325 research outputs found
Π‘ΠΈΠ½ΡΠ΅Π· Π½ΠΎΠ²ΠΈΡ ΡΠΏΡΡΠΎΡΠΈΠΊΠ»ΡΡΠ½ΠΈΡ N-Π°ΡΠΈΠ»Π·Π°ΠΌΡΡΠ΅Π½ΠΈΡ 2-ΡΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½-4,6-Π΄ΡΠΎΠ½ΡΠ²
A convenient and efficient method for the synthesis of new unsaturated spiro-annulated N-aryl-4,6-dioxopyrimidine-2-thione derivatives has been developed. The resulting compounds can be potential biological active molecules or precursors for further chemical modification.Aim. To develop the methods for the synthesis of new unsaturated spiro-annulated 2-thiopyrimidine-4,6-dione derivatives, which can be used as potentially biological active molecules or precursors for their formation.Results and discussion. By condensation of N-aryl-substituted thioureas and allylmalonic acid using acetic anhydride or acetyl chloride the series of 5-allyl-substituted 2-thiopyrimidinediones has been synthesized. Their further alkylation with allyl bromide or metallyl chloride led to formation of 5,5-dialkenyl derivatives, which were converted to the corresponding unsaturated spirocyclic dioxopyrimidine-2-thiones by ring-closing metathesis.Β Experimental part. The synthesis of the starting compounds and title products was performed by preparative chemical methods, TLC and column chromatography, elemental analysis, NMR-spectroscopy.Conclusions. The efficient three-step synthetic route of new unsaturated spiro-annulated N-aryl-4,6-dioxopyrimidine-2-thione derivatives from the starting N-arylsubstituted thioureas and allylmalonic acid has been developed. The spiro-annulated products obtained can find application in biological and pharmaceutical science or as starting substrates for further chemical modification.Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½ ΡΠ΄ΠΎΠ±Π½ΡΠΉ ΠΈ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΡΠΈΠ½ΡΠ΅Π·Π° Π½ΠΎΠ²ΡΡ
Π½Π΅Π½Π°ΡΡΡΠ΅Π½Π½ΡΡ
ΡΠΏΠΈΡΠΎ-Π°Π½Π½Π΅Π»ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
N-Π°ΡΠΈΠ»Π·Π°ΠΌΠ΅ΡΠ΅Π½Π½ΡΡ
2-ΡΠΈΠΎΠΏΠΈΡΠΈΠΌΠΈΠ΄ΠΈΠ½-4,6-Π΄ΠΈΠΎΠ½ΠΎΠ². ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΡ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΡΠΌΠΈ Π±ΠΈΠΎΠ°ΠΊΡΠΈΠ²Π½ΡΠΌΠΈ ΠΌΠΎΠ»Π΅ΠΊΡΠ»Π°ΠΌΠΈ ΠΈΠ»ΠΈ ΠΈΡΡ
ΠΎΠ΄Π½ΡΠΌΠΈ Π²Π΅ΡΠ΅ΡΡΠ²Π°ΠΌΠΈ Π΄Π»Ρ Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅ΠΉ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ.Π¦Π΅Π»Ρ ΡΠ°Π±ΠΎΡΡ β ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠ° ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΡ Π½ΠΎΠ²ΡΡ
Π½Π΅Π½Π°ΡΡΡΠ΅Π½Π½ΡΡ
