• Title/Summary/Keyword: Field symmetry

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THE RELATIONSHIP BETWEEN NONCOMMUTATIVE AND LORENTZVIOLATING PARAMETERS IN QUANTUM

  • HEIDARI, A.;GHORBANI, F.;GHORBANI, M.
    • Journal of the Korean Society for Industrial and Applied Mathematics
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    • v.16 no.3
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    • pp.205-216
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    • 2012
  • When it comes to Lorentz symmetry violation, there are generally two approaches to studying noncommutative field theory: 1) conventional fields are equivalent to noncommutative fields; however, symmetry groups are larger. 2) The symmetry group is the same as conventional standard model's symmetry group; but fields here are written based on the Seiberg-Witten map. Here by adopting the first approach, we aim to connect Lorentz violation coefficients with noncommutative parameters and compare the results with the second approach's results. Through the experimental values obtained for the Lorentz-violating parameters, we obtain a limit of noncommutative symmetry.

NMR Chemical Shift for 4d$^n$ System (Ⅱ). Calculation of the Pseudo Contact Shift for a 4d$^1$ System in a Strong Crystal Field Environment of Octahedral Symmetry

  • Sang-woon Ahn;Se-Woong Oh;Eui-suh Park
    • Bulletin of the Korean Chemical Society
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    • v.4 no.2
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    • pp.64-67
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    • 1983
  • NMR shift arising from the electron orbital angular momentum and the electron spin dipolar-nuclear spin angular momentum interactions has been investigated for a $4d^{1}$ system in a strong crystal field of octahedral symmetry. To examine the NMR shif for a $4d^{1}$ system in a strong crystal field of octahedral symmetry, we derive a general expression for ${\Delta}$B/B using a nonmultipole expansion technique. From this expression all the multipolar terms are determined. For the $4d^{1}$ system in a strong crystal field of octahedral symmetry the exact solution for NMR shift, ${\Delta}$B, is compared with the multipolar results. ${\Delta}$B/B for the $4d^{1}$ system is also compared with that for the $3d^{1}$ system. It is found that the $1/R^{7}$ term contributes dominantly to the NMR shift. However, there is good agreement between the nonmultipole and multipolar results for R-values larger than 0.2 nm for the $4d^{1}$ system but for R-values larger than 0.4 nm for the $3d^{1}$ system.

A STATISTICAL ANALYSIS METHOD FOR ESTIMATING GROUNDWATER CONTAMINANT CONCENTRATION

  • LEE, YOUNG CHEON
    • Honam Mathematical Journal
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    • v.26 no.1
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    • pp.87-103
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    • 2004
  • A practical estimation method for groundwater contaminant concentration is introduced. Using geostatistical techniques and symmetry, experimental variograms show significant improved correlation compared with those from conventional techniques. Numrical experiments are performed using a field data set.

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Three-fold Symmetry Effect on Mn2+ Centers in a LiNbO3 Crystal

  • Park, II-Woo
    • Journal of the Korean Magnetic Resonance Society
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    • v.12 no.2
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    • pp.103-110
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    • 2008
  • Spin Hamiltonian for the paramagnetic center with a three-fold symmetry and high spin ($S{\geq}2$) multiplicity should contain the fourth order zero-field splitting (ZFS) terms. Electron magnetic resonance transition lines of the center with S = 5/2 are expected to split in a pair when the magnetic field is applied off the principal axes of ZFS, while they are superimposed when the magnetic field is applied parallel to the principal axes of ZFS. In this study we report that the transition lines of $Mn^{2+}$ centers at the three-fold symmetric sites in $LiNbO_3$, chemically equivalent but physically different, split in two due to the nonzero fourth order ZFS term.

ADDITIVE OPERATORS PRESERVING RANK-ADDITIVITY ON SYMMETRY MATRIX SPACES

  • Tang, Xiao-Min;Cao, Chong-Guang
    • Journal of applied mathematics & informatics
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    • v.14 no.1_2
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    • pp.115-122
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    • 2004
  • We characterize the additive operators preserving rank-additivity on symmetry matrix spaces. Let $S_{n}(F)$ be the space of all $n\;\times\;n$ symmetry matrices over a field F with 2, $3\;\in\;F^{*}$, then T is an additive injective operator preserving rank-additivity on $S_{n}(F)$ if and only if there exists an invertible matrix $U\;\in\;M_n(F)$ and an injective field homomorphism $\phi$ of F to itself such that $T(X)\;=\;cUX{\phi}U^{T},\;\forallX\;=\;(x_{ij)\;\in\;S_n(F)$ where $c\;\in;F^{*},\;X^{\phi}\;=\;(\phi(x_{ij}))$. As applications, we determine the additive operators preserving minus-order on $S_{n}(F)$ over the field F.

