• 제목/요약/키워드: Fast electrons

검색결과 46건 처리시간 0.019초

산소결핍 페롭스카이트 La1/3Sr2/3FeO2.96의 외부 자기장 하에서의 Mössbauer분광학적 연구 ([Mössbauer] Spectroscopic Study of La1/3Sr2/3FeO2.96 under the External Magnetic Field)

  • 윤성현;정종용
    • 한국자기학회지
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    • 제15권2호
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    • pp.81-84
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    • 2005
  • 다결정성 $La_{1/3}Sr_{2/3}FeO_{2.96}$에서의 전하불균형(charge disproportionation, CD) 전이의 근원에 대해 x선 회절법과 외부장 $M\ddot{o}ssbauer$ 분광법을 이용하여 알아보았다. 전이온도 이상에서 외부 자기장에 의한 효과를 알아보기 위해 시료의 온도를 225K로 유지한 상태에서 6 T이하의 외부 자기장을 감마선의 진행방향에 대해 각각 수직과 수평으로 걸어주었다. 외부장이 없을 경우 평균원자가 $Fe^{3.6+}$에 기인하는 상자성 단일 흡수선이 나타났다. 자기장이 감마선의 방향과 평행할 경우, 면적비가 3:0:1:1:0:3인 자기적 Zeeman 스펙트럼이 중앙의 단일선(singlet)에 중첩되어 나타났다. 하지만 자기장이 감마선의 방향에 수직일 경우엔 중앙의 단일선은 사라지고 면적비 3:4:1:1:4:3인 6-선 스펙트럼만 나타나서 큰 이방성을 보였다. 외부장 하에서 단일 흡수선의 존재는 Fe 이온간의 전자의 재빠른 도약 현상으로 설명하였다. 외부장 하에서도 단일흡수선이 존재해, 자기장이 전자의 도약에 의한 전도메커니즘에 큰 영향을 주지 못하는 것으로 나타났다.

${\iota}$-Sparteine의 전기화학적 산화반응에 대한 메카니즘의 연구 (Mechanistic Studies for Electrochemical Oxidation of ${\iota}$-Sparteine)

  • 박진효;진창수;최성락;심윤보
    • 대한화학회지
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    • 제37권8호
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    • pp.711-716
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    • 1993
  • 천연 알칼로이드의 하나인 ${\iota}$-sparteine (SP)의 전기화학적 산화반응을 아세토니트릴 용액 중에서 조사하였다. SP의 순환전압전류그림(CV)은 Ag/AgCl (0.1M AgNO$_3$ in acetonitrile) 전극에 대하여 +0.75 V and +1.45 V에서 두 개의 비가역적 산화봉우리를 나타내었다. 두 과정은 각각 약 1.2~1.3개의 전자반응에 해당함을 전기량법을 이용하여 확인하였다. SP 의 첫 단계산화는 SP의 질소원자 하나가 산화되어 SP 라디칼 양이온을 형성하고, 라디칼 양이온은 뒤 이은 빠른 탈수소반응에 의하여 중성의 이민 라디칼을 형성한다. 이 중성 라디칼은 두 가지 반응 경로가 가능하다:대부분의 중성 라디칼은 불균등화 반응에 의하여 SP와 엔아민으로 된다. 또한 일부의 중성 라디칼은 다시 일전자 산화반응에 의해 1,2-dehydrosparteinium 양이온을 생성하게 된다. 이 양이온을 KOH로 처리하면 (+)-lupanine으로 된다. SP를 전기분해하여 얻은 생성물들을 분리한 후 적외선분광법, 질량분석법, 자외선-가시광선 분광법 및 얇은 막 전기분광화학법을 이용하여 확인하였다.

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프리스탠딩 저항형 가스 센서용 산화구리 무전해 도금 탄소스펀지 제조 및 일산화질소 감지 (Fabrication of Copper(II) Oxide Plated Carbon Sponge for Free-standing Resistive Type Gas Sensor and Its Application to Nitric Oxide Detection)

