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11月8日托福阅读真题

11月8日托福阅读真题

新东方谢真真:2014年11月08日托福阅读真题智课网整理第一套题第一篇:版本一:生命组成元素elements有很多,主要有氢和氦,还说了一些惰性元素,虽然不同星球元素比例不同但是所须具备的元素都有。

生命必须存在于有atmosphere和liquid的星球,两个条件同时满足,因为atmosphere可以防止辐射,liquid可以让元素之间反应从而形成organic的分子版本二:生命组成元素,element有九十多种,life element包括25种;然后讲了一下heavy element和氢、氦占元素的百分比,古老星球的heavy element百分比很低;地球生物最重要的元素是碳,其他星球具有生命所需的元素,所以可能有生命存在,并且可以based on 碳或者硅或者其他元素;atmosphere和liquid必须存在,有利于元素相互反应,形成生命。

词汇题不太记得了,貌似有一个widespread among第二篇:版本一:美国十九世纪lumber开始是农民卖,后来产业化,还说了technology促进了发展,有方法可以让开采全面进行而不是在冬天停滞,另外有方法解决冬天结冰导致木材搬运不同的问题,还说有铁路建设,尽管有些地方很偏远,但是由于对木材的持续需求建了版本二:讲美国五大湖地区的lumber,在十九世纪开始产业化,技术的发展使木材可以搬运到全国各地,stream水运木材,有一个啥技术可以控制水运的方向,使运输更快速;还有一个是在dry冬天,freeze减少摩擦力,解决冬天木材很难运的问题,可以运很重的木材了;另外就是铁路运输。

其他的细节就不太记得了第三篇:版本一:megafauna为什么灭绝说了一个主要的原因是人类活动,有两人还制作了模型检验,另外一个人支持这个观点,也有什么证据,说有remains在人类活动的地方,后来反驳,说few remains在那个地方,然后前面制作数学模型的人就说这反而能支持他们的观点,但是又有一个人说新西兰也有一个地方的什么动物,灭绝也是因为人类活动,但却留下很多evidence版本二:magafauna灭绝的问题,科学家提出是人类kill的,解释了一下为什么climate不会是灭绝的原因:很久之前有一次climate变化但没导致m灭绝,这次climate变化也不会导致灭绝。

博士入学考试英语中常见的翻译词汇 (1)

博士入学考试英语中常见的翻译词汇 (1)

百度文库 - 让每个人平等地提升自我!分类词汇homogeneous 同质的 homo + gene +ous(<> heterogeneous)^ homo***ual, hetero***ual mainstream 主流主流的dialect 方言 (v.s. accent)discrepancy 差异misconception 误解 (mis + concept + ion)= misunderstandingbarrier 障碍(物)~ bar, = barricadediscrimination 区别,歧视 racial/***ual discrimination? discriminate (+against)hierarchy 等级制度 heir + arch(govern) + yinsularity 岛国性质 (? insular, ^island)British industry has often been criticized for its linguistic insularity.microcosm 小天地 micro + cosm(os)nostalgia = homesicknesspatriot 爱国者 (<>traitor)à patriotic, patriotismnotoriety 恶名 (? notorious)counterpart 对应人,对等物Who’s George Bush’s counterpart in China?^ counterculture, counterbalancepeer 同等的人凝视,窥视(~ peep)subordinate 下级下级的<> superiortactics 战术,技巧 v.s. strategy (战略,策略)marketing strategy v.s. selling tacticsnuance a subtle difference in meaningcompatriot 同胞同胞的 com + patriotvernacular 本地的,本国的本地话,本国话 the vernacular languages of IndiaHispanic An American whose first language was Spanishimmigration 移入~ immigrant, immigratev.s. emigration (~ emigrant, emigrate)antipodes Any two places or regions on diametrically opposite sides of the Earth“from North America to the Antipodes”permeate 渗透,弥漫 Smoke permeated the house.entrepreneur 企业家(~ enterprise)à entrepreneurshippractitioner 开业者,从业者 praction(practice) + ercelebrity a famous person= luminary, VIPproxy 代理人anecdote 轶事(à anecdotal)benchmarking 类比分析punctual 准时的,守时的(à punctuality)absenteeism 旷工absent à absentee à absenteeismflextime 弹性工作时间 flex(flexible) + timeharass 骚扰(à harassment)Mary said that Gary had ***ually harassed her. redundancy 冗余,冗员 network redundancydownsize 裁员 (~ lay off)ballot 投票 (= vote)impartial 不偏不倚的 (<> partial)lobby 大堂(n.) 游说(v.)dubbing 配音录制1百度文库 - 让每个人平等地提升自我!vogue 时尚 ^ chicbizarre 奇异的 v.s. weird (怪异的)mediocre 平庸的dietitian 饮食学家 (~ diet)connoisseur 行家,鉴赏家^ entrée, a la carteshortlist (BE) a list of applicants who have been deemed suitable and from which the successful person will be chosen à (v.)equilibrium 平衡,均衡questionnaire 调查表,问卷quantitative 定量的 (<> qualitative)contingency 偶然性,偶然事件incur 招致 incur debts/hatred/dangerv.s. occur, concur, recurethical 伦理的,符合伦理的 ~ ethics, <> unethicaldubious 疑惑的,可疑的 (~ doubt)People were dubious about the result.manifestation 显示,证明 (? manifest)subtitle 字幕,副标题 (sub + title)^ subsidiary, submarine, subway (BE: underground, tube), suburb(~ downtown, uptown, outskirts考博英语翻译中可能涉及的热点词汇总裁助理 assistant president综合治理 comprehensive treatment安居工程 housing project for low-income urban residents信息化 information-based; informationization智力密集型 concentration of brain power; knowledge-intensive外资企业 overseas-funded enterprises下岗职工 laid-off workers分流 reposition of redundant personnel三角债 chain debts素质教育 education for all-round development豆腐渣工程 jerry-built projects社会治安情况 law-and-order situation民族国家 nation 台独"independence 台湾当局 Taiwan 台湾同胞 Taiwan stateof Taiwan" authorities compatriots台湾是中国领土不可分割的一部分。

专四专八词汇辨析

专四专八词汇辨析

专四专八必背一百组近义词辨析第一组:abide, adhere, conform, comply这四个研究生入学考试中的高频考词都有“遵守”的意思,但是它们的搭配不同。

abide v.后接by表示“遵守,同意”。

I will abide by the director' decision.我将遵从主任的决定。

adhere v.后接to表示“遵守”。

(当然adhere一词的其它意思如“坚持;粘附”也经常被考到。

)Car drivers must adhere to the rules of driving.汽车司机必须遵守驾驶规则。

conform v.后接to表示“遵守,符合”。

All individuals are required to conform to the laws made by their governments.每个人都应该遵守政府制订的法律。

comply v.后接with表示“遵守,服从”,用于正式的场合。

Our company complies with governmental regulations on payingtaxes.我们公司遵守政府有关纳税的规定。

第二组:abnormal, uncommon, disordered这三个单词都有“反常的”之意,在考研和CET-6当中经常让考生们辨析它们的细微差别。

abnormal a.不正常的,反常的(但并非罕见),指行为或现象(如气候)的异常。

His body temperature has been abnormal for 3 days, the highest point reaching 40.5 degreecentigrade.他的体温三天来一直都不正常,最高的时候达到40.5摄氏度。

(尽管身体发烧不正常,但生活中也时有发生。

)uncommon a.罕见的,不平常的,指很少经历或很少见到的状况;特别的,出色的。

翻译硕士考研词汇辨析总结

翻译硕士考研词汇辨析总结

翻译硕士考研词汇辨析总结apparent, evident, manifest, obvious, distinctapparent, evident, manifest, obvious, distinct这一组形容词都有“明显的”之意。

apparent a.明显的,显而易见的,尤其指容易观察到或认识到的事物。

He is very unhappy, and it is apparent that he wants to leave now.他很不高兴,显然他现在想走了。

evident a.明白的,明显的,与apparent基本同意,多用于推理或由事实证明的事物。

It is evident that he is guilty; his fingerprints were found at the crime scene.显然他是有罪的,在犯罪现场发现了他的指纹。

manifest a.清楚的,明显的,多指根据外部特征或迹象便能看出或了解其意义,常作表语。

Her ability is manifest, but she is not attractive.她才能出众,但长相并不动人。

obvious a.明显的,显而易见的,含有无可辩白,不需证明之意。

It is obvious that that woman has had too much to drink.很显然,那个妇女酒喝的太多了。

distinct a.清楚的,明显的;不同的,独特的。

修饰性质明显不同的东西。

Medical care has made a distinct improvement in his health.治疗已使他的健康有了明显的好转applaud, clap, commend, praiseapplaud, clap, commend, praise的区别applaud v.鼓掌,赞扬,指因精湛表演或某种行为得到别人的赞许,大声叫好或热烈鼓掌。

雅思Test 4 Passage 3 阅读译文

雅思Test 4 Passage 3 阅读译文

GENERICIDE商标退化(Latin gener-, stem of genus 'kind, origin' -cide = word-forming element meaning 'killer')A Occasionally a company's brand name becomes so deeply ingrained in the minds of everyday consumers that it enters the popular lexicon of its time and becomes a catch-all term for the generic product or activity in question. At first glance, this might appear to be the pinnacle of successful marketing. Indeed, companies around the world spend billions of dollars every year conjuring up catchy jingles, memorable catch phrases and cute characters in an effort to ensure their brand is the first to spring into consumers' minds when those consumers realise they require a particular product or service.在少数情况下,当一个公司的商标名字在日常消费者的脑中变得根深蒂固时,就会被收入词典,并由此成为未定的一类商品或活动的统称。

乍看我们会觉得这像是成功市场的顶峰。

国信ca注释

国信ca注释

国信ca注释The world is a vast canvas, filled with countless colors and shapes. Each culture, each nation, each individual contributes their unique hues and contours to this ever-evolving masterpiece. As we traverse this globe, we encounter diverse landscapes, rich histories, and fascinating traditions.世间犹如一幅宏大的画卷,充满了无数色彩与形状。

每一种文化、每一个国家、每一个个体,都为这幅不断演变的杰作贡献着独特的色彩与轮廓。

当我们踏遍全球时,会遇见各式各样的风景、丰富的历史和引人入胜的传统。

One such culture that has captivated the imagination of many is the ancient civilization of China. With a history spanning thousands of years, China has a rich tapestry of traditions and customs that have stood the test of time. The country's art, music, literature, and philosophy have all left a profound impact on the world.其中一种令许多人遐想联翩的文化便是中国古老的文明。

