2 Óaeãîðîäñüêèé ÍÒÖ ÌÎͲ ²íñòèòóòó ïðîáëåì ðåºñòðàö³¿ ³íôîðìàö³¿ ÍÀÍ Óêðà¿íè, 88000, Óaeãîðîä, âóë. Çàìêîâ³ ñõîäè, 4 3 ²íñòèòóò åëåêòðîííî¿ ô³çèêè ÍÀÍ Óêðà¿íè, 88000, Óaeãîðîä, âóë.Óí³âåðñèòåòñüêà, 21 ÁÀÐÈ×ÍÀ ÏÎÂÅIJÍÊÀ IJÅËÅÊÒÐÈ×Íί ÏÐÎÍÈÊÍÎÑÒ²  ÊÐÈÑÒÀËÀÕ TlGaSe 2 Î. Î. Ãîìîííàé, Ì. Þ. Ðèãàí, ². Þ. Ðîìàí, Ï. Ï. Ãóðàíè÷, Î. Ã. ÑëèâêàÀíîòàö³ÿ. Äîñë³äaeåíî øàðóâàò³ ñåãíåòîåëåêòðèêè TlGaSe 2 ç íåñï³âì³ðíîþ ôàçîþ ïðè âèñîêèõ ã³äðîñòàòè÷íèõ òèñêàõ (p àòì ≤p≤ 660 ÌÏà). Âñòàíîâëåíî, ùî ïðè çá³ëüøåíí³ òèñêó ñïîñòåð³ãàºòüñÿ çì³ùåííÿ àíîìàë³é ä³åëåêòðè÷íî¿ ïðîíèêíîñò³ â îáëàñòü âèùèõ òåìïåðàòóð, çì³íà òåìïåðàòóð õàðàêòåðíèõ àíîìàë³é ìຠë³í³éíèé õàðàêòåð ³ âèçíà÷åíî ¿õ áàðè÷í³ êîåô³ö³ºíòè ó äîñë³äaeóâàíîìó ³íòåðâàë³ òèñê³â. Çà ðåçóëüòàòàìè äîñë³äaeåíü áàðè÷íèõ çàëåaeíîñòåé ä³åëåêðè÷íî¿ ïðîíèêíîñò³, ï³ðîåëåêòðè÷íîãî êîåô³ö³ºíòà òà ïåòåëü ã³ñòåðåçèñó ïîáóäîâàíà (p,T)-ä³àãðàìà êðèñòàë³â TlGaSe 2 .Êëþ÷îâ³ ñëîâà: øàðóâàòèé êðèñòàë, ôàçîâèé ïåðåõ³ä, ã³äðîñòàòè÷íèé òèñê Abstract. Layered TlGaSe 2 ferroelectrics with an incommensurate phase are studied at high hydrostatic pressures (p atm ≤p≤ 660 MPa). With the pressure increase a shift of anomalies of dielectric permeability towards higher temperatures is observed. The variation of temperatures of the characteristic anomalies is linear, the pressure coefficients are determined. Based on the studies of pressure dependences of dielectric permeability, pyroelectric coefficient and hystheresis loops, a (p,T) phase diagram of TlGaSe 2 crystals is built.