• 제목/요약/키워드: spin-up

검색결과 268건 처리시간 0.033초

Flow Characteristics in Spin-Up of a Three-Layer Fluid

  • Sviridov Evgeny;Hyun Jae Min
    • Journal of Mechanical Science and Technology
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    • 제20권2호
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    • pp.271-277
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    • 2006
  • A numerical study is made of the spin-up from rest of a three-layer fluid in a closed, vertically-mounted cylinder. The densities in the upper layer $\rho_1$, middle layer $\rho_2$ and lower layer $\rho_3\;are\;\rho_3\;>\;\rho_2\;>\;\rho_1$, and the kinematic viscosities are left arbitrary. The representative system Ekman number is small. Numerical solutions are obtained to the time-dependent axisymmetric Navier-Stokes equations, and the treatment of the interfaces is modeled by use of the Height of Liquid method. Complete three-component velocity fields, together with the evolution of the interface deformations, are depicted. At small times, when the kinematic viscosity in the upper layer is smaller than in the middle layer, the top interface rises (sinks) in the central axis (peripheral) region. When the kinematic viscosity in the lower layer is smaller than in the middle layer, the bottom interface rises (sinks) in the periphery (axis) region. Detailed shapes of interfaces are illustrated for several cases of exemplary viscosity ratios.

Period changes in the Intermediate Polar MU Camelopardalis

  • Park, Jiwon;Yoon, Jho-Na;Kim, Yonggi;Andronov, I.L.
    • 천문학회보
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    • 제40권1호
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    • pp.89.1-89.1
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    • 2015
  • Period changes found in the 10 years CCD BVR photometry data (2005 - 2014) of the Intermediate Polar MU Cam will be discussed. The timings of extrema of the data are determined and the new ephemeris for the spin period and orbital period have been calculated by using multi-periodic approximation as follows: BJD(orb)=2454085.46(19)+0.19664 $10(26){\cdot}E$ and BJD(spin)=2454085.50725(91)+0.013740942(13) ${\cdot}$ $E-1.51(10){\times}10^{-12}{\cdot}E^2$. The O-C diagram shows an increasing of the spin period as $P=-2.20(14){\cdot}10^{-12}s/s$. It is also found in MU Cam that the white dwarf's rotation seems to be switched from a state of spin-down to spin-up by the white dwarf's equilibrium spin period in 2005.

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Interface Engineering in Quasi-Magnetic Tunnel Junctions with an Organic Barrier

  • Choi, Deung-Jang;Lee, Nyun-Jong;Kim, Tae-Hee
    • Journal of Magnetics
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    • 제15권4호
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    • pp.185-189
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    • 2010
  • Spin polarized tunneling through a hybrid tunnel barrier of a Spin filter (SF) based on a EuO ferro-magnetic semiconductor and an organic semiconductor (OSC) (rubrene in this case) was investigated. For quasi-magnetic tunnel junction (MTJ) structures, such as Co/rubrene/EuO/Al, we observed a strong spin filtering effect of the EuO layer exhibiting I-V curves with high spin polarization (P) of up to 99% measured at 4 K. However, a magnetoresistance (MR) value of 9% was obtained at 4.2 K. The low MR compared to the high P could be attributed to spin scattering caused by structural defects at the interface between the EuO and rubrene, due to nonstoichiometry in the EuO.

Differential Expression of Spin Transcripts: Oocyte and Somatic Types

  • Oh, Bermseok;Hwang, Sue-Yun;Solter, Davor;Knowles, Barbara
    • Animal cells and systems
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    • 제5권1호
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    • pp.71-75
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    • 2001
  • Spin is an abundant maternal transcript comprising up to 0.2% of the total mRNA stock in mouse oocyte, whose protein product is associated with the meiotic spindle. We have identified a new isoform of Spin transcript containing a distinct 5'-untranslated region and the N-terminus of encoded protein. Northern blot and RT-PCR analysis showed that the new isoform is expressed in embryos and most of adult tissues, while the previously identified transcript is expressed solely in mouse oocyte. We thus designated these two Spin isoforms as somatic type and oocyte type, respectively. To investigate the underlying mechanism for the differential expression, genomic structure of Spin was examined. Spin exists as multiple copies in the genome, some of which appears to be pseudogenes, and characterization of Spin genomic clones indicates that oocyte- and somatic-isoforms were generated by alternative splicing. The complex organization of Spin genomic locus and its multifaceted control of expression provide a good model to study the molecular mechanisms of elaborate genome usage in mammals.

