Управление потоками заряда и тепла в наноразмерных квазиодномерных проводниках тема диссертации и автореферата по ВАК РФ 01.04.07, кандидат наук Бубис Антон Владимирович

  • Бубис Антон Владимирович
  • кандидат науккандидат наук
  • 2022, ФГАОУ ВО «Национальный исследовательский университет «Высшая школа экономики»
  • Специальность ВАК РФ01.04.07
  • Количество страниц 83
Бубис Антон Владимирович. Управление потоками заряда и тепла в наноразмерных квазиодномерных проводниках: дис. кандидат наук: 01.04.07 - Физика конденсированного состояния. ФГАОУ ВО «Национальный исследовательский университет «Высшая школа экономики». 2022. 83 с.

Оглавление диссертации кандидат наук Бубис Антон Владимирович

Contents

1 Introduction

2 Experimental methods

2.1 Fabrication of HgTe QW based devices

2.1.1 Mesa etching

2.1.2 Contact metalization

2.1.3 Gate

2.2 Fabrication of InAs NW based devices

2.3 Shot noise measurements

2.3.1 Langevin approach for RF circuit

2.3.2 Calibration

2.3.3 Nonequilibrium noise measurement

2.3.4 Noise spectrum measurement

3 Chitosan-based lithography for delicate materials

3.1 Resist development principle

3.2 Optimization of resist performance

3.2.1 Sensitivity

3.2.2 Contrast

3.2.3 Resist residues and lift-off

3.3 Recipes

3.4 Organic semiconductors patterning

3.5 Electrical devices

3.6 Conclusion

4 Localization of helical edges in HgTe QW

4.1 Processing influence on 2DEG

4.2 Nonlocal transport

4.3 Localization in the absence of magnetic field

4.3.1 Low-temperature localization

4.3.2 Theoretical outlook

4.3.3 Magnetic field behavior

4.4 Shot noise

4.5 Conclusion

5 Heat transport in proximitized InAs nanowires

5.1 Theory

5.1.1 Semiclassical model

5.1.2 Electronic energy distributions

5.1.3 A suppression due to nonequilibrium EED

5.1.4 Shot noise

5.2 Shot noise measurement

5.3 Charge neutrality of transmitted quasiparticles

5.4 Conclusion

6 Summary and outlook

7 Acknowledgments

Введение диссертации (часть автореферата) на тему «Управление потоками заряда и тепла в наноразмерных квазиодномерных проводниках»

1 Introduction

Topic relevance One of the most promising research directions of modern condensed matter physics is the investigation of the topological aspects of electronic band theory. Unlike the classical Bloch theory of crystals, here, the interconnection of the spin and spatial degrees of freedom originating from strong spin-orbit interaction plays the central role. It turns out that this relationship takes place in entire classes of new materials, for example, in topological insulators.1,2 In these materials, tuning of the Fermi level in the bulk energy gap does not lead to vanishing of electrical conductivity due to the presence of gapless helical states. These states emerge on the boundary between topological and trivial insulators (surface in the three-dimensional case or edge in the two-dimensional case), and the spin and the momentum of such states are rigidly locked.

A fundamental property of the helical states is the complete backscattering suppression, which has a purely quantum origin and is also called topological protection. The most impressive manifestation of topologically protected states occurs in a one-dimensional case. They provide ballistic transfer of a spin-polarized electric current along the edge of a quantum spin Hall insulator.3 In addition to the edge states of the spin Hall insulator, helical states can also be realized in pure semiconductor nanowires with strong spin-orbit interaction placed into a high parallel to a nanowire magnetic field.4

The helical states are of great interest, particularly due to predictions for Majorana zero modes (MZMs) emergence valuable for fault-tolerant quantum computing. Among several proposals for MZM implementations in the real systems, proximitized semiconducting nanowires with strong spin-orbit coupling and topological insulator-superconductor hybrids got the most attention from the scientific community. Nowadays, still, there is no unambiguous observation of all signatures of Majorana zero modes in a single experiment. Thus, the experimental research in this area mainly focuses on the fabrication advances to obtain better devices (mostly growth techniques) and on the novel detection schemes for topological phase transition.

This work is dedicated to the most widespread materials used in Majorana research: topological insulators and proximitized nanowires. There was no goal to observe signatures of MZM in the experiment but to investigate the electronic transport in the helical edges and to implement a new measurement technique in the semiconductor-superconductor hybrid structures. A significant part of this work is dedicated to the development of fabrication techniques for delicate materials. The thesis is organized as follows:

• Chapter 2 is dedicated to description of fabrication and measurement used in this study. The implementation of lithographic methods for fabrication of HgTe quantum wells (QW) and InAs nanowires (NW) based devices is discussed in detail. Also shot noise and noise spectrum measurement procedure is described thoroughly.

• Chapter 3 is devoted to the advanced lithographic technique developed for delicate objects. It is proposed to utilize chitosan derivatives (CD) - bio-inspired and water-soluble polysaccharides as an e-beam and deep-ultraviolet resist. CD exhibits molecular scissoring under irradiation, similar to commonly used poly(methyl methacrylate) (PMMA). In

the proposed technology, the key feature is the chelation reaction, which allowed achieving clean enough development and, thus, lift-off capability while keeping the fabrication routine gentle and water-based.