中国拥有数千年的历史,其丰富多样的传统和习俗经受住了时间的考验。

该国的艺术、音乐、文学和哲学都为世界留下了深远的影响。

关于实验是检验真理的唯一标准英语作文

关于实验是检验真理的唯一标准英语作文

关于实验是检验真理的唯一标准英语作文全文共3篇示例,供读者参考篇1Experiment: The Only Yardstick for Measuring TruthTruth, that elusive and coveted prize that humanity has chased after for millennia. We've constructed elaborate philosophies, devised ingenious thought experiments, and spent countless hours pondering and debating what constitutes truth and how to discern it from fiction. Yet, amid this intellectual odyssey, one approach has emerged as the undisputed champion, a beacon of light cutting through the fog of speculation and conjecture – the scientific experiment.As a student, I've been taught to revere the sanctity of the scientific method, to view it as the ultimate arbiter of truth in a world often clouded by biases, assumptions, and unfounded beliefs. Through rigorous experimentation, we can strip away the veneers of preconceived notions and subject our hypotheses to the unforgiving crucible of empirical evidence.The strength of the experiment lies in its objectivity and replicability. It transcends the limitations of individualperspectives, cultural biases, and ideological leanings, offering a universal language that any rational mind can comprehend. When conducted with precision and adherence to established protocols, an experiment becomes a testament to the pursuit of truth, a beacon guiding us through the labyrinth of uncertainty.Consider the countless breakthroughs and paradigm shifts that have reshaped our understanding of the world, from Galileo's revolutionary observations of the heavens to the groundbreaking experiments of Marie Curie that unveiled the mysteries of radioactivity. Each of these monumental discoveries was forged not in the realm of abstract theorizing but through meticulous experimentation, where hypotheses were put to the ultimate test, and nature itself was allowed to speak its truth.The beauty of the experiment lies in its ability to challenge our preconceptions and shatter long-held beliefs. It acts as a bulwark against the insidious influence of dogma, forcing us to confront reality head-on and embrace the uncomfortable truths that may contradict our cherished notions. The annals of science are replete with examples of experiments that have upended conventional wisdom, from the earth's revolution around the sun to the counterintuitive principles of quantum mechanics.Moreover, the experiment fosters a culture of intellectual humility, a recognition that our understanding of the universe is ever-evolving and subject to constant refinement. It reminds us that truth is not a static entity to be grasped once and for all but a dynamic pursuit, a journey of continuous exploration and discovery. Through experimentation, we acknowledge the limitations of our current knowledge and remain open to the possibility of revising our beliefs in the face of new evidence.Yet, the power of the experiment extends far beyond the realms of natural sciences. In the social sciences, carefully designed experiments have illuminated the intricate workings of human behavior, shedding light on topics as diverse as decision-making, social dynamics, and cognitive biases. By isolating and manipulating variables in controlled environments, researchers can tease apart the complex tapestry of human interactions, uncovering truths that would otherwise remain obscured by the noise of everyday life.Even in the abstract domains of mathematics and logic, the experiment plays a crucial role. Through the construction of formal systems and the derivation of theorems, mathematicians and logicians engage in a form of intellectual experimentation, subjecting their axioms and conjectures to the rigors of logicalscrutiny. The truth of a mathematical statement is not determined by mere assertion but by its ability to withstand the relentless probing of logical deduction and proof.Of course, the experiment is not without its limitations. It is a tool, and like any tool, it can be misused or misinterpreted. Flawed experimental designs, measurement errors, and selective reporting of results can lead us astray, obscuring the truth rather than revealing it. This is why the scientific community places such emphasis on rigorous peer review, replication studies, and a commitment to transparency and integrity in the experimental process.Furthermore, there are realms of inquiry where the experiment may not be applicable or practical, such as in the study of historical events or in the exploration of certain metaphysical and philosophical questions. In these domains, we must rely on other modes of inquiry, such as textual analysis, logical argumentation, and reasoned discourse, while maintaining a healthy skepticism and a willingness to revise our beliefs in the face of new evidence.Yet, despite these caveats, the experiment remains the gold standard for testing truth, a beacon that guides us through the murky waters of uncertainty and conjecture. It is a testament tothe human spirit's insatiable curiosity and our relentless pursuit of knowledge, a pursuit that has yielded countless wonders and revelations about the universe we inhabit.As a student, I have been indelibly shaped by this reverence for the experiment and the scientific method. It has instilled in me a deep appreciation for the power of evidence, a respect for the rigor of the scientific process, and a commitment to intellectual honesty. It has taught me to question assumptions, to embrace uncertainty, and to remain open to revising my beliefs in the face of compelling evidence.More importantly, the experiment has imbued me with a sense of wonder and awe at the grandeur of the universe and the boundless potential of human inquiry. Each time a hypothesis is tested, a new door is opened, revealing glimpses of truth that were previously obscured. It is a journey of endless discovery, where each answer begets a multitude of new questions, propelling us ever forward in our quest for understanding.In a world often beset by dogmatism, misinformation, and the allure of convenient fictions, the experiment stands as a beacon of hope, a reminder that truth is not a matter of opinion or belief but a pursuit rooted in evidence and reason. It is a call to embrace intellectual humility, to shed our preconceptions,and to fearlessly confront the unknown, armed with the tools of scientific inquiry and a steadfast commitment to uncovering the truths that lie beyond the veil of our limited perceptions.So, as I embark on my academic and professional journey, I carry with me this unwavering conviction: the experiment is not merely a tool for testing truth but a way of life, a embodiment of the human spirit's insatiable thirst for knowledge and understanding. It is a torch that illuminates the path forward, guiding us towards a future where truth reigns supreme, and the boundaries of our understanding are continually pushed ever outward, into the vast expanse of the unknown.篇2Experimentation: The Sole Criterion of Truth?As a student grappling with the complexities of epistemology – the study of knowledge and its acquisition – I find myself drawn to the notion that experimentation is the sole criterion of truth. This assertion challenges the traditional methods of acquiring knowledge and raises pertinent questions about the nature of truth itself. In this essay, I will delve into the merits and limitations of this stance, drawing upon philosophicalinsights and empirical evidence to present a comprehensive analysis.The proposition that experimentation is the sole arbiter of truth finds its roots in the empirical tradition, which emerged during the Scientific Revolution of the 16th and 17th centuries. Thinkers such as Francis Bacon and René Descartes advocated for a systematic and methodical approach to understanding the natural world, rejecting the authority of ancient texts and embracing the power of observation and experimentation.Proponents of this view assert that truth can only be established through controlled, replicable experiments that test hypotheses against empirical data. This approach places a premium on objectivity, rigorous methodology, and the ability to reproduce results. By subjecting our assumptions to the scrutiny of empirical inquiry, we can weed out unfounded beliefs and superstitions, allowing us to uncover the underlying principles that govern the universe.The success of the scientific method in unveiling the mysteries of the natural world lends credence to this perspective. Through experimentation, we have unraveled the intricacies of physics, chemistry, biology, and myriad other disciplines, enabling technological advancements that have transformed ourlives. The theories and laws derived from empirical investigations have withstood the test of time, serving as the bedrock of our understanding of the universe.Moreover, the reliance on experimentation fosters a spirit of skepticism and critical thinking, which are essential for the pursuit of truth. By constantly challenging our assumptions and subjecting them to empirical verification, we safeguard against the pitfalls of dogmatism and blind acceptance of authority. This approach encourages intellectual humility, as even the most well-established theories must be continuously scrutinized and refined in the face of new evidence.However, it would be remiss to adopt an unwavering stance on experimentation as the sole criterion of truth without acknowledging its limitations and the existence of other legitimate modes of inquiry. While experimentation excels in the realm of the natural sciences, it may fall short in addressing questions of ethics, aesthetics, and metaphysics, which often defy empirical verification.For instance, how can we experimentally determine the inherent value of human life or the moral implications of our actions? The realm of ethics and morality is rooted in philosophical reasoning, cultural traditions, and subjectiveexperiences, which may not lend themselves readily to experimental methodologies. Similarly, our appreciation of art and beauty, while grounded in neural and psychological processes, transcends mere empirical analysis and involves subjective interpretations shaped by individual experiences and cultural contexts.Furthermore, the pursuit of truth is not solely confined to the observable and measurable aspects of reality. Metaphysical inquiries into the nature of existence, consciousness, and the fundamental constituents of the universe often engage with realms that lie beyond the reach of direct experimentation. While empirical evidence can inform and constrain our metaphysical theories, the ultimate truths about the origin and essence of reality may elude the confines of the experimental method.It is also important to acknowledge the inherent limitations of experimentation itself. Despite our best efforts to maintain objectivity and rigor, our experiments are subject to the constraints of our current technological capabilities, theoretical frameworks, and human biases. The history of science is replete with instances where flawed experimental designs, faulty data analysis, or cognitive biases led to erroneous conclusions that were later overturned by more rigorous investigations.Moreover, the reductionist approach inherent in experimentation may fail to capture the holistic and emergent properties of complex systems, leading to an incomplete understanding of the phenomena under study. The interplay of multiple factors, non-linear dynamics, and the inherent unpredictability of certain systems may defy the controlled conditions and simplifying assumptions of experiments, necessitating the integration of alternative modes of inquiry.In light of these considerations, a more nuanced perspective emerges: while experimentation is an indispensable tool in our quest for truth, it should not be regarded as the sole criterion. Instead, we must embrace a pluralistic approach that recognizes the complementary roles of various modes of inquiry, each contributing to our understanding of the world in unique and invaluable ways.Philosophical reasoning, introspection, and subjective experiences offer insights into the realms of ethics, aesthetics, and consciousness, domains that may elude the grasp of empirical investigation. Cultural traditions and indigenous ways of knowing can provide alternative perspectives and enrich our understanding of the human experience. Mathematical and logical reasoning can unveil truths about abstract concepts andformal systems, transcending the boundaries of the physical world.Ultimately, the pursuit of truth is a multifaceted endeavor that requires a synthesis of diverse modes of inquiry, each illuminating different facets of reality. Experimentation remains a pivotal component of this pursuit, providing a rigorous and systematic method for testing hypotheses and uncovering the underlying principles that govern the natural world. However, it is not the sole criterion of truth, but rather a powerful tool that must be wielded in conjunction with other modes of inquiry to achieve a more comprehensive and holistic understanding of the world we inhabit.As students and seekers of knowledge, our task is to cultivate a spirit of intellectual humility, recognizing the limitations of any single approach while embracing the richness and diversity of human inquiry. By integrating the insights gleaned from experimentation with those derived from philosophical, cultural, and subjective modes of understanding, we can navigate the complexities of truth with greater wisdom and depth, ultimately enriching our collective knowledge and enhancing our ability to comprehend the mysteries that surround us.篇3Experiment as the Sole Criterion of TruthThe quest for truth and knowledge has been an enduring pursuit throughout human history. As we navigate the complexities of the natural world, we are confronted with numerous assertions, theories, and beliefs that compete for our acceptance. In this landscape, the question arises: How can we discern truth from falsehood? Is there a universal standard by which we can evaluate the validity of claims? Many philosophers and scientists have grappled with this fundamental inquiry, and one perspective that has gained significant traction is the notion that experiment is the sole criterion of truth.At first glance, this proposition may seem overly simplistic or even radical. After all, the realm of human knowledge encompasses a vast array of disciplines, from the abstract realms of mathematics and philosophy to the tangible domains of the natural sciences. How can a single standard encompass such diversity? However, upon closer examination, the argument for experiment as the ultimate arbiter of truth holds considerable weight.The essence of this perspective lies in the recognition that empirical evidence, derived from carefully controlled and replicable experiments, provides the most reliable foundation for establishing objective truth. Unlike mere speculation, anecdotal accounts, or subjective interpretations, experiments offer a systematic and rigorous approach to testing hypotheses and uncovering the fundamental principles that govern the universe.One of the strongest arguments in favor of this view is the remarkable success of the scientific method, which relies heavily on experimentation. Throughout history, countless discoveries and technological advancements have been made possible through the application of experimental techniques. From the groundbreaking work of pioneers like Galileo and Newton to the cutting-edge research in fields like particle physics and molecular biology, experiments have consistently yielded insights that have reshaped our understanding of the world.Moreover, the power of experimentation lies in its ability to challenge and refine existing theories. By subjecting hypotheses to rigorous testing and scrutiny, experiments can either confirm or refute proposed explanations. This process of continuous questioning and verification is essential for advancing ourknowledge and ensuring that our beliefs align with empirical reality.Critics of this perspective may argue that not all domains of knowledge are amenable to experimental investigation. For instance, how can one conduct experiments to explore abstract philosophical concepts or subjective experiences? While this objection holds some merit, it is important to recognize that even in these realms, the principles of empiricism and verifiability remain paramount. Philosophical arguments and theories that cannot be subjected to any form of empirical scrutiny or logical analysis run the risk of becoming mere speculation or dogma.Furthermore, the notion of experiment as the sole criterion of truth does not necessarily preclude other forms of inquiry or knowledge acquisition. Rather, it suggests that any claim, whether derived from reason, intuition, or revelation, must ultimately be subjected to the litmus test of empirical verification through experimentation. This process may involve indirect methods, such as the analysis of observable phenomena or the construction of logical arguments based on empirical premises.Another compelling argument in favor of this perspective is the inherent objectivity and universality of experimental results. Unlike subjective interpretations or culturally specific beliefs,well-designed experiments transcend personal biases and can be replicated and verified by researchers across different geographical and cultural contexts. This universality of empirical evidence fosters a shared understanding of the natural world and promotes scientific collaboration on a global scale.However, it is crucial to acknowledge the limitations and potential pitfalls associated with experimental research. Experiments can be influenced by a variety of factors, including flawed experimental designs, measurement errors, and unconscious biases. Additionally, the interpretation of experimental results may be subject to varying theoretical frameworks or philosophical assumptions. These challenges underscore the importance of rigorous peer review, replication studies, and a commitment to continually refining experimental methodologies.Despite these limitations, the weight of evidence supporting the primacy of experimentation as the ultimate arbiter of truth is overwhelming. From the remarkable achievements of modern science to the consistent ability of experiments to challenge and revise longstanding beliefs, the empirical approach has proven itself as the most reliable path to uncovering objective truth.In conclusion, the proposition that experiment is the sole criterion of truth represents a powerful and compelling perspective. While acknowledging the limitations and potential objections, the overwhelming success of the scientific method and the inherent objectivity of empirical evidence strongly support this view. As we continue to explore the mysteries of the universe and seek to expand the boundaries of human knowledge, the principles of experimentation and empirical verification must remain at the forefront of our endeavors. Only through a steadfast commitment to empiricism and a willingness to subject our beliefs to rigorous testing can we hope to uncover the deepest truths of the natural world.。

Unit2Theuniversallanguage词汇知识点清单-高中英语译林版(2020)选择性

Unit2Theuniversallanguage词汇知识点清单-高中英语译林版(2020)选择性

1.music n.音乐musical adj.音乐的musician adj.音乐家2.pose v.作曲poser v.作曲家position n.作品3.please v.取悦pleased adj.开心的pleasant adj.令人愉悦的pleasure n.愉快,荣幸4.bine v.结合bination n.结合5.adapt v.适应;改编adaptation n.改编本;适应6.defend v.防御defence n.防御7.greet v. 打招呼greeting n.问候8.suit v.适合suitable adj.适合的9.distant adj.遥远的;冷淡的distance n.距离;疏远10.breath n.呼吸breathe v.呼吸11.pany n.陪伴acpany v.陪伴panion n.伴侣,伙伴12.expect v.期待expectation n.期待13.enthusiastic adj.热情的enthusiasm n.热情14.gift n.天赋gifted adj.有天赋的15.predict v.预测prediction n.预测16.depress v.使...沮丧/抑郁depression n. 沮丧,抑郁depressed adj.沮丧的depressing adj.使人沮丧的17.possess v.拥有possession n.拥有18.transform v.转变transformation v.转变19.explode v.爆炸explosion n.爆炸20.satisfy v.使满意satisfying/satisfactory adj.令人满意的satisfied v.满意的satisfaction n.满意21.recognize v.认出;意识到recognition n.认识;赞赏22.rely v.依赖,信赖reliable adj.值得信赖的23.surround v.包围surrounding adj.周围的surroundings n.环境24.determine v.决心,决定determination n.决心determined adj.坚定的25.admit v.承认;允许进入admission n.承认;准入进入;入场费三、固定短语1. a wide range of types 种类繁多2. a piece of music 一首音乐3. a live music performance 现场音乐演出4.deserve to be done 值得被...5.the twists and turns 曲折,跌宕起伏6.tear apart使(关系密切的人)分离,开7.weep bitterly over the loss of... 因失去...而痛哭8.be overe with sorrow悲痛欲绝9.have one`s roots in起源于10.rely on依赖,依靠;信任11.it turns out that... 原来,结果是...12.throw in sth额外赠送13.give the public more access to music 给大众更多接触音乐的机会14.put on a series of free concerts 举办一系列免费音乐会15.bine…and/with…把…和…结合起来16.the munist Party of China中国共产党17.overe the Japanese invaders战胜日本侵略者18.in particular 尤其,特别19.deserve a mention 值得一提20.end with以...结尾21.think highly of 高度评价22.get tired of 厌倦23.it`s no use doing做...是没有用的24.be capable of 能够25.get down to (doing) sth开始着手做...26.have trouble doing sth 做某事有困难27.every other week 每隔一周28.in a state of 处在…的状态中29.turn up the volume调高音量30.stare at 凝视,盯住31.hold one`s breath屏住呼吸32.uncover the beauty of the song 发现歌曲的美33.grab the attention of sb 抓住某人的注意力34.sweep along席卷,使深受影响35.at the top of my voice 用最大的声音36.reflect on 反思37.a crowd of 一群38.stream into涌入39.break into enthusiastic cheers爆发出热情的欢呼40.be unaware of未意识到,没察觉到41.a sea of people 一群人42.enjoy a reputation as… 享誉…的盛名43.take a sharp turn 急转弯44.be determined to do sth 决定做...45.all of a sudden 突然46.strong will 坚强的意志47.with ease 从容地,熟练地48.be regarded as 被看作…三、好句积累1.It’s a piece that really deserves to be heard.这部作品真的值得一听。

