Corpus description.
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Released this past November, the list is based on data collected from the Web of Science and highlights some of the world’s most influential scientific minds by naming the researchers whose publications over the previous decade have included a high number of Highly Cited Papers placing them among the top 1% most-cited.
\\n\\nWe wish to congratulate all of the researchers named and especially our authors on this amazing accomplishment! We are happy and proud to share in their success!
Note: Edited in March 2021
\\n"}]',published:!0,mainMedia:{caption:"Highly Cited",originalUrl:"/media/original/117"}},components:[{type:"htmlEditorComponent",content:'IntechOpen is proud to announce that 191 of our authors have made the Clarivate™ Highly Cited Researchers List for 2020, ranking them among the top 1% most-cited.
\n\nThroughout the years, the list has named a total of 261 IntechOpen authors as Highly Cited. Of those researchers, 69 have been featured on the list multiple times.
\n\n\n\nReleased this past November, the list is based on data collected from the Web of Science and highlights some of the world’s most influential scientific minds by naming the researchers whose publications over the previous decade have included a high number of Highly Cited Papers placing them among the top 1% most-cited.
\n\nWe wish to congratulate all of the researchers named and especially our authors on this amazing accomplishment! We are happy and proud to share in their success!
Note: Edited in March 2021
\n'}],latestNews:[{slug:"intechopen-supports-asapbio-s-new-initiative-publish-your-reviews-20220729",title:"IntechOpen Supports ASAPbio’s New Initiative Publish Your Reviews"},{slug:"webinar-introduction-to-open-science-wednesday-18-may-1-pm-cest-20220518",title:"Webinar: Introduction to Open Science | Wednesday 18 May, 1 PM CEST"},{slug:"step-in-the-right-direction-intechopen-launches-a-portfolio-of-open-science-journals-20220414",title:"Step in the Right Direction: IntechOpen Launches a Portfolio of Open Science Journals"},{slug:"let-s-meet-at-london-book-fair-5-7-april-2022-olympia-london-20220321",title:"Let’s meet at London Book Fair, 5-7 April 2022, Olympia London"},{slug:"50-books-published-as-part-of-intechopen-and-knowledge-unlatched-ku-collaboration-20220316",title:"50 Books published as part of IntechOpen and Knowledge Unlatched (KU) Collaboration"},{slug:"intechopen-joins-the-united-nations-sustainable-development-goals-publishers-compact-20221702",title:"IntechOpen joins the United Nations Sustainable Development Goals Publishers Compact"},{slug:"intechopen-signs-exclusive-representation-agreement-with-lsr-libros-servicios-y-representaciones-s-a-de-c-v-20211123",title:"IntechOpen Signs Exclusive Representation Agreement with LSR Libros Servicios y Representaciones S.A. de C.V"},{slug:"intechopen-expands-partnership-with-research4life-20211110",title:"IntechOpen Expands Partnership with Research4Life"}]},book:{item:{type:"book",id:"5265",leadTitle:null,fullTitle:"Metallic Glasses - Formation and Properties",title:"Metallic Glasses",subtitle:"Formation and Properties",reviewType:"peer-reviewed",abstract:"Metallic glasses and amorphous materials have attracted much more attention in the last two decades. A noncrystalline solid produced by continuous cooling from the liquid state is known as a glass. From the other point of view, a noncrystalline material, obtained by any other process, for example, vapor deposition or solid-state processing methods such as mechanical alloying, but not directly from the liquid state, is referred to as an amorphous material. At this moment, bulk metallic glasses (BMG) are appearing as a new class of metallic materials with unique physical and mechanical properties for structural and functional usage. Extreme values of strength, fracture toughness, magnetic properties, corrosion resistance, and other properties have been registered in BMG materials.",isbn:"978-953-51-2512-9",printIsbn:"978-953-51-2511-2",pdfIsbn:"978-953-51-6667-2",doi:"10.5772/61764",price:119,priceEur:129,priceUsd:155,slug:"metallic-glasses-formation-and-properties",numberOfPages:178,isOpenForSubmission:!1,isInWos:null,isInBkci:!1,hash:"53998537d86484c3c753b5af0d11595a",bookSignature:"Behrooz Movahedi",publishedDate:"August 17th 2016",coverURL:"https://cdn.intechopen.com/books/images_new/5265.jpg",numberOfDownloads:11872,numberOfWosCitations:13,numberOfCrossrefCitations:10,numberOfCrossrefCitationsByBook:1,numberOfDimensionsCitations:19,numberOfDimensionsCitationsByBook:1,hasAltmetrics:0,numberOfTotalCitations:42,isAvailableForWebshopOrdering:!0,dateEndFirstStepPublish:"November 4th 2015",dateEndSecondStepPublish:"November 25th 2015",dateEndThirdStepPublish:"February 29th 2016",dateEndFourthStepPublish:"May 29th 2016",dateEndFifthStepPublish:"June 28th 2016",currentStepOfPublishingProcess:5,indexedIn:"1,2,3,4,5,6,7",editedByType:"Edited by",kuFlag:!1,featuredMarkup:null,editors:[{id:"92198",title:"Dr.",name:"Behrooz",middleName:null,surname:"Movahedi",slug:"behrooz-movahedi",fullName:"Behrooz Movahedi",profilePictureURL:"https://mts.intechopen.com/storage/users/92198/images/2100_n.jpg",biography:"Dr. Behrooz Movahedi obtained his PhD degree in Materials Engineering\r\nat Isfahan University of Technology (IUT) in Iran in 2010.\r\nDuring t his period, while on a sabbatical l eave he visited the\r\nSchool of Materials Science and Engineering in Nanyang Technological\r\nUniversity (NTU) in Singapore. After that he joined the Department of Nanotechnology Engineering in the University of Isfahan (UI) as an Associate Professor.\r\nRecently, he is the head of the Nanotechnology Engineering Department in Faculty of Advanced Sciences and Technologies. Dr. Behrooz Movahedi has over 10 years of experience in the nanotechnology, amorphous materials, optical ceramics, and advanced thermal spray coatings for environmental and industrial applications. He was invited as a reviewer in some potential ISI journals such as Materials & Design, Journal of Alloys and Compounds, Surface and Coatings Technology, Applied Surface Science, Journal of Materials Engineering and Performance, Materials Science & Engineering B...",institutionString:null,position:null,outsideEditionCount:0,totalCites:0,totalAuthoredChapters:"2",totalChapterViews:"0",totalEditedBooks:"1",institution:{name:"University of Isfahan",institutionURL:null,country:{name:"Iran"}}}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,coeditorOne:null,coeditorTwo:null,coeditorThree:null,coeditorFour:null,coeditorFive:null,topics:[{id:"944",title:"Metallurgy",slug:"metals-and-nonmetals-metallurgy"}],chapters:[{id:"50742",title:"Metallic Glasses from the Bottom-up",doi:"10.5772/63514",slug:"metallic-glasses-from-the-bottom-up",totalDownloads:1842,totalCrossrefCites:0,totalDimensionsCites:1,hasAltmetrics:0,abstract:"The main challenge in understanding the relation between the structure and properties of metallic glasses is describing their structure at the atomic level. Currently, their structures are considered simply disordered and indeed our understanding of their structure is as undefined as this term. Following the most advanced structural models of metallic glasses that are based on metal clusters, a bottom-up approach to fabrication of metallic glasses using cluster beam technology is introduced. Using metal clusters to fabricate metallic glasses from the bottom-up, that is, formation of cluster-assembled metallic glasses, provides us with the possibility of varying their structure at the atomic level while keeping their composition unchanged. A unique feature working with cluster-assembled metallic glasses is the independent control of their structure and composition. The advantages of this approach are presented, and its potential toward the resolution of structure–property puzzle in metallic glasses is demonstrated along with the main challenges.",signatures:"Aras Kartouzian and Jerzy Antonowicz",downloadPdfUrl:"/chapter/pdf-download/50742",previewPdfUrl:"/chapter/pdf-preview/50742",authors:[{id:"181509",title:"Dr.",name:"Aras",surname:"Kartouzian",slug:"aras-kartouzian",fullName:"Aras Kartouzian"},{id:"185249",title:"Dr.",name:"Jerzy",surname:"Antonowicz",slug:"jerzy-antonowicz",fullName:"Jerzy Antonowicz"}],corrections:null},{id:"51656",title:"Structural and Dynamical Properties of Metallic Glassy Films",doi:"10.5772/64107",slug:"structural-and-dynamical-properties-of-metallic-glassy-films",totalDownloads:1347,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"In this chapter, a series of molecular dynamics simulations have been carried out to explore structural and dynamical features of monatomic liquid metallic films during rapid cooling. Results show a semi‐ordered inhomogeneous morphology containing crystal‐like and disordered regions. The icosahedron contributes to nucleation through the synergy with other short‐range ordered structures and participates in crystal growth via assimilation, but the pinning effect should be overcome. The second‐peak splitting in pair correlation functions is found as the result of a statistical average of crystal‐like and disordered structural regions, not just the amorphous structure. The splitting can be viewed as a prototype of crystal‐like peaks exhibiting distorted and vestigial features. Besides, we use the parameter P(a, τ, ν) for predicting both local structural order and motion propensity. The fraction of crystalline clusters follows a negative power‐law scaling with the cooling rate increasing, which is the inverse of P(a, τ, ν).",signatures:"Hui Li, Weikang Wu and Kun Zhang",downloadPdfUrl:"/chapter/pdf-download/51656",previewPdfUrl:"/chapter/pdf-preview/51656",authors:[{id:"6986",title:"Prof.",name:"Hui",surname:"Li",slug:"hui-li",fullName:"Hui Li"},{id:"185755",title:"Dr.",name:"Weikang",surname:"Wu",slug:"weikang-wu",fullName:"Weikang Wu"},{id:"185756",title:"Dr.",name:"Kun",surname:"Zhang",slug:"kun-zhang",fullName:"Kun Zhang"}],corrections:null},{id:"51226",title:"Structure of the Metallic Glass and Evolution of Electronical Properties during Glass Transition in Atomic