Abstract

We report on an 888 nm-pumped Nd:GdVO$_4$ ring laser operational over a wavelength range from 1340.3 nm to 1342.1 nm with a maximum output power of 7.4 W at 1341.2 nm and a beam quality parameter $M^2 < 1.1$. To our knowledge this is the highest single-longitudinal-mode power obtained with a Nd:GdVO$_4$ crystal laser. We use a commercial frequency-doubling cavity to achieve 1.2 W at 671.0 nm and 4.0 W at 670.6 nm for use in lithium cold atom experiments. Respectively, these wavelengths are approximately resonant with and 250 GHz blue-detuned from the lithium $D$-lines. Thus, this source provides ample power for laser cooling of lithium atoms while also offering substantial power for experiments requiring light 10’s to 100’s of GHz blue-detuned from the primary lithium transitions.

© 2019 Optical Society of America under the terms of the OSA Open Access Publishing Agreement

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    [Crossref]
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2018 (1)

2017 (1)

C. S. Goldenstein, V. A. Miller, R. M. Spearrin, and C. L. Strand, “SpectraPlot.com: Integrated spectroscopic modeling of atomic and molecular gases,” J. Quant. Spectrosc. Radiat. Transfer 200, 249–257 (2017).
[Crossref]

2015 (4)

Y. Miake, T. Mukaiyama, K. M. O’Hara, and S. Gensemer, “A self-injected, diode-pumped, solid-state ring laser for laser cooling of Li atoms,” Rev. Sci. Instrum. 86(4), 043113 (2015).
[Crossref]

P. Koch, F. Ruebel, J. Bartschke, and J. A. L’Huillier, “5.7 W CW single-frequency laser at 671 nm by single-pass second harmonic generation of a 17.2 W injection-locked 1342 nm Nd:YVO$_4$4 ring laser using periodically poled MgO:LiNbO$_3$3,” Appl. Opt. 54(33), 9954–9959 (2015).
[Crossref]

Y. T. Wang, R. H. Zhang, J. H. Li, and W. J. Li, “Power scaling of single-longitudinal-mode Nd:GdVO$_4$4 laser at 1342 nm,” Laser Phys. 25(6), 065003 (2015).
[Crossref]

M. F. Parsons, F. Huber, A. Mazurenko, C. S. Chiu, W. Setiawan, K. Wooley-Brown, S. Blatt, and M. Greiner, “Site-resolved imaging of fermionic $^{6}\mathrm {Li}$6Li in an optical lattice,” Phys. Rev. Lett. 114(21), 213002 (2015).
[Crossref]

2014 (3)

A. Burchianti, G. Valtolina, J. A. Seman, E. Pace, M. De Pas, M. Inguscio, M. Zaccanti, and G. Roati, “Efficient all-optical production of large $^{6}\mathrm {Li}$6Li quantum gases using ${D}_{1}$D1 gray-molasses cooling,” Phys. Rev. A 90(4), 043408 (2014).
[Crossref]

S. Bennetts, G. D. McDonald, K. S. Hardman, J. E. Debs, C. C. N. Kuhn, J. D. Close, and N. P. Robins, “External cavity diode lasers with 5 kHz linewidth and 200 nm tuning range at 1.55 $\mu$μm and methods for linewidth measurement,” Opt. Express 22(9), 10642–10654 (2014).
[Crossref]

Y. T. Wang, R. H. Zhang, J. H. Li, W. J. Li, C. Tan, and B. L. Zhang, “A diode-end-pumped continuous-wave single-longitudinal-mode Nd:GdVO$_4$4-LBO red laser at 670 nm,” Laser Phys. 24(3), 035001 (2014).
[Crossref]

2013 (4)

Y. Wang, W. Li, L. Pan, J. Yu, and R. Zhang, “Diode-end-pumped continuous wave single-longitudinal-mode Nd:GdVO4 laser at 1342 nm,” Appl. Opt. 52(9), 1987–1991 (2013).
[Crossref]

U. Eismann, A. Bergschneider, F. Sievers, N. Kretzschmar, C. Salomon, and F. Chevy, “2.1-watts intracavity-frequency-doubled all-solid-state light source at 671 nm for laser cooling of lithium,” Opt. Express 21(7), 9091–9102 (2013).
[Crossref]

A. T. Grier, I. Ferrier-Barbut, B. S. Rem, M. Delehaye, L. Khaykovich, F. Chevy, and C. Salomon, “${\Lambda }$Λ-enhanced sub-doppler cooling of lithium atoms in ${D}_{1}$D1 gray molasses,” Phys. Rev. A 87(6), 063411 (2013).
[Crossref]

