175 research outputs found

    Π‘ΠΈΠ½Ρ‚Π΅Π· Ρ‚Π° Π±Ρ–ΠΎΠ»ΠΎΠ³Ρ–Ρ‡Π½Π° ΠΎΡ†Ρ–Π½ΠΊΠ° [[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-3-Ρ–Π»]Π°Ρ†Π΅Ρ‚Π°ΠΌΡ–Π΄Ρ–Π² Π· 1,2,4-ΠΎΠΊΡΠ°Π΄Ρ–Π°Π·ΠΎΠ»ΡŒΠ½ΠΈΠΌ Ρ†ΠΈΠΊΠ»ΠΎΠΌ Ρƒ 6, 7 Ρ‚Π° 8 ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½Π½Ρ–

    Get PDF
    Fused heterocyclic 1,2,4-triazoles have provided much attention due to variety of their interesting biological properties.Aim. To develop the method for the synthesis of novel 2-[(1,2,4-oxadiazol-5-yl)-[1,2,4]triazolo[4,3-a]pyridine-3-yl]acetamides and conduct the biological assessment of the compounds synthesized.Results and discussion. A diverse set of acetamides newly synthesized consists of 32 analogs bearing an 1,2,4-oxadiazole cycle in positions 6, 7 and 8. A convenient scheme of the synthesis starts from commercially available 2-chloropyridine-3-, 2-chloropyridine-4-, 2-chloropyridine-5-carboxylic acids with amidoximes to form the corresponding 2-chloro-[3-R1-1,2,4-oxadiazol-5-yl]pyridines, then follows the reaction ofΒ  hydrazinolysis with an excess of hydrazine hydrate. The process continues via the ester formation with the pyridine ring closure, then the amide formations of the end products are obtained by hydrolysis into acetic acid.Experimental part. A series of new 2-[6-(1,2,4-oxadiazol-5-yl)-, 2-[7-(1,2,4-oxadiazol-5-yl)-, 2-[8-(1,2,4-oxadiazol-5-yl)-[1,2,4]triazolo[4,3-a]pyridine-3-yl]acetamides were obtained in good yields, and their structures were proven by the method of 1H NMR spectroscopy. The prognosis and study of their pharmacological activity were also conducted.Conclusions. The synthetic approach of obtaining the representatives of 2-[(1,2,4-oxadiazol-5-yl)-[1,2,4]triazolo[4,3-a]pyridine-3-yl]acetamides previously unknown can be used as an applicable method for the synthesis of diverse functionalized [1,2,4]triazolo[4,3-a]pyridine derivatives.ΠšΠΎΠ½Π΄Π΅Π½ΡΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Π΅ гСтСроцикличСскиС 1,2,4-Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»Ρ‹ ΠΏΡ€ΠΈΠ²Π»Π΅ΠΊΠ°ΡŽΡ‚ большоС Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ Ρ€Π°Π·Π½ΠΎΠΎΠ±Ρ€Π°Π·ΠΈΠ΅ΠΌ интСрСсных биологичСских свойств.ЦСль Ρ€Π°Π±ΠΎΡ‚Ρ‹. Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Ρ‚ΡŒ ΠΌΠ΅Ρ‚ΠΎΠ΄ синтСза Π½ΠΎΠ²Ρ‹Ρ… 2-[(1,2,4-оксадиазол-5-ΠΈΠ»)- [1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-a]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-3-ΠΈΠ»]Π°Ρ†Π΅Ρ‚Π°ΠΌΠΈΠ΄ΠΎΠ² ΠΈ провСсти Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ ΠΎΡ†Π΅Π½ΠΊΡƒ синтСзированных соСдинСний.