Level",doi:"10.5772/63676",slug:"structure-of-the-metallic-glass-and-evolution-of-electronical-properties-during-glass-transition-in-",totalDownloads:1267,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"Metallic glass (MGs) has many unique properties such as low density, low Young's modulus, and so on. These unique physical and mechanical properties attract much attention on their application in manufacturing production. While, structural properties such as complete absence of the long‐range order and most MGs are consist of equal or more than ternary constituent which complex factors make that the atomic level structure of metallic glass still have not well known by researchers. The limited methods and data sets obtained by experiment make the acknowledge in uncovering atomic structure of melt states of alloy, and the supercooled liquid about the alloy is absent as well. These messages are important to improve and increase the understanding of MGs, as we know that glasses are essentially frozen liquid made by quenching of their high‐temperature melts. Computer simulation method is an useful tool to obtain structure messages of melt and the supercooled liquid. The static, dynamical properties as a function of temperature can also be investigated by ab initio MD simulation. The atomic level rearrangement consists of both local topological structure change and chemical reordering and evolution of electronic properties of the Al87Ni7Nd6 and Ca50Mg20Cu30 alloy during the glass transition process is investigated, and the discussion of the results is given in this chapter.",signatures:"HaiJun Chang",downloadPdfUrl:"/chapter/pdf-download/51226",previewPdfUrl:"/chapter/pdf-preview/51226",authors:[{id:"183096",title:"Dr.",name:"Chang",surname:"Haijun",slug:"chang-haijun",fullName:"Chang Haijun"}],corrections:null},{id:"51475",title:"Corrosion Resistance and Electrocatalytic Properties of Metallic Glasses",doi:"10.5772/63677",slug:"corrosion-resistance-and-electrocatalytic-properties-of-metallic-glasses",totalDownloads:2783,totalCrossrefCites:4,totalDimensionsCites:10,hasAltmetrics:0,abstract:"Metallic glasses exhibit excellent corrosion resistance and electrocatalytic properties, and present extensive potential applications as anticorrosion, antiwearing, and catalysis materials in many industries. The effects of minor alloying element, microstructure, and service environment on the corrosion resistance, pitting corrosion, and electrocatalytic efficiency of metallic glasses are reviewed. Some scarcities in corrosion behaviors, pitting mechanism, and eletrocatalytic reactive activity for hydrogen are discussed. It is hoped that the overview is beneficial for some researcher paying attention to metallic glasses.",signatures:"Shanlin Wang",downloadPdfUrl:"/chapter/pdf-download/51475",previewPdfUrl:"/chapter/pdf-preview/51475",authors:[{id:"182701",title:"Prof.",name:"Shanlin",surname:"Wang",slug:"shanlin-wang",fullName:"Shanlin Wang"}],corrections:null},{id:"51279",title:"Structure and Mechanical Behaviour of Cu‐Zr‐Ni‐Al Amorphous Alloys Produced by Rapid Solidification",doi:"10.5772/63513",slug:"structure-and-mechanical-behaviour-of-cu-zr-ni-al-amorphous-alloys-produced-by-rapid-solidification",totalDownloads:1374,totalCrossrefCites:1,totalDimensionsCites:1,hasAltmetrics:0,abstract:"The amorphous ribbons of Cu50Zr40Ni5Al5 alloy were manufactured by rapid solidification. The ribbons were investigated by X‐ray diffraction (XRD), scanning electron microscopy coupled with energy dispersive spectroscopy (SEM‐EDX) and differential scanning calorimetry (DSC). The activation energy of the crystallisation in amorphous alloys was determined by Kissenger technique. The mechanical properties of the ribbons were characterized using Vickers microhardness (HV) tester. According to the XRD and SEM results, the Cu50Zr40Ni5Al5 alloys have a fully amorphous structure. The EDX analysis of the ribbons showed that compositional homogeneity of the Cu50Zr40Ni5Al5 alloy was fairly high. From the DSC curves of the amorphous ribbons, it was determined that glass transition temperature (Tg) is around 440–442°C and super‐cooled liquid region (ΔTx = Tx - Tx) before crystallisation is around 61–64°C. The microhardness of the as‐quenched ribbons was measured about 550 HV. However, this microhardness value decreased with increasing annealing temperature and it was calculated about 465 HV after annealing temperature of 800°C.",signatures:"Celal Kursun and Musa Gogebakan",downloadPdfUrl:"/chapter/pdf-download/51279",previewPdfUrl:"/chapter/pdf-preview/51279",authors:[{id:"181811",title:"Ph.D.",name:"Celal",surname:"Kurşun",slug:"celal-kursun",fullName:"Celal Kurşun"},{id:"182484",title:"Prof.",name:"Musa",surname:"Gogebakan",slug:"musa-gogebakan",fullName:"Musa Gogebakan"}],corrections:null},{id:"51549",title:"Mechanical Behavior of Zr-Based Metallic Glasses and Their Nanocomposites",doi:"10.5772/64221",slug:"mechanical-behavior-of-zr-based-metallic-glasses-and-their-nanocomposites",totalDownloads:1913,totalCrossrefCites:4,totalDimensionsCites:5,hasAltmetrics:0,abstract:"In the present chapter, results of our recent investigations on the role of gallium (Ga) on the aluminum (Al) site in Zr69.5Al7.5-xGaxCu12Ni11 metallic glass (MG) composition have been discussed. The material tailoring and cooling rate effects on the mechanical behavior of Zr-based metallic glasses and their nanocomposites have been studied. The substitution of Ga on the Al site in Zr–Al–Cu–Ni alloy affects the nucleation and growth characteristics of quasicrystals (QCs) and consequently changes the morphology of nanoquasicrystals. The Zr69.5Al7.5-xGaxCu12Ni11 system displayed metallic glass formation in the range of x = 0–7.5. In this process, we have come out with a new glass composition; Zr-Ga-Cu-Ni with glass transition temperature (Tg)—614 K. The effect of cooling rate on the glass forming ability (GFA) and mechanical properties for this new metallic glass composition has been discussed and compared with some other Zr-based metallic glasses. The various indentation parameters such as microhardness, yield strength, strain hardening constant, nature of shear band formation, and so on for the alloys have been analyzed. The study is focused on investigations of these materials to understand the structure (microstructure) property correlations.",signatures:"Devinder Singh, R.K. Mandal, R.S. Tiwari and O.N. Srivastava",downloadPdfUrl:"/chapter/pdf-download/51549",previewPdfUrl:"/chapter/pdf-preview/51549",authors:[{id:"106764",title:"Prof.",name:"Rajiv Kumar",surname:"Mandal",slug:"rajiv-kumar-mandal",fullName:"Rajiv Kumar Mandal"},{id:"184180",title:"Dr.",name:"Devinder",surname:"Singh",slug:"devinder-singh",fullName:"Devinder Singh"},{id:"184181",title:"Prof.",name:"R.S.",surname:"Tiwari",slug:"r.s.-tiwari",fullName:"R.S. Tiwari"},{id:"184182",title:"Prof.",name:"O.N.",surname:"Srivastava",slug:"o.n.-srivastava",fullName:"O.N. Srivastava"}],corrections:null},{id:"51366",title:"On the Prospects of Using Metallic Glasses for In-vessel Mirrors for Plasma Diagnostics in ITER",doi:"10.5772/63885",slug:"on-the-prospects-of-using-metallic-glasses-for-in-vessel-mirrors-for-plasma-diagnostics-in-iter",totalDownloads:1347,totalCrossrefCites:1,totalDimensionsCites:2,hasAltmetrics:0,abstract:"This chapter reviews main results obtained on mirror-like samples made of several grades of bulk metallic glasses (BMG). Experiments were carried out under simulated conditions typical for the operation of plasma facing in-vessel mirrors of optical plasma diagnostics in fusion reactor ITER. Bombardment with D0 and T0 atoms radiated from burning plasma was predicted to be the main reason for the degradation of optical properties of such mirrors. Therefore, to simulate the behavior of mirrors in ITER, mirror-like samples were subjected to bombardment by ions of deuterium plasma with fixed or wide energy distribution. The effects of ion bombardment on optical properties, development of roughness, uptake of deuterium, appearance of blisters, and manifestation of some chemical processes are presented and discussed.",signatures:"Vladimir S. Voitsenya, Alexandra F. Bardamid, Martin Balden, Flaviu Gostin, Sergey V. Khovrich, Vladimir G. Konovalov, Konstantin V. Kovtun, Petro M. Lytvyn, Sergey V. Ketov, Dmitri V. Luzguine-Luzgin, Sergei I. Solodovchenko, Anatoly N. Shapoval, Anatoly F. Shtan’, Vladislav N. Bondarenko, Ivan V. Ruzhkov, Ol’ga O. Skoryk and Andrei A. Vasil’ev",downloadPdfUrl:"/chapter/pdf-download/51366",previewPdfUrl:"/chapter/pdf-preview/51366",authors:[{id:"183133",title:"Dr.",name:"Vladimir",surname:"Voitsenya",slug:"vladimir-voitsenya",fullName:"Vladimir Voitsenya"}],corrections:null}],productType:{id:"1",title:"Edited Volume",chapterContentType:"chapter",authoredCaption:"Edited by"},subseries:null,tags:null},relatedBooks:[{type:"book",id:"3817",title:"Developments in Corrosion Protection",subtitle:null,isOpenForSubmission:!1,hash:"8ff86fac7ac8bce142fdc3c0e5a79f30",slug:"developments-in-corrosion-protection",bookSignature:"M. 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We start by providing a discussion on Bayesian learning and the reasons behind choosing BART among another classifiers, then we illustrate the technical details of BART. BART is a Bayesian approach, thus it inherits all the advantages from Bayesian learning. There are various advantages of Bayesian learning when compared to other statistical approaches. As opposed to the frequentist approach for defining the probability of an uncertain event, here one needs a record of past information of an event. Yet, if this information is not available, then the frequentist approach cannot be used to define the degree of belief in the uncertain event. On the other hand, the Bayesian approach allows us to reason about beliefs under conditions of uncertainty. Thus, it helps in modeling uncertainty in a probabilistic way (Neal, 1995). In addition, Bayesian inference is regarded as a good approach to tackle the problem of data modeling (Kandola, 2001). A model is designed for a particular application and adapted according to the data while the data arrives from the application. The model then provides a representation of the prior beliefs about the application and the information derived from the data (Bishop, 1995).
