• Journal of Magnetics
• /
• 제20권4호
• /
• pp.347-352
• /
• 2015

The magnetoelectric (ME) characteristics for Terfenol-D/PZT laminate composite dependence on bias magnetic field is investigated. At low frequency, ME response is determined by the piezomagnetic coefficient $d_{33,m}$ and the elastic compliance $s_{33}^H$ of magnetostrictive material, $d_{33,m}$ and $s_{33}^H$ for Terfenol-D are inherently nonlinear and dependent on $H_{dc}$, leading to the influence of $H_{dc}$ on low-frequency ME voltage coefficient. At resonance, the mechanical quality factor $Q_m$ dependences on $H_{dc}$ results in the differences between the low-frequency and resonant ME voltage coefficient with $H_{dc}$. In terms of ${\Delta}E$ effect, the resonant frequency shift is derived with respect to the bias magnetic field. Considering the nonlinear effect of magnetostrictive material and $Q_m$ dependence on $H_{dc}$c, it predicts the low-frequency and resonant ME voltage coefficients as a function of the dc bias magnetic field. A good agreement between the theoretical results and experimental data is obtained and it is found that ME characteristics dependence on $H_{dc}$ are mainly influenced by the nonlinear effect of magnetostrictive material.

• 한국전기전자재료학회논문지
• /
• 제11권9호
• /
• pp.687-692
• /
• 1998

Silicon doped $Al_{0.32}Ga_{0.68}As$ were growth by molecular beam epitaxy. Electroreflectance(ER) spectra of the $E_1$ transition of Schottky barrier Au/n-$Al_{0.32}Ga_{0.68}As$ have been measured at various modulation voltage($V_{ac}$) and dc bias voltage($V_{bias}$). from the $E_1$peak, band gap energy of the $Al_{0.32}Ga_{0.68}As$ is 1.883 eV which corresponds to an Al composition of 32%. As modulation voltage($V_{bias}$) is changed, a line shape at the $E_1$transition does not change, but its amplitude varies linearly. The amplitude of $E_1$signal decrease with increasing the forward dc bias voltage($V_{bias}$), but the line shape does not change. It suggests that the low field theory rather than Franz-Keldysh oscillation is Required to interpret spectra. Also, spectra at the $E_1$transition were broadened with increasing the reverse dc bias voltage($V_{bias}$) which suggests the presence of Field-induced broadening.

• 전기전자학회논문지
• /
• 제27권4호
• /
• pp.418-424
• /
• 2023

본 연구에서는 더블게이트 실리콘 나노시트 (SiNS) 피드백 전계효과 트랜지스터(FBFET)의 전기적 특성에 열처리가 미치는 영향을 분석하였다. 1000 초 동안 바이어스 스트레스를 인가했을 때 더블게이트 SiNS FBFET는 inversion layer의 전자에 의한 계면 트랩의 증가로 인해 채널 모드와 무관하게 negative bias stress 보다는 positive bias stress의 영향을 더 많이 받았다. 300 ℃에서 10 분 동안 열처리를 진행한 이후 소자는 원래의 특성을 완전히 회복하였으며 다시 1000 초 동안 바이어스 스트레스를 인가해도 특성이 변하지 않았다.

• 대한전기학회논문지
• /
• 제38권10호
• /
• pp.840-847
• /
• 1989

It is an important problem that the plasma of high B value is to be confined safely in the research of plasma fusion. So, the Reversed Field Pinch (RFP) plasma has been studied. RFP is stable pinch having self-reversal phenomenon that forms reversed field of itself, but its process of formation is unstable. Therefore, in this paper, we configured the stable RFP by supplying the radio-frequency rotating field just before the RFP is configured by self-reversal phenomenon. Moreover, when conductivity wall is used, toroidal configured by self-reversal phenomenon. Moreover, when conductivity wall is used, toroidal flux is subject to heavy fluctuation in case of high bias field compared with low bias field.

• 한국전기전자재료학회논문지
• /
• 제15권8호
• /
• pp.713-719
• /
• 2002

In this study, the vertically well-aligned CNTs were synthesized by DC bias-assisted inductively coupled plasma hot-filament chemical vapor deposition (ICPHFCVD) using radio-frequence plasma of high density and that CNTs were vertically grown on Ni(300 )/Cr(200 )-deposited glass substrates at 58$0^{\circ}C$. This system(ICPHFCVD) added to tungsten filament in order to get thermal decompound and DC bias in order to vertically grow to general Inductively Coupled Plasma CVD. The grown CNTs by ICPHFCVD were developed to higher graphitization and fewer field emission properties than those by general ICPCVD. In this system, DC bias was effect of vortical alignment to growing CNTs. The measured turn-on fields of field emission property by general ICPCVD and DC bias-assisted ICPHFCVD were 5 V/${\mu}{\textrm}{m}$ and 3 V/${\mu}{\textrm}{m}$, respectively.

