Photic driving in the electroencephalogram of children and adolescents: harmonic structure and relation to the resting state

In order to identify latent bioelectrical oscillators, 15 normal subjects (aged 9-17 years, 8 males, 7 females) were subjected to intermittent photic stimulation. The EEG amplitude spectra corresponding to the 11 fixed frequencies of stimulation presented (3-24 Hz) were combined to form "profiles" of the driving reaction in the right occipital area. The driving response varied with frequency, and was demonstrable in 70-100% of cases (using as criterion peak amplitudes 20% larger than those of the neighbors). The strongest responses were observed at the frequency closest to the alpha peak of the resting EEG. A secondary profile maximum was in the theta band. In 10 subjects, this maximum exceeded half the alpha peak (with an average of 72.4% of the alpha peak), while in the resting spectra, theta amplitudes were much lower than the alpha maxima. This responsiveness in theta activity seems to be characteristic of prepubertal and pubertal subjects. The profiles and resting EEG spectra showed a highly significant Pearson's correlation, with the peak in the theta band of the profiles being the main difference observed between them. The correlation coefficient was significantly correlated with the ratio of the maxima in the theta and alpha bands (R = -0.77, P<0.001). The correlation coefficient between profile and resting spectrum may be a useful indicator in screening methods used to reveal latent cerebral oscillators. Profiles for the second and third harmonics were correlated with those of the first harmonic (fundamental frequency), when considering the corresponding EEG frequencies. Peak frequencies in all three profiles were close to those of the individual's background alpha rhythm, and peak amplitudes in higher harmonics were not much lower than those of the fundamental frequency (mean values of 84 and 63%, for second and third harmonics, respectively).

Enthalpy-entropy compensation based on isotherms of mango

Moisture equilibrium data of mango pulp were determined using the static gravimetric method. Adsorption and desorption isotherms were obtained in the range of 30-70 ºC, to water activities (a w) from 0.02 to 0.97. The application of the GAB model to the experimental results, using direct nonlinear regression analysis, provided agreement between experimental and calculated values. The net isosteric heat of sorption was estimated from equilibrium sorption data, using the Clausius-Clapeyron equation. Isosteric heats of sorption were found to increase with increasing temperature and could be well adjusted by an exponential relationship. The enthalpy-entropy compensation theory was applied to sorption isotherms and plots of deltaH versus deltaS provided the isokinetic temperatures, indicating an enthalpy controlled sorption process.

Steps towards more effective antitrust system in EU – The Damages Directive’s effect on victim’s right to compensation for antitrust harm

