•¨«Šî‘bHŠwŒ¤‹†ƒOƒ‹[ƒv@(“c’‡Œ¤)
@
2018”N“x| 2017”N“x| 2016”N“x| 2015”N“x| 2014”N“x| 2013”N“x| 2012”N“x


2018”N“x


2017”N“x


“úŽž 2018”N1ŒŽ18“ú
“à—e M2’†ŠÔ•ñ
u‰‰ŽÒ ‘å‹´ ‹P“¹(M2), –쑺 ‘ñl(M2)

“úŽž 2017”N12ŒŽ18“ú
“à—e ’†ŠÔ•ñ
u‰‰ŽÒ ‹´–{ Ž÷(D3)

“úŽž 2017”N12ŒŽ11“ú
“à—e ’†ŠÔ•ñ
u‰‰ŽÒ Cássio S. Amorim(D3)

“úŽž 2017”N12ŒŽ7“ú
“à—e ’†ŠÔ•ñ
u‰‰ŽÒ ^ OŽÀ(D3)

“úŽž 2017”N11ŒŽ27“ú
“à—e ’†ŠÔ•ñ
u‰‰ŽÒ ‘å‹´ ‹P“¹(M2), ¬ŽR 仉›(M2), –쑺 ‘ñl(M2)

“úŽž 2017”N11ŒŽ20“ú
“à—e ’†ŠÔ•ñ
u‰‰ŽÒ ‰Hª“c ˜a‹I(M2)

“úŽž 2017”N10ŒŽ12“ú
u‰‰‘è–Ú Coupled-wire construction of multi-component
quantum Hall states
u‰‰ŽÒ “¡ —z•½(—‰»ŠwŒ¤‹†Š)

“úŽž 2017”N10ŒŽ5“ú
u‰‰‘è–Ú —â‹pŒ´Žq‹C‘Ì‚ð—p‚¢‚½—ÊŽqƒVƒ~ƒ…ƒŒ[ƒVƒ‡ƒ“
u‰‰ŽÒ ‚{ —m‰î(‹ž“s‘åŠw)

“úŽž 2017”N9ŒŽ25“ú
u‰‰‘è–Ú Quantization of Conductance Minimum and Index Theorem
u‰‰ŽÒ ’r’J ‘(–kŠC“¹‘åŠw)

“úŽž 2017”N8ŒŽ28“ú
u‰‰‘è–Ú Ž¥ê’†‚Ì‹[1ŽŸŒ³‹­‘ŠŠÖ“dŽqŒn‚É‚¨‚¯‚é
ŠïŽü”g”E‹ôŽü”g”’´“`“±‚̍¬‡
u‰‰ŽÒ •Ÿˆä ‹B—E(“Œ‹ž‘åŠw)

“úŽž 2017”N7ŒŽ31“ú
u‰‰ŽÒ •ŸŒ³ •q”V(D2), ¡Ž} —§ŽŠ(D2)

“úŽž 2017”N7ŒŽ25“ú
u‰‰ŽÒ •ž•” ˆ»ŽÀ(D2)

“úŽž 2017”N7ŒŽ18“ú
u‰‰ŽÒ ^ OŽÀ(D3)

“úŽž 2017”N6ŒŽ29“ú
u‰‰ŽÒ Anffany Chen(ƒuƒŠƒeƒBƒbƒVƒ…EƒRƒƒ“ƒrƒA‘åŠw)

“úŽž 2017”N6ŒŽ26“ú
u‰‰ŽÒ Serge Richard(G30‹³ˆõ)

“úŽž 2017”N6ŒŽ19“ú
u‰‰ŽÒ Cássio S. Amorim(D3)

“úŽž 2017”N6ŒŽ12“ú
u‰‰‘è–Ú ”÷¬‚ȃgƒ|ƒƒWƒJƒ‹’´“d“±‘Ì‚É‚¨‚¯‚éíŽ¥«ƒ}ƒCƒXƒi[Œø‰Ê
u‰‰ŽÒ —é–Ø C(PD)

“úŽž 2017”N6ŒŽ5“ú
u‰‰ŽÒ “c‘º x(PD)

“úŽž 2017”N5ŒŽ29“ú
u‰‰ŽÒ “cŒû Ÿ‹v(PD)

“úŽž 2017”N5ŒŽ22“ú
u‰‰ŽÒ ŒÃì r•ã(“Œ‹ž‘åŠw)

“úŽž 2017”N5ŒŽ15“ú
u‰‰ŽÒ Jorrit de Boer(ƒgƒFƒ“ƒe‘åŠw)

“úŽž 2017”N5ŒŽ8“ú
u‰‰ŽÒ ¬—Ñ LŒá(“Á”C•‹³)

