Browsing by Issue Date, starting with "2011-01-20"
Now showing 1 - 20 of 42325
- Results Per Page
- Sort Options
Item type:Item, Heterogeneous and Homogeneous Nucleation of Epitaxial NiSi(2) in [110] Si Nanowires(2011-01-20) ;Chou, Yi-Chia ;Wu, Wen-Wei ;Lee, Chung-Yang ;Liu, Chun-YiChen, Lih-JuannWe report here both heterogeneous and homogeneous nucleation of epitaxial suicide of NiSi(2) in Si nanowires grown in [110] direction by in situ observation in high-resolution transmission electron microscopy (TEM). Owing to the excellent lattice match between Si and NiSi(2), a giant epitaxial step of 2-8 nm wide forms at the interface between Si and NiSi(2) during the growth of the latter. The step formation results in two suicide/Si interfaces parallel to each other in TEM observations. Heterogeneous nucleation of NiSi(2) occurs at the intersection where the step meets the interfaces. However, we have also observed the epitaxial growth of NiSi(2) having a single interface with the Si, i.e., without a giant step. Homogeneous nucleation of NiSi(2) occurs on the single interface. Incubation time of heterogeneous nucleation of NiSi(2) has been measured by high-resolution video to be much shorter than that of homogeneous nucleation. The overall growth rate of NiSi(2) for the case of heterogeneous nucleation is faster than that for the case of homogeneous nucleation. Kinetic analysis of both types of nucleation is presented for a direct comparison in order to have a better understanding of the nucleation events.Item type:Item, Heterogeneous and Homogeneous Nucleation of Epitaxial NiSi2 in [110] Si Nanowires(2011-01-20) ;Chou, Yi-Chia ;Wu, Wen-Wei ;Lee, Chung-Yang ;Liu, Chun-YiChen, Lih-JuannWe report here both heterogeneous and homogeneous nucleation of epitaxial suicide of NiSi2 in Si nanowires grown in [110] direction by in situ observation in high-resolution transmission electron microscopy (TEM). Owing to the excellent lattice match between Si and NiSi2, a giant epitaxial step of 2-8 nm wide forms at the interface between Si and NiSi2 during the growth of the latter. The step formation results in two suicide/Si interfaces parallel to each other in TEM observations. Heterogeneous nucleation of NiSi2 occurs at the intersection where the step meets the interfaces. However, we have also observed the epitaxial growth of NiSi2 having a single interface with the Si, i.e., without a giant step. Homogeneous nucleation of NiSi2 occurs on the single interface. Incubation time of heterogeneous nucleation of NiSi2 has been measured by high-resolution video to be much shorter than that of homogeneous nucleation. The overall growth rate of NiSi2 for the case of heterogeneous nucleation is faster than that for the case of homogeneous nucleation. Kinetic analysis of both types of nucleation is presented for a direct comparison in order to have a better understanding of the nucleation events.Item type:Item, 自己整合薄膜トランジスタの製造方法とその構造体(2011-01-20) ;周政偉 ;冉暁▲ブン▼蔡娟娟【課題】自己整合薄膜トランジスタ(TFT)の製造方法を提供する。【解決手段】先ず、透明基板の第1表面上に酸化物ゲート、誘電体層、及びフォトレジスト層を順に堆積する。次に、該透明基板の第1表面と反対側の第2表面に紫外光を照射することで、該フォトレジスト層を露光する。この時、該酸化物ゲートからなるゲートはマスクとして働き、該フォトレジスト層の該酸化物ゲートに対応する部分に照射される紫外光を吸収する。次に、該露光されたフォトレジスト層を除去し、該フォトレジスト層の未露光部分と該誘電体層との上に透明導電層を堆積する。次に、該透明導電層にパターン形成プロセスを実行して、ソースとドレインとを形成し、ソース、ドレイン、及び誘電体層を覆うようアクティブ層を形成して、自己整合TFT構造体が完成する。【選択図】図1Item type:Item, Drug Delivery Nanodevice, its Preparation Method and Uses Thereof(2011-01-20) ;Chen, San-Yuan ;Hu, Shang-Hsiu ;Liu, Dean-MoKuo, Kun-TingNanodevice and method for in vivo monitoring and release of drugs are provided. The disclosed nanodevice is characterized in having a drug-loaded nanosphere that is capable of releasing the encapsulated drugs upon magnetically stimulation. The nanodevice may also be used as a contrast agent for in vivo imaging and monitoring the concentration and distribution of the released drugs and/or active compounds injected separately into a target site of a subject.Item type:Item, Direct spectroscopic evidence of charge reversal at the Pb(Zr(0.2)Ti(0.8))O(3)/La(0.7)Sr(0.3)MnO(3) heterointerface(2011-01-21) ;Wu, Chung-Lin ;Lee, Pei-Wei ;Chen, Yi-Chun ;Chang, Lo-YuehChen, Chia-HaoAt the heterointerface of a top ferroelectric Pb(Zr(0.2)Ti(0.8))O(3) (PZT) ultrathin film and a bottom La(0.7)Sr(0.3)MnO(3) (LSMO) electrode, we used continuous synchrotron-radiation photoelectron spectroscopy to probe in situ and demonstrated that the interfacial charges are reversible and their affected