Complex holographic elements in photo-thermo-refractive glass for the visible spectral region

Planar holographic optical elements (volume Bragg gratings, VBGs) recorded in photo-thermo-refractive (PTR) glass are widely used for fine spectral filtering and laser beam control. PTR glass provides photosensitivity in near UV region. Therefore, while planar holographic elements operate in the whole window of transparency - near UV, visible and near IR spectral regions, application of complex (nonplanar) elements is restricted to near UV. A method has been proposed to create high-efficiency diffractive optical elements in PTR glass using visible light. The method employs excited state absorption in PTR glass doped with Tb3+. UV radiation was used for excitation to a metastable level of Tb3+ and pulsed radiation at 532 nm was used for hologram recording. Both planar VBGs and holographic lenses operating at 532 nm were demonstrated. Complex holographic optical elements in PTR glass can provide attractive solutions for lasers and spectroscopy replacing conventional optical components.

[1]  Leonid B. Glebov,et al.  Holographically encoded volume phase masks , 2015 .

[2]  L. B. Glebov Photochromic and Photo‐Thermo‐Refractive Glasses , 2002 .

[3]  V. Smirnov,et al.  Spectral Combining and Coherent Coupling of Lasers by Volume Bragg Gratings , 2009, IEEE Journal of Selected Topics in Quantum Electronics.

[4]  Leonid B. Glebov Volume Holographic Elements in a Photo-Thermo-Refractive Glass , 2009 .

[5]  Thomas D. Wilkerson,et al.  Holographic Optical Elements as Scanning Lidar Telescopes , 2006 .

[6]  D. Macquigg,et al.  Hologram fringe stabilization method. , 1977, Applied optics.

[7]  Vadim Smirnov,et al.  Volume-chirped Bragg gratings: monolithic components for stretching and compression of ultrashort laser pulses , 2014 .

[8]  Vadim Smirnov,et al.  Longitudinal mode selection in laser cavity by moiré volume Bragg grating , 2012, LASE.

[9]  L. Glebov,et al.  Measurement of the induced refractive index in a photothermorefractive glass by a liquid-cell shearing interferometer. , 2002, Applied optics.

[10]  Dichromated gelatin for volume holographic recording with high sensitivity. Part I , 1982 .

[11]  D. H. Close Holographic Optical Elements , 1975 .

[12]  Xuelu Zou,et al.  Spectroscopic properties and mechanisms of excited state absorption and energy transfer upconversion for Er3+-doped glasses , 1993 .

[13]  B. J. Chang,et al.  Dichromated gelatin for the fabrication of holographic optical elements. , 1979, Applied optics.

[14]  Igor V. Ciapurin,et al.  New approach to robust optics for HEL systems , 2002, SPIE Defense + Commercial Sensing.

[15]  C. Thiel,et al.  PHOTONIC MATERIALS AND DEVICES Progress in relating rare-earth ion 4f and 5d energy levels to host bands in optical materials for hole burning, quantum information and phosphors , 2002 .

[16]  P. Dorenbos The 5d level positions of the trivalent lanthanides in inorganic compounds , 2000 .

[17]  R. R. A. Syms,et al.  Practical volume holography , 1990 .

[18]  K. Biswas,et al.  Concentration Dependent Luminescence of Tb3+ ions inhigh Calcium-Alumino-Silicate Glasses , 2009 .

[19]  Leonid Glebov High-Performance Solid-State and Fiber Lasers Controlled by Volume Bragg Gratings , 2013 .

[20]  Vadim Smirnov,et al.  Volume Bragg gratings as ultra-narrow and multiband optical filters , 2012, Photonics Europe.

[21]  Krut Schwartz,et al.  The Physics of Optical Recording , 1994 .

[22]  Leonid B. Glebov,et al.  Photo-thermo-refractive glass with sensitivity to visible and near IR radiation , 2016 .

[23]  F. Auzel Upconversion and anti-Stokes processes with f and d ions in solids. , 2004, Chemical reviews.