“úŽž 2017”N5ŒŽ1“ú
u‰‰ŽÒ –î“c Œ\Ži(•‹³)

“úŽž 2017”N4ŒŽ24“ú
u‰‰ŽÒ ìŒû —R‹I(y‹³Žö)

“úŽž 2017”N4ŒŽ17“ú
u‰‰ŽÒ “c’‡ —RŠì•v(‹³Žö)

“úŽž 2017”N4ŒŽ3“ú
“à—e M2’†ŠÔ”­•\—ûK



2016”N“x


“úŽž 2017”N3ŒŽ9“ú
“à—e Šw‰ï”­•\—ûK

“úŽž 2017”N2ŒŽ27“ú
“à—e B4‘²˜_”­•\—ûK

“úŽž 2017”N2ŒŽ23“ú
“à—e B4‘²˜_”­•\—ûK

“úŽž 2017”N2ŒŽ20“ú
“à—e B4‘²˜_”­•\—ûK

“úŽž 2017”N2ŒŽ2“úA13“ú
“à—e B4’†ŠÔ•ñ

“úŽž 2017”N1ŒŽ26“úA30“úE2ŒŽ6“ú
“à—e M2C˜_”­•\—ûK

“úŽž 2017”N1ŒŽ12“úA16“úA23“ú
“à—e M2’†ŠÔ•ñ

“úŽž 2016”N12ŒŽ26“ú
u‰‰ŽÒ Î“c _“ñ (M2)

“úŽž 2016”N12ŒŽ22“ú
u‰‰ŽÒ ‰Í‡ N•½ (M2)

“úŽž 2016”N12ŒŽ19“ú
u‰‰ŽÒ [’J —D—œ (M2)

“úŽž 2016”N12ŒŽ15“ú
u‰‰ŽÒ ŒF Œ³X (M2)

“úŽž 2016”N12ŒŽ8“ú
u‰‰ŽÒ •ŸŒ³ •q”V (D1)

“úŽž 2016”N12ŒŽ1“úA5“ú
u‰‰ŽÒ Kyrylo Snizhko (ƒƒCƒcƒ}ƒ“Œ¤‹†Š)

“úŽž 2016”N11ŒŽ24“ú
u‰‰ŽÒ —MŒ´ ~Ži (–¼ŒÃ‰®‘åŠw HŠwŒ¤‹†‰È)

“úŽž 2016”N11ŒŽ21“ú
u‰‰‘è–Ú Paramagnetic Meissner effect of small topological superconductors
u‰‰ŽÒ —é–Ø C (–kŠC“¹‘åŠw)

“úŽž 2016”N11ŒŽ16“ú
u‰‰‘è–Ú Anomalous Hall Effects in a Chiral Superfluids
u‰‰ŽÒ J.A.Sauls (ƒm[ƒXƒEƒGƒXƒg‘åŠw)

“úŽž 2016”N11ŒŽ14“ú
u‰‰ŽÒ •ž•” ˆ»ŽÀ (D1)

“úŽž 2016”N11ŒŽ10“ú
u‰‰ŽÒ ¡Ž} —§ŽŠ (D1)

“úŽž 2016”N11ŒŽ9“ú
u‰‰‘è–Ú Chiral p-wave superconductivity in proximity with a rough surface: DOS, edge current, impedance
u‰‰ŽÒ S.V.Bakurskiy (ƒ‚ƒXƒNƒ‘åŠw)

“úŽž 2016”N10ŒŽ31“ú
u‰‰ŽÒ ^ OŽÀ (D2)

“úŽž 2016”N10ŒŽ17“ú
u‰‰‘è–Ú Stability of weyl points and chiral anomaly in Type-II weyl system and Majorana many-body system
u‰‰ŽÒ ‰F“cì «•¶ (ŠwK‰@‘åŠw)

“úŽž 2016”N10ŒŽ13“ú
u‰‰ŽÒ Cassio S. Amorim (D2)

“úŽž 2016”N9ŒŽ26“ú
u‰‰ŽÒ “c‘º x (PD)

“úŽž 2016”N9ŒŽ10“ú
“à—e “ú–{•¨—Šw‰ï”­•\—ûK

“úŽž 2016”N8ŒŽ30“ú
u‰‰ŽÒ “cŒû Ÿ‹v (PD)

“úŽž 2016”N8ŒŽ1“ú
u‰‰ŽÒ Bo Lu (PD)