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Determination of Strongly Interacting Spin Exchange Paths in Cu2(O3PCH2PO3) on the Basis of Spin Dimer Analysis

  • Bae, Hyun-Woo;Koo, Hyun-Joo
    • Bulletin of the Korean Chemical Society
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    • 제29권1호
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    • pp.122-126
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    • 2008
  • The magnetic properties of the organic/inorganic hybrid copper-methylenediphosphonate, Cu2(O3PCH2PO3) were examined by performing the spin dimer analysis based on the extended Hckel tight binding method. In Cu2(O3PCH2PO3) the CuO3 chains made up of edge-sharing CuO5 square pyramidal units are inter-linked by O-P-O bridges. The Cu-O-Cu superexchange interactions of the CuO3 chains are negligibly weak compared with the Cu-O…O-Cu super-superexchange interactions that occur between the CuO3 chains. The spin exchange interactions of Cu2(O3PCH2PO3) are dominated by three super-superexchange interactions, which leads to a three-dimensional antiferromagnetic spin lattice. The strongest spin exchange interactions form isolated spin dimers, which suggests that, to a first approximation, the magnetic properties can be described in terms of an isolated spin dimer model.

Spin Wave Interference in Magnetic Nanostructures

  • Yang, Hyun-Soo;Kwon, Jae-Hyun;Mukherjee, Sankha Subhra;Jamali, Mahdi;Hayashi, Masamitsu
    • 한국자기학회:학술대회 개요집
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    • 한국자기학회 2011년도 자성 및 자성재료 국제학술대회
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    • pp.7-8
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    • 2011
  • Although yttrium iron garnet (YIG) has provided a great vehicle for the study of spin waves in the past, associated difficulties in film deposition and device fabrication using YIG had limited the applicability of spin waves to practical devices. However, microfabrication techniques have made it possible to characterize both the resonant as well as the travelling characteristics of spin waves in permalloy (Py). A variety of methods have been used for measuring spin waves, including Brillouin light scattering (BLS), magneto-optic Kerr effect (MOKE), vector network analyzer ferromagnetic resonance (VNA-FMR), and pulse inductive microwave magnetometry (PIMM). PIMM is one of the most preferred methodologies of measuring travelling spin waves. In this method, an electrical impulse is applied at one of two coplanar waveguides patterned on top of oxide-insulated Py, producing a local disturbance in the magnetization of the Py. The resulting disturbance travels down the Py in the form of waves, and is inductively picked up by the other coplanar waveguide. We investigate the effect of the pulse width of excitation pulses on the generated spin wave packets using both experimental results and micromagnetic simulations. We show that spin wave packets generated from electrical pulses are a superposition of two separate spin wave packets, one generated from the rising edge and the other from the falling edge, which interfere either constructively or destructively with one another, depending upon the magnitude and direction of the field bias conditions. A method of spin wave amplitude modulation is also presented by the linear superposition of spin waves. We use interfering spin waves resulting from two closely spaced voltage impulses for the modulation of the magnitude of the resultant spin wave packets.

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Generalization of the Curie-Weiss Model to the D-dimensional Spin System

  • Hyung-june Woo;Eun Kyung Lee;Eok-Kyun Lee
    • Bulletin of the Korean Chemical Society
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    • 제14권4호
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    • pp.485-487
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    • 1993
  • The critical behavior of the classical D-dimensional spin model (D${\ge}$2), which is intermediate model that link up the Ising (D = 1) and the spherical model (D = ${\infty}$), is studied for the case of constant coupling interaction independent of the spin-spin distance (Curie-Weiss model). Analytical results show that the critical behavior of the present model is in quantitative agreement with the prediction of the phenomenological mean-field theory independent of D. Critical temperature is calculated to be T$_c$=k/JD. This gives a quantitative explanation of the relationship between the spin degree of freedom and the critical temperature.

