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These media are characterized by a strong electron\u2013phonon coupling. Using the Fr\u00f6hlich Hamiltonian to describe the electron\u2013phonon coupling in such media, we analyze the operation of the system above the lasing threshold. We show that below a critical value of the Fr\u00f6hlich constant, the laser can only operate in the conventional regime: namely, there are coherent cavity photons but no coherent phonons. Above the critical value, a new pump rate threshold appears. Above this threshold, either joint self-oscillations of coherent phonons in the gain medium and photons in a cavity or a chaotic regime are established. We also find a range of the values of the Fr\u00f6hlich constant, the pump rate, and the resonator eigenfrequency, in which more than one dynamical regime of the system is stable. In this case the laser dynamics is determined by the initial values of the resonator field, the active medium polarization, the population inversion, and phonon amplitude.<\/jats:p>","DOI":"10.1038\/s41598-022-11588-9","type":"journal-article","created":{"date-parts":[[2022,5,9]],"date-time":"2022-05-09T16:02:46Z","timestamp":1652112166000},"update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":4,"title":["Operational regimes of lasers based on gain media with a large Raman scattering cross-section"],"prefix":"10.1038","volume":"12","author":[{"given":"E. A.","family":"Tereshchenkov","sequence":"first","affiliation":[],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"E. S.","family":"Andrianov","sequence":"additional","affiliation":[],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"A. 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