ΡΠΏΠΈΡΠΎ-Π°Π½Π½Π΅Π»ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΡΡ
2-ΡΠΈΠΎΠΏΠΈΡΠΈΠΌΠΈΠ΄ΠΈΠ½-4,6-Π΄ΠΈΠΎΠ½Π° ΠΊΠ°ΠΊ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΡΡ
Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈ Π°ΠΊΡΠΈΠ²Π½ΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΈΠ»ΠΈ ΠΏΠΎΠ»ΡΠΏΡΠΎΠ΄ΡΠΊΡΠΎΠ² Π΄Π»Ρ ΠΈΡ
ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΡ.Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈ ΠΈΡ
ΠΎΠ±ΡΡΠΆΠ΄Π΅Π½ΠΈΠ΅. ΠΠΎΠ½Π΄Π΅Π½ΡΠ°ΡΠΈΠ΅ΠΉ N-Π°ΡΠΈΠ»Π·Π°ΠΌΠ΅ΡΠ΅Π½Π½ΡΡ
ΡΠΈΠΎΠΌΠΎΡΠ΅Π²ΠΈΠ½ ΠΈ Π°Π»Π»ΠΈΠ»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΠΉ ΠΊΠΈΡΠ»ΠΎΡΡ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠΊΡΡΡΠ½ΠΎΠ³ΠΎ Π°Π½Π³ΠΈΠ΄ΡΠΈΠ΄Π° ΠΈΠ»ΠΈ Π°ΡΠ΅ΡΠΈΠ»Ρ
Π»ΠΎΡΠΈΠ΄Π° ΡΠΈΠ½ΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ ΡΡΠ΄ 5-Π°Π»Π»ΠΈΠ»Π·Π°ΠΌΠ΅ΡΠ΅Π½Π½ΡΡ
2-ΡΠΈΠΎΠΏΠΈΡΠΈΠΌΠΈΠ΄ΠΈΠ½Π΄ΠΈΠΎΠ½ΠΎΠ². ΠΡΠΈ ΠΈΡ
ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅ΠΌ Π°Π»ΠΊΠΈΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ Π°Π»Π»ΠΈΠ»Π±ΡΠΎΠΌΠΈΠ΄ΠΎΠΌ ΠΈΠ»ΠΈ ΠΌΠ΅ΡΠ°Π»Π»ΠΈΠ»Ρ
Π»ΠΎΡΠΈΠ΄ΠΎΠΌ ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ 5,5-Π΄ΠΈΠ°Π»ΠΊΠ΅Π½ΠΈΠ»ΡΠ½ΡΠ΅ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΡΠ΅, ΠΊΠΎΡΠΎΡΡΠ΅ ΡΠ΅Π°ΠΊΡΠΈΡΠΌΠΈ ΠΌΠ΅ΡΠ°ΡΠ΅Π·ΠΈΡΠ° Ρ Π·Π°ΠΊΡΡΡΠΈΠ΅ΠΌ ΡΠΈΠΊΠ»Π° Π±ΡΠ»ΠΈ ΠΊΠΎΠ½Π²Π΅ΡΡΠΈΡΠΎΠ²Π°Π½Ρ Π² ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΠ΅ Π½Π΅ΠΏΡΠ΅Π΄Π΅Π»ΡΠ½ΡΠ΅ ΡΠΏΠΈΡΠΎΡΠΈΠΊΠ»ΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π΄ΠΈΠΎΠΊΡΠΎΠΏΠΈΡΠΈΠΌΠΈΠ΄ΠΈΠ½-2-ΡΠΈΠΎΠ½Ρ.Β Β ΠΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½Π°Ρ ΡΠ°ΡΡΡ. Π‘ΠΈΠ½ΡΠ΅Π· ΠΈΡΡ
ΠΎΠ΄Π½ΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΈ ΡΠ΅Π»Π΅Π²ΡΡ
ΠΏΡΠΎΠ΄ΡΠΊΡΠΎΠ² ΠΊΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΈΠ²Π½ΠΎΠΉ Ρ
ΠΈΠΌΠΈΠΈ; ΠΎΡΠΈΡΡΠΊΠ° ΠΈ ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΡ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈΡΡ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΡΠΎΠ½ΠΊΠΎΡΠ»ΠΎΠΉΠ½ΠΎΠΉ ΠΈ ΠΊΠΎΠ»ΠΎΠ½ΠΎΡΠ½ΠΎΠΉ Ρ
ΡΠΎΠΌΠ°ΡΠΎΠ³ΡΠ°ΡΠΈΠΈ, ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π°, ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠ΅ΠΉ Π―ΠΠ .ΠΡΠ²ΠΎΠ΄Ρ. Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠΉ ΡΡΠ΅Ρ
ΡΡΠ°Π΄ΠΈΠΉΠ½ΡΠΉ ΠΏΡΡΡ ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΡ ΠΈΠ· ΠΈΡΡ
ΠΎΠ΄Π½ΡΡ
ΡΠΈΠΎΠΌΠΎΡΠ΅Π²ΠΈΠ½ ΠΈ Π°Π»Π»ΠΈΠ»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΠΉ ΠΊΠΈΡΠ»ΠΎΡΡ Π½ΠΎΠ²ΡΡ
Π½Π΅Π½Π°ΡΡΡΠ΅Π½Π½ΡΡ
ΡΠΏΠΈΡΠΎ-Π°Π½Π½Π΅Π»ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΡΡ
