Superconducting Qubits Coupled to Nanoelectromechanical Resonators An Architecture for Soli

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四苯基乙烯衍生物的合成与生物成像研究

四苯基乙烯衍生物的合成与生物成像研究

中文摘要四苯基乙烯衍生物的合成与生物成像研究生物成像已成为当今生物研究中的有力工具,因为它提供了一种独特的方法来可视化细胞的形态细节。

荧光成像是实时,非侵入性监测生物分子的最强大的生物成像技术之一。

在过去几十年中,荧光探针的发展已促进细胞生物学的重大进展。

各种荧光探针,如半导体量子点,荧光碳点,Ln离子掺杂纳米材料,光致发光硅纳米颗粒,金属纳米团簇,有机小分子和有机荧光纳米颗粒已被合成并广泛研究用于生物应用。

聚集诱导发光(AIE)材料由于其优异的光学性质在生物成像领域得到了广泛的研究。

本论文基于四苯基乙烯(TPE),合成了一系列具有聚集诱导发光性质的荧光材料,并利用这些材料制备的纳米粒子进行生物成像。

具体研究内容如下:1.以四苯基乙烯为核,通过选择电子供体(D)和受体(A)的适当组合来设计和合成AIE红光分子。

通过将二甲胺和氰基部分引入TPE中,合成了具有不同AIE特性的四种新的红光化合物1,2,3和4。

四种化合物在固态下的最高量子产率可达到40%。

该化合物可以容易地制造成均一稳定的荧光纳米粒子。

并且化合物1负载的Pluronic F127 纳米粒子的发射主峰位在650nm处,并且高荧光量子产率为15.2%。

化合物1和2的纳米粒子对A549肺癌细胞的生物学成像表明这些化合物是癌细胞的有效荧光探针。

2.基于四苯基乙烯,合成出一种新型有机荧光染料TPE-2NH2。

这种材料发绿光,在NO存在下能与其发生反应生成的产物发红光,因此这种材料具有检测NO的性质。

由于材料的疏水性,我们将此染料负载到二氧化硅介孔纳米粒子中,制备了的纳米粒子均一,稳定,具有120nm的平均粒径,良好的生物相容性,较高的灵敏度。

将此纳米粒子与MCF-7细胞共培养,在细胞质中发现红光信号。

因此,此探针在细胞内检测到NO,表现出良好的应用价值。

关键词:聚集诱导发光,四苯基乙烯,生物成像1AbstractSynthesis and Bioimaging Application of TetraphenyletheneDerivativesBiological imaging (bioimaging) has become a powerful tool in biological research today because it offers a unique approach to visualize the morphological details of cells. Fluorescence imaging is one of the most powerful bioimaging techniques for real-time, non-invasive monitoring of biomolecules of interest in their native environments with high spatial and temporal resolution, and is instrumental for revealing fundamental insights into the production, localization, trafficking, and biological roles of biomolecules in complex living systems. The development of fluorescent probes has facilitated the recent significant advances in cell biology and medical diagnostic imaging. Over the past few decades, a variety of fluorescent probes, such as semiconductor quantum dots, fluorescent carbon dots, Ln ion doped nanomaterials, photo-luminescent silicon nanoparticles, metallic nanoclusters, organic small molecules and organic fluorescent nanoparticles have been synthesized and extensively investigated for biological applications. Aggregation Induce Emision (AIE) materials have been extensively studied in the field of biomimetic imaging due to their excellent optical properties. In this paper, based on tetraphenyl ethylene (TPE), a series of fluorescent materials with aggregation induced luminescent properties were synthesized and biologically imaged using the nanoparticles prepared by these materials. The specific research contents are as follows:1. Organic fluorescent probes play an important role in modernbiomedical research, such as biological sensing and imaging. However, the development of organic fluorophores with efficient aggregate state emissions expanded to the red to near-infrared region is still challenging. Here, we present a series of highly efficient Far Red/Near-Infrared (FR/NIR)2fluorescent compounds with aggregation-induced emission (AIE) properties by attaching electron donor and accepter to tetraphenylethene (TPE) moieties through a simple synthesis method. These compounds exhibit the pronounced fluorescence enhancement in aggregate state, the red to near infrared emission, and facile fabrication into uniform compouds-loaded Pluronic F127 NPs. The emission maximum of the NPs fabricated by the self assembly method is in the range of 550nm-850nm and the highest fluorescent quantum yield is 15.2%. The biological imaging of NPs of compound 1 and 2 for A549 lung cancer cell indicates that these compounds are effective fluorescent probes for cancer cell with high specificity, high photostability and good fluorescence contrast.2. Based on tetraphenylethylene, a novel organic fluorescent dye TPE-2NH2 was synthesized. This material is green emision, it can be reacted and the product generated red emision the presence of NO, so this material has the nature of the detection of NO. Due to the hydrophobicity of the material, we loaded the dye into the silica mesoporous nanoparticles. The prepared nanoparticles were homogeneous and stable, with an average particle size of 120 nm, good biocompatibility and high sensitivity. The nanoparticles were co-cultured with MCF-7 cells, and red light was found in the cytoplasm. Therefore, this probe in the cell to detect NO, showing a good application value.Keywords:Aggregation-induced emission,Tetraphenylethene,bioimaging3目录第1章前言 (1)1.1引言 (1)1.2具有AIE性质的化合物 (3)1.3AIE小分子生物探针的制备及其应用 (16)1.4负载AIE化合物的荧光纳米粒子的制备及其应用 (28)1.5本论文设计思想和主要内容 (32)1.6参考文献 (33)第2章具有AIE性质的高效红光分子的合成及细胞成像 (45)2.1引言 (45)2.2实验部分 (46)2.3结果与讨论 (49)2.4本章小结 (57)2.5参考文献 (60)第3章基于AIE染料的RNS荧光探针的合成及性质研究 (62)3.1引言 (62)3.2实验部分 (63)3.3结果与讨论 (65)3.4本章小结 (70)3.5参考文献 (71)第4章结论 (74)作者简介 (83)致谢 (84)41第1章 前言1.1引言人们在分子水平上理解基本的发光过程已经取得了显著的成就。

Superconducting qubits II Decoherence

Superconducting qubits II Decoherence
present address: Physics Department and Insitute for Quantum Computing, University of Waterloo, Waterloo, Ontario N2L 3G1, Canada; fwilhelm@iqc.ca ‡ mgeller@
The transition from quantum to classical physics, now known as decoherence, has intrigued physicists since the formulation of quantum mechanics (Giulini et al., 1996; Leggett, 2002; Peres, 1993; Feynman and Vernon, 1963; Zurek, 1993). It has been put into the poignant Schr¨ odinger cat paradox (Schr¨ odinger, 1935) and was considered an open fundamental question for a long time.
and compare it to the corresponding classical mixture leading to the same expectation value of σz 1 1 0 ρmix = (2) 2 0 1 we can see that the von-Neumann entropy ρ = −kB Tr [ρ log ρ] rises from Spure = 0 to Smix = kB ln 2. Hence, decoherence taking ρpure to ρmix creates entropy and is irreversible. Quantum mechanics, on the other hand, is always reversible. It can be shown, that any isolated quantum system is described by the Liouville von-Neumann equation i¯ hρ ˙ = [H, ρ] (3)

journal of lightwave technologies -回复

journal of lightwave technologies -回复

journal of lightwave technologies -回复光波技术(Lightwave Technologies)是一种基于光子学原理和技术的领域,旨在利用光的特性来实现高速、高带宽和低能耗的通信、传感和计算。