A REVIEW OF IMAGE DENOISING ALGORITHMS, WITH A NEW ONE

A REVIEW OF IMAGE DENOISING ALGORITHMS, WITH A NEW ONE

A REVIEW OF IMAGE DENOISING ALGORITHMS,WITH A NEWONE.A.BUADES†‡,B.COLL†,AND J.M.MOREL‡Abstract.The search for efficient image denoising methods still is a valid challenge,at the crossing of functional analysis and statistics.In spite of the sophistication of the recently proposed methods,most algorithms have not yet attained a desirable level of applicability.All show an out-standing performance when the image model corresponds to the algorithm assumptions,but fail in general and create artifacts or remove imagefine structures.The main focus of this paper is,first,to define a general mathematical and experimental methodology to compare and classify classical image denoising algorithms,second,to propose an algorithm(Non Local Means)addressing the preservation of structure in a digital image.The mathematical analysis is based on the analysis of the“method noise”,defined as the difference between a digital image and its denoised version.The NL-means algorithm is proven to be asymptotically optimal under a generic statistical image model.The de-noising performance of all considered methods are compared in four ways;mathematical:asymptotic order of magnitude of the method noise under regularity assumptions;perceptual-mathematical:the algorithms artifacts and their explanation as a violation of the image model;quantitative experi-mental:by tables of L2distances of the denoised version to the original image.The most powerful evaluation method seems,however,to be the visualization of the method noise on natural images. The more this method noise looks like a real white noise,the better the method.Key words.Image restoration,non parametric estimation,PDE smoothingfilters,adaptive filters,frequency domainfiltersAMS subject classifications.62H351.Introduction.1.1.Digital images and noise.The need for efficient image restoration meth-ods has grown with the massive production of digital images and movies of all kinds, often taken in poor conditions.No matter how good cameras are,an image improve-ment is always desirable to extend their range of action.A digital image is generally encoded as a matrix of grey level or color values.In the case of a movie,this matrix has three dimensions,the third one corresponding to time.Each pair(i,u(i))where u(i)is the value at i is called pixel,for“picture element”.In the case of grey level images,i is a point on a2D grid and u(i)is a real value.In the case of classical color images,u(i)is a triplet of values for the red, green and blue components.All of what we shall say applies identically to movies, 3D images and color or multispectral images.For a sake of simplicity in notation and display of experiments,we shall here be contented with rectangular2D grey-level images.The two main limitations in image accuracy are categorized as blur and noise. Blur is intrinsic to image acquisition systems,as digital images have afinite number of samples and must satisfy the Shannon-Nyquist sampling conditions[32].The second main image perturbation is noise.†Universitat de les Illes Balears,Anselm Turmeda,Ctra.Valldemossa Km.7.5,07122Palma de Mallorca,Spain.Authorfinanced by the Ministerio de Ciencia y Tecnologia under grant TIC2002-02172.During this work,thefirst author had a fellowship of the Govern de les Illes Balears for the realization of his PhD.‡Centre de Mathmatiques et Leurs Applications.ENS Cachan61,Av du Prsident Wilson94235 Cachan,France.Authorfinanced by the Centre National d’Etudes Spatiales(CNES),the Office of Naval Research under grant N00014-97-1-0839,the Direction Gnrale des Armements(DGA),the Ministre de la Recherche et de la Technologie.12 A.BUADES,B.COLL AND J.M MORELEach one of the pixel values u(i)is the result of a light intensity measurement, usually made by a CCD matrix coupled with a light focusing system.Each captor of the CCD is roughly a square in which the number of incoming photons is being counted for afixed period corresponding to the obturation time.When the light source is constant,the number of photons received by each pixelfluctuates around its average in accordance with the central limit theorem.In other terms one can expectfluctuations of order√n for n incoming photons.In addition,each captor,if not adequately cooled,receives heat spurious photons.The resulting perturbation is usually called“obscurity noise”.In afirst rough approximation one can writev(i)=u(i)+n(i),where i∈I,v(i)is the observed value,u(i)would be the“true”value at pixel i, namely the one which would be observed by averaging the photon counting on a long period of time,and n(i)is the noise perturbation.As indicated,the amount of noise is signal-dependent,that is n(i)is larger when u(i)is larger.In noise models,the normalized values of n(i)and n(j)at different pixels are assumed to be independent random variables and one talks about“white noise”.1.2.Signal and noise ratios.A good quality photograph(for visual inspec-tion)has about256grey level values,where0represents black and255represents white.Measuring the amount of noise by its standard deviation,σ(n),one can define the signal noise ratio(SNR)asSNR=σ(u)σ(n),whereσ(u)denotes the empirical standard deviation of u,σ(u)= 1|I| i∈I(u(i)−u)2 12and u=1|I| i∈I u(i)is the average grey level value.The standard deviation of the noise can also be obtained as an empirical measurement or formally computed whenthe noise model and parameters are known.A good quality image has a standarddeviation of about60.The best way to test the effect of noise on a standard digital image is to adda gaussian white noise,in which case n(i)are i.i.d.gaussian real variables.Whenσ(n)=3,no visible alteration is usually observed.Thus,a603≃20signal to noise ratio is nearly invisible.Surprisingly enough,one can add white noise up to a21 ratio and still see everything in a picture!This fact is illustrated in Figure1.1and constitutes a major enigma of human vision.It justifies the many attempts todefine convincing denoising algorithms.As we shall see,the results have been ratherdeceptive.Denoising algorithms see no difference between small details and noise,andtherefore remove them.In many cases,they create new distortions and the researchersare so much used to them as to have created a taxonomy of denoising artifacts:“ringing”,“blur”,“staircase effect”,“checkerboard effect”,“wavelet outliers”,etc.This fact is not quite a surprise.Indeed,to the best of our knowledge,all denoisingalgorithms are based on•a noise model•a generic image smoothness model,local or global.A REVIEW OF IMAGE DENOISING ALGORIHTMS WITH A NEW ONE3Fig.1.1.A digital image with standard deviation55,the same with noise added(standard deviation3),the signal noise ratio being therefore equal to18,and the same with signal noise ratio slightly larger than2.In this second image,no alteration is visible.In the third,a conspicuous noise with standard deviation25has been added but,surprisingly enough,all details of the original image still are visible.In experimental settings,the noise model is perfectly precise.So the weak point of the algorithms is the inadequacy of the image model.All of the methods assume that the noise is oscillatory,and that the image is smooth,or piecewise smooth.So they try to separate the smooth or patchy part(the image)from the oscillatory one.Actually, manyfine structures in images are as oscillatory as noise is;conversely,white noise has low frequencies and therefore smooth components.Thus a separation method based on smoothness arguments only is hazardous.1.3.The“method noise”.All denoising methods depend on afiltering pa-rameter h.This parameter measures the degree offiltering applied to the image.For most methods,the parameter h depends on an estimation of the noise varianceσ2. One can define the result of a denoising method D h as a decomposition of any image v as(1.1)v=D h v+n(D h,v),where1.D h v is more smooth than v2.n(D h,v)is the noise guessed by the method.Now,it is not enough to smooth v to ensure that n(D h,v)will look like a noise. The more recent methods are actually not contented with a smoothing,but try to recover lost information in n(D h,v)[19],[25].So the focus is on n(D h,v).Definition1.1(Method noise).Let u be a(not necessarily noisy)image and D h a denoising operator depending on h.Then we define the method noise of u as the image difference(1.2)n(D h,u)=u−D h(u).This method noise should be as similar to a white noise as possible.In addition, since we would like the original image u not to be altered by denoising methods,the method noise should be as small as possible for the functions with the right regularity.According to the preceding discussion,four criteria can and will be taken into account in the comparison of denoising methods:•a display of typical artifacts in denoised images.4 A.BUADES,B.COLL AND J.M MOREL•a formal computation of the method noise on smooth images,evaluating howsmall it is in accordance with image local smoothness.•a comparative display of the method noise of each method on real imageswithσ=2.5.We mentioned that a noise standard deviation smaller than3issubliminal and it is expected that most digitization methods allow themselvesthis kind of noise.•a classical comparison receipt based on noise simulation:it consists of takinga good quality image,add gaussian white noise with knownσand then com-pute the best image recovered from the noisy one by each method.A tableof L2distances from the restored to the original can be established.The L2distance does not provide a good quality assessment.However,it reflects wellthe relative performances of algorithms.On top of this,in two cases,a proof of asymptotic recovery of the image can be obtained by statistical arguments.1.4.Which methods to compare?.We had to make a selection of the de-noising methods we wished to compare.Here a difficulty arises,as most original methods have caused an abundant literature proposing many improvements.So we tried to get the best available version,but keeping the simple and genuine character of the original method:no hybrid method.So we shall analyze:1.the Gaussian smoothing model(Gabor[16]),where the smoothness of u is measured by the Dirichlet integral |Du|2;2.the anisotropicfiltering model(Perona-Malik[28],Alvarez et al.[1]);3.the Rudin-Osher-Fatemi[31]total variation model and two recently proposediterated total variation refinements[36,25];4.the Yaroslavsky([42],[40])neighborhoodfilters and an elegant variant,theSUSANfilter(Smith and Brady)[34];5.the Wiener local empiricalfilter as implemented by Yaroslavsky[40];6.the translation invariant wavelet thresholding[8],a simple and performingvariant of the wavelet thresholding[10];7.DUDE,the discrete universal denoiser[24]and the UINTA,UnsupervisedInformation-Theoretic,Adaptive Filtering[3],two very recent new approaches;8.the non local means(NL-means)algorithm,which we introduce here.This last algorithm is given by a simple closed formula.Let u be defined in a bounded domainΩ⊂R2,thenNL(u)(x)=1C(x) e−(G a∗|u(x+.)−u(y+.)|2)(0)h2u(y)d y,where x∈Ω,G a is a Gaussian kernel of standard deviation a,h acts as afiltering parameter and C(x)= e−(G a∗|u(x+.)−u(z+.)|2)(0)h2d z is the normalizing factor.In order to make clear the previous definition,we recall that(G a∗|u(x+.)−u(y+.)|2)(0)= R2G a(t)|u(x+t)−u(y+t)|2d t.This amounts to say that NL(u)(x),the denoised value at x,is a mean of the values of all pixels whose gaussian neighborhood looks like the neighborhood of x.1.5.What is left.We do not draw into comparison the hybrid methods,in particular the total variation+wavelets([7],[11],[17]).Such methods are significant improvements of the simple methods but are impossible to draw into a benchmark:A REVIEW OF IMAGE DENOISING ALGORIHTMS WITH A NEW ONE5 their efficiency depends a lot upon the choice of wavelet dictionaries and the kind ofimage.Second,we do not draw into the comparison the method introduced recently byY.Meyer[22],whose aim it is to decompose the image into a BV part and a texturepart(the so called u+v methods),and even into three terms,namely u+v+w whereu is the BV part,v is the“texture”part belonging to the dual space of BV,denotedby G,and w belongs to the Besov space˙B∞−1,∞,a space characterized by the fact that the wavelet coefficients have a uniform bound.G is proposed by Y.Meyer as the rightspace to model oscillatory patterns such as textures.The main focus of this methodis not denoising,yet.Because of the different and more ambitious scopes of theMeyer method,[2,37,26],which makes it parameter and implementation-dependent,we could not draw it into the st but not least,let us mention thebandlets[27]and curvelets[35]transforms for image analysis.These methods alsoare separation methods between the geometric part and the oscillatory part of theimage and intend tofind an accurate and compressed version of the geometric part.Incidentally,they may be considered as denoising methods in geometric images,as theoscillatory part then contains part of the noise.Those methods are closely related tothe total variation method and to the wavelet thresholding and we shall be contentedwith those simpler representatives.1.6.Plan of the paper.Section2computes formally the method noise for thebest elementary local smoothing methods,namely gaussian smoothing,anisotropicsmoothing(mean curvature motion),total variation minimization and the neighbor-hoodfilters.For all of them we prove or recall the asymptotic expansion of thefilterat smooth points of the image and therefore obtain a formal expression of the methodnoise.This expression permits to characterize places where thefilter performs welland where it fails.In section3,we treat the Wiener-like methods,which proceed bya soft or hard threshold on frequency or space-frequency coefficients.We examinein turn the Wiener-Fourierfilter,the Yaroslavsky local adaptive DCT basedfiltersand the wavelet threshold method.Of course the gaussian smoothing belongs to bothclasses offilters.We also describe the universal denoiser DUDE,but we cannot drawit into the comparison as its direct application to grey level images is unpracticalso far(we discuss its feasibility).Finally,we examine the UINTA algorithms whoseprinciples stand close to the NL-means algorithm.In section5,we introduce the NonLocal means(NL-means)filter.This method is not easily classified in the preced-ing terminology,since it can work adaptively in a local or non local way.Wefirstgive a proof that this algorithm is asymptotically consistent(it