Beam shaping with a plano-aspheric lens pair

A pair of plano-aspheric lenses can be used to transform a collimated, radially symmetric, Gaussian beam to a radially symmetric flat-top beam. Diffraction of the output beam due to the choice of irradiance profile, as well as the finite aperture of the optics, must be considered if a propagating beam is required. Choosing both lenses to be positive, one can show that the aspheric surfaces are strictly convex, which facilitates fabrication by magnetorheological figuring. A fused silica lens pair is demonstrated, which can be used at any wavelength from 250 to 1550 nm to transform a Gaussian to a flat-top beam. Measurements of both the irradiance profile and phase of the output beam are presented and compared to the ideal design. These optics transform 78% of the total input beam power into the flat-top region of the output beam, which is uniform to better than 5% rms. For applications requiring uniform illumination, this represents a fourfold improvement in power utilization over the Gaussian input. The output wavefront is flat to a quarter wave at 514 nm, resulting in a beam that propagates approximately 0.5 m without significant change in profile.

[1]  William Kordonski,et al.  Magnetorheological finishing (MRF) in commercial precision optics manufacturing , 1999, Optics + Photonics.

[2]  Anthony E. Siegman,et al.  New developments in laser resonators , 1990, Photonics West - Lasers and Applications in Science and Engineering.

[3]  Geoffrey W. Burr,et al.  IBM Holographic Digital Data Storage Test Platforms , 2000 .

[4]  Fred M. Dickey,et al.  Gaussian laser beam profile shaping , 1996 .

[5]  Louis A. Romero,et al.  Lossless laser beam shaping , 1996 .

[6]  B. Frieden,et al.  Lossless conversion of a plane laser wave to a plane wave of uniform irradiance. , 1965 .

[7]  C. M. Jefferson,et al.  Design and performance of a refractive optical system that converts a Gaussian to a flattop beam. , 2000, Applied optics.

[8]  R. Burnham,et al.  Near-diffraction-limited laser beam shaping with diamond-turned aspheric optics. , 1997, Optics letters.

[9]  J. Shapiro Holographic generation of squeezed states , 1996 .

[10]  N. Kristianpoller,et al.  Optical Properties of “Liumogen”: A Phosphor for Wavelength Conversion , 1964 .

[11]  D L Shealy,et al.  Refractive optical systems for irradiance redistribution of collimated radiation: their design and analysis. , 1980, Applied optics.

[12]  David L. Shealy,et al.  Design and testing of a refractive reshaping system , 1993, Optics & Photonics.

[13]  Franco Gori,et al.  Shape-invariance error for axially symmetric light beams , 1998 .

[14]  Fred M. Dickey,et al.  Gaussian Beam Shaping: Diffraction Theory and Design , 2000 .

[15]  John A. Hoffnagle Sensitivity of a refractive beam reshaper to figure error , 2002, SPIE Optics + Photonics.

[16]  Franco Gori,et al.  Flattened gaussian beams , 1994 .

[17]  M. Morin,et al.  Propagation of super-Gaussian field distributions , 1992 .

[18]  David L. Shealy,et al.  Optical design and testing of a holographic projection system , 1994, Photonics West - Lasers and Applications in Science and Engineering.

[19]  John A. Hoffnagle,et al.  Measured performance of a refractive Gauss-to-flattop reshaper for deep-UV through near-IR wavelengths , 2001, Optics + Photonics.

[20]  F. Gori,et al.  Shape-invariance range of a light beam. , 1996, Optics letters.