N-Π°ΡΠΈΠ»-4,6-Π΄ΠΈΠΎΠΊΡΠΎΠΏΠΈΡΠΈΠΌΠΈΠ΄ΠΈΠ½-2-ΡΠΈΠΎΠ½Π°. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠΏΠΈΡΠΎΡΠΈΠΊΠ»ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΡΠΎΠ΄ΡΠΊΡΡ ΠΌΠΎΠ³ΡΡ Π½Π°ΠΉΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π² Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΈ ΡΠ°ΡΠΌΠ°ΡΠ΅Π²ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π½Π°ΡΠΊΠ΅, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°ΡΡΡΡ ΠΊΠ°ΠΊ ΠΈΡΡ
ΠΎΠ΄Π½ΡΠ΅ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΡ Π΄Π»Ρ Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅ΠΉ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ.Π ΠΎΠ·ΡΠΎΠ±Π»Π΅Π½ΠΎ Π·ΡΡΡΠ½ΠΈΠΉ ΡΠ° Π΅ΡΠ΅ΠΊΡΠΈΠ²Π½ΠΈΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΡΠΈΠ½ΡΠ΅Π·Ρ Π½ΠΎΠ²ΠΈΡ
Π½Π΅Π½Π°ΡΠΈΡΠ΅Π½ΠΈΡ
ΡΠΏΡΡΠΎ-Π°Π½Π΅Π»ΡΠΎΠ²Π°Π½ΠΈΡ
N-Π°ΡΠΈΠ»Π·Π°ΠΌΡΡΠ΅Π½ΠΈΡ
2-ΡΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½-4,6-Π΄ΡΠΎΠ½ΡΠ². ΠΠ΄Π΅ΡΠΆΠ°Π½Ρ ΡΠΏΠΎΠ»ΡΠΊΠΈ ΠΌΠΎΠΆΡΡΡ Π±ΡΡΠΈ ΠΏΠΎΡΠ΅Π½ΡΡΠΉΠ½ΠΈΠΌΠΈ Π±ΡΠΎΠ°ΠΊΡΠΈΠ²Π½ΠΈΠΌΠΈ ΠΌΠΎΠ»Π΅ΠΊΡΠ»Π°ΠΌΠΈ Π°Π±ΠΎ ΠΏΡΠ΅ΠΊΡΡΡΠΎΡΠ°ΠΌΠΈ Π΄Π»Ρ ΠΏΠΎΠ΄Π°Π»ΡΡΠΎΡ Ρ
ΡΠΌΡΡΠ½ΠΎΡ ΠΌΠΎΠ΄ΠΈΡΡΠΊΠ°ΡΡΡ. ΠΠ΅ΡΠ° ΡΠΎΠ±ΠΎΡΠΈ β ΡΠΎΠ·ΡΠΎΠ±ΠΊΠ° ΠΌΠ΅ΡΠΎΠ΄ΡΠ² ΠΎΠ΄Π΅ΡΠΆΠ°Π½Π½Ρ Π½ΠΎΠ²ΠΈΡ
Π½Π΅Π½Π°ΡΠΈΡΠ΅Π½ΠΈΡ
ΡΠΏΡΡΠΎ-Π°Π½Π΅Π»ΡΠΎΠ²Π°Π½ΠΈΡ
ΠΏΠΎΡ
ΡΠ΄Π½ΠΈΡ
2-ΡΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½-4,6-Π΄ΡΠΎΠ½Ρ ΡΠΊ ΠΏΠΎΡΠ΅Π½ΡΡΠΉΠ½ΠΈΡ
Π±ΡΠΎΠ»ΠΎΠ³ΡΡΠ½ΠΎ Π°ΠΊΡΠΈΠ²Π½ΠΈΡ
ΡΠΏΠΎΠ»ΡΠΊ Π°Π±ΠΎ Π½Π°ΠΏΡΠ²ΠΏΡΠΎΠ΄ΡΠΊΡΡΠ² Π΄Π»Ρ ΡΡ
ΠΎΡΡΠΈΠΌΠ°Π½Π½Ρ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΠΈ ΡΠ° ΡΡ
ΠΎΠ±Π³ΠΎΠ²ΠΎΡΠ΅Π½Π½Ρ. ΠΠΎΠ½Π΄Π΅Π½ΡΠ°ΡΡΡΡN-Π°ΡΠΈΠ»Π·Π°ΠΌΡΡΠ΅Π½ΠΈΡ
ΡΡΠΎΡΠ΅ΡΠΎΠ²ΠΈΠ½ ΡΠ° Π°Π»ΡΠ»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΡ ΠΊΠΈΡΠ»ΠΎΡΠΈ ΡΠ· Π·Π°ΡΡΠΎΡΡΠ²Π°Π½Π½ΡΠΌ ΠΎΡΡΠΎΠ²ΠΎΠ³ΠΎ Π°Π½Π³ΡΠ΄ΡΠΈΠ΄Ρ Π°Π±ΠΎ Π°ΡΠ΅ΡΠΈΠ»Ρ
Π»ΠΎΡΠΈΠ΄Ρ ΡΠΈΠ½ΡΠ΅Π·ΠΎΠ²Π°Π½ΠΎ ΡΠ΅ΡΡΡ 5-Π°Π»ΡΠ»Π·Π°ΠΌΡΡΠ΅Π½ΠΈΡ
2-ΡΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½Π΄ΡΠΎΠ½ΡΠ². ΠΡΠΈ ΠΏΠΎΠ΄Π°Π»ΡΡΠΎΠΌΡ ΡΡ
Π°Π»ΠΊΡΠ»ΡΠ²Π°Π½Π½Ρ Π°Π»ΡΠ»Π±ΡΠΎΠΌΡΠ΄ΠΎΠΌ Π°Π±ΠΎ ΠΌΠ΅ΡΠ°Π»ΡΠ»Ρ
Π»ΠΎΡΠΈΠ΄ΠΎΠΌ ΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΎ 5,5-Π΄ΡΠ°Π»ΠΊΠ΅Π½ΡΠ»ΡΠ½Ρ ΠΏΠΎΡ
ΡΠ΄Π½Ρ, ΡΠΊΡ ΡΠ΅Π°ΠΊΡΡΡΠΌΠΈ ΠΌΠ΅ΡΠ°ΡΠ΅Π·ΠΈΡΡ ΡΠ· Π·Π°ΠΊΡΠΈΡΡΡΠΌ ΡΠΈΠΊΠ»Ρ Π±ΡΠ»ΠΎ ΠΏΠ΅ΡΠ΅ΡΠ²ΠΎΡΠ΅Π½ΠΎ Π½Π° Π²ΡΠ΄ΠΏΠΎΠ²ΡΠ΄Π½Ρ Π½Π΅Π½Π°ΡΠΈΡΠ΅Π½Ρ ΡΠΏΡΡΠΎΡΠΈΠΊΠ»ΡΡΠ½Ρ Π΄ΡΠΎΠΊΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½-2-ΡΡΠΎΠ½ΠΈ.ΠΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½Π° ΡΠ°ΡΡΠΈΠ½Π°. Π‘ΠΈΠ½ΡΠ΅Π· Π²ΠΈΡ
ΡΠ΄Π½ΠΈΡ
ΡΠΏΠΎΠ»ΡΠΊ ΡΠ° ΡΡΠ»ΡΠΎΠ²ΠΈΡ
ΠΏΡΠΎΠ΄ΡΠΊΡΡΠ² ΠΊΠ»Π°ΡΠΈΡΠ½ΠΈΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΈΠ²Π½ΠΎΡ Ρ
