Creating and Characterizing a Single Molecule Device for Quantitative Surface Science Matthew Felix Blishen Green
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ey Technologies ey K Schlüsseltechnologien Creating and characterizing an SMD and characterizing Creating 181 Creating and characterizing a single molecule device for quantitative surface science Matthew Felix Blishen Green Schlüsseltechnologien / Key Technologies Schlüsseltechnologien / Key Technologies Band / Volume 181 Band / Volume 181 ISBN 978-3-95806-352-5 ISBN 978-3-95806-352-5 Matthew Felix Blishen Green Felix Matthew Schriften des Forschungszentrums Jülich Reihe Schlüsseltechnologien / Key Technologies Band / Volume 181 Forschungszentrum Jülich GmbH Peter Grünberg Institut (PGI) Functional Nanostructures at Surfaces (PGI-3) Creating and characterizing a single molecule device for quantitative surface science Matthew Felix Blishen Green Schriften des Forschungszentrums Jülich Reihe Schlüsseltechnologien / Key Technologies Band / Volume 181 ISSN 1866-1807 ISBN 978-3-95806-352-5 Bibliografische Information der Deutschen Nationalbibliothek. Die Deutsche Nationalbibliothek verzeichnet diese Publikation in der Deutschen Nationalbibliografie; detaillierte Bibliografische Daten sind im Internet über http://dnb.d-nb.de abrufbar. Herausgeber Forschungszentrum Jülich GmbH und Vertrieb: Zentralbibliothek, Verlag 52425 Jülich Tel.: +49 2461 61-5368 Fax: +49 2461 61-6103 [email protected] www.fz-juelich.de/zb Umschlaggestaltung: Grafische Medien, Forschungszentrum Jülich GmbH Druck: Grafische Medien, Forschungszentrum Jülich GmbH Copyright: Forschungszentrum Jülich 2018 Schriften des Forschungszentrums Jülich Reihe Schlüsseltechnologien / Key Technologies, Band / Volume 181 D 82 (Diss., RWTH Aachen University, 2018) ISSN 1866-1807 ISBN 978-3-95806-352-5 Vollständig frei verfügbar über das Publikationsportal des Forschungszentrums Jülich (JuSER) unter www.fz-juelich.de/zb/openaccess. This is an Open Access publication distributed under the terms of the Creative Commons Attribution License 4.0, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. It is fair to state that we are not going to experiment with single particles any more than we will raise dinosaurs in the zoo. —Erwin Schrödinger iv Acknowledgments There are many people without whom this dissertation would have been impossible to complete. For this reason I would like to thank • Prof. Dr. Stefan Tautz for the opportunity to perform exciting research at PGI-3. When discussing the nature of our work, he once said ‘the molecules will do what they have to do’, and this rigour, respect but mostly love of his for physics and science helped me greatly during my time in Jülich. His enthusiasm for an enormous range of topics led to many lively lunchtime conversations, which however after the 23rd of June 2016 often revolved around one topic in particular. • Dr. Ruslan Temirov for his excellent scientific supervision. His relentless search for the truth inspired me and he can often be found saying ‘there are no miracles’, a sentiment which gave me the impetus to look at many problems in a different way. I am very grateful for the countless discussions on science and beyond that we shared and the stimulating working environment he created. • Dr. Christian Wagner for all his support but also the good times we enjoyed together in the lab. Without his advice and contributions this work would certainly have been less successful. • Philipp Leinen and Dr. Taner Esat for our fruitful collaboration throughout the years. They were always around for interesting discussions, to help out in the lab or just to kick a football around the office. • Dr. Norman Fournier for showing me the ropes, not only in the LT-STM/AFM lab but in Cologne-Ehrenfeld too. v • Alexander Grötsch for our collaboration with the motion tracking system and for speaking so much German with me in the lab; this certainly contributed to us not having to speak much English later on! • All the members of PGI-3/ICS-7 who contributed to the very enjoyable work- ing atmosphere in the institute. • The many great friends I made while travelling to the research centre with the Rurtalbahn. No matter how delayed the RE1 was, the quality time spent with them provided me with a joyful start and end to the working day. • My parents and step-parents Jo, Russ, Stuart and Isobel and my sisters Anna and Sasha for everything they do for me. Knowing that they are there for me makes life’s challenges seem a little less insurmountable. • Last but most importantly, my closest companion in life Sonja for her love, patience and support through all the highs and lows of the last several years. In fact, I couldn’t imagine it without her. vi Contents Introduction 1 1. Theoretical background and experimental techniques 5 1.1. Introduction to scanning tunnelling microscopy . 6 1.2. Introduction to atomic force microscopy . 10 1.3. Experimental details . 13 1.3.1. Experimental setup . 13 1.3.2. Sample and tip preparation . 17 2. Patterning a hydrogen-bonded molecular monolayer with a hand-controlled SPM 19 Introduction . 20 2.1. Patterning a hydrogen-bonded molecular monolayer with a hand- controlled SPM . 