valence-band barrier height becomes modulated upon switching the polarization in the top layer. By monitoring the core-level shifting of the buried LSMO layer under continuous illumination of synchrotron radiation, we directly observed a temporal screening of polarization induced by the photon-generated carriers in the top PZT layer. This dynamic characterization of the core-level shifting of the buried layer demonstrates an effective method to probe the electric conduction and ferroelectric polarization of an ultrathin ferroelectric oxide thin film.Item type:Item, Direct spectroscopic evidence of charge reversal at the Pb(Zr0.2Ti0.8)O-3/La0.7Sr0.3MnO3 heterointerface(2011-01-21) ;Wu, Chung-Lin ;Lee, Pei-Wei ;Chen, Yi-Chun ;Chang, Lo-YuehChen, Chia-HaoAt the heterointerface of a top ferroelectric Pb(Zr0.2Ti0.8)O-3 (PZT) ultrathin film and a bottom La0.7Sr0.3MnO3 (LSMO) electrode, we used continuous synchrotron-radiation photoelectron spectroscopy to probe in situ and demonstrated that the interfacial charges are reversible and their affected valence-band barrier height becomes modulated upon switching the polarization in the top layer. By monitoring the core-level shifting of the buried LSMO layer under continuous illumination of synchrotron radiation, we directly observed a temporal screening of polarization induced by the photon-generated carriers in the top PZT layer. This dynamic characterization of the core-level shifting of the buried layer demonstrates an effective method to probe the electric conduction and ferroelectric polarization of an ultrathin ferroelectric oxide thin film.Item type:Item, Solute-solvent intermolecular vibronic coupling as manifested by the molecular near-field effect in resonance hyper-Raman scattering(2011-01-21) ;Shimada, Rintaro ;Hamaguchi, Hiro-o ;應用化學系 ;應用化學系分子科學碩博班Department of Applied ChemistryVibronic coupling within the excited electronic manifold of the solute all-trans-beta-carotene through the vibrational motions of the solvent cyclohexane is shown to manifest as the "molecular near-field effect," in which the solvent hyper-Raman bands are subject to marked intensity enhancements under the presence of all-trans-beta-carotene. The resonance hyper-Raman excitation profiles of the enhanced solvent bands exhibit similar peaks to those of the solute bands in the wavenumber region of 21 700-25 000 cm(-1) (10 850-12 500 cm(-1) in the hyper-Raman exciting wavenumber), where the solute all-trans-beta-carotene shows a strong absorption assigned to the 1A(g) -> 1B(u) transition. This fact indicates that the solvent hyper-Raman bands gain their intensities through resonances with the electronic states of the solute. The observed excitation profiles are quantitatively analyzed and are successfully accounted for by an extended vibronic theory of resonance hyper-Raman scattering that incorporates the vibronic coupling within the excited electronic manifold of all-trans-beta-carotene through the vibrational motions of cyclohexane. It is shown that the major resonance arises from the B-term (vibronic) coupling between the first excited vibrational level (v = 1) of the 1B(u) state and the ground vibrational level (v = 0) of a nearby A(g) state through ungerade vibrational modes of both the solute and the solvent molecules. The inversion symmetry of the solute all-trans-beta-carotene is preserved, suggesting the weak perturbative nature of the solute-solvent interaction in the molecular near-field effect. The present study introduces a new concept, " intermolecular vibronic coupling," which may provide an experimentally accessible/theoretically tractable model for understanding weak solute-solvent interactions in liquid. (C) 2011 American Institute of Physics. [doi:10.1063/1.3512923]Item type:Item, 空時編碼/正交分頻多工系統中合併通道估計與資料偵測方法(2011-01-21) ;古孟霖黃家齊本發明係以最佳化方法合併通道估計及資料偵測,利用資料子載波與稀疏領航子載波追蹤通道變化;其特徵在於使用牛頓法及資料子載波達到合併通道估計及資料偵測之最佳化,並利用稀疏領航子載波所形成之最大相似函數之一階部分微分方向向量做為通道估計器追蹤通道變化之初始參考方向以得到更好的通道估計。本發明在高車行速度及大通道延遲環境下具有良好系統效能表現。