Another advantage of the Bayesian approach is that one does not need to update the model entirely when acquiring new knowledge. Yet, the new data can be used to update the current model instead of re-fitting the entire model. This feature comes handy especially in phishing detection since phishing attacks change frequently and vastly to lure filters and detection mechanisms. Assuming that one needs to re-fit the entire model when new batch of emails arrives, the procedure becomes very computationally extensive and time consuming, thus impractical.
Furthermore, BART is a model-based Bayesian approach. As opposed to to those algorithm-based learning methods, model-based approaches can provide full and accurate assessment of uncertainty in predictions, while remaining highly competitive in terms of predictive accuracy. In addition, model-based approaches are considered non-greedy, hence opposed to selecting the best solution at the time being and not worrying about the future (i.e. whether the solution is efficient or not), the solution is interchangeable accordingly. Also, model-based approaches are non-adhoc, hence the provided solution is not only selected to a particular problem; however, it can be used as a general case.
BART automatically selects variables from a large pool of input predictors, while searching for models with highest posterior probabilities for future prediction, via a backfitting Markov chain Monte Carlo (MCMC) algorithm (see section 3.1 for further details). Compared to other Bayesian methods, such as Naive Bayes and Bayesian Networks, the latter approaches require variable selection to be done separately, otherwise they use all the variables supplied for training, thus the performance of the classifier will be very poor. Also, it is well known that variable selection in a high dimensional space is a very difficult problem that often requires intensive computations. As we mentioned earlier, phishing emails change regularly and vastly to lure detection mechanisms and the variables may change over time as well. Yet, the above nice feature of BART comes handy when training on newly arriving emails on a regular basis. With no additional requirements to perform variable selection, BART simultaneously accomplishes variable selection during the training phase.
In addition, in phishing detection hundreds of potential features are extracted from raw emails. Only an unknown subset of them are useful for prediction and others are irrelevant. Blindly including all the variables in the step of training often leads to overfitting, and hence predicting new attacks may be poor. However, with the automatic variable selection feature in BART this problem is solved.
Further, many other Bayesian learning approaches require very careful prior specification, and hence extra effort and operational cost in training models. However, BART, as shown in (Chipman et al., 2006), appears to be relatively insensitive to small changes in the prior specification and the choice of the number of trees. According to (Chipman et al., 2006), the default priors work very well, which enables BART to be an objective and automatic training procedure. This is desirable in situations in which there is no prior information available or no human intervention is preferred.
Furthermore, BART is a class of Bayesian additive models with multivariate components of binary trees. Using binary trees as model components makes BART more exible in practice, as opposed to common regression approaches, since the structure of binary trees has been proved to approximate well nonlinear and nonsmooth functional forms in many applications (Hastie et al., 2001).
Also, BART uses a sum-of-trees-model which is more exible than any single tree model that can hardly account for additive effects. Each tree component is regarded as a
Moreover, the rich structure of BART leads to its excellent learning ability, even in the presence of a very complicated structure embedded in data. Since phishing emails look very similar to legitimate emails, actually they are duplicates of legitimate emails with some changes, learning is a challenging problem and perhaps involves discovering an elaborate and subtle relationship from data.
(Chandrasekaran et al., 2006) proposed a technique to classify phishing based on structural properties of phishing emails. They used a total of 25 features mixed between style markers (e.g. the words suspended, account, and security) and structural attributes, such as the structure of the subject line of the email and the structure of the greeting in the body. They tested 200 emails (100 phishing and 100 legitimate). They applied simulated annealing as an algorithm for feature selection. After a feature set was chosen, they used information gain (IG) to rank these features based on their relevance. They applied one-class SVM to classify phishing emails based on the selected features. Their results claim a detection rate of 95% of phishing emails with a low false positive rate.
(Fette et al., 2007) compared a number of commonly-used learning methods through their performance in phishing detection on a past phishing data set, and finally Random Forests were implemented in their algorithm PILFER. Their methods can be used to detect phishing websites as well. They tested 860 phishing emails and 6950 legitimate emails. The proposed method detected correctly 96% of the phishing emails with a false positive rate of 0.1%. They used ten features handpicked for training and their phishing dataset was collected in 2002 and 2003. As pointed out by the authors themselves, their implementation is not optimal and further work in this area is warranted.
(Abu-Nimeh et al., 2007) compared six machine learning techniques to classify phishing emails. Their phishing corpus consisted of a total of 2889 emails and they used 43 features (variables). They showed that, by merely using a
In the literature, there exist several machine learning techniques for binary classification, e.g., logistic regression, neural networks (NNet), binary trees and their derivatives, discriminant analysis (DA), Bayesian networks (BN), nearest neighbor (NN), support vector machines (SVM), boosting, bagging, etc. The interested reader can refer to (Hastie et al., 2001) and the references therein for a detailed overview. Here we describe the application of Bayesian Additive Regression Trees (BART) for learning from data, combined with a probit setup for binary responses, to detect phishing emails.
Most of the machine learning algorithms discussed here are categorized as
Applying any supervised machine learning algorithm to phishing detection consists of two steps: training and classification. During the
Bayesian Additive Regression Trees (BART) is a new learning technique, proposed by (Chipman et al., 2006), to discover the unknown relationship between a continuous output and a dimensional vector of inputs. The original model of BART was not designed for classification problems, therefore, a modified version, hereafter CBART, which is applicable to classification problems in general and phishing classification in particular is used. Note that BART is a learner to predict quantitative outcomes from observations via regression. There is a distinction between regression and classification problems. Regression is the process of predicting quantitative outputs. However, when predicting qualitative (categorical) outputs this is called a classification problem. Phishing prediction is a binary classification problem, since we measure two outputs of email either phishing =1 or legitimate =0 (Hastie et al., 2001).
BART discovers the unknown relationship
each
A binary tree structure
Let
Figure 2 depicts an example of a binary tree in the BART model. Note that the BART contains multiple binary trees, since it is an additive model. Each node in the tree represents a feature in the dataset and the terminal nodes represent the probability that a specific email is phishing, given that it contains certain features. For example, if an email contains HTML code, contains javascript, and the javascript contains form validation, then the probability that this email is phishing is 80% (refer to Figure 2). These features are discussed in more details in Section 4.1.1.
Example of a binary tree.
BART is fully model-based and Bayesian in the sense that a
To specify a
For the
Now given the
Repeat
Sample
Sample
Repeat the above steps
Sample σ given
Since this is a Markov chain, simulation
It is worth mentioning that BART has several appealing features, which make it competitive compared to other learning methods and motivate our study as well. Rather than using a single regression tree, BART uses a sum- of-trees model that can account for additive effects. Also, the binary tree structure helps in approximating well nonlinear and non-smooth relationships (Hastie et al., 2001). Furthermore, BART can conduct automatic variable selection of inputs while searching for models with highest posterior probabilities during MCMC simulation. In addition, by applying Bayesian learning, BART can use newly coming data to update the current model instead of re-fitting the entire model.
Despite the advantages mentioned earlier, it is well known that a Bayesian approach usually brings heavy computation time due to its nature. Predicting the
As mentioned in Section 3.1, BART requires the output variable to be continuous, instead of binary. Let
where
where Φ(·) is the cumulative density function of
Under the above setup of the latent variable
Before we describe the algorithm, let
rather than drawing from
in the original algorithm. A typical draw from the new posterior (5) entails
followed by a draw of
Note that there is no need to draw σ in our new algorithm since it is set to 1.
We proceed to discuss how to implement (6) and (7). First, we claim that the first step is essentially the same as in the original algorithm. This is because in (6), no extra information is given by
As shown above, BART is well suited for binary classification, under the probit setup with the use of the latent variable. In this case, it is even easier than before because σ is no longer an unknown parameter and the draws of
We now briey discuss how to use BART for prediction. In an MCMC run, we can simply pick up the “best”
CART or Classification and Regression Trees (Breiman et al., 1984) is a model that describes the conditional distribution of
CART is exible in practice in the sense that it can easily model nonlinear or nonsmooth relationships. It has the ability of interpreting interactions among predictors. It also has great interpretability due to its binary structure. However, CART has several drawbacks such as it tends to overfit the data. In addition, since one big tree is grown, it is hard to account for additive effects.