“úŽž 2016”N7ŒŽ26“ú
“à—e M2’†ŠÔ”­•\

“úŽž 2016”N7ŒŽ11“ú
u‰‰‘è–Ú ”Ċ֐”‚­‚肱‚ÝŒQ(RG)‚É‚æ‚é’´“`“±—˜_
u‰‰ŽÒ “cà —¢“Þ (–¼ŒÃ‰®‘åŠw —ŠwŒ¤‹†‰È)

“úŽž 2016”N7ŒŽ4“ú
u‰‰ŽÒ ¬—Ñ LŒá (“Á”C•‹³)

“úŽž 2016”N6ŒŽ28“ú
u‰‰ŽÒ ŽR‰e ‘Š (“Á”C•‹³)

“úŽž 2016”N6ŒŽ21“ú
u‰‰ŽÒ H“¡ ˜aŒb (‚¨’ƒ‚̐…—Žq‘åŠw)

“úŽž 2016”N6ŒŽ13“ú
u‰‰‘è–Ú Effect of Electron-electron Interaction 2D Dirac Fermion System
u‰‰ŽÒ ¼–ì Œ³Ž÷ (–¼ŒÃ‰®‘åŠw —ŠwŒ¤‹†‰È)

“úŽž 2016”N6ŒŽ6“ú
u‰‰ŽÒ –î“c Œ\Ži (•‹³)

“úŽž 2016”N6ŒŽ1“ú
u‰‰‘è–Ú Ising Superconductivity in Transition Metal Dichalcogenides
u‰‰ŽÒ Kam Tuen Law (`‰È‹Z‘åŠw)

“úŽž 2016”N5ŒŽ30“ú
u‰‰ŽÒ ìŒû —R‹I (y‹³Žö)

“úŽž 2016”N5ŒŽ23“ú
u‰‰ŽÒ “c’‡ —RŠì•v (‹³Žö)

“úŽž 2016”N5ŒŽ9“ú
u‰‰‘è–Ú From an array of quantum wires to three-dimensional topological insulators
u‰‰ŽÒ Eran Sagi (ƒƒCƒcƒ}ƒ“‰ÈŠwŒ¤‹†Š)

“úŽž 2016”N4ŒŽ18“ú
u‰‰‘è–Ú All electrical generation and control of odd-frequency
s-wave Cooper pairs in double quantum dots
u‰‰ŽÒ Pablo Burset (PD)

“úŽž 2016”N4ŒŽ12“ú
u‰‰‘è–Ú Dark Matter Problem and Axion
u‰‰ŽÒ ’† —³‘å (–¼ŒÃ‰®‘åŠw —ŠwŒ¤‹†‰È)