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΈ ΠΈΡ… обсуТдСниС. Π‘ΠΈΠ½Ρ‚Π΅Π·ΠΈΡ€ΠΎΠ²Π°Π½ ряд Π½ΠΎΠ²Ρ‹Ρ… ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ… Π°Ρ†Π΅Ρ‚Π°ΠΌΠΈΠ΄ΠΎΠ², ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ состоит ΠΈΠ· 32 Π°Π½Π°Π»ΠΎΠ³ΠΎΠ², содСрТащих 1,2,4-ΠΎΠΊΡΠ°Π΄ΠΈΠ°Π·ΠΎΠ»ΡŒΠ½Ρ‹ΠΉ Ρ†ΠΈΠΊΠ» Π² 6, 7 ΠΈ 8 полоТСниях. Удобная схСма синтСза начинаСтся с коммСрчСски доступных 2-Ρ…Π»ΠΎΡ€ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-3, 2-Ρ…Π»ΠΎΡ€ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-4, 2-Ρ…Π»ΠΎΡ€ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-5-ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΎΠ²Ρ‹Ρ… кислот с амидоксимами с ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… 2-Ρ…Π»ΠΎΡ€-[3-R1-1,2,4-оксадиазол-5-ΠΈΠ»]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½ΠΎΠ², послС Ρ‡Π΅Π³ΠΎ слСдуСт рСакция Π³ΠΈΠ΄Ρ€Π°Π·ΠΈΠ½ΠΎΠ»ΠΈΠ·Π° с ΠΈΠ·Π±Ρ‹Ρ‚ΠΊΠΎΠΌ Π³ΠΈΠ΄Ρ€Π°Π·ΠΈΠ½ Π³ΠΈΠ΄Ρ€Π°Ρ‚Π°. ΠŸΡ€ΠΎΡ†Π΅ΡΡ продолТаСтся ΠΏΡƒΡ‚Π΅ΠΌ образования эфира с Π·Π°ΠΊΡ€Ρ‹Ρ‚ΠΈΠ΅ΠΌ ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½ΠΎΠ²ΠΎΠ³ΠΎ ΠΊΠΎΠ»ΡŒΡ†Π°, Π·Π°Ρ‚Π΅ΠΌ Ρ‡Π΅Ρ€Π΅Π· Π³ΠΈΠ΄Ρ€ΠΎΠ»ΠΈΠ· ΠΊ уксусной кислотС ΠΌΡ‹ ΠΏΠΎΠ»ΡƒΡ‡Π°Π΅ΠΌ Π°ΠΌΠΈΠ΄Π½Ρ‹Π΅ образования ΠΊΠΎΠ½Π΅Ρ‡Π½Ρ‹Ρ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ².Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π°Ρ Ρ‡Π°ΡΡ‚ΡŒ. Ряд Π½ΠΎΠ²Ρ‹Ρ… 2-[6-(1,2,4-оксадиазол-5-ΠΈΠ»)-, 2-[7-(1,2,4-оксадиазол-5-ΠΈΠ»)-, 2-[8-(1,2,4-оксадиазол-5-ΠΈΠ»)-[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°] ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-3-ΠΈΠ»]Π°Ρ†Π΅Ρ‚Π°ΠΌΠΈΠ΄ΠΎΠ² Π±Ρ‹Π» ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ с Ρ…ΠΎΡ€ΠΎΡˆΠΈΠΌΠΈ Π²Ρ‹Ρ…ΠΎΠ΄Π°ΠΌΠΈ, Π° ΠΈΡ… структуры ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π΅Π½Ρ‹ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ЯМР 1H-спСктроскопии. Π’Π°ΠΊΠΆΠ΅ Π±Ρ‹Π» ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ ΠΏΡ€ΠΎΠ³Π½ΠΎΠ· ΠΈ ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΠ΅ ΠΈΡ… фармакологичСской активности.Π’Ρ‹Π²ΠΎΠ΄Ρ‹. БинтСтичСский ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ получСния Ρ€Π°Π½Π΅Π΅ нСизвСстных прСдставитСлСй 2-[(1,2,4-оксадиазол-5-ΠΈΠ»)-[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ4,3-Π°]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-3-ΠΈΠ»]Π°Ρ†Π΅Ρ‚Π°ΠΌΠΈΠ΄ΠΎΠ² ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ для синтСза Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… [1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½ΠΎΠ²Ρ‹Ρ… ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ….ΠšΠΎΠ½Π΄Π΅Π½ΡΠΎΠ²Π°Π½Ρ– Π³Π΅Ρ‚Π΅Ρ€ΠΎΡ†ΠΈΠΊΠ»Ρ–Ρ‡Π½Ρ– 1,2,4-Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΈ ΠΏΡ€ΠΈΠ²Π΅Ρ€Ρ‚Π°ΡŽΡ‚ΡŒ Π²Π΅Π»ΠΈΠΊΡƒ ΡƒΠ²Π°Π³Ρƒ Π΄ΠΎ сСбС Ρ€Ρ–Π·Π½ΠΎΠΌΠ°Π½Ρ–Ρ‚Π½Ρ–ΡΡ‚ΡŽ Ρ†Ρ–ΠΊΠ°Π²ΠΈΡ… Π±Ρ–ΠΎΠ»ΠΎΠ³Ρ–Ρ‡Π½ΠΈΡ… властивостСй.