• Chapter 4 is devoted to the first and well-studied 2D topological insulator, HgTe QW. Its bulk gap is quite large, « 30meV, so the temperature of 4.2 K (liquid He) is already sufficient to get rid of bulk conduction, provided the Fermi level is tuned to the bulk gap. Of great interest is the main ingredient of topological protection - time-reversal symmetry (TRS), which protects the helical edges from a single particle backscattering. If TRS is broken, e.g., by an external magnetic field, the helical edges localize due to disorder. This work demonstrates that these edges can localize at low enough temperature even without an external magnetic field. Theoretically, several scenarios are known for such behavior, and in this chapter, they are discussed in view of the experimental observations.

• In Chapter 5 the alternative scheme for detecting topological phase transition is discussed using the example of hybrid semiconductor-superconductor structures based on InAs nanowires. The idea is to measure the heat conductance of the proximitized segment of a nanowire, which acquires a universal value at the point of topological phase transition. Although studied devices cannot exhibit topological phase, they serve as a minimal toy model to study the heat transport in proximitized nanowires. Using the semiclassical approach, it is demonstrated that heat conductance in such devices can be obtained from nonlocal shot noise measurement, which is possible thanks to the charge-heat separation occurring at the normal metal-superconductor (NS) interface.

Aims and objectives

1. Development and tuning of fabrication routine for devices based on HgTe QWs, investigation of the different processing steps influence onto properties of a 2D electron gas. Measurement of the typical conductance against the magnetic field at the charge neutrality point to estimate Luttinger liquid constant, K.

2. Analytical derivation for the current noise spectral density in NSN-devices based on a diffusive nanowire with either grounded central superconducting terminal or floating superconducting island. Calculation of superconducting gap suppression in the floating island geometry due to nonequilibrium electronic energy distribution (EED). Fabrication of InAs NW based devices with central superconducting terminal and normal contacts on both sides.

3. Development of delicate lithographic technique and its basis - water-soluble resist. Investigation of developer properties influence on the development procedure, proof of chelation-dissolution mechanism. Tailoring of lithographic parameters to obtain 100 nm-wide lifted-off metal individual lines.

Key aspects to be defended

1. For the first time, localization of 2D TI edges of 8nm HgTe QW was demonstrated at millikelvin temperatures in the absence of an external magnetic field. The behavior of typical conductance at the charge neutrality point suggests Luttinger liquid constant K « 0.8-0.9, which on its own theoretically does not explain the observed localization. Current noise measurements revealed the Fano factor F « 0.5-0.7, greater than values for diffusive conductors even with strong electron-electron scattering. The latter can point to the disordered nature of the electronic transport through the edge and be the signature of upcoming localization, but still, the main scattering mechanism is unclear.

2. The expressions for local and nonlocal shot noise are obtained analytically for NSN diffusive devices with either grounded central superconducting terminal or floating superconducting island. It is demonstrated that the thermal conductance of the proximitized nanowire segment can be extracted from the nonlocal current noise slope dS/dV. In the layout with the floating superconducting island, the nonequilibrium EED suppresses the superconducting gap for the arbitrary asymmetry between normal nanowire segments, which manifests itself in two stable branches of A(V). Experimentally nonlocal shot noise is measured in InAs NSN devices, and its subgap values can be fitted with a single parameter - thermal conductance. The average charge of a transmitted through proximitized segment quasiparticle is estimated from above using both nonlocal shot noise and nonlocal conductance.

3. Genuine water-based lithographic technique was developed and employed to fabricate devices based on delicate materials. The main lithographic processing liquids are a chitosan derivative (resist), an aqueous solution of transition metal salt (developer), and a solution of a weak acid (remover). The chelation-dissolution competition allows achieving residue-free development and lift-off capability. The best obtained sensitivity is « 130 ^C/cm2 (at 50kV accelerating voltage), the narrowest individual metal line obtained via lift-off is 100nm-wide. This lithographic approach was successfully utilized to fabricate carbon nanotube, organic semiconductor, and porcine brain microtubule-based devices.

Approbation of the results This work results were reported on the following conferences: Interaction between Radiation and Quantum devices (November 2020, Moscow), XXV Symposium "Nanophysics and Nanoelectronics" (March 2021, Nizhny Novgorod). The papers [A1-A4] are published in peer-reviewed scientific journals and [A5] is uploaded to arXiv.

Похожие диссертационные работы по специальности «Физика конденсированного состояния», 01.04.07 шифр ВАК

Заключение диссертации по теме «Физика конденсированного состояния», Бубис Антон Владимирович

5.4 Conclusion

In this section, the electronic transport in NSN devices based on diffusive nanowires is considered theoretically and experimentally. Following the semiclassical approach, the analytical expressions for shot noise were obtained in two geometries: the superconducting grounded reservoir and floating superconducting island. It was shown that both of these setups are capable of extraction of energy dependent thermal conductance, Gth(e), of nanowire segment beneath superconductor. Gth(e) is of great importance because it contains information about the proximity effect. The shot noise measurements were conducted in the grounded geometry, and the experimental data perfectly follow all theoretically obtained features.

6 Summary and outlook

The main conclusions of this thesis can be formulated as follows:

1. For the first time, localization of 2D TI edges of 8nm HgTe QW was demonstrated at millikelvin temperatures in the absence of an external magnetic field. The behavior of typical conductance at the charge neutrality point suggests Luttinger liquid constant K « 0.8-0.9, which on its own theoretically does not explain the observed localization. Current noise measurements revealed the Fano factor F « 0.5-0.7, greater than values for diffusive conductors even with strong electron-electron scattering. The latter can point to the disordered nature of the electronic transport through the edge and be the signature of upcoming localization, but still, the main scattering mechanism is unclear.

