325 research outputs found

    Π‘ΠΈΠ½Ρ‚Π΅Π· Π½ΠΎΠ²ΠΈΡ… спіроциклічних N-Π°Ρ€ΠΈΠ»Π·Π°ΠΌΡ–Ρ‰Π΅Π½ΠΈΡ… 2-Ρ‚Ρ–ΠΎΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½-4,6-Π΄Ρ–ΠΎΠ½Ρ–Π²

    Get PDF
    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·Ρ€Π°Π±ΠΎΡ‚Π°Π½ ΡƒΠ΄ΠΎΠ±Π½Ρ‹ΠΉ ΠΈ эффСктивный ΠΌΠ΅Ρ‚ΠΎΠ΄ синтСза Π½ΠΎΠ²Ρ‹Ρ… нСнасыщСнных спиро-Π°Π½Π½Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… N-Π°Ρ€ΠΈΠ»Π·Π°ΠΌΠ΅Ρ‰Π΅Π½Π½Ρ‹Ρ… 2-Ρ‚ΠΈΠΎΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½-4,6-Π΄ΠΈΠΎΠ½ΠΎΠ². ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ соСдинСния ΠΌΠΎΠ³ΡƒΡ‚ Π±Ρ‹Ρ‚ΡŒ ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΌΠΈ Π±ΠΈΠΎΠ°ΠΊΡ‚ΠΈΠ²Π½Ρ‹ΠΌΠΈ ΠΌΠΎΠ»Π΅ΠΊΡƒΠ»Π°ΠΌΠΈ ΠΈΠ»ΠΈ исходными вСщСствами для дальнСйшСй химичСской ΠΌΠΎΠ΄ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ.ЦСль Ρ€Π°Π±ΠΎΡ‚Ρ‹ – Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠ° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² получСния Π½ΠΎΠ²Ρ‹Ρ… нСнасыщСнных спиро-Π°Π½Π½Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ… 2-Ρ‚ΠΈΠΎΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½-4,6-Π΄ΠΈΠΎΠ½Π° ΠΊΠ°ΠΊ ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… биологичСски Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… соСдинСний ΠΈΠ»ΠΈ ΠΏΠΎΠ»ΡƒΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ² для ΠΈΡ… получСния.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΈ ΠΈΡ… обсуТдСниС. ΠšΠΎΠ½Π΄Π΅Π½ΡΠ°Ρ†ΠΈΠ΅ΠΉ N-Π°Ρ€ΠΈΠ»Π·Π°ΠΌΠ΅Ρ‰Π΅Π½Π½Ρ‹Ρ… Ρ‚ΠΈΠΎΠΌΠΎΡ‡Π΅Π²ΠΈΠ½ ΠΈ Π°Π»Π»ΠΈΠ»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΠΉ кислоты с использованиСм уксусного Π°Π½Π³ΠΈΠ΄Ρ€ΠΈΠ΄Π° ΠΈΠ»ΠΈ Π°Ρ†Π΅Ρ‚ΠΈΠ»Ρ…Π»ΠΎΡ€ΠΈΠ΄Π° синтСзирован ряд 5-Π°Π»Π»ΠΈΠ»Π·Π°ΠΌΠ΅Ρ‰Π΅Π½Π½Ρ‹Ρ… 2-Ρ‚ΠΈΠΎΠΏΠΈΡ€ΠΈΠΌΠΈΠ΄ΠΈΠ½Π΄ΠΈΠΎΠ½ΠΎΠ². ΠŸΡ€ΠΈ ΠΈΡ… ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅ΠΌ Π°Π»ΠΊΠΈΠ»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠΈ Π°Π»Π»ΠΈΠ»Π±Ρ€ΠΎΠΌΠΈΠ΄ΠΎΠΌ ΠΈΠ»ΠΈ ΠΌΠ΅Ρ‚Π°Π»Π»ΠΈΠ»Ρ…Π»ΠΎΡ€ΠΈΠ΄ΠΎΠΌ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ 5,5-Π΄ΠΈΠ°Π»ΠΊΠ΅Π½ΠΈΠ»ΡŒΠ½Ρ‹Π΅ ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Π΅, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ рСакциями мСтатСзиса с Π·Π°ΠΊΡ€Ρ‹Ρ‚ΠΈΠ΅ΠΌ Ρ†ΠΈΠΊΠ»Π° Π±Ρ‹Π»ΠΈ ΠΊΠΎΠ½Π²Π΅Ρ€Ρ‚ΠΈΡ€ΠΎΠ²Π°Π½Ρ‹ Π² ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΠ΅ Π½Π΅ΠΏΡ€Π΅Π΄Π΅Π»ΡŒΠ½Ρ‹Π΅ спироцикличСскиС диоксопиримидин-2-Ρ‚ΠΈΠΎΠ½Ρ‹.