• 제목/요약/키워드: single-atom

검색결과 192건 처리시간 0.027초

A Numerical Analysis of The Single Trapped Atom Laser

  • Chough, Young-Tak;Moon, Hee-Jong;Kim, Jung-Bog;An, Kyung-Won
    • 한국광학회:학술대회논문집
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    • 한국광학회 1999년도 제16회 광학 및 양자전자 학술발표회Proceedings of 16th Optics and Quantum Electronics Conference, 1999
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    • pp.26-27
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    • 1999
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Strain Dependence of Adsorption Energy of Single Layer MoS2: Possibility of Catalytic Usage

  • 전부경;이창희
    • EDISON SW 활용 경진대회 논문집
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    • 제5회(2016년)
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    • pp.355-356
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    • 2016
  • It is shown that the maximum value of exchange current is obtained where hydrogen adsorption energy is near 0. This enables to estimate catalytic efficiency of a material with hydrogen adsorption energy, which is relatively easier to calculate with density fuctional theory (DFT) method. Strain dependence of the adsorption energy was studied with DFT method and adsorption energy of 0.04 eV per hydrogen atom is obtained at 30% strain.

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Surface-enhanced Raman Scattering(SERS) of Benzylcyanide in Silver Sol

  • 부두완;김관;김명수
    • Bulletin of the Korean Chemical Society
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    • 제9권1호
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    • pp.27-29
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    • 1988
  • The surface-enhanced Raman scattering(SERS) of benzylcyanide in a silver sol was investigated. It was concluded that the molecule adsorbed onto the silver surface via the ${\pi}$ system of the CN group. The molecule was assumed to coordinate with either a single atom or two silver atoms. According to the SERS selection rule, the benzene ring of the adsorbed species seemed to assume a flat stance with respect to the silver surface.

Physics on cancer and its curing

  • Oh, Hung-Kuk
    • 한국감성과학회:학술대회논문집
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    • 한국감성과학회 2000년도 추계학술대회 논문집
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    • pp.91-97
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    • 2000
  • The conventional model did not take momentum conservation into consideration when the electron absorbs and emits the photons. II-ray provides momentum conservations on any directions of the entering photons, and also the electrons have radial momentum conservations and fully elastic bouncing between two atoms, in the new atom model. Conventional atom model must be criticized on the following four points. (1) Natural motions between positive and negative entities are not circular motions but linear going and returning ones, for examples sexual motion, tidal motion, day and night etc. Because the radius of hydrogen atom's electron orbit is the order of 10$^{-11}$ m and the radia of the nucleons in the nucleus are the order of 10$^{-l4}$m and then the converging n-gamma rays to the nucleus have so great circular momentum, the electron can not have a circular motion. We can say without doubt that any elementary mass particle can have only linear motion because of the n-rays' hindrances, near the nucleus. (2) Potential energy generation was neglected when electron changes its orbit from outer one to inner one. The h v is the kinetic energy of the photo-electron. The total energy difference between orbits comprises kinetic and potential energies. (3) The structure of the space must be taken into consideration because the properties of the electron do not change during the transition from outer orbit to inner one even though it produces photon. (4) Total energy conservation law applies to the energy flow between mind and matter because we daily experiences a interconnection between mind and body. An understanding of the mechanisms responsible for the control of normal proliferation and differentiation of the various cell types which make up the human body will undoubtedly allow a greater insight into the abnormal growth of cells, A large body of biochemical evidence was eventually used to generate a receptor model with an external ligand binding domain linked through a single trans-membrane domain to the cytoplasmic tyrosine kinase and autophosphory-lation domains. The ligand induced conformational change in the external domain generates either a push-pull or rotational signal which is transduced from the outside to the inside of cell.l.ell.

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Structural characterization and thermal behaviour of the bis(2-aminothiazole)bis(isothiocyanato)zinc(II) complex, Zn(NCS)2(C3H4N2S)2

  • Suh, Seung Wook;Kim, Inn Hoe;Kim, Chong-Hyeak
    • 분석과학
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    • 제18권5호
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    • pp.386-390
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    • 2005
  • The zinc(II) complex, $Zn(NCS)_2(C_3H_4N_2S)_2$, I, has been synthesized and characterized by single crystal X-ray diffraction, thermal analysis and infrared spectroscopy. The complex I crystallizes in the triclinic system, $P\bar{1}$ space group with a = 7.587(1), b = 8.815(1), $c=12.432(2){\AA}$, ${\alpha}=75.584(8)$, ${\beta}=83.533(9)$, ${\gamma}=68.686(8)^{\circ}$, $V=750.0(2){\AA}^3$, Z = 2, $R_1=0.036$ and ${\omega}R_2=0.101$. The central Zn(II) atom has a tetrahedral coordination geometry, with the heterocyclic nitrogen atoms of 2-aminothiazole ligands and the nitrogen atoms of isothiocyanate ligands. The crystal structure is stabilized by one-dimensional networks of the intermolecular $N-H{\cdots}S$ hydrogen bonds between the amino group of 2-aminothiazole ligands and the sulfur atom of isothiocyanate ligands. Based on the results of thermal analysis, the thermal decomposition reaction of complex I was analyzed to have three distinctive stages such as the loss of 2-aminothiazole, the decomposition of isothiocyanate and the formation of metal oxide.