2. The expressions for local and nonlocal shot noise are obtained analytically for NSN diffusive devices with either grounded central superconducting terminal or floating superconducting island. It is demonstrated that the thermal conductance of the proximitized nanowire segment can be extracted from the nonlocal current noise slope dS/dV. In the layout with the floating superconducting island, the nonequilibrium EED suppresses the superconducting gap for the arbitrary asymmetry between normal nanowire segments, which manifests itself in two stable branches of A(V). Experimentally nonlocal shot noise is measured in InAs NSN devices, and its subgap values can be fitted with a single parameter - thermal conductance. The average charge of a transmitted through proximitized segment quasiparticle is estimated from above using both nonlocal shot noise and nonlocal conductance.

3. Genuine water-based lithographic technique was developed and employed to fabricate devices based on delicate materials. The main lithographic processing liquids are a chitosan derivative (resist), an aqueous solution of transition metal salt (developer), and a solution of a weak acid (remover). The chelation-dissolution competition allows achieving residue-free development and lift-off capability. The best obtained sensitivity is « 130 ^C/cm2 (at 50kV accelerating voltage), the narrowest individual metal line obtained via lift-off is 100nm-wide. This lithographic approach was successfully utilized to fabricate carbon nanotube, organic semiconductor, and porcine brain microtubule-based devices.

The fabrication of hybrid devices based on topological insulators is one of modern condensed matter research milestones. Numerous experiments demonstrate the absence of robust conductance quantization in the QSH effect, which motivated theoretical investigations of the possible origin for such behavior. Several of the considered scattering mechanisms were predicted to result in localization of the helical edge states without external magnetic field, which

was observed experimentally in 8 nm HgTe QW. Although the unambiguous reason for the observed localization was not found, the interaction of the helical states is most probably one of the prerequisites. There are several ways to investigate the interaction of the helical edges (Luttinger liquid parameter K). The first approach is to implement tunnel junction and extract exponent from power-law fits of Zsd-Vsd curves. The second one valuable for HgTe quantum wells is measurements of conductance and current correlations in corner junctions. Such experiments can shed light on the strength of e-e interaction in the edges and thus better describe the observed localization.

Semiconducting nanowire-superconductor hybrids deserved huge attention because of the proposed MZMs emergence in such systems. The research frontier in this area is split into two parts: the advances of nanowire synthesis and the novel methods for detecting topological phase transition. One of these methods is proposed earlier measurement of the thermal conductance of the proximitized nanowire segment. The application of shot noise allowed us to conduct such measurements on the model NSN diffusive InAs nanowire-based system. Also, the theoretical study demonstrates the possibility of utilizing different device layouts for thermal conductance extraction. Altogether this approach opens a new pathway for MZM detection, and it definitely deserves employment in the Majorana device.

The aforementioned materials HgTe QWs and some semiconducting nanowires (e.g., InSb or InAsSb) cannot withstand the common nanofabrication processing and require a low temperature of all the processes, including e-beam lithography. In the case of these materials, it is sufficient to decrease resist bake temperature to minimize damage during EBL. However, many emergent materials are easily damaged by the harsh processing liquids accompanied by conventional lithography. In this work, the genuine water-based resist is developed and employed for several prototype delicate materials. This approach can be implemented further to investigate the most delicate objects like biological and organic samples. Also, the proposed technology can be employed by the microfabrication industry because of its environmental friendliness.

Список литературы диссертационного исследования кандидат наук Бубис Антон Владимирович, 2022 год

Bibliography

1. Hasan, M. Z. & Kane, C. L. Colloquium: Topological Insulators. Rev. Mod. Phys. 82, 3045-3067 (2010).

2. Qi, X.-L. & Zhang, S.-C. Topological Insulators and Superconductors. Rev. Mod. Phys. 83, 1057-1110(2011).

3. König, M. et al. Quantum Spin Hall Insulator State in HgTe Quantum Wells. Science 318, 766-770 (2007).

4. Alicea, J. New Directions in the Pursuit of Majorana Fermions in Solid State Systems. Rep. Prog. Phys. 75, 076501 (2012).

5. Srivastav, V., Pal, R. & Vyas, H. P. Overview of Etching Technologies Used for HgCdTe. Opto-Electron. Rev. 13, 197-211 (2005).

6. König, M. et al. The Quantum Spin Hall Effect: Theory and Experiment. J. Phys. Soc. Jpn. 77, 031007 (2008).

7. Olshanetsky, E. B. et al. Quantum Hall Liquid-Insulator and Plateau-to-Plateau Transitions in a High Mobility 2D Electron Gas in an HgTe Quantum Well. Jetp Lett. 84, 565-569 (2007).

8. Bendias, K. et al. High Mobility HgTe Microstructures for Quantum Spin Hall Studies. Nano Lett. 18, 4831-4836 (2018).

9. Bendias, M. K. Quantum Spin Hall Effect - A New Generation of Microstructures (Universität Würzburg, 2018).

10. Leech, P. W., Kibel, M. H. & Gwynn, P. J. The Chemical Etching of II - VI / GaAs Heterostructures in Aqueous I : KI : HBr Solutions. J. Electrochem. Soc. 137, 705-707 (1990).

