• 한국자기학회지
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• 제25권1호
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• pp.22-26
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• 2015

이 논문에서 Ni-Zn 페라이트 코어와 칩캐패시터를 이용하여 제작한 주기적인 연결구조에서 발생하는 자기유도파(magneto-inductive wave)에 대한 실험적 결과를 보고 한다. 주기적 연결구조는 동일한 공진주파수를 가진 LC공진기(LC resonator)로 되었으며, 개별 공진기는 도선과 칩캐패시터로 구성되었다. 인접하는 공진기들은 패라이트코어를 통해서 자기적으로 결합되었다. 제작된 주기적 구조의 특성을 검토하기 위해서 네트워크 아날라이저를 이용한 S-파라미터를 분석하여 신호전송특성을 평가하였다. 5개의 LC공진기를 1차원적으로 연결하여 제작한 주기구조의 신호전송 중심주파수는 32 MHz~38 MHz였으며, 이는 인가자계의 크기에 의해서 조정할 수 있었다.

• 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.