“úŽž 2016”N4ŒŽ4“ú
“à—e M2’†ŠÔ”­•\—ûK




2015”N“x


“úŽž 2015”N3ŒŽ17“ú
u‰‰‘è–Ú Šw‰ï”­•\—ûK

“úŽž 2015”N2ŒŽ19“ú
u‰‰‘è–Ú B4 ‘²˜_”­•\—ûK

“úŽž 2015”N2ŒŽ8“ú
u‰‰‘è–Ú M2 C˜_”­•\—ûK

“úŽž 2015”N2ŒŽ4“ú
u‰‰‘è–Ú M2 C˜_”­•\—ûK

“úŽž 2015”N1ŒŽ25“ú
u‰‰‘è–Ú M2 ’†ŠÔ”­•\

“úŽž 2015”N1ŒŽ22“ú
u‰‰ŽÒ “Œ‹ž‘åŠw –¾Î—ɉî

“úŽž 2015”N1ŒŽ21“ú
u‰‰‘è–Ú M2 ’†ŠÔ”­•\

“úŽž 2015”N1ŒŽ4“ú
u‰‰ŽÒ D1 ^OŽÀ

“úŽž 2015”N12ŒŽ24“ú
u‰‰‘è–Ú M2 ’†ŠÔ”­•\

“úŽž 2015”N12ŒŽ21“ú
u‰‰‘è–Ú M2 ’†ŠÔ”­•\

“úŽž 2015”N12ŒŽ17“ú
u‰‰ŽÒ “Œ‹ž‘åŠw ŒÃìr•ã

“úŽž 2015”N11ŒŽ9“ú
u‰‰ŽÒ “Œ‹ž‘åŠw ¯–ìW‘¾˜Y

“úŽž 2015”N10ŒŽ26“ú
u‰‰ŽÒ PD Pablo Burset

“úŽž 2015”N10ŒŽ22“ú
u‰‰ŽÒ “Œ‹ž‘åŠw ‘哈r”V

“úŽž 2015”N10ŒŽ15“ú
u‰‰ŽÒ y‹³Žö ìŒû—R‹I

“úŽž 2015”N9ŒŽ14“ú
u‰‰‘è–Ú Šw‰ï”­•\—ûK

“úŽž 2015”N8ŒŽ17“ú
u‰‰‘è–Ú M2 ’†ŠÔ”­•\

“úŽž 2015”N7ŒŽ28“ú
u‰‰‘è–Ú M2 ’†ŠÔ”­•\

“úŽž 2015”N7ŒŽ27“ú
u‰‰‘è–Ú M2 ’†ŠÔ”­•\

“úŽž 2015”N7ŒŽ21“ú
u‰‰ŽÒ D1 ^OŽÀ

“úŽž 2015”N7ŒŽ13“ú
u‰‰ŽÒ à–žŒ¤‹†Žº “Á”CuŽt •àV¹Žu

“úŽž 2015”N6ŒŽ29“ú
u‰‰ŽÒ D1 Cassio S. Amorim

“úŽž 2015”N6ŒŽ23“ú
u‰‰‘è–Ú ‹ÇŠŽ¥‹Cƒ‚[ƒƒ“ƒgŒ`¬‚ª—U‹N‚·‚éS”gƒXƒsƒ“ŽOd€’´“`“±
u‰‰ŽÒ “Œ‹ž‘åŠw ¯–ìW‘¾˜Y

“úŽž 2015”N6ŒŽ22“ú
u‰‰ŽÒ D2 ‹´–{Ž÷

“úŽž 2015”N6ŒŽ15“ú
u‰‰ŽÒ PD Bo Lu

“úŽž 2015”N6ŒŽ8“ú
u‰‰ŽÒ PD ¬—ѐLŒá

“úŽž 2015”N6ŒŽ1“ú
u‰‰ŽÒ “Á”C•‹³ ŽR‰e‘Š

“úŽž 2015”N5ŒŽ18“ú
u‰‰ŽÒ •‹³ –î“cŒ\Ži

“úŽž 2014”N5ŒŽ12“ú
u‰‰ŽÒ y‹³Žö ²“¡¹—˜

“úŽž 2015”N4ŒŽ27“ú
u‰‰ŽÒ PD “cŒûŸ‹v

“úŽž 2015”N4ŒŽ20“ú
u‰‰‘è–Ú M2 ’†ŠÔ”­•\

“úŽž 2015”N4ŒŽ13“ú
u‰‰ŽÒ ‹³Žö@“c’‡—RŠì•v



2014”N“x


“úŽž 2015”N3ŒŽ16“ú
u‰‰‘è–Ú Šw‰ï”­•\—ûK

“úŽž 2015”N2ŒŽ26“ú
u‰‰‘è–Ú B4 ”­•\—ûK

“úŽž 2015”N2ŒŽ23“ú
u‰‰‘è–Ú B4 ”­•\—ûK

“úŽž 2015”N2ŒŽ19“ú
u‰‰ŽÒ University of Basel Jelena Klinovaja

“úŽž 2015”N2ŒŽ14“ú
u‰‰‘è–Ú B4 ”­•\—ûK

“úŽž 2015”N2ŒŽ9“ú
u‰‰‘è–Ú M2 ”­•\—ûK

“úŽž 2015”N2ŒŽ2“ú
u‰‰‘è–Ú M2 ”­•\—ûK

“úŽž 2015”N1ŒŽ22“ú
u‰‰‘è–Ú M2 CŽm˜_•¶•ñ

“úŽž 2015”N1ŒŽ15“ú
u‰‰ŽÒ “Œ‹ž‘åŠw ŽR’n—m•½

“úŽž 2015”N1ŒŽ15“ú
u‰‰ŽÒ “Œ‹ž‘åŠw ŽR’n—m•½

“úŽž 2015”N1ŒŽ8“ú
u‰‰‘è–Ú B4 ’†ŠÔ•ñ

“úŽž 2014”N12ŒŽ22“ú
u‰‰‘è–Ú M2 ’†ŠÔ”­•\

“úŽž 2014”N12ŒŽ11“ú
u‰‰ŽÒ “Œ–k‘åŠw ŠÖª‘•F

“úŽž 2014”N12ŒŽ11“ú
u‰‰‘è–Ú M2 ’†ŠÔ”­•\

“úŽž 2014”N12ŒŽ8“ú
u‰‰ŽÒ “Œ‹žH‹Æ‘åEw ùì’’j

“úŽž 2014”N11ŒŽ17“ú
u‰‰‘è–Ú Weyl semimetal phase in spin-orbit coupled semiconductor
u‰‰ŽÒ “Œ–k‘åŠw –쑺Œ’‘¾˜Y