L. S. Rothman, I. E. Gordon, Y. Babikov, A. Barbe, D. C. Benner, P. F. Bernath, M. Birk, L. Bizzocchi, V. Boudon, L. R. Brown, A. Campargue, K. Chance, E. A. Cohen, L. H. Coudert, V. M. Devi, B. J. Drouin, A. Fayt, J. M. Flaud, R. R. Gamache, J. J. Harrison, J. M. Hartmann, C. Hill, J. T. Hodges, D. Jacquemart, A. Jolly, J. Lamouroux, R. J. Le Roy, G. Li, D. A. Long, O. M. Lyulin, C. J. Mackie, S. T. Massie, S. Mikhailenko, H. S. P. Mueller, O. V. Naumenko, A. V. Nikitin, J. Orphal, V. Perevalov, A. Perrin, E. R. Polovtseva, C. Richard, M. A. H. Smith, E. Starikova, K. Sung, S. Tashkun, J. Tennyson, G. C. Toon, V. G. Tyuterev, and G. Wagner, “The HITRAN2012 molecular spectroscopic database,” J. Quant. Spectrosc. Radiat. Transfer 130, 4–50 (2013).
[Crossref]

2012 (1)

U. Eismann, F. Gerbier, C. Canalias, A. Zukauskas, G. Trenec, J. Vigue, F. Chevy, and C. Salomon, “An all-solid-state laser source at 671 nm for cold-atom experiments with lithium,” Appl. Phys. B: Lasers Opt. 106(1), 25–36 (2012).
[Crossref]

2011 (2)

F. Y. Hou, L. Yu, X. J. Jia, Y. H. Zheng, C. D. Xie, and K. C. Peng, “Experimental generation of optical non-classical states of light with 1.34 $\mu$μm wavelength,” Eur. Phys. J. D 62(3), 433–437 (2011).
[Crossref]

X. Délen, F. Balembois, O. Musset, and P. Georges, “Characteristics of laser operation at 1064 nm in Nd:YVO4 under diode pumping at 808 and 914 nm,” J. Opt. Soc. Am. B 28(1), 52–57 (2011).
[Crossref]

2010 (1)

F. A. Camargo, T. Zanon-Willette, T. Badr, N. U. Wetter, and J.-J. Zondy, “Tunable Single-Frequency Nd:YVO$_4$4 BiB$_3$3O$_6$6 Ring Laser at 671 nm,” IEEE J. Quantum Electron. 46(5), 804–809 (2010).

2009 (3)

Y. F. Lü, X. H. Zhang, J. Xia, X. D. Yin, A. F. Zhang, L. Bao, D. Wang, and H. Quan, “Highly efficient intracavity frequency-doubled Nd:GdVO$_4$4-LBO red laser at 670 nm under direct 880 nm pumping,” Laser Phys. 19(12), 2174–2178 (2009).
[Crossref]

W. S. Bakr, J. I. Gillen, A. Peng, S. Foelling, and M. Greiner, “A quantum gas microscope for detecting single atoms in a Hubbard-regime optical lattice,” Nature 462(7269), 74–77 (2009).
[Crossref]

F. Lenhardt, M. Nittmann, T. Bauer, J. Bartschke, and J. A. L’Huillier, “High-power 888-nm-pumped Nd:YVO$_4$4 1342-nm oscillator operating in the TEM$_{00}$00 mode,” Appl. Phys. B: Lasers Opt. 96(4), 803–807 (2009).
[Crossref]

2008 (1)

H. Müller, S.-w. Chiow, Q. Long, S. Herrmann, and S. Chu, “Atom interferometry with up to 24-photon-momentum-transfer beam splitters,” Phys. Rev. Lett. 100(18), 180405 (2008).
[Crossref]

2006 (3)

A. Miffre, M. Jacquey, M. Büchner, G. Trénec, and J. Vigué, “Atom interferometry measurement of the electric polarizability of lithium,” Eur. Phys. J. D 38(2), 353–365 (2006).
[Crossref]

L. McDonagh, R. Wallenstein, R. Knappe, and A. Nebel, “High-efficiency 60 W TEM$_{00}$00 Nd:YVO$_4$4 oscillator pumped at 888 nm,” Opt. Lett. 31(22), 3297–3299 (2006).
[Crossref]

S. Chénais, F. Druon, S. Forget, F. Balembois, and P. Georges, “On thermal effects in solid-state lasers: The case of ytterbium-doped materials,” Prog. Quantum Electron. 30(4), 89–153 (2006).
[Crossref]

2005 (3)

2004 (1)

2002 (2)

1998 (2)

D. Brown, “Heat, fluorescence, and stimulated-emission power densities and fractions in Nd : YAG,” IEEE J. Quantum Electron. 34(3), 560–572 (1998).
[Crossref]

L. Fornasiero, S. Kuck, T. Jensen, G. Huber, and B. Chai, “Excited state absorption and stimulated emission of Nd$^{3+}$3+ in crystals. Part 2: YVO$_4$4, GdVO$_4$4, and Sr$_5$5(PO$_4$4)$_3$3F,” Appl. Phys. B: Lasers Opt. 67(5), 549–553 (1998).
[Crossref]

1997 (1)

Y. Chen, T. Huang, C. Kao, C. Wang, and S. Wang, “Optimization in scaling fiber-coupled laser-diode end-pumped lasers to higher power: Influence of thermal effect,” IEEE J. Quantum Electron. 33(8), 1424–1429 (1997).
[Crossref]

1994 (3)

