Extended depth of field optical systems

• US 8,004,762 B2
• Filed: 10/13/2008
• Issued: 08/23/2011
• Est. Priority Date: 02/03/1995
• Status: Expired due to Term

• Current Assignee: The Board of Regents of the University of Colorado (University of Colorado System)
• Original Assignee: The Board of Regents of the University of Colorado (University of Colorado System)
• Inventors: Dowski, Edward Raymond Jr., Cathey, Wade Thomas Jr.
• Primary Examiner(s): Chang; Audrey Y
• Application Number:
  US12/250,343
• Publication Number:
  US 20090109535A1
• Time in Patent Office: 1,044 Days
• Field of Search: 359/558, 382/232, 382/254
• US Class Current: 359/558
• CPC Class Codes: G01S 11/12 using electromagnetic waves other than radio waves
• CPC Class Codes: G01S 3/7835 using coding masks
• CPC Class Codes: G02B 21/14 affording illumination for phase-contrast observation
• CPC Class Codes: G02B 27/0025 for optical correction, e.g. distorsion, aberration
• CPC Class Codes: G02B 27/46 Systems using spatial filters
• CPC Class Codes: G02B 27/52 Phase contrast optics in microscopes G02B21/14
• CPC Class Codes: G02B 5/00 Optical elements other than lenses light guides G02B6/00; optical logic elements G02F3/00
• CPC Class Codes: G02B 7/365 by analysis of the spatial frequency components of the image
• CPC Class Codes: G02B 7/40 using time delay of the reflected waves, e.g. of ultrasonic waves

Abstract

Systems and methods for generating an optical image include forming an optical image with at least one optical element of an optical imager while modifying wavefront phase. Modifying the phase does not reduce an optical bandpass limited by an aperture of the optical imager. The systems and methods also include detecting the optical image over a range of spatial frequencies such that there are no zeros in an optical transfer function of the optical imager over detected spatial frequencies within the optical bandpass and over an extended depth of focus that is larger than a depth of focus occurring without modifying wavefront phase.

Claims

1. A method for generating an optical image, comprising:

forming an optical image with at least one optical element of an optical imaging system while modifying wavefront phase, wherein modifying wavefront phase comprises imparting one of a linear phase modulation and a cubic phase modulation to a wavefront forming the optical image, and

detecting the optical image over a range of spatial frequencies such that there are no zeros in an optical transfer function of the optical imaging system over detected spatial frequencies within the optical bandpass over an extended depth of focus that is larger than a depth of focus occurring without modifying wavefront phase.

2. A system for forming an image, comprising

a lens and one or more phase masks that cooperate to form an optical image characterized by an optical transfer function that has no zeros within detected spatial frequencies of a detector that detects the optical image over a larger depth of focus than without the one or more phase masks, wherein the one or more phase masks do not reduce an optical bandpass limited by an aperture of the lens or of the phase masks,

the one or more phase masks imparting one of a linear phase modulation and a cubic phase modulation.

3. An extended depth of field optical system, comprising:

optics for imaging electromagnetic energy, the optics forming an optical aperture through which the electromagnetic energy passes, the optics and the aperture limiting an optical bandpass of the optical system; and

one or more phase masks that modify phase but not amplitude of the electromagnetic energy, such that the one or more phase masks, the optics and the aperture are characterized by a modified optical transfer function that has no zeroes (a) within the optical bandpass and (b) over a wider range of misfocus values than an unmodified optical transfer function characterizing the aperture and the optics alone, the one or more phase masks imparting one of a linear phase modulation and a cubic phase modulation.

4. In an optical system having optics for imaging electromagnetic energy, the optics forming an aperture through which the electromagnetic energy passes, the optics and the aperture limiting an optical bandpass of the optical system, an unmodified optical transfer function characterizing the aperture and the optics alone, an improvement comprising:

a phase mask that modifies phase but not amplitude of the electromagnetic energy, and that cooperates with the aperture and the optics such that the optical system with the phase mask is characterized by a modified optical transfer function that has no zeroes within the optical bandpass, and over a wider range of misfocus values than the unmodified optical transfer function, the phase mask imparting one of a linear phase modulation and a cubic phase modulation.