“úŽž 2014”N10ŒŽ10“ú
u‰‰ŽÒ “Œ‹ž‘åŠw ‰F“cì«•¶

“úŽž 2014”N10ŒŽ2“ú
u‰‰‘è–Ú B4 ‘²Œ¤ƒe[ƒ}Ð‰î

“úŽž 2014”N9ŒŽ29“ú
u‰‰‘è–Ú 2ŽŸŒ³ƒJƒCƒ‰ƒ‹’´—¬“®‘Ì‚É‚¨‚¯‚éŠp‰^“®—Ê
u‰‰ŽÒ “Œ‘啨«Œ¤ ‘½“c–õŒ[

“úŽž 2014”N9ŒŽ25“ú
u‰‰‘è–Ú ƒVƒŠƒZƒ“AƒQƒ‹ƒ}ƒlƒ“AƒXƒ^ƒlƒ“Aƒgƒ|ƒƒWƒJƒ‹â‰‘̂ƃgƒ|ƒƒWƒJƒ‹’´“`“±
u‰‰ŽÒ “Œ‹ž‘åŠw ]àV‰ë•F

“úŽž 2014”N8ŒŽ18“ú
u‰‰ŽÒ —Œ¤ Bohm-Jung Yang

“úŽž 2014”N8ŒŽ4“ú
u‰‰ŽÒ ’}”g‘åŠw ‰ŠLˆÀO

“úŽž 2014”N7ŒŽ17“ú
u‰‰‘è–Ú ‚l‚Q ’†ŠÔ”­•\

“úŽž 2014”N7ŒŽ14“ú
u‰‰‘è–Ú ‚l‚Q ’†ŠÔ”­•\

“úŽž 2014”N7ŒŽ7“ú
u‰‰ŽÒ PD Bo Lu

“úŽž 2014”N6ŒŽ30“ú
u‰‰ŽÒ PD “cŒûŸ‹v

“úŽž 2014”N6ŒŽ23“ú
u‰‰ŽÒ PD ŽR‰e‘Š

“úŽž 2014”N6ŒŽ16“ú
u‰‰ŽÒ PD ¬—ѐLŒá

“úŽž 2014”N6ŒŽ9“ú
u‰‰ŽÒ PD –î“cŒ\Ži

“úŽž 2014”N6ŒŽ2“ú
u‰‰ŽÒ ”’ÎŒ¤ ô•½¹W

“úŽž 2014”N5ŒŽ27“ú
u‰‰‘è–Ú Superconducting Hybrids with Mixed Singlet & Triplet States
u‰‰ŽÒ Pablo Burset

“úŽž 2014”N5ŒŽ26“ú
u‰‰ŽÒ •‹³ ‘听½ˆê˜Y

“úŽž 2014”N5ŒŽ19“ú
u‰‰ŽÒ y‹³Žö ²“¡¹—˜

“úŽž 2014”N4ŒŽ28“ú
u‰‰‘è–Ú Weyl and Dirac semimetals with Z2 topological charge
u‰‰ŽÒ —Œ¤@X–{‚—T

“úŽž 2014”N4ŒŽ21“ú
u‰‰‘è–Ú Dirac Materials
u‰‰ŽÒ Alexander Balatsky

“úŽž 2014”N4ŒŽ14“ú
u‰‰ŽÒ ‹³Žö “c’‡—RŠì•v



2013”N“x


“úŽž 2014”N2ŒŽ17“ú
u‰‰‘è–Ú ƒ}ƒ‹ƒ`ƒ`ƒƒƒ“ƒlƒ‹‹ß“¡ŠiŽq‚É‚¨‚¯‚é
ŠïŽü”g”’´“`“±‚Æ“dŽ¥‰ž“š
u‰‰ŽÒ “Œ‹ž‘åŠw ¯–ìW‘¾˜Y

“úŽž 2014”N1ŒŽ27“ú
u‰‰‘è–Ú ‚l‚Q ’†ŠÔ”­•\

“úŽž 2014”N1ŒŽ20“ú
u‰‰‘è–Ú ‚l‚Q ’†ŠÔ”­•\

“úŽž 2013”N12ŒŽ16“ú
u‰‰‘è–Ú ‚l‚Q ’†ŠÔ”­•\

“úŽž 2013”N12ŒŽ9“ú
u‰‰‘è–Ú ‚l‚Q ’†ŠÔ”­•\

“úŽž 2013”N12ŒŽ5“ú
u‰‰‘è–Ú Density functional theory for
plasmon-assisted superconductivity
u‰‰ŽÒ “Œ‹ž‘åŠw –¾Î—ɉî

