• 제목/요약/키워드: symmetric near-ring

검색결과 19건 처리시간 0.022초

P-STRONGLY REGULAR NEAR-RINGS

  • Dheena, P.;Jenila, C.
    • 대한수학회논문집
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    • 제27권3호
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    • pp.483-488
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    • 2012
  • In this paper we introduce the notion of P-strongly regular near-ring. We have shown that a zero-symmetric near-ring N is P-strongly regular if and only if N is P-regular and P is a completely semiprime ideal. We have also shown that in a P-strongly regular near-ring N, the following holds: (i) $Na$ + P is an ideal of N for any $a{\in}N$. (ii) Every P-prime ideal of N containing P is maximal. (iii) Every ideal I of N fulfills I + P = $I^2$ + P.

An Alternative Perspective of Near-rings of Polynomials and Power series

  • Shokuhifar, Fatemeh;Hashemi, Ebrahim;Alhevaz, Abdollah
    • Kyungpook Mathematical Journal
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    • 제62권3호
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    • pp.437-453
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    • 2022
  • Unlike for polynomial rings, the notion of multiplication for the near-ring of polynomials is the substitution operation. This leads to somewhat surprising results. Let S be an abelian left near-ring with identity. The relation ~ on S defined by letting a ~ b if and only if annS(a) = annS(b), is an equivalence relation. The compressed zero-divisor graph 𝚪E(S) of S is the undirected graph whose vertices are the equivalence classes induced by ~ on S other than [0]S and [1]S, in which two distinct vertices [a]S and [b]S are adjacent if and only if ab = 0 or ba = 0. In this paper, we are interested in studying the compressed zero-divisor graphs of the zero-symmetric near-ring of polynomials R0[x] and the near-ring of the power series R0[[x]] over a commutative ring R. Also, we give a complete characterization of the diameter of these two graphs. It is natural to try to find the relationship between diam(𝚪E(R0[x])) and diam(𝚪E(R0[[x]])). As a corollary, it is shown that for a reduced ring R, diam(𝚪E(R)) ≤ diam(𝚪E(R0[x])) ≤ diam(𝚪E(R0[[x]])).

A KIND OF NORMALITY RELATED TO REGULAR ELEMENTS

  • Huang, Juan;Piao, Zhelin
    • 호남수학학술지
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    • 제42권1호
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    • pp.93-103
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    • 2020
  • This article concerns a property of Abelain π-regular rings. A ring R shall be called right quasi-DR if for every a ∈ R there exists n ≥ 1 such that C(R)an ⊆ aR, where C(R) means the monoid of regular elements in R. The relations between the right quasi-DR property and near ring theoretic properties are investigated. We next show that the class of right quasi-DR rings is quite large.

Ultrathin Metamaterial for Polarization Independent Perfect Absorption and Band-pass Filter

  • Zhang, Xu;Gong, Zhijie
    • Journal of the Optical Society of Korea
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    • 제19권6호
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    • pp.665-672
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    • 2015
  • We demonstrate an ultrathin metamaterial for polarization independent perfect absorption as well as a band-pass filter (BPF) which works at a higher frequency band compared to the perfect absorption band. The planar metamaterial is comprised of three layers, symmetric split ring resonators (SSRRs) at the front and structured ground plane (SGP) at the back separated by a dielectric layer. The perfect metamaterial absorber (MA) can realize near 100% absorption due to high electromagnetic losses from the electric and/or magnetic resonances within a certain frequency band. The thickness of the structure is only 1/28 of the maximum absorption wavelength.

On Comaximal Graphs of Near-rings

배경회전 하의 수평 보텍스의 거동 (Motion of a Horizontal Vortex Under a Background Rotation)

  • 서용권;여창호
    • 대한기계학회논문집B
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    • 제29권10호
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    • pp.1101-1110
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    • 2005
  • In this paper we present the numerical results of the behavior of the horizontal vortex generated by ejecting a liquid vertically upward from an orifice into the bulk fluid above the orifice. The numerical calculation has been performed for the axi-symmetric Navier-Stokes equation. A simple flow-visualization experiment was also conducted to qualitatively verify the numerical solutions. Three cases of the flow configurations studied in this paper are; firstly, the vortex was generated without any background rotation, secondly, the vortex was made under a full background rotation, and thirdly, the vortex was made during the spin-up process such that only the region adjacent to the side wall was set into motion viewed in the inertial frame of reference. It was shown that the swirl flow at the inlet boundary affects considerably the formation and development of the vortex for the second case. In the third case, it was remarkable to see that the vortex cannot penetrate into the region near to the side wall of the tank, because of the strong swirl flow and corresponding high pressure gradient in the region.

루비듐 증기와 반응한 $Ag^+$ 이온과 $Ca^{2+}$ 이온으로 치환된 제올라이트 A의 결정학적 연구 (Crystallographic Studies of $Ag^+$-and $Ca^{2+}$- Exchanged Zeolite A Reacting with Rubidium Vapor)

  • 한영욱;송승환;김양
    • 한국광물학회지
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    • 제4권1호
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    • pp.22-31
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    • 1991
  • 세 개의 탈수한 $Ag^+$이온과 $Ca^{2+}$ 이온으로 치환한 제올라이트 $A(Ag_4Ca_4-A,\;Ag_^Ca_3-A,\;Ag_8Ca_2-A)$를 0.1 Torr의 Rb 증기로 처리한 결정구조를 공간군 Pm3m을 써서 단결정 X-선 회절법으로 결정하였다. (단위세포상수 a는 각각 $12.271(1){\AA},\;12.255(1){\AA}$$12.339(1){\AA}$이다). 이들 구조의 최종 오차인수 R(무게)는 $I>3{\rho}(I)$가 되는 130 회절반사로 0.072, 110 회절반사로 0.050 및 86 회절반사로 0.082이었다. 각각의 구조에서 Rb 종은 세개의 다른 결정학적 위치에 위치하고 있다. 즉 단위세포당 3개의 $Rb^+$이온은 8-링 중심에 위치하고 약 2.5개 내지 3.0개의 $Rb^+$이온은 소다라이트 동공내 3회 회전축상에 위치한다. 또 Ag 종이 두 개의 다른 결정학적 위치에 위치하고 약 0.7∼2.1개의 $Ag^+$이온은 4-링과 마주보는 위치에, 약 2.2∼4.8개의 Ag 원자는 큰 동공 중심 가까이에 위치한다. 이들 구조에서 단위 세포당 Ag 원자이 수는 각각 2.2, 2.4 및 4.8개이었고 이들은 큰 동공 중심에 헥사실버 클라스터를 만든다. $Rb^+$이온은 8-링을 막고 있어서 Ag가 골조 밖으로 이동하는 것을 막고 있고 각각의 헥사실버 클라스터는 13개의 $Rb^+$ 이온과 배위하여 안정화된다. 단위 세포당 약 0.8개의 Rb원자가 과잉으로 존재하여 삼각 대칭형의 $(Rb_3)^{2+}$클라스터가 소다라이트 동공내의 존재한다. 적어도 하나의 큰 동공의 6-링 $Rb^+$ 이온은 소다라이트 동공의 $(Rb_3)^{2+}$클라스터에 접근하므로 이들 클라스터는 $(Rb)_4^{3+}$, $(Rb)_5^{4+}$ 혹은 $(Rb)_6^{5+}$가 형성될 수도 있다.

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