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s -wave scattering lengths for the Be7+p system from an R -matrix analysis
Paneru, S. N.,Brune, C. R.,Giri, R.,Livesay, R. J.,Greife, U.,Blackmon, J. C.,Bardayan, D. W.,Chipps, K. A.,Davids, B.,Connolly, D. S.,Chae, K. Y.,Champagne, A. E.,Deibel, C.,Jones, K. L.,Johnson, M. American Physical Society 2019 Physical Review C Vol.99 No.4
Chae, K.Y.,Ahn, S.,Ayres, A.,Bardayan, D.W.,Bey, A.,Greife, U.,Howard, M.E.,Jones, K.L.,Kozub, R.L.,Matoš,, M.,Moazen, B.H.,Nesaraja, C.D.,O’Malley, P.D.,Peters, W.A.,Pittman, S.T.,Smith, M.S. Elsevier 2018 Nuclear Instruments & Methods in Physics Research. Vol.900 No.-
<P><B>Abstract</B></P> <P>Direct measurements of ( α , p ) reactions of astrophysical interest with radioactive beams presents serious challenges because of the difficult nature of helium targets and the typical low intensities of the beams. To address this, a new technique has been developed for measurements of low-energy ( α , p ) reactions with heavy ion beams using an extended <SUP> 4 </SUP> He gas target and a newly developed gas recirculating system. The system was used to measure the <SUP> 4 </SUP> He(<SUP>19</SUP>F, <SUP> 1 </SUP> H)<SUP>22</SUP>Ne reaction as a demonstration. Excitation functions of the <SUP>19</SUP>F( α , p )<SUP>22</SUP>Ne and <SUP>19</SUP>F( α , <SUP> p ′ </SUP> )<SUP>22</SUP>Ne <SUP> ∗ </SUP> reactions were successfully measured to show the viability of this technique. Details of the approach and future plans are given.</P>
고출력 레이저 어블레이션에 의한 실리콘 가공시 발생하는 상폭발현상에 관한 연구
정성호,Yoo, J.H.,Greif, R.,Russo, R.E. 한국레이저가공학회 2000 한국레이저가공학회지 Vol.3 No.3
The volume and depth of the craters produced on silicon samples during high power laser ablation show a strong nonlinear change as the laser irradiance in closes across a threshold value, approximately 2.2X1010 W/cm². Time-resolved shadowgraph images of the ablation plume reveal the ejection of large particulates from the sample for laser irradiance above the threshold, with a time delay of about 300-400 ns. The numerically estimated thickness of the superheated liquid layer, considering the transformation of liquid metal into liquid dielectric near the critical state, agrees with the measured agrees with crater depths. It is suggested that a phase explosion of the deep superheated liquid layer near the critical state is responsible for the measured sudden increase of crater volume and the ejection of large particulates.