“úŽž 2013”N11ŒŽ25“ú
u‰‰‘è–Ú Magnetic and Orbital Ordered State
and Superconductivity in LaFeAsO1-xHx
Basd on the Multiorbital Extended Hubbard Model
u‰‰ŽÒ ‚rŒ¤ ŽRì—mˆê

“úŽž 2013”N11ŒŽ18“ú
u‰‰‘è–Ú Anormalous transport phenomena
in high-Tc superconductors:
Role of current vertex correction
u‰‰ŽÒ ‚rŒ¤ ®’J_

“úŽž 2013”N11ŒŽ11“ú
u‰‰‘è–Ú Weyl semimetals and Weyl superconducters
u‰‰ŽÒ PD Bo Lu

“úŽž 2013”N10ŒŽ28“ú
u‰‰‘è–Ú ƒgƒ|ƒƒWƒJƒ‹â‰‘Ì‚É‚¨‚¯‚鎥‹C’ïRŒø‰Ê
u‰‰ŽÒ PD “cŒûŸ‹v

“úŽž 2013”N10ŒŽ21“ú
u‰‰‘è–Ú Twente‘åŠw‘؍ݕñ
u‰‰ŽÒ PD –î“cŒ\Ži

“úŽž 2013”N‚WŒŽ23“ú
u‰‰‘è–Ú Ž¥«Œ³‘f‚ðŠÜ‚Ü‚È‚¢’´ŠiŽqŒ^GeSbTe‘Š•Ï‰»ƒƒ‚ƒŠ‚©‚ç‚Ì
Žº‰·‹‘厥‹C’ïR•Ï‰»‚Æ’´ŠiŽq\‘¢‚ɐö‚Þ
ƒgƒ|ƒƒWƒJƒ‹â‰‘̂ɂ‚¢‚Ä
u‰‰ŽÒ ŽY‘Œ¤ •x‰i~“ñ

“úŽž 2013”N‚VŒŽ29“ú
u‰‰‘è–Ú ƒ}ƒ‹ƒ`ƒtƒFƒƒbƒN•¨Ž¿’†‚É‚¨‚¯‚鎥‹CƒXƒLƒ‹ƒ~ƒIƒ“
u‰‰ŽÒ “Œ‹ž‘åŠw@ŠÖ^ˆê˜Y

“úŽž 2013”N‚VŒŽ22“ú
u‰‰ŽÒ SŒ¤@‘å–ì—C•ã

“úŽž 2013”N‚VŒŽ‚W“ú
u‰‰‘è–Ú ƒXƒsƒ“‚ɍì—p‚·‚é—LŒø“dŽ¥ê
u‰‰ŽÒ —‰»ŠwŒ¤‹†Š@‘½X—ÇŒ¹

“úŽž 2013”N7ŒŽ1“ú
u‰‰ŽÒ Cheng

“úŽž 2013”N6ŒŽ24“ú
u‰‰ŽÒ –k‹ž‘åŠw@Bo Lu

“úŽž 2013”N6ŒŽ17“ú
u‰‰‘è–Ú —L‹@ƒfƒBƒ‰ƒbƒN“dŽqŒn‚ÌŽ¥ê’†“d‹C“`“±‚Æ“dŽqó‘Ô
u‰‰ŽÒ “Œ‹ž‘åŠw@’·“crl

“úŽž 2013”N6ŒŽ10“ú
u‰‰‘è–Ú 3He-B‚̃gƒ|ƒƒWƒJƒ‹’´—¬“®‘¼
u‰‰ŽÒ ‰ªŽR‘åŠw@…“‡Œ’