本文将从光波技术的基本概念、应用领域、发展历程以及未来展望等方面进行详细讨论。

光波技术是一种利用光传输信息、进行数据处理和通信的技术。

与传统的电子方式相比,光波技术具有更高的传输速率、更大的带宽和更低的能耗。

这是因为光信号可以在光纤中通过光的全内反射进行传输,而不受电信号在导线中存在的电阻和电容的影响。

借助光波技术,人们可以实现高速、高容量的数据通信和存储。

例如,在光纤通信中,光信号可以通过激光器发射,经过光纤传输,然后通过光二极管接收。

传统的电信号需要通过电缆传输,信号强度会逐渐衰减并容易受到干扰,而光信号则可以长距离传输而不损失信号质量。

光波技术还可以用于光子传感和光子计算等领域。

在光子传感中,光信号可以用于测量和检测物理量,如温度、压力和湿度。

由于光传感器具有高灵敏度和低噪声的特点,可以实现高精度的传感。

在光子计算中,光信号可以传输和处理大量的数据,并具有并行计算的能力。

这使得光子计算在大规模数据处理和高性能计算方面具有潜在的应用前景。

光波技术的发展历程可以追溯到20世纪60年代。

最初,光纤通信只能传输低速率的信号。

然而,随着激光器和光纤材料的不断改进,光波技术的传输速率和传输距离也有了显著提高。

20世纪80年代,光波技术开始在长距离通信中得到广泛应用。

21世纪以来,随着光通信和光计算技术的进一步发展,光波技术逐渐成为实现大容量和高速率数据传输的主流技术。

未来,光波技术有望在多个领域得到进一步应用和发展。

首先,随着互联网的普及和数据需求的不断增长,光波技术将继续推进数据通信的速度和容量。

其次,光波技术在传感和计算领域的应用也将得到拓展。

例如,在医疗诊断中,光子传感可以用于实现无创的医学检测和成像。

有机和量子点太阳能电池中激子的扩散和离解

有机和量子点太阳能电池中激子的扩散和离解

有机和量子点太阳能电池中激子的扩散和离解下载提示:该文档是本店铺精心编制而成的,希望大家下载后,能够帮助大家解决实际问题。

文档下载后可定制修改,请根据实际需要进行调整和使用,谢谢!本店铺为大家提供各种类型的实用资料,如教育随笔、日记赏析、句子摘抄、古诗大全、经典美文、话题作文、工作总结、词语解析、文案摘录、其他资料等等,想了解不同资料格式和写法,敬请关注!Download tips: This document is carefully compiled by this editor. I hope that after you download it, it can help you solve practical problems. The document can be customized and modified after downloading, please adjust and use it according to actual needs, thank you! In addition, this shop provides you with various types of practical materials, such as educational essays, diary appreciation, sentence excerpts, ancient poems, classic articles, topic composition, work summary, word parsing, copy excerpts, other materials and so on, want to know different data formats and writing methods, please pay attention!引言在太阳能电池领域,有机和量子点太阳能电池是备受关注的研究方向之一。

凝聚态物理材料物理专业考博量子物理领域英文高频词汇

凝聚态物理材料物理专业考博量子物理领域英文高频词汇

凝聚态物理材料物理专业考博量子物理领域英文高频词汇1. Quantum Mechanics - 量子力学2. Wavefunction - 波函数3. Hamiltonian - 哈密顿量4. Schrödinger Equation - 薛定谔方程5. Quantum Field Theory - 量子场论6. Quantum Entanglement - 量子纠缠7. Uncertainty Principle - 不确定性原理8. Quantum Tunneling - 量子隧穿9. Quantum Superposition - 量子叠加10. Quantum Decoherence - 量子退相干11. Spin - 自旋12. Quantum Computing - 量子计算13. Quantum Teleportation - 量子纠缠传输14. Quantum Interference - 量子干涉15. Quantum Information - 量子信息16. Quantum Optics - 量子光学17. Quantum Dots - 量子点18. Quantum Hall Effect - 量子霍尔效应19. Bose-Einstein Condensate - 玻色-爱因斯坦凝聚态20. Fermi-Dirac Statistics - 费米-狄拉克统计中文翻译:1. Quantum Mechanics - 量子力学2. Wavefunction - 波函数3. Hamiltonian - 哈密顿量4. Schrödinger Equation - 薛定谔方程5. Quantum Field Theory - 量子场论6. Quantum Entanglement - 量子纠缠7. Uncertainty Principle - 不确定性原理8. Quantum Tunneling - 量子隧穿9. Quantum Superposition - 量子叠加10. Quantum Decoherence - 量子退相干11. Spin - 自旋12. Quantum Computing - 量子计算13. Quantum Teleportation - 量子纠缠传输14. Quantum Interference - 量子干涉15. Quantum Information - 量子信息16. Quantum Optics - 量子光学17. Quantum Dots - 量子点18. Quantum Hall Effect - 量子霍尔效应19. Bose-Einstein Condensate - 玻色-爱因斯坦凝聚态20. Fermi-Dirac Statistics - 费米-狄拉克统计。

物理学专业英语

物理学专业英语

华中师范大学物理学院物理学专业英语仅供内部学习参考!2014一、课程的任务和教学目的通过学习《物理学专业英语》,学生将掌握物理学领域使用频率较高的专业词汇和表达方法,进而具备基本的阅读理解物理学专业文献的能力。

通过分析《物理学专业英语》课程教材中的范文,学生还将从英语角度理解物理学中个学科的研究内容和主要思想,提高学生的专业英语能力和了解物理学研究前沿的能力。

培养专业英语阅读能力,了解科技英语的特点,提高专业外语的阅读质量和阅读速度;掌握一定量的本专业英文词汇,基本达到能够独立完成一般性本专业外文资料的阅读;达到一定的笔译水平。

要求译文通顺、准确和专业化。

要求译文通顺、准确和专业化。

二、课程内容课程内容包括以下章节:物理学、经典力学、热力学、电磁学、光学、原子物理、统计力学、量子力学和狭义相对论三、基本要求1.充分利用课内时间保证充足的阅读量(约1200~1500词/学时),要求正确理解原文。