L. DeShazer, “Vanadate Crystals Exploit Diode-Pump Technology,” Laser Focus World 30, 88 (1994).

T. Jensen, V. G. Ostroumov, J. P. Meyn, G. Huber, A. I. Zagumennyi, and I. A. Shcherbakov, “Spectroscopic characterization and laser performance of diode-laser-pumped Nd-GdVO$_4$4,” Appl. Phys. B: Lasers Opt. 58(5), 373–379 (1994).
[Crossref]

S. A. Payne, L. K. Smith, R. J. Beach, B. H. T. Chai, J. H. Tassano, L. D. Deloach, W. L. Kway, R. W. Solarz, and W. F. Krupke, “Properties of Cr:LiSrAlF$_6$6 crystals for laser operation,” Appl. Opt. 33(24), 5526–5536 (1994).
[Crossref]

1991 (1)

Z. Lin, K. Shimizu, M. S. Zhan, F. Shimizu, and H. Takuma, “Laser cooling and trapping of Li,” Jpn. J. Appl. Phys. 30(Part 2, No. 7B), L1324–L1326 (1991).
[Crossref]

1986 (1)

1983 (1)

R. W. P. Drever, J. L. Hall, F. V. Kowalski, J. Hough, G. M. Ford, A. J. Munley, and H. Ward, “Laser phase and frequency stabilization using an optical-resonator,” Appl. Phys. B: Photophys. Laser Chem. 31(2), 97–105 (1983).
[Crossref]

Agnesi, A.

Babikov, Y.

L. S. Rothman, I. E. Gordon, Y. Babikov, A. Barbe, D. C. Benner, P. F. Bernath, M. Birk, L. Bizzocchi, V. Boudon, L. R. Brown, A. Campargue, K. Chance, E. A. Cohen, L. H. Coudert, V. M. Devi, B. J. Drouin, A. Fayt, J. M. Flaud, R. R. Gamache, J. J. Harrison, J. M. Hartmann, C. Hill, J. T. Hodges, D. Jacquemart, A. Jolly, J. Lamouroux, R. J. Le Roy, G. Li, D. A. Long, O. M. Lyulin, C. J. Mackie, S. T. Massie, S. Mikhailenko, H. S. P. Mueller, O. V. Naumenko, A. V. Nikitin, J. Orphal, V. Perevalov, A. Perrin, E. R. Polovtseva, C. Richard, M. A. H. Smith, E. Starikova, K. Sung, S. Tashkun, J. Tennyson, G. C. Toon, V. G. Tyuterev, and G. Wagner, “The HITRAN2012 molecular spectroscopic database,” J. Quant. Spectrosc. Radiat. Transfer 130, 4–50 (2013).
[Crossref]

Badr, T.

F. A. Camargo, T. Zanon-Willette, T. Badr, N. U. Wetter, and J.-J. Zondy, “Tunable Single-Frequency Nd:YVO$_4$4 BiB$_3$3O$_6$6 Ring Laser at 671 nm,” IEEE J. Quantum Electron. 46(5), 804–809 (2010).

Bakr, W. S.

W. S. Bakr, J. I. Gillen, A. Peng, S. Foelling, and M. Greiner, “A quantum gas microscope for detecting single atoms in a Hubbard-regime optical lattice,” Nature 462(7269), 74–77 (2009).
[Crossref]

Balembois, F.

X. Délen, F. Balembois, O. Musset, and P. Georges, “Characteristics of laser operation at 1064 nm in Nd:YVO4 under diode pumping at 808 and 914 nm,” J. Opt. Soc. Am. B 28(1), 52–57 (2011).
[Crossref]

S. Chénais, F. Druon, S. Forget, F. Balembois, and P. Georges, “On thermal effects in solid-state lasers: The case of ytterbium-doped materials,” Prog. Quantum Electron. 30(4), 89–153 (2006).
[Crossref]

Bao, L.

Y. F. Lü, X. H. Zhang, J. Xia, X. D. Yin, A. F. Zhang, L. Bao, D. Wang, and H. Quan, “Highly efficient intracavity frequency-doubled Nd:GdVO$_4$4-LBO red laser at 670 nm under direct 880 nm pumping,” Laser Phys. 19(12), 2174–2178 (2009).
[Crossref]

Barbe, A.

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L. S. Rothman, I. E. Gordon, Y. Babikov, A. Barbe, D. C. Benner, P. F. Bernath, M. Birk, L. Bizzocchi, V. Boudon, L. R. Brown, A. Campargue, K. Chance, E. A. Cohen, L. H. Coudert, V. M. Devi, B. J. Drouin, A. Fayt, J. M. Flaud, R. R. Gamache, J. J. Harrison, J. M. Hartmann, C. Hill, J. T. Hodges, D. Jacquemart, A. Jolly, J. Lamouroux, R. J. Le Roy, G. Li, D. A. Long, O. M. Lyulin, C. J. Mackie, S. T. Massie, S. Mikhailenko, H. S. P. Mueller, O. V. Naumenko, A. V. Nikitin, J. Orphal, V. Perevalov, A. Perrin, E. R. Polovtseva, C. Richard, M. A. H. Smith, E. Starikova, K. Sung, S. Tashkun, J. Tennyson, G. C. Toon, V. G. Tyuterev, and G. Wagner, “The HITRAN2012 molecular spectroscopic database,” J. Quant. Spectrosc. Radiat. Transfer 130, 4–50 (2013).
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C. S. Goldenstein, V. A. Miller, R. M. Spearrin, and C. L. Strand, “SpectraPlot.com: Integrated spectroscopic modeling of atomic and molecular gases,” J. Quant. Spectrosc. Radiat. Transfer 200, 249–257 (2017).
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Sung, K.