연속적 라비 진동과 불연속적 양자도약의 양립성 (Compatibility of Continuous Rabi Oscillation and Discontinuous Quantum Jumps)

  • 조영탁;김기식
    • 한국광학회지
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    • 제23권2호
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    • pp.77-86
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    • 2012
  • 양자물리학적 패러다임이 발견된 이래, 라비(Rabi) 진동과 같은 전자(electron)의 에너지 준위 간 연속적인 천이(transition)와 보어(Bohr) 모형으로 대표되는 불연속적 양자 도약(quantum jump)의 상충성(incompatibility)은 현재까지도 서로 자연스럽게 연결하기가 어려운 오랜 개념적 어려움으로 남아 있다. 본 연구에서는 그러나, 빛과 물질의 상호작용을 기술하는 현대적 이론 중의 하나인 양자궤적이론(quantum trajectory theory)의 관점에서 단일 모드 공진기 장(single mode cavity field)과 상호작용하는 단일 원자의 행동을 관찰한 바, 원자-장 간 상호작용의 강도(strength)가 줄어듦에 따라서 원자의 행동이 연속적 라비 진동으로부터 불연속적 양자도약의 양상으로 점진적으로 변화하여 가는 과정을 발견하고, 이 단순하면서도 흥미로운 현상에 대하여 보고한다.

1,6-Anhydropyranose의 분자구조의 역학적응용 (Application of Molecular Mechanics to the Structure of 1,6-Anhydropyranoses)

  • ;박영자
    • 대한화학회지
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    • 제23권4호
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    • pp.206-209
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    • 1979
  • Empirical force-field method를 단결정 회절방법으로 구조가 연구된 여덟개의 1,6-anhydropyranose 분자구조$^{13{\sim}21}$에 적용하였다. 이론적 계산에서도 분자들간의 pyranose고리 conformation의 $^1C_4$$E_0$ 사이간의 차이는 실험치와 비슷하게 얻어졌다. Five-membered anhydro 고리의 분자들간의 작은 conformation 차이는 잘 예측되지 않았다. C-C결합 길이의 계산치는 실험치와 0.012${\AA}$내에서, C-O결합 길이는 0.027${\AA}$내에서, non-hydrogen atom의 결합각은 1.9$^{\circ}$이내에서 일치되고 있다

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Thiocyanat 및 1,2-Diaminocyclohexane 리간드로 구성된 카드뮴(II) 착물의 합성 및 결정구조 (Synthesis and Crystal Structure of the Cadmium(II) Complex with Thiocyanate and 1,2-Diaminocyclohexane Ligands)

  • 김인회;서승욱;김종혁;김진규;서일환
    • 한국결정학회지
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    • 제12권4호
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    • pp.207-211
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    • 2001
  • Cd(SCN)₂{CH/sub 6/H/sub 10/(NH₂)₂}₂(1) 착물을 합성하고 단결성 X-선 회절법으로 구조를 규명하였다. 이 착물은 단사정계, 공간국 P2₁/ space group with a=11.842(2), b=7.926(2), c=11.291(2) Å, β=106.73(3)°V=1014.8(4)Ų, Z=2 로 결정화되었으며, 1775 개의 독립적인 회절반점에 대한 최종 신뢰도 인자 R₁및 ωR₂값은 각각 0.0518 및 0.1315이었다. 착물의 결정 구조는 2개의1,2-Diaminocyclohexane리간드의 질소 원자 xy 평면에서 Cd(II) 금속원자에 chelate 되어 5-membered ring을 형성하며, 2개의 thiocyanate 리간드의 황 원자가 z 축 방향으로 Cd(II) 금속 원자에 트란스 형태로 결합함으로 써 z축 방향으로 약간 늘러진 팔면체 구조의 착물을 형성한다.

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Terahertz time domain spectroscopy of GdBCO superconducting thin films

  • Ji, Gangseon;Park, Woongkyu;Lee, Hyoung-Taek;Song, Chang-Yun;Seo, Choongwon;Park, Minjo;Kang, Byeongwon;Kim, Kyungwan;Kim, Dai-Sik;Park, Hyeong-Ryeol
    • 한국초전도ㆍ저온공학회논문지
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    • 제21권1호
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    • pp.15-17
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    • 2019
  • We present terahertz optical properties of $GdBa_2Cu_3O_{7-x}$ (GdBCO) superconducting thin films. GdBCO films with a thickness of about 105 nm were grown on a $LaAlO_3$ (LAO) single crystal substrate using a conventional pulsed laser deposition (PLD) technique. Using an Ar ion milling system, the thickness of the GdBCO film was reduced to 58 nm, and its surface was also smoothened. Terahertz (THz) transmission spectra through two different GdBCO films are measured over the range between 0.2 and 1.5 THz using THz time domain spectroscopy. Interestingly, the THz transmission of the thinner GdBCO film has been increased to six times larger than that of the thicker one, while the thinner film is still maintaining its superconducting property at below 90 K.