2.泛读适量课外相关英文读物,要求基本理解原文主要内容。

3.掌握基本专业词汇(不少于200词)。

4.应具有流利阅读、翻译及赏析专业英语文献,并能简单地进行写作的能力。

四、参考书目录1 Physics 物理学 (1)Introduction to physics (1)Classical and modern physics (2)Research fields (4)V ocabulary (7)2 Classical mechanics 经典力学 (10)Introduction (10)Description of classical mechanics (10)Momentum and collisions (14)Angular momentum (15)V ocabulary (16)3 Thermodynamics 热力学 (18)Introduction (18)Laws of thermodynamics (21)System models (22)Thermodynamic processes (27)Scope of thermodynamics (29)V ocabulary (30)4 Electromagnetism 电磁学 (33)Introduction (33)Electrostatics (33)Magnetostatics (35)Electromagnetic induction (40)V ocabulary (43)5 Optics 光学 (45)Introduction (45)Geometrical optics (45)Physical optics (47)Polarization (50)V ocabulary (51)6 Atomic physics 原子物理 (52)Introduction (52)Electronic configuration (52)Excitation and ionization (56)V ocabulary (59)7 Statistical mechanics 统计力学 (60)Overview (60)Fundamentals (60)Statistical ensembles (63)V ocabulary (65)8 Quantum mechanics 量子力学 (67)Introduction (67)Mathematical formulations (68)Quantization (71)Wave-particle duality (72)Quantum entanglement (75)V ocabulary (77)9 Special relativity 狭义相对论 (79)Introduction (79)Relativity of simultaneity (80)Lorentz transformations (80)Time dilation and length contraction (81)Mass-energy equivalence (82)Relativistic energy-momentum relation (86)V ocabulary (89)正文标记说明:蓝色Arial字体(例如energy):已知的专业词汇蓝色Arial字体加下划线(例如electromagnetism):新学的专业词汇黑色Times New Roman字体加下划线(例如postulate):新学的普通词汇1 Physics 物理学1 Physics 物理学Introduction to physicsPhysics is a part of natural philosophy and a natural science that involves the study of matter and its motion through space and time, along with related concepts such as energy and force. More broadly, it is the general analysis of nature, conducted in order to understand how the universe behaves.Physics is one of the oldest academic disciplines, perhaps the oldest through its inclusion of astronomy. Over the last two millennia, physics was a part of natural philosophy along with chemistry, certain branches of mathematics, and biology, but during the Scientific Revolution in the 17th century, the natural sciences emerged as unique research programs in their own right. Physics intersects with many interdisciplinary areas of research, such as biophysics and quantum chemistry,and the boundaries of physics are not rigidly defined. New ideas in physics often explain the fundamental mechanisms of other sciences, while opening new avenues of research in areas such as mathematics and philosophy.Physics also makes significant contributions through advances in new technologies that arise from theoretical breakthroughs. For example, advances in the understanding of electromagnetism or nuclear physics led directly to the development of new products which have dramatically transformed modern-day society, such as television, computers, domestic appliances, and nuclear weapons; advances in thermodynamics led to the development of industrialization; and advances in mechanics inspired the development of calculus.Core theoriesThough physics deals with a wide variety of systems, certain theories are used by all physicists. Each of these theories were experimentally tested numerous times and found correct as an approximation of nature (within a certain domain of validity).For instance, the theory of classical mechanics accurately describes the motion of objects, provided they are much larger than atoms and moving at much less than the speed of light. These theories continue to be areas of active research, and a remarkable aspect of classical mechanics known as chaos was discovered in the 20th century, three centuries after the original formulation of classical mechanics by Isaac Newton (1642–1727) 【艾萨克·牛顿】.University PhysicsThese central theories are important tools for research into more specialized topics, and any physicist, regardless of his or her specialization, is expected to be literate in them. These include classical mechanics, quantum mechanics, thermodynamics and statistical mechanics, electromagnetism, and special relativity.Classical and modern physicsClassical mechanicsClassical physics includes the traditional branches and topics that were recognized and well-developed before the beginning of the 20th century—classical mechanics, acoustics, optics, thermodynamics, and electromagnetism.Classical mechanics is concerned with bodies acted on by forces and bodies in motion and may be divided into statics (study of the forces on a body or bodies at rest), kinematics (study of motion without regard to its causes), and dynamics (study of motion and the forces that affect it); mechanics may also be divided into solid mechanics and fluid mechanics (known together as continuum mechanics), the latter including such branches as hydrostatics, hydrodynamics, aerodynamics, and pneumatics.Acoustics is the study of how sound is produced, controlled, transmitted and received. Important modern branches of acoustics include ultrasonics, the study of sound waves of very high frequency beyond the range of human hearing; bioacoustics the physics of animal calls and hearing, and electroacoustics, the manipulation of audible sound waves using electronics.Optics, the study of light, is concerned not only with visible light but also with infrared and ultraviolet radiation, which exhibit all of the phenomena of visible light except visibility, e.g., reflection, refraction, interference, diffraction, dispersion, and polarization of light.Heat is a form of energy, the internal energy possessed by the particles of which a substance is composed; thermodynamics deals with the relationships between heat and other forms of energy.Electricity and magnetism have been studied as a single branch of physics since the intimate connection between them was discovered in the early 19th century; an electric current gives rise to a magnetic field and a changing magnetic field induces an electric current. Electrostatics deals with electric charges at rest, electrodynamics with moving charges, and magnetostatics with magnetic poles at rest.Modern PhysicsClassical physics is generally concerned with matter and energy on the normal scale of1 Physics 物理学observation, while much of modern physics is concerned with the behavior of matter and energy under extreme conditions or on the very large or very small scale.For example, atomic and nuclear physics studies matter on the smallest scale at which chemical elements can be identified.The physics of elementary particles is on an even smaller scale, as it is concerned with the most basic units of matter; this branch of physics is also known as high-energy physics because of the extremely high energies necessary to produce many types of particles in large particle accelerators. On this scale, ordinary, commonsense notions of space, time, matter, and energy are no longer valid.The two chief theories of modern physics present a different picture of the concepts of space, time, and matter from that presented by classical physics.Quantum theory is concerned with the discrete, rather than continuous, nature of many phenomena at the atomic and subatomic level, and with the complementary aspects of particles and waves in the description of such phenomena.The theory of relativity is concerned with the description of phenomena that take place in a frame of reference that is in motion with respect to an observer; the special theory of relativity is concerned with relative uniform motion in a straight line and the general theory of relativity with accelerated motion and its connection with gravitation.Both quantum theory and the theory of relativity find applications in all areas of modern physics.Difference between classical and modern physicsWhile physics aims to discover universal laws, its theories lie in explicit domains of applicability. Loosely speaking, the laws of classical physics accurately describe systems whose important length scales are greater than the atomic scale and whose motions are much slower than the speed of light. Outside of this domain, observations do not match their predictions.Albert Einstein【阿尔伯特·爱因斯坦】contributed the framework of special relativity, which replaced notions of absolute time and space with space-time and allowed an accurate description of systems whose components have speeds approaching the speed of light.Max Planck【普朗克】, Erwin Schrödinger【薛定谔】, and others introduced quantum mechanics, a probabilistic notion of particles and interactions that allowed an accurate description of atomic and subatomic scales.Later, quantum field theory unified quantum mechanics and special relativity.General relativity allowed for a dynamical, curved space-time, with which highly massiveUniversity Physicssystems and the large-scale structure of the universe can be well-described. General relativity has not yet been unified with the other fundamental descriptions; several candidate theories of quantum gravity are being developed.Research fieldsContemporary research in physics can be