Β  Β Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π°Ρ Ρ‡Π°ΡΡ‚ΡŒ. Π‘ΠΈΠ½Ρ‚Π΅Π· исходных соСдинСний ΠΈ Ρ†Π΅Π»Π΅Π²Ρ‹Ρ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ² классичСскими ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΈΠ²Π½ΠΎΠΉ Ρ…ΠΈΠΌΠΈΠΈ; очистка ΠΈ идСнтификация ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… соСдинСний ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈΡΡŒ ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ тонкослойной ΠΈ ΠΊΠΎΠ»ΠΎΠ½ΠΎΡ‡Π½ΠΎΠΉ Ρ…Ρ€ΠΎΠΌΠ°Ρ‚ΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ, ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ элСмСнтного Π°Π½Π°Π»ΠΈΠ·Π°, спСктроскопиСй ЯМР.Π’Ρ‹Π²ΠΎΠ΄Ρ‹. Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½ эффСктивный трСхстадийный ΠΏΡƒΡ‚ΡŒ получСния ΠΈΠ· исходных Ρ‚ΠΈΠΎΠΌΠΎΡ‡Π΅Π²ΠΈΠ½ ΠΈ Π°Π»Π»ΠΈΠ»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΠΉ кислоты Π½ΠΎΠ²Ρ‹Ρ… нСнасыщСнных спиро-Π°Π½Π½Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ… N-Π°Ρ€ΠΈΠ»-4,6-диоксопиримидин-2-Ρ‚ΠΈΠΎΠ½Π°. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ спироцикличСскиС ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Ρ‹ ΠΌΠΎΠ³ΡƒΡ‚ Π½Π°ΠΉΡ‚ΠΈ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π² Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΈ фармацСвтичСской Π½Π°ΡƒΠΊΠ΅, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΠΎΠ²Π°Ρ‚ΡŒΡΡ ΠΊΠ°ΠΊ исходныС соСдинСния для дальнСйшСй химичСской ΠΌΠΎΠ΄ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ.Π ΠΎΠ·Ρ€ΠΎΠ±Π»Π΅Π½ΠΎ Π·Ρ€ΡƒΡ‡Π½ΠΈΠΉ Ρ‚Π° Π΅Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΈΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ синтСзу Π½ΠΎΠ²ΠΈΡ… нСнасичСних спіро-Π°Π½Π΅Π»ΡŒΠΎΠ²Π°Π½ΠΈΡ… N-Π°Ρ€ΠΈΠ»Π·Π°ΠΌΡ–Ρ‰Π΅Π½ΠΈΡ… 2-Ρ‚Ρ–ΠΎΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½-4,6-Π΄Ρ–ΠΎΠ½Ρ–Π². ΠžΠ΄Π΅Ρ€ΠΆΠ°Π½Ρ– сполуки ΠΌΠΎΠΆΡƒΡ‚ΡŒ Π±ΡƒΡ‚ΠΈ ΠΏΠΎΡ‚Π΅Π½Ρ†Ρ–ΠΉΠ½ΠΈΠΌΠΈ Π±Ρ–ΠΎΠ°ΠΊΡ‚ΠΈΠ²Π½ΠΈΠΌΠΈ ΠΌΠΎΠ»Π΅ΠΊΡƒΠ»Π°ΠΌΠΈ Π°Π±ΠΎ прСкурсорами для ΠΏΠΎΠ΄Π°Π»ΡŒΡˆΠΎΡ— Ρ…Ρ–ΠΌΡ–Ρ‡Π½ΠΎΡ— ΠΌΠΎΠ΄ΠΈΡ„Ρ–ΠΊΠ°Ρ†Ρ–Ρ—. ΠœΠ΅Ρ‚Π° Ρ€ΠΎΠ±ΠΎΡ‚ΠΈ – Ρ€ΠΎΠ·Ρ€ΠΎΠ±ΠΊΠ° ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ–Π² одСрТання Π½ΠΎΠ²ΠΈΡ… нСнасичСних спіро-Π°Π½Π΅Π»ΡŒΠΎΠ²Π°Π½ΠΈΡ… ΠΏΠΎΡ…Ρ–Π΄Π½ΠΈΡ… 2-Ρ‚Ρ–ΠΎΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½-4,6-Π΄Ρ–ΠΎΠ½Ρƒ як ΠΏΠΎΡ‚Π΅Π½Ρ†Ρ–ΠΉΠ½ΠΈΡ… Π±Ρ–ΠΎΠ»ΠΎΠ³Ρ–Ρ‡Π½ΠΎ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΈΡ… сполук Π°Π±ΠΎ Π½Π°ΠΏΡ–Π²ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Ρ–Π² для Ρ—Ρ… отримання. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Ρ‚Π° Ρ—Ρ… обговорСння. ΠšΠΎΠ½Π΄Π΅Π½ΡΠ°Ρ†Ρ–Ρ”ΡŽN-Π°Ρ€ΠΈΠ»Π·Π°ΠΌΡ–Ρ‰Π΅Π½ΠΈΡ… тіосСчовин Ρ‚Π° Π°Π»Ρ–Π»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΡ— кислоти Ρ–Π· застосуванням ΠΎΡ†Ρ‚ΠΎΠ²ΠΎΠ³ΠΎ Π°Π½Π³Ρ–Π΄Ρ€ΠΈΠ΄Ρƒ Π°Π±ΠΎ Π°Ρ†Π΅Ρ‚ΠΈΠ»Ρ…Π»ΠΎΡ€ΠΈΠ΄Ρƒ синтСзовано ΡΠ΅Ρ€Ρ–ΡŽ 5-Π°Π»Ρ–Π»Π·Π°ΠΌΡ–Ρ‰Π΅Π½ΠΈΡ… 2-Ρ‚Ρ–ΠΎΠΏΡ–Ρ€ΠΈΠΌΡ–Π΄ΠΈΠ½Π΄Ρ–ΠΎΠ½Ρ–Π². ΠŸΡ€ΠΈ ΠΏΠΎΠ΄Π°Π»ΡŒΡˆΠΎΠΌΡƒ Ρ—Ρ… Π°Π»ΠΊΡ–Π»ΡƒΠ²Π°Π½Π½Ρ– Π°Π»Ρ–Π»Π±Ρ€ΠΎΠΌΡ–Π΄ΠΎΠΌ Π°Π±ΠΎ ΠΌΠ΅Ρ‚Π°Π»Ρ–Π»Ρ…Π»ΠΎΡ€ΠΈΠ΄ΠΎΠΌ ΠΎΠ΄Π΅Ρ€ΠΆΠ°Π½ΠΎ 5,5-Π΄Ρ–Π°Π»ΠΊΠ΅Π½Ρ–Π»ΡŒΠ½Ρ– ΠΏΠΎΡ…Ρ–Π΄Π½Ρ–, які рСакціями мСтатСзису Ρ–Π· закриттям Ρ†ΠΈΠΊΠ»Ρƒ Π±ΡƒΠ»ΠΎ ΠΏΠ΅Ρ€Π΅Ρ‚Π²ΠΎΡ€Π΅Π½ΠΎ Π½Π° Π²Ρ–Π΄ΠΏΠΎΠ²Ρ–Π΄Π½Ρ– нСнасичСні спіроциклічні діоксопіримідин-2-Ρ‚Ρ–ΠΎΠ½ΠΈ.Π•ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π° частина. Π‘ΠΈΠ½Ρ‚Π΅Π· Π²ΠΈΡ…Ρ–Π΄Π½ΠΈΡ… сполук Ρ‚Π° Ρ†Ρ–Π»ΡŒΠΎΠ²ΠΈΡ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Ρ–Π² класичними ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΈΠ²Π½ΠΎΡ— Ρ…Ρ–ΠΌΡ–Ρ—; очистку Ρ‚Π° Ρ–Π΄Π΅Π½Ρ‚ΠΈΡ„Ρ–ΠΊΠ°Ρ†Ρ–ΡŽ ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½ΠΈΡ… сполук здійснСно ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ Ρ‚ΠΎΠ½ΠΊΠΎΡˆΠ°Ρ€ΠΎΠ²ΠΎΡ— Ρ‚Π° ΠΊΠΎΠ»ΠΎΠ½ΠΊΠΎΠ²ΠΎΡ— Ρ…Ρ€ΠΎΠΌΠ°Ρ‚ΠΎΠ³Ρ€Π°Ρ„Ρ–Ρ—, Π΅Π»Π΅ΠΌΠ΅Π½Ρ‚Π½ΠΈΠΌ Π°Π½Π°Π»Ρ–Π·ΠΎΠΌ, ЯМР-ΡΠΏΠ΅ΠΊΡ‚Ρ€ΠΎΡΠΊΠΎΠΏΡ–Ρ”ΡŽ.