said TOE system, and further including memory storing a distance-vs-phase calibration model used to calibrate said TOF system, said calibration model obtained according to a method comprising the following steps: (a) disposing a target object a distance Zx from said TOF system, said distance Zx being within operating distance range of said TOF system; (b) causing said means for altering known phase to vary said known phase of said emitted optical energy by at least two known phase values; (c) for each known phase value of said emitted optical energy, determining from detected reflected optical energy a corresponding phase shift relative to said known phase; (d) using corresponding relative phase shift determined at step (c) to form an electrical model of detection characteristics of said TOE system; (e) storing data representing said electrical model in said memory; wherein data stored in memory at step (e) is useable during run-time operation of said TOF system to provide calibrated values of Z responsive to phase shift in detected reflected optical energy. 18. The TOF system of claim 17, wherein at step (a), said Zx is a shortest distance Zf whereat elliptical error arising from geometry of phase detection of said TOF system is negligible. 19. The TOF system of claim 17, wherein said memory further includes an elliptical model of detection characteristics of said TOF system that are substantially independent of electrical characteristics, said elliptical model being used at distances Z<Zf, where Zf is a shortest distance at which elliptical error is substantially negligible. 20. The TOF system of claim 19, wherein said elliptical model of detection characteristics stored in said memory is formed as follows: (i) disposing a target object at at least one distance Zy<Zf from said TOF system, where Zf is a shortest distance whereat elliptical error arising from geometry of phase detection of said TOE system is negligible; (ii) for each said distance Zy, determine from detected reflected optical energy a corresponding phase shift relative to said known phase; (iii) for each said distance Zy, obtain a phase value from said electrical model formed at step (d); (iv) obtain a difference in phase value between phase determined at step (ii) and phase obtained from step (iii), and use said difference in phase to form an elliptical error model; wherein said elliptical error model is useable during run-time operation of said TOF system to provide improved calibrated values of Z<Zf responsive to phase shift in detected reflected optical energy.