admin 2019-12-22 20:53:40 6137
æ¥åé¢ç®ïŒððšð¯ðð¥ ððððð¥âðð§ð¬ð®ð¥ðððšð« ðð«ðð§ð¬ð¢ðð¢ðšð§ð¬ ð¢ð§ 2D ðð¥ðððð«ðšð§ ððð¬ðð¬
æ¥åæ¶éŽïŒ2019-12-27 14:00 (ææäº)
æ¥åå°ç¹ïŒåæŽåæ ¡åº32æ218宀
æ¥å人ïŒçåè£ ææïŒéŠæž¯ç§æ倧åŠïŒ
æ¥å人æèŠïŒ
Inthis talk, I will start with the conventional wisdom of the Andersonlocalization transitions. Namely, allsystems can be classified into three ensembles: the Gaussian orthogonalensembles (GOE) when a system has both time-reversal and spin-rotational symmetries;the Gaussian unitary ensembles (GUE) when a system has neither time-reversalnor spin-rotational symmetries; and the Gaussian symplectic ensembles (GSE)when a system has time-reversal symmetry, but without spin-rotational symmetry.At the critical dimension of 2, no extended states exist in GOE at an arbitraryweak disorder, and extended states could exist in a GSE or a GUE when a strongperpendicular magnetic field is applied to drive the system into quantum Hallregion. Then I will argue the intrinsic inconsistency of this standardpicture. It turns out that spin-orbitinteractions play a crucial role. The types of Anderson-localizationtransitions (metal-insulator transitions) in a two-dimensional system aresensitive to the types and strength of spin-orbit interactions. I will presentseveral simple models that support Berezinskii-Kosterlitz-Thouless typetransition from a band of localized states to a band of critical states; or aBerezinskii-Kosterlitz-Thouless type transition from a band of conventionalextended states to a band of critical states. In contrast to the conventionalwisdom, I will also provide the evidences that support the existence ofextended states in a GUE at a weak magnetic field.
This work is supported by the NationalNatural Science Foundation of China (Grants No. 11774296 and 1974296) and HongKong RGC (Grants No. 16301518, 16301619 and 16300117).
æ¥å人ç®ä»
çåè£ïŒéŠæž¯ç§æ倧åŠç»èº«ææïŒ1984幎æ¯äžäºæŠæ±å€§åŠç©çç³»ïŒ1990幎åšçŸåœçœåœ»æ¯ç¹å€§åŠ(Universityof Rochester)è·å士åŠäœã
ç 究æ¹åïŒåèæç论ïŒç 究é¢åå
æ¬éåéå°æåºïŒéå±-ç»çŒäœçžåïŒè¶
æ¶æ Œä»¥åç£åšååŠäžïŒè¿ä»å·²åšåœé
æåšåŠæ¯æå¿å衚论æè¿çŸç¯ã
åžžçšéŸæ¥ å€©æŽ¥å€§åŠ æ¬ç§æççœ ç 究çæççœ SmartMat
å°åïŒå€©æŽ¥å€§åŠåæŽåæ ¡åº32æåŠæ¥ŒBåº | é®çŒïŒ300350Designed by 2014级ç©çç³»æ¬ç§çèåžå¯
Copyright © 2024 倩接倧åŠç©çåŠç³». All rights reserved. | Designed by 2014级ç©çç³»æ¬ç§çèåžå¯
æ«ç å ³æ³š