L. S. Rothman, I. E. Gordon, Y. Babikov, A. Barbe, D. C. Benner, P. F. Bernath, M. Birk, L. Bizzocchi, V. Boudon, L. R. Brown, A. Campargue, K. Chance, E. A. Cohen, L. H. Coudert, V. M. Devi, B. J. Drouin, A. Fayt, J. M. Flaud, R. R. Gamache, J. J. Harrison, J. M. Hartmann, C. Hill, J. T. Hodges, D. Jacquemart, A. Jolly, J. Lamouroux, R. J. Le Roy, G. Li, D. A. Long, O. M. Lyulin, C. J. Mackie, S. T. Massie, S. Mikhailenko, H. S. P. Mueller, O. V. Naumenko, A. V. Nikitin, J. Orphal, V. Perevalov, A. Perrin, E. R. Polovtseva, C. Richard, M. A. H. Smith, E. Starikova, K. Sung, S. Tashkun, J. Tennyson, G. C. Toon, V. G. Tyuterev, and G. Wagner, “The HITRAN2012 molecular spectroscopic database,” J. Quant. Spectrosc. Radiat. Transfer 130, 4–50 (2013).
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Z. Lin, K. Shimizu, M. S. Zhan, F. Shimizu, and H. Takuma, “Laser cooling and trapping of Li,” Jpn. J. Appl. Phys. 30(Part 2, No. 7B), L1324–L1326 (1991).
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Y. T. Wang, R. H. Zhang, J. H. Li, W. J. Li, C. Tan, and B. L. Zhang, “A diode-end-pumped continuous-wave single-longitudinal-mode Nd:GdVO$_4$4-LBO red laser at 670 nm,” Laser Phys. 24(3), 035001 (2014).
[Crossref]

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L. S. Rothman, I. E. Gordon, Y. Babikov, A. Barbe, D. C. Benner, P. F. Bernath, M. Birk, L. Bizzocchi, V. Boudon, L. R. Brown, A. Campargue, K. Chance, E. A. Cohen, L. H. Coudert, V. M. Devi, B. J. Drouin, A. Fayt, J. M. Flaud, R. R. Gamache, J. J. Harrison, J. M. Hartmann, C. Hill, J. T. Hodges, D. Jacquemart, A. Jolly, J. Lamouroux, R. J. Le Roy, G. Li, D. A. Long, O. M. Lyulin, C. J. Mackie, S. T. Massie, S. Mikhailenko, H. S. P. Mueller, O. V. Naumenko, A. V. Nikitin, J. Orphal, V. Perevalov, A. Perrin, E. R. Polovtseva, C. Richard, M. A. H. Smith, E. Starikova, K. Sung, S. Tashkun, J. Tennyson, G. C. Toon, V. G. Tyuterev, and G. Wagner, “The HITRAN2012 molecular spectroscopic database,” J. Quant. Spectrosc. Radiat. Transfer 130, 4–50 (2013).
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Tennyson, J.