Kaikkien kansalaisten ja yritysten, jotka kärsivät vahinkoa Euroopan Unionin kilpailusääntöjen (SEUT 101 ja 102 artiklan) rikkomisen vuoksi, on voitava vaatia korvauksia vahingon aiheuttaneelta osapuolelta. Euroopan unionin tuomioistuin on ratkaisuillaan Courage ja Manfredi vahvistanut vahinkoa kärsineen oikeuden saada korvausta kärsimästään vahingosta. Suomessa kilpailuoikeudellista vahingonkorvausta koskeva oikeuskäytäntö on ollut vähäistä, vaikkakin viime aikoina on annettu muutama merkittävä vahingonkorvausratkaisu, näistä kenties tunnetuimpana asvalttikartelliratkaisu. Kilpailuoikeuden rikkomisesta vahinkoa kärsineet saavat kuitenkin vain harvoin korvausta kärsimästään vahingosta, mikä on ollut seurausta erilaisista lainsäädännöllisistä ja menettelyistä johtuvista esteistä jäsenvaltioiden säännöissä. Komission pitkään kestänyt lainsäädäntöhanke EU:n kilpailuoikeuden täytäntöönpanojärjestelmän selkeyttämiseksi päättyi marraskuussa 2014, kun Euroopan parlamentin ja neuvoston direktiivi tietyistä säännöistä, joita sovelletaan jäsenvaltioiden ja Euroopan unionin kilpailuoikeuden rikkomisen johdosta kansallisen lainsäädännön nojalla nostettuihin vahingonkorvauskanteisiin (2014/104/ EU) hyväksyttiin. Direktiivi julkaistiin Euroopan unionin virallisessa lehdessä 5. joulukuuta 2014, ja jäsenvaltioilla on 27.12.2016 asti aikaa implementoida direktiivi osaksi kansallista lainsäädäntöä. Direktiivin tavoitteena on EU:n kilpailusääntöjen tehokas täytäntöönpano sekä kilpailuoikeuden julkisoikeudellisen ja yksityisoikeudellisen täytäntöönpanon selkeyttäminen. Lisäksi direktiivi pyrkii varmistamaan, että vahingonkärsijät voivat saada täyden korvauksen kärsimästään vahingosta, sekä poistamaan esteitä ja pienentämään kustannuksia vahingon todistamisessa, samalla harmonisoiden eri jäsenmaissa toimivien yritysten oikeussuojan tasoa. Tarkastelen pro gradu –tutkielmassani kilpailuoikeudellisen vahingonkorvauksen kehitystä sekä uuden EU:n vahingonkorvausdirektiivin vaikutuksia erityisesti vahingonkärsijän näkökulmasta, eli sitä kuinka direktiivi vaikuttaa vahingonkärsijän mahdollisuuteen saada korvausta kärsimästään vahingosta, joka johtuu EU:n kilpailusääntöjen rikkomisesta. Lisäksi tarkastelen lyhyesti direktiivin tuomia muutoksia Suomen lainsäädäntöön. Tutkielmani loppupäätelmä on, että vaikka vahingonkorvausdirektiivi ei täydellisesti paranna vahingonkärsijän asemaa, se selkeyttää monella tavalla kilpailuoikeudellisten vahingonkorvauskanteiden nykyistä tilaa, ja saattaa tietyssä määrin rohkaista vahingonkärsijiä hakemaan korvausta kärsimästään vahingosta.

The solutions and tunneling properties for a linear potential and an inverted harmonic oscillator in an infinite well

In this work we look at two different 1-dimensional quantum systems. The potentials for these systems are a linear potential in an infinite well and an inverted harmonic oscillator in an infinite well. We will solve the Schrödinger equation for both of these systems and get the energy eigenvalues and eigenfunctions. The solutions are obtained by using the boundary conditions and numerical methods. The motivation for our study comes from experimental background. For the linear potential we have two different boundary conditions. The first one is the so called normal boundary condition in which the wave function goes to zero on the edge of the well. The second condition is called derivative boundary condition in which the derivative of the wave function goes to zero on the edge of the well. The actual solutions are Airy functions. In the case of the inverted oscillator the solutions are parabolic cylinder functions and they are solved only using the normal boundary condition. Both of the potentials are compared with the particle in a box solutions. We will also present figures and tables from which we can see how the solutions look like. The similarities and differences with the particle in a box solution are also shown visually. The figures and calculations are done using mathematical software. We will also compare the linear potential to a case where the infinite wall is only on the left side. For this case we will also show graphical information of the different properties. With the inverted harmonic oscillator we will take a closer look at the quantum mechanical tunneling. We present some of the history of the quantum tunneling theory, its developers and finally we show the Feynman path integral theory. This theory enables us to get the instanton solutions. The instanton solutions are a way to look at the tunneling properties of the quantum system. The results are compared with the solutions of the double-well potential which is very similar to our case as a quantum system. The solutions are obtained using the same methods which makes the comparison relatively easy. All in all we consider and go through some of the stages of the quantum theory. We also look at the different ways to interpret the theory. We also present the special functions that are needed in our solutions, and look at the properties and different relations to other special functions. It is essential to notice that it is possible to use different mathematical formalisms to get the desired result. The quantum theory has been built for over one hundred years and it has different approaches. Different aspects make it possible to look at different things.