gives back the con-ditional expectation of each pixel value given an observed neighborhood)under theassumption that the image is a fairly general stationary random process.The worksof Efros and Leung[13]and Levina[15]have shown that this assumption is soundfor images having enough samples in each texture patch.In section6,we compareall algorithms from several points of view,do a performance classification and ex-plain why the NL-means algorithm shares the consistency properties of most of theaforementioned algorithms.2.Local smoothingfilters.The original image u is defined in a boundeddomainΩ⊂R2,and denoted by u(x)for x=(x,y)∈R2.This continuous image isusually interpreted as the Shannon interpolation of a discrete grid of samples,[32]andis therefore analytic.The distance between two consecutive samples will be denotedbyε.The noise itself is a discrete phenomenon on the sampling grid.According to6 A.BUADES,B.COLL AND J.M MORELthe usual screen and printing visualization practice,we do not interpolate the noise samples n i as a band limited function,but rather as a piecewise constant function,constant on each pixel i and equal to n i .We write |x |=(x 2+y 2)12and x 1.x 2=x 1x 2+y 1y 2their scalar product anddenote the derivatives of u by u x =∂u ∂x ,u y =∂u ∂y ,u xy =∂2u ∂x∂y .The gradient of uis written as Du =(u x ,u y )and the Laplacian of u as ∆u =u xx +u yy .2.1.Gaussian smoothing.By Riesz theorem,image isotropic linear filtering boils down to a convolution of the image by a linear radial kernel.The smoothing requirement is usually expressed by the positivity of the kernel.The paradigm of suchkernels is of course the gaussian x →G h (x )=1(4πh 2)e −|x |24h 2.In that case,G h hasstandard deviation h and it is easily seen thatTheorem 2.1(Gabor 1960).The image method noise of the convolution with a gaussian kernel G h isu −G h ∗u =−h 2∆u +o (h 2).A similar result is actually valid for any positive radial kernel with bounded variance,so one can keep the gaussian example without loss of generality.The preceding estimate is valid if h is small enough.On the other hand,the noise reduction properties depend upon the fact that the neighborhood involved in the smoothing is large enough,so that the noise gets reduced by averaging.So in the following we assume that h =kε,where k stands for the number of samples of the function u and noise n in an interval of length h .The spatial ratio k must be much larger than 1to ensure a noise reduction.The effect of a gaussian smoothing on the noise can be evaluated at a reference pixel i =0.At this pixel,G h ∗n (0)= i ∈I P i G h (x )n (x )d x = i ∈Iε2G h (i )n i ,where we recall that n (x )is being interpolated as a piecewise constant function,the P i square pixels centered in i have size ε2and G h (i )denotes the mean value of the function G h on the pixel i .Denoting by V ar (X )the variance of a random variable X ,the additivity of variances of independent centered random variables yieldsV ar (G h ∗n (0))= iε4G h (i )2σ2≃σ2ε2 G h (x )2d x =ε2σ28πh 2.So we have provedTheorem 2.2.Let n (x )be a piecewise constant white noise,with n (x )=n i on each square pixel i .Assume that the n i are i.i.d.with zero mean and variance σ2.Then the “noise residue”after a gaussian convolution of n by G h satisfiesV ar (G h ∗n (0))≃ε2σ28πh 2.In other terms,the standard deviation of the noise,which can be interpreted as the noise amplitude,is multiplied by εh √8π.Theorems 2.1and 2.2traduce the delicate equilibrium between noise reduction and image destruction by any linear smoothing.Denoising does not alter the imageA REVIEW OF IMAGE DENOISING ALGORIHTMS WITH A NEW ONE7 at points where it is smooth at a scale h much larger than the sampling scaleε. Thefirst theorem tells us that the method noise of the gaussian denoising method is zero in harmonic parts of the image.A Gaussian convolution is optimal on harmonic functions,and performs instead poorly on singular parts of u,namely edges or texture, where the Laplacian of the image is large.See Figure2.2.2.2.Anisotropicfilters and curvature motion.The anisotropicfilter(A F) attempts to avoid the blurring effect of the gaussian by convolving the image u at x only in the direction orthogonal to Du(x).The idea of suchfilter goes back to Perona and Malik[28]and actually again to Gabor[16].SetA F h u(x)= G h(t)u(x+t Du(x)⊥|Du(x)|)dt,for x such that Du(x)=0and where(x,y)⊥=(−y,x)and G h(t)=1√2πh e−t22h2isthe one-dimensional Gauss function with variance h2.At points where Du(x)=0an isotropic gaussian mean is usually applied and the result of Theorem2.1holds at those points.If one assumes that the original image u is twice continuously differentiable (C2)at x,it is easily shown by a second order Taylor expansion that Theorem2.3.The image method noise of an anisotropicfilter A F h isu(x)−A F h u(x)≃−12h2D2u(Du⊥|Du|,Du⊥|Du|)=−12h2|Du|curv(u)(x),where the relation holds when Du(x)=0.By curv(u)(x),we denote the curvature,i.e.the signed inverse of the radius of curvature of the level line passing by x.When Du(x)=0,this meanscurv(u)=u xx u2y−2u xy u x u y+u yy u2x(u2x+u2y)32.This method noise is zero wherever u behaves locally like a one variable function, u(x,y)=f(ax+by+c).In such a case,the level line of u is locally the straight line with equation ax+by+c=0and the gradient of f may instead be very large. In other terms,with anisotropicfiltering,an edge can be maintained.On the other hand,we have to evaluate the gaussian noise reduction.This is easily done by a one-dimensional adaptation of Theorem2.2.Notice that the noise on a grid is not isotropic;so the gaussian average when Du is parallel to one coordinate axis is made roughly on√2more samples than the gaussian average in the diagonal direction.Theorem2.4.By anisotropic gaussian smoothing,whenεis small enough with respect to h,the noise residue satisfiesVar(A F h(n))≤ε√2πhσ2.In other terms,the standard deviation of the noise n is multiplied by a factor at most equal to(ε√2πh)1/2,this maximal value being attained in the diagonals.Proof.Let L be the line x+t Du⊥(x)|Du(x)|passing by x,parameterized by t∈R and denote by P i,i∈I the pixels which meet L,n(i)the noise value,constant on pixel8 A.BUADES,B.COLL AND J.M MORELP i,andεi the length of the intersection of L∩P i.Denote by g(i)the average of G h(x+t Du⊥(x)|Du(x)|)on L∩P i.Then,one hasA F h n(x)≃ iεi n(i)g(i).The n(i)are i.i.d.with standard variationσand thereforeV ar(A F h(n))= iε2iσ2g(i)2≤σ2max(εi) iεi g(i)2.This yieldsVar(A F h(n))≤√2εσ2 G h(t)2dt=ε√2πhσ2.There are many versions of A F h,all yielding an asymptotic estimate equivalent to the one in Theorem2.3:the famous medianfilter[14],an inf-supfilter on segments centered at x[5],and the clever numerical implementation of the mean curvature equation in[21].So all of thosefilters have in common the good preservation of edges, but they perform poorly onflat regions and are worse there than a gaussian blur.This fact derives from the comparison of the noise reduction estimates of Theorems2.1and 2.4,and is experimentally patent in Figure2.2.2.3.Total variation.The Total variation minimization was introduced by Rudin, Osher and Fatemi[30,31].The original image u is supposed to have a simple ge-ometric description,namely a set of connected sets,the objects,along with their smooth contours,or edges.The image is smooth inside the objects but with jumps across the boundaries.The functional space modelling these properties is BV(Ω),the space of integrable functions withfinite total variation T VΩ(u)= |Du|,where Du is assumed to be a Radon measure.Given a noisy image v(x),the above mentioned authors proposed to recover the original image u(x)as the solution of the constrained minimization problemarg minu T VΩ(u),(2.1)subject to the noise constraintsΩ(u(x)−v(x))d x=0and Ω|u(x)−v(x)|2d x=σ2.The solution u must be as regular as possible in the sense of the total variation, while the difference v(x)−u(x)is treated as an error,with a prescribed energy.The constraints prescribe the right mean and variance to u−v,but do not ensure that it be similar to a noise(see a thorough discussion in[22]).The preceding problem is naturally linked to the unconstrained problemarg minu T VΩ(u)+λ Ω|v(x)−u(x)|2d x,(2.2)A REVIEW OF IMAGE DENOISING ALGORIHTMS WITH A NEW ONE9 for a given Lagrange multiplierλ.The above functional is strictly convex and lower semicontinuous with respect to the weak-star topology of BV.Therefore the minimum exists,is unique and computable(see(e.g.)[6].)The parameterλcontrols the trade offbetween the regularity andfidelity terms.Asλgets smaller the weight of the regularity term increases.Thereforeλis related to the degree offiltering of the solution of the minimization problem.Let us denote by TVFλ(v)the solution of problem(2.2)for a given value ofλ.The Euler Lagrange equation associated with the minimization problem is given by(u(x)−v(x))−12λcurv(u)(x)=0,(see[30]).Thus,Theorem2.5.The image method noise of the total variation minimization(2.2) isu(x)−TVFλ(u)(x)=−12λcurv(TVFλ(u))(x).As in the anisotropic case,straight edges are maintained because of their small curvature.However,details and texture can be over smoothed ifλis too small,as is shown in Figure2.2.2.4.Iterated Total Variation refinement.In the original TV model the removed noise,v(x)−u(x),is treated as an error and is no longer studied.In practice, some structures and texture are present in this error.Several recent works have tried to avoid this effect[36,25].2.4.1.The Tadmor et al.approach.In[36],the authors have proposed to use the Rudin-Osher-Fatemi iteratively.They decompose the noisy image,v=u0+n0 by the total variation model.So taking u0to contain only geometric information,they decompose by the very same model n0=u1+n1,where u1is assumed to be again a geometric part and n1contains less geometric information than n0.Iterating this process,one obtains u=u0+u1+u2+...+u k as a refined geometric part and n k as the noise residue.This strategy is in some sense close to the matching pursuit methods [20].Of course,the weight parameter in the Rudin-Osher-Fatemi has to grow at each iteration and the authors propose a geometric seriesλ,2λ,....,2kλ.In that way,the extraction of the geometric part n k becomes twice more asking at each step.Then, the new algorithm is as follows:1.Starting with an initial scaleλ=λ0,v=u0+n0,[u0,n0]=arg minv=u+n |Du|+λ0 |v(x)−u(x)|2d x.2.Proceed with successive applications of the dyadic refinement n j=u j+1+n j+1,[u j+1,n j+1]=arg minn j=u+n |Du|+λ02j+1 |n j(x)−u(x)|2d x.3.After k steps,we get the following hierarchical decomposition of vv=u0+n0=u0+u1+n1=.....=u0+u1+...+u k+n k.10 A.BUADES,B.COLL AND J.M MORELThe denoised image is given by the partial sum k j =0u j and n k is the noise residue.This is a multilayered decomposition of v which lies in an intermediate scale of spaces,in between BV and L 2.Some theoretical results on the convergence of this expansion are presented in [36].2.4.2.The Osher et al.approach.The second algorithm due to Osher et al.[25],also consists of an iteration of the original model.The new algorithm is as follows.1.First solve the original TV modelu 1=arg min u ∈BV|∇u (x )|d x +λ (v (x )−u (x ))2d x ,to obtain the decomposition v =u 1+n 1.2.Perform a correction step to obtainu 2=arg min u ∈BV|∇u (x )|d x +λ (v (x )+n 1(x )−u (x ))2d x ,where n 1is the noise estimated by the first step.The correction step adds this first estimate of the noise to the original image and raises the following decomposition v +n 1=u 2+n 2.3.Iterate :compute u k +1as a minimizer of the modified total variation mini-mization,u k +1=arg min u ∈BV|∇u (x )|d x +λ (v (x )+n k (x )−u (x ))2d x ,wherev +n k =u k +1+n k +1.Some results are presented in [25]which clarify the nature of the above sequence:•{u k }k converges monotonically in L 2to v ,the noisy image,as k →∞.•{u k }k approaches the noisy free image monotonically in the Bregman distance associated with the BV seminorm,at least until u ¯k −u ≤σ2,where u is the original image and σis the standard deviation of the added noise.These two results indicate how to stop the sequence and choose u ¯k .It is enough to proceed iteratively until the result gets noisier or the distance u ¯k −u 2gets smaller than σ2.The new solution has more details preserved,as Figure 2.2shows.The above iterated denoising strategy being quite general,one can make the computations for a linear denoising operator T as well.In that case,this strategyT (v +n 1)=T (v )+T (n 1)amounts to say that the first estimated noise n 1is filtered again and its smooth components added back to the original,which is in fact the Tadmor et al.strategy.2.5.Neighborhood filters.The previous filters are based on a notion of spa-tial neighborhood or proximity.Neighborhood filters instead take into account grey level values to define neighboring pixels.In the simplest and more extreme case,the denoised value at pixel i is an average of values at pixels which have a grey level value close to u (i ).The grey level neighborhood is thereforeB (i,h )={j ∈I |u (i )−h <u (j )<u (i )+h }.。

存在任意长的等差素数数列

存在任意长的等差素数数列
1 p p −1 k −1
if p if p
k k.
1−
k −1 p
In particular we compute1
γ3 = 2
p 3
1− 1−
1 ≈ 1.32032 (p − 1)2 3p − 1 ≈ 2.85825. (p − 1)3
and γ4 =
9 2p
5
What we actually prove is a somewhat more precise version of Theorem 1.1, which gives a lower bound falling short of the Hardy-Littlewood conjecture by just a constant factor.
k −1 j =0
Ej ≈ 1/(log N )k .
For fixed k , and in fact for k nearly as large as 2 log N/ log log N , this is an increasing function of N . This suggests that there are infinitely many k -term arithmetic progressions of primes for any fixed k , and thus arbitrarily long such progressions. Of course, the assumption that the events Ej are independent was totally unjustified. If E0 , E1 and E2 all hold then one may infer that x is odd and d is even, which increases the chance that E3 also holds by a factor of two. There are, however, more sophisticated heuristic arguments available, which take account of the fact that the primes > q fall only in those residue classes a(mod q ) with a coprime to q . There are very general conjectures of Hardy-Littlewood which derive from such heuristics, and a special case of these conjectures applies to our problem. It turns out that the extremely na¨ ıve heuristic we gave above only misses the mark by a constant factor: Conjecture 1.2 (Hardy-Littlewood conjecture on k -term APs). For each k we have #{x, d ∈ {1, . . . , N } : x, x + d, . . . , x + (k − 1)d are all prime } = where γk =