  • 김석진;하성민;명성재;이영석
    • 공업화학
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    • 제33권6호
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    • pp.630-635
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    • 2022
  • 멜라민 스펀지를 열처리하여 제조된 질소함유 탄소 스펀지에 산화구리(CuO)를 무전해 도금하여 기판없이 작동하는 일산화질소(NO) 가스 센서를 제조하였다. 탄소 스펀지 표면의 CuO 함량은 도금 시간이 증가함에 따라 증가하였으나, NO 가스 흡착을 유도한다고 알려져 있는 질소의 함량은 CuO 표면 함량이 증가함에 따라 감소하였다. 미처리 탄소스펀지는 NO 가스에 대하여 18 min에 최대 저항 변화(5.0%)를 나타내었다. 반면에, CuO가 도금된 샘플(CuO30s-CS)은 8 min만에 최대 18.3%의 저항변화를 보였다. 이러한 NO 가스 감지 능력 향상은 CuO로 인하여 탄소 스펀지의 정공 캐리어 수 증가 및 전자전달 촉진에 기인하는 것으로 판단된다. 그러나, 60 s 동안 CuO 무전해 도금된 탄소 스펀지의 NO가스 감지 저항은 1.9%로 오히려 감소하였다. 이는 탄소 스펀지 표면에 CuO로 완전히 도금되어 NO 가스 흡착 능력이 떨어져 저항변화가 감소한 것으로 판단된다. 따라서, CuO가 도금된 탄소 스펀지는 빠르고 우수한 저항변화 특성을 가지고 있어 유용한 NO 가스 센서로 사용할 수 있으나, CuO가 탄소 스펀지 표면을 완전히 도금해서는 안 된다.

Improvement of lower hybrid current drive systems for high-power and long-pulse operation on EAST

  • M. Wang;L. Liu;L.M. Zhao;M.H. Li ;W.D. Ma;H.C. Hu ;Z.G. Wu;J.Q. Feng ;Y. Yang ;L. Zhu ;M. Chen ;T.A. Zhou;H. Jia;J. Zhang ;L. Cao ;L. Zhang ;R.R. Liang;B.J. Ding ;X.J. Zhang ;J.F. Shan;F.K. Liu ;A. Ekedahl ;M. Goniche ;J. Hillairet;L. Delpech
    • Nuclear Engineering and Technology
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    • 제54권11호
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    • pp.4102-4110
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    • 2022
  • Aiming at high-power and long-pulse operation up to 1000 s, some improvements have been made for both 2.45 GHz and 4.6 GHz lower hybrid (LH) systems during the recent 5 years. At first, the guard limiters of the LH antennas with graphite tiles were upgraded to tungsten, the most promising material for plasma facing components in nuclear fusion devices. These new guard limiters can operate at a peak power density of 12.9 MW/m2. Strong hot spots were usually observed on the old graphite limiters when 4.6 GHz system operated with power >2.0 MW [B. N. Wan et al., Nucl. Fusion 57 (2017) 102019], leading to a reduction of the maximum power capability. With the new limiters, 4.6 GHz LH system, the main current drive (CD) and electron heating tool for EAST, can be operated with power >2.5 MW routinely. Long-pulse operation up to 100 s with 4.6 GHz LH power of 2.4 MW was achieved in 2021 and the maximal temperature on the guard limiters measured by an infrared (IR) camera was about 540 ℃, much below the permissible value of tungsten material (~1200 ℃). A discharge with a duration of 1056 s was achieved and the 4.6 GHz LH energy injected into the plasma was up to 1.05 GJ. Secondly, the fully-active-multijunction (FAM) launcher of 2.45 GHz system was upgraded to a passive-active-multijunction (PAM), for which the density of optimum coupling was relatively low (below the cut-off value). Good coupling with reflection coefficient ~3% has been achieved with plasma-antenna distance up to 11 cm for the new PAM. Finally, in order to eliminate the effect of ion cyclotron range of frequencies (ICRF) wave on 4.6 GHz LH wave coupling, the location of the ICRF launcher was changed to a port that is located 157.5° toroidally from the 4.6 GHz LH system and is not magnetically connected.

Lead-free inorganic metal perovskites beyond photovoltaics: Photon, charged particles and neutron shielding applications

  • Srilakshmi Prabhu;Dhanya Y. Bharadwaj;S.G. Bubbly;S.B. Gudennavar
    • Nuclear Engineering and Technology
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    • 제55권3호
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    • pp.1061-1070
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    • 2023
  • Over the last few years, lead-free inorganic metal perovskites have gained impressive ground in empowering satellites in space exploration owing to their material stability and performance evolution under extreme space environments. The present work has examined the versatility of eight such perovskites as space radiation shielding materials by computing their photon, charged particles and neutron interaction parameters. Photon interaction parameters were calculated for a wide energy range using PAGEX software. The ranges of heavy charged particles (H, He, C, N, O, Ne, Mg, Si and Fe ions) in these perovskites were estimated using SRIM software in the energy range 1 keV-10 GeV, and that of electrons was computed using ESTAR NIST software in the energy range 0.01 MeV-1 GeV. Further, the macroscopic fast neutron removal cross-sections were also calculated to estimate the neutron shielding efficiencies. The examined shielding parameters of the perovskites varied depending on the radiation type and energy. Among the selected perovskites, Cs2TiI6 and Ba2AgIO6 displayed superior photon attenuation properties. A 3.5 cm thick Ba2AgIO6-based shield could reduce the incident radiation intensity to half its initial value, a thickness even lesser than that of Pb-glass. Besides, CsSnBr3 and La0.8Ca0.2Ni0.5Ti0.5O3 displayed the highest and lowest range values, respectively, for all heavy charged particles. Ba2AgIO6 showed electron stopping power (on par with Kovar) better than that of other examined materials. Interestingly, La0.8Ca0.2Ni0.5Ti0.5O3 demonstrated neutron removal cross-section values greater than that of standard neutron shielding materials - aluminium and polyethylene. On the whole, the present study not only demonstrates the employment prospects of eco-friendly perovskites for shielding space radiations but also suggests future prospects for research in this direction.