ΠœΠ΅Ρ‚Π° Ρ€ΠΎΠ±ΠΎΡ‚ΠΈ. Π ΠΎΠ·Ρ€ΠΎΠ±ΠΈΡ‚ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄ синтСзу Π½ΠΎΠ²ΠΈΡ… 2-[(1,2,4-оксадіазол-5-Ρ–Π»)-[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-3-Ρ–Π»]Π°Ρ†Π΅Ρ‚Π°ΠΌΡ–Π΄Ρ–Π² Ρ‚Π° провСсти Π±Ρ–ΠΎΠ»ΠΎΠ³Ρ–Ρ‡Π½Ρƒ ΠΎΡ†Ρ–Π½ΠΊΡƒ синтСзованих сполук.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Ρ‚Π° Ρ—Ρ… обговорСння. Π‘ΠΈΠ½Ρ‚Π΅Π·ΠΎΠ²Π°Π½ΠΎ Π½ΠΈΠ·ΠΊΡƒ Π½ΠΎΠ²ΠΈΡ… ΠΏΠΎΡ…Ρ–Π΄Π½ΠΈΡ… Π°Ρ†Π΅Ρ‚Π°ΠΌΡ–Π΄Ρ–Π², яка ΡΠΊΠ»Π°Π΄Π°Ρ”Ρ‚ΡŒΡΡ Π· 32 Π°Π½Π°Π»ΠΎΠ³Ρ–Π², Ρ‰ΠΎ ΠΌΡ–ΡΡ‚ΡΡ‚ΡŒ 1,2,4-ΠΎΠΊΡΠ°Π΄Ρ–Π°Π·ΠΎΠ»ΡŒΠ½ΠΈΠΉ Ρ†ΠΈΠΊΠ» Ρƒ 6, 7 Ρ‚Π° 8 полоТСннях. Π—Ρ€ΡƒΡ‡Π½Π° схСма синтСзу ΠΏΠΎΡ‡ΠΈΠ½Π°Ρ”Ρ‚ΡŒΡΡ Π· ΠΊΠΎΠΌΠ΅Ρ€Ρ†Ρ–ΠΉΠ½ΠΎ доступних 2-Ρ…Π»ΠΎΡ€ΠΎΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-3-, 2-Ρ…Π»ΠΎΡ€ΠΎΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-4-, 2-Ρ…Π»ΠΎΡ€ΠΎΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-5-ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΎΠ²ΠΈΡ… кислот Π· амідоксимами Π· утворСнням Π²Ρ–Π΄ΠΏΠΎΠ²Ρ–Π΄Π½ΠΈΡ… 2-Ρ…Π»ΠΎΡ€ΠΎ-[3-R1-1,2,4-оксадіазол-5-Ρ–Π»]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½Ρ–Π², після Ρ‡ΠΎΠ³ΠΎ ΠΏΠ΅Ρ€Π΅Π±Ρ–Π³Π°Ρ” рСакція Π³Ρ–Π΄Ρ€Π°Π·ΠΈΠ½ΠΎΠ»Ρ–Π·Ρƒ Π· надлишком Π³Ρ–Π΄Ρ€Π°Π·ΠΈΠ½ Π³Ρ–Π΄Ρ€Π°Ρ‚Ρƒ. ΠŸΡ€ΠΎΡ†Π΅Ρ ΠΏΡ€ΠΎΠ΄ΠΎΠ²ΠΆΡƒΡ”Ρ‚ΡŒΡΡ ΡˆΠ»ΡΡ…ΠΎΠΌ утворСння Π΅Ρ„Ρ–Ρ€Ρƒ Π· закриттям ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½ΠΎΠ²ΠΎΠ³ΠΎ ΠΊΡ–Π»ΡŒΡ†Ρ, ΠΏΠΎΡ‚Ρ–ΠΌ Ρ‡Π΅Ρ€Π΅Π· Π³Ρ–Π΄Ρ€ΠΎΠ»Ρ–Π· Π΄ΠΎ ΠΎΡ†Ρ‚ΠΎΠ²ΠΎΡ— кислоти ΠΌΠΈ ΠΎΡ‚Ρ€ΠΈΠΌΡƒΡ”ΠΌΠΎ Π°ΠΌΡ–Π΄Π½Ρ– утворСння ΠΊΡ–Π½Ρ†Π΅Π²ΠΈΡ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Ρ–Π².Π•ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π° частина. Ряд Π½ΠΎΠ²ΠΈΡ… 2-[6-(1,2,4-оксадіазол-5-Ρ–Π»)-, 2-[7-(1,2,4-оксадіазол-5-Ρ–Π»)-, 2-[8-(1,2,4-оксадіазол-5-Ρ–Π»)-[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-3-Ρ–Π»]Π°Ρ†Π΅Ρ‚Π°ΠΌΡ–Π΄Ρ–Π² Π±ΡƒΠ² ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½ΠΈΠΉ Π· Π΄ΠΎΠ±Ρ€ΠΈΠΌΠΈ Π²ΠΈΡ…ΠΎΠ΄Π°ΠΌΠΈ, Π° Ρ—Ρ… структури ΠΏΡ–Π΄Ρ‚Π²Π΅Ρ€Π΄ΠΆΠ΅Π½Ρ– ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ЯМР 1H-спСктроскопії. Π’Π°ΠΊΠΎΠΆ Π±ΡƒΠ»ΠΎ Π·Ρ€ΠΎΠ±Π»Π΅Π½ΠΎ ΠΏΡ€ΠΎΠ³Π½ΠΎΠ· Ρ‚Π° вивчСння Ρ—Ρ… Ρ„Π°Ρ€ΠΌΠ°ΠΊΠΎΠ»ΠΎΠ³Ρ–Ρ‡Π½ΠΎΡ— активності.Висновки. Π‘ΠΈΠ½Ρ‚Π΅Ρ‚ΠΈΡ‡Π½ΠΈΠΉ ΠΏΡ–Π΄Ρ…Ρ–Π΄ Π΄ΠΎ отримання Ρ€Π°Π½Ρ–ΡˆΠ΅ Π½Π΅Π²Ρ–Π΄ΠΎΠΌΠΈΡ… прСдставників 2-[(1,2,4-оксадіазол-5-Ρ–Π»)-[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-3-Ρ–Π»]Π°Ρ†Π΅Ρ‚Π°ΠΌΡ–Π΄Ρ–Π² ΠΌΠΎΠΆΠ΅ Π±ΡƒΡ‚ΠΈ застосований для синтСзу Ρ€Ρ–Π·Π½ΠΎΠΌΠ°Π½Ρ–Ρ‚Π½ΠΈΡ… Ρ„ΡƒΠ½ΠΊΡ†Ρ–ΠΎΠ½Π°Π»Ρ–Π·ΠΎΠ²Π°Π½ΠΈΡ… [1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½ΠΎΠ²ΠΈΡ… ΠΏΠΎΡ…Ρ–Π΄Π½ΠΈΡ…