量子信息——连续变量篇

量子信息——连续变量篇

Quantum information with continuous variablesSamuel L.BraunsteinComputer Science,University of York,York YO105DD,United KingdomPeter van LoockNational Institute of Informatics(NII),Tokyo101-8430,Japan and Institute of TheoreticalPhysics,Institute of Optics,Information and Photonics(Max-Planck Forschungsgruppe),Universität Erlangen-Nürnberg,D-91058Erlangen,Germany͑Published29June2005͒Quantum information is a rapidly advancing area of interdisciplinary research.It may lead to real-world applications for communication and computation unavailable without the exploitation of quantum properties such as nonorthogonality or entanglement.This article reviews the progress in quantum information based on continuous quantum variables,with emphasis on quantum optical implementations in terms of the quadrature amplitudes of the electromagneticfield.CONTENTSI.Introduction513II.Continuous Variables in Quantum Optics516A.The quadratures of the quantizedfield516B.Phase-space representations518C.Gaussian states519D.Linear optics519E.Nonlinear optics520F.Polarization and spin representations522G.Necessity of phase reference523 III.Continuous-Variable Entanglement523A.Bipartite entanglement5251.Pure states5252.Mixed states and inseparability criteria526B.Multipartite entanglement5291.Discrete variables5292.Genuine multipartite entanglement5303.Separability properties of Gaussian states5304.Generating entanglement5315.Measuring entanglement533C.Bound entanglement534D.Nonlocality5341.Traditional EPR-type approach5352.Phase-space approach5363.Pseudospin approach536E.Verifying entanglement experimentally537 IV.Quantum Communication with Continuous Variables538A.Quantum teleportation5401.Teleportation protocol5412.Teleportation criteria5433.Entanglement swapping546B.Dense coding546rmation:A measure5472.Mutual information5473.Classical communication5474.Classical communication via quantum states5475.Dense coding548C.Quantum error correction550D.Quantum cryptography5501.Entanglement-based versus prepare andmeasure5502.Early ideas and recent progress5513.Absolute theoretical security5524.Verifying experimental security5535.Quantum secret sharing553E.Entanglement distillation554F.Quantum memory555V.Quantum Cloning with Continuous Variables555A.Local universal cloning5551.Beyond no-cloning5552.Universal cloners556B.Local cloning of Gaussian states5571.Fidelity bounds for Gaussian cloners5572.An optical cloning circuit for coherentstates558C.Telecloning559 VI.Quantum Computation with Continuous Variables560A.Universal quantum computation560B.Extension of the Gottesman-Knill theorem563 VII.Experiments with Continuous Quantum Variables565A.Generation of squeezed-state EPR entanglement5651.Broadband entanglement via opticalparametric amplification5652.Kerr effect and linear interference567B.Generation of long-lived atomic entanglement568C.Generation of genuine multipartite entanglement569D.Quantum teleportation of coherent states569E.Experimental dense coding570F.Experimental quantum key distribution571G.Demonstration of a quantum memory effect572 VIII.Concluding Remarks572 Acknowledgments573 References573I.INTRODUCTIONQuantum information is a relatively young branch of physics.One of its goals is to interpret the concepts of quantum physics from an information-theoretic point of view.This may lead to a deeper understanding of quan-REVIEWS OF MODERN PHYSICS,VOLUME77,APRIL20050034-6861/2005/77͑2͒/513͑65͒/$50.00©2005The American Physical Society513tum theory.Conversely,information and computation are intrinsically physical concepts,since they rely on physical systems in which information is stored and by means of which information is processed or transmitted. Hence physical concepts,and at a more fundamental level quantum physical concepts,must be incorporated in a theory of information and computation.Further-more,the exploitation of quantum effects may even prove beneficial for various kinds of information pro-cessing and communication.The most prominent ex-amples of this are quantum computation and quantum key distribution.Quantum computation means in par-ticular cases,in principle,computation faster than any known classical computation.Quantum key distribution makes possible,in principle,unconditionally secure communication as opposed to communication based on classical key distribution.From a conceptual point of view,it is illuminating to consider continuous quantum variables in quantum in-formation theory.This includes the extension of quan-tum communication protocols from discrete to continu-ous variables and hence fromfinite to infinite dimensions.For instance,the original discrete-variable quantum teleportation protocol for qubits and other finite-dimensional systems͑Bennett et al.,1993͒was soon after its publication translated into the continuous-variable setting͑Vaidman,1994͒.The main motivation for dealing with continuous variables in quantum infor-mation,however,originated in a more practical observa-tion:efficient implementation of the essential steps in quantum communication protocols,namely,preparing, unitarily manipulating,and measuring͑entangled͒quan-tum states,is achievable in quantum optics utilizing con-tinuous quadrature amplitudes of the quantized electro-magneticfield.For example,the tools for measuring a quadrature with near-unit efficiency or for displacing an optical mode in phase space are provided by homodyne-detection and feedforward techniques,respectively. Continuous-variable entanglement can be efficiently produced using squeezed light͓in which the squeezing of a quadrature’s quantumfluctuations is due to a non-linear optical interaction͑Walls and Milburn,1994͔͒and linear optics.A valuable feature of quantum optical implementa-tions based upon continuous variables,related to their high efficiency,is their unconditionalness.Quantum re-sources such as entangled states emerge from the non-linear optical interaction of a laser with a crystal͑supple-mented if necessary by some linear optics͒in an unconditional fashion,i.e.,every inverse bandwidth time.This unconditionalness is hard to obtain in discrete-variable qubit-based implementations using single-photon states.In that case,the desired prepara-tion due to the nonlinear optical interaction depends on particular͑coincidence͒measurement results ruling out the unwanted͑in particular,vacuum͒contributions in the outgoing state vector.However,the unconditional-ness of the continuous-variable implementations has its price:it is at the expense of the quality of the entangle-ment of the prepared states.This entanglement and hence any entanglement-based quantum protocol is al-ways imperfect,the degree of imperfection depending on the amount of squeezing of the laser light involved. Good quality and performance require large squeezing which is technologically demanding,but to a certain ex-tent͓about10dB͑Wu et al.,1986͔͒already state of the art.Of course,in continuous-variable protocols that do not rely on entanglement,for instance,coherent-state-based quantum key distribution,these imperfections do not occur.To summarize,in the most commonly used optical ap-proaches,the continuous-variable implementations al-ways work pretty well͑and hence efficiently and uncon-ditionally͒,but never perfectly.Their discrete-variable counterparts only work sometimes͑conditioned upon rare successful events͒,but they succeed,in principle, perfectly.A similar tradeoff occurs when optical quan-tum states are sent through noisy channels͑opticalfi-bers͒,for example,in a realistic quantum key distribu-tion scenario.Subject to losses,the continuous-variable states accumulate noise and emerge at the receiver as contaminated versions of the sender’s input states.The discrete-variable quantum information encoded in single-photon states is reliably conveyed for each photon that is not absorbed during transmission.Due to the recent results of Knill,Laflamme,and Mil-burn͑Knill et al.,2001͒,it is now known that efficient quantum information processing is possible,in principle, solely by means of linear optics.Their scheme is formu-lated in a discrete-variable setting in which the quantum information is encoded in single-photon states.Apart from entangled auxiliary photon states,generated off-line without restriction to linear optics,conditional dy-namics͑feedforward͒is the essential ingredient in mak-ing this approach work.Universal quantum gates such as a controlled-NOT gate can,in principle,be built using this scheme without need of any Kerr-type nonlinear op-tical interaction͑corresponding to an interaction Hamil-tonian quartic in the optical modes’annihilation and creation operators͒.This Kerr-type interaction would be hard to obtain on the level of single photons.However, the off-line generation of the complicated auxiliary states needed in the Knill-Laflamme-Milburn scheme seems impractical too.Similarly,in the continuous-variable setting,when it comes to more advanced quantum information proto-cols,such as universal quantum computation or,in a communication scenario,entanglement distillation,it turns out that tools more sophisticated than mere Gaussian operations are needed.In fact,the Gaussian operations are effectively those described by interaction Hamiltonians at most quadratic in the optical modes’annihilation and creation operators,thus leading to lin-ear input-output relations as in beam-splitter or squeez-ing transformations.Gaussian operations,mapping Gaussian states onto Gaussian states,also include ho-modyne detections and phase-space displacements.In contrast,the non-Gaussian operations required for ad-vanced continuous-variable quantum communication͑in particular,long-distance communication based on en-514S.L.Braunstein and P.van Loock:Quantum information with continuous variables Rev.Mod.Phys.,Vol.77,No.2,April2005tanglement distillation and swapping,quantum memory,and teleportation͒are due either to at least cubic non-linear optical interactions or to conditional transforma-tions depending on non-Gaussian measurements such asphoton counting.It seems that,at this very sophisticatedlevel,the difficulties and requirements of the discrete-and continuous-variable implementations are analogous.In this review,our aim is to highlight the strengths ofthe continuous-variable approaches to quantum infor-mation processing.Therefore we focus on those proto-cols that are based on Gaussian states and their feasiblemanipulation through Gaussian operations.This leads tocontinuous-variable proposals for the implementation ofthe simplest quantum communication protocols,such asquantum teleportation and quantum key distribution,and includes the efficient generation and detection ofcontinuous-variable entanglement.Before dealing with quantum communication andcomputation,in Sec.II,wefirst introduce continuousquantum variables within the framework of quantumoptics.The discussions about the quadratures of quan-tized electromagnetic modes,about phase-space repre-sentations,and about Gaussian states include the nota-tions and conventions that we use throughout thisarticle.We conclude Sec.II with a few remarks on linearand nonlinear optics,on alternative polarization andspin representations,and on the necessity of a phasereference in continuous-variable implementations.Thenotion of entanglement,indispensable in many quantumprotocols,is described in Sec.III in the context of con-tinuous variables.We discuss pure and mixed entangledstates,entanglement between two͑bipartite͒and be-tween many͑multipartite͒parties,and so-called bound ͑undistillable͒entanglement.The generation,measure-ment,and verification͑both theoretical and experimen-tal͒of continuous-variable entanglement are here of par-ticular interest.As for the properties of the continuous-variable entangled states related with theirinseparability,we explain how the nonlocal character ofthese states is revealed.This involves,for instance,vio-lations of Bell-type inequalities imposed by local real-ism.Such violations,however,cannot occur when themeasurements considered are exclusively of continuous-variable type.This is due to the strict positivity of theWigner function of the Gaussian continuous-variable en-tangled states,which allows for a hidden-variable de-scription in terms of the quadrature observables.In Sec.IV,we describe the conceptually and practi-cally most important quantum communication protocols formulated in terms of continuous variables and thus utilizing the continuous-variable͑entangled͒states. These schemes include quantum teleportation and en-tanglement swapping͑teleportation of entanglement͒, quantum͑super͒dense coding,quantum error correc-tion,quantum cryptography,and entanglement distilla-tion.Since quantum teleportation based on nonmaxi-mum continuous-variable entanglement,usingfinitely squeezed two-mode squeezed states,is always imperfect, teleportation criteria are needed both for the theoretical and for the experimental verification.As is known from classical communication,light,propagating at high speed and offering a broad range of different frequen-cies,is an ideal carrier for the transmission of informa-tion.This applies to quantum communication as well. However,light is less suited for the storage of informa-tion.In order to store quantum information,for in-stance,at the intermediate stations in a quantum re-peater,atoms are more appropriate media than light. Significantly,as another motivation to deal with continu-ous variables,a feasible light-atom interface can be built via free-space interaction of light with an atomic en-semble based on the alternative polarization and spin-type variables.No strong cavity QED coupling is needed as with single photons.The concepts of this transfer of quantum information from light to atoms and vice versa, as the essential ingredients of a quantum memory,are discussed in Sec.IV.FSection V is devoted to quantum cloning with con-tinuous variables.One of the most fundamental͑and historically one of thefirst͒“laws”of quantum informa-tion theory is the so-called no-cloning theorem͑Dieks, 1982;Wootters and Zurek,1982͒.It forbids the exact copying of arbitrary quantum states.However,arbitrary quantum states can be copied approximately,and the resemblance͑in mathematical terms,the overlap orfi-delity͒between the clones may attain an optimal value independent of the original states.Such optimal cloning can be accomplished locally by sending the original states͑together with some auxiliary system͒through a local unitary quantum circuit.Optimal cloning of Gauss-ian continuous-variable states appears to be more inter-esting than that of