The solutions and tunneling properties for a linear potential and an inverted harmonic oscillator in an infinite well

In this work we look at two different 1-dimensional quantum systems. The potentials for these systems are a linear potential in an infinite well and an inverted harmonic oscillator in an infinite well. We will solve the Schrödinger equation for both of these systems and get the energy eigenvalues and eigenfunctions. The solutions are obtained by using the boundary conditions and numerical methods. The motivation for our study comes from experimental background. For the linear potential we have two different boundary conditions. The first one is the so called normal boundary condition in which the wave function goes to zero on the edge of the well. The second condition is called derivative boundary condition in which the derivative of the wave function goes to zero on the edge of the well. The actual solutions are Airy functions. In the case of the inverted oscillator the solutions are parabolic cylinder functions and they are solved only using the normal boundary condition. Both of the potentials are compared with the particle in a box solutions. We will also present figures and tables from which we can see how the solutions look like. The similarities and differences with the particle in a box solution are also shown visually. The figures and calculations are done using mathematical software. We will also compare the linear potential to a case where the infinite wall is only on the left side. For this case we will also show graphical information of the different properties. With the inverted harmonic oscillator we will take a closer look at the quantum mechanical tunneling. We present some of the history of the quantum tunneling theory, its developers and finally we show the Feynman path integral theory. This theory enables us to get the instanton solutions. The instanton solutions are a way to look at the tunneling properties of the quantum system. The results are compared with the solutions of the double-well potential which is very similar to our case as a quantum system. The solutions are obtained using the same methods which makes the comparison relatively easy. All in all we consider and go through some of the stages of the quantum theory. We also look at the different ways to interpret the theory. We also present the special functions that are needed in our solutions, and look at the properties and different relations to other special functions. It is essential to notice that it is possible to use different mathematical formalisms to get the desired result. The quantum theory has been built for over one hundred years and it has different approaches. Different aspects make it possible to look at different things.

Loistehon kompensoinnin ja yliaaltosuodattimien nykytila sekä kehityskohteet Kemira Chemicals Oy:n Joutsenon tehtaalla

Tutkimuksessa käsitelty kemikaalitehdas on 110 kV:n kantaverkkoon liittyvä tehointensiivinen teollisuuslaitos. Prosessien käyttöön mukautetut sähkönjakeluverkon yliaaltosuodattimet ja niiden käyttökytkennät ovat tärkeässä asemassa loistehon tuoton hallitsemiseksi liittymän loistehoikkunaan ja riittävän yliaaltosuodatuksen järjestämiseksi häviöt minimoiden. Kohteena olleen kemikaalitehtaan sähkönjakeluverkon kompensointia ja yliaaltosuodatusta on viimeksi tutkittu vuonna 2003. Tämän jälkeen verkostokomponentit ovat ikääntyneet, prosessien käyttö sekä pienjänniteverkko ovat muuttuneet ja tehdasta käyttävät osittain eri henkilöt. Nykytilaselvitykselle ja verkon kehityskohteiden analysoinnille on tullut tarve edellisen selvityksen jatkoksi. Tutkimus painottuu vahvasti kenttämittauksiin, joiden perusteella sekä kirjallisuutta ja tehtaan järjestelmiä hyödyntäen määritetään loistehotasot verkon keskeisimmissä kohteissa pien-, keski- ja suurjännitetasoilla. Tutkimuksessa esitetään lipeätehtaan suotimien uudelleenjärjestely 4. yliaallon vähentämiseksi ja yksikkökoon pienentämiseksi. Kantaverkon liittymäpisteen tilanne oli hyväksyttävä. Tutkimus esittää pienjännitekompensointia KF-4-100 keskukseen varayhteyden kapasiteettia lisäten. Tutkimus tuotti yleistietoutta verkon käytöstä ja selvitti parhaat käyttökytkennät loistehoikkunan hallitsemiseksi ilman loistehokustannuksia.