broadly divided into condensed matter physics; atomic, molecular, and optical physics; particle physics; astrophysics; geophysics and biophysics. Some physics departments also support research in Physics education.Since the 20th century, the individual fields of physics have become increasingly specialized, and today most physicists work in a single field for their entire careers. "Universalists" such as Albert Einstein (1879–1955) and Lev Landau (1908–1968)【列夫·朗道】, who worked in multiple fields of physics, are now very rare.Condensed matter physicsCondensed matter physics is the field of physics that deals with the macroscopic physical properties of matter. In particular, it is concerned with the "condensed" phases that appear whenever the number of particles in a system is extremely large and the interactions between them are strong.The most familiar examples of condensed phases are solids and liquids, which arise from the bonding by way of the electromagnetic force between atoms. More exotic condensed phases include the super-fluid and the Bose–Einstein condensate found in certain atomic systems at very low temperature, the superconducting phase exhibited by conduction electrons in certain materials,and the ferromagnetic and antiferromagnetic phases of spins on atomic lattices.Condensed matter physics is by far the largest field of contemporary physics.Historically, condensed matter physics grew out of solid-state physics, which is now considered one of its main subfields. The term condensed matter physics was apparently coined by Philip Anderson when he renamed his research group—previously solid-state theory—in 1967. In 1978, the Division of Solid State Physics of the American Physical Society was renamed as the Division of Condensed Matter Physics.Condensed matter physics has a large overlap with chemistry, materials science, nanotechnology and engineering.Atomic, molecular and optical physicsAtomic, molecular, and optical physics (AMO) is the study of matter–matter and light–matter interactions on the scale of single atoms and molecules.1 Physics 物理学The three areas are grouped together because of their interrelationships, the similarity of methods used, and the commonality of the energy scales that are relevant. All three areas include both classical, semi-classical and quantum treatments; they can treat their subject from a microscopic view (in contrast to a macroscopic view).Atomic physics studies the electron shells of atoms. Current research focuses on activities in quantum control, cooling and trapping of atoms and ions, low-temperature collision dynamics and the effects of electron correlation on structure and dynamics. Atomic physics is influenced by the nucleus (see, e.g., hyperfine splitting), but intra-nuclear phenomena such as fission and fusion are considered part of high-energy physics.Molecular physics focuses on multi-atomic structures and their internal and external interactions with matter and light.Optical physics is distinct from optics in that it tends to focus not on the control of classical light fields by macroscopic objects, but on the fundamental properties of optical fields and their interactions with matter in the microscopic realm.High-energy physics (particle physics) and nuclear physicsParticle physics is the study of the elementary constituents of matter and energy, and the interactions between them.In addition, particle physicists design and develop the high energy accelerators,detectors, and computer programs necessary for this research. The field is also called "high-energy physics" because many elementary particles do not occur naturally, but are created only during high-energy collisions of other particles.Currently, the interactions of elementary particles and fields are described by the Standard Model.●The model accounts for the 12 known particles of matter (quarks and leptons) thatinteract via the strong, weak, and electromagnetic fundamental forces.●Dynamics are described in terms of matter particles exchanging gauge bosons (gluons,W and Z bosons, and photons, respectively).●The Standard Model also predicts a particle known as the Higgs boson. In July 2012CERN, the European laboratory for particle physics, announced the detection of a particle consistent with the Higgs boson.Nuclear Physics is the field of physics that studies the constituents and interactions of atomic nuclei. The most commonly known applications of nuclear physics are nuclear power generation and nuclear weapons technology, but the research has provided application in many fields, including those in nuclear medicine and magnetic resonance imaging, ion implantation in materials engineering, and radiocarbon dating in geology and archaeology.University PhysicsAstrophysics and Physical CosmologyAstrophysics and astronomy are the application of the theories and methods of physics to the study of stellar structure, stellar evolution, the origin of the solar system, and related problems of cosmology. Because astrophysics is a broad subject, astrophysicists typically apply many disciplines of physics, including mechanics, electromagnetism, statistical mechanics, thermodynamics, quantum mechanics, relativity, nuclear and particle physics, and atomic and molecular physics.The discovery by Karl Jansky in 1931 that radio signals were emitted by celestial bodies initiated the science of radio astronomy. Most recently, the frontiers of astronomy have been expanded by space exploration. Perturbations and interference from the earth's atmosphere make space-based observations necessary for infrared, ultraviolet, gamma-ray, and X-ray astronomy.Physical cosmology is the study of the formation and evolution of the universe on its largest scales. Albert Einstein's theory of relativity plays a central role in all modern cosmological theories. In the early 20th century, Hubble's discovery that the universe was expanding, as shown by the Hubble diagram, prompted rival explanations known as the steady state universe and the Big Bang.The Big Bang was confirmed by the success of Big Bang nucleo-synthesis and the discovery of the cosmic microwave background in 1964. The Big Bang model rests on two theoretical pillars: Albert Einstein's general relativity and the cosmological principle (On a sufficiently large scale, the properties of the Universe are the same for all observers). Cosmologists have recently established the ΛCDM model (the standard model of Big Bang cosmology) of the evolution of the universe, which includes cosmic inflation, dark energy and dark matter.Current research frontiersIn condensed matter physics, an important unsolved theoretical problem is that of high-temperature superconductivity. Many condensed matter experiments are aiming to fabricate workable spintronics and quantum computers.In particle physics, the first pieces of experimental evidence for physics beyond the Standard Model have begun to appear. Foremost among these are indications that neutrinos have non-zero mass. These experimental results appear to have solved the long-standing solar neutrino problem, and the physics of massive neutrinos remains an area of active theoretical and experimental research. Particle accelerators have begun probing energy scales in the TeV range, in which experimentalists are hoping to find evidence for the super-symmetric particles, after discovery of the Higgs boson.Theoretical attempts to unify quantum mechanics and general relativity into a single theory1 Physics 物理学of quantum gravity, a program ongoing for over half a century, have not yet been decisively resolved. The current leading candidates are M-theory, superstring theory and loop quantum gravity.Many astronomical and cosmological phenomena have yet to be satisfactorily explained, including the existence of ultra-high energy cosmic rays, the baryon asymmetry, the acceleration of the universe and the anomalous rotation rates of galaxies.Although much progress has been made in high-energy, quantum, and astronomical physics, many everyday phenomena involving complexity, chaos, or turbulence are still poorly understood. Complex problems that seem like they could be solved by a clever application of dynamics and mechanics remain unsolved; examples include the formation of sand-piles, nodes in trickling water, the shape of water droplets, mechanisms of surface tension catastrophes, and self-sorting in shaken heterogeneous collections.These complex phenomena have received growing attention since the 1970s for several reasons, including the availability of modern mathematical methods and computers, which enabled complex systems to be modeled in new ways. Complex physics has become part of increasingly interdisciplinary research, as exemplified by the study of turbulence in aerodynamics and the observation of pattern formation in biological systems.Vocabulary★natural science 自然科学academic disciplines 学科astronomy 天文学in their own right 凭他们本身的实力intersects相交,交叉interdisciplinary交叉学科的,跨学科的★quantum 量子的theoretical breakthroughs 理论突破★electromagnetism 