22 3. Scanning Quantum Dot Microscopy 31 Introduction . 32 3.1. Scanning Quantum Dot Microscopy . 33 3.2. Scanning Quantum Dot Microscopy: Supplemental Information . 39 3.3. A quantitative method to measure local electrostatic potential near surfaces . 47 4. Quantitative modelling of single electron charging events 55 Introduction . 56 4.1. Single electron box model . 57 4.1.1. Experimental data . 59 4.1.2. Free energy of the system . 64 vii Contents 4.1.3. Charging events of the QD . 66 4.1.4. Charging force . 73 4.1.5. Applying the theory to experimental data . 76 4.2. Point charge model . 81 4.2.1. Predictions of the point charge model . 81 4.2.2. Discrepancy in α ......................... 86 4.2.3. Energy level position and Coulomb repulsion . 92 4.3. Discussion . 95 Conclusion and outlook . 100 4.A. Appendix . 102 4.A.1. Interplay of frequency shift and tunnelling current . 102 4.A.2. Determining the electronic coupling between tip and QD . 104 5. Accurate work function changes measured with scanning quantum dot microscopy 109 Introduction . 110 5.1. Point charge model to obtain change in work function . 112 5.1.1. An expression for local potential . 112 5.1.2. Removing the influence of the tip’s properties . 115 5.2. Change in work function of Ag(111) after PTCDA adsorption . 117 5.2.1. Constant height KPFM results . 117 5.2.2. SQDM results . 119 5.2.3. Discussion . 120 Conclusion and outlook . 126 Summary 129 Bibliography 133 List of Figures 141 viii Introduction As the technological needs of today’s global society continue to increase, the pres- sure to develop more powerful, more efficient and above all more compact electronic devices increases simultaneously. In 1965 Moore [1] exhibited a correlation between the number of transistors on an integrated circuit and the number of years following the invention of the integrated circuit in 1958 — the transistor count seemed to be roughly doubling every year. This prediction was modified to doubling every two years, which until several years ago had been fulfilled rather exactly. However the miniaturization limit of the current field effect transistor technology is gradually be- ing reached [2], and a shift in the electronics paradigm will soon be required. There are several promising avenues currently at the focus of research for next-generation information technology; 2D materials, multiferroics and spin- and valleytronics form several examples [3–6]. A further example is the exciting field of molecular-scale elec- tronics, where single molecules forming functional electronic devices is the ultimate goal [7, 8]. Aviram and Ratner’s calculation of electronic transport through a single molecule [9] is often heralded as the beginning of modern molecular electronics. Their idea was that a single, polar molecule could act as a rectifier, which converts an alternat- ing current into a direct current. However they were ahead of their time; the lack of appropriate technology prevented their ideas from being built upon in experiment. The advent of scanning tunnelling microscopy (STM) in the early 1980s [10] was the stimulus that molecular-scale electronics needed. Several seminal STM as well as mechanically controllable break junction experiments were the first to demonstrate transport through single molecules [11, 12]. In the years since then, a wide variety of functions have been demonstrated using single molecules, including transistor func- tionality [13–15] and rectification [16, 17], but also electromechanical amplification [18], switching [19, 20], memristance [21] and directional, mechanical motion [22]. 1 Introduction The central challenges, besides economic considerations, that the integration of molecular electronic components into real world applications faces can be summa- rized into two general categories: control of electronic properties and control of geo- metrical properties. The understanding of electron transport through molecules is a key point where much research effort has been focused in the last decade [23]. How- ever as Ratner [7] stated, with the estimated number of possible molecular structures at ∼1060 for small organic molecules, there is still much to be discovered in this area. As far as control over the geometry of a molecular system is concerned, bottom-up rather than top-down fabrication processes must be employed in order to allow for the tuning of of the properties of individual molecules. Here there are two main approaches: allowing molecules to arrange themselves into a pre-designed structure, known as self-assembly, or building a structure with the molecules as the ‘building blocks’. Both approaches can in principle lead to extended structures defined at the molecular scale, and can even be employed in conjunction as will be displayed in this thesis. Seminal works, where single CO as well as C60 molecules were individually positioned on surfaces, demonstrated the feasibility of STM for molecular manipu- lation [24, 25]. However deterministic control over complex molecules at all stages of the manipulation procedure, vital for molecular-scale construction, has not yet been presented.