Abstract:Lasing-relevant processing and physical properties of Yb-doped Ca3(NbGa)5O12-CNGG-type disordered garnet crystals are discussed. Future directions for Yb3+ bandwidth and laser performance improvements are foreseen.
“…These obtained results were superior to the previously reported values for CNGG crystals (55.08′′). 15 Furthermore, the quality of our Yb:CNGG crystal was also comparable to large-sized garnet crystals, such as Yb:YAG (approximately 36.00′′), 27 Yb:GGG (37.00′′), 28 and Yb:GAGG (43.34′′), 29 which further confirms the importance of optimizing the temperature field during high-quality crystal growth, especially if the goal is to grow large-sized crystals.…”
Section: Resultssupporting
confidence: 71%
“…Such a disordered coordination structure results in an abundance of Yb 3+ ions in the local coordination environment. 15,[23][24][25] XRPD analysis was employed to investigate the crystalline phase of the as-grown Yb:CNGG crystal. As depicted in Fig.…”
Section: Crystal Structure and Chemical Compositionmentioning
confidence: 99%
“…The Yb doping concentration was determined to be 1.12 at% with a segregation coefficient of 0.93, which is slightly lower than the literature value of 1.12. 15 Furthermore, the chemical formula of the bulk crystal was Yb 0.032 Ca 2.855 -Nb 1.611 Ga 3.379 O 12 , which was consistent with the refined result (Yb 0.033 Ca 2.855 Nb 1.665 Ga 3.045 O 12 ), but exhibited a slight compositional deviation from previously reported highly doped Yb:CNGG crystals (Yb 0.475 Ca 2.514 Nb 1.269 Ga 3.505 O 12 ). 14 Specifically, the content of Nb 5+ ions in our as-grown Yb: CNGG was more similar to the stoichiometric ratio than to that of the highly doped Yb:CNGG crystal.…”
Section: Crystal Structure and Chemical Compositionmentioning
confidence: 99%
“…Previous crystal growth on Yb:CNGG was typically concentrated in a size less than Φ30 mm, [12][13][14] and numerous studies were performed to examine the local coordination structure, spectral broadening mechanisms, continuous-wave lasers, and ultrafast lasers. 13,15,16 However, the crystal size of the laser gain media applied in the amplification systems of high-energy lasers typically necessitates a diameter of Φ50 mm or larger, thereby creating an urgent demand for the growth of large-sized Yb:CNGG crystals with high quality.…”
High-energy solid-state pulsed lasers arouse intriguing applications in various fields, typically requiring the amplification gain media with large dimensions, low pump saturation density, moderate emission saturation flux, and superior energy...
“…These obtained results were superior to the previously reported values for CNGG crystals (55.08′′). 15 Furthermore, the quality of our Yb:CNGG crystal was also comparable to large-sized garnet crystals, such as Yb:YAG (approximately 36.00′′), 27 Yb:GGG (37.00′′), 28 and Yb:GAGG (43.34′′), 29 which further confirms the importance of optimizing the temperature field during high-quality crystal growth, especially if the goal is to grow large-sized crystals.…”
Section: Resultssupporting
confidence: 71%
“…Such a disordered coordination structure results in an abundance of Yb 3+ ions in the local coordination environment. 15,[23][24][25] XRPD analysis was employed to investigate the crystalline phase of the as-grown Yb:CNGG crystal. As depicted in Fig.…”
Section: Crystal Structure and Chemical Compositionmentioning
confidence: 99%
“…The Yb doping concentration was determined to be 1.12 at% with a segregation coefficient of 0.93, which is slightly lower than the literature value of 1.12. 15 Furthermore, the chemical formula of the bulk crystal was Yb 0.032 Ca 2.855 -Nb 1.611 Ga 3.379 O 12 , which was consistent with the refined result (Yb 0.033 Ca 2.855 Nb 1.665 Ga 3.045 O 12 ), but exhibited a slight compositional deviation from previously reported highly doped Yb:CNGG crystals (Yb 0.475 Ca 2.514 Nb 1.269 Ga 3.505 O 12 ). 14 Specifically, the content of Nb 5+ ions in our as-grown Yb: CNGG was more similar to the stoichiometric ratio than to that of the highly doped Yb:CNGG crystal.…”
Section: Crystal Structure and Chemical Compositionmentioning
confidence: 99%
“…Previous crystal growth on Yb:CNGG was typically concentrated in a size less than Φ30 mm, [12][13][14] and numerous studies were performed to examine the local coordination structure, spectral broadening mechanisms, continuous-wave lasers, and ultrafast lasers. 13,15,16 However, the crystal size of the laser gain media applied in the amplification systems of high-energy lasers typically necessitates a diameter of Φ50 mm or larger, thereby creating an urgent demand for the growth of large-sized Yb:CNGG crystals with high quality.…”
High-energy solid-state pulsed lasers arouse intriguing applications in various fields, typically requiring the amplification gain media with large dimensions, low pump saturation density, moderate emission saturation flux, and superior energy...
“…CaCO 3 (99.95% purity), Li 2 CO 3 (99.998 purity), Nb 2 O 5 (99.9985% purity), Ga 2 O 3 , Nd 2 O 3 , and Yb 2 O 3 (of 5N purity) were used as raw materials. Considering that Nd 3+ and Yb 3+ dopant ions replace Ca 2+ ions in the CLNGG host matrix and the values of the effective segregation coefficients (k eff ) of Nd 3+ and Yb 3+ in the CLNGG crystal are 0.55 [7] and 0.91 [17], respectively, the chemical compositions of the starting materials were established to be 1.28-at.% Nd:CLNGG and 8-at.% Yb:CLNGG, respectively. The raw materials were weighed according to the chemical equations:…”
Buried depressed-cladding waveguides were fabricated in 0.7-at.% Nd:Ca3Li0.275Nb1.775Ga2.95O12 (Nd:CLNGG) and 7.28-at.% Yb:CLNGG disordered laser crystals grown by Czochralski method. Circular waveguides with 100 μm diameters were inscribed in both crystals with picosecond (ps) laser pulses at 532 nm of 0.15 μJ energy at 500 kHz repetition rate. A line-by-line writing technique at 1 mm/s scanning speed was used. Laser emission at 1.06 μm (with 0.35 mJ pulse energy) and at 1.03 μm (with 0.16 mJ pulse energy) was obtained from the waveguide inscribed in Nd:CLNGG and Yb:CLNGG, respectively, employing quasi-continuous wave pumping with fiber-coupled diode lasers. The waveguide realized in RE3+-doped CLNGG crystals using ps-laser pulses at high repetition rates could provide Q-switched or mode-locked miniaturized lasers for a large number of photonic applications.
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