Logistic regression is the most widely used statistical model in many fields for binary data (0/1 response) prediction, due to its simplicity and great interpretability. As a member of generalized linear models it typically uses the
where
Logistic regression performs well when the relationship in the data is approximately linear. However, it performs poorly if complex nonlinear relationships exist between the variables. In addition, it requires more statistical assumptions before being applied than other techniques. Also, the prediction rate gets affected if there is missing data in the data set.
A neural network is structured as a set of interconnected identical units (neurons). The interconnections are used to send signals from one neuron to the other. In addition, the interconnections have weights to enhance the delivery among neurons (Marques de Sa, 2001). The neurons are not powerful by themselves, however, when connected to others they can perform complex computations. Weights on the interconnections are updated when the network is trained, hence significant interconnection play more role during the testing phase. Figure 3 depicts an example of neural network. The neural network in the figure consists of one input layer, one hidden layer, and one output layer. Since interconnections do not loop back or skip other neurons, the network is called
Neural Network.
Although competitive in learning ability, the fitting of neural network models requires some experience, since multiple local minima are standard and delicate regularization is required.
Random forests are classi_ers that combine many tree predictors, where each tree depends on the values of a random vector sampled independently. Furthermore, all trees in the forest have the same distribution (Breiman, 2001). In order to construct a tree we assume that
Random forests can handle large numbers of variables in a data set. Also, during the forest building process they generate an internal unbiased estimate of the generalization error. In addition, they can estimate missing data well. A major drawback of random forests is the lack of reproducibility, as the process of building the forest is random. Further, interpreting the final model and subsequent results is difficult, as it contains many independent decisions trees.
Support Vector Machines (SVM) are one of the most popular classifiers these days. The idea here is to find the optimal separating hyperplane between two classes by maximizing the margin between the classes closest points. Assume that we have a linear discriminating function and two linearly separable classes with target values +1 and -1. A discriminating hyperplane will satisfy:
Now the distance of any point
Support Vector Machines.
Though SVMs are very powerful and commonly used in classification, they suffer from several drawbacks. They require high computations to train the data. Also, they are sensitive to noisy data and hence prone to overfitting.
The phishing dataset constitutes of 6561 raw emails. The total number of phishing emails in the dataset is 1409 emails. These emails are donated by (Nazario, 2007) covering many of the new trends in phishing and collected between August 7, 2006 and August 7, 2007. The total number of legitimate email is 5152 emails. These emails are a combination of financial-related and other regular communication emails. The financial-related emails are received from financial institutions such as Bank of America, eBay, PayPal, American Express, Chase, Amazon, AT&T, and many others. As shown in Table 1, the percentage of these emails is 3% of the complete dataset. The other part of the legitimate set is collected from the authors\' mailboxes. These emails represent regular communications, emails about conferences and academic events, and emails from several mailing lists.
Corpus | No. of Emails | Percentage (%) |
---|---|---|
Phishing | 1409 | 21% |
Legitimate (financial) | 178 | 3% |
Legitimate (other) | 4974 | 76% |
Total | 6561 | 100% |
Corpus description.
The analysis of emails consists of two steps: First,
Phishing email after conversion to XML.
Afterwards, each email is converted into a vector
Feature | Binary/Continuous | Value | Description |
---|---|---|---|
1 | binary | 0/1 | class of email, phishing or legitimate |
2-61 | continuous | TF/IDF | frequency of terms |
62 | binary | 0/1 | link mismatch |
63 | binary | 0/1 | URL contains IP |
64 | binary | 0/1 | email contains javascript |
65 | binary | 0/1 | email contains images that link to external server |
66 | binary | 0/1 | email contains from validation |
67 | binary | 0/1 | URL contains non-standard ports |
68 | continuous | maximum total | total number of dots in URL |
69 | continuous | total | total number of links in email |
70 | binary | 0/1 | email contains URL redirection |
71 | binary | 0/1 | email contains URL encoding |
Feature description.
Building the phishing dataset.
As we mentioned earlier we start by stripping all
Thus, we filter out
Textual analysis generates the first 60 features in the dataset and the last 10 features are generated using structural analysis. Unlike textual analysis, here we only strip the attachments of emails keeping HTML tags and elements for further analysis. First, we perform HTML analysis, in which we analyze
Form validation in phishing email.
Similarly, legitimate emails rarely contain
Javascript to validate account number.
Spammers have used images that link to external servers in their emails, also dubbed as
Image linking to an external server.
The second part in structural analysis involves the
When identifying a link mismatch we compare links that are displayed to the user with their actual destination address in the
URL mismatch in link.
A commonly used technique, but easily detected even by naive users, is the use of IP addresses in URLs (i.e. unresolved domain names). This has been and is still seen in many phishing emails. It is unlikely to see unresolved domain names in legitimate emails; however, phishers use this technique frequently, as it is more convenient and easier to setup a phishing site. If the email contains a URL with an unresolved name, then the corresponding feature in the dataset is set to 1, otherwise, it is set to 0. Phishers often trick victims by displaying a legitimate URL and hiding the unresolved address of the phishing site in the
Since phishing sites are sometimes hosted at compromised sites or botnets, they use nonstandard port numbers in URLs to redirect the victim\'s traffic. For example instead of using port 80 for http or port 443 for https traffic, they use different port numbers. If the email contains a URL that redirects to a non-standard port number, then the corresponding feature in the dataset is set to 1, otherwise it is set to 0. Figure 11 shows an example of a phishing URL using a non-standard port number.
Phishing URL using non-standard port number.
We count the number of links in an email. Usually, phishing emails contain more links compared to legitimate ones. This is a commonly used technique in spam detection, where messages that contain a number of links more than a certain threshold are filtered as spam. However, since phishing emails are usually duplicate copies of legitimate ones, this feature might not help in distinguishing phishing from financial-related legitimate emails; however, it helps in distinguishing phishing from other regular legitimate messages.
Since phishing URLs usually contain multiple sub-domains so the URL looks legitimate, the number of dots separating sub-domains, domains, and TLDs in the URLs are usually more than those in legitimate URLs. Therefore, in each email we find the link that has the maximum number of dots. The maximum total number of dots in a link in an email thus is used as a feature in the dataset. Figure 12 shows an example of a Nationwide spoof link. Note the dots separating different domains and sub-domains.
Number of dots in a Nationwide spoof URL.
Phishers usually use open redirectors to trick victims when they see legitimate site names in the URL. Specifically, they target open redirectors in well known sites such as aol.com, yahoo.com, and google.com. This technique comes handy when combined with other techniques, especially URL encoding, as naive users will not be able to translate the encoding in the URL. Figure 13 shows an example of an AOL open redirector.
Open redirector at AOL.
The last technique that we analyze here is URL encoding. URL encoding is used to transfer characters that have a special meaning in HTML during http requests. The basic idea is to replace the character with the “%” symbol, followed by the two-digit hexadecimal representation of the ISO-Latin code for the character. Phishers have been using this approach to mask spoofed URL and hide the phony addresses of these sites. However, they encode not only special characters in the URL, but also the complete URL. As we mentioned earlier, when this approach is combined with other techniques, it makes the probability of success for the attack higher, as the spoofed URL looks more legitimate to the naive user. Figure 14 shows an example of URL encoding combined with URL redirection.
URL encoding combined with URL redirection.
Figure 6 depicts a block diagram of the approach used in building the dataset. It shows both textual and structural analysis and the procedures involved therein.
We use the area under the receiver operating characteristic (ROC) curve (AUC) to measure and compare the performance of classifiers. According to (Huang & Ling, 2005), AUC is a better measure than accuracy when comparing the performance of classifiers. The ROC curve plots false positives (FP) vs. true positives (TP) using various threshold values. It compares the classifiers\' performance across the entire range of class distributions and error costs (Huang & Ling, 2005).
Let
True positives are phishing emails that are classified as phishing, hence the true positive rate (TP) is denoted as:
False negatives are phishing emails that are classified as legitimate, hence the false negative rate (FN) is denoted as:
True negatives are legitimate emails that are classified as legitimate, hence the true negative rate (TN) is denoted as:
Further we evaluate the predictive accuracy of classifiers, by applying the
In addition, we use several other measures to evaluate the performance of classifiers. We use the phishing
We use the AUC as the primary measure, as it allows us to gauge the trade off between the FP and TP rates at different cut-off points. Although the error rate
We optimize the classifiers’ performance by testing them using different input parameters. In order to find the maximum AUC, we test the classifiers using the complete dataset applying different input parameters. Also, we apply
We test NNet using different numbers of units in the hidden layer (i.e. different sizes (
RF is optimized by choosing the number of trees used. Specifically, the number of trees we consider in this experiment is between 30 and 500. When using 50 trees on our dataset, RF achieves the maximum AUC of 95.48%.
We use the L1-SVM C-Classification machine with radial basis function (RBF) kernels. L1SVM can automatically select input variables by suppressing parameters of irrelevant variables to zero. To achieve the maximum AUC over different parameter values, we consider cost of constraints violation values (i.e. the “c” constant of the regularization term in the Lagrange formulation) between 1 and 16, and values of the γ parameter in the kernels between 1 ×10−8 and 2. We find that γ= 0
We use two BART models; the first is the original model and as usual, we refer to this as “BART”. The second model is the one we modify so as to be applicable to classification, referred to as “CBART”. We test both models using different numbers of trees ranging from 30 to 300. Also, we apply different power parameters for the tree prior, to specify the depth of the tree, ranging from 0.1 to 2.5. We find that BART with 300 trees and
In this section we present the experimental results be measuring the AUC using the complete dataset. In addition, we compare the
ROC for all classifiers using the complete dataset.