L. S. Rothman, I. E. Gordon, Y. Babikov, A. Barbe, D. C. Benner, P. F. Bernath, M. Birk, L. Bizzocchi, V. Boudon, L. R. Brown, A. Campargue, K. Chance, E. A. Cohen, L. H. Coudert, V. M. Devi, B. J. Drouin, A. Fayt, J. M. Flaud, R. R. Gamache, J. J. Harrison, J. M. Hartmann, C. Hill, J. T. Hodges, D. Jacquemart, A. Jolly, J. Lamouroux, R. J. Le Roy, G. Li, D. A. Long, O. M. Lyulin, C. J. Mackie, S. T. Massie, S. Mikhailenko, H. S. P. Mueller, O. V. Naumenko, A. V. Nikitin, J. Orphal, V. Perevalov, A. Perrin, E. R. Polovtseva, C. Richard, M. A. H. Smith, E. Starikova, K. Sung, S. Tashkun, J. Tennyson, G. C. Toon, V. G. Tyuterev, and G. Wagner, “The HITRAN2012 molecular spectroscopic database,” J. Quant. Spectrosc. Radiat. Transfer 130, 4–50 (2013).
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L. S. Rothman, I. E. Gordon, Y. Babikov, A. Barbe, D. C. Benner, P. F. Bernath, M. Birk, L. Bizzocchi, V. Boudon, L. R. Brown, A. Campargue, K. Chance, E. A. Cohen, L. H. Coudert, V. M. Devi, B. J. Drouin, A. Fayt, J. M. Flaud, R. R. Gamache, J. J. Harrison, J. M. Hartmann, C. Hill, J. T. Hodges, D. Jacquemart, A. Jolly, J. Lamouroux, R. J. Le Roy, G. Li, D. A. Long, O. M. Lyulin, C. J. Mackie, S. T. Massie, S. Mikhailenko, H. S. P. Mueller, O. V. Naumenko, A. V. Nikitin, J. Orphal, V. Perevalov, A. Perrin, E. R. Polovtseva, C. Richard, M. A. H. Smith, E. Starikova, K. Sung, S. Tashkun, J. Tennyson, G. C. Toon, V. G. Tyuterev, and G. Wagner, “The HITRAN2012 molecular spectroscopic database,” J. Quant. Spectrosc. Radiat. Transfer 130, 4–50 (2013).
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U. Eismann, F. Gerbier, C. Canalias, A. Zukauskas, G. Trenec, J. Vigue, F. Chevy, and C. Salomon, “An all-solid-state laser source at 671 nm for cold-atom experiments with lithium,” Appl. Phys. B: Lasers Opt. 106(1), 25–36 (2012).
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A. Miffre, M. Jacquey, M. Büchner, G. Trénec, and J. Vigué, “Atom interferometry measurement of the electric polarizability of lithium,” Eur. Phys. J. D 38(2), 353–365 (2006).
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L. S. Rothman, I. E. Gordon, Y. Babikov, A. Barbe, D. C. Benner, P. F. Bernath, M. Birk, L. Bizzocchi, V. Boudon, L. R. Brown, A. Campargue, K. Chance, E. A. Cohen, L. H. Coudert, V. M. Devi, B. J. Drouin, A. Fayt, J. M. Flaud, R. R. Gamache, J. J. Harrison, J. M. Hartmann, C. Hill, J. T. Hodges, D. Jacquemart, A. Jolly, J. Lamouroux, R. J. Le Roy, G. Li, D. A. Long, O. M. Lyulin, C. J. Mackie, S. T. Massie, S. Mikhailenko, H. S. P. Mueller, O. V. Naumenko, A. V. Nikitin, J. Orphal, V. Perevalov, A. Perrin, E. R. Polovtseva, C. Richard, M. A. H. Smith, E. Starikova, K. Sung, S. Tashkun, J. Tennyson, G. C. Toon, V. G. Tyuterev, and G. Wagner, “The HITRAN2012 molecular spectroscopic database,” J. Quant. Spectrosc. Radiat. Transfer 130, 4–50 (2013).
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A. Burchianti, G. Valtolina, J. A. Seman, E. Pace, M. De Pas, M. Inguscio, M. Zaccanti, and G. Roati, “Efficient all-optical production of large $^{6}\mathrm {Li}$6Li quantum gases using ${D}_{1}$D1 gray-molasses cooling,” Phys. Rev. A 90(4), 043408 (2014).
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U. Eismann, F. Gerbier, C. Canalias, A. Zukauskas, G. Trenec, J. Vigue, F. Chevy, and C. Salomon, “An all-solid-state laser source at 671 nm for cold-atom experiments with lithium,” Appl. Phys. B: Lasers Opt. 106(1), 25–36 (2012).
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A. Miffre, M. Jacquey, M. Büchner, G. Trénec, and J. Vigué, “Atom interferometry measurement of the electric polarizability of lithium,” Eur. Phys. J. D 38(2), 353–365 (2006).
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Wagner, G.

L. S. Rothman, I. E. Gordon, Y. Babikov, A. Barbe, D. C. Benner, P. F. Bernath, M. Birk, L. Bizzocchi, V. Boudon, L. R. Brown, A. Campargue, K. Chance, E. A. Cohen, L. H. Coudert, V. M. Devi, B. J. Drouin, A. Fayt, J. M. Flaud, R. R. Gamache, J. J. Harrison, J. M. Hartmann, C. Hill, J. T. Hodges, D. Jacquemart, A. Jolly, J. Lamouroux, R. J. Le Roy, G. Li, D. A. Long, O. M. Lyulin, C. J. Mackie, S. T. Massie, S. Mikhailenko, H. S. P. Mueller, O. V. Naumenko, A. V. Nikitin, J. Orphal, V. Perevalov, A. Perrin, E. R. Polovtseva, C. Richard, M. A. H. Smith, E. Starikova, K. Sung, S. Tashkun, J. Tennyson, G. C. Toon, V. G. Tyuterev, and G. Wagner, “The HITRAN2012 molecular spectroscopic database,” J. Quant. Spectrosc. Radiat. Transfer 130, 4–50 (2013).
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Y. F. Lü, X. H. Zhang, J. Xia, X. D. Yin, A. F. Zhang, L. Bao, D. Wang, and H. Quan, “Highly efficient intracavity frequency-doubled Nd:GdVO$_4$4-LBO red laser at 670 nm under direct 880 nm pumping,” Laser Phys. 19(12), 2174–2178 (2009).
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Wang, S.

Y. Chen, T. Huang, C. Kao, C. Wang, and S. Wang, “Optimization in scaling fiber-coupled laser-diode end-pumped lasers to higher power: Influence of thermal effect,” IEEE J. Quantum Electron. 33(8), 1424–1429 (1997).
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Wang, Y.