general continuous-variable states, because the latter can be mimicked by a simple coin toss.We describe a non-entanglement-based implemen-tation for the optimal local cloning of Gaussian continuous-variable states.In addition,for Gaussian continuous-variable states,an optical implementation exists of optimal cloning at a distance͑telecloning͒.In this case,the optimality requires entanglement.The cor-responding multiparty entanglement is again producible with nonlinear optics͑squeezed light͒and linear optics ͑beam splitters͒.Quantum computation over continuous variables,dis-cussed in Sec.VI,is a more subtle issue than the in some sense straightforward continuous-variable extensions of quantum communication protocols.Atfirst sight,con-tinuous variables do not appear well suited for the pro-cessing of digital information in a computation.On the other hand,a continuous-variable quantum state having an infinite-dimensional spectrum of eigenstates contains a vast amount of quantum information.Hence it might be promising to adjust the continuous-variable states theoretically to the task of computation͑for instance,by discretization͒and yet to exploit their continuous-variable character experimentally in efficient͑optical͒implementations.We explain in Sec.VI why universal quantum computation over continuous variables re-quires Hamiltonians at least cubic in the position and momentum͑quadrature͒operators.Similarly,any quan-tum circuit that consists exclusively of unitary gates from515S.L.Braunstein and P.van Loock:Quantum information with continuous variables Rev.Mod.Phys.,Vol.77,No.2,April2005the continuous-variable Clifford group can be efficientlysimulated by purely classical means.This is acontinuous-variable extension of the discrete-variableGottesman-Knill theorem in which the Clifford groupelements include gates such as the Hadamard͑in thecontinuous-variable case,Fourier͒transform or the con-trolled NOT͑CNOT͒.The theorem applies,for example,to quantum teleportation which is fully describable by CNOT’s and Hadamard͑or Fourier͒transforms of some eigenstates supplemented by measurements in thateigenbasis and spin or phaseflip operations͑or phase-space displacements͒.Before some concluding remarks in Sec.VIII,wepresent some of the experimental approaches to squeez-ing of light and squeezed-state entanglement generationin Sec.VII.A.Both quadratic and quartic optical nonlin-earities are suitable for this,namely,parametric downconversion and the Kerr effect,respectively.Quantumteleportation experiments that have been performed al-ready based on continuous-variable squeezed-state en-tanglement are described in Sec.VII.D.In Sec.VII,wefurther discuss experiments with long-lived atomic en-tanglement,with genuine multipartite entanglement ofoptical modes,experimental dense coding,experimentalquantum key distribution,and the demonstration of aquantum memory effect.II.CONTINUOUS VARIABLES IN QUANTUM OPTICSFor the transition from classical to quantum mechan-ics,the position and momentum observables of the par-ticles turn into noncommuting Hermitian operators inthe Hamiltonian.In quantum optics,the quantized elec-tromagnetic modes correspond to quantum harmonicoscillators.The modes’quadratures play the roles of theoscillators’position and momentum operators obeyingan analogous Heisenberg uncertainty relation.A.The quadratures of the quantizedfieldFrom the Hamiltonian of a quantum harmonic oscil-lator expressed in terms of͑dimensionless͒creation and annihilation operators and representing a single mode k, Hˆk=ប␻k͑aˆk†aˆk+12͒,we obtain the well-known form writ-ten in terms of“position”and“momentum”operators ͑unit mass͒,Hˆk=12͑pˆk2+␻k2xˆk2͒,͑1͒withaˆk=1ͱ2ប␻k͑␻k xˆk+ipˆk͒,͑2͒aˆk†=1ͱ2ប␻k͑␻k xˆk−ipˆk͒,͑3͒or,conversely,xˆk=ͱប2␻k͑aˆk+aˆk†͒,͑4͒pˆk=−iͱប␻k2͑aˆk−aˆk†͒.͑5͒Here,we have used the well-known commutation rela-tion for position and momentum,͓xˆk,pˆkЈ͔=iប␦kkЈ,͑6͒which is consistent with the bosonic commutation rela-tions͓aˆk,aˆkЈ†͔=␦kkЈ,͓aˆk,aˆkЈ͔=0.In Eq.͑2͒,we see that up to normalization factors the position and the momentum are the real and imaginary parts of the annihilation op-erator.Let us now define the dimensionless pair of con-jugate variables,Xˆkϵͱ␻k2បxˆk=Re aˆk,Pˆkϵ1ͱ2ប␻k pˆk=Im aˆk.͑7͒Their commutation relation is then͓Xˆk,PˆkЈ͔=i2␦kkЈ.͑8͒In other words,the dimensionless position and momen-tum operators,Xˆk and Pˆk,are defined as if we setប=1/2.These operators represent the quadratures of a single mode k,in classical terms corresponding to the real and imaginary parts of the oscillator’s complex am-plitude.In the following,by using͑Xˆ,Pˆ͒or equivalently ͑xˆ,pˆ͒,we shall always refer to these dimensionless quadratures as playing the roles of position and momen-tum.Hence͑xˆ,pˆ͒will also stand for a conjugate pair of dimensionless quadratures.The Heisenberg uncertainty relation,expressed in terms of the variances of two arbitrary noncommuting observables Aˆand Bˆfor an arbitrary given quantum state,͗͑⌬Aˆ͒2͘ϵŠ͑Aˆ−͗Aˆ͒͘2‹=͗Aˆ2͘−͗Aˆ͘2,͗͑⌬Bˆ͒2͘ϵŠ͑Bˆ−͗Bˆ͒͘2‹=͗Bˆ2͘−͗Bˆ͘2,͑9͒becomes͗͑⌬Aˆ͒2͗͑͘⌬Bˆ͒2͘ജ14͉͓͗Aˆ,Bˆ͔͉͘2.͑10͒Inserting Eq.͑8͒into Eq.͑10͒yields the uncertainty re-lation for a pair of conjugate quadrature observables of a single mode k,xˆk=͑aˆk+aˆk†͒/2,pˆk=͑aˆk−aˆk†͒/2i,͑11͒namely,͗͑⌬xˆk͒2͗͑͘⌬pˆk͒2͘ജ14͉͓͗xˆk,pˆk͔͉͘2=116.͑12͒Thus,in our units,the quadrature variance for a vacuum or coherent state of a single mode is1/4.Let us further516S.L.Braunstein and P.van Loock:Quantum information with continuous variables Rev.Mod.Phys.,Vol.77,No.2,April2005illuminate the meaning of the quadratures by looking at a single frequency mode of the electric field ͑for a single polarization ͒,E ˆk ͑r ,t ͒=E 0͓a ˆk ei ͑k ·r −␻k t ͒+a ˆk †e −i ͑k ·r −␻k t ͔͒.͑13͒The constant E 0contains all the dimensional prefactors.By using Eq.͑11͒,we can rewrite the mode asE ˆk ͑r ,t ͒=2E 0͓x ˆk cos ͑␻k t −k ·r ͒+pˆk sin ͑␻k t −k ·r ͔͒.͑14͒Clearly,the position and momentum operators xˆk and p ˆk represent the in-phase and out-of-phase components of the electric-field amplitude of the single mode k with respect to a ͑classical ͒reference wave ϰcos ͑␻k t −k ·r ͒.The choice of the phase of this wave is arbitrary,of course,and a more general reference wave would lead us to the single-mode descriptionE ˆk ͑r ,t ͒=2E 0͓x ˆk ͑⌰͒cos ͑␻k t −k ·r −⌰͒+pˆk ͑⌰͒sin ͑␻k t −k ·r −⌰͔͒,͑15͒with the more general quadraturesxˆk ͑⌰͒=͑a ˆk e −i ⌰+a ˆk †e +i ⌰͒/2,͑16͒p ˆk ͑⌰͒=͑a ˆk e −i ⌰−a ˆk †e +i ⌰͒/2i .͑17͒These new quadratures can be obtained from x ˆk and p ˆk via the rotationͩx ˆk ͑⌰͒pˆk ͑⌰͒ͪ=ͩcos ⌰sin ⌰−sin ⌰cos ⌰ͪͩxˆk pˆk ͪ.͑18͒Since this is a unitary transformation,we again end upwith a pair of conjugate observables fulfilling the com-mutation relation ͑8͒.Furthermore,because pˆk ͑⌰͒=x ˆk ͑⌰+␲/2͒,the whole continuum of quadratures is cov-ered by x ˆk ͑⌰͒with ⌰෈͓0,␲͒.This continuum of observ-ables is indeed measurable by relatively simple means.Such a so-called homodyne detection works as follows.A photodetector measuring an electromagnetic mode converts the photons into electrons and hence into an electric current,called the photocurrent i ˆ.It is therefore sensible to assume i ˆϰn ˆ=a ˆ†a ˆor i ˆ=qaˆ†a ˆwhere q is a con-stant ͑Paul,1995͒.In order to detect a quadrature of themode aˆ,the mode must be combined with an intense local oscillator at a 50:50beam splitter.The local oscil-lator is assumed to be in a coherent state with large photon number,͉␣LO ͘.It is therefore reasonable to de-scribe this oscillator by a classical complex amplitude␣LO rather than by an annihilation operator aˆLO .The two output modes of the beam splitter,͑aˆLO +a ˆ͒/ͱ2and ͑a ˆLO −a ˆ͒/ͱ2͑see Sec.II.D ͒,may then be approximated byaˆ1=͑␣LO +a ˆ͒/ͱ2,aˆ2=͑␣LO −a ˆ͒/ͱ2.͑19͒This yields the photocurrentsi ˆ1=qa ˆ1†aˆ1=q ͑␣LO *+a ˆ†͒͑␣LO +a ˆ͒/2,i ˆ2=qa ˆ2†aˆ2=q ͑␣LO *−a ˆ†͒͑␣LO −a ˆ͒/2.͑20͒The actual quantity to be measured will be the differ-ence photocurrent␦i ˆϵi ˆ1−i ˆ2=q ͑␣LO *aˆ+␣LO a ˆ†͒.͑21͒By introducing the phase ⌰of the local oscillator,␣LO=͉␣LO ͉exp ͑i ⌰͒,we recognize that the quadrature observ-able xˆ͑⌰͒from Eq.͑16͒is measured ͑without mode index k ͒.Now adjustment of the local oscillator’s phase ⌰෈͓0,␲͔enables us to detect any quadrature from thewhole continuum of quadratures xˆ͑⌰͒.A possible way to realize quantum tomography ͑Leonhardt,1997͒,i.e.,the reconstruction of the mode’s quantum state given by its Wigner function,relies on this measurement method,called ͑balanced ͒homodyne detection .A broadband rather than a single-mode description of homodyne de-tection can be found in the work of Braunstein and Crouch ͑1991͒,who also investigate the influence of a quantized local oscillator.We have now seen that it is not too hard to measure the quadratures of an electromagnetic mode.Unitary transformations such as quadrature displacements ͑phase-space displacements ͒can also be relatively easily performed via the so-called feedforward technique,as opposed to,for example,photon number displacements.This simplicity and the high efficiency when measuring and manipulating continuous quadratures are the main reasons why continuous-variable schemes appear more attractive than those based on discrete variables such as the photon number.In the following,we shall refer mainly to the conju-gate pair of quadratures xˆk and p ˆk ͑position and momen-tum,i.e.,⌰=0and ⌰=␲/2͒.In terms of these quadra-tures,the number operator becomesn ˆk =a ˆk †a ˆk =x ˆk 2+p ˆk 2−12,͑22͒using Eq.͑8͒.Let us finally review some useful formulas for the single-mode quadrature eigenstates,xˆ͉x ͘=x ͉x ͘,pˆ͉p ͘=p ͉p ͘,͑23͒where we have now dropped the mode index k .They are orthogonal,͗x ͉x Ј͘=␦͑x −x Ј͒,͗p ͉p Ј͘=␦͑p −p Ј͒,͑24͒and complete,͵−ϱϱ͉x ͗͘x ͉dx =1,͵−ϱϱ͉p ͗͘p ͉dp =1.͑25͒Just as for position and momentum eigenstates,the quadrature eigenstates are mutually related to each other by a Fourier transformation,͉x ͘=1ͱ␲͵−ϱϱe −2ixp ͉p ͘dp ,͑26͒517S.L.Braunstein and P .van Loock:Quantum information with continuous variablesRev.Mod.Phys.,Vol.77,No.2,April 2005͉p͘=1ͱ͵−ϱϱe+2ixp͉x͘dx.͑27͒Despite being unphysical and not square integrable,the quadrature eigenstates can be very useful in calculations involving the wave functions␺͑x͒=͗x͉␺͘,etc.,and inidealized quantum communication protocols based on continuous variables.For instance,a vacuum state infi-nitely squeezed in position may be expressed by a zero-position eigenstate͉x=0͘=͉͐p͘dp/ͱ␲.The physical,fi-nitely squeezed states are characterized by the quadrature probability distributions͉␺͑x͉͒2,etc.,ofwhich the widths correspond to the quadrature uncer-tainties.B.Phase-space representationsThe Wigner function is particularly suitable as a “quantum phase-space distribution”for describing the effects on the quadrature observables that may arise from quantum theory and classical statistics.It behaves partly as a classical probability distribution,thus en-abling us to calculate measurable quantities such as mean values and variances of the quadratures in a classical-like fashion.On the other hand,in contrast to a classical probability distribution,the Wigner function can become negative.The Wigner function was originally proposed by Wigner in his1932paper“On the quantum correction for thermodynamic equilibrium”͑Wigner,1932͒.There, he gave an expression for the Wigner function in terms of the position basis which reads͑with x and p being a dimensionless pair of quadratures in our units withប=1/2as introduced in the previous section;Wigner, 1932͒W͑x,p͒=2␲͵dye+4iyp͗x−y͉␳ˆ͉x+y͘.͑28͒Here and throughout,unless otherwise specified,the in-tegration will be over the entire space of the integration variable͑i.e.,here the integration goes from−ϱtoϱ͒. We gave Wigner’s original formula for only one mode or one particle͓Wigner’s͑1932͒original equation was in N-particle form͔because it simplifies the understanding of the concept behind the Wigner function approach. The extension to N modes is straightforward.Why does W͑x,p͒resemble a classical-like probability distribution?The most important attributes that explain this are the proper normalization,͵W͑␣͒d2␣=1,͑29͒the property of yielding the correct marginal distribu-tions,͵W͑x,p͒dx=͗p͉␳ˆ͉p͘,͵W͑x,p͒dp=͗x͉␳ˆ͉x͘,͑30͒and the equivalence to a probability distribution in clas-sical averaging when mean values of a certain class of operators Aˆin a quantum state␳ˆare to be calculated,͗Aˆ͘=Tr͑␳ˆAˆ͒=͵W͑␣͒A͑␣͒d2␣,͑31͒with a function A͑␣͒related to the operator Aˆ.The measure of integration is in our case d2␣=d͑Re␣͒d͑Im␣͒=dxdp with W͑␣=x+ip͒ϵW͑x,p͒,and we shall use d2␣and dxdp interchangeably.The opera-tor Aˆrepresents a particular class of functions of aˆand aˆ†or xˆand pˆ.The marginal distribution for p,͗p͉␳ˆ͉p͘,is obtained by changing the integration variables͑x−y =u,x+y=v͒and using Eq.͑26͒,that for x,͗x͉␳ˆ͉x͘,by using͐exp͑+4iyp͒dp=͑␲/2͒␦͑y͒.The normalization of the Wigner function then follows from Tr͑␳ˆ͒=1.For any symmetrized operator͑Leonhardt,1997͒,the so-called Weyl correspondence͑Weyl,1950͒,Tr͓␳ˆS͑xˆn pˆm͔͒=͵W͑x,p͒x n p m dxdp,͑32͒provides a rule for calculating quantum-mechanical ex-pectation values in a classical-like fashion according to Eq.͑31͒.Here,S͑xˆn pˆm͒indicates symmetrization.For example,S͑xˆ2pˆ͒=͑xˆ2pˆ+xˆpˆxˆ+pˆxˆ2͒/3corresponds to x2p ͑Leonhardt,1997͒.Such a classical-like formulation of quantum optics in terms of quasiprobability distributions is not unique.In fact,there is a whole family of distributions P͑␣,s͒of which each member corresponds to a particular value of a real parameter s,P͑␣,s͒=1␲2͵␹͑␤,s͒exp͑i␤␣*+i␤*␣͒d2␤,͑33͒with the s-parametrized characteristic functions ␹͑␤,s͒=Tr͓␳ˆexp͑−i␤aˆ†−i␤*aˆ͔͒exp͑s͉␤͉2/2͒.͑34͒The mean values of operators normally and antinor-mally ordered in aˆand aˆ†may be calculated via the so-called P function͑s=1͒and Q function͑s=−1͒,re-spectively.The Wigner function͑s=0͒and its character-istic function␹͑␤,0͒are perfectly suited to provide ex-pectation values of quantities symmetric in aˆand aˆ†such as the quadratures.Hence the Wigner function,though not always positive definite,appears to be a good com-promise in describing quantum states in terms of quan-tum phase-space variables such as single-mode quadra-tures.We may formulate various quantum states relevant to continuous-variable quantum communica-tion by means of the Wigner representation.These par-ticular quantum states exhibit extremely nonclassical features such as entanglement and nonlocality.Yet their Wigner functions are positive definite,and thus belong to the class of Gaussian states.518S.L.Braunstein and P.van Loock:Quantum information with continuous variables Rev.Mod.Phys.,Vol.77,No.2,April2005。