Table 3 illustrates the AUC, FP, FN,
AUC | P | R | F1 | FP | FN | ||
---|---|---|---|---|---|---|---|
CBART | 99.19% | 4.41% | 97.02% | 88.86% | 92.8% | 2.98% | 11.14% |
NNet | 98.80% | 4.31% | 93.84% | 85.68% | 89.53% | 6.16% | 14.32% |
SVM | 97.18% | 2.39% | 94.57% | 86.23% | 90.17% | 5.43% | 13.77% |
BART | 97.31% | 4.74% | 93.82% | 83.52% | 88.32% | 6.18% | 16.48% |
CART | 96.06% | 7.00% | 88.45% | 77.90% | 82.67% | 11.55% | 22.10% |
RF | 95.48% | 3.68% | 95.75% | 86.80% | 91.02% | 4.25% | 13.20% |
LR | 54.45% | 5.34% | 92.71% | 81.62% | 86.77% | 7.29% | 18.38% |
Classifiers AUC,
In Table 4, we compare
Classifier | p-value |
---|---|
RF | 0.03711 |
SVM | 0.1602 |
NNet | 0.625 |
Comparing the p-value using the Wilcoxon-signed ranked test
Here we investigate the application of a modified version of BART for phishing detection. The results demonstrate that CBART outperforms other classifiers on the phishing dataset, achieving the maximum AUC of 99.19%. The results show that CBART has the highest AUC, followed by NNet with 98.80%, BART with 97.31%, SVM with 97.18%, CART with 96.06%, RF with 95.48%, and LR with 54.45% respectively. Apparently the AUC for CBART has improved by 1.88% compared to the original BART model.
The results show that CBART\'s error rate is comparable to other classifiers (merely RF, SVM, and NNet). When the error rates for the 10 subsamples are compared using the Wilcoxon-singed ranked test, the
SVM achieves the minimum error rate (maximum accuracy) of 2.39%, followed by RF with 3.68%, NNet with 4.31%, CBART with 4.41%, BART with 4.74%, LR with 5.34%, and CART with 7% respectively. Note that the accuracy of CBART has improved, insignificantly though, by 0.33%.
CBART achieves the minimum FP rate of 2.98%, followed by RF with 4.24%, SVM with 5.43%, NNet with 6.16%, BART with 6.18%, LR with 7.29%, and CART with 11.55%. The minimum FN rate is achieved by CBART with 11.14%, followed by RF with 13.20%, SVM with 13.77%, NNet 14.32%, BART 16.48%, LR 18.38%, and CART 22.10% respectively.
It is well known that LR performs very well when the relationship underlying data is linear. We believe that the comparatively low predictive accuracy of LR is an indication of a nonlinear relationship among the features and the response in the dataset.
With its superior classification performance, relatively high predictive accuracy, relatively low FP rate, and distinguished features, CBART proves to be a competitive and a practical method for phishing detection.
A modified version of Bayesian Additive Regression Trees (CBART) proved to be suitable as a phishing detection technique. The performance of CBART was compared against well-known classification methods on a phishing dataset with both textual and structural features.
The results showed that CBART is a promising technique for phishing detection and it has several features that make it competitive. Further, the results demonstrated that the performance of the modified BART model outperforms other well-known classifiers and comparatively achieves low error rate and false positives. CBART outperformed all the other classifiers and achieved the maximum AUC of 99.19% on the phishing dataset we built, decreasing by 1.88% compared to AUC of BART prior to the modification. SVM achieved the minimum error rate of 2.39% leaving behind, RF with 3.68% and NNet with 4.31% followed by CBART with 4.41%. In addition, CBART achieved the minimum FP rate of 2.98% followed by RF with 4.25%, SVM with 5.43%, NNet with 6.16%, and BART with 6.18%.
Automatic variable selection in BART motivates future work to explore BART as a variable selection technique. This includes comparing its performance to other well known variable selection methods.
Liquid crystal display devices are a kind of spatial light modulators (SLMs). SLMs are able to relate electronic data to spatially modulated coherent light. In particular, twisted nematic liquid crystal spatial light modulators (TNLC-SLMs) are kind of relatively low-cost electro-optics devices widely used in many branches of optical information processing, such as digital holography [1, 2], spatially-variant polarized beams [3], coherent diffraction imaging [4], generating vector beams [5, 6, 7], pattern recognition and optical correlators [8], Fresnel lenses [9, 10], and optical cryptosystem [11, 12, 13].
On the other side, highly focused beams and their properties have been investigated in many fields, such as nonlinear optics, super-resolution microscopy, tomography, and optical tweezers [14, 15, 16, 17, 18, 19, 20, 21]. Tightly focused beams attract much attention because of the non-neglectable component of the electric field in the direction of propagation.
Since SLMs change the properties of light, such as amplitude, phase, and polarization, it is necessary to find the proper operating conditions to control the SLM’s response. The twisted angle and the birefringence of a TNLC are two main parameters that control the modulation. There are several proposed methods and configurations to find these parameters to introduce the Jones matrix of TNLC [22, 23, 24, 25, 26]. On the contrary, Martín-Badosa et al. proposed a method to characterize liquid crystal displays (LCDs) based on the fringe analysis obtained by a Mach-Zehnder interferometer configuration, without the necessity of finding the physical properties of LCD [27]. Nevertheless, their approach is based on counting the displacement of the fringes and is time-consuming. Wang et al. proposed a faster method to characterize SLM based on extracting the phase values of the Fourier spectra of the interference pattern directly [28]. They indicated that analyzing the phase values in the frequency domain is sufficient to obtain the imposed modulated phase. Their mathematical approach is based on Fresnel diffraction considering the transfer function. However, this approach can be modified by adding a 4-f imaging system to the Mach-Zehnder interferometer.
The double-pixel hologram Arrizón’s approach is a cell-oriented computer-generated hologram (CGH) encoding. In the cell-oriented method, each encoding point is split into a couple of holographic cells [29]. He proposed a modification of the previous works regarding a double-phase CGH method with an on-axis reconstruction field [30, 31, 32]. His approach improved the signal-to-noise ratio (SNR) in the reconstruction plane using two pixels of SLM to encode one holographic cell [33]. Since then, he generalized his approach to producing a more symmetric and high-SNR-signal domain using four pixels of SLM, the so-called modified Double-Pixel Hologram (DPH) [34]. Although his approach was suggested for encoding phase-only SLMs, he adjusted the method to encoding complex modulation with a transmission TNLC as a low-resolution spatial light modulator [35, 36, 37].
This chapter aims to present a modification of the method proposed by Martín-Badosa et al. and Wang et al. to characterize LCDs and review the DPH Arrizón’s approach to generating an on-axis CGH proper for encoding TNLCs. Since the codification algorithm is time-consuming, a fast algorithm using the k-NN classifier is presented. The application of this codification is extended to provide vector beams using a high-NA microscope objective.
The following text is organized as follows: Section 2 briefly describes the physical and optical properties of a TNLC display. Section 3 describes the characterizing process based on the modified Mach-Zehnder interferometer and fringe analysis in the Fourier domain. Section 4 reviews the DPH Arrizón’s approach. Section 5 introduces a fast algorithm to generate DPHs applying the k-NN machine learning algorithm. Section 6 demonstrates the experimental setup to produce and analyze highly focused beams with arbitrary beam profiles.
A twisted nematic liquid crystal display is constructed by sandwiching a nematic liquid crystal between two transparent glass plates. Different voltages impose an external electric field through the medium using electrodes connected to each glass plate. Nematic molecules inside the medium have a helical structure parallel to their elongated direction with an optical axis. In this regard, TNLCs are a sort of birefringent medium with ordinary and extraordinary refractive indices (
Regarding specific situations, including the state of polarization, the wavelength of input beams and applied voltages, three different modulations are mainly interesting: amplitude-only, phase-only, and complex amplitude-phase. Applying different voltages to SLM results in different degrees of birefringence that can be practically obtained by displaying different gray values on the LCD, ranging from 0 to 255. Accordingly, the phase and intensity of the input beam alter passing through the SLM differently. Hence, the effect of a TNLC display in the optical system can be described by
where
Martín-Badosa et al. applied a Mach-Zehnder interferometer for characterizing LCDs. With the same optical setup and a different mathematical description, Wang et al. proposed a faster and more convenient way to obtain phase modulation. Since the digital holography approach used in this work is based on DPH Arrizón’s approach, the Mach-Zehnder interferometer should be accordingly modified in order to eliminate the off-axis diffraction orders caused by the codification algorithm (it is explained in Section 4). Therefore, the optical setup used in this work is modified by adding a 4-f spatial filtering system. Accordingly, the mathematical analysis based on this experimental setup is presented.
As shown in Figure 1, the optical setup consists of a Mach-Zehnder interferometer plus a 4-f spatial filtering system. The coherent beam provided by a pig-tailed laser (Thorlabs LP520-SF15A) with
The experimental setup. LP, BS, HWP, QWP, M, SF, and CCD stand for the linear polarizer, beam splitter, the half-wave plate, the quarte-wave plate, mirror, spatial filter, and charged-coupled device, respectively.