Висновки. Π ΠΎΠ·Ρ€ΠΎΠ±Π»Π΅Π½ΠΎ Π΅Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΈΠΉ тристадійний ΡˆΠ»ΡΡ… отримання Π· Π²ΠΈΡ…Ρ–Π΄Π½ΠΈΡ… тіосСчовин Ρ‚Π° Π°Π»Ρ–Π»ΠΌΠ°Π»ΠΎΠ½ΠΎΠ²ΠΎΡ— кислоти Π½ΠΎΠ²ΠΈΡ… нСнасичСних спіро-Π°Π½Π΅Π»ΡŒΠΎΠ²Π°Π½ΠΈΡ… ΠΏΠΎΡ…Ρ–Π΄Π½ΠΈΡ… N-Π°Ρ€ΠΈΠ»-4,6-діоксопіримідин-2-Ρ‚Ρ–ΠΎΠ½Ρƒ. ΠžΠ΄Π΅Ρ€ΠΆΠ°Π½Ρ– спіроциклічні ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΈ ΠΌΠΎΠΆΡƒΡ‚ΡŒ Π·Π½Π°ΠΉΡ‚ΠΈ застосування Π² Π±Ρ–ΠΎΠ»ΠΎΠ³Ρ–Ρ— Ρ‚Π° Ρ„Π°Ρ€ΠΌΠ°Ρ†Π΅Π²Ρ‚ΠΈΡ‡Π½Ρ–ΠΉ Π½Π°ΡƒΡ†Ρ–, Π°Π±ΠΎ Π²ΠΈΠΊΠΎΡ€ΠΈΡΡ‚ΠΎΠ²ΡƒΠ²Π°Ρ‚ΠΈΡΡŒ як Π²ΠΈΡ…Ρ–Π΄Π½Ρ– сполуки для ΠΏΠΎΠ΄Π°Π»ΡŒΡˆΠΎΡ— Ρ…Ρ–ΠΌΡ–Ρ‡Π½ΠΎΡ— ΠΌΠΎΠ΄ΠΈΡ„Ρ–ΠΊΠ°Ρ†Ρ–Ρ—

    Retrotransposon activation contributes to neurodegeneration in a Drosophila TDP-43 model of ALS

    Get PDF
    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

    Full text link
    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

    Full text link
    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 Ξ”\Delta and TKT_K 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 Ο€\pi. Calculating the Josephson current through the impurity, we find that Ο€\pi-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

    Full text link
    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

    Full text link
    We investigate the groundstates of weakly interacting bosons in a rotating trap as a function of the number of bosons, NN, and the average number of vortices, NVN_V. We identify the filling fraction ν≑N/NV\nu\equiv N/N_V as the parameter controlling the nature of these states. We present results indicating that, as a function of Ξ½\nu, 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

    Full text link
    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 ckσjc_{k \sigma j}, 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

    Full text link
    A review is given on theoretical studies concerning the pairing symmetry in organic superconductors. In particular, we focus on (TMTSF)2_2X and ΞΊ\kappa-(BEDT-TTF)2_2X, 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

    Full text link
    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 gcβ‰ˆ0.6g_c \approx 0.6, 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

    Full text link
    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
    • …
    corecore