THE CURRENT STATUS OF BIOMEDICAL ENGINEERING IN THE USA

  • Webster, John G.
    • 대한의용생체공학회:학술대회논문집
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    • 대한의용생체공학회 1992년도 춘계학술대회
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    • pp.27-47
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    • 1992
  • Engineers have developed new instruments that aid in diagnosis and therapy Ultrasonic imaging has provided a nondamaging method of imaging internal organs. A complex transducer emits ultrasonic waves at many angles and reconstructs a map of internal anatomy and also velocities of blood in vessels. Fast computed tomography permits reconstruction of the 3-dimensional anatomy and perfusion of the heart at 20-Hz rates. Positron emission tomography uses certain isotopes that produce positrons that react with electrons to simultaneously emit two gamma rays in opposite directions. It locates the region of origin by using a ring of discrete scintillation detectors, each in electronic coincidence with an opposing detector. In magnetic resonance imaging, the patient is placed in a very strong magnetic field. The precessing of the hydrogen atoms is perturbed by an interrogating field to yield two-dimensional images of soft tissue having exceptional clarity. As an alternative to radiology image processing, film archiving, and retrieval, picture archiving and communication systems (PACS) are being implemented. Images from computed radiography, magnetic resonance imaging (MRI), nuclear medicine, and ultrasound are digitized, transmitted, and stored in computers for retrieval at distributed work stations. In electrical impedance tomography, electrodes are placed around the thorax. 50-kHz current is injected between two electrodes and voltages are measured on all other electrodes. A computer processes the data to yield an image of the resistivity of a 2-dimensional slice of the thorax. During fetal monitoring, a corkscrew electrode is screwed into the fetal scalp to measure the fetal electrocardiogram. Correlations with uterine contractions yield information on the status of the fetus during delivery To measure cardiac output by thermodilution, cold saline is injected into the right atrium. A thermistor in the right pulmonary artery yields temperature measurements, from which we can calculate cardiac output. In impedance cardiography, we measure the changes in electrical impedance as the heart ejects blood into the arteries. Motion artifacts are large, so signal averaging is useful during monitoring. An intraarterial blood gas monitoring system permits monitoring in real time. Light is sent down optical fibers inserted into the radial artery, where it is absorbed by dyes, which reemit the light at a different wavelength. The emitted light travels up optical fibers where an external instrument determines O2, CO2, and pH. Therapeutic devices include the electrosurgical unit. A high-frequency electric arc is drawn between the knife and the tissue. The arc cuts and the heat coagulates, thus preventing blood loss. Hyperthermia has demonstrated antitumor effects in patients in whom all conventional modes of therapy have failed. Methods of raising tumor temperature include focused ultrasound, radio-frequency power through needles, or microwaves. When the heart stops pumping, we use the defibrillator to restore normal pumping. A brief, high-current pulse through the heart synchronizes all cardiac fibers to restore normal rhythm. When the cardiac rhythm is too slow, we implant the cardiac pacemaker. An electrode within the heart stimulates the cardiac muscle to contract at the normal rate. When the cardiac valves are narrowed or leak, we implant an artificial valve. Silicone rubber and Teflon are used for biocompatibility. Artificial hearts powered by pneumatic hoses have been implanted in humans. However, the quality of life gradually degrades, and death ensues. When kidney stones develop, lithotripsy is used. A spark creates a pressure wave, which is focused on the stone and fragments it. The pieces pass out normally. When kidneys fail, the blood is cleansed during hemodialysis. Urea passes through a porous membrane to a dialysate bath to lower its concentration in the blood. The blind are able to read by scanning the Optacon with their fingertips. A camera scans letters and converts them to an array of vibrating pins. The deaf are able to hear using a cochlear implant. A microphone detects sound and divides it into frequency bands. 22 electrodes within the cochlea stimulate the acoustic the acoustic nerve to provide sound patterns. For those who have lost muscle function in the limbs, researchers are implanting electrodes to stimulate the muscle. Sensors in the legs and arms feed back signals to a computer that coordinates the stimulators to provide limb motion. For those with high spinal cord injury, a puff and sip switch can control a computer and permit the disabled person operate the computer and communicate with the outside world.

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