Item type:Item, 交大e-News第087期(2011-01-21) ;Secretariat國立交通大學秘書室Item type:Item, Integration structure of semiconductor circuit and microprobe sensing elements and method for fabricating the same(2011-01-25) ;Chiou ;Jin-Chern ;ChangChih-WeiThe present invention discloses an integration structure of a semiconductor circuit and microprobe sensing elements and a method for fabricating the same. In the method of the present invention, a semiconductor circuit is fabricated on one surface of a semiconductor substrate, and the other surface of the semiconductor substrate is etched to form a microprobe structure for detect physiological signals. Next, a deposition method is used to sequentially form an electrical isolated layer and an electrical conductive layer on the microprobes. Then, an electrical conductive material is used to electrically connect the electrical conductive layer with the electrical pads of the semiconductor circuit. Thus is achieved the integration of a semiconductor circuit and microprobe sensing elements in an identical semiconductor substrate with the problem of electric electrical isolated being solved simultaneously. Thereby, the voltage level detected by the microprobes will not interfere with the operation of the semiconductor circuit.Item type:Item, Seebeck coefficients in nanoscale junctions: Effects of electron-vibration scattering and local heating(2011-01-25) ;Hsu, Bailey C. ;Liu, Yu-Shen ;Lin, Sheng Hsien ;Chen, Yu-Chang電子物理學系We report first-principles calculations of inelastic Seebeck coefficients in an aluminum monatomic junction. We compare the elastic and inelastic Seebeck coefficients with and without local heating. In the low-temperature regime, the signature of normal modes in the profiles of the inelastic Seebeck effects is salient. The inelastic Seebeck effects are enhanced by the normal modes and further magnified by local heating. In the high-temperature regime, the inelastic Seebeck effects are weakly suppressed due to the quasiballistic transport.Item type:Item, Investigation of low-temperature electroluminescence of InGaN/GaN based nanorod light emitting arrays(2011-01-28) ;Huang, Ying-Yuan ;Chen, Liang-Yi ;Chang, Chun-Hsiang ;Sun, Yu-HsuanCheng, Yun-WeiFor InGaN/GaN based nanorod devices using a top-down etching process, the optical output power is affected by non-radiative recombination due to sidewall defects (which decrease light output efficiency) and the mitigated quantum confined Stark effect (QCSE) due to strain relaxation (which increases internal quantum efficiency). Therefore, the exploration of low-temperature optical behaviors of nanorod light emitting diodes (LEDs) will help identify the correlation between these two factors. In this work, low-temperature electroluminescent (EL) spectra of InGaN/GaN nanorod arrays were explored and compared with those of planar LEDs. The nanorod LED exhibits a much higher optical output percentage increase when the temperature decreases. The increase is mainly attributed to the increased carriers in the quantum wells for radiative recombination. Also, due to a better spatial overlap of electrons and holes in the quantum wells, the increased number of carriers can be more efficiently recombined in the nanorod device. Next, while the nanorod array shows nearly constant peak energy in the EL spectra at various injection currents at the temperature of 300 K, a blue shift has been observed at 190 K. The results suggest that with less non-radiative recombination and thus more carriers in the quantum wells, carrier screening and band filling still prevail in the partially strain relaxed nanorods. Moreover, when the temperature drops to 77 K, the blue shift of both nanorod and planar devices disappears and the optical output power decreases since there are fewer carriers in the quantum wells for radiative recombination.Item type:Item, Association structures of ionic liquid/DMSO mixtures studied by high-pressure infrared spectroscopy(2011-01-28) ;Jiang, Jyh-Chiang ;Lin, Kuan-Hung ;Li, Sz-Chi ;Shih, Pao-MingHung, Kai-ChanUsing high-pressure infrared methods, we have investigated close interactions of charge-enhanced C-H-O type in ionic liquid/dimethyl sulfoxide (DMSO) mixtures. The solvation and association of the 1-butyl-3-methylimidazolium tetrafluoroborate (BMI(+)BF(4)(-)) and 1-butyl-2,3-dimethylimidazolium tetrafluoroborate (BMM(+)BF(4)(-)) in DMSO-d(6) were examined by analysis of C-H spectral features. Based on our concentration-dependent results, the imidazolium C-H groups are more sensitive sites for C-H-O than the alkyl C-H groups and the dominant imidazolium C-H species in dilute ionic liquid/DMSO-d(6) should be assigned to the isolated (or dissociated) structures. As the dilute mixtures were compressed by high pressures, the loss in intensity of the bands attributed to the isolated structures was observed. In other words, high pressure can be used to perturb the