    True Dielectric and Ideal Conductor in Theory of the Dielectric Function for Coulomb System

    Full text link
    On the basis of the exact relations the general formula for the static dielectric permittivity e(q,0) for Coulomb system is found in the region of small wave vectors q. The obtained formuladescribes the dielectric function e(q,0) of the Coulomb system in both states in the "metallic" state and in the "dielectric" one. The parameter which determines possible states of the Coulomb system - from the "true" dielectric till the "ideal" conductor is found. The exact relation for the pair correlation function for two-component system of electrons and nuclei g_ei(r) is found for the arbitrary thermodynamic parameters.Comment: 5 pages, no figure

    Linear theory of nonlocal transport in a magnetized plasma

    Full text link
    A system of nonlocal electron-transport equations for small perturbations in a magnetized plasma is derived using the systematic closure procedure of V. Yu. Bychenkov et al., Phys. Rev. Lett. 75, 4405 (1995). Solution to the linearized kinetic equation with a Landau collision operator is obtained in the diffusive approximation. The Fourier components of the longitudinal, oblique, and transversal electron fluxes are found in an explicit form for quasistatic conditions in terms of the generalized forces: the gradients of density and temperature, and the electric field. The full set of nonlocal transport coefficients is given and discussed. Nonlocality of transport enhances electron fluxes across magnetic field above the values given by strongly collisional local theory. Dispersion and damping of magnetohydrodynamic waves in weakly collisional plasmas is discussed. Nonlocal transport theory is applied to the problem of temperature relaxation across the magnetic field in a laser hot spot.Comment: 27 pages, 13 figure

    Comment on ``Damping of energetic gluons and quarks in high-temperature QCD''

    Full text link
    Burgess and Marini have recently pointed out that the leading contribution to the damping rate of energetic gluons and quarks in the QCD plasma, given by γ=cg2ln⁑(1/g)T\gamma=c g^2\ln(1/g)T, can be obtained by simple arguments obviating the need of a fully resummed perturbation theory as developed by Braaten and Pisarski. Their calculation confirmed previous results of Braaten and Pisarski, but contradicted those proposed by Lebedev and Smilga. While agreeing with the general considerations made by Burgess and Marini, I correct their actual calculation of the damping rates, which is based on a wrong expression for the static limit of the resummed gluon propagator. The effect of this, however, turns out to be cancelled fortuitously by another mistake, so as to leave all of their conclusions unchanged. I also verify the gauge independence of the results, which in the corrected calculation arises in a less obvious manner.Comment: 5 page

    ΠŸΠΎΡˆΡƒΠΊ Π½ΠΎΠ²ΠΈΡ… ΠΏΠΎΡ‚Π΅Π½Ρ†Ρ–ΠΉΠ½ΠΈΡ… Ρ–Π½Π³Ρ–Π±Ρ–Ρ‚ΠΎΡ€Ρ–Π² ΠΏΡ€ΠΎΡ‚Π΅Ρ—Π½ΠΊΡ–Π½Π°Π·ΠΈ Pim-1 сСрСд Π°ΠΌΡ–Π΄Ρ–Π² 1,2,4-Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-3-ΠΌΠ΅Ρ‚Π°Π½Π°ΠΌΡ–Π½Ρƒ Π· 1,2,4-ΠΎΠΊΡΠ°Π΄Ρ–Π°Π·ΠΎΠ»ΡŒΠ½ΠΈΠΌ Ρ†ΠΈΠΊΠ»ΠΎΠΌ Ρƒ 7 Ρ‚Π° 8 полоТСннях