11. Srivastav, V. et al. Etching of Mesa Structures in HgCdTe. Journal of Elec Materi 34, 1440-1445 (2005).

12. Ivanits'ka, V. G. et al. A Slightly Oxidizing Etchant for Polishing of CdTe and CdZnTe Surfaces. Journal of Elec Materi 42, 3059-3065 (2013).

13. Microchemicals. Etching with Hydrofluoric Acid. https : //www. microchemicals . com/technical_information/hf_etching.pdf (2013).

14. Kvon, Z. D., Olshanetsky, E. B., Kozlov, D. A., Mikhailov, N. N. & Dvoretskii, S. A. Two-Dimensional Electron-Hole System in a HgTe-based Quantum Well. Jetp Lett. 87, 502-505 (2008).

15. Gusev, G. M. et al. Transport in Disordered Two-Dimensional Topological Insulators. Phys. Rev. B 84, 121302 (2011).

16. Hart, S. et al. Induced Superconductivity in the Quantum Spin Hall Edge. Nature Phys 10, 638-643 (2014).

17. Hart, S. et al. Controlled Finite Momentum Pairing and Spatially Varying Order Parameter in Proximitized HgTe Quantum Wells. Nature Phys 13, 87-93 (2017).

18. Lunczer, L. et al. Approaching Quantization in Macroscopic Quantum Spin Hall Devices through Gate Training. Phys. Rev. Lett. 123, 047701 (2019).

19. Strunz, J. et al. Interacting Topological Edge Channels. Nat. Phys. 16, 83-88 (2020).

20. Minkov, G. M. et al. Weak Antilocalization in HgTe Quantum Wells with Inverted Energy Spectra. Phys. Rev. B 85, 235312 (2012).

21. Minkov, G. M. et al. Two-Dimensional Semimetal in a Wide HgTe Quantum Well: Magnetotransport and Energy Spectrum. Phys. Rev. B 88, 155306 (2013).

22. Khan, S. A. Epitaxy of Hybrid Nanowires, Shadow Junctions and Networks (University of Copenhagen, 2020).

23. Negrov, D. V. et al. Integration of Functional Elements of Resistive Nonvolative Memory with 1T-1R Topology. Russ Microelectron 45, 383-395 (2016).

24. Bubis, A. V. et al. Proximity Effect and Interface Transparency in Al/InAs-nanowire/Al Diffusive Junctions. Semicond. Sci. Technol. 32, 094007 (2017).

25. Tikhonov, E. S. Исследование дробового шума в низкоразмерных электронных системах (ISSP RAS, 2016).

26. Piatrusha, S. U. Электронный транспорт, локализация и статистика протекания заряда в квазиодномерных проводниках (ISSP RAS, 2019).

27. Tikhonov, E. S. et al. Nonlinear Transport and Noise Thermometry in Quasiclassical Ballistic Point Contacts. Phys. Rev. B 90, 161405 (2014).

28. Kogan, S. Electronic Noise and Fluctuations in Solids (Cambridge Univ. Press, Cambridge, 2008).

29. Heikkilä, T. T. The Physics of Nanoelectronics: Transport and Fluctuation Phenomena at Low Temperatures (Oxford University Press, 2013).

30. Linder, V., Gates, B. D., Ryan, D., Parviz, B. A. & Whitesides, G. M. Water-Soluble Sacrificial Layers for Surface Micromachining. Small 1, 730-736 (2005).

31. Kim, S. etal. All-Water-Based Electron-Beam Lithography Using Silk as aResist. Nature Nanotech 9, 306-310 (2014).

32. Sun, Y.-L. et al. Aqueous Multiphoton Lithography with Multifunctional Silk-Centred Bio-Resists. Nat Commun 6, 8612 (2015).

33. Park, J. et al. Eco-Friendly Photolithography Using Water-Developable Pure Silk Fibroin. RSCAdv. 6, 39330-39334 (2016).

34. Takei, S. et al. Application of Natural Linear Polysaccharide to Green Resist Polymers for Electron Beam and Extreme-Ultraviolet Lithography. Jpn. J. Appl. Phys. 53, 116505 (2014).

35. Jiang, B. et al. Water-Based Photo- and Electron-Beam Lithography Using Egg White as a Resist. Adv. Mater. Interfaces 4, 1601223 (2017).

36. Wang, D. et al. 2D Protein Supramolecular Nanofilm with Exceptionally Large Area and Emergent Functions. Adv. Mater. 28, 7414-7423 (2016).

37. Voznesenskiy, S. S., Nepomnyaschiy, A. & Kulchin, Y. N. Study of Biopolymer Chitosan as Resist for Submicron Electronic Lithography. Solid State Phenomena 213, 180-185 (2014).

38. Caillau, M. et al. Fifty Nanometer Lines Patterned into Silica Using Water Developable Chitosan Bioresist and Electron Beam Lithography. Journal of Vacuum Science & Technology B 35, 06GE01 (2017).

39. Yoksan, R., Akashi, M., Biramontri, S. & Chirachanchai, S. Hydrophobic Chain Conjugation at Hydroxyl Group onto y-Ray Irradiated Chitosan. Biomacromolecules 2, 10381044 (2001).

40. Sionkowska, A. et al. Thermal and Mechanical Properties of UV Irradiated Colla-gen/Chitosan Thin Films. Polymer Degradation and Stability 91, 3026-3032 (2006).