• Journal of Magnetics
• /
• 제10권4호
• /
• pp.133-136
• /
• 2005

The NiMn/NiFe bilayer structure which was short time annealed in order to induce unidirectional anisotropy were studied as a function of annealing temperature. The maximum exchange bias field of NiMn/NiFe bilayer was presented at $250^{\circ}C$ after short time annealing process with no external field. The appearance of exchange bias was due to phase transformation of NiMn layer. In plane angular dependence of a resonance field distribution which measured by FMR was analysed as a combined effect of unidirectional anisotropy and uniaxial anisotropy. The resonance field and the line width from FMR measurement were also analysed with annealing temperature.

• 한국자기학회지
• /
• 제13권5호
• /
• pp.198-203
• /
• 2003

경자성박막을 이용한 자기임피던스센서의 바이어스 자계 인가의 유용성을 알아보기 위해서, SmCo 경자성박막의 조성에 따른 자기적 특성과 이 박막이 아몰퍼스 CoZrNb 연자성박막에 미치는 바이어스 효과에 대하여 조사하였다. 아몰퍼스상을 가지는 SmCo 경자성박막의 포화자화는 Sm 조성이 증가함에 따라 감소하였으며, 보자력은 Sm 조성의 증가에 따라 증가하다가 28 at% 부근에서 약 500 Oe를 나타낸 후 다시 감소하였다. SmCo 박막에 의해서 발생된 바이어스 자계가 CoZrNb 박막에 미치는 효과는 자화곡선과 투자율의 측정, 그리고 자구관찰을 통하여 조사되었다. MI센서로 사용이 가능한 3${\times}$0.5 $\textrm{mm}^2$ 크기의 박막시료에 있어서, 약 60 Oe의 바이어스 자계가 얻어졌으며, 센서의 감도를 최적화하기에 충분한 바이어스 자계를 경자성박막을 이용하여 발생시킬 수 있음을 입증하였다.

• 무역학회지
• /
• 제46권1호
• /
• pp.23-38
• /
• 2021

This paper investigated the preference change of payment terms in international trade along with counteroffer or first offer conditions of the other parties. Studies on trade payment terms have mainly focused on payment term determination factors such as firm size, product price level, country credit rate, etc. We tried to find other factors affecting payment terms choice, during the negotiation process. We applied behavioral economics theories such as 'Status Quo Bias' and 'Anchoring effect' to build our research model. To prove the existence of the above effects, we proceeded with field experiments to the exporting companies in Alibaba.com. Both 'Status Quo Bias' and 'Anchoring effect' were found in the field experiment. Most of the exporting companies preferred traditional payment methods to new payment methods. And an initial request for a low advance payment ratio led to a lower advance payment ratio. Also, the experience of using new payment methods could diminish status quo bias. This paper applied behavioral economics theories and field experiment methodology to the payment term studies in international trades. These attempts could contribute to expanding the diversity of methodology and scope of international trade studies.

• Journal of Magnetics
• /
• 제16권4호
• /
• pp.453-456
• /
• 2011

Demagnetization for a tube sample which was made of a galvanized steel sheet was performed by applying a magnetic field with a decrement to remove the remanent magnetization of the material. An orthogonal fluxgate magnetic field sensor was used to measure a magnetic field created from a ferromagnetic material. To evaluate the remanent magnetization, the measured magnetic fields were separated into two magnetic field components by the remnant magnetization and the induced one. The horizontal and the vertical bias fields should be controlled separately during demagnetization to remove the horizontal and the vertical components of the remanent magnetization of the tube sample.

• Journal of Magnetics
• /
• 제15권1호
• /
• pp.17-20
• /
• 2010

The relationship between ferromagnet anisotropic magnetization and the antiferromagnet atomic spin configuration was investigated for various angles of the uniaxial deposition magnetic field of the FeMn layer in the Corning glass/Ta(5nm)/NiFe(7nm)/FeMn(25nm)/Ta(5nm) multilayer that was prepared by the ion beam sputter deposition. The exchange bias field ($H_{ex}$) obtained from the measurement of the easy-axis MR loop decreased to 40 Oe at the deposition field angle of $45^{\circ}$, and to 0 Oe at the angle of $90^{\circ}$. When the difference between the uniaxial axis between the ferromagnet NiFe and the antiferromagnet FeMn was $90^{\circ}$, the strong antiferromagnetic dipole moment of FeMn caused the weak ferromagnetic dipole moment of NiFe to rotate in the interface.