The left arm of the interferometer, which the reference beam passes through, includes a half-wave plate (HWP2). Subsequently, the interference occurs when the two beams reach the second beam splitter (BS2). Then the interferometric pattern passing through the second linear polarizer (LP2) reaches the CCD camera’s sensor plane through the 4-f imaging system.
Regarding the experimental setup, LCD is placed at the back focal plane of lens A (LA), and the CCD camera is placed at the front focal plane of lens B (LB). Besides, the diffraction orders (except zero-order) caused by the pixelated structure of LCD and the digital holography approach are removed using the spatial filter (SF) placed at the common focal plane of LA and LB. Mirror M2 is properly tilted in such a way that the fringes are aligned in the y-direction, as shown in Figure 2a. HWP2 is used to adjust the contrast intensity of the interference pattern. The orientation of axes of linear polarizers, LP1 and LP2, and fast axes of HWP1 and QWP1 with respect to each other define the modulated characteristic of the TNLC display. Hence, the desired modulation can be obtained by some practical attempts.
(a) The interferometric pattern recorded by CCD. (b) The corresponding Fourier spectra.
The fringe pattern recorded by the CCD can be expressed mathematically in the following form:
where
with
The Fourier transform of Eq. (3) gives
where the capital letters denote the Fourier spectra,
Since the spatial variations of
Once the configuration of the experiment, for instance, wavelength and the optical path difference between the reference and object beam, remains constant, the position of the peaks in the frequency domain remains unchanged. Thereby, the modulated phase can be obtained by analyzing either
where
The subscripts
The gray-level images should be synthesized in such a way that the images are divided into two parts corresponding with the reference part (zero value) and the variable part (ranging from 0 to 255), as explained previously. These images loading on SLM cause different phase shifts between the variable and reference part resulting in a displacement of fringes. The amount of this phase shift depends directly on the orientation axes of retarders and linear polarizers and can be obtained mathematically by means of Eq. (9). The first row of Figure 3 demonstrates three examples of the gray-level images loading on the LCD, whereas the second row indicates the corresponding interference patterns recorded by the CCD camera. The fringes were experimentally obtained by setting the axes of LP1 and LP2 at 0 and 90 degrees, respectively, with respect to the x-axis. In addition, the fast axes of HWP2, HWP1, and QWP1 were rotated −20, −63, and 45 degrees, respectively, with respect to the x-axis.
The first row demonstrates three examples of gray-level images loaded on the LCD. The second row indicates the corresponding interference patterns recorded by the CCD camera.
Then, two equal regions of the reference and variable part of each interference pattern should be selected for calculating the 2D fast Fourier transform, as indicated by the red rectangles in Figure 4b. As a result, the modulated phase can be obtained by applying Eq. (9) to the known frequency
(a) An example of synthesized gray-level image loading on LCD. (b) The recorded fringe pattern. The red selected rectangles have been used for calculating the 2D Fourier transform. (c) The Fourier domain.
In this practical case, the maximum achievable phase imposed by SLM is around 1.75
(a) The phase modulation. (b) The amplitude modulation. (c) The polar plot of the phase-mostly modulation.
With the same configuration without changing the direction axes of linear polarizers or retarders, the amplitude curve can be obtained as follows: First, blocking the left arm of the Mach-Zehnder interferometer. Then, providing 256 gray-level images in which the entire images have the same gray value. Loading gray-level images on the LCD and subsequently recording the intensity pattern by the CCD camera. The modulated amplitude versus each gray value can be obtained by calculating the square root of the mean value of the recorded intensities and normalizing them to the maximum obtained amplitude. Also, this process can be done by using an intensity detector. The experimentally obtained amplitude curve versus gray values is shown in Figure 5b. Finally, Eq. (1) can be obtained for each gray value by combining the amplitude and phase responses of the SLM in consequence of the present configuration. This process is called the characterization or calibration of SLM. The polar plot shown in Figure 5c indicates the obtained phase-mostly modulation curve.
Very often, TNLCs provide a coupled amplitude-phase modulation, as indicated in Figure 5. This section aims to review the DPH Arrizón’s approach to expanding the accessible modulations beyond the restricted SLM response. Then, we review the modified DPH approach by applying 4 pixels to encode one holographic cell adapted to the experimentally obtained modulation curve. As a result, the approach is able to generate an on-axis computer-generated hologram with the optimum reconstruction efficiency, maximum signal bandwidth, and high SNR suitable for encoding arbitrary complex modulation into a low-resolution TNLC display.
Considering the obtained phase-mostly modulation curve shown in Figure 5, assume each complex modulation point belongs to the modulation curve as follows:
where subscript
To encode a desired complex modulation value
Arrizón employed the holographic double pixel shown in Figure 6, whose pixels have the complex modulation
The DPH configuration.
To explain this, considering the modulation points on the modulation curve (
The codification algorithm.
Regarding the experimental modulation curve, all possible complex values that can be obtained with this codification algorithm are shown with the green points in Figure 8. However, only those complex values that fall inside the blue circle with a radius
The red and green points show the experimental modulation curve and all possible complex values using the DPH approach. The green points inside the blue circle with the radius A0 = 0.29 are those accessible complex values to encode a complex function.
To go through Arrizón’s approach in more detail, assume the transmittance of the CGH that can be displayed on the LCD is
where
where
then, the Fourier transform of Eq. (17) gives
The error spectrum,
He demonstrated that the optimal choice
According to Eqs. (17) to (21),
Since both function
belong to the SLM modulation curve. Note that Eqs.(23) and (24) are the general forms of Eqs. (13) and (14). The constant value
Since the set of the modulation points is finite and discrete, we should find the nearest accessible complex value denoted
The remaining issue is to select the position of
Selection 1:
Selection 2:
(a) Selection 1 (b) selection 2.
On one side, he showed that the appropriate position-selection of the pair modulation points to encode a discrete modulation
This configuration is shown in Figure 10.
The representation of the modified DPH at the LCD plane applying selection 1.
On the other side, he demonstrated that the appropriate position-selection for the pair modulation points to encode complex functions of the type
This configuration is shown in Figure 11. The display plane is divided into two areas: Area U corresponds
The representation of the modified DPH at the LCD plane applying selections 1 and 2. The order of the distribution of values
This encoding algorithm is also appropriate for encoding continuous functions of the type
As explained in Section 4, generating CGHs in the way that Arrizón proposed requires an extensive search of the minimum Euclidean distance between the desired complex values (
The k-NN classifier is a type of nonparametric supervised machine learning algorithm [41]. Nonparametric models are characterized by memorizing the training datasets instead of learning them. This technique aims to train a dataset to label them into different known classes based on defined features. This algorithm can be described in three main steps:
To select the optimum number of k based on a distance metric.
To find the k nearest neighbors of the samples to be classified.
To predict the class label by majority vote.
In those cases where there is no majority vote, the machine predicts the class label based on the defined weight. We used the Scikit-learn Python library to implement the k-NN algorithm. Regarding the KNeighborsClassifier module, three parameters should be determined: k, weight, and metrics. Besides, a matrix with a-samples and b-features should be defined to train the machine. In this case, the number of samples is the number of all accessible complex points, while the features are chosen based on the real and imaginary value of each accessible complex point. According to the experimental modulation curve, the total number of classified samples (green points inside the blue circle shown in Figure 8) is 3540 (a = 3540) with two features (b = 2). The machine is trained based on data that come from the experimental modulation curve, while the machine will predict the nearest accessible complex values to the desired ones for each holographic cell. The optimum results are obtained by choosing k = 1, weights = distance, and metrics = Euclidean distance. On the one hand, a look-up matrix is made from all accessible complex values (
(a) The provided look-up matrix with 3540 rows and 3 columns. (b) the configuration of labeled training dataset with 3540 samples and two features.
So, the machine predicts the class label of the nearest accessible complex value to the desired one. According to the predicted label and look-up matrix, the pair of gray-level (
Here, two beam profiles are considered to generate their CGHs. The first one is a (1,1)-Hermite-Gaussian (
where
The first row shows the distribution of the amplitude and phase of HG11, respectively. The second row shows their nearest values predicted by the k-NN classifier according to the experimental modulation curve.
The second beam profile is a (0,1)-Laguerre-Gaussian (
The amplitude and phase distribution of
The first row shows the numerical distribution of the amplitude and phase of
The CGHs correspond with (a)
Table 1 indicates the required time to generate CGHs corresponding with
Pixels | 250 × 250 | 512 × 512 | 768 × 1024 | 1152 × 1920 |
---|---|---|---|---|
0.16 | 0.64 | 1.92 | 5.47 | |
0.38 | 1.54 | 5.53 | 16.39 |
Processing time (in seconds) for generating CGHs using the k-NN classifier.
The experimental setup (sketched in Figure 1) is modified in order to generate and analyze the beam at the entrance pupil and focal plane of a highly focusing system, as shown in Figure 16.
The sketch of the experimental setup to capture the beam profile at the SLM and focal plane. R stands for a retarder that can be a QWP or vortex for providing circularly or radially polarized beam, respectively. MO stands for microscope objective. MS stands for the movable stage.
The left arm of the Mach-Zehnder interferometer is blocked by an obstacle. A vortex retarder (ThorLab, WPV10L-532) or a QWP (R) is added after LP2 to provide a radially or circularly polarized beam, respectively. In order to provide a radial polarization, the fast axis of the vortex retarder is placed parallel to the y-axis. In order to provide a circular polarization, the fast axis of QWP is rotated 45° with respect to the x-axis.