On the formulation and the calculation of the harmonic contributions to the Debye-Waller factor in metals (sodium)

The algebraic expressions for the anharmonic contributions to the Debye-Waller factor up to 0(A ) and 0 L% ) £ where ^ is the scattering wave-vector] have been derived in a form suitable for cubic metals with small ion cores where the interatomic potential extends to many neighbours. This has been achieved in terms of various wave-vector dependent tensors, following the work of Shukla and Taylor (1974) on the cubic anharmonic Helmholtz free energy. The contribution to the various wave-vector dependent tensors from the coulomb and the electron-ion terms in the interatomic metallic potential has been obtained by the Ewald procedure. All the restricted multiple whole B r i l l o u i n zone (B.Z.) sums are reduced to single whole B.Z. sums by using the plane wave representation of the delta function. These single whole B.Z. sums are further reduced to the •%?? portion of the B.Z. following Shukla and Wilk (1974) and Shukla and Taylor (1974). Numerical calculations have been performed for sodium where the Born-Mayer term in the interatomic potential has been neglected because i t is small £ Vosko (1964)3 • *n o^er to compare our calculated results with the experimental results of Dawton (1937), we have also calculated the r a t io of the intensities at different temperatures for the lowest five reflections (110), (200), (220), (310) and (400) . Our calculated quasi-harmonic results agree reasonably well with the experimental results at temperatures (T) of the order of the Debye temperature ( 0 ). For T » © ^ 9 our calculated anharmonic results are found to be in good agreement with the experimental results.The anomalous terms in the Debye-Waller factor are found not to be negligible for certain reflections even for T ^ ©^ . At temperature T yy Op 9 where the temperature is of the order of the melting temperature (Xm) » "the anomalous terms are found to be important almost for all the f i ve reflections.

CEO Compensation, Compensation Risk, and Corporate Governance: Evidence from Technology Firms

Literature suggests that CEOs of technology firms earn higher pay than CEOs of non-technology firms. I investigate whether compensation risk explains the difference in compensation between technology firms and non-technology firms. Controlling for firm size and performance, I find that CEOs in technology firms have higher pay, but also have much higher compensation risk compared to non-technology firms. Compensation risk explains the major part of the difference in CEO pay. My study is consistent with the labor market economics view that CEOs earn competitive risk-adjusted total compensation.

Managerial Risk-Taking and CEO Excess Compensation

This paper examines risk taking and CEO excess compensation problems in U.S firms to determine their impact on shareholders wealth. Literature suggests a positive effect of CEO incentive risk and strong corporate governance on CEO risk taking. Furthermore, the strong governance mitigates excess compensation problem. Controlling for governance quality and incentive risk, I provide empirical evidence of a significant association between risk taking and CEO excess compensation. When I also control for pay-performance sensitivity (delta) and feedback effects of incentive compensation on CEO risk taking, I find that higher use of incentive pay encourages risk taking, and due to a high exposure to risk CEOs draws excess compensation. Furthermore, I find that the excess compensation problem is more serious with CEOs taking high risk than with those taking low risk. Finally, I find that CEO risk taking also has structural impacts on CEO compensation

Effect of executive compensation on firm performance

The paper finds evidence that the equity-based CEO pay is positively related to firm performance and risk-taking. Both stock price and operating performance as well as firm's riskiness increase in the pay-performance sensitivities (PPS) provided by CEO stock options and stock holdings. PPS can explain stock returns better as an additional factor to the Fama-French 3-factor model. When CEOs are compensated with higher PPS, firms experience higher return on asset (ROA). The higher PPS also leads to the higher risk-taking. While CEO incentive compensation has been perceived mixed on its effectiveness, this study provides support to the equity-based CEO compensation in reducing agency conflicts between CEOs and shareholders.

Firms Performance and CEO Compensation in Canada.

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