    Get PDF
    The Pim-1 enzyme from the serine/threonine protein kinase family is a likely target for the targeted therapy of tumors of hematopoietic and lymphoid tissues. Triazolopyridine is an universal scaffold upon which international scientific programs have been launched to develop potential anticancer agents.Aim. To create a pharmacophore model to find new potential Pim-1 inhibitors; conduct a virtual screening of a simulated base of new 1,2,4-triazolo[4,3-a]pyridine derivatives; develop a method for the synthesis of 1,2,4-triazolo[4,3-a]pyridine-3-methanamines with the 1,2,4-isoxadiazole cycle.Results and discussion. In this study, a ligand-based pharmacophore model for Pim-1 inhibitors was constructed and validated. A virtual screening of the library with 912 compounds resulted in a hit list of 175 compounds. For the synthesis, 15 compounds were selected with the highest pharmacophore-fit score. 15 compounds were synthesized as potential inhibitors of Pim-1 kinase.Experimental part. The synthetic approach has been developed, and systematic series of new amides of (7-(1,2,4-oxadiazol-5-yl)-[1,2,4]triazolo[4,3-a]pyridin-3-yl)methanamine and (8-(1,2,4-oxadiazol-5-yl)-[1,2,4]triazolo[4,3-a]pyridin-3-yl)methanamine have been synthesized.Conclusions. The compounds obtained are potential inhibitors of Pim-1 kinase. Further studies will focus on the determination of the antitumor activity of the compounds synthesized by in vitro and in vivo methods.Π€Π΅Ρ€ΠΌΠ΅Π½Ρ‚ Pim-1 ΠΈΠ· сСмСйства сСрин/Ρ‚Ρ€Π΅ΠΎΠ½ΠΈΠ½ ΠΏΡ€ΠΎΡ‚Π΅ΠΈΠ½ΠΊΠΈΠ½Π°Π·Ρ‹ являСтся вСроятной мишСнью для Ρ‚Π°Ρ€Π³Π΅Ρ‚Π½ΠΎΠΉ Ρ‚Π΅Ρ€Π°ΠΏΠΈΠΈ ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅ΠΉ ΠΊΡ€ΠΎΠ²Π΅Ρ‚Π²ΠΎΡ€Π½ΠΎΠΉ ΠΈ Π»ΠΈΠΌΡ„ΠΎΠΈΠ΄Π½ΠΎΠΉ Ρ‚ΠΊΠ°Π½Π΅ΠΉ. Π’Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½Ρ‹ – это ΡƒΠ½ΠΈΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½Ρ‹ΠΉ скаффолд, Π½Π° Π±Π°Π·Π΅ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ³ΠΎ проводятся ΠΌΠ΅ΠΆΠ΄ΡƒΠ½Π°Ρ€ΠΎΠ΄Π½Ρ‹Π΅ Π½Π°ΡƒΡ‡Π½Ρ‹Π΅ ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΡ‹ ΠΏΠΎ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠ΅ ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΡ€Π°ΠΊΠΎΠ²Ρ‹Ρ… срСдств.