41. Chmielewski, A. G. Chitosan and Radiation Chemistry. Radiation Physics and Chemistry 79, 272-275 (2010).

42. Garcia, M. A. et al. Effect of Molecular Weight Reduction by Gamma Irradiation on the Antioxidant Capacity of Chitosan from Lobster Shells. Journal of Radiation Research and Applied Sciences 8, 190-200 (2015).

43. Pestov, A. & Bratskaya, S. Chitosan and Its Derivatives as Highly Efficient Polymer Ligands. Molecules 21, 330 (2016).

44. Yang, F., Liu, H., Qu, J. & Paul Chen, J. Preparation and Characterization of Chitosan Encapsulated Sargassum Sp. Biosorbent for Nickel Ions Sorption. Bioresource Technology 102, 2821-2828 (2011).

45. Matienzo, J., Yin, L. I., Grim, S. O. & Swartz, W. E. X-Ray Photoelectron Spectroscopy of Nickel Compounds. Inorg. Chem. 12, 2762-2769 (1973).

46. McIntyre, N. S. & Cook, M. G. X-Ray Photoelectron Studies on Some Oxides and Hydroxides of Cobalt, Nickel, and Copper. Anal. Chem. 47, 2208-2213 (1975).

47. Vieira, R. S., Oliveira, M. L. M., Guibal, E., Rodríguez-Castellón, E. & Beppu, M. M. Copper, Mercury and Chromium Adsorption on Natural and Crosslinked Chitosan Films: An XPS Investigation of Mechanism. Colloids and Surfaces A: Physicochemical and Engineering Aspects 374, 108-114 (2011).

48. Lakhdhar, I., Belosinschi, D., Mangin, P. & Chabot, B. Development of a Bio-Based Sorbent Media for the Removal of Nickel Ions from Aqueous Solutions. Journal of Environmental Chemical Engineering 4, 3159-3169 (2016).

49. Li, J., Du, Y. & Liang, H. Low Molecular Weight Water-Soluble Chitosans: Preparation with the Aid of Cellulase, Characterization, and Solubility. Journal of Applied Polymer Science 102, 1098-1105 (2006).

50. T. Koev, S. et al. Chitosan: An Integrative Biomaterial for Lab-on-a-Chip Devices. Lab on a Chip 10, 3026-3042 (2010).

51. Pradhan, S., Shukla, S. S. & Dorris, K. L. Removal of Nickel from Aqueous Solutions Using Crab Shells. Journal of Hazardous Materials 125, 201-204 (2005).

52. Moreau, W. M. Semiconductor Lithography (Springer US, Boston, MA, 1988).

53. Bowden, M. J. The Physics and Chemistry of the Lithographic Process. J. Electrochem. Soc. 128, 195C (1981).

54. Mende, M., Schwarz, D., Steinbach, C., Boldt, R. & Schwarz, S. The Influence of Salt Anions on Heavy Metal Ion Adsorption on the Example of Nickel. Materials 11, 373 (2018).

55. Menard, E. et al. High-Performance n- and p-Type Single-Crystal Organic Transistors with Free-Space Gate Dielectrics. Adv. Mater. 16, 2097-2101 (2004).

56. Cho, J., Heuzey, M.-C., Bégin, A. & Carreau, P. J. Viscoelastic Properties of Chitosan Solutions: Effect of Concentration and Ionic Strength. Journal of Food Engineering 74, 500-515 (2006).

57. Fusella, M. A. et al. Use of an Underlayer for Large Area Crystallization of Rubrene Thin Films. Chem. Mater. 29, 6666-6673 (2017).

58. Choi, H. H. et al. Hall Effect in Polycrystalline Organic Semiconductors: The Effect of Grain Boundaries. Adv. Funct. Mater. 30, 1903617 (2020).

59. Moisala, A. et al. Single-Walled Carbon Nanotube Synthesis Using Ferrocene and Iron Pentacarbonyl in a Laminar Flow Reactor. Chemical Engineering Science 61,4393-4402 (2006).

60. Charlier, J.-C., Blase, X. & Roche, S. Electronic and Transport Properties of Nanotubes. Rev. Mod. Phys. 79, 677-732 (2007).

61. Laird, E. A. et al. Quantum Transport in Carbon Nanotubes. Rev. Mod. Phys. 87,703-764 (2015).

62. Franklin, A. D. et al. Sub-10 Nm Carbon Nanotube Transistor. Nano Lett. 12, 758-762 (2012).

63. Choi, H. H., Cho, K., Frisbie, C. D., Sirringhaus, H. & Podzorov, V. Critical Assessment of Charge Mobility Extraction in FETs. Nature Mater 17, 2-7 (2018).

64. Manka, R. & Ogrodnik, B. A Model of Soliton Transport along Microtubules. J Biol Phys 18, 185-189 (1991).

65. Sataric, M. V., Tuszynski, J. A. & Zakula, R. B. Kinklike Excitations as an Energy-Transfer Mechanism in Microtubules. Phys. Rev. E 48, 589-597 (1993).

66. Kane, C. L. & Mele, E. J. Z2 Topological Order and the Quantum Spin Hall Effect. Phys. Rev. Lett. 95, 146802 (2005).

67. Kane, C. L. & Mele, E. J. Quantum Spin Hall Effect in Graphene. Phys. Rev. Lett. 95, 226801 (2005).

68. Bernevig, B. A., Hughes, T. L. & Zhang, S.-C. Quantum Spin Hall Effect and Topological Phase Transition in HgTe Quantum Wells. Science 314, 1757-1761 (2006).

