Organic Glass Scintillators

Author(s):  
Patrick L. Feng ◽  
Nicholas R. Myllenbeck ◽  
Joseph S. Carlson
Keyword(s):  
Author(s):  
A. C. Faberge

Benzylamine tartrate (m.p. 63°C) seems to be a better and more convenient substrate for making carbon films than any of those previously proposed. Using it in the manner described, it is easy consistently to make batches of specimen grids as open as 200 mesh with no broken squares, and without individual handling of the grids. Benzylamine tartrate (hereafter called B.T.) is a viscous liquid when molten, which sets to a glass. Unlike polymeric substrates it does not swell before dissolving; such swelling of the substrate seems to be a principal cause of breakage of carbon film. Mass spectroscopic examination indicates a vapor pressure less than 10−9 Torr at room temperature.


Polymers ◽  
2021 ◽  
Vol 13 (2) ◽  
pp. 294
Author(s):  
Helena Švajdlenková ◽  
Ondrej Šauša ◽  
Sergey V. Adichtchev ◽  
Nikolay V. Surovtsev ◽  
Vladimir N. Novikov ◽  
...  

We report on the reorientation dynamics of small spin probe 2,2,6,6-tetramethylpiperidinyl-1-oxyl (TEMPO) in cis-1,4-poly(isoprene) (cis-1,4-PIP10k) from electron spin resonance (ESR) and the free volume of cis-1,4-PIP10k from positron annihilation lifetime spectroscopy (PALS) in relation to the high-frequency relaxations of cis-1,4-PIP10k using light scattering (LS) as well as to the slow and fast processes from broadband dielectric spectroscopy (BDS) and neutron scattering (NS). The hyperfine coupling constant, 2Azz′(T), and the correlation times, τc(T), of cis-1,4-PIP10k/TEMPO system as a function of temperature exhibit several regions of the distinct spin probe TEMPO dynamics over a wide temperature range from 100 K up to 350 K. The characteristic ESR temperatures of changes in the spin probe dynamics in cis-1,4-PIP10k/TEMPO system are closely related to the characteristic PALS ones reflecting changes in the free volume expansion from PALS measurement. Finally, the time scales of the slow and fast dynamics of TEMPO in cis-1,4-PIP10k are compared with all of the six known slow and fast relaxation modes from BDS, LS and NS techniques with the aim to discuss the controlling factors of the spin probe reorientation mobility in polymer, oligomer and small molecular organic glass-formers.


2013 ◽  
Vol 102 (3) ◽  
pp. 031912 ◽  
Author(s):  
Qiuyun Ouyang ◽  
Hailong Yu ◽  
Zheng Xu ◽  
Yue Zhang ◽  
Chunyan Li ◽  
...  

2012 ◽  
Vol 48 (11) ◽  
pp. 1638-1640 ◽  
Author(s):  
Tanja Gnutzmann ◽  
Klaus Rademann ◽  
Franziska Emmerling
Keyword(s):  

2012 ◽  
Vol 22 (7) ◽  
pp. 2848 ◽  
Author(s):  
Brian T. Makowski ◽  
Brent Valle ◽  
Kenneth D. Singer ◽  
Christoph Weder

2008 ◽  
Vol 130 (3) ◽  
Author(s):  
J. Y. Chen ◽  
H. L. Chen ◽  
E. Pan

Reflection and transmission coefficients of plane waves with oblique incidence to a multilayered system of piezomagnetic and/or piezoelectric materials are investigated in this paper. The general Christoffel equation is derived from the coupled constitutive and balance equations, which is further employed to solve the elastic displacements and electric and magnetic potentials. Based on these solutions, the reflection and transmission coefficients in the corresponding layered structures are subsequently obtained by virtue of the propagator matrix method. Two layered examples are selected to verify and illustrate our solutions. One is the purely elastic layered system composed of aluminum and organic glass materials. The other layered system is composed of the novel magnetoelectroelastic material and the organic glass. Numerical results are presented to demonstrate the variation of the reflection and transmission coefficients with different incident angles, frequencies, and boundary conditions, which could be useful to nondestructive evaluation of this novel material structure based on wave propagations.


2020 ◽  
pp. 2049-2089
Author(s):  
Sushmit Goyal ◽  
Hyunhang Park ◽  
Sung Hoon Lee ◽  
Mathew McKenzie ◽  
Aravind Rammohan ◽  
...  
Keyword(s):  

2010 ◽  
Vol 105 (21) ◽  
Author(s):  
M. Sikorski ◽  
C. Gutt ◽  
Y. Chushkin ◽  
M. Lippmann ◽  
H. Franz

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