scholarly journals On the origin of negative target currents during laser ablation of polyethylene

2018 ◽  
Vol 167 ◽  
pp. 04006
Author(s):  
Domenico Delle Side ◽  
Anna Paola Caricato ◽  
Josef Krása ◽  
Vincenzo Nassisi

The exposure of a target to a focused laser beam results in the occurrence of a time-varying current between the target itself and the grounded vacuum chamber. This current is composed by three distinct phases, namely the ignition phase, in which the laser pulse drives the electron emission, while electrons coming from the ground through the target holder balance the positive charge generated on the target. The active phase appears at post-pulse times and it is characterized by the presence of peaked structures in the time-resolved current, representing characteristics of the target composition. Lastly, the afterglow phase is determined by a current of electrons flowing from the target to the ground. During the active phase of the target current resulting from polymers ablation with an UV KrF laser, negative target current peaks are observed, whose origin is still unknown. We investigate the dependence of these current structures on the dimensions of the target, using ultra-high molecular weight polyethylene disks of different thickness.

2017 ◽  
Vol 35 (1) ◽  
pp. 170-176 ◽  
Author(s):  
J. Krása ◽  
E. Giuffreda ◽  
D. Delle Side ◽  
V. Nassisi ◽  
D. Klír ◽  
...  

AbstractA current flowing between the ground and target exposed to the nanosecond laser radiation is analyzed to complete characteristics of laser ablation. Three phases of the target current are distinguished. During the ignition phase, the electron emission is driven by the laser pulse and the positive charge generated on the target is balanced by electrons coming from the ground through the target holder. At post-pulse times, a peaked waveform of the target current is typical for the active phase of the plasma and can give information on the material composition of the ablated surface layers. The afterglow phase is determined by a current of electrons flowing from the target to the ground. Experiment shows that the time-resolved target current is very sensitive to the actual composition of the surface layer of irradiated target and laser parameters.


SPIN ◽  
2020 ◽  
Vol 10 (01) ◽  
pp. 2050008
Author(s):  
Hai-Lin Hu ◽  
Jia-Qi Yan ◽  
Wei Li ◽  
Xiao-Yu Yang ◽  
Shi-Tao Lou ◽  
...  

Exchange bias and intrinsic Gilbert damping [Formula: see text] are two important parameters in magnetic multilayers. To explore the correlation between exchange coupling and damping, the samples Ta (2.6[Formula: see text]nm)/Pt (2.5[Formula: see text]nm)/Co[Formula: see text]Fe[Formula: see text]B[Formula: see text] (0.63[Formula: see text]nm)/Pt (0.5[Formula: see text]nm)/Mn[Formula: see text]Ir[Formula: see text] ([Formula: see text])/Ta (4[Formula: see text]nm) are deposited by using pulsed-DC magnetron sputtering. The static and dynamic magnetic responses with different thickness of antiferromagnetic MnIr are investigated using vibrating sample magnetometer (VSM) and the pump-probe time-resolved magneto-optical Kerr effect (TR-MOKE). The exchange bias initially increases and then decreases with increasing thickness of MnIr layer, which is associated with the interfacial exchange coupling. The dynamic results demonstrate that the Gilbert damping of CoFeB/Pt/MnIr can increase by up to 40% compared with CoFeB/Pt. Based on the fact that the spin pumping has been excluded because of the Pt interlayer, we attribute the enhancement in Gilbert damping to the exchange coupling between AFM and FM.


1994 ◽  
Vol 28 (2) ◽  
pp. 121-127 ◽  
Author(s):  
N. B Zhitenev ◽  
R. J Haug ◽  
K. v Klitzing ◽  
K Eberi

In a paper published in the ‘Philosophical Magazine’ of May, 1913, an account is given of some experiments which show that the raising of a cloud of dust is accompanied by the production of a large amount of electricity. The dust was usually blown away from the surface of a Hat piece of material or from the end of a tube. Large quantities of electricity were produced by this means and the sign of the charge seemed to depend upon the nature of the material used to form the dust cloud. Basic bodies generally acquired a negative charge, and acidic bodies a positive charge. It might be suggested that the origin of the charges lay in the friction of the particles of material against the surface from which they were blown, but this, however, is not altogether the case, as the following experiment will show. An insulated brass tube, 25 cm. in length and 1·5 cm. in diameter, was connected to an electroscope. Tubes of different materials and of a slightly smaller diameter were provided to fit inside it so that the nature of the surface from which the dust was blown could be varied. Under these circumstances it might be expected that the charge carried away by the dust, and also that retained by the tube, would vary with the nature of the surface, but this was not the case, for with the same substance for creating the dust, the electrification was always the same no matter what was the nature of the surface from which it was blown. For example, sand always furnished a positive charge and red lead a negative one, and other materials gave charges of the signs given in the paper referred to. Again, the nature of the surface against which the dust was projected was also without influence upon the charge acquired. Clouds of dust were raised by blowing a current of air through the dust contained in a small wash-bottle, and the cloud projected against an insulated plate connected to an electroscope. The charge gained by the plate was of the same sign whether the plate was rough or smooth, or coated with different materials, so that it appears evident that the charge is actually produced upon the dust cloud itself. It has been shown that the charge upon the dust is apparently accompanied by one of opposite sign upon the air, and a convenient arrangement for showing the presence of these two charges is given in fig. 1. The dust raised by blowing air through W is projected against the wire gauze screen G and the greater portion is caught, but the air accompanying the dust is carried on. At some distance (50-100 cm.) behind the gauze a small radium-coated plate E served to collect any charge present upon the air. Electroscopes E 2 and E 1 indicate the charges acquired by G and R. A few typical cases are given in Table I.