Wang, Y. T.

Y. T. Wang, R. H. Zhang, J. H. Li, and W. J. Li, “Power scaling of single-longitudinal-mode Nd:GdVO$_4$4 laser at 1342 nm,” Laser Phys. 25(6), 065003 (2015).
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Y. T. Wang, R. H. Zhang, J. H. Li, W. J. Li, C. Tan, and B. L. Zhang, “A diode-end-pumped continuous-wave single-longitudinal-mode Nd:GdVO$_4$4-LBO red laser at 670 nm,” Laser Phys. 24(3), 035001 (2014).
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R. W. P. Drever, J. L. Hall, F. V. Kowalski, J. Hough, G. M. Ford, A. J. Munley, and H. Ward, “Laser phase and frequency stabilization using an optical-resonator,” Appl. Phys. B: Photophys. Laser Chem. 31(2), 97–105 (1983).
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T. Kinoshita, T. Wenger, and D. S. Weiss, “All-optical Bose-Einstein condensation using a compressible crossed dipole trap,” Phys. Rev. A 71(1), 011602 (2005).
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T. Kinoshita, T. Wenger, and D. S. Weiss, “All-optical Bose-Einstein condensation using a compressible crossed dipole trap,” Phys. Rev. A 71(1), 011602 (2005).
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F. A. Camargo, T. Zanon-Willette, T. Badr, N. U. Wetter, and J.-J. Zondy, “Tunable Single-Frequency Nd:YVO$_4$4 BiB$_3$3O$_6$6 Ring Laser at 671 nm,” IEEE J. Quantum Electron. 46(5), 804–809 (2010).

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M. F. Parsons, F. Huber, A. Mazurenko, C. S. Chiu, W. Setiawan, K. Wooley-Brown, S. Blatt, and M. Greiner, “Site-resolved imaging of fermionic $^{6}\mathrm {Li}$6Li in an optical lattice,” Phys. Rev. Lett. 114(21), 213002 (2015).
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Y. F. Lü, X. H. Zhang, J. Xia, X. D. Yin, A. F. Zhang, L. Bao, D. Wang, and H. Quan, “Highly efficient intracavity frequency-doubled Nd:GdVO$_4$4-LBO red laser at 670 nm under direct 880 nm pumping,” Laser Phys. 19(12), 2174–2178 (2009).
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Xie, C. D.

F. Y. Hou, L. Yu, X. J. Jia, Y. H. Zheng, C. D. Xie, and K. C. Peng, “Experimental generation of optical non-classical states of light with 1.34 $\mu$μm wavelength,” Eur. Phys. J. D 62(3), 433–437 (2011).
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Yan, M.-C.

Yao, X.-C.

Yatagai, T.

Yin, X. D.

Y. F. Lü, X. H. Zhang, J. Xia, X. D. Yin, A. F. Zhang, L. Bao, D. Wang, and H. Quan, “Highly efficient intracavity frequency-doubled Nd:GdVO$_4$4-LBO red laser at 670 nm under direct 880 nm pumping,” Laser Phys. 19(12), 2174–2178 (2009).
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Yu, J.

Yu, L.

F. Y. Hou, L. Yu, X. J. Jia, Y. H. Zheng, C. D. Xie, and K. C. Peng, “Experimental generation of optical non-classical states of light with 1.34 $\mu$μm wavelength,” Eur. Phys. J. D 62(3), 433–437 (2011).
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Yu, Y.

Yuan, T.

Zaccanti, M.

A. Burchianti, G. Valtolina, J. A. Seman, E. Pace, M. De Pas, M. Inguscio, M. Zaccanti, and G. Roati, “Efficient all-optical production of large $^{6}\mathrm {Li}$6Li quantum gases using ${D}_{1}$D1 gray-molasses cooling,” Phys. Rev. A 90(4), 043408 (2014).
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T. Jensen, V. G. Ostroumov, J. P. Meyn, G. Huber, A. I. Zagumennyi, and I. A. Shcherbakov, “Spectroscopic characterization and laser performance of diode-laser-pumped Nd-GdVO$_4$4,” Appl. Phys. B: Lasers Opt. 58(5), 373–379 (1994).
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F. A. Camargo, T. Zanon-Willette, T. Badr, N. U. Wetter, and J.-J. Zondy, “Tunable Single-Frequency Nd:YVO$_4$4 BiB$_3$3O$_6$6 Ring Laser at 671 nm,” IEEE J. Quantum Electron. 46(5), 804–809 (2010).

Zeng, C.

Zeng, F.

Zhan, M. S.

Z. Lin, K. Shimizu, M. S. Zhan, F. Shimizu, and H. Takuma, “Laser cooling and trapping of Li,” Jpn. J. Appl. Phys. 30(Part 2, No. 7B), L1324–L1326 (1991).
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Y. F. Lü, X. H. Zhang, J. Xia, X. D. Yin, A. F. Zhang, L. Bao, D. Wang, and H. Quan, “Highly efficient intracavity frequency-doubled Nd:GdVO$_4$4-LBO red laser at 670 nm under direct 880 nm pumping,” Laser Phys. 19(12), 2174–2178 (2009).
[Crossref]

Zhang, B. L.