ΡΠΌΡΡ; ΠΎΡΠΈΡΡΠΊΡ ΡΠ° ΡΠ΄Π΅Π½ΡΠΈΡΡΠΊΠ°ΡΡΡ ΠΎΡΡΠΈΠΌΠ°Π½ΠΈΡ
ΡΠΏΠΎΠ»ΡΠΊ Π·Π΄ΡΠΉΡΠ½Π΅Π½ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΡΠΎΠ½ΠΊΠΎΡΠ°ΡΠΎΠ²ΠΎΡ ΡΠ° ΠΊΠΎΠ»ΠΎΠ½ΠΊΠΎΠ²ΠΎΡ Ρ
ΡΠΎΠΌΠ°ΡΠΎΠ³ΡΠ°ΡΡΡ, Π΅Π»Π΅ΠΌΠ΅Π½ΡΠ½ΠΈΠΌ Π°Π½Π°Π»ΡΠ·ΠΎΠΌ, Π―ΠΠ -ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΡΡΡ.ΠΠΈΡΠ½ΠΎΠ²ΠΊΠΈ. Π ΠΎΠ·ΡΠΎΠ±Π»Π΅Π½ΠΎ Π΅ΡΠ΅ΠΊΡΠΈΠ²Π½ΠΈΠΉ ΡΡΠΈΡΡΠ°Π΄ΡΠΉΠ½ΠΈΠΉ ΡΠ»ΡΡ
ΠΎΡΡΠΈΠΌΠ°Π½Π½Ρ Π· Π²ΠΈΡ
ΡΠ΄Π½ΠΈΡ
ΡΡΠΎΡΠ΅ΡΠΎΠ²ΠΈΠ½ ΡΠ° Π°Π»ΡΠ»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΡ ΠΊΠΈΡΠ»ΠΎΡΠΈ Π½ΠΎΠ²ΠΈΡ
Π½Π΅Π½Π°ΡΠΈΡΠ΅Π½ΠΈΡ
ΡΠΏΡΡΠΎ-Π°Π½Π΅Π»ΡΠΎΠ²Π°Π½ΠΈΡ
ΠΏΠΎΡ
ΡΠ΄Π½ΠΈΡ
N-Π°ΡΠΈΠ»-4,6-Π΄ΡΠΎΠΊΡΠΎΠΏΡΡΠΈΠΌΡΠ΄ΠΈΠ½-2-ΡΡΠΎΠ½Ρ. ΠΠ΄Π΅ΡΠΆΠ°Π½Ρ ΡΠΏΡΡΠΎΡΠΈΠΊΠ»ΡΡΠ½Ρ ΠΏΡΠΎΠ΄ΡΠΊΡΠΈ ΠΌΠΎΠΆΡΡΡ Π·Π½Π°ΠΉΡΠΈ Π·Π°ΡΡΠΎΡΡΠ²Π°Π½Π½Ρ Π² Π±ΡΠΎΠ»ΠΎΠ³ΡΡ ΡΠ° ΡΠ°ΡΠΌΠ°ΡΠ΅Π²ΡΠΈΡΠ½ΡΠΉ Π½Π°ΡΡΡ, Π°Π±ΠΎ Π²ΠΈΠΊΠΎΡΠΈΡΡΠΎΠ²ΡΠ²Π°ΡΠΈΡΡ ΡΠΊ Π²ΠΈΡ
ΡΠ΄Π½Ρ ΡΠΏΠΎΠ»ΡΠΊΠΈ Π΄Π»Ρ ΠΏΠΎΠ΄Π°Π»ΡΡΠΎΡ Ρ
ΡΠΌΡΡΠ½ΠΎΡ ΠΌΠΎΠ΄ΠΈΡΡΠΊΠ°ΡΡΡ
Retrotransposon activation contributes to neurodegeneration in a Drosophila TDP-43 model of ALS
Amyotrophic lateral sclerosis (ALS) and frontotemporal lobar degeneration (FTLD) are two incurable neurodegenerative disorders that exist on a symptomological spectrum and share both genetic underpinnings and pathophysiological hallmarks. Functional abnormality of TAR DNA-binding protein 43 (TDP-43), an aggregation-prone RNA and DNA binding protein, is observed in the vast majority of both familial and sporadic ALS cases and in ~40% of FTLD cases, but the cascade of events leading to cell death are not understood. We have expressed human TDP-43 (hTDP-43) in Drosophila neurons and glia, a model that recapitulates many of the characteristics of TDP-43-linked human disease including protein aggregation pathology, locomotor impairment, and premature death. We report that such expression of hTDP-43 impairs small interfering RNA (siRNA) silencing, which is the major post-transcriptional mechanism of retrotransposable element (RTE) control in somatic tissue. This is accompanied by de-repression of a panel of both LINE and LTR families of RTEs, with somewhat different elements being active in response to hTDP-43 expression in glia versus neurons. hTDP-43 expression in glia causes an early and severe loss of control of a specific RTE, the endogenous retrovirus (ERV) gypsy. We demonstrate that gypsy causes the degenerative phenotypes in these flies because we are able to rescue the toxicity of glial hTDP-43 either by genetically blocking expression of this RTE or