The beam is separately imaged at the entrance pupil of microscope objective MO1 (Nikon Plan Fluorite N40X-PF with NA = 0.75) and at the sensor plane of CCD1 by means of the 4f-system and BS3. Microscope objective MO2 (Nikon with NA = 0.8) is mounted on a movable stage driven by a motorized device (Newport LTA-HL) with uni-directional repeatability of
We recently used this experimental setup to estimate the longitudinal component of a highly focused beam using a phase retrieval algorithm and Gauss’s theorem. The method is able to retrieve transverse and longitudinal components of a highly focused electromagnetic field (for more details, see [43]).
Since the intensity pattern of a beam at the focal plane strongly depends on its polarization state at the entrance pupil of MO1 [44], two different polarization states have been considered to compromise the experimental results with the numerical ones. The numerical calculations have been implemented by applying the focused field calculation method introduced in [16]. Figure 17 shows the intensity patterns recorded by CCD1 regarding
The intensity patterns recorded by CCD1 correspond to (a)
Figure 18 indicates the intensity patterns of the circularly polarized
The stokes images correspond to the circularly polarized
In a similar way, Figure 19 indicates the Stokes images correspond to the radially polarized
The stokes images correspond to the radially polarized
This chapter provided all the necessary steps to generate complex beams with arbitrary intensity and phase distribution using a translucent TNLC display in one frame. Characterizing a TNLC-SLM accompanied by the DPH Arrizon’s approach has been widely reviewed, and the k-NN classifier has been applied to generate CGHs faster than conventional calculation. Two wave functions have been experimentally assessed at the SLM and the focal plane of a high-NA microscope objective. Finally, the experimental setup has been described in order to generate focused vector beams and measure the corresponding Stokes images.
The author acknowledges support from the PredocsUB program.
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\\n\\nThe University of Massachusetts, Amherst is pledging funds via the Knowledge Unlatched program to ensure academics can publish Open Access content more easily.
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\\n\\nThe University of Surrey is pledging funds via the Knowledge Unlatched program to ensure academics can publish Open Access content more easily.
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\n\nThe University of Massachusetts, Amherst is pledging funds via the Knowledge Unlatched program to ensure academics can publish Open Access content more easily.
\n\nCorresponding authors will receive a 10% discount on their Open Access Publication Fees (OAPF) for Open Access book chapters or monograph publications. To use the discount you will need to verify your institutional email address. These discounts are valid from 2020 to 2022.
\n\nThe University of Surrey is pledging funds via the Knowledge Unlatched program to ensure academics can publish Open Access content more easily.
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Experimentation is an application of treatments applied to experimental units and is then part of a scientific method based on the measurement of one or more responses. It is necessary to observe the process and the operation of the system well. For this reason, in order to obtain a final result, an experimenter must plan and design experiments and analyzes the results. One of the most commonly used experimental designs for optimization is the response surface methodology (RSM). Because it allows evaluating the effects of multiple factors and their interactions on one or more response variables it is a useful method. In this section, recent studies have been compiled which aim to extraction of plant material in high yield and quality and determine optimum conditions for this extraction process.",book:{id:"5856",slug:"statistical-approaches-with-emphasis-on-design-of-experiments-applied-to-chemical-processes",title:"Statistical Approaches With Emphasis on Design of Experiments Applied to Chemical Processes",fullTitle:"Statistical Approaches With Emphasis on Design of Experiments Applied to Chemical Processes"},signatures:"Alev Yüksel Aydar",authors:[{id:"218870",title:"Dr.",name:"Alev Yüksel",middleName:null,surname:"Aydar",slug:"alev-yuksel-aydar",fullName:"Alev Yüksel Aydar"}]},{id:"56460",doi:"10.5772/intechopen.69501",title:"Application of Taguchi-Based Design of Experiments for Industrial Chemical Processes",slug:"application-of-taguchi-based-design-of-experiments-for-industrial-chemical-processes",totalDownloads:3223,totalCrossrefCites:27,totalDimensionsCites:54,abstract:"Design of experiment is the method, which is used at a very large scale to study the experimentations of industrial processes. It is a statically approach where we develop the mathematical models through experimental trial runs to predict the possible output on the basis of the given input data or parameters. The aim of this chapter is to stimulate the engineering community to apply Taguchi technique to experimentation, the design of experiments, and to tackle quality problems in industrial chemical processes that they deal with. Based on years of research and applications, Dr. G. Taguchi has standardized the methods for each of these DOE application steps. Thus, DOE using Taguchi approach has become a much more attractive tool to practicing engineers and scientists. And since the last four decades, there were limitations when conventional experimental design techniques were applied to industrial experimentation. And Taguchi, also known as orthogonal array design, adds a new dimension to conventional experimental design. Taguchi method is a broadly accepted method of DOE, which has proven in producing high-quality products at subsequently low cost.",book:{id:"5856",slug:"statistical-approaches-with-emphasis-on-design-of-experiments-applied-to-chemical-processes",title:"Statistical Approaches With Emphasis on Design of Experiments Applied to Chemical Processes",fullTitle:"Statistical Approaches With Emphasis on Design of Experiments Applied to Chemical Processes"},signatures:"Rahul Davis and Pretesh John",authors:[{id:"199438",title:"Mr.",name:"Rahul",middleName:null,surname:"Davis",slug:"rahul-davis",fullName:"Rahul Davis"}]},{id:"14634",doi:"10.5772/15998",title:"The Application of FT-IR Spectroscopy in Waste Management",slug:"the-application-of-ft-ir-spectroscopy-in-waste-management",totalDownloads:6651,totalCrossrefCites:18,totalDimensionsCites:34,abstract:null,book:{id:"1574",slug:"fourier-transforms-new-analytical-approaches-and-ftir-strategies",title:"Fourier Transforms",fullTitle:"Fourier Transforms - New Analytical Approaches and FTIR Strategies"},signatures:"Ena Smidt, Katharina Böhm and Manfred Schwanninger",authors:[{id:"20376",title:"Dr.",name:"Katharina",middleName:null,surname:"Böhm",slug:"katharina-bohm",fullName:"Katharina Böhm"},{id:"22840",title:"Dr.",name:"Ena",middleName:null,surname:"Smidt",slug:"ena-smidt",fullName:"Ena Smidt"},{id:"22915",title:"Dr.",name:"Manfred",middleName:null,surname:"Schwanninger",slug:"manfred-schwanninger",fullName:"Manfred Schwanninger"}]},{id:"15157",doi:"10.5772/15959",title:"Fourier Transform Mass Spectrometry for the Molecular Level Characterization of Natural Organic Matter: Instrument Capabilities, Applications, and Limitations",slug:"fourier-transform-mass-spectrometry-for-the-molecular-level-characterization-of-natural-organic-matt",totalDownloads:4347,totalCrossrefCites:6,totalDimensionsCites:34,abstract:null,book:{id:"122",slug:"fourier-transforms-approach-to-scientific-principles",title:"Fourier Transforms",fullTitle:"Fourier Transforms - Approach to Scientific Principles"},signatures:"Rachel L. 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In this paper, the basic concepts of robust optimization are developed, the different types of robustness are defined in detail, the main areas in which it has been applied are described and finally, the future lines of research that appear in this area are included.",book:{id:"6587",slug:"nature-inspired-methods-for-stochastic-robust-and-dynamic-optimization",title:"Nature-inspired Methods for Stochastic, Robust and Dynamic Optimization",fullTitle:"Nature-inspired Methods for Stochastic, Robust and Dynamic Optimization"},signatures:"José García and Alvaro Peña",authors:[{id:"227809",title:"Ph.D.",name:"Jose",middleName:null,surname:"Garcia",slug:"jose-garcia",fullName:"Jose Garcia"},{id:"240407",title:"Dr.",name:"Alvaro",middleName:null,surname:"Peña",slug:"alvaro-pena",fullName:"Alvaro Peña"}]}],mostDownloadedChaptersLast30Days:[{id:"59209",title:"Utilization of Response Surface Methodology in Optimization of Extraction of Plant Materials",slug:"utilization-of-response-surface-methodology-in-optimization-of-extraction-of-plant-materials",totalDownloads:5469,totalCrossrefCites:64,totalDimensionsCites:97,abstract:"Experimental design plays an important role in several areas of science and industry. Experimentation is an application of treatments applied to experimental units and is then part of a scientific method based on the measurement of one or more responses. It is necessary to observe the process and the operation of the system well. For this reason, in order to obtain a final result, an experimenter must plan and design experiments and analyzes the results. One of the most commonly used experimental designs for optimization is the response surface methodology (RSM). Because it allows evaluating the effects of multiple factors and their interactions on one or more response variables it is a useful method. In this section, recent studies have been compiled which aim to extraction of plant material in high yield and quality and determine optimum conditions for this extraction process.",book:{id:"5856",slug:"statistical-approaches-with-emphasis-on-design-of-experiments-applied-to-chemical-processes",title:"Statistical Approaches With Emphasis on Design of Experiments Applied to Chemical Processes",fullTitle:"Statistical Approaches With Emphasis on Design of Experiments Applied to Chemical Processes"},signatures:"Alev Yüksel Aydar",authors:[{id:"218870",title:"Dr.",name:"Alev Yüksel",middleName:null,surname:"Aydar",slug:"alev-yuksel-aydar",fullName:"Alev Yüksel Aydar"}]},{id:"74096",title:"Time Frequency Analysis of Wavelet and Fourier Transform",slug:"time-frequency-analysis-of-wavelet-and-fourier-transform",totalDownloads:1283,totalCrossrefCites:6,totalDimensionsCites:8,abstract:"Signal processing has long been dominated by the Fourier transform. However, there is an alternate transform that has gained popularity recently and that is the wavelet transform. The wavelet transform has a long history starting in 1910 when Alfred Haar created it as an alternative to the Fourier transform. In 1940 Norman Ricker created the first continuous wavelet and proposed the term wavelet. Work in the field has proceeded in fits and starts across many different disciplines, until the 1990’s when the discrete wavelet transform was developed by Ingrid Daubechies. 