association-dissociation equilibrium in the polar region. This result is remarkably different from what is revealed for the imidazolium C-H in the BMM(+)BF(4)(-)/D(2)O mixtures. DFT-calculations are in agreement with our experimental results indicating that C(4)-H-O and C(5)-H-O interactions seem to play non-negligible roles for BMM(+)BF(4)(-)/DMSO mixtures. (C) 2011 American Institute of Physics. [doi:10.1063/1.3526485]Item type:Item, Molecular structural property and potential energy dependence on nonequilibrium-thermodynamic state point of liquid n-hexadecane under shear(2011-01-28) ;Tseng, Huan-Chang ;Chang, Rong-Yeu ;Wu, Jiann-Shing ;應用化學系Department of Applied ChemistryExtensive computer experiments have been conducted in order to shed light on the macroscopic shear flow behavior of liquid n-hexadecane fluid under isobaric-isothermal conditions through the nonequilibrium molecular dynamic methodology. With respect to shear rates, the accompanying variations in structural properties of the fluid span the microscopic range of understanding from the intrinsic to extrinsic characteristics. As drawn from the average value of bond length and bond angle, the distribution of dihedral angle, and the radius distribution function of intramolecular and intermolecular van der Waals distances, these intrinsic structures change with hardness, except in the situation of extreme shear rates. The shear-induced variation of thermodynamic state curve along with the shear rate studied is shown to consist of both the quasiequilibrium state plateau and the nonequilibrium-thermodynamic state slope. Significantly, the occurrence of nonequilibrium-thermodynamic state behavior is attributed to variations in molecular potential energies, which include bond stretching, bond bending, bond torsion, and intra-and intermolecular van der Waals interactions. To unfold the physical representation of extrinsic structural deformation, under the aggressive influence of a shear flow field, the molecular dimension and appearance can be directly described via the squared radius of gyration and the sphericity angle, R(g)(2) and phi, respectively. In addition, a specific orientational order S(x) defines the alignment of the molecules with the flow direction of the x-axis. As a result, at low shear rates, the overall molecules are slightly stretched and shaped in a manner that is increasingly ellipsoidal. Simultaneously, there is an obvious enhancement in the order. In contrast to high shear rates, the molecules spontaneously shrink themselves with a decreased value of R(g)(2), while their shape and order barely vary with an infinite value of phi and S(x). It is important to note that under different temperatures and pressures, these three parameters are integrated within a molecular description in response to thermodynamic state variable of density and rheological material function of shear viscosity. (C) 2011 American Institute of Physics. [doi:10.1063/1.3541825]Item type:Item, Compact microdisk cavity laser with type-II GaSb/GaAs quantum dots(2011-01-31) ;Hsu, K. S. ;Chiu, T. T. ;Lin, Wei-Hsun ;Chen, K. L.Shih, M. H.Microdisk lasers with active region made of type-II GaSb/GaAs quantum dots on the GaAs substrate have been demonstrated. A microdisk cavity with diameter of 3.9 mu m was fabricated from a 225-nm-thick GaAs layer filled with GaSb quantum dots. Lasing at wavelengths near 1000 nm at 150 K was achieved for this microdisk. A high threshold characteristic temperature of 77 K was also observed. It is found that the lasing wavelength matches closely with the first-order whispering-gallery mode of the cavity as obtained from the finite-element method simulation. (c) 2011 American Institute of Physics. [doi: 10.1063/1.3543839]Item type:Item, A reflective polarizer-free electro-optical switch using dye-doped polymer-stabilized blue phase liquid crystals(2011-01-31) ;Lin, Yi-Hsin ;Chen, Hung-Shan ;Chiang, Tsung-Han ;Wu, Chun-HungHsu, Hsu-KuanWe demonstrate a reflective polarizer-free electro-optical switch using dye-doped polymer-stabilized blue phase liquid crystals (DDPSBP-LC). At the voltage-off state, the dye molecules and liquid crystals form the structure of the double twist cylinders. As a result, the DDPSBP-LC is in dark state due to the combination of Bragg reflection and light absorption. At the voltage-on state, the blue phase structure is unwound locally. The DDPSBP-LC is then in bright state because of the small light absorption