拓扑超导Majorana束缚态的探索

梁奇锋; 王志; 川上拓人; 胡晓

doi:10.7498/aps.69.20190959

摘要

Majorana束缚态具有非阿贝尔量子统计特性, 是极具潜力的拓扑量子计算方案的核心. 近期有多项实验研究提供了Majorana束缚态在某些超导体系中的存在证据, 使其成为近期凝聚态物理以及量子计算领域的前沿焦点之一. 本文介绍拓扑超导的机理、Majorana束缚态的新奇物理特性、实验观测和操作的方法以及相关量子器件的设计, 最后展望该研究方向的发展前景.

关键词:

Majorana bound states are considered useful for realizing topological quantum computation since they obey the non-Abelian quantum statistics. Recent experiments have provided evidences for their existence in some superconducting systems, triggering significant interests from scientists in the field of condensed matter physics and related materials science. In this article, we briefly review the basic concepts and recent developments in the study of Majorana bound states. We first discuss about the origin of the nontrivial topology in superconducting systems within the Bogoliubov-de Gennes mean-field scheme. Then we show the construction of Majorana quasiparticle excitations from an electronic state, and the realization of non-Abelian statistics based on position exchanges of the Majorana bound states hosted in superconductivity vortices. Afterwards we talk about specific one-dimensional and two-dimensional topological superconductors, and propose possible experimental methods for detecting Majorana bound states and operating the Majorana qubits. In particular, a quantum device for Majorana braiding without moving vortices is introduced. Finally, perspectives of the study on Majorana bound states are provided.

Keywords:

作者及机构信息

1.
绍兴文理学院物理系, 绍兴　312000

2.
中山大学物理系, 广州　510275

3.
日本大阪大学大学院理学研究科物理学专攻, 大阪　565-0871, 日本

4.
日本国立物质材料研究机构，国际物质纳米结构学研究中心, 筑波　305-0044, 日本

5.
中国科学院大学, 卡弗里理论物理研究所, 北京　100190

通信作者: 胡晓, Hu.Xiao@nims.go.jp

Authors and contacts

1.
Department of Physics, Shaoxing University, Shaoxing 312000, China

2.
Department of Physics, Sun Yet-San University, Guangzhou 510275, China

3.
Department of Physics, Graduate School of Science, Osaka University, Osaka 565-0871, Japan

4.
International Center for Materials Nanoarchitectonics, National Institute for Materials Science, Tsukuba 305-0044, Japan

5.
Kavli Institute for Theoretical Physics, University of Chinese Academy of Sciences, Beijing 100190, China

Corresponding author: Hu Xiao, Hu.Xiao@nims.go.jp

文章全文 : translate this paragraph

参考文献

[1]	Klitzing K V, Dorda G, Pepper M 1980 Phys. Rev. Lett. 45 494 Google Scholar
[2]	Thouless D J, Kohmoto M, Nightingale M P, den Nijs M 1982 Phys. Rev. Lett. 49 405 Google Scholar
[3]	Haldane F D M 1988 Phys. Rev. Lett. 61 2015 Google Scholar
[4]	Hasan M Z, Kane C L 2010 Rev. Mod. Phys. 82 3045 Google Scholar
[5]	Qi XL, Zhang SC 2011 Rev. Mod. Phys. 83 1057 Google Scholar
[6]	Nayak C, Simon S H, Stern A, Freedman M, Das Sarma S 2008 Rev. Mod. Phys. 80 1083 Google Scholar
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[10]	Beenakker C W J 2013 Ann. Rev. Cond. Matt. Phys. 4 113 Google Scholar
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[12]	Weng H, Yu R, Hu X, Dai X, Fang Z 2015 Adv.Phys. 64 227 Google Scholar
[13]	Majorana E 2008 Il Nuovo Cimento (1924-1942) 14 171
[14]	Ivanov D A 2001 Phys. Rev. Lett. 86 268 Google Scholar
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[18]	Sau J D, Lutchyn R M, Tewari S, Das Sarma S 2010 Phys. Rev. Lett. 104 040502 Google Scholar
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[25]	Wang Z, Huang W C, Liang Q F, Hu X 2018 Sci. Rep. 8 7920 Google Scholar
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施引文献

图 1 (a) 量子霍尔效应及量子反常霍尔效应; (b)量子自旋霍尔效应; (c) 拓扑超导的体能带结构(红线和蓝线)和边缘态(绿色)的色散关系; (d)实空间边缘态的示意图

Fig. 1. Schematic energy band structures for (a) quantum Hall effect and quantum anomalous Hall effect, (b) quantum spin Hall effect, (c) a topological superconductor and (d) sche-matic diagram of topological edge/surface states in real space.

下载: 全尺寸图片幻灯片

图 2 拓扑超导约化能隙$ {{g}}\left({{k}}\right)/\left|{{g}}\left({{k}}\right)\right| $的动量空间分布

Fig. 2. Distribution of normalized topological superconduc-tivity gap $ {{g}}\left({{k}}\right)/\left|{{g}}\left({{k}}\right)\right| $ in momentum space.