1995 ◽  
Vol 403 ◽  
Author(s):  
Silva K. Theiss ◽  
J. A. Prybyla

AbstractWe have performed time-resolved studies of the electromigration (EM) – induced formation, growth, migration, and spatial distribution of Al2Cu precipitates in submicron Al(0.5 wt. % Cu) runners. Of particular interest is the formation of the precipitates in relationship to the local microstructure of the runners, and the formation of voids and hillocks with respect to the location of the Al2Cu precipitates. Runners of widths 0.3, 0.5, 0.8, and 1.0 ýtm were tested at a current density of 2×106 A/cm2 and temperatures between 200 and 300°C. The evolution of the microstructure of the runners was evaluated using plan-view TEM, SEM, and EDX. The formation of voids and hillocks, and the growth of precipitates proceeds more rapidly as the width of the runners increases. However, a far greater number of precipitates nucleate in the 0.3 μm-wide line than in any of the others. As expected, voids are most likely to form near the cathode and hillocks near the anode. Large Al2Cu precipitates form near the anode long before failure occurs. Interestingly, the cathode-side bonding pad is not observed to serve as a good reservoir of Cu for the runners. Although the formation of voids near the cathode seems to be associated with the depletion of Cu in this region, hillocks and voids elsewhere are more likely to form at precipitates than in other parts of the line. Thus Al2Cu precipitates can act as sites for preferential EM-damage, reducing interconnect reliability.


Polymer ◽  
2004 ◽  
Vol 45 (16) ◽  
pp. 5641-5652 ◽  
Author(s):  
A. Mahendrasingam ◽  
D.J. Blundell ◽  
A.K. Wright ◽  
V. Urban ◽  
T. Narayanan ◽  
...  

2021 ◽  
Vol 217 (3) ◽  
Author(s):  
S. Maurice ◽  
R. C. Wiens ◽  
P. Bernardi ◽  
P. Caïs ◽  
S. Robinson ◽  
...  

AbstractOn the NASA 2020 rover mission to Jezero crater, the remote determination of the texture, mineralogy and chemistry of rocks is essential to quickly and thoroughly characterize an area and to optimize the selection of samples for return to Earth. As part of the Perseverance payload, SuperCam is a suite of five techniques that provide critical and complementary observations via Laser-Induced Breakdown Spectroscopy (LIBS), Time-Resolved Raman and Luminescence (TRR/L), visible and near-infrared spectroscopy (VISIR), high-resolution color imaging (RMI), and acoustic recording (MIC). SuperCam operates at remote distances, primarily 2–7 m, while providing data at sub-mm to mm scales. We report on SuperCam’s science objectives in the context of the Mars 2020 mission goals and ways the different techniques can address these questions. The instrument is made up of three separate subsystems: the Mast Unit is designed and built in France; the Body Unit is provided by the United States; the calibration target holder is contributed by Spain, and the targets themselves by the entire science team. This publication focuses on the design, development, and tests of the Mast Unit; companion papers describe the other units. The goal of this work is to provide an understanding of the technical choices made, the constraints that were imposed, and ultimately the validated performance of the flight model as it leaves Earth, and it will serve as the foundation for Mars operations and future processing of the data.


2021 ◽  
Author(s):  
Manisha Yadav ◽  
Michael Skinner ◽  
Rukmini Reddy ◽  
Matthew Wong ◽  
Kevin Chon ◽  
...  

<p>A fast (~5 min), time-resolved fluorescence resonance energy transfer based immunoassay (Procise FCP<a>™</a>) was developed for the point-of-care quantitative detection of fecal calprotectin (FCP) using 15 mg of fecal specimen eluted in collection fluid from the Procise Stool Collection Device™. Studies were performed to characterize analytical performance of the Procise FCP assay on the ProciseDx™ analyzer.</p><p><br></p> <p>The Procise FCP assay showed good analytical performance with respect to sensitivity, specificity, linearity, and precision suitable for routine clinical use in a point-of-care setting as well as excellent analytical agreement with a current commercial FCP measurement method.</p><p><br></p> <p>Results indicate that the Procise FCP assay is sensitive, specific, and precise yielding results in less than 5 minutes. This indicates the Procise FCP assay is useful for obtaining fast and accurate FCP quantitation, thus avoiding delays inherent to current methods and enabling immediate clinical assessment to be made during a single patient visit.</p>


2021 ◽  
Author(s):  
Manisha Yadav ◽  
Michael Skinner ◽  
Rukmini Reddy ◽  
Matthew Wong ◽  
Kevin Chon ◽  
...  

<p>A fast (~5 min), time-resolved fluorescence resonance energy transfer based immunoassay (Procise FCP<a>™</a>) was developed for the point-of-care quantitative detection of fecal calprotectin (FCP) using 15 mg of fecal specimen eluted in collection fluid from the Procise Stool Collection Device™. Studies were performed to characterize analytical performance of the Procise FCP assay on the ProciseDx™ analyzer.</p><p><br></p> <p>The Procise FCP assay showed good analytical performance with respect to sensitivity, specificity, linearity, and precision suitable for routine clinical use in a point-of-care setting as well as excellent analytical agreement with a current commercial FCP measurement method.</p><p><br></p> <p>Results indicate that the Procise FCP assay is sensitive, specific, and precise yielding results in less than 5 minutes. This indicates the Procise FCP assay is useful for obtaining fast and accurate FCP quantitation, thus avoiding delays inherent to current methods and enabling immediate clinical assessment to be made during a single patient visit.</p>


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