69. Fu, L. & Kane, C. L. Topological Insulators with Inversion Symmetry. Phys. Rev. B 76, 045302 (2007).

70. Roth, A. et al. Nonlocal Transport in the Quantum Spin Hall State. Science 325,294-297 (2009).

71. Büttiker, M. Four-Terminal Phase-Coherent Conductance. Phys. Rev. Lett. 57,1761-1764 (1986).

72. Büttiker, M. Absence of Backscattering in the Quantum Hall Effect in Multiprobe Conductors. Phys. Rev. B 38, 9375-9389 (1988).

73. Olshanetsky, E. B. et al. Persistence of a Two-Dimensional Topological Insulator State in Wide HgTe Quantum Wells. Phys. Rev. Lett. 114, 126802 (2015).

74. Grabecki, G. et al. Nonlocal Resistance and Its Fluctuations in Microstructures of Band-Inverted HgTe/(Hg,Cd)Te Quantum Wells. Phys. Rev. B 88, 165309 (2013).

75. Nowack, K. C. et al. Imaging Currents in HgTe Quantum Wells in the Quantum Spin Hall Regime. Nature Materials 12, 787-791 (2013).

76. Ma, E. Y. et al. Unexpected Edge Conduction in Mercury Telluride Quantum Wells under Broken Time-Reversal Symmetry. Nat Commun 6, 7252 (2015).

77. Brüne, C. et al. Evidence for the Ballistic Intrinsic Spin Hall Effect in HgTe Nanostruc-tures. Nature Physics 6, 448-454 (2010).

78. Gusev, G. M. et al. Temperature Dependence of the Resistance of a Two-Dimensional Topological Insulator in a HgTe Quantum Well. Phys. Rev. B 89, 125305 (2014).

79. Wu, C., Bernevig, B. A. & Zhang, S.-C. Helical Liquid and the Edge of Quantum Spin Hall Systems. Phys. Rev. Lett. 96, 106401 (2006).

80. Xu, C. & Moore, J. E. Stability of the Quantum Spin Hall Effect: Effects of Interactions, Disorder, and Z2 Topology. Phys. Rev. B 73, 045322 (2006).

81. Raichev, O. E. Effective Hamiltonian, Energy Spectrum, and Phase Transition Induced by in-Plane Magnetic Field in Symmetric HgTe Quantum Wells. Phys. Rev. B 85,045310 (2012).

82. Piatrusha, S. U. et al. Topological Protection Brought to Light by the Time-Reversal Symmetry Breaking. Phys. Rev. Lett. 123, 056801 (2019).

83. König, M. Spin-Related Transport Phenomena in HgTe-based Quantum Well Structures (Universität Würzburg, 2007).

84. Skolasinski, R., Pikulin, D. I., Alicea, J. & Wimmer, M. Robust Helical Edge Transport in Quantum Spin Hall Quantum Wells. Phys. Rev. B 98, 201404 (2018).

85. Durnev, M. V. & Tarasenko, S. A. Magnetic Field Effects on Edge and Bulk States in Topological Insulators Based on HgTe/CdHgTe Quantum Wells with Strong Natural Interface Inversion Asymmetry. Phys. Rev. B 93, 075434 (2016).

86. Tikhonov, E. S. et al. Shot Noise of the Edge Transport in the Inverted Band HgTe Quantum Wells. Jetp Lett. 101, 708-713 (2015).

87. Piatrusha, S. U. et al. Edge States in Lateral p - n Junctions in Inverted-Band HgTe Quantum Wells. Phys. Rev. B 96, 245417 (2017).

88. Beenakker, C. W. J. Random-Matrix Theory of Quantum Transport. Rev. Mod. Phys. 69, 731-808 (1997).

89. Aseev, P. P. & Nagaev, K. E. Shot Noise in the Edge States of Two-Dimensional Topological Insulators. Phys. Rev. B 94, 045425 (2016).

90. Lezmy, N., Oreg, Y. & Berkooz, M. Single and Multiparticle Scattering in Helical Liquid with an Impurity. Phys. Rev. B 85, 235304 (2012).

91. Kainaris, N., Gornyi, I. V., Carr, S. T. & Mirlin, A. D. Conductivity of a Generic Helical Liquid. Phys. Rev. B 90, 075118 (2014).

92. Mesoscopic Electron Transport (eds Sohn, L. L., Kouwenhoven, L. P. & Schön, G.) (Springer Netherlands, Dordrecht, 1997).

93. Schmidt, T. L., Rachel, S., von Oppen, F. & Glazman, L. I. Inelastic Electron Backscat-tering in a Generic Helical Edge Channel. Phys. Rev. Lett. 108, 156402 (2012).

94. Chou, Y.-Z., Nandkishore, R. M. & Radzihovsky, L. Gapless Insulating Edges of Dirty Interacting Topological Insulators. Phys. Rev. B 98, 054205 (2018).

95. Gornyi, I. V., Mirlin, A. D. & Polyakov, D. G. Electron Transport in a Disordered Luttinger Liquid. Phys. Rev. B 75, 085421 (2007).

96. Teo, J. C. Y. & Kane, C. L. Critical Behavior of a Point Contact in a Quantum Spin Hall Insulator. Phys. Rev. B 79, 235321 (2009).