电影种类英语作文

电影种类英语作文

When discussing the various genres of films in English,its important to understand the wide range of categories that exist to cater to different tastes and preferences.Here is an overview of some of the most common film genres:1.Action Films:These movies are characterized by fastpaced,thrilling sequences,often involving physical feats,fights,and chases.They usually feature heroes who save the day through their physical prowess.edies:Comedies are designed to make audiences laugh.They can be slapstick, situational,or witty,and often involve humorous dialogue and characters.3.Dramas:Drama films are serious narratives that deal with reallife situations and emotions.They often explore deep themes and character development.4.Horror Films:These films aim to scare and unsettle the audience,often involving supernatural elements,monsters,or psychological terror.5.Science Fiction SciFi:SciFi movies explore imaginative and futuristic concepts,often involving space travel,time travel,or advanced technology.6.Fantasy Films:Fantasy films are set in worlds where magic and supernatural elements are common.They often feature mythical creatures and heroes on grand quests.7.Romance:Romance films focus on the development of a romantic relationship between characters,often culminating in a happy or tragic ending.8.Thrillers:Thrillers keep audiences on the edge of their seats with suspense,tension, and often a race against time to solve a mystery or prevent a disaster.9.Westerns:A genre that originated in the early20th century,Westerns are set in the American Old West and often involve cowboys,lawmen,and outlaws.10.Documentaries:These are nonfiction films that provide a factual record or report on a particular subject,often exploring social,political,or historical issues.11.War Films:War films depict war stories or military history.They can be actionpacked or introspective,focusing on the human side of war.12.Animation:Animated films use a variety of techniques to bring characters and stories to life,often appealing to both children and adults.13.Musicals:Musicals are films that integrate song and dance into the narrative,with characters often expressing their emotions through song.14.Adventure Films:Adventure movies often involve exploration or a quest,with characters facing challenges and obstacles in exotic locations.15.Mystery Films:Mystery films revolve around a puzzle that the characters must solve, often involving a detective or amateur sleuth.16.Biographical Films:These films tell the story of a real persons life,often focusing on significant events or periods in their life.17.Historical Films:Historical films are set in the past and aim to depict historical events, cultures,or people accurately.18.Crime Films:Crime films focus on criminal activities,often involving heists,law enforcement,or the criminal underworld.19.Family Films:Family films are suitable for all ages and often contain themes of adventure,friendship,and moral lessons.20.Superhero Films:Superhero films feature characters with extraordinary abilities, often battling villains to save the world.Each genre has its own conventions and tropes,and filmmakers often blend elements from different genres to create unique and engaging cinematic experiences. Understanding these genres can help you better appreciate the art of filmmaking and the diverse stories that can be told through the medium of film.。

全球化的利弊 英语作文

全球化的利弊 英语作文

Globalization has become an integral part of our lives,connecting people, economies,and cultures across the world.While it offers numerous benefits,it also presents several challenges.Here,we will explore both the advantages and disadvantages of globalization.Advantages of Globalization:1.Economic Growth:Globalization has led to increased trade and investment among nations,which has boosted economic panies can access larger markets, leading to economies of scale and increased efficiency.2.Cultural Exchange:The sharing of ideas,art,and culture across borders has enriched societies and promoted understanding and tolerance among different ethnic groups.3.Technological Advancement:The spread of technology has been accelerated by globalization,allowing for innovations to be shared and adapted worldwide,improving living standards and solving complex problems.4.Job Opportunities:Globalization has created new job opportunities in various sectors, particularly in developing countries,as multinational companies establish operations and supply chains.5.Access to Goods and Services:Consumers now have access to a wider variety of goods and services from around the world,often at competitive prices,due to the reduction of trade barriers.Disadvantages of Globalization:1.Economic Disparity:While some regions and individuals benefit greatly from globalization,others may be left behind,leading to increased economic disparities both within and between countries.2.Cultural Homogenization:The dominance of certain cultures,particularly Western culture,can lead to the erosion of local traditions and identities,as global brands and media influence local tastes and preferences.3.Environmental Impact:The increase in production and transportation for global markets can contribute to environmental degradation,including pollution,deforestation, and climate change.4.Job Displacement:Globalization can lead to job losses in certain sectors,particularly in developed countries,as companies outsource labor to places with lower wages or invest in automation.5.Vulnerability to Global Crises:The interconnectedness of the global economy means that problems in one part of the world can quickly spread,as seen with financial crises or pandemics.Balancing the Pros and Cons:To maximize the benefits of globalization while minimizing its drawbacks,it is essential for governments,businesses,and individuals to work together.This includes implementing policies that protect workers and the environment,fostering sustainable development,and promoting cultural diversity.In conclusion,globalization is a complex phenomenon with farreaching implications.It is not without its challenges,but with careful management and a commitment to fairness and sustainability,it can be a powerful force for positive change in the world.。

尊重他人显素质的英语作文

尊重他人显素质的英语作文

Respecting others is a fundamental aspect of social interaction and a hallmark of good character.It is a quality that not only reflects our upbringing but also our understanding of the world around us.Here are some points to consider when discussing the importance of respecting others in an English essay:1.Understanding Respect:Begin by defining what respect means in the context of social behavior.It can be the acknowledgment of another persons feelings,rights,and dignity.2.Cultural Significance:Discuss how respect is valued across different cultures and societies.It is a universal concept that transcends geographical and cultural boundaries.3.Importance in Relationships:Explain how respect is crucial in building and maintaining healthy relationships,whether they are personal,professional,or social.4.Respect and Communication:Highlight the role of respect in effective communication. It involves listening to others,being empathetic,and avoiding disrespectful language or actions.5.Respecting Differences:Emphasize the importance of respecting individual differences, such as opinions,beliefs,and lifestyles.This includes accepting and valuing diversity.6.Respect and SelfEsteem:Discuss how showing respect to others can also enhance ones selfesteem.When we treat others with respect,we are more likely to receive the same in return,which can boost our selfworth.7.Respect in the Workplace:Elaborate on the significance of respect in a professional environment.It can lead to a more harmonious and productive workplace.8.Teachings and Examples:Mention the teachings of various philosophers,religious texts,or influential figures who have emphasized the importance of respect.9.Consequences of Disrespect:Address the negative outcomes of disrespect,such as damaged relationships,conflict,and a negative reputation.10.Promoting Respect:Offer suggestions on how individuals can promote a culture of respect,such as through education,setting personal examples,and advocating for respectful behavior in all aspects of life.11.Respect and Social Harmony:Conclude by discussing how a society that practices respect can achieve greater social harmony and progress.Remember to use clear and concise language,provide relevant examples,and structure your essay in a logical manner.The conclusion should summarize the main points and reinforce the significance of respecting others in fostering a positive and inclusive society.。

礼仪传承礼仪的英语作文

礼仪传承礼仪的英语作文

In the vast tapestry of human civilization,etiquette plays a pivotal role in shaping our interactions and fostering a harmonious society.The art of etiquette is not merely a set of rules but a reflection of our cultural heritage and values.It is through the practice of etiquette that we demonstrate respect,consideration,and an understanding of social norms.Etiquette has been passed down through generations,evolving with the changing times yet retaining its core principles.It is a universal language that transcends cultural boundaries,promoting mutual respect and understanding among people from diverse backgrounds.In the realm of social interactions,etiquette serves as a guide to appropriate behavior.It encompasses a wide range of practices,from the way we greet others to the manner in which we express gratitude or condolences.For instance,a simple handshake or a bow can convey respect and acknowledgment.Similarly,the act of saying please and thank you is a basic yet powerful way to show politeness and appreciation.In professional settings,etiquette is equally important.It helps establish a positive work environment and facilitates effective communication.Punctuality,active listening,and maintaining a professional demeanor are all aspects of workplace etiquette that contribute to a productive and respectful atmosphere.Dining etiquette is another facet of this tradition that has been passed down through generations.The manner in which we eat,the way we use cutlery,and the customs surrounding mealtime are all part of a rich tapestry of dining practices that vary from one culture to another.These practices not only reflect our cultural identity but also demonstrate our consideration for others at the table.In the digital age,the principles of etiquette have expanded to include online interactions. As we communicate more frequently through digital platforms,it is crucial to apply the same principles of respect and consideration in our online behavior.This includes being mindful of our language,respecting others privacy,and avoiding the spread of misinformation.The transmission of etiquette from one generation to the next is a testament to its enduring value.It is through the teaching of etiquette to children and young adults that we ensure its continuity.Parents,educators,and role models play a crucial role in instilling these values,guiding the youth to navigate social situations with grace and respect.In conclusion,the practice of etiquette is a timeless tradition that enriches our lives and strengthens our communities.It is a bridge that connects us across cultures,fostering understanding and respect.As we continue to pass down the art of etiquette,we uphold the values that have been cherished for centuries and ensure that they remain relevant in our everevolving world.。

SAT写作中关于文化交流的高级词汇

SAT写作中关于文化交流的高级词汇

SAT写作中关于文化交流的高级词汇下面是天道留学搜集整理的SAT写作中关于文化交流的高级词汇:homogeneous 同质的mainstream 主流主流的dialect 方言discrepancy 差异misconception 误解barrier 障碍discrimination 区别,歧视hierarchy 等级制度insularity 岛国性质microcosm 小天地patriot 爱国者compatriot 同胞的vernacular 本地的immigration 移入permeate 渗透,弥漫entrepreneur 企业家practitioner 开业者,从业者proxy 代理人anecdote 轶事notoriety 恶名counterpart 对应人,对等物peer 凝视,窥视subordinate 下级下级的tactics 战术,技巧punctual 准时的,守时的absenteeism 旷工flextime 弹性工作时间harass 骚扰redundancy 冗余,冗员downsize 裁员ballot 投票impartial 不偏不倚的equilibrium 平衡,均衡questionnaire 调查表,问卷quantitative 定量的contingency 偶然性,偶然事件incur 招致ethical 伦理的,符合伦理的dubious 疑惑的,可疑的manifestation 显示,证明subtitle 字幕,副标题dubbing 配音录制vogue 时尚bizarre 奇异的mediocre 平庸的dietitian 饮食学家connoisseur 行家,鉴赏家。

12年新托福测试词汇辅导(9)

12年新托福测试词汇辅导(9)

12年新托福测试词汇辅导(9)disc laser 圆盘形激光器disc of confusion 弥散斑disc storage 磁盘存储器disc type shutter 圆盘快门discerning method 分辨法,鉴别法discernment (1)分辨(2)分辨力discharge (1)释放(2)放电discharge chamber 放电室discharge current noise 放电流噪声discharge excited 放电激发的discharge tube 放电管 www.examw.comdischarger (1)放电器(2)火花隙discoloration 褪色,去色disconnection 分开,断开,断路discontinuity (1)不连续性(2)突变性(3)突变点 discontinuous wave 非连续波discrete (1)分立的(2)离散的discrete channel 离散信道discrete component 分立元件discrete distribution 离散分布discrete energy state 分立能态discrete Fourier transform 离散傅里叶变换discrete maximum principle 离散值原理discrete message 离散信息discrete mode spectrum 离散模谱discrete picture 离散图像discrete random process 离散随权过程discrete signal 离散信号discrete source 离散信源discrete spectrum 离散谱discrete value 分立值discrete-carrier hologram 离散载体全息图discretely tunable infrared laser 不连续可调红外激光器discreteness (1)分位性(2)离散性discriminablility (1)鉴别力(2)鉴频能力。