by pharmacologically inhibiting RTE reverse transcriptase activity. Moreover, we provide evidence that activation of DNA damage-mediated programmed cell death underlies both neuronal and glial hTDP-43 toxicity, consistent with RTE-mediated effects in both cell types. Our findings suggest a novel mechanism in which RTE activity contributes to neurodegeneration in TDP-43-mediated diseases such as ALS and FTLD
Feasibility of a Small, Rapid Optical-to-IR Response, Next Generation Gamma Ray Burst Mission
We present motivations for and study feasibility of a small, rapid optical to
IR response gamma ray burst (GRB) space observatory. By analyzing existing GRB
data, we give realistic detection rates for X-ray and optical/IR instruments of
modest size under actual flight conditions. Given new capabilities of fast
optical/IR response (about 1 s to target) and simultaneous multi-band imaging,
such an observatory can have a reasonable event rate, likely leading to new
science. Requiring a Swift-like orbit, duty cycle, and observing constraints, a
Swift-BAT scaled down to 190 square cm of detector area would still detect and
locate about 27 GRB per yr. for a trigger threshold of 6.5 sigma. About 23
percent of X-ray located GRB would be detected optically for a 10 cm diameter
instrument (about 6 per yr. for the 6.5 sigma X-ray trigger).Comment: Elaborated text version of a poster presented at 2012 Malaga/Marbella
symposiu
Loss of Pi-Junction Behaviour in an Interacting Impurity Josephson Junction
Using a generalization of the non-crossing approximation which incorporates
Andreev reflection, we study the properties of an infinite-U Anderson impurity
coupled to two superconducting leads. In the regime where and
are comparable, we find that the position of the sub-gap resonance in the
impurity spectral function develops a strong anomalous phase dependence-- its
energy is a minimum when the phase difference between the superconductors is
equal to . Calculating the Josephson current through the impurity, we find
that -junction behaviour is lost as the position of the bound-state moves
above the Fermi energy.Comment: 4 pages, 4 figures; labelling of Fig. 3 corrected; final published
form, only trivial change
Quantum Melting and Absence of Bose-Einstein Condensation in Two-Dimensional Vortex Matter
We demonstrate that quantum fluctuations suppress Bose-Einstein condensation
of quasi-two-dimensional bosons in a rapidly-rotating trap. Our conclusions