N홉 접근보장의 백본을 이용한 무선 센서 네트워크 데이터 전송 프로토콜 (WSN Data Dissemination Protocol by N-hop Access Guarantee Backbone)

  • 김문성;조상훈;추현승
    • 인터넷정보학회논문지
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    • 제10권1호
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    • pp.43-50
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    • 2009
  • 잘 알려진 무선 센서 네트워크의 프로액티브 프로토콜인 Flooding과 SPIN은 싱크 노드의 요청 없이 감지한 데이터를 즉각적으로 전송한다. 그러나 이러한 전송방법은 그 데이터가 필요하지 않는 노드들에게까지 전송하기에 에너지 효율성 측면에서 비효율적이다. 본 논문에서는 이러한 단점을 극복하기 위해서 전체 노드 대신에 적절한 일부 노드들에게만 전송할 수 있는 세미프로액티브 프로토콜을 제안한다. 따라서 만일 싱크노드와 같은 어떠한 노드가 감지한 데이터를 필요로 할 경우 미리 설정한 몇 홉 이내에 그 데이터를 쉽게 얻을 수 있다. 시뮬레이션 결과는 잘 알려진 SPIN과 비교하여 노드의 에너지 효율성이 약 83%까지 높다는 것을 보여주었다.

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Spin-On Dopants를 이용한 결정질 실리콘 태양전지의 n+ 에미터 형성에 관한 연구 (Investigation of n+ Emitter Formation Using Spin-On Dopants for Crystalline Si Solar Cells)

  • 조경연;이지훈;최준영;이수홍
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2007년도 추계학술대회 논문집
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    • pp.68-69
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    • 2007
  • To make cost-effective solar cells, We have to use low cost material or make short process time or high temperature process. In solar cells, formation of emitter is basic and important technique according to build-up P-N junction. Diffusion process using spin-on dopants has all of this advantage. In this paper, We investigated n+ emitter formation spin-on dopants to apply crystalline silicon solar cells. We known variation of sheet resistance according to variation of temperature and single-crystalline and multi-crystalline silicon wafer using Honeywell P-8545 phosphorus spin-on dopants. We obtain uniformity of sheet resistance within 3~5% changing RPM of spin coater.

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진보된 혼돈 대각화 방법을 이용한 상호작용하는 페르미온 계의 기저상태 계산 (Ground State Computation of Interacting Fermion Systems by using Advanced Stochastic Diagonalization)

  • 안설아;조명원
    • 한국콘텐츠학회:학술대회논문집
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    • 한국콘텐츠학회 2007년도 추계 종합학술대회 논문집
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    • pp.209-211
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    • 2007
  • 2차원 상호작용하는 페르미온 계에 대한 혼돈 대각화 계산의 컴퓨터 계산 시간이, 대칭성 연산과 같은 여러 가지 방법을 이용함으로써 감소되었다. 첫째로, 각각의 격자를 업스핀(${\uparrow}$) 격자와 다운스핀(${\downarrow}$) 격자로 나누어서 2부분 격자가 가능케 했다. 이에 따라, 유효한 바탕 상태는 업스핀 배열에 다운스핀 배열을 겹침으로써 얻어진다. 결과적으로, 시험 바탕 상태를 저장하는데 사용되는 메모리 공간이 현저하게 감소되었다. 두 번째로, 바탕 상태 집합을 구성할 때, 해밀토니안 행렬의 원소들을 순람표에 기록하였다. 그럼으로써, 혼돈 대각화 과정에서 해밀토니안 행렬의 원소들을 반복적으로 계산하는 것을 피했다. 세 번째로, 바탕 상태 집합에 대칭성 연산을 적용함으로써 원 바탕 상태 집합이 대칭성 연산의 고유벡터들로 구성된 새로운 바탕 상태 집합으로 변환되었다. 기저 상태 파동함수는 대칭적인 바탕상태 (결합상태) 집합으로부터 구성되었다. 결과로서, 대칭성 연산을 이용함으로써, 혼돈 대각화 계산에 쓰이는 바탕상태의 총 개수가 50%까지 감소되었다.

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