ЦСль. Π‘ΠΎΠ·Π΄Π°Ρ‚ΡŒ Ρ„Π°Ρ€ΠΌΠ°ΠΊΠΎΡ„ΠΎΡ€Π½ΡƒΡŽ модСль для поиска Π½ΠΎΠ²Ρ‹Ρ… ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… ΠΈΠ½Π³ΠΈΠ±ΠΈΡ‚ΠΎΡ€ΠΎΠ² Pim-1. ΠŸΡ€ΠΎΠ²Π΅ΡΡ‚ΠΈ Π²ΠΈΡ€Ρ‚ΡƒΠ°Π»ΡŒΠ½Ρ‹ΠΉ скрининг смодСлированной Π±Π°Π·Ρ‹ Π½ΠΎΠ²Ρ‹Ρ… ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ… 1,2,4-Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½ΠΎΠ² ΠΈ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Ρ‚ΡŒ ΠΌΠ΅Ρ‚ΠΎΠ΄ синтСза Π°ΠΌΠΈΠ΄ΠΎΠ² 1,2,4-Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-3-ΠΌΠ΅Ρ‚Π°Π½Π°ΠΌΠΈΠ½Π°, содСрТащих 1,2,4-ΠΈΠ·ΠΎΠΊΡΠ°Π΄ΠΈΠ°Π·ΠΎΠ»ΡŒΠ½Ρ‹ΠΉ Ρ†ΠΈΠΊΠ».Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΈ обсуТдСниС. Π‘ΠΎΠ·Π΄Π°Π½Π° ΠΈ Π²Π°Π»ΠΈΠ΄ΠΈΡ€ΠΎΠ²Π°Π½Π° фармакофорная модСль ΠΈΠ½Π³ΠΈΠ±ΠΈΡ‚ΠΎΡ€ΠΎΠ² Pim-1 Π½Π° основС извСстной ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ ΠΎ структурах Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… Π»ΠΈΠ³Π°Π½Π΄ΠΎΠ². ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ Π²ΠΈΡ€Ρ‚ΡƒΠ°Π»ΡŒΠ½Ρ‹ΠΉ скрининг Π±ΠΈΠ±Π»ΠΈΠΎΡ‚Π΅ΠΊΠΈ ΠΈΠ· 912 соСдинСний, Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠΌ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ³ΠΎ стал список Ρ…ΠΈΡ‚ΠΎΠ² ΠΈΠ· 175 соСдинСний. Для синтСза Π±Ρ‹Π»ΠΈ ΠΎΡ‚ΠΎΠ±Ρ€Π°Π½Ρ‹ 15 соСдинСний с Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ высокой Ρ„Π°Ρ€ΠΌΠ°ΠΊΠΎΡ„ΠΎΡ€Π½ΠΎΠΉ ΠΎΡ†Π΅Π½ΠΊΠΎΠΉ. Π‘ΠΈΠ½Ρ‚Π΅Π·ΠΈΡ€ΠΎΠ²Π°Π½Ρ‹ 15 соСдинСний, ΡΠ²Π»ΡΡŽΡ‰ΠΈΡ…ΡΡ ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΌΠΈ ΠΈΠ½Π³ΠΈΠ±ΠΈΡ‚ΠΎΡ€Π°ΠΌΠΈ ΠΊΠΈΠ½Π°Π·Ρ‹ Pim-1.Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π°Ρ Ρ‡Π°ΡΡ‚ΡŒ. Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Π° схСма, ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠΈ синтСза ΠΈ синтСзированы систСматичСскиС ряды Π½ΠΎΠ²Ρ‹Ρ… Π°ΠΌΠΈΠ΄ΠΎΠ² (7-(1,2,4-оксадиазол-5-ΠΈΠ»)-[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-3-ΠΈΠ»)ΠΌΠ΅Ρ‚Π°Π½Π°ΠΌΠΈΠ½Π° ΠΈ (8-(1,2,4-оксадиазол-5-ΠΈΠ»)-[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΠΈΡ€ΠΈΠ΄ΠΈΠ½-3-ΠΈΠ»)ΠΌΠ΅Ρ‚Π°Π½Π°ΠΌΠΈΠ½Π°.Π’Ρ‹Π²ΠΎΠ΄Ρ‹. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ соСдинСния ΡΠ²Π»ΡΡŽΡ‚ΡΡ ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΌΠΈ ΠΈΠ½Π³ΠΈΠ±ΠΈΡ‚ΠΎΡ€Π°ΠΌΠΈ ΠΊΠΈΠ½Π°Π·Ρ‹ Pim-1. Π”Π°Π»ΡŒΠ½Π΅ΠΉΡˆΠΈΠ΅ исслСдования Π±ΡƒΠ΄ΡƒΡ‚ Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½Ρ‹ Π½Π° выявлСниС ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²ΠΎΠΉ активности синтСзированных соСдинСний ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ in vitro ΠΈ in vivo.