rest in part on an effective-Lagrangian description of the triangular vortex
lattice, and in part on microscopic Bogoliubov equations in the rapid-rotation
limit. We obtain analytic expressions for the collective-excitation dispersion,
which, in a rotating system, is quadratic rather than linear. Our estimates for
the boson filling factor at which the vortex lattice melts at zero temperature
due to quantum fluctuations are consistent with recent exact-diagonalization
calculations.Comment: 4 pages, 1 figures, version to appear in Phys. Rev. Let
Quantum Phases of Vortices in Rotating Bose-Einstein Condensates
We investigate the groundstates of weakly interacting bosons in a rotating
trap as a function of the number of bosons, , and the average number of
vortices, . We identify the filling fraction as the
parameter controlling the nature of these states. We present results indicating
that, as a function of , there is a zero temperature {\it phase
transition} between a triangular vortex lattice phase, and strongly-correlated
vortex liquid phases. The vortex liquid phases appear to be the Read-Rezayi
parafermion states
Simple Bosonization Solution of the 2-channel Kondo Model: I. Analytical Calculation of Finite-Size Crossover Spectrum
We present in detail a simple, exact solution of the anisotropic 2-channel
Kondo (2CK) model at its Toulouse point. We reduce the model to a quadratic
resonant-level model by generalizing the bosonization-refermionization approach
of Emery and Kivelson to finite system size, but improve their method in two
ways: firstly, we construct all boson fields and Klein factors explicitly in
terms of the model's original fermion operators , and secondly
we clarify explicitly how the Klein factors needed when refermionizing act on
the original Fock space. This enables us to explicitly follow the adiabatic
evolution of the 2CK model's free-fermion states to its exact eigenstates,
found by simply diagonalizing the resonant-level model for arbitrary magnetic
fields and spin-flip coupling strengths. In this way we obtain an {\em
analytic} description of the cross-over from the free to the non-Fermi-liquid
fixed point. At the latter, it is remarkably simple to recover the conformal
field theory results for the finite-size spectrum (implying a direct proof of
Affleck and Ludwig's fusion hypothesis). By analyzing the finite-size spectrum,
we directly obtain the operator content of the 2CK fixed point and the
dimension of various relevant and irrelevant perturbations. Our method can