下载: 全尺寸图片幻灯片

图 3 利用拓扑超导量子涡旋里的Majorana束缚态实现非阿贝尔统计的示意图, 其中黑色箭号代表量子涡旋位置交换的轨迹, 当量子涡旋跨越红线时超导相位发生2π的不连续跳跃

Fig. 3. Schematics of realization of non-Abelian statistics using Majorana bound states in vortex cores of a topological superconductor. Black arrows denote the exchanging paths of two quantum vortices. Superconducting phase takes a 2π jump when a vortex crosses the red cuts.

下载: 全尺寸图片幻灯片

图 4 (a)具有自旋轨道耦合的半导体纳米线和s波超导的混合系统的示意图; (b)半导体纳米线在有限磁场(实线)和零磁场(虚线)下的色散关系

Fig. 4. (a) Schematics of a heterostructure consisting of a spin-orbital coupling semiconductor nanowire and an s wave superconductor; (b) the band dispersion of the nanowire with finite magnetic field (solid lines) and zero magnetic field (dashed lines).

下载: 全尺寸图片幻灯片

图 5 (a) 通过电压差控制Majorana量子比特的设计; (b) Majorana量子比特的两能级系统; (c)-(e) 量子比特在电流脉冲下的LZS震荡: (c)短脉冲, (d)长脉冲, (e)序列脉冲^[25]

Fig. 5. (a) Schematic design of a universal quantum gate for Majorana qubit, where the qubit is manipulated by voltage across the Josephson-Majorana junction; (b) the two energy levels of the Majorana qubit depending on the phase difference across the junction; (c)-(e) the LZS oscillation of Majorana qubit under current pulse: (c) a short pulse, (d) a long pulse, (e) a sequence of pulses^[25].

下载: 全尺寸图片幻灯片

图 6 (a) Majorana束缚态与量子点耦合体系; (b)两个量子点的占据态关联函数^[28]

Fig. 6. (a) System with couplings between Majorana bound states and two quantum dots; (b) correlation between the electron occupations on the two quantum dots^[28].

下载: 全尺寸图片幻灯片

图 7 三维拓扑绝缘体(TI)色散关系(a)及TI-s波超导(SC)的异质结(b)的示意图, (b)中的红点代表Majorana束缚态^[29]

Fig. 7. (a) Schematic of the linear dispersion of surface state of a 3D TI; (b) schematic of a TI/s-SC heterostructure, where the red points denote the Majorana bound states at the center of a quantum vortex^[29].

下载: 全尺寸图片幻灯片

图 8 (a)拓扑超导量子涡旋里的低能准粒子激发的自旋分辨波函数; (b)准粒子激发的自旋向上态密度和自旋向下态密度之比的能量-空间分布^[29]

Fig. 8. (a) Spin-resolved wavefunctions of the low energy quasiparticle states in the vortex core of a topological superconductor; (b) spectrum of the ratio between densities of states for the spin-up and spin-down components^[29].

下载: 全尺寸图片幻灯片

图 9 (a), (c), (e), (g)为利用栅极电压移动边界Majorana束缚态的示意图; (b), (d), (f)给出了与(a), (c), (e) 相对应的Majorana束缚态的波函数分布^[32]

Fig. 9. (a), (c), (e), (g) Schematic of the device which transports edge Majorana states using gate voltages; (b), (d), (f) corresponding wavefunctions of the edge Majorana states in (a), (c), (e)^[32].

下载: 全尺寸图片幻灯片

图 10 (a), (b) Majorana量子比特的NOT量子门操作; (c), (d) 基于边界Mojorana束缚态的单电子泵^[34]

Fig. 10. (a), (b) NOT quantum gate operation of the Majorana qubit; (c), (d) a single-electron pumping based on the edge Majorana states^[34].