Π€Π΅Ρ€ΠΌΠ΅Π½Ρ‚ Pim-1 Π· сімСйства сСрин/Ρ‚Ρ€Π΅ΠΎΠ½Ρ–Π½ ΠΏΡ€ΠΎΡ‚Π΅Ρ—Π½ΠΊΡ–Π½Π°Π· Ρ” ΠΉΠΌΠΎΠ²Ρ–Ρ€Π½ΠΎΡŽ ΠΌΡ–ΡˆΠ΅Π½Π½ΡŽ для Ρ‚Π°Ρ€Π³Π΅Ρ‚Π½ΠΎΡ— Ρ‚Π΅Ρ€Π°ΠΏΡ–Ρ— ΠΏΡƒΡ…Π»ΠΈΠ½ ΠΊΡ€ΠΎΠ²ΠΎΡ‚Π²ΠΎΡ€Π½ΠΎΡ— Ρ‚Π° Π»Ρ–ΠΌΡ„ΠΎΡ—Π΄Π½ΠΎΡ— Ρ‚ΠΊΠ°Π½ΠΈΠ½ΠΈ. Π’Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½ΠΈ – Ρ†Π΅ ΡƒΠ½Ρ–Π²Π΅Ρ€ΡΠ°Π»ΡŒΠ½ΠΈΠΉ скафолд, Π½Π° Π±Π°Π·Ρ– якого Ρ€Π΅Π°Π»Ρ–Π·ΡƒΡŽΡ‚ΡŒΡΡ ΠΌΡ–ΠΆΠ½Π°Ρ€ΠΎΠ΄Π½Ρ– Π½Π°ΡƒΠΊΠΎΠ²Ρ– ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΈ Π· Ρ€ΠΎΠ·Ρ€ΠΎΠ±ΠΊΠΈ ΠΏΠΎΡ‚Π΅Π½Ρ†Ρ–ΠΉΠ½ΠΈΡ… ΠΏΡ€ΠΎΡ‚ΠΈΡ€Π°ΠΊΠΎΠ²ΠΈΡ… засобів.ΠœΠ΅Ρ‚Π°. Π‘Ρ‚Π²ΠΎΡ€ΠΈΡ‚ΠΈ Ρ„Π°Ρ€ΠΌΠ°ΠΊΠΎΡ„ΠΎΡ€Π½Ρƒ модСль для ΠΏΠΎΡˆΡƒΠΊΡƒ Π½ΠΎΠ²ΠΈΡ… ΠΏΠΎΡ‚Π΅Π½Ρ†Ρ–ΠΉΠ½ΠΈΡ… Ρ–Π½Π³Ρ–Π±Ρ–Ρ‚ΠΎΡ€Ρ–Π² Pim-1. ΠŸΡ€ΠΎΠ²Π΅ΡΡ‚ΠΈ Π²Ρ–Ρ€Ρ‚ΡƒΠ°Π»ΡŒΠ½ΠΈΠΉ скринінг Π·ΠΌΠΎΠ΄Π΅Π»ΡŒΠΎΠ²Π°Π½ΠΎΡ— Π±Π°Π·ΠΈ Π½ΠΎΠ²ΠΈΡ… ΠΏΠΎΡ…Ρ–Π΄Π½ΠΈΡ… 1,2,4-Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½Ρƒ Ρ‚Π° Ρ€ΠΎΠ·Ρ€ΠΎΠ±ΠΈΡ‚ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄ синтСзу Π°ΠΌΡ–Π΄Ρ–Π² 1,2,4-Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-3-ΠΌΠ΅Ρ‚Π°Π½Π°ΠΌΡ–Π½Ρƒ, Ρ‰ΠΎ ΠΌΡ–ΡΡ‚ΡΡ‚ΡŒ 1,2,4-Ρ–Π·ΠΎΠΊΡΠ°Π΄Ρ–Π°Π·ΠΎΠ»ΡŒΠ½ΠΈΠΉ Ρ†ΠΈΠΊΠ».Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Ρ‚Π° обговорСння. Π‘Ρ‚Π²ΠΎΡ€Π΅Π½ΠΎ Ρ‚Π° Π²Π°Π»Ρ–Π΄ΠΎΠ²Π°Π½ΠΎ Ρ„Π°Ρ€ΠΌΠ°ΠΊΠΎΡ„ΠΎΡ€Π½Ρƒ модСль Ρ–Π½Π³Ρ–Π±Ρ–Ρ‚ΠΎΡ€Ρ–Π² Pim-1 Π½Π° основі Π²Ρ–Π΄ΠΎΠΌΠΎΡ— Ρ–Π½Ρ„ΠΎΡ€ΠΌΠ°Ρ†Ρ–Ρ— ΠΏΡ€ΠΎ структури Π°ΠΊΡ‚ΠΈΠ²Π½ΠΈΡ… Π»Ρ–Π³Π°Π½Π΄Ρ–Π². ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Π²Ρ–Ρ€Ρ‚ΡƒΠ°Π»ΡŒΠ½ΠΈΠΉ скринінг Π±Ρ–Π±Π»Ρ–ΠΎΡ‚Π΅ΠΊΠΈ Π· 912 сполук, Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠΌ якого став список Ρ…Ρ–Ρ‚Ρ–Π² Ρ–Π· 175 сполук. Для синтСзу Π±ΡƒΠ»ΠΎ Π²Ρ–Π΄Ρ–Π±Ρ€Π°Π½ΠΎ 15 сполук Π· Π½Π°ΠΉΠ²ΠΈΡ‰ΠΎΡŽ Ρ„Π°Ρ€ΠΌΠ°ΠΊΠΎΡ„ΠΎΡ€Π½ΠΎΡŽ ΠΎΡ†Ρ–Π½ΠΊΠΎΡŽ. Π‘ΠΈΠ½Ρ‚Π΅Π·ΠΎΠ²Π°Π½ΠΎ 15 сполук, Ρ‰ΠΎ Ρ” ΠΏΠΎΡ‚Π΅Π½Ρ†Ρ–ΠΉΠ½ΠΈΠΌΠΈ Ρ–Π½Π³Ρ–Π±Ρ–Ρ‚ΠΎΡ€Π°ΠΌΠΈ ΠΊΡ–Π½Π°Π·ΠΈ Pim-1.Π•ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π° частина. Π ΠΎΠ·Ρ€ΠΎΠ±Π»Π΅Π½ΠΎ схСму, ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠΈ синтСзу Ρ‚Π° синтСзовано систСматичні ряди Π½ΠΎΠ²ΠΈΡ… Π°ΠΌΡ–Π΄Ρ–Π² (7-(1,2,4-оксадіазол-5-Ρ–Π»)-[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-3-Ρ–Π»)ΠΌΠ΅Ρ‚Π°Π½Π°ΠΌΡ–Π½Ρƒ Ρ‚Π° (8-(1,2,4-оксадіазол-5-Ρ–Π»)-[1,2,4]Ρ‚Ρ€ΠΈΠ°Π·ΠΎΠ»ΠΎ[4,3-Π°]ΠΏΡ–Ρ€ΠΈΠ΄ΠΈΠ½-3-Ρ–Π»)ΠΌΠ΅Ρ‚Π°Π½Π°ΠΌΡ–Π½Ρƒ.Висновки. ΠžΡ‚Ρ€ΠΈΠΌΠ°Π½Ρ– сполуки Ρ” ΠΏΠΎΡ‚Π΅Π½Ρ†Ρ–ΠΉΠ½ΠΈΠΌΠΈ Ρ–Π½Π³Ρ–Π±Ρ–Ρ‚ΠΎΡ€Π°ΠΌΠΈ ΠΊΡ–Π½Π°Π·ΠΈ Pim-1. ΠŸΠΎΠ΄Π°Π»ΡŒΡˆΡ– дослідТСння Π±ΡƒΠ΄ΡƒΡ‚ΡŒ спрямовані Π½Π° виявлСння ΠΏΡ€ΠΎΡ‚ΠΈΠΏΡƒΡ…Π»ΠΈΠ½Π½ΠΎΡ— активності синтСзованих сполук ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ in vitro Ρ‚Π° in vivo