电磁学dramatically显著地★thermodynamics热力学★calculus微积分validity★classical mechanics 经典力学chaos 混沌literate 学者★quantum mechanics量子力学★thermodynamics and statistical mechanics热力学与统计物理★special relativity狭义相对论is concerned with 关注,讨论,考虑acoustics 声学★optics 光学statics静力学at rest 静息kinematics运动学★dynamics动力学ultrasonics超声学manipulation 操作,处理,使用University Physicsinfrared红外ultraviolet紫外radiation辐射reflection 反射refraction 折射★interference 干涉★diffraction 衍射dispersion散射★polarization 极化,偏振internal energy 内能Electricity电性Magnetism 磁性intimate 亲密的induces 诱导,感应scale尺度★elementary particles基本粒子★high-energy physics 高能物理particle accelerators 粒子加速器valid 有效的,正当的★discrete离散的continuous 连续的complementary 互补的★frame of reference 参照系★the special theory of relativity 狭义相对论★general theory of relativity 广义相对论gravitation 重力,万有引力explicit 详细的,清楚的★quantum field theory 量子场论★condensed matter physics凝聚态物理astrophysics天体物理geophysics地球物理Universalist博学多才者★Macroscopic宏观Exotic奇异的★Superconducting 超导Ferromagnetic铁磁质Antiferromagnetic 反铁磁质★Spin自旋Lattice 晶格,点阵,网格★Society社会,学会★microscopic微观的hyperfine splitting超精细分裂fission分裂,裂变fusion熔合,聚变constituents成分,组分accelerators加速器detectors 检测器★quarks夸克lepton 轻子gauge bosons规范玻色子gluons胶子★Higgs boson希格斯玻色子CERN欧洲核子研究中心★Magnetic Resonance Imaging磁共振成像,核磁共振ion implantation 离子注入radiocarbon dating放射性碳年代测定法geology地质学archaeology考古学stellar 恒星cosmology宇宙论celestial bodies 天体Hubble diagram 哈勃图Rival竞争的★Big Bang大爆炸nucleo-synthesis核聚合,核合成pillar支柱cosmological principle宇宙学原理ΛCDM modelΛ-冷暗物质模型cosmic inflation宇宙膨胀1 Physics 物理学fabricate制造,建造spintronics自旋电子元件,自旋电子学★neutrinos 中微子superstring 超弦baryon重子turbulence湍流,扰动,骚动catastrophes突变,灾变,灾难heterogeneous collections异质性集合pattern formation模式形成University Physics2 Classical mechanics 经典力学IntroductionIn physics, classical mechanics is one of the two major sub-fields of mechanics, which is concerned with the set of physical laws describing the motion of bodies under the action of a system of forces. The study of the motion of bodies is an ancient one, making classical mechanics one of the oldest and largest subjects in science, engineering and technology.Classical mechanics describes the motion of macroscopic objects, from projectiles to parts of machinery, as well as astronomical objects, such as spacecraft, planets, stars, and galaxies. Besides this, many specializations within the subject deal with gases, liquids, solids, and other specific sub-topics.Classical mechanics provides extremely accurate results as long as the domain of study is restricted to large objects and the speeds involved do not approach the speed of light. When the objects being dealt with become sufficiently small, it becomes necessary to introduce the other major sub-field of mechanics, quantum mechanics, which reconciles the macroscopic laws of physics with the atomic nature of matter and handles the wave–particle duality of atoms and molecules. In the case of high velocity objects approaching the speed of light, classical mechanics is enhanced by special relativity. General relativity unifies special relativity with Newton's law of universal gravitation, allowing physicists to handle gravitation at a deeper level.The initial stage in the development of classical mechanics is often referred to as Newtonian mechanics, and is associated with the physical concepts employed by and the mathematical methods invented by Newton himself, in parallel with Leibniz【莱布尼兹】, and others.Later, more abstract and general methods were developed, leading to reformulations of classical mechanics known as Lagrangian mechanics and Hamiltonian mechanics. These advances were largely made in the 18th and 19th centuries, and they extend substantially beyond Newton's work, particularly through their use of analytical mechanics. Ultimately, the mathematics developed for these were central to the creation of quantum mechanics.Description of classical mechanicsThe following introduces the basic concepts of classical mechanics. For simplicity, it often2 Classical mechanics 经典力学models real-world objects as point particles, objects with negligible size. The motion of a point particle is characterized by a small number of parameters: its position, mass, and the forces applied to it.In reality, the kind of objects that classical mechanics can describe always have a non-zero size. (The physics of very small particles, such as the electron, is more accurately described by quantum mechanics). Objects with non-zero size have more complicated behavior than hypothetical point particles, because of the additional degrees of freedom—for example, a baseball can spin while it is moving. However, the results for point particles can be used to study such objects by treating them as composite objects, made up of a large number of interacting point particles. The center of mass of a composite object behaves like a point particle.Classical mechanics uses common-sense notions of how matter and forces exist and interact. It assumes that matter and energy have definite, knowable attributes such as where an object is in space and its speed. It also assumes that objects may be directly influenced only by their immediate surroundings, known as the principle of locality.In quantum mechanics objects may have unknowable position or velocity, or instantaneously interact with other objects at a distance.Position and its derivativesThe position of a point particle is defined with respect to an arbitrary fixed reference point, O, in space, usually accompanied by a coordinate system, with the reference point located at the origin of the coordinate system. It is defined as the vector r from O to the particle.In general, the point particle need not be stationary relative to O, so r is a function of t, the time elapsed since an arbitrary initial time.In pre-Einstein relativity (known as Galilean relativity), time is considered an absolute, i.e., the time interval between any given pair of events is the same for all observers. In addition to relying on absolute time, classical mechanics assumes Euclidean geometry for the structure of space.Velocity and speedThe velocity, or the rate of change of position with time, is defined as the derivative of the position with respect to time. In classical mechanics, velocities are directly additive and subtractive as vector quantities; they must be dealt with using vector analysis.When both objects are moving in the same direction, the difference can be given in terms of speed only by ignoring direction.University PhysicsAccelerationThe acceleration , or rate of change of velocity, is the derivative of the velocity with respect to time (the second derivative of the position with respect to time).Acceleration can arise from a change with time of the magnitude of the velocity or of the direction of the velocity or both . If only the magnitude v of the velocity decreases, this is sometimes referred to as deceleration , but generally any change in the velocity with time, including deceleration, is simply referred to as acceleration.Inertial frames of referenceWhile the position and velocity and acceleration of a particle can be referred to any observer in any state of motion, classical mechanics assumes the existence of a special family of reference frames in terms of which the mechanical laws of nature take a comparatively simple form. These special reference frames are called inertial frames .An inertial frame is such that when an object without any force interactions (an idealized situation) is viewed from it, it appears either to be at rest or in a state of uniform motion in a straight line. This is the fundamental definition of an inertial frame. They are characterized by the requirement that all forces entering the observer's physical laws originate in identifiable sources (charges, gravitational bodies, and so forth).A non-inertial reference frame is one accelerating with respect to an inertial one, and in such a non-inertial frame a particle is subject to acceleration by fictitious forces that enter the equations of motion solely as a result of its accelerated motion, and do not originate in identifiable sources. These fictitious forces are in addition to the real forces recognized in an inertial frame.A key concept of inertial frames is the method for identifying them. For practical purposes, reference frames that are un-accelerated with respect to the distant stars are regarded as good approximations to inertial frames.Forces; Newton's second lawNewton was the first to mathematically express the relationship between force and momentum . Some physicists interpret Newton's second law of motion as a definition of force and mass, while others consider it a fundamental postulate, a law of nature. Either interpretation has the same mathematical consequences, historically known as "Newton's Second Law":a m t v m t p F ===d )(d d dThe quantity m v is called the (canonical ) momentum . The net force on a particle is thus equal to rate of change of momentum of the particle with time.So long as the force acting on a particle is known, Newton's second law is sufficient to。

