UV-Visible Lasers Based on Rare-Earth Ions

An issue on novel applications of materials doped with rare-earth (RE) ions can scarcely fail to address lasers, but it need not address all RE-based lasers. Some Nd 3+ -doped lasers, particularly Nd:YAG (Y 3 Al 5 O 12 , yttrium aluminum garnet), emitting light with a wavelength of 1064 nm, are very well-established commercial products—by no means novelties.1 Some other near-infrared (NIR) lasers, based on Er 3+ or Tm 3+ , are also available commercially. That wavelength region is relatively easy for RE laser ions, involving energy spacings between initial and final energy levels small enough to give large stimulated emission cross sections for useful, long upper-state life-times, yet large enough to minimize thermal deexcitation mechanisms. On the other hand, RE-doped lasers for ultraviolet (UV) and visible wavelengths are quite novel, since efficient laser operation is more difficult to achieve in these spectral ranges. Intriguing progress on such devices has been made in recent years, driven by several important applications. In this article, we begin by noting some of the alternative ways to obtain laser light at these wavelengths, including their advantages and drawbacks. We then discuss basic properties of RE-doped laser materials and how these can be advantageous. We then review a few of the most important and recent RE-doped laser materials and techniques for obtaining UV and visible output.

[1]  E. Heumann,et al.  Green Er(3+):YLiF(4) upconversion laser at 551nm with Yb(3+) codoping: a novel pumping scheme. , 1997, Optics letters.

[2]  D. Shepherd,et al.  Laser operation of an Nd:Gd3Ga5O12 thin‐film optical waveguide fabricated by pulsed laser deposition , 1996 .

[3]  B. Offrein,et al.  Nonlinear refractive index of erbium-doped Y(2)O(3) integrated-optical waveguides. , 1993, Optics letters.

[4]  François Salin,et al.  Linear- and nonlinear-optical properties of a new gadolinium calcium oxoborate crystal, Ca 4 GdO(BO 3 ) 3 , 1997 .

[5]  Leslie Brandon Shaw,et al.  A 7-/spl mu/m praseodymium-based solid-state laser , 1996 .

[6]  D. Shepherd,et al.  Laser operation of a Nd:LaF3 thin film grown by molecular-beam epitaxy , 1999 .

[7]  Georges Boulon,et al.  Spectroscopic investigation of Nd3+ ion in LiNbO3, MgO:LiNbO3 and LiTaO3 single crystals relevant for laser applications , 1996 .

[8]  William F. Krupke,et al.  Ultraviolet laser emission properties of Ce 3+ -doped LiSrAlF 6 and LiCaAlF 6 , 1994 .

[9]  L. L. Holladay Action of a Light-Source in the Field of View in Lowering Visibility , 1927 .

[10]  T. R. Gosnell,et al.  Room-temperature upconversion fiber laser tunable in the red, orange, green, and blue spectral regions. , 1995, Optics letters.

[11]  R. Scheps Upconversion laser processes , 1996 .

[12]  E. Lallier,et al.  Nd:MgO:LiNbO/sub 3/ channel waveguide laser devices , 1991 .

[13]  Christian Pedrini,et al.  Efficient and stable pulsed laser operation of Ce:LiLuF4 around 308 nm , 1998 .

[14]  L. Johnson,et al.  Upconversion laser emission from Yb 3+ -sensitized Tm 3+ in BaY 2 F 8 , 1994 .

[15]  Hiroyuki Furuya,et al.  Crystal Growth and Optical Characterization of Rare-Earth (Re) Calcium Oxyborate ReCa4O(BO3)3 (Re=Y or Gd) as New Nonlinear Optical Material , 1997 .

[16]  James Gary Eden,et al.  Ultraviolet (381 nm), room temperature laser in neodymium-doped fluorozirconate fibre , 1994 .

[17]  Robert S. Feigelson,et al.  Pulling optical fibers , 1986 .

[18]  N Sarukura,et al.  All-Solid-State Tunable Ultraviolet Subnanosecond Laser with Direct Pumping by the Fifth Harmonic of a Nd:YAG laser. , 1998, Applied optics.

[19]  M. Joubert,et al.  Photon avalanche upconversion in rare earth laser materials , 1999 .

[20]  Steven T. Davey,et al.  Low threshold, diode pumped operation of a green, Er/sup 3+/ doped fluoride fibre laser , 1993 .

[21]  S. Field,et al.  Growth and low-threshold laser oscillation of an epitaxially grown Nd:YAG waveguide. , 1992, Optics letters.

[22]  R. Waynant,et al.  Vacuum ultraviolet laser emission from Nd+3:LaF3 , 1985 .

[23]  M. J. Stevenson,et al.  SPECTROSCOPY AND OPTICAL MASER ACTION IN SrF$sub 2$:Sm$sup 2$$sup +$ , 1962 .

[24]  M. Imaeda,et al.  Homogeneity and SHG properties of K3Li2 − xNb5 + xO15 + 2x single crystals grown by micro-pulling-down technique , 1997 .

[25]  Michel J. F. Digonnet,et al.  Nd:MgO:LiNbO 3 spectroscopy and laser devices , 1986 .

[26]  C. Garrett,et al.  FLUORESCENCE AND OPTICAL MASER EFFECTS IN CaF$sub 2$: Sm$sup +$$sup +$ , 1961 .

[27]  Ishwar D. Aggarwal,et al.  High power upconversion lasing at 810 nm, in Tm:ZBLAN fibre , 1994 .

[28]  Alexander K. Naumov,et al.  Ce3+-doped colquiriite : a new concept of all-solid-state tunable ultraviolet laser , 1993 .

[29]  Leon Esterowitz,et al.  High performance Ce3+:LiSrAlF6/LiCaAlF6 UV lasers with extended tunability , 1995 .

[30]  Helen M. Pask,et al.  Practical 580 nm source based on frequency doubling of an intracavity-Raman-shifted Nd:YAG laser , 1998 .