Symmetry and Spectra of Complexes of Azo-Substituted Copper Phthalocyanine (Copper Phthalocyanine과 그 Azo 置換錯鹽들의 對稱과 Spectra)

  • Cho Nam-Sook;Kim Ki-Hwan;Hahn Chi-Sun
    • Journal of the Korean Chemical Society
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    • v.16 no.6
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    • pp.378-384
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    • 1972
  • The UV absorption spectra of the copper phthalocyanine and its azo derivatives in pyridine have been examined on the basis of symmetry operation, ligand field theory and molecular orbital consideration. The above treatment was also employed to determine the structure of the synthesized complexes.

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The Derivation of Generalized Quasi-Three Dimensional Displacement Field Equations for the Analysis of Composite Laminates (복합재료 적층판의 해석을 위한 일반화 준 3차원 변위식의 도출)

  • 김택현
    • Journal of the Korean Society of Manufacturing Technology Engineers
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    • v.7 no.4
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    • pp.21-27
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    • 1998
  • In the case of existing in free-edge delaminations of composite laminates which are symmetry with respect to mid-plane in laminates also, in the case of asymmetry and anti-symmetry, the generalized quasi-three dimensional displacement field equations developed from quasi-three dimensional displacement field equations can be applied to solve above cases. We introduce three paramenters in this paper, which have not been used in quasi-three dimensional displacement field equations until now. To the laminate subjected to the axial extension strain $\varepsilon$0(C1) in $\chi$-direction, the bending deformation $\chi$$\chi$(C$_2$) around у-direction, the bending deformation w$\chi$(C$_4$) around z-direction and the twisting deformation $\chi$$\chi$y(C$_3$) around $\chi$-direction .The generalized quasi-three dimensional displacement field equations are able to be analyzed efectively.

Magnetic field detwinning in FeTe

  • Kim, Younsik;Huh, Soonsang;Kim, Jonghyuk;Choi, Youngjae;Kim, Changyoung
    • Progress in Superconductivity and Cryogenics
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    • v.21 no.4
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    • pp.6-8
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    • 2019
  • Iron-based superconductors (IBSs) possess nematic phases in which rotational symmetry of the electronic structure is spontaneously broken. This novel phase has attracted much attention as it is believed to be closely linked to the superconductivity. However, observation of the symmetry broken phase by using a macroscopic experimental tool is a hard task because of naturally formed twin domains. Here, we report on a novel detwinning method by using a magnetic field on FeTe single crystal. Detwinning effect was measured by resistivity anisotropy using the Montgomery method. Our results show that FeTe was detwinned at 2T, which is a relatively weak field compared to the previously reported result. Furthermore, detwinning effect is retained even when the field is turned off after field cooling, making it an external stimulation-free detwinning method.

The NMR Chemical Shift for 4d$^n$ Systems(Ⅲ). Calculation of the NMR Shift for a 4d$^1$ System in a Strong Crystal Field Enviroment of Tetragonal Symmetry

  • Ahn, Sang-Woon;Park, Eui-Suh;Oh, Se-Woung
    • Bulletin of the Korean Chemical Society
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    • v.5 no.2
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    • pp.55-60
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    • 1984
  • The NMR shift arising from the electron angular momentum and electron spin dipolar-nuclear spin angular momentum interactions has been investigated for a $4d^1$system in a strong crystal field environment of tetragonal symmetry. A general formula for NMR shift is used to compute the NMR shifts along the (100), (010), (001), (110) and (111) axes. We find that from the computed results, the NMR shift along the (100) and (010) axes is consistent with each other in a strong crystal field environment of tetragonal symmetry, but the NMR shift along the (001) axis is about triply greater in magnitude than those along the (100) and (010) axes and is opposite in sign to those along (100) and (010) axes. In this work, we express the expansion coefficients $a_1^{(i)}$ and $b_1^{(i)}$ of $A_i$ and $B_i$ in terms of $g_m^{(i)}$ and $h_m^{(i)}$ and two matrices $c_{lm}$ and $d_{lm}$ of radial dependence. The NMR shift is also separated into the contributions of multipolar terms. We find that $1/R^3$ term contributes dominantly to the NMR shift along the (100), (010), (001) and (110) axes while along the (111) axis $1/R^5$ term dominantly contributes. However, the contribtions of the other terms may not be negligible.

A Consideration on the Characteristics of Electron Beam Dose Distributions for Clinical Applications (임상적용을 위한 전자선의 선량분포 특성에 대한 고찰)

  • Cha, Dong-Soo
    • Korean Journal of Digital Imaging in Medicine
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    • v.12 no.1
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    • pp.65-69
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    • 2010
  • High energy electron beams were to concentrically dose inside a tumor and more energy is a shape decreased of dose. Therefore, it is useful to radiation therapy of a tumor. Also high energy electron beams ionized into collision with a atom in structure material of tissue and it has big changes to dose distribution by multiple scattering. The study had to establish characteristic of electron beams from interaction of electron beams and materials. Experiment method was to measure dependence of electron beam central axis for depth dose curve, field flatness and symmetry and field size dependence. The results were able to evaluate data for a datum pint of electron beam. Also radiotherapy has to be considered for not only energy pencil of lines but characteristic, electron guide and isodose curves distribution.

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