Abstract
The existence of the spherical aberration of the thermal lens in the crystal has a certain regulatory effect on the distribution of laser modes. In this paper, using the impact of this aberration on the superposition area of TEM01 and TEM10 modes, we carry out an experimental study of a 1064 nm hollow beam and its nonlinear frequency conversion providing a 532 nm hollow beam. Using a plano-concave cavity structure, under 21.92 W pump power at 808 nm, a 1064 nm hollow beam with an output power of 4.01 W is generated. Based on this result, a 532 nm hollow beam with an output power of 1.08 W is obtained by intracavity frequency doubling with type I phase matching in an LBO crystal. The conversion efficiency is 26.9%.
This is a preview of subscription content, log in via an institution to check access.
Similar content being viewed by others
References
A. Stein, IEEE J. Quantum Electron., 10, 427 (1974).
Y. Lumer, I. Moshe, S. Jackel, and A. Meir, J. Opt. Soc. Am. B, 27, 1337 (2010).
Z. Zhao, Y. Dong, S. Pan, et al., Chin. J. Lasers, 37, 2409 (2010).
V. Magni, Appl. Opt., 25, 2039 (1986).
S. De Silvestri, P. Laporta, and V. Magni, Opt. Commun., 59, 43 (1986).
C. Liu, J. H. Ge, Z. Xiang, and J. Chen, Acta Phys. Sin., 57, 1704 (2008).
Z. Zhao, S. Pan, Z. Xiang, et al., Opt. Express, 20, 10605 (2012).
R. M. Herd and J. S. Dover, Dermatol. Clin., 15, 355 (1997).
J. Frauchiger and H. P. Weber, Proc. SPIE, 1865, 74 (1993).
M. W. Beijersbergen, R. P. C. Coerwinkel, M. Kristensen, and J. P. Woerdman, Opt. Commun., 112, 321 (1994).
A. Jesacher, C. Maurer, A. Schwaighofer, et al., Opt. Express, 16, 2597 (2008).
N. Gonzlez, G. Molina-Terriza, and J. P. Torres, Opt. Express, 14, 9093 (2006).
L. Carbone, C. Bogan, P. Fulda, et al., Phys. Rev. Lett., 110, 251101 (2013).
Z. Rong, C. Kuang, Y. Fang, et al., Opt. Commun., 354, 71 (2015).
T. H. Kim, J. S. Park, J. W. Kim, et al., J. Korean Phys. Soc., 75, 557 (2019).
D. Pohl, Appl. Phys. Lett., 20, 266 (1972).
Y. Kozawa and S. Sato, Opt. Lett., 30, 3063 (2005).
G. Machavariani, Y. Lumer, I. Moshe, et al., Appl. Opt., 46, 3304 (2007).
K. Yonezawa, Y. Kozawa, and S. Sato, Jpn. J. Appl. Phys., 46, 5160 (2014).
M. A. Ahmed, A. Voss, M. M. Vogel, and T. Graf, Opt. Lett., 32, 3272 (2007).
Chr. Tamm and C. O. Weiss, J. Opt. Soc. Am. B, 7, 1034 (1990).
G. A. Turnbull, D. A. Robertson, G. M. Smith, et al., Opt. Commun., 127, 183 (1996).
M. V. Berry, J. Opt. A: Pure Appl. Opt., 5, 259 (2004).
S. P. Chard, P. C. Shardlow, and M. J. Damzen, Appl. Phys. B: Lasers Opt., 97, 275 (2009).
X. Huang, B. Xu, and S. Cui, IEEE J. Sel. Top. Quantum Electron., 24, 1 (2018).
K. Dholakia, N. B. Simpson, M. J. Padgett, and L. Allen, Phys. Rev. A, 54, R3742 (1996).
J. Courtial, K. Dholakia, L. Allen, and M. J. Padgett, Phys. Rev. A, 56, 4193 (1997).
W. T. Buono, L. F. C. Moraes, J. A. O. Huguenin, et al., New J. Phys., 16, 093041 (2014).
Z. Y. Zhou, D. S. Ding, Y. K. Jiang, et al., Opt. Express, 22, 20298 (2014).
Author information
Authors and Affiliations
Corresponding author
Rights and permissions
About this article
Cite this article
Wang, L., Jin, GY., Dong, Y. et al. Generation of a 532 nm Hollow Beam by Adjusting the Superposition Area of TEM01 and TEM10 Modes by Spherical Aberration of the Thermal Lens. J Russ Laser Res 42, 75–81 (2021). https://doi.org/10.1007/s10946-020-09931-4
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s10946-020-09931-4