Combining SAXS and DLS for simultaneous measurements and time-resolved monitoring of nanoparticle synthesis

Author(s):  
A. Schwamberger ◽  
B. De Roo ◽  
D. Jacob ◽  
L. Dillemans ◽  
L. Bruegemann ◽  
...  
1998 ◽  
Vol 72 (23) ◽  
pp. 2987-2989 ◽  
Author(s):  
David B. Geohegan ◽  
Alex A. Puretzky ◽  
Gerd Duscher ◽  
Stephen J. Pennycook

1981 ◽  
Vol 4 ◽  
Author(s):  
Dae M. Kim ◽  
Rajiv R. Shah ◽  
D. Von Der Linde ◽  
D.L. Crosthwait

ABSTRACTWe report simultaneous measurements of time resolved reflection and transmission of low intensity 1.06 μm, 35 ps pulses subsequent to excitation of 50 KeV, 1016 cm−2 boron implanted silicon by 0.53 μm 35 ps pulses of varying energy densities. The samples are examined by optical and scanning electron microscopy in conjunction with defect etching. These data are discussed from the point of view of both the thermal melting model and plasma model.


2021 ◽  
Vol 33 (11) ◽  
pp. 115101
Author(s):  
Wenwu Zhou ◽  
Xu Zhang ◽  
Chuangxin He ◽  
Xin Wen ◽  
Jisheng Zhao ◽  
...  

1986 ◽  
Vol 4 (3-4) ◽  
pp. 495-498 ◽  
Author(s):  
W. Lampart ◽  
J. E. Balmer

High-temperature plasmas were produced by focusing 1·05 μm, 100 psec laser pulses onto Al layer targets at a mean irradiation of 3·1013 Watt/cm2. By means of simultaneous measurements of the thermal x-ray emission and the frequency-quadrupled laser pulse we observe a 20 ± 15 psec delay of the x-ray peak relative to the peak of the incident laser pulse. In addition, modulations on the trailing edge of the driving pulse appear strongly enhanced in the x-ray signature.


Author(s):  
Eva-Maria Mandelkow ◽  
Eckhard Mandelkow ◽  
Joan Bordas

When a solution of microtubule protein is changed from non-polymerising to polymerising conditions (e.g. by temperature jump or mixing with GTP) there is a series of structural transitions preceding microtubule growth. These have been detected by time-resolved X-ray scattering using synchrotron radiation, and they may be classified into pre-nucleation and nucleation events. X-ray patterns are good indicators for the average behavior of the particles in solution, but they are difficult to interpret unless additional information on their structure is available. We therefore studied the assembly process by electron microscopy under conditions approaching those of the X-ray experiment. There are two difficulties in the EM approach: One is that the particles important for assembly are usually small and not very regular and therefore tend to be overlooked. Secondly EM specimens require low concentrations which favor disassembly of the particles one wants to observe since there is a dynamic equilibrium between polymers and subunits.


Author(s):  
David C. Joy

Electron channeling patterns (ECP) were first found by Coates (1967) while observing a large bulk, single crystal of silicon in a scanning electron microscope. The geometric pattern visible was shown to be produced as a result of the changes in the angle of incidence, between the beam and the specimen surface normal, which occur when the sample is examined at low magnification (Booker, Shaw, Whelan and Hirsch 1967).A conventional electron diffraction pattern consists of an angularly resolved intensity distribution in space which may be directly viewed on a fluorescent screen or recorded on a photographic plate. An ECP, on the other hand, is produced as the result of changes in the signal collected by a suitable electron detector as the incidence angle is varied. If an integrating detector is used, or if the beam traverses the surface at a fixed angle, then no channeling contrast will be observed. The ECP is thus a time resolved electron diffraction effect. It can therefore be related to spatially resolved diffraction phenomena by an application of the concepts of reciprocity (Cowley 1969).


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