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In all cases, cyclical ups and downs depend not only on internal system cyclical processes and their factors in countries but also on the consequences of intercountry interaction. The ability to measure and predict business cycles, taking into account their mutual influence, is a prerequisite for the development of an adequate business policy of countries and their associations.",book:{id:"6703",slug:"statistics-growing-data-sets-and-growing-demand-for-statistics",title:"Statistics",fullTitle:"Statistics - Growing Data Sets and Growing Demand for Statistics"},signatures:"Elena Zarova",authors:null},{id:"54366",title:"Solution of Differential Equations with Applications to Engineering Problems",slug:"solution-of-differential-equations-with-applications-to-engineering-problems",totalDownloads:6866,totalCrossrefCites:5,totalDimensionsCites:8,abstract:"Over the last hundred years, many techniques have been developed for the solution of ordinary differential equations and partial differential equations. While quite a major portion of the techniques is only useful for academic purposes, there are some which are important in the solution of real problems arising from science and engineering. In this chapter, only very limited techniques for solving ordinary differential and partial differential equations are discussed, as it is impossible to cover all the available techniques even in a book form. The readers are then suggested to pursue further studies on this issue if necessary. After that, the readers are introduced to two major numerical methods commonly used by the engineers for the solution of real engineering problems.",book:{id:"5513",slug:"dynamical-systems-analytical-and-computational-techniques",title:"Dynamical Systems",fullTitle:"Dynamical Systems - Analytical and Computational Techniques"},signatures:"Cheng Yung Ming",authors:[{id:"191017",title:"Dr.",name:"Cheng",middleName:null,surname:"Y.M.",slug:"cheng-y.m.",fullName:"Cheng Y.M."}]},{id:"56538",title:"Stochastic Resonance and Related Topics",slug:"stochastic-resonance-and-related-topics",totalDownloads:1718,totalCrossrefCites:1,totalDimensionsCites:1,abstract:"The stochastic resonance (SR) is the phenomenon which can emerge in nonlinear dynamic systems. In general, it is related with a bistable nonlinear system of Duffing type under additive excitation combining deterministic periodic force and Gaussian white noise. It manifests as a stable quasiperiodic interwell hopping between both stable states with a small random perturbation. Classical definition and basic features of SR are regarded. The most important methods of investigation outlined are: analytical, semi-analytical, and numerical procedures of governing physical systems or relevant Fokker-Planck equation. Stochastic simulation is mentioned and experimental way of results verification is recommended. Some areas in Engineering Dynamics related with SR are presented together with a particular demonstration observed in the aeroelastic stability. Interaction of stationary and quasiperiodic parts of the response is discussed. Some nonconventional definitions are outlined concerning alternative operators and driving processes are highlighted. The chapter shows a large potential of specific basic, applied and industrial research in SR. This strategy enables to formulate new ideas for both development of nonconventional measures for vibration damping and employment of SR in branches, where it represents an operating mode of the system itself. Weaknesses and empty areas where the research effort of SR should be oriented are indicated.",book:{id:"6128",slug:"resonance",title:"Resonance",fullTitle:"Resonance"},signatures:"Jiří Náprstek and Cyril Fischer",authors:[{id:"207472",title:"Dr.",name:"Jiri",middleName:null,surname:"Naprstek",slug:"jiri-naprstek",fullName:"Jiri Naprstek"},{id:"213311",title:"Dr.",name:"Cyril",middleName:null,surname:"Fischer",slug:"cyril-fischer",fullName:"Cyril Fischer"}]}],onlineFirstChaptersFilter:{topicId:"15",limit:6,offset:0},onlineFirstChaptersCollection:[{id:"83034",title:"Optimal N-of-1 Clinical Trials for Individualized Patient Care and Aggregated N-of-1 Designs",slug:"optimal-n-of-1-clinical-trials-for-individualized-patient-care-and-aggregated-n-of-1-designs",totalDownloads:2,totalDimensionsCites:0,doi:"10.5772/intechopen.106352",abstract:"Precision medicine typically refers to the use of genomic signatures of patients to assign more effective therapies to treat patients, or, for improved diagnosis of the early onset of a disease so that interventions can be delivered to prevent or delay the disease progression. Because the aim is to provide individualized patient treatment, such single-person trials are called N-of-1 trials. This chapter reviews fundamental ideas, models, and construction of optimal designs for N-of-1 trials, which are invariably constructed from crossover trials, where each patient receives a random sequence of trial treatments over time. We construct examples of universally optimal N-of-1 designs for comparing two treatments under various correlation structure assumptions and discuss how N-of-1 trials may be combined to form optimal aggregated N-of-1 trials for assessing average treatment effects for two or more treatments.",book:{id:"10678",title:"Biostatistics",coverURL:"https://cdn.intechopen.com/books/images_new/10678.jpg"},signatures:"Yin Li, Weng Kee Wong and Keumhee Chough Carriere"},{id:"83029",title:"Quasi Conformally Flat Quasi Einstein-Weyl Manifolds",slug:"quasi-conformally-flat-quasi-einstein-weyl-manifolds",totalDownloads:3,totalDimensionsCites:0,doi:"10.5772/intechopen.105683",abstract:"The aim of this work is to study on quasi conformally flat quasi Einstein-Weyl manifolds. In this book chapter, firstly, an interesting relationship between complementary vector field and generator of the quasi Einstein-Weyl manifold is obtained and supported by an example. Then, it is investigated that quasi conformally flat quasi Einstein-Weyl manifolds are of quasi constant curvature, recurrent and semi-symmetric under which conditions after obtaining the expression of the curvature tensor of the quasi conformally flat quasi Einstein-Weyl manifold. 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In this sense, the chapter shows a methodology to estimate the probability to be involved in a road accident, considering the road education and the socioeconomic characteristics of the population of a specific region, taking the Santiago de Querétaro city (in México) as a study case. Through a logit model estimation and a survey applied to pedestrian, cyclist, motorcyclist, car driver, and freight driver allow us to determine which socioeconomic variables and road education are significant to determine the probability of being involved in a road accident.",book:{id:"12021",title:"Applied Probability Theory - New Perspectives, Recent Advances and Trends",coverURL:"https://cdn.intechopen.com/books/images_new/12021.jpg"},signatures:"Saúl Antonio, Obregón Biosca, José Luis Reyes Araiza and Miguel Angel Pérez Lara y Hernández"},{id:"82947",title:"Some Tauberian Theorems under Triple Statistically Nörlund-Cesáro Summability Method",slug:"some-tauberian-theorems-under-triple-statistically-n-rlund-ces-ro-summability-method",totalDownloads:3,totalDimensionsCites:0,doi:"10.5772/intechopen.106141",abstract:"In this paper, we extend the notion presented by Braha (2020) in a higher dimension, we introduce the notion of Np,qn,m,gCn,m,g1,1,1-statistically convergence and show necessity and sufficiency conditions under which the existence of the limit st-limn,m,g→∞xn,m,g=L follows from that st-limn,m,g→∞Np,qn,m,gCn,m,g1,1,1=L. These conditions are one-sided or two-sided if xn,m,g is a sequence of real or complex numbers, respectively.",book:{id:"11503",title:"Functional Calculus - Recent Advances and Development",coverURL:"https://cdn.intechopen.com/books/images_new/11503.jpg"},signatures:"Carlos Granados"},{id:"82847",title:"A Chaos Auto-Associative Model with Chebyshev Activation Function",slug:"a-chaos-auto-associative-model-with-chebyshev-activation-function",totalDownloads:5,totalDimensionsCites:0,doi:"10.5772/intechopen.106147",abstract:"In this work, we shall put forward a novel chaos memory retrieval model with a Chebyshev-type activation function as an artificial chaos neuron. According to certain numerical analyses of the present association model with autocorrelation connection matrix between neurons, the dependence of memory retrieval properties on the initial Hamming distance between the input pattern and a target pattern to be retrieved among the embedded patterns will be presented to examine the retrieval abilities, i.e. the memory capacity of the associative memory.",book:{id:"12019",title:"Chaos Theory - Recent Advances, New Perspectives and Applications",coverURL:"https://cdn.intechopen.com/books/images_new/12019.jpg"},signatures:"Masahiro Nakagawa"},{id:"82826",title:"A Brief Look at the Calderón and Hilbert Operators",slug:"a-brief-look-at-the-calder-n-and-hilbert-operators",totalDownloads:2,totalDimensionsCites:0,doi:"10.5772/intechopen.106027",abstract:"The Calderón operator is the sum of the Hardy averaging operator and its adjoint, and plays an important role in the theory of real interpolation. On the other hand, the Hilbert operator arises from the continuous version of Hilbert’s inequality. Both operators appear in different contexts and have numerous applications within harmonic analysis. In this chapter we will briefly review the Calderón and Hilbert operators, showing some of the most relevant results within functional analysis and finally we will present recent results on these operators within Fourier analysis.",book:{id:"11503",title:"Functional Calculus - Recent Advances and Development",coverURL:"https://cdn.intechopen.com/books/images_new/11503.jpg"},signatures:"Guillermo J. 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