SAT考试常见互换词汇

SAT考试常见互换词汇

SAT考试常见互换词汇。

留洋网小编吐血整理,希望对各位有所帮助。

十月份的考试近在眼前,考前冲刺不要忽略了词汇的背诵和整理工作。

Important=crucial a.至关紧要的(extremely important), significant (amount or effect large enough to be important)2. Common=universal a.普遍的, ubiquitous adj.普遍存在的(if something is ubiquitous, it seems to be everywhere)3. Abundant=ample (enough and usually extra), plentiful (enough for people’s needs and wants)4. Stick=adhere a.粘附, cling (hold on something tightly)5. Neglect v.忽视=ignore. (Difference: neglect means someone has not paid enough attention to something; ignore means no attention.)6. Near=adjacent (two things next to each other), adjoin (the same as adjacent)7. Pursue=woo (man woos woman, old-fashioned), seek (if you seek sth, you try to obtain it. FORMAL)8. Accurate=precise (precise is exact and accurate in all details), exact (correct in every detail)9. Vague a.含糊的=obscure (unknown or known by only a few people)10. Top=peak, summit点击下载:SAT新版og真题10套全(带答案及解析)pdf11. Competitor=rival, opponent (especially in sports and politics)12. Blame n. /vt.责备,过失 =condemn (if you condemn something, you say it is very bad and unacceptable)13. Opinon=perspective, standpoint (means looking at an event or situation in a particular way)14. Fame=prestige (describe those who are admired), reputation15. Build=erect (you can erect something as buildings, FORMAL), establish16. Insult n. /vt. 侮辱,凌辱=humiliate (do something or say something which makes people feel ashamed or stupid)17. Complain=grumble (complain something in a bad-tempered way)18. Primary=radical (very important and great in degree), fundamental19. Relieve=alleviate (alleviate means you make pain or sufferings less intense or severe)20. Force=coerce sb into (coerce means you make someone do something s/he does not want to), compel21. Enlarge=magnify (magnify means make something larger than it really is)22. Complex=intricate (if something is intricate, it often has many small parts and details)23. Lonely=solitary a. 孤独的 (if someone is solitary, there is no one near him/her)24. Small=minuscule (very small), minute25. Praise=extol (stronger than praise), compliment (polite and political)26. hard-working=assiduous (someone who is assiduous works hard or does things very thoroughly)27. Difficult=arduous (if something is arduous, it is difficult and tiring, and involves a lot of efforts)28. Poor (soil) =barren n.荒地, infertile (used to describe the soil is so poor that plants cannot be planted on it)29. Fragile=brittle a.易碎的,脆弱的, vulnerable (someone who is vulnerable is easily hurt emotionally or physically)30. Show=demonstrate (to demonstrate a fact means to make it clear to people.)31. Big=massive (large in size, quantity, or extent), colossal (use this word, you emphasize something is large), tremendous (INFORMAL)32. avoid=shun(if someone shuns something, s/he deliberately a.故意的 avoid that something or keep away from it.)33. Fair=impartial (someone who is impartial is able to give a fair opinion or decision on something.)34. Attack=assault (physically attack someone), assail (attack violently)35. Dislike=abhor (abhor means you hate something to a extreme extent for moral reasons), loathe (dislike very much)36. ruin v.使破产,使毁灭 n.毁灭=devastate(it means damage something very badly, or utterlya.完全的,彻底的 destroy it.)37. Disaster=catastrophe (a catastrophe is an unexpected event that cause great suffering and damages)38. finally=eventually(especially after a lot of delays), ultimately adv.最后,终于(after complicated series of events)39. Always=invariably (the same as always, but better than always)40. Forever=perpetual (a perpetual state never changes), immutable (something immutable will never change or be changed)41. Surprise=startle (it means surprise you slightly), astound (surprise you to a large degree), astonish (the same as astound)42. Enthusiasm n.狂热,热心=zeal(a great enthusiasm), fervency(sincere a.诚挚,真诚and enthusiasm)43. Quiet=tranquil (calm and peaceful), serene (calm and quiet)44. Expensive=exorbitant (it means too expensive that it should be)45.luxurious=lavish adj.浪费的 vt.浪费,慷慨给与(impressive and very expensive), sumptuous(grand and very expensive)46. Boring=tedious (if you describe something tedious, you mean it is boring and frustrating)47. Respect=esteem (if you esteem someone, you respect and admire v.赞美him/her. FORMAL)48. Worry=fret (if you fret about something, you worry about it)49. Cold=chilly a.寒冷的(unpleasantly cold), icy (extremely cold)50. Hot=boiling (very hot)51. Dangerous=perilous (very dangerous), hazardous (dangerous, especially to people’s safety and health)52. Nowadays=currently53. Only=unique (the only one of its kind), distinctive a.与众不同的54. Stop=cease (if something ceases, it stops happening or existing)55. Part=component (the components of something are the parts that it is made of)56. Result=consequence (the results or effects of something)57. Obvious=apparent, manifest a.显然的58. Based on=derived from 得自, 由来, 衍生59. Remarkable=conspicuous (if something is conspicuous a.显著的, people can see or notice them very easily)60. Quite=fairly61. Pathetic=lamentable (very uncomfortable and disappointing)62. Field=domain (a particular field of thought, activities or interest)63. Appear=emerge (come into existence)64. Whole=entire (the whole of something)65. Wet=moist (slightly wet), damp (slightly wet), humid (very damp and hot)66. Difficult=formidable68. Change=convert (change into another form)69. Typical=quintessential (this word means represent a typical example of something)70. Careful=cautious (very careful in order to avoid danger), prudent (careful and sensible)71. Ability=capacity, capability (the same as ability)72. Strange=eccentric (if some one is eccentric, s/he behaves in a strange way, or his/her opinion is different from most people)73. Rich=affluent (if you are affluent, you have a lot of money)74. Use=utilize (the same as use)75. Dubious=skeptical (if you are skeptical about something, you have doubts on it.)76. Satisfy=gratify (if you are gratified by something, it gives you pleasure and satisfaction)77. Short=fleeting, ephemeral (if something is ephemeral, it lasts a short time)78. Scholarship=fellowship79. Angry=enraged (extremely angry)80. Smelly=malodorous (used to describe an unpleasant smell)81. Ugly=hideous (if something is hideous, it is very ugly or unattractive)82. Attractive=appealing (pleasing and attractive), absorbing (something absorbing can attract you a great deal)83. Diverse=miscellaneous (a miscellaneous groups consists of many different kinds of things)84. Disorder n.杂乱,混乱 v.扰乱=disarray v.混乱, chaos n.混乱,混沌85. Crazily=frantically (used to describe someone who behaves in a wild and uncontrolled way)86. Rapid=meteoric (ATTENTION: meteoric is only used to describe someone achieves success quickly)87. Ordinary=mundane (very ordinary and not at interesting or unusual)88. Despite prep.尽管=notwithstanding (FORMAL)89. Best=optimal (used to describe the best level something can achieve)90. Sharp=acute (severe adj.严厉的,剧烈的and intense)91. Unbelievable=inconceivable (if you deem something inconceivable, you think it very unlike to happen)92. Puzzle=perplex (something perplex someone means it confuses and worries him/her because he/she does not understand it)93. Method=avenue (a way of getting something done)94. Famous=distinguished (used to describe people who are successful in their career)95. Ancient=archaic (extremely old and extremely old-fashioned)96. Decorate=embellish (embellish means make something look more attractive via decorating it with something else)97. Possible=feasible (if something is feasible, it can be done, made or achieved)98. So=consequently, accordingly99. Rare=infrequent (does not happen often)100. Greedy=rapacious (greedy and selfish)短语101. In my opinion=from my perspective102. Very much=a great deal103. For example=to give a demonstration104. However=as a matter of fact, it is the other way around105. Agree with=uphold (support and maintain v.维持,主张)106. be full of=be saturated with (be filled with sth completely)107. By=via108. According to=in the light of109. When it comes to=in terms of110. From a XXX perspective=in XXX sense111. Find a job=land a job112. Latest=up to date113. Achieve a goal=attain an accomplishment114. At the same time=simultaneously115. At the start of=on the threshold of 在……的开头,在……的前夕116. Certainly=to a certain extent117. Without doubt=indubitably adv.无疑地118. In XXX means=via XXX avenue119. Disagree with=be the last one to uphold 120. As fast as=apace with. .。

数学专业英语翻译2-3

数学专业英语翻译2-3
我们用专用记号来表示x是S的元素或者x属于S。如果x不属于
S,我们记为。
如果方便,我们可以用在大括号中列出元素的方式来表示集合。 例如,小于10的正偶数的集合表示为{2,4,6,8},而所有正偶数 的集合表示为{2,4,6,…}, 三个圆点表示 “等等”。
The dots are used only when the meaning of “and so on” is clear. The method of listing the members of a set within braces is sometimes referred to as the roster notation.
In fact, the empty set contains no elements, whereas the set has one element. Sets consisting of exactly one element are sometimes called one-element sets.
一个给定的集合S可以产生新的集合,这些集合叫做S的子集。 例如,由可被4除尽的并且小于10的正整数所组成的集合是 小于10的所有偶数所组成集合的子集。一般来说,我们有如 下定义。
In all our applications of set theory, we have a fixed set S given in advance, and we are concerned only with subsets of this given set. The underlying set S may vary from one application to another; it will be referred to as the universal set of each particular discourse. (35页第二段)
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Байду номын сангаас
I{i: k + 1 5 i 5 n - k,zflL = u1,zi = b , ~ ia = ~ } a+ + Ur
ISIT 2003,Yokohama,Japan,June 29 -July 4, 2003
Universal Discrete Denoising: Known Channel
Tsachy Weissman13, Erik Ordentlich', Gadiel Seroussi' , Sergio Verdii2 and Marcel0 Weinbergerl emails: , , , verdu@, marcelo@ Finite-alphabet signals corrupted by discrete noisy chan- for k 1 5 i 5 n - k (the value at i 5 k and i > n - k is nels arise naturally in a wide range of applications span- arbitrarily-assigned), where X " l k ( ~ n ) denotes the i-th coor[i] ning many fields of science and engineering. In the Shan- dinate of X n V k ( z n ) . Finally, for a given sequence {kn) (which non paradigm, redundancy is added t o the noiseless signal will be specified below) we let, for each n , XrniV X n i k n .A = in order t o protect it from the channel noise, and a decoder natural implementation of the denoising algorithm makes two that knows the codebook and the channel statistics can re- passes through the observations z". The counts m(zn,u1, U,.) cover the noiseless signal with arbitrary reliability, provided are accumulated and stored in the first pass while the actual that the coding scheme respects the fundamental limits of in- denoising is performed in the second pass. This can be shown formation theory. In contrast, there are many applications t o require a linear number of register-level operations and subwhere no channel coding is performed and the recovery of the linear working storage size relative t o the input data length. corrupted signal can only be accomplished with a certain disIn order t o state the optimality results of the DUDE we tortion. Examples include typing correction, hidden Markov need the following definitions: Let L R , (z", 2") denote the model state estimation, DNA sequence analysis, image en- normalized cumulative loss, as measured by A, of the denoiser hancement, pattern recognition, blind equalization, and joint Xn when the observed seauence is Z" E A" and the underlvinn" source-channel decoding, t o name a few. A unzversal dis- one is Z" E A", i.e., Lk,, (z", = z") A(zi, X " ( z " ) [ i ] ) . crete denoiser is a scheme that (asymptotically) attains the We define the k-th order sliding-window minimum loss by optimum distribution-dependent performance with no a priori knowledge of the source statistics. Despite the importance of the problem, there is no universal discrete denoiser available in the literature. Furthermore, some of the denoising By Semi-Stochastic Setting we refer t o the case where x is schemes that have been suggested for the universal setting are not practical in that their complexity grows exponentially a n individual sequence and Z is its noise-corrupted version, with the size of the noisy data. The main contribution of this i.e., Z is the output of the memoryless channel, II, whose work is a discrete universal denoiser (DUDE) that attains o p input is x. In the statement of the following result we assume timum (distribution-dependent) performance with computa- the semi-stochastic setting. tional complexity that grows linearly with the data size. Theorem 1 For all x E A", the sequence of denoisers with limn+m k, = co satisfies We shall assume (cf. [l]for a discussion of the more gen- {XfniV} eral case) that the components of the clean, as well as of the n-oo [ L R ~ ~ JZ") - Dk,(Zn, lim Z~, Z")] = O a s . , noise-corrupted signal, take their values in the same M-ary alphabet A = {I,. . . , M } , that the corruption mechanism provided k,MZkn = o(n/ logn). is a discrete memoryless channel (DMC) represented by the Assume now that the noiseless signal is a stationary 3 (II(i,j) denoting the probability matrix I = { I I ( i , j ) } z , j e ~ of a channel output symbol j when the input is 2) which is stochastic process X. Letting Pxn , fi denote, respecknown and invertible, and that there is a given loss function tively, the distributions of X", X, and V,, denote the A : d ---t [0, co),represented by the matrix A = { A ( i , j ) } a , , E ~ class of all n-block denoisers, we define D ( P p , n ) = ' (A(i,j) denoting the loss incurred by estimating the sym- minknEDnE L 2 , , ( X n ,Z"), the expectation on the right side " bol i with the symbol j ) . We let 7ra denote the i-th col- assuming that X " N PXn and that 2 is the noisy obumn of n, and A, denote the j-th column of A. Hence, servation of X" (corrupted by the DMC n). Define now (where the limit can be II = [7r1 1 ... 1 7 r ~ ] * A = (A1 1 . . . 1 A,]. , An n-block de- D ( P x , n ) = l i m , + , D ( P p , n ) noiser is a mapping X" : A" + A". We now describe the shown t o exist by subadditivity). By definition, D ( P x , I l ) is DUDE: For 2k < n and ul, U,. E Ak let m(z", ul, U,.) de- the (distribution-dependent) optimum asymptotic denoising note the M-dimensional column vector whose b-th compo- performance attainable when the noiseless signal is emitted by the source PX and corrupted by the channel II. nent, /3 E d,is given by
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