Y. T. Wang, R. H. Zhang, J. H. Li, W. J. Li, C. Tan, and B. L. Zhang, “A diode-end-pumped continuous-wave single-longitudinal-mode Nd:GdVO$_4$4-LBO red laser at 670 nm,” Laser Phys. 24(3), 035001 (2014).
[Crossref]

Zhang, H.

Zhang, R.

Zhang, R. H.

Y. T. Wang, R. H. Zhang, J. H. Li, and W. J. Li, “Power scaling of single-longitudinal-mode Nd:GdVO$_4$4 laser at 1342 nm,” Laser Phys. 25(6), 065003 (2015).
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Y. T. Wang, R. H. Zhang, J. H. Li, W. J. Li, C. Tan, and B. L. Zhang, “A diode-end-pumped continuous-wave single-longitudinal-mode Nd:GdVO$_4$4-LBO red laser at 670 nm,” Laser Phys. 24(3), 035001 (2014).
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Zhang, W.-Z.

Zhang, X. H.

Y. F. Lü, X. H. Zhang, J. Xia, X. D. Yin, A. F. Zhang, L. Bao, D. Wang, and H. Quan, “Highly efficient intracavity frequency-doubled Nd:GdVO$_4$4-LBO red laser at 670 nm under direct 880 nm pumping,” Laser Phys. 19(12), 2174–2178 (2009).
[Crossref]

Zheng, Y. H.

F. Y. Hou, L. Yu, X. J. Jia, Y. H. Zheng, C. D. Xie, and K. C. Peng, “Experimental generation of optical non-classical states of light with 1.34 $\mu$μm wavelength,” Eur. Phys. J. D 62(3), 433–437 (2011).
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Zhu, L.

Zondy, J.-J.

F. A. Camargo, T. Zanon-Willette, T. Badr, N. U. Wetter, and J.-J. Zondy, “Tunable Single-Frequency Nd:YVO$_4$4 BiB$_3$3O$_6$6 Ring Laser at 671 nm,” IEEE J. Quantum Electron. 46(5), 804–809 (2010).

Zukauskas, A.

U. Eismann, F. Gerbier, C. Canalias, A. Zukauskas, G. Trenec, J. Vigue, F. Chevy, and C. Salomon, “An all-solid-state laser source at 671 nm for cold-atom experiments with lithium,” Appl. Phys. B: Lasers Opt. 106(1), 25–36 (2012).
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Appl. Phys. B: Lasers Opt. (4)

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U. Eismann, F. Gerbier, C. Canalias, A. Zukauskas, G. Trenec, J. Vigue, F. Chevy, and C. Salomon, “An all-solid-state laser source at 671 nm for cold-atom experiments with lithium,” Appl. Phys. B: Lasers Opt. 106(1), 25–36 (2012).
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Eur. Phys. J. D (2)

F. Y. Hou, L. Yu, X. J. Jia, Y. H. Zheng, C. D. Xie, and K. C. Peng, “Experimental generation of optical non-classical states of light with 1.34 $\mu$μm wavelength,” Eur. Phys. J. D 62(3), 433–437 (2011).
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A. Miffre, M. Jacquey, M. Büchner, G. Trénec, and J. Vigué, “Atom interferometry measurement of the electric polarizability of lithium,” Eur. Phys. J. D 38(2), 353–365 (2006).
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IEEE J. Quantum Electron. (3)

F. A. Camargo, T. Zanon-Willette, T. Badr, N. U. Wetter, and J.-J. Zondy, “Tunable Single-Frequency Nd:YVO$_4$4 BiB$_3$3O$_6$6 Ring Laser at 671 nm,” IEEE J. Quantum Electron. 46(5), 804–809 (2010).

Y. Chen, T. Huang, C. Kao, C. Wang, and S. Wang, “Optimization in scaling fiber-coupled laser-diode end-pumped lasers to higher power: Influence of thermal effect,” IEEE J. Quantum Electron. 33(8), 1424–1429 (1997).
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Z. Lin, K. Shimizu, M. S. Zhan, F. Shimizu, and H. Takuma, “Laser cooling and trapping of Li,” Jpn. J. Appl. Phys. 30(Part 2, No. 7B), L1324–L1326 (1991).
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Laser Phys. (3)

Y. F. Lü, X. H. Zhang, J. Xia, X. D. Yin, A. F. Zhang, L. Bao, D. Wang, and H. Quan, “Highly efficient intracavity frequency-doubled Nd:GdVO$_4$4-LBO red laser at 670 nm under direct 880 nm pumping,” Laser Phys. 19(12), 2174–2178 (2009).
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Y. T. Wang, R. H. Zhang, J. H. Li, W. J. Li, C. Tan, and B. L. Zhang, “A diode-end-pumped continuous-wave single-longitudinal-mode Nd:GdVO$_4$4-LBO red laser at 670 nm,” Laser Phys. 24(3), 035001 (2014).
[Crossref]