    Enhanced inverse bremsstrahlung heating rates in a strong laser field

    Full text link
    Test particle studies of electron scattering on ions, in an oscillatory electromagnetic field have shown that standard theoretical assumptions of small angle collisions and phase independent orbits are incorrect for electron trajectories with drift velocities smaller than quiver velocity amplitude. This leads to significant enhancement of the electron energy gain and the inverse bremsstrahlung heating rate in strong laser fields. Nonlinear processes such as Coulomb focusing and correlated collisions of electrons being brought back to the same ion by the oscillatory field are responsible for large angle, head-on scattering processes. The statistical importance of these trajectories has been examined for mono-energetic beam-like, Maxwellian and highly anisotropic electron distribution functions. A new scaling of the inverse bremsstrahlung heating rate with drift velocity and laser intensity is discussed.Comment: 12 pages, 12 figure

    High Temperature Response Functions and the Non-Abelian Kubo Formula

    Full text link
    We describe the relationship between time-ordered and retarded response functions in a plasma. We obtain an expression, including the proper iΟ΅i\epsilon-prescription, for the induced current due to hard thermal loops in a non-Abelian theory, thus giving the non-Abelian generalization of the Kubo formula. The result is closely related to the eikonal for a Chern-Simons theory and is relevant for a gauge-invariant description of Landau damping in the quark-gluon plasma at high temperature.Comment: 14 pages in LaTeX, MIT CTP #2205 and CU-TP #59

    Heating mechanisms in radio frequency driven ultracold plasmas

    Get PDF
    Several mechanisms by which an external electromagnetic field influences the temperature of a plasma are studied analytically and specialized to the system of an ultracold plasma (UCP) driven by a uniform radio frequency (RF) field. Heating through collisional absorption is reviewed and applied to UCPs. Furthermore, it is shown that the RF field modifies the three body recombination process by ionizing electrons from intermediate high-lying Rydberg states and upshifting the continuum threshold, resulting in a suppression of three body recombination. Heating through collisionless absorption associated with the finite plasma size is calculated in detail, revealing a temperature threshold below which collisionless absorption is ineffective.Comment: 14 pages, 7 figure

    Kinetic Equations for Longwavelength Excitations of the Quark-Gluon Plasma

    Get PDF
    We show that longwavelength excitations of the quark-gluon plasma are described by simple kinetic equations which represent the exact equations of motion at leading order in gg. Properties of the so-called ``hard thermal loops'', i.e. the dominant contributions to amplitudes with soft external lines, find in this approach a natural explanation. In particular, their generating functional appears here as the effective action describing long wavelength excitations of the plasma.Comment: January 8, 1993; 8 pages; SPhT/93-
    • …
    corecore