97

98

99

100

101

102

103

104

105

106

107

108

109

110

111

112

113

Ström, A. & Johannesson, H. Tunneling between Edge States in a Quantum Spin Hall System. Phys. Rev. Lett. 102, 096806 (2009).

Li, T. et al. Observation of a Helical Luttinger Liquid in InAs/GaSb Quantum Spin Hall Edges. Phys. Rev. Lett. 115, 136804 (2015).

Stühler, R. et al. Tomonaga-Luttinger Liquid in the Edge Channels of a Quantum Spin Hall Insulator. Nature Physics 16, 47-51 (2020).

Väyrynen, J. I., Geissler, F. & Glazman, L. I. Magnetic Moments in a Helical Edge Can Make Weak Correlations Seem Strong. Phys. Rev. B 93, 241301 (2016).

König, M. et al. Spatially Resolved Study of Backscattering in the Quantum Spin Hall State. Phys. Rev. X 3, 021003 (2013).

Maciejko, J. et al. Kondo Effect in the Helical Edge Liquid of the Quantum Spin Hall State. Phys. Rev. Lett. 102, 256803 (2009).

Tanaka, Y., Furusaki, A. & Matveev, K. A. Conductance of a Helical Edge Liquid Coupled to a Magnetic Impurity. Phys. Rev. Lett. 106, 236402 (2011).

Altshuler, B. L., Aleiner, I. L. & Yudson, V. I. Localization at the Edge of a 2D Topological Insulator by Kondo Impurities with Random Anisotropies. Phys. Rev. Lett. 111, 086401 (2013).

Kurilovich, P. D., Kurilovich, V. D., Burmistrov, I. S. & Goldstein, M. Helical Edge Transport in the Presence of a Magnetic Impurity. Jetp Lett. 106, 593-599 (2017).

Väyrynen, J. I. & Glazman, L. I. Current Noise from a Magnetic Moment in a Helical Edge. Phys. Rev. Lett. 118, 106802 (2017).

Kurilovich, P. D., Kurilovich, V. D., Burmistrov, I. S., Gefen, Y. & Goldstein, M. Unrestricted Electron Bunching at the Helical Edge. Phys. Rev. Lett. 123, 056803 (2019).

Bernevig, B. A. & Zhang, S.-C. Quantum Spin Hall Effect. Phys. Rev. Lett. 96, 106802 (2006).

Ström, A., Johannesson, H. & Japaridze, G. I. Edge Dynamics in a Quantum Spin Hall State: Effects fromRashba Spin-Orbit Interaction. Phys. Rev. Lett. 104, 256804 (2010).

Del Maestro, A., Hyart, T. & Rosenow, B. Backscattering between Helical Edge States via Dynamic Nuclear Polarization. Phys. Rev. B 87, 165440 (2013).

Geissler, F., Crepin, F. & Trauzettel, B. Random Rashba Spin-Orbit Coupling at the Quantum Spin Hall Edge. Phys. Rev. B 89, 235136 (2014).

Lunde, A. M. & Platero, G. Hyperfine Interactions in Two-Dimensional HgTe Topological Insulators. Phys. Rev. B 88, 115411 (2013).

Hsu, C.-H., Stano, P., Klinovaja, J. & Loss, D. Nuclear-Spin-Induced Localization of Edge States in Two-Dimensional Topological Insulators. Phys. Rev. B 96, 081405 (2017).

114

115

116

117

118

119

120

121

122

123

124

125

126

127

128

129

130

Hsu, C.-H., Stano, P., Klinovaja, J. & Loss, D. Effects of Nuclear Spins on the Transport Properties of the Edge of Two-Dimensional Topological Insulators. Phys. Rev. B 97, 125432 (2018).

Kimchi, I., Chou, Y.-Z., Nandkishore, R. M. & Radzihovsky, L. Anomalous Localization at the Boundary of an Interacting Topological Insulator. Phys. Rev. B101,035131 (2020).

Schottky, W. Über spontane Stromschwankungen in verschiedenen Elektrizitätsleitern. Ann. Phys. 362, 541-567 (1918).

Blanter, Y. M. & Büttiker, M. Shot Noise in Mesoscopic Conductors. Physics Reports 336, 1-166 (2000).

Nagaev, K. On the Shot Noise in Dirty Metal Contacts. Phys Lett A 169,103-107 (1992).

Beenakker, C. W. J. & Büttiker, M. Suppression of Shot Noise in Metallic Diffusive Conductors. Phys. Rev. B 46, 1889-1892 (1992).

Nagaev, K. E. Influence of Electron-Electron Scattering on Shot Noise in Diffusive Contacts. Phys. Rev. B 52, 4740-4743 (1995).

Piatrusha, S. U. et al. Noise Insights into Electronic Transport. Jetp Lett. 108, 71-83 (2018).

De Picciotto, R., Stormer, H. L., Pfeiffer, L. N., Baldwin, K. W. & West, K. W. Four-Terminal Resistance of a Ballistic Quantum Wire. Nature 411, 51-54 (2001).

Tikhonov, E. S., Khrapai, V. S., Shovkun, D. V. & Schuh, D. Finite-Size Effect in Shot Noise in Hopping Conduction. Jetp Lett. 98, 121-126 (2013).

Fu, L. & Kane, C. L. Superconducting Proximity Effect and Majorana Fermions at the Surface of a Topological Insulator. Phys. Rev. Lett. 100, 096407 (2008).