easily be generalized to include various symmetry-breaking perturbations.
Furthermore it establishes instructive connections between different
renormalization group schemes such as poor man's scaling, Anderson-Yuval type
scaling, the numerical renormalization group and finite-size scaling.Comment: 35 pages Revtex, 7 figures, submitted to Phys. Rev.
Pairing Symmetry Competition in Organic Superconductors
A review is given on theoretical studies concerning the pairing symmetry in
organic superconductors. In particular, we focus on (TMTSF)X and
-(BEDT-TTF)X, in which the pairing symmetry has been extensively
studied both experimentally and theoretically. Possibilities of various pairing
symmetry candidates and their possible microscopic origin are discussed. Also
some tests for determining the actual pairing symmtery are surveyed.Comment: 16 pages, 8 figures, to be published in J. Phys. Soc. Jpn., special
issue on "Organic Conductors
Vortex liquids and vortex quantum Hall states in trapped rotating Bose gases
We discuss the feasibility of quantum Hall states of vortices in trapped
low-density two-dimensional Bose gases with large particle interactions. For
interaction strengths larger than a critical dimensionless 2D coupling constant
, upon increasing the rotation frequency, the system is shown
to spatially separate into vortex lattice and melted vortex lattice (vortex
liquid) phases. At a first critical frequency, the lattice melts completely,
and strongly correlated vortex and particle quantum Hall liquids coexist in
inner respectively outer regions of the gas cloud. Finally, at a second
critical frequency, the vortex liquid disappears and the strongly correlated
particle quantum Hall state fills the whole sample.Comment: 11 pages, 3 figures; to appear in J. Phys.
Thermal conductivity via magnetic excitations in spin-chain materials
We discuss the recent progress and the current status of experimental
investigations of spin-mediated energy transport in spin-chain and spin-ladder
materials with antiferromagnetic coupling. We briefly outline the central
results of theoretical studies on the subject but focus mainly on recent
experimental results that were obtained on materials which may be regarded as
adequate physical realizations of the idealized theoretical model systems. Some
open questions and unsettled issues are also addressed.Comment: 17 pages, 4 figure
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