核磁共振中常用的英文缩写和中文称号[整理版]

核磁共振中常用的英文缩写和中文称号[整理版]

NMR中常用的英文缩写和中文名称收集了一些NMR中常用的英文缩写,译出其中文名称,供初学者参考,不妥之处请指出,也请继续添加.相关附件NMR中常用的英文缩写和中文名称APT Attached Proton Test 质子连接实验ASIS Aromatic Solvent Induced Shift 芳香溶剂诱导位移BBDR Broad Band Double Resonance 宽带双共振BIRD Bilinear Rotation Decoupling 双线性旋转去偶(脉冲)COLOC Correlated Spectroscopy for Long Range Coupling 远程偶合相关谱COSY( Homonuclear chemical shift ) COrrelation SpectroscopY(同核化学位移)相关谱CP Cross Polarization 交叉极化CP/MAS Cross Polarization / Magic Angle Spinning 交叉极化魔角自旋CSA Chemical Shift Anisotropy 化学位移各向异性CSCM Chemical Shift Correlation Map 化学位移相关图CW continuous wave 连续波DD Dipole-Dipole 偶极-偶极DECSY Double-quantum Echo Correlated Spectroscopy 双量子回波相关谱DEPT Distortionless Enhancement by Polarization Transfer 无畸变极化转移增强2DFTS two Dimensional FT Spectroscopy 二维傅立叶变换谱DNMR Dynamic NMR 动态NMRDNP Dynamic Nuclear Polarization 动态核极化DQ(C) Double Quantum (Coherence) 双量子(相干)DQD Digital Quadrature Detection 数字正交检测DQF Double Quantum Filter 双量子滤波DQF-COSY Double Quantum Filtered COSY双量子滤波COSYDRDS Double Resonance Difference Spectroscopy 双共振差谱EXSY Exchange Spectroscopy 交换谱FFT Fast Fourier Transformation 快速傅立叶变换FID Free Induction Decay 自由诱导衰减H,C-COSY1H,13C chemical-shift COrrelation SpectroscopY 1H,13C化学位移相关谱H,X-COSY1H,X-nucleus chemical-shift COrrelation SpectroscopY1H,X-核化学位移相关谱HETCOR Heteronuclear Correlation Spectroscopy 异核相关谱HMBC Heteronuclear Multiple-Bond Correlation 异核多键相关HMQC Heteronuclear Multiple Quantum Coherence异核多量子相干HOESY Heteronuclear Overhauser Effect Spectroscopy 异核Overhause效应谱HOHAHA Homonuclear Hartmann-Hahn spectroscopy 同核Hartmann-Hahn谱HR High Resolution 高分辨HSQC Heteronuclear Single Quantum Coherence 异核单量子相干INADEQUA TE Incredible Natural Abundance Double Quantum Transfer Experiment 稀核双量子转移实验(简称双量子实验,或双量子谱)INDOR Internuclear Double Resonance 核间双共振INEPT Insensitive Nuclei Enhanced by Polarization 非灵敏核极化转移增强INVERSE H,X correlation via 1H detection 检测1H的H,X核相关IR Inversion-Recovery 反(翻)转回复JRES J-resolved spectroscopy J-分解谱LIS Lanthanide (chemical shift reagent ) Induced Shift 镧系(化学位移试剂)诱导位移LSR Lanthanide Shift Reagent 镧系位移试剂MAS Magic-Angle Spinning 魔角自旋MQ(C) Multiple-Quantum ( Coherence ) 多量子(相干)MQF Multiple-Quantum Filter 多量子滤波MQMAS Multiple-Quantum Magic-Angle Spinning 多量子魔角自旋MQS Multi Quantum Spectroscopy 多量子谱NMR Nuclear Magnetic Resonance 核磁共振NOE Nuclear Overhauser Effect 核Overhauser效应(NOE)NOESY Nuclear Overhauser Effect Spectroscopy 二维NOE谱NQR Nuclear Quadrupole Resonance 核四极共振PFG Pulsed Gradient Field 脉冲梯度场PGSE Pulsed Gradient Spin Echo 脉冲梯度自旋回波PRFT Partially Relaxed Fourier Transform 部分弛豫傅立叶变换PSD Phase-sensitive Detection 相敏检测PW Pulse Width 脉宽RCT Relayed Coherence Transfer 接力相干转移RECSY Multistep Relayed Coherence Spectroscopy 多步接力相干谱REDOR Rotational Echo Double Resonance 旋转回波双共振RELAY Relayed Correlation Spectroscopy 接力相关谱RF Radio Frequency 射频ROESY Rotating Frame Overhauser Effect Spectroscopy 旋转坐标系NOE谱ROTO ROESY-TOCSY Relay ROESY-TOCSY接力谱SC Scalar Coupling 标量偶合SDDS Spin Decoupling Difference Spectroscopy 自旋去偶差谱SE Spin Echo 自旋回波SECSY Spin-Echo Correlated Spectroscopy自旋回波相关谱SEDOR Spin Echo Double Resonance 自旋回波双共振SEFT Spin-Echo Fourier Transform Spectroscopy (with J modulation) (J-调制)自旋回波傅立叶变换谱SELINCOR Selective Inverse Correlation 选择性反相关SELINQUA TE Selective INADEQUA TE 选择性双量子(实验)SFORD Single Frequency Off-Resonance Decoupling 单频偏共振去偶SNR or S/N Signal-to-noise Ratio 信/ 燥比SQF Single-Quantum Filter 单量子滤波SR Saturation-Recovery 饱和恢复TCF Time Correlation Function 时间相关涵数TOCSY Total Correlation Spectroscopy 全(总)相关谱TORO TOCSY-ROESY Relay TOCSY-ROESY接力TQF Triple-Quantum Filter 三量子滤波WALTZ-16 A broadband decoupling sequence 宽带去偶序列WA TERGA TE Water suppression pulse sequence 水峰压制脉冲序列WEFT Water Eliminated Fourier Transform 水峰消除傅立叶变换ZQ(C) Zero-Quantum (Coherence) 零量子相干ZQF Zero-Quantum Filter 零量子滤波T1 Longitudinal (spin-lattice) relaxation time for MZ 纵向(自旋-晶格)弛豫时间T2 Transverse (spin-spin) relaxation time for Mxy 横向(自旋-自旋)弛豫时间tm mixing time 混合时间τ c rotational correlation time 旋转相关时间。

Thermoelectric transport through a quantum dot coupled to a normal metal and BCS supercondu

Thermoelectric transport through a quantum dot coupled to a normal metal and BCS supercondu