Lutchyn, R. M., Sau, J. D. & Das Sarma, S. Majorana Fermions and a Topological Phase Transition in Semiconductor-Superconductor Heterostructures. Phys. Rev. Lett. 105, 077001 (2010).

Oreg, Y., Refael, G. & von Oppen, F. Helical Liquids and Majorana Bound States in Quantum Wires. Phys. Rev. Lett. 105, 177002 (2010).

Mourik, V. et al. Signatures of Majorana Fermions in Hybrid Superconductor-Semiconductor Nanowire Devices. Science 336, 1003-1007 (2012).

Krogstrup, P. et al. Epitaxy of Semiconductor-Superconductor Nanowires. Nature Materials 14, 400-406 (2015).

Gül, Ö. etal. Ballistic Majorana Nanowire Devices. Nature Nanotechnology 13,192-197 (2018).

Yu, P. et al. Non-Majorana States Yield Nearly Quantized Conductance in Proximatized Nanowires. Nat. Phys. 17, 482-488 (2021).

131

132

133

134

135

136

137

138

139

140

141

142

143

144

145

146

Menard, G. C. et al. Conductance-Matrix Symmetries of a Three-Terminal Hybrid Device. Phys. Rev. Lett. 124, 036802 (2020).

Puglia, D. et al. Closing of the Induced Gap in a Hybrid Superconductor-Semiconductor Nanowire. arXiv: 2006.01275 [cond-mat] (2020).

Lai, Y.-H., Sau, J. D. & Das Sarma, S. Presence versus Absence of End-to-End Nonlocal Conductance Correlations in Majorana Nanowires: Majorana Bound States versus Andreev Bound States. Phys. Rev. B 100, 045302 (2019).

Rosdahl, T. Ö., Vuik, A., Kjaergaard, M. & Akhmerov, A. R. Andreev Rectifier: A Nonlocal Conductance Signature of Topological Phase Transitions. Phys. Rev. B 97, 045421 (2018).

Akhmerov, A. R., Dahlhaus, J. P., Hassler, F., Wimmer, M. & Beenakker, C. W. J. Quantized Conductance at the Majorana Phase Transition in a Disordered Superconducting Wire. Phys. Rev. Lett. 106, 057001 (2011).

Pan, H., Sau, J. D. & Das Sarma, S. Three-Terminal Nonlocal Conductance in Majorana Nanowires: Distinguishing Topological and Trivial in Realistic Systems with Disorder and Inhomogeneous Potential. Phys. Rev. B 103, 014513 (2021).

Andreev, A. F. The Thermal Conductivity of the Intermediate State in Superconductors. Sov. Phys. JETP 19, 1228-1231 (1964).

Andreev, A. F. Thermal Conductivity of the Intermediate State of Superconductors. II. Sov. Phys. JETP 20, 1490-1494 (1965).

Nagaev, K. E. & Büttiker, M. Semiclassical Theory of Shot Noise in Disordered Superconductor-Normal-Metal Contacts. Phys. Rev. B 63, 081301 (2001).

Nagaev, K. E. Nonlocal Effects in the Shot Noise of Diffusive Superconductor-Normal-Metal Systems. Phys. Rev. B 64, 081304 (2001).

Nazarov, Y. V. & Stoof, T. H. Diffusive Conductors as Andreev Interferometers. Phys. Rev. Lett. 76, 823-826 (1996).

Blonder, G. E., Tinkham, M. & Klapwijk, T. M. Transition from Metallic to Tunneling Regimes in Superconducting Microconstrictions: Excess Current, Charge Imbalance, and Supercurrent Conversion. Phys. Rev. B 25, 4515-4532 (1982).

Kopnin, N. B. Theory of Nonequilibrium Superconductivity (Clarendon Press; Oxford University Press, 2001).

Keizer, R. S., Flokstra, M. G., Aarts, J. & Klapwijk, T. M. Critical Voltage of aMesoscopic Superconductor. Phys. Rev. Lett. 96, 147002 (2006).

Pothier, H., Gueron, S., Birge, N. O., Esteve, D. & Devoret, M. H. Energy Distribution Function of Quasiparticles in Mesoscopic Wires. Phys. Rev. Lett. 79, 3490-3493 (1997).

Tikhonov, E. S. et al. Spatial and Energy Resolution of Electronic States by Shot Noise. Phys. Rev. B 102, 085417 (2020).

147. Snyman, I. & Nazarov, Y. V. Bistability in Voltage-Biased Normal-Metal/Insulator/Superconductor/Insulator/Normal-Metal Structures. Phys. Rev. B 79, 014510(2009).

148. Tikhonov, E. S. et al. Andreev Reflection in an s -Type Superconductor Proximized 3D Topological Insulator. Phys. Rev. Lett. 117, 147001 (2016).

149. Chang, W. et al. Hard Gap in Epitaxial Semiconductor-Superconductor Nanowires. Nature Nanotech 10, 232-236 (2015).

150. Kjaergaard, M. et al. Quantized Conductance Doubling and Hard Gap in a Two-Dimensional Semiconductor-Superconductor Heterostructure. Nat Commun 7, 12841 (2016).

151. Jehl, X., Sanquer, M., Calemczuk, R. & Mailly, D. Detection of Doubled Shot Noise in Short Normal-Metal/ Superconductor Junctions. Nature 405, 50-53 (2000).

152. Claughton, N. R. & Lambert, C. J. Thermoelectric Properties of Mesoscopic Superconductors. Phys. Rev. B 53, 6605-6612 (1996).

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