“úŽž 2013”N6ŒŽ3“ú
u‰‰‘è–Ú M2 ’†ŠÔ•ñ

“úŽž 2013”N5ŒŽ27“ú
u‰‰‘è–Ú ‘Ώ̐«‚É‚æ‚éƒfƒBƒ‰ƒbƒN“dŽq‚Ì—A‘—§Œä
u‰‰ŽÒ PD@ŽR‰e‘Š

“úŽž 2013”N‚TŒŽ20“ú
u‰‰ŽÒ PD@“cŒûŸ‹v

“úŽž 2013”N‚TŒŽ‚P‚U“ú
u‰‰ŽÒ PD@¬—ѐLŒá

“úŽž 2013”N‚TŒŽ‚V“ú
u‰‰ŽÒ ‹³Žö@“c’‡—RŠì•v

“úŽž 2013”N‚SŒŽ‚R‚O“ú
u‰‰ŽÒ •‹³@‘听½ˆê˜Y

“úŽž 2013”N‚SŒŽ‚Q‚Q“ú
u‰‰ŽÒ y‹³Žö@²“¡¹—˜

“úŽž 2013”N‚SŒŽ‚P‚T“ú
u‰‰ŽÒ PD@–î“cŒ\Ži

“úŽž 2013”N‚SŒŽ‚W“ú
u‰‰ŽÒ ‹³Žö@“c’‡—RŠì•v



2012”N“x


“úŽž ‚Q‚O‚P‚R”N‚RŒŽ‚P‚P“ú
u‰‰‘è–Ú M1 ’†ŠÔ•ñ

“úŽž ‚Q‚O‚P‚R”N‚RŒŽ‚P“ú
u‰‰ŽÒ Vinokur

“úŽž ‚Q‚O‚P‚R”N‚QŒŽ‚Q‚T“ú
u‰‰‘è–Ú B4@‘²˜_”­•\—\s

“úŽž ‚Q‚O‚P‚R”N‚QŒŽ‚Q‚P“ú
u‰‰ŽÒ J.D.Sau

“úŽž ‚Q‚O‚P‚R”N‚QŒŽ‚P‚W“ú
u‰‰‘è–Ú B4 ‘²˜_”­•\—ûK

“úŽž ‚Q‚O‚P‚R”N‚QŒŽ‚V“ú
u‰‰‘è–Ú M2 C˜_”­•\—\s

“úŽž ‚Q‚O‚P‚R”N‚QŒŽ‚P‚S“ú
u‰‰ŽÒ ‘åã‘åŠw@‹g‰ª—R‰F

“úŽž ‚Q‚O‚P‚R”N‚PŒŽ‚R‚P“ú
u‰‰‘è–Ú M2 C˜_”­•\—ûK

“úŽž ‚Q‚O‚P‚R”N‚PŒŽ‚Q‚P“ú
u‰‰‘è–Ú B4 ’†ŠÔ•ñ

“úŽž ‚Q‚O‚P‚R”N‚PŒŽ‚P‚U“ú
u‰‰ŽÒ Fominov

“úŽž ‚Q‚O‚P‚R”N‚PŒŽ‚V“ú
u‰‰ŽÒ Ioselevich

“úŽž ‚Q‚O‚P‚Q”N‚P‚QŒŽ‚Q‚V“ú
u‰‰ŽÒ “Œ‹ž‘åŠw@‘åŠâ Œ°

“úŽž ‚Q‚O‚P‚Q”N‚P‚QŒŽ‚U“ú
u‰‰‘è–Ú ’†ŠÔ”­•\
u‰‰ŽÒ D3@d“cŒ[‰î

“úŽž ‚Q‚O‚P‚Q”N‚P‚PŒŽ‚P‚X“ú
u‰‰‘è–Ú M2 ’†ŠÔ•ñ

“úŽž ‚Q‚O‚P‚Q”N‚P‚PŒŽ‚P‚Q“ú
u‰‰‘è–Ú M2 ’†ŠÔ•ñ

“úŽž ‚Q‚O‚P‚Q”N‚P‚PŒŽ‚T“ú
u‰‰‘è–Ú ’†ŠÔ”­•\
u‰‰ŽÒ D3@d“cŒ[‰î

“úŽž ‚Q‚O‚P‚Q”N‚P‚OŒŽ‚Q‚X“ú
u‰‰‘è–Ú Majorana Fermions in Gapped and Gapless Topological Superconducters
u‰‰ŽÒ K.T.Law

“úŽž ‚Q‚O‚P‚Q”N‚P‚OŒŽ‚Q‚T“ú
u‰‰‘è–Ú RuŽ_‰»•¨‚É‚¨‚¯‚é‹O“¹—h‚炬‚Æ“dŽqƒlƒ}ƒeƒBƒbƒN‘Š
u‰‰ŽÒ –¼ŒÃ‰®‘åŠw@“yŽË’Ϲ‹v

“úŽž ‚Q‚O‚P‚Q”N‚P‚OŒŽ‚P‚W“ú
u‰‰ŽÒ A. A. Golubov

“úŽž ‚Q‚O‚P‚Q”N‚P‚OŒŽ‚P‚T“ú
u‰‰ŽÒ A.V.Burmistrova

“úŽž ‚Q‚O‚P‚Q”N‚P‚OŒŽ‚P‚P“ú
u‰‰ŽÒ I.A.Devyatov

“úŽž ‚Q‚O‚P‚Q”N‚XŒŽ‚T“ú
u‰‰‘è–Ú Au-AI-Yb€Œ‹»‚É‚¨‚¯‚é—ÊŽq—ÕŠEŒ»Û
u‰‰ŽÒ MŒ¤@oŒû˜a•F