Y. T. Wang, R. H. Zhang, J. H. Li, and W. J. Li, “Power scaling of single-longitudinal-mode Nd:GdVO$_4$4 laser at 1342 nm,” Laser Phys. 25(6), 065003 (2015).
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[Crossref]

Prog. Quantum Electron. (1)

S. Chénais, F. Druon, S. Forget, F. Balembois, and P. Georges, “On thermal effects in solid-state lasers: The case of ytterbium-doped materials,” Prog. Quantum Electron. 30(4), 89–153 (2006).
[Crossref]

Rev. Sci. Instrum. (1)

Y. Miake, T. Mukaiyama, K. M. O’Hara, and S. Gensemer, “A self-injected, diode-pumped, solid-state ring laser for laser cooling of Li atoms,” Rev. Sci. Instrum. 86(4), 043113 (2015).
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Other (1)

A. E. Siegman, Lasers (University Science Books, 1986), Revised ed.

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Figures (8)

Fig. 1.
Fig. 1. (a) Energy level diagram of Nd $^{+3}$ in a GdVO $_4$ host material. The relevant transitions for pumping, lasing, and excited state absorption are labeled. (b) Absorption coefficient for a 0.5% at. doped Nd:GdVO $_4$ crystal near the 880 nm and 888 nm pumping transitions. (c) Gain and excited state absorption spectrum.
Fig. 2.
Fig. 2. A schematic of the laser setup. The laser is pumped by a fiber-coupled diode bar. Lenses L1 and L2 image the end of the pump fiber onto the Nd:GdVO $_4$ crystal. Mirrors M1 – M4, which are all flat, form a bow-tie cavity with a round trip path length of 450 mm. The physical distance between mirrors M1 and M2 is 45 mm and that between M3 and M4 is 156 mm. M4 is the output coupler. Uni-directional operation is enforced by the combination of the $\lambda /2$ waveplate and the TGG crystal placed in a high magnetic field to provide Faraday rotation. The rotatable thin etalon is used to tune the operating wavelength. The beam output from M4 is collimated by L3 and passes through an optical isolator before being sent to a commercial build-up cavity for second harmonic generation.
Fig. 3.
Fig. 3. Output power as a function of absorbed pump power. The line is $P_{\mathrm {out}} = \eta _{sl} (P_{\mathrm {abs}} - P_{\mathrm {th}})$ where the threshold power $P_{\mathrm {th}} = 13.1\, {\mathrm {W}}$ , the slope efficiency $\eta _{sl} = 24 \%$ and $P_{\mathrm {abs}}$ is the absorbed pump power.
Fig. 4.
Fig. 4. Dioptric power as a function of absorbed pump power. The curve is Eq. (1) with the fractional thermal heat load $\eta _h$ given by Eq. (5). These equations provide a model of the thermal lensing in our system with no free parameters.
Fig. 5.
Fig. 5. (a) Fabry-Perot spectrum showing single-longitudinal mode operations. (b) Beat note between the free-running Nd:GdVO $_4$ and an extended cavity diode laser demonstrating an upper bound on the fundamental laser linewidth of $450 \, {\mathrm {kHz}}$ .
Fig. 6.
Fig. 6. Measurement of the laser caustic for the 1342 nm laser in the (a) vertical and (b) horizontal directions. (c) Measurement of the laser caustic for the 671 nm laser beam. The inset shows a typical beam profile of the 671 nm laser beam as recorded by the CCD camera. The solid lines are fits to Eq. (8) used to determine the beam quality parameter $M^2$ .
Fig. 7.
Fig. 7. (a) Fundamental and second harmonic output power versus wavelength. The power of the fundamental laser is measured after the optical isolator in Fig. 2, just before entering the SHG cavity. (b) Spectrum of water absorption coefficient at $300^\circ \, {\mathrm {K}}$ and 50% relative humidity [37,38].
Fig. 8.
Fig. 8. (a) Fundamental and second harmonic output power over several hours. The fundamental power is measured after the optical isolator, just before entering the SHG cavity. (b) One-sided power spectral density of the residual intensity noise of the frequency-doubled laser output.

Equations (9)

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D = η h d n d t P a b s 2 π K c w p 2 ,
w p = 0 L w p 0 1 + θ p 2 w p 0 2 ( z z 0 ) 2 exp ( α z ) d z 0 L exp ( α z ) d z ,
d N d t = α p λ p h c I p N t f ( σ e + σ e s a ) λ l h c I c i r c N .
N = λ p h c t f α p I p 1 + I c i r c / I s a t ,
η h = Q h Q p = 1 ( t f t r a d λ p λ f + I c i r c I s a t ( σ e σ e + σ e s a ) λ p λ l 1 + I c i r c / I s a t ) .
η n o n = 1 t f t r a d λ p λ f , a n d η l a s e = 1 ( σ e σ e + σ e s a ) λ p λ l .
I c i r c = P o u t ( 1 R ) π w l 2 η s l ( P a b s P t h ) ( 1 R ) π w p 2 ,
w ( z ) = w 0 1 + ( M 2 ) 2 ( z z 0 ) 2 z R 2
S R I N = lim T 2 T | 0 T ϵ ( t ) e + i 2 π f d t | 2

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