下载: 全尺寸图片幻灯片

[1]	Klitzing K V, Dorda G, Pepper M 1980 Phys. Rev. Lett. 45 494 Google Scholar
[2]	Thouless D J, Kohmoto M, Nightingale M P, den Nijs M 1982 Phys. Rev. Lett. 49 405 Google Scholar
[3]	Haldane F D M 1988 Phys. Rev. Lett. 61 2015 Google Scholar
[4]	Hasan M Z, Kane C L 2010 Rev. Mod. Phys. 82 3045 Google Scholar
[5]	Qi XL, Zhang SC 2011 Rev. Mod. Phys. 83 1057 Google Scholar
[6]	Nayak C, Simon S H, Stern A, Freedman M, Das Sarma S 2008 Rev. Mod. Phys. 80 1083 Google Scholar
[7]	Read N, Green D 2000 Phys. Rev. B 61 10267 Google Scholar
[8]	Sato M 2014 BUTSURI 69 297
[9]	Alicea J 2012 Rep. Prog. Phys. 75 076501 Google Scholar
[10]	Beenakker C W J 2013 Ann. Rev. Cond. Matt. Phys. 4 113 Google Scholar
[11]	Berry M V 1984 Proc. Roy. Soc. London A: Math. Phys. Sci. 392 45
[12]	Weng H, Yu R, Hu X, Dai X, Fang Z 2015 Adv.Phys. 64 227 Google Scholar
[13]	Majorana E 2008 Il Nuovo Cimento (1924-1942) 14 171
[14]	Ivanov D A 2001 Phys. Rev. Lett. 86 268 Google Scholar
[15]	Kitaev A Y 2001 Physics-Uspekhi 44 131 Google Scholar
[16]	Fu L, Kane C L 2008 Phys. Rev. Lett. 100 096407 Google Scholar
[17]	Sato M, Takahashi Y, Fujimoto S 2009 Phys. Rev. Lett. 103 020401 Google Scholar
[18]	Sau J D, Lutchyn R M, Tewari S, Das Sarma S 2010 Phys. Rev. Lett. 104 040502 Google Scholar
[19]	Lutchyn R M, Sau J D, Das Sarma S 2010 Phys. Rev. Lett. 105 077001 Google Scholar
[20]	Mourik V, Zuo K, Frolov S M, Plissard S R, Bakkers E P A M, Kouwenhoven L P 2012 Science 336 1003 Google Scholar
[21]	NadjPerge S, Drozdov I K, Li J, Chen H, Jeon S, Seo J, MacDonald A H, Bernevig B A, Yazdani A 2014 Science 346 602 Google Scholar
[22]	Xu J P, Wang M X, Liu Z L, Ge J F, Yang X, Liu C, Xu Z A, Guan D, Gao C L, Qian D, Liu Y, Wang Q H, Zhang F C, Xue Q K, Jia J F 2015 Phys. Rev. Lett. 114 017001 Google Scholar
[23]	Wiedenmann J, Bocquillon E, Deacon R S, Hartinger S, Herrmann O, Klapwijk T M, Maier L, Ames C, Brüne C, Gould C, Oiwa A, Ishibashi K, Tarucha S, Buhmann H, Molenkamp L W 2016 Nat. Comm. 7 10303 Google Scholar
[24]	Albrecht S M, Higginbotham A P, Madsen M, Kuemmeth F, Jespersen T S, Nygård J, Krogstrup P, Marcus C M 2016 Nature 531 206 Google Scholar
[25]	Wang Z, Huang W C, Liang Q F, Hu X 2018 Sci. Rep. 8 7920 Google Scholar
[26]	Hu X, Lin SZ 2010 Supercond. Sci. Tech. 23 053001 Google Scholar
[27]	Fu L 2010 Phys. Rev. Lett. 104 056402 Google Scholar
[28]	Wang Z, Hu XY, Liang Q F, Hu X 2013 Phys. Rev. B 87 214513 Google Scholar
[29]	Kawakami T, Hu X 2015 Phys. Rev. Lett. 115 177001 Google Scholar
[30]	Teo J C Y, Kane C L 2010 Phys. Rev. B 82 115120 Google Scholar
[31]	Sun H H, Zhang K W, Hu L H, Li C, Wang G Y, Ma H Y, Xu Z A, Gao C L, Guan D D, Li Y Y, Liu C, Qian D, Zhou Y, Fu L, Li SC, Zhang F C, Jia J F 2016 Phys. Rev. Lett. 116 257003 Google Scholar
[32]	Liang Q F, Wang Z, Hu X 2012 Europhys. Lett. 99 50004 Google Scholar
[33]	Wu LH, Liang Q F, Hu X 2014 Sci.Tech. Adv. Mat. 15 064402 Google Scholar
[34]	Liang Q F, Wang Z, Hu X 2014 Phys. Rev. B 89 224514 Google Scholar
[35]	Maeno Y, Kittaka S, Nomura T, Yonezawa S, Ishida K 2011 J. Phys. Soc. Japan 81 011009
[36]	Tsutsumi Y, Ishikawa M, Kawakami T, Mizushima T, Sato M, Ichioka M, Machida K 2013 J. Phys. Soc. Japan 82 113707 Google Scholar
[37]	Sakano M, Okawa K, Kanou M, Sanjo H, Okuda T, Sasagawa T, Ishizaka K 2015 Nat. Comm. 6 8595 Google Scholar
[38]	Yonezawa S, Tajiri K, Nakata S, Nagai Y, Wang Z, Segawa K, Ando Y, Maeno Y 2016 Nat. Phys. 13 123
[39]	Matano K, Kriener M, Segawa K, Ando Y, Zheng G Q 2016 Nat. Phys. 12 852 Google Scholar
[40]	Mizushima T, Tsutsumi Y, Kawakami T, Sato M, Ichioka M, Machida K 2016 J. Phys. Soc. Japan 85 022001 Google Scholar

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拓扑超导Majorana束缚态的探索