“úŽž ‚Q‚O‚P‚Q”N‚XŒŽ‚T“ú
u‰‰‘è–Ú Topological classification
of vortex-core structures
of a spinor Bose-Einstein condensate
u‰‰ŽÒ “Œ‹ž‘åŠw@¬—ѐLŒá

“úŽž ‚Q‚O‚P‚Q”N‚VŒŽ‚Q‚T“ú
u‰‰‘è–Ú Topological Excitations in Spinor
Bose-Einstein Condensates
u‰‰ŽÒ “Œ‹ž‘åŠw@ìŒû—R‹I

“úŽž ‚Q‚O‚P‚Q”N‚VŒŽ‚Q‚R“ú
u‰‰ŽÒ ‹³Žö@“c’‡—RŠì•v

“úŽž ‚Q‚O‚P‚Q”N‚VŒŽ‚X“ú
u‰‰‘è–Ú M2 ’†ŠÔ•ñ

“úŽž ‚Q‚O‚P‚Q”N‚VŒŽ‚S“ú
u‰‰‘è–Ú M2 ’†ŠÔ•ñ

“úŽž ‚Q‚O‚P‚Q”N‚UŒŽ‚Q‚O“ú
u‰‰‘è–Ú d‚¢“dŽqŒn’´“`“±‘ÌUPt3‚̃MƒƒƒbƒvŠÖ”
u‰‰ŽÒ —‰»ŠwŒ¤‹†Š@’çN‰ë

“úŽž ‚Q‚O‚P‚Q”N‚UŒŽ‚P‚R“ú
u‰‰‘è–Ú 2‘wRashbaŒn‚É‚¨‚¯‚éƒgƒ|ƒƒWƒJƒ‹’´“`“±
u‰‰ŽÒ “Œ‹ž‘åŠw@’†‰Í¼ãÄ

“úŽž ‚Q‚O‚P‚Q”N‚UŒŽ‚P‚P“ú
u‰‰‘è–Ú Œõ—U‹Nƒgƒ|ƒƒWƒJƒ‹‘Š“]ˆÚ‚Ì—˜_
u‰‰ŽÒ “Œ‹ž‘åŠw@‰ª—²Žj

“úŽž ‚Q‚O‚P‚Q”N‚UŒŽ‚U“ú
u‰‰‘è–Ú “SŒn’´“`“±‘Ì‚É‚¨‚¯‚é‹O“¹—h‚炬‚¨‚æ‚Ñ
’´“`“±”­Œ»‹@\
u‰‰ŽÒ •‹³@‘听½ˆê˜Y

“úŽž ‚Q‚O‚P‚Q”N‚TŒŽ‚Q‚W“ú
u‰‰‘è–Ú ƒgƒ|ƒƒWƒJƒ‹—ÊŽq‘Š‚Ì•¨—
u‰‰ŽÒ ISSP@²“¡¹—˜

“úŽž ‚Q‚O‚P‚Q”N‚TŒŽ‚V“ú
u‰‰‘è–Ú ‹­‘ŠŠÖ“dŽqŒn‚É‚¨‚¯‚é’´“`“±“dŽq‘΂̑Ώ̐«
u‰‰ŽÒ D3@d“cŒ[‰î

“úŽž ‚Q‚O‚P‚Q”N‚TŒŽ‚Q“ú
u‰‰‘è–Ú ’´“`“±ƒgƒ|ƒƒWƒJƒ‹â‰‘Ì‚É‚¨‚¯‚é
ƒgƒ“ƒlƒ‹•ªŒõ‚Ì—˜_
-•\–ʏó‘Ԃ̍\‘¢“]ˆÚ‚ƃgƒ“ƒlƒ‹ƒRƒ“ƒ_ƒNƒ^ƒ“ƒX-
u‰‰ŽÒ PD@ŽR‰e‘Š

“úŽž ‚Q‚O‚P‚Q”N‚SŒŽ‚Q‚T“ú
u‰‰‘è–Ú ƒgƒ|ƒƒWƒJƒ‹’´“`“±/â‰‘Ì
u‰‰ŽÒ PD@–î“cŒ\Ži

“úŽž ‚Q‚O‚P‚Q”N‚SŒŽ‚Q‚R“ú
u‰‰‘è–Ú ‹­‘ŠŠÖ“dŽqŒn‚Ì’´“`“±‚¨‚æ‚эŋ߂̌¤‹†
u‰‰ŽÒ •‹³@‘听½ˆê˜Y

“úŽž ‚Q‚O‚P‚Q”N‚SŒŽ‚P‚U“ú
u‰‰‘è–Ú ’´“`“±Ú‡—˜_‚̐i“W
u‰‰ŽÒ ‹³Žö@“c’‡—RŠì•v


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