a r X i v :0803.28v1[c ond-ma t.m es-hall]3Mar28Thermoelectric transport through a quantum dot coupled to a normal metal and BCS superconductor Mariusz Krawiec Institute of Physics,M.Curie-Sk l odowska University,pl.M.Curie-Sk l odowskiej 1,20-031Lublin,Poland I discuss thermoelectric properties of a quantum dot coupled to one nor-mal and one superconducting lead in the presence of Kondo effect and An-dreev scattering.I will focus on conductance,thermal conductance,ther-mopower and related quantities like thermoelectric figure of merit which is a direct measure of the usefulness of the system for applications and Wiedemann-Franz ratio which indicates if the system is in the Fermi liquid state.I will show that the superconductivity strongly modifies the ther-mal properties of the system.In particular,the thermopower is strongly enhanced near the superconducting transition temperature.Moreover,the Andreev reflections are suppressed due to strong on-dot Coulomb repul-sion.The suppression of the Andreev reflections leads to a violation of the Wiedemann-Franz law and to a non-Fermi liquid ground state.PACS numbers:73.63.Kv,73.23.-b,73.50.Lw,72.15.Qm,74.45.+c 1.Introduction Quantum dot (QD)devices provide a unique opportunity to study the interplay between different basic quantum phenomena.A prime example is the interaction of a localized spin (magnetic impurity)with surrounding itinerant electron spins [1].This,known as Kondo effect,manifests itself asa quasiparticle resonance in local density of states at the Fermi level at low temperatures.In quantum dots coupled to normal electrodes,it leads to an increase of conductance at zero source-drain voltage.Originally,the Kondo effect in quantum dots was predicted theoretically in the late 1980s [2]-[4]and later demonstrated in a number of experiments [5]-[12].Experiments have confirmed the validity of the theoretical picture but also discovered new phenomena.Those include observation of the Kondo resonance at non-zero source-drain voltage [7,8],absence of even-odd parity effects expected for these systems [9],observation of singlet-triplet transition(1)2nsqdtherm printed on March3,2008in magneticfield[10],splitting of the Kondo resonance due to the ferromag-netism in the leads[11]or interplay between magnetism(Kondo effect)and superconductivity in carbon nanotube quantum dots[12,13].When the quantum dot is connected to superconducting electrodes(S-QD-S),the low energy transport is mediated by the Andreev reflections,ac-cording to which an electron impinging on a normal metal-superconductor interface is reflected back as a hole and the Cooper pair is created in the superconductor[14].This mechanism is known to play a crucial role in var-ious hybrid mesoscopic superconducting devices[15].In the S-QD-S system the Andreev transport is strongly affected by the Kondo effect,leading to the sign change of Josephson current[16,17].The strong Coulomb inter-action prevents the tunneling of Cooper pairs into QD,and the electrons tunnel via virtual processes.Thus the electron transport is strongly sup-pressed.This argument is valid when the Kondo temperature T K is smaller than the superconducting order parameter∆.On the other hand,when T K>∆,the Kondo effect is restored[18].This picture has been confirmed experimentally in carbon nanotube QD[12].In the present work I consider a slightly different setup with a quantum dot coupled to one normal and one superconducting electrode(N-QD-S). This system has extensively been studied both theoretically[19]-[31]and experimentally[32].Early theoretical works have predicted the enhance-ment of the conductance due to the Andreev reflections[21,20],while the others have predicted the suppression of it[19,22,23,26].Later on,it has been shown that the behavior of the Andreev conductance depends on the model parameters and can be enhanced or suppressed[23].The exper-iment by Graber et al.[32]shows that the conductance of N-QD-S system is suppressed in the Kondo regime.The investigations of the N-QD-S systems have focused on electron transport only,and there is no study of thermoelectric properties.However, as is well known,the thermoelectric properties are the source of additional information to that obtained from other transport characteristics.Thermal properties(thermopower and thermal conductance)of strongly interacting quantum dot coupled to the normal and ferromagnetic leads have recently been investigated showing that thermopower is very sensitive and powerful tool to study the Kondo effect[33]-[39].It is the purpose of the present work to study the thermoelectric prop-erties of the quantum dot coupled to one normal and one superconducting electrode.I will focus on the electric and thermal conductance,thermopower and related quantities like thermoelectricfigure of merit which is a direct measure of the usefulness of the system for applications and Wiedemann-Franz ratio which indicates if the system is in the Fermi liquid state.I will show that the superconductivity strongly modifies the thermal properties ofnsqdtherm printed on March3,20083 the system leading to an increase of thermopower at low temperatures and to non-Fermi liquid ground state.Rest of the paper is organized as follows.In Sec.2I present the model and briefly discuss the approach.Results of calculations are presented and discussed in Sec.3.Summary and conclusions are given in Sec.4.2.Formulation of the problemThe system is described by single impurity Anderson model with very strong on-dot Coulomb repulsion(U→∞).In this limit there might be at most a single electron on the dot.To project out double occupied states it is convenient to introduce slave boson representation[40,41],in which the real dot electron operator dσis replaced by the product of boson b and fermion fσoperators(dσ=b+fσ)subject to the constraint b+b+ σf+σfσ=1.The resulting Hamiltonian readsH= λkσǫλk c+λkσcλkσ+ k ∆c+S k↑c+S−k↓+H.c.+εd σf+σfσ+ λkσ Vλk c+λkσb+fσ+H.c. ,(1)whereλ=N(S)denotes normal(superconducting)electrode,c+λkσ(cλkσ) is the creation(annihilation)operator for a conducting electron with the wave vector k,spinσin the leadλ,and Vλk is the hybridization parameter between localized electron on the dot with energyεd and conducting electron of energyǫλk in the leadλ.∆is the superconducting order parameter in the lead S,and its temperature dependence is chosen in the form:∆(T)=∆0dωT sp(ω)[f(ω−eV)−f(ω)]he+dωT sp(ω)(ω−eV)[f(ω−eV)−f(ω)]h1+4nsqdtherm printed on March3,2008Fermi distribution function,and eV=µN−µS.T sp(ω)and T A(ω)are the transmittances associated with single particle tunneling and with Andreevreflections,respectively.Theexplicit form of T sp(A)(ω)and the details ofcalculations can be found in Ref.[26].In the linear regime,i.e.for small voltages eV→0and small tem-perature gradientsδT=T N−T S→0,one defines the electric conduc-tance G=−e2eTL12T2 L22−L212hdωT tot(ω) ∂f(ω)hdωT tot(ω) ∂f(ω)hdωT tot(ω)(ω−eV) ∂f(ω)3.52).The reason for such a behavior istwofold.First,at T=0the single particle transport is completely blocked due to the lack of the electron states in superconducting electrode for ener-gies smaller than∆.Thus the only contribution to electric transport comes from the Andreev reflections.Note that the Andreev reflections do not con-tribute to the thermal transport(at T=0),as the electron in converted into hole,and thus there is no energy transfer through the interface.At the same time the Andreev scattering is only the mechanism which gives rise to electron transport(the charge of2e is transferred through the interface). However,strong Coulomb interactions on the dot prevent the tunneling of Cooper pairs into QD,and the electrons in each pair can only tunnel one by one via virtual processes[19,22,23,26].As a result,the Andreev tunnelingnsqdtherm printed on March 3,20085 0.0 0.20.40.60.810 -310 -210 -110 010 1G [e 2/h ]T/Γ∆ =0.000.010.101.00 0.0 0.10.2 0.310 -310 -210 -110 010 1κ/Γ [1/h ]T/Γ∆ =0.000.010.101.00Fig.1.Temperature dependence of electric (left panel)and thermal conductance (right panel)for various values of superconducting order parameter.The dot energy level εd =−1.75Γ,and the Kondo temperature T K (∆=0)=2·10−2Γ.