only. The applications of such a switch are shutter glass of 3D displays, and electronic papers. (C) 2011 Optical Society of AmericaItem type:Item, Stacked GeO/SrTiO(x) Resistive Memory with Ultralow Resistance Currents(2011-01-31) ;Cheng, C. H. ;Chin, Albert ;Yeh, F. S. ;電子工程學系及電子研究所Department of Electronics Engineering and Institute of ElectronicsWe report a high performance and low-power operated resistive memory. Using stacked covalent-bond-dielectric GeO(x) on metal-oxide SrTiO(x) to form the cost-effective Ni/GeO(x)/SrTiO(x)/TaN resistive random access memory, ultralow set power of small 1 mu W (0.9 mu A at 1.2 V), reset power of 13 pW (0.13 nA at 0.1 V), fast 50 ns switching time and good 10(6) cycling endurance are realized. (C) 2011 American Institute of Physics. [doi:10.1063/1.3549689]Item type:Item, Implementation issues of the nearfield equivalent source imaging microphone array(2011-01-31) ;Bai, Mingsian R. ;Lin, Jia-Hong ;Tseng, Chih-Wen ;機械工程學系Department of Mechanical EngineeringThis paper revisits a nearfield microphone array technique termed nearfield equivalent source imaging (NESI) proposed previously. In particular, various issues concerning the implementation of the NESI algorithm are examined. The NESI can be implemented in both the time domain and the frequency domain. Acoustical variables including sound pressure, particle velocity, active intensity and sound power are calculated by using multichannel inverse filters. Issues concerning sensor deployment are also investigated for the nearfield array. The uniform array outperformed a random array previously optimized for far-field imaging, which contradicts the conventional wisdom in far-field arrays. For applications in which only a patch array with scarce sensors is available, a virtual microphone approach is employed to ameliorate edge effects using extrapolation and to improve imaging resolution using interpolation. To enhance the processing efficiency of the time-domain NESI, an eigensystem realization algorithm (ERA) is developed. Several filtering methods are compared in terms of computational complexity. Significant saving on computations can be achieved using ERA and the frequency-domain NESI, as compared to the traditional method. The NESI technique was also experimentally validated using practical sources including a 125 cc scooter and a wooden box model with a loudspeaker fitted inside. The NESI technique proved effective in identifying broadband and non-stationary sources produced by the sources. (C) 2010 Elsevier Ltd. All rights reserved.Item type:Item, Nitrogenated amorphous InGaZnO thin film transistor(2011-01-31) ;Liu, Po-Tsun ;Chou, Yi-Teh ;Teng, Li-Feng ;Li, Fu-HaiShieh, Han-PingThis work presents the electrical characteristics of the nitrogenated amorphous InGaZnO thin film transistor (a-IGZO:N TFT). The a-IGZO: N film acting as a channel layer of a thin film transistor (TFT) device was prepared by dc reactive sputter with a nitrogen and argon gas mixture at room temperature. Experimental results show that the in situ nitrogen incorporation to IGZO film can properly adjust the threshold voltage and enhance the ambient stability of a TFT device. Furthermore, the a-IGZO: N TFT has a 44% increase in the carrier mobility and electrical reliability and uniformity also progress obviously while comparing with those not implementing a nitrogen doping process. (C) 2011 American Institute of Physics. [doi:10.1063/1.3551537]Item type:Item, A facile route to prepare PdPt alloys for ethanol electro-oxidation in alkaline electrolyte(2011-01-31) ;Lin, Sheng-Chieh ;Chen, Jing-Yu ;Hsieh, Yi-Fan ;Wu, Pu-Wei材料科學與工程學系We adopted a displacement reaction in acidic solution that enabled the spontaneous reduction of Pd and Pt cations in conjunction with corrosive dissolution of Ni. The composition for the PdPt was adjusted by varying the concentration of Pd and Pt cations. From SEM images and XRD patterns, the PdPt formed an fcc alloy uniformly deposited on the Ni substrate. Electro-oxidation of ethanol was conducted in alkaline electrolyte for samples of Pd, Pt, and PdPt alloys. In cyclic voltammetric profiles, the Pd(77)Pt(23) revealed the highest electrocatalytic ability in both apparent current and mass activity, followed by Pd(87)Pt(13), Pd, and Pt. Similar behaviors were observed in life time measurements in which stable performances for ethanol electro-oxidation were obtained. (C) 2010 Elsevier B.V. All rights reserved.