Clad-pumped bismuth fibre laser emitting in the wavelength range from 1.3 to 1.4 \u03bcm<\/strong><\/a> Picosecond Raman fibre laser with a wavelength of 2.84 \u03bcm<\/a><\/strong> 1-W transversely diode-pumped metastable Ar* laser<\/a><\/strong> Radiation divergence of microsecond lasers based on a solution of rhodamine 6G and a solid-state laser based on a perylene-activated nanocomposite<\/a><\/strong> Highly efficient 1610-nm in-band cw Tm:LSO laser<\/strong><\/a> Comparison of mode-locking regimes based on nonlinear rotation of the polarization plane in erbium-doped fibre lasers with dumbbell-shaped and ring cavities<\/strong><\/a> Energies of X-ray laser pulses and stimulated emission wavelengths achievable by pumping X-ray lasers using the National Ignition Facility<\/a><\/strong> Parallel modes at pulsed two-frequency resonance in the \u039b-scheme of degenerate quantum levels<\/strong><\/a> Effect of the thickness of the passivating reactive titanium layer of mirror facets on the electrical characteristics of diode lasers<\/a><\/strong> Counter-propagating four-wave mixing on phase–amplitude holographic gratings in a cubic photorefractive crystal<\/a><\/strong> Laser synthesis of nanopowders based on zinc selenide for the preparation of highly transparent ceramics<\/a><\/strong> Soliton mode beams with positive and negative group velocities in a thin left-handed film on a right-handed Kerr substrate<\/a><\/strong> Formation of two-dimensional image contours in zero and plus second diffraction orders in the process of double Bragg diffraction<\/a><\/strong> Statistics of nonlinear noise in a high-speed optical communication line without dispersion compensation<\/a><\/strong> Simulation of the limiting parameters of a polarimetric fibre-optic current sensor on a spun fibre<\/a><\/strong> Lasers Clad-pumped bismuth fibre laser emitting in the wavelength range from 1.3 to 1.4 \u03bcm A. S. Vakhrushev, A. V. Kharakhordin, A. M. Khegai, S. V. Alyshev, K. E. Riumkin, E. G. Firstova, A. A. Umnikov, A. S. Lobanov, F. V. Afanas’ev, A. N. Gur’yanov, M. A. Mel’kumov, S. V. Firstov 681\u2013684 Picosecond Raman fibre\u2026 Read More »<\/a><\/span><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"class_list":["post-7365","post","type-post","status-publish","format-standard","hentry","category-stats"],"_links":{"self":[{"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/posts\/7365","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/comments?post=7365"}],"version-history":[{"count":0,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/posts\/7365\/revisions"}],"wp:attachment":[{"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/media?parent=7365"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/categories?post=7365"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/tags?post=7365"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}
\nA. S. Vakhrushev, A. V. Kharakhordin, A. M. Khegai, S. V. Alyshev, K. E. Riumkin, E. G. Firstova, A. A. Umnikov, A. S. Lobanov, F. V. Afanas’ev, A. N. Gur’yanov, M. A. Mel’kumov, S. V. Firstov 681\u2013684<\/p>\n
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