-3-2-112310 -310 -210 -110 010 1S [1/e ]T/Γ∆ =0.000.010.101.00Fig.2.Linear thermopower S as a function of temperature for various values of superconducting order parameter ∆.is strongly suppressed.This is the second reason for such suppression of the electric conductance.Corresponding linear thermopower S is shown in Fig.2.This quantity is very useful measure of the Kondo correlations [33]-[39].At high temper-atures thermopower is positive indicating hole-like transport and at T ≈Γshows a broad maximum associated with single particle excitations.At low T ,where the transport is electron-like,the thermopower is negative.In the case of normal leads,the thermopower changes sign at the Kondo tempera-ture T K (solid line in Fig.2).The sign change can be also understood from the fact that S is sensitive to the slope of the density of states (DOS)at the Fermi level.With lowering of temperature,the Kondo correlations lead to the development of a narrow resonance in the DOS slightly above the Fermi energy,and thus to a slope change at the E F .In the presence of supercon-6nsqdtherm printed on March 3,2008ductivity in one of the leads,S changes sign at superconducting transition temperature T c ,rather than at the Kondo temperature.The sign change of S and its behavior near T c is associated with the shape of superconducting DOS,which is reflected in QD density of states.Figure 3(left panel)shows the temperature dependence of the Wiedemann-Franz (WF)law which relates thermal and electric conductance via the re-lation 3e 2/π2(κ/T G )=1.This relation describes transport in Fermi liquid0 3691210 -310 -210 -110 010 13κ/π2T G T/Γ∆ =0.000.010.101.00 0.0 0.2 0.4 0.6 0.810 -310 -210 -110 010 1Z T T/Γ∆ =0.000.010.101.00Fig.3.The Wiedemann-Franz ratio 3e 2/π2(κ/T G )(left panel)and thermoelectric figure of merit ZT =S 2GT/κ(right panel)as a function of temperature T .bulk metals,and usually is violated in nanoscale systems.However,below the Kondo temperature,the WF law is recovered,and the system has the Fermi liquid ground state [33,37,39].In the high temperature regime,the WF law is violated as the transport is due to sequential processes leading to the suppression of the thermal transport [37].This picture is valid for QD coupled to normal or to ferromagnetic electrodes.In the presence of super-conductivity,this law is violated even at low temperatures (see left panel of Fig.3),indicating non-Fermi liquid ground state of the system.However,the superconductivity in one of the electrodes alone is not enough to violate the WF law.There must be strong Coulomb repulsion between electrons on the dot.In non-interacting QD (U =0)the WF law is still obeyed at low T .The violation of the WF law in strongly interacting QD has its origin in suppression of the Andreev reflections,leading to smaller values of the linear conductance G in comparison to non-interacting QD.At the same time,the Andreev reflections do not contribute to thermal transport,thus the thermal conductance remains unchanged.This explains the violation of the WF law in strongly interacting N-QD-S system.Thermoelectric figure of merit Z =S 2G/κis a direct measure of the usefulness of the system for applications.For simple systems Z is inversely proportional to operating temperature,therefore it is convenient to plot ZT .The right panel of Fig.3shows ZT as a function of temperature.nsqdtherm printed on March3,20087 The value of ZT never exceeds1,which indicates limited applicability of the system for thermoelectric power generators or cooling systems.Note the enhancement of ZT in superconducting state,which is due to the larger values of thermopower in this temperature range(see Fig.2).4.Summary and conclusionsIn summary,I have studied thermal properties of strongly correlated quantum dot coupled to one normal and one superconducting electrode. The superconductivity strongly modifies thermal properties of the system. In particular is responsible for an enhancement of thermopower at tempera-tures close to the superconducting transition temperature.The suppression of Andreev reflections,which is due to strong on-dot Coulomb repulsion, leads to a violation of the Wiedemann-Franz relation and to non-Fermi liq-uid ground state.AcknowledgmentsThis work has been supported by the Grant No N N202146833of the Polish Ministry of Education and Science.REFERENCES[1]A.C.Hewson,The Kondo Problem to Heavy Fermions,Cambridge University Press,Cambridge(1993).[2]L.I.Glazman,M.E.Raikh,JETP Lett.47,452(1988).[3]T.K.Ng,P.A.Lee,Phys.Rev.Lett.61,1768(1988).[4]A.Kawabata,J.Phys.Soc.Japan60,3222(1991).[5]D.Goldhaber-Gordon,H.Shtrikman, D.Mahalu, D.Abusch-Magder,U. 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Michael R. Geller1 and Andrew N. Cleland2 1Department of Physics and Astronomy, University of Georgia, Athens, Georgia 30602-2451 2Department of Physics and iQUEST, University of California, Santa Barbara, California 93106
arXiv:quant-ph/0409179v1 26 Sep 2004
Superconducting qubits coupled to nanoelectromechanical resonators: An architecture for solid-state quantum information processing
tal accomplishments have followed,9,10,11,12,13,14,15,16 each “atom”, and control the “electromagnetic” interac-
including the impressive demonstration of controlled- tion strength. This analogy makes it clear that our design
(Dated: September 25, 2004)
We describe the design for a scalable, solid-state quantum-information-processing architecture based on the integration of GHz-frequency nanomechanical resonators with Josephson tunnel junctions, which has the potential for demonstrating a variety of single- and multi-qubit operations critical to quantum computation. The computational qubits are eigenstates of large-area, currentbiased Josephson junctions, manipulated and measured using strobed external circuitry. Two or more of these phase qubits are capacitively coupled to a high-quality-factor piezoelectric nanoelectromechanical disk resonator, which forms the backbone of our architecture, and which enables coherent coupling of the qubits. The integrated system is analogous to one or more few-level atoms (the Josephson junction qubits) in an electromagnetic cavity (the nanomechanical resonator). However, unlike existing approaches using atoms in electromagnetic cavities, here we can individually tune the level spacing of the “atoms” and control their “electromagnetic” interaction strength. We show theoretically that quantum states prepared in a Josephson junction can be passed to the nanomechanical resonator and stored there, and then can be passed back to the original junction or transferred to another with high fidelity. The resonator can also be used to produce maximally entangled Bell states between a pair of Josephson junctions. Many such junction-resonator complexes can assembled in a hub-and-spoke layout, resulting in a large-scale quantum circuit. Our proposed architecture combines desirable features of both solid-state and cavity quantum electrodynamics approaches, and could make quantum information processing possible in a scalable, solid-state environment.
NOT logic with charge qubits,12 and a large body of is sufficiently flexible to be able to carry out essentially
theoretical work is beginning to address these and related any operation that can be done using other architectures,
perform many logical operations during the available cavities,15,27,28,29 or other types of oscillators,30,31,32 to coherence lifetime.52 Here ∆E is the qubit energy-level couple JJs together. We note that although harmonic os-
PACS numbers: 03.67.Lx, 85.25.Cp, 85.85.+j
I. INTRODUCTION
gesting that GHz-frequency nanoelectromechanical res-
onators can be used to coherently couple two or more
and measured using the external circuitry developed by Martinis et al.3 These superconducting phase qubits are
given that they exhibit robust macroscopic quantum capacitively coupled to a high-quality-factor piezoelectric
interest in the potential for superconductor–based in an electromagnetic cavity (the resonator). However,
quantum computation.7,8 Several additional experimen- here we can individually tune the energy level spacing of
and of both Rabi oscillations and Ramsey fringes in our architecture. We shall show that the integrated sys-
a Cooper-pair box,4,5,6 have generated significant new tem is analogous to one or more few-level atoms (the JJs)
behavior.1 Demonstrations of long-lived Rabi oscilla- dilatational disk resonator, cooled on a dilution refriger-
tions in current-biased Josephson tunnel junctions,2,3 ator to the quantum limit, which forms the backbone of
coherent quality factors Qϕ ≡ τϕ ∆E/ of the order of 105, indicating that these systems should be able to
Several investigators have proposed the use of LC resonators,17,18,19,20,21,22,23,24,25,26 superconducting
to make a flexible and scalable solid-state quantuminformation-processing architecture.51 The computa